Two approaches are proposed for obtaining heterospin complexes with an anion-radical of difurazanopyrazine L – a paramagnetic derivative of 4H,8H-bis(1,2,5-oxadiazolo)[3,4-b:3′,4′-e]pyrazine. Aqua 3d metal complexes [ML2(H2O)4]·2H2O (M = Ni and Co) were synthesized using saturated solutions of reagents with a large excess of M(NO3)2. Ammine complexes [ML2(NH3)4] (M = Ni and Cu) were obtained from the reaction of M(NO3)2 with NaL(H2O)3 in a stoichiometric ratio in the presence of concentrated aqueous ammonia (28%). In all complexes, metal ions coordinate L via N atoms of the pyrazine ring. Molecules of the complexes are linked into a framework by hydrogen bonds. It was found that in [ML2(NH3)4] strong antiferromagnetic exchange interactions are realized between anion-radicals from neighboring molecules, determining the magnetic behavior of the phase as a whole. Whereas in [ML2(H2O)4]·2H2O, the exchange interactions are ferromagnetic in nature. This is due to the presence of water molecules in the structure, which provide a displacement of the complex molecules relative to each other and, as a consequence, a weakening of the interactions between adjacent L.
{"title":"Aqua and ammine 3d metal complexes with the anion-radical of difurazanopyrazine","authors":"Sergey Fokin, Svyatoslav Tolstikov, Vitaly Morozov, Arkady Samsonenko, Galina Romanenko and Artem Bogomyakov","doi":"10.1039/D5CE00836K","DOIUrl":"https://doi.org/10.1039/D5CE00836K","url":null,"abstract":"<p >Two approaches are proposed for obtaining heterospin complexes with an anion-radical of difurazanopyrazine L – a paramagnetic derivative of 4<em>H</em>,8<em>H</em>-bis(1,2,5-oxadiazolo)[3,4-b:3′,4′-<em>e</em>]pyrazine. Aqua 3d metal complexes [ML<small><sub>2</sub></small>(H<small><sub>2</sub></small>O)<small><sub>4</sub></small>]·2H<small><sub>2</sub></small>O (M = Ni and Co) were synthesized using saturated solutions of reagents with a large excess of M(NO<small><sub>3</sub></small>)<small><sub>2</sub></small>. Ammine complexes [ML<small><sub>2</sub></small>(NH<small><sub>3</sub></small>)<small><sub>4</sub></small>] (M = Ni and Cu) were obtained from the reaction of M(NO<small><sub>3</sub></small>)<small><sub>2</sub></small> with NaL(H<small><sub>2</sub></small>O)<small><sub>3</sub></small> in a stoichiometric ratio in the presence of concentrated aqueous ammonia (28%). In all complexes, metal ions coordinate L <em>via</em> N atoms of the pyrazine ring. Molecules of the complexes are linked into a framework by hydrogen bonds. It was found that in [ML<small><sub>2</sub></small>(NH<small><sub>3</sub></small>)<small><sub>4</sub></small>] strong antiferromagnetic exchange interactions are realized between anion-radicals from neighboring molecules, determining the magnetic behavior of the phase as a whole. Whereas in [ML<small><sub>2</sub></small>(H<small><sub>2</sub></small>O)<small><sub>4</sub></small>]·2H<small><sub>2</sub></small>O, the exchange interactions are ferromagnetic in nature. This is due to the presence of water molecules in the structure, which provide a displacement of the complex molecules relative to each other and, as a consequence, a weakening of the interactions between adjacent L.</p>","PeriodicalId":70,"journal":{"name":"CrystEngComm","volume":" 48","pages":" 7902-7908"},"PeriodicalIF":2.6,"publicationDate":"2025-10-29","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"145698271","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":3,"RegionCategory":"化学","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Summaya Khazir, Abdul Haseeb Shah, Jose V. Parambil and Aijaz A. Dar
Drug discovery and development is an indispensable sector of R&D, and it is of immense significance due to its relevance and direct impact on human life. However, the discovery of new drugs is an evolving and onerous process with critically low success rates, and the majority of potential drugs face physicochemical limitations. Among the known drugs, poor solubility is a serious limitation, and about 90% of discovered drugs and 40% of commercial drugs are class II and IV drugs with poor aqueous solubility. Crystal engineering has appeared as a facile, quicker, and green approach to address the physicochemical limitations of drugs, including their poor aqueous solubility, through a non-covalent strategy involving the development of polymorphs, pharmaceutical co-crystals, and organic salts. This perspective includes a discussion on the definition, classification, and nomenclature of binary crystal forms; a basic understanding of the design method of pharmaceutical co-crystals (ΔpKa rule, coformer screening, and synthon concept); synthetic methods and scale-up processes of co-crystallization; crystal nucleation; phase diagrams; and opportunities and challenges in the area.
