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Keywords = tunability of emission wavelength

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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
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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Figure 1
<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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10 pages, 2021 KiB  
Communication
Stable Fluorenyl Radicals Showing Tunable Doublet Emission
by Xudong Hou, Tingting Xu, Jun Zhu, Shaofei Wu and Jishan Wu
Chemistry 2025, 7(1), 21; https://doi.org/10.3390/chemistry7010021 - 7 Feb 2025
Abstract
Neutral organic radicals with intrinsic spin-allowed doublet emission have emerged as a promising class of luminescent materials, garnering significant research interest. However, the development of stable luminescent radicals with tunable emission remains challenging. Herein, we present the synthesis of a series of 9-(2,4,6-trichlorophenyl)-substituted [...] Read more.
Neutral organic radicals with intrinsic spin-allowed doublet emission have emerged as a promising class of luminescent materials, garnering significant research interest. However, the development of stable luminescent radicals with tunable emission remains challenging. Herein, we present the synthesis of a series of 9-(2,4,6-trichlorophenyl)-substituted fluorenyl radicals functionalized with various substituents at the 3,6-positions. These radicals exhibit enhanced stability through efficient spin delocalization and kinetic protection. Notably, they display red-shifted photoluminescence compared to traditional polychlorotriphenylmethyl radicals, with maximum emission wavelengths ranging from 679 nm to 744 nm. The mechanisms underlying the doublet emission, as well as their electrochemical properties, have been thoroughly investigated. Full article
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Graphical abstract

Graphical abstract
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<p>The structures of some reported stable radicals with room-temperature doublet emission, and the new luminescent fluorenyl radicals in this report.</p>
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<p>(<b>a</b>) UV−vis absorption and normalized fluorescence (FL) spectra of <b>FL-R1</b>, <b>FL-R2</b>, <b>FL-R3</b>, and <b>FL-R4</b> measured in DCM. The excitation wavelengths for FL are 380, 384, 389, and 371 nm, respectively; (<b>b</b>) cyclic voltammograms of <b>FL-R1</b>, <b>FL-R2</b>, <b>FL-R3</b>, and <b>FL-R4</b> measured in DCM (with 0.1 M <span class="html-italic">n</span>Bu<sub>4</sub>N•PF<sub>6</sub> as supporting electrolyte, scan rate: 100 mV/s); (<b>c</b>) ESR spectrum of <b>FL-R1</b> recorded in DCM at room temperature; (<b>d</b>) calculated (UB3LYP/6-31G(d,p)) spin-density distribution map for the <b>FL-R1</b>.</p>
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<p>(<b>a</b>) The calculated (UB3LYP/6-31G(d,p)) frontier molecular orbital profiles and energy diagram of <b>FL-R1</b>; (<b>b</b>) a summary of the calculated UB3LYP/6-31G(d,p)) energy diagrams of <b>FL-R1</b>, <b>FL-R2</b>, <b>FL-R3</b>, and <b>FL-R4</b>.</p>
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<p>The time-dependent decay of the absorbance at the absorption maximums of <b>FL-R1</b>, <b>FL-R2</b>, <b>FL-R3</b>, and <b>FL-R4</b> in DCM (1 × 10<sup>−4</sup> M) under ambient air and light conditions.</p>
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<p>The synthetic route of the new fluorenyl radicals.</p>
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27 pages, 10263 KiB  
Review
Recent Advances and Challenges in Metal Halide Perovskite Quantum Dot-Embedded Hydrogels for Biomedical Application
by Junyi Yu, Chengran Zhang, Lijun Kong and Zhengtao Deng
Molecules 2025, 30(3), 643; https://doi.org/10.3390/molecules30030643 - 31 Jan 2025
Abstract
Metal halide perovskite quantum dots (MHP QDs), as a kind of fluorescent material, have attracted much attention due to their excellent photoluminescence (PL) quantum yield (QY), narrow full width at half maximum (FWHM), broad absorption, and tunable emission wavelength. However, the instability and [...] Read more.
Metal halide perovskite quantum dots (MHP QDs), as a kind of fluorescent material, have attracted much attention due to their excellent photoluminescence (PL) quantum yield (QY), narrow full width at half maximum (FWHM), broad absorption, and tunable emission wavelength. However, the instability and biological incompatibility of MHP QDs greatly hinder their application in the field of biomedicine. Hydrogels are three-dimensional polymer networks that are widely used in biomedicine because of their high transparency and excellent biocompatibility. This review not only introduces the latest research progress in improving the mechanical and optical properties of hydrogels/MHP QDs but also combines it with the existing methods for enhancing the stability of MHP QDs in hydrogels, aiming to provide new ideas for researchers in material selection and methods for constructing MHP QD-embedded hydrogels. Finally, their application prospects and future challenges are introduced. Full article
(This article belongs to the Special Issue Emerging Topics in Luminescent Materials)
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<p>The luminous mechanism of MHP QDs.</p>
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<p>The application prospects of hydrogels.</p>
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<p>The application of visual-digital strain sensors with stretchable luminescent perovskite-polymer hydrogels. (<b>a</b>) Schematic diagram of the synthesis process of perovskite-based fluorescent hydrogels. (<b>b</b>) The design concept of the stretchable visual-digital strain sensor textile. Reprinted with permission from ref. [<a href="#B54-molecules-30-00643" class="html-bibr">54</a>]. Copyright 2023 Springer Nature.</p>
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<p>The design of the all-dipole fluorine elastomer using the copolymer of 2,2,2-trifluoroethyl methacrylate (TFEMA) and 2,2,3,4,4,4-hexafluorobutyl acrylate (HFBA) to protect the QDs (namely, TFE-HF-QD). Reprinted with permission from ref. [<a href="#B57-molecules-30-00643" class="html-bibr">57</a>]. Copyright 2022 Springer Nature.</p>
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<p>(<b>a</b>) Schematic diagram of sensing for monitoring of organophosphorus pesticides. (<b>b</b>) Feasibility of sensing principle. (<b>c</b>) Comparison of detection limit of sensing platform with other methods. (<b>d</b>) Schematic diagram of PMCP PNC-based hydrogel-sensing platform. (<b>e</b>) SEM image of PMCP PNC-based hydrogel surface (<b>left</b>) and intersecting surface (<b>right</b>). The circles in subfigure are for PNCs. (<b>f</b>) Element mapping of PMCP PNC-based hydrogel. (<b>g</b>) Comparison of PL intensity between liquid-phase sensing platform and hydrogel-sensing platform. Reprinted with permission from ref. [<a href="#B58-molecules-30-00643" class="html-bibr">58</a>]. Copyright 2024 WILEY.</p>
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<p>(<b>a</b>) Schematic of One-Pot Sequential Synthesis of OEG/PAAm Double-Network Hydrogels. (<b>b</b>) Self-healing properties of the sacrificial network in the OEG/PAAm DN hydrogel. (<b>a</b>,<b>b</b>) Second cyclic loading–unloading curves of specimens annealed at 25 °C (<b>a</b>) and 50 °C (<b>b</b>) for different times after first cycle. The curves marked “original” are first cyclic loading–unloading curves. (<b>c</b>,<b>d</b>) Waiting time dependence of recovery ratios of Young’s modulus (<b>c</b>) and dissipation energy (<b>d</b>) of OEG/PAAm DN hydrogels. The OEG content and MBAA concentration in gels are 5 wt.% and 0.1% of AAm in moles, respectively. Measurements are performed at 25 °C. Reprinted with permission from ref. [<a href="#B96-molecules-30-00643" class="html-bibr">96</a>]. Copyright 2022 American Chemical Society.</p>
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<p>(<b>a</b>,<b>b</b>) WAXS and SAXS patterns of SR0.18 (<b>a</b>) and SR-0.38 (<b>b</b>) during a loading–unloading cycle. The white double arrows denote the stretching direction. (<b>c</b>) WAX profiles of SR-0.18 and SR-0.38 gels in the direction perpendicular to stretching. (<b>d</b>) Structure of planar zigzag PEG and its triclinic crystal. (<b>e</b>) Structure of 7/2 helix PEG and its monoclinic crystal. Reprinted with permission from ref. [<a href="#B102-molecules-30-00643" class="html-bibr">102</a>]. Copyright 2021 AAAS.</p>
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<p>(<b>a</b>) TEM image of CsPbBr<sub>3</sub>/ZnS core/shell NCs showing cubic morphology. Inset shows HRTEM image of an NC near the core/shell interface. (<b>b</b>) UV–visible absorption and PL spectra showing little red shift for CsPbBr<sub>3</sub>/ZnS core/shell NCs. (<b>c</b>) Comparison of PL decay shows a huge increase in PL lifetime for CsPbBr<sub>3</sub>/ZnS core/shell NCs. (<b>d</b>) Schematic showing pseudo type-II band alignment at the CsPbBr<sub>3</sub>/ZnS core/shell interface, where the electron is confined inside the core but the hole is delocalized over both core and shell. (<b>e</b>) PL decay of CsPbBr<sub>3</sub>/ZnS core/shell NCs film deposited on glass, TiO<sub>2</sub>, and spiro-OMeTAD. (<b>f</b>) Digital photographs of the films of CsPbBr<sub>3</sub>/ZnS core/shell NCs and CsPbBr<sub>3</sub>–OAmBr NCs dipped in beakers full of water and excited with UV lamp (365 nm). Reprinted with permission from ref. [<a href="#B123-molecules-30-00643" class="html-bibr">123</a>]. Copyright 2020 American Chemical Society.</p>
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<p>(<b>a</b>) Schematic diagram of PMCP PNC formation. (<b>b</b>) TEM image and corresponding size distribution of PMCP PNCs. (<b>c</b>) HRTEM images of PMCP PNCs. The two crystal lattices show that PNCs have a heterogeneous core/shell structure. (<b>d</b>) SAED of PMCP PNCs. The two diffraction rings show the coexistence of CsPbCl<sub>3</sub>/CsPb<sub>2</sub>Cl<sub>5</sub> heterostructures in PNCs. (<b>e</b>) XRD images of PMCP PNCs. (<b>f</b>) FTIR spectra of PMCP PNCs, OA, OLA, and NH<sub>2</sub>-PEG-COOH. (<b>g</b>) UV-vis spectrum and PL spectrum of PMCP PNCs. (<b>h</b>) Storage stability of PMCP PNCs, PNCs without Mn<sup>2+</sup>, and PNCs without NH<sub>2</sub>-PEG-COOH in solutions. (<b>i</b>) Water stability of PMCP PNCs under 70 °C heat treatment for 240 min. (<b>j</b>) Biological toxicity of PMCP PNCs in Hela and Huvec cells. (<b>k</b>) Trinity strategies for improving the stability of PMCP PNCs. (<b>l</b>) PL intensity of PMCP PNCs in air, N<sub>2</sub>, and O<sub>2</sub> environments. Reprinted with permission from ref. [<a href="#B58-molecules-30-00643" class="html-bibr">58</a>]. Copyright 2024 WILEY.</p>
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<p>(<b>a</b>–<b>d</b>) Photographs of CsPbBr<sub>3</sub> QDs and CsPbBr<sub>3</sub>/CsPb<sub>2</sub>Br<sub>5</sub> core–shell QDs excited at 365 nm in water and ethanol atmosphere. (<b>e</b>,<b>f</b>) Absorption spectra and PL spectra of CsPbBr<sub>3</sub> QDs and CsPbBr<sub>3</sub>/CsPb<sub>2</sub>Br<sub>5</sub> core–shell QDs, before and after ethanol being added, respectively. (<b>g</b>,<b>h</b>) The crystal structure of CsPbBr<sub>3</sub> and CsPb<sub>2</sub>Br<sub>5</sub>. Reprinted with permission from ref. [<a href="#B131-molecules-30-00643" class="html-bibr">131</a>]. Copyright 2017 IOP Publishing Ltd.</p>
