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Nanomaterials, Volume 9, Issue 11 (November 2019) – 139 articles

Cover Story (view full-size image): The Surface-Enhanced Raman Spectroscopy (SERS) immunoassay consists in bioconjugates of gold nanostars (AuNSs) functionalised with 4-mercaptobenzoic acid as a Raman reporter, and polyclonal anti-horseradish peroxidase antibodies as the detection moiety. Agarose gel electrophoresis is instrumental in determining an effective functionalisation of the AuNSs by the Raman reporter, further conjugation with antibodies and to mimic the final SERS sandwich immunoassay. The optimised SERS-active bioconjugates allowed effective SERS detection down to 0.01 nM of bioconjugates, corresponding to an antigen peroxidase activity of 50 µU. Our results are a proof-of-concept for a SERS-based immunoassay with easy adaptation to alternative antibody–antigen pairs. View this paper.
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14 pages, 3886 KiB  
Article
Synthesis of Au@Pt Core—Shell Nanoparticles as Efficient Electrocatalyst for Methanol Electro-Oxidation
by América Higareda, Siva Kumar-Krishnan, Amado F. García-Ruiz, José Maya-Cornejo, José L. Lopez-Miranda, Daniel Bahena, Gerardo Rosas, Ramiro Pérez and Rodrigo Esparza
Nanomaterials 2019, 9(11), 1644; https://doi.org/10.3390/nano9111644 - 19 Nov 2019
Cited by 24 | Viewed by 6671
Abstract
Bimetallic Au@Pt nanoparticles (NPs) with Pt monolayer shell are of much interest for applications in heterogeneous catalysts because of enhanced catalytic activity and very low Pt-utilization. However, precisely controlled synthesis with uniform Pt-monolayers and stability on the AuNPs seeds remain elusive. Herein, we [...] Read more.
Bimetallic Au@Pt nanoparticles (NPs) with Pt monolayer shell are of much interest for applications in heterogeneous catalysts because of enhanced catalytic activity and very low Pt-utilization. However, precisely controlled synthesis with uniform Pt-monolayers and stability on the AuNPs seeds remain elusive. Herein, we report the controlled deposition of Pt-monolayer onto uniform AuNPs seeds to obtain Au@Pt core–shell NPs and their Pt-coverage dependent electrocatalytic activity for methanol electro-oxidation. The atomic ratio between Au/Pt was effectively tuned by varying the precursor solution ratio in the reaction solution. The morphology and atomic structure of the Au@Pt NPs were analyzed by high-resolution scanning transmission electron microcopy (HR-STEM) and X-ray diffraction (XRD) techniques. The results demonstrated that the Au@Pt core–shell NPs with Pt-shell thickness (atomic ratio 1:2) exhibit higher electrocatalytic activity for methanol electro-oxidation reaction, whereas higher and lower Pt ratios showed less overall catalytic performance. Such higher catalytic performance of Au@Pt NPs (1:2) can be attributed to the weakened CO binding on the Pt/monolayers surface. Our present synthesis strategy and optimization of the catalytic activity of Au@Pt core–shell NPs catalysts provide promising approach to rationally design highly active catalysts with less Pt-usage for high performance electrocatalysts for applications in fuel cells. Full article
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Figure 1
<p>(<b>a</b>) UV–vis absorption spectra and (<b>b</b>) fourth-derivative absorption spectra of the obtained Au, Pt and Au@Pt NPs with different nominal compositions. The inset in <a href="#nanomaterials-09-01644-f001" class="html-fig">Figure 1</a>a shows a photograph of the corresponding samples.</p>
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<p>(<b>a</b>) XRD patterns of Au@Pt NPs with (1:1), (1:2), and (1:3) composition;(<b>b</b>) (111) reflections of Au and Pt structures; and (<b>c</b>) elemental composition of Au and Pt.</p>
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<p>BF-STEM images, size distribution histograms and EDS spectrum of Au@Pt NPs supported on carbon black Vulcan XC-72R with different nominal atomic compositions: (<b>a</b>) (1:1), (<b>b</b>) (1:2), and (<b>c</b>) (1:3).</p>
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<p>High-resolution HAADF-STEM images with their FFT of (<b>a</b>) AuNPs and(<b>b</b>) Au@Pt (1:3) NPs, and SAED patterns of (<b>c</b>) AuNPs and (<b>d</b>) AuPt (1:3) NPs.</p>
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<p>(<b>a</b>) HAADF-STEM image, (<b>b</b>) EDS line-scan profile of Au@Pt (1:1) NPs, (<b>c</b>) HAADF-STEM image, (<b>d</b>) EDS line-scan profile, and (<b>e</b>) EDS elemental mappings of Au@Pt (1:3) NPs. Green represents Au component and red represents Pt component.</p>
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<p>Voltammograms (CVs) of carbon supported Au@Pt/C NPs catalysts with different nominal compositions and Pt/C commercial in a 0.3 M aqueous solution of KOH at a scan rate of 50 mVs<sup>−1</sup>.</p>
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<p>CV profiles of the catalysts for methanol oxidation reaction. CV curves for (<b>a</b>) Au@Pt/C NPs with different nominal compositions and (<b>b</b>) commercial Pt/C electrocatalysts and Au@Pt/C (1:2) NPs in 0.3 M KOH + 1 M MeOH mixed solution at a sweep rate of 20 mVs<sup>−1</sup>.</p>
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15 pages, 3577 KiB  
Article
Enhanced Visible-Light Photocatalytic Activity of Ag QDs Anchored on CeO2 Nanosheets with a Carbon Coating
by Xiaogang Zheng, Qian Chen, Sihao Lv, Xiaojin Fu, Jing Wen and Xinhui Liu
Nanomaterials 2019, 9(11), 1643; https://doi.org/10.3390/nano9111643 - 19 Nov 2019
Cited by 29 | Viewed by 3874
Abstract
Ag quantum dots (QDs) anchored on CeO2 nanosheets with a carbon coating (Ag/CeO2@C) (composites) were prepared via an in situ reduction approach for the photocatalytic degradation of Cr(VI) and tetracycline hydrochloride (TCH) in the visible-light region. The photocatalytic activity of [...] Read more.
Ag quantum dots (QDs) anchored on CeO2 nanosheets with a carbon coating (Ag/CeO2@C) (composites) were prepared via an in situ reduction approach for the photocatalytic degradation of Cr(VI) and tetracycline hydrochloride (TCH) in the visible-light region. The photocatalytic activity of Ag/CeO2@C was greatly affected by carbon content, Ag-doping content, Cr(VI) concentration, pH value, and inorganic ions. Enhanced photocatalytic activity was obtained by Ag/CeO2@C (compared to CeO2 and CeO2@C), of which 3-Ag/CeO2@C-2 with an Ag-doping content of 5.41% presented the best removal efficiency and the most superior stability after five cycles. ·O2 and ·OH radicals were crucial for the photocatalytic capacity of 3-Ag/CeO2@C-2. The combined effect of the surface plasma resonance (SPR) of Ag QDs, an electron trapper of carbon shells, and the redox activity of the Ce(III)/Ce(IV) coupling induced efficient charge transfer and separation, suppressing the recombination of electron–hole pairs. Full article
(This article belongs to the Special Issue Photocatalytic Nanomaterials)
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<p>XRD patterns of CeO<sub>2</sub>@C-2 and Ag/CeO<sub>2</sub>@C-2.</p>
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<p>Ce 3d (<b>A</b>), O 1s (<b>B</b>), C 1s (<b>C</b>), and Ag 3d (<b>D</b>) X-ray photoelectron spectroscopy (XPS) spectra of fresh and used 3-Ag/CeO<sub>2</sub>@C-2.</p>
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<p>SEM images (<b>A</b>,<b>B</b>), TEM images (<b>C</b>,<b>D</b>), high-resolution TEM (HRTEM) images (<b>E</b>,<b>F</b>), and elemental mapping images (<b>G</b>–<b>J</b>) of 3-Ag/CeO<sub>2</sub>@C-2.</p>
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<p>UV–Vis spectra of CeO<sub>2</sub>, CeO<sub>2</sub>@C-2, and 3-Ag/CeO<sub>2</sub>@C-2.</p>
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<p>Photoluminescence (PL) spectra of CeO<sub>2</sub>, CeO<sub>2</sub>@C-2, and 3-Ag/CeO<sub>2</sub>@C-2.</p>
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<p>Photocurrent–time response (<b>A</b>) and electrochemical impedance spectroscopy (EIS) Nyquist plots (<b>B</b>) of 3-Ag/CeO<sub>2</sub>@C-2.</p>
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<p>Effect of Ag content on the photocatalytic activity of CeO<sub>2</sub>@C-2 (<b>A</b>) and the effects of Cr(VI) concentration (<b>B</b>), pH value (<b>C</b>), and inorganic ions (<b>D</b>) on the photocatalytic activity of 3-Ag/CeO<sub>2</sub>@C-2.</p>
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<p>Photocatalytic stability of 3-Ag/CeO<sub>2</sub>@C-2 in Cr(VI) removal in the visible-light region.</p>
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<p>Electron spin resonance (ESR) spectra of 3-Ag/CeO<sub>2</sub>@C-2 for DMPO–·O<sub>2</sub><sup>−</sup> in methanol (<b>A</b>) and DMPO–·OH in aqueous (<b>B</b>).</p>
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<p>Photocatalytic mechanism of 3-Ag/CeO<sub>2</sub>@C-2.</p>
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10 pages, 1545 KiB  
Communication
Methane-Mediated Vapor Transport Growth of Monolayer WSe2 Crystals
by Hyeon-Sik Jang, Jae-Young Lim, Seog-Gyun Kang, Sang-Hwa Hyun, Sana Sandhu, Seok-Kyun Son, Jae-Hyun Lee and Dongmok Whang
Nanomaterials 2019, 9(11), 1642; https://doi.org/10.3390/nano9111642 - 19 Nov 2019
Cited by 5 | Viewed by 4743
Abstract
The electrical and optical properties of semiconducting transition metal dichalcogenides (TMDs) can be tuned by controlling their composition and the number of layers they have. Among various TMDs, the monolayer WSe2 has a direct bandgap of 1.65 eV and exhibits p-type or [...] Read more.
The electrical and optical properties of semiconducting transition metal dichalcogenides (TMDs) can be tuned by controlling their composition and the number of layers they have. Among various TMDs, the monolayer WSe2 has a direct bandgap of 1.65 eV and exhibits p-type or bipolar behavior, depending on the type of contact metal. Despite these promising properties, a lack of efficient large-area production methods for high-quality, uniform WSe2 hinders its practical device applications. Various methods have been investigated for the synthesis of large-area monolayer WSe2, but the difficulty of precisely controlling solid-state TMD precursors (WO3, MoO3, Se, and S powders) is a major obstacle to the synthesis of uniform TMD layers. In this work, we outline our success in growing large-area, high-quality, monolayered WSe2 by utilizing methane (CH4) gas with precisely controlled pressure as a promoter. When compared to the catalytic growth of monolayered WSe2 without a gas-phase promoter, the catalytic growth of the monolayered WSe2 with a CH4 promoter reduced the nucleation density to 1/1000 and increased the grain size of monolayer WSe2 up to 100 ?m. The significant improvement in the optical properties of the resulting WSe2 indicates that CH4 is a suitable candidate as a promoter for the synthesis of TMD materials, because it allows accurate gas control. Full article
(This article belongs to the Section Nanocomposite Materials)
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<p>The schematic illustration of methane-mediated WSe<sub>2</sub> synthesis. (<b>a</b>) Sketch of homemade tube-type chemical vapor deposition (CVD) setup. (<b>b</b>) Schematic image of WSe<sub>2</sub> crystal growth by vapor-solid transport mechanism and its growth morphology difference between (<b>c</b>) without and (<b>d</b>) with methane (CH<sub>4</sub>) gas.</p>
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<p>Size control of the WSe<sub>2</sub> domain by tuning the methane carrier gas ratio. Typical SEM images of WSe<sub>2</sub> grains synthesized on a SiO<sub>2</sub>/Si substrate with a flow of (<b>a</b>) CH<sub>4</sub>:Ar = 0:200, (<b>b</b>) CH<sub>4</sub>:Ar = 50:150, (<b>c</b>) CH<sub>4</sub>:Ar = 100:100, and (<b>d</b>) CH<sub>4</sub>:Ar = 150:50 sccm. (<b>e</b>) Edge length (black) and nucleation density (blue) of WSe<sub>2</sub> domains as a function of the CH<sub>4</sub> gas ratio. The error bars represent the edge length variations of WSe<sub>2</sub> domains obtained at the same CH<sub>4</sub> gas flow.</p>
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<p>Raman and photoluminescence (PL) investigation of the synthesized WSe<sub>2</sub> according to the catalytic effects of methane. Raman mapping results of (<b>a</b>) CH<sub>4</sub>:Ar = 150:50 sccm, (<b>b</b>) Ar gas only as carrier gas, and (<b>c</b>) representative Raman spectrum of each mapping result. PL mapping results of (<b>d</b>) CH<sub>4</sub>:Ar = 150:50 sccm, (<b>e</b>) Ar gas only as carrier gas, And (<b>f</b>) representative PL spectrum of each mapping result. Raman and PL results were obtained from a micro-Raman instrument with a wavelength of 532 nm laser. Inset is an OM image corresponding to each mapping region.</p>
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<p>(<b>a</b>) Atomice force microscopy (AFM) image of the synthesized monolayer WSe<sub>2</sub>. The inset graph is the height profile corresponding to the blue dot line. (<b>b</b>) Surface potential mapping image of WSe<sub>2</sub> by Kelvin probe force microscopy (KPFM). The inset graph is the surface potential profile corresponding to the white dot line. X-ray photoelectron spectroscopy (XPS) analysis of (<b>c</b>) W-4f and (<b>d</b>) Se-3d of synthesized WSe<sub>2</sub>.</p>
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13 pages, 4057 KiB  
Article
Antireflection Enhancement by Composite Nanoporous Zeolite 3A–Carbon Thin Film
by Maksym Stetsenko, Salvatore A. Pullano, Tetiana Margitych, Lidia Maksimenko, Ali Hassan, Serhii Kryvyi, Rui Hu, Chun Huang, Roman Ziniuk, Sergii Golovynskyi, Ivan Babichuk, Βaikui Li, Junle Qu and Antonino S. Fiorillo
Nanomaterials 2019, 9(11), 1641; https://doi.org/10.3390/nano9111641 - 19 Nov 2019
Cited by 15 | Viewed by 3771
Abstract
A straightforward and effective spin-coating technique at 120 °C was investigated for the deposition of a thin nanoporous layer with antireflection properties onto glass and indium tin oxide (ITO) coated glass. A mixture of zeolite 3A powder and high iodine value vegetable oil [...] Read more.
A straightforward and effective spin-coating technique at 120 °C was investigated for the deposition of a thin nanoporous layer with antireflection properties onto glass and indium tin oxide (ITO) coated glass. A mixture of zeolite 3A powder and high iodine value vegetable oil was deposited, creating a carbonic paste with embedded nanoporous grains. Experimental results evidenced excellent broadband antireflection over the visible-near-infrared wavelength range (450–850 nm), with a diffuse reflectance value of 1.67% and 1.79%. Structural and optical characteristics stabilized over time. The results are promising for the accessible and cost-effective fabrication of an antireflective surface for optoelectronic devices. Full article
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<p>(<b>a</b>) Stages of the zeolite 3A deposition onto substrates. SEM surface morphologies for the samples deposited on (<b>b</b>) glass (scale bar 50 μm) and (<b>c</b>) ITO/glass (scale bar 10 μm).</p>
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<p>XRD patterns of (<b>a</b>) the ITO/glass, (<b>b</b>) zeolite/glass, and (<b>c</b>) zeolite/ITO/glass samples along with (<b>d</b>) an SEM cross-section of the zeolite/glass.</p>
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<p>Raman spectra of the zeolite 3A—carbon layers (<span class="html-italic">λ<sub>Ex</sub></span> = 532.5 nm): (<b>a</b>) laser power of 45 mW, (<b>b</b>) laser power—15 mW.</p>
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<p>Spectra of (<b>a</b>) specular and diffuse reflectance and (<b>b</b>) extinction for the glass, nanofilms ITO, zeolite/glass, and zeolite/ITO/glass.</p>
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<p>Polarization spectral characteristics of the zeolite 3A–carbon coatings: (<b>a</b>) amplitude and (<b>b</b>) phase anisotropy.</p>
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<p>Excitation–emission two-dimensional plots for the zeolite 3A–carbon layers on glass and ITO/glass.</p>
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<p>Fluorescence microscopy images of the zeolite/glass and zeolite/ITO/glass under blue (<b>a</b>), green (<b>b</b>) and UV excitations (<b>c</b>,<b>d</b>). The images (<b>a</b>–<b>c</b>) were obtained through the band-pass filters of different wavelengths; the images (<b>d</b>) were captured within visible range (scale bar—100μm).</p>
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<p>Fluorescence decays of (<b>a</b>) the zeolite/glass and (<b>b</b>) zeolite/ITO/glass (<span class="html-italic">λ<sub>Ex</sub></span> = 370 nm, <span class="html-italic">λ<sub>Em</sub></span> = 470 nm).</p>
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9 pages, 1268 KiB  
Article
Direct Observation of Monolayer MoS2 Prepared by CVD Using In-Situ Differential Reflectance Spectroscopy
by Yina Wang, Lei Zhang, Chenhui Su, Hang Xiao, Shanshan Lv, Faye Zhang, Qingmei Sui, Lei Jia and Mingshun Jiang
Nanomaterials 2019, 9(11), 1640; https://doi.org/10.3390/nano9111640 - 19 Nov 2019
Cited by 22 | Viewed by 5286
Abstract
The in-situ observation is of great significance to the study of the growth mechanism and controllability of two-dimensional transition metal dichalcogenides (TMDCs). Here, the differential reflectance spectroscopy (DRS) was performed to monitor the growth of molybdenum disulfide (MoS2) on a SiO [...] Read more.