{"title":"Crystal engineering considerations for pharmaceutical co-crystals","authors":"Summaya Khazir, Abdul Haseeb Shah, Jose V. Parambil and Aijaz A. Dar","doi":"10.1039/D5CE00820D","DOIUrl":"https://doi.org/10.1039/D5CE00820D","url":null,"abstract":"<p >Drug discovery and development is an indispensable sector of R&D, and it is of immense significance due to its relevance and direct impact on human life. However, the discovery of new drugs is an evolving and onerous process with critically low success rates, and the majority of potential drugs face physicochemical limitations. Among the known drugs, poor solubility is a serious limitation, and about 90% of discovered drugs and 40% of commercial drugs are class II and IV drugs with poor aqueous solubility. Crystal engineering has appeared as a facile, quicker, and green approach to address the physicochemical limitations of drugs, including their poor aqueous solubility, through a non-covalent strategy involving the development of polymorphs, pharmaceutical co-crystals, and organic salts. This perspective includes a discussion on the definition, classification, and nomenclature of binary crystal forms; a basic understanding of the design method of pharmaceutical co-crystals (Δp<em>K</em><small><sub>a</sub></small> rule, coformer screening, and synthon concept); synthetic methods and scale-up processes of co-crystallization; crystal nucleation; phase diagrams; and opportunities and challenges in the area.</p>","PeriodicalId":70,"journal":{"name":"CrystEngComm","volume":" 46","pages":" 7418-7442"},"PeriodicalIF":2.6,"publicationDate":"2025-10-29","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"145584715","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":3,"RegionCategory":"化学","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Lili Liu, Mengyuan Gu, Aonan Zong, Fei Chen and Weitao Su
Two-dimensional (2D) layered transition metal dichalcogenides (TMDCs) can form spiral structures via a screw-dislocation-driven mechanism, which leads to changes in their crystal symmetry and layer stackings that generate attractive physical properties different from their bulk and few-layer crystals. However, the controllable growth of 2D spiral TMDC crystals is still challenging, and the width-dependent optical properties of these spiral structures with different widths need to be further studied. Here, we report the controllable growth of high-yield 2D spiral WS2 flakes through a chemical vapor deposition route via utilizing spin-coated Na2WO4 and Na2MoO4 powders as the precursors. Systematic characterizations elucidated that these 2D spiral WS2 flakes consist of triangular monolayer flakes as the bottom part and spiral microribbons with different widths as the upper part, and the microribbons stacked on the triangular monolayer flakes present a width-dependent optical performance. Finally, the growth mechanism of these unique structures is ascribed to the existence of screw dislocations. These spiral TMDC structures are prospective candidates for probing the physical properties of layered materials and exploring novel applications in functional nanoelectronic and optoelectronic devices.
{"title":"CVD growth and width-dependent optical properties of spiral WS2 microribbons on 2D triangular monolayer WS2 flakes","authors":"Lili Liu, Mengyuan Gu, Aonan Zong, Fei Chen and Weitao Su","doi":"10.1039/D5CE00907C","DOIUrl":"https://doi.org/10.1039/D5CE00907C","url":null,"abstract":"<p >Two-dimensional (2D) layered transition metal dichalcogenides (TMDCs) can form spiral structures <em>via</em> a screw-dislocation-driven mechanism, which leads to changes in their crystal symmetry and layer stackings that generate attractive physical properties different from their bulk and few-layer crystals. However, the controllable growth of 2D spiral TMDC crystals is still challenging, and the width-dependent optical properties of these spiral structures with different widths need to be further studied. Here, we report the controllable growth of high-yield 2D spiral WS<small><sub>2</sub></small> flakes through a chemical vapor deposition route <em>via</em> utilizing spin-coated Na<small><sub>2</sub></small>WO<small><sub>4</sub></small> and Na<small><sub>2</sub></small>MoO<small><sub>4</sub></small> powders as the precursors. Systematic characterizations elucidated that these 2D spiral WS<small><sub>2</sub></small> flakes consist of triangular monolayer flakes as the bottom part and spiral microribbons with different widths as the upper part, and the microribbons stacked on the triangular monolayer flakes present a width-dependent optical performance. Finally, the growth mechanism of these unique structures is ascribed to the existence of screw dislocations. These spiral TMDC structures are prospective candidates for probing the physical properties of layered materials and exploring novel applications in functional nanoelectronic and optoelectronic devices.</p>","PeriodicalId":70,"journal":{"name":"CrystEngComm","volume":" 47","pages":" 7697-7706"},"PeriodicalIF":2.6,"publicationDate":"2025-10-29","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"145625459","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":3,"RegionCategory":"化学","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Thomas Hagger, Helena Rabelo Freitas, Chiara Mastropasqua, Ahmed El Alouani, Stefano Marinoni, Nico Kawashima, Raphael Lemerle, Kamil Artur Wodzislawski, Didem Dede, Silvana Botti, Maria Chiara Spadaro, Valerio Piazza, Adrien Michon, Jordi Arbiol, Anna Fontcuberta I Morral