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<p>(<b>a</b>) Schematic diagrams of X, Z, and L-type ligands. Reprinted with permission from ref. [<a href="#B136-molecules-30-00643" class="html-bibr">136</a>]. Copyright2018 American Chemical Society. (<b>b</b>) Schematic illustration of the dynamic stability of brominated oleylamine on the surface of PQDs. Reprinted with permission from ref. [<a href="#B138-molecules-30-00643" class="html-bibr">138</a>]. Copyright2016 American Chemical Society. (<b>c</b>) The effect of different carbon chain lengths on the synthesis of PQDs. (<b>d</b>) Schematic diagrams of oleic acid, oleylamine, and sulfonic acid as ligands for PQDs. Reprinted with permission from ref. [<a href="#B140-molecules-30-00643" class="html-bibr">140</a>]. Copyright2019 John Wiley and Sons.</p>
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<p>(<b>a</b>) Schematic diagram of the formation process of CsPbBr<sub>3</sub>/SiO<sub>2</sub> NCs and their water resistance stability. Reprinted with permission from ref. [<a href="#B141-molecules-30-00643" class="html-bibr">141</a>]. Copyright2023 American Chemical Society. (<b>b</b>) Preparation of CsPbBr<sub>3</sub>@PMMA composite fluorescent microspheres via electrospray and their water stability. Reprinted with permission from ref. [<a href="#B142-molecules-30-00643" class="html-bibr">142</a>]. Copyright2021 Elsevier BV. (<b>c</b>) Water stability of CsPbBr<sub>3</sub>@PS-PAA composites. Reprinted with permission from ref. [<a href="#B143-molecules-30-00643" class="html-bibr">143</a>]. Copyright2021 Elsevier BV. (<b>d</b>) CTAB-CsPbBr<sub>3</sub> composites exhibiting enhanced water resistance and thermal stability. Reprinted with permission from ref. [<a href="#B144-molecules-30-00643" class="html-bibr">144</a>]. Copyright2021 Springer-Verlag GmbH Germany. (<b>e</b>) CsPbBr<sub>3</sub>@PDMS microspheres demonstrating excellent optical performance and stability in water, acid, and alkaline solutions. Reprinted with permission from ref. [<a href="#B55-molecules-30-00643" class="html-bibr">55</a>]. Copyright2017 American Chemical Society.</p>
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40 pages, 9917 KiB  
Review
Roadmap for Designing Donor-π-Acceptor Fluorophores in UV-Vis and NIR Regions: Synthesis, Optical Properties and Applications
by Guliz Ersoy and Maged Henary
Biomolecules 2025, 15(1), 119; https://doi.org/10.3390/biom15010119 - 14 Jan 2025
Viewed by 597
Abstract
Donor acceptor (D-π-A) fluorophores containing a donor unit and an acceptor moiety at each end connected by a conjugated linker gained attention in the last decade due to their conjugated system and ease of tunability. These features make them good candidates [...] Read more.
Donor acceptor (D-π-A) fluorophores containing a donor unit and an acceptor moiety at each end connected by a conjugated linker gained attention in the last decade due to their conjugated system and ease of tunability. These features make them good candidates for various applications such as bioimaging, photovoltaic devices and nonlinear optical materials. Upon excitation of the D-π-A fluorophore, intramolecular charge transfer (ICT) occurs, and it polarizes the molecule resulting in the ‘push–pull’ system. The emission wavelengths of fluorophores can be altered from UV-vis to NIR region by modifying the donor unit, acceptor moiety and the π linker between them. The NIR emitting fluorophores with restricted molecular rotations are used in aggregation-induced emission (AIE). D-π-A fluorophores with carboxylic acid and cyano groups are preferred in photovoltaic applications, and fluorophores with large surface area are used for two photon absorbing applications. Herein, we report the synthesis, optical properties, and applications of various D-π-A fluorophores in UV-vis and NIR region. Full article
(This article belongs to the Special Issue Novel Materials for Biomedical Applications: 2nd Edition)
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<p>Representation of D-π-A fluorophores.</p>
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<p>Representation of the D-<math display="inline"><semantics> <mrow> <mi mathvariant="sans-serif">π</mi> </mrow> </semantics></math>-A system containing SF<sub>5</sub>.</p>
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<p>D-<math display="inline"><semantics> <mrow> <mi mathvariant="sans-serif">π</mi> </mrow> </semantics></math>-A dyes’ diphenylamino donor, SF<sub>5</sub> acceptor and different π linkers.</p>
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<p>Energy band gap of fluorophores with SF<sub>5</sub> acceptor from <b>1a</b>–<b>f</b> [<a href="#B9-biomolecules-15-00119" class="html-bibr">9</a>].</p>
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<p>Tripodal and quadrupolar donor acceptor structures.</p>
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<p>Structures of fluorophores with triphenylamine core.</p>
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<p>Structure of fluorene containing fluorophores.</p>
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<p>Structure of BODIPY unit.</p>
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<p>Electronic diagram showing one- and two-photon absorption processes.</p>
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<p>(<b>A</b>) HeLa cells stained with carbazole containing fluorophores <b>63</b>, <b>64</b>, <b>68</b> and <b>69</b> (from left to right), Mitotracker Green and merged images. (<b>B</b>) Fluorescence images of normal cells (HLF and LX2) and cancer cells (HepG2, B16, A549 and HeLa) stained with fluorophore <b>69</b> (1 <math display="inline"><semantics> <mrow> <mo> </mo> <mi mathvariant="sans-serif">μ</mi> </mrow> </semantics></math>M). (<b>C</b>) Relative fluorescence intensity of different cells incubated with fluorophore <b>69</b> for 30 min. (Reproduced from open access article [<a href="#B49-biomolecules-15-00119" class="html-bibr">49</a>]).</p>
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<p>NIR-II images of (<b>a</b>) mouse hind limb (<b>c</b>) brain. Emission intensity profiles of the images (<b>a</b>,<b>c</b>), respectively, in (<b>b</b>,<b>d</b>), (<b>e</b>) NIR-II images of 4T1 tumor at different times after the injection, (<b>f</b>) ex vivo studies of fluorophore <b>113</b> NPs at 4 h under 808 nm laser radiation, (<b>g</b>) signal-to-background ratio of tumor at different times. (Reproduced with permission from [<a href="#B72-biomolecules-15-00119" class="html-bibr">72</a>]).</p>
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<p>Fluorescence microscopy images of A549 cells with DAPI, (<b>a</b>) styryl dye with pyridinium acceptor and (<b>b</b>) styryl dye with quinolinium acceptor. Image reproduced from open access article [<a href="#B102-biomolecules-15-00119" class="html-bibr">102</a>].</p>
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<p>Cytotoxicity data of fluorophores <b>131</b>–<b>134</b> compared to docetaxel, against triple negative breast cancer cell lines (image reproduced from [<a href="#B15-biomolecules-15-00119" class="html-bibr">15</a>]).</p>
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<p>Emission profiles of probes containing quinolinium units <b>140</b> (Probe A) and <b>141</b> (Probe B), each with 10 <math display="inline"><semantics> <mrow> <mi mathvariant="sans-serif">μ</mi> </mrow> </semantics></math>M, in varying NADH concentrations of 0–50 μ M in pH 7.4 phosphate buffer containing 10% DMSO. (Image reproduced with permission from [<a href="#B102-biomolecules-15-00119" class="html-bibr">102</a>]).</p>
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<p>Synthesis of dyes <b>1a</b>, <b>1c</b> and <b>1f</b> via Suzuki and Heck coupling reactions.</p>
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<p>Synthesis of 2iazine c2ntaining fluorophores <b>5</b>–<b>7</b>.</p>
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<p>Synthesis of chromophores with TT linker system.</p>
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<p>Synthesis of fluorophores using TT as donor group.</p>
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<p>Synthesis of triphenylamine core structures.</p>
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<p>Synthesis of fluorophores with pyrimidine acceptor core.</p>
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<p>Synthesis of fluorophores with pyrimidine core as acceptor unit.</p>
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<p>Synthesis of tripolar fluorophore with pyrimidine acceptor core.</p>
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<p>Synthesis of fluorene containing fluorophores.</p>
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<p>Synthesis of D-π-A fluorophores with benzothiazole and diphenylamino groups.</p>
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<p>Synthesis of fluorophores <b>51a</b>–<b>c</b> with carbazole donor unit.</p>
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<p>Synthesis of fluorophores <b>55</b>–<b>57</b> with alternating length of thiophene bridge.</p>
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<p>Synthesis of fluorophores <b>61a</b> and <b>61b</b> with thiophene linker.</p>
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<p>Synthesis of fluorophores <b>63</b> and <b>64</b> with carbazole donor unit.</p>
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<p>Synthesis of fluorophores <b>68</b> and <b>69</b> with carbazole linker unit.</p>
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<p>Synthesis of monoiodinated and diiodinated carbazole moieties.</p>
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<p>Synthesis of star-shaped carbazole donor containing fluorophores.</p>
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<p>Synthesis of fluorophores <b>83a</b>,<b>b</b> and <b>86a</b>,<b>b</b> with tetracyano acceptor group.</p>
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<p>Quinoxaline linker containing fluorophores with cyanoacetic acid acceptor unit and bulky donor units.</p>
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<p>Synthesis of EDOT containing fluorophores <b>93</b>–<b>95</b>.</p>
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<p>Synthesis of fluorophores <b>97</b>–<b>99</b> with TCF acceptor unit.</p>
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<p>Synthesis of tetracyano moiety containing fluorophores.</p>
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<p>Synthesis of aza-BODIPY dyes with CF<sub>3</sub>, CN, NMe<sub>2</sub> and NMe<sub>3</sub><sup>+</sup> groups <b>106</b>–<b>109</b>.</p>
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<p>Synthesis of aza-BODIPY fluorophores in NIR-II region.</p>
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<p>Synthesis of fluorophores with phenothiazine donor <b>120</b> and <b>121</b>.</p>
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<p>Synthesis of phenothiazine fluorophores.</p>
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<p>Synthesis of fluorophores <b>131</b>–<b>137</b> with chloroacrylic acid moiety.</p>
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15 pages, 4833 KiB  
Article
Fluorescent Polymers via Coordination of bis-Terpyridine Ligands with Transition Metals and Their pH Response Properties
by Tao Zhang, Fengxue Liu, Yongxin Liu, Kaixiu Li, Zhengguang Li, Yaqin Li, Fan Fu, Mingliang Liu, Yiming Li, Die Liu and Pingshan Wang
Polymers 2025, 17(1), 87; https://doi.org/10.3390/polym17010087 - 31 Dec 2024
Viewed by 643
Abstract
Stimulus-responsive luminescent materials are pivotal in the field of sensing. Fluorescent transition metal complexes with a charge transfer excited state, especially terpyridine-coordinated polymers, are of particular interest due to their tunable emission. In this paper, a novel bis-terpyridine ligand was synthesized and assembled [...] Read more.
