Lin Li, , , Haibing Han, , , Yuying Fu, , and , Jinjian Liu*,
In this work, two functional two-dimensional (2D) Zn(II) metal–organic frameworks (Zn-MOFs), {[Zn(NDC)(CEbpy)]·H2O}n (1) and {[Zn(HBTC)(CV)0.5(H2O)]·0.5(CV)·6H2O}n (2), were synthesized using two viologen-carboxylate ligands (CEbpy = 1-carboxyethyl-4,4′-bipyridine; CV = N,N′-4,4′-bipyridiniodipropionate) in the presence of secondary linkers (H2NDC = 1,4-naphthalenedicarboxylic acid; H3BTC = 1,3,5-benzenetricarboxylic acid). Owing to the successful construction of the donor–acceptor (D–A) system, both Zn-MOFs exhibited excellent electron-transfer photochromic properties, and their photoproducts remained stable in air for several days. Additionally, compounds 1 and 2 exhibited potential for photocontrolled luminescence and demonstrated clear and legible printing capabilities, making them suitable for use as light-controlled switch and inkless erasable printing media.
{"title":"Two Functional Two-Dimensional Photochromic Zn-MOFs Derived from the Viologen-Carboxylate Ligands","authors":"Lin Li, , , Haibing Han, , , Yuying Fu, , and , Jinjian Liu*, ","doi":"10.1021/acs.cgd.5c01327","DOIUrl":"https://doi.org/10.1021/acs.cgd.5c01327","url":null,"abstract":"<p >In this work, two functional two-dimensional (2D) Zn(II) metal–organic frameworks (Zn-MOFs), {[Zn(NDC)(CEbpy)]·H<sub>2</sub>O}<sub><i>n</i></sub> (<b>1</b>) and {[Zn(HBTC)(CV)<sub>0.5</sub>(H<sub>2</sub>O)]·0.5(CV)·6H<sub>2</sub>O}<sub><i>n</i></sub> (<b>2</b>), were synthesized using two viologen-carboxylate ligands (CEbpy = 1-carboxyethyl-4,4′-bipyridine; CV = <i>N</i>,<i>N</i>′-4,4′-bipyridiniodipropionate) in the presence of secondary linkers (H<sub>2</sub>NDC = 1,4-naphthalenedicarboxylic acid; H<sub>3</sub>BTC = 1,3,5-benzenetricarboxylic acid). Owing to the successful construction of the donor–acceptor (D–A) system, both Zn-MOFs exhibited excellent electron-transfer photochromic properties, and their photoproducts remained stable in air for several days. Additionally, compounds <b>1</b> and <b>2</b> exhibited potential for photocontrolled luminescence and demonstrated clear and legible printing capabilities, making them suitable for use as light-controlled switch and inkless erasable printing media.</p>","PeriodicalId":34,"journal":{"name":"Crystal Growth & Design","volume":"26 2","pages":"785–793"},"PeriodicalIF":3.4,"publicationDate":"2025-12-27","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"146015475","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":2,"RegionCategory":"化学","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
This paper focuses on the enhancing effect of doped Bi3+ and Ce3+ ions on the specific Faraday rotation angle of the terbium iron garnet (TIG) magneto-optical crystal. By means of structural design, a large-radius Ce3+ is doped into the dodecahedron sites of the bismuth-doped terbium iron garnet (Bi:TIG) structure. The cell volume of the crystal is enlarged to accommodate higher content of Bi3+ and Ce3+. Centimeter-sized, high-quality cerium- and bismuth-codoped terbium iron garnet (Ce,Bi:TIG) and Bi:TIG crystals were successfully grown by the top-seeded solution growth (TSSG) method using a lead-free Bi2O3–Fe2O3 flux. Among these as-grown crystals, the transmittance of Ce0.13Bi0.60Tb2.27Fe4.85Ga0.15O12 is 70.7% and the specific Faraday rotation angle is up to −800 deg cm–1 at 1550 nm. The Faraday rotation temperature coefficients (FTC) and the wavelength coefficients (FWC) of Ce0.13Bi0.60Tb2.27Fe4.85Ga0.15O12 are −1.72 × 10–3 K–1 and 1.40 × 10–3 nm–1, respectively. Ce,Bi:TIG crystal is expected to be applied in magneto-optical isolators at 1550 nm.