Zn3P2, made from earth-abundant elements, is a promising candidate for thin-film solar cells but faces limitations due to difficulties in achieving n-type doping and its large lattice mismatch with commercial substrates and a high thermal expansion coefficient, causing defects and cracks. Graphene substrates can address these challenges thanks to its weak van der Waals interactions with Zn3P2 allowing for mechanical transfer of the thin film and strain-free growth. This study compares five graphene substrates for quasi-van der Waals epitaxial (q-vdWe) growth of polycrystalline Zn3P2 thin films using molecular beam epitaxy. Surface features like steps and wrinkles on graphene were identified as main nucleation sites for Zn3P2, provided the graphene has minimal point defects. The highest-quality thin films, with the largest grain sizes, were grown on H-CVD graphene on the Si-face of 6H-SiC, featuring solely terraces of atomic height. All substrates showed comparable growth windows for crystalline Zn3P2, with higher growth temperatures improving crystal quality, as indicated by enhanced photoluminescence. Cryo-cathodoluminescence measurements revealed spatially localized sub-bandgap emissions, potentially linked to localized strain fields at grain boundaries of up to ±3% as identified by cross-sectional transmission electron microscopy. This work provides insights into advantages and drawbacks of utilising q-vdWe to produce Zn3P2 thin films for solar cell applications and highlights the effects of graphene substrate choice and growth parameters on Zn3P2 film quality.
{"title":"Link between graphene features and the resulting functionality of quasi-van der Waals Zn<sub>3</sub>P<sub>2</sub>.","authors":"Thomas Hagger, Helena Rabelo Freitas, Chiara Mastropasqua, Ahmed El Alouani, Stefano Marinoni, Nico Kawashima, Raphael Lemerle, Kamil Artur Wodzislawski, Didem Dede, Silvana Botti, Maria Chiara Spadaro, Valerio Piazza, Adrien Michon, Jordi Arbiol, Anna Fontcuberta I Morral","doi":"10.1039/d5ce00351b","DOIUrl":"10.1039/d5ce00351b","url":null,"abstract":"<p><p>Zn<sub>3</sub>P<sub>2</sub>, made from earth-abundant elements, is a promising candidate for thin-film solar cells but faces limitations due to difficulties in achieving n-type doping and its large lattice mismatch with commercial substrates and a high thermal expansion coefficient, causing defects and cracks. Graphene substrates can address these challenges thanks to its weak van der Waals interactions with Zn<sub>3</sub>P<sub>2</sub> allowing for mechanical transfer of the thin film and strain-free growth. This study compares five graphene substrates for quasi-van der Waals epitaxial (q-vdWe) growth of polycrystalline Zn<sub>3</sub>P<sub>2</sub> thin films using molecular beam epitaxy. Surface features like steps and wrinkles on graphene were identified as main nucleation sites for Zn<sub>3</sub>P<sub>2</sub>, provided the graphene has minimal point defects. The highest-quality thin films, with the largest grain sizes, were grown on H-CVD graphene on the Si-face of 6H-SiC, featuring solely terraces of atomic height. All substrates showed comparable growth windows for crystalline Zn<sub>3</sub>P<sub>2</sub>, with higher growth temperatures improving crystal quality, as indicated by enhanced photoluminescence. Cryo-cathodoluminescence measurements revealed spatially localized sub-bandgap emissions, potentially linked to localized strain fields at grain boundaries of up to ±3% as identified by cross-sectional transmission electron microscopy. This work provides insights into advantages and drawbacks of utilising q-vdWe to produce Zn<sub>3</sub>P<sub>2</sub> thin films for solar cell applications and highlights the effects of graphene substrate choice and growth parameters on Zn<sub>3</sub>P<sub>2</sub> film quality.</p>","PeriodicalId":70,"journal":{"name":"CrystEngComm","volume":" ","pages":""},"PeriodicalIF":2.6,"publicationDate":"2025-10-29","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"https://www.ncbi.nlm.nih.gov/pmc/articles/PMC12621204/pdf/","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"145547354","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":3,"RegionCategory":"化学","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"OA","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Fazheng Huang, Xiaowei Lin, Qingyi Liu, Yan Yu, Dongfeng Xue and Lingyun Li
CaGdAlO4 (CGA) crystals are promising gain media for ultrafast lasers due to their favorable thermal and optical properties. However, color center defects often introduce unwanted optical absorption, degrading laser performance. This study identifies interstitial oxygen atoms (Oi) as the dominant source of coloration in CGA crystals through a combination of X-ray photoelectron spectroscopy, optical absorption measurements, and density functional theory calculations. The remarkable consistency between the measured and calculated absorption spectra unequivocally identifies Oi as the primary defect responsible for coloration. The incorporation of Oi introduces mid-gap electronic states, leading to strong absorption in the 250–450 nm range and imparting a yellow color. We demonstrate that controlling the atmosphere during polycrystalline synthesis is crucial, i.e., using a reducing atmosphere yields white, defect-free polycrystalline powders, which subsequently enable the growth of high-quality, colorless CGA single crystals via the Czochralski method under a N2/H2 mixed atmosphere. This work clarifies the defect origin in CGA and provides an effective strategy for producing high-optical-quality crystals for advanced photonic applications.
