Tim Patten, Sebastian H. Röttger, Peter G. Jones, Daniel B. Werz, Anna Krawczuk
Understanding how molecular packing governs solid-state fluorescence is key to unlocking new emissive materials. A comprehensive study of BODIPY derivatives with diverse substitution patterns is presented, showing how these modifications govern intermolecular interactions, packing motifs, and ultimately photophysical behavior in the solid state. Substituent effects dictate whether π–π stacking, hydrogen bonding, or halogen interactions dominate, resulting in distinct emission shifts and variations in fluorescence quantum yield. While increased chromophore overlap often leads to bathochromic emission, it also correlates with reduced quantum efficiency because of enhanced non-radiative relaxation processes. Notably, compounds with similar degrees of overlap can exhibit different emission profiles, underscoring the pivotal role of substituent-controlled packing. These insights provide a foundation for rational design of solid-state luminescent materials based on BODIPY scaffolds.
{"title":"Tuning Solid-State Fluorescence in BODIPY Dyes through Substitution-Controlled Packing Motifs","authors":"Tim Patten, Sebastian H. Röttger, Peter G. Jones, Daniel B. Werz, Anna Krawczuk","doi":"10.1002/adom.202502067","DOIUrl":"https://doi.org/10.1002/adom.202502067","url":null,"abstract":"<p>Understanding how molecular packing governs solid-state fluorescence is key to unlocking new emissive materials. A comprehensive study of BODIPY derivatives with diverse substitution patterns is presented, showing how these modifications govern intermolecular interactions, packing motifs, and ultimately photophysical behavior in the solid state. Substituent effects dictate whether <i>π–π</i> stacking, hydrogen bonding, or halogen interactions dominate, resulting in distinct emission shifts and variations in fluorescence quantum yield. While increased chromophore overlap often leads to bathochromic emission, it also correlates with reduced quantum efficiency because of enhanced non-radiative relaxation processes. Notably, compounds with similar degrees of overlap can exhibit different emission profiles, underscoring the pivotal role of substituent-controlled packing. These insights provide a foundation for rational design of solid-state luminescent materials based on BODIPY scaffolds.</p>","PeriodicalId":116,"journal":{"name":"Advanced Optical Materials","volume":"14 2","pages":""},"PeriodicalIF":7.2,"publicationDate":"2025-11-23","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"https://advanced.onlinelibrary.wiley.com/doi/epdf/10.1002/adom.202502067","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"145970204","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":2,"RegionCategory":"材料科学","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"OA","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
The development of blue-excitable deep-red phosphors represents a key advancement in next-generation agricultural lighting systems. Herein, a low-coordination polyhedral engineering strategy is proposed using novel K3Y1-xLux(BO3)2:Eu2+ to enable tunable broadband emission from 650 to 690 nm via Y3+→Lu3+ substitution, achieving blue-light-excitable deep-red luminescence that is uncommon among borate phosphors. Structural analysis reveals that Lu-induced lattice compression shortens the bond lengths in KO6 and Lu/YO6 octahedra, enhancing crystal field splitting and enabling deep-red emission with a full width at half maximum (FWHM) of 147 nm. Simultaneously, the photoluminescence quantum yield and thermal stability are significantly improved due to optimized Eu2+ site occupancy and suppression of non-radiative transitions. Density functional theory calculations and Hirshfeld surface analysis confirm that the shortened bond lengths and distorted polyhedra contribute to the enhanced luminescence properties. Prototype phosphor-converted LEDs based on K3Lu(BO3)2:Eu2+ demonstrate excellent spectral overlap with chlorophyll and phytochrome absorption, accelerating wheat growth by 20% under tailored illumination. This work not only addresses the long-standing challenge of achieving deep-red emission in borate phosphors but also introduces a promising material for next-generation agricultural lighting applications.