Stimulus-responsive luminescent materials are pivotal in the field of sensing. Fluorescent transition metal complexes with a charge transfer excited state, especially terpyridine-coordinated polymers, are of particular interest due to their tunable emission. In this paper, a novel bis-terpyridine ligand was synthesized and assembled into a coordination polymer, which showed intense visible light absorption and fluorescence emission in the solid state that could be regulated by an acidic or basic pH. After being protonated by acid, the fluorescence of the polymer P2 was quenched. The emission of the polymer split from 635 nm to two peaks of 674 and 440 nm, and then stabilized at 728 nm for 7 days, which showed a significant red-shift and good protonation stability. The fluorescence emission wavelength of the protonated polymers recovered after alkalization, and the fluorescence intensity of the polymer was greatly improved after alkalization, showing interesting acid–base-response luminescence characteristics. The sensitive response of the synthesized coordination polymers to acids and bases will contribute to expanding the application of linear coordination polymers in sensing and other fields. Full article
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<p><sup>1</sup>H NMR spectra of (<b>a</b>) <b>L2</b> (CDCl<sub>3</sub>), (<b>b</b>) <b>P2</b> (DMSO-d<sub>6</sub>), (<b>c</b>) <b>L1</b> (CDCl<sub>3</sub>) and (<b>d</b>) <b>P1</b> (DMSO-d<sub>6</sub>).</p>
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<p>(<b>a</b>) SEM and mapping (EDS) images of <b>P2</b>; (<b>b</b>) SEM image of <b>P1</b>; (<b>c</b>)TEM image of <b>P1</b>.</p>
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<p>(<b>a</b>) Abs of mixture of <b>L3</b> (9.316 μM) and [Zn<sup>2+</sup>] (0.0–1.0 eq) stirred for 4 h. (<b>b</b>) Plot of (A<sub>0</sub>/(A − A<sub>0</sub>) as a function of 1/[Zn<sup>2+</sup>]. The apparent association constant Ka corresponding to the interaction between <b>L3</b> (9.316 μM) and [Zn<sup>2+</sup>] (0.0–1.0 eq) was determined using the Benesi–Hilderbrand equation A<sub>0</sub>/(A − A<sub>0</sub>) = (A<sub>0</sub>/(Amax − A<sub>0</sub>))((1/Ka)[Zn<sup>2+</sup>]<sup>−1</sup> + 1).</p>
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<p>(<b>a</b>) UV-Vis and (<b>b</b>) Fluorescence spectrum of <b>L1</b>, <b>L2</b>, <b>P1</b>, <b>P2</b> (1 × 10<sup>−5</sup> mol·L<sup>−1</sup> in CH<sub>3</sub>CN), LOD and LOQ of <b>L1</b>, <b>L2</b>, <b>P1</b>, <b>P2</b> can be seen in <a href="#app1-polymers-17-00087" class="html-app">Figure S29</a>; (<b>c</b>) Fluorescence spectrum of solid <b>L1</b>, <b>L2</b>, <b>P1</b>, <b>P2</b>; (<b>d</b>) Acid–base response of <b>P2</b>, the Fluorescence spectrum of solid <b>P2</b>, <b>P2</b> fumigated with concentrated hydrochloric acid (30 s), fumigated <b>P2</b> after 7 days and fumigated <b>P2</b> fumed with ammonium hydroxide. Inset: Photos of ligands and polymers under sunlight (<b>top</b>) and ultraviolet light (<b>bottom</b>).</p>
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<p>(<b>a</b>) Infrared spectrum of solid <b>P2</b>, <b>P2</b> fumigated with concentrated hydrochloric acid (30 s), fumigated <b>P2</b> after 7 days and fumigated <b>P2</b> fumed with ammonium hydroxide; (<b>b</b>) Thermogravimetric and differential thermogravimetric analysis diagram of <b>P1</b> and <b>P2</b> (the red line represents <b>P2</b>, the black line represents <b>P1</b>, the solid line represents thermogravimetric analysis, and the dashed line represents differential thermogravimetric analysis).</p>
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<p>Synthesis route of the terpyridine ligands <b>L1</b>/<b>L2</b> and coordination polymers <b>P1</b>/<b>P2</b> (I: a. CH<sub>3</sub>CH<sub>2</sub>OH, NaOH; b. NH<sub>3</sub>·H<sub>2</sub>O, refluxed; II: KOH, THF, CH<sub>3</sub>OH, Ar, refluxed; III: Zn(NO<sub>3</sub>)<sub>2</sub>·6H<sub>2</sub>O, CHCl<sub>3</sub>/CH<sub>3</sub>OH).</p>
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16 pages, 10770 KiB  
Article
A Tunable and Switchable Multi-Wavelength Erbium-Doped Fiber Laser Based on a Curvature Mach–Zehnder Interferometer Filter Using Thin-Core Fiber
by Christian Perezcampos-Mayoral, Jaime Gutiérrez-Gutiérrez, José Luis Cano-Pérez, Marciano Vargas-Treviño, Lorenzo Tepech-Carrillo, Erick Israel Guerra-Hernández, Itandehui Belem Gallegos-Velasco, Pedro Antonio Hernández-Cruz, Eeduardo Pérez-Campos-Mayoral, Victor Hugo Ojeda-Meixueiro, Julián Moisés Estudillo-Ayala, Juan Manuel Sierra-Hernandez and Roberto Rojas-Laguna
Appl. Sci. 2024, 14(24), 11578; https://doi.org/10.3390/app142411578 - 11 Dec 2024
Viewed by 659
Abstract
We propose and demonstrate a tunable and switchable multi-wavelength fiber ring laser configuration based on a Mach–Zehnder interferometer (MZI) filter. The MZI was fabricated using a core-offset splicing technique, with a 2 cm piece of thin-core erbium-doped fiber (TCEDF), with a core diameter [...] Read more.
We propose and demonstrate a tunable and switchable multi-wavelength fiber ring laser configuration based on a Mach–Zehnder interferometer (MZI) filter. The MZI was fabricated using a core-offset splicing technique, with a 2 cm piece of thin-core erbium-doped fiber (TCEDF), with a core diameter of 2.90 µm, coupled in the central region of the MZI between two segments of single-mode fiber (SMF). By applying curvature to the MZI filter, we generated lasing single-, double-, triple-, and quadruple-emission lines with a curvature range from 2.3452 m−1 to 6.0495 m−1. A single-emission lasing line can be tuned from 1556.63 nm to 1564.25 nm with a tuning span of 7.62 nm and an SMSR of 49.80 dB. The laser emission can be switched to quadruple- and triple-emission lasing signals, with SMSR values of 39.96 dB and 36.83 dB, respectively. The dual-narrow emission lasing signal can be tuned from 1564.56 nm to 1561.34 nm, with an SMSR of 40.46 dB. Another lasing dual-emission signal can be tuned from 1585.69 nm to 1576.89 nm, producing an 8.8 nm tuning range, and from 1572.53 nm to 1563.66 nm, producing an 8.87 nm range, with the best SMSR of 42.35 dB. Full article
(This article belongs to the Special Issue Recent Trends in Fiber Optic Sensor: Technology and Applications)
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<p>Fiber clamping for SMF/TCEDF/SMF splices. (<b>a</b>) This demonstrates how to adhere the fiber to the metric rod with the masking tape and (<b>b</b>) illustrates how splicing is accomplished with the fusion splicer.</p>
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<p>Core-offset splice SMF/TCEDF/SMF design. (<b>a</b>) Illustrates the splicing between fibers, (<b>b</b>) shows the TCEDF cut, (<b>c</b>) U-shape of the MZI filter, (<b>d</b>) exhibits the z-side view of the MZI.</p>
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<p>(<b>a</b>) Interference spectra generated in the optical cavity of each MZI filter, (<b>b</b>) spatial frequency of the transmission spectrum generated by every filter.</p>
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<p>Diagram of the MTEFL ring array: (<b>a</b>) illustrates the configuration scheme, and (<b>b</b>) depicts the process for inducing curvature in the MZI filter to generate wavelength-switchable tunable emission lines.</p>
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<p>MTEFL emission tuning and switching cases generated for single (state-a), quadruple (state-b), triple (state-c), narrow-double (state-d), and double (state-e) lasing signals.</p>
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<p>(State-a) single-emission signal. (<b>a</b>) Tuning lines, (<b>b</b>) emission samples of curvature and SNR, (<b>c</b>) SMSR and SNR of the most significant peaks and their comparison, (<b>d</b>) the polynomial fit between the curvature data and its wavelength shift.</p>
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<p>Switch with quad-emission line. (<b>a</b>) SMSR on each peak, (<b>b</b>) power difference between the peaks and their separation.</p>
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<p>(State-c) double switch of triple-emission signals: (<b>a</b>) SMSR on the first switch, (<b>b</b>) separation and power of peaks, (<b>c</b>) SMSR of the second switch, (<b>d</b>) separation and the power of peaks.</p>
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<p>(State-c) double switch of triple-emission signals: (<b>a</b>) SMSR on the first switch, (<b>b</b>) separation and power of peaks, (<b>c</b>) SMSR of the second switch, (<b>d</b>) separation and the power of peaks.</p>
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<p>Narrow-dual-emission signals (state-d). (<b>a</b>) Tuning and the potential difference between peaks and their wavelength comparisons, (<b>b</b>) most significative peaks and power comparison, (<b>c</b>) sensitivity compared to the dispersion of curvature samples.</p>
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<p>Double-emission signal (state-e). (<b>a</b>) Tuning and most significant power peaks, (<b>b</b>) separation comparison, (<b>c</b>) peaks power comparison, (<b>d</b>) sensitivity generated with the curvature/wavelength samples.</p>
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<p>Double-emission signal (state-e). (<b>a</b>) Tuning and most significant power peaks, (<b>b</b>) separation comparison, (<b>c</b>) peaks power comparison, (<b>d</b>) sensitivity generated with the curvature/wavelength samples.</p>
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<p>(<b>a</b>) Stability test of the single initial and final emission, (<b>b</b>) power variation, (<b>c</b>) wavelength variation.</p>
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<p>First and last emissions signals of the dual-narrow lasing lines. (<b>a</b>) Stability test, (<b>b</b>) power fluctuation, (<b>c</b>) wavelength stability.</p>
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<p>Stability tests of the dual lasing lines. (<b>a</b>) Stability test on the first emission, (<b>b</b>) power fluctuation, (<b>c</b>) wavelength stability, (<b>a’</b>) stability test on the last emission, (<b>b’</b>) power fluctuation, (<b>c’</b>) wavelength stability.</p>
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<p>(<b>a</b>) Stability tests of the quad-emission line, (<b>b</b>) power variation, (<b>c</b>) wavelength variation.</p>
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<p>Stability tests of the triple emissions. (<b>a</b>) On the first switch, (<b>b</b>) power variation, (<b>c</b>) wavelength variation, (<b>a’</b>) test on the second switch, (<b>b’</b>) power variation, (<b>c’</b>) wavelength variation.</p>
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11 pages, 3543 KiB  
Article
Wavelength-Switchable Ytterbium-Doped Fiber Laser Based on All-Fiber Lyot Interferometer Filter
by Yizhang Wang, Qi Liu, Kai Ren and Yanlong Cao
Appl. Sci. 2024, 14(24), 11572; https://doi.org/10.3390/app142411572 - 11 Dec 2024
Viewed by 509
Abstract
A wavelength-switchable ring-cavity ytterbium-doped fiber laser utilizing an all-fiber Lyot interferometer filter was proposed and experimentally demonstrated. Firstly, the Lyot filter was constructed using a polarization-maintaining fiber (PMF) to obtain a comb interferometer effect, and the free spectrum ranges corresponding to 2.5 and [...] Read more.