{"title":"Growth, High Optical Transmittance, and Strong Magneto-Optical Properties at 1550 nm of Ce,Bi-Codoped Tb3Fe5O12 Crystals","authors":"Junying Wu, , , Chunhan Chen, , , Haipeng Liu, , , Yanduan Yang, , , Wenjing Guan, , , Teng Gao, , , Xin Chen, , , Xiaolin Hu*, , and , Naifeng Zhuang*, ","doi":"10.1021/acs.cgd.5c01338","DOIUrl":"https://doi.org/10.1021/acs.cgd.5c01338","url":null,"abstract":"<p >This paper focuses on the enhancing effect of doped Bi<sup>3+</sup> and Ce<sup>3+</sup> ions on the specific Faraday rotation angle of the terbium iron garnet (TIG) magneto-optical crystal. By means of structural design, a large-radius Ce<sup>3+</sup> is doped into the dodecahedron sites of the bismuth-doped terbium iron garnet (Bi:TIG) structure. The cell volume of the crystal is enlarged to accommodate higher content of Bi<sup>3+</sup> and Ce<sup>3+</sup>. Centimeter-sized, high-quality cerium- and bismuth-codoped terbium iron garnet (Ce,Bi:TIG) and Bi:TIG crystals were successfully grown by the top-seeded solution growth (TSSG) method using a lead-free Bi<sub>2</sub>O<sub>3</sub>–Fe<sub>2</sub>O<sub>3</sub> flux. Among these as-grown crystals, the transmittance of Ce<sub>0.13</sub>Bi<sub>0.60</sub>Tb<sub>2.27</sub>Fe<sub>4.85</sub>Ga<sub>0.15</sub>O<sub>12</sub> is 70.7% and the specific Faraday rotation angle is up to −800 deg cm<sup>–1</sup> at 1550 nm. The Faraday rotation temperature coefficients (FTC) and the wavelength coefficients (FWC) of Ce<sub>0.13</sub>Bi<sub>0.60</sub>Tb<sub>2.27</sub>Fe<sub>4.85</sub>Ga<sub>0.15</sub>O<sub>12</sub> are −1.72 × 10<sup>–3</sup> K<sup>–1</sup> and 1.40 × 10<sup>–3</sup> nm<sup>–1</sup>, respectively. Ce,Bi:TIG crystal is expected to be applied in magneto-optical isolators at 1550 nm.</p>","PeriodicalId":34,"journal":{"name":"Crystal Growth & Design","volume":"26 2","pages":"794–802"},"PeriodicalIF":3.4,"publicationDate":"2025-12-27","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"146015476","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":2,"RegionCategory":"化学","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Plastic crystals are a unique class of dynamic crystalline materials that combine long-range order with partial molecular mobility, resulting in remarkable mechanical properties, such as plasticity and flexibility. These crystals have emerged as promising candidates for advanced flexible devices and pharmaceutical applications. In this study, we investigate the plastic behavior of 3-bromo-5-chlorobenzoic acid (3B5CBA), a globular halogenated aromatic compound. Crystals of 3B5CBA grown via a fast evaporation technique exhibited plastic bending when stressed along the (001) plane. Thermal analysis of crystals revealed a sublimation onset at approximately 70 °C and a melting point of 195.3 °C. Single-crystal X-ray diffraction (SCXRD) analysis and energy framework calculation revealed strong 2D sheet-like interactions parallel to the (001) plane (−299.9 kJ/mol) and weaker interlayer C–Br···O interactions (−79.6 kJ/mol) forming low-energy slip planes. Nanoindentation on the (001) face confirmed homogeneous plastic deformation with a moderate hardness of 217.48 ± 19.87 MPa and a Young’s modulus of 2.94 ± 0.35 GPa. Furthermore, shape analysis using Hirshfeld surface parameters showed high globularity (G = 0.808) and low asphericity (Ω = 0.108). Together, these results showed that 3B5CBA being an organic aromatic compound with a nearly globular shape, hydrogen and halogen synthon-forming functional groups on its periphery can show long-range disordered crystal structure, sublimation ability, and irreversible plastic deformation, offering new insights into the design of aromatic plastic molecular solids.
{"title":"Plastic Behavior of 3-Bromo-5-chlorobenzoic Acid: Structural, Thermal, and Plastic Deformation Analysis","authors":"Deepak Rajput, and , Sameer V. Dalvi*, ","doi":"10.1021/acs.cgd.5c01256","DOIUrl":"https://doi.org/10.1021/acs.cgd.5c01256","url":null,"abstract":"<p >Plastic crystals are a unique class of dynamic crystalline materials that combine long-range order with partial molecular mobility, resulting in remarkable mechanical properties, such as plasticity and flexibility. These crystals have emerged as promising candidates for advanced flexible devices and pharmaceutical applications. In this study, we investigate the plastic behavior of 3-bromo-5-chlorobenzoic acid (3B5CBA), a globular halogenated aromatic compound. Crystals of 3B5CBA grown via a fast evaporation technique exhibited plastic bending when stressed along the (001) plane. Thermal analysis of crystals revealed a sublimation onset at approximately 70 °C and a melting point of 195.3 °C. Single-crystal X-ray diffraction (SCXRD) analysis and energy framework calculation revealed strong 2D sheet-like interactions parallel to the (001) plane (−299.9 kJ/mol) and weaker interlayer C–Br···O interactions (−79.6 kJ/mol) forming low-energy slip planes. Nanoindentation on the (001) face confirmed homogeneous plastic deformation with a moderate hardness of 217.48 ± 19.87 MPa and a Young’s modulus of 2.94 ± 0.35 GPa. Furthermore, shape analysis using Hirshfeld surface parameters showed high globularity (<i>G</i> = 0.808) and low asphericity (Ω = 0.108). Together, these results showed that 3B5CBA being an organic aromatic compound with a nearly globular shape, hydrogen and halogen synthon-forming functional groups on its periphery can show long-range disordered crystal structure, sublimation ability, and irreversible plastic deformation, offering new insights into the design of aromatic plastic molecular solids.