{"title":"Activating Deep-Red Emission in Borate Phosphors via Low-Coordination Engineering for Efficient Plant Lighting","authors":"Dehong Li, Yawen Deng, Chengyan Gao, Qiufeng Shi, Haijie Guo, Lei Wang, Xiao-jun Wang, Jianwei Qiao","doi":"10.1002/adom.202502204","DOIUrl":"https://doi.org/10.1002/adom.202502204","url":null,"abstract":"<p>The development of blue-excitable deep-red phosphors represents a key advancement in next-generation agricultural lighting systems. Herein, a low-coordination polyhedral engineering strategy is proposed using novel K<sub>3</sub>Y<sub>1-</sub><i><sub>x</sub></i>Lu<i><sub>x</sub></i>(BO<sub>3</sub>)<sub>2</sub>:Eu<sup>2+</sup> to enable tunable broadband emission from 650 to 690 nm via Y<sup>3+</sup>→Lu<sup>3+</sup> substitution, achieving blue-light-excitable deep-red luminescence that is uncommon among borate phosphors. Structural analysis reveals that Lu-induced lattice compression shortens the bond lengths in KO<sub>6</sub> and Lu/YO<sub>6</sub> octahedra, enhancing crystal field splitting and enabling deep-red emission with a full width at half maximum (FWHM) of 147 nm. Simultaneously, the photoluminescence quantum yield and thermal stability are significantly improved due to optimized Eu<sup>2+</sup> site occupancy and suppression of non-radiative transitions. Density functional theory calculations and Hirshfeld surface analysis confirm that the shortened bond lengths and distorted polyhedra contribute to the enhanced luminescence properties. Prototype phosphor-converted LEDs based on K<sub>3</sub>Lu(BO<sub>3</sub>)<sub>2</sub>:Eu<sup>2+</sup> demonstrate excellent spectral overlap with chlorophyll and phytochrome absorption, accelerating wheat growth by 20% under tailored illumination. This work not only addresses the long-standing challenge of achieving deep-red emission in borate phosphors but also introduces a promising material for next-generation agricultural lighting applications.</p>","PeriodicalId":116,"journal":{"name":"Advanced Optical Materials","volume":"14 2","pages":""},"PeriodicalIF":7.2,"publicationDate":"2025-11-23","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"145970206","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":2,"RegionCategory":"材料科学","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Bjoern F. Hill, Jiaqi Li, Norman Labedzki, Christina Derichsweiler, Janus A. C. Wartmann, Krisztian Neutsch, Luise Erpenbeck, Sebastian Kruss
The near infrared (NIR, >800 nm) or short wave infrared (SWIR) range of the electromagnetic spectrum overlays with the tissue transparency window and the telecommunication window, which makes it important for photonics.
Here, a persistent NIR tail and a feature at 923 nm is observed during the photochemical generation of singlet oxygen using various photosensitizers. This feature initially appears to originate from singlet oxygen as its energy fits to known higher order optical and vibrational transitions, and it occurs simultaneously with the characteristic singlet oxygen phosphorescence at 1275 nm. The emission is present under all photochemical conditions (photosensitizers, solvents, excitation sources and optical setups) but it is not observed for chemically generated singlet oxygen. Its intensity correlates with photosensitizer concentration (1 µM – 1 mM), excitation intensity, and the visible fluorescence intensity, but does not require the presence of oxygen.
A simulation shows that this feature arises from the NIR-tail of (visible) photosensitizer emission and the non-linear increase of detector sensitivities in the range between 900– 950 nm. At the same time, this signal correlates with photochemically generated singlet oxygen concentration. Thus, this NIR signal contains valuable information, but careful interpretation is required.