{"title":"Identification of interstitial oxygen color centers in CaGdAlO4 single crystals and their elimination strategy","authors":"Fazheng Huang, Xiaowei Lin, Qingyi Liu, Yan Yu, Dongfeng Xue and Lingyun Li","doi":"10.1039/D5CE00858A","DOIUrl":"https://doi.org/10.1039/D5CE00858A","url":null,"abstract":"<p >CaGdAlO<small><sub>4</sub></small> (CGA) crystals are promising gain media for ultrafast lasers due to their favorable thermal and optical properties. However, color center defects often introduce unwanted optical absorption, degrading laser performance. This study identifies interstitial oxygen atoms (O<small><sub>i</sub></small>) as the dominant source of coloration in CGA crystals through a combination of X-ray photoelectron spectroscopy, optical absorption measurements, and density functional theory calculations. The remarkable consistency between the measured and calculated absorption spectra unequivocally identifies O<small><sub>i</sub></small> as the primary defect responsible for coloration. The incorporation of O<small><sub>i</sub></small> introduces mid-gap electronic states, leading to strong absorption in the 250–450 nm range and imparting a yellow color. We demonstrate that controlling the atmosphere during polycrystalline synthesis is crucial, <em>i.e.</em>, using a reducing atmosphere yields white, defect-free polycrystalline powders, which subsequently enable the growth of high-quality, colorless CGA single crystals <em>via</em> the Czochralski method under a N<small><sub>2</sub></small>/H<small><sub>2</sub></small> mixed atmosphere. This work clarifies the defect origin in CGA and provides an effective strategy for producing high-optical-quality crystals for advanced photonic applications.</p>","PeriodicalId":70,"journal":{"name":"CrystEngComm","volume":" 46","pages":" 7540-7546"},"PeriodicalIF":2.6,"publicationDate":"2025-10-28","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"145584742","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":3,"RegionCategory":"化学","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Miao Wang, Ting Chen, Xiaohui Shen, Yanfeng Tang and Tongming Sun
A p–n BiOBr/ZnWO4 (BZ) heterojunction was synthesized and used for the photocatalytic degradation of RhB in aqueous solution under visible-light irradiation. Notably, an optimized 0.15BZ composite (mole ratio) exhibited excellent photocatalytic activity, which is 14.7 times higher than that of bare ZnWO4. The integration of p–n heterojunction at the interface of hierarchical nanoflake-assembled BiOBr flowers and nanoflake-assembled yolk–shell microspheres of ZnWO4 can efficiently promote charge separation and migration, thus significantly improving the photocatalytic performance. Electron paramagnetic resonance (EPR) spectra proved that ·OH radicals were the key reactive components. Moreover, a degradation efficiency of 89.8% was maintained after four cycles, representing good durability for the BZ photocatalyst. This work offers a reasonable way for the economic synthesis of heterojunction materials, and the high-efficiency and chemically stable BiOBr/ZnWO4 heterojunction composite might act as a promising photocatalyst in water purification applications.