The in-situ observation is of great significance to the study of the growth mechanism and controllability of two-dimensional transition metal dichalcogenides (TMDCs). Here, the differential reflectance spectroscopy (DRS) was performed to monitor the growth of molybdenum disulfide (MoS2) on a SiO2/Si substrate prepared by chemical vapor deposition (CVD). A home-built in-situ DRS setup was applied to monitor the growth of MoS2 in-situ. The formation and evolution of monolayer MoS2 are revealed by differential reflectance (DR) spectra. The morphology, vibration mode, absorption characteristics and thickness of monolayer MoS2 have been confirmed by optical microscopy, Raman spectroscopy, ex-situ DR spectra, and atomic force microscopy (AFM) respectively. The results demonstrated that DRS was a powerful tool for in-situ observations and has great potential for growth mechanism and controllability of TMDCs prepared by CVD. To the best of the authors’ knowledge, it was the first report in which the CVD growth of two-dimensional TMDCs has been investigated in-situ by reflectance spectroscopy. Full article
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<p>Scheme of the in-situ experiment device.</p>
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<p>(<b>a</b>) Optical images of MoS<sub>2</sub> thin films (front) and independent triangular crystals (back) on two different regions of the same SiO<sub>2</sub>/Si substrate; (<b>b</b>) Raman spectra of MoS<sub>2</sub> films and independent triangular crystals; (<b>c</b>) Ex-situ differential reflectance spectroscopy (DRS) obtained on an optical platform at room temperature; (<b>d</b>) The height profile of MoS<sub>2</sub>. The inset shows an atomic force microscopy (AFM) image. The black solid line is the measurement route of a probe. The darker region is the area without MoS<sub>2</sub>, which marked with white dashed lines.</p>
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<p>(<b>a</b>) The temperature curves of temperature-zone І (black line) and ІІ (red line) during the chemical vapor deposition (CVD) growth, respectively. The preparation process is divided into the stage І, stage ІІ, and stage ІІІ. (<b>b</b>) In-situ differential reflectance (DR) spectra recorded in the stage ІІ during CVD preparation of monolayer MoS<sub>2</sub> on a SiO<sub>2</sub>/Si substrate. The time interval between successive spectra is 120 s. The black arrow indicates the direction of spectral change at 1.83 eV. (<b>c</b>) In-situ DR spectra recorded in the stage ІІІ. The temperature interval is 40 °C and the temperature range is 730–50 °C. The black arrow indicates the direction of temperature reduction. (<b>d</b>) The increment of DR spectra during the stage ІІІ. (<b>e</b>) The intensities of DR signals at 1.83 eV and 1.99 eV as a function of time, respectively.</p>
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8 pages, 3032 KiB  
Article
Influence of Annealing Temperature on Weak-Cavity Top-Emission Red Quantum Dot Light Emitting Diode
by Chun-Yu Lee, Ya-Pei Kuo, Peng-Yu Chen, Hsieh-Hsing Lu and Ming Yi Lin
Nanomaterials 2019, 9(11), 1639; https://doi.org/10.3390/nano9111639 - 19 Nov 2019
Cited by 14 | Viewed by 4441
Abstract
In this report, we show that the annealing temperature in QDs/Mg-doped ZnO film plays a very important role in determining QLEDs performance. Measurements of capacitance and single carrier device reveal that the change of the device efficiency with different annealing temperatures is related [...] Read more.
In this report, we show that the annealing temperature in QDs/Mg-doped ZnO film plays a very important role in determining QLEDs performance. Measurements of capacitance and single carrier device reveal that the change of the device efficiency with different annealing temperatures is related to the balance of both electron and hole injection. A comparison of annealing temperatures shows that the best performance is demonstrated with 150 °C-annealing temperature. With the improved charge injection and charge balance, a maximum current efficiency of 24.81 cd/A and external quantum efficiency (EQE) of 20.09% are achievable in our red top-emission QLEDs with weak microcavity structure. Full article
(This article belongs to the Special Issue Quantum Dots and Micro-LED Display)
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<p>(<b>a</b>) Schematic of the device structure. (<b>b</b>) Optical transmittance of the IZO/glass substrate. (<b>c</b>) Energy band diagram of the red top-emission QLEDs. The inset is a photograph of the working device.</p>
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<p>Cross-sectional transmission electron microscopy image of the red top-emission QLEDs.</p>
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<p>Device performance of the red top-emission QLEDs at different anneal temperatures. (<b>a</b>) Current density–voltage (J–V) characteristics. (<b>b</b>) Luminance–current density (L–J) characteristics. (<b>c</b>) Current efficiency-luminance characteristics. (<b>d</b>) EQE-luminance characteristics. (<b>e</b>) Normalized EL spectra. (<b>f</b>) CIEx-luminance characteristics.</p>
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<p>The capacitance–voltage characteristics of the red top-emission QLEDs at different anneal temperatures.</p>
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<p>Current density–voltage (J–V) characteristics of (<b>a</b>) electron-only devices and (<b>b</b>) hole-only devices at different anneal temperatures.</p>
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10 pages, 3311 KiB  
Article
V3S4 Nanosheets Anchored on N, S Co-Doped Graphene with Pseudocapacitive Effect for Fast and Durable Lithium Storage
by Naiteng Wu, Di Miao, Xinliang Zhou, Lilei Zhang, Guilong Liu, Donglei Guo and Xianming Liu
Nanomaterials 2019, 9(11), 1638; https://doi.org/10.3390/nano9111638 - 18 Nov 2019
Cited by 22 | Viewed by 3671
Abstract
Construction of a suitable hybrid structure has been considered an important approach to address the defects of metal sulfide anode materials. V3S4 nanosheets anchored on an N, S co-coped graphene (VS/NSG) aerogel were successfully fabricated by an efficient self-assembled strategy. [...] Read more.
Construction of a suitable hybrid structure has been considered an important approach to address the defects of metal sulfide anode materials. V3S4 nanosheets anchored on an N, S co-coped graphene (VS/NSG) aerogel were successfully fabricated by an efficient self-assembled strategy. During the heat treatment process, decomposition, sulfuration and N, S co-doping occurred. This hybrid structure was not only endowed with an enhanced capability to buffer the volume expansion, but also improved electron conductivity as a result of the conductive network that had been constructed. The dominating pseudocapacitive contribution (57.78% at 1 mV s−1) enhanced the electrochemical performance effectively. When serving as anode material for lithium ion batteries, VS/NSG exhibits excellent lithium storage properties, including high rate capacity (480 and 330 mAh g−1 at 5 and 10 A g−1, respectively) and stable cyclic performance (692 mAh g−1 after 400 cycles at 2 A g−1). Full article
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<p>(<b>a</b>) Schematic illustration of preparation process of VS/NSG; (<b>b</b>) XRD pattern of as-prepared VS/NSG; (<b>c</b>) the structure of V<sub>3</sub>S<sub>4</sub> along the c-axis.</p>
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<p>(<b>a</b>,<b>b</b>) SEM images of as-prepared VS/NSG at different magnifications; (<b>c</b>,<b>d</b>) TEM image, HRTEM image, and FFT patterns in the marked white box of VS/NSG.</p>
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<p>XPS survey (<b>a</b>) V 2p, (<b>b</b>) S 2p, (<b>c</b>) N 1s, and (<b>d</b>) C 1s of as-prepared VS/NSG.</p>
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<p>(<b>a</b>) The initial discharge–charge curves of VS/NSG at 0.05 A g<sup>−1</sup>; (<b>b</b>) CV curves of VS/NSG at a scan rate of 0.1 mV s<sup>−1</sup>; and (<b>c</b>) the cyclic stability and (<b>d</b>) rate capability of VS/NSG electrode.</p>
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<p>Kinetic analyses of VS/NSG electrode. (<b>a</b>) CV curves at different scanning rates; (<b>b</b>) log(<span class="html-italic">i</span>) vs. log (<span class="html-italic">v</span>) plots at different peaks; (<b>c</b>) capacitive contribution (blue region) to the charge storage at 1 mV s<sup>−1</sup>; (<b>d</b>) the contribution ratio of pseudocapacitive and diffusion-controlled current at different scanning rates.</p>
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13 pages, 3716 KiB  
Article
DOPO-Functionalized Molybdenum Disulfide and its Impact on the Thermal Properties of Polyethylene and Poly(Lactic Acid) Composites
by Karolina Wenelska, Piotr Homa, Stefan Popovic, Klaudia Maslana and Ewa Mijowska
Nanomaterials 2019, 9(11), 1637; https://doi.org/10.3390/nano9111637 - 18 Nov 2019
Cited by 7 | Viewed by 2708
Abstract
The fabrication of conventional or biodegradable polymers with improved thermal and fire-resistant properties is an important task for their successful application in various branches of the industry. In this work, few-layered molybdenum disulfide was functionalized with 9,10-dihydro-9-oxa-10-phosphaphenanthrene-10-oxide and introduced into polyethylene and poly(lactic [...] Read more.
The fabrication of conventional or biodegradable polymers with improved thermal and fire-resistant properties is an important task for their successful application in various branches of the industry. In this work, few-layered molybdenum disulfide was functionalized with 9,10-dihydro-9-oxa-10-phosphaphenanthrene-10-oxide and introduced into polyethylene and poly(lactic acid) matrixes. The obtained polyethylene composite samples displayed improved thermal stability, significant reduction in CO emissions, improved fire-resistant properties, and over 100% increases in thermal conductivity. Poly(lactic acid) composites displayed less impressive results, but have managed to improve some values, such as CO emissions, peak heat release rate, and total heat release in comparison to pristine polymer. Full article
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<p>Transmission electron microscopy (TEM) (<b>A</b>) and atomic force microscopy (AFM) (<b>B</b>) images, along with AFM height profiles (<b>C</b>) of few-layered MoS<sub>2.</sub></p>
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<p>Raman spectroscopy of bulk and few-layered MoS<sub>2</sub>.</p>
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<p>TEM images of MoS<sub>2</sub>/Ni<sub>2</sub>O<sub>3</sub> nanoparticles (<b>A</b>–<b>C</b>).</p>
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<p>TEM (<b>A–C</b>) and SEM (<b>D</b>–<b>F</b>) images of MoS<sub>2</sub>/Ni<sub>2</sub>O<sub>3</sub>/DOPO nanoparticles.</p>
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<p>TGA curves of PE (<b>A</b>) and PLA (<b>B</b>) composites compared to pristine polymers.</p>
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<p>CO emissions of PE and PLA composites compared to pristine polymers.</p>
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<p>Examples of heat release rate (HRR) curves obtained for PE (<b>A</b>) and PLA (<b>B</b>) composites compared to pristine polymers.</p>
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10 pages, 2603 KiB  
Article
One-Step Hydrothermal Synthesis of P25 @ Few Layered MoS2 Nanosheets toward Enhanced Bi-catalytic Activities: Photocatalysis and Electrocatalysis
by Fang Zhou, Zhiguang Zhang, Zhihua Wang, Yajing Wang, Liping Xu, Qiang Wang and Wenjun Liu
Nanomaterials 2019, 9(11), 1636; https://doi.org/10.3390/nano9111636 - 18 Nov 2019
Cited by 8 | Viewed by 3123
Abstract
P25 loaded few layered molybdenum disulfide (MoS2) nanosheets (P25@MoS2) are successfully synthesized through a facile one-step hydrothermal process. The bi-catalytic activities, i.e., photocatalytic and electrocatalytic activities, of the as-prepared nanomaterials have been investigated. For the as-prepared products, the photocatalytic [...] Read more.
P25 loaded few layered molybdenum disulfide (MoS2) nanosheets (P25@MoS2) are successfully synthesized through a facile one-step hydrothermal process. The bi-catalytic activities, i.e., photocatalytic and electrocatalytic activities, of the as-prepared nanomaterials have been investigated. For the as-prepared products, the photocatalytic performances were investigated by degrading simulated pollutant under sunlight irradiation, and the hydrogen evolution reaction evaluated the electrocatalytic performances. The results indicate that P25@MoS2 possesses excellent activities in both photocatalysis and electrocatalysis. The presence of MoS2 broadens the light absorption range of P25 and improves the separation and transformation efficiency of photogenerated carriers, thus improving its photocatalytic performance. The existence of P25 inhibits the aggregation of MoS2 to form more dispersed MoS2 nanosheets with only few layers increasing its active sites. Thereby, the electrocatalytic performance is heightened. The excellent multifunction makes the as-prepared P25@MoS2 a promising material in the fields of environment and energy. Full article
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<p>X-ray diffraction (XRD) patterns of pure P25, PM21, PM11, PM12, and molybdenum disulfide (MoS<sub>2</sub>).</p>
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<p>(<b>a</b>) Field emission scanning electron microscopy (FESEM) image of pure MoS<sub>2</sub>. (<b>b</b>) Low and (<b>c</b>) high magnification FESEM images of PM11 respectively. (<b>d</b>) Transmission electron microscope (TEM) image of PM11. (<b>e</b>,<b>f</b>) High resolution transmission electron microscope (HRTEM) images of PM11 corresponding to the selected areas in (d).</p>
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<p>High-resolution X-ray photoelectron spectra (XPS) spectra of PM11: (<b>a</b>) Ti 2p, (<b>b</b>) O 1s, (<b>c</b>) Mo 3d, and (<b>d</b>) S 2p.</p>
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<p>(<b>a</b>) UV-Vis diffuse reflectance spectra and (<b>b</b>) PL spectra of P25, MoS<sub>2</sub>, PM21, PM11, and PM12.</p>
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<p>(<b>a</b>) The curves of C/C<sub>0</sub> vs. time for photodegrading rhodamine B (RhB). (<b>b</b>) The degradation efficiency in recycling of PM11.</p>
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<p>(<b>a</b>) Polarization curves and (<b>b</b>) corresponding Tafel plots.</p>
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12 pages, 5522 KiB  
Article
Synthesis of Mn0.5Zn0.5SmxEuxFe1.8?2xO4 Nanoparticles via the Hydrothermal Approach Induced Anti-Cancer and Anti-Bacterial Activities
by Sultan Akhtar, Suriya Rehman, Munirah A. Almessiere, Firdos Alam Khan, Yassine Slimani and Abdulhadi Baykal
Nanomaterials 2019, 9(11), 1635; https://doi.org/10.3390/nano9111635 - 18 Nov 2019
Cited by 64 | Viewed by 4224
Abstract
Manganese metallic nanoparticles are attractive materials for various biological and medical applications. In the present study, we synthesized unique Mn0.5Zn0.5SmxEuxFe1.8−2xO4 (0.01 ≤ x ≤ 0.05) nanoparticles (NPs) by using the hydrothermal approach. [...] Read more.
