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18 pages, 2586 KiB  
Review
Quantum Dot Applications Using Kinetic Data: A Promising Approach for Enhanced Analytical Determinations
by Rafael C. Castro, Ricardo N. M. J. Páscoa, David S. M. Ribeiro and João L. M. Santos
Biosensors 2025, 15(3), 167; https://doi.org/10.3390/bios15030167 - 5 Mar 2025
Viewed by 118
Abstract
The acquisition of kinetic data in QD-based PL sensing methodologies has been revealed to be an auspicious alternative in applying these nanomaterials in analytical chemistry, enabling enhanced discrimination and quantification of analytes, even in complex sample matrices. The accessibility of kinetic measurements, which [...] Read more.
The acquisition of kinetic data in QD-based PL sensing methodologies has been revealed to be an auspicious alternative in applying these nanomaterials in analytical chemistry, enabling enhanced discrimination and quantification of analytes, even in complex sample matrices. The accessibility of kinetic measurements, which use routine laboratory instrumentation, is a significant advantage that increases the practicality of this methodology. The simple acquisition of these kinds of second-order data combined with chemometric analysis can ensure accurate results in environmental, biomedical, and food monitoring applications. These developments emphasize the vital importance of kinetic approaches in increasing sensitivity, improving analyte discrimination, and making the application of QDs in complex samples possible. Full article
(This article belongs to the Special Issue Biosensors for Monitoring and Diagnostics)
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Figure 1

Figure 1
<p>Summary of the different data structures that can be obtained for a sample using PL-based methodologies. (<b>a</b>) Zeroth-order data, representing fluorescence intensity at a single wavelength as a function of analyte concentration (red cross); (<b>b</b>) First-order data, corresponding to the fluorescence emission spectrum at a fixed excitation wavelength; and (<b>c</b>) Second-order data, related to an Excitation-emission matrix or the evolution of the sample’s PL spectrum over time at a fixed excitation wavelength. Adapted with permission from [<a href="#B37-biosensors-15-00167" class="html-bibr">37</a>]. Copyright 2021 Elsevier.</p>
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<p>Second-order data using QD-based methodologies: (<b>a</b>) excitation–emission spectra (λ<sub>em</sub> ranging from 330 nm to 380 nm and λ<sub>ex</sub> ranging from 400 to 500 nm) of CDs and (<b>b</b>) PL kinetics data of the combined nanoprobe encompassing CdTe/AgInS<sub>2</sub> QDs upon interaction with acetylsalicylic acid over 10 min. The colors represent the intensity of the emission, with red indicating higher intensity and blue indicating lower intensity. Adapted with permission from [<a href="#B38-biosensors-15-00167" class="html-bibr">38</a>,<a href="#B39-biosensors-15-00167" class="html-bibr">39</a>]. Copyright 2024 Elsevier and MDPI 2023.</p>
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<p>(<b>a</b>) Variation in the PL signal of GSH-CdTe QDs during 20 min without and with Fe<sup>2+</sup> and Fe<sup>3+</sup>. (<b>b</b>) Kinetic behavior of GSH-CdTe in the presence of different transition metal ions. Adapted with permission from [<a href="#B48-biosensors-15-00167" class="html-bibr">48</a>]. Copyright 2009 American Chemical Society.</p>
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<p>Alternative approaches for achieving effective kinetics-based sensing platforms using QDs: (<b>a</b>) nanoprobe with a single emitter for oxytetracycline detection; (<b>b</b>) multi-emission nanoprobe with distinct emission spectra in a ratiometric probe for the detection of histamine in foodstuffs; and (<b>c</b>) PL spectra of the nanohybrid probe composed of MES-CdTe/MPA-AgInS<sub>2</sub> with the overlap of both individual nanoparticle emission bands by the determination of acetylsalicylic acid in pharmaceutical formulations. The colors represent the intensity of the emission, with red indicating higher intensity and blue indicating lower intensity.Adapted with permission from [<a href="#B37-biosensors-15-00167" class="html-bibr">37</a>,<a href="#B39-biosensors-15-00167" class="html-bibr">39</a>,<a href="#B50-biosensors-15-00167" class="html-bibr">50</a>]. Copyright 2021 Elsevier, 2023 Elsevier, 2023 MDPI.</p>
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<p>(<b>a</b>) Progression of the PL emission intensity of the AIS QDs at the maximum emission wavelength over time, both in the absence of OTC and upon the addition of increasing concentrations of OTC. (<b>b</b>) Schematic representation summarizing the detection principle of AFB1 via the photocatalytic process involving the mycotoxin and AIS QDs and AFB1 determination using the U-PLS model. (<b>c</b>) Second-order data PL spectra of the combined nanoprobe before and after the interaction with 35.6 mg L<sup>−1</sup> of acetylsalicylic acid over 30 min. The colors represent the intensity of the emission, with red indicating higher intensity and blue indicating lower intensity. Adapted with permission from [<a href="#B37-biosensors-15-00167" class="html-bibr">37</a>,<a href="#B39-biosensors-15-00167" class="html-bibr">39</a>,<a href="#B59-biosensors-15-00167" class="html-bibr">59</a>]. Copyright 2021 Elsevier, 2023 Elsevier, 2023 MDPI.</p>
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21 pages, 6223 KiB  
Article
Preliminary Analysis of Quantum Dots as a Marking Technique for Ceratitis capitata
by Richard Wimbush, Pia Addison, Francois Bekker, Minette Karsten, Melissa Powell, George Marais, Aaisha Moerat, Anandie Bierman and John S. Terblanche
Insects 2025, 16(3), 270; https://doi.org/10.3390/insects16030270 - 4 Mar 2025
Viewed by 129
Abstract
This study evaluates the potential of quantum dots (QDs) as a marking method for Mediterranean fruit flies (Ceratitis capitata) (Medfly) in comparison to traditional fluorescent powder. As a highly destructive pest impacting a wide variety of fruit crops, an effective marking [...] Read more.