{"title":"Surface functionalization of hierarchical BiOBr/ZnWO4 heterojunctions as visible-light driven photocatalysts","authors":"Miao Wang, Ting Chen, Xiaohui Shen, Yanfeng Tang and Tongming Sun","doi":"10.1039/D5CE00868A","DOIUrl":"https://doi.org/10.1039/D5CE00868A","url":null,"abstract":"<p >A p–n BiOBr/ZnWO<small><sub>4</sub></small> (BZ) heterojunction was synthesized and used for the photocatalytic degradation of RhB in aqueous solution under visible-light irradiation. Notably, an optimized 0.15BZ composite (mole ratio) exhibited excellent photocatalytic activity, which is 14.7 times higher than that of bare ZnWO<small><sub>4</sub></small>. The integration of p–n heterojunction at the interface of hierarchical nanoflake-assembled BiOBr flowers and nanoflake-assembled yolk–shell microspheres of ZnWO<small><sub>4</sub></small> can efficiently promote charge separation and migration, thus significantly improving the photocatalytic performance. Electron paramagnetic resonance (EPR) spectra proved that ·OH radicals were the key reactive components. Moreover, a degradation efficiency of 89.8% was maintained after four cycles, representing good durability for the BZ photocatalyst. This work offers a reasonable way for the economic synthesis of heterojunction materials, and the high-efficiency and chemically stable BiOBr/ZnWO<small><sub>4</sub></small> heterojunction composite might act as a promising photocatalyst in water purification applications.</p>","PeriodicalId":70,"journal":{"name":"CrystEngComm","volume":" 45","pages":" 7295-7302"},"PeriodicalIF":2.6,"publicationDate":"2025-10-28","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"145529587","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":3,"RegionCategory":"化学","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Sukhendu Bikash Samanta, Soumalya Roy, Atanu Dey and Sourav Das
In coordination chemistry research, magneto-chiral dichroism (MChD) is a unique phenomenon that occurs via the interaction of light with a magnetized chiral system. Among the various sophisticated spectroscopic techniques, MChD has become a cornerstone for probing electronic transitions in magneto-optical materials. Nevertheless, achieving strong magneto-optical responses remains a significant challenge, both experimentally, in terms of measurable signal intensity, and theoretically, in terms of accurately modelling and predicting MChD from complex electronic structures. The growing research interest in MChD stems from its dual significance: it not only offers insights into the magnetic, electronic, and chiroptical properties of molecular systems but also holds promise for technological applications such as the development of standalone optical readout mechanisms for magnetic information. The chiral heterometallic 3d–4f systems are particularly promising candidates for MChD research. Intrinsic features such as strong spin–orbit coupling, unique electronic configurations, diverse optical transitions, flexible coordination environments, and pronounced magnetic anisotropy create a molecular platform for advancing the understanding and exploration of this fascinating phenomenon. This perspective primarily highlights the current state of MChD properties in a wide range of 3d–4f coordination complexes, distilling key findings that can guide the rational design of systems with enhanced MChD effects. This article concludes by proposing experimental strategies and research directions aimed at deepening our understanding of MChD and advancing its practical applications.
{"title":"Exploring magneto-chiral dichroism in heterometallic 3d–4f complexes: recent advances and future prospects","authors":"Sukhendu Bikash Samanta, Soumalya Roy, Atanu Dey and Sourav Das","doi":"10.1039/D5CE00717H","DOIUrl":"https://doi.org/10.1039/D5CE00717H","url":null,"abstract":"<p >In coordination chemistry research, magneto-chiral dichroism (MChD) is a unique phenomenon that occurs <em>via</em> the interaction of light with a magnetized chiral system. Among the various sophisticated spectroscopic techniques, MChD has become a cornerstone for probing electronic transitions in magneto-optical materials. Nevertheless, achieving strong magneto-optical responses remains a significant challenge, both experimentally, in terms of measurable signal intensity, and theoretically, in terms of accurately modelling and predicting MChD from complex electronic structures. The growing research interest in MChD stems from its dual significance: it not only offers insights into the magnetic, electronic, and chiroptical properties of molecular systems but also holds promise for technological applications such as the development of standalone optical readout mechanisms for magnetic information. The chiral heterometallic 3d–4f systems are particularly promising candidates for MChD research. Intrinsic features such as strong spin–orbit coupling, unique electronic configurations, diverse optical transitions, flexible coordination environments, and pronounced magnetic anisotropy create a molecular platform for advancing the understanding and exploration of this fascinating phenomenon. This perspective primarily highlights the current state of MChD properties in a wide range of 3d–4f coordination complexes, distilling key findings that can guide the rational design of systems with enhanced MChD effects. This article concludes by proposing experimental strategies and research directions aimed at deepening our understanding of MChD and advancing its practical applications.