Manganese metallic nanoparticles are attractive materials for various biological and medical applications. In the present study, we synthesized unique Mn0.5Zn0.5SmxEuxFe1.8−2xO4 (0.01 ≤ x ≤ 0.05) nanoparticles (NPs) by using the hydrothermal approach. The structure and surface morphology of the products were determined by X-ray powder diffraction (XRD), transmission electron and scanning electron microcopies (TEM and SEM), along with energy dispersive X-ray spectroscopy (EDX). We evaluated the impact of Mn0.5Zn0.5SmxEuxFe1.8−2xO4 NPs on both human embryonic stem cells (HEK-293) (normal cells) and human colon carcinoma cells (HCT-116) (cancerous cells). We found that post-48 h of treatment of all products showed a significant decline in the cancer cell population as revealed by microscopically and the (3-(4,5-dimethylthiazol-2-yl)-2,5-diphenyltetrazolium bromide) tetrazolium (MTT) assay. The inhibitory concentration (IC50) values of the products ranged between 0.75 and 2.25 µg/mL. When tested on normal and healthy cells (HEK-293), we found that the treatment of products did not produce any effects on the normal cells, which suggests that all products selectively targeted the cancerous cells. The anti-bacterial properties of the samples were also evaluated by Minimum Inhibitory Concentration (MIC) and Minimum Bactericidal Concentration (MBC) assays, which showed that products also inhibited the bacterial growth. Full article
(This article belongs to the Special Issue Functional Nanomagnetics and Magneto-Optical Nanomaterials)
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<p>XRD powder patterns of Mn<sub>0.5</sub>Zn<sub>0.5</sub>Eu<sub>x</sub>Sm<sub>x</sub>Fe<sub>1.5−2x</sub>O<sub>4</sub> (0.01 ≤ x ≤ 0.05) NPs.</p>
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<p>SEM of Mn<sub>0.5</sub>Zn<sub>0.5</sub>Eu<sub>x</sub>Sm<sub>x</sub>Fe<sub>1.5−2x</sub>O<sub>4</sub> for x = 0.01, 0.03, and 0.05 and EDX x = 0.03 NPs.</p>
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<p>TEM of Mn<sub>0.5</sub>Zn<sub>0.5</sub>Eu<sub>x</sub>Sm<sub>x</sub>Fe<sub>1.5−2x</sub>O<sub>4</sub> (x = 0.03 and 0.05) NPs.</p>
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<p>Cancer cells stained with <b>4′,6-diamidino-2-phenylindole</b> (DAPI). HCT-116 cells treated with Mn<sub>0.5</sub>Zn<sub>0.5</sub>Sm<sub>x</sub>Eu<sub>x</sub>Fe<sub>1.8−2x</sub>O<sub>4</sub> (0.01 ≤ x ≤ 0.05) NPs for 48 h. (<b>A</b>) is control without treatment, (<b>B</b>) treated with Mn<sub>0.5</sub>Zn<sub>0.5</sub>Sm<sub>x</sub>Eu<sub>x</sub>Fe<sub>1.8−2x</sub>O<sub>4</sub> NPs for x = 0.01 concentration (2.35 µg/mL), and (<b>C</b>) treated with Mn<sub>0.5</sub>Zn<sub>0.5</sub>Sm<sub>x</sub>Eu<sub>x</sub>Fe<sub>1.8−2x</sub>O<sub>4</sub> NPs for x = 0.05 concentration (2.33 µg/mL). Arrows in B and C indicate the loss of nuclear staining. 200× magnifications.</p>
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<p>MIC/MBC of Mn<sub>0.5</sub>Zn<sub>0.5</sub>Sm<sub>x</sub>Eu<sub>x</sub>Fe<sub>1.8−2x</sub>O<sub>4</sub> (0.01 ≤ x ≤ 0.05) against (<b>A</b>) <span class="html-italic">E. coli</span> (<b>B</b>) <span class="html-italic">S. aureus.</span></p>
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<p>SEM micrographs of Mn<sub>0.5</sub>Zn<sub>0.5</sub>Sm<sub>x</sub>Eu<sub>x</sub>Fe<sub>1.8−2x</sub>O<sub>4</sub> (0.01 ≤ x ≤ 0.05) NPs treated <b>(I)</b> <span class="html-italic">E. coli</span>, <b>(II)</b> <span class="html-italic">S. aureus.</span> (<b>a</b>) untreated cells (control), (<b>b</b>) x = 0.01, (<b>c</b>) 0.02, (<b>d</b>) 0.03, (<b>e</b>) 0.04, and (<b>f</b>) 0.05.</p>
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12 pages, 4014 KiB  
Article
Reveal the Deformation Mechanism of (110) Silicon from Cryogenic Temperature to Elevated Temperature by Molecular Dynamics Simulation
by Jing Han, Yuanming Song, Wei Tang, Cong Wang, Liang Fang, Hua Zhu, Jiyun Zhao and Jiapeng Sun
Nanomaterials 2019, 9(11), 1632; https://doi.org/10.3390/nano9111632 - 18 Nov 2019
Cited by 12 | Viewed by 2954
Abstract
Silicon undergoes a brittle-to-ductile transition as its characteristic dimension reduces from macroscale to nanoscale. The thorough understanding of the plastic deformation mechanism of silicon at the nanoscale is still challenging, although it is essential for developing Si-based micro/nanoelectromechanical systems (MEMS/NEMS). Given the wide [...] Read more.
Silicon undergoes a brittle-to-ductile transition as its characteristic dimension reduces from macroscale to nanoscale. The thorough understanding of the plastic deformation mechanism of silicon at the nanoscale is still challenging, although it is essential for developing Si-based micro/nanoelectromechanical systems (MEMS/NEMS). Given the wide application of silicon in extreme conditions, it is, therefore, highly desirable to reveal the nanomechanical behavior of silicon from cryogenic temperature to elevated temperature. In this paper, large-scale molecular dynamics (MD) simulations were performed to reveal the spherical nanoindentation response and plastic deformation mechanism of (110)Si at the temperature range of 0.5 K to 573 K. Special attention was paid to the effect of temperature. Multiple pop-ins detected in load/pressure-indentation strain curves are impacted by temperature. Four featured structures induced by nanoindentation, including high-pressure phases, extrusion of α-Si, dislocations, and crack, are observed at all temperatures, consistent with experiment results. The detailed structure evolution of silicon was revealed at the atomic scale and its dependence on temperature was analyzed. Furthermore, structure changes were correlated with pop-ins in load/pressure-indentation strain curves. These results may advance our understanding of the mechanical properties of silicon. Full article
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<p>Molecular dynamics model.</p>
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<p>(<b>a</b>) <span class="html-italic">L</span>-<span class="html-italic">ε</span> curves, (<b>b</b>) <span class="html-italic">P<sub>m</sub></span>-<span class="html-italic">ε</span> curve, and (<b>c</b>) indentation modulus under nanoindentation of Si(110) at different temperatures, where <span class="html-italic">L</span> is load, <span class="html-italic">ε</span> is indentation strain, <span class="html-italic">P<sub>m</sub></span> is mean contact pressure, PI is pop-in.</p>
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<p>The indentation strain and contact pressure for (<b>a</b>) PI-A, (<b>b</b>) PI-B, (<b>c</b>) PI-C, and (<b>d</b>) PI-D depending on temperature.</p>
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<p>The longitudinal section view of phase distribution induced by nanoindentation on (110)Si near the PI-A and PI-B (as shown in <a href="#nanomaterials-09-01632-f002" class="html-fig">Figure 2</a>c) at the temperature of (<b>a</b>) 0.5 K, (<b>b</b>) 300 K, and (<b>c</b>) 573 K. The atoms are color-coded by MCN. The dark blue, lawn green, and yellow atoms are Si-II, bct5, and surface atoms, respectively.</p>
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<p>The longitudinal section and cross-section view of phase distribution induced by nanoindentation on (110)Si near the PI-C at the temperature of (<b>a</b>) 0.5 K, (<b>b</b>) 300 K, and (<b>c</b>) 573 K. The atoms are color-coded by MCN. The dark blue, lawn green, and yellow atoms are Si-II, bct5, and surface atoms, respectively.</p>
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<p>The longitudinal section view of phase distribution induced by nanoindentation on (110)Si near the PI-D at the temperature of (<b>a</b>) 0.5 K, (<b>b</b>) 300 K, and (<b>c</b>) 573 K. The atoms are color-coded by MCN. The dark blue, lawn green, and yellow atoms are Si-II, bct5, and surface atoms, respectively.</p>
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<p>The longitudinal section view of phase distribution induced by nanoindentation on (110)Si near the PI-E at 573 K. The atoms are color-coded by MCN. The dark blue, lawn green, and yellow atoms are Si-II, bct5, and surface atoms, respectively.</p>
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<p>The development of dislocations at (<b>a</b>) 0.5 K, (<b>b</b>) 300 K, and (<b>c</b>) 573 K. The atoms are colored by SV.</p>
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<p>The microstructure morphology of (110)Si at (<b>a</b>) 0.5 K at <span class="html-italic">ε</span> = 0.197, (<b>b</b>) 300 K at <span class="html-italic">ε</span> = 0.196, and (<b>c</b>) 573 K at <span class="html-italic">ε</span> = 0.197. The atoms are color-coded by MCN. The dark blue, lawn green, and yellow atoms are Si-II, bct5, and surface atoms, respectively.</p>
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14 pages, 8387 KiB  
Article
Heteroepitaxial Growth of High-Quality and Crack-Free AlN Film on Sapphire Substrate with Nanometer-Scale-Thick AlN Nucleation Layer for AlGaN-Based Deep Ultraviolet Light-Emitting Diodes
by Jie Zhao, Hongpo Hu, Yu Lei, Hui Wan, Liyan Gong and Shengjun Zhou
Nanomaterials 2019, 9(11), 1634; https://doi.org/10.3390/nano9111634 - 17 Nov 2019
Cited by 15 | Viewed by 4162
Abstract
High-quality and crack-free aluminum nitride (AlN) film on sapphire substrate is the foundation for high-efficiency aluminum gallium nitride (AlGaN)-based deep ultraviolet light-emitting diodes (DUV LEDs). We reported the growth of high-quality and crack-free AlN film on sapphire substrate with a nanometer-scale-thick AlN nucleation [...] Read more.
High-quality and crack-free aluminum nitride (AlN) film on sapphire substrate is the foundation for high-efficiency aluminum gallium nitride (AlGaN)-based deep ultraviolet light-emitting diodes (DUV LEDs). We reported the growth of high-quality and crack-free AlN film on sapphire substrate with a nanometer-scale-thick AlN nucleation layer (NL). Three kinds of nanometer-scale-thick AlN NLs, including in situ low-temperature AlN (LT-AlN) NL, oxygen-undoped ex situ sputtered AlN NL, and oxygen-doped ex situ sputtered AlN NL, were prepared for epitaxial growth of AlN films on sapphire substrates. The influence of nanoscale AlN NL thickness on the optical transmittance, strain state, surface morphology, and threading dislocation (TD) density of the grown AlN film on sapphire substrate were carefully investigated. The average optical transmittance of AlN film on sapphire substrate with oxygen-doped sputtered AlN NL was higher than that of AlN films on sapphire substrates with LT-AlN NL and oxygen-undoped sputtered AlN NL in the 200–270 nm wavelength region. However, the AlN film on sapphire substrate with oxygen-undoped sputtered AlN NL had the lowest TD density among AlN films on sapphire substrates. The AlN film on sapphire substrate with the optimum thickness of sputtered AlN NL showed weak tensile stress, a crack-free surface, and low TD density. Furthermore, a 270-nm AlGaN-based DUV LED was grown on the high-quality and crack-free AlN film. We believe that our results offer a promising and practical route for obtaining high-quality and crack-free AlN film for DUV LED. Full article
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<p>(<b>a</b>) Schematic illustration of aluminum nitride (AlN) film on sapphire substrate. (<b>b</b>) Cross-sectional scanning electron microscopy (SEM) image of AlN film on sapphire substrate with an AlN nucleation layer (NL). (<b>c</b>) Photograph of the 2-in. AlN film on sapphire substrate showing a crack-free surface.</p>
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<p>(<b>a</b>) Optical transmittance spectra of Sample A1, Sample B1, and Sample C1. (<b>b</b>) SIMS depth profiles of oxygen in Sample C1.</p>
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<p>Normalized Raman spectra of E<sub>2</sub> (high) mode for Sample A1, Sample B1, and Sample C1.</p>
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<p>Plan-view optical differential interference contrast (DIC) images of (<b>a</b>) Sample A1, (<b>b</b>) Sample B1, and (<b>c</b>) Sample C1 conducted at the magnification of 1000 times.</p>
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<p>(<b>a</b>) Symmetric (002) and (<b>b</b>) asymmetric (102) ω-scan rocking curves of Sample A1, Sample B1, and Sample C1.</p>
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<p>Atomic force microscopy (AFM) images (5 × 5 μm<sup>2</sup>) of etching pits in (<b>a</b>) Sample A1, (<b>b</b>) Sample B1, and (<b>c</b>) Sample C1 after molten KOH etching at 185 °C for 10 min.</p>
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<p>Normalized Raman spectra of E<sub>2</sub> (high) mode for Sample B1, Sample B2, and Sample B3.</p>
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<p>Plan-view optical DIC images of (<b>a</b>) Sample B2, (<b>b</b>) Sample B1, and (<b>c</b>) Sample B3 conducted at the magnification of 1000 times.</p>
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<p>(<b>a</b>) Symmetric (002) and (<b>b</b>) asymmetric (102) ω-scan rocking curves with normalized peak intensity for Sample B1, Sample B2, and Sample B3.</p>
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<p>Normalized Raman spectra of the E<sub>2</sub> (high) mode for Sample C2, Sample C3, Sample C4, and Sample C5.</p>
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<p>Plan-view optical DIC images of (<b>a</b>) Sample C2, (<b>b</b>) Sample C3, (<b>c</b>) Sample C4, and (<b>d</b>) Sample C5 conducted at the magnification of 1000 times.</p>
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<p>(<b>a</b>) Symmetric (002) and (<b>b</b>) asymmetric (102) ω-scan rocking curves with normalized peak intensity for Sample C2, Sample C3, Sample C4, and Sample C5.</p>
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<p>(<b>a</b>) Schematic representation of the deep-ultraviolet light-emitting diode (DUV LED) structure. (<b>b</b>,<b>c</b>) Cross-sectional transmission electron microscopy (TEM) images of the DUV LED epitaxial structure. (<b>d</b>) Photoluminescence (PL) spectrum (T = 300 K) of the DUV LED. (<b>e</b>) Current versus voltage characteristic of DUV LED.</p>
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11 pages, 4613 KiB  
Article
The Growth of Graphene on Ni–Cu Alloy Thin Films at a Low Temperature and Its Carbon Diffusion Mechanism
by Yibo Dong, Sheng Guo, Huahai Mao, Chen Xu, Yiyang Xie, Chuantong Cheng, Xurui Mao, Jun Deng, Guanzhong Pan and Jie Sun
Nanomaterials 2019, 9(11), 1633; https://doi.org/10.3390/nano9111633 - 17 Nov 2019
Cited by 11 | Viewed by 3816
Abstract
Carbon solid solubility in metals is an important factor affecting uniform graphene growth by chemical vapor deposition (CVD) at high temperatures. At low temperatures, however, it was found that the carbon diffusion rate (CDR) on the metal catalyst surface has a greater impact [...] Read more.
Carbon solid solubility in metals is an important factor affecting uniform graphene growth by chemical vapor deposition (CVD) at high temperatures. At low temperatures, however, it was found that the carbon diffusion rate (CDR) on the metal catalyst surface has a greater impact on the number and uniformity of graphene layers compared with that of the carbon solid solubility. The CDR decreases rapidly with decreasing temperatures, resulting in inhomogeneous and multilayer graphene. In the present work, a Ni–Cu alloy sacrificial layer was used as the catalyst based on the following properties. Cu was selected to increase the CDR, while Ni was used to provide high catalytic activity. By plasma-enhanced CVD, graphene was grown on the surface of Ni–Cu alloy under low pressure using methane as the carbon source. The optimal composition of the Ni–Cu alloy, 1:2, was selected through experiments. In addition, the plasma power was optimized to improve the graphene quality. On the basis of the parameter optimization, together with our previously-reported, in-situ, sacrificial metal-layer etching technique, relatively homogeneous wafer-size patterned graphene was obtained directly on a 2-inch SiO2/Si substrate at a low temperature (~600 °C). Full article
(This article belongs to the Section Nanocomposite Materials)
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<p>(<b>a</b>)–(<b>e</b>) The Raman spectra and corresponding optical images of the graphene on SiO<sub>2</sub>/Si substrates catalyzed by Ni–Cu alloys with different compositions (Ni:Cu = 1:10 (<b>a</b>), 1:3 (<b>b</b>), 1:2 (<b>c</b>), 1:1 (<b>d</b>) and 2:1 (<b>e</b>), respectively).</p>
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<p>(<b>a</b>,<b>c</b>,<b>e</b>) The AFM, optical and SEM images of the graphene grown on the Ni1Cu3 alloy, respectively. (<b>b</b>,<b>d</b>,<b>f</b>) The AFM, optical and SEM images of the graphene grown on the Ni2Cu1 alloy, respectively. (<b>g</b>,<b>h</b>) The diffusion mechanism of carbon atoms on Cu and Ni surfaces, respectively.</p>
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<p>Theoretically determined tracer diffusivity (10<sup>-12</sup> m<sup>2</sup>/s) for (<b>a</b>) the bulk diffusion rate of carbon atoms in alloys with different Ni–Cu ratios at 600 °C. (<b>b</b>) The bulk diffusion rate of carbon atoms in alloys with different Ni–Cu ratios at 600 °C and 800 °C.</p>
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<p>(<b>a</b>) Raman spectra of the graphene grown with and without plasma at 600 °C. (<b>b</b>) Raman spectra of the graphene grown with different plasma powers. (<b>c</b>) The photograph of the growth chamber. (<b>d</b>) The photograph taken during the growth process.</p>
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<p>(<b>a</b>–<b>d</b>) Schematic illustration of the etching process of our in-situ, transfer-free growth method. (<b>a</b>) After the graphene growth, PMMA coating is spun on the sample surface. (<b>b</b>) When the sample is immersed in the metal etchant, the etchant can efficiently penetrate through the molecular gap of PMMA and the grain boundary of the graphene to achieve the metal etching. (<b>c</b>,<b>d</b>) After the metal is completely etched away, the PMMA/graphene films will fall on the substrate. (<b>e</b>,<b>f</b>) Wafer-level graphene growth. The photograph of the sample before (<b>e</b>) and after (<b>f</b>) the metal sacrificial layer etching. (<b>g</b>) An optical image of the graphene at 1000× magnification. (<b>h</b>,<b>i</b>) Raman mapping of the D/G and G/2D ratios of the graphene over 50 × 50 μm.</p>
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20 pages, 1506 KiB  
Review
Metal Oxide Nanoparticles in Therapeutic Regulation of Macrophage Functions
by Marina S. Dukhinova, Artur. Y. Prilepskii, Alexander A. Shtil and Vladimir V. Vinogradov
Nanomaterials 2019, 9(11), 1631; https://doi.org/10.3390/nano9111631 - 16 Nov 2019
Cited by 61 | Viewed by 8636
Abstract
Macrophages are components of the innate immune system that control a plethora of biological processes. Macrophages can be activated towards pro-inflammatory (M1) or anti-inflammatory (M2) phenotypes depending on the cue; however, polarization may be altered in bacterial and viral infections, cancer, or autoimmune [...] Read more.