{"title":"A Near Infrared Emission Feature from Visible Fluorescence Tails and its Correlation with Singlet Oxygen","authors":"Bjoern F. Hill, Jiaqi Li, Norman Labedzki, Christina Derichsweiler, Janus A. C. Wartmann, Krisztian Neutsch, Luise Erpenbeck, Sebastian Kruss","doi":"10.1002/adom.202502942","DOIUrl":"https://doi.org/10.1002/adom.202502942","url":null,"abstract":"<p>The near infrared (NIR, >800 nm) or short wave infrared (SWIR) range of the electromagnetic spectrum overlays with the tissue transparency window and the telecommunication window, which makes it important for photonics.</p><p>Here, a persistent NIR tail and a feature at 923 nm is observed during the photochemical generation of singlet oxygen using various photosensitizers. This feature initially appears to originate from singlet oxygen as its energy fits to known higher order optical and vibrational transitions, and it occurs simultaneously with the characteristic singlet oxygen phosphorescence at 1275 nm. The emission is present under all photochemical conditions (photosensitizers, solvents, excitation sources and optical setups) but it is not observed for chemically generated singlet oxygen. Its intensity correlates with photosensitizer concentration (1 µM – 1 mM), excitation intensity, and the visible fluorescence intensity, but does not require the presence of oxygen.</p><p>A simulation shows that this feature arises from the NIR-tail of (visible) photosensitizer emission and the non-linear increase of detector sensitivities in the range between 900– 950 nm. At the same time, this signal correlates with photochemically generated singlet oxygen concentration. Thus, this NIR signal contains valuable information, but careful interpretation is required.</p>","PeriodicalId":116,"journal":{"name":"Advanced Optical Materials","volume":"14 2","pages":""},"PeriodicalIF":7.2,"publicationDate":"2025-11-23","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"https://advanced.onlinelibrary.wiley.com/doi/epdf/10.1002/adom.202502942","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"145970203","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":2,"RegionCategory":"材料科学","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"OA","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Although high-efficiency blue fluorescent TBPe-based organic light-emitting diodes (OLEDs) are reported, the microscopic mechanisms of excited states in TBPe emitters remain vague. Here, using fingerprint magneto-electroluminescence probing tools, hot excitons and their high-level reverse inter-system crossing (HL-RISC, S1←T2) and triplet fusion (T2F, T2+T2→Sn→S1) in TBPe are discovered for the first time, which is also consistently demonstrated by their transient-electroluminescence. Interestingly, all their rich microscopic physical behaviors can be reasonably explained within the framework of excited state dynamics involved in these TBPe-based OLEDs. The carrier mobility, polarity, and triplet energy of host materials can significantly affect the number of generated T2,TBPe hot-excitons and thus the probabilities of HL-RISC and T2F channels, which are further modulated by exothermic low-level Dexter energy transfer (DET) or endothermic high-level DET channels of cold or hot excitons. Moreover, utilizing the HL-RISC channel of hot excitons in TBPe dopants with the conventional low-level RISC channel of an exciplex co-host, a relatively high external quantum efficiency of 7.09% is achieved from blue fluorescent TBPe-doped OLEDs. Thus, this work renews the physical understanding of the microscopic evolution channels of excited states in TBPe emitters and lays a solid foundation for further designing high-efficiency blue fluorescent OLEDs.
{"title":"Discovery of Hot Excitons from the Conventional Blue Fluorescent TBPe Emitter and their Microscopic Evolution Channels Mediated by Host Materials","authors":"Jingjing Wang, Jing Chen, Jun Yang, Yinqiong Zhou, Keyi Zhang, Feng Chen, Qiang Li, Yuanjun Li, Jinfeng Guo, Zuhong Xiong","doi":"10.1002/adom.202501580","DOIUrl":"https://doi.org/10.1002/adom.202501580","url":null,"abstract":"<p>Although high-efficiency blue fluorescent TBPe-based organic light-emitting diodes (OLEDs) are reported, the microscopic mechanisms of excited states in TBPe emitters remain vague. Here, using fingerprint magneto-electroluminescence probing tools, hot excitons and their high-level reverse inter-system crossing (HL-RISC, S<sub>1</sub>←T<sub>2</sub>) and triplet fusion (T<sub>2</sub>F, T<sub>2</sub>+T<sub>2</sub>→S<sub>n</sub>→S<sub>1</sub>) in TBPe are discovered for the first time, which is also consistently demonstrated by their transient-electroluminescence. Interestingly, all their rich microscopic physical behaviors can be reasonably explained within the framework of excited state dynamics involved in these TBPe-based OLEDs. The carrier