This study evaluates the potential of quantum dots (QDs) as a marking method for Mediterranean fruit flies (Ceratitis capitata) (Medfly) in comparison to traditional fluorescent powder. As a highly destructive pest impacting a wide variety of fruit crops, an effective marking technique is essential for improving the biological understanding and management of Medflies, including control strategies like the Sterile Insect Technique (SIT). Through multiple controlled experiments, we examined the effects of QDs and fluorescent powder markers on Medfly flight ability, marker retention rates, and marker durability and stability under diverse storage conditions. Fluorescent powder demonstrated consistently high reliability across all parameters, whereas QDs showed reduced retention, particularly when applied to pupae, and had a more pronounced negative effect on flight ability. This was illustrated by the field trials, which did not recapture any of the QD-marked flies, highlighting the current limitations in QD application methods. Additionally, fluorescent powders outperformed QDs in both long-term storage conditions and short-term stability tests. These findings indicate that while QDs possess potential as marking agents, further refinement of application techniques is required to achieve comparable efficacy to fluorescent powders in pest management contexts. Full article
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Figure 1
<p>(<b>A</b>) The percentage of Medflies marked after 8 days using three marking techniques: QDs applied during the adult stage (QA), QDs applied during the pupal stage (QP), and fluorescent powder applied during the pupal stage (P). A total of 240 Medflies (N = 240) were used across the experiment, with each treatment group consisting of 20 specimens per replicate, repeated four times. Vertical bars indicate 95% confidence intervals. Significant differences between treatments are denoted by different letters (a, b, c), where <span class="html-italic">p</span> &lt; 0.01, indicating that marking retention varied significantly between the groups. (<b>B</b>) Comparison of the marking percentages across sexes (male and female) for the different marking treatments. The same three marking techniques were evaluated, with males and females analyzed separately to assess potential sex-based differences in marking retention. Vertical bars represent 95% confidence intervals.</p>
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<p>The total number of Medflies able to fly under different marking treatments when attracted by a food and light source. Medflies were marked using one of two techniques: QDs applied during the adult stage (QD) or fluorescent powder applied during the pupal stage (FP). A control group (C) of unmarked Medflies was also included for comparison. A total of 240 Medflies (N = 240) were tested in a controlled flight trial, with each treatment group consisting of 20 specimens per replicate, repeated four times. Vertical bars indicate the number of observations, with the percentage of individuals from each marking treatment that could fly displayed on each bar.</p>
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<p>The total number of Medflies combined at 24, 48, and 72 h, categorized as flyers, non-flyers, or those that did not emerge during the mark–release–recapture study. Medflies were marked with either fluorescent powder (<b>A</b>), yellow QDs (<b>B</b>), red QDs (<b>C</b>), or orange QDs (<b>D</b>) during the pupal stage to assess the persistence and effectiveness of QD markings in comparison to fluorescent powder. A total of 12,000 Medflies were marked and released (N = 12,000), with equal distribution across all marking groups (3000 Medflies per group, repeated across three experimental replicates). Bars indicate the total number of observations, with percentage breakdown of the different categories displayed on each bar. Environmental conditions during the study varied across replicates, with temperatures ranging from 15.8 °C to 19.2 °C. The experiment was conducted over two seasons (Autumn and Spring), allowing for assessment under different climatic conditions.</p>
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<p>The percentage of Medflies that remained successfully marked with QDs during the six storage treatments (T1–T6) across all time intervals (2, 4, and 8 weeks). The treatments represent different storage and handling conditions, including storage in ethanol at different temperatures (−20 °C (T1), −80 °C (T2), and room temperature(T3)), dry storage at room temperature (T4), and rinsing in water (T5) or ethanol (T6) before dry storage. This experiment aimed to assess the retention and persistence of QD markings on Medflies under different storage conditions, compared to traditional fluorescent powders. The fluorescent powder retained 100% of its markings across all treatments and time intervals, and was therefore not included in the graph. For the entire experimental study, a total of 2160 Medflies were used, evenly distributed across all six treatments and time periods (N = 2160). Vertical bars indicate 95% confidence intervals. Retention of markings was evaluated under UV light, with flies examined at each time point to determine the stability of QDs and fluorescent powders over time.</p>
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<p>Visualization of fluorescent powder marking on Medflies under different lighting conditions. The left image shows a marked fly under normal light and the right image shows the same marking under UV illumination.</p>
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<p>Visualization of QD fluorescence in marked Medflies under UV light using a stereomicroscope. (<b>A</b>) displays all three QD colors—orange, yellow, and red—side by side for comparison. (<b>B</b>–<b>D</b>) show the individual fluorescence of orange, yellow, and red QDs, respectively. These images are intended to illustrate the emission properties of each QD color under UV illumination and do not represent the actual quantity used in experimental applications. While red and orange may appear visually similar in the images, their differences are more distinct when observed directly.</p>
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<p>Fluorescence of Mediterranean fruit flies (<span class="html-italic">Ceratitis capitata</span>) marked with orange quantum dots (QDs) under UV light. These adult Medflies were marked with QDs as part of the “suitable marking technique” experiment and imaged using a stereomicroscope under UV illumination. The fluorescence observed indicates the retention and distribution of QDs on the insect exoskeleton post-marking.</p>
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30 pages, 2206 KiB  
Review
Advancing Cancer Therapy with Quantum Dots and Other Nanostructures: A Review of Drug Delivery Innovations, Applications, and Challenges
by Ashutosh Pareek, Deepanjali Kumar, Aaushi Pareek and Madan Mohan Gupta
Cancers 2025, 17(5), 878; https://doi.org/10.3390/cancers17050878 - 4 Mar 2025
Viewed by 172
Abstract
Nanotechnology, particularly quantum dots (QDs), has ushered in a transformative era in the pharmaceutical and medical industries, offering notable opportunities for nanoscale advancements. These nanoscale particles, known for their exceptional optical properties and quantum confinement, have emerged as indispensable tools in cancer drug [...] Read more.
Nanotechnology, particularly quantum dots (QDs), has ushered in a transformative era in the pharmaceutical and medical industries, offering notable opportunities for nanoscale advancements. These nanoscale particles, known for their exceptional optical properties and quantum confinement, have emerged as indispensable tools in cancer drug delivery and bioimaging. This review delves into various drug conjugation techniques with QDs, including covalent linking, non-covalent conjugation, click chemistry, disulfide linkage, and pH-sensitive linkage. Each method provides distinct advantages, such as enhanced stability, reversibility, specificity, and controlled drug release. Moreover, QDs have demonstrated significant promise in oncology by efficiently delivering drugs to cancerous tissues while minimising systemic toxicity. Investigations into their applications in different cancers, such as blood, brain, cervical, breast cancers, etc., reveal their efficacy in targeted drug delivery, real-time imaging, and improved therapeutic outcomes. However, challenges such as potential toxicity, stability, pharmacokinetics, and targeting specificity must be addressed to fully harness the benefits of QDs in cancer therapy. Future research should focus on developing biocompatible QDs, optimising conjugation techniques, and elucidating their safety profiles and long-term effects in biological systems. Overall, QDs represent a promising frontier in cancer treatment, offering multifaceted capabilities that hold the potential for enhanced therapeutic outcomes and reduced side effects across various cancers. Full article
(This article belongs to the Section Cancer Drug Development)
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<p>Classification of quantum dots based on material composition.</p>
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<p>Schematic illustration of covalent conjugation using EDC-NHS chemistry, which enables the formation of bonds with free amino groups, proteins, peptides, and antibodies.</p>
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<p>Schematic representation of different drug conjugation strategies with QDs, including non-covalent interactions, click chemistry, disulfide linkages, and pH-sensitive linkers.</p>
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<p>This schematic illustrates the targeted action of drug-ligand-conjugated QDs in delivering chemotherapeutic drugs to varied cancers that bind to specific receptors on tumour cells in an acidic tumour microenvironment (pH &lt; 7). Upon entering the tumour site, QDs release the drugs, leading to enhanced tumour treatment outcomes, as shown by tumour blebbing and necrosis post-treatment.</p>
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18 pages, 3409 KiB  
Review
Advancements and Challenges in Colloidal Quantum Dot Infrared Photodetectors: Strategies for Short-Wave Infrared, Mid-Wave Infrared, and Long-Wave Infrared Applications
by Lijing Yu, Pin Tian and Kun Liang
Quantum Beam Sci. 2025, 9(1), 9; https://doi.org/10.3390/qubs9010009 - 3 Mar 2025
Viewed by 111
Abstract
Colloidal quantum dots (QDs) have emerged as promising materials for the development of infrared photodetectors owing to their tunable band gaps, cost-effective manufacturing, and ease of processing. This paper provides a comprehensive overview of the fundamental properties of quantum dots and the operating [...] Read more.