Macrophages are components of the innate immune system that control a plethora of biological processes. Macrophages can be activated towards pro-inflammatory (M1) or anti-inflammatory (M2) phenotypes depending on the cue; however, polarization may be altered in bacterial and viral infections, cancer, or autoimmune diseases. Metal (zinc, iron, titanium, copper, etc.) oxide nanoparticles are widely used in therapeutic applications as drugs, nanocarriers, and diagnostic tools. Macrophages can recognize and engulf nanoparticles, while the influence of macrophage-nanoparticle interaction on cell polarization remains unclear. In this review, we summarize the molecular mechanisms that drive macrophage activation phenotypes and functions upon interaction with nanoparticles in an inflammatory microenvironment. The manifold effects of metal oxide nanoparticles on macrophages depend on the type of metal and the route of synthesis. While largely considered as drug transporters, metal oxide nanoparticles nevertheless have an immunotherapeutic potential, as they can evoke pro- or anti-inflammatory effects on macrophages and become essential for macrophage profiling in cancer, wound healing, infections, and autoimmunity. Full article
(This article belongs to the Special Issue Immune Responses to Nanomaterials for Biomedical Applications)
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<p>Macrophage polarization: M1 (classical, pro-inflammatory) and M2 (alternative, anti-inflammatory). M1 polarization can be triggered by lipopolysaccharides (LPS) and/or interferon gamma (INFγ). M1 macrophages express high CD80 and MHCII and produce pro-inflammatory cytokines to stimulate the innate and adaptive immune activity of monocytes, neutrophils, T- and B-lymphocytes. M2 cells are characterized by surface markers Ym1, CD206, and mannose receptor, as well as by cytokines that have a potential for immunosuppression and tissue regeneration. Tumor-associated macrophages develop an M2 phenotype and promote the immune escape of tumor cells.</p>
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<p>Systemic and local routes of NPs delivery and distribution. (<b>A</b>). At the systemic level, NPs can enter the organism with water/food/drug uptake or i.v. injections. Local contact with NPs occurs from skin contact, inhalation, and tumor therapy. Eventually, NPs are distributed throughout the organism in a cell free form or can be phagocytized. (<b>B</b>). When the phagocytized NPs are moving with the blood flow, they are accumulated in the heart. Air NPs primarily interact with alveolar MФs. Inhaled and injected NPs can penetrate the blood-brain barrier where they contact with microglia. The ultimate destinations of NPs are the liver and the spleen.</p>
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<p>Molecular mechanisms of pro- and anti-inflammatory effects of NPs on MФs. NPs interact with cell surface receptors and can enter the cells via endocytosis/pinocytosis. (<b>A</b>). Pro-inflammatory signaling of NPs activates Toll-like (TLRs), Fcγ, and SR-A1 and MARCO scavenger receptor pathways with involved downstream MAPK/mTOR cascades and transcription factors STATs, NFkB and IRFs. NPs stimulate cytokine production and release, inflammasome formation, and phagocytic activity, thereby prompting M1 polarization. The immunostimulatory effect of NPs re-shapes the immunosuppressive microenvironment and boosts up antimicrobial or anticancer immunity. (<b>B</b>). The anti-inflammatory activity of NPs is applied to M1 committed MФs, as in chronic inflammatory disorders, autoimmunity, and neurodegeneration. NPs activate transcription factor PPARγ and arginase 1 to inhibit pro-inflammatory NFκB, modulate Jak/STAT pathway, and limit inflammation.</p>
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15 pages, 4412 KiB  
Article
Fractal Silver Dendrites as 3D SERS Platform for Highly Sensitive Detection of Biomolecules in Hydration Conditions
by Maria José Lo Faro, Cristiano D’Andrea, Antonio Alessio Leonardi, Dario Morganti, Alessia Irrera and Barbara Fazio
Nanomaterials 2019, 9(11), 1630; https://doi.org/10.3390/nano9111630 - 16 Nov 2019
Cited by 33 | Viewed by 4852
Abstract
In this paper, we report on the realization of a highly sensitive and low cost 3D surface-enhanced Raman scattering (SERS) platform. The structural features of the Ag dendrite network that characterize the SERS material were exploited, attesting a remarked self-similarity and scale invariance [...] Read more.
In this paper, we report on the realization of a highly sensitive and low cost 3D surface-enhanced Raman scattering (SERS) platform. The structural features of the Ag dendrite network that characterize the SERS material were exploited, attesting a remarked self-similarity and scale invariance over a broad range of length scales that are typical of fractal systems. Additional structural and optical investigations confirmed the purity of the metal network, which was characterized by low oxygen contamination and by broad optical resonances introduced by the fractal behavior. The SERS performances of the 3D fractal Ag dendrites were tested for the detection of lysozyme as probe molecule, attesting an enhancement factor of ~2.4 × 106. Experimental results assessed the dendrite material as a suitable SERS detection platform for biomolecules investigations in hydration conditions. Full article
(This article belongs to the Special Issue Nanomaterials Based on IV-Group Semiconductors)
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<p>Ag dendrite synthesis. Schematic depicting the growth of Ag dendrites from (<b>a</b>) the dissolution of AgNO<sub>3</sub> salts in a HF/H<sub>2</sub>O solvent, leading to the formation of Ag nanoparticles that subsequently precipitate onto the Si bulk. (<b>b</b>) Ag dendrites were developed by further incorporating the Ag<sup>+</sup> ions onto the initial seeds. (<b>c</b>) Cross-section SEM microscopy of the produced carpet of Ag dendrites onto the Si bulk.</p>
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<p>Fractal Ag dendrites: Schematic and plan view scanning electron microscopies of Ag dendrites acquired at three different magnification scales of (<b>a</b>–<b>c</b>) in order to test the scale invariance of the fractal.</p>
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<p>Compositional characterization. Energy dispersive X-ray spectroscopy (EDX) compositional maps of the (<b>b</b>) Si (in green), (<b>c</b>) Ag (in blue) and (<b>d</b>) O (in red) X-ray signals in comparison to (<b>a</b>) the SEM cross-section of stored Ag dendrites. (<b>e</b>) The EDX elemental profiles acquired for Si, Ag and O X-ray emission lines along the green line reported in (<b>a</b>) are also shown.</p>
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<p>Ag plasmon resonance. Apparent absorbance spectra of the Ag reference film [<a href="#B55-nanomaterials-09-01630" class="html-bibr">55</a>,<a href="#B56-nanomaterials-09-01630" class="html-bibr">56</a>] (red spectrum) and Ag fractal dendrites (blue spectrum) obtained from the reflectance spectra carried out with an integrating sphere.</p>
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<p>Surface-enhanced Raman scattering (SERS) performance of Ag dendrites. (<b>a</b>) Comparison between the Raman spectra of the lysozyme dry powder (red line), the pure phosphate buffer saline (PBS) solution (dark yellow line), and lysozyme in the PBS solution at 10 mM (black line). Notice that for these latter two spectra performed onto liquid samples, we used glass microcells as holders. (<b>b</b>) shows the Raman spectrum acquired on the bare Ag dendrites, while the blue spectrum in (<b>c</b>) shows the SERS response of 10<sup>−5</sup> M of lysozyme onto the Ag dendrite platform. For all the spectra, we used the same 100× microscope objective with an integration time of 30 s. We used a laser power of 4.5 mW for the Raman spectra in (<b>a</b>,<b>b</b>) and 45 μW in the spectrum shown in (<b>c</b>).</p>
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<p>SERS signal from lysozyme target protein (Lyz) hydration region. (<b>a</b>) SERS spectra of lysozyme (10<sup>−5</sup> M) measured on three different samples, as representative for the ensemble of measurements, presented in the low and high frequency regions. (<b>b</b>) Enhancement factors measured on the three spectra reported in (<b>a</b>) for the phenylalanine (Phe) peaks at 1006 and 1031 cm<sup>−1</sup>. The magenta line and dashed rectangle indicate the enhancement factors (EFs) calculated average value. For all the SERS spectra in (<b>a</b>), we used the same 100× microscope objective with an integration time of 30 s and a laser power of 45 μW.</p>
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<p>SERS signal from lysozyme target protein (Lyz) hydration region. (<b>a</b>) SERS spectra of lysozyme (10<sup>−5</sup> M) measured on three different samples, as representative for the ensemble of measurements, presented in the low and high frequency regions. (<b>b</b>) Enhancement factors measured on the three spectra reported in (<b>a</b>) for the phenylalanine (Phe) peaks at 1006 and 1031 cm<sup>−1</sup>. The magenta line and dashed rectangle indicate the enhancement factors (EFs) calculated average value. For all the SERS spectra in (<b>a</b>), we used the same 100× microscope objective with an integration time of 30 s and a laser power of 45 μW.</p>
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<p>SERS signal from Lyz in the hydration region. Highlight of the SERS fingerprint of lysozyme onto Ag dendrites (in red) versus the lysozyme powder Raman spectrum (in black) in the water hydration region. For a better comparison, the spectra of the PBS solution drop casted onto the Ag dendrites (in blue), the water drop casted onto the Ag dendrites (in green), and liquid water are also presented (dark yellow). For all the spectra, we used the same 100× microscope objective with an integration time of 30 s, while we adopted a laser power of 4.5 mW for the Raman spectra and a laser power of 45 μW for the SERS one (red line in (<b>a</b>)). For the spectrum measured of the liquid sample (dark yellow line in (<b>b</b>)), we used glass microcells as sample holders.</p>
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21 pages, 547 KiB  
Review
Application of Polyphenol-Loaded Nanoparticles in Food Industry
by Danijel D. Milinčić, Dušanka A. Popović, Steva M. Lević, Aleksandar Ž. Kostić, Živoslav Lj. Tešić, Viktor A. Nedović and Mirjana B. Pešić
Nanomaterials 2019, 9(11), 1629; https://doi.org/10.3390/nano9111629 - 16 Nov 2019
Cited by 112 | Viewed by 8513
Abstract
Nanotechnology is an emerging field of science, and nanotechnological concepts have been intensively studied for potential applications in the food industry. Nanoparticles (with dimensions ranging from one to several hundred nanometers) have specific characteristics and better functionality, thanks to their size and other [...] Read more.
Nanotechnology is an emerging field of science, and nanotechnological concepts have been intensively studied for potential applications in the food industry. Nanoparticles (with dimensions ranging from one to several hundred nanometers) have specific characteristics and better functionality, thanks to their size and other physicochemical properties. Polyphenols are recognized as active compounds that have several putative beneficial properties, including antioxidant, antimicrobial, and anticancer activity. However, the use of polyphenols as functional food ingredients faces numerous challenges, such as their poor stability, solubility, and bioavailability. These difficulties could be solved relatively easily by the application of encapsulation. The objective of this review is to present the most recent accomplishments in the usage of polyphenol-loaded nanoparticles in food science. Nanoparticles loaded with polyphenols and their applications as active ingredients for improving physicochemical and functional properties of food, or as components of active packaging materials, were critically reviewed. Potential adverse effects of polyphenol-loaded nanomaterials are also discussed. Full article
(This article belongs to the Special Issue Nanotechnology in Agriculture and Food Industry)
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<p>Schematic view of use of nanomaterials in food science and technology (adapted from Ramachandraiah et al. [<a href="#B13-nanomaterials-09-01629" class="html-bibr">13</a>], with permission from publisher Asian-Australasian Journal of Animal Science, 2015).</p>
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13 pages, 4101 KiB  
Article
Effect of Heterointerface on NO2 Sensing Properties of In-Situ Formed TiO2 QDs-Decorated NiO Nanosheets
by Congyi Wu, Jian Zhang, Xiaoxia Wang, Changsheng Xie, Songxin Shi and Dawen Zeng
Nanomaterials 2019, 9(11), 1628; https://doi.org/10.3390/nano9111628 - 16 Nov 2019
Cited by 13 | Viewed by 3030
Abstract
In this work, TiO2 QDs-modified NiO nanosheets were employed to improve the room temperature NO2 sensing properties of NiO. The gas sensing studies showed that the response of nanocomposites with the optimal ratio to 60 ppm NO2 was nearly 10 [...] Read more.
In this work, TiO2 QDs-modified NiO nanosheets were employed to improve the room temperature NO2 sensing properties of NiO. The gas sensing studies showed that the response of nanocomposites with the optimal ratio to 60 ppm NO2 was nearly 10 times larger than that of bare NiO, exhibiting a potential application in gas sensing. Considering the commonly reported immature mechanism that the effective charge transfer between two phases contributes to an enhanced sensitivity, the QDs sensitization mechanism was further detailed by designing a series of contrast experiments. First, the important role of the QDs size effect was revealed by comparing the little enhanced sensitivity of TiO2 particle-modified NiO with the largely enhanced sensitivity of TiO2 QDs-NiO. Second, and more importantly, direct evidence of the heterointerface charge transfer efficiency was detailed by the extracted interface bond (Ti-O-Ni) using XPS peak fitting. This work can thus provide guidelines to design more QDs-modified nanocomposites with higher sensitivity for practical applications. Full article
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<p>(<b>a</b>) Dynamic sensitivity–recovery curves and (<b>b</b>) responses of the bare NiO nanosheets and the NiO nanosheets modified with different quantities of TiO<sub>2</sub> QDs to different concentrations of NO<sub>2</sub> at room temperature; (<b>c</b>) Responses of NiO nanosheets modified with different sizes of TiO<sub>2</sub> nanoparticle to 60 ppm NO<sub>2</sub> at room temperature.</p>
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<p>TEM images of (<b>a</b>) bare NiO nanosheets, and (<b>b</b>) bare TiO<sub>2</sub> QDs. Low- and high-magnification images of (<b>c</b>,<b>d</b>) TiO<sub>2</sub>QDs-NiO, (<b>e</b>) TiO<sub>2</sub>15-NiO, and (<b>f</b>) TiO<sub>2</sub>30-NiO.</p>
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<p>(<b>a</b>) The UPS spectra of TiO<sub>2</sub> QDs; (<b>b</b>) The XPS spectrum of TiO<sub>2</sub> QDs; (<b>c</b>) The plot of (αhυ)<sup>2</sup> against photon energy (hυ) for TiO<sub>2</sub> QDs; (<b>d</b>) The corresponding energy band structure of TiO<sub>2</sub> QDs based on the UPS, XPS, and UV-vis results.</p>
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<p>(<b>a</b>) Ni 2p spectra of the bare NiO and the TiO<sub>2</sub>QDs-NiO nanohybrids. (<b>b</b>) With the increase of the TiO<sub>2</sub> QDs content, a comparison between the variation of the responses to 60 ppm NO<sub>2</sub> and the variation of the binding energy shift values is shown. (<b>c</b>) Ni 2p spectra of the bare NiO and the 5TiO<sub>2</sub>QDs-NiO, 20TiO215-NiO, and 50TiO230-NiO. (<b>d</b>) With the increase of the TiO<sub>2</sub> nanoparticle size, a comparison between the variation of the maximum responses to 60 ppm NO<sub>2</sub> and the variation of the binding energy shift values is shown. (<b>e</b>) O 1s spectra of the 5TiO<sub>2</sub>QDs-NiO. (<b>f</b>) With the increase of the TiO<sub>2</sub> QDs content, a comparison between the variation of the responses to 60 ppm NO<sub>2</sub> and the variation of the peak area ratio of Ni-O-Ti is shown.</p>
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<p>(<b>a</b>) The energy band diagram of the as-prepared samples, before and after contact. (<b>b</b>) The schematic of the interfacial interaction between the TiO<sub>2</sub>-NiO<sub>2</sub> nanohybrids structure and NO<sub>2</sub> molecules. (<b>c</b>) Comparison of the surface band bending between NiO nanosheets, large TiO<sub>2</sub> nanoparticle-modified NiO nanosheets, and TiO<sub>2</sub> QDs-modified NiO nanosheets.</p>
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13 pages, 5054 KiB  
Article
Optimizing the Interface between Hole Transporting Material and Nanocomposite for Highly Efficient Perovskite Solar Cells
by Zeinab Safari, Mahmood Borhani Zarandi, Antonella Giuri, Francesco Bisconti, Sonia Carallo, Andrea Listorti, Carola Esposito Corcione, Mohamad Reza Nateghi, Aurora Rizzo and Silvia Colella
Nanomaterials 2019, 9(11), 1627; https://doi.org/10.3390/nano9111627 - 16 Nov 2019
Cited by 26 | Viewed by 6246
Abstract
The performances of organometallic halide perovskite-based solar cells severely depend on the device architecture and the interface between each layer included in the device stack. In particular, the interface between the charge transporting layer and the perovskite film is crucial, since it represents [...] Read more.