mobility, polarity, and triplet energy of host materials can significantly affect the number of generated T<sub>2,TBPe</sub> hot-excitons and thus the probabilities of HL-RISC and T<sub>2</sub>F channels, which are further modulated by exothermic low-level Dexter energy transfer (DET) or endothermic high-level DET channels of cold or hot excitons. Moreover, utilizing the HL-RISC channel of hot excitons in TBPe dopants with the conventional low-level RISC channel of an exciplex co-host, a relatively high external quantum efficiency of 7.09% is achieved from blue fluorescent TBPe-doped OLEDs. Thus, this work renews the physical understanding of the microscopic evolution channels of excited states in TBPe emitters and lays a solid foundation for further designing high-efficiency blue fluorescent OLEDs.</p>","PeriodicalId":116,"journal":{"name":"Advanced Optical Materials","volume":"14 2","pages":""},"PeriodicalIF":7.2,"publicationDate":"2025-11-23","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"145970132","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":2,"RegionCategory":"材料科学","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Giovanna Palermo, Bryan Guilcapi, Radoslaw Kolkowski, Alexa Guglielmelli, Dante M. Aceti, Liliana Valente, Joseph Zyss, Lucia Petti, Giuseppe Strangi
The design and optical characterization of a plasmonic metasurface engineered to exhibit strong polarization anisotropy under both linearly and circularly polarized light is presented. The metasurface consists of geometrically asymmetric gold nanostructures arranged periodically on a glass substrate. Each nanostructure is formed by the fusion of three equilateral triangles. The nanostructures simultaneously break mirror and inversion symmetries, resulting in chiral and pseudo-chiral optical responses that manifest as linear and circular polarization-dependent spectral features. The numerical and experimental results reveal clear chiroptical effects in both near- and far-field. Near-field scanning optical microscopy confirms the excitation of polarization-selective localized plasmonic modes, with spatially distinct hot-spots lighting up under different incident polarizations. Furthermore, it is demonstrated that the metasurface exhibits a measurable enantiospecific optical response when coated with thin left- or right-handed chiral overlayers. The differential circular dichroism signals observed in the presence of opposite enantiomers highlight the potential of the metasurface for label-free chiral sensing. These findings provide new insights into the interplay between structural anisotropy, pseudo-chirality, and enantioselective interactions in planar plasmonic systems, highlighting their ability to emulate chiral optical behavior without requiring volumetric 3D structures.
{"title":"Plasmonic Metasurfaces with Structural Chirality and Pseudo-Chirality for Enhanced Circular Dichroism and Enantiomeric Recognition","authors":"Giovanna Palermo, Bryan Guilcapi, Radoslaw Kolkowski, Alexa Guglielmelli, Dante M. Aceti, Liliana Valente, Joseph Zyss, Lucia Petti, Giuseppe Strangi","doi":"10.1002/adom.202502488","DOIUrl":"https://doi.org/10.1002/adom.202502488","url":null,"abstract":"<p>The design and optical characterization of a plasmonic metasurface engineered to exhibit strong polarization anisotropy under both linearly and circularly polarized light is presented. The metasurface consists of geometrically asymmetric gold nanostructures arranged periodically on a glass substrate. Each nanostructure is formed by the fusion of three equilateral triangles. The nanostructures simultaneously break mirror and inversion symmetries, resulting in chiral and pseudo-chiral optical responses that manifest as linear and circular polarization-dependent spectral features. The numerical and experimental results reveal clear chiroptical effects in both near- and far-field. Near-field scanning optical microscopy confirms the excitation of polarization-selective localized plasmonic modes, with spatially distinct hot-spots lighting up under different incident polarizations. Furthermore, it is demonstrated that the metasurface exhibits a measurable enantiospecific optical response when coated with thin left- or right-handed chiral overlayers. The differential circular dichroism signals observed in the presence of opposite enantiomers highlight the potential of the metasurface for label-free chiral sensing. These findings provide new insights into the interplay between structural anisotropy, pseudo-chirality, and enantioselective interactions in planar plasmonic systems, highlighting their ability to emulate chiral optical behavior without requiring volumetric 3D structures.