Colloidal quantum dots (QDs) have emerged as promising materials for the development of infrared photodetectors owing to their tunable band gaps, cost-effective manufacturing, and ease of processing. This paper provides a comprehensive overview of the fundamental properties of quantum dots and the operating principles of various infrared detectors. We review the latest advancements in short-wave infrared (SWIR), mid-wave infrared (MWIR), and long-wave infrared (LWIR) detectors employing colloidal quantum dots. Despite their potential, these detectors face significant challenges compared to conventional infrared technologies. Current commercial applications are predominantly limited to the near-infrared and short-wave bands, with medium- and long-wave applications still under development. The focus has largely been on lead and mercury-based quantum dots, which pose environmental concerns, underscoring the need for high-performance, non-toxic materials. Looking forward, the development of large array and small pixel detectors and improving compatibility with readout circuits are critical for future progress. This paper discusses these hurdles and offers insight into potential strategies to overcome them, paving the way for next-generation infrared sensing technologies. Full article
(This article belongs to the Special Issue Quantum Beam Science: Feature Papers 2024)
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<p>Band gap of bulk materials and quantum dots.</p>
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<p>Absorption spectra of PbS quantum dots of different sizes [<a href="#B20-qubs-09-00009" class="html-bibr">20</a>].</p>
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<p>Diagram of the surface of a quantum dot coated with oleic acid-capped and passivated by ligand exchange [<a href="#B21-qubs-09-00009" class="html-bibr">21</a>].</p>
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<p>Solution-processed photodetector. (<b>a</b>) Method of depositing colloidal quantum dots [<a href="#B29-qubs-09-00009" class="html-bibr">29</a>]. (<b>b</b>) Process diagram of colloidal quantum dot infrared focal plane detector [<a href="#B30-qubs-09-00009" class="html-bibr">30</a>]. (<b>c</b>) Cross-section of colloidal quantum dot infrared focal plane arrays [<a href="#B30-qubs-09-00009" class="html-bibr">30</a>].</p>
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<p>SWIR detector based on colloidal quantum dots. (<b>a</b>) Absorption spectrum of PbS CQDs [<a href="#B56-qubs-09-00009" class="html-bibr">56</a>]. (<b>b</b>) The process of combining PbS-QDs with the hybrid perovskite. (<b>c</b>) Energy level diagram for the PbS-QD + hybrid perovskite structure. (<b>d</b>) Device architecture of HgTe CQD photodetectors with ETL [<a href="#B58-qubs-09-00009" class="html-bibr">58</a>]. (<b>e</b>) Simulated current−voltage characteristics in the dark (dashed) and the light (solid). (<b>f</b>) The energy band from SCAPS modeling for HgTe CQD photodetectors. (<b>g</b>) Schematic of ROIC-integrated Ag<sub>2</sub>Te QD SWIR imager [<a href="#B59-qubs-09-00009" class="html-bibr">59</a>]. (<b>h</b>) Photograph of the imager and zoomed-in view of the ROIC die.</p>
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<p>MWIR detector based on colloidal quantum dots. (<b>a</b>) Synthesized HgTe quantum dots using HgBr2 as mercury source [<a href="#B81-qubs-09-00009" class="html-bibr">81</a>]. (<b>b</b>) TEM image of HgTe CQDs. (<b>c</b>) Structure diagram of the photoconductive detector. (<b>d</b>) Schematic of the architecture of the ultra-broadband imager [<a href="#B82-qubs-09-00009" class="html-bibr">82</a>]. (<b>e</b>) Photograph (above) and cross-sectional SEM image (bottom) of the ultra-broadband imager. (<b>f</b>) Thermal images captured by the ultra-broadband FPA imager with an MWIR optical filter. (<b>g</b>) Intraband transition of HgSe [<a href="#B83-qubs-09-00009" class="html-bibr">83</a>]. (<b>h</b>) TEM of HgSe CQDs before and after ligand exchange. (<b>i</b>) Photoresponse spectra of the HgSe CQD photoconductor. The right inset graph shows infrared hot images by a HgSe intraband CQD photodetector.</p>
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10 pages, 673 KiB  
Article
Optical Nonreciprocity Based on the Four-Wave Mixing Effect in Semiconductor Quantum Dots
by Zelin Lin, Han Yang, Fei Xu, Yihong Qi, Yueping Niu and Shangqing Gong
Nanomaterials 2025, 15(5), 380; https://doi.org/10.3390/nano15050380 - 1 Mar 2025
Viewed by 168
Abstract
Optical nonreciprocity and nonreciprocal devices such as optical diodes have broad and promising applications in various fields, ranging from optical communication to signal process. Here, we propose a magnet-free nonreciprocal scheme based on the four-wave mixing (FWM) effect in semiconductor quantum dots (SQDs). [...] Read more.
Optical nonreciprocity and nonreciprocal devices such as optical diodes have broad and promising applications in various fields, ranging from optical communication to signal process. Here, we propose a magnet-free nonreciprocal scheme based on the four-wave mixing (FWM) effect in semiconductor quantum dots (SQDs). Via controlling the directions of the coupling fields, the probe field can achieve high transmission in the forward direction within a certain frequency range due to the FWM effect. And the transmission of the probe field in the backward direction undergoes significant reduction, as the FWM effect is absent. The calculation results show a wide nonreciprocal transmission window with isolation greater than 12 dB and insertion loss lower than 0.08 dB. The influences of the Rabi frequencies of the coupling fields, the medium length, and the decay rates on the nonreciprocal propagation of the probe field are also studied, showing the requirements of these parameters for good nonreciprocal performances. Our work may offer an insight for developing optical nonreciprocal devices based on the FWM process and the SQD system. Full article
(This article belongs to the Special Issue Nanophotonics and Plasmonics)
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Figure 1
<p>Schematic of the laser coupling schemes and the possible experimental proposal in the GaAs/AlGaAs SQD system. (<b>a</b>) Presence of the FWM field when the probe field propagates in the forward direction, (<b>b</b>) absence of the FWM field when the probe field propagates in the backward direction, and (<b>c</b>) schematic diagram of the interaction between the SQD sample and laser fields.</p>
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<p>Transmission of the probe field for the forward (red solid) and backward (black dashed) cases. The right figure shows an enlarged view of the nonreciprocal window.</p>
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<p>Isolation (<b>a</b>) and insertion loss (<b>b</b>) within the nonreciprocal window. The parameters used in the calculation are the same as in <a href="#nanomaterials-15-00380-f002" class="html-fig">Figure 2</a>.</p>
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<p>Transmission of the probe field for forward (red solid) and backward (black dashed) cases versus the Rabi frequencies <math display="inline"><semantics> <mo>Ω</mo> </semantics></math> under a large probe detuning <math display="inline"><semantics> <mrow> <msub> <mo>Δ</mo> <mi>p</mi> </msub> <mo>=</mo> <mn>16.5</mn> <mspace width="0.166667em"/> <mi>meV</mi> </mrow> </semantics></math>. The other parameters are the same as in <a href="#nanomaterials-15-00380-f002" class="html-fig">Figure 2</a>.</p>
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<p>Transmission of the probe field for forward (red solid) and backward (black dashed) cases versus the penetration depths, where the probe detuning is set to be <math display="inline"><semantics> <mrow> <msub> <mo>Δ</mo> <mi>p</mi> </msub> <mo>=</mo> <mn>7</mn> </mrow> </semantics></math> meV. The other parameters are the same as in <a href="#nanomaterials-15-00380-f002" class="html-fig">Figure 2</a>.</p>
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<p>Transmission of the probe field for forward (red solid) and backward (black dashed) cases versus the decay rates, where the probe detuning is set to be <math display="inline"><semantics> <mrow> <msub> <mo>Δ</mo> <mi>p</mi> </msub> <mo>=</mo> <mn>7</mn> </mrow> </semantics></math> meV. The other parameters are the same as in <a href="#nanomaterials-15-00380-f002" class="html-fig">Figure 2</a>.</p>
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13 pages, 3194 KiB  
Article
Fluorescence Quenching of Graphene Quantum Dots from Orange Peel for Methyl Orange Detection
by Weitao Li, Yang Liu, Xinglong Pang, Yuanhao Huang, Zeyun Dong, Qian Niu, Yuping Xiong, Shang Li, Shuai Li, Lei Wang, Huazhang Guo, Saisai Cui, Shenpeng Hu, Yuenan Li, Tiantian Cha and Liang Wang
Nanomaterials 2025, 15(5), 376; https://doi.org/10.3390/nano15050376 - 28 Feb 2025
Viewed by 249
Abstract
Methyl orange (MO) is an organic synthetic dye widely used in laboratory and industrial applications. In laboratory settings, it serves as an acid–base indicator due to its distinct color change in both acidic and alkaline environments. Industrially, it is primarily utilized in the [...] Read more.