The performances of organometallic halide perovskite-based solar cells severely depend on the device architecture and the interface between each layer included in the device stack. In particular, the interface between the charge transporting layer and the perovskite film is crucial, since it represents both the substrate where the perovskite polycrystalline film grows, thus directly influencing the active layer morphology, and an important site for electrical charge extraction and/or recombination. Here, we focus on engineering the interface between a perovskite-polymer nanocomposite, recently developed by our group, and different commonly employed polymeric hole transporters, namely PEDOT: PSS [poly(3,4-ethylenedioxythiophene):poly(styrenesulfonate)], PEDOT, PTAA [poly(bis 4-phenyl}{2,4,6-trimethylphenyl}amine)], Poly-TPD [Poly(N,N′-bis(4-butylphenyl)-N,N′-bis(phenyl)-benzidine] Poly-TPD, in inverted planar perovskite solar cell architecture. The results show that when Poly-TPD is used as the hole transfer material, perovskite film morphology improved, suggesting an improvement in the interface between Poly-TPD and perovskite active layer. We additionally investigate the effect of the Molecular Weight (MW) of Poly-TPD on the performance of perovskite solar cells. By increasing the MW, the photovoltaic performances of the cells are enhanced, reaching power conversion efficiency as high as 16.3%. Full article
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<p>Water contact angle on PEDOT: PSS deposited on Glass/Indium Tin oxide (ITO) (<b>a</b>). Atomic Force Microcopy (AFM) images (5 × 5 nm) of Perovskite/starch film deposited on PEDOT: PSS film (Rq = 1.11 nm) (<b>b</b>). A Scanning Electron Microscopy (SEM) image of perovskite/starch deposited on PEDOT: PSS film (<b>c</b>).</p>
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<p>AFM images (5 × 5 μm) of Poly-TPD (Rq = 1.72 nm) (<b>a</b>), PEDOT (Rq = 3.10 nm) (<b>b</b>), and PTAA (Rq = 1.01 nm) (<b>c</b>).</p>
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<p>Water contact angle of the p-type polymer films of interest: Poly-TPD (<b>a</b>), PEDOT (<b>b</b>), and PTAA (<b>c</b>).</p>
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<p>Top view SEM images of perovskite/starch crystals grown on Poly-TPD (<b>a</b>), PEDOT (<b>b</b>), and PTAA (<b>c</b>).</p>
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<p>Structure of perovskite solar cells. (<b>a</b>) Device architecture and (<b>b</b>) energy-band diagram of the devices with PEDOT: PSS, PEDOT, Poly-TPD, and PTAA as the HTLs.</p>
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<p>Statistics of photovoltaic parameters, (<b>a</b>) fill factors (FF), (<b>b</b>) V<sub>oc</sub>, (<b>c</b>) J<sub>sc</sub>, and (<b>d</b>) power conversion efficiency (PCE) for different HTLs.</p>
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<p>Water contact angle of (<b>a</b>) Poly-TPD, (<b>b</b>) Treated Poly-TPD High Molecular weight (HMW), (<b>c</b>) Treated Poly-TPD with O<sub>2</sub> plasma, and (<b>d</b>) Treated Poly-TPD (HMW) with O<sub>2</sub> plasma.</p>
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<p>AFM images (5 × 5 μm) of the treated Poly-TPD (Rq = 1.79 nm) (<b>a</b>), the treated Poly-TPD (HMW) (Rq = 2.00 nm) (<b>b</b>), the treated Poly-TPD with Oxygen plasma (Rq = 1.72 nm) (<b>c</b>), and the treated Poly-TPD (HMW) with Oxygen plasma (Rq = 1.86 nm) (<b>d</b>).</p>
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<p>Current–voltage characteristics of champion devices based on perovskite/starch film deposited on the treated Poly-TPD (HMW) layer by UV-Ozone (UVO).</p>
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20 pages, 2963 KiB  
Article
Development of Superparamagnetic Nanoparticles Coated with Polyacrylic Acid and Aluminum Hydroxide as an Efficient Contrast Agent for Multimodal Imaging
by Manuel Antonio González-Gómez, Sarah Belderbos, Susana Yañez-Vilar, Yolanda Piñeiro, Frederik Cleeren, Guy Bormans, Christophe M. Deroose, Willy Gsell, Uwe Himmelreich and José Rivas
Nanomaterials 2019, 9(11), 1626; https://doi.org/10.3390/nano9111626 - 15 Nov 2019
Cited by 73 | Viewed by 5592
Abstract
Early diagnosis of disease and follow-up of therapy is of vital importance for appropriate patient management since it allows rapid treatment, thereby reducing mortality and improving health and quality of life with lower expenditure for health care systems. New approaches include nanomedicine-based diagnosis [...] Read more.
Early diagnosis of disease and follow-up of therapy is of vital importance for appropriate patient management since it allows rapid treatment, thereby reducing mortality and improving health and quality of life with lower expenditure for health care systems. New approaches include nanomedicine-based diagnosis combined with therapy. Nanoparticles (NPs), as contrast agents for in vivo diagnosis, have the advantage of combining several imaging agents that are visible using different modalities, thereby achieving high spatial resolution, high sensitivity, high specificity, morphological, and functional information. In this work, we present the development of aluminum hydroxide nanostructures embedded with polyacrylic acid (PAA) coated iron oxide superparamagnetic nanoparticles, Fe3O4@Al(OH)3, synthesized by a two-step co-precipitation and forced hydrolysis method, their physicochemical characterization and first biomedical studies as dual magnetic resonance imaging (MRI)/positron emission tomography (PET) contrast agents for cell imaging. The so-prepared NPs are size-controlled, with diameters below 250 nm, completely and homogeneously coated with an Al(OH)3 phase over the magnetite cores, superparamagnetic with high saturation magnetization value (Ms = 63 emu/g-Fe3O4), and porous at the surface with a chemical affinity for fluoride ion adsorption. The suitability as MRI and PET contrast agents was tested showing high transversal relaxivity (r2) (83.6 mM−1 s−1) and rapid uptake of 18F-labeled fluoride ions as a PET tracer. The loading stability with 18F-fluoride was tested in longitudinal experiments using water, buffer, and cell culture media. Even though the stability of the 18F-label varied, it remained stable under all conditions. A first in vivo experiment indicates the suitability of Fe3O4@Al(OH)3 nanoparticles as a dual contrast agent for sensitive short-term (PET) and high-resolution long-term imaging (MRI). Full article
(This article belongs to the Special Issue Frontiers in Nanomaterials for Clinical Imaging and Selective Therapy)
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<p>X-ray diffraction (XRD) pattern of the core/shell structure of magnetite/aluminum hydroxide nanoparticles, compared to the XRD pattern of magnetite from the JCPDS 19-0629 data base.</p>
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<p>Fourier transform infrared (FTIR) spectra of aluminum hydroxide nanoparticles (NPs), magnetite coated with polyacrylic acid NPs and polyacrylic acid magnetic nanoparticles coated with aluminum hydroxide.</p>
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<p>Magnetic hysteresis loop of a representative sample of Fe<sub>3</sub>O<sub>4</sub>@Al(OH)<sub>3</sub> NPs, normalized to the magnetite content and showing nearly superparamagnetic (SPM) behavior, with negligible values of coercivity and remanence.</p>
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<p>(<b>a</b>) Transmission electron microscopy (TEM) micrograph and (<b>b</b>) size distribution of the Fe<sub>3</sub>O<sub>4</sub>@PAA nanoparticles. The size distribution was performed by measuring a sample consisting of 486 magnetic nanoparticles with the ImageJ software.</p>
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<p>Scanning electron microscopy (SEM) (<b>a</b>) and TEM (<b>b</b>) micrographs of the Fe<sub>3</sub>O<sub>4</sub>@Al(OH)<sub>3</sub> NPs.</p>
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<p>(<b>a</b>) STEM micrograph and mapping with energy dispersive X-ray (EDX) emitted by the elements present in the Fe<sub>3</sub>O<sub>4</sub>@Al(OH)<sub>3</sub> samples: (<b>b</b>) oxygen, O (<b>c</b>) iron, Fe, (<b>d</b>) aluminum, Al, and (<b>e</b>) overlay of Fe (purple color) and Al (green colour) signal.</p>
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<p>Equilibrium isotherm of fluoride adsorption by Fe<sub>3</sub>O<sub>4</sub>@Al(OH)<sub>3</sub> NPs at 25 °C, pH 6.5.</p>
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<p>(<b>a</b>) STEM micrograph and mapping with EDX emitted by the elements present in the fluoride loaded Fe<sub>3</sub>O<sub>4</sub>@Al(OH)<sub>3</sub> samples: (<b>b</b>) fluoride, F (<b>c</b>) iron, Fe, and (<b>d</b>) aluminum, Al.</p>
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<p>Time course of the radiolabeling of Fe<sub>3</sub>O<sub>4</sub>@Al(OH)<sub>3</sub> NPs with [<sup>18</sup>F]F<sup>−</sup>. (<b>A</b>) Graphical representation of the percentage of [<sup>18</sup>F]F<sup>−</sup> bound to NPs containing 1.34 mg/mL iron after two, five or ten minutes of labeling with 5, 10, or 30 MBq [<sup>18</sup>F]NaF. No significant differences were found between the different conditions (two-way repeated-measures ANOVA, Bonferroni correction), (<b>B</b>) Representative autoradiography of iTLC of (left) NPs loaded with [<sup>18</sup>F]F<sup>−</sup> and (right) free [<sup>18</sup>F]NaF. The retardation factor (R<sub>f</sub>) of the labeled NPs indicates the complexation of the tracer to the NPs.</p>
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<p>PET/MRI contrast properties of Fe<sub>3</sub>O<sub>4</sub>@Al(OH)<sub>3</sub> NPs labeled with [<sup>18</sup>F]F<sup>-</sup> and mouse mesenchymal stem cells (mMSCs) labeled with such NPs: (<b>A</b>) Upper row: The different conditions measured with the estimated radioactivity present at the start of measurements. Samples (100 µL) were diluted ½ with agar. Middle: <sup>18</sup>F-positron emission tomography (PET) images and Bottom: T<sub>2</sub> maps of the agar phantoms loaded with either radiolabeled Fe<sub>3</sub>O<sub>4</sub>@Al(OH)<sub>3</sub> NPs (left) or mMSCs labeled with radiolabeled Fe<sub>3</sub>O<sub>4</sub>@Al(OH)<sub>3</sub> NPs (right). (<b>B</b>,<b>C</b>) Relaxation rate (R<sub>1</sub>/<sub>2</sub>/<sub>2</sub>*) plotted against (<b>B</b>) iron concentration (mM) of Fe<sub>3</sub>O<sub>4</sub>@Al(OH)<sub>3</sub> NPs or (<b>C</b>) intracellular iron concentration (mM) of mMSCs labeled with different amounts of radiolabeled Fe<sub>3</sub>O<sub>4</sub>@Al(OH)<sub>3</sub> NPs. The following cell densities were studied: 12,500, 25,000, and 50,000 cells in 200 µL: 62,500 cells/mL, 125,000 cells/mL, and 250,000 cells/mL, respectively. The intracellular iron concentrations were obtained for 50,000 labeled cells.</p>
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<p>(<b>A</b>) Cell viability relative to the unlabeled control MSC was determined 12 h after exposure to Fe<sub>3</sub>O<sub>4</sub>@Al(OH)<sub>3</sub> NPs post-labeling: A significant reduction in the cell survival was seen for concentrations &gt; 100 μg NP mL<sup>−1</sup>. (<b>B</b>) Population doubling times (PDT) were determined after exposure of MSC to NPs for 12 h and subsequent incubation in NP-free medium for two days (solid bares) and six days (striped bares). Significant differences with respect to PDTs were only seen for concentrations of 250 μg NP mL<sup>−1</sup> at two days after the removal of NPs from the medium. Three replicates were measured per condition. Differences relative to unlabeled cells were assessed based on a one-way ANOVA with Bonferroni correction. * <span class="html-italic">p</span> &lt; 0.05 and *** <span class="html-italic">p</span> &lt; 0.001.</p>
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24 pages, 6498 KiB  
Article
Polymer Membranes Sonocoated and Electrosprayed with Nano-Hydroxyapatite for Periodontal Tissues Regeneration
by Julia Higuchi, Giuseppino Fortunato, Bartosz Woźniak, Agnieszka Chodara, Sebastian Domaschke, Sylwia Męczyńska-Wielgosz, Marcin Kruszewski, Alex Dommann and Witold Łojkowski
Nanomaterials 2019, 9(11), 1625; https://doi.org/10.3390/nano9111625 - 15 Nov 2019
Cited by 40 | Viewed by 4721
Abstract
Diseases of periodontal tissues are a considerable clinical problem, connected with inflammatory processes and bone loss. The healing process often requires reconstruction of lost bone in the periodontal area. For that purpose, various membranes are used to prevent ingrowth of epithelium in the [...] Read more.