</p>","PeriodicalId":34,"journal":{"name":"Crystal Growth & Design","volume":"26 1","pages":"277–288"},"PeriodicalIF":3.4,"publicationDate":"2025-12-26","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"145903850","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":2,"RegionCategory":"化学","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Chintan K. Tandel, , , Yash N. Doshi*, , , David D. Kokni, , , Sanket P. Sikligar, , , Piyush B. Patel, , , Hiren N. Desai*, , , Jitendra M. Dhimmar, , and , Bharat P. Modi,
SnCl2 and CdCl2-assisted doping was employed to tune the defect landscape and functional properties of SnSe crystals synthesized by direct vapor transport. Structural and compositional analyses confirm successful dopant incorporation, where SnCl2 passivates Se vacancy-related defects and expands the lattice, while CdCl2 induces controlled lattice distortion via Cd2+ substitution. These effects tune the optical band gap from 1.27 eV in pristine SnSe to 1.49 and 1.38 eV in SnCl2:SnSe and CdCl2:SnSe, respectively. Temperature-dependent transport measurements reveal the elimination of the positive TCR behavior observed in undoped SnSe and the establishment of stable thermally activated conduction in the doped systems. Hall measurements indicate a transition from p- to n-type conduction, accompanied by an increase in the electron concentration, consistent with vacancy passivation and defect compensation. Both doped crystals exhibit modest yet measurable improvements in photocurrent and noise characteristics, while photocatalytic studies show better methylene blue degradation efficiencies, with SnCl2:SnSe outperforming CdCl2:SnSe. These results demonstrate that chloride-based doping tailors SnSe for better optoelectronic and photocatalytic performance effectively.
{"title":"Complementary Defect Tuned Modulation of Optoelectronic and Catalytic Performance in SnSe via SnCl2 and CdCl2 Doping","authors":"Chintan K. Tandel, , , Yash N. Doshi*, , , David D. Kokni, , , Sanket P. Sikligar, , , Piyush B. Patel, , , Hiren N. Desai*, , , Jitendra M. Dhimmar, , and , Bharat P. Modi, ","doi":"10.1021/acs.cgd.5c01126","DOIUrl":"https://doi.org/10.1021/acs.cgd.5c01126","url":null,"abstract":"<p >SnCl<sub>2</sub> and CdCl<sub>2</sub>-assisted doping was employed to tune the defect landscape and functional properties of SnSe crystals synthesized by direct vapor transport. Structural and compositional analyses confirm successful dopant incorporation, where SnCl<sub>2</sub> passivates Se vacancy-related defects and expands the lattice, while CdCl<sub>2</sub> induces controlled lattice distortion via Cd<sup>2+</sup> substitution. These effects tune the optical band gap from 1.27 eV in pristine SnSe to 1.49 and 1.38 eV in SnCl<sub>2</sub>:SnSe and CdCl<sub>2</sub>:SnSe, respectively. Temperature-dependent transport measurements reveal the elimination of the positive TCR behavior observed in undoped SnSe and the establishment of stable thermally activated conduction in the doped systems. Hall measurements indicate a transition from p- to n-type conduction, accompanied by an increase in the electron concentration, consistent with vacancy passivation and defect compensation. Both doped crystals exhibit modest yet measurable improvements in photocurrent and noise characteristics, while photocatalytic studies show better methylene blue degradation efficiencies, with SnCl<sub>2</sub>:SnSe outperforming CdCl<sub>2</sub>:SnSe. These results demonstrate that chloride-based doping tailors SnSe for better optoelectronic and photocatalytic performance effectively.</p>","PeriodicalId":34,"journal":{"name":"Crystal Growth & Design","volume":"26 1","pages":"176–190"},"PeriodicalIF":3.4,"publicationDate":"2025-12-26","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"145903849","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":2,"RegionCategory":"化学","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
<p >Flexible porous coordination polymers (PCPs) and metal–organic frameworks (MOFs) that undergo structural changes upon guest removal/uptake have a wide range of potential applications. However, detailed characterization of the guest removal/uptake-promoted changes of these materials is frequently limited by the occurrence of crystal fragmentation, which produces nanocrystals that are unsuitable for single-crystal X-ray diffraction analysis. An example of this limitation was encountered in our recent study of the flexible PCP [Cu(CF<sub>3</sub>SO<sub>3</sub>)<sub>2</sub>(bpp)<sub>2</sub>] (bpp = 1,3-bis(4-pyridyl)propane), which we demonstrated can exist in two PCP polymorphs: the one-dimensional (1D) form <b>1</b> obtained by removal of guest acetone molecules from the 1D acetone-inclusion form [Cu(CF<sub>3</sub>SO<sub>3</sub>)(bpp)<sub>2</sub>]·CF<sub>3</sub>SO<sub>3</sub>·2acetone (<b>1</b>·2acetone) and the two-dimensional (2D) form <b>2</b> obtained by removal of guest water molecules from the 2D water-inclusion form [Cu(CF<sub>3</sub>SO<sub>3</sub>)<sub>2</sub>(bpp)<sub>2</sub>]·H<sub>2</sub>O (<b>2</b>·H<sub>2</sub>O). Although we speculated that adsorption/desorption of H<sub>2</sub>O by <b>2</b> occurs in conjunction with a transient interlayer expansion process, confirmatory evidence could not be obtained because the crystal structure of the desolvated form <b>2</b> could not be determined and, therefore, a comparison of the structures in the presence and absence of guests was not possible. In the current study, we employed the microcrystal electron diffraction (MicroED) technique to elucidate the local and overall structural changes associated with guest H<sub>2</sub>O removal/uptake by <b>2</b>. Comparative analysis of these structures shows that H<sub>2</sub>O guests in <b>2</b>·H<sub>2</sub>O are trapped in isolated pores and that all bpp ligands in the H<sub>2</sub>O-incorporated form exist in the <i>TT</i> (<i>T</i> = <i>trans</i>) conformation. On the other hand, the dehydrated form <b>2</b> possesses a more densely packed structure with smaller discrete cavities, and the conformations of the bpp ligands in <b>2</b> are partially converted from <i>TT</i> to <i>TG</i> (<i>G</i> = <i>gauche</i>). The results of the structural analysis and theoretical calculations show that a drastic transient structural change involving interlayer expansion/shrinkage and/or continuous partial deformation of the framework of <b>2</b> takes place during H<sub>2</sub>O adsorption/desorption. In addition, observations made in temperature-dependent powder X-ray diffraction and H<sub>2</sub>O adsorption/desorption experiments reveal that H<sub>2</sub>O guests present in <b>2</b>·H<sub>2</sub>O interact with the CF<sub>3</sub>SO<sub>3</sub> anions in the framework via moderate hydrogen bonds.</p><p >Flexible porous coordination polymers (PCPs) and metal−organic frameworks (MOFs) that respond to guest molecules hold significant promise for various applic
{"title":"Structural Characterization of a Desolvated Flexible Porous Coordination Polymer Using MicroED","authors":"Yuki Masuda, , , Umme Fariha Tasnim, , , Yuan Huang, , , Takanori Nakane, , , Akihiro Kawamoto, , , Genji Kurisu, , , Yuh Hijikata, , and , Shin-ichiro Noro*, ","doi":"10.1021/acs.cgd.5c01361","DOIUrl":"https://doi.org/10.1021/acs.cgd.5c01361","url":null,"abstract":"<p >Flexible porous coordination polymers (PCPs) and metal–organic frameworks (MOFs) that undergo structural changes upon guest removal/uptake have a wide range of potential applications. However, detailed characterization of the guest removal/uptake-promoted changes of these materials is frequently limited by the occurrence of crystal fragmentation, which produces nanocrystals that are unsuitable for single-crystal X-ray diffraction analysis. An example of this limitation was encountered in our recent study of the flexible PCP [Cu(CF<sub>3</sub>SO<sub>3</sub>)<sub>2</sub>(bpp)<sub>2</sub>] (bpp = 1,3-bis(4-pyridyl)propane), which we demonstrated can exist in two PCP polymorphs: the one-dimensional (1D) form <b>1</b> obtained by removal of guest acetone molecules from the 1D acetone-inclusion form [Cu(CF<sub>3</sub>SO<sub>3</sub>)(bpp)<sub>2</sub>]·CF<sub>3</sub>SO<sub>3</sub>·2acetone (<b>1</b>·2acetone) and the two-dimensional (2D) form <b>2</b> obtained by removal of guest water molecules from the 2D water-inclusion form [Cu(CF<sub>3</sub>SO<sub>3</sub>)<sub>2</sub>(bpp)<sub>2</sub>]·H<sub>2</sub>O (<b>2</b>·H<sub>2</sub>O). Although we speculated that adsorption/desorption of H<sub>2</sub>O by <b>2</b> occurs in conjunction with a transient interlayer expansion process, confirmatory evidence could not be obtained because the crystal structure of the desolvated form <b>2</b> could not be determined and, therefore, a comparison of the structures in the presence and absence of guests was not possible. In the current study, we employed the microcrystal electron diffraction (MicroED) technique to elucidate the local and overall structural changes associated with guest H<sub>2</sub>O removal/uptake by <b>2</b>. Comparative analysis of these structures shows that H<sub>2</sub>O guests in <b>2</b>·H<sub>2</sub>O are trapped in isolated pores and that all bpp ligands in the H<sub>2</sub>O-incorporated form exist in the <i>TT</i> (<i>T</i> = <i>trans</i>) conformation. On the other hand, the dehydrated form <b>2</b> possesses a more densely packed structure with smaller discrete cavities, and the conformations of the bpp ligands in <b>2</b> are partially converted from <i>TT</i> to <i>TG</i> (<i>G</i> = <i>gauche</i>). The results of the structural analysis and theoretical calculations show that a drastic transient structural change involving interlayer expansion/shrinkage and/or continuous partial deformation of the framework of <b>2</b> takes place during H<sub>2</sub>O adsorption/desorption. In addition, observations made in temperature-dependent powder X-ray diffraction and H<sub>2</sub>O adsorption/desorption experiments reveal that H<sub>2</sub>O guests present in <b>2</b>·H<sub>2</sub>O interact with the CF<sub>3</sub>SO<sub>3</sub> anions in the framework via moderate hydrogen bonds.</p><p >Flexible porous coordination polymers (PCPs) and metal−organic frameworks (MOFs) that respond to guest molecules hold significant promise for various applic","PeriodicalId":34,"journal":{"name":"Crystal Growth & Design","volume":"26 1","pages":"438–445"},"PeriodicalIF":3.4,"publicationDate":"2025-12-26","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"https://pubs.acs.org/doi/pdf/10.1021/acs.cgd.5c01361","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"145903853","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":2,"RegionCategory":"化学","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"OA","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Mayra S. Coutinho, , , Thomaz de A. Costa, , , Alan Imperatori, , , Andrei A. Patrascu, , , Isabela Man, , , Maria G. F. Vaz, , , Simona Nica*, , , Marius Andruh*, , and , Pedro N. Batalha*,