</p>","PeriodicalId":116,"journal":{"name":"Advanced Optical Materials","volume":"14 1","pages":""},"PeriodicalIF":7.2,"publicationDate":"2025-11-21","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"https://advanced.onlinelibrary.wiley.com/doi/epdf/10.1002/adom.202502488","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"145964393","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":2,"RegionCategory":"材料科学","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"OA","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Flexible perovskite solar cells (F-PSCs) have attracted extensive research attention due to their high power-to-weight ratios, low cost, and scalable production, as well as their potential applications in self-powered wearable devices, space photovoltaics, and the Internet of Things. The power conversion efficiency (PCE) of F-PSCs has increased remarkably to 25.44%, and their mechanical and environmental stability have also been substantially enhanced through advancements in the development of novel materials for each functional layer and interface, as well as the refinement of fabrication techniques. This review provides a systematic overview of recent progress in novel materials for obtaining high-quality functional layers and effective strategies for optimizing the interface between the charge-transport layer and the perovskite. The fabrication techniques from the laboratory to industrial production, as well as the potential applications of F-PSCs, are also discussed. Finally, the future prospects for the further development of F-PSCs are outlined, including the development of novel materials, the advancement of fabrication techniques, and the realization of commercial applications.
{"title":"A Comprehensive Review of Recent Advances in Flexible Perovskite Solar Cells: Materials, Fabrication, and Applications","authors":"Zexia Liu, Yaxin Wang, Dawei Luo, Zhuang Xie, Zhike Liu, Qiang Peng, Shengzhong (Frank) Liu, Yuwei Duan","doi":"10.1002/adom.202501157","DOIUrl":"https://doi.org/10.1002/adom.202501157","url":null,"abstract":"<p>Flexible perovskite solar cells (F-PSCs) have attracted extensive research attention due to their high power-to-weight ratios, low cost, and scalable production, as well as their potential applications in self-powered wearable devices, space photovoltaics, and the Internet of Things. The power conversion efficiency (PCE) of F-PSCs has increased remarkably to 25.44%, and their mechanical and environmental stability have also been substantially enhanced through advancements in the development of novel materials for each functional layer and interface, as well as the refinement of fabrication techniques. This review provides a systematic overview of recent progress in novel materials for obtaining high-quality functional layers and effective strategies for optimizing the interface between the charge-transport layer and the perovskite. The fabrication techniques from the laboratory to industrial production, as well as the potential applications of F-PSCs, are also discussed. Finally, the future prospects for the further development of F-PSCs are outlined, including the development of novel materials, the advancement of fabrication techniques, and the realization of commercial applications.</p>","PeriodicalId":116,"journal":{"name":"Advanced Optical Materials","volume":"14 1","pages":""},"PeriodicalIF":7.2,"publicationDate":"2025-11-21","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"145964394","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":2,"RegionCategory":"材料科学","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Chiral hybrid metal halides (CHMHs) have attracted extensive attention in the field of circularly polarized luminescence (CPL) due to their fascinating intrinsic chirality, simple synthetic method, and excellent photoelectric properties. However, it remains a huge challenge to simultaneously boost the CPL dissymmetry factor (glum) and the photoluminescence quantum yield (PLQY). In this study, a pair of non-emissive indium-based CHMHs, namely (R/S-C5H13NO)3InCl6, is first synthesized. Then, sequential incorporation of NH4+ and Sb3+ ions progressively boosted self-trapped exciton (STE) emission. The resultant (R/S-C5H13NO)2NH4InCl6:Sb (2-R/SInSb) not only achieves near-unity PLQYs but also exhibits remarkable glum of +9.4 × 10−3/−9.1 × 10−3. Experimental investigations reveal that the introduction of NH4+ increases the distortion of metal-halogen octahedra, thus strengthening the STE emission. In addition, NH4+ can modulate the distribution of hydrogen bonds around inorganic octahedra and chiral cations, which is conducive to the transmission and amplification of chiral signals. Based on the efficient CPL characteristics, 2-SInSb is further employed in a scintillation film, achieving a spatial resolution of 8.7 lp mm−1 and high-quality X-ray imaging. These findings highlight the potential of indium-based CHMHs as high-performance CPL emitters and underscore their promise for X-ray imaging applications.
