[go: up one dir, main page]
More Web Proxy on the site http://driver.im/
You seem to have javascript disabled. Please note that many of the page functionalities won't work as expected without javascript enabled.
 
 
molecules-logo

Journal Browser

Journal Browser

Exclusive Feature Papers in Inorganic Chemistry, 2nd Edition

A special issue of Molecules (ISSN 1420-3049). This special issue belongs to the section "Inorganic Chemistry".

Deadline for manuscript submissions: 31 December 2024 | Viewed by 51097

Special Issue Editors


E-Mail Website
Guest Editor
Department of Chemistry, University of Florence, Via della Lastruccia, 3-13, 50019 Sesto Fiorentino, Firenze, Italy
Interests: synthetic inorganic chemistry; coordination chemistry; polyamine ligands; anion coordination; supramolecular chemistry; weak interactions; coordination of toxic metals and anions; reactive oxygen species (ROS); ROS generation/scavenging by metals and their complexes
Special Issues, Collections and Topics in MDPI journals

E-Mail Website
Guest Editor
Dipartimento di Scienze Chimiche e Geologiche, Università degli Studi di Cagliari, Cagliari, Italy
Interests: coordination chemistry of macrocyclic ligands; fluorescent molecular sensors for metal ion and anions; selenium and tellurium containing molecules; crystal engineering; coordination polymers
Special Issues, Collections and Topics in MDPI journals

Special Issue Information

Dear Colleagues,

It is our pleasure to announce a new Special Issue entitled “Exclusive Feature Papers in Inorganic Chemistry, 2nd Edition”. This is a collection of important high-quality papers (original research articles or comprehensive review papers) published in open access format by Editorial Board Members or prominent scholars invited by the Editorial Office and the Guest Editors. This Special Issue aims to discuss new knowledge or new cutting-edge developments in the inorganic chemistry research field through selected works, in the hope of making a great contribution to the community. We intend for this Issue to be the best forum for disseminating excellent research findings as well as sharing innovative ideas in the field.

Dr. Andrea Bencini
Prof. Dr. Vito Lippolis
Guest Editors

Manuscript Submission Information

Manuscripts should be submitted online at www.mdpi.com by registering and logging in to this website. Once you are registered, click here to go to the submission form. Manuscripts can be submitted until the deadline. All submissions that pass pre-check are peer-reviewed. Accepted papers will be published continuously in the journal (as soon as accepted) and will be listed together on the special issue website. Research articles, review articles as well as short communications are invited. For planned papers, a title and short abstract (about 100 words) can be sent to the Editorial Office for announcement on this website.

Submitted manuscripts should not have been published previously, nor be under consideration for publication elsewhere (except conference proceedings papers). All manuscripts are thoroughly refereed through a single-blind peer-review process. A guide for authors and other relevant information for submission of manuscripts is available on the Instructions for Authors page. Molecules is an international peer-reviewed open access semimonthly journal published by MDPI.

Please visit the Instructions for Authors page before submitting a manuscript. The Article Processing Charge (APC) for publication in this open access journal is 2700 CHF (Swiss Francs). Submitted papers should be well formatted and use good English. Authors may use MDPI's English editing service prior to publication or during author revisions.

Benefits of Publishing in a Special Issue

  • Ease of navigation: Grouping papers by topic helps scholars navigate broad scope journals more efficiently.
  • Greater discoverability: Special Issues support the reach and impact of scientific research. Articles in Special Issues are more discoverable and cited more frequently.
  • Expansion of research network: Special Issues facilitate connections among authors, fostering scientific collaborations.
  • External promotion: Articles in Special Issues are often promoted through the journal's social media, increasing their visibility.
  • e-Book format: Special Issues with more than 10 articles can be published as dedicated e-books, ensuring wide and rapid dissemination.

Further information on MDPI's Special Issue polices can be found here.

Published Papers (36 papers)

Order results
Result details
Select all
Export citation of selected articles as:

Research

Jump to: Review

14 pages, 2097 KiB  
Article
Synthesis and Characterization of Novel Co(III)/Ru(II) Heterobimetallic Complexes as Hypoxia-Activated Iron-Sequestering Anticancer Prodrugs
by Tan Ba Tran, Éva Sipos, Attila Csaba Bényei, Sándor Nagy, István Lekli and Péter Buglyó
Molecules 2024, 29(24), 5967; https://doi.org/10.3390/molecules29245967 - 18 Dec 2024
Viewed by 250
Abstract
Heterobimetallic complexes of an ambidentate deferiprone derivative, 3-hydroxy-2-methyl-1-(3-((pyridin-2-ylmethyl)amino)propyl)pyridin-4(1H)-one (PyPropHpH), incorporating an octahedral [Co(4N)]3+ (4N = tris(2-aminoethyl)amine (tren) or tris(2-pyridylmethyl)amine (tpa)) and a half-sandwich type [(η6-p-cym)Ru]2+ (p-cym = p-cymene) entity have been synthesized and characterized [...] Read more.
Heterobimetallic complexes of an ambidentate deferiprone derivative, 3-hydroxy-2-methyl-1-(3-((pyridin-2-ylmethyl)amino)propyl)pyridin-4(1H)-one (PyPropHpH), incorporating an octahedral [Co(4N)]3+ (4N = tris(2-aminoethyl)amine (tren) or tris(2-pyridylmethyl)amine (tpa)) and a half-sandwich type [(η6-p-cym)Ru]2+ (p-cym = p-cymene) entity have been synthesized and characterized by various analytical techniques. The reaction between PyPropHpH and [Co(4N)Cl]Cl2 resulted in the exclusive (O,O) coordination of the ligand to Co(III) yielding [Co(tren)PyPropHp](PF6)2 (1) and [Co(tpa)PyPropHp](PF6)2 (2). This binding mode was further supported by the molecular structure of [Co(tpa)PyPropHp]2(ClO4)3(OH)·6H2O (5) and [Co(tren)PyPropHpH]Cl(PF6)2·2H2O·C2H5OH (6), respectively, obtained via the slow evaporation of the appropriate reaction mixtures and analyzed using X-ray crystallography. Subsequent treatment of 1 or 2 with [Ru(η6-p-cym)Cl2]2 in a one-pot reaction afforded the corresponding heterobimetallic complexes, [Co(tren)PyPropHp(η6-p-cym)RuCl](PF6)3 (3) and [Co(tpa)PyPropHp(η6-p-cym)RuCl](PF6)3 (4), in which the piano-stool Ru core is coordinated by the (N,N) chelating set of the ligand. Cyclic voltammetric measurements revealed that the tpa complexes can be reduced at less negative potentials, suggesting their capability to be bioreductively activated under hypoxia (1% O2). Hypoxia activation of 2 and 4 was demonstrated by cytotoxicity studies on the MCF-7 human breast cancer cell line. PyPropHpH was shown to be a typical iron-chelating anticancer agent, raising the mRNA levels of TfR1, Ndrg1 and p21. Further qRT-PCR studies provided unambiguous evidence for the bioreduction of 2 after 72 h incubation under hypoxia, in which the characteristic gene induction profile caused by the liberated iron-sequestering PyPropHpH was observed. Full article
(This article belongs to the Special Issue Exclusive Feature Papers in Inorganic Chemistry, 2nd Edition)
Show Figures

Figure 1

Figure 1
<p>Structural formulas of the studied and model ligands as well as the metal building blocks.</p>
Full article ">Figure 2
<p>Ortep view of the molecular structure of [Co(tren)(PyPropHpH)]<sup>3+</sup> (<b>top</b>) and [Co(tpa)(PyPropHp)]<sup>2+</sup> (<b>bottom</b>) cations. The anions and solvent molecules are omitted for clarity.</p>
Full article ">Figure 3
<p>(<b>A</b>) Cell viability after 72 h treatment of PyPropHpH under normoxia (black) and hypoxia (gray). (<b>B</b>) Cell viability after 72 h treatment with the complexes under normoxia (black) and hypoxia (gray). Data points are presented as mean (SD). Multiple paired <span class="html-italic">t</span> test and Holm–Šidák post hoc test were used to analyze the data. Significance level: ns: <span class="html-italic">p</span> &gt; 0.05, *: <span class="html-italic">p</span> ≤ 0.05, **: <span class="html-italic">p</span> ≤ 0.01, ***: <span class="html-italic">p</span> ≤ 0.001, ****: <span class="html-italic">p</span> ≤ 0.0001.</p>
Full article ">Figure 4
<p>Gene expression level changes calculated by 2<sup>40-ct</sup> method after (<b>A</b>) 24 h treatment with PyPropHpH, (<b>B</b>) 24 h treatment with PyPropHpH and <b>2</b> at 200 μM and (<b>C</b>) 72 h treatment with PyPropHpH and <b>2</b> at 100 μM under normoxia (black) and hypoxia (gray). Data points are presented as mean (SD). Two-way ANOVA for (<b>A</b>,<b>B</b>) and one-way ANOVA for (<b>C</b>) followed by Dunett’s post hoc test for (<b>A</b>) and Tukey’s post hoc test for (<b>B</b>,<b>C</b>) were used to analyze the data. Significance level: ns: <span class="html-italic">p</span> &gt; 0.05, *: <span class="html-italic">p</span> ≤ 0.05, **: <span class="html-italic">p</span> ≤ 0.01, ***: <span class="html-italic">p</span> ≤ 0.001, ****: <span class="html-italic">p</span> ≤ 0.0001.</p>
Full article ">Scheme 1
<p>Synthetic procedure of the Co(III) complexes and Co(III)/Ru(II) heterobimetallic complexes. The structures of Co(III)-based geometric isomers are shown. Stereogenic centers are denoted with *.</p>
Full article ">
17 pages, 2438 KiB  
Article
Synthesis and Characterisation of Phosphino-Aryloxide Rare Earth Complexes
by Elias Alexopoulos, Yu Liu, Alex W. J. Bowles, Benjamin L. L. Réant and Fabrizio Ortu
Molecules 2024, 29(23), 5757; https://doi.org/10.3390/molecules29235757 - 5 Dec 2024
Viewed by 527
Abstract
A series of homoleptic rare earth (RE) complexes bearing phosphino-aryloxide ligands (1-RE, 2-La) has been prepared. The complexes have been characterised using multinuclear NMR and IR spectroscopy, X-ray crystallography and elemental analysis. Structural characterisation highlighted the different RE–P interactions as [...] Read more.
A series of homoleptic rare earth (RE) complexes bearing phosphino-aryloxide ligands (1-RE, 2-La) has been prepared. The complexes have been characterised using multinuclear NMR and IR spectroscopy, X-ray crystallography and elemental analysis. Structural characterisation highlighted the different RE–P interactions as a result of differing Lewis acidity and ionic size across the series, hinting at the possibility of FLP-type activity. The potential reactivity of these complexes has been tested by reacting them with small molecules (H2, CO, CO2). A series of side-products (3-RE) has also been observed, isolated and characterised, featuring the incorporation of a phosphonium-aryloxide ligand. Full article
(This article belongs to the Special Issue Exclusive Feature Papers in Inorganic Chemistry, 2nd Edition)
Show Figures

Graphical abstract

Graphical abstract
Full article ">Figure 1
<p>Examples of Zr (<b>I</b>) and RE complexes (<b>I</b>–<b>IV</b>) that display FLP-like reactivity, and selected phosphino-aryloxide complexes (<b>V</b>) [<a href="#B22-molecules-29-05757" class="html-bibr">22</a>,<a href="#B24-molecules-29-05757" class="html-bibr">24</a>,<a href="#B26-molecules-29-05757" class="html-bibr">26</a>,<a href="#B27-molecules-29-05757" class="html-bibr">27</a>,<a href="#B41-molecules-29-05757" class="html-bibr">41</a>].</p>
Full article ">Figure 2
<p>Crystal structures of <b>1-La</b> and <b>2-La</b>. Ellipsoids are shown at 30% probability level, hydrogen atoms are omitted, <span class="html-italic">tert</span>-butyl and <span class="html-italic">iso</span>-propyl groups are shown as wireframe for clarity. Symmetry operation used to generate equivalent atoms: i = 1 − <span class="html-italic">x</span>, 1 − <span class="html-italic">y</span>, 1 − <span class="html-italic">z</span>.</p>
Full article ">Figure 3
<p>Crystal structure of <b>1-Sm</b>. Ellipsoids are shown at 30% probability level, hydrogen atoms are omitted and <span class="html-italic">tert</span>-butyl groups are shown as wireframe for clarity.</p>
Full article ">Figure 4
<p>Crystal structures of <b>3-Y</b> and <b>3-Pr</b>. Ellipsoids are shown at 30% probability level, hydrogen atoms are omitted and <span class="html-italic">tert</span>-butyl groups are shown as wireframe for clarity, with the exception of phosphonium proton.</p>
Full article ">Figure 5
<p>Crystal structures of <b>3-La</b> and <b>3-Sm</b>. Ellipsoids are shown at 30% probability level, hydrogen atoms are omitted and <span class="html-italic">tert</span>-butyl groups are shown as wireframe for clarity, with the exception of phosphonium proton.</p>
Full article ">Scheme 1
<p>Synthesis of <b>1-RE</b>, <b>2-La</b> and <b>3-RE</b>. Crystalline yields are reported in brackets (* denotes spectroscopic yield).</p>
Full article ">Scheme 2
<p>Synthesis of <b>4</b>.</p>
Full article ">Scheme 3
<p>Reactivity of <b>3-RE</b> (RE = Y, La) with B(C<sub>6</sub>F<sub>5</sub>)<sub>3</sub> and formation of <b>1-RE</b> and <b>5</b>.</p>
Full article ">
19 pages, 3441 KiB  
Article
The Relationship Between Spin Crossover (SCO) Behaviors, Cation and Ligand Motions, and Intermolecular Interactions in a Series of Anionic SCO Fe(III) Complexes with Halogen-Substituted Azobisphenolate Ligands
by Mai Hirota, Suguru Murata, Takahiro Sakurai, Hitoshi Ohta and Kazuyuki Takahashi
Molecules 2024, 29(22), 5473; https://doi.org/10.3390/molecules29225473 - 20 Nov 2024
Viewed by 848
Abstract
To investigate the halogen substitution effect on the anionic spin crossover (SCO) complexes, azobisphenolate ligands with 5,5′-dihalogen substituents from fluorine to iodine were synthesized, and their anionic FeIII complexes 1F, 1Cl, 1Br, and 1I were isolated. The temperature dependence [...] Read more.
To investigate the halogen substitution effect on the anionic spin crossover (SCO) complexes, azobisphenolate ligands with 5,5′-dihalogen substituents from fluorine to iodine were synthesized, and their anionic FeIII complexes 1F, 1Cl, 1Br, and 1I were isolated. The temperature dependence of magnetic susceptibility and crystal structure revealed that 1F, 1Cl, and 1Br are all isostructural and exhibit SCO with the rotational motion of the cation and ligands, whereas 1I shows incomplete SCO. Note that 1Cl and 1Br showed irreversible and reversible cooperative SCO transitions, respectively. Short intermolecular contacts between the FeIII complex anions were found despite Coulomb repulsions for all the complexes. The topological analysis of the electron density distributions revealed the existence of X···X halogen bonds, C–H···X, C–H···N, and C–H···O hydrogen bonds, and C–H···π interactions are evident. The dimensionality of intermolecular interactions is suggested to be responsible for the cooperative SCO transitions in 1Cl and 1Br, whereas the disorder due to the freezing of ligand rotations in 1Cl is revealed to inhibit the SCO cooperativity. Full article
(This article belongs to the Special Issue Exclusive Feature Papers in Inorganic Chemistry, 2nd Edition)
Show Figures

Graphical abstract

Graphical abstract
Full article ">Figure 1
<p>Structural formula of 2,2′-azobisphenol <b>H<sub>2</sub>L<sup>X</sup></b> (<b>a</b>); (TMA)[Fe<sup>III</sup>(<b>L<sup>X</sup></b>)<sub>2</sub>] <b>1X</b> [TMA = tetramethylammonium cation] (<b>b</b>).</p>
Full article ">Figure 2
<p>The <span class="html-italic">χ</span><sub>M</sub><span class="html-italic">T</span> vs. <span class="html-italic">T</span> product for the Fe(III) complexes <b>1X</b>.</p>
Full article ">Figure 3
<p>ORTEP drawings of 50% probability with selected atomic numbering for the asymmetric unit. (<b>a</b>) <b>1F</b> at 90 K; (<b>b</b>) <b>1I</b> at 90 K. See text for the occupancy of the TMA cation.</p>
Full article ">Figure 4
<p>(<b>a</b>) Two-dimensional molecular network of the [Fe(<b>L<sup>Br</sup></b>)<sub>2</sub>]<sup>−</sup> anions in <b>1Br</b> along the <span class="html-italic">a</span> axis at 90 K. (<b>b</b>) Molecular arrangement between two-dimensional networks in <b>1Br</b> along the <span class="html-italic">b</span> axis at 90 K. Letters P–V with or without a prime are a label of the [Fe(<b>L<sup>X</sup></b>)<sub>2</sub>]<sup>−</sup> anion molecules with fractional coordinates described in the text and <a href="#molecules-29-05473-t003" class="html-table">Table 3</a>. Dot lines indicate selected intermolecular short contacts between the central reference [Fe(<b>L<sup>X</sup></b>)<sub>2</sub>]<sup>−</sup> anion molecule and the labeled one.</p>
Full article ">Figure 5
<p>(<b>a</b>) Two-dimensional molecular network of [Fe(<b>L<sup>I</sup></b>)<sub>2</sub>]<sup>−</sup> anions in <b>1I</b> at 90 K. (<b>b</b>) Molecular arrangement between two-dimensional networks in <b>1I</b> along the <span class="html-italic">c</span> axis at 90 K. Letters P–V with or without a prime are a label of the [Fe(<b>L<sup>I</sup></b>)<sub>2</sub>]<sup>−</sup> anion molecules with fractional coordinates described in the text and <a href="#molecules-29-05473-t004" class="html-table">Table 4</a>. Dot lines indicate selected intermolecular short contacts between the central reference [Fe(<b>L<sup>I</sup></b>)<sub>2</sub>]<sup>−</sup> anion molecule and the labeled one.</p>
Full article ">Scheme 1
<p>Synthesis of halogen-substituted azp ligands (<b>H<sub>2</sub>L<sup>X</sup></b>). * The yields of <b>4Cl</b> and <b>H<sub>2</sub>L<sup>Cl</sup></b> in the literature [<a href="#B43-molecules-29-05473" class="html-bibr">43</a>] were 41% and 56%, respectively.</p>
Full article ">
14 pages, 2057 KiB  
Article
Exploring the Impact of Water Content in Solvent Systems on Photochemical CO2 Reduction Catalyzed by Ruthenium Complexes
by Yusuke Kuramochi, Masaya Kamiya and Hitoshi Ishida
Molecules 2024, 29(20), 4960; https://doi.org/10.3390/molecules29204960 - 20 Oct 2024
Viewed by 977
Abstract
To achieve artificial photosynthesis, it is crucial to develop a catalytic system for CO2 reduction using water as the electron source. However, photochemical CO2 reduction by homogeneous molecular catalysts has predominantly been conducted in organic solvents. This study investigates the impact [...] Read more.
To achieve artificial photosynthesis, it is crucial to develop a catalytic system for CO2 reduction using water as the electron source. However, photochemical CO2 reduction by homogeneous molecular catalysts has predominantly been conducted in organic solvents. This study investigates the impact of water content on catalytic activity in photochemical CO2 reduction in N,N-dimethylacetamide (DMA), using [Ru(bpy)3]2+ (bpy: 2,2′-bipyridine) as a photosensitizer, 1-benzyl-1,4-dihydronicotinamide (BNAH) as an electron donor, and two ruthenium diimine carbonyl complexes, [Ru(bpy)2(CO)2]2+ and trans(Cl)-[Ru(Ac-5Bpy-NHMe)(CO)2Cl2] (5Bpy: 5′-amino-2,2′-bipyridine-5-carboxylic acid), as catalysts. Increasing water content significantly decreased CO and formic acid production. The similar rates of decrease for both catalysts suggest that water primarily affects the formation efficiency of free one-electron-reduced [Ru(bpy)3]2+, rather than the intrinsic catalytic activity. The reduction in cage-escape efficiency with higher water content underscores the challenges in replacing organic solvents with water in photochemical CO2 reduction. Full article
(This article belongs to the Special Issue Exclusive Feature Papers in Inorganic Chemistry, 2nd Edition)
Show Figures

Figure 1

Figure 1
<p>Chemical structures of [Ru(bpy)<sub>3</sub>]<sup>2+</sup>, BNAH, and ruthenium diimine carbonyl complexes.</p>
Full article ">Figure 2
<p>Effects of water content on the reduction products after 1h of irradiation (λ &gt; 400 nm) using (<b>a</b>) [Ru(bpy)<sub>2</sub>(CO)<sub>2</sub>](PF<sub>6</sub>)<sub>2</sub> (1.0 × 10<sup>−4</sup> M) [<a href="#B25-molecules-29-04960" class="html-bibr">25</a>] and (<b>b</b>) <span class="html-italic">trans</span>(Cl)-[Ru(Ac-<b>5Bpy</b>-NHMe)(CO)<sub>2</sub>Cl<sub>2</sub>] (1.0 × 10<sup>−4</sup> M) [<a href="#B34-molecules-29-04960" class="html-bibr">34</a>] in DMA containing [Ru(bpy)<sub>3</sub>](PF<sub>6</sub>)<sub>2</sub> (5.0 × 10<sup>−4</sup> M) and BNAH (0.10 M) under CO<sub>2</sub> atmosphere: CO (○), HCOOH (■), H<sub>2</sub> (Δ), and CO+HCOOH (+).</p>
Full article ">Figure 3
<p>Reaction mechanism for the photocatalytic CO<sub>2</sub> reduction, consisting of the electron–relay cycle and the catalytic cycle [<a href="#B8-molecules-29-04960" class="html-bibr">8</a>,<a href="#B51-molecules-29-04960" class="html-bibr">51</a>].</p>
Full article ">Figure 4
<p>Viscosity as a function of water content in the DMA and water-mixed solvent. These plots are reconstructed using the values reported in reference [<a href="#B61-molecules-29-04960" class="html-bibr">61</a>,<a href="#B62-molecules-29-04960" class="html-bibr">62</a>].</p>
Full article ">Figure 5
<p>Plots of (<span class="html-italic">RT</span> ln <span class="html-italic">k<sub>q</sub></span>’ + λ<sub>o</sub>/4) vs. ∆<span class="html-italic">G<sub>ET</sub></span> in DMA/water at 298 K. The line is drawn with slope = 1/2.</p>
Full article ">Figure 6
<p>(<b>a</b>) Values of the electrostatic work term (blue diamonds) and viscosity term (red squares) in Equation (10) as a function of water content. (<b>b</b>) Relationship between the relative ratio of the cage-escape rate constants corrected by the quenching constants (black circles) and the relative TONs in the photochemical CO<sub>2</sub> reduction catalysed by [Ru(bpy)<sub>2</sub>(CO)<sub>2</sub>]<sup>2+</sup> (red points) and <span class="html-italic">trans</span>(Cl)-[Ru(Ac-<b>5Bpy</b>-NHMe)(CO)<sub>2</sub>Cl<sub>2</sub>] (blue points).</p>
Full article ">
11 pages, 2933 KiB  
Article
Relaxivity Modulation of Gd-HPDO3A-like Complexes by Introducing Polar and Protic Peripheral Groups
by Sara Camorali, Loredana Leone, Laura Piscopo and Lorenzo Tei
Molecules 2024, 29(19), 4663; https://doi.org/10.3390/molecules29194663 - 30 Sep 2024
Viewed by 736
Abstract
In the last three decades, high-relaxivity Magnetic Resonance Imaging (MRI) contrast agents (CAs) have been intensively sought, aiming at a reduction in the clinically injected dose while maintaining the safety of the CA and obtaining the same pathological information. Thus, four new Gd(III) [...] Read more.
In the last three decades, high-relaxivity Magnetic Resonance Imaging (MRI) contrast agents (CAs) have been intensively sought, aiming at a reduction in the clinically injected dose while maintaining the safety of the CA and obtaining the same pathological information. Thus, four new Gd(III) complexes based on modified 10-(2-hydroxypropyl)-1,4,7,10-tetraazacyclododecane-1,4,7-triacetic acid (HP-DO3A) macrocyclic structure were designed and synthesized by introducing further polar and protic functional groups (amides, phosphonates, and diols) adjacent to the metal-coordinated hydroxyl group. A detailed 1H NMR relaxometric analysis allowed us to investigate the effect of these functional groups on the relaxivity, which showed a 20–60% increase (at 0.5 T, 298 K, and pH 7.4) with respect to that of clinically approved CAs. The contribution of the water molecules H-bonded to these peripheral functional groups on the relaxivity was evaluated in terms of the second sphere effect or prototropic exchange of labile protons. Full article
(This article belongs to the Special Issue Exclusive Feature Papers in Inorganic Chemistry, 2nd Edition)
Show Figures

Figure 1

Figure 1
<p>HPDO3A-like ligands discussed in the text.</p>
Full article ">Figure 2
<p>Novel HPDO3A-like ligands synthesized in this work.</p>
Full article ">Figure 3
<p>(<b>A</b>): comparison between the <span class="html-italic">r</span><sub>1</sub> values as a function of pH (20 MHz, 298 K) for GdHPPDO3A (black squares) and GdHPPEtDO3A (blue diamonds); (<b>B</b>): <span class="html-italic">r</span><sub>1</sub> values as a function of pH (20 MHz, 298 K) for GdHPADO3A-MP (red diamonds) and GdHPADO3A-Ser (black squares) compared to the variable pH profile reported for the secondary amide analogue GdBzHPADO3A [<a href="#B21-molecules-29-04663" class="html-bibr">21</a>] (blue triangles).</p>
Full article ">Figure 4
<p>(<b>A</b>): <sup>1</sup>H NMRD profiles at 298 K for GdHPPDO3A (black squares) and GdHPPEtDO3A (blue diamonds); (<b>B</b>): <sup>1</sup>H NMRD profiles at 298 K for GdHPADO3A-MP (red diamonds), GdHPADO3A-Ser (black squares), and GdBzHPADO3A (blue triangles). The solid lines correspond to the fits of the data as described in the text.</p>
Full article ">Scheme 1
<p>Synthesis of HPPEtDO3A and HPPDO3A. i: <span class="html-italic">t</span>BuOH, reflux, 18 h; ii: TFA, DCM 1:1, 18 h; iii: BrSi(CH<sub>3</sub>)<sub>3</sub>, DCM, 0 °C, 15 min, then RT, 18 h.</p>
Full article ">Scheme 2
<p>Synthesis of HPADO3A-MP. iv: <span class="html-italic">t-</span>Butyl-2-aminomethylphosphonate, HATU, DIPEA, 0 °C, 3 h; ii: TFA/DCM 1:1, RT, 18 h.</p>
Full article ">Scheme 3
<p>Synthesis of HPADO3A-Ser. v: 10 eq. serinol, MeOH, RT, 24 h; ii: TFA/DCM 1:1, 18 h.</p>
Full article ">Scheme 4
<p>Synthesis of the Gd(III) complexes of the ligands reported in this work.</p>
Full article ">
18 pages, 3424 KiB  
Article
Large Number of Direct or Pseudo-Direct Band Gap Semiconductors among A3TrPn2 Compounds with A = Li, Na, K, Rb, Cs; Tr = Al, Ga, In; Pn = P, As
by Sabine Zeitz, Yulia Kuznetsova and Thomas F. Fässler
Molecules 2024, 29(17), 4087; https://doi.org/10.3390/molecules29174087 - 28 Aug 2024
Viewed by 786
Abstract
Due to the high impact of semiconductors with respect to many applications for electronics and energy transformation, the search for new compounds and a deep understanding of the structure–property relationship in such materials has a high priority. Electron-precise Zintl compounds of the composition [...] Read more.
Due to the high impact of semiconductors with respect to many applications for electronics and energy transformation, the search for new compounds and a deep understanding of the structure–property relationship in such materials has a high priority. Electron-precise Zintl compounds of the composition A3TrPn2 (A = Li − Cs, Tr = Al − In, Pn = P, As) have been reported for 22 possible element combinations and show a large variety of different crystal structures comprising zero-, one-, two- and three-dimensional polyanionic substructures. From Li to Cs, the compounds systematically lower the complexity of the anionic structure. For an insight into possible crystal–structure band–structure relations for all compounds (experimentally known or predicted), their band structures, density of states and crystal orbital Hamilton populations were calculated on a basis of DFT/PBE0 and SVP/TZVP basis sets. All but three (Na3AlP2, Na3GaP2 and Na3AlAs2) compounds show direct or pseudo-direct band gaps. Indirect band gaps seem to be linked to one specific structure type, but only for Al and Ga compounds. Arsenides show smaller band gaps than phosphides due to weaker Tr-As bonds. The bonding situation was confirmed by a Mullikan analysis, and most states close to the Fermi level were assigned to non-bonding orbitals. Full article
(This article belongs to the Special Issue Exclusive Feature Papers in Inorganic Chemistry, 2nd Edition)
Show Figures