Cocrystal engineering has become an essential strategy in materials science, enabling the design of new solid-state systems through the rational combination of organic components guided by noncovalent interactions. In this study, the cocrystallization of a bis-pyridyl-azine substrate with three different coformers, namely, 1,3,5-triiodo-2,4,6-trifluorobenzene, 1,2-diiodotetrafluorobenzene, and 4,4′-biphenol, led to the formation of five new cocrystal systems. The supramolecular architectures of these materials were investigated with a focus on the role of halogen bonding and hydrogen bonding in crystal packing. All observed noncovalent interactions were investigated using density functional theory (DFT) calculations carried out with the ωB97XD functional and the def2-TZVPP. The results emphasize the influence of molecular recognition in the self-assembly process and reveal how halogen and hydrogen bonds act as key driving forces in the formation and stabilization of these cocrystals.
Five new cocrystals formed from a bis(pyridyl)azine derivative and halogen- or hydrogen-bond donors are reported, showcasing how subtle electronic effects and packing preferences govern the balance between I···N, I···F, I···I, O−H···N, and C−H···F interactions, enabling the fine-tuning of distinct supramolecular architectures.
{"title":"Engineering Supramolecular Systems with a Bis(pyridyl)azine Derivative and Different Hydrogen and Halogen Donors","authors":"Mayra S. Coutinho, , , Thomaz de A. Costa, , , Alan Imperatori, , , Andrei A. Patrascu, , , Isabela Man, , , Maria G. F. Vaz, , , Simona Nica*, , , Marius Andruh*, , and , Pedro N. Batalha*, ","doi":"10.1021/acs.cgd.5c01135","DOIUrl":"https://doi.org/10.1021/acs.cgd.5c01135","url":null,"abstract":"<p >Cocrystal engineering has become an essential strategy in materials science, enabling the design of new solid-state systems through the rational combination of organic components guided by noncovalent interactions. In this study, the cocrystallization of a bis-pyridyl-azine substrate with three different coformers, namely, 1,3,5-triiodo-2,4,6-trifluorobenzene, 1,2-diiodotetrafluorobenzene, and 4,4′-biphenol, led to the formation of five new cocrystal systems. The supramolecular architectures of these materials were investigated with a focus on the role of halogen bonding and hydrogen bonding in crystal packing. All observed noncovalent interactions were investigated using density functional theory (DFT) calculations carried out with the ωB97XD functional and the def2-TZVPP. The results emphasize the influence of molecular recognition in the self-assembly process and reveal how halogen and hydrogen bonds act as key driving forces in the formation and stabilization of these cocrystals.</p><p >Five new cocrystals formed from a bis(pyridyl)azine derivative and halogen- or hydrogen-bond donors are reported, showcasing how subtle electronic effects and packing preferences govern the balance between I···N, I···F, I···I, O−H···N, and C−H···F interactions, enabling the fine-tuning of distinct supramolecular architectures.</p>","PeriodicalId":34,"journal":{"name":"Crystal Growth & Design","volume":"26 1","pages":"198–209"},"PeriodicalIF":3.4,"publicationDate":"2025-12-26","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"https://pubs.acs.org/doi/pdf/10.1021/acs.cgd.5c01135","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"145903852","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":2,"RegionCategory":"化学","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"OA","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
A novel high-entropy laser crystal of 30 at. % Er:GdLuYSGG was grown by the Cz method. The crystal exhibits high crystalline quality, evidenced by an X-ray rocking curve FWHM of 0.007°. The thermal expansion coefficient and thermal conductivity are determined to be 1.52 × 10–5 K–1 and 4.10 W m–1 K–1, respectively. A broadened fluorescence band around 2760–2840 nm is observed and attributed to the lattice distortion effect of the high-entropy crystal, indicating the Er:GdLuYSGG crystal is beneficial for realizing tunable or ultrafast lasers. By a 973 nm LD end-pumping, a continuous-wave 2.8 μm laser is achieved with a maximum output power of 1062 mW, corresponding to a slope efficiency of 17.99%. The Mx2/My2 factors are 1.35 and 1.37, suggesting a high laser beam quality. The results imply that the high-entropy Er:GdLuYSGG crystal is a promising broadband gain medium for high-performance 2.8 μm mid-infrared laser, which might be particularly suited for applications in space radiation environments.