Methyl orange (MO) is an organic synthetic dye widely used in laboratory and industrial applications. In laboratory settings, it serves as an acid–base indicator due to its distinct color change in both acidic and alkaline environments. Industrially, it is primarily utilized in the textile industry for its ultraviolet (UV) absorption properties. However, the discharge and leakage of methyl orange into the environment can cause severe ecological damage and pose potential carcinogenic and teratogenic risks to human health. Therefore, detecting and quantifying the concentration of methyl orange in various matrices is crucial. This study reports the synthesis of graphene quantum dots (GQDs) from orange peel as a precursor, using ethanol and dimethylformamide (DMF) as solvents. Cyan (c-GQDs) and yellow (y-GQDs) graphene quantum dots were synthesized through a bottom-up hydrothermal method. The difference in color is attributed to the redshift caused by the varying ratio of pyridine nitrogen to pyrrole nitrogen. These GQDs exhibited notable optical properties, with c-GQDs emitting cyan fluorescence and y-GQDs emitting yellow fluorescence under UV light. To investigate fluorescence quenching effects, nine commonly used dyes were tested, and all were found to quench the fluorescence of y-GQDs, with methyl orange having the most significant effect. The fluorescence quenching of orange peel-derived GQDs in the presence of methyl orange is attributed to poor dispersion in DMF solution. Additionally, the GQDs possess high specific surface area, abundant surface functional groups, and excellent electronic conductivity, which contribute to their effective fluorescence quenching performance. The average thickness of y-GQDs (the vertical dimension from the substrate upwards) was 3.51 nm, confirming their graphene-like structure. They emitted yellow fluorescence within the wavelength range of 450–530 nm. Notably, a significant linear correlation was found between the concentration of methyl orange and the fluorescence intensity of y-GQDs (regression coefficient = 0.9954), indicating the potential of GQDs as effective sensing materials for organic pollutant detection. Full article
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Graphical abstract

Graphical abstract
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<p>(<b>a</b>,<b>b</b>) AFM plots and height distribution of c-GQDs and y-GQDs. (<b>c</b>,<b>d</b>) TEM images and relative size distributions of c-GQDs and y-GQDs. (<b>e</b>,<b>f</b>) High-resolution TEM images of c-GQDs and y-GQDs.</p>
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<p>(<b>a</b>) XRD patterns of y-GQDs and c-GQDs, (<b>b</b>) FT-IR patterns of y-GQDs and c-GQDs, (<b>c</b>) Raman patterns of y-GQDs and c-GQDs. (<b>d</b>) Fluorescence lifetime of y-GQDs before and after MO addition. Exponential fitting of fluorescence lifetime of y-GQDs with MO (<b>e</b>) and without MO (<b>f</b>).</p>
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<p>(<b>a</b>) Excitation wavelength dependence of y-GQDs; (<b>b</b>) photoluminescence (PL), photoluminescence excitation (PLE), and UV absorption spectra of y-GQDs; (<b>c</b>) excitation wavelength dependence of c-GQDs; (<b>d</b>) photoluminescence (PL), photoluminescence excitation (PLE), and UV absorption spectra of c-GQDs.</p>
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<p>(<b>a</b>) Full XPS spectrum of y-GQDs; (<b>b</b>–<b>d</b>) high-resolution C 1s, N 1s, and O 1s spectra of y-GQDs.</p>
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<p>(<b>a</b>) Fluorescence intensity histograms of c-GQDs and y-GQDs in different dye solutions. (<b>b</b>) Fluorescence spectra of c-GQDs and (<b>c</b>) y-GQDs in various dye solutions. Images of y-GQDs and c-GQDs in different dye solutions under UV light (<b>e</b>) and natural light (<b>d</b>). (<b>f</b>) Variation in the luminescence intensity of y-GQDs at different methyl orange concentrations.</p>
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<p>Changes in fluorescence intensity of (<b>a</b>) y-GQDs and (<b>b</b>) c-GQDs after seven days of placement. (<b>c</b>) Dispersion stability of y-GQDs; (<b>d</b>) dispersion stability of c-GQDs.</p>
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<p>The synthesis and utilization of b-GQDs and c-GQDs for the detection of dyes.</p>
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11 pages, 4127 KiB  
Article
Optimizing Semiconductor Saturable Absorption Mirrors Using Subwavelength Dielectric Gratings for Fiber Lasers
by Chaoqun Wei, Xiansheng Jia, Hongmei Chen, Boyuan Liu, Ziyang Zhang and Cheng Jiang
Photonics 2025, 12(3), 213; https://doi.org/10.3390/photonics12030213 - 28 Feb 2025
Viewed by 162
Abstract
Ultrafast fiber lasers have shown exceptional performance across various domains, including material processing, medical applications, and optoelectronic communication. The semiconductor saturable absorber mirror (SESAM) is a key enabler of ultrafast laser operation. However, the narrow wavelength range and limited modulation depth of conventional [...] Read more.
Ultrafast fiber lasers have shown exceptional performance across various domains, including material processing, medical applications, and optoelectronic communication. The semiconductor saturable absorber mirror (SESAM) is a key enabler of ultrafast laser operation. However, the narrow wavelength range and limited modulation depth of conventional SESAMs pose challenges to further advancing ultrafast fiber laser technology. To address these limitations, we explored the integration of guided mode resonance (GMR) effects to enhance light–matter interaction within the absorption layer. By incorporating subwavelength dielectric film gratings onto the cap layer of SESAMs, we excited GMR and formed a microcavity structure in conjunction with the distributed Bragg mirror (DBR). This design significantly improved the absorption efficiency of InAs quantum dots. The experimental results demonstrate that the modulation depth of the SESAM increased from 6.7% to 17.3%, while the pulse width was reduced by 2.41 times. These improvements facilitated the realization of a high-quality, stable ultrafast fiber laser. This study not only broadens the application potential of ultrafast lasers in diverse fields but also offers a practical pathway for advancing SESAM technology toward industrial-scale deployment. Full article
(This article belongs to the Special Issue Fiber Lasers: Recent Advances and Applications)
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<p>Sample preparation flowchart and the saturable absorption characteristics of quantum dots.</p>
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<p>The surface morphology of (<b>a</b>) S<sub>1</sub> and (<b>b</b>) S<sub>2</sub>. (<b>c</b>) The cross-section morphology of sample S<sub>1</sub>. (<b>d</b>) The cross-section morphology of sample S<sub>2</sub> and the distributed Bragg mirror. (<b>e</b>) The underlying physical mechanism and two-dimensional pattern of the prepared micro and nano structures. (<b>f</b>) The single-port system features a resonant structure, a subwavelength dielectric film grating, a gallium-arsenic overlay, an InAs quantum dot layer, and a distributed Bragg mirror.</p>
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<p>(<b>a</b>) Reflection and absorption spectra of S<sub>0</sub>, S<sub>1</sub> and S<sub>2</sub>. (<b>b</b>) Raman spectrum characterization of S<sub>0</sub>, S<sub>1</sub>, and S<sub>2</sub>. Surface E-field distribution of (<b>c</b>) S<sub>1</sub> and (<b>d</b>) S<sub>2</sub>, respectively. Cross-section E-field map of (<b>e</b>) S<sub>1</sub> and (<b>f</b>) S<sub>2</sub>.</p>
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<p>(<b>a</b>) The test schematic diagram of the dual probe system. The optical nonlinearity of sample (<b>b</b>) S<sub>0</sub>, (<b>c</b>) S<sub>1</sub>, and (<b>d</b>) S<sub>2</sub>.</p>
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<p>(<b>a</b>) The test principle diagram of the ring cavity laser. The output spectrogram of (<b>b</b>) S<sub>0</sub>, (<b>c</b>) S<sub>1</sub>, and (<b>d</b>) S<sub>2</sub> integrated into the laser. The output pulse width diagram of (<b>e</b>) S<sub>0</sub>, (<b>f</b>) S<sub>1</sub>, and (<b>g</b>) S<sub>2</sub> integrated into the laser.</p>
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<p>(<b>a</b>) A mode-locked pulse train of sample S<sub>2</sub> integrated into an ultrafast fiber laser. (<b>b</b>) The output frequency spectrum of sample S<sub>2</sub> integrated into an ultrafast fiber laser. (<b>c</b>) The signal-to-noise ratio of ultrafast fiber lasers. (<b>d</b>) The average power output of ultrafast fiber lasers and the operating stability test of sample S<sub>2</sub> integrated into an ultrafast fiber laser.</p>
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9 pages, 3341 KiB  
Article
Quantum Dot Waveguide Array for Broadband Light Sources
by Dongyang Li, Yufei Chu, Qingbo Xu, Dong Liu, Junying Ruan, Hao Sun, Jianwei Li, Chengde Guo, Xiaoyun Pu and Yuanxian Zhang
Photonics 2025, 12(3), 212; https://doi.org/10.3390/photonics12030212 - 28 Feb 2025
Viewed by 160
Abstract
In this paper, we demonstrate a broadband and simultaneous waveguide array light source based on water-soluble CdSe/ZnS quantum dots (QDs). We initially measure the fluorescence intensity for various cladding solution concentrations along the fiber axis to assess their impact on the propagation loss; [...] Read more.