Diseases of periodontal tissues are a considerable clinical problem, connected with inflammatory processes and bone loss. The healing process often requires reconstruction of lost bone in the periodontal area. For that purpose, various membranes are used to prevent ingrowth of epithelium in the tissue defect and enhance bone regeneration. Currently-used membranes are mainly non-resorbable or are derived from animal tissues. Thus, there is an urgent need for non-animal-derived bioresorbable membranes with tuned resorption rates and porosity optimized for the circulation of body nutrients. We demonstrate membranes produced by the electrospinning of biodegradable polymers (PDLLA/PLGA) coated with nanohydroxyapatite (nHA). The nHA coating was made using two methods: sonocoating and electrospraying of nHA suspensions. In a simulated degradation study, for electrosprayed membranes, short-term calcium release was observed, followed by hydrolytic degradation. Sonocoating produced a well-adhering nHA layer with full coverage of the fibers. The layer slowed the polymer degradation and increased the membrane wettability. Due to gradual release of calcium ions the degradation-associated acidity of the polymer was neutralized. The sonocoated membranes exhibited good cellular metabolic activity responses against MG-63 and BJ cells. The collected results suggest their potential use in Guided Tissue Regeneration (GTR) and Guided Bone Regeneration (GBR) periodontal procedures. Full article
(This article belongs to the Special Issue Nanomaterials and Nanotechnology in Dentistry)
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<p>Electrospinning setup combined with electrospraying.</p>
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<p>Schematic view of ultrasonic coating setup and ultrasonic cavitation phenomenon occurring near the membrane surface during the process.</p>
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<p>SEM images of PLGA, PDLLA and PDLLA/PLGA samples top view (<b>A</b>–<b>C</b>) and fractured in liquid nitrogen cross-sections (<b>D</b>–<b>F</b>). For each material, fiber diameter histograms are given. Scale bar is 50 μm.</p>
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<p>SEM images and morphology scheme of PDLLA/PLGA membrane fibers: (<b>A</b>) Pristine PDLLA/PLGA fiber; (<b>B</b>) fiber electrospray covered with nHA beads; (<b>C</b>) fiber sonocoated with GoHAP 3; (<b>D</b>) fiber sonocoated with GoHAP 6; (<b>E</b>) fiber layer-by-layer sonocoated with GoHAP 6 and GoHAP 3, respectively.</p>
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<p>FTIR spectra of a: nHA, PDLLA, PDLLA/PLGA, and PDLLA/PLGA coated with nHA.</p>
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<p>XPS spectra of GoHAP 3 and 6 powders compared with natural bone apatite.</p>
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<p>XPS spectra of unmodified and nHA double-layer sonocoated materials: (<b>A</b>) PDLLA; (<b>B</b>) PDLLA/PLGA; and (<b>C</b>) PLGA.</p>
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<p>TG (<b>A</b>) and DTG (<b>B</b>) curves at heating rate b = 10 °C min<sup>−1</sup> of a PDLLA/PLGA (1), PDLLA/PLGA/nHA electrosprayed (2), PDLLA/PLGA/nHA sonocoated, and (3) and nHA (4).</p>
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<p>SEM images and water contact angle measurement values of materials and composites: (<b>A</b>–<b>C</b>) PLGA; (<b>D</b>–<b>F</b>) PDLLA; (<b>G</b>–<b>I</b>) PDLLA/PLGA.</p>
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<p>Graphs of ICP-OES calcium release and pH changes profiles, and SEM images of PDLLA/PLGA/nHA Electrosprayed fibers, (<b>A</b>–<b>H</b>) PDLLA/PLGA/nHA Sonocoated fibers (<b>I</b>–<b>P</b>), after 2,4,8,10 weeks of degradation (from the top down, respectively).</p>
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<p>Graph of molecular weight (Mw) changes in the function of degradation time.</p>
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<p>(<b>A</b>) Nominal strain-stress curve for coated and non-coated samples. All graphs show mean and standard deviation (shaded areas) from <span class="html-italic">n</span> = 3. SEM images of samples after tensile tests: (<b>B</b>) PDLLA/PLGA; (<b>C</b>) PDLLA/PLGA/nHA electrosprayed, and (<b>D</b>) PDLLA/PLGA/nHA sonocoated. Optical CCD camera images of (<b>E</b>) PDLLA/PLGA and (<b>F</b>) PDLLA/PLGA/nHA sonocoated during tensile properties testing in PBS.</p>
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<p>Metabolic activity of BJ (<b>A</b>) and MG-63 (<b>D</b>) cells seeded on PDLLA/PLGA and PDLLA/PLGA/nHA sonocoated materials after 24 h, 72 h, and 7 days. SEM colorized images of MG-63 cells attachment after 24 h on (<b>B</b>,<b>C</b>) PDLLA/PLGA and (<b>E</b>,<b>F</b>) PDLLA/PLGA/nHA sonocoated materials. (<b>B</b>,<b>E</b>): magnification 10kx; (<b>C</b>,<b>F</b>): magnification 25kx. Metabolic activity expressed as a percentage of the control, mean ± SD from three independent experiments. (*denotes statistically significant difference from unexposed control, <span class="html-italic">p</span> &lt; 0.05).</p>
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<p>Scheme of particles release mechanism and SEM images of Electrosprayed (<b>top</b>) and Sonocoated (<b>down</b>) PDLLA/PLGA fibers after 10 weeks of degradation.</p>
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12 pages, 4343 KiB  
Article
A Facile, One-Step Synthesis of Silicon/Silicon Carbide/Carbon Nanotube Nanocomposite as a Cycling-Stable Anode for Lithium Ion Batteries
by Yi Zhang, Kai Hu, Yunlei Zhou, Yingbin Xia, Nengfei Yu, Guanglei Wu, Yusong Zhu, Yuping Wu and Haibo Huang
Nanomaterials 2019, 9(11), 1624; https://doi.org/10.3390/nano9111624 - 15 Nov 2019
Cited by 49 | Viewed by 6533
Abstract
Silicon/carbon nanotube (Si/CNTs) nanocomposite is a promising anode material for lithium ion batteries (LIBs). Challenges related to the tricky synthesis process, as well as the weak interaction between Si and CNTs, hinder practical applications. To address these issues, a facile, one-step method to [...] Read more.
Silicon/carbon nanotube (Si/CNTs) nanocomposite is a promising anode material for lithium ion batteries (LIBs). Challenges related to the tricky synthesis process, as well as the weak interaction between Si and CNTs, hinder practical applications. To address these issues, a facile, one-step method to synthesize Si/CNTs nanocomposite by using silica (SiO2) as a reactant via a magnesium reduction process was developed. In this synthesis, the heat released enables the as-obtained Si to react with CNTs in the interfacial region to form silicon carbide (SiC). By virtue of the unique structure composed of Si nanoparticles strongly anchored to conductive CNTs network with stable Si–C chemical bonding, the Si/SiC/CNT nanocomposite delivers a stable capacity of ~1100 mAh g−1 and a capacity retention of about 83.8% after 200 cycles at a current density of 100 mA g−1. Our studies may provide a convenient strategy for the preparation of the Si/C anode of LIBs. Full article
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<p>The schematic illustration of Si/SiC/carbon nanotubes’ (CNTs) nanocomposite preparation.</p>
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<p>SEM images of crude CNTs (<b>a</b>) and purified CNTs (<b>b</b>), and TEM images of crude CNTs (<b>c</b>) and purified CNTs (<b>d</b>).</p>
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<p>(<b>a</b>) XRD patterns of crude CNTs and purified CNTs; (<b>b</b>) FTIR spectrum of crude CNTs and purified CNTs; (<b>c</b>) the pictures of crude CNTs and purified CNTs dispersed in ethanol.</p>
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<p>(<b>a</b>) XRD patterns of the Si/SiC/CNT nanocomposite; (<b>b</b>) TGA of Si/SiC/CNT nanocomposite; (<b>c</b>) Raman spectrum of Si/SiC/CNT nanocomposite.</p>
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<p>(<b>a</b>,<b>b</b>) SEM images of Si/SiC/CNT nanocomposite; (<b>c</b>) EDX spectrum of Si/SiC/CNT nanocomposite. Element mappings of Si/SiC/CNT nanocomposite: Si (<b>d</b>); C (<b>e</b>); O (<b>f</b>).</p>
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<p>(<b>a</b>,<b>b</b>) TEM images of Si/SiC/CNT nanocomposite; (<b>c</b>) HRTEM image of Si/SiC/CNT nanocomposite; (<b>d</b>) SAED pattern of Si/SiC/CNT nanocomposite.</p>
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<p>(<b>a</b>) Galvanostatic charge/discharge profiles of Si/SiC/CNT nanocomposite; (<b>b</b>) CV on Si/SiC/CNT nanocomposite electrode at the scan rate of 0.2 mV s<sup>−1</sup>; (<b>c</b>) cycling performance and Coulombic efficiency of pure Si and Si/SiC/CNT nanocomposites; (<b>d</b>) rate performances of Si/SiC/CNT nanocomposite and pure Si.</p>
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<p>SEM images of Si/SiC/CNT composite before cycling (<b>a</b>) and after 100 cycles (<b>b</b>). SEM image of Si/SiC/CNT electrode after 100 cycles (<b>c</b>). SEM images of pure Si material before cycling (<b>d</b>) and after 100 cycles (<b>e</b>). SEM image of pure Si electrode after 100 cycles (<b>f</b>).</p>
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<p>The EIS spectra of Si/SiC/CNT anode and pure Si anode after 100 cycles.</p>
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17 pages, 3721 KiB  
Article
Synergistical Use of Electrostatic and Hydrophobic Interactions for the Synthesis of a New Class of Multifunctional Nanohybrids: Plasmonic Magneto-Liposomes
by Gabriela Fabiola Știufiuc, Ștefan Nițică, Valentin Toma, Cristian Iacoviță, Dietrich Zahn, Romulus Tetean, Emil Burzo, Constantin Mihai Lucaciu and Rareș Ionuț Știufiuc
Nanomaterials 2019, 9(11), 1623; https://doi.org/10.3390/nano9111623 - 15 Nov 2019
Cited by 8 | Viewed by 2834
Abstract
By carefully controlling the electrostatic interactions between cationic liposomes, which already incorporate magnetic nanoparticles in the bilayers, and anionic gold nanoparticles, a new class of versatile multifunctional nanohybrids (plasmonic magneto-liposomes) that could have a major impact in drug delivery and controlled release applications [...] Read more.
By carefully controlling the electrostatic interactions between cationic liposomes, which already incorporate magnetic nanoparticles in the bilayers, and anionic gold nanoparticles, a new class of versatile multifunctional nanohybrids (plasmonic magneto-liposomes) that could have a major impact in drug delivery and controlled release applications has been synthesized. The experimental results confirmed the successful synthesis of hydrophobic superparamagnetic iron oxide nanoparticles (SPIONs) and polyethylene glycol functionalized (PEGylated) gold nanoparticles (AuNPs). The SPIONs were incorporated in the liposomal lipidic bilayers, thus promoting the formation of cationic magnetoliposomes. Different concentrations of SPIONs were loaded in the membrane. The cationic magnetoliposomes were decorated with anionic PEGylated gold nanoparticles using electrostatic interactions. The successful incorporation of SPIONs together with the modifications they generate in the bilayer were analyzed using Raman spectroscopy. The plasmonic properties of the multifunctional nanohybrids were investigated using UV-Vis absorption and (surface-enhanced) Raman spectroscopy. Their hyperthermic properties were recorded at different frequencies and magnetic field intensities. After the synthesis, the nanosystems were extensively characterized in order to properly evaluate their potential use in drug delivery applications and controlled release as a result of the interaction with an external stimulus, such as an NIR laser or alternating magnetic field. Full article
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<p>TEM image of the as-synthesized Fe<sub>3</sub>O<sub>4</sub> SPIONs.</p>
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<p>Hysteresis curves recorded at 5 and 300 K for the SPIONs samples.</p>
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<p>Transmission electron microscopy (TEM) image of PEGylated gold nanoparticles (<b>a</b>); TEM image of a single gold nanoparticle showing the presence of the polyethylene glycol (PEG) layer surrounding the nanoparticle (NP) (inset a). Statistical distribution of NPs sizes calculated from TEM images (<b>b</b>). UV-Vis absorption spectrum of the gold colloid (<b>c</b>); optical image of the gold colloid (inset c).</p>
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<p>TEM images of magneto-liposomes (MLP50) (<b>left</b>); unstained TEM image of a single magneto-liposome (MLP50) (<b>right</b>). The inset magnifies a membrane portion highlighting the incorporation of SPIONs in the lipid bilayer.</p>
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<p>Raman spectra of dioleoyloxi-3-trimethylammonium-propane chloride (DOTAP) lipids (green spectrum), soybean phosphatidyl-choline (SPC) lipids (blue spectrum), and DOTAP/SPC liposomes (magenta spectrum).</p>
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<p>(<b>a</b>) The black Raman spectrum was recorded of the SPION powder. (<b>b</b>) Superposition of the Raman spectra recorded of pure (unloaded) liposomes (magenta curve) with those recorded of the four classes of MLPs.</p>
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<p>VIS absorption spectra of the PEGylated gold colloids (1), and of the complexes they formed with pure liposomes (2) and MLPs containing different amounts of MNPs in their bilayers (3–6). The inset shows the optical images of the gold colloids and their liposomal complexes with their respective liposomal batch number: 1–0 μL, 2–10 μL, 3–50 μL, 4–250 μL, 5–1000 μL. The samples were diluted four times before image recording.</p>
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<p>TEM image of incomplete decorated magneto-liposomes (MLP50). The inset highlights the presence of PEGylated AuNPs on the outer surface of the liposomes and of SPIONs inside the lipidic bilayer (<b>a</b>). TEM image of a single plasmonic magneto-liposome (MLP50) (<b>b</b>).</p>
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<p>A typical SER spectrum of the fully decorated plasmonic magneto-liposomes recorded in liquid conditions using a 785 nm excitation.</p>
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19 pages, 5162 KiB  
Article
Preparation of Anisotropic Aerogels with Pristine Graphene by Heat Flow and Study of Their Effects on Heat Transfer in Paraffin
by Jinhui Huang, Buning Zhang, Ming He, Xue Huang, Guoqiang Yin and Yingde Cui
Nanomaterials 2019, 9(11), 1622; https://doi.org/10.3390/nano9111622 - 15 Nov 2019
Cited by 3 | Viewed by 2925
Abstract
In this study, anisotropic graphene/graphene oxide (GO) aerogels (AGAs) were obtained by freeze-drying after direct participation of pristine graphene in the self-assembly of anisotropic gel by the heat flow method. After vacuum microwave treatment, the physical, chemical and structural characteristics of the AGAs [...] Read more.
In this study, anisotropic graphene/graphene oxide (GO) aerogels (AGAs) were obtained by freeze-drying after direct participation of pristine graphene in the self-assembly of anisotropic gel by the heat flow method. After vacuum microwave treatment, the physical, chemical and structural characteristics of the AGAs were investigated. The results show that AGAs, in which the internal graphene sheets are parallel to the heat flow direction, are successfully prepared. After microwave treatment, the amount of oxygen and nitrogen reduces significantly and the sp2 domain increases. However, at the same time, many fragments and holes are generated in the graphene sheets. The effects of AGAs on the phase transition of paraffin is studied, and the results show that the melting enthalpy, solidification enthalpy and initial melting temperature of AGA/paraffin composites decreases as the GO content in the AGAs increases, whereas the melting range, solidifying range and subcooling degree increases. The highest axial thermal conductivity of the AGA/paraffin composite is 1.45 W/(mK), and the thermal conductivity enhancement efficiency is 884% (AGA content was 0.53 vol %). Compared with previously investigated, similar AGA/paraffin composites, the aerogels fabricated in this study have the obvious advantages of a simple fabrication process, a low cost and a high thermal conductivity enhancement efficiency. These aerogels possess the potential for application in phase-change energy storage (PES), thermal energy management and other fields. Full article
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<p>Schematic diagram of anisotropic graphene/graphene oxide (GO) aerogels (AGAs) preparation steps. A digital image of the graphene dispersion (<b>a</b>) and a digital image of the AGA’s transverse section (<b>b</b>); a digital image of the AGA before (<b>c</b>) and after microwave treatment (<b>d</b>); a digital image of the AGA’s longitudinal section (<b>e</b>).</p>
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<p>The scanning electron microscopy (SEM) images of AGA. (<b>a</b>–<b>c</b>) are electron microscope images of different positions in the longitudinal section of AGA.</p>
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<p>SEM images of graphene sheets in AGA with different microwave treatment times ((<b>a1</b>,<b>a2</b>) were unmicrowaved, (<b>b1</b>,<b>b2</b>) were microwaved for 1 min, (<b>c1</b>,<b>c2</b>) were microwaved for 5 min, (<b>d1</b>,<b>d2</b>) were microwaved for 20 min).</p>
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<p>TGA curves of different samples.</p>
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<p>C1s X-ray photoelectron spectroscopy (XPS) fitting curves of different samples.</p>
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<p>O1s XPS fitting curves of different samples.</p>
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<p>N1s XPS fitting curves of different samples.</p>
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<p>Raman curves of AGAs with different microwave processing times.</p>
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<p>Raman curves of AGAs with different graphene oxide (GO) concentrations (The arrows indicate the blue shift).</p>
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<p>XRD curves of different samples.</p>
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<p>XRD curves of AGAs with different GO concentrations.</p>
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<p>TGA curves of paraffin and PC12W20E5.</p>
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<p>DSC curves of different AGA/paraffin composites ((<b>a</b>) was the complete curve, (<b>b</b>) and (<b>c</b>) were the local enlarged pictures of the melting and solidification curves respectively); Figure (<b>d</b>) compared the relevant thermal properties of samples with different GO concentrations and the same other conditions. Figure (<b>e</b>) compared the relevant thermal properties of samples with different microwave treatment times and the same other conditions. (T<span class="html-italic"><sub>ms</sub></span>, the initial melting temperature; T<span class="html-italic"><sub>mr</sub></span>, the melting range; ∆H<span class="html-italic"><sub>m</sub></span>, melting enthalpy; T<span class="html-italic"><sub>fr</sub></span>, solidifying range; ∆H<span class="html-italic"><sub>f</sub></span>, solidification enthalpy; T<span class="html-italic"><sub>c</sub></span>, subcooling degree. See <a href="#nanomaterials-09-01622-t001" class="html-table">Table 1</a> for specific values).</p>
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<p>DSC curves of C12W5E15 after several thermal cycles ((<b>a</b>,<b>b</b>) were digital photos taken before and after 100 cycles respectively).</p>
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<p>Thermal conductivity and thermal enhancement efficiency of AGA/paraffin composites (where * was prepared by non-heat flow method).</p>
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<p>Comparison of thermal conductivity enhancement of graphene/paraffin composites (■ [<a href="#B47-nanomaterials-09-01622" class="html-bibr">47</a>] ● [<a href="#B46-nanomaterials-09-01622" class="html-bibr">46</a>] ▲ [<a href="#B49-nanomaterials-09-01622" class="html-bibr">49</a>] ▼ [<a href="#B50-nanomaterials-09-01622" class="html-bibr">50</a>] ► [<a href="#B33-nanomaterials-09-01622" class="html-bibr">33</a>] ◆ [<a href="#B51-nanomaterials-09-01622" class="html-bibr">51</a>] ★ [<a href="#B34-nanomaterials-09-01622" class="html-bibr">34</a>] □ [<a href="#B52-nanomaterials-09-01622" class="html-bibr">52</a>] ○ [<a href="#B53-nanomaterials-09-01622" class="html-bibr">53</a>]).</p>
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<p>Thermal imaging images of *PC12W0E0 (left) and PC12W5E15 (right). (<b>a</b>) was the digital image taken before heating; (<b>b</b>), (<b>c</b>) and (<b>d</b>) were the thermal imaging images taken at 4 min, 8 min and 12 min respectively.</p>
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15 pages, 4644 KiB  
Article
Complexes Formed by Hydrophobic Interaction between Ag-Nanospheres and Adsorbents for the Detection of Methyl Salicylate VOC
by Jinhyuk Park, J. Alex Thomasson, Sandun Fernando, Kyung-Min Lee and Timothy J. Herrman
Nanomaterials 2019, 9(11), 1621; https://doi.org/10.3390/nano9111621 - 15 Nov 2019
Cited by 7 | Viewed by 3414
Abstract
Surface-enhanced Raman spectroscopy (SERS) has been widely investigated in many applications. However, only little work has been done on using SERS for the detection of volatile organic compounds (VOCs), primarily due to the challenges associated with fabricating SERS substrates with sufficient hotspots for [...] Read more.
