The structures of seven A(2)Cu(4)X(10) compounds containing quasi-planar oligomers are reported: bis(1,2,4-trimethylpyridinium) hexa-μ-chlorido-tetrachloridotetracuprate(II), (C(8)H(12)N)(2)[Cu(4)Cl(10)], (I), and the hexa-μ-bromido-tetrabromidotetracuprate(II) salts of 1,2,4-trimethylpyridinium, (C(8)H(12)N)(2)[Cu(4)Br(10)], (II), 3,4-dimethylpyridinium, (C(7)H(10)N)(2)[Cu(4)Br(10)], (III), 2,3-dimethylpyridinium, (C(7)H(10)N)(2)[Cu(4)Br(10)], (IV), 1-methylpyridinium, (C(6)H(8)N)(2)[Cu(4)Br(10)], (V), trimethylphenylammonium, (C(9)H(14)N)(2)[Cu(4)Br(10)], (VI), and 2,4-dimethylpyridinium, (C(7)H(10)N)(2)[Cu(4)Br(10)], (VII). The first four are isomorphous and contain stacks of tetracopper oligomers aggregated through semicoordinate Cu···X bond formation in a 4(5/2,1/2) stacking pattern. The 1-methylpyridinium salt also contains oligomers stacked in a 4(5/2,1/2) pattern, but is isomorphous with the known chloride analog instead. The trimethylphenylammonium salt contains stacks of oligomers arranged in a 4(3/2,1/2) stacking pattern similar to the tetramethylphosphonium analog. These six structures feature inversion-related organic cation pairs and hybrid oligomer/organic cation layers derived from the parent CuX(2) structure. The 2,4-dimethylpyridinium salt is isomorphous with the known (2-amino-4-methylpyridinium)(2)Cu(4)Cl(10) structure, in which isolated stacks of organic cations and of oligomers in a 4(1/2,1/2) pattern are found. In bis(3-chloro-1-methylpyridinium) octa-μ-bromido-tetrabromidopentacuprate(II), (C(6)H(7)ClN)[Cu(5)Br(12)], (VIII), containing the first reported fully halogenated quasi-planar pentacopper oligomer, the oligomers stack in a 5(3/2,1/2) stacking pattern as the highest nuclearity [Cu(n)X(2n+2)](2-) oligomer compound known with isolated stacking. Bis(2-chloro-1-methylpyridinium) dodeca-μ-bromido-tetrabromidoheptacuprate(II), (C(6)H(7)ClN)(2)[Cu(7)Br(16)], (IX), contains the second heptacopper oligomer reported and consists of layers of interleaved oligomer stacks with a 7[(7/2,1/2)][(-9/2,-1/2)] pattern isomorphous with that of the known 1,2-dimethylpyridinium analog. All the oligomers reported here are inversion symmetric.
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http://dx.doi.org/10.1107/S0108270110049024 | DOI Listing |
Nat Mater
January 2025
School of Materials Science and Engineering, Georgia Institute of Technology, Atlanta, GA, USA.
Anode-free solid-state batteries contain no active material at the negative electrode in the as-manufactured state, yielding high energy densities for use in long-range electric vehicles. The mechanisms governing charge-discharge cycling of anode-free batteries are largely controlled by electro-chemo-mechanical phenomena at solid-solid interfaces, and there are important mechanistic differences when compared with conventional lithium-excess batteries. This Perspective provides an overview of the factors governing lithium nucleation, growth, stripping and cycling in anode-free solid-state batteries, including mechanical deformation of lithium, the chemical and mechanical properties of the current collector, microstructural effects, and stripping dynamics.
View Article and Find Full Text PDFWe report the photoluminescence and thermal stability correlation between blue emitting mononuclear gold(I)-NHC chloride complexes, N-(9-anthracenyl)-N'(n-alkyl)imidazol-2-ylidene gold(I) chloride (alkyl = n-butyl (1), n-pentyl (2), n-hexyl (3)). The solid-state study reveals a unique molecular packing due to hydrogen bonding, aurophillic interaction, and CH···π interactions in all 1-3. In addition, the π···π stacking has been found in 1.
View Article and Find Full Text PDFPhys Chem Chem Phys
January 2025
School of Chemistry and Environmental Engineering, Changchun University of Science and Technology, Jilin Provincial Science and Technology Innovation Center of Optical Materials and Chemistry, Jilin Provincial International Joint Research Center of Photo-functional Materials and Chemistry, Changchun, 130022, China.
Ternary solar cells have been rapidly developed in the realm of organic solar cells (OSCs). The incorporation of a third component into a cell results in a complicated active layer morphology, and the relation of this morphology to power conversion efficiency remains elusive. In this work, two ternary active layers, B1:Y7 (10 wt%):BO-4Cl and B1:Y7 (50 wt%):BO-4Cl are constructed, and the reasons for the differences in PCE caused by varying the Y7 content are investigated using theoretical calculations.
View Article and Find Full Text PDFACS Nano
January 2025
Center for High Pressure Science (CHiPS), State Key Laboratory of Metastable Materials Science & Technology, Yanshan University, Qinhuangdao 066004, China.
Moiré superlattices, created by stacking different van der Waals materials at twist angles, have emerged as a versatile platform for exploring intriguing phenomena such as topological properties, superconductivity, the quantum anomalous Hall effect, and the unconventional Stark effect. Additionally, the formation of moiré superlattice potential can generate spontaneous symmetry breaking, leading to an anisotropic optical response and electronic transport behavior. Herein, we propose a two-step chemical vapor deposition (CVD) strategy for synthesizing WS/SbS moiré superlattices.
View Article and Find Full Text PDFSci Rep
December 2024
School of Computer and Information Engineering, Hubei Normal University, Huangshi, 435002, China.
For finely representation of complex reservoir units, higher computing overburden and lower spatial resolution are limited to traditional stochastic simulation. Therefore, based on Generative Adversarial Networks (GANs), spatial distribution patterns of regional variables can be reproduced through high-order statistical fitting. However, parameters of GANs cannot be optimized under insufficient training samples.
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