In this paper, we demonstrate a broadband and simultaneous waveguide array light source based on water-soluble CdSe/ZnS quantum dots (QDs). We initially measure the fluorescence intensity for various cladding solution concentrations along the fiber axis to assess their impact on the propagation loss; the experimental results show that the fluorescent intensity decreases with fiber length, with higher concentrations showing a more pronounced decrease. Then, we showcase a synchronous QD light source in an optofluidic chip that fluoresces in red, green, and blue (RGB) within a microfluidic channel. Finally, a 3 × 3 QD array of a fluorescent display on a single PDMS chip is demonstrated. The QD waveguide represents a compact and stable structure that is readily manufacturable, making it an ideal light source for advancing high-throughput biochemical sensing and on-chip spectroscopic analysis. Full article
(This article belongs to the Special Issue Optical Sensing Technologies, Devices and Their Data Applications)
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<p>(<b>a</b>) Schematic structures of CdSe/ZnS QDs. (<b>b</b>) Chemical structures of organic dye, disodium fluorescein. (<b>c</b>) Normalized fluorescence intensity of the same concentration of QDs and disodium fluorescein varied with time. The pump power was fixed at 5 mw.</p>
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<p>(<b>a</b>) Fluorescence spectra of QDs with different path lengths (QD concentration: 5 µM). (<b>b</b>) Fluorescence spectra intensity of QDs versus the optical path length (QD concentration of 1, 5, 10 µM, respectively). (<b>c</b>) Fluorescence intensity attenuation with various optical path lengths. The error bars are calculated with five repeated measurements.</p>
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<p>(<b>a</b>) The schematic design diagram of the PDMS optofluidic device for a red–green–blue three-color fluorescent light source. (<b>b</b>) The absorption of CdSe/ZnS QDs with different emission wavelengths. (<b>c</b>) Image of the red–green–blue three-color fluorescent light source in operation. (<b>d</b>) The spectra of fluorescence emission of the broadband light source from different channels. The blue, green, and red shades are the fluorescence spectra of CdSe/ZnS QDs (emission wavelengths of 450 nm, 530 nm, and 650 nm) with a concentration of 5 µM, respectively.</p>
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<p>(<b>a</b>) The design diagram for a 3 × 3 fluorescence array. The red, green, and blue pipes represent the 450 nm, 530 nm, and 650 nm CdSe/ZnS QD solution injections, respectively. (<b>b</b>) Photograph of PDMS chip with 3 × 3 fluorescence array. (<b>c</b>) Photograph of RGB fluorescence emission by using a 3 × 3 fluorescence array. (<b>d</b>) Photograph of a fluorescence display prototype showing “YNU” based on a 3 × 3 fluorescence array.</p>
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22 pages, 3685 KiB  
Review
Hybrid Systems of Gels and Nanoparticles for Cancer Therapy: Advances in Multifunctional Therapeutic Platforms
by Kibeom Kim
Gels 2025, 11(3), 170; https://doi.org/10.3390/gels11030170 - 26 Feb 2025
Viewed by 178
Abstract
Cancer is a global health concern. Various therapeutic approaches, including chemotherapy, photodynamic therapy, and immunotherapy, have been developed for cancer treatment. Silica nanoparticles, quantum dots, and metal–organic framework (MOF)-based nanomedicines have gained interest in cancer therapy because of their selective accumulation in tumors [...] Read more.
Cancer is a global health concern. Various therapeutic approaches, including chemotherapy, photodynamic therapy, and immunotherapy, have been developed for cancer treatment. Silica nanoparticles, quantum dots, and metal–organic framework (MOF)-based nanomedicines have gained interest in cancer therapy because of their selective accumulation in tumors via the enhanced permeability and retention (EPR) effect. However, bare nanoparticles face challenges including poor biocompatibility, low stability, limited drug-loading capacity, and rapid clearance by the reticuloendothelial system (RES). Gels with unique three-dimensional network structures formed through various interactions such as covalent and hydrogen bonds are emerging as promising materials for addressing these challenges. Gel hybridization enhances biocompatibility, facilitates controlled drug release, and confers cancer-targeting abilities to nanoparticles. This review discusses gel–nanoparticle hybrid systems for cancer treatment developed in the past five years and analyzes the roles of gels in these systems. Full article
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<p>Schematic illustration of (<b>a</b>) the preparation of PTX-loaded nanoparticle-incorporated hydrogel and (<b>b</b>) the tissue-adhesive hydrogel as a local drug delivery system for effective antitumor chemotherapy in the 4T1 model in vivo. In vivo experimental data of PTX-loaded nanoparticle-incorporated hydrogel. (<b>c</b>) Average tumor volume curves with time (n = 5); (<b>d</b>) bodyweights over time (n = 5); (<b>e</b>) survival curve in different groups (n = 6). (* <span class="html-italic">p</span> &lt; 0.05, and *** <span class="html-italic">p</span> &lt; 0.001). Reproduced with permission [<a href="#B83-gels-11-00170" class="html-bibr">83</a>]. Copyright (2024): American Chemical Society.</p>
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<p>Schematic illustration of (<b>a</b>) preparation of DOX@Pd gel and the anticancer capacity of combined chemo-photothermal therapy. (<b>b</b>) Characterization of DOX@Pd Gel. Photographs of Pd NS aqueous dispersion (<b>I</b>), 4arm-PEG-thiol solution (<b>II</b>), Pd gel (<b>III</b>) and DOX@Pd gel (<b>IV</b>). Reproduced with permission [<a href="#B87-gels-11-00170" class="html-bibr">87</a>]. Copyright (2020): The Royal Society of Chemistry.</p>
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<p>Schematic illustration of (<b>a</b>) the preparation process of injectable TIMmH<sub>SD</sub> hydrogel and (<b>b</b>) the mechanism of TIMmH<sub>SD</sub>-mediated thermal immunotherapy. In vivo synergistic therapeutic effect of TIMmH<sub>SD</sub> hydrogel on primary tumor volume (<b>c</b>) and distant tumor volume (<b>d</b>) in mice following systemic treatment with PBS, TIMmH<sub>S</sub>, or TIMmH<sub>SD</sub> via local injection with and without 1064 nm laser irradiation (1 W/cm<sup>2</sup>, 5 min). (* <span class="html-italic">p</span> &lt; 0.05, ** <span class="html-italic">p</span> &lt; 0.01, and *** <span class="html-italic">p</span> &lt; 0.001). Reproduced with permission [<a href="#B97-gels-11-00170" class="html-bibr">97</a>]. Copyright (2022): Elsevier.</p>
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<p>ADHG hydrogels are initially crosslinked via electrostatic interactions between calcium cations and the carboxylate groups of Alg-DA. Their stability is further enhanced by incorporating polydopamine nanoparticles, which induce hydrogen bonding and π–π stacking interactions with the catechol groups of Alg-DA chains. Reproduced with permission [<a href="#B98-gels-11-00170" class="html-bibr">98</a>]. Copyright (2025): American Chemical Society.</p>
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<p>Schematic illustration of (<b>a</b>) the preparation process of RIC NPs@PLEL hydrogels and (<b>b</b>) photothermal immune therapy to prevent post-surgery tumor reoccurrence. (<b>c</b>) Temperature changes of PLEL hydrogel under NIR laser irradiation. (<b>d</b>) Reversible sol–gel transformation photos of PLEL hydrogels and RIC NPs@PLEL hydrogels. Reproduced with permission [<a href="#B108-gels-11-00170" class="html-bibr">108</a>]. Copyright (2020): John Wiley &amp; Sons.</p>
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<p>Schematic illustration of (<b>a</b>) the fabricated DOX-loaded TPU-PLGA NPs incorporated into chitosan hydrogel for anticancer drug delivery in HeLa cancer cells. (<b>b</b>) In vitro release profile of TPU-PLGA-DOX NPs and CTP-DOX NP hydrogels. (<b>c</b>) A cell viability assay was performed to analyze the effect of the nano-formulations on HeLa cells using 8.5 μg/mL (IC<sub>50</sub>) DOX. Dunnett’s test was performed for statistical analysis (** <span class="html-italic">p</span> &lt; 0.05, *** <span class="html-italic">p</span> &lt; 0.001). Reproduced with permission [<a href="#B111-gels-11-00170" class="html-bibr">111</a>]. Copyright (2023): Elsevier.</p>
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<p>(<b>a</b>) Schematic illustration of the synthesis and intracellular action mechanism of ZIF@HAgel-GOx. (<b>b</b>) Cell viability plotted against concentration of ZIF-DOX, ZIF-DOX@HA, and ZIF-DOX@HA gel, which were co-incubated with HepG2 cells for 4, 12, and 24 h. (<b>c</b>) Cell viability plotted against concentration of ZIF@HA-GOx, ZIF@HAgel-GOx, and ZIF@HA-BDA-GOx, which were co-incubated with HepG2 cells for 4, 12, and 24 h. *** <span class="html-italic">p</span> &lt; 0.001, ** <span class="html-italic">p</span> &lt; 0.01, and * <span class="html-italic">p</span> &lt; 0.05; ns: not significant. Reproduced with permission [<a href="#B118-gels-11-00170" class="html-bibr">118</a>]. Copyright (2024): American Chemical Society.</p>
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9 pages, 4227 KiB  
Article
Ionic Liquid Capsules as Flame-Retardant Additives for Emulsion Paint Systems
by Rong Ma, Bingqian Wu and Qingsheng Wang
Polymers 2025, 17(5), 626; https://doi.org/10.3390/polym17050626 - 26 Feb 2025
Viewed by 177
Abstract
To develop a highly efficient and environmentally friendly flame-retardant system, ionic liquids (ILs) have recently emerged as promising candidates. However, the addition of ILs into emulsion paint disrupts emulsion stability, leading to rapid demulsification due to electrostatic effects. Herein, IL–silica capsules were developed [...] Read more.