Surface-enhanced Raman spectroscopy (SERS) has been widely investigated in many applications. However, only little work has been done on using SERS for the detection of volatile organic compounds (VOCs), primarily due to the challenges associated with fabricating SERS substrates with sufficient hotspots for signal enhancement and with the surface interfacially compatible for the VOCs. This study investigated the phase transfer of Ag-nanospheres (AgNSs) from the aqueous phase to the non-aqueous phase by electrostatic interaction induced by cationic surfactants, and the feasibility of the transferred AgNSs as SERS substrates for the determination of methyl salicylate VOC. Results indicated that one of three cationic surfactants, tetraoctylammonium bromide (TOAB) dissolved in organic solvent showed successful phase transfer of the AgNSs confirmed by several characterization analyses. The complex formed by hydrophobic interaction between the transferred AgNSs and Tenax-TA adsorbent polymer was able to be utilized as a SERS substrate, and the volatile of methyl salicylate could be easily determined from SERS measurements at 4 h static volatile collection. Therefore, the proposed new techniques can be effectively employed to areas where many VOCs relevant to food and agriculture need to be analyzed. Full article
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<p>Phase transfer of AgNSs from water to dichloromethane by different cationic surfactants (BKC, CTAB, and TOAB).</p>
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<p>TEM images of AgNCs and AgNSs before/after phase transfer. (<b>a</b>): AgNCs, (<b>b</b>): AgNSs before phase transfer, (<b>c</b>): Transferred AgNSs, (<b>d</b>): Transferred AgNSs with high resolution).</p>
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<p>EDX spectra of AgNSs before/after phase transfer.</p>
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<p>Crystal diffraction pattern of AgNSs (<b>a</b>) before phase transfer and (<b>b</b>) after phase transfer.</p>
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<p>UV/Vis absorption spectrum of AgNSs before/after phase transfer.</p>
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<p>Scheme of transferred AgNSs-polymer complex-based SERS substrate.</p>
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<p>SERS spectra of MeSA VOCs according to the collection times. M1 4HR: Mixture with 1 mg of polymer for 4 h, M2 4HR: Mixture with 2 of mg polymer for 4 h, M3 4HR: Mixture with 3 mg of polymer for 4 h, overnight: Averaged over three concentrations overnight. MeSA standard Raman spectrum is available in the <a href="#app1-nanomaterials-09-01621" class="html-app">Supplementary Materials, Figure S1</a>.</p>
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<p>The effect of adsorbent on SERS spectra of MeSA VOC. MeSA standard Raman spectrum is available in the <a href="#app1-nanomaterials-09-01621" class="html-app">Supplementary Materials, Figure S1</a>.</p>
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<p>Schemes of several possible interfacial phenomena for phase transfer. (<b>a</b>) Effect of the hydrophobic tail area according to the surfactants. (<b>b</b>) One possible interaction between AgNS and the added surfactant with a small hydrophobic tail (BKC, CTAB) in the water phase (Blue: water, Pink: dichloromethane): Surfactant insertion into AgNS. (<b>c</b>) Another possible interaction between AgNS and the added surfactant with a small hydrophobic tail (BKC, CTAB) in the water phase (Blue: water, Pink: dichloromethane): Surfactant attraction to AgNS. (<b>d</b>) Successful phase transfer of AgNS by the added TOAB dissolved in dichloromethane.</p>
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12 pages, 3793 KiB  
Article
Reconfigurable Local Photoluminescence of Atomically-Thin Semiconductors via Ferroelectric-Assisted Effects
by Changhyun Ko
Nanomaterials 2019, 9(11), 1620; https://doi.org/10.3390/nano9111620 - 15 Nov 2019
Cited by 3 | Viewed by 3196
Abstract
Combining a pair of materials of different structural dimensions and functional properties into a hybrid material system may realize unprecedented multi-functional device applications. Especially, two-dimensional (2D) materials are suitable for being incorporated into the heterostructures due to their colossal area-to-volume ratio, excellent flexibility, [...] Read more.
Combining a pair of materials of different structural dimensions and functional properties into a hybrid material system may realize unprecedented multi-functional device applications. Especially, two-dimensional (2D) materials are suitable for being incorporated into the heterostructures due to their colossal area-to-volume ratio, excellent flexibility, and high sensitivity to interfacial and surface interactions. Semiconducting molybdenum disulfide (MoS2), one of the well-studied layered materials, has a direct band gap as one molecular layer and hence, is expected to be one of the promising key materials for next-generation optoelectronics. Here, using lateral 2D/3D heterostructures composed of MoS2 monolayers and nanoscale inorganic ferroelectric thin films, reversibly tunable photoluminescence has been demonstrated at the microscale to be over 200% upon ferroelectric polarization reversal by using nanoscale conductive atomic force microscopy tips. Also, significant ferroelectric-assisted modulation in electrical properties has been achieved from field-effect transistor devices based on the 2D/3D heterostructrues. Moreover, it was also shown that the MoS2 monolayer can be an effective electric field barrier in spite of its sub-nanometer thickness. These results would be of close relevance to exploring novel applications in the fields of optoelectronics and sensor technology. Full article
(This article belongs to the Special Issue Preparation and Properties of 2D Materials)
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<p>ML-MoS<sub>2</sub>/PZT heterostructure preparation and optical characterization. Optical microscopy images of (<b>a</b>) as-grown ML-MoS<sub>2</sub> flakes on a SiO<sub>2</sub>/Si substrate and (<b>b</b>) a representative ML-MoS<sub>2</sub> flake wet-transferred on a PZT thin film surface. (<b>c</b>) PL and (<b>d</b>) Raman spectra measured from the ML-MoS<sub>2</sub> flake displayed in (<b>a</b>) and the bare PZT surface as a reference.</p>
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<p>Schematic of the poling process on AFM. (<b>a</b>) Up-polarized (P<sub>↑</sub>) and (<b>b</b>) down-polarized (P<sub>↓</sub>) states are achieved when a PZT thin films are applied by negative and positive <span class="html-italic">V<sub>P</sub></span> above the threshold voltage for polarization reversal using a conductive AFM tip, respectively. During the poling process, a metallic SRO layer is grounded electrically.</p>
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<p>Poling effects on the ML-MoS<sub>2</sub>/PZT heterostructure. (<b>a</b>) Optical microscopy (OM) image of a ML-MoS<sub>2</sub> flake with a scale bar which works for all the other images. PFM images of (<b>b</b>) the ML-MoS<sub>2</sub> flake on the PZT thin film whose left and right half areas are polarized in the P<sub>↑</sub> and P<sub>↓</sub> states by the poling process with the <span class="html-italic">V<sub>P</sub></span> of −12 V and +12 V, respectively, and (<b>c</b>) vice versa. (<b>d</b>) Topography AFM image of the ML-MoS<sub>2</sub> flake simultaneously obtained with the PFM image including the representative height profile for the corresponding green line, verifying the thickness of ML-MoS<sub>2</sub> flake. PL peak area maps of the identical ML-MoS<sub>2</sub> flake in (<b>e</b>–<b>g</b>) were scanned before poling and after the poling processes of (<b>b</b>,<b>c</b>), in order. (<b>h</b>–<b>j</b>) PL peak position maps displayed in the same sequence as in (<b>e</b>–<b>g</b>). (<b>k</b>) PL spectra measured from the spots of P<sub>↑</sub> and P<sub>↓</sub> regions marked in (<b>f</b>) along with that of the bare PZT as a reference. X and X<sup>−</sup> denote the emissions of neutral and negatively-charged excitons, respectively.</p>
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<p>Electrical back-gated experiments on the ML-MoS<sub>2</sub>/PZT heterostructures. (<b>a</b>) Optical microscopy image of a ML-MoS<sub>2</sub> sheet with a metal electrode. (<b>b</b>) Schematics of back-gating experiment. In this experiment, no voltage is applied between the source and drain. (<b>c</b>–<b>f</b>) Set of images of the PL peak area measured after back gating with <span class="html-italic">V<sub>G</sub></span> of −5 V, +5 V, +10 V, and again −5 V in order. (<b>g</b>–<b>j</b>) The set of images of PL peak position measured in a series in the same order of (<b>c</b>–<b>f</b>).</p>
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<p>Electrical transport characterization of the ML-MoS<sub>2</sub>/PZT heterostructures. (<b>a</b>) Optical microscopy image and (<b>b</b>) topography AFM image of a device with a channel based on two ML-MoS<sub>2</sub> sheets and metal electrodes on a PZT thin film. PL peak area maps of (<b>c</b>,<b>d</b>) were scanned after the poling process with <span class="html-italic">V<sub>P</sub></span> of −12 V and +12 V, respectively. (<b>e</b>) Device schematics for FET measurements with the circuit. (<b>f</b>) FET characteristic curves of drain current (<span class="html-italic">I<sub>D</sub></span>) vs. gate voltage (<span class="html-italic">V<sub>G</sub></span>) measured at the source-drain voltage (<span class="html-italic">V<sub>SD</sub></span>) of 1.0 V in the P<sub>↑</sub> and P<sub>↓</sub> states, respectively. The leakage current (<span class="html-italic">I<sub>G</sub></span>) vs. <span class="html-italic">V<sub>G</sub></span> are also plotted as dashed lines for both states. Note that the absolute values were taken for <span class="html-italic">I<sub>D</sub></span> and <span class="html-italic">I<sub>G</sub></span>.</p>
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<p>The ultrathin electric field shield. PFM images of a ML-MoS<sub>2</sub> flake on a BFO thin film scanned (<b>a</b>) as-prepared before poling and after poling with the <span class="html-italic">V<sub>P</sub></span> of (<b>b</b>) +8 V and (<b>c</b>) +10 V, respectively. Up to <span class="html-italic">V<sub>P</sub></span> of +8 V, the area of the BFO thin film beneath the ML-MoS<sub>2</sub> flake was not poled well, indicating that a ML-MoS<sub>2</sub> flake prevents field penetration into the BFO thin film.</p>
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19 pages, 5025 KiB  
Article
Ullmann Reactions of Carbon Nanotubes—Advantageous and Unexplored Functionalization toward Tunable Surface Chemistry
by Anna Kolanowska, Anna Wioleta Kuziel, Rafał Grzegorz Jędrysiak, Maciej Krzywiecki, Emil Korczeniewski, Marek Wiśniewski, Artur Piotr Terzyk and Sławomir Boncel
Nanomaterials 2019, 9(11), 1619; https://doi.org/10.3390/nano9111619 - 15 Nov 2019
Cited by 11 | Viewed by 4438
Abstract
We demonstrate Ullmann-type reactions as novel and advantageous functionalization of carbon nanotubes (CNTs) toward tunable surface chemistry. The functionalization routes comprise O-, N-, and C-arylation of chlorinated CNTs. We confirm the versatility and efficiency of the reaction allowing functionalization degrees [...] Read more.
We demonstrate Ullmann-type reactions as novel and advantageous functionalization of carbon nanotubes (CNTs) toward tunable surface chemistry. The functionalization routes comprise O-, N-, and C-arylation of chlorinated CNTs. We confirm the versatility and efficiency of the reaction allowing functionalization degrees up to 3.5 mmol g−1 by applying both various nanotube substrates, i.e., single-wall (SWCNTs) and multi-wall CNTs (MWCNTs) of various chirality, geometry, and morphology as well as diverse Ullmann-type reagents: phenol, aniline, and iodobenzene. The reactivity of nanotubes was correlatable with the nanotube diameter and morphology revealing SWCNTs as the most reactive representatives. We have determined the optimized conditions of this two-step synthetic protocol as: (1) chlorination using iodine trichloride (ICl3), and (2) Ullmann-type reaction in the presence of: copper(I) iodide (CuI), 1,10-phenanthroline as chelating agent and caesium carbonate (Cs2CO3) as base. We have analyzed functionalized CNTs using a variety of techniques, i.e., scanning and transmission electron microscopy, energy dispersive spectroscopy, thermogravimetry, comprehensive Raman spectroscopy, and X-ray photoelectron spectroscopy. The analyses confirmed the purely covalent nature of those modifications at all stages. Eventually, we have proved the elaborated protocol as exceptionally tunable since it enabled us: (a) to synthesize superhydrophilic films from—the intrinsically hydrophobic—vertically aligned MWCNT arrays and (b) to produce printable highly electroconductive pastes of enhanced characteristics—as compared for non-modified and otherwise modified MWCNTs—for textronics. Full article
(This article belongs to the Special Issue Carbon Nanotube: Synthesis, Characteristics and Applications)
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<p>General scheme of the preferential sites of chlorination of carbon nanotubes (CNTs) by their treatment with ICl<sub>3</sub> (<b>A</b>); optimized conditions for Ullmann-type reactions of CNTs (<b>B</b>); for clarity, only a fragment of the (outer) nanotube wall is shown; ∅ stands for an empty set, i.e., no atoms in the case of <span class="html-italic">C</span>-arylation. The figure was prepared on the basis of a hypothesis made by Abdelkader et al. [<a href="#B33-nanomaterials-09-01619" class="html-bibr">33</a>].</p>
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<p>High-Resolution Transmission Microscope images (HRTEM) of chlorinated TUBALL™ single-walled carbon nanotubes (SWCNTs) by their treatment with: ICl<sub>3</sub> (<b>A</b>), subjected to an Ullmann-type reaction with phenol (<b>B</b>), subjected to Ullmann-type reaction with iodobenzene (<b>C</b>), subjected to Ullmann-type reaction with aniline (<b>D</b>).</p>
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<p>The Radial Breathing Mode (RBM) region of pristine and functionalized SWCNTs.</p>
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<p>The G-band (<b>A</b>) and D-band (<b>B</b>) region of SWCNT samples; (<b>C</b>) I<sub>D</sub>/I<sub>G</sub> and I<sub>D</sub>/I<sub>G’</sub> ratios presented as blue and red bars, respectively.</p>
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<p>The G-band range after deconvolution for pristine and functionalized single-walled carbon nanotubes (SWCNTs).</p>
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<p>Thermogravimetric (TG) curve for 1,3,5-trihydroxybenzene (THB) modified in-house vs. a pristine MWCNT array sample.</p>
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<p>O-1s region X-ray photoelectron spectroscopy (XPS) signals and deconvoluted peaks for <span class="html-italic">O</span>-arylated Nanocyl NC7000<sup>TM</sup> MWCNTs modified via reaction of chlorinated nanotubes with phenol (<b>A</b>) and 1,3,5-trihydroxybenzene (<b>B</b>).</p>
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<p>High resolution X-ray photoelectron spectroscopy (XPS) of Nanocyl NC7000<sup>TM</sup> MWCNTs obtained in the C 1s bonding energy region for: halogenated CNTs with ICl<sub>3</sub> (<b>A</b>), halogenated CNTs using ICl (<b>B</b>), <span class="html-italic">O</span>-arylated CNTs (<b>C</b>), <span class="html-italic">N</span>-arylated CNTs (<b>D</b>), <span class="html-italic">C</span>-arylated CNTs (<b>E</b>), modified with 1,3,5-trihydroxybenzene (THB) (<b>F</b>).</p>
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<p>High resolution X-ray photoelectron spectroscopy (XPS) of Nanocyl NC7000<sup>TM</sup> MWCNTs obtained in the N 1s bonding energy region for <span class="html-italic">N</span>-arylated MWCNTs.</p>
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<p>Aqueous dispersions of in-house MWCNT array tiny flakes: pristine (<b>A</b>) and covalently modified by Ullmann-type reaction of chlorinated arrays with 1,3,5-trihydroxybenzene—identical weight and no ultrasonication applied (<b>B</b>); wetting dynamics of 1,3,5-trihydroxybenzene (THB) covalently modified in-house ‘MWCNT carpet’—snapshots of photographs in the timescale of seconds for a drop released from a goniometer (<b>C</b>); the correlation between wetting contact angle (WCA) and the enthalpy of immersion for three samples: pristine, blank experiment (no catalyst in the Ullmann reaction) and non-covalently treated with 1,3,5-trihydroxybenzene in-house vertically aligned MWCNT array (<b>D</b>).</p>
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24 pages, 8437 KiB  
Article
Hall Amplifier Nanoscale Device (HAND): Modeling, Simulations and Feasibility Analysis for THz Sensor
by Avi Karsenty and Raz Mottes
Nanomaterials 2019, 9(11), 1618; https://doi.org/10.3390/nano9111618 - 14 Nov 2019
Cited by 4 | Viewed by 3732
Abstract
HAND (Hall Amplifier Nanoscale Device), a new nano-metric device, was designed, simulated, and modeled for feasibility analysis, with the challenge of combining a well-known macro effect into the nanoscale world. HAND is based on the well-known Hall Effect, and it may enable circuitry [...] Read more.