Figure 1

Figure 1
<p>Overview of all known structure types within the <span class="html-italic">A</span><sub>3</sub><span class="html-italic">TrPn</span><sub>2</sub> system (with <span class="html-italic">A</span> = Li − Cs, <span class="html-italic">Tr</span> = Al, Ga, In, <span class="html-italic">Pn</span> = P, As). The respective structure types (denoted as (<b>A</b>–<b>H</b>) in the picture) are used to reference the structures. For all structures, the alkali metal <span class="html-italic">A</span> is depicted in red, the pnictide <span class="html-italic">Pn</span> in purple and the triel element <span class="html-italic">Tr</span> in grey.</p>
Full article ">Figure 2
<p>(<b>a</b>) Band structure and density of states of Li<sub>3</sub>AlP<sub>2</sub> (type <b>F</b>) with a direct band gap of 3.06 eV green arrow); (<b>b</b>) band structure and density of states of Cs<sub>3</sub>AlP<sub>2</sub> (type <b>A</b>) with a pseudo-direct band gap of 2.54 eV (green arrow) and an indirect band gap of 2.56 eV (orange arrow).</p>
Full article ">Figure 3
<p>(<b>a</b>) Band structure and density of states of Na<sub>3</sub>AlP<sub>2</sub> (type <b>E</b>) with an indirect band gap of 3.34 eV; (<b>b</b>) band structure and density of states of K<sub>3</sub>InP<sub>2</sub> (type <b>E</b>) with a direct band gap of 2.89 eV.</p>
Full article ">Figure 4
<p>(<b>a</b>) COHP for all heteroatomic interactions in Li<sub>3</sub>AlP<sub>2</sub> and Na<sub>3</sub>AlP<sub>2</sub>. (<b>b</b>) COHP for Tr-Tr interactions for Na<sub>3</sub>AlP<sub>2</sub> and K<sub>3</sub>InP<sub>2</sub>. (<b>c</b>) Al-P bond projected COHP for Li<sub>3</sub>AlP<sub>2</sub> and Cs<sub>3</sub>AlP<sub>2</sub>. For all plots, the red line represents the Fermi level at 0 eV and the grey, dashed line the top of the band gap. For Cs<sub>3</sub>AlP<sub>2</sub>, the atomic positions in the projected DOS refer to the assigned positions in the scheme.</p>
Full article ">Scheme 1
<p>Polyanions in compounds of the composition A<sub>5</sub>TtP<sub>3</sub> and A<sub>10</sub>Tt<sub>2</sub>P<sub>6</sub> (A = Li − Cs; Tt = Si − Sn).</p>
Full article ">Scheme 2
<p>Lewis valence structures of the various building units in A<sub>3</sub>TrPn<sub>2</sub> Zintl phases. Mesomere valence formulae <b>1a</b> and <b>1b</b> of the “zero”-dimensional [<span class="html-italic">Tr</span><sub>2</sub><span class="html-italic">Pn</span><sub>4</sub>]<sup>6−</sup> unit of two edge-sharing triangular planar units. The dimeric [<span class="html-italic">Tr</span><sub>2</sub><span class="html-italic">Pn</span><sub>4</sub>]<sup>6−</sup> unit <b>2</b> and the one-dimensional <math display="inline"><semantics> <mrow> <mmultiscripts> <mrow> <mo>[</mo> <mi>T</mi> <mi>r</mi> <msub> <mrow> <mi>P</mi> <mi>n</mi> </mrow> <mrow> <mn>4</mn> <mo>/</mo> <mn>2</mn> </mrow> </msub> <mo>]</mo> </mrow> <none/> <mrow> <mn>3</mn> <mo>−</mo> </mrow> <mprescripts/> <mrow> <mo>∞</mo> </mrow> <mrow> <mn>1</mn> </mrow> </mmultiscripts> </mrow> </semantics></math> string <b>3</b> of edge-sharing tetrahedra, a TrPn<sub>4</sub> tetrahedra <b>4</b> and the adamantane type subunit <b>5</b>. Further connecting atoms are represented in grey colour without formal charges.</p>
Full article ">
24 pages, 7874 KiB  
Article
A Mechanistic Study on Iron-Based Styrene Aziridination: Understanding Epoxidation via Nitrene Hydrolysis
by Dóra Lakk-Bogáth, Patrik Török, Dénes Pintarics and József Kaizer
Molecules 2024, 29(15), 3470; https://doi.org/10.3390/molecules29153470 - 24 Jul 2024
Viewed by 905
Abstract
Transition-metal-catalyzed nitrene transfer reactions are typically performed in organic solvents under inert and anhydrous conditions due to the involved air and water-sensitive nature of reactive intermediates. Overall, this study provides insights into the iron-based ([FeII(PBI)3](CF3SO3) [...] Read more.
Transition-metal-catalyzed nitrene transfer reactions are typically performed in organic solvents under inert and anhydrous conditions due to the involved air and water-sensitive nature of reactive intermediates. Overall, this study provides insights into the iron-based ([FeII(PBI)3](CF3SO3)2 (1), where PBI = 2-(2-pyridyl)benzimidazole), catalytic and stoichiometric aziridination of styrenes using PhINTs ([(N-tosylimino)iodo]benzene), highlighting the importance of reaction conditions including the effects of the solvent, co-ligands (para-substituted pyridines), and substrate substituents on the product yields, selectivity, and reaction kinetics. The aziridination reactions with 1/PhINTs showed higher conversion than epoxidation with 1/PhIO (iodosobenzene). However, the reaction with PhINTs was less selective and yielded more products, including styrene oxide, benzaldehyde, and 2-phenyl-1-tosylaziridine. Therefore, the main aim of this study was to investigate the potential role of water in the formation of oxygen-containing by-products during radical-type nitrene transfer catalysis. During the catalytic tests, a lower yield was obtained in a protic solvent (trifluoroethanol) than in acetonitrile. In the case of the catalytic oxidation of para-substituted styrenes containing electron-donating groups, higher yield, TON, and TOF were achieved than those with electron-withdrawing groups. Pseudo-first-order kinetics were observed for the stoichiometric oxidation, and the second-order rate constants (k2 = 7.16 × 10−3 M−1 s−1 in MeCN, 2.58 × 10−3 M−1 s−1 in CF3CH2OH) of the reaction were determined. The linear free energy relationships between the relative reaction rates (logkrel) and the total substituent effect (TE, 4R-PhCHCH2) parameters with slopes of 1.48 (MeCN) and 1.89 (CF3CH2OH) suggest that the stoichiometric aziridination of styrenes can be described through the formation of a radical intermediate in the rate-determining step. Styrene oxide formation during aqueous styrene aziridination most likely results from oxygen atom transfer via in situ iron oxo/oxyl radical complexes, which are formed through the hydrolysis of [FeIII(N•Ts)] under experimental conditions. Full article
(This article belongs to the Special Issue Exclusive Feature Papers in Inorganic Chemistry, 2nd Edition)
Show Figures

Figure 1

Figure 1
<p>The yield of products for the catalytic oxidation of styrene at 323 K in MeCN with PhINTs and PhI(OAc)<sub>2</sub> (PhIO): benzaldehyde (<span style="color:#4472C4">▪</span>), styrene oxide (<span style="color:#ED7D31">▪</span>), and 2-phenyl-1-tosylaziridine (<span style="color:#A6A6A6">▪</span>). [1]<sub>0</sub> = 1 × 10<sup>−3</sup> M, [PhIO or PhINTs]<sub>0</sub> = 1 × 10<sup>−1</sup> M, and [styrene]<sub>0</sub> = 3 × 10<sup>−1</sup> M under air.</p>
Full article ">Figure 2
<p>The catalytic oxidation of styrene at 323 K in MeCN at different times. (<b>a</b>) The yields of benzaldehyde (<span style="color:#4472C4">▪</span>), styrene oxide (<span style="color:#ED7D31">▪</span>), and 2-phenyl-1-tosylaziridine (<span style="color:#A6A6A6">▪</span>) for this reaction. (<b>b</b>) The yields of benzaldehyde (<span style="color:#4472C4">▪</span>), styrene oxide (<span style="color:#ED7D31">▪</span>), and 2-phenyl-1-tosylaziridine (<span style="color:#A6A6A6">▪</span>) and the decrease in the styrene concentration (<span style="color:#FFD966">▪</span>) as a function of time for the catalytic oxidation of styrene at 323 K in MeCN. [1]<sub>0</sub> = 1 × 10<sup>−3</sup> M, [PhINTs]<sub>0</sub> = 1 × 10<sup>−1</sup> M, and [styrene]<sub>0</sub> = 3 × 10<sup>−1</sup> M under air.</p>
Full article ">Figure 3
<p>The self-decay of <b>1</b> in the absence of a substrate at 323 K in MeCN. [1]<sub>0</sub>= 1 × 10<sup>−3</sup> M; [PhINTs]<sub>0</sub> = 1.2 × 10<sup>−3</sup> M. Inset: the change in the absorbance of the <b>1</b>/PhINTs adduct at 760 nm and the total yield as a function of time for the catalytic oxidation of styrene at 323 K in MeCN. [1]<sub>0</sub> = 1 × 10<sup>−3</sup> M, [PhINTs]<sub>0</sub> = 1 × 10<sup>−1</sup> M, and [styrene]<sub>0</sub> = 3 × 10<sup>−1</sup> M.</p>
Full article ">Figure 4
<p>The catalytic oxidation of styrene at different temperatures in MeCN. (<b>a</b>) The yields of Bz, benzaldehyde (<span style="color:#4472C4">▪</span>); SO, styrene oxide (<span style="color:#ED7D31">▪</span>); and SNTs, 2-phenyl-1-tosylaziridine (<span style="color:#A6A6A6">▪</span>) for this reaction. (<b>b</b>) The yields of Bz (<span style="color:#4472C4">▪</span>), SO (<span style="color:#ED7D31">▪</span>), and SNTs (<span style="color:#A6A6A6">▪</span>) and the total yield (<span style="color:#FFD966">▪</span>) as a function of temperature for the catalytic oxidation of styrene in MeCN. [1]<sub>0</sub>= 1 × 10<sup>−3</sup> M, [PhINTs]<sub>0</sub> = 1 × 10<sup>−1</sup> M, and [styrene]<sub>0</sub> = 3 × 10<sup>−1</sup> M under air.</p>
Full article ">Figure 5
<p>The catalytic oxidation of styrene at different metal concentrations in MeCN at 323 K. (<b>a</b>) The yields of Bz, benzaldehyde (<span style="color:#4472C4">▪</span>); SO, styrene oxide (<span style="color:#ED7D31">▪</span>); and SNTs, 2-phenyl-1-tosylaziridine (<span style="color:#A6A6A6">▪</span>) for this reaction. (<b>b</b>) The yields of benzaldehyde (<span style="color:#4472C4">▪</span>), styrene oxide (<span style="color:#ED7D31">▪</span>), and 2-phenyl-1-tosylaziridine (<span style="color:#A6A6A6">▪</span>) and the total yield (<span style="color:#FFD966">▪</span>) as a function of the iron concentration for the catalytic oxidation of styrene in MeCN at 323 K. [PhINTs]<sub>0</sub> = 1 × 10<sup>−1</sup> M; [styrene]<sub>0</sub> = 3 × 10<sup>−1</sup> M under air.</p>
Full article ">Figure 6
<p>The catalytic oxidation of different <span class="html-italic">para</span>-substituted styrenes at 323 K in MeCN. (<b>a</b>) The yields of products for this reaction: aldehyde (<span style="color:#4472C4">▪</span>), styrene oxide (<span style="color:#ED7D31">▪</span>), and tosylaziridine (<span style="color:#A6A6A6">▪</span>). (<b>b</b>) The plot of log<span class="html-italic">k</span><sub>rel</sub> against σ<sub>p</sub> of <span class="html-italic">para</span>-substituted styrenes. [1]<sub>0</sub> = 1 × 10<sup>−3</sup> M, [PhINTs]<sub>0</sub> = 1 × 10<sup>−1</sup> M, and [styrene]<sub>0</sub> = 3 × 10<sup>−1</sup> M under air.</p>
Full article ">Figure 7
<p>The TON (<span style="color:#4472C4">▪</span>) and TOF (<span style="color:#ED7D31">▪</span>) (1/h) values for the catalytic oxidation of <span class="html-italic">para</span>-substituted styrenes at 323 K in MeCN. [1]<sub>0</sub> = 1 × 10<sup>−3</sup> M, [PhINTs]<sub>0</sub> = 1 × 10<sup>−1</sup> M, and [styrene]<sub>0</sub> = 3 × 10<sup>−1</sup> M under air.</p>
Full article ">Figure 8
<p>The catalytic oxidation of different <span class="html-italic">para</span>-substituted styrenes at 323 K in CF<sub>3</sub>CH<sub>2</sub>OH. (<b>a</b>) The yields of products for this reaction: aldehyde (<span style="color:#4472C4">▪</span>), styrene oxide (<span style="color:#ED7D31">▪</span>), and tosylaziridine (<span style="color:#A6A6A6">▪</span>), (<b>b</b>) The plot of log<span class="html-italic">k</span><sub>rel</sub> against σ<sub>p</sub> of <span class="html-italic">para</span>-substituted styrenes. [1]<sub>0</sub> = 1 × 10<sup>−3</sup> M, [PhINTs]<sub>0</sub> = 1 × 10<sup>−1</sup> M, and [styrene]<sub>0</sub> = 3 × 10<sup>−1</sup> M under air.</p>
Full article ">Figure 9
<p>The TON (<span style="color:#4472C4">▪</span>) and TOF (<span style="color:#ED7D31">▪</span>) (1/h) values for the catalytic oxidation of <span class="html-italic">para</span>-substituted styrenes at 323 K in CF<sub>3</sub>CH<sub>2</sub>OH. [1]<sub>0</sub> = 1 × 10<sup>−3</sup> M, [PhINTs]<sub>0</sub> = 1 × 10<sup>−1</sup> M, and [styrene]<sub>0</sub> = 3 × 10<sup>−1</sup> M under air.</p>
Full article ">Figure 10
<p>The effect of water for the catalytic oxidation of styrene. (<b>a</b>) The yields of products for this reaction (Bz, benzaldehyde (<span style="color:#4472C4">▪</span>); SO, styrene oxide (<span style="color:#ED7D31">▪</span>); and SNTs, 2-phenyl-1-tosylaziridine (<span style="color:#A6A6A6">▪</span>)). (<b>b</b>) The epoxide/aziridine ratio and the benzaldehyde/epoxide ratio as functions of the H<sub>2</sub>O concentration; [1]<sub>0</sub> = 1 × 10<sup>−3</sup> M, [PhINTs]<sub>0</sub> = 1 × 10<sup>−1</sup> M, and [styrene]<sub>0</sub> = 3 × 10<sup>−1</sup> M under air.</p>
Full article ">Figure 11
<p>The effects of water, D<sub>2</sub>O, and the buffer for the catalytic oxidation of styrene. (<b>a</b>) The yields of products for this reaction: benzaldehyde (<span style="color:#4472C4">▪</span>), styrene oxide (<span style="color:#ED7D31">▪</span>), and 2-phenyl-1-tosylaziridine (<span style="color:#A6A6A6">▪</span>). (<b>b</b>) The change in wavelength due to water and the pH 4.7 buffer. [1]<sub>0</sub> = 1 × 10<sup>−3</sup> M, [PhINTs]<sub>0</sub> = 1 × 10<sup>−1</sup> M, [styrene]<sub>0</sub> = 3 × 10<sup>−1</sup> M, [H<sub>2</sub>O, D<sub>2</sub>O]<sub>0</sub> = 1.5 × 10<sup>−2</sup> M, and [buffer]<sub>0</sub> = 2 × 10<sup>−1</sup> mL under air.</p>
Full article ">Figure 12
<p>The GC-MS analysis for the catalytic oxidation of styrene in MeCN at 323 K in the presence of water, H<sub>2</sub>O<sup>18</sup>. [1]<sub>0</sub> = 1 × 10<sup>−3</sup> M, [PhINTs]<sub>0</sub> = 1 × 10<sup>−1</sup> M, [styrene]<sub>0</sub> = 3 × 10<sup>−1</sup> M, and [H<sub>2</sub>O<sup>18</sup>]<sub>0</sub> = 1.5 × 10<sup>−2</sup> M under air.</p>
Full article ">Figure 13
<p>The catalytic oxidation of different <span class="html-italic">para</span>-substituted pyridines at 323 K in MeCN. (<b>a</b>) The yields of products for this reaction: benzaldehyde (<span style="color:#4472C4">▪</span>), styrene oxide (<span style="color:#ED7D31">▪</span>), and 2-phenyl-1-tosylaziridine (<span style="color:#A6A6A6">▪</span>). (<b>b</b>) The plot of log<span class="html-italic">k</span><sub>rel</sub> against σ<sub>p</sub> of <span class="html-italic">para</span>-substituted pyridines. [1]<sub>0</sub> = 1 × 10<sup>−3</sup> M, [PhINTs]<sub>0</sub> = 1 × 10<sup>−1</sup> M, [styrene]<sub>0</sub> = 3 × 10<sup>−1</sup> M, and [<span class="html-italic">para</span>-substituted pyridine]<sub>0</sub> = 1 × 10<sup>−2</sup> M under air.</p>
Full article ">Figure 14
<p>The catalytic oxidation of different <span class="html-italic">para</span>-substituted pyridines at 323 K in MeCN. The epoxide/aziridine ratio as a function of σ<sub>p</sub>. [1]<sub>0</sub> = 1 × 10<sup>−3</sup> M, [PhINTs]<sub>0</sub> = 1 × 10<sup>−1</sup> M, [styrene]<sub>0</sub> = 3 × 10<sup>−1</sup> M, and [<span class="html-italic">para</span>-substituted pyridine]<sub>0</sub> = 1 × 10<sup>−2</sup> M under air.</p>
Full article ">Figure 15
<p>(<b>a</b>) UV-vis spectral change of Fe<sup>III</sup>(OIPh) with PhINTs at 293 K in MeCN. Fe<sup>III</sup>(OIPh) was generated in situ by reaction of <b>1</b> with PhI(OAc)<sub>2</sub>. (<b>b</b>) UV-vis spectral change of Fe<sup>III</sup>(OINTs) with PhIO at 293 K in MeCN. Fe<sup>III</sup>(OINTs) was generated in situ by reaction of <b>1</b> with PhINTs. [1]<sub>0</sub> = 1 × 10<sup>−3</sup> M, [PhINTs]<sub>0</sub> = 4 × 10<sup>−3</sup> M, and [PhIO]<sub>0</sub> = 4 × 10<sup>−3</sup> M.</p>
Full article ">Figure 16
<p>(<b>a</b>) FT-IR solid spectra of <b>1</b> (green) and <b>1</b>/PhINTs (1:1) adduct (brown). (<b>b</b>) FT-IR solid spectra of PhINTs (black) and <b>1</b>/PhINTs (1:1) adduct (brown).</p>
Full article ">Figure 17
<p>Cyclic voltammograms at 293 K in MeCN. (<b>a</b>) Cyclic voltammograms of <b>1</b> (<span style="color:#5B9BD5">-</span>) and <b>1</b> with PhINTs (<span style="color:red">-</span>). (<b>b</b>) Cyclic voltammograms of <b>1</b> with PhIO (-) and <b>1</b> with PhINTs (<span style="color:red">-</span>). [1]<sub>0</sub> = 1.0 × 10<sup>−3</sup> M, PhIO = 2.0 × 10<sup>−3</sup> M, and PhINTs = 2.0 × 10<sup>−3</sup> M in (0.1 M TBAClO<sub>4</sub>) MeCN (10 cm<sup>3</sup>); scan rate: 500 mV/s.</p>
Full article ">Figure 18
<p>The stoichiometric oxidation of styrene with the <b>1</b>/PhINTs adduct at 293 K in MeCN. (<b>a</b>) The UV-vis spectral changes of the <b>1</b>/PhINTs adduct upon the addition of styrene. (<b>b</b>) The change in absorbance vs. <span class="html-italic">t</span> in the reaction of the <b>1</b>/PhINTs adduct and styrene at 770 nm in MeCN (<span style="color:#C00000">•</span>) and in CF<sub>3</sub>CH<sub>2</sub>OH (<span style="color:#4472C4">•</span>). [1]<sub>0</sub> = 0.5 × 10<sup>−3</sup> M, [PhINTs]<sub>0</sub> = 1 × 10<sup>−3</sup> M, and [styrene]<sub>0</sub> = 9 × 10<sup>−1</sup> M.</p>
Full article ">Figure 19
<p>The stoichiometric oxidation of styrene at 293 K. (<b>a</b>) The reaction rate of <b>1</b>/PhIO (<span style="color:#4472C4">•</span>) or <b>1</b>/PhINTs (<span style="color:#ED7D31">•</span>) with styrene in MeCN. (<b>b</b>) The reaction rate of the <b>1</b>/PhINTs adduct with styrene in MeCN (<span style="color:#4472C4">•</span>) or in CF<sub>3</sub>CH<sub>2</sub>OH (<span style="color:#ED7D31">•</span>) at 293 K. [1]<sub>0</sub> = 1 × 10<sup>−3</sup> M; [PhINTs]<sub>0</sub> = 1 × 10<sup>−3</sup> M.</p>
Full article ">Figure 20
<p>The dependence of <span class="html-italic">v<sub>i</sub></span> on the initial complex concentration in the reaction of the <b>1</b>/PhINTs adduct and styrene in MeCN (<span style="color:#4472C4">•</span>) or in CF<sub>3</sub>CH<sub>2</sub>OH (<span style="color:#ED7D31">•</span>) at 293 K. [styrene]<sub>0</sub> = 6 × 10<sup>−1</sup> M; [PhINTs]<sub>0</sub> = 1 × 10<sup>−3</sup> M.</p>
Full article ">Figure 21
<p>The Eyring plot of the reaction of the <b>1</b>/PhINTs adduct with styrene in MeCN (<span style="color:#4472C4">•</span>) or in CF<sub>3</sub>CH<sub>2</sub>OH (<span style="color:#ED7D31">•</span>). [1]<sub>0</sub> = 1 × 10<sup>−3</sup> M, [PhINTs]<sub>0</sub> = 1 × 10<sup>−3</sup> M, and [styrene]<sub>0</sub> = 1.5 × 10<sup>0</sup> M.</p>
Full article ">Figure 22
<p>Stoichiometric oxidation of different <span class="html-italic">para</span>-substituted styrenes at 293 K in MeCN. (<b>a</b>) Plot of log(<span class="html-italic">k</span><sub>X</sub>/<span class="html-italic">k</span><sub>H</sub>) against σ<sub>p</sub> of <span class="html-italic">para</span>-substituted styrenes. (<b>b</b>) Plot of log(<span class="html-italic">k</span><sub>X</sub>/<span class="html-italic">k</span><sub>H</sub>) against TE of <span class="html-italic">para</span>-substituted styrenes. [1]<sub>0</sub> = 1 × 10<sup>−3</sup> M, [PhINTs]<sub>0</sub> = 1 × 10<sup>−3</sup> M, and [styrenes]<sub>0</sub> = 5 × 10<sup>−1</sup> M.</p>
Full article ">Figure 23
<p>Stoichiometric oxidation of different <span class="html-italic">para</span>-substituted styrenes at 293 K in CF<sub>3</sub>CH<sub>2</sub>OH. (<b>a</b>) Plot of log(<span class="html-italic">k</span><sub>X</sub>/<span class="html-italic">k</span><sub>H</sub>) against σ<sub>p</sub> of <span class="html-italic">para</span>-substituted styrenes. (<b>b</b>) Plot of log(<span class="html-italic">k</span><sub>X</sub>/<span class="html-italic">k</span><sub>H</sub>) against TE of <span class="html-italic">para</span>-substituted styrenes. [1]<sub>0</sub> = 1 × 10<sup>−3</sup> M, [PhINTs]<sub>0</sub> = 1 × 10<sup>−3</sup> M, and [styrenes]<sub>0</sub> = 5 × 10<sup>−1</sup> M.</p>
Full article ">Scheme 1
<p>Products formed during stoichiometric and catalytic aziridination of styrene and structures of PhINTs and [Fe<sup>II</sup>(PBI)<sub>3</sub>(CF<sub>3</sub>SO<sub>3</sub>)<sub>2</sub>] (<b>1</b>).</p>
Full article ">Scheme 2
<p>The proposed mechanisms for the Fe<sup>III</sup>(NTs)-mediated aziridination reactions.</p>
Full article ">
10 pages, 1739 KiB  
Article
Tuning the Coordination Environment of Ru(II) Complexes with a Tailored Acridine Ligand
by Ali Awada, Pierre-Henri Lanoë, Christian Philouze, Frédérique Loiseau and Damien Jouvenot
Molecules 2024, 29(15), 3468; https://doi.org/10.3390/molecules29153468 - 24 Jul 2024
Viewed by 855
Abstract
A novel tridentate ligand featuring an acridine core and pyrazole rings, namely 2,7- di-tert-butyl-4,5-di(pyrazol-1-yl)acridine, L, was designed and used to create two ruthenium(II) complexes: [RuL2](PF6)2 and [Ru(tpy)L](PF6)2. Surprisingly, [...] Read more.
A novel tridentate ligand featuring an acridine core and pyrazole rings, namely 2,7- di-tert-butyl-4,5-di(pyrazol-1-yl)acridine, L, was designed and used to create two ruthenium(II) complexes: [RuL2](PF6)2 and [Ru(tpy)L](PF6)2. Surprisingly, the ligand adopted different coordination modes in the complexes: facial coordination for the homoleptic complex and meridional coordination for the heteroleptic complex. The electronic absorption and electrochemical properties were evaluated. Although both complexes exhibited favorable electronic properties for luminescence, neither emitted light at room temperature nor at 77 K. This study highlights the complex interplay between ligand design, coordination mode, and luminescence in ruthenium(II) complexes. Full article
(This article belongs to the Special Issue Exclusive Feature Papers in Inorganic Chemistry, 2nd Edition)
Show Figures

Graphical abstract

Graphical abstract
Full article ">Figure 1
<p>The assigned aromatic region of the <sup>1</sup>H-NMR spectra of the complex [Ru(<b>L</b>)<sub>2</sub>]<sup>2+</sup> (red top), ligand <b>L</b> (black middle), and complex [Ru(tpy)<b>L</b>]<sup>2+</sup> (blue bottom) recorded in acetone-<span class="html-italic">d</span><sub>6</sub> at 500 MHz. Signals with an asterisk indicate peaks attributable to the tpy ligand.</p>
Full article ">Figure 2
<p>Different projections of the crystal structure of the complex [Ru(<b>L</b>)<sub>2</sub>]<sup>2+</sup> (40% ellipsoids). Solvent molecules (co-crystallized acetone molecules), hydrogen atoms, and PF<sub>6</sub><sup>−</sup> counterions are omitted for clarity.</p>
Full article ">Figure 3
<p>Different projections of the crystal structure of the complex [Ru(tpy)<b>L</b>]<sup>2+</sup> (40% ellipsoids). Solvent molecules (co-crystallized acetone molecules), hydrogen atoms, and PF<sub>6</sub><sup>−</sup> counter anions are omitted for clarity.</p>
Full article ">Figure 4
<p>The UV–visible absorption spectra of [Ru(<b>L</b>)<sub>2</sub>]<sup>2+</sup> (red) and [Ru(tpy)<b>L</b>]<sup>2+</sup> (blue) recorded in an acetonitrile solution. Inset: zoom on the visible region of the spectra.</p>
Full article ">Scheme 1
<p>Synthesis of ligand <b>L</b>.</p>
Full article ">Scheme 2
<p>Syntheses of complexes [Ru<b>L</b><sub>2</sub>](PF<sub>6</sub>)<sub>2</sub> and [Ru(tpy)<b>L</b>](PF<sub>6</sub>)<sub>2</sub>.</p>
Full article ">
12 pages, 1918 KiB  
Article
Assembly of Homochiral Magneto-Optical Dy6 Triangular Clusters by Fixing Carbon Dioxide in the Air
by Cai-Ming Liu, Xiang Hao and Xi-Li Li
Molecules 2024, 29(14), 3402; https://doi.org/10.3390/molecules29143402 - 19 Jul 2024
Cited by 3 | Viewed by 1303
Abstract
A new hydrazone Schiff base bridging ligand (H2LSchiff (E)-N′-((1-hydroxynaphthalen-2-yl)methylene)pyrazine-2-carbohydrazide) and L/D-proline were used to construct a pair of homochiral Dy6 cluster complexes, [Dy6(CO3)(L-Pro)6(LSchiff [...] Read more.
A new hydrazone Schiff base bridging ligand (H2LSchiff (E)-N′-((1-hydroxynaphthalen-2-yl)methylene)pyrazine-2-carbohydrazide) and L/D-proline were used to construct a pair of homochiral Dy6 cluster complexes, [Dy6(CO3)(L-Pro)6(LSchiff)4(HLSchiff)2]·5DMA·2H2O (L-1, L-HPro = L-proline; DMA = N,N-dimethylacetamide) and [Dy6(CO3)(D-Pro)6(LSchiff)4(HLSchiff)2]·5DMA·2H2O (D-1, D-HPro = D-proline), which show a novel triangular Dy6 topology. Notably, the fixation of CO2 in the air formed a carbonato central bridge, playing a key role in assembling L-1/D-1. Magnetic measurements revealed that L-1/D-1 displays intramolecular ferromagnetic coupling and magnetic relaxation behaviours. Furthermore, L-1/D-1 shows a distinct magneto-optical Faraday effect and has a second harmonic generation (SHG) response (1.0 × KDP) at room temperature. The results show that the immobilization of CO2 provides a novel pathway for homochiral multifunctional 4f cluster complexes. Full article
(This article belongs to the Special Issue Exclusive Feature Papers in Inorganic Chemistry, 2nd Edition)
Show Figures

Figure 1

Figure 1
<p>Crystal structures of <span class="html-italic">L</span>-<b>1</b> (<b>a</b>) and <span class="html-italic">D</span>-<b>1</b> (<b>b</b>). Color code: C, grey; N, blue; O, red; Dy, green. All disordered pyrrolidine rings show only one of two sets, and all H atoms and solvent molecules are omitted for clarity.</p>
Full article ">Figure 2
<p>Plot of χ<sub>M</sub>T vs. T of <span class="html-italic">L</span>-<b>1</b> (H<sub>dc</sub> = 1000 Oe).</p>
Full article ">Figure 3
<p>Plots of χ″ vs. T for <span class="html-italic">L</span>-<b>1</b> (H<sub>dc</sub> = 0 Oe).</p>
Full article ">Figure 4
<p>CD spectra of <span class="html-italic">L</span>-<b>1</b> and <span class="html-italic">D</span>-<b>1</b> in DMF solution (c = 0.2 gL<sup>−1</sup>; H = 0 T) (<b>above</b>) and UV-vis spectra of <span class="html-italic">L</span>-<b>1</b> and <span class="html-italic">D</span>-<b>1</b> in DMF solution (c = 0.2 gL<sup>−1</sup>; H = 0 T) (<b>below</b>).</p>
Full article ">Figure 5
<p>CD spectra of <span class="html-italic">L</span>-<b>1</b> and <span class="html-italic">D</span>-<b>1</b> in DMF solution under an NS (+1.6 T) or SN (−1.6 T) field (c = 0.2 gL<sup>−1</sup>; optical path = 5 mm).</p>
Full article ">Figure 6
<p>SHG spectra of crystalline samples of <span class="html-italic">L</span>-<b>1</b> and KDP under excitation at λ = 1550 nm (T<sub>int =</sub> 0.5 s).</p>
Full article ">Scheme 1
<p>Synthesis pathway of the new hydrazone Schiff base ligand H<sub>2</sub>L<sub>Schiff</sub>.</p>
Full article ">
18 pages, 5147 KiB  
Article
Electrocatalytic Properties of Quasi-2D Oxides LaSrMn0.5M0.5O4 (M = Co, Ni, Cu, and Zn) for Hydrogen and Oxygen Evolution Reactions
by Kinithi M. K. Wickramaratne and Farshid Ramezanipour
Molecules 2024, 29(13), 3107; https://doi.org/10.3390/molecules29133107 - 29 Jun 2024
Viewed by 854
Abstract
Designing cost-effective and highly efficient electrocatalysts for water splitting is a significant challenge. We have systematically investigated a series of quasi-2D oxides, LaSrMn0.5M0.5O4 (M = Co, Ni, Cu, Zn), to enhance the electrocatalytic properties of the two half-reactions [...] Read more.
Designing cost-effective and highly efficient electrocatalysts for water splitting is a significant challenge. We have systematically investigated a series of quasi-2D oxides, LaSrMn0.5M0.5O4 (M = Co, Ni, Cu, Zn), to enhance the electrocatalytic properties of the two half-reactions of water-splitting, namely oxygen and hydrogen evolution reactions (OER and HER). The four materials are isostructural, as confirmed by Rietveld refinements with X-ray diffraction. The oxygen contents and metal valence states were determined by iodometric titrations and X-ray photoelectron spectroscopy. Electrical conductivity measurements in a wide range of temperatures revealed semiconducting behavior for all four materials. Electrocatalytic properties were studied for both half-reactions of water-splitting, namely, oxygen-evolution and hydrogen-evolution reactions (OER and HER). For the four materials, the trends in both OER and HER were the same, which also matched the trend in electrical conductivities. Among them, LaSrMn0.5Co0.5O4 showed the best bifunctional electrocatalytic activity for both OER and HER, which may be attributed to its higher electrical conductivity and favorable electron configuration. Full article
(This article belongs to the Special Issue Exclusive Feature Papers in Inorganic Chemistry, 2nd Edition)
Show Figures