To develop a highly efficient and environmentally friendly flame-retardant system, ionic liquids (ILs) have recently emerged as promising candidates. However, the addition of ILs into emulsion paint disrupts emulsion stability, leading to rapid demulsification due to electrostatic effects. Herein, IL–silica capsules were developed using a soft-template method. These capsules can be directly added to an acrylic emulsion paint system as flame-retardant additives. Incorporating 5 wt% IL–silica capsules into the system and coating it on fabric reduced flammability by 53% compared to untreated fabric. This work provides a novel and practical approach to enhance flame retardancy in emulsion paint systems without compromising their stability. Full article
(This article belongs to the Section Polymer Chemistry)
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<p>The preparation of C12-IL–silica capsules or C18-IL–silica capsules.</p>
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<p>Emulsification behavior of IL/W using (<b>a</b>) Tween 80 (left) and Tween 20 (right) surfactants and (<b>b</b>) amphiphilic GQDs with concentration 0.5, 0.1, 0.05, 0.01 <span class="html-italic">wt</span>% (from left to right) to stabilize for 1 h and 5 h. (<b>c</b>) Microscope images of IL/W emulsions with different concentrations of C12-GQDs: 0.5, 0.1, 0.05, and 0.01 <span class="html-italic">wt</span>% (from left to right).</p>
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<p>Characterization of prepared IL–silica capsules. (<b>a</b>) ATR−FTIR, (<b>b</b>) SEM image, (<b>c</b>) EDS mapping of Si and P, and (<b>d</b>) TGA curves of IL−silica capsules.</p>
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<p>The stability of emulsion paint systems. (<b>a</b>) IL, IL/W Pickering emulsion, and C12-IL–silica capsules in paint (from left to right) 5 min after mixing; (<b>b</b>) IL/W Pickering emulsion (left) and C12-IL–silica capsules in paint (right) 3 h after mixing; C12-IL–silica capsules in paint (<b>c</b>) 24 h and (<b>d</b>) 48 h after mixing.</p>
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<p>MCC result of emulsion paint with loadings of (<b>a</b>) 2.5 wt%, (<b>b</b>) 5 wt%, and (<b>c</b>) 7.5 wt% of IL–silica capsules. (<b>d</b>) Mechanism of IL–silica capsules as flame-retardant additives in emulsion coating system.</p>
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10 pages, 2777 KiB  
Article
An In-Plane Single-Photon Emitter Combining a Triangular Split-Ring Micro-Optical Resonator and a Colloidal Quantum Dot
by Kohki Mukai, Kyosuke Uchiyama, Kohei Iwata and Issei Pribyl
Nanomaterials 2025, 15(5), 335; https://doi.org/10.3390/nano15050335 - 21 Feb 2025
Viewed by 163
Abstract
We propose a simple and innovative configuration consisting of a quantum dot and micro-optical resonator that emits single photons with good directionality in a plane parallel to the substrate. In this device, a single quantum dot is placed as a light source between [...] Read more.
We propose a simple and innovative configuration consisting of a quantum dot and micro-optical resonator that emits single photons with good directionality in a plane parallel to the substrate. In this device, a single quantum dot is placed as a light source between the slits of a triangular split-ring micro-optical resonator (SRR) supported in an optical polymer film with an air-bridge structure. Although most of the previous single photon emitters in solid-state devices emitted photons upward from the substrate, operation simulations confirmed that this configuration realizes lateral light emission in narrow regions above, below, left, and right in the optical polymer film, despite the absence of a light confinement structure such as an optical waveguide. This device can be fabricated using silica-coated colloidal quantum dots, focused ion beam (FIB) lithography, and wet etching using an oxide layer on a silicon substrate as a sacrificial layer. The device has a large tolerance to the variation in the position of the SRR in the optical polymer film and the height of the air-bridge. We confirmed that Pt-SRRs can be formed on the optical polymer film using FIB lithography. This simple lateral photon emitter is suitable for coupling with optical fibers and for fabricating planar optical quantum solid-state circuits, and is useful for the development of quantum information processing technology. Full article
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<p>The proposed single photon emitter with a triangular SRR metamaterial unit arranged around a QD. (<b>a</b>) A bird’s-eye view of the device, and (<b>b</b>) the design dimensions (units in nanometers).</p>
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<p>The simulation results of the light emission characteristics of the device. (<b>a</b>) The resonant 227.6 THz light emission, and (<b>b</b>) the view of the emitted light from the direction of emission, (<b>c</b>) the emitted light pattern showing directivity, and (<b>d</b>) the electric field inside the SRR.</p>
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<p>The effect of the deviation of the structure dimensions on the S11 parameter. (<b>a</b>) The SRR thickness, (<b>b</b>) the length of the nanoantenna close to the SRR, and (<b>c</b>) the length of the nanoantenna far from the SRR.</p>
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<p>The prototype of SRR made of Pt on a PMMA layer. (<b>a</b>) Device dimensions from the top, and (<b>b</b>) device dimensions from the side.</p>
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<p>The effect of increasing the height of the air bridge. (<b>a</b>) The S11 parameter spectrum, (<b>b</b>) the light emission angle.</p>
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14 pages, 5958 KiB  
Article
Effect of Concentration and pH on the Photoluminescent Properties of CQDs Obtained from Actinidia deliciosa
by Carlos Alfredo Zamora-Valencia, María Isabel Reyes-Valderrama, Luis Escobar-Alarcón, Vicente Garibay-Febles and Ventura Rodríguez-Lugo
Crystals 2025, 15(3), 206; https://doi.org/10.3390/cryst15030206 - 21 Feb 2025
Viewed by 259
Abstract
This study investigates the synthesis and photoluminescent properties of carbon quantum dots (CQDs) derived from Actinidia deliciosa using the hydrothermal method. The effect of concentration and pH on the composition, structure, and optical properties of CQDs was analyzed using characterization techniques such as [...] Read more.