</p>","PeriodicalId":70,"journal":{"name":"CrystEngComm","volume":" 47","pages":" 7615-7632"},"PeriodicalIF":2.6,"publicationDate":"2025-10-27","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"145625447","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":3,"RegionCategory":"化学","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Clare L. Stubbs, Mathew J. Bryant, Lauren E. Hatcher and Paul R. Raithby
Colour-changing chemical sensors have found important applications in the detection of low concentrations of volatile organic compounds (VOCs). Among the most promising molecular materials are platinum pincer complexes that display rapid colour changes when exposed to a variety of VOCs. In the solid state, these rapid responses have been linked to changes in non-covalent interactions between the platinum pincer molecules and the guest VOCs. To gain a better understanding of the interactions involved, we have studied the manipulation of vapochromic or solvatochromic properties in a series of square planar platinum(II) pincer complexes through structural modification of the monodentate ligand occupying the fourth coordination site. The platinum(II) complexes are based on the 1,3-di(pyridine)benzene tridentate linker (N^C^N) skeleton with the fourth site occupied by a monodentate, anionic ligand L. The formulae of the complexes synthesised are [Pt(N^C(C(O)OMe)^N)(L)] (L = (NCO) (6), (NCS) (7), (OC(O)Me) (8), (OC(O)CF3) (9), (OS(O)2CF3) (10), and (OS(O)2(C6H4Me)) (11)), and the crystalline solids and solutions of these materials have been tested for solvatochromic or vapochromic changes with VOCs including dichloromethane, acetonitrile, diethyl ether, methanol and water. The complexes 6 and 7 crystallised as yellow solids, with no solvent voids in the crystal lattice. Single-crystal X-ray analyses showed that the intermolecular Pt⋯Pt separations were too long for direct Pt⋯Pt interactions. Neither material displayed solvatochromic or vapochromic properties. However, when the fourth ligand was an acetate group, complex 8, the solid displayed vapochromism, changing colour from an orange water-containing crystalline form to an anhydrous yellow form, and a blue form when treated with methanol vapour. A crystal structure analysis showed that in the orange form adjacent pincer molecules were linked together through a hydrogen bonding network involving lattice water molecules, supported by π⋯π stacking interactions. Complexes 9 and 10 both showed solvatochromism, forming a bright yellow solid when crystallised from dichloromethane but forming an orange solid when recrystallised from acetonitrile. Complex 11 displayed both vapochromic and solvatochromic properties. This complex was isolated as a purple solid, turning yellow upon treatment with methanol droplets or vapour, but this colour change could be reversed upon addition of acetonitrile.
{"title":"Manipulating vapochromic or solvatochromic properties of platinum(ii) pincer complexes through ligand modifications","authors":"Clare L. Stubbs, Mathew J. Bryant, Lauren E. Hatcher and Paul R. Raithby","doi":"10.1039/D5CE00747J","DOIUrl":"https://doi.org/10.1039/D5CE00747J","url":null,"abstract":"<p >Colour-changing chemical sensors have found important applications in the detection of low concentrations of volatile organic compounds (VOCs). Among the most promising molecular materials are platinum pincer complexes that display rapid colour changes when exposed to a variety of VOCs. In the solid state, these rapid responses have been linked to changes in non-covalent interactions between the platinum pincer molecules and the guest VOCs. To gain a better understanding of the interactions involved, we have studied the manipulation of vapochromic or solvatochromic properties in a series of square planar platinum(<small>II</small>) pincer complexes through structural modification of the monodentate ligand occupying the fourth coordination site. The platinum(<small>II</small>) complexes are based on the 1,3-di(pyridine)benzene tridentate linker (N^C^N) skeleton with the fourth site occupied by a monodentate, anionic ligand L. The formulae of the complexes synthesised are [Pt(N^C(C(O)OMe)^N)(L)] (L = (NCO) (<strong>6</strong>), (NCS) (<strong>7</strong>), (OC(O)Me) (<strong>8</strong>), (OC(O)CF<small><sub>3</sub></small>) (<strong>9</strong>), (OS(O)<small><sub>2</sub></small>CF<small><sub>3</sub></small>) (<strong>10</strong>), and (OS(O)<small><sub>2</sub></small>(C<small><sub>6</sub></small>H<small><sub>4</sub></small>Me)) (<strong>11</strong>)), and the crystalline solids and solutions of these materials have been tested for solvatochromic or vapochromic changes with VOCs