Figure 1

Figure 1
<p>Rietveld refinement profiles using powder X-ray diffraction data of (<b>a</b>) LaSrMn<sub>0.5</sub>Co<sub>0.5</sub>O<sub>4</sub>, (<b>b</b>) LaSrMn<sub>0.5</sub>Ni<sub>0.5</sub>O<sub>4</sub>, (<b>c</b>) LaSrMn<sub>0.5</sub>Cu<sub>0.5</sub>O<sub>4-δ</sub>, and (<b>d</b>) LaSrMn<sub>0.5</sub>Zn<sub>0.5</sub>O<sub>4</sub>. The cross symbols, solid red line, olive vertical tick marks, and lower magenta line correspond to experimental data, the calculated pattern for the structural model, Bragg peak positions, and the difference plot, respectively.</p>
Full article ">Figure 2
<p>Crystal structure of LaSrMn<sub>0.5</sub>M<sub>0.5</sub>O<sub>4</sub> (M = Co, Ni, Cu, Zn). Pink spheres denote La/Sr, small red spheres indicate oxygen, and green spheres represent Mn/M.</p>
Full article ">Figure 3
<p>Scanning electron microscopy (SEM) images of (<b>a</b>) LaSrMn<sub>0.5</sub>Co<sub>0.5</sub>O<sub>4</sub>, (<b>b</b>) LaSrMn<sub>0.5</sub>Ni<sub>0.5</sub>O<sub>4</sub>, (<b>c</b>) LaSrMn<sub>0.5</sub>Cu<sub>0.5</sub>O<sub>4-δ</sub>, and (<b>d</b>) LaSrMn<sub>0.5</sub>Zn<sub>0.5</sub>O<sub>4</sub>.</p>
Full article ">Figure 4
<p>XPS data showing the manganese spectra for all four materials. The purple dashed line is drawn to show that the binding energy for the 2p<sub>3/2</sub> peak of LaSrMn<sub>0.5</sub>Zn<sub>0.5</sub>O<sub>4</sub> is shifted to higher energy compared to those of the other three materials.</p>
Full article ">Figure 5
<p>XPS data showing the spectra for (<b>a</b>) cobalt in LaSrMn<sub>0.5</sub>Co<sub>0.5</sub>O<sub>4</sub>, (<b>b</b>) nickel in LaSrMn<sub>0.5</sub>Ni<sub>0.5</sub>O<sub>4</sub>, (<b>c</b>) copper in LaSrMn<sub>0.5</sub>Cu<sub>0.5</sub>O<sub>4–δ</sub>, and (<b>d</b>) zinc in LaSrMn<sub>0.5</sub>Zn<sub>0.5</sub>O<sub>4</sub>. The peak marked by * is the lanthanum 3d<sub>3/2</sub> peak, which appears very close to the nickel 2p<sub>3/2</sub>.</p>
Full article ">Figure 6
<p>(<b>a</b>) Electrical conductivities as a function of temperature. (<b>b</b>) Arrhenius plots to determine the activation energies (E<sub>a</sub>) for the temperature-activated increase in conductivity.</p>
Full article ">Figure 7
<p>(<b>a</b>) Polarization curves for HER in 0.5 M H<sub>2</sub>SO<sub>4</sub>. The inset shows chronopotentiometry data for the best-performing material, LaSrMn<sub>0.5</sub>Co<sub>0.5</sub>O<sub>4</sub>. (<b>b</b>) Tafel plots and slopes. (<b>c</b>) X-ray diffraction data for LaSrMn<sub>0.5</sub>Co<sub>0.5</sub>O<sub>4</sub> before and after 100 cycles of HER in 0.5 M H<sub>2</sub>SO<sub>4</sub>. (<b>d</b>) HER mass activities at different overpotentials in 0.5 M H<sub>2</sub>SO<sub>4</sub>.</p>
Full article ">Figure 8
<p>Plots of j<sub>avg</sub> against ν in 0.5 M H<sub>2</sub>SO<sub>4</sub>. The slopes indicate double-layer capacitance, C<sub>dl</sub>.</p>
Full article ">Figure 9
<p>(<b>a</b>) HER polarization curves in 1 M KOH. The inset shows chronopotentiometry data for the best-performing material LaSrMn<sub>0.5</sub>Co<sub>0.5</sub>O<sub>4</sub>. (<b>b</b>) Tafel plots and slopes. (<b>c</b>) X-ray diffraction data for LaSrMn<sub>0.5</sub>Co<sub>0.5</sub>O<sub>4</sub> before and after 100 cycles of HER in 1 M KOH. (<b>d</b>) HER mass activities at different overpotentials in 1 M KOH.</p>
Full article ">Figure 10
<p>Plots of j<sub>avg</sub> against ν in 1 M KOH. The slopes indicate double-layer capacitance, C<sub>dl</sub>.</p>
Full article ">Figure 11
<p>(<b>a</b>) Polarization curves for OER in 1 M KOH. The inset shows chronopotentiometry data for the best-performing material, LaSrMn<sub>0.5</sub>Co<sub>0.5</sub>O<sub>4</sub>. (<b>b</b>) Tafel plots and slopes. (<b>c</b>) X-ray diffraction data for LaSrMn<sub>0.5</sub>Co<sub>0.5</sub>O<sub>4</sub> before and after 100 cycles of OER in 1 M KOH. (<b>d</b>) OER mass activities at different overpotentials in 1 M KOH.</p>
Full article ">Figure 12
<p>The TEM data (<b>a</b>) before and (<b>b</b>) after chronopotentiometry experiment under OER conditions.</p>
Full article ">
12 pages, 2030 KiB  
Article
Ab Initio Electronic, Magnetic, and Optical Properties of Fe Phthalocyanine on Cr2O3(0001)
by Marco Marino, Elena Molteni, Simona Achilli, Giovanni Onida and Guido Fratesi
Molecules 2024, 29(12), 2889; https://doi.org/10.3390/molecules29122889 - 18 Jun 2024
Viewed by 736
Abstract
The organic molecules adsorbed on antiferromagnetic surfaces can produce interesting interface states, characterized by charge transfer mechanisms, hybridization of molecular-substrate orbitals, as well as magnetic couplings. Here, we apply an ab initio approach to study the adsorption of Fe phthalocyanine on stoichiometric Cr [...] Read more.
The organic molecules adsorbed on antiferromagnetic surfaces can produce interesting interface states, characterized by charge transfer mechanisms, hybridization of molecular-substrate orbitals, as well as magnetic couplings. Here, we apply an ab initio approach to study the adsorption of Fe phthalocyanine on stoichiometric Cr2O3(0001). The molecule binds via a bidentate configuration forming bonds between two opposite imide N atoms and two protruding Cr ones, making this preferred over the various possible adsorption structures. In addition to the local modifications at these sites, the electronic structure of the molecule is weakly influenced. The magnetic structure of the surface Cr atoms shows a moderate influence of molecule adsorption, not limited to the atoms in the close proximity of the molecule. Upon optical excitation at the onset, electron density moves toward the molecule, enhancing the ground state charge transfer. We investigate this movement of charge as a mechanism at the base of light-induced modifications of the magnetic structure at the interface. Full article
(This article belongs to the Special Issue Exclusive Feature Papers in Inorganic Chemistry, 2nd Edition)
Show Figures

Graphical abstract

Graphical abstract
Full article ">Figure 1
<p>(<b>a</b>) Top view and (<b>b</b>) side view of the <math display="inline"><semantics> <mrow> <mn>4</mn> <mo>×</mo> <mn>4</mn> </mrow> </semantics></math> surface supercell used for the calculations, with primitive cell of Cr<sub>2</sub>O<sub>3</sub>(0001) indicated in (<b>a</b>) (shaded). (<b>c</b>) Model of FePc/Cr<sub>2</sub>O<sub>3</sub>(0001), indicating the angle between the N-Fe-N axis and the surface <math display="inline"><semantics> <mrow> <mo>[</mo> <mn>2</mn> <mover accent="true"> <mn>1</mn> <mo stretchy="false">¯</mo> </mover> <mover accent="true"> <mn>1</mn> <mo stretchy="false">¯</mo> </mover> <mn>0</mn> <mo>]</mo> </mrow> </semantics></math> direction (Black lines centered on Fe atom). Color scheme as follows: yellow: topmost Cr atoms (named Cr1); light and dark blue: Cr atoms of the subsurface trilayer, according to their respective height (light higher Cr2, dark lower Cr3) in the bilayer 3O-2Cr-3O; red: O atoms. The magnetization of the Cr3 is parallel to that of the Cr1 atoms and opposite to that of the Cr2 atoms. Three of the O atoms are in the surface trilayer (O-up) and three in the subsurface trilayer (O-dn). Brown: Fe.</p>
Full article ">Figure 2
<p>Optimized geometry for FePc/Cr<sub>2</sub>O<sub>3</sub>(0001) for the adsorption configurations considered: (<b>a</b>) on a Cr1 site at <math display="inline"><semantics> <msup> <mn>22</mn> <mo>∘</mo> </msup> </semantics></math>, (<b>b</b>) on a Cr2 site at <math display="inline"><semantics> <msup> <mn>22</mn> <mo>∘</mo> </msup> </semantics></math>, (<b>c</b>) on a Cr3 site at <math display="inline"><semantics> <msup> <mn>0</mn> <mo>∘</mo> </msup> </semantics></math>, (<b>d</b>) on an O-up site at <math display="inline"><semantics> <msup> <mn>22</mn> <mo>∘</mo> </msup> </semantics></math>, (<b>e</b>) on an O-dn site at <math display="inline"><semantics> <msup> <mn>45</mn> <mo>∘</mo> </msup> </semantics></math>, and (<b>f</b>) on a B site at <math display="inline"><semantics> <msup> <mn>15</mn> <mo>∘</mo> </msup> </semantics></math>. The color scheme is the same as in <a href="#molecules-29-02889-f001" class="html-fig">Figure 1</a>.</p>
Full article ">Figure 3
<p>Electronic PDOS of FePc/Cr<sub>2</sub>O<sub>3</sub>(0001) summed over (<b>a</b>) all molecule atoms; (<b>b</b>) C; (<b>c</b>) N; (<b>d</b>) Fe; (<b>e</b>) substrate atoms. Substrate color codes: black: all substrate atoms; red: all Cr atoms with “up” magnetic moment; blue: all O atoms. Solid/dash-dotted lines indicate adsorbed and gas phase molecules, respectively. Spin-down components are shown as negative values. All values in states/eV/cell. The position of the Fermi energy in the gap is arbitrary. In the inset, we report the spin-up contributions from the bonding imide N and Cr1 (lines) atoms over the other imide N and Cr1 atoms (gray area).</p>
Full article ">Figure 4
<p>On the left, (<b>a</b>) top view; on the right, (<b>b</b>,<b>c</b>) side-view of the charge density variation in the FePc/Cr<sub>2</sub>O<sub>3</sub>(0001) minimum energy adsorption configuration (isovalues in the range of 0.001 Å × <math display="inline"><semantics> <msup> <mn>10</mn> <mrow> <mo>−</mo> <mn>3</mn> </mrow> </msup> </semantics></math>). Note the bondings between the imide N and the Cr1 and between the phenyl rings and the Cr1. Color scheme the same as in <a href="#molecules-29-02889-f001" class="html-fig">Figure 1</a>.</p>
Full article ">Figure 5
<p>Variations in the atomic magnetic moments of FePc/Cr<sub>2</sub>O<sub>3</sub>(0001), seen from the top, with respect to the isolated systems, on (<b>a</b>) the surface and on the molecule (<b>b</b>). Corresponding variations in the electronic density (<b>d</b>,<b>e</b>). (Positive = increase in electron population.) Side view of the variations: (<b>c</b>) magnetic moments and (<b>f</b>) charge density. The positions of the molecule atoms are marked by green/blue letters in panels (<b>a</b>,<b>c</b>,<b>d</b>,<b>f</b>). Notice that few values in the plot exceed the maximum ones on the scale bar.</p>
Full article ">Figure 6
<p>Optical absorption spectra (independent particle): polarizability of Cr<sub>2</sub>O<sub>3</sub>(0001) (blue), FePc/Cr<sub>2</sub>O<sub>3</sub>(0001) (red), and an FePc molecular layer such as in FePc/Cr<sub>2</sub>O<sub>3</sub>(0001) (green). The arbitrary units are chosen by normalizing the molecular peak at ≃1.5 eV (green line) to 1. The transitions are broadened by <math display="inline"><semantics> <mrow> <mn>0.01</mn> </mrow> </semantics></math> eV. Bottom inset: the intensities (red) of the main transitions contributing to the FePc/Cr<sub>2</sub>O<sub>3</sub>(0001) spectrum in the spin-up (top) and spin-down (bottom) channels, normalized with respect to the largest one at ≃1.1 eV. Only values greater than <math display="inline"><semantics> <mrow> <mn>10</mn> <mo>%</mo> </mrow> </semantics></math> are shown. Top inset: the percentage of projection of the respective valence(bottom)/conduction(top) level on the molecule (yellow), characterizing the main transitions.</p>
Full article ">
11 pages, 981 KiB  
Article
Cobalt(III)–Macrocyclic Scaffolds with Anti-Cancer Stem Cell Activity
by Jiaxin Fang, Philipp Gerschel, Kuldip Singh, Ulf-Peter Apfel and Kogularamanan Suntharalingam
Molecules 2024, 29(12), 2743; https://doi.org/10.3390/molecules29122743 - 8 Jun 2024
Viewed by 975
Abstract
Cobalt(III) compounds with tetradentate ligands have been widely employed to deliver cytotoxic and imaging agents into cells. A large body of work has focused on using cobalt(III)–cyclam scaffolds for this purpose. Here, we investigate the cytotoxic properties of cobalt(III) complexes containing 14-membered macrocycles [...] Read more.
Cobalt(III) compounds with tetradentate ligands have been widely employed to deliver cytotoxic and imaging agents into cells. A large body of work has focused on using cobalt(III)–cyclam scaffolds for this purpose. Here, we investigate the cytotoxic properties of cobalt(III) complexes containing 14-membered macrocycles related to cyclam. A breast cancer stem cell (CSC) in vitro model was used to gauge efficacy. Specifically, [Co(1,4,7,11-tetraazacyclotetradecane)Cl2]+ (1) and [Co(1-oxa-4,8,12-triazacyclotetradecane)Cl2]+ (2) were synthesised and characterised, and their breast CSC activity was determined. The cobalt(III) complexes 1 and 2 displayed micromolar potency towards bulk breast cancer cells and breast CSCs grown in monolayers. Notably, 1 and 2 displayed selective potency towards breast CSCs over bulk breast cancer cells (up to 4.5-fold), which was similar to salinomycin (an established breast CSC-selective agent). The cobalt(III) complexes 1 and 2 were also able to inhibit mammosphere formation at low micromolar doses (with respect to size and number). The mammopshere inhibitory effect of 2 was similar to that of salinomycin. Our studies show that cobalt(III) complexes with 1,4,7,11-tetraazacyclotetradecane and 1-oxa-4,8,12-triazacyclotetradecane macrocycles could be useful starting points for the development of new cobalt-based delivery systems that can transport cytotoxic and imaging agents into breast CSCs. Full article
(This article belongs to the Special Issue Exclusive Feature Papers in Inorganic Chemistry, 2nd Edition)
Show Figures

Figure 1

Figure 1
<p>(<b>A</b>) Reaction scheme for the preparation of [Co(1,4,7,11-tetraazacyclotetradecane)Cl<sub>2</sub>]Cl (<b>1</b>). The X-ray structure of <b>1</b> is also shown. Thermal ellipsoids are drawn at 50% probability. C atoms are shown in grey, N in dark blue, Cl in green, and Co in cobalt blue. The H atoms, co-crystallising solvent molecules, and the counter-anion have been omitted for clarity. (<b>B</b>) Reaction scheme for the preparation of [Co(1-oxa-4,8,12-triazacyclotetradecane)Cl<sub>2</sub>]½CoCl<sub>4</sub> (<b>2</b>). The X-ray structure of <b>2</b> is also shown. Thermal ellipsoids are drawn at 50% probability. C atoms are shown in grey, N in dark blue, Cl in green, O in red, and Co in cobalt blue. The H atoms and the counter-anion have been omitted for clarity.</p>
Full article ">Figure 2
<p>(<b>A</b>) Representative dose–response curves for the treatment of HMLER, HMLER-shEcad, and BEAS-2B cells with <b>1</b> after 72 h incubation; and (<b>B</b>) representative dose–response curves for the treatment of HMLER, HMLER-shEcad, and BEAS-2B cells with <b>2</b> after 72 h incubation.</p>
Full article ">Figure 3
<p>(<b>A</b>) Quantification of mammosphere formation with HMLER-shEcad cells untreated and treated with <b>1</b>, <b>2</b>, <b>3</b>, salinomycin or cisplatin (at 2 µM, 5 days). Error bars represent standard deviations; and (<b>B</b>) representative bright-field images (×10) of HMLER-shEcad mammospheres in the absence and presence of <b>1</b>, <b>2</b> or <b>3</b> (at 2 µM, 5 days).</p>
Full article ">
12 pages, 3444 KiB  
Article
Bimetallic Perthiocarbonate Complexes of Cobalt: Synthesis, Structure and Bonding
by Alaka Nanda Pradhan, Shivankan Mishra, Urminder Kaur, Bikram Keshari Rout, Jean-François Halet and Sundargopal Ghosh
Molecules 2024, 29(11), 2688; https://doi.org/10.3390/molecules29112688 - 6 Jun 2024
Viewed by 1049
Abstract
The syntheses and structural elucidation of bimetallic thiolate complexes of early and late transition metals are described. Thermolysis of the bimetallic hydridoborate species [{Cp*CoPh}{µ-TePh}{µ-TeBH3-ĸ2Te,H}{Cp*Co}] (Cp* = ɳ5-C5Me5) ( [...] Read more.
The syntheses and structural elucidation of bimetallic thiolate complexes of early and late transition metals are described. Thermolysis of the bimetallic hydridoborate species [{Cp*CoPh}{µ-TePh}{µ-TeBH3-ĸ2Te,H}{Cp*Co}] (Cp* = ɳ5-C5Me5) (1) in the presence of CS2 afforded the bimetallic perthiocarbonate complex [(Cp*Co)2(μ-CS4-κ1S:κ2S′)(μ-S2-κ2S″:κ1S‴)] (2) and the dithiolene complex [(Cp*Co)(μ-C3S5-κ1S,S′] (3). Complex 2 contains a four-membered metallaheterocycle (Co2S2) comprising a perthiocarbonate [CS4]2− unit and a disulfide [S2]2− unit, attached opposite to each other. Complex 2 was characterized by employing different multinuclear NMR, infrared spectroscopy, mass spectrometry, and single-crystal X-ray diffraction studies. Preliminary studies show that [Cp*VCl2]3 (4) with an intermediate generated from CS2 and [LiBH4·THF] yielded thiolate species, albeit different from the cobalt system. Furthermore, a computational analysis was performed to provide insight into the bonding of this bimetallic perthiocarbonate complex. Full article
(This article belongs to the Special Issue Exclusive Feature Papers in Inorganic Chemistry, 2nd Edition)
Show Figures

Graphical abstract

Graphical abstract
Full article ">Figure 1
<p>Molecular structure and labeling diagram of <b>2</b>. Selected bond lengths (Å) and bond angles (°): Co1–S4 2.200(3), Co1–S3 2.264(4), S5–S6 2.043(14), Co2–S5 2.202(4), Co2–S6 2.258(15), Co1···Co2 3.332, C41–S1 1.663(10), C41–S2 1.724(12), C41–S3 1.722(10), S2–S4 2.080(4), S3–C41–S2 119.3(6), Co1–S4–Co2 95.97(12), S4–Co1–S5 83.08(13), S5–Co2–S6 54.5(4), Co2–S5–Co1 96.91(13), S5–S6–Co2 61.4(4).</p>
Full article ">Figure 2
<p>(<b>a</b>) HOMO-12, (<b>b</b>) HOMO-17, and (<b>c</b>) HOMO-26 of <b>2</b>. Contour isodensity values for isosurface are ±0.045 (e/bohr<sup>3</sup>)<sup>1/2</sup>. (<b>d</b>,<b>e</b>), Laplacian maps of the electron density distribution computed for <b>2</b> in the Co2–S5–S6 plane and the S1–S2–S3 plane, respectively.</p>
Full article ">Figure 3
<p>UV–vis spectrum of <b>2</b> in CH<sub>2</sub>Cl<sub>2</sub>.</p>
Full article ">Figure 4
<p>Cyclic voltammogram (CV) recorded for complex <b>2</b> in DMF at 298 K.</p>
Full article ">Chart 1
<p>Different binding modes of CS<sub>2</sub>-based ligands (<b>A</b>–<b>F</b>) in transition metal complexes.</p>
Full article ">Scheme 1
<p>Synthesis of the perthiocarbonate (<b>2</b>) and dithiolene (<b>3</b>) complexes of cobalt.</p>
Full article ">
12 pages, 5726 KiB  
Article
Gallium Trichloride Fluid: Dimer Dissociation Mechanism, Local Structure, and Atomic Dynamics
by Maxim Khomenko, Anton Sokolov, Andrey Tverjanovich, Maria Bokova, Mohammad Kassem, Takeshi Usuki and Eugene Bychkov
Molecules 2024, 29(6), 1358; https://doi.org/10.3390/molecules29061358 - 19 Mar 2024
Viewed by 1131
Abstract
Molten gallium trichloride emerges as a promising solvent for oxidative metal recycling. The use of supercritical fluid enhances the performance and kinetics of metal dissolution due to significantly lower viscosity in the reaction media. Additionally, the dual molecular nature of gallium trichloride, existing [...] Read more.
Molten gallium trichloride emerges as a promising solvent for oxidative metal recycling. The use of supercritical fluid enhances the performance and kinetics of metal dissolution due to significantly lower viscosity in the reaction media. Additionally, the dual molecular nature of gallium trichloride, existing as edge-sharing ES-Ga2Cl6 dimers at low temperatures and high pressure, or flat trigonal GaCl3 monomers in the vicinity of the critical point and low pressures, creates the possibility to tailor the chemical geometry to a particular metallic species. Nevertheless, the mechanism of dimer dissociation, local structure, and atomic dynamics in supercritical gallium trichloride fluids are not known. Using first-principles molecular dynamics, validated by comparison with our high-energy X-ray diffraction results, we illustrate the elementary steps in dimer dissociation. These include the formation of intermediate corner-sharing CS-Ga2Cl6 dimers, the partial disproportionation of GaCl3 monomers at high temperatures and low pressures, changes in the local environment of molecular entities, and unusual atomic dynamics in supercritical fluids. Full article
(This article belongs to the Special Issue Exclusive Feature Papers in Inorganic Chemistry, 2nd Edition)
Show Figures

Figure 1

Figure 1
<p>Calculating the parameters of the dissociation reaction Ga<sub>2</sub>Cl<sub>6</sub> ⇌ 2GaCl<sub>3</sub> using the reported total and partial vapor pressures of Ga<sub>2</sub>Cl<sub>6</sub> and GaCl<sub>3</sub> [<a href="#B16-molecules-29-01358" class="html-bibr">16</a>]: (<b>a</b>) the dissociation constant <math display="inline"><semantics> <mrow> <msub> <mi>K</mi> <mi mathvariant="normal">m</mi> </msub> <mrow> <mo>(</mo> <mi>T</mi> <mo>)</mo> </mrow> </mrow> </semantics></math> as a function of temperature and (<b>b</b>) the molar fraction <math display="inline"><semantics> <mrow> <msub> <mi>x</mi> <mrow> <msub> <mrow> <mi>GaCl</mi> </mrow> <mn>3</mn> </msub> </mrow> </msub> <mrow> <mo>(</mo> <mi>T</mi> <mo>)</mo> </mrow> </mrow> </semantics></math> as a function of temperature under different pressure conditions. The insert in (<b>a</b>) represents one of the pressure measurement experiments [<a href="#B16-molecules-29-01358" class="html-bibr">16</a>]. The calculation details are given in the <a href="#app1-molecules-29-01358" class="html-app">Supporting Information</a>.</p>
Full article ">Figure 2
<p>FPMD-derived X-ray interference functions <math display="inline"><semantics> <mrow> <mi>Q</mi> <mo stretchy="false">[</mo> <msub> <mi>S</mi> <mi mathvariant="normal">X</mi> </msub> <mrow> <mo>(</mo> <mi>Q</mi> <mo>)</mo> </mrow> <mo>−</mo> <mn>1</mn> <mo stretchy="false">]</mo> </mrow> </semantics></math> for molten GaCl<sub>3</sub> at (<b>a</b>) 400 K and (<b>b</b>) 750 K, compared to experimental data at comparable temperatures; FPMD and experimental X-ray total correlation functions <math display="inline"><semantics> <mrow> <msub> <mi>T</mi> <mi mathvariant="normal">X</mi> </msub> <mrow> <mo>(</mo> <mi>r</mi> <mo>)</mo> </mrow> </mrow> </semantics></math> at (<b>c</b>) 400 K and (<b>d</b>) 750 K. The solid lines represent FPMD results, and the solid squares denote experimental data. The difference in the <math display="inline"><semantics> <mrow> <msub> <mi>T</mi> <mi mathvariant="normal">X</mi> </msub> <mrow> <mo>(</mo> <mi>r</mi> <mo>)</mo> </mrow> </mrow> </semantics></math> level at higher <math display="inline"><semantics> <mi>r</mi> </semantics></math> between the experimental and FPMD results is caused by variations in number density, with a significantly smaller value at 750 K (0.00902 atoms Å<sup>−3</sup>) compared to 723 K (0.013 atoms Å<sup>−3</sup>).</p>
Full article ">Figure 3
<p>Experimental (magenta) and FPMD-derived (purple) monomeric fraction <math display="inline"><semantics> <mrow> <msub> <mi>x</mi> <mrow> <msub> <mrow> <mi>GaCl</mi> </mrow> <mn>3</mn> </msub> </mrow> </msub> </mrow> </semantics></math> in liquid and supercritical gallium trichloride as a function of (<b>a</b>) temperature, and (<b>b</b>) relative pressure <math display="inline"><semantics> <mrow> <mi>P</mi> <mo>/</mo> <msub> <mi>P</mi> <mi mathvariant="normal">c</mi> </msub> </mrow> </semantics></math>; population of CS-Ga<sub>2</sub>Cl<sub>6</sub> dimers <math display="inline"><semantics> <mrow> <msub> <mi>f</mi> <mrow> <mi>CS</mi> </mrow> </msub> </mrow> </semantics></math> as a function of (<b>c</b>) temperature, and (<b>d</b>) relative pressure <math display="inline"><semantics> <mrow> <mi>P</mi> <mo>/</mo> <msub> <mi>P</mi> <mi mathvariant="normal">c</mi> </msub> </mrow> </semantics></math>.</p>
Full article ">Figure 4
<p>FPMD-derived partial pair-distribution functions <math display="inline"><semantics> <mrow> <msub> <mi>g</mi> <mrow> <mi>ij</mi> </mrow> </msub> <mrow> <mo>(</mo> <mi>r</mi> <mo>)</mo> </mrow> </mrow> </semantics></math> at (<b>a</b>) 800 K (<math display="inline"><semantics> <mrow> <mi>P</mi> <mo>/</mo> <msub> <mi>P</mi> <mi mathvariant="normal">c</mi> </msub> </mrow> </semantics></math> = 2.1) and (<b>b</b>) 800 K (<math display="inline"><semantics> <mrow> <mi>P</mi> <mo>/</mo> <msub> <mi>P</mi> <mi mathvariant="normal">c</mi> </msub> </mrow> </semantics></math> = 3.6); (<b>c</b>) fitting the Ga-Ga partial correlation function <math display="inline"><semantics> <mrow> <msub> <mi>T</mi> <mrow> <mi>GaGa</mi> </mrow> </msub> <mrow> <mo>(</mo> <mi>r</mi> <mo>)</mo> </mrow> </mrow> </semantics></math> at different temperatures and pressures; short Ga-Ga second neighbor contacts at 3.2 Å correspond to edge-sharing ES-Ga<sub>2</sub>Cl<sub>6</sub> dimers (the insert in (<b>b</b>)), and long Ga-Ga contacts at 3.8 Å correspond to corner-sharing CS-Ga<sub>2</sub>Cl<sub>6</sub> dimers (the insert in (<b>a</b>)). The Cl-Cl and Ga-Ga nearest neighbors (NNs) at 2.0 and 2.4 Å, respectively, indicate a partial disproportionation of GaCl<sub>3</sub> monomers (GaCl<sub>3</sub> ⇌ GaCl + Cl<sub>2</sub>) above the critical temperature and at lower pressure (<math display="inline"><semantics> <mrow> <mi>P</mi> <mo>/</mo> <msub> <mi>P</mi> <mi mathvariant="normal">c</mi> </msub> </mrow> </semantics></math> = 2.1).</p>
Full article ">Figure 5
<p>Schematics of ① ES-Ga<sub>2</sub>Cl<sub>6</sub> dimer dissociation and ② GaCl<sub>3</sub> monomer disproportionation.</p>
Full article ">Figure 6
<p>FPMD-derived bond angle distributions: <math display="inline"><semantics> <mrow> <msub> <mi>B</mi> <mrow> <mi>ClGaCl</mi> </mrow> </msub> <mrow> <mo>(</mo> <mi>θ</mi> <mo>)</mo> </mrow> </mrow> </semantics></math> for (<b>a</b>) four-fold Ga<sub>4F</sub> and (<b>b</b>) three-fold Ga<sub>3F</sub> coordinated gallium species at different temperatures; (<b>c</b>) <math display="inline"><semantics> <mrow> <msub> <mi>B</mi> <mrow> <mi>GaClGa</mi> </mrow> </msub> <mrow> <mo>(</mo> <mi>θ</mi> <mo>)</mo> </mrow> </mrow> </semantics></math> for Ga<sub>4F</sub> atoms at 400, 750, and 800 K; and (<b>d</b>) <math display="inline"><semantics> <mrow> <msub> <mi>B</mi> <mrow> <mi>GaGaCl</mi> </mrow> </msub> <mrow> <mo>(</mo> <mi>θ</mi> <mo>)</mo> </mrow> </mrow> </semantics></math> at 800 K (<math display="inline"><semantics> <mrow> <mi>P</mi> <mo>/</mo> <msub> <mi>P</mi> <mi mathvariant="normal">c</mi> </msub> </mrow> </semantics></math> = 2.1). The insert in d shows a transient species GaCl<sub>3</sub> + GaCl. See the text for further details.</p>
Full article ">Figure 7
<p>Orientational order parameter <math display="inline"><semantics> <mi>q</mi> </semantics></math> for 4-fold Ga<sub>4F</sub> and 3-fold Ga<sub>3F</sub> coordinated Ga-Cl entities: (<b>a</b>) Ga<sub>4F</sub> at 400 K, (<b>b</b>) Ga<sub>3F</sub> at 750 K, (<b>c</b>) Ga<sub>4F</sub> at 800 K (<math display="inline"><semantics> <mrow> <mi>P</mi> <mo>/</mo> <msub> <mi>P</mi> <mi mathvariant="normal">c</mi> </msub> </mrow> </semantics></math> = 2.1), and (<b>d</b>) Ga<sub>3F</sub> at 800 K (<math display="inline"><semantics> <mrow> <mi>P</mi> <mo>/</mo> <msub> <mi>P</mi> <mi mathvariant="normal">c</mi> </msub> </mrow> </semantics></math> = 2.1). The inserts show typical Ga-Cl units of different symmetry. See the text for further details.</p>
Full article ">Figure 8
<p>Gallium <math display="inline"><semantics> <mrow> <mo stretchy="false">〈</mo> <msubsup> <mi>r</mi> <mrow> <mi>G</mi> <mi>a</mi> </mrow> <mn>2</mn> </msubsup> <mrow> <mo>(</mo> <mi>t</mi> <mo>)</mo> </mrow> <mo stretchy="false">〉</mo> </mrow> </semantics></math> and chlorine <math display="inline"><semantics> <mrow> <mo stretchy="false">〈</mo> <msubsup> <mi>r</mi> <mrow> <mi>Cl</mi> </mrow> <mn>2</mn> </msubsup> <mrow> <mo>(</mo> <mi>t</mi> <mo>)</mo> <mo stretchy="false">〉</mo> </mrow> </mrow> </semantics></math> mean-square displacements on (<b>a</b>) log–log and (<b>b</b>) linear scales; (<b>c</b>) experimental GaCl<sub>3</sub> viscosity <math display="inline"><semantics> <mrow> <mi>η</mi> <mrow> <mo>(</mo> <mrow> <mi>T</mi> <mo>,</mo> <mi>P</mi> </mrow> <mo>)</mo> </mrow> </mrow> </semantics></math> at ambient pressure between 340 and 363 K [<a href="#B25-molecules-29-01358" class="html-bibr">25</a>], and DFT-derived viscosity at 800 K and different pressure (2.1 ≤ <math display="inline"><semantics> <mrow> <mi>P</mi> <mo>/</mo> <msub> <mi>P</mi> <mi mathvariant="normal">c</mi> </msub> </mrow> </semantics></math> ≤ 3.6) (this work). See the text for further details.</p>
Full article ">
10 pages, 2445 KiB  
Article
Synthesis of Alkenylgold(I) Complexes Relevant to Catalytic Carboxylative Cyclization of Unsaturated Amines and Alcohols
by Shun Hase, Kyohei Yamashita and Yoshihito Kayaki
Molecules 2024, 29(6), 1331; https://doi.org/10.3390/molecules29061331 - 16 Mar 2024
Viewed by 1241
Abstract
The carboxylation of unsaturated amine and alcohol compounds, including 4-benzylamino-1-phenyl-1-butyne (homopropargylamine), 2-butyne-1-ol (propargylic alcohol), and 2,3-butadiene-1-ol (allenylmethyl alcohol), using the hydroxidogold(I) complex, AuOH(IPr) [IPr = 1,3-bis(2,6-diisopropylphenyl)-imidazol-2-ylidene], produces corresponding alkenylgold(I) complexes with a cyclic urethane or carbonate framework in high yields. The reaction takes [...] Read more.
The carboxylation of unsaturated amine and alcohol compounds, including 4-benzylamino-1-phenyl-1-butyne (homopropargylamine), 2-butyne-1-ol (propargylic alcohol), and 2,3-butadiene-1-ol (allenylmethyl alcohol), using the hydroxidogold(I) complex, AuOH(IPr) [IPr = 1,3-bis(2,6-diisopropylphenyl)-imidazol-2-ylidene], produces corresponding alkenylgold(I) complexes with a cyclic urethane or carbonate framework in high yields. The reaction takes place in aprotic THF at room temperature under the atmospheric pressure of CO2 in the absence of base additives. The products were characterized by NMR spectroscopy, elemental analysis, and X-ray crystallography. The functionalized alkenyl complexes prepared from the alkynes can be protonated by treatment with an equimolar amount of acetic acid to afford five- or six-membered carboxylation products, whereas the related alkenyl complex derived from allenylmethyl alcohol decomposed to recover the starting allene via ring-opening decarboxylation. Full article
(This article belongs to the Special Issue Exclusive Feature Papers in Inorganic Chemistry, 2nd Edition)
Show Figures