This study investigates the synthesis and photoluminescent properties of carbon quantum dots (CQDs) derived from Actinidia deliciosa using the hydrothermal method. The effect of concentration and pH on the composition, structure, and optical properties of CQDs was analyzed using characterization techniques such as TEM, EDS, FTIR, UV-Vis, and photoluminescence (PL) spectroscopy. The CQDs exhibited particle sizes ranging from 1 to 10 nm, with a graphitic structure and oxygen-containing functional groups, as identified by FTIR bands corresponding to OH, C=O, and C=C. The stability analysis revealed particle agglomeration over 30 days, increasing the size up to <40 nm. Regarding the optical properties, the CQDs displayed absorption peaks at 225 and 280 nm and a bandgap of ~3.78–3.82 eV. The PL characterization demonstrated tunable emission from violet to green, depending on the excitation wavelength. CQDs synthesized at an acidic pH of 2 exhibited enhanced luminescence due to protonation effects, whereas an alkaline pH led to a reduction in emission intensity. The hydrothermal method enabled a simple and eco-friendly synthesis, using water as the sole solvent, yielding stable CQDs with a luminescence lifespan exceeding 30 days. Their optical and electronic properties make them promising candidates for photocatalysis, heavy metal detection, and bioimaging applications. Full article
(This article belongs to the Special Issue Advances in Nanocomposites: Structure, Properties and Applications)
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<p>TEM images of CQDs: (<b>a</b>) 1:10, (<b>b</b>) 1:4, (<b>c</b>) 1:2, (<b>d</b>) 1:1.33, (<b>e</b>) 1:1, and (<b>f</b>) sediment for CQDs at 1:1.</p>
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<p>TEM images: (<b>a</b>) HRTEM of CQDs at 1:1, (<b>b</b>) pH 2.00, (<b>c</b>) pH 3.27, (<b>d</b>) pH 4.00, (<b>e</b>) pH 7.00, and (<b>f</b>) pH 10.00.</p>
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<p>EDS characterization of CQDs varying by (<b>a</b>) concentration and (<b>b</b>) pH.</p>
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<p>FTIR spectra of CQDs varying by (<b>a</b>) concentration and (<b>b</b>) pH.</p>
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<p>UV-Vis spectra of CQDs varying by (<b>a</b>) concentration and (<b>b</b>) pH, and the Tauc method varying by (<b>c</b>) concentration and (<b>d</b>) pH. Additionally, the arrows indicate the value of the band gap at the intersection with the x-axis.</p>
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<p>Scanning at different excitation wavelengths of CQDs.</p>
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<p>PL spectra of the CQDs varying by concentration at (<b>a</b>) day 0 and (<b>b</b>) day 30, and varying pH at (<b>c</b>) day 0 and (<b>d</b>) day 30.</p>
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<p>(<b>a</b>) Scheme of the loss of luminescence intensity in 30 days between varying concentrations: (<b>b</b>) scheme of concentration and effect of luminescence, (<b>c</b>) scheme of luminescence intensity loss in 30 days by varying the pH, and (<b>d</b>) scheme of pH and effect of luminescence.</p>
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<p>Scheme of luminescence mechanisms of CQDs: (<b>a</b>) band transition and (<b>b</b>) surface modification.</p>
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21 pages, 2799 KiB  
Article
Numerical Simulation and Hole Transport Layers Optimization of a Lead Sulfide-Based Solar Cell with a Power Conversion Efficiency of Above 22%
by Edson L. Meyer, Inam Vulindlela, Athandwe Paca, Mojeed A. Agoro and Nicholas Rono
Coatings 2025, 15(3), 255; https://doi.org/10.3390/coatings15030255 - 20 Feb 2025
Viewed by 236
Abstract
Recently, the numerical simulation of solar cells has attracted tantamount scientific attention in the photovoltaic community because it saves on research time and resources before the actual fabrication of the devices in the laboratories. Despite significant advancements in the fabrication of quantum dot-sensitized [...] Read more.
Recently, the numerical simulation of solar cells has attracted tantamount scientific attention in the photovoltaic community because it saves on research time and resources before the actual fabrication of the devices in the laboratories. Despite significant advancements in the fabrication of quantum dot-sensitized solar cells (QDSSCs), the power conversion efficiency (PCE) is still low when compared to other solar cells such as perovskite. This efficiency gap poses a substantial challenge in harnessing the full potential of QDSSCs for widespread adoption in renewable energy applications. Enhancing the efficiency of QDSSCs is imperative for their commercial viability and widespread deployment. In this work, SCAPS-1D was used in the simulation of QDSSCs. The solar cell with a general configuration of FTO/TiO2/PbS/HTL/Au was investigated. In the device, PbS quantum dots were inserted as the absorber layer, TiO2 as the electron transport layer (ETL), gold as the back contact, and the following inorganic materials, i.e., copper (I) iodide (CuI), copper (I) oxide (Cu2O), cadmium zinc telluride selenide (CZTSe), copper iron tin sulfide (CFTS), and copper zinc tin sulfide selenide (CZTSSe) were tested as HTL materials, and FTO acted as the conductive substrate. The best HTL material (CZTSSe) exhibited a PCE of 22.61%, with a fill factor (FF) of 84.67%, an open circuit voltage (Voc) of 0.753 V, and a current density (Jsc) of 35.48 mA cm−2. This study contributes to the field by employing SCAPS-1D simulations to optimize QDSSCs, exploring novel inorganic HTL materials for these solar cells and identifying CZTSSe as a promising low-cost HTL that significantly enhances both the performance and commercial viability of QDSSCs. Full article
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<p>(<b>a</b>) Architecture of PbS-based quantum dot solar cells and (<b>b</b>) band alignment diagram of the device.</p>
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<p>Quantum efficiency characteristics of the PbS-based device with various HTL materials.</p>
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<p>J-V curve of the PbS-based device with various HTL materials.</p>
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<p>Impact of changing the thickness of the PbS absorber layer on device performance: (<b>a</b>) efficiency and FF, and (<b>b</b>) J<sub>sc</sub> and V<sub>oc</sub>.</p>
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<p>Influence of varying temperature on devices with CFTS and CZTSSe as the HTL materials on (<b>A</b>) efficiency (<b>B</b>) FF, (<b>C</b>) V<sub>oc</sub> and (<b>D</b>) J<sub>sc</sub>.</p>
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<p>The impact of varying the series resistance for devices with CFTS and CZTSSe as the HTL materials on the (<b>A</b>) efficiency, (<b>B</b>) FF, (<b>C</b>) V<sub>oc</sub>, and (<b>D</b>) J<sub>sc</sub>.</p>
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<p>The impact of varying the shunt resistance for devices with CFTS and CZTSSe as HTL materials on the (<b>A</b>) efficiency, (<b>B</b>) FF, (<b>C</b>) V<sub>oc</sub>, and (<b>D</b>) J<sub>sc</sub>.</p>
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<p>The impact of variations in the HTL’s doping density on the performance of the solar device: (<b>a</b>) efficiency, (<b>b</b>) FF, (<b>c</b>) V<sub>oc</sub>, and (<b>d</b>) J<sub>sc</sub>.</p>
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<p>Effects of different metal back contacts on PbS-based devices’ photovoltaic performance. Efficiency and FF in (<b>a</b>), V<sub>oc</sub> and J<sub>sc</sub> in (<b>b</b>).</p>
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17 pages, 3109 KiB  
Article
Surface Grafting of Graphene Flakes with Fluorescent Dyes: A Tailored Functionalization Approach
by Ylea Vlamidis, Carmela Marinelli, Aldo Moscardini, Paolo Faraci, Stefan Heun and Stefano Veronesi
Nanomaterials 2025, 15(5), 329; https://doi.org/10.3390/nano15050329 - 20 Feb 2025
Viewed by 288
Abstract
The controlled functionalization of graphene is critical for tuning and enhancing its properties, thereby expanding its potential applications. Covalent functionalization offers a deeper tuning of the geometric and electronic structure of graphene compared to non-covalent methods; however, the existing techniques involve side reactions [...] Read more.