A wavelength-switchable ring-cavity ytterbium-doped fiber laser utilizing an all-fiber Lyot interferometer filter was proposed and experimentally demonstrated. Firstly, the Lyot filter was constructed using a polarization-maintaining fiber (PMF) to obtain a comb interferometer effect, and the free spectrum ranges corresponding to 2.5 and 1 m PMF were 2.2 and 6.4 nm, respectively. Then, wavelength-switchable ytterbium-doped fiber emission was realized in the experiment, and the tunable range for the single-wavelength laser was from 1073.76 to 1086.78 nm, with a power variation of less than 1.959 dB. During the experiment, four different sets of double-wavelength lasers were achieved by adjusting the polarization controller (PC) from 1071.64 to 1081.65 nm; in addition, three different sets of triple-wavelength lasers were realized, and the signal-to-noise ratio (SNR) was more than 33.031 dB. For stable single-, double-, and triple-wavelength lasers, the power shifts were less than 0.574, 0.631, and 1.195 dB, respectively. Through adjusting the PC, quadruple-wavelength-switchable lasers could be realized with an SNR exceeding 26.233 dB. Full article
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<p>Schematic diagram of proposed YDFL.</p>
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<p>Laser generation and comb filter spectrum: (<b>a</b>) laser output without filter; (<b>b</b>) Lyot comb spectrum with 2.5 m PMF; (<b>c</b>) Lyot comb spectrum with 1 m PMF; (<b>d</b>) frequency spectrum.</p>
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<p>Wavelength-switchable single-wavelength generation: (<b>a</b>) single-wavelength laser spectrum; (<b>b</b>) power fluctuations for different single-wavelength lasers.</p>
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<p>Wavelength-switchable double-wavelength generation: (<b>a</b>) double-wavelength laser generation; (<b>b</b>) double-wavelength laser spectrum analysis.</p>
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<p>Wavelength-switchable triple-wavelength generation: (<b>a</b>) triple-wavelength laser generation; (<b>b</b>) triple-wavelength laser spectrum analysis.</p>
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<p>Quadruple-wavelength laser generation: (<b>a</b>) quadruple-wavelength laser spectrum; (<b>b</b>) different cases of quadruple-wavelength laser generation.</p>
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<p>Multi-wavelength laser stability: (<b>a</b>) single-wavelength laser spectrum; (<b>b</b>) single-wavelength laser power fluctuation; (<b>c</b>) double-wavelength laser spectrum; (<b>d</b>) double-wavelength laser power fluctuation; (<b>e</b>) triple-wavelength laser spectrum; (<b>f</b>) triple-wavelength laser power fluctuation.</p>
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<p>Multi-wavelength laser stability: (<b>a</b>) single-wavelength laser spectrum; (<b>b</b>) single-wavelength laser power fluctuation; (<b>c</b>) double-wavelength laser spectrum; (<b>d</b>) double-wavelength laser power fluctuation; (<b>e</b>) triple-wavelength laser spectrum; (<b>f</b>) triple-wavelength laser power fluctuation.</p>
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19 pages, 3256 KiB  
Review
Carbon Quantum Dots as Phosphors in LEDs: Perspectives and Limitations—A Critical Review of the Literature
by Katarzyna Bucka, Robert P. Socha and Marek Wojnicki
Electronics 2024, 13(22), 4481; https://doi.org/10.3390/electronics13224481 - 15 Nov 2024
Viewed by 894
Abstract
The enduring interest in carbon quantum dots (CQDs) as photoluminescent material arises from their significant advantages over inorganic quantum dots (QDs), such as low toxicity and biocompatibility, which enables their application in bioimaging and drug delivery. This review is focused on the use [...] Read more.
The enduring interest in carbon quantum dots (CQDs) as photoluminescent material arises from their significant advantages over inorganic quantum dots (QDs), such as low toxicity and biocompatibility, which enables their application in bioimaging and drug delivery. This review is focused on the use of CQDs for light emitting devices (LED) technology and provides a guide on how to synthesize CQDs that emit blue, green, and red light, which is necessary to produce RGB LEDs. Consideration was given to the precursors, solvents, methods, and conditions of the processes, the excitation wavelength, the emission wavelength, and the photoluminescence quantum yield (QY). These unique, organic nanoparticles have the potential to revolutionize lighting and, above all, the electronics market due to their low cost and eco-friendliness, as well as the possibility of using various precursors, including waste. Full article
(This article belongs to the Special Issue Feature Papers in Electronic Materials)
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<p>Number of documents displayed in Scopus for a search query that included “carbon quantum dots” in title, abstract, or keywords, up to the end of 2023.</p>
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<p>Schematic of the CQD synthesis via hydrothermal, solvothermal, microwave-assisted, and electrolytic methods.</p>
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<p>Types of precursors used in CQD synthesis: small organic particles, aromatic organic compounds, and organic wastes, and their examples.</p>
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<p>The dependence of the emitted wavelength of CQDs on the excitation wavelength for the blue-, green-, and red-emissive CQDs.</p>
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<p>The number of publications in which only inorganic (blue) and organic (green) solvents were used for the synthesis of CQDs in relation to the wavelengths they emit.</p>
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<p>Temperature (<b>a</b>) and time (<b>b</b>) dependence of solvothermal and hydrothermal syntheses on the quantum yield of CQDs. Colors on the plots are an indication of the light that CQDs emit: blue—emission of blue light, green—green light, and red—red light.</p>
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11 pages, 3801 KiB  
Article
Tunable Color Emissions in a Single CdTe Nanowire Based on Complex Optical Transverse Nonlinear Effects
by Lijun Guo, Lihao Xu, Changjiang Fan, Yunfei Zhang, Hao Yang, Mengwei Li and Chenguang Xin
Photonics 2024, 11(11), 1068; https://doi.org/10.3390/photonics11111068 - 14 Nov 2024
Viewed by 651
Abstract
Tunable color emissions, emerging from a single CdTe nanowire, are demonstrated experimentally based on optical transverse nonlinear effects. The pumping light at different wavelengths (e.g., 1064 nm and 980 nm) is coupled to a nanowire at both ends via evanescent-field coupling. The light [...] Read more.
Tunable color emissions, emerging from a single CdTe nanowire, are demonstrated experimentally based on optical transverse nonlinear effects. The pumping light at different wavelengths (e.g., 1064 nm and 980 nm) is coupled to a nanowire at both ends via evanescent-field coupling. The light at different wavelengths (e.g., 510 nm, 532 nm, and 713 nm) can be simultaneously assessed using complex optical transverse nonlinear effects, including transverse sum-frequency generation (TSFG), transverse second-harmonic generation (TSHG), and two-photon absorption (TPA)-induced fluorescence. By changing the wavelength and the power of the pumping lights, the spectra of the transverse light emissions change as well, leading to tunable color emissions at the single-nanowire level with a Rec. 2020 coverage of ~21.6%. The results indicate the potential of transverse nonlinear effects in applications ranging from optical display and spectroscopy to communication. Full article
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<p>A Schematic diagram of the experiment. A CdTe single nanowire is suspended in free space via tapered optical fibers to avoid interaction with the substrate. As a result of different transverse nonlinear effect, different colors emit in the direction perpendicular to the axis of the nanowire.</p>
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<p>Optical and scanning electron microscope images. (<b>a</b>) Optical microscope image of a ~280 nm diameter CdTe nanowire suspended in free space. The pumping lights are coupled inside the nanowire via the two tapered optical fibers. (<b>b</b>,<b>c</b>) Scanning electron microscope images of the CdTe nanowire. (<b>d</b>–<b>f</b>) The optical microscope images of the nanowire with 1064 nm wavelength pump light coupled in from the left, right, and both sides, respectively.</p>
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<p>Optical emitting properties of a nanowire pumped by 1064 nm wavelength light from one single side. (<b>a</b>) An optical microscope image of the nanowire subjected to an input power of ~1.90 mW from the left side. (<b>b</b>) Optical spectra of the TPA-induced fluorescence when the nanowire is subjected to a different input power, indicating a strong peak at a wavelength of 713 nm and a weak peak at a wavelength of 532 nm. The inset image is an enlarged view of the peak at a 532 nm wavelength. (<b>c</b>) The relationship between the normalized intensity of the peak at a 713 nm wavelength and the input power, corresponding to (<b>b</b>).</p>
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<p>Optical emitting properties of the nanowire when pumped with 1064 nm wavelength light from both sides. (<b>a</b>) Optical spectra of the transverse emitting light with different input powers. The peaks at wavelength of 713 nm and 532 nm correspond to the TPA-induced fluorescence and TSHG, respectively. (<b>b</b>) The relationship between the normalized intensity of the two peaks and the input power. (<b>c</b>) Normalized optical spectra when using a 600 nm short-pass optical filter. (<b>d</b>) Normalized optical spectra when using a 600 nm long-pass optical filter. (<b>e</b>) The optical microscope images of the nanowire with different input powers.</p>
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<p>Optical emitting properties of the nanowire pumped by 1064 nm wavelength light and 980 nm wavelength light coupled to the two sides of the nanowire, respectively. (<b>a</b>) Optical spectra of the transverse emitting light. The peaks at wavelengths of 713 nm, 532 nm, and 510 nm correspond to the TPA-induced fluorescence, TSHG, and TSFG, respectively. (<b>b</b>) The relationship between the normalized intensity of the three peaks and the input power of 1064 nm wavelength pumping light. (<b>c</b>) The optical microscope images with different input powers of 1064 nm wavelength pumping light.</p>
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<p>The gamut of the transverse emitting light in the CIE 1931 <span class="html-italic">xy</span> chromaticity diagram. The circle represents the case with a single peak in the spectra, while the square, diamond, and triangle represent cases with two distinct peaks. The pentagram represents the case with three peaks.</p>
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<p>The shifts in the CIE 1931 <span class="html-italic">xy</span> coordinates for (<b>a</b>) the three-peak cases and for the two-peak case with wavelengths of (<b>b</b>) 532 nm and 713 nm, (<b>c</b>) 510 nm and 532 nm, and (<b>d</b>) 510 nm and 713 nm, respectively. The input power of the left-side 980 nm wavelength pumping light remains unchanged at ~2.00 mW, and the input power of the right-side 1064 nm wavelength pumping light increases gradually.</p>
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<p>Scanning electron microscope image and optical emitting properties of a nanowire pumped with 1064 nm wavelength light from one single side. (<b>a</b>) Scanning electron microscope image of a ~385 nm diameter CdTe nanowire. (<b>b</b>) Optical microscope image of the nanowire from one single side. (<b>c</b>) Optical spectra of the TPA-induced fluorescence, indicating a strong peak at a wavelength of 713 nm and a weak peak at a wavelength of 532 nm. The inset image is an enlarged view of the peak at a 532 nm wavelength.</p>
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<p>The uncertainty of the measured intensity for the TPA-induced fluorescence. Four spectra are measured with a time interval of ~10 s between each other. The inset image is an enlarged view of the region around the peak of the spectrum.</p>
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16 pages, 16410 KiB  
Article
A Tunable and Switchable Multi-Wavelength Erbium-Doped Fiber Ring Laser Enabled by Adjusting the Spectral Fringe Visibility of a Mach-Zehnder Fiber Interferometer
by Romeo Emmanuel Nuñez Gomez, Gilberto Anzueto Sánchez, Alejando Martínez Ríos, Ariel Fong González, Alfredo Olarte Paredes, Areli Marlen Salgado Delgado, Jesús Castrellón Uribe and René Salgado Delgado
Appl. Sci. 2024, 14(21), 9846; https://doi.org/10.3390/app14219846 - 28 Oct 2024
Viewed by 1278
Abstract
This paper presents a tunable, switchable multi-wavelength emission from an erbium-doped fiber ring laser, enabled by adjusting the spectral fringe visibility of a fiber interferometer filter. The filter is formed with specially designed concatenated tapered fibers to configure a Mach-Zehnder fiber interferometer (MZFI). [...] Read more.