{"title":"Progressive Enhancement of Circularly Polarized Luminescence in Chiral Hybrid Indium Halides via Incorporating NH4+ and Sb3+ Ions for X-ray Imaging","authors":"Yongkang Zhu, Yong Yang, Xinyu Gao, Feiyang Li, Lifan Zeng, Yongjing Deng, Shujuan Liu, Qiang Zhao","doi":"10.1002/adom.202502972","DOIUrl":"https://doi.org/10.1002/adom.202502972","url":null,"abstract":"<p>Chiral hybrid metal halides (CHMHs) have attracted extensive attention in the field of circularly polarized luminescence (CPL) due to their fascinating intrinsic chirality, simple synthetic method, and excellent photoelectric properties. However, it remains a huge challenge to simultaneously boost the CPL dissymmetry factor (g<sub>lum</sub>) and the photoluminescence quantum yield (PLQY). In this study, a pair of non-emissive indium-based CHMHs, namely (R/S-C<sub>5</sub>H<sub>13</sub>NO)<sub>3</sub>InCl<sub>6</sub>, is first synthesized. Then, sequential incorporation of NH<sub>4</sub><sup>+</sup> and Sb<sup>3+</sup> ions progressively boosted self-trapped exciton (STE) emission. The resultant (R/S-C<sub>5</sub>H<sub>13</sub>NO)<sub>2</sub>NH<sub>4</sub>InCl<sub>6</sub>:Sb (2-R/SInSb) not only achieves near-unity PLQYs but also exhibits remarkable g<sub>lum</sub> of +9.4 × 10<sup>−3</sup>/−9.1 × 10<sup>−3</sup>. Experimental investigations reveal that the introduction of NH<sub>4</sub><sup>+</sup> increases the distortion of metal-halogen octahedra, thus strengthening the STE emission. In addition, NH<sub>4</sub><sup>+</sup> can modulate the distribution of hydrogen bonds around inorganic octahedra and chiral cations, which is conducive to the transmission and amplification of chiral signals. Based on the efficient CPL characteristics, 2-SInSb is further employed in a scintillation film, achieving a spatial resolution of 8.7 lp mm<sup>−1</sup> and high-quality X-ray imaging. These findings highlight the potential of indium-based CHMHs as high-performance CPL emitters and underscore their promise for X-ray imaging applications.</p>","PeriodicalId":116,"journal":{"name":"Advanced Optical Materials","volume":"14 2","pages":""},"PeriodicalIF":7.2,"publicationDate":"2025-11-21","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"145969990","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":2,"RegionCategory":"材料科学","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Ricardo Chavez-Jimenez, Gustavo González-Gaitano, Julio Fernandez-Cestau, Mattia Nieddu, Juan Pablo Fuenzalida-Werner
Materials and supramolecular structures with the ability to emit circularly polarized luminescence (CPL) are a necessity because they represent an advancement in photonic technologies for encoding, imaging, data manipulation, and chiral catalysis. However, current CPL materials often suffer from low luminescence dissymmetry and brightness, alongside sustainability challenges. This review discusses the emerging potential of biogenic molecules—specifically proteins, peptides, polysaccharides, and nucleotides—as a sustainable and effective strategy to tune and improve the CPL emission of natural or artificial organic chromophores. It highlights their structural advantages, such as hierarchical chirality, structural rigidity, and precise chromophore organization control, which significantly enhance CPL signals. Peptide-based assemblies are shown to leverage supramolecular interactions and chirality transfer mechanisms to amplify CPL. At the same time, fluorescent proteins utilize chromophore rigidity and exciton coupling to achieve a high CPL brightness. Nucleotide-based systems further showcase control over chromophore alignment, enabling dynamic and reversible CPL emission. Polysaccharides of different classes provide versatile, chiral scaffolds for inducing CPL through ordered aggregation and templating effects that can also be generated in vivo. Collectively, these biogenic approaches are key candidates for next-generation CPL-active materials.