A novel high-entropy Er:GdLuYSGG crystal was successfully grown. The absorption and fluorescence bands were both broadened, an enhanced continuous-wave 2.8 μm laser was achieved with a maximum output power of 1062 mW. The high-entropy Er:GdLuYSGG crystal is a promising broadband gain medium for high-performance 2.8 μm mid-infrared laser.
{"title":"Structure, Spectroscopy and Enhanced 2.8 μm Laser Performance of a High-Entropy Er:GdLuYSGG Crystal","authors":"Huili Zhang, , , Dunlu Sun*, , , Cong Quan, , , Maojie Cheng, , , Kunpeng Dong, , , Zhentao Wang, , , Hongyuan Li, , , Xinjie Li, , and , Shiji Dou, ","doi":"10.1021/acs.cgd.5c01447","DOIUrl":"https://doi.org/10.1021/acs.cgd.5c01447","url":null,"abstract":"<p >A novel high-entropy laser crystal of 30 at. % Er:GdLuYSGG was grown by the Cz method. The crystal exhibits high crystalline quality, evidenced by an X-ray rocking curve FWHM of 0.007°. The thermal expansion coefficient and thermal conductivity are determined to be 1.52 × 10<sup>–5</sup> K<sup>–1</sup> and 4.10 W m<sup>–1</sup> K<sup>–1</sup>, respectively. A broadened fluorescence band around 2760–2840 nm is observed and attributed to the lattice distortion effect of the high-entropy crystal, indicating the Er:GdLuYSGG crystal is beneficial for realizing tunable or ultrafast lasers. By a 973 nm LD end-pumping, a continuous-wave 2.8 μm laser is achieved with a maximum output power of 1062 mW, corresponding to a slope efficiency of 17.99%. The <i>M</i><sub><i>x</i></sub><sup>2</sup>/<i>M</i><sub><i>y</i></sub><sup>2</sup> factors are 1.35 and 1.37, suggesting a high laser beam quality. The results imply that the high-entropy Er:GdLuYSGG crystal is a promising broadband gain medium for high-performance 2.8 μm mid-infrared laser, which might be particularly suited for applications in space radiation environments.</p><p >A novel high-entropy Er:GdLuYSGG crystal was successfully grown. The absorption and fluorescence bands were both broadened, an enhanced continuous-wave 2.8 μm laser was achieved with a maximum output power of 1062 mW. The high-entropy Er:GdLuYSGG crystal is a promising broadband gain medium for high-performance 2.8 μm mid-infrared laser.</p>","PeriodicalId":34,"journal":{"name":"Crystal Growth & Design","volume":"26 1","pages":"534–541"},"PeriodicalIF":3.4,"publicationDate":"2025-12-26","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"https://pubs.acs.org/doi/pdf/10.1021/acs.cgd.5c01447","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"145903851","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":2,"RegionCategory":"化学","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"OA","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Fatma Amraoui, , , Madani Labed, , , Lobna Messeddek, , , Nouredine Sengouga*, , , Jang Hyeok Park, , and , You Seung Rim,
Due to its ultrawide bandgap and robust physical properties, β-Ga2O3 is a promising candidate for solar-blind UV photodetectors. However, conventional fabrication methods are often costly and complex. In this study, we demonstrate a cost-effective spin-coating technique to fabricate Sn-doped β-Ga2O3 thin films and systematically investigate the effect of Sn concentration on their structural, optical, electrical, and photodetection properties. The results show that controlled Sn doping effectively enhances device performance by tuning the material’s optoelectronic characteristics. Sn-doped β-Ga2O3 thin films were deposited at room temperature onto sapphire substrates using spin coating, with tin concentrations systematically varied from 0 to 20 wt %. X-ray diffraction analysis confirmed that all films crystallized in the monoclinic β-Ga2O3 phase with a nanocrystalline structure. The optical results showed high transmittance in the visible region and a progressive narrowing of the bandgap with increasing concentration of Sn doping. Electrical characterization revealed that the carrier concentration, electrical conductivity, and electron mobility increased with Sn doping up to 15 wt %. However, at 20 wt % Sn, a reduction in mobility was observed, likely due to enhanced carrier scattering or the introduction of defect states. Furthermore, metal–semiconductor–metal (MSM) photodetectors were fabricated to evaluate the influence of increasing Sn wight percentage on device performance. The results demonstrated that with increasing Sn concentration, UV responsivity, detectivity, and response speed were significantly enhanced, highlighting the potential of Sn-doped β-Ga2O3 thin films for high-performance and cost-effective optoelectronic applications.