Graphical abstract

Graphical abstract
Full article ">Figure 1
<p>X-ray crystal structure of <b>7</b>. The hydrogen atoms are omitted for clarity. Thermal ellipsoids are shown at the 30% probability level.</p>
Full article ">Figure 2
<p>X-ray crystal structure of <b>9</b>. The hydrogen atoms are omitted for clarity. Thermal ellipsoids are shown at the 30% probability level.</p>
Full article ">Figure 3
<p>X-ray crystal structure of <b>11</b>. The hydrogen atoms are omitted for clarity. Thermal ellipsoids are shown at the 30% probability level.</p>
Full article ">Scheme 1
<p>Au-catalyzed carboxylative cyclization of propargylamines.</p>
Full article ">Scheme 2
<p>Synthesis of alkenylgold complexes using propargylic amine (<b>A</b>) and allenylmethylamine (<b>B</b>) as catalytic intermediates.</p>
Full article ">Scheme 3
<p>Synthesis of alkenylgold <b>7</b> from <b>1</b>, homopropargylamine, and CO<sub>2</sub>.</p>
Full article ">Scheme 4
<p>Synthesis of alkenylgold <b>9</b> from <b>1</b>, propargylic alcohol, and CO<sub>2</sub>.</p>
Full article ">Scheme 5
<p>Synthesis of alkenylgold <b>11</b> from <b>1</b>, allenylmethyl alcohol, and CO<sub>2</sub>.</p>
Full article ">Scheme 6
<p>Protonolysis of alkenylgold complexes <b>7</b>, <b>9</b>, and <b>11</b>.</p>
Full article ">
18 pages, 3579 KiB  
Article
Metal Complexes Containing Homoleptic Diorganoselenium(II) Ligands: Synthesis, Characterization and Investigation of Optical Properties
by Darius Dumitraș, Emese Gal, Cristian Silvestru and Alexandra Pop
Molecules 2024, 29(4), 792; https://doi.org/10.3390/molecules29040792 - 8 Feb 2024
Viewed by 1265
Abstract
[(Z)-2′-{2-C6H5-(4H)-oxazol-5-one}CHC6H4]2Se (5, L1) and [(Z)-4′-{2-C6H5-(4H)-oxazol-5-one}CHC6H4]2Se (6, L [...] Read more.
[(Z)-2′-{2-C6H5-(4H)-oxazol-5-one}CHC6H4]2Se (5, L1) and [(Z)-4′-{2-C6H5-(4H)-oxazol-5-one}CHC6H4]2Se (6, L2) were prepared, structurally characterized and used as ligands to obtain new metal complexes of types [MX(Ln)] [L1: M = Ag, X = OTf (7); M = Au, X = Cl (13); L2: M = Ag, X = OTf (8); M = Au, X = Cl (14)], [(MX)2(Ln)] [M = Ag, X = OTf, L1 (9); L2 (10)], [ZnCl2(Ln)] [L1 (15); L2 (16)] and [Ag(Ln)][PF6] [L1 (11); L2 (12)]. The silver complexes 7 and 8 were ionic species (1:1 electrolytes) in a MeCN solution, while in the solid state, the triflate fragments were bonded to the silver cations. Similarly, the 2:1 complexes 9 and 10 were found to behave as 1:2 electrolytes in a MeCN solution, but single-crystal X-ray diffraction demonstrated that compound 9 showed the formation of a dimer in the solid state: a tetranuclear [Ag(OTf)]4 built through bridging triflate ligands was coordinated by two bridging organoselenium ligands through the nitrogen from the oxazolone ring and the selenium atoms in a 1κN:2κSe fashion. Supramolecular architectures supported by intermolecular C−H∙∙∙π, C−H∙∙∙O, Cl∙∙∙H and F∙∙∙H interactions were observed in compounds 4, 5 and 9. The compounds exhibited similar photophysical properties, with a bathochromic shift in the UV-Vis spectra caused by the position of the oxazolone ring on the phenyl ring attached to the selenium atoms. Full article
(This article belongs to the Special Issue Exclusive Feature Papers in Inorganic Chemistry, 2nd Edition)
Show Figures

Figure 1

Figure 1
<p>(<b>a</b>) Normalized UV–Vis absorption spectra of <b>5</b>, <b>7</b>, <b>11</b>, <b>13</b> and <b>15</b>; (<b>b</b>) normalized emission spectra of <b>5</b>, <b>7</b>, <b>11</b>, <b>13</b> and <b>15</b>; (<b>c</b>) normalized absorption and emission spectra of <b>13</b>, and (<b>d</b>) normalized emission spectra of <b>15</b> and <b>16</b>.</p>
Full article ">Figure 2
<p>Thermal ellipsoid (probability 50%) representation of the molecular structure of compound <b>4</b>. Hydrogen atoms, except those of the aldehyde substituents, were omitted for clarity. Selected bond lengths (Å) and angles (°): Se1‒C1 1.916(2); Se1‒C8 1.907(2); C7‒O1 1.182(3); C14‒O2 1.220(3); C1‒Se1‒C8 101.15(9).</p>
Full article ">Figure 3
<p>Polymeric chain association in the crystal of <b>4</b> [symmetry equivalent positions (−1/2+x, 3/2−y, −1/2+z) and (1/2+x, 3/2−y, 1/2+z) are given by “prime” and “double prime”, respectively]. Only the hydrogen atoms of the aldehyde substituents and those involved in intermolecular interactions are shown.</p>
Full article ">Figure 4
<p>Thermal ellipsoid (probability 50%) representation of the molecular structure of compound <b>5</b> [symmetry equivalent position (−x, 1−y, z) is given by “prime”]. Hydrogen atoms, except those attached to the C7 and C7ʹatoms, were omitted for clarity. Selected bond lengths (Å) and angles (°): Se1‒C1 1.946(3); O1‒C9 1.399(4); O1‒C10 1.385(4); O2‒C9 1.193(4); N1‒C8 1.401(4); N1‒C10 1.295(4); C2‒C7 1.453(4); C7‒C8 1.354(4); C8‒C9 1.474(4); C1‒Se1‒C1’ 96.02(18); O1‒C9‒C8 104.5(3); C9‒O1‒C10 105.6(2); O1‒C10‒N1 116.0(3); C8‒N1‒C10 105.2(3); N1‒C8‒C9 108.7(3); C7‒C8‒C9 121.7(3); O2‒C9‒C8 133.6(3); O1‒C9‒O2 122.0(3).</p>
Full article ">Figure 5
<p>Thermal ellipsoid (probability 50%) representation of the molecular structure of <b>9</b>·4CHCl<sub>3</sub> in the asymmetric unit. Hydrogen atoms and the molecules of CHCl<sub>3</sub> were omitted for clarity.</p>
Full article ">Figure 6
<p>Tetranuclear structure in the crystal of <b>9</b>·4CHCl<sub>3</sub> [symmetry equivalent position (2−x, 1−y, 1−z) is given by “prime”]. Hydrogen atoms and the molecules of CHCl<sub>3</sub> were omitted for clarity.</p>
Full article ">Scheme 1
<p>Synthesis of diorganoselenium(II) compounds <b>1</b>–<b>6</b>.</p>
Full article ">Scheme 2
<p>Synthesis of complexes <b>7</b>–<b>16</b>: <span class="html-italic">(i)</span> and <span class="html-italic">(ii)</span> acetone; <span class="html-italic">(iii)</span> and <span class="html-italic">(iv)</span> CH<sub>3</sub>Cl; <span class="html-italic">(<b>v</b>)</span> CH<sub>3</sub>Cl/EtOH.</p>
Full article ">Scheme 3
<p>Numbering scheme for NMR assignments in compounds <b>1</b>–<b>16</b>.</p>
Full article ">
15 pages, 2985 KiB  
Article
New Stable Gallium(III) and Indium(III) Complexes with Thiosemicarbazone Ligands: A Biological Evaluation
by Lorenzo Verderi, Mirco Scaccaglia, Martina Rega, Cristina Bacci, Silvana Pinelli, Giorgio Pelosi and Franco Bisceglie
Molecules 2024, 29(2), 497; https://doi.org/10.3390/molecules29020497 - 19 Jan 2024
Cited by 1 | Viewed by 2076
Abstract
The aim of this work is to explore a new library of coordination compounds for medicinal applications. Gallium is known for its various applications in this field. Presently, indium is not particularly important in medicine, but it shares a lot of chemical traits [...] Read more.
The aim of this work is to explore a new library of coordination compounds for medicinal applications. Gallium is known for its various applications in this field. Presently, indium is not particularly important in medicine, but it shares a lot of chemical traits with its above-mentioned lighter companion, gallium, and is also used in radio imaging. These metals are combined with thiosemicarbazones, ligating compounds increasingly known for their biological and pharmaceutical applications. In particular, the few ligands chosen to interact with these hard metal ions share the ideal affinity for a high charge density. Therefore, in this work we describe the synthesis and the characterization of the resulting coordination compounds. The yields of the reactions vary from a minimum of 21% to a maximum of 82%, using a fast and easy procedure. Nuclear Magnetic Resonance (NMR) and Infra Red (IR) spectroscopy, mass spectrometry, elemental analysis, and X-ray Diffraction (XRD) confirm the formation of stable compounds in all cases and a ligand-to-metal 2:1 stoichiometry with both cations. In addition, we further investigated their chemical and biological characteristics, via UV-visible titrations, stability tests, and cytotoxicity and antibiotic assays. The results confirm a strong stability in all explored conditions, which suggests that these compounds are more suitable for radio imaging applications rather than for antitumoral or antimicrobic ones. Full article
(This article belongs to the Special Issue Exclusive Feature Papers in Inorganic Chemistry, 2nd Edition)
Show Figures

Figure 1

Figure 1
<p>Chosen thiosemicarbazonic ligands for Ga(III) and In(III) coordination, previously described [<a href="#B27-molecules-29-00497" class="html-bibr">27</a>].</p>
Full article ">Figure 2
<p>Representation of the cationic moiety of <b>In1</b> complex.</p>
Full article ">Figure 3
<p>Plausible structure of the synthesized compounds, according to characterization and <b>In1</b> XRD information.</p>
Full article ">Figure 3 Cont.
<p>Plausible structure of the synthesized compounds, according to characterization and <b>In1</b> XRD information.</p>
Full article ">Figure 4
<p>Titration profiles of the synthesized coordination compounds (* the baseline raised through the titration due to slight formation of precipitate).</p>
Full article ">Figure 5
<p>Stability assays of the coordination compounds.</p>
Full article ">Figure 5 Cont.
<p>Stability assays of the coordination compounds.</p>
Full article ">
16 pages, 3688 KiB  
Article
Aluminium 8-Hydroxyquinolinate N-Oxide as a Precursor to Heterometallic Aluminium–Lanthanide Complexes
by Elisa Gallo, Luca Bellucci, Silvia Carlotto, Gregorio Bottaro, Luca Babetto, Luca Giordano, Fabio Marchetti, Simona Samaritani, Lidia Armelao and Luca Labella
Molecules 2024, 29(2), 451; https://doi.org/10.3390/molecules29020451 - 17 Jan 2024
Cited by 2 | Viewed by 2058
Abstract
A reaction in anhydrous toluene between the formally unsaturated fragment [Ln(hfac)3] (Ln3+ = Eu3+, Gd3+ and Er3+; Hhfac = hexafluoroacetylacetone) and [Al(qNO)3] (HqNO = 8-hydroxyquinoline N-oxide), here prepared for the first time [...] Read more.
A reaction in anhydrous toluene between the formally unsaturated fragment [Ln(hfac)3] (Ln3+ = Eu3+, Gd3+ and Er3+; Hhfac = hexafluoroacetylacetone) and [Al(qNO)3] (HqNO = 8-hydroxyquinoline N-oxide), here prepared for the first time from [Al(OtBu)3] and HqNO, affords the dinuclear heterometallic compounds [Ln(hfac)3Al(qNO)3] (Ln3+ = Eu3+, Gd3+ and Er3+) in high yields. The molecular structures of these new compounds revealed a dinuclear species with three phenolic oxygen atoms bridging the two metal atoms. While the europium and gadolinium complexes show the coordination number (CN) 9 for the lanthanide centre, in the complex featuring the smaller erbium ion, only two oxygens bridge the two metal atoms for a resulting CN of 8. The reaction of [Eu(hfac)3] with [Alq3] (Hq = 8-hydroxyquinoline) in the same conditions yields a heterometallic product of composition [Eu(hfac)3Alq3]. A recrystallization attempt from hot heptane in air produced single crystals of two different morphologies and compositions: [Eu2(hfac)6Al2q4(OH)2] and [Eu2(hfac)6(µ-Hq)2]. The latter compound can be directly prepared from [Eu(hfac)3] and Hq at room temperature. Quantum mechanical calculations confirm (i) the higher stability of [Eu(hfac)3Al(qNO)3] vs. the corresponding [Eu(hfac)3Alq3] and (ii) the preference of the Er complexes for the CN 8, justifying the different behaviour in terms of the Lewis acidity of the metal centre. Full article
(This article belongs to the Special Issue Exclusive Feature Papers in Inorganic Chemistry, 2nd Edition)
Show Figures

Graphical abstract

Graphical abstract
Full article ">Figure 1
<p>Molecular structure of the two independent molecules of [Eu<sub>2</sub>(hfac)<sub>6</sub>Al<sub>2</sub>q<sub>4</sub>(OH)<sub>2</sub>] (light green, europium; pink, aluminium; grey, carbon; red, oxygen; blue, nitrogen; yellow, fluorine).</p>
Full article ">Figure 2
<p>Polyhedral representation of [Eu<sub>2</sub>(hfac)<sub>6</sub>Al<sub>2</sub>q<sub>4</sub>(OH)<sub>2</sub>], <b>2</b> (light green, europium; pink, aluminium; grey, carbon; red, oxygen; blue, nitrogen; yellow, fluorine).</p>
Full article ">Figure 3
<p>Molecular structure of [Eu<sub>2</sub>(hfac)<sub>6</sub>(µ-Hq)<sub>2</sub>], <b>3</b> (light green, europium; pink, aluminium; grey, carbon; red, oxygen; blue, nitrogen; yellow, fluorine).</p>
Full article ">Figure 4
<p>(<b>Left</b>) molecular structure of [Eu(hfac)<sub>3</sub>Al(qNO)<sub>3</sub>], <b>5</b>; (<b>Right</b>) projection along an approximated ternary axis. Lattice toluene has been omitted for clarity, (light green, europium; pink, aluminium; grey, carbon; red, oxygen; blue, nitrogen; yellow, fluorine).</p>
Full article ">Figure 5
<p>ATR-IR of [Er(hfac)<sub>3</sub>Al(qNO)<sub>3</sub>] (orange) and [Eu(hfac)<sub>3</sub>Al(qNO)<sub>3</sub>] (blue).</p>
Full article ">Figure 6
<p>Molecular structure of [Er(hfac)<sub>3</sub>Al(qNO)<sub>3</sub>], <b>7</b>, with a polyhedral representation on the right, (green, erbium; pink, aluminium; grey, carbon; red, oxygen; blue, nitrogen; yellow, fluorine).</p>
Full article ">Scheme 1
<p>8-hydroxyquinoline (Hq) and the aluminium complex [Alq<sub>3</sub>].</p>
Full article ">Scheme 2
<p>8-hydroxyquinoline <span class="html-italic">N</span>-oxide (HqNO).</p>
Full article ">Scheme 3
<p>Hydrolytic path for decomposition of [Eu(hfac)<sub>3</sub>Alq<sub>3</sub>], <b>1</b>.</p>
Full article ">
19 pages, 3055 KiB  
Article
Photocatalytic Reduction of CO2 into CO with Cyclometalated Pt(II) Complexes of N^C^N Pincer Dipyridylbenzene Ligands: A DFT Study
by Antonia Sarantou and Athanassios Tsipis
Molecules 2024, 29(2), 403; https://doi.org/10.3390/molecules29020403 - 14 Jan 2024
Viewed by 1481
Abstract
In this work, density functional theory (DFT) calculations were employed to study the photocatalytic reduction of CO2 into CO using a series of Pt(II) square planar complexes with the general formula [Pt(5-R-dpb)Cl] (dpb = 1,3-di(2-pyridyl)benzene anion, R = H, N,N [...] Read more.
In this work, density functional theory (DFT) calculations were employed to study the photocatalytic reduction of CO2 into CO using a series of Pt(II) square planar complexes with the general formula [Pt(5-R-dpb)Cl] (dpb = 1,3-di(2-pyridyl)benzene anion, R = H, N,N-dimethylaniline,T thiophene, diazaborinine). The CO2-into-CO conversion process is thought to proceed via two main steps, namely the photocatalytic/reduction step and the main catalytic step. The simulated absorption spectra exhibit strong bands in the range 280–460 nm of the UV-Vis region. Reductive quenching of the T1 state of the complexes under study is expected to be favorable since the calculated excited state redox potentials for the reaction with sacrificial electron donors are highly positive. The redox potentials reveal that the reductive quenching of the T1 state, important to the overall process, could be modulated by suitable changes in the N^C^N pincer ligands. The CO2 fixation and activation by the three coordinated Pt(II) catalytically active species are predicted to be favorable, with the Pt–CO2 bond dissociation energies D0 in the range of −36.9–−10.3 kcal/mol. The nature of the Pt–CO2 bond of the Pt(II) square planar intermediates is complex, with covalent, hyperconjugative and H-bonding interactions prevailing over the repulsive electrostatic interactions. The main catalytic cycle is estimated to be a favorable exergonic process. Full article
(This article belongs to the Special Issue Exclusive Feature Papers in Inorganic Chemistry, 2nd Edition)
Show Figures

Figure 1

Figure 1
<p>Proposed calculated mechanism for the CO<sub>2</sub>-into-CO photocatalytic reduction by the [Pt(5-R-dpb)Cl], <b>1</b>–<b>5</b> Pt(II) complexes.</p>
Full article ">Figure 2
<p>Optimized geometries of <b>1</b> in (<b>a</b>) S<sub>0</sub> ground state, (<b>b</b>) in T<sub>1</sub> excited state and (<b>c</b>) of One-Electron-Reduced form, <b>1_OER</b>, calculated at the PBE0-GD3BJ/Def2-TZVP level, in DCM solvent.</p>
Full article ">Figure 3
<p>Simulated absorption spectra of <b>1</b>–<b>4</b> in DCM at the TDDFT/PBE0/Def2-TZVP level.</p>
Full article ">Figure 4
<p>NTO pairs for the most significant electronic transitions of the simulated absorption spectra of <b>1</b> (hole <span class="html-italic">h</span><sup>+</sup> on the left, electron <span class="html-italic">e<sup>−</sup></span> on the right).</p>
Full article ">Figure 5
<p>(<b>a</b>) Optimized geometry of <b>1_ImC</b>, (<b>b</b>) 3D surface plot of HOMO, (<b>c</b>) BCPs (orange spheres) and (<b>d</b>) 3D surface of RDG function.</p>
Full article ">Figure 6
<p>3D isosurface plots of (<b>a</b>) <span class="html-italic">σ</span>(Pt–C) BD NBO and (<b>b</b>) of donor and acceptor NBOs participating in the Pt–C hyperconjugative interactions.</p>
Full article ">Figure 7
<p>Free energy, Δ<span class="html-italic">G</span> (in kcal/mol), reaction profiles of <b>1</b>–<b>4</b> in DCM solvent calculated at the PBE0-GD3BJ/Def2-TZVP level (numbers in blue for <b>1</b>, in green for <b>2</b>, in orange for <b>3</b> and in red for <b>4</b>).</p>
Full article ">Scheme 1
<p>The molecular structures of Pt(II) complexes under study.</p>
Full article ">Scheme 2
<p>Born–Haber cycle for calculation of ground-state reduction potentials <span class="html-italic">E</span><sup>0</sup><sub>red</sub> (<b>above</b>), Latimer diagram for the calculation of T<sub>1</sub> excited state reduction potentials <span class="html-italic">E</span><sup>0*</sup><sub>red</sub> (<b>middle</b>) and Born–Haber cycle for calculation of sacrificial electron donor <span class="html-italic">D</span> (=TEOA or TEA) reduction potentials (<b>below</b>).</p>
Full article ">Scheme 3
<p>Orbital interaction diagram for the formation of <b>1_ImC</b> (Complex) from fragments [Pt(dpb)]<sup>−</sup> (Fragm. 1) and CO<sub>2</sub> (Fragm. 2).</p>
Full article ">Scheme 4
<p>(<b>a</b>) SOMO<span class="html-italic"><sup>β</sup></span> of <b>1_T<sub>1</sub></b> species (<b>left</b>) and SOMO of <b>1_OER</b> (<b>right</b>) and (<b>b</b>) LUMO of <b>1_ImF</b> (<b>left</b>) and SOMO<span class="html-italic"><sup>β</sup></span> of <b>1_G</b> (<b>right</b>).</p>
Full article ">
13 pages, 3248 KiB  
Article
{GdIII7} and {GdIII14} Cluster Formation Based on a Rhodamine 6G Ligand with a Magnetocaloric Effect
by Lin Miao, Cai-Ming Liu and Hui-Zhong Kou
Molecules 2024, 29(2), 389; https://doi.org/10.3390/molecules29020389 - 12 Jan 2024
Cited by 2 | Viewed by 1128
Abstract
Heptanuclear {GdIII7} (complex 1) and tetradecanuclear {GdIII14} (complex 2) were synthesized using the rhodamine 6G ligand HL (rhodamine 6G salicylaldehyde hydrazone) and characterized. Complex 1 has a rare disc-shaped structure, where the central Gd ion [...] Read more.
Heptanuclear {GdIII7} (complex 1) and tetradecanuclear {GdIII14} (complex 2) were synthesized using the rhodamine 6G ligand HL (rhodamine 6G salicylaldehyde hydrazone) and characterized. Complex 1 has a rare disc-shaped structure, where the central Gd ion is connected to the six peripheral GdIII ions via CH3O3-OH bridges. Complex 2 has an unexpected three-layer double sandwich structure with a rare μ6-O2− ion in the center of the cluster. Magnetic studies revealed that complex 1 exhibits a magnetic entropy change of 17.4 J kg−1 K−1 at 3 K and 5 T. On the other hand, complex 2 shows a higher magnetic entropy change of 22.3 J kg−1 K−1 at 2 K and 5 T. Full article
(This article belongs to the Special Issue Exclusive Feature Papers in Inorganic Chemistry, 2nd Edition)
Show Figures

Figure 1

Figure 1
<p>Transformation of ring-opened and ring-closed form of rhodamine-6G-type ligands and their reactions.</p>
Full article ">Figure 2
<p>UV-Vis (<b>a</b>) and fluorescent spectra (λ<sub>ex</sub> = 354 nm) (<b>b</b>) for the ligand HL and the reaction mixture containing HL and Gd(NO<sub>3</sub>)<sub>3</sub> with different amounts of Et<sub>3</sub>N in MeOH.</p>
Full article ">Figure 3
<p>(<b>a</b>) The structure of the {Gd<sup>III</sup><sub>7</sub>} cation for complex <b>1</b>. Hydrogen atoms and solvents have been omitted for clarity. (<b>b</b>) The core skeleton graph of complex <b>1</b>. Color code: Gd<sup>III</sup> green; O red; N blue; C gray.</p>
Full article ">Figure 4
<p>Schematic diagram of two different coordination modes of ring-closed rhodamine ligands L<sup>−</sup>. (<b>a</b>) Tridentate chelating mode; (<b>b</b>) phenolic oxygen bridging mode.</p>
Full article ">Figure 5
<p>(<b>a</b>) The structure of complex <b>2</b>. Hydrogen atoms and solvents have been omitted for clarity. (<b>b</b>) The core skeleton of complex <b>2</b>. Color code: Gd<sup>III</sup> green; O red; N blue; C gray.</p>
Full article ">Figure 6
<p>Temperature dependence of <span class="html-italic">χ</span><sub>M</sub><span class="html-italic">T</span> for {Gd<sub>7</sub>} and {Gd<sub>14</sub>} under a 1000 Oe magnetic field in the range of 2–300 K.</p>
Full article ">Figure 7
<p>Experimental −Δ<span class="html-italic">S</span><sub>m</sub> values of <b>1</b> (<b>a</b>) and <b>2</b> (<b>b</b>) for multiple temperatures and magnetic fields calculated from magnetization data.</p>
Full article ">
13 pages, 1490 KiB  
Article
Cd2+-Selective Fluorescence Enhancement of Bisquinoline Derivatives with 2-Aminoethanol Skeleton
by Yuji Mikata, Aya Tsuruta, Hinata Koike, Sunao Shoji and Hideo Konno
Molecules 2024, 29(2), 369; https://doi.org/10.3390/molecules29020369 - 11 Jan 2024
Cited by 1 | Viewed by 1060
Abstract
The development of fluorescent Cd2+ sensors requires strict selectivity over Zn2+ because of the high availability of Zn2+ in the natural environment. In this paper, bisquinoline-based fluorescent sensors with a 2-aminoethanol backbone were investigated. The weak coordination ability of quinoline [...] Read more.
The development of fluorescent Cd2+ sensors requires strict selectivity over Zn2+ because of the high availability of Zn2+ in the natural environment. In this paper, bisquinoline-based fluorescent sensors with a 2-aminoethanol backbone were investigated. The weak coordination ability of quinoline compared to well-studied pyridine is suitable for Cd2+ selectivity rather than Zn2+. In the presence of 3 equiv. of metal ions, TriMeO-N,O-BQMAE (N,O-bis(5,6,7-trimethoxy-2-quinolylmethyl)-2-methylaminoethanol (3)), as well as its N,N-isomer TriMeO-N,N-BQMAE (N,N-bis(5,6,7-trimethoxy-2-quinolylmethyl)-2-methoxyethylamine (6)), exhibits Cd2+-selective fluorescence enhancement over Zn2+ in DMF-HEPES buffer (1:1, 50 mM HEPES, 0.1 M KCl, pH = 7.5) (IZn/ICd = 26–34%), which has similar selectivity in comparison to the corresponding ethylenediamine derivative TriMeOBQDMEN (N,N’-bis(5,6,7-trimethoxy-2-quinolylmethyl)-N,N’-dimethylethylenediamine) under the same experimental condition (IZn/ICd = 24%). The fluorescence mechanisms of N,O- and N,N-isomers of BQMAE are quite different, judging from the fluorescence lifetimes of their metal complexes. The Cd2+ complex with TriMeO-N,O-BQMAE (3) exhibits a long fluorescence lifetime similar to that of TriMeOBQDMEN via intramolecular excimer emission, whereas the Cd2+ complex with TriMeO-N,N-BQMAE (6) exhibits a short lifetime from monomer emission. Full article
(This article belongs to the Special Issue Exclusive Feature Papers in Inorganic Chemistry, 2nd Edition)
Show Figures