including dichloromethane, acetonitrile, diethyl ether, methanol and water. The complexes <strong>6</strong> and <strong>7</strong> crystallised as yellow solids, with no solvent voids in the crystal lattice. Single-crystal X-ray analyses showed that the intermolecular Pt⋯Pt separations were too long for direct Pt⋯Pt interactions. Neither material displayed solvatochromic or vapochromic properties. However, when the fourth ligand was an acetate group, complex <strong>8</strong>, the solid displayed vapochromism, changing colour from an orange water-containing crystalline form to an anhydrous yellow form, and a blue form when treated with methanol vapour. A crystal structure analysis showed that in the orange form adjacent pincer molecules were linked together through a hydrogen bonding network involving lattice water molecules, supported by π⋯π stacking interactions. Complexes <strong>9</strong> and <strong>10</strong> both showed solvatochromism, forming a bright yellow solid when crystallised from dichloromethane but forming an orange solid when recrystallised from acetonitrile. Complex <strong>11</strong> displayed both vapochromic and solvatochromic properties. This complex was isolated as a purple solid, turning yellow upon treatment with methanol droplets or vapour, but this colour change could be reversed upon addition of acetonitrile.</p>","PeriodicalId":70,"journal":{"name":"CrystEngComm","volume":" 46","pages":" 7498-7513"},"PeriodicalIF":2.6,"publicationDate":"2025-10-27","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"https://pubs.rsc.org/en/content/articlepdf/2025/ce/d5ce00747j?page=search","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"145584738","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":3,"RegionCategory":"化学","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"OA","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
The optical floating zone method was utilized to generate a series of single crystals (Lu1−xTmx)3Al5O12 (x = 0, 0.005, 0.010, 0.015, 0.020), abbreviated as Tm:LuAG. The concentration of activated ions has a considerable impact on luminous material performance. Thus, this research focuses on the effect of Tm3+ concentration on the micro-structure and luminescence properties of lutetium aluminum garnet single crystals. According to XRD diffraction data processed using Rietveld refinement, the micro-structure of LuAG single crystals would be distorted by Tm3+ doping. When the concentration of Tm3+ is 0.015, the lattice symmetry is the lowest. Upon examining the emission spectra of Tm:LuAG, emission peaks of Tm3+ ions were identified. Various strengths of emission peaks were seen within the range of 400 to 600 nm, with the peak at 449 nm exhibiting the highest intensity, accompanied by a phenomenon of energy level splitting at this wavelength. The luminescence intensity of the Tm:LuAG single crystal reaches its highest point when the doping concentration is 0.015. As the doping concentration surpasses 0.015, the luminescence intensity gradually reduces, which causes a concentration quenching event. The optimum doping concentration of the sample is 0.015. The Blasse formula yields a critical distance of 20.80 Å in Tm:LuAG single crystals. The reason for concentration quenching in LuAG crystals is that the interaction between the electric dipole and the electric quadrupole of Tm3+ ions occurs. Furthermore, when the concentration of Tm3+ ions increases, the fluorescence lifetime decreases. Tm:LuAG single crystals have certain application potential in areas such as three-dimensional display and biological imaging.
{"title":"The effect of Tm3+ concentration on the structure and luminescence characteristics of LuAG single crystals","authors":"Lipeng Huang, Hao Ren, Guozhu Xiong, Jiaxin Liu, Hongyi Zhang, Cunli Wang, Zehang Huang, Shoulei Xu, Yuyang Huang and Wen Deng","doi":"10.1039/D5CE00972C","DOIUrl":"https://doi.org/10.1039/D5CE00972C","url":null,"abstract":"<p >The optical floating zone method was utilized to generate a series of single crystals (Lu<small><sub>1−<em>x</em></sub></small>Tm<small><sub><em>x</em></sub></small>)<small><sub>3</sub></small>Al<small><sub>5</sub></small>O<small><sub>12</sub></small> (<em>x</em> = 0, 0.005, 0.010, 0.015, 0.020), abbreviated as Tm:LuAG. The concentration of activated ions has a considerable impact on luminous material performance. Thus, this research focuses on the effect of Tm<small><sup>3+</sup></small> concentration on the micro-structure and luminescence properties of lutetium aluminum garnet single crystals. According to XRD diffraction data processed using Rietveld refinement, the micro-structure of LuAG single crystals would be distorted by Tm<small><sup>3+</sup></small> doping. When the concentration of Tm<small><sup>3+</sup></small> is 0.015, the lattice symmetry is the lowest. Upon examining the emission spectra of Tm:LuAG, emission peaks of Tm<small><sup>3+</sup></small> ions were identified. Various strengths of emission peaks were seen within the range of 400 to 600 nm, with the peak at 449 nm exhibiting the highest