{"title":"Biogenic Next-Gen CPL Emitters: Strategies with Proteins, Polysaccharides, and Nucleotides","authors":"Ricardo Chavez-Jimenez, Gustavo González-Gaitano, Julio Fernandez-Cestau, Mattia Nieddu, Juan Pablo Fuenzalida-Werner","doi":"10.1002/adom.202502221","DOIUrl":"https://doi.org/10.1002/adom.202502221","url":null,"abstract":"<p>Materials and supramolecular structures with the ability to emit circularly polarized luminescence (CPL) are a necessity because they represent an advancement in photonic technologies for encoding, imaging, data manipulation, and chiral catalysis. However, current CPL materials often suffer from low luminescence dissymmetry and brightness, alongside sustainability challenges. This review discusses the emerging potential of biogenic molecules—specifically proteins, peptides, polysaccharides, and nucleotides—as a sustainable and effective strategy to tune and improve the CPL emission of natural or artificial organic chromophores. It highlights their structural advantages, such as hierarchical chirality, structural rigidity, and precise chromophore organization control, which significantly enhance CPL signals. Peptide-based assemblies are shown to leverage supramolecular interactions and chirality transfer mechanisms to amplify CPL. At the same time, fluorescent proteins utilize chromophore rigidity and exciton coupling to achieve a high CPL brightness. Nucleotide-based systems further showcase control over chromophore alignment, enabling dynamic and reversible CPL emission. Polysaccharides of different classes provide versatile, chiral scaffolds for inducing CPL through ordered aggregation and templating effects that can also be generated in vivo. Collectively, these biogenic approaches are key candidates for next-generation CPL-active materials.</p>","PeriodicalId":116,"journal":{"name":"Advanced Optical Materials","volume":"14 1","pages":""},"PeriodicalIF":7.2,"publicationDate":"2025-11-21","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"https://advanced.onlinelibrary.wiley.com/doi/epdf/10.1002/adom.202502221","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"145983702","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":2,"RegionCategory":"材料科学","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"OA","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
The recombination rate and the exciton annihilation rates are crucial for understanding the exciton dynamics in organic light-emitting diodes (OLEDs). In this work, the recombination rate is determined from the relative carrier mobility estimated using a time-correlated single photon counting-based transient electroluminescence measurement. The estimation of the recombination rate from the carrier mobility for the thermally activated delayed fluorescence (TADF) emitter dimethyl-9,10-dihydropyridine-diphenyl sulphone (DMAC-DPS) and its blends helps to understand the effect of the host and dopants. The pristine devices show an enhanced recombination rate compared to the blended device, due to the high-field dependence factor estimated from the Poole–Frenkel behavior. Furthermore, the exciton–exciton annihilation rates in both systems are quantified using a kinetic model for optical excitation employing a global optimization method based on a genetic algorithm. The results indicate that in the blended DMAC-DPS system, the exciton–exciton annihilations are significantly reduced in comparison to the pristine system. Comparison of pristine and blended systems reveals the host–guest interactions governing recombination dynamics and exciton losses in practical OLEDs.