Figure 1

Figure 1
<p>(<b>a</b>,<b>c</b>,<b>e</b>,<b>g</b>) Fluorescence spectral changes and (<b>b</b>,<b>d</b>,<b>f</b>,<b>h</b>) relative fluorescence intensity of 34 µM (<b>a</b>,<b>b</b>) <span class="html-italic">N,O</span>-BQMAE (<b>1</b>) (λ<sub>ex</sub> = 317 nm), (<b>c</b>,<b>d</b>) 6-MeO<span class="html-italic">-N,O</span>-BQMAE (<b>2</b>) (λ<sub>ex</sub> = 336 nm), (<b>e</b>,<b>f</b>) TriMeO-<span class="html-italic">N,O</span>-BQMAE (<b>3</b>) (λ<sub>ex</sub> = 338 nm), and (<b>g</b>,<b>h</b>) TriMeOBQDMEN (λ<sub>ex</sub> = 335 nm) in DMF-HEPES buffer (1:1, 50 mM HEPES, 0.1 M KCl, pH = 7.5) at 25 °C (<b>a</b>,<b>c</b>,<b>e</b>,<b>g</b>) in the presence of increasing concentrations of Cd<sup>2+</sup> and (<b>b</b>,<b>d</b>,<b>f</b>,<b>h</b>) in the presence of 3 equiv. of metal ions. <span class="html-italic">I</span><sub>0</sub> is the emission intensity of free ligand.</p>
Full article ">Figure 1 Cont.
<p>(<b>a</b>,<b>c</b>,<b>e</b>,<b>g</b>) Fluorescence spectral changes and (<b>b</b>,<b>d</b>,<b>f</b>,<b>h</b>) relative fluorescence intensity of 34 µM (<b>a</b>,<b>b</b>) <span class="html-italic">N,O</span>-BQMAE (<b>1</b>) (λ<sub>ex</sub> = 317 nm), (<b>c</b>,<b>d</b>) 6-MeO<span class="html-italic">-N,O</span>-BQMAE (<b>2</b>) (λ<sub>ex</sub> = 336 nm), (<b>e</b>,<b>f</b>) TriMeO-<span class="html-italic">N,O</span>-BQMAE (<b>3</b>) (λ<sub>ex</sub> = 338 nm), and (<b>g</b>,<b>h</b>) TriMeOBQDMEN (λ<sub>ex</sub> = 335 nm) in DMF-HEPES buffer (1:1, 50 mM HEPES, 0.1 M KCl, pH = 7.5) at 25 °C (<b>a</b>,<b>c</b>,<b>e</b>,<b>g</b>) in the presence of increasing concentrations of Cd<sup>2+</sup> and (<b>b</b>,<b>d</b>,<b>f</b>,<b>h</b>) in the presence of 3 equiv. of metal ions. <span class="html-italic">I</span><sub>0</sub> is the emission intensity of free ligand.</p>
Full article ">Figure 2
<p>(<b>a</b>,<b>c</b>,<b>e</b>) Fluorescence spectral changes and (<b>b</b>,<b>d</b>,<b>f</b>) relative fluorescence intensity of 34 µM (<b>a</b>,<b>b</b>) <span class="html-italic">N,N</span>-BQMAE (<b>4</b>) (λ<sub>ex</sub> = 317 nm), (<b>c</b>,<b>d</b>) 6-MeO<span class="html-italic">-N,N</span>-BQMAE (<b>5</b>) (λ<sub>ex</sub> = 337 nm), and (<b>e</b>,<b>f</b>) TriMeO-<span class="html-italic">N,N</span>-BQMAE (<b>6</b>) (λ<sub>ex</sub> = 340 nm) in DMF-HEPES buffer (1:1, 50 mM HEPES, 0.1 M KCl, pH = 7.5) at 25 °C (<b>a</b>,<b>c</b>,<b>e</b>) in the presence of increasing concentrations of Cd<sup>2+</sup> and (<b>b</b>,<b>d</b>,<b>f</b>) in the presence of 3 equiv. of metal ions. <span class="html-italic">I</span><sub>0</sub> is the emission intensity of free ligand.</p>
Full article ">Figure 2 Cont.
<p>(<b>a</b>,<b>c</b>,<b>e</b>) Fluorescence spectral changes and (<b>b</b>,<b>d</b>,<b>f</b>) relative fluorescence intensity of 34 µM (<b>a</b>,<b>b</b>) <span class="html-italic">N,N</span>-BQMAE (<b>4</b>) (λ<sub>ex</sub> = 317 nm), (<b>c</b>,<b>d</b>) 6-MeO<span class="html-italic">-N,N</span>-BQMAE (<b>5</b>) (λ<sub>ex</sub> = 337 nm), and (<b>e</b>,<b>f</b>) TriMeO-<span class="html-italic">N,N</span>-BQMAE (<b>6</b>) (λ<sub>ex</sub> = 340 nm) in DMF-HEPES buffer (1:1, 50 mM HEPES, 0.1 M KCl, pH = 7.5) at 25 °C (<b>a</b>,<b>c</b>,<b>e</b>) in the presence of increasing concentrations of Cd<sup>2+</sup> and (<b>b</b>,<b>d</b>,<b>f</b>) in the presence of 3 equiv. of metal ions. <span class="html-italic">I</span><sub>0</sub> is the emission intensity of free ligand.</p>
Full article ">Figure 3
<p>Effect of pH on the fluorescence intensity of (<b>a</b>) TriMeO-<span class="html-italic">N,O</span>-BQMAE (<b>3</b>) and (<b>b</b>) TriMeO-<span class="html-italic">N,N</span>-BQMAE (<b>6</b>) in the absence (blue) and presence (red) of 3 equiv. of Cd<sup>2+</sup> in DMF-HEPES buffer (1:1, 50 mM HEPES, 0.1 M KCl, pH = 7.5) at 25 °C.</p>
Full article ">Scheme 1
<p>Structure of ligands.</p>
Full article ">
13 pages, 2415 KiB  
Article
A Pair of Multifunctional Cu(II)–Dy(III) Enantiomers with Zero–Field Single–Molecule Magnet Behaviors, Proton Conduction Properties and Magneto–Optical Faraday Effects
by Shui-Dong Zhu, Yu-Lin Zhou, Fang Liu, Yu Lei, Sui-Jun Liu, He-Rui Wen, Bin Shi, Shi-Yong Zhang, Cai-Ming Liu and Ying-Bing Lu
Molecules 2023, 28(22), 7506; https://doi.org/10.3390/molecules28227506 - 9 Nov 2023
Cited by 2 | Viewed by 1479
Abstract
Multifunctional materials with a coexistence of proton conduction properties, single–molecule magnet (SMM) behaviors and magneto–optical Faraday effects have rarely been reported. Herein, a new pair of Cu(II)–Dy(III) enantiomers, [DyCu2(RR/SS–H2L)2(H2O)4(NO3) [...] Read more.
Multifunctional materials with a coexistence of proton conduction properties, single–molecule magnet (SMM) behaviors and magneto–optical Faraday effects have rarely been reported. Herein, a new pair of Cu(II)–Dy(III) enantiomers, [DyCu2(RR/SS–H2L)2(H2O)4(NO3)2]·(NO3)·(H2O) (R1 and S1) (H4L = [RR/SS] –N,N′–bis [3–hydroxysalicylidene] –1,2–cyclohexanediamine), has been designed and prepared using homochiral Schiff–base ligands. R1 and S1 contain linear Cu(II)–Dy(III)–Cu(II) trinuclear units and possess 1D stacking channels within their supramolecular networks. R1 and S1 display chiral optical activity and strong magneto–optical Faraday effects. Moreover, R1 shows a zero–field SMM behavior. In addition, R1 demonstrates humidity– and temperature–dependent proton conductivity with optimal values of 1.34 × 10−4 S·cm−1 under 50 °C and 98% relative humidity (RH), which is related to a 1D extended H–bonded chain constructed by water molecules, nitrate and phenol groups of the RR–H2L ligand. Full article
(This article belongs to the Special Issue Exclusive Feature Papers in Inorganic Chemistry, 2nd Edition)
Show Figures

Graphical abstract

Graphical abstract
Full article ">Figure 1
<p>The enantiomeric structures of <b><span class="html-italic">R</span></b>–<b>1</b> and <b><span class="html-italic">S</span></b>–<b>1</b>. The coordinated water molecules, coordinated nitrate oxygen atoms and the H atoms are omitted for clarity. Symmetric code: B: 1 − x, y, 2 − z.</p>
Full article ">Figure 2
<p>The 1D H–bonding chain and the potential proton transport pathway of <b><span class="html-italic">R</span></b>–<b>1</b>.</p>
Full article ">Figure 3
<p>CD spectra of <b><span class="html-italic">R</span></b>−<b>1</b> and <b><span class="html-italic">S</span></b>−<b>1</b> in CH<sub>3</sub>CN solution (c = 1.6 × 10<span class="html-italic"><sup>−</sup></span><sup>5</sup> molL<sup>−1</sup>; <span class="html-italic">H</span> = 0 and ±1.0 T; optical path = 1 mm) in the range of (<b>a</b>) 200–750 nm; and partially enlarged view of (<b>b</b>) 200–265 nm, (<b>c</b>) 265–450 nm and (<b>d</b>) MCD spectra of enantiomers <b><span class="html-italic">R</span></b>–<b>1</b> and <b><span class="html-italic">S</span></b>–<b>1</b> in a CH<sub>3</sub>CN solution (c = 1.6 × 10<span class="html-italic"><sup>−</sup></span><sup>5</sup> molL<sup>−1</sup>) at room temperature; and partially enlarged view of CD spectra of (<b>e</b>) <b><span class="html-italic">R</span></b>–<b>1</b> and (<b>f</b>) <b><span class="html-italic">R</span></b>–<b>1</b> in the range of 260–450 nm.</p>
Full article ">Figure 4
<p>Temperature dependence of the in−phase (<b>a</b>) and out−of−phase (<b>b</b>) components of the ac magnetic susceptibility for <b><span class="html-italic">R</span></b>–<b>1</b> in zero–dc fields with an oscillation of 2.5 Oe.</p>
Full article ">Figure 5
<p>(<b>a</b>) Nyquist plot for <b><span class="html-italic">R</span></b>−<b>1</b> at 25 °C under different RH levels; (<b>b</b>) plot of proton conductivity for <b><span class="html-italic">R</span></b>−<b>1</b> vs. RH at 25 °C; (<b>c</b>) Nyquist plot for <b><span class="html-italic">R</span></b>−<b>1</b> at different temperatures under 100% RH; (<b>d</b>) Plots of ln(σT) vs. 1000/T for <b><span class="html-italic">R</span></b>−<b>1</b> under 100% RH.</p>
Full article ">
14 pages, 1573 KiB  
Article
Antimicrobial Activity of Manganese(I) Tricarbonyl Complexes Bearing 1,2,3-Triazole Ligands
by Sofia Friães, Cândida Trigueiros, Clara S. B. Gomes, Alexandra R. Fernandes, Oscar A. Lenis-Rojas, Marta Martins and Beatriz Royo
Molecules 2023, 28(21), 7453; https://doi.org/10.3390/molecules28217453 - 6 Nov 2023
Cited by 2 | Viewed by 2194
Abstract
Background. Antimicrobial resistance is one of the most pressing health issues of our time. The increase in the number of antibiotic-resistant bacteria allied to the lack of new antibiotics has contributed to the current crisis. It has been predicted that if this situation [...] Read more.
Background. Antimicrobial resistance is one of the most pressing health issues of our time. The increase in the number of antibiotic-resistant bacteria allied to the lack of new antibiotics has contributed to the current crisis. It has been predicted that if this situation is not dealt with, we will be facing 10 million deaths due to multidrug resistant infections per year by 2050, surpassing cancer-related deaths. This alarming scenario has refocused attention into researching alternative drugs to treat multidrug-resistant infections. Aims. In this study, the antimicrobial activities of four manganese complexes containing 1,2,3,-triazole and clotrimazole ligands have been evaluated. It is known that azole antibiotics coordinated to manganese tricarbonyl complexes display interesting antimicrobial activities against several microbes. In this work, the effect of the introduction of 1,2,3,-triazole-derived ligands in the [Mn(CO)3(clotrimazole)] fragment has been investigated against one Gram-positive bacterium and five Gram-negative bacteria. Methods. The initial antimicrobial activity of the above-mentioned complexes was assessed by determining the minimum inhibitory and bactericidal concentrations using the broth microdilution method. Growth curves in the presence and absence of the complexes were performed to determine the effects of these complexes on the growth of the selected bacteria. A possible impact on cellular viability was determined by conducting the MTS assay on human monocytes. Results. Three of the Mn complexes investigated (46) had good antimicrobial activities against all the bacteria tested, with values ranging from 1.79 to 61.95 µM with minimal toxicity. Conclusions. Due to the increased problem of antibiotic resistance and a lack of new antibacterial drugs with no toxicity, these results are exciting and show that these types of complexes can be an avenue to pursue in the future. Full article
(This article belongs to the Special Issue Exclusive Feature Papers in Inorganic Chemistry, 2nd Edition)
Show Figures

Graphical abstract

Graphical abstract
Full article ">Figure 1
<p>ORTEP representation of complex <b>3</b>. Hydrogen atoms and co-crystalised solvent molecules are omitted for clarity. Selected bond lengths: Mn1–Br1 2.5366(3) Å, Mn1–N1 2.0195(16) Å, Mn1–N4 2.0780(16) Å, 1.8075(19) Å, and &lt; Mn1–C<sub>CO</sub> &lt; 1.812(2) Å. Selected bond angles: N1–Mn1–N4 78.30(6)°, N1–Mn1–C16 173.01(7)°, N4–Mn1–C17 170.99(8)°, and Br1–Mn1–C16 178.98(7)°.</p>
Full article ">Figure 2
<p>Selected metal complexes reported in the literature as antimicrobial drugs.</p>
Full article ">Figure 3
<p>Growth kinetics of <span class="html-italic">S. aureus</span> ATCC25923, <span class="html-italic">E. coli</span> ATCC 25922, and <span class="html-italic">Salmonella typhimurium</span> 14028S in the presence of <b>4</b>. Effects of the complexes on the growth of selected bacteria when these were cultured in MH broth. The results correspond to the average of three independent experiments ± standard deviation (SD).</p>
Full article ">Figure 4
<p>Effect of the complexes on the cellular viability of human monocytes (THP-1 cell line). Human monocytes were exposed to the complexes for 24 h at 37 °C with 5% CO<sub>2</sub>. The assay was performed for all the complexes using concentrations ranging from ¼ MBC to 4× MBC for each compound. The results presented correspond to the average of two independent experiments ± standard deviation (SD); the percentage was compared to controls from two independent biological replicates.</p>
Full article ">Scheme 1
<p>Synthesis of Mn(I) tricarbonyl complexes <b>1</b>–<b>6</b>.</p>
Full article ">
15 pages, 2590 KiB  
Article
A Norbornadiene-Based Molecular System for the Storage of Solar–Thermal Energy in an Aqueous Solution: Study of the Heat-Release Process Triggered by a Co(II)-Complex
by Franco Castro, Jorge S. Gancheff, Juan C. Ramos, Gustavo Seoane, Carla Bazzicalupi, Antonio Bianchi, Francesca Ridi and Matteo Savastano
Molecules 2023, 28(21), 7270; https://doi.org/10.3390/molecules28217270 - 25 Oct 2023
Cited by 2 | Viewed by 2586
Abstract
It is urgent yet challenging to develop new environmentally friendly and cost-effective sources of energy. Molecular solar thermal (MOST) systems for energy capture and storage are a promising option. With this in mind, we have prepared a new water-soluble (pH > 6) norbornadiene [...] Read more.
It is urgent yet challenging to develop new environmentally friendly and cost-effective sources of energy. Molecular solar thermal (MOST) systems for energy capture and storage are a promising option. With this in mind, we have prepared a new water-soluble (pH > 6) norbornadiene derivative (HNBD1) whose MOST properties are reported here. HNBD1 shows a better matching to the solar spectrum compared to unmodified norbornadiene, with an onset absorbance of λonset = 364 nm. The corresponding quadricyclane photoisomer (HQC1) is quantitatively generated through the light irradiation of HNBD1. In an alkaline aqueous solution, the MOST system consists of the NBD1/QC1 pair of deprotonated species. QC1 is very stable toward thermal back-conversion to NBD1; it is absolutely stable at 298 K for three months and shows a marked resistance to temperature increase (half-life t½ = 587 h at 371 K). Yet, it rapidly (t½ = 11 min) releases the stored energy in the presence of the Co(II) porphyrin catalyst Co-TPPC (ΔHstorage = 65(2) kJ∙mol−1). Under the explored conditions, Co-TPPC maintains its catalytic activity for at least 200 turnovers. These results are very promising for the creation of MOST systems that work in water, a very interesting solvent for environmental sustainability, and offer a strong incentive to continue research towards this goal. Full article
(This article belongs to the Special Issue Exclusive Feature Papers in Inorganic Chemistry, 2nd Edition)
Show Figures

Graphical abstract

Graphical abstract
Full article ">Figure 1
<p>(<b>a</b>) NBD and QC structures. (<b>b</b>) Schematic representation of a MOST-based plant for domestic use. (<b>c</b>) Photochemical and thermodynamic functioning of MOST molecules.</p>
Full article ">Figure 2
<p>HNBD1, HQC1 and Co-TPPC structures.</p>
Full article ">Figure 3
<p>UV-Vis spectra of HNBD1 and HQC1 recorded at different pH values in the range 2.0–11.0. [HNBD1] = [HQC1] = 1.1 × 10<sup>−4</sup> M; 298 K, 0.1 M NaCl; Spectra in the pH range 6.0–11.0 are identical. Color code: red, spectra recorded at pH 2; blue, spectra recorded in the pH range 6.0–11.0.</p>
Full article ">Figure 4
<p>pH dependence of the λ<sub>onset</sub> for HNBD1/NBD1<sup>−</sup>.</p>
Full article ">Figure 5
<p>DSC thermogram recorded for HQC1 with a rate of temperature increase of 2 °C∙min<sup>−1</sup>.</p>
Full article ">Figure 6
<p>(<b>a</b>) <sup>1</sup>H-NMR spectra (D<sub>2</sub>O, pH 11, 298 K, 400 MHz) showing the evolution with time of the catalyzed back-conversion of QC1<sup>−</sup> to NBD1<sup>−</sup>. Spectrum 1 corresponds to QC1<sup>−</sup> without catalysts, spectrum 2 was recorded after catalyst addition and mixing (230 s), and then the reaction was left to freely progress; spectrum 18 corresponds to 3086 s total time. (<b>b</b>) Left: variation of the integral of the <sup>1</sup>H-NMR signal of QC1<sup>−</sup> at 2.5 ppm with time and fitting of the corresponding logarithmic curve. Right: Fitting details and parameters.</p>
Full article ">Figure 7
<p>Schematic procedure for the synthesis of HNBD1.</p>
Full article ">
26 pages, 9014 KiB  
Article
Effects of Ferrocene and Ferrocenium on MCF-7 Breast Cancer Cells and Interconnection with Regulated Cell Death Pathways
by Cristina Favaron, Elisabetta Gabano, Ilaria Zanellato, Ludovica Gaiaschi, Claudio Casali, Maria Grazia Bottone and Mauro Ravera
Molecules 2023, 28(18), 6469; https://doi.org/10.3390/molecules28186469 - 6 Sep 2023
Cited by 2 | Viewed by 2140
Abstract
The effects of ferrocene (Fc) and ferrocenium (Fc+) induced in triple negative human breast cancer MCF-7 cells were explored by immunofluorescence, flow cytometry, and transmission electron microscopy analysis. The different abilities of Fc and Fc+ to produce [...] Read more.
The effects of ferrocene (Fc) and ferrocenium (Fc+) induced in triple negative human breast cancer MCF-7 cells were explored by immunofluorescence, flow cytometry, and transmission electron microscopy analysis. The different abilities of Fc and Fc+ to produce reactive oxygen species and induce oxidative stress were clearly observed by activating apoptosis and morphological changes after treatment, but also after tests performed on the model organism D. discoideum, particularly in the case of Fc+. The induction of ferroptosis, an iron-dependent form of regulated cell death driven by an overload of lipid peroxides in cellular membranes, occurred after 2 h of treatment with Fc+ but not Fc. However, the more stable Fc showed its effects by activating necroptosis after a longer-lasting treatment. The differences observed in terms of cell death mechanisms and timing may be due to rapid interconversion between the two oxidative forms of internalized iron species (from Fe2+ to Fe3+ and vice versa). Potential limitations include the fact that iron metabolism and mitophagy have not been investigated. However, the ability of both Fc and Fc+ to trigger different and interregulated types of cell death makes them suitable to potentially overcome the shortcomings of traditional apoptosis-mediated anticancer therapies. Full article
(This article belongs to the Special Issue Exclusive Feature Papers in Inorganic Chemistry, 2nd Edition)
Show Figures

Graphical abstract

Graphical abstract
Full article ">Figure 1
<p>Sketch of ferrocene (<b>Fc</b>) and ferrocenium tetrafluoroborate ([<b>Fc<sup>+</sup></b>][BF<sub>4</sub>]<sup>−</sup>).</p>
Full article ">Figure 2
<p>(<b>Top</b>) Cytofluorimetric analysis. Graphs showing DNA content after PI staining on human MCF-7 cells in control condition and after 2, 6, 12, 24, and 48 h of CT with <b>Fc</b> and <b>Fc<sup>+</sup></b> (200 μM). (<b>Bottom</b>) Histograms showing the distribution of cells across the different cell cycle phases under control conditions and after <b>Fc</b> and <b>Fc<sup>+</sup></b> treatments.</p>
Full article ">Figure 3
<p>(<b>Top</b>) Double immunocytochemical reaction for mitochondria (green fluorescence) and COXIV (red fluorescence); DNA counterstaining with Hoechst 33258 (blue fluorescence) in control condition and samples treated with <b>Fc</b> and <b>Fc<sup>+</sup></b> (200 μM). Bar = 20 μm; magnification: 60×. See the main text for the meaning of the arrows. (<b>Bottom</b>) The histogram represents the relative expression of COXIV. Statistical analysis (one-way Anova): <span class="html-italic">p</span> &lt; 0.0001. Statistical significance between * control condition and treated samples; statistical significance between <span>$</span> <b>Fc</b><span class="underline">-</span> and <b>Fc<sup>+</sup></b>-treated samples (two-tailed unpaired <span class="html-italic">t</span>-test); <span class="html-italic">p</span>-values: (**) <span class="html-italic">p</span> &lt; 0.01; (<span>$</span><span>$</span><span>$</span>), (***) <span class="html-italic">p</span> &lt; 0.005; n.s. = not significant.</p>
Full article ">Figure 4
<p>(<b>Top</b>) Double immunocytochemical reaction for mitochondria (green fluorescence) and nitrotyrosine (red fluorescence); DNA counterstaining with Hoechst 33258 (blue fluorescence) under control condition and treated samples with <b>Fc</b> and <b>Fc<sup>+</sup></b> (200 μM). Bar = 20 μm; magnification: 60×. See the main text for the meaning of the arrows. (<b>Bottom</b>) The histogram represents the relative expression of nitrotyrosine. Statistical analysis (one-way Anova): <span class="html-italic">p</span> = 0.0002. Statistical significance between * control condition and treated samples; statistical significance between <span>$</span> <b>Fc</b>- and <b>Fc<sup>+</sup></b>-treated samples (two-tailed unpaired <span class="html-italic">t</span>-test); <span class="html-italic">p</span>-values: (*) <span class="html-italic">p</span> &lt; 0.05; (<span>$</span><span>$</span>), (**) <span class="html-italic">p</span> &lt; 0.01; n.s. = not significant.</p>
Full article ">Figure 5
<p>ROS increase induced by increasing concentrations of (<b>a</b>) <b>Fc</b> and (<b>b</b>) <b>Fc<sup>+</sup></b> measured by the dichlorofluorescein (DCF) assay. After 2, 4, 24, and 48 h of continuous treatment, dicty cells were washed and loaded with 2′,7′-Dichlorodihydrofluorescein diacetate (H<sub>2</sub>-DCF-DA) (15 min), then washed and read.</p>
Full article ">Figure 6
<p>Stability in solution vs. aging time in different model solutions (H<sub>2</sub>O; phosphate-buffered saline, PBS, pH = 7.4; RPMI 1460 and dicty medium) at 25 °C. Data were obtained by using cyclic voltammetry (peak current, <span class="html-italic">i</span><sub>p</sub>) or UV-vis spectroscopy (absorption A at λ<sub>max</sub> around 618 nm, depending on the solution). To compare the results, concentrations were normalized against the <span class="html-italic">i</span><sub>p</sub> or A values at time zero.</p>
Full article ">Figure 7
<p>Dissolved oxygen vs. time determined by a Clark-type O<sub>2</sub> electrode in the absence (black squares, <span class="html-fig-inline" id="molecules-28-06469-i001"><img alt="Molecules 28 06469 i001" src="/molecules/molecules-28-06469/article_deploy/html/images/molecules-28-06469-i001.png"/></span>) or presence of 2.7 mM concentrations of <b>Fc</b> (in PBS + 2.7% <span class="html-italic">v/v</span> DMSO; red squares, <span class="html-fig-inline" id="molecules-28-06469-i002"><img alt="Molecules 28 06469 i002" src="/molecules/molecules-28-06469/article_deploy/html/images/molecules-28-06469-i002.png"/></span>) and <b>Fc<sup>+</sup></b> (in PBS; dark yellow, <span class="html-fig-inline" id="molecules-28-06469-i003"><img alt="Molecules 28 06469 i003" src="/molecules/molecules-28-06469/article_deploy/html/images/molecules-28-06469-i003.png"/></span>).</p>
Full article ">Figure 8
<p>Iron uptake of <b>Fc</b> (light grey) and <b>Fc<sup>+</sup></b> (dark grey) in dicty cells treated for 30 min with 100 µM concentrations of the compounds in isotonic buffer (control experiment is in white). Data are the mean ± sd of three independent replicates and were compared using a one-way Anova analysis of the variance-Tukey test. Statistical analysis (<b>Fc</b> and <b>Fc<sup>+</sup></b> vs. control): (**) <span class="html-italic">p</span> &lt; 0.01; (***) <span class="html-italic">p</span> &lt; 0.001; (<b>Fc</b> vs. <b>Fc<sup>+</sup></b>): (§§§) <span class="html-italic">p</span> &lt; 0.001.</p>
Full article ">Figure 9
<p>(<b>Top</b>) Double immunocytochemical reaction for PARP-1 (green fluorescence) and tubulin (red fluorescence); DNA counterstaining with Hoechst 33258 (blue fluorescence) under control condition and samples treated with <b>Fc</b> and <b>Fc<sup>+</sup></b> (200 μM). Bar = 20 μm; magnification: 60×. See the main text for the meaning of the arrows. (<b>Bottom</b>) The histogram represents the relative expression of PARP-1. Statistical analysis (one-way Anova): <span class="html-italic">p</span> &lt; 0.0001. Statistical significance between * control condition and treated samples; statistical significance between <span>$</span> <b>Fc</b>- and <b>Fc<sup>+</sup></b>-treated samples (two-tailed unpaired <span class="html-italic">t</span>-test <b>Fc<sup>+</sup></b> vs. <b>Fc</b>); <span class="html-italic">p</span>-values: (*) <span class="html-italic">p</span> &lt; 0.05; (***) <span class="html-italic">p</span> &lt; 0.005; (<span>$</span><span>$</span><span>$</span><span>$</span>), (****) <span class="html-italic">p</span> &lt; 0.0001; n.s. = not significant.</p>
Full article ">Figure 10
<p>(<b>Top</b>) Double immunocytochemical reaction for RIP1 (green fluorescence) and actin (red fluorescence); DNA counterstaining with Hoechst 33258 (blue fluorescence) in control conditions and <b>Fc</b>- and <b>Fc<sup>+</sup></b>-treated samples (200 μM). Bar = 20 μm; magnification: 60×. See the main text for the meaning of the arrows. (<b>Bottom</b>). The histogram represents the relative expression of RIP1. Statistical analysis (one-way Anova): <span class="html-italic">p</span> &lt; 0.0001. Statistical significance between * control condition and treated samples; statistical significance between <span>$</span> <b>Fc</b>- and <b>Fc<sup>+</sup></b>-treated samples (two-tailed unpaired <span class="html-italic">t</span>-test <b>Fc<sup>+</sup></b> vs. <b>Fc</b>); <span class="html-italic">p</span>-values: (*) <span class="html-italic">p</span> &lt; 0.05, (****) <span class="html-italic">p</span> &lt; 0.0001; n.s. = not significant.</p>
Full article ">Figure 11
<p>(<b>Top</b>) Double immunocytochemical reaction for actin (green fluorescence) and MLKL (red fluorescence); DNA counterstaining with Hoechst 33258 (blue fluorescence) under control conditions and <b>Fc</b>- and <b>Fc<sup>+</sup></b>-treated samples (200 μM). Bar = 20 μm; magnification: 60×. See the main text for the meaning of the arrows. (<b>Bottom</b>) The histogram represents the relative expression of MLKL. Statistical analysis (one-way Anova): <span class="html-italic">p</span> &lt; 0.0001. Statistical significance between * control condition and treated samples; statistical significance between <span>$</span> <b>Fc</b>- and <b>Fc<sup>+</sup></b>-treated samples (two-tailed unpaired <span class="html-italic">t</span>-test <b>Fc<sup>+</sup></b> vs. <b>Fc</b>); <span class="html-italic">p</span>-values: (*) <span class="html-italic">p</span> &lt; 0.05; (**) <span class="html-italic">p</span> &lt; 0.01; (***) <span class="html-italic">p</span> &lt; 0.005; (<span>$</span><span>$</span><span>$</span><span>$</span>); n.s. = not significant.</p>
Full article ">Figure 12
<p>(<b>Top</b>) Double immunocytochemical reaction for Gpx4 (green fluorescence) and mitochondria (red fluorescence); DNA counterstaining with Hoechst 33258 (blue fluorescence) in control conditions and <b>Fc-</b> and <b>Fc<sup>+</sup></b>-treated samples (200 μM). Bar = 20 μm; magnification: 60×. (<b>Bottom</b>) The histogram represents the relative expression of GPX4. Statistical analysis (one-way Anova): <span class="html-italic">p</span> &lt; 0.0001. Statistical significance between * control condition and treated samples; statistical significance between <span>$</span> <b>Fc-</b> and <b>Fc<sup>+</sup></b>-treated samples (two-tailed unpaired <span class="html-italic">t</span>-test <b>Fc<sup>+</sup></b> vs. <b>Fc</b>); <span class="html-italic">p</span>-values: (<span>$</span>), (*) <span class="html-italic">p</span> &lt; 0.05; (<span>$</span><span>$</span>) <span class="html-italic">p</span> &lt; 0.01; (<span>$</span><span>$</span><span>$</span><span>$</span>), (****) <span class="html-italic">p</span> &lt; 0.0001; n.s. = not significant.</p>
Full article ">Figure 13
<p>Ultrastructural analysis by TEM. (<b>A</b>–<b>C</b>) MCF-7 cells under control (CTR) conditions. (<b>B</b>,<b>C</b>) Healthy mitochondria with well-organized cristae, indicated by arrows. (<b>D</b>,<b>F</b>) Cells after 2 h of continuous treatment with <b>Fc</b> 200 μM. (<b>D</b>) Apoptotic and (<b>E</b>) necroptotic cells with altered mitochondria (indicated by an asterisk in <b>E</b>) and a detached perinuclear space, highlighted by arrows in (<b>E</b>,<b>F</b>). (<b>G</b>,<b>H</b>) Cells exposed for 48 h to <b>Fc</b> 200 μM. Advanced necroptotic phase showing an electron-lucent cytoplasm (indicated by an asterisk in <b>G</b>), a more condensed chromatin, and an extreme enlargement of the perinuclear space (arrows). (<b>I</b>,<b>J</b>) Cells treated for 2 h with <b>Fc<sup>+</sup></b> 200 μM. No enlargement of the perinuclear space was observed (arrow in <b>I</b>). Examples of altered mitochondria with impaired cristae structure (highlighted by asterisk in <b>I</b>) and ferroptotic cell with a decondensed chromatin (pointed by asterisk in <b>J</b>). (<b>K</b>,<b>L</b>) Cells after 48 h of CT with <b>Fc<sup>+</sup></b> 200 μM. Examples of late ferroptosis (<b>K</b>,<b>L</b>) characterized by decondensed chromatin (asterisk in <b>K</b>) and severely impaired mitochondria (highlighted by arrows in <b>K</b>,<b>L</b>).</p>
Full article ">Figure 14
<p>Both <b>Fc</b> and even more <b>Fc<sup>+</sup></b> exposure resulted in the apoptotic cell death of MCF-7 cancer cells at the tested time points. Furthermore, the intrinsic instability of <b>Fc<sup>+</sup></b> caused the release of the central iron atom and the early activation of ferroptosis, followed by an increase in oxidative stress. Ferroptotic cells showed enlarged mitochondria with abnormal cristae and extreme decondensed chromatin. On the other hand, the more stable <b>Fc</b> led to the activation of the necroptotic cell death mechanism, especially after longer-lasting treatments, because of the immediate production of ROS and the consequent RNS accumulation. These cells appeared with altered mitochondria and more condensed chromatin. The image was made with <a href="http://BioRender.com" target="_blank">BioRender.com</a> (accessed on 1 September 2023).</p>
Full article ">
13 pages, 7623 KiB  
Article
The Preparation of a Challenging Superconductor Nb3Al by Exploiting Nano Effect
by Chengkai Luan, Xiyue Cheng, Xiuping Gao, Jürgen Köhler and Shuiquan Deng
Molecules 2023, 28(18), 6455; https://doi.org/10.3390/molecules28186455 - 6 Sep 2023
Viewed by 1487
Abstract
The Nb3Al superconductor with excellent physical and working properties is one of the most promising materials in high-magnetic-field applications. However, it is difficult to prepare high-quality Nb3Al with a desired superconducting transition temperature (Tc) because of [...] Read more.
The Nb3Al superconductor with excellent physical and working properties is one of the most promising materials in high-magnetic-field applications. However, it is difficult to prepare high-quality Nb3Al with a desired superconducting transition temperature (Tc) because of its narrow phase formation area at high temperatures (>1940 °C). This work reports a method to prepare stoichiometric Nb3Al powder samples at a relatively low temperature (1400 °C) by exploiting the nano effect of Nb particles with pretreatment of Nb powder under H2/Ar atmosphere. The obtained Nb3Al samples exhibit high Tc’s of ~16.8K. Based on density functional theory (DFT) calculations and statistical mechanics analysis, the crucial role of quantum effect in leading to the success of the preparation method was studied. A new measure of surface energy (MSE) of a model particle is introduced to study its size and face dependence. A rapid convergence of the MSE with respect to the size indicates a quick approach to the solid limit, while the face dependence of MSE reveals a liquid-like behavior. The surface effect and quantum fluctuation of the Nbn clusters explain the success of the preparation method. Full article
(This article belongs to the Special Issue Exclusive Feature Papers in Inorganic Chemistry, 2nd Edition)
Show Figures