This paper presents a tunable, switchable multi-wavelength emission from an erbium-doped fiber ring laser, enabled by adjusting the spectral fringe visibility of a fiber interferometer filter. The filter is formed with specially designed concatenated tapered fibers to configure a Mach-Zehnder fiber interferometer (MZFI). The laser emission is highly flexible and reconfigurable, allowing for tuning between single- and dual-wavelength operation. The laser can switch sequentially from one up to six wavelengths by fixing the curvature and adjusting the polarization state. The lasing emission is generated over a stable wavelength range between 1559.59 nm and 1563.54 nm, exhibiting an optical signal-to-noise ratio (OSNR) exceeding ~35 dB. The performance of amplitude and wavelength fluctuations were evaluated, indicating an appropriate stability of ~3 dB and a shift less than 0.1 nm within a 45 min period at room temperature. A detailed comparison with the literature is given. Full article
(This article belongs to the Special Issue Recent Trends in Fiber Optic Sensor: Technology and Applications)
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<p>Experimental erbium-doped fiber ring laser cavity setup for tunable and multi-wavelength emission.</p>
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<p>(<b>a</b>) MZFI structure formed with a pair of tapered sections fabricated on SMF-28, (<b>b</b>) displacement mechanism to used induce curvature in the MZFI.</p>
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<p>ASE spectrum as the light source from the EDF (black line) and the modified spectrum after passing through the MZFI (red line). The laser oscillation at 1563.07 nm is shown by the blue line.</p>
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<p>(<b>a</b>) The progressive modification of ASE spectrum with increasing curvature applied to the MZFI, (<b>b</b>) an inset in the range of 1541 to 1560 nm demonstrates an FSR of 5 nm.</p>
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<p>The wavelength shifts as a function of curvature (0 m<sup>−1</sup> to 2.93 m<sup>−1</sup>) and the variation of the measured fringe visibility.</p>
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<p>Tunable single laser wavelength between 1563.705 nm to 1558.05 nm for the curvatures from 0 m<sup>−1</sup> to 2.79 m<sup>−1</sup>.</p>
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<p>(<b>a</b>). Switchable dual-wavelength emissions generated at curvatures of 1.53 m<sup>−1</sup> with 1559.07 nm and 1563.66 nm, (<b>b</b>) 2.33 m<sup>−1</sup> with 1543.21 nm and 1549.287 nm, (<b>c</b>) 2.5 m<sup>−1</sup> with 1554.61 nm and 1559.667 nm, (<b>d</b>) 2.75 m<sup>−1</sup> with 1556.8 nm and 1561.877 nm.</p>
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<p>(<b>a</b>) Single-wavelength oscillation at 1562.22 nm, (<b>b</b>) dual-wavelength oscillation (1562.22–1562.875 nm), (<b>c</b>) triple-wavelength oscillation (1560.175–1562.22–1562.88 nm).</p>
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<p>(<b>a</b>) Quadruple-wavelength emission (1560.85–1561.51–1562.26–1562.86 nm), (<b>b</b>) quintuple-wavelength emission (1559.59–1560.91–1561.58–1562.93–1563.61 nm), and (<b>c</b>) sextuple-wavelength emission (1560.25–1560.97–1561.63–1562.29–1562.98–1563.64 nm).</p>
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<p>(<b>a</b>) Spectral distribution stability of a single laser oscillation at 1562.22 nm, with high-intensity uniformity across the spectrum, (<b>b</b>) a maximum wavelength shift of 0.01 nm, and (<b>c</b>) output power fluctuations of less than 0.12 dB.</p>
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<p>(<b>a</b>). Stability of the dual-wavelength laser oscillation at 1562.22–1562.785 nm with uniform intensity, (<b>b</b>) a maximum wavelength shift of 0.07 nm, and (<b>c</b>) output power fluctuations of less than 0.25 dB.</p>
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<p>(<b>a</b>) Power stability of the triple-wavelength laser system, (<b>b</b>) maximum wavelength shift of 0.07 nm, and (<b>c</b>) maximum amplitude fluctuation of 0.51dB for the 1562.88 nm line.</p>
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<p>(<b>a</b>) Power stability of the quadruple-wavelength laser system, (<b>b</b>) maximum wavelength shift of 0.22 nm, and (<b>c</b>) maximum amplitude fluctuation of 3 dB for the 1562.83 nm line.</p>
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<p>(<b>a</b>) Power stability of the quintuple-wavelength laser system, (<b>b</b>) maximum wavelength shift of 0.07 nm, and (<b>c</b>) maximum amplitude fluctuation of 1.7 dB for the 1561.58 nm line.</p>
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<p>(<b>a</b>) Power stability of the sextuple-wavelength laser system, (<b>b</b>) negligible wavelength shift, and (<b>c</b>) maximum amplitude fluctuation of 2.71 dB for the 1562.98 nm line.</p>
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18 pages, 6433 KiB  
Article
Dual-Wavelength Interferometric Detection Technology for Wind and Temperature Fields in the Martian Middle and Upper Atmosphere Based on LCTF
by Yanqiang Wang, Biyun Zhang, Chunmin Zhang, Shiping Guo, Tingyu Yan, Yifan He and William Ward
Remote Sens. 2024, 16(19), 3591; https://doi.org/10.3390/rs16193591 - 26 Sep 2024
Viewed by 627
Abstract
A dual-wavelength spaceborne Martian polarized wind imaging Michelson interferometer based on liquid crystal tunable filters (LCTF-MPWIMI) has been proposed for the remote sensing detection of dynamic parameters such as wind speed and temperature in the middle and upper atmosphere of Mars. Using the [...] Read more.
A dual-wavelength spaceborne Martian polarized wind imaging Michelson interferometer based on liquid crystal tunable filters (LCTF-MPWIMI) has been proposed for the remote sensing detection of dynamic parameters such as wind speed and temperature in the middle and upper atmosphere of Mars. Using the detected Martian oxygen atom emission lines at 557.7 nm and 630.0 nm as observation spectral lines, this technology extends the detection altitude range for Martian atmospheric wind speed and temperature to 60–180 km. By leveraging the different spectral line visibility of the interferograms at the two wavelengths, a novel method for measuring Martian atmospheric temperature is proposed: the dual-wavelength spectral line visibility product method. This new approach reduces the uncertainty of temperature detection compared to traditional single spectral line visibility methods, while maintaining the precision of wind speed measurements. The feasibility of the LCTF-MPWIMI for measuring wind and temperature fields in the Martian middle and upper atmosphere has been validated through theoretical modeling and computer simulations. The interferometer, as a key component of the system, has been designed and analyzed. The proposed LCTF-MPWIMI instrument is free of mechanical moving parts, offering flexible wavelength selection and facilitating miniaturization. The dual-wavelength temperature measurement method introduced in this work provides superior temperature measurement precision compared to any single spectral line when the signal-to-noise ratio (SNR) of the interferograms is comparable. Moreover, this method does not impose specific requirements on the atomic state of the spectral lines, making it broadly applicable to similar interferometric wind measurement instruments. These innovations offer advanced tools and methodologies for measuring wind speeds and temperatures in the atmospheres of Mars and other planets. Full article
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<p>Optical layout of the LCTF-MPWIMI. The LCTF serves both as an optical filter and as a linear polarizer, with the red arrow indicating that its transmission axis forms a 45° angle with the <span class="html-italic">x</span>-axis. P<sub>2</sub> refers to an array of linear polarizers, consisting of four sub-linear polarizers with their transmission axes at angles of 0°, 45°, 90°, and 135° relative to the <span class="html-italic">x</span>-axis, respectively.</p>
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<p>Mars atmospheric wind field detection with LCTF-MPWIMI: (<b>a</b>) single-field-of-view Limb; (<b>b</b>) dual-Field-of-view limb geometry.</p>
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<p>The limb profiles of [Oi] 557.7 nm dayglow intensity observed with UVIS on 28 April 2019 (green dots) [<a href="#B10-remotesensing-16-03591" class="html-bibr">10</a>].</p>
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<p>Wind velocity error variations with OPD and SNR.</p>
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<p>Emissions line visibility with OPD and atmospheric temperature.</p>
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<p>Simulated four normalized zero-wind interferograms of 557.7 nm airglow. The phase steps are 0°, 90°, 180°, and 270°, respectively. From the center to the edge of the images, the incident angle varies from 0° to 9.3°. The simulated atmospheric temperature is 150 K.</p>
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<p>Simulated four normalized zero wind interferograms of 630.0 nm airglow. The phase steps are 0°, 90°, 180°, and 270°, respectively. From the center to the edge of the images, the incident angle varies from 0° to 9.3°. The simulated atmospheric temperature is 150 K.</p>
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<p>Typical wind speed and temperature data from the Mars climate database [<a href="#B19-remotesensing-16-03591" class="html-bibr">19</a>]: (<b>a</b>) typical Martian atmospheric wind speed map; (<b>b</b>) typical Martian atmospheric temperature map.</p>
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<p>Four-phase stepping wind imaging interferograms for the 557.7 nm airglow spectral lines (<span class="html-italic">SNR</span> = 300).</p>
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<p>Four-phase stepping wind imaging interferograms for the 630.0 nm airglow spectral lines (<span class="html-italic">SNR</span> = 115).</p>
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<p>Retrieval of Martian atmospheric wind speed using 557.7 nm interferograms: (<b>a</b>) retrieved wind speed map; (<b>b</b>) wind speed error map.</p>
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<p>Retrieval of Martian atmospheric temperature using two spectral lines: (<b>a</b>) retrieved temperature map from single spectral line; (<b>b</b>) single spectral line temperature error map; (<b>c</b>) retrieved temperature map from dual-spectral line; (<b>d</b>) dual-spectral line temperature error map.</p>
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<p>Typical wind speed and temperature profiles from the Mars Climate Database [<a href="#B19-remotesensing-16-03591" class="html-bibr">19</a>], along with their gradients with respect to height, at a solar longitude of Ls = 250°, local time of 12:00, and a Martian longitude and latitude of 0°: (<b>a</b>) horizontal wind speed profile; (<b>b</b>) calculated horizontal wind speed gradient; (<b>c</b>) temperature profile; (<b>d</b>) calculated temperature gradient.</p>
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21 pages, 3867 KiB  
Review
A Review of Deep-Red (650–700 nm)-Emitting Semiconductor Nanocrystals
by Geyu Jin, Fangze Liu, Jing Wei and Hongbo Li
Crystals 2024, 14(9), 788; https://doi.org/10.3390/cryst14090788 - 5 Sep 2024
Viewed by 1037
Abstract
Deep-red light has significant application value in various fields, including biomedicine, plant cultivation, and displays. The development of high-efficiency deep-red luminescent materials is therefore of great importance. Semiconductor nanocrystals have been extensively studied as novel luminescent materials due to their wavelength tunability, narrow [...] Read more.