HAND (Hall Amplifier Nanoscale Device), a new nano-metric device, was designed, simulated, and modeled for feasibility analysis, with the challenge of combining a well-known macro effect into the nanoscale world. HAND is based on the well-known Hall Effect, and it may enable circuitry working at very high frequencies (tens of Tera-Hertz). The architecture, design, and simulations were performed while using Comsol Multi-Physics Package Software. Complementary accurate analytical models were developed to support the understanding of the device functionality, including treatment of specific phenomena, such as heat transfer, and mega-magnet feasibility inside integrated circuits. This new device, combining both the Hall Effect and nanoscale dimensions, holds the potential to change the computing rates in the microelectronics circuitry world, and can serve as a game changer. Full article
(This article belongs to the Special Issue Nano Fabrications of Solid-State Sensors and Sensor Systems)
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<p>Proposed structure and parameter names of the Hall Amplifier.</p>
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<p>Materials composing the design.</p>
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<p>Hall Bar geometry for the simulations.</p>
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<p>Mesh for three-dimensional (3D) simulation set-up.</p>
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<p>Mesh for two-dimensional (2D) simulation of the Hall Bar.</p>
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<p>Magnetic flux density norm (T) produced by 30 nm copper coil at a of distance CD = 70 nm, and with electric current input of 30 µA.</p>
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<p>Magnetic flux density norm (T) produced by 25 nm copper coil at varying distance CD, and this time with an electric current input of 30 mA. (<b>a</b>) CD = 80 nm; (<b>b</b>) CD = 85 nm; (<b>c</b>) CD = 90 nm; (<b>d</b>) CD = 95 nm; and, (<b>e</b>) CD = 100 nm.</p>
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<p>Magnetic flux density norm (T), produced by several lengths of copper coil at a distance of CD = 100 nm, and with an electric current input of 30 mA. (<b>a</b>) 15 nm copper coil; (<b>b</b>) 20 nm copper coil; (<b>c</b>) 25 nm copper coil; (<b>d</b>) 30 nm copper coil; (<b>e</b>) 35 nm copper coil; and, (<b>f</b>) 40 nm copper coil.</p>
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<p>Magnetic flux density norm (T), produced by 15 nm copper coil with five loops, and an input electric current of 30 µA. (<b>a</b>) Face-view; and, (<b>b</b>) Cross-view.</p>
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<p>Magnetic flux density norm (T), produced by 15 nm copper coil with 10 loops, and an input electric current of 30 µA. (<b>a</b>) Face-view; and, (<b>b</b>) Cross-view.</p>
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<p>Magnetic flux density norm (T), produced by 15 nm copper coil with 15 loops, and an input electric current of 30 µA. (<b>a</b>) Face-view; and, (<b>b</b>) Cross-view.</p>
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<p>Magnetic flux density norm (T), produced by 15 nm copper coil with 20 loops, and an input electric current of 30 µA. (<b>a</b>) Face-view; and, (<b>b</b>) Cross-view.</p>
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<p>The temperature as a function of the input electric current.</p>
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<p>The temperature as a function of the input electric current. The temperature with input electric current: (<b>a</b>) 30 µA; (<b>b</b>) 45 µA; and, (<b>c</b>) 55 µA.</p>
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<p>The temperature produced by varying lengths of copper coil and input electric current of 30 µA: (<b>a</b>) 20 nm; (<b>b</b>) 25 nm; (<b>c</b>) 30 nm; (<b>d</b>) 35 nm; and, (<b>e</b>) 40 nm.</p>
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<p>Simulation of the voltage difference across the Hall Bar that is caused by the perpendicular magnetic field.</p>
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<p>Hall Voltage as a function of the frequency in half log scale.</p>
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<p>Hall Voltage as a function of the frequency in half log scale for several V<sub>dd</sub> values.</p>
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<p>Hall Voltage as a function of the frequency for different scattering times in log-log scale.</p>
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<p>Hall Voltage as a function of the frequency for heterodyne Hall conductivity.</p>
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15 pages, 5705 KiB  
Article
Influence of Nanoscale Textured Surfaces and Subsurface Defects on Friction Behaviors by Molecular Dynamics Simulation
by Ruiting Tong, Zefen Quan, Yangdong Zhao, Bin Han and Geng Liu
Nanomaterials 2019, 9(11), 1617; https://doi.org/10.3390/nano9111617 - 14 Nov 2019
Cited by 13 | Viewed by 3053
Abstract
In nanomaterials, the surface or the subsurface structures influence the friction behaviors greatly. In this work, nanoscale friction behaviors between a rigid cylinder tip and a single crystal copper substrate are studied by molecular dynamics simulation. Nanoscale textured surfaces are modeled on the [...] Read more.
In nanomaterials, the surface or the subsurface structures influence the friction behaviors greatly. In this work, nanoscale friction behaviors between a rigid cylinder tip and a single crystal copper substrate are studied by molecular dynamics simulation. Nanoscale textured surfaces are modeled on the surface of the substrate to represent the surface structures, and the spacings between textures are seen as defects on the surface. Nano-defects are prepared at the subsurface of the substrate. The effects of depth, orientation, width and shape of textured surfaces on the average friction forces are investigated, and the influence of subsurface defects in the substrate is also studied. Compared with the smooth surface, textured surfaces can improve friction behaviors effectively. The textured surfaces with a greater depth or smaller width lead to lower friction forces. The surface with 45° texture orientation produces the lowest average friction force among all the orientations. The influence of the shape is slight, and the v-shape shows a lower average friction force. Besides, the subsurface defects in the substrate make the sliding process unstable and the influence of subsurface defects on friction forces is sensitive to their positions. Full article
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<p>MD model of the sliding contact.</p>
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<p>Textured surfaces with different depths. (<b>a</b>) Smooth surface; (<b>b</b>) <span class="html-italic">d</span> = 0.3615 nm; (<b>c</b>) <span class="html-italic">d</span> = 0.723 nm; (<b>d</b>) <span class="html-italic">d</span> = 1.0845 nm.</p>
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<p>Average friction forces of the smooth surface and textured surfaces with different depths.</p>
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<p>Textured surfaces with different widths. (<b>a</b>) <span class="html-italic">w</span> = 0.3615 nm; (<b>b</b>) <span class="html-italic">w</span> = 0.723 nm; (<b>c</b>) <span class="html-italic">w</span> = 1.0845 nm.</p>
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<p>Average friction forces of textured surfaces with different widths.</p>
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<p>Atoms distributions during sliding process (<span class="html-italic">w</span> = 0.723 nm). (<b>a</b>) initial stage; (<b>b</b>) intermediate stage; (<b>c</b>) final stage.</p>
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<p>Atom accumulation in sliding process. (<b>a</b>) <span class="html-italic">w</span> = 0.3615 nm; (<b>b</b>) <span class="html-italic">w</span> = 1.0845 nm.</p>
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<p>Components of friction force.</p>
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<p>The definition of the texture orientation.</p>
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<p>Average friction forces of textured surfaces with different orientations.</p>
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<p>Schematic of the Frenkel–Kontorova–Tomlinson (FKT) model [<a href="#B39-nanomaterials-09-01617" class="html-bibr">39</a>]. (<b>a</b>) Commensurate; (<b>b</b>) incommensurate.</p>
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<p>Atom accumulation in sliding process. (<b>a</b>) <span class="html-italic">θ</span> = 0°; (<b>b</b>) <span class="html-italic">θ</span> = 45°.</p>
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<p>Components of friction force.</p>
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<p>Textured surfaces with different shapes. (<b>a</b>) #-shape; (<b>b</b>) rectangular; (<b>c</b>) v-shape.</p>
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<p>Average friction forces of textured surfaces with different shapes.</p>
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<p>Sliding contact model with subsurface defects in substrate.</p>
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<p>Average friction forces for different depths of defects.</p>
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<p>The dislocation of substrate during sliding process. (<b>a</b>) Perfect substrate; (<b>b</b>) substrate with defects (<span class="html-italic">h</span> = 3.615 nm).</p>
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17 pages, 2865 KiB  
Article
Nanoparticulate Metal Oxide Top Electrode Interface Modification Improves the Thermal Stability of Inverted Perovskite Photovoltaics
by Ioannis T. Papadas, Fedros Galatopoulos, Gerasimos S. Armatas, Nir Tessler and Stelios A. Choulis
Nanomaterials 2019, 9(11), 1616; https://doi.org/10.3390/nano9111616 - 14 Nov 2019
Cited by 15 | Viewed by 4077
Abstract
Solution processed γ-Fe2O3 nanoparticles via the solvothermal colloidal synthesis in conjunction with ligand-exchange method are used for interface modification of the top electrode in inverted perovskite solar cells. In comparison to more conventional top electrodes such as PC(70)BM/Al and PC(70)BM/AZO/Al, [...] Read more.
Solution processed γ-Fe2O3 nanoparticles via the solvothermal colloidal synthesis in conjunction with ligand-exchange method are used for interface modification of the top electrode in inverted perovskite solar cells. In comparison to more conventional top electrodes such as PC(70)BM/Al and PC(70)BM/AZO/Al, we show that incorporation of a γ-Fe2O3 provides an alternative solution processed top electrode (PC(70)BM/γ-Fe2O3/Al) that not only results in comparable power conversion efficiencies but also improved thermal stability of inverted perovskite photovoltaics. The origin of improved stability of inverted perovskite solar cells incorporating PC(70)BM/ γ-Fe2O3/Al under accelerated heat lifetime conditions is attributed to the acidic surface nature of γ-Fe2O3 and reduced charge trapped density within PC(70)BM/ γ-Fe2O3/Al top electrode interfaces. Full article
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Graphical abstract

Graphical abstract
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<p>Schematic illustration of the ligand exchange method for the preparation of BF<sub>4</sub><sup>−</sup>-capped <span class="html-italic">γ</span>-Fe<sub>2</sub>O<sub>3</sub> NPs.</p>
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<p>(<b>a</b>) Typical TEM image, (<b>b</b>) SAED pattern, (<b>c</b>) XRD pattern of γ-Fe<sub>2</sub>O<sub>3</sub> NPs. The standard pattern of maghemite phase, γ-Fe<sub>2</sub>O<sub>3</sub>, (JCPDS No. 39-1346) is also illustrated for collation (magenta bars) and (<b>d</b>) UV-Vis diffuse reflectance spectra versus energy (hv) for the γ-Fe<sub>2</sub>O<sub>3</sub> NPs.</p>
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<p>(<b>a</b>) Room-temperature PL emission spectra of the γ-Fe<sub>2</sub>O<sub>3</sub> NPs. PL measurement was performed on γ-Fe<sub>2</sub>O<sub>3</sub> films on the glass substrate at an excitation wavelength of 550 nm. (<b>b</b>) Mott-Schottky plot of the inverse square space-charge capacitance (1/C<sub>SC</sub><sup>2</sup>) as a function of applied voltage (E) relative to the redox potential of Ag/AgCl (3 M KCl) for the γ-Fe<sub>2</sub>O<sub>3</sub> NPs ETL.</p>
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<p>(<b>a</b>) Schematic representation of the device structure used and (<b>b</b>) the corresponding energy level diagram under study.</p>
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<p>Normalized (<b>a</b>) Voc, (<b>b</b>) Jsc, (<b>c</b>) FF and (<b>d</b>) PCE for three different top electrodes: PC(70)BM/Al, PC(70)BM/AZO/Al, PC(70)BM/γ-Fe<sub>2</sub>O<sub>3</sub>/Al.</p>
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<p>(<b>a</b>) Illuminated J-V characteristics and (<b>b</b>) dark J-V characteristics, respectively.</p>
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<p>(<b>a</b>) Mott Schottky measurements of fresh devices at f = 100 kHz and f = 500 Hz and (<b>b</b>) fresh and aged devices at f = 5 kHz.</p>
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11 pages, 3674 KiB  
Article
Fabrication of Cu2ZnSnS4 Thin Films from Ball-Milled Nanoparticle inks under Various Annealing Temperatures
by Xianfeng Zhang, Engang Fu, Maoxi Zheng and Yuehui Wang
Nanomaterials 2019, 9(11), 1615; https://doi.org/10.3390/nano9111615 - 14 Nov 2019
Cited by 7 | Viewed by 2940
Abstract
Cu2ZnSnS4 (CZTS) has been recognized as a promising thin-film absorber material of chalcopyrite-related solar cells. A two-stage method for fabricating CZTS films using CZTS nanoparticles was developed. Nanocrystal inks fabricated by a ball-milling method was utilized to °C deposit CZTS [...] Read more.
Cu2ZnSnS4 (CZTS) has been recognized as a promising thin-film absorber material of chalcopyrite-related solar cells. A two-stage method for fabricating CZTS films using CZTS nanoparticles was developed. Nanocrystal inks fabricated by a ball-milling method was utilized to °C deposit CZTS precursors by spin-coating approach. The CZTS precursors were annealed in the sulfur atmosphere under different annealing temperatures ranging from 550 °C to 650 °C. Influences of annealing temperature on grain growth, composition, crystallinity, and photovoltaic properties of CZTS films were characterized. With the increase of annealing temperature, grain growth was enhanced, while the sulfur atomic ratio fist increased then decreased. The crystallinity of the films was significantly improved after the annealing, and the obvious peak of the secondary phase of ZnS, were observed from the X-ray diffraction results, when the annealing temperature increased to 625 °C. However, the secondary phase was not detected from the surface Raman spectrum. Through comparing the Raman spectrum of different areas of the CZTS film, secondary phases of ZnS and SnS were observed, indicating the decomposition of CZTS films, due to the high temperature. The highest conversion efficiency of 7.5% was obtained when the annealing temperature was 600 °C. Full article
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<p>Surface morphology of CZTS films; (<b>a</b>) precursor; (<b>b</b>) 550 °C; (<b>c</b>) 575 °C; (<b>d</b>) 600 °C; (<b>e</b>) 625 °C; (<b>f</b>) 650 °C.</p>
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<p>Cross-sectional morphology of CZTS films; (<b>a</b>) precursor (<b>b</b>) 550 °C; (<b>c</b>) 575 °C; (<b>d</b>) 600 °C; (<b>e</b>) 625 °C; (<b>f</b>) 650 °C.</p>
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<p>XRD pattern of CZTS precursor and annealed films.</p>
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<p>XRD pattern of (112) plane of annealed CZTS films.</p>
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<p>Raman spectra of CZTS films with different annealing temperatures (magnification of object lens: 100×).</p>
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<p>3D microscope image of CZTS film annealed at 625 °C. The marks illustrated the area where Raman measurement were conducted.</p>
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<p>Raman spectra of different areas marked in <a href="#nanomaterials-09-01615-f005" class="html-fig">Figure 5</a> (magnification of object lens: 0.9×).</p>
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<p>Growth mechanism of CZTS films.</p>
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<p>Dependence of solar cell performance on the annealing temperature.</p>
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<p>Quantum efficiency of the best CZTS solar cells annealed at 600 °C.</p>
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