{"title":"Effect of Sn Doping on Structural, Optical, and Electrical Properties of β-Ga2O3 Thin Films Prepared via Spin Coating for MSM Photodetector Applications","authors":"Fatma Amraoui, , , Madani Labed, , , Lobna Messeddek, , , Nouredine Sengouga*, , , Jang Hyeok Park, , and , You Seung Rim, ","doi":"10.1021/acs.cgd.5c01185","DOIUrl":"https://doi.org/10.1021/acs.cgd.5c01185","url":null,"abstract":"<p >Due to its ultrawide bandgap and robust physical properties, β-Ga<sub>2</sub>O<sub>3</sub> is a promising candidate for solar-blind UV photodetectors. However, conventional fabrication methods are often costly and complex. In this study, we demonstrate a cost-effective spin-coating technique to fabricate Sn-doped β-Ga<sub>2</sub>O<sub>3</sub> thin films and systematically investigate the effect of Sn concentration on their structural, optical, electrical, and photodetection properties. The results show that controlled Sn doping effectively enhances device performance by tuning the material’s optoelectronic characteristics. Sn-doped β-Ga<sub>2</sub>O<sub>3</sub> thin films were deposited at room temperature onto sapphire substrates using spin coating, with tin concentrations systematically varied from 0 to 20 wt %. X-ray diffraction analysis confirmed that all films crystallized in the monoclinic β-Ga<sub>2</sub>O<sub>3</sub> phase with a nanocrystalline structure. The optical results showed high transmittance in the visible region and a progressive narrowing of the bandgap with increasing concentration of Sn doping. Electrical characterization revealed that the carrier concentration, electrical conductivity, and electron mobility increased with Sn doping up to 15 wt %. However, at 20 wt % Sn, a reduction in mobility was observed, likely due to enhanced carrier scattering or the introduction of defect states. Furthermore, metal–semiconductor–metal (MSM) photodetectors were fabricated to evaluate the influence of increasing Sn wight percentage on device performance. The results demonstrated that with increasing Sn concentration, UV responsivity, detectivity, and response speed were significantly enhanced, highlighting the potential of Sn-doped β-Ga<sub>2</sub>O<sub>3</sub> thin films for high-performance and cost-effective optoelectronic applications.</p>","PeriodicalId":34,"journal":{"name":"Crystal Growth & Design","volume":"26 1","pages":"245–255"},"PeriodicalIF":3.4,"publicationDate":"2025-12-25","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"145903848","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":2,"RegionCategory":"化学","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
To address limitations in real-time 3D morphology acquisition for crystal growth kinetics, this study pioneers an ultrasound–visual dual-modal monitoring system integrating stereoscopic imaging, ultrasonic attenuation, and molecular simulation. The system achieves 37% lower edge-length error in 3D reconstruction vs 2D projection and enables real-time concentration tracking via a PCA-GA-BP neural network (R2 = 0.9998). Kinetic experiments (n = 50) demonstrate that the (200) plane grows 14.5% faster than (111) (0.544 vs 0.475 μm/min) with higher temperature sensitivity (18% enhancement at 323.15 K). Molecular simulations reveal stronger water adsorption on (111) planes (−41.26 vs −10.84 kcal/mol), while the Modified Adsorption Energy (MAE) model corrects solvent-accessible area effects: the (111) plane proportion decreases from 67.14% to 47.44%, whereas (200) increases to 52.56%, aligning with experimental habits. This integrated methodology provides cross-scale insights for inorganic salt crystallization mechanisms and industrial process optimization.
为了解决晶体生长动力学实时三维形态采集的局限性,本研究开创了一种集成立体成像、超声衰减和分子模拟的超声视觉双峰监测系统。与2D投影相比,该系统在3D重建中边长误差降低37%,并通过PCA-GA-BP神经网络实现实时浓度跟踪(R2 = 0.9998)。动力学实验(n = 50)表明,(200)平面比(111)平面生长速度快14.5% (0.544 μm/min vs 0.475 μm/min),温度敏感性提高(323.15 K时提高18%)。分子模拟结果表明(111)面对水的吸附更强(- 41.26 vs - 10.84 kcal/mol),而修正吸附能(MAE)模型修正了溶剂可及面积效应:(111)面所占比例从67.14%下降到47.44%,而(200)面所占比例增加到52.56%,与实验习惯一致。这种集成的方法为无机盐结晶机制和工业过程优化提供了跨尺度的见解。
{"title":"Multiscale Investigation into the Growth Kinetics of Strontium Nitrate Crystals Based on an Ultrasound–Visual Dual-Modal Monitoring System","authors":"Chunlai Yang, , , Xingwu Zou*, , , Qihang Zhu, , , Zhanhua Lei, , , Fei Shao, , , Bo Li, , , Shuxuan Wang, , and , Xiaoqiang Li, ","doi":"10.1021/acs.cgd.5c01492","DOIUrl":"https://doi.org/10.1021/acs.cgd.5c01492","url":null,"abstract":"<p >To address limitations in real-time 3D morphology acquisition for crystal growth kinetics, this study pioneers an ultrasound–visual dual-modal monitoring system integrating stereoscopic imaging, ultrasonic attenuation, and molecular simulation. The system achieves 37% lower edge-length error in 3D reconstruction vs 2D projection and enables real-time concentration tracking via a PCA-GA-BP neural network (<i>R</i><sup>2</sup> = 0.9998). Kinetic experiments (<i>n</i> = 50) demonstrate that the (200) plane grows 14.5% faster than (111) (0.544 vs 0.475 μm/min) with higher temperature sensitivity (18% enhancement at 323.15 K). Molecular simulations reveal stronger water adsorption on (111) planes (−41.26 vs −10.84 kcal/mol), while the Modified Adsorption Energy (MAE) model corrects solvent-accessible area effects: the (111) plane proportion decreases from 67.14% to 47.44%, whereas (200) increases to 52.56%, aligning with experimental habits. This integrated methodology provides cross-scale insights for inorganic salt crystallization mechanisms and industrial process optimization.