Deep-red light has significant application value in various fields, including biomedicine, plant cultivation, and displays. The development of high-efficiency deep-red luminescent materials is therefore of great importance. Semiconductor nanocrystals have been extensively studied as novel luminescent materials due to their wavelength tunability, narrow emission linewidth, and high luminescence efficiency. However, the advancement of deep-red nanocrystals has lagged behind that of red, green, and blue nanocrystals, primarily due to material selection limitations. This review summarizes the recent progress in the synthesis of deep-red nanocrystals based on their material composition, including II-VI, III-V, I-III-VI, and perovskite nanocrystals. Full article
(This article belongs to the Special Issue Advances of Perovskite Solar Cells—2nd Edition)
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<p>Relationship between the composition and the absorption/emission energies for homogeneous CdSe<sub>1−x</sub>Te<sub>x</sub> quantum dots at different sizes: (<b>a</b>) UV–-Vis absorption and photoluminescence spectra of CdSe<sub>0.34</sub>Te<sub>0.66</sub> quantum dots in the size range of 2.7–8.6 nm; (<b>b</b>) plots of the absorption onset energy (in eV) as a function of tellurium content; and (<b>c</b>) plots of the emission peak wavelength (nm) as a function of tellurium content. Note that the absorption onsets are slightly lower in energy than the emission maxima. Reproduced with permission of reference [<a href="#B25-crystals-14-00788" class="html-bibr">25</a>].</p>
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<p>Schematic of band energy changes in quantum dots induced by lattice strain. (<b>a</b>) Lattice strain of ordinary and strained (CdTe)ZnSe nanocrystals. (<b>b</b>) Valence and conduction band energy levels for the corresponding structures in a. The wavy arrows and their colors indicate band-edge fluorescence emission and their approximate wavelengths. The horizontal band lengths correspond to the thicknesses of the core and the shell. Relaxed nanostructures form standard type-I heterojunctions but are converted to type-II behavior when the core is ‘squeezed’ and the shell is ‘stretched’ by the strain from heteroepitaxial growth. Reproduced with permission of reference [<a href="#B34-crystals-14-00788" class="html-bibr">34</a>].</p>
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<p>(<b>a</b>) PLQYs and corresponding FWHM’s of the obtained CdTe/CdSe core/shell QDs with different PL emission wavelengths. The emission wavelength of 560 nm corresponds to CdTe core nanocrystals. (<b>b</b>) PL spectra (λ<sub>ex</sub> = 400 nm) of CdTe/CdSe (1 ML CdSe) and CdTe/CdSe/ZnS nanocrystals (1 ML CdSe, 2 ML ZnS) before (chloroform solutions) and after (aqueous solutions) phase transfer with the use of MPA. All colloidal solutions exhibit identical optical densities at the excitation wavelength. Reproduced with permission of reference [<a href="#B39-crystals-14-00788" class="html-bibr">39</a>].</p>
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<p>(<b>a</b>). Schematic of CdSe/CdS NRs with a giant shell; (<b>b</b>) Absorbance and (<b>c</b>) PL spectra of CdSe/CdS NRs with different CdSe core diameters excited by 450 nm. Reproduced with permission of reference [<a href="#B45-crystals-14-00788" class="html-bibr">45</a>].</p>
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<p>(<b>a</b>) Schematic of (CdSe/CdS)@(CdS/ZnS) NPLs. (<b>b</b>) TEM images of NPLs showing maintained 2D shape. (<b>c</b>) Band alignment of CdSe, CdS, and CdZnS. (<b>d</b>) Absorption (black line) and PL spectra (red line) of (CdSe/CdS)@(CdS/ZnS) NPLs. Inset: photographs of the NPL solution under daylight (<b>top</b>) and 365 nm UV light (<b>below</b>). Reproduced with permission of reference [<a href="#B49-crystals-14-00788" class="html-bibr">49</a>].</p>
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<p>(<b>a</b>) Schematic of InP/ZnS QDs; (<b>b</b>) Steady-state PL spectra of deep-red InP/ZnS QDs with shelling time; (<b>c</b>) FWHM and PLQY as a function of PL peak position; (<b>d</b>) PL spectra of InP QDs synthesized with InI, InBr, and InCl. Reproduced with permission of reference [<a href="#B69-crystals-14-00788" class="html-bibr">69</a>].</p>
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<p>(<b>a</b>) Absorption spectra of different-sized CuInS<sub>2</sub> QDs. (<b>b</b>) The size-dependent absorption band edge of CuInS<sub>2</sub> QDs. (<b>c</b>) Photoluminescence properties of CuInS2/ZnS core–shell QDs. (<b>d</b>) The PLE, PL, and absorption spectra of CuInS<sub>2</sub>/ZnS QDs after size selection. Reproduced with permission of reference [<a href="#B102-crystals-14-00788" class="html-bibr">102</a>].</p>
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<p>Colloidal perovskite CsPbX<sub>3</sub> NCs (X = Cl, Br, I) exhibit size- and composition-tunable band gap energies covering the entire visible spectral region with narrow and bright emission: (<b>a</b>) colloidal solutions in toluene under UV lamp (λ = 365 nm); (<b>b</b>) representative PL spectra (λ<sub>exc</sub> = 400 nm for all but 350 nm for CsPbCl<sub>3</sub> samples); (<b>c</b>) typical optical absorption and PL spectra; (<b>d</b>) time-resolved PL decays for all samples shown in (<b>c</b>) except CsPbCl<sub>3</sub>. Reproduced with permission of reference [<a href="#B108-crystals-14-00788" class="html-bibr">108</a>].</p>
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<p>(<b>a</b>) PL intensity comparison between pristine CsPbI<sub>3</sub> NC and CsPbI<sub>3</sub>/ZnSe NC solutions after 4 months of storage under ambient condition, with the inset showing the decrease in PL intensity (in percentage). (<b>b</b>–<b>d</b>) PL intensity comparison, with insets showing photographs of CsPbI<sub>3</sub>/ZnSe NCs (left side) and pristine CsPbI<sub>3</sub> NCs (right side) for (<b>b</b>) their colloidal solutions subjected to 302 nm UV irradiation (8 W) for 6 h, and (<b>c</b>,<b>d</b>) heat treatment of their thin films at 60 °C for 10 h and 100 °C for 4 h, respectively. Reproduced with permission of reference [<a href="#B116-crystals-14-00788" class="html-bibr">116</a>].</p>
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18 pages, 10994 KiB  
Article
Electro-Optic Response of Polymer-Stabilized Cholesteric Liquid Crystals with Different Polymer Concentrations
by Lotfi Saadaoui, Donghao Yang, Faheem Hassan, Ziyang Qiu, Yu Wang, Yujie Fan, Irena Drevensek-Olenik, Yigang Li, Xinzheng Zhang and Jingjun Xu
Polymers 2024, 16(17), 2436; https://doi.org/10.3390/polym16172436 - 28 Aug 2024
Viewed by 1903
Abstract
Polymer-stabilized cholesteric liquid crystals (PSCLCs) have emerged as promising candidates for one-dimensional photonic lattices that enable precise tuning of the photonic band gap (PBG). This work systematically investigates the effect of polymer concentrations on the AC electric field-induced tuning of the PBG in [...] Read more.