The controlled functionalization of graphene is critical for tuning and enhancing its properties, thereby expanding its potential applications. Covalent functionalization offers a deeper tuning of the geometric and electronic structure of graphene compared to non-covalent methods; however, the existing techniques involve side reactions and spatially uncontrolled functionalization, pushing research toward more selective and controlled methods. A promising approach is 1,3-dipolar cycloaddition, successfully utilized with carbon nanotubes. In the present work, this method has been extended to graphene flakes with low defect concentration. A key innovation is the use of a custom-synthesized ylide with a protected amine group (Boc), facilitating subsequent attachment of functional molecules. Indeed, after Boc cleavage, fluorescent dyes (Atto 425, 465, and 633) were covalently linked via NHS ester derivatization. This approach represents a highly selective method of minimizing structural damage. Successful functionalization was demonstrated by Raman spectroscopy, photoluminescence spectroscopy, and confocal microscopy, confirming the effectiveness of the method. This novel approach offers a versatile platform, enabling its use in biological imaging, sensing, and advanced nanodevices. The method paves the way for the development of sensors and devices capable of anchoring a wide range of molecules, including quantum dots and nanoparticles. Therefore, it represents a significant advancement in graphene-based technologies. Full article
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<p>Schematic flowchart describing the multi-step functionalization of graphene flakes with fluorescent molecules.</p>
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<p>(<b>a</b>) AFM topography with (<b>b</b>) height profile along the white line indicated in (<b>a</b>). (<b>c</b>,<b>d</b>) SEM images at different magnification of the graphene flakes drop-cast on Si/SiO<sub>2</sub> from a chloroform suspension.</p>
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<p>(<b>a</b>) Representative normalized Raman spectra acquired from pristine and linker-functionalized graphene flakes on Si/SiO<sub>2</sub>. The inset shows a histogram of the I(D)/I(G) peak intensity ratio extracted from the Raman spectra (statistical analysis of 75 spectra acquired from different flakes). Histogram colors are used according to the colors of the curves shown in panel (<b>a</b>). (<b>b</b>) Optical bright field microscopy image (100× objective) of functionalized graphene flakes drop-casted onto a silica substrate for Raman measurements.</p>
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<p>(<b>a</b>) PL spectra acquired at 473 nm excitation for Atto 465-labeled graphene flakes and the pristine sample. (<b>b</b>) PL spectra of functionalized graphene flakes (black curve) and control samples: graphene flakes functionalized with only the linker molecule (red line) and graphene flakes not subjected to the first reaction step (no linker), merely kept in contact with the fluorophore (blue line). (<b>c</b>) Normalized fluorescence spectra acquired with a confocal microscope under excitation at 470 nm, showing the graphene flakes before and after functionalization with Atto 465 NHS. The inset in panel (<b>c</b>) shows a fluorescence image of the flakes. (<b>d</b>) Normalized fluorescence decay curves of the sample functionalized with Atto 465 compared to the pure fluorophores in chloroform (3 μg μL<sup>−1</sup>), obtained from FLIM images.</p>
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<p>Fluorescence spectra of graphene flakes functionalized with (<b>a</b>) Atto 425 NHS and (<b>b</b>) Atto 633 NHS compared with the blank signal. The data were acquired with a confocal microscope under excitation at 440 nm and 640 nm, respectively. The insets show representative fluorescence images of the flakes.</p>
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<p>Schematic of synthesis of the linker molecule (Boc-protected amino groups) from hexamethylenediamine.</p>
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<p>Schematic representation of the functionalization reactions: reaction mechanism of the 1,3-DC between the linker and the graphene flakes and attachment of a fluorophore to the linker molecule after deprotection of the amino group.</p>
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12 pages, 6817 KiB  
Article
Synthesis of Eco-Friendly Narrow-Band CuAlSe2/Ga2S3/ZnS Quantum Dots for Blue Quantum Dot Light-Emitting Diodes
by Shenghua Yuan, Liyuan Liu, Xiaofei Dong, Xianggao Li, Shougen Yin and Jingling Li
Coatings 2025, 15(2), 245; https://doi.org/10.3390/coatings15020245 - 19 Feb 2025
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Abstract
Quantum dot light-emitting diodes (QLEDs) based on high-color-purity blue quantum dots (QDs) are crucial for the development of next-generation displays. I-III-VI type QDs have been recognized as eco-friendly luminescent materials for QLED applications due to their tunable band gap and high-stable properties. However, [...] Read more.
Quantum dot light-emitting diodes (QLEDs) based on high-color-purity blue quantum dots (QDs) are crucial for the development of next-generation displays. I-III-VI type QDs have been recognized as eco-friendly luminescent materials for QLED applications due to their tunable band gap and high-stable properties. However, efficient blue-emitting I-III-VI QDs remain rare owing to the high densities of the intrinsic defects and the surface defects. Herein, narrow-band blue-emissive CuAlSe2/Ga2S3/ZnS QDs is synthesized via a facile strategy. The resulting QDs exhibit a sharp blue emission peak at 450 nm with a full width at half maximum (FWHM) of 35 nm, achieved by coating a double-shell structure of Ga2S3 and ZnS, which is associated with the near-complete passivation of Cu-related defects (e.g., Cu vacancies) that enhances the band-edge emission, accompanied by an improvment in photoluminescence quantum yield up to 69%. QLEDs based on CuAlSe2/Ga2S3/ZnS QDs are fabricated, exhibiting an electroluminescence peak at 453 nm with a FWHM of 39 nm, a current efficiency of 3.16 cd A−1, and an external quantum efficiency of 0.35%. This research paves the way for the development of high-efficiency eco-friendly blue QLEDs. Full article
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Figure 1

Figure 1
<p>HRTEM images of (<b>a</b>) CuAlSe<sub>2</sub>, (<b>b</b>) CuAlSe<sub>2</sub>/Ga<sub>2</sub>S<sub>3</sub>, and (<b>c</b>) CuAlSe<sub>2</sub>/Ga<sub>2</sub>S<sub>3</sub>/ZnS QDs; (<b>d–f</b>) the corresponding size distribution histograms.</p>
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<p>XRD patterns of CuAlSe<sub>2</sub>, CuAlSe<sub>2</sub>/Ga<sub>2</sub>S<sub>3</sub>, and CuAlSe<sub>2</sub>/Ga<sub>2</sub>S<sub>3</sub>/ZnS QDs.</p>
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<p>(<b>a</b>) UV-Vis absorption spectra of CuAlSe<sub>2</sub>, CuAlSe<sub>2</sub>/Ga<sub>2</sub>S<sub>3</sub>, and CuAlSe<sub>2</sub>/Ga<sub>2</sub>S<sub>3</sub>/ZnS QDs; (<b>b</b>) the corresponding (α<span class="html-italic">һν</span>)<sup>2</sup> (where α represent absorption coefficient) as a function of photon energy (<span class="html-italic">һν</span>).</p>
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<p>(<b>a</b>) Normalized PL spectra of CuAlSe<sub>2</sub>, CuAlSe<sub>2</sub>/Ga<sub>2</sub>S<sub>3</sub>, and CuAlSe<sub>2</sub>/Ga<sub>2</sub>S<sub>3</sub>/ZnS QDs monitored at an excitation wavelength of 370 nm; (<b>b</b>) the corresponding statistical distributions of PL quantum yield (PL QY) for the 8 QDs.</p>
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<p>(<b>a–c</b>) PL spectra of CuAlSe<sub>2</sub> and CuAlSe<sub>2</sub>/Ga<sub>2</sub>S<sub>3</sub> resolved into three subspectra, along with CuAlSe<sub>2</sub>/Ga<sub>2</sub>S<sub>3</sub>/ZnS QDs resolved into two subspectra; (<b>d</b>) the corresponding decomposed emission peaks via Gaussian fitting.</p>
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<p>(<b>a</b>) PL decay traces of CuAlSe<sub>2</sub>, CuAlSe<sub>2</sub>/Ga<sub>2</sub>S<sub>3</sub>, and CuAlSe<sub>2</sub>/Ga<sub>2</sub>S<sub>3</sub>/ZnS QDs monitored at the emission wavelengths of 458, 455, and 450 nm, respectively; (<b>b</b>) TG-DSC curves of CuAlSe<sub>2</sub>/Ga<sub>2</sub>S<sub>3</sub>/ZnS QDs.</p>
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<p>(<b>a</b>) Schematic structure of device C with CuAlSe<sub>2</sub>/Ga<sub>2</sub>S<sub>3</sub>/ZnS QDs as EML; (<b>b</b>) EL spectrum of CuAlSe<sub>2</sub>/Ga<sub>2</sub>S<sub>3</sub>/ZnS QDs-based blue QLEDs and the corresponding PL spectrum; (<b>c</b>) <span class="html-italic">J</span>-<span class="html-italic">L</span>-<span class="html-italic">V</span> curves of QLEDs; (<b>d</b>) Current efficiency and external quantum efficiency <span class="html-italic">versus</span> current density characteristics of the device.</p>
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