Graphical abstract

Graphical abstract
Full article ">Figure 1
<p>Powder XRD patterns of Nb<sub>p</sub> samples (<b>a</b>) treated at various temperatures for 3 h; (<b>b</b>) treated under various temperatures for 3 h with 2θ from 37° to 39°; (<b>c</b>) sintered under 380 °C with reaction time (1 h~5 h). SEM image of (<b>d</b>) Nb raw material and T-3 h (T = (<b>e</b>) 321 °C; (<b>f</b>) 380 °C).</p>
Full article ">Figure 2
<p>XRD patterns of Nb<sub>3</sub>Al samples (<b>a</b>) prepared at different temperatures for 10 h and (<b>b</b>) at 1400 °C for 10 h with different Nb<sub>p</sub>:Al ratios; (<b>c</b>) indexing pattern of the sample (1400 °C-10 h-Nb<sub>p</sub>:Al = 3.0:1) together with an SEM image of the sample as inset.</p>
Full article ">Figure 3
<p>(<b>a</b>) Temperature dependence of the magnetization curves for samples sintered at 1400 °C for 10 h with different r (Nb<sub>p</sub>:Al); (<b>b</b>) the <span class="html-italic">T</span><sub>c</sub>–r curves for samples sintered at 1400 °C for 10 h (the inset shows M-T curve for the sample with r = 3.0).</p>
Full article ">Figure 4
<p>Structure of Nb units used for calculations of surface energies: (<b>a</b>) Chain model along [010] direction; (<b>b</b>) Cubic model expanded along &lt;100&gt; equivalent directions; (<b>c</b>) Rhombic dodecahedron model expanded along &lt;110&gt; directions; (<b>d</b>) Octahedron model expanded along &lt;111&gt; directions.</p>
Full article ">Figure 5
<p>(<b>a</b>) The four curves showing the relation between MSE and the number of atoms in each type of model; (<b>b</b>) The curves of total surface area vs. number of atoms for the four types of models.</p>
Full article ">
12 pages, 3362 KiB  
Article
Terbium and Europium Chlorocyananilate-Based 2D Coordination Polymers
by Mariangela Oggianu, Alexandre Abhervé, Daniela Marongiu, Francesco Quochi, José Ramón Galán-Mascarós, Federica Bertolotti, Norberto Masciocchi, Narcis Avarvari and Maria Laura Mercuri
Molecules 2023, 28(18), 6453; https://doi.org/10.3390/molecules28186453 - 6 Sep 2023
Cited by 4 | Viewed by 1390
Abstract
Two-dimensional layered coordination polymers based on the hetero-substituted 3-chloro-6-cyano-2,5-dihydroxybenzoquinone ligands, hereafter ClCNAn2− anilate, and LnIII ions (Tb and Eu) are reported. Compounds 1 and 2, formulated as Ln2(ClCNAn)3(DMSO)6 (LnIII = Tb, 1; Eu, [...] Read more.
Two-dimensional layered coordination polymers based on the hetero-substituted 3-chloro-6-cyano-2,5-dihydroxybenzoquinone ligands, hereafter ClCNAn2− anilate, and LnIII ions (Tb and Eu) are reported. Compounds 1 and 2, formulated as Ln2(ClCNAn)3(DMSO)6 (LnIII = Tb, 1; Eu, 2), and their related intermediates 1′ and 2′, formulated as Ln2(ClCNAn)3(H2O)x·yH2O (x + y likely = 12, Ln = Tb, 1′; and Eu, 2′), were prepared by a conventional one-pot reaction (the latter) and recrystallized from DMSO solvent (the former). Polyhydrated intermediates 1′ and 2′ show very similar XRPD patterns, while, despite their common stoichiometry, 1 and 2 are not isostructural. Compound 1 consists of a 2D coordination framework of 3,6 topology, where [Tb(DMSO)3]III moieties are bridged by three bis-chelating ClCNAn2− ligands, forming distorted hexagons. Ultrathin nanosheets of 1 were obtained by exfoliation via the liquid-assisted sonication method and characterized by atomic force microscopy, confirming the 2D nature of 1. The crystal structure of 2, still showing the presence of 2D sheets with a “hexagonal” mesh and a common (3,6) connectivity, is based onto flat, non-corrugated slabs. Indeed, at a larger scale, the different “rectangular tiles” show clear roofing in 1, which is totally absent in 2. The magnetic behavior of 1 very likely indicates depopulation of the highest crystal-field levels, as expected for TbIII compounds. Full article
(This article belongs to the Special Issue Exclusive Feature Papers in Inorganic Chemistry, 2nd Edition)
Show Figures

Graphical abstract

Graphical abstract
Full article ">Figure 1
<p>Schematic representation of the synthesis of compounds <b>1</b> and <b>2</b>, via the intermediacy of <b>1′</b> and <b>2′</b>.</p>
Full article ">Figure 2
<p>XRPD raw data (blue line) and Le Bail fits (red line) for polycrystalline <b>1′</b> (<b>a</b>) and <b>2′</b> (<b>b</b>) species. Difference plot and tick markers are shown in black at the bottom.</p>
Full article ">Figure 3
<p>(<b>a</b>) Full coordination environment around Tb<sup>III</sup>; (<b>b</b>) sketch of the distorted tricapped trigonal prismatic geometry around Tb<sup>III</sup> (hydrogen and disordered C,S ghosts removed for clarity); (<b>c</b>) view of one pseudo-rectangular cavity in ac plane; (<b>d</b>) view of three consecutive layers stacking parallel to the (<b>a</b>–<b>c</b>) vector. Color code: Tb—dark green; O—red; C—gray; S—yellow; Cl—green; N—blue.</p>
Full article ">Figure 4
<p>(<b>a</b>) The interdigitation of symmetry-related (and heavily corrugated) 2D layers of compound <b>1</b>. The orientation of the crystal axes (not to scale) is also shown (bottom left). The double arrow addresses the length of the <b>a</b>–<b>c</b> vector (18 Å) corresponding to two corrugated layers; (<b>b</b>) AFM characterization of drop-casted nanosheets of <b>1</b>: topographic image and, in the inset, cross-sectional height profiles, showing that flat or terraced nanosheets are formed, with ca. 9 Å steps.</p>
Full article ">Figure 5
<p>Sketches of the main structural features of <b>1</b> CP. (<b>a</b>) A fragment of the CP, showing the local environment of the Eu<sup>III</sup> ions; (<b>b</b>,<b>c</b>) the brick-wall connectivity of a flat slab in <b>2</b>, viewed down the axis normal to the CP extension, and from the side, respectively; (<b>d</b>) the overall crystal packing viewed down the <b>a</b> axis, showing that slabs, interacting only through weak van der Waals contacts mostly attributed to the DMSO ligands, stack along <b>b</b> with a ca. 9.7 Å periodicity.</p>
Full article ">Figure 6
<p>(<b>a</b>) Plot of the χmT product as a function of temperature for <b>1</b>. (<b>b</b>) In-phase (χ′) and out-of-phase (χ″) dynamic susceptibility for <b>1</b> at different frequencies as a function of temperature.</p>
Full article ">Figure 7
<p>Final Rietveld refinement plot for species <b>2</b>. Observed data in blue; calculated data in red. The difference plot (in black) and tick markers for peak positions are shown at the bottom.</p>
Full article ">Chart 1
<p>Potassium chlorocyananilate (<b>left</b>) and coordination mode of the ligand (<b>right</b>).</p>
Full article ">
13 pages, 2159 KiB  
Article
The Anti-Breast Cancer Stem Cell Potency of Copper(I)-Non-Steroidal Anti-Inflammatory Drug Complexes
by Alice Johnson, Xiao Feng, Kuldip Singh, Fabrizio Ortu and Kogularamanan Suntharalingam
Molecules 2023, 28(17), 6401; https://doi.org/10.3390/molecules28176401 - 1 Sep 2023
Cited by 3 | Viewed by 1635
Abstract
Cancer stem cells (CSCs) are thought to be partly responsible for metastasis and cancer relapse. Currently, there are no effective therapeutic options that can remove CSCs at clinically safe doses. Here, we report the synthesis, characterisation, and anti-breast CSC properties of a series [...] Read more.
Cancer stem cells (CSCs) are thought to be partly responsible for metastasis and cancer relapse. Currently, there are no effective therapeutic options that can remove CSCs at clinically safe doses. Here, we report the synthesis, characterisation, and anti-breast CSC properties of a series of copper(I) complexes, comprising of non-steroidal anti-inflammatory drugs (NSAIDs) and triphenylphosphine ligands (13). The copper(I) complexes are able to reduce the viability of breast CSCs grown in two- and three-dimensional cultures at micromolar concentrations. The potency of the copper(I) complexes towards breast CSCs was similar to salinomycin (an established anti-breast CSC agent) and cisplatin (a clinically used metallopharmaceutical). Cell-based studies showed that the copper(I) complexes are readily, and similarly, internalised by breast CSCs. The copper(I) complexes significantly increase the intracellular reactive oxygen species (ROS) levels in breast CSCs, and their ROS generation profile with respect to time is dependent on the NSAID component present. The generation of intracellular ROS by the copper(I) complexes could be part of the underlying mechanism by which they evoke breast CSC death. As far as we are aware, this is the first study to explore the anti-breast CSC properties of copper(I) complexes. Full article
(This article belongs to the Special Issue Exclusive Feature Papers in Inorganic Chemistry, 2nd Edition)
Show Figures

Figure 1

Figure 1
<p>X-ray structures of the copper(I) complexes (<b>A</b>) <b>2</b> and (<b>B</b>) <b>3</b>, comprising triphenylphosphine and naproxen or salicylate, respectively. Ellipsoids are shown at 50% probability. C atoms are in grey, P in purple, O in red, and Cu in blue. H atoms and disorder components have been omitted for clarity.</p>
Full article ">Figure 2
<p>Copper content (ng of Cu/ 10<sup>6</sup> cells) in HMLER-shEcad cells treated with <b>1</b>–<b>3</b> (5 µM for 24 h).</p>
Full article ">Figure 3
<p>(<b>A</b>) Quantification of mammosphere formation with HMLER-shEcad cells, untreated, and treated with <b>1</b>–<b>3</b>, cisplatin, or salinomycin at 0.5 µM for 5 days. Error bars = SD. (<b>B</b>) Representative bright-field images (×10) of the mammospheres, in the absence and presence of <b>1</b>–<b>3</b>, at 0.5 µM for 5 days.</p>
Full article ">Figure 4
<p>Normalised ROS activity in untreated HMLER-shEcad cells (control) and HMLER-shEcad cells treated with <b>3</b> (2 × IC<sub>50</sub> value, 0.5–24 h).</p>
Full article ">Scheme 1
<p>Reaction scheme for the preparation of copper(I) complexes containing triphenylphosphine ligands and diclofenac, naproxen, or salicylate moieties (<b>1</b>–<b>3</b>).</p>
Full article ">
16 pages, 16575 KiB  
Article
Aldiminium Cations as Countercations to Discrete Main Group Fluoroanions
by Evelin Gruden and Gašper Tavčar
Molecules 2023, 28(17), 6270; https://doi.org/10.3390/molecules28176270 - 27 Aug 2023
Viewed by 1212
Abstract
The reactions of group 14 tetrafluorides (SiF4, GeF4, and SnF4) and group 15 pentafluorides (PF5, AsF5, and SbF5) with the CAAC-based trifluoride reagent [MeCAACH][F(HF)2] led to the [...] Read more.
The reactions of group 14 tetrafluorides (SiF4, GeF4, and SnF4) and group 15 pentafluorides (PF5, AsF5, and SbF5) with the CAAC-based trifluoride reagent [MeCAACH][F(HF)2] led to the isolation of salts containing discrete 5- or 6-coordinated fluoroanions. The syntheses of [MeCAACH][SiF5], [MeCAACH][GeF5], [MeCAACH][(THF)SnF5], and the structurally related [MeCAACH][(dioxane)SnF5], [MeCAACH][PF6], [MeCAACH][AsF6], and [MeCAACH][SbF6] are effective, selective and in high yield. All compounds were characterized by X-ray single-crystal structure analysis, NMR and Raman spectroscopy. It is worth noting that the synthesized [MeCAACH][GeF5] is a rare example of a structurally characterized compound with discrete [GeF5] anion, while [MeCAACH][(THF)SnF5] and [MeCAACH][(dioxane)SnF5] represent the first compounds with discrete octahedrally coordinated tin fluoride anions with incorporated solvent molecules. Finally, the aldiminium-based cation [MeCAACH]+ proved to be suitable for the stabilization of rare discrete main group fluoride anions. Full article
(This article belongs to the Special Issue Exclusive Feature Papers in Inorganic Chemistry, 2nd Edition)
Show Figures

Graphical abstract

Graphical abstract
Full article ">Figure 1
<p>Structure of the asymmetric unit of (<b>a</b>) [<sup>Me</sup>CAACH][SiF<sub>5</sub>] and (<b>b</b>) [<sup>Me</sup>CAACH][GeF<sub>5</sub>]. The ellipsoids are drawn at 50% probability. The positions of the fluorine atoms in both anions are disordered. For clarity, only the fluorine atoms in domain A are shown and all hydrogen atoms except those on the aldiminium ring are omitted.</p>
Full article ">Figure 2
<p>Crystal structure of (<b>a</b>) [<sup>Me</sup>CAACH][(THF)SnF<sub>5</sub>] and (<b>b</b>) [<sup>Me</sup>CAACH][(dioxane)SnF<sub>5</sub>]. The ellipsoids are drawn at 50% probability. For clarity, all hydrogen atoms except those on the heterocyclic ring are omitted.</p>
Full article ">Figure 3
<p>Structure of the asymmetric units of (<b>a</b>) [<sup>Me</sup>CAACH][PF<sub>6</sub>] and (<b>b</b>) [<sup>Me</sup>CAACH][AsF<sub>6</sub>]. The ellipsoids are drawn at 50% probability. For clarity, all hydrogen atoms except those on the heterocyclic ring are omitted.</p>
Full article ">Figure 4
<p>Structure of the asymmetric unit of [<sup>Me</sup>CAACH][BF<sub>4</sub>]. The ellipsoids are drawn at 50% probability. The positions of the fluorine atoms in the anion are disordered. For clarity, only the fluorine atoms in domain A are shown and all hydrogen atoms except those on the heterocyclic ring are omitted.</p>
Full article ">Figure 5
<p>Crystal structures of (<b>a</b>) [<sup>Me</sup>CAACH][Cl] and (<b>b</b>) [<sup>Me</sup>CAACH][OTf]. The ellipsoids are drawn at 50% probability. For clarity, all hydrogen atoms except those on the heterocyclic ring are omitted.</p>
Full article ">Scheme 1
<p>Synthesis of [<sup>Me</sup>CAACH][SiF<sub>5</sub>] and [<sup>Me</sup>CAACH][GeF<sub>5</sub>].</p>
Full article ">Scheme 2
<p>Synthesis of [<sup>Me</sup>CAACH][(THF)SnF<sub>5</sub>].</p>
Full article ">Scheme 3
<p>Synthesis of [<sup>Me</sup>CAACH][PF<sub>6</sub>] and [<sup>Me</sup>CAACH][AsF<sub>6</sub>].</p>
Full article ">Scheme 4
<p>Synthesis of [<sup>Me</sup>CAACH][SbF<sub>6</sub>].</p>
Full article ">Scheme 5
<p>Synthesis of [<sup>Me</sup>CAACH][BF<sub>4</sub>].</p>
Full article ">
12 pages, 3578 KiB  
Article
Observation of Two-Step Spin Transition in Graphene Oxide-Based Hybrids with Iron(II) 4-amino-1,2,4-triazole Spin Crossover Nanoparticles
by Nikolia Lalioti, Alexander Charitos, John Parthenios, Ondrej Malina, Michaela Polaskova, Martin Petr and Vassilis Tangoulis
Molecules 2023, 28(15), 5816; https://doi.org/10.3390/molecules28155816 - 2 Aug 2023
Cited by 2 | Viewed by 1385
Abstract
A novel experimental protocol based on a reverse micellar method is presented for the synthesis of graphene oxide (GO)-based hybrids with spin crossover nanoparticles (SCO NPs) of the 1D iron(II) coordination polymer with the formula [Fe(NH2trz)3](Br2). By [...] Read more.
A novel experimental protocol based on a reverse micellar method is presented for the synthesis of graphene oxide (GO)-based hybrids with spin crossover nanoparticles (SCO NPs) of the 1D iron(II) coordination polymer with the formula [Fe(NH2trz)3](Br2). By introducing different quantities of 0.5% and 1.0% of GO (according to iron(II)) into the aqueous phase, two hybrids, NP4 and NP5, were synthesized, respectively. The morphological homogeneity of the NPs on the surface of the GO flakes is greatly improved in comparison to the pristine [Fe(NH2trz)3](Br2) NPs. From the magnetic point of view and at a low magnetic sweep rate of 1 K/min, a two-step hysteretic behavior is observed for NP4 and NP5, where the onset of the low-temperature second step appeared at 40% and 30% of the HS fraction, respectively. For faster sweep rates of 5–10 K/min, the two steps from the cooling branch are progressively smeared out, and the critical temperatures observed are T1/2 = 343 K and T1/2 = 288 K, with a thermal width of 55 K for both NP4 and NP5. A Raman laser power-assisted protocol was used to monitor the thermal tolerance of the hybrids, while XPS analysis revealed electronic interactions between the SCO NPs and the GO flakes. Full article
(This article belongs to the Special Issue Exclusive Feature Papers in Inorganic Chemistry, 2nd Edition)
Show Figures

Figure 1

Figure 1
<p>TEM images of the GO-decorated <b>NP5</b>. The highlighted regions are shown in the enlarged images guided by the arrows. The Gaussian distribution of sizes is also shown in the figure.</p>
Full article ">Figure 2
<p>XPS spectra of Fe2p for <b>NP4</b>, <b>NP5,</b> and pristine [Fe(NH<sub>2</sub>trz)<sub>3</sub>](Br)<sub>2</sub> NPs (<b>SCO</b>).</p>
Full article ">Figure 3
<p>Sweep rate-dependent magnetic susceptibility measurements (third thermal cycle) carried out at 1 K/min (red solid line and spheres), 5 K/min (brown solid line and spheres), and 10 K/min (blue solid line and spheres) for (<b>a</b>) <b>NP4</b> and (<b>b</b>) <b>NP5</b> (see text for details).</p>
Full article ">Figure 4
<p>Comparison of HS Raman spectra (blue line) and LS Raman spectra (red line) in the range of 150–500 cm<sup>−1</sup> and 850–1700 cm<sup>−1</sup> of <b>NP4</b> (<b>a</b>,<b>d</b>), <b>NP5</b> (<b>b</b>,<b>e</b>), and pristine [Fe(NH<sub>2</sub>trz)<sub>3</sub>]Br<sub>2</sub> NPs (<b>c</b>,<b>f</b>), respectively. The experimental conditions of spectra are the following: (<b>a</b>) LS spectra: laser power 84 μW, exposure time 150 s. (<b>b</b>) HS spectra: laser power 340 μW, exposure time 150 s. A percentage of the LS state is depicted in a low-intensity band at 248 cm<sup>−1</sup> (presented with an asterisk), denoting the increased thermal tolerance of the hybrids.</p>
Full article ">Figure 5
<p>Comparison of HS/LS Raman spectra of <b>NP5</b> (blue line) and pristine [Fe(NH<sub>2</sub>trz)<sub>3</sub>]Br<sub>2</sub> NPs <b>SCO</b> (red line), with GO (orange line) in the range of 1100–1700 cm<sup>−1</sup>.</p>
Full article ">
31 pages, 94288 KiB  
Article
Syntheses, Structures, and Corrosion Inhibition of Various Alkali Metal Carboxylate Complexes
by Vidushi P. Vithana, Zhifang Guo, Glen B. Deacon and Peter C. Junk
Molecules 2023, 28(14), 5515; https://doi.org/10.3390/molecules28145515 - 19 Jul 2023
Viewed by 1882
Abstract
Complexes of the alkali metals Li-Cs with 3-thiophenecarboxylate (3tpc), 2-methyl-3-furoate (2m3fur), 3-furoate (3fur), 4-hydroxycinnamate (4hocin), and 4-hydroxybenzoate (4hob) ions were prepared via neutralisation reactions, and the structures of [Li2(3tpc)2]n (1Li); [K2(3tpc)2]n [...] Read more.
Complexes of the alkali metals Li-Cs with 3-thiophenecarboxylate (3tpc), 2-methyl-3-furoate (2m3fur), 3-furoate (3fur), 4-hydroxycinnamate (4hocin), and 4-hydroxybenzoate (4hob) ions were prepared via neutralisation reactions, and the structures of [Li2(3tpc)2]n (1Li); [K2(3tpc)2]n (1K); [Rb(3tpc)(H2O)]n (1Rb); [Cs{H(3tpc)2}]n (1Cs); [Li2(2m3fur)2(H2O)3] (2Li); [K2(2m3fur)2(H2O)]n (2K); [Li(3fur)]n(3Li); [K(4hocin](H2O)3]n (4K); [Rb{H(4hocin)2}]n.nH2O (4Rb); [Cs(4hocin)(H2O)]n (4Cs); [Li(4hob)]n (5Li); [K(4hob)(H2O)3]n (5K); [Rb(4hob)(H2O)]n (5Rb); and [Cs(4hob)(H2O)]n (5Cs) were determined via X-ray crystallography. Bulk products were also characterised via XPD, IR, and TGA measurements. No sodium derivatives could be obtained as crystallographically suitable single crystals. All were obtained as coordination polymers with a wide variety of carboxylate-binding modes, except for dinuclear 2Li. Under conditions that normally gave coordinated carboxylate ions, the ligation of hydrogen dicarboxylate ions was observed in 1Cs and 4Rb, with short H-bonds and short O…O distances associated with the acidic hydrogen. The alkali-metal carboxylates showed corrosion inhibitor properties inferior to those of the corresponding rare-earth carboxylates. Full article
(This article belongs to the Special Issue Exclusive Feature Papers in Inorganic Chemistry, 2nd Edition)
Show Figures