Polymer-stabilized cholesteric liquid crystals (PSCLCs) have emerged as promising candidates for one-dimensional photonic lattices that enable precise tuning of the photonic band gap (PBG). This work systematically investigates the effect of polymer concentrations on the AC electric field-induced tuning of the PBG in PSCLCs, in so doing it explores a range of concentrations and provides new insights into how polymer concentration affects both the stabilization of cholesteric textures and the electro-optic response. We demonstrate that low polymer concentrations (≈3 wt. %) cause a blue shift in the short wavelength band edge, while high concentrations (≈10 wt. %) lead to a contraction and deterioration of the reflection band. Polarization optical microscopy was conducted to confirm the phase transition induced by the application of an electric field. The observations confirm that increased polymer concentration stabilizes the cholesteric texture. Particularly, the highly desired fingerprint texture was stabilized in a sample with 10 wt. % of the polymer, whereas it was unstable for lower polymer concentrations. Additionally, higher polymer concentrations also improved the dissymmetry factor and stability of the lasing emission, with the dissymmetry factor reaching the value of around 2 for samples with 10 wt. % of polymer additive. Our results provide valuable comprehension into the design of advanced PSCLC structures with tunable optical properties, enhancing device performance and paving the way for innovative photonic applications. Full article
(This article belongs to the Section Polymer Applications)
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<p>(Upper panels) Schematic illustration of the three PSCLC samples: (<b>a</b>) S1 (3 wt. %), (<b>b</b>) S2 (6 wt. %), and (<b>c</b>) S3 (10 wt. %); (lower panels) the PBG spectra for each sample, along with their corresponding microscopic observations.</p>
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<p>(<b>a</b>) Experimental setup to measure the spectral response of the pure CLC and PCLC samples and (<b>b</b>) experimental setup to test the lasing performance.</p>
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<p>(<b>a</b>) The transmission spectra showing the blue shift of the PBG as an E-field is applied to the pure CLC sample (without reactive mesogen). (<b>b</b>) Plots of the LWBE (λ<sub>L</sub>(EXP)), SWBE (λ<sub>s</sub>(EXP)) wavelengths (black and red curve), central wavelength (λ<sub>c</sub>(EXP): green curve), and FWHM (blue curve) as a function of the applied electric field, the error bars indicate the standard deviation. The blue and yellow rectangles show the position of the PBG at zero field and 1.5 V/µm respectively. (<b>c</b>–<b>h</b>) POM images showing the birefringence change of the planar texture. The scale bars represent 100 μm.</p>
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<p>Transmission spectra for samples (<b>a</b>) S1, (<b>b</b>) S2, and (<b>c</b>) S3. The changes of <span class="html-italic">λ<sub>LWBE</sub></span>, <span class="html-italic">λ<sub>SWBE</sub></span> and FWHM with the applied voltages for (<b>d</b>) S1, (<b>e</b>) S2, and (<b>f</b>) S3. Transparency at the LWBE (black rectangles) and SWBE (red rectangles) of the PBGs for samples (<b>g</b>) S1, (<b>h</b>) S2, and (<b>i</b>) S3.</p>
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<p>POM images showing the textures under different applied electric fields for S1 (<b>a</b>), S2 (<b>b</b>), and S3 (<b>c</b>).</p>
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<p>Schematic illustration describing the mechanism of light scattering for S1, S2, and S3 at zero field (<b>a</b>–<b>c</b>) and under E-field (<b>d</b>–<b>f</b>). T: transmission, FP: fingerprint.</p>
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<p>The measured right (<span class="html-italic">I<sub>R</sub></span>) and left (<span class="html-italic">I<sub>L</sub></span>) CP transmission spectra for S1 (<b>a</b>,<b>b</b>) and S3 (<b>d</b>,<b>e</b>), and the CPD (<span class="html-italic">g</span>(<span class="html-italic">λ</span>)) for transmitted light for S1 (<b>c</b>) and S3 (<b>f</b>) under various E-field amplitudes.</p>
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<p>The maximum dissymmetry factor gmax (<b>a</b>) for S1, and (<b>b</b>) for S3, and LCP lasing emission spectra obtained from PM597 + S1 and DCM + S3 samples. The error bars (red bars) indicate the standard deviation. Insets in (<b>c</b>,<b>d</b>) show the positions of laser peaks.</p>
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14 pages, 863 KiB  
Article
Interferometrically Enhanced Intensity and Wavelength Modulation in Tunable Diode Laser Spectroscopy
by Sander Vervoort and Marcus Wolff
Photonics 2024, 11(8), 740; https://doi.org/10.3390/photonics11080740 - 8 Aug 2024
Viewed by 915
Abstract
Tunable diode laser spectroscopy (TDLS) is a measurement technique with high spectral resolution. It is based on tuning the emission wavelength of a semiconductor laser by altering its current and/or its temperature. However, adjusting the wavelength leads to a change in emission intensity. [...] Read more.
Tunable diode laser spectroscopy (TDLS) is a measurement technique with high spectral resolution. It is based on tuning the emission wavelength of a semiconductor laser by altering its current and/or its temperature. However, adjusting the wavelength leads to a change in emission intensity. For applications that rely on modulated radiation, the challenge is to isolate the true spectrum from the influence of extraneous instrumental contributions, particularly residual intensity and wavelength modulation. We present a novel approach combining TDLS with interferometric techniques, exemplified by the use of a Mach–Zehnder interferometer, to enable the separation of intensity and wavelength modulation. With interferometrically enhanced intensity modulation, we reduced the residual wavelength modulation by 83%, and with interferometrically enhanced wavelength modulation, we almost completely removed the residual derivative of the signal. A reduction in residual wavelength modulation enhances the spectral resolution of intensity-modulated measurements, whereas a reduction in residual intensity modulation improves the signal-to-noise ratio and the sensitivity of wavelength-modulated measurements. Full article
(This article belongs to the Special Issue Photonics: 10th Anniversary)
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<p>Balanced Mach–Zehnder interferometer.</p>
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<p>(<b>a</b>) Wavelength <math display="inline"><semantics> <mi>λ</mi> </semantics></math> of ICL for currents <math display="inline"><semantics> <msub> <mi>I</mi> <mi>electric</mi> </msub> </semantics></math> from 30 mA to 120 mA at three different temperatures. (<b>b</b>) Optical power <span class="html-italic">P</span> of ICL for currents <math display="inline"><semantics> <msub> <mi>I</mi> <mi>electric</mi> </msub> </semantics></math> up to 120 mA. The data were provided by Nanoplus (Meiningen, Germany).</p>
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<p>Experimental setup for interferometrically enhanced modulation.</p>
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<p>Influences on the interference efficiency factor include (<b>a</b>) beam divergence, (<b>b</b>) beam misalignment, and (<b>c</b>) the source emission spectrum.</p>
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<p>Tilted window with the angle of incidence <math display="inline"><semantics> <mi>α</mi> </semantics></math> and the angle of refraction <math display="inline"><semantics> <mi>β</mi> </semantics></math> inside the window.</p>
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<p>Measured intensities <math display="inline"><semantics> <mover accent="true"> <mi>I</mi> <mo>^</mo> </mover> </semantics></math>, scaled with respect to the intensity at 100 mA laser current <math display="inline"><semantics> <mrow> <msub> <mi>I</mi> <mrow> <mi>ICL</mi> <mo>@</mo> <mn>100</mn> <mi>mA</mi> </mrow> </msub> </mrow> </semantics></math>: (<b>a</b>) beam intensities <math display="inline"><semantics> <msub> <mover accent="true"> <mi>I</mi> <mo>^</mo> </mover> <mi mathvariant="normal">a</mi> </msub> </semantics></math> and <math display="inline"><semantics> <msub> <mover accent="true"> <mi>I</mi> <mo>^</mo> </mover> <mi mathvariant="normal">b</mi> </msub> </semantics></math> separately; (<b>b</b>) interference of <math display="inline"><semantics> <msub> <mover accent="true"> <mi>I</mi> <mo>^</mo> </mover> <mi mathvariant="normal">a</mi> </msub> </semantics></math> and <math display="inline"><semantics> <msub> <mover accent="true"> <mi>I</mi> <mo>^</mo> </mover> <mi mathvariant="normal">b</mi> </msub> </semantics></math> generating <math display="inline"><semantics> <msub> <mover accent="true"> <mi>I</mi> <mo>^</mo> </mover> <mi>MZI</mi> </msub> </semantics></math>.</p>
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<p>Measurement <math display="inline"><semantics> <msub> <mover accent="true"> <mi>I</mi> <mo>^</mo> </mover> <mi>MZI</mi> </msub> </semantics></math> and calculation <math display="inline"><semantics> <msub> <mi>I</mi> <mi>MZI</mi> </msub> </semantics></math> of the interferometer intensity of a laser current–wavelength sweep. For the calculation, <math display="inline"><semantics> <mrow> <mi>d</mi> <mi>n</mi> </mrow> </semantics></math> was set to 10.55 mm and <math display="inline"><semantics> <msub> <mi>η</mi> <mi>MZI</mi> </msub> </semantics></math> to 0.51.</p>
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<p>Traditional intensity modulation <math display="inline"><semantics> <msub> <mi>I</mi> <mi>ICL</mi> </msub> </semantics></math> and IE intensity modulation <math display="inline"><semantics> <msub> <mover accent="true"> <mi>I</mi> <mo>^</mo> </mover> <mi>MZI</mi> </msub> </semantics></math>. Intensities scaled with respect to the intensity emitted at 100 mA laser current <math display="inline"><semantics> <mrow> <msub> <mi>I</mi> <mrow> <mi>ICL</mi> <mo>@</mo> <mn>100</mn> <mi>mA</mi> </mrow> </msub> </mrow> </semantics></math>.</p>
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<p>Traditional wavelength modulation <math display="inline"><semantics> <msub> <mi>I</mi> <mi>ICL</mi> </msub> </semantics></math> and IE wavelength modulation <math display="inline"><semantics> <msub> <mover accent="true"> <mi>I</mi> <mo>^</mo> </mover> <mi>MZI</mi> </msub> </semantics></math>. Intensities scaled with respect to the intensity emitted at 100 mA laser current <math display="inline"><semantics> <mrow> <msub> <mi>I</mi> <mrow> <mi>ICL</mi> <mo>@</mo> <mn>100</mn> <mi>mA</mi> </mrow> </msub> </mrow> </semantics></math>.</p>
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<p>Angle of incidence <math display="inline"><semantics> <mi>α</mi> </semantics></math> and angle of refraction <math display="inline"><semantics> <mi>β</mi> </semantics></math> of a refracted ray in a CaF<sub>2</sub> window.</p>
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12 pages, 2127 KiB  
Article
Tunable Radiation Patterns on Temperature-Dependent Materials
by Lin Cheng, Fan Wu and Kun Huang
Photonics 2024, 11(7), 646; https://doi.org/10.3390/photonics11070646 - 8 Jul 2024
Cited by 1 | Viewed by 859
Abstract
The utilization of optical antennas for active control of far-field radiation at the subwavelength scale is crucial in various scientific and technological applications. We propose a thermally tunable disk design of indium tin oxide (ITO) and aluminum gallium nitride ( [...] Read more.