intensity, accompanied by a phenomenon of energy level splitting at this wavelength. The luminescence intensity of the Tm:LuAG single crystal reaches its highest point when the doping concentration is 0.015. As the doping concentration surpasses 0.015, the luminescence intensity gradually reduces, which causes a concentration quenching event. The optimum doping concentration of the sample is 0.015. The Blasse formula yields a critical distance of 20.80 Å in Tm:LuAG single crystals. The reason for concentration quenching in LuAG crystals is that the interaction between the electric dipole and the electric quadrupole of Tm<small><sup>3+</sup></small> ions occurs. Furthermore, when the concentration of Tm<small><sup>3+</sup></small> ions increases, the fluorescence lifetime decreases. Tm:LuAG single crystals have certain application potential in areas such as three-dimensional display and biological imaging.</p>","PeriodicalId":70,"journal":{"name":"CrystEngComm","volume":" 48","pages":" 7807-7816"},"PeriodicalIF":2.6,"publicationDate":"2025-10-27","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"145698290","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":3,"RegionCategory":"化学","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Corey L. Brown, Scarlett H. Elliott, Sian E. Woodfine and Chris S. Hawes
Here we report a new tetratopic carboxylic acid ligand H4L1 containing a fluorescent pyrrolo[3,2-b]pyrrole core, and examine its structural chemistry in two solvated forms with amide solvents and a porous strontium(II) MOF. The two solvates H4L1·2DMF and H4L1·4DMA exhibit similar hydrogen bonding characteristics at the N-aryl position, but are differentiated by the hydrogen bonding behaviour of the C-aryl position; while the DMF solvate forms a one-dimensional chain via carboxylic acid dimers, the DMA solvate is fully enclosed by solvent molecules occupying all hydrogen bonding sites. The tendency for the electron-rich core to avoid close π⋯π interactions in these solvates is further evident in the structure of poly-[Sr2(L1)(DMF)2(OH2)]·DMF·H2O 1, a 3-dimensional rod-packed MOF with narrow linear solvent channels. Exchange of the lattice solvent with methanol, with retention of single crystallinity, gives a framework which can be readily desolvated, and exhibits a maximum CO2 uptake of 8 wt% at 283 K and 1 atm. The ligand is strongly fluorescent in DMSO in its protonated and deprotonated forms and exhibits characteristic solvatochromism, which is pronounced in solution and remains evident, to a lesser degree, in the fluorescent MOF 1.
{"title":"Structural chemistry and environment-dependent fluorescence of a tetratopic pyrrolo[3,2-b]pyrrole ligand","authors":"Corey L. Brown, Scarlett H. Elliott, Sian E. Woodfine and Chris S. Hawes","doi":"10.1039/D5CE00926J","DOIUrl":"https://doi.org/10.1039/D5CE00926J","url":null,"abstract":"<p >Here we report a new tetratopic carboxylic acid ligand <strong>H</strong><small><sub><strong>4</strong></sub></small><strong>L1</strong> containing a fluorescent pyrrolo[3,2-<em>b</em>]pyrrole core, and examine its structural chemistry in two solvated forms with amide solvents and a porous strontium(<small>II</small>) MOF. The two solvates <strong>H</strong><small><sub><strong>4</strong></sub></small><strong>L1</strong>·2DMF and <strong>H</strong><small><sub><strong>4</strong></sub></small><strong>L1</strong>·4DMA exhibit similar hydrogen bonding characteristics at the <em>N</em>-aryl position, but are differentiated by the hydrogen bonding behaviour of the <em>C</em>-aryl position; while the DMF solvate forms a one-dimensional chain <em>via</em> carboxylic acid dimers, the DMA solvate is fully enclosed by solvent molecules occupying all hydrogen bonding sites. The tendency for the electron-rich core to avoid close π⋯π interactions in these solvates is further evident in the structure of poly-[Sr<small><sub>2</sub></small>(<strong>L1</strong>)(DMF)<small><sub>2</sub></small>(OH<small><sub>2</sub></small>)]·DMF·H<small><sub>2</sub></small>O <strong>1</strong>, a 3-dimensional rod-packed MOF with narrow linear solvent channels. Exchange of the lattice solvent with methanol, with retention of single crystallinity, gives a framework which can be readily desolvated, and exhibits a maximum CO<small><sub>2</sub></small> uptake of 8 wt% at 283 K and 1 atm. The ligand is strongly fluorescent in DMSO in its protonated and deprotonated forms and exhibits characteristic solvatochromism, which is pronounced in solution and remains evident, to a lesser degree, in the fluorescent MOF <strong>1</strong>.</p>","PeriodicalId":70,"journal":{"name":"CrystEngComm","volume":" 45","pages":" 7358-7366"},"PeriodicalIF":2.6,"publicationDate":"2025-10-27","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"https://pubs.rsc.org/en/content/articlepdf/2025/ce/d5ce00926j?page=search","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"145529543","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":3,"RegionCategory":"化学","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"OA","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}