Graphical abstract

Graphical abstract
Full article ">Figure 1
<p>Different coordination modes observed for 3tpc, 2m3fur, 3fur, 4hocin, and 4hob ions.</p>
Full article ">Figure 2
<p>The asymmetric unit of [Li<sub>2</sub>(3tpc)<sub>2</sub>]<sub>n</sub> <b>1Li</b> expanded to show the Li coordination spheres. Symmetry code: <sup>#1</sup> + X,1 + Y, + Z; <sup>#2</sup> 1/2 + X,1/2-Y, + Z; <sup>#3</sup> -1/2 + X,1/2-Y, + Z; <sup>#4</sup> + X,-1 + Y, + Z.</p>
Full article ">Figure 3
<p>Projection along the c-axis showing the crystal packing of <b>1Li</b> into a <b>2D</b> network.</p>
Full article ">Figure 4
<p>The asymmetric unit of [K<sub>2</sub>(3tpc)<sub>2</sub>]<sub>n</sub> <b>1K</b> expanded to show the K coordination. Symmetry code: <sup>#1</sup> + X,-1 + Y, + Z; <sup>#2</sup> + X,1 + Y, + Z; <sup>#4</sup>1/2 + X,-Y, + Z; <sup>#6</sup>-1/2 + X,1-Y, + Z.</p>
Full article ">Figure 5
<p>A c-axis projection of the crystal packing of <b>1K</b>. Symmetry code: <sup>#1</sup> + X,-1 + Y, + Z; <sup>#2</sup> + X,1 + Y, + Z; <sup>#3</sup> 1/2 + X,1-Y, + Z; <sup>#4</sup> 1/2 + X,-Y, + Z; <sup>#5</sup> -1/2 + X,-Y, + Z; <sup>#6</sup> -1/2 + X,1-Y, + Z.</p>
Full article ">Figure 6
<p>The immediate coordination environment around Rb metal atom in [Rb(3tpc)(H<sub>2</sub>O)]<sub>n</sub><b>1Rb</b>. Symmetry code: <sup>#1</sup> 1-X,1/2 + Y,3/2-Z; <sup>#2</sup> + X,1 + Y, + Z; <sup>#4</sup> + X,-1 + Y, + Z; <sup>#6</sup> + X,1/2-Y,1/2 + Z; <sup>#7</sup> 1-X,2-Y,1-Z; <sup>#8</sup> 1-X,-1/2 + Y,3/2-Z.</p>
Full article ">Figure 7
<p>Projection along the b-axis of <b>1Rb</b> showing the 2D network.</p>
Full article ">Figure 8
<p>The asymmetric unit of [Cs{H(3tpc)<sub>2</sub>}]<sub>n</sub> <b>1Cs</b> expanded to illustrate the Cs coordination, highlighting the presence of a centrosymmetric hydrogen atom located between the two carboxylate groups. Symmetry code: <sup>#1</sup> + X,1 + Y, + Z; <sup>#2</sup> + X,-1 + Y, + Z; <sup>#3</sup> 1-X,2-Y,1-Z; <sup>#4</sup> 1-X,1-Y,1-Z; <sup>#5</sup> 1-X, + Y,1/2-Z; <sup>#7</sup> 1-X,1 + Y,1/2-Z; <sup>#8</sup> + X,2-Y,1/2 + Z.</p>
Full article ">Figure 9
<p>The crystal packing of <b>1Cs</b> is shown in a b-axis projection. The hydrogen atoms, except for those forming symmetrical hydrogen bonds, have been omitted for clarity.</p>
Full article ">Figure 10
<p>Molecular diagram of the dinuclear [Li<sub>2</sub>(2m3fur)<sub>2</sub>(H<sub>2</sub>O)<sub>3</sub>] (<b>2Li</b>). Symmetry code: <sup>#1</sup> 1-X, + Y,1/2-Z.</p>
Full article ">Figure 11
<p>The expanded asymmetric unit of [K<sub>2</sub>(2m3fur)<sub>2</sub>(H<sub>2</sub>O)]<sub>n</sub><b>2K</b> extended to show the K1 and K2 coordination sphere. Symmetry code: <sup>#1</sup> + X,3/2-Y,-1/2 + Z; <sup>#2</sup> 1-X,1-Y,1-Z; <sup>#3</sup> 1-X,1/2 + Y,3/2-Z; <sup>#4</sup> 1-X,1-Y,2-Z; <sup>#5</sup> 1-X,-1/2 + Y,3/2-Z; <sup>#6</sup> + X,1/2-Y,1/2 + Z. <sup>#7</sup> 1-X,1 + Y,1/2-Z; <sup>#8</sup> + X,2-Y,1/2 + Z.</p>
Full article ">Figure 12
<p>An a-axis projection of the crystal packing of <b>2K</b> (2-methyl-3-furan rings have been omitted for clarity). Symmetry code: <sup>#3</sup> 1-X,1/2 + Y,3/2-Z; <sup>#4</sup> 1-X,1-Y,2-Z; <sup>#7</sup> 1-X,1 + Y,1/2-Z; <sup>#8</sup> + X,2-Y,1/2 + Z; <sup>#9</sup> 1-X,2-Y,1-Z.</p>
Full article ">Figure 13
<p>The asymmetric unit of [Li(3fur)]<sub>n</sub> (<b>3Li</b>) expanded to show the Li coordination sphere. Symmetry code: <sup>#1</sup> 1-X,1/2 + Y,3/2-Z; <sup>#3</sup> 1-X,-Y,1-Z; <sup>#4</sup> 1-X,-1/2 + Y,3/2-Z; <sup>#5</sup> + X,-1 + Y, + Z.</p>
Full article ">Figure 14
<p>Crystal packing of <b>3Li</b> into a <b>2D</b> network (aromatic H atoms- are omitted for clarity).</p>
Full article ">Figure 15
<p>The immediate coordination environment of potassium in [K(4hocin)(H<sub>2</sub>O)<sub>3</sub>]<sub>n</sub> (<b>4K</b>) (hydrogen atoms, except for those forming H-bonds, are omitted for clarity). Symmetry code: <sup>#1</sup> + X,3/2-Y,1/2 + Z; <sup>#2</sup> + X,3/2-Y,-1/2 + Z; <sup>#3</sup> -X,2-Y,-Z.</p>
Full article ">Figure 16
<p>(<b>a</b>) A projection along the a-axis of <b>4K</b>. (<b>b</b>) H-bonded interaction in [K(4hocin)(H<sub>2</sub>O)<sub>3</sub>]<sub>n.</sub> (<b>c</b>) The hydrogen-bonded network formed by the 4hocin and water molecules. (K–O coordination bonds are omitted for clarity). Symmetry code: <sup>#1</sup> + X,3/2-Y,-1/2 + Z; <sup>#2</sup> 1-X,1-Y,1-Z; <sup>#3</sup> 1-X,1/2 + Y,3/2-Z; <sup>#4</sup> 1-X,1-Y,2-Z; <sup>#6</sup> + X,1/2-Y,1/2 + Z.</p>
Full article ">Figure 17
<p>The expanded asymmetric unit of <b>4Rb</b> reveals the coordination of Rb atoms. (H atoms of the ligand, except for the phenolic hydroxyl group, are omitted for clarity; H of H(4hocin)<sub>2</sub>—is H1.) Symmetry Code: <sup>#1</sup> 3/2-X,3/2-Y,1-Z; <sup>#2</sup> -1/2 + X,3/2-Y,-1/2 + Z; <sup>#3</sup> + X,1-Y,1/2 + Z; <sup>#4</sup> 1-X,1-Y,-Z; <sup>#5</sup> 1-X, + Y,1/2-Z.</p>
Full article ">Figure 18
<p>(<b>a</b>) A c-axis projection of the crystal packing of <b>4Rb</b>. (<b>b</b>) An alternative view of the crystal packing by omitting the Rb-O coordination to show the hydrogen bonds forming an extended 3D packing arrangement. <sup>#1</sup> + X,3/2-Y,-1/2 + Z; <sup>#2</sup> 1-X,1-Y,1-Z; <sup>#3</sup> 1-X,1/2 + Y,3/2-Z; <sup>#4</sup> 1-X,1-Y,2-Z; <sup>#5</sup> 1-X,-1/2 + Y,3/2-Z; <sup>#6</sup> + X,1/2-Y,1/2 + Z. <sup>#7</sup> 1-X,1 + Y,1/2-Z; <sup>#8</sup> + X,2-Y,1/2 + Z.</p>
Full article ">Figure 19
<p>The asymmetric unit of [Cs(4hocin)(H<sub>2</sub>O)]<sub>n</sub> (<b>4Cs</b>) expanded to show the complete Cs coordination sphere. Symmetry code: <sup>#1</sup> 1 + X, + Y, + Z; <sup>#2</sup> -X,1/2 + Y,2-Z; <sup>#3</sup> 1-X,1/2 + Y,2-Z; <sup>#4</sup> + X, + Y,-1 + Z; <sup>#5</sup> -1 + X, + Y,-1 + Z.</p>
Full article ">Figure 20
<p>(<b>a</b>) A projection along the ac-plane shows the formation of a 2D-layer network of <b>4Cs</b> (H atoms, except for those forming H-bonds, are omitted for clarity). (<b>b</b>) A projection along the a-axis showing interaction that links the 2D networks together. Symmetry code: <sup>#1</sup> + X,3/2-Y,-1/2 + Z; <sup>#3</sup> 1-X,1/2 + Y,3/2-Z; <sup>#4</sup> 1-X,1-Y,2-Z; <sup>#5</sup> 1-X,-1/2 + Y,3/2-Z; <sup>#6</sup> + X,1/2-Y,1/2 + Z; <sup>#7</sup> 1-X,1 + Y,1/2-Z; <sup>#9</sup> 1+X,+ Y,1+Z.</p>
Full article ">Figure 20 Cont.
<p>(<b>a</b>) A projection along the ac-plane shows the formation of a 2D-layer network of <b>4Cs</b> (H atoms, except for those forming H-bonds, are omitted for clarity). (<b>b</b>) A projection along the a-axis showing interaction that links the 2D networks together. Symmetry code: <sup>#1</sup> + X,3/2-Y,-1/2 + Z; <sup>#3</sup> 1-X,1/2 + Y,3/2-Z; <sup>#4</sup> 1-X,1-Y,2-Z; <sup>#5</sup> 1-X,-1/2 + Y,3/2-Z; <sup>#6</sup> + X,1/2-Y,1/2 + Z; <sup>#7</sup> 1-X,1 + Y,1/2-Z; <sup>#9</sup> 1+X,+ Y,1+Z.</p>
Full article ">Figure 21
<p>The asymmetric unit of [Li(4hob)]<sub>n</sub> (<b>5Li</b>) expanded to show the Li coordination sphere. Symmetry code: <sup>#1</sup> 1-X,1/2 + Y,1/2-Z; <sup>#2</sup> +X,1 + Y, + Z; <sup>#3</sup> 1-X,-Y,1-Z; <sup>#4</sup> 1-X,-1/2 + Y,1/2-Z; <sup>#5</sup> + X,-1 + Y, + Z.</p>
Full article ">Figure 22
<p>Extended diagram of <b>5Li</b> (aromatic C-H bonds are omitted for clarity).</p>
Full article ">Figure 23
<p>The asymmetric unit of [K(4hob)(H<sub>2</sub>O)<sub>3</sub>]<sub>n</sub> (<b>5K</b>) expanded to show the K coordination. Symmetry code: <sup>#1</sup> + X,3/2-Y,-1/2 + Z; <sup>#2</sup> + X,3/2-Y,1/2 + Z; <sup>#3</sup> 2-X,2-Y,1-Z; <sup>#4</sup> 2-X,-1/2 + Y,1/2-Z.</p>
Full article ">Figure 24
<p>The packing diagram of the 1D polymeric chains of <b>5K</b> linked by O…H...O hydrogen bonds into a 2D network. (The 1D polymeric chain is propagating along the <span class="html-italic">c</span>-axis). Symmetry code: <sup>#1</sup> + X,3/2-Y,-1/2 + Z; <sup>#2</sup> + X,3/2-Y,1/2 + Z; <sup>#4</sup> 2-X,-1/2 + Y,1/2-Z.</p>
Full article ">Figure 25
<p>The asymmetric unit of [Rb(4hob)(H<sub>2</sub>O)]<sub>n</sub> (<b>5Rb</b>) showing the total coordination sphere (hydrogen atoms are omitted for clarity). Symmetry code: <sup>#1</sup> + X,1/2-Y,-1/2 + Z; <sup>#2</sup> -1 + X, + Y, + Z; <sup>#3</sup> -1 + X,1/2-Y,-1/2 + Z; <sup>#4</sup> -X,-1/2 + Y,3/2-Z; <sup>#5</sup> -X,1-Y,1-Z; <sup>#6</sup> -X,-Y,1-Z.</p>
Full article ">Figure 26
<p>(<b>a</b>) A projection along the ac-plane showing the formation of a 2D-layer network of <b>5Rb</b>. (<b>b</b>) A projection along the a-axis of <b>5b</b> showing alternative four- and eight-membered rings (circled) that link the 2D networks together. Symmetry code: <sup>#1</sup> + X,3/2-Y,-1/2 + Z; <sup>#2</sup> 1-X,1-Y,1-Z; <sup>#4</sup> 1-X,1-Y,2-Z; <sup>#6</sup> + X,1/2-Y,1/2 + Z; <sup>#7</sup> 1-X,1 + Y,1/2-Z.</p>
Full article ">Figure 27
<p>Molecular diagram of [Cs(4hob)(H<sub>2</sub>O)]<sub>n</sub><b>5Cs</b> indicating the immediate coordination environment around Cs1. Hydrogen atoms, except for those involved in forming H-bonds, are omitted for clarity. (The 1D polymeric chain propagates along the <span class="html-italic">c</span>-axis, while a 2D framework forms in the ac-plane. The 2D polymeric chains are linked by alternative four- and eight-membered rings, resulting in the formation of a 3D network along the <span class="html-italic">b</span>-axis). Symmetry code: <sup>#1</sup> + X,1/2-Y,1/2 + Z; <sup>#2</sup> 1 + X, + Y, + Z; <sup>#3</sup> 1 + X,1/2-Y,1/2 + Z; <sup>#4</sup> 2-X,-1/2 + Y,1/2-Z; <sup>#5</sup> 2-X,1-Y,1-Z,; <sup>#6</sup> 2-X,-Y,1-Z; <sup>#7</sup> + X,1/2-Y,-1/2 + Z.</p>
Full article ">Chart 1
<p>Structures of (<b>1</b>) 3-thiophenecarboxylic acid (3tpcH), (<b>2</b>) 2-methyl-3-furoic acid (2m3furH), (<b>3</b>) 3-furoic acid (3furH), (<b>4</b>) 4-hydroxycinnamic acid (4hocinH), and (<b>5</b>) 4-hydroxybenzoic acid (4hobH).</p>
Full article ">Scheme 1
<p>The synthesis of alkali-metal carboxylate complexes.</p>
Full article ">
17 pages, 15144 KiB  
Article
Ge–Cu-Complexes Ph(pyO)Ge(μ2-pyO)2CuCl and PhGe(μ2-pyO)4CuCl—Representatives of Cu(I)→Ge(IV) and Cu(II)→Ge(IV) Dative Bond Systems
by Jörg Wagler and Robert Gericke
Molecules 2023, 28(14), 5442; https://doi.org/10.3390/molecules28145442 - 16 Jul 2023
Cited by 1 | Viewed by 1432
Abstract
Phenylgermaniumpyridine-2-olate PhGe(pyO)3 (compound 1Ge) and CuCl react with the formation of the heteronuclear complex Ph(pyO)Ge(μ2-pyO)2CuCl (2Ge’) rather than forming the expected compound PhGe(μ2-pyO)3CuCl (2Ge). Single-point calculations (at the B2T-PLYP [...] Read more.
Phenylgermaniumpyridine-2-olate PhGe(pyO)3 (compound 1Ge) and CuCl react with the formation of the heteronuclear complex Ph(pyO)Ge(μ2-pyO)2CuCl (2Ge’) rather than forming the expected compound PhGe(μ2-pyO)3CuCl (2Ge). Single-point calculations (at the B2T-PLYP level) of the optimized molecular structures confirmed the relative stability of isomer 2Ge’ over 2Ge and, for the related silicon congeners, the relative stability of 2Si over 2Si’. Decomposition of a solution of 2Ge’ upon access to air provided access to some crystals of the copper(II) compound PhGe(μ2-pyO)4CuCl (3Ge). Compounds 2Ge’ and 3Ge were characterized by single-crystal X-ray diffraction analyses, and the Ge–Cu bonds in these compounds were analyzed with the aid of quantum chemical calculations, e.g., Natural Bond Orbital analyses (NBO), Non-Covalent Interactions descriptor (NCI), and topology of the electron density at bond critical point using Quantum Theory of Atoms-In-Molecules (QTAIM) in conjunction with the related silicon compounds PhSi(μ2-pyO)3CuCl (2Si), PhSi(μ2-pyO)4CuCl (3Si), as well as the potential isomers Ph(pyO)Si(μ2-pyO)2CuCl (2Si’) and PhGe(μ2-pyO)3CuCl (2Ge). Pronounced Cu→Ge (over Cu→Si) lone pair donation was found for the Cu(I) compounds, whereas in Cu(II) compounds 3Si and 3Ge, this σ-donation is less pronounced and only marginally enhanced in 3Ge over 3Si. Full article
(This article belongs to the Special Issue Exclusive Feature Papers in Inorganic Chemistry, 2nd Edition)
Show Figures

Figure 1

Figure 1
<p>Examples of compounds that feature donor-acceptor bonds between a d-block element donor site and a p-block element acceptor site (compounds <b>I</b>–<b>XIV</b>) as well as the starting material for the current study (<b>1Ge</b>). Note: The donor-acceptor bonds vary in strength and have simply been accounted for by drawing a bond in compounds <b>I</b>–<b>IX</b>. For the compounds of particular interest in the current study, the presence of rather weak donor-acceptor interactions in <b>X</b>–<b>XII</b> and <b>XIV</b> is underlined by the use of a dashed line rather than a solid bond. Compounds <b>XV</b>–<b>XVII</b> represent selected examples of Cu–Ge-compounds with germyl- or germylene-type Cu–Ge bonds (Cu–Ge bond length in Å is given in parentheses).</p>
Full article ">Figure 2
<p>Molecular structure of <b>2Ge’</b> in the crystal (displacement ellipsoids drawn at the 50% probability level, selected atoms labeled; H atoms are omitted for clarity). Selected interatomic distances (Å) and angles (deg.): Ge1–Cu1 2.7886(3), Ge1–O1 1.7919(14), Ge1–O2 1.7794(14), Ge1–O3 1.7894(14), Ge1⋯N3 2.6840(17), Ge1–C16 1.9217(19), Cu1–Cl1 2.2669(5), Cu1–N1 1.9767(16), Cu1–N2 1.9782(16), Cu1⋯C16 2.6044(18), Cu1–Ge1–O1 84.23(5), Cu1–Ge1–O2 83.63(4), Cu1–Ge1–O3 174.78(5), Cu1–Ge1–C16 64.07(5), O1–Ge1–O2 104.58(7), O1–Ge1–O3 90.72(6), O2–Ge1–O3 98.94(6), O1–Ge1–C16 112.66(8), O2–Ge1–C16 126.41(7), O3–Ge1–C16 117.10(7), O1–Ge1–N3 147.52(6), Ge1–Gu1–Cl1 156.38(2), Cl1–Cu1–N1 108.80(5), Cl1–Cu1–N2 106.63(5), N1–Cu1–N2 135.69(7).</p>
Full article ">Figure 3
<p>Molecular structure of <b>3Ge</b> in the crystal (displacement ellipsoids drawn at the 50% probability level, selected atoms labeled; H atoms are omitted for clarity). Selected interatomic distances (Å) and angles (deg.): Ge1–Cu1 2.8969(4), Ge1–O1 1.8856(18), Ge1–O2 1.8543(19), Ge1–O3 1.8785(18), Ge1–O4 1.8691(18), Ge1–C21 1.915(3), Cu1–Cl1 2.4027(7), Cu1–N1 2.043(2), Cu1–N2 2.033(2), Cu1–N3 2.027(2), Cu1–N4 2.034(2), Cu1–Ge1–C21 177.85(8), O1–Ge1–O3 155.96(8), O2–Ge1–O4 154.10(8), Ge1–Cu1–Cl1 177.59(2), N1–Cu1–N3 161.77(9), N2–Cu1–N4 161.61(9).</p>
Full article ">Figure 4
<p>Pairs of isomers <b>2Si</b>/<b><span class="html-italic">2Si’</span></b> and <b><span class="html-italic">2Ge</span></b>/<b>2Ge’</b> optimized at the PBE0 level of theory and their relative energy values in kcal mol<sup>−1</sup> from single-point calculation at the B2T-PLYP level.</p>
Full article ">Figure 5
<p>Non-Covalent Interactions descriptor (NCI) for pairs of congeners <b>2Si</b>/<b><span class="html-italic">2Ge</span></b>, <b><span class="html-italic">2Si’</span></b>/<b>2Ge,’</b> and <b>3Si</b>/<b>3Ge</b> with color scale (RDG iso-value 0.45; blue zones indicate attractive interactions, red zones indicate repulsive interactions). Particular features (<b>A</b>–<b>E</b>), which are mentioned in the discussion, are pointed out with red arrows.</p>
Full article ">Figure 6
<p>Graphical representation of the Electron Localization Function (ELF) for pairs of congeners <b>2Si</b>/<b><span class="html-italic">2Ge</span></b>, <b><span class="html-italic">2Si’</span></b>/<b>2Ge’,</b> and <b>3Si</b>/<b>3Ge</b> with color scale. In all graphics, the Cu–<span class="html-italic">E</span> (<span class="html-italic">E</span> = Si, Ge) bond is in the plane. For compounds <b><span class="html-italic">2Si’</span></b> and <b>2Ge’</b>, the phenyl ipso-C is located in the plane as well. Red arrows point at this atom’s influence on the electron localization near the Cu–<span class="html-italic">E</span> (<span class="html-italic">E</span> = Si, Ge) bond.</p>
Full article ">Figure 7
<p>Visualization of NLMOs (isosurface 0.05 au) involved in σ-Cu–<span class="html-italic">E</span> bonding in compounds <b>2Si</b>, <b><span class="html-italic">2Si’</span></b>, <b><span class="html-italic">2Ge</span></b>, <b>2Ge’</b>, <b>3Si,</b> and <b>3Ge</b>.</p>
Full article ">Figure 8
<p>Visualization of NBOs (isosurface 0.05 au) involved in electron density donation from the tetrel-bound phenyl group (from the tetrel−C<sub>ipso</sub> bond (<b>a</b>) and from a phenyl π-bond (<b>b</b>)) toward the Cu atom in compounds <b><span class="html-italic">2Si’</span></b> and <b>2Ge’</b>. For each donor-acceptor interaction shown, the interaction energy is given in kcal mol<sup>−1</sup>.</p>
Full article ">Scheme 1
<p>Syntheses of the compounds under investigation. (The compound codes of the potential isomers <b><span class="html-italic">2Ge</span></b> and <b><span class="html-italic">2Si’</span></b>, which have not been isolated or identified experimentally but will be included in computational analyses, are italicized.)</p>
Full article ">

Review

Jump to: Research

38 pages, 19100 KiB  
Review
Polyanion Condensation in Inorganic and Hybrid Fluoridometallates (IV) of Octahedrally Coordinated Ti, Zr, Hf, V, Cr, W, Mn, Ge, Sn, and Pb
by Zoran Mazej
Molecules 2024, 29(6), 1361; https://doi.org/10.3390/molecules29061361 - 19 Mar 2024
Viewed by 1089
Abstract
In fluorides, the M4+ cations of M = Ti, V, Cr, Mn, Ge, Sn, and Pb favour the octahedral coordination of six F ligands. Some examples of M4+ with larger cations (M = Zr, Hf, W) in octahedral coordination are also [...] Read more.
In fluorides, the M4+ cations of M = Ti, V, Cr, Mn, Ge, Sn, and Pb favour the octahedral coordination of six F ligands. Some examples of M4+ with larger cations (M = Zr, Hf, W) in octahedral coordination are also known. If not enough F ligands are available to have isolated MIVF6 octahedra, they must share their F ligands. The crystal structures of such fluoride metalates (IV) show the variety of possible structural motifs of the zero-dimensional oligomeric anions [M2F11]3− (M = Ti, Cr), [M3F15]3− (M = Zr, Hf), [M3F16]4− (M = Ge), [M4F18]2− (M = Ti, W), [M4F19]3− (M = Ti), [M4F20]4− (M = Ti), [M5F23]3− (M = Ti), [M6F27]3− (M = Ti), [M6F28]4− (M = Ti), [M8F36]4− (M = Ti, Mn), [M10F45]5− (M = Ti) to one-dimensional chains ([MF5]) (M = V, Ti, Cr, Ge, Sn, Pb), double chains ([M2F9]) (M = Ti, Mn), columns ([M3F13]) (M = Ti), ([M4F19]3−) (M = Ti), ([M7F30]2−) (M = Ti), ([M9F38]2−)) (M = Ti), two-dimensional layers ([M2F9]) (M = Cr), ([M8F33]) (M = Ti), and three-dimensional ([M6F27]3−) (M = Ti) architectures. A discrete monomeric [M2F9] anion with two MIVF6 octahedra sharing a common face has not yet been experimentally demonstrated, while two examples containing discrete dimeric [M2F10]2− anions (M = Ti) with two MIVF6 octahedra sharing an edge are still in question. Full article
(This article belongs to the Special Issue Exclusive Feature Papers in Inorganic Chemistry, 2nd Edition)
Show Figures

Figure 1

Figure 1
<p>Hypothetical dimeric [M<sub>2</sub>F<sub>9</sub>]<sup>−</sup> anion (M = Ti, Ge) with two M<sup>IV</sup>F<sub>6</sub> octahedra sharing a common face.</p>
Full article ">Figure 2
<p>Hypothetical dimeric [M<sub>2</sub>F<sub>10</sub>]<sup>2−</sup> anion (M = M<sup>4+</sup>) with two M<sup>IV</sup>F<sub>6</sub> octahedra sharing a common edge.</p>
Full article ">Figure 3
<p>Two crystallographically different dimeric [Ti<sub>2</sub>F<sub>11</sub>]<sup>−</sup> anions in the crystal structure of [C<sub>3</sub>H<sub>5</sub>N<sub>2</sub>]<sub>3</sub>[Ti<sub>2</sub>F<sub>11</sub>] with two TiF<sub>6</sub> octahedra sharing a common vertex.</p>
Full article ">Figure 3 Cont.
<p>Two crystallographically different dimeric [Ti<sub>2</sub>F<sub>11</sub>]<sup>−</sup> anions in the crystal structure of [C<sub>3</sub>H<sub>5</sub>N<sub>2</sub>]<sub>3</sub>[Ti<sub>2</sub>F<sub>11</sub>] with two TiF<sub>6</sub> octahedra sharing a common vertex.</p>
Full article ">Figure 4
<p>Dimeric [Ti<sub>2</sub>F<sub>11</sub>]<sup>3−</sup> anion in the crystal structure of [C<sub>5</sub>H<sub>6</sub>N]<sub>2</sub>[H<sub>3</sub>O][Ti<sub>2</sub>F<sub>11</sub>]·H<sub>2</sub>O with two TiF<sub>6</sub> octahedra sharing a common vertex.</p>
Full article ">Figure 5
<p>Dimeric [Cr<sub>2</sub>F<sub>11</sub>]<sup>−</sup> anion in the crystal structure of K<sub>3</sub>Cr<sub>2</sub>F<sub>11</sub>·2HF with two CrF<sub>6</sub> octahedra sharing a common vertex.</p>
Full article ">Figure 6
<p>Theoretical models for trimeric [Ti<sub>3</sub>F<sub>13</sub>]<sup>−</sup> anion (<b>left</b>) and [Ge<sub>3</sub>F<sub>13</sub>]<sup>−</sup> anion (<b>right</b>). Copyright (2018) Elsevier. Used with permission from Ref. [<a href="#B7-molecules-29-01361" class="html-bibr">7</a>].</p>
Full article ">Figure 7
<p>Trimeric [M<sub>3</sub>F<sub>15</sub>]<sup>3−</sup> anion (M = Zr, Hf) in the crystal structure of [IDiPPH]<sub>3</sub>[M<sub>3</sub>F<sub>15</sub>]·4thf ·0.55(CH<sub>2</sub>Cl<sub>2</sub>) (IDiPP = 1,3-(2,6-di-isopropylphenyl)imidazol-2-ylidene).</p>
Full article ">Figure 8
<p>Trimeric [Ge<sub>3</sub>F<sub>16</sub>]<sup>4−</sup> anion in the crystal structure of [(CH<sub>2</sub>)<sub>2</sub>SOH][Ge<sub>3</sub>F<sub>16</sub>].</p>
Full article ">Figure 9
<p>Trimeric [Ge<sub>3</sub>F<sub>16</sub>]<sup>4−</sup> anion in the crystal structure of [C(NH<sub>2</sub>)<sub>2</sub>(NH<sub>3</sub>)<sub>2</sub>][Ge<sub>3</sub>F<sub>16</sub>]·2HF.</p>
Full article ">Figure 10
<p>Trimeric [Ge<sub>3</sub>F<sub>16</sub>]<sup>4−</sup> anion in the crystal structure of [C(NH<sub>2</sub>)<sub>2</sub>(NH<sub>3</sub>)<sub>2</sub>][Ge<sub>3</sub>F<sub>16</sub>]·HF.</p>
Full article ">Figure 11
<p>Tetrameric [M<sub>4</sub>F<sub>18</sub>]<sup>2−</sup> anion (M = Ti, W) in the crystal structures of [TiF<sub>2</sub>([15]crown-5)][Ti<sub>4</sub>F<sub>18</sub>]⋅0.5MeCN, [N(CH<sub>3</sub>)<sub>4</sub>]<sub>2</sub>[Ti<sub>4</sub>F<sub>18</sub>], [(C<sub>6</sub>H<sub>5</sub>)<sub>4</sub>P]<sub>2</sub>[Ti<sub>4</sub>F<sub>18</sub>], [o-C<sub>6</sub>H<sub>4</sub>(P(C<sub>6</sub>H<sub>5</sub>)<sub>2</sub>H)<sub>2</sub>][Ti<sub>4</sub>F<sub>18</sub>], o-C<sub>6</sub>H<sub>4</sub>(As(CH<sub>3</sub>)<sub>2</sub>H)<sub>2</sub>][Ti<sub>4</sub>F<sub>18</sub>], [H<sup>i</sup>PrS(CH<sub>2</sub>)<sub>2</sub>S<sup>i</sup>PrH][Ti<sub>4</sub>F<sub>18</sub>], and [WCl<sub>2</sub>(cp)<sub>2</sub>][W<sub>4</sub>F<sub>18</sub>] (cp = η-C<sub>6</sub>H<sub>5</sub>).</p>
Full article ">Figure 12
<p>Tetrameric [Ti<sub>4</sub>F<sub>19</sub>]<sup>3−</sup> anion in the crystal structure of [XeF<sub>5</sub>]<sub>3</sub>[Ti<sub>4</sub>F<sub>19</sub>].</p>
Full article ">Figure 13
<p>Tetrameric [Ti<sub>4</sub>F<sub>20</sub>]<sup>4−</sup> anion in the crystal structure of α-[C<sub>3</sub>H<sub>5</sub>N<sub>2</sub>]<sub>4</sub>[Ti<sub>4</sub>F<sub>20</sub>].</p>
Full article ">Figure 14
<p>Tetrameric [Ti<sub>4</sub>F<sub>20</sub>]<sup>4−</sup> anion in the crystal structure of β-[C<sub>3</sub>H<sub>5</sub>N<sub>2</sub>]<sub>4</sub>[Ti<sub>4</sub>F<sub>20</sub>].</p>
Full article ">Figure 15
<p>Tetrameric [Ti<sub>4</sub>F<sub>20</sub>]<sup>4−</sup> anion in the crystal structure of [C(NH<sub>2</sub>)<sub>3</sub>]<sub>4</sub>[Ti<sub>4</sub>F<sub>20</sub>].</p>
Full article ">Figure 16
<p>Tetrameric [Ti<sub>4</sub>F<sub>20</sub>]<sup>4−</sup> anion in the crystal structure of [C(NH<sub>2</sub>)<sub>3</sub>]<sub>4</sub>(H<sub>3</sub>O)<sub>4</sub>[Ti<sub>4</sub>F<sub>20</sub>][TiF<sub>5</sub>]<sub>4</sub>.</p>
Full article ">Figure 17
<p>Pentameric [Ti<sub>5</sub>F<sub>23</sub>]<sup>3−</sup> anion in the crystal structure of [ImH]<sub>3</sub>[Ti<sub>5</sub>F<sub>23</sub>].</p>
Full article ">Figure 18
<p>Hexameric [Ti<sub>6</sub>F<sub>27</sub>]<sup>3−</sup> anion in the crystal structures of [C(NH<sub>2</sub>)<sub>3</sub>]<sub>3</sub>[Ti<sub>6</sub>F<sub>27</sub>]·SO<sub>2</sub> and [C<sub>3</sub>H<sub>5</sub>N<sub>2</sub>]<sub>2</sub>[H<sub>3</sub>O][Ti<sub>6</sub>F<sub>27</sub>].</p>
Full article ">Figure 19
<p>Hexameric [Ti<sub>6</sub>F<sub>28</sub>]<sup>4−</sup> anion in the crystal structure of [ImH]<sub>8−n</sub>[X]<sub>n</sub>[Ti<sub>8</sub>F<sub>36</sub>][Ti<sub>6</sub>F<sub>28</sub>] (X = unknown cation).</p>
Full article ">Figure 20
<p>Octameric [Ti<sub>8</sub>F<sub>36</sub>]<sup>4−</sup> anion in the crystal structures of K<sub>4</sub>[Ti<sub>8</sub>F<sub>36</sub>]·8HF, Rb<sub>4</sub>[Ti<sub>8</sub>F<sub>36</sub>]·6HF, and [H<sub>5</sub>O<sub>2</sub>]<sub>4</sub>[Ti<sub>8</sub>F<sub>36</sub>].</p>
Full article ">Figure 21
<p>Octameric [Mn<sub>8</sub>F<sub>36</sub>]<sup>4−</sup> anion in the crystal structure of [XeF<sub>5</sub>]<sub>4</sub>[Mn<sub>8</sub>F<sub>36</sub>].</p>
Full article ">Figure 22
<p>Decameric [Ti<sub>10</sub>F<sub>45</sub>]<sup>5−</sup> anion in the crystal structure of [XeF<sub>5</sub>]<sub>5</sub>[Ti<sub>10</sub>F<sub>45</sub>].</p>
Full article ">Figure 23
<p>Polymeric trans-([GeF<sub>5</sub>]<sup>−</sup>)<sub>∞</sub> chain in the crystal structure of XeF<sub>5</sub>GeF<sub>5</sub>.</p>
Full article ">Figure 24
<p>Polymeric trans-([CrF<sub>5</sub>]<sup>−</sup>)<sub>∞</sub> chain in the crystal structure of XeF<sub>2</sub>·CrF<sub>4</sub>.</p>
Full article ">Figure 25
<p>Polymeric cis-([TiF<sub>5</sub>]<sup>−</sup>)<sub>∞</sub> chain in the crystal structure of H<sub>3</sub>OTiF<sub>5</sub>.</p>
Full article ">Figure 26
<p>Polymeric cis-([TiF<sub>5</sub>]<sup>−</sup>)<sub>∞</sub> chain in the crystal structure of NH<sub>4</sub>TiF<sub>5</sub>.</p>
Full article ">Figure 27
<p>Polymeric cis-([TiF<sub>5</sub>]<sup>−</sup>)<sub>∞</sub> chain in the crystal structure of NaTiF<sub>5</sub>·HF.</p>
Full article ">Figure 28
<p>Polymeric cis-([TiF<sub>5</sub>]<sup>−</sup>)<sub>∞</sub> chain in the crystal structure of KTiF<sub>5</sub>.</p>
Full article ">Figure 29
<p>Polymeric cis-([TiF<sub>5</sub>]<sup>−</sup>)<sub>∞</sub> chain in the crystal structures of KTiF<sub>5</sub>·HF and RbTiF<sub>5</sub>·HF.</p>
Full article ">Figure 30
<p>Polymeric cis-([TiF<sub>5</sub>]<sup>−</sup>)<sub>∞</sub> chain in the crystal structure of CsTiF<sub>5</sub>.</p>
Full article ">Figure 31
<p>Polymeric cis-([TiF<sub>5</sub>]<sup>−</sup>)<sub>∞</sub> chain in the crystal structure of [enH<sub>2</sub>](TiF<sub>5</sub>)<sub>2</sub> (en = ethane-1,2-diamine).</p>
Full article ">Figure 32
<p>Polymeric cis-([VF<sub>5</sub>]<sup>−</sup>)<sub>∞</sub> chain in the crystal structure of [H<sub>3</sub>N(CH<sub>2</sub>)<sub>2</sub>NH<sub>2</sub>][VF<sub>5</sub>].</p>
Full article ">Figure 33
<p>Polymeric cis-([CrF<sub>5</sub>]<sup>−</sup>)<sub>∞</sub> chain in the crystal structure of RbCrF<sub>5</sub>.</p>
Full article ">Figure 34
<p>Polymeric cis-([CrF<sub>5</sub>]<sup>−</sup>)<sub>∞</sub> chain in the crystal structure of CsCrF<sub>5</sub>.</p>
Full article ">Figure 35
<p>Polymeric cis-([GeF<sub>5</sub>]<sup>−</sup>)<sub>∞</sub> chain in the crystal structure of O<sub>2</sub>GeF<sub>5</sub>·HF.</p>
Full article ">Figure 36
<p>Polymeric cis-([SnF<sub>5</sub>]<sup>−</sup>)<sub>∞</sub> chain in the crystal structure of ClO<sub>2</sub>SnF<sub>5</sub>.</p>
Full article ">Figure 37
<p>Polymeric cis-([MF<sub>5</sub>]<sup>−</sup>)<sub>∞</sub> chain (M = Sn, Pb) in the crystal structure of ClOF<sub>2</sub>MF<sub>5</sub> (M = Sn, Pb).</p>
Full article ">Figure 38
<p>Polymeric cis-([CrF<sub>5</sub>]<sup>−</sup>)<sub>∞</sub> chain in the crystal structure of XeF<sub>5</sub>CrF<sub>5</sub>.</p>
Full article ">Figure 39
<p>Polymeric cis-[(MnF<sub>5</sub>]<sup>−</sup>)<sub>∞</sub> chain in the crystal structure of XeF<sub>5</sub>MnF<sub>5</sub>.</p>
Full article ">Figure 40
<p>Polymeric cis-(TiF<sub>5</sub>]<sup>−</sup>)<sub>∞</sub> chain in the crystal structure of [C(NH<sub>2</sub>)<sub>3</sub>]<sub>4</sub>(H<sub>3</sub>O)<sub>4</sub>[Ti<sub>4</sub>F<sub>20</sub>][TiF<sub>5</sub>]<sub>4</sub>.</p>
Full article ">Figure 41
<p>Polymeric cis-(GeF<sub>5</sub>]<sup>−</sup>)<sub>∞</sub> chain in the crystal structure of ClO<sub>2</sub>GeF<sub>5</sub>.</p>
Full article ">Figure 42
<p>Polymeric cis-and trans-([CrF<sub>5</sub>]<sup>−</sup>)<sub>∞</sub> chain in the crystal structure of (XeF<sub>5</sub>CrF<sub>5</sub>)<sub>4</sub>·XeF<sub>4</sub>.</p>
Full article ">Figure 43
<p>Polymeric chain-like ([Sn<sub>2</sub>F<sub>9</sub>]<sup>−</sup>)<sub>∞</sub> anion in the crystal structure of α-O<sub>2</sub>Sn<sub>2</sub>F<sub>9</sub>.</p>
Full article ">Figure 44
<p>Polymeric chain-like ([Ti<sub>2</sub>F<sub>9</sub>]<sup>−</sup>)<sub>∞</sub> anion in the crystal structure of α-[H<sub>3</sub>O][Ti<sub>2</sub>F<sub>9</sub>].</p>
Full article ">Figure 45
<p>Polymeric chain-like ([Ti<sub>2</sub>F<sub>9</sub>]<sup>−</sup>)<sub>∞</sub> anion in the crystal structure of β-[H<sub>3</sub>O][Ti<sub>2</sub>F<sub>9</sub>].</p>
Full article ">Figure 46
<p>Polymeric chain-like ([Ti<sub>2</sub>F<sub>9</sub>]<sup>−</sup>)<sub>∞</sub> anion in the crystal structure of NaTi<sub>2</sub>F<sub>9</sub>·HF.</p>
Full article ">Figure 47
<p>Polymeric chain-like ([Ti<sub>2</sub>F<sub>9</sub>]<sup>−</sup>)<sub>∞</sub> anions in the crystal structure of RbTi<sub>2</sub>F<sub>9</sub>.</p>
Full article ">Figure 48
<p>Polymeric chain-like ([Ti<sub>2</sub>F<sub>9</sub>]<sup>−</sup>)<sub>∞</sub> anion in the crystal structure of CsTi<sub>2</sub>F<sub>9</sub>.</p>
Full article ">Figure 49
<p>Polymeric chain-like ([Ti<sub>2</sub>F<sub>9</sub>]<sup>−</sup>)<sub>∞</sub> anion in the crystal structure of α-[ImH][Ti<sub>2</sub>F<sub>9</sub>].</p>
Full article ">Figure 50
<p>Polymeric chain-like ([Ti<sub>2</sub>F<sub>9</sub>]<sup>−</sup>)<sub>∞</sub> anion in the crystal structure of β-[ImH][Ti<sub>2</sub>F<sub>9</sub>].</p>
Full article ">Figure 51
<p>Polymeric chain-like ([Ti<sub>2</sub>F<sub>9</sub>]<sup>−</sup>)<sub>∞</sub> anion in the crystal structure of [gvH][Ti<sub>2</sub>F<sub>9</sub>].</p>
Full article ">Figure 52
<p>Polymeric chain-like ([Ti<sub>2</sub>F<sub>9</sub>]<sup>−</sup>)<sub>∞</sub> anions in the crystal structure of [ClO<sub>2</sub>][Ti<sub>2</sub>F<sub>9</sub>].</p>
Full article ">Figure 53
<p>Polymeric chain-like ([Mn<sub>2</sub>F<sub>9</sub>]<sup>−</sup>)<sub>∞</sub> anion in the crystal structure of [O<sub>2</sub>][Mn<sub>2</sub>F<sub>9</sub>].</p>
Full article ">Figure 54
<p>Polymeric column-like ([Ti<sub>2</sub>F<sub>13</sub>]<sup>−</sup>)<sub>∞</sub> anion in the crystal structure of [XeF<sub>5</sub>][Ti<sub>3</sub>F<sub>13</sub>].</p>
Full article ">Figure 55
<p>Polymeric column-like ([Ti<sub>4</sub>F<sub>19</sub>]<sup>3−</sup>)<sub>∞</sub> anion in the crystal structure of Cs<sub>3</sub>[Ti<sub>4</sub>F<sub>19</sub>].</p>
Full article ">Figure 56
<p>Polymeric column-like ([Ti<sub>7</sub>F<sub>30</sub>]<sup>2−</sup>)<sub>∞</sub> anion in the crystal structure of (O<sub>2</sub>)<sub>2</sub>[Ti<sub>7</sub>F<sub>30</sub>].</p>
Full article ">Figure 57
<p>Polymeric column-like ([Ti<sub>9</sub>F<sub>38</sub>]<sup>2−</sup>)<sub>∞</sub> anion in the crystal structure of [XeF]<sub>2</sub>[Ti<sub>9</sub>F<sub>38</sub>].</p>
Full article ">Figure 58
<p>Packing of polymeric anionic layers ([Ti<sub>8</sub>F<sub>33</sub>]<sup>−</sup>)<sub>∞</sub> in the crystal structure of CsTi<sub>8</sub>F<sub>3</sub>.</p>
Full article ">Figure 59
<p>Packing of polymeric anionic layers ([Ti<sub>8</sub>F<sub>33</sub>]<sup>−</sup>)<sub>∞</sub> in the crystal structure of [Xe<sub>2</sub>F<sub>3</sub>][Ti<sub>8</sub>F<sub>33</sub>].</p>
Full article ">Figure 60
<p>Packing of polymeric anionic layers ([Cr<sub>2</sub>F<sub>9</sub>]<sup>−</sup>)<sub>∞</sub> in the crystal structure of XeF<sub>2</sub>·2CrF<sub>4</sub>.</p>
Full article ">Figure 61
<p>Three-dimensional framework of the ([Ti<sub>6</sub>F<sub>27</sub>]<sup>3−</sup>)<sub>∞</sub> anion in the crystal structure of [H<sub>3</sub>O]<sub>3</sub>[Ti<sub>6</sub>F<sub>27</sub>].</p>
Full article ">
18 pages, 7634 KiB  
Review
Biomedical Applications of Sulfonylcalix[4]arene-Based Metal–Organic Supercontainers
by Ya-Wen Fan, Meng-Xue Shi, Zhenqiang Wang, Feng-Rong Dai and Zhong-Ning Chen
Molecules 2024, 29(6), 1220; https://doi.org/10.3390/molecules29061220 - 8 Mar 2024
Cited by 1 | Viewed by 1524
Abstract
Coordination cages sustained by metal–ligand interactions feature polyhedral architectures and well-defined hollow structures, which have attracted significant attention in recent years due to a variety of structure-guided promising applications. Sulfonylcalix[4]arenes-based coordination cages, termed metal–organic supercontainers (MOSCs), that possess unique multi-pore architectures containing an [...] Read more.
Coordination cages sustained by metal–ligand interactions feature polyhedral architectures and well-defined hollow structures, which have attracted significant attention in recent years due to a variety of structure-guided promising applications. Sulfonylcalix[4]arenes-based coordination cages, termed metal–organic supercontainers (MOSCs), that possess unique multi-pore architectures containing an endo cavity and multiple exo cavities, are emerging as a new family of coordination cages. The well-defined built-in multiple binding domains of MOSCs allow the efficient encapsulation of guest molecules, especially for drug delivery. Here, we critically discuss the design strategy, and, most importantly, the recent advances in research surrounding cavity-specified host–guest chemistry and biomedical applications of MOSCs. Full article
(This article belongs to the Special Issue Exclusive Feature Papers in Inorganic Chemistry, 2nd Edition)
Show Figures