The utilization of optical antennas for active control of far-field radiation at the subwavelength scale is crucial in various scientific and technological applications. We propose a thermally tunable disk design of indium tin oxide (ITO) and aluminum gallium nitride (Al0.18Ga0.82As), enabling a switch between absorption and scattering. Furthermore, the control of far-field radiation pattern can be easily realized by combining ITO and Al0.18Ga0.82As to enhance or suppress emission. Our results demonstrate that hybrid structures can be dynamically tuned with temperature variations. In the proposed design, a frequency is achieved at the wavelength of 1240 nm. The thermal tunability of hybrid structures introduces new multifunctional possibilities for light manipulation, thereby enhancing the potential applications of new devices in the near-infrared range. Full article
(This article belongs to the Section Optoelectronics and Optical Materials)
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<p>Temperature-dependent materials. Refractive indices of <math display="inline"><semantics> <mi>ITO</mi> </semantics></math> and <math display="inline"><semantics> <mrow> <msub> <mi>Al</mi> <mrow> <mn>0.18</mn> </mrow> </msub> <msub> <mi>Ga</mi> <mrow> <mn>0.82</mn> </mrow> </msub> <mi>As</mi> </mrow> </semantics></math> as a function of temperature at a wavelength of <math display="inline"><semantics> <mrow> <mi>λ</mi> <mo>=</mo> <mn>1240</mn> </mrow> </semantics></math> nm.</p>
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<p>Optical response of the epsilon-near-zero (ENZ) material. (<b>a</b>) Total scattering cross-section (normalized to <math display="inline"><semantics> <mrow> <msup> <mi>λ</mi> <mn>2</mn> </msup> <mo>/</mo> <mn>2</mn> <mi>π</mi> </mrow> </semantics></math>) and contributions from various electric and magnetic multipole moments as a function of the temperature for the <math display="inline"><semantics> <mi>ITO</mi> </semantics></math> antenna. (<b>b</b>) Scattering, absorption, and extinction cross-sections as functions of temperature for <math display="inline"><semantics> <mrow> <mi>H</mi> <mo>=</mo> <mn>150</mn> </mrow> </semantics></math> nm, and <math display="inline"><semantics> <mrow> <mi>D</mi> <mo>=</mo> <mn>600</mn> </mrow> </semantics></math> nm. (<b>c1</b>–<b>c5</b>) Far-field radiation patterns at five temperatures.</p>
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<p>Optical response of the <math display="inline"><semantics> <mrow> <msub> <mi>Al</mi> <mrow> <mn>0.18</mn> </mrow> </msub> <msub> <mi>Ga</mi> <mrow> <mn>0.82</mn> </mrow> </msub> </mrow> </semantics></math> material. (<b>a</b>) Total scattering cross-section <math display="inline"><semantics> <msub> <mi>C</mi> <mi>sca</mi> </msub> </semantics></math> (normalized to <math display="inline"><semantics> <mrow> <msup> <mi>λ</mi> <mn>2</mn> </msup> <mo>/</mo> <mn>2</mn> <mi>π</mi> </mrow> </semantics></math>) of the ITO antenna as a function of height <span class="html-italic">H</span> and the temperature <span class="html-italic">T</span>, where the diameter of the antenna <math display="inline"><semantics> <mrow> <mi>D</mi> <mo>=</mo> <mn>600</mn> </mrow> </semantics></math> nm. (<b>b</b>) Total scattering cross-section (normalized to <math display="inline"><semantics> <mrow> <msup> <mi>λ</mi> <mn>2</mn> </msup> <mo>/</mo> <mn>2</mn> <mi>π</mi> </mrow> </semantics></math>) and contribution of different electric and magnetic multipole moments as a function of the temperature for the <math display="inline"><semantics> <mi>ITO</mi> </semantics></math> antenna with <math display="inline"><semantics> <mrow> <mi>H</mi> <mo>=</mo> <mn>150</mn> </mrow> </semantics></math> nm, <math display="inline"><semantics> <mrow> <mi>D</mi> <mo>=</mo> <mn>600</mn> </mrow> </semantics></math> nm. (<b>c1</b>–<b>c5</b>) Far-field radiation patterns in five temperatures when the <math display="inline"><semantics> <mi>ITO</mi> </semantics></math> antenna with <math display="inline"><semantics> <mrow> <mi>H</mi> <mo>=</mo> <mn>150</mn> </mrow> </semantics></math> nm, <math display="inline"><semantics> <mrow> <mi>D</mi> <mo>=</mo> <mn>600</mn> </mrow> </semantics></math> nm.</p>
Full article ">Figure 4
<p>Scattering of hybrid antenna. (<b>a</b>) The hybrid structure for the top and bottom illumination directions, i.e., <math display="inline"><semantics> <mrow> <mi mathvariant="bold">k</mi> <mo>=</mo> <mo>±</mo> <msub> <mi>k</mi> <mn>0</mn> </msub> <msub> <mi mathvariant="bold">e</mi> <mi>z</mi> </msub> </mrow> </semantics></math>; (b) total extinction (<math display="inline"><semantics> <msubsup> <mi>C</mi> <mrow> <mi>ext</mi> </mrow> <mo>±</mo> </msubsup> </semantics></math>), scattering (<math display="inline"><semantics> <msubsup> <mi>C</mi> <mrow> <mi>sca</mi> </mrow> <mo>±</mo> </msubsup> </semantics></math>), and absorption (<math display="inline"><semantics> <msubsup> <mi>C</mi> <mrow> <mi>abs</mi> </mrow> <mo>±</mo> </msubsup> </semantics></math>) cross-section (normalized to <math display="inline"><semantics> <mrow> <msup> <mi>λ</mi> <mn>2</mn> </msup> <mo>/</mo> <mn>2</mn> <mi>π</mi> </mrow> </semantics></math>) of the hybrid antenna as a function of the temperature for the <math display="inline"><semantics> <mi>ITO</mi> </semantics></math> antenna. Total scattering cross-section (normalized to <math display="inline"><semantics> <mrow> <msup> <mi>λ</mi> <mn>2</mn> </msup> <mo>/</mo> <mn>2</mn> <mi>π</mi> </mrow> </semantics></math>) and contribution of different electric and magnetic multipole moments as a function of the temperature (<b>c</b>) for the bottom illumination (<b>d</b>) for the top illumination. The diameter is 600 nm, the height of ITO and <math display="inline"><semantics> <mrow> <msub> <mi>Al</mi> <mrow> <mn>0.18</mn> </mrow> </msub> <msub> <mi>Ga</mi> <mrow> <mn>0.82</mn> </mrow> </msub> <mi>As</mi> </mrow> </semantics></math> are <math display="inline"><semantics> <mrow> <msub> <mi>H</mi> <mi>ITO</mi> </msub> <mo>=</mo> <mn>400</mn> </mrow> </semantics></math> nm and <math display="inline"><semantics> <mrow> <msub> <mi>H</mi> <mrow> <msub> <mi>Al</mi> <mrow> <mn>0.18</mn> </mrow> </msub> <msub> <mi>Ga</mi> <mrow> <mn>0.82</mn> </mrow> </msub> <mi>As</mi> </mrow> </msub> <mo>=</mo> <mn>150</mn> </mrow> </semantics></math> nm, respectively.</p>
Full article ">Figure 5
<p>Radiation patterns of hybrid antenna. (<b>a1</b>–<b>a5</b>) Evolution of representative radiation patterns for the bottom illumination direction, i.e., <math display="inline"><semantics> <mrow> <mi mathvariant="bold">k</mi> <mo>=</mo> <mo>+</mo> <msub> <mi>k</mi> <mn>0</mn> </msub> <msub> <mi mathvariant="bold">e</mi> <mi>z</mi> </msub> </mrow> </semantics></math>, increases 299 to 2000 <math display="inline"><semantics> <mi mathvariant="normal">K</mi> </semantics></math>. (<b>b1</b>–<b>b5</b>) The radiation patterns for the top illumination direction, i.e., <math display="inline"><semantics> <mrow> <mi mathvariant="bold">k</mi> <mo>=</mo> <mo>−</mo> <msub> <mi>k</mi> <mn>0</mn> </msub> <msub> <mi mathvariant="bold">e</mi> <mi>z</mi> </msub> </mrow> </semantics></math>, increases from 299 to 2000 <math display="inline"><semantics> <mi mathvariant="normal">K</mi> </semantics></math>.</p>
Full article ">Figure A1
<p>(<b>a</b>) The radiation patterns in (<b>a</b>) XZ plane, (<b>b</b>) YZ plane, (<b>c</b>) XY plane in different height <math display="inline"><semantics> <mrow> <mi>H</mi> <mo>=</mo> <mn>200</mn> <mo>,</mo> <mn>400</mn> <mo>,</mo> <mn>600</mn> <mo>,</mo> <mn>800</mn> <mo>,</mo> <mn>1000</mn> </mrow> </semantics></math> nm with the diameter <math display="inline"><semantics> <mrow> <mi>D</mi> <mo>=</mo> <mn>200</mn> </mrow> </semantics></math> nm. (<b>d</b>–<b>f</b>) Same as (<b>a</b>–<b>c</b>) in different height <math display="inline"><semantics> <mrow> <mi>H</mi> <mo>=</mo> <mn>200</mn> <mo>,</mo> <mn>400</mn> <mo>,</mo> <mn>600</mn> <mo>,</mo> <mn>800</mn> <mo>,</mo> <mn>1000</mn> </mrow> </semantics></math> nm with the diameter <math display="inline"><semantics> <mrow> <mi>D</mi> <mo>=</mo> <mn>1000</mn> </mrow> </semantics></math> nm.</p>
Full article ">Figure A2
<p>The extinction, absorption, and scattering cross-section of the ITO antenna as a function of height <span class="html-italic">H</span> (<b>a</b>) with diameter <math display="inline"><semantics> <mrow> <mi>D</mi> <mo>=</mo> <mn>200</mn> </mrow> </semantics></math> nm. (<b>b</b>) With diameter <math display="inline"><semantics> <mrow> <mi>D</mi> <mo>=</mo> <mn>1000</mn> </mrow> </semantics></math> nm. (<b>c</b>) When diameter <math display="inline"><semantics> <mrow> <mi>D</mi> <mo>=</mo> <mn>200</mn> </mrow> </semantics></math> nm, the contribution of different multipole moments ED, MD, EQ, and MQ, respectively. (<b>d</b>) When diameter <math display="inline"><semantics> <mrow> <mi>D</mi> <mo>=</mo> <mn>1000</mn> </mrow> </semantics></math> nm, the contribution of different multipole moments ED, MD, EQ, and MQ, respectively.</p>
Full article ">Figure A3
<p>(<b>a</b>–<b>l</b>) When the diameter <math display="inline"><semantics> <mrow> <mi>D</mi> <mo>=</mo> <mn>600</mn> </mrow> </semantics></math> nm, the contribution of different multipole moments ED, MD, EQ, MQ, and the scattering cross-section (normalized to <math display="inline"><semantics> <mrow> <msup> <mi>λ</mi> <mn>2</mn> </msup> <mo>/</mo> <mn>2</mn> <mi>π</mi> </mrow> </semantics></math>) as a function of the temperature for different height <span class="html-italic">H</span>.</p>
Full article ">Figure A4
<p>(<b>a1</b>–<b>a5</b>) Far-field radiation patterns in five temperatures when the ITO antenna with <math display="inline"><semantics> <mrow> <mi>H</mi> <mo>=</mo> <mn>600</mn> </mrow> </semantics></math> nm, <math display="inline"><semantics> <mrow> <mi>D</mi> <mo>=</mo> <mn>600</mn> </mrow> </semantics></math> nm.</p>
Full article ">Figure A5
<p>(<b>a</b>) The electric field distribution in <math display="inline"><semantics> <mrow> <mi>X</mi> <mi>Z</mi> </mrow> </semantics></math> plane of the hybrid structure for opposite illumination for the bottom illumination direction when <math display="inline"><semantics> <mrow> <mi>T</mi> <mo>=</mo> <mn>299</mn> </mrow> </semantics></math> K. (<b>b</b>) The field distribution in <math display="inline"><semantics> <mrow> <mi>X</mi> <mi>Z</mi> </mrow> </semantics></math> plane of the hybrid structure for opposite illumination for the bottom illumination direction when <math display="inline"><semantics> <mrow> <mi>T</mi> <mo>=</mo> <mn>2000</mn> </mrow> </semantics></math> K. (<b>c</b>,<b>d</b>) Same as (<b>a</b>,<b>b</b>) for the top illumination.</p>
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