{"title":"Elucidating the Recombination and Annihilation Rates in Blue Thermally Activated Delayed Fluorescence Emitter-Based OLEDs Using Transient Measurements","authors":"Dinesh Kumar Shanmugham, Dhruvajyoti Barah, Debdutta Ray, Jayeeta Bhattacharyya","doi":"10.1002/adom.202502165","DOIUrl":"https://doi.org/10.1002/adom.202502165","url":null,"abstract":"<p>The recombination rate and the exciton annihilation rates are crucial for understanding the exciton dynamics in organic light-emitting diodes (OLEDs). In this work, the recombination rate is determined from the relative carrier mobility estimated using a time-correlated single photon counting-based transient electroluminescence measurement. The estimation of the recombination rate from the carrier mobility for the thermally activated delayed fluorescence (TADF) emitter dimethyl-9,10-dihydropyridine-diphenyl sulphone (DMAC-DPS) and its blends helps to understand the effect of the host and dopants. The pristine devices show an enhanced recombination rate compared to the blended device, due to the high-field dependence factor estimated from the Poole–Frenkel behavior. Furthermore, the exciton–exciton annihilation rates in both systems are quantified using a kinetic model for optical excitation employing a global optimization method based on a genetic algorithm. The results indicate that in the blended DMAC-DPS system, the exciton–exciton annihilations are significantly reduced in comparison to the pristine system. Comparison of pristine and blended systems reveals the host–guest interactions governing recombination dynamics and exciton losses in practical OLEDs.</p>","PeriodicalId":116,"journal":{"name":"Advanced Optical Materials","volume":"14 1","pages":""},"PeriodicalIF":7.2,"publicationDate":"2025-11-21","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"145958130","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":2,"RegionCategory":"材料科学","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
With the growing demand for smart sensing and information encryption technologies, stimuli-responsive luminescent materials are emerging as key candidates for temperature monitoring and security applications. This study presents a Mn2+-based hybrid halide, (MAMP)MnBr3·Br [MAMP = 2-[(methylamino)methyl]pyridine], exhibiting reversible thermochromic luminescence, ideal for smart thermal sensing. The material undergoes a red-to-green emission shift triggered by a heat-induced coordination transformation, transitioning from octahedral [MnBr6]4− to tetrahedral [MnBr4]2− units. Upon heating to 455 K, the Mn-Br bonds are broken, leading to a structural transformation from octahedral [MnBr6]4− to tetrahedral [MnBr4]2−. This coordination change causes a red-to-green luminescence shift (651–515 nm). The material delivers strong red emission at 651 nm with an internal quantum efficiency of 21.6%, exhibits high thermal stability, and demonstrates efficient X-ray scintillation. These properties make it suitable for non-contact temperature sensing and dynamic information encryption. The material's excellent performance opens new opportunities for applications in temperature history tracking, anti-counterfeiting, and flexible optoelectronic devices.
{"title":"Coordination-Driven Reversible Thermochromic Luminescence in a Hybrid Manganese Halide for Thermal Sensing","authors":"Yibo Cui, Jiawei Lin, Kunjie Liu, Yuhe Shao, Ruibin Hao, Ruonan Yao, Zhongnan Guo, Jing Zhao, Quanlin Liu","doi":"10.1002/adom.202502522","DOIUrl":"https://doi.org/10.1002/adom.202502522","url":null,"abstract":"<p>With the growing demand for smart sensing and information encryption technologies, stimuli-responsive luminescent materials are emerging as key candidates for temperature monitoring and security applications. This study presents a Mn<sup>2+</sup>-based hybrid halide, (MAMP)MnBr<sub>3</sub>·Br [MAMP = 2-[(methylamino)methyl]pyridine], exhibiting reversible thermochromic luminescence, ideal for smart thermal sensing. The material undergoes a red-to-green emission shift triggered by a heat-induced coordination transformation, transitioning from octahedral [MnBr<sub>6</sub>]<sup>4−</sup> to tetrahedral [MnBr<sub>4</sub>]<sup>2−</sup> units. Upon heating to 455 K, the Mn-Br bonds are broken, leading to a structural transformation from octahedral [MnBr<sub>6</sub>]<sup>4−</sup> to tetrahedral [MnBr<sub>4</sub>]<sup>2−</sup>. This coordination change causes a red-to-green luminescence shift (651–515 nm). The material delivers strong red emission at 651 nm with an internal quantum efficiency of 21.6%, exhibits high thermal stability, and demonstrates efficient X-ray scintillation. These properties make it suitable for non-contact temperature sensing and dynamic information encryption. The material's excellent performance opens new opportunities for applications in temperature history tracking, anti-counterfeiting, and flexible optoelectronic devices.</p>","PeriodicalId":116,"journal":{"name":"Advanced Optical Materials","volume":"14 2","pages":""},"PeriodicalIF":7.2,"publicationDate":"2025-11-21","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"145983701","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":2,"RegionCategory":"材料科学","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}