</p>","PeriodicalId":34,"journal":{"name":"Crystal Growth & Design","volume":"26 2","pages":"893–903"},"PeriodicalIF":3.4,"publicationDate":"2025-12-25","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"146015474","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":2,"RegionCategory":"化学","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
γ-CuI with zinc blende structure has emerged as a next-generation electrical material, but its current two-step chemical vapor deposition (CVD) method still faces problems including high I-residue/vacancy and low film uniformness. The strategy of one-step CVD using a single-source precursor (SSP) could be a feasible solution. In this work, a tetra-nuclear cubane cluster Cu4I4(TMOP)4 (TMOP = tris(4-methoxyphenyl)phosphine) was constructed and used as SSP in γ-CuI deposition first. As indicated by structural analysis of this SSP, the introduction of methoxy on the p-position of PPh3 and the absence of π–π/C–H···π interactions can improve its solubility in organic solvent. More importantly, cuprophilic interactions and fluctuant Cu–I bonds can be beneficial for fracture and reconstitution on the substrate surface during the CVD process. Upon optimization of the substrate, deposition sites, gas velocities, and deposition temperatures, the continuous γ-CuI film with an ultralow roughness (Rq = 4.60 nm) under optimal CVD conditions has been obtained, which has been characterized by XRD, SEM, AFM, XPS, and Raman spectra. The {111} preferential growth mechanism of this γ-CuI has been clarified: the anchoring of Cu4I4 clusters by the size-matched SnO2(110) surface, the Cu–I fracture/reconstitution restricted by cuprophilic interactions, and final growth along the {111} direction. This one-step CVD process using the copper iodide cubane cluster as SSP could pave a new way for the large-scale production of high-quality γ-CuI films.
{"title":"One-Step Chemical Vapor Deposition of High-Quality γ-CuI Films Using Copper Iodide Cubane Clusters as the Single-Source Precursor and Growth Mechanism on the Size-Matched Surface","authors":"Junwei Liang, , , Kun You, , , Xueru Zhou, , , Lintao Fan, , , Liang Zhu, , , Jingjing Chen*, , , Haohong Li*, , and , Huidong Zheng*, ","doi":"10.1021/acs.cgd.5c01482","DOIUrl":"https://doi.org/10.1021/acs.cgd.5c01482","url":null,"abstract":"<p >γ-CuI with zinc blende structure has emerged as a next-generation electrical material, but its current two-step chemical vapor deposition (CVD) method still faces problems including high I-residue/vacancy and low film uniformness. The strategy of one-step CVD using a single-source precursor (SSP) could be a feasible solution. In this work, a tetra-nuclear cubane cluster Cu<sub>4</sub>I<sub>4</sub>(TMOP)<sub>4</sub> (TMOP = tris(4-methoxyphenyl)phosphine) was constructed and used as SSP in γ-CuI deposition first. As indicated by structural analysis of this SSP, the introduction of methoxy on the <i>p</i>-position of PPh<sub>3</sub> and the absence of π–π/C–H···π interactions can improve its solubility in organic solvent. More importantly, cuprophilic interactions and fluctuant Cu–I bonds can be beneficial for fracture and reconstitution on the substrate surface during the CVD process. Upon optimization of the substrate, deposition sites, gas velocities, and deposition temperatures, the continuous γ-CuI film with an ultralow roughness (<i>R</i><sub>q</sub> = 4.60 nm) under optimal CVD conditions has been obtained, which has been characterized by XRD, SEM, AFM, XPS, and Raman spectra. The {111} preferential growth mechanism of this γ-CuI has been clarified: the anchoring of Cu<sub>4</sub>I<sub>4</sub> clusters by the size-matched SnO<sub>2</sub>(110) surface, the Cu–I fracture/reconstitution restricted by cuprophilic interactions, and final growth along the {111} direction. This one-step CVD process using the copper iodide cubane cluster as SSP could pave a new way for the large-scale production of high-quality γ-CuI films.</p>","PeriodicalId":34,"journal":{"name":"Crystal Growth & Design","volume":"26 1","pages":"599–607"},"PeriodicalIF":3.4,"publicationDate":"2025-12-24","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"145903842","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":2,"RegionCategory":"化学","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}