Graphical abstract

Graphical abstract
Full article ">Figure 1
<p>Structural regulation of MOSCs by judicious design of various carboxylate linkers.</p>
Full article ">Figure 2
<p>(<b>a</b>) The structures of <b>MOSC-1-Co</b> and drug guests (<b>D1</b> and <b>D2</b>), and the processes of drug encapsulation. The Co<sup>2+</sup> centers are shown in green. The spheres serve to guide the eyes representing the <span class="html-italic">endo</span> cavity (purple), six <span class="html-italic">exo</span> cavities (yellow), and one of the eight external pockets (gray). (<b>b</b>) Plots of <b>D1</b>/<b>MOSC-1-Co</b> molar ratio vs. absorbance at 360 nm based on the titration experiment. (<b>c</b>) The nonlinear form fits to the Hill equation of UV–Vis titration experiments based on the absorption band centered at 370 nm in the [<b>D1</b>]/[<b>MOSC-1-Co</b>]. Adapted with permission from [<a href="#B55-molecules-29-01220" class="html-bibr">55</a>].</p>
Full article ">Figure 3
<p>Schematic representation of (<b>a</b>) stepwise drug encapsulation by <span class="html-italic">endo</span> and <span class="html-italic">exo</span> cavities of MgDHIA; (<b>b</b>) stepwise drug-release processes of RAPA-FA@MgDHIA. (<b>c</b>) Live (green) and dead (red) staining plots of cells after 24 h of treatment with different concentrations of MgHDIA. Reproduced from [<a href="#B56-molecules-29-01220" class="html-bibr">56</a>]. Copyright (2021), with permission from Elsevier.</p>
Full article ">Figure 4
<p>(<b>a</b>) Crystal structure of coordination container ZnPMTC. The spheres serve to guide the eyes representing the <span class="html-italic">endo</span> cavity (yellow) and <span class="html-italic">exo</span> cavities (blue). (<b>b</b>) Accumulated drug release of NPX@ZnPMTC, DCF@ZnPMTC, and AP@ZnPMTC in PBS solution at pH = 5.0, 6.0, and 7.4. (<b>c</b>) Live (green) and dead (red) staining plots of cells after 24 h of treatment with varying concentrations of ZnPMTC. Reproduced with permission from [<a href="#B57-molecules-29-01220" class="html-bibr">57</a>]. Copyright © 2021, American Chemical Society.</p>
Full article ">Figure 5
<p>(<b>a</b>) Design of proton-responsive fluorescent MOSCs. The metal centers are shown in green, the -NH- groups are shown in blue ball, and the pyrenyl units are shown in red spacefill. (<b>b</b>) Switching “on” and “off” of Zn-NH-pyr with CF<sub>3</sub>COOH/Et<sub>3</sub>N can be repeated in multiple cycles. Reproduced with permission from [<a href="#B46-molecules-29-01220" class="html-bibr">46</a>].</p>
Full article ">Figure 6
<p>(<b>top</b>) Luminescence intensities of <b>Tb-TBSC</b> (544 nm) with various urine constituents in the CH<sub>3</sub>CN/H<sub>2</sub>O (<span class="html-italic">v</span>:<span class="html-italic">v</span> = 4:1) solution in the absence or presence of 1-OHP (<span class="html-italic">λ</span><sub>ex</sub> = 346 nm). (<b>bottom</b>) Photographs of the emission colors of <b>Tb-TBSC</b> with various urine constituents in the CH<sub>3</sub>CN/H<sub>2</sub>O (<span class="html-italic">v</span>:<span class="html-italic">v</span> = 4:1) solution under the irradiation of UV light at 365 nm. Reproduced with permission from [<a href="#B59-molecules-29-01220" class="html-bibr">59</a>].</p>
Full article ">Figure 7
<p>(<b>a</b>) Cargo encapsulation and release of PCC-1 and PCC-2. (<b>b</b>) Cell viability of CPT, CPT@PCC-1, CPT@PCC-2, and CPT@PCC-3 at concentration of 5.0, 10, and 15 µg mL<sup>−1</sup> (*** <span class="html-italic">p</span> &lt; 0.05; Student’s <span class="html-italic">t</span>-test), measured by Sytox Green assay. Reproduced with permission from [<a href="#B38-molecules-29-01220" class="html-bibr">38</a>]. Copyright © 2018 by John Wiley and Sons.</p>
Full article ">Figure 8
<p>In vivo biodistribution and radiographic evaluation of Drugs@MgDHIA systems on CFA-induced TMJ inflammation. (<b>a</b>) Schematic diagram of CFA induced TMJ Inflammation in Sprague–Dawley (SD) rats. (<b>b</b>) IVIS imaging showing the biodistribution of macrophagetargeted MgDHIA (RB-FA@MgDHIA) in control and CFA groups. (<b>c</b>) Distribution of RB-FA@MgDHIA injected into the joint cavity by cryostat serial section. Reproduced with permission from [<a href="#B56-molecules-29-01220" class="html-bibr">56</a>].</p>
Full article ">Figure 9
<p>Schematic illustration of the synthesis, encapsulation, and application of 4-OI@Zn-NH-pyr for enhanced therapy in severe joint inflammation. Reproduced with permission from [<a href="#B58-molecules-29-01220" class="html-bibr">58</a>].</p>
Full article ">
18 pages, 8970 KiB  
Review
Recent Progress on Perovskite-Based Electrocatalysts for Efficient CO2 Reduction
by Tong Wu, Lihua Zhang, Yinbo Zhan, Yilin Dong, Zheng Tan, Bowei Zhou, Fei Wei, Dongliang Zhang and Xia Long
Molecules 2023, 28(24), 8154; https://doi.org/10.3390/molecules28248154 - 18 Dec 2023
Cited by 1 | Viewed by 2460
Abstract
An efficient carbon dioxide reduction reaction (CO2RR), which reduces CO2 to low-carbon fuels and high-value chemicals, is a promising approach for realizing the goal of carbon neutrality, for which effective but low-cost catalysts are critically important. Recently, many inorganic perovskite-based [...] Read more.
An efficient carbon dioxide reduction reaction (CO2RR), which reduces CO2 to low-carbon fuels and high-value chemicals, is a promising approach for realizing the goal of carbon neutrality, for which effective but low-cost catalysts are critically important. Recently, many inorganic perovskite-based materials with tunable chemical compositions have been applied in the electrochemical CO2RR, which exhibited advanced catalytic performance. Therefore, a timely review of this progress, which has not been reported to date, is imperative. Herein, the physicochemical characteristics, fabrication methods and applications of inorganic perovskites and their derivatives in electrochemical CO2RR are systematically reviewed, with emphasis on the structural evolution and product selectivity of these electrocatalysts. What is more, the current challenges and future directions of perovskite-based materials regarding efficient CO2RR are proposed, to shed light on the further development of this prospective research area. Full article
(This article belongs to the Special Issue Exclusive Feature Papers in Inorganic Chemistry, 2nd Edition)
Show Figures

Figure 1

Figure 1
<p>Schematic representation of the main content of this review.</p>
Full article ">Figure 2
<p>Three main steps on the catalyst surface of CO<sub>2</sub>RR processes. Black spheres represent carbon atoms; red spheres represent oxygen atoms; white spheres represent hydrogen atoms; orange atoms represent the CO<sub>2</sub>RR catalyst.</p>
Full article ">Figure 3
<p>Crystal structures of (<b>a</b>) SrSnO<sub>3</sub> and (<b>b</b>) Sr<sub>2</sub>SnO<sub>4</sub>, reprinted with permission from ref [<a href="#B66-molecules-28-08154" class="html-bibr">66</a>]. Copyright Royal Society of Chemistry, 2022; (<b>c</b>) structure–performance relationship of Ba<sub>1−x</sub>Sr<sub>x</sub>SnO<sub>3</sub>, reprinted with permission from ref. [<a href="#B72-molecules-28-08154" class="html-bibr">72</a>]. Copyright Wiley VCH GmbH, 2023; (<b>d</b>) doping effect of Cu<sup>2+</sup> on SrSnO<sub>3</sub> perovskite oxides, reprinted with permission from ref. [<a href="#B67-molecules-28-08154" class="html-bibr">67</a>]. Copyright Wiley VCH GmbH, 2022.</p>
Full article ">Figure 4
<p>(<b>a</b>) FE (CO) and (<b>b</b>) FE (formate) over Sn<sub>x</sub>Zn<sub>y</sub>O<sub>z</sub> catalysts; Different coordination numbers (CN) calculated based on in-situ extended X-ray absorption fine structure (EXAFS) results for (<b>c</b>,<b>d</b>) Sn<sub>0.5</sub>Zn<sub>0.5</sub>O<sub>y</sub>, (<b>e</b>) ZnO<sub>y</sub>, and (<b>f</b>) SnO<sub>y</sub>, measured under electrochemical CO<sub>2</sub>RR at potentials of open circuit voltage, 0.8, 0.9, 1.0, and 1.1 V. vs. RHE, reprinted with permission from ref. [<a href="#B73-molecules-28-08154" class="html-bibr">73</a>]. Copyright Elsevier Ltd., 2022.</p>
Full article ">Figure 5
<p>The transmission electron microscope (TEM) images of (<b>a</b>) Cs<sub>3</sub>Bi<sub>2</sub>Br<sub>9</sub> NCs and (<b>b</b>) Cs<sub>3</sub>Bi<sub>2</sub>Br<sub>9</sub>/Carbon black composite, reprinted with permission from ref. [<a href="#B78-molecules-28-08154" class="html-bibr">78</a>]. Copyright Wiley VCH GmbH, 2022; TEM images of (<b>c</b>) CsPbI<sub>3</sub> NCs and (<b>d</b>) CsPbI<sub>3</sub>/rGO composite, reprinted with permission from ref [<a href="#B79-molecules-28-08154" class="html-bibr">79</a>]. Copyright Springer Ltd., 2023, red arrows and yellow arrows in (<b>b</b>,<b>d</b>) point to perovskite nanocubes and carbon materials, respectively; (<b>e</b>) the structural evolution of BaBiO<sub>3</sub> perovskite during CO<sub>2</sub>RR, reprinted with permission from ref. [<a href="#B76-molecules-28-08154" class="html-bibr">76</a>]. Copyright Elsevier Ltd., 2022; (<b>f</b>) the conversion of Cs<sub>3</sub>Bi<sub>2</sub>I<sub>9</sub> nanocrystals to bismuth with I<sup>−</sup> and Cs<sup>+</sup> dual modification, reprinted with permission from ref [<a href="#B75-molecules-28-08154" class="html-bibr">75</a>]. Copyright Wiley VCH GmbH, 2023.</p>
Full article ">Figure 6
<p>(<b>a</b>) XRD patterns of La<sub>1.8</sub>Sr<sub>0.2</sub>O<sub>4</sub> before and after CO<sub>2</sub>RR, reprinted with permission from ref. [<a href="#B93-molecules-28-08154" class="html-bibr">93</a>]. Copyright The Electrochemical Society Inc, 1993; (<b>b</b>) La<sub>2-x</sub>Sr<sub>x</sub>CuO<sub>4</sub> synthesized by Mignard et al., reprinted with permission from ref. [<a href="#B95-molecules-28-08154" class="html-bibr">95</a>]. Copyright Elsevier Ltd., 2014; (<b>c</b>) illustration of crystal structure properties of L<sub>2</sub>C, L<sub>1.9</sub>C, L<sub>1.8</sub>C, and L<sub>1.7</sub>C, reprinted with permission from ref. [<a href="#B96-molecules-28-08154" class="html-bibr">96</a>]. Copyright Wiley VCH GmbH, 2021.</p>
Full article ">Figure 7
<p>(<b>a</b>) Illustration of electrospinning approach to prepare La<sub>2</sub>CuO<sub>4</sub> NBs, reprinted with permission from ref. [<a href="#B69-molecules-28-08154" class="html-bibr">69</a>]. Copyright ACS Publications, 2021; (<b>b</b>) the high-resolution transmission electron microscope (HRTEM) images of grain boundaries in La<sub>2</sub>CuO<sub>4</sub> with different micro-morphologies, reprinted with permission from ref. [<a href="#B69-molecules-28-08154" class="html-bibr">69</a>]. Copyright ACS Publications, 2021; (<b>c</b>) schematic illustrations of microstructure evolutions during the LSTr-Cu formation, reprinted with permission from ref. [<a href="#B100-molecules-28-08154" class="html-bibr">100</a>]. Copyright Wiley VCH GmbH, 2022; (<b>d</b>) the SMSIs for the LSTr-Cu catalyst, reprinted with permission from ref. [<a href="#B100-molecules-28-08154" class="html-bibr">100</a>]. Copyright Wiley VCH GmbH, 2022.</p>
Full article ">
16 pages, 4824 KiB  
Review
Chiral Metal Halide Perovskites: Focus on Lead-Free Materials and Structure-Property Correlations
by Clarissa Coccia, Marco Moroni and Lorenzo Malavasi
Molecules 2023, 28(16), 6166; https://doi.org/10.3390/molecules28166166 - 21 Aug 2023
Cited by 4 | Viewed by 3111
Abstract
Hybrid organic–inorganic perovskites (HOIPs) are promising materials in several fields related to electronics, offering long carrier-diffusion lengths, high absorption coefficients, tunable band gaps, and long spin lifetimes. Recently, chiral perovskites have attracted huge interest thanks to the possibility of further widening the applications [...] Read more.
Hybrid organic–inorganic perovskites (HOIPs) are promising materials in several fields related to electronics, offering long carrier-diffusion lengths, high absorption coefficients, tunable band gaps, and long spin lifetimes. Recently, chiral perovskites have attracted huge interest thanks to the possibility of further widening the applications of HOIPs. Chiral materials, being intrinsically non-centrosymmetric, display several attractive physicochemical properties, including circular dichroism, circularly polarized photoluminescence, nonlinear optics, ferroelectricity, and spin-related effects. Recent studies have shown that chirality can be transferred from the chiral organic ligands into the inorganic perovskite framework, resulting in materials combining the advantages of both chirality and perovskite superior optoelectronic characteristics. As for HOIPs for photovoltaics, strong interest is currently devoted towards the development of lead-free chiral perovskites to overcome any toxicity issue. While considering the basic and general features of chiral HOIPs, this review mainly focuses on lead-free materials. It highlights the first attempts to understand the correlation between the crystal structure characteristics and the chirality-induced functional properties in lead and lead-free chiral perovskites. Full article
(This article belongs to the Special Issue Exclusive Feature Papers in Inorganic Chemistry, 2nd Edition)
Show Figures

Figure 1

Figure 1
<p>Structure of Chiral Perovskites: (<b>a</b>) 1D structure; (<b>b</b>) 2D structure; (<b>c</b>) 3D structure. Reprinted with permission from Ref. [<a href="#B4-molecules-28-06166" class="html-bibr">4</a>]. 2021, Wiley.</p>
Full article ">Figure 2
<p>(<b>a</b>) Structure of (<span class="html-italic">R</span>-MPEA)<sub>2</sub>SnBr<sub>6</sub>; (<b>b</b>) SHG measurement; (<b>c</b>) UV-Vis and (<b>d</b>) CD spectra. Reprinted with permission from Ref. [<a href="#B17-molecules-28-06166" class="html-bibr">17</a>]. 2021, Wiley.</p>
Full article ">Figure 3
<p>(<b>a</b>) Structure of (<span class="html-italic">R/rac</span>-MBA)<sub>4</sub>Bi<sub>2</sub>I<sub>10</sub>; (<b>b</b>) UV-Vis spectra; (<b>c</b>) CD spectra. Reprinted with permission from Ref. [<a href="#B18-molecules-28-06166" class="html-bibr">18</a>]. 2022, American Chemical Society.</p>
Full article ">Figure 4
<p>(<b>a</b>) Structure of (<span class="html-italic">R/S</span>-MBA)<sub>4</sub>Bi<sub>2</sub>Br<sub>10</sub>; (<b>b</b>) UV-Vis and CD spectra of (<span class="html-italic">R/S</span>-MBA)<sub>4</sub>Bi<sub>2</sub>Br<sub>10</sub>; (<b>c</b>) UV-Vis and CD spectra of <span class="html-italic">R/S</span>-MPA)<sub>2</sub>BiBr<sub>5</sub>. Reprinted with permission from Ref. [<a href="#B19-molecules-28-06166" class="html-bibr">19</a>]. 2023, Wiley.</p>
Full article ">Figure 5
<p>Structure of [R-β-MPA]<sub>4</sub>AgBiI<sub>8</sub> where BiI<sub>6</sub> octahedra, purple; AgI<sub>6</sub> octahedra, blue. Reprinted with permission from Ref. [<a href="#B20-molecules-28-06166" class="html-bibr">20</a>]. 2021, Wiley.</p>
Full article ">Figure 6
<p>(<b>a</b>) CD spectra; (<b>b</b>) UV-Vis spectra. Reprinted with permission from Ref. [<a href="#B20-molecules-28-06166" class="html-bibr">20</a>]. 2021, Wiley.</p>
Full article ">Figure 7
<p>(<b>a</b>–<b>f</b>) Evolution of ferroelastic domains under the variation of temperature for [<span class="html-italic">R</span>-EQ]PbI<sub>3</sub> with the scale bar of 100 μm. Reprinted with permission from Ref. [<a href="#B21-molecules-28-06166" class="html-bibr">21</a>]. 2022, American Chemical Society.</p>
Full article ">Figure 8
<p>Structure of (<span class="html-italic">R/S</span>-MBA)<sub>2</sub>PbI<sub>4</sub>. Reprinted with permission from Ref. [<a href="#B23-molecules-28-06166" class="html-bibr">23</a>]. 2019, American Chemical Society.</p>
Full article ">Figure 9
<p>Normalized absorption (<b>a</b>) and steady-state PL spectra (<b>b</b>) of (<span class="html-italic">R</span>-MBA)<sub>2</sub>PbI<sub>4</sub>, (<span class="html-italic">S</span>-MBA)<sub>2</sub>PbI<sub>4</sub>, and (<span class="html-italic">rac</span>-MBA)<sub>2</sub>PbI<sub>4</sub> microplates obtained by mechanical exfoliation. (<b>c</b>) CD spectra of (<span class="html-italic">R</span>-, <span class="html-italic">S</span>-, and <span class="html-italic">rac</span>-MBA)<sub>2</sub>PbI<sub>4</sub> films. Reprinted with permission from Ref. [<a href="#B23-molecules-28-06166" class="html-bibr">23</a>]. 2019, American Chemical Society.</p>
Full article ">Figure 10
<p>(<b>a</b>) Structure of [(R)-1-(4-F)PEA]<sub>4</sub>[Sb<sub>2</sub>Cl<sub>10</sub>]; (<b>b</b>) UV-Vis spectra of all compounds. Reprinted with permission from Ref. [<a href="#B24-molecules-28-06166" class="html-bibr">24</a>]. 2020, American Chemical Society.</p>
Full article ">Figure 11
<p>Structure of compounds (<span class="html-italic">R/S/rac</span>-MBA)<sub>2</sub>SnI<sub>4</sub> [<a href="#B25-molecules-28-06166" class="html-bibr">25</a>]. Reprinted with permission from Ref. [<a href="#B25-molecules-28-06166" class="html-bibr">25</a>]. 2020, American Chemical Society.</p>
Full article ">Figure 12
<p>(<b>a</b>) CD spectra of (<span class="html-italic">R/S/rac</span>-MBA)<sub>2</sub>SnI<sub>4</sub>; (<b>b</b>) CD spectra of (<span class="html-italic">R/S/rac</span>-MBA)<sub>2</sub>Pb<sub>1−X</sub>Sn<sub>x</sub>I<sub>4</sub>. Reprinted with permission from Ref. [<a href="#B25-molecules-28-06166" class="html-bibr">25</a>]. 2020, American Chemical Society.</p>
Full article ">Figure 13
<p>UV–vis–NIR absorption spectra (<b>a</b>) and CD spectra (<b>b</b>) of (<span class="html-italic">R</span>-MPEA)<sub>2</sub>CuCl<sub>4</sub>, (<span class="html-italic">S</span>-MPEA)<sub>2</sub>CuCl<sub>4</sub>, and (<span class="html-italic">rac</span>-MPEA)<sub>2</sub>CuCl<sub>4</sub>. Reprinted with permission from Ref. [<a href="#B26-molecules-28-06166" class="html-bibr">26</a>]. 2020, American Chemical Society.</p>
Full article ">Figure 14
<p>CD spectra of the <span class="html-italic">R</span>- (blue), <span class="html-italic">S</span>- (red), and <span class="html-italic">rac</span>- (black) fabricated HOIPs films including (MBA)<sub>2</sub>PbI<sub>4</sub>, (FMBA)<sub>2</sub>PbI<sub>4</sub>, (ClMBA)<sub>2</sub>PbI<sub>4</sub> (BrMBA)<sub>2</sub>PbI<sub>4</sub>, and (IMBA)<sub>2</sub>PbI<sub>4</sub> series. Reprinted with permission from Ref. [<a href="#B28-molecules-28-06166" class="html-bibr">28</a>]. 2021, Wiley.</p>
Full article ">
Back to TopTop