首页> 外文期刊>Inorganic Chemistry: A Research Journal that Includes Bioinorganic, Catalytic, Organometallic, Solid-State, and Synthetic Chemistry and Reaction Dynamics >WEAK INTER- AND INTRALAYER EXCHANGE COUPLING BETWEEN COPPER(II) DIMERS AND A TRIPLET DENSITY EFFECT IN EPR OF TRIS(ETHYLENEDIAMINE) COBALT(III) BIS(MU-CHLORO)BIS[TRICHLOROCUPRATE(II)] DICHLORIDE DIHYDRATE
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WEAK INTER- AND INTRALAYER EXCHANGE COUPLING BETWEEN COPPER(II) DIMERS AND A TRIPLET DENSITY EFFECT IN EPR OF TRIS(ETHYLENEDIAMINE) COBALT(III) BIS(MU-CHLORO)BIS[TRICHLOROCUPRATE(II)] DICHLORIDE DIHYDRATE

机译:铜(II)直径之间的弱层间和层间交换耦合和三乙撑双乙胺(双氯)双[三氯双膦酸盐]二水合物的EPR中的三重态密度效应

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Low-temperature EPR spectra of Co(en)(3)CuCl5 . H2O single crystals were studied at X-band. The crystals contain layers of antiferromagnetically coupled Cu2Cl84- dimers, with singlet-triplet splitting 2J(0) = -14.8 cm(-1), separated by diamagnetic Co(en)(3) molecules. Superexchange coupling between dimers located in neighboring layers, determined from the merging effect of EPR lines from inequivalent sites, is J(1) = 0.00712 cm(-1) at room temperature, decreases to 0.00325 cm(-1) below 100 K, and then is temperature independent. Below 15 K the fine structure lines from S = 1 are resolved with the following zero-field splitting parameters: D-z = -0.0200 cm(-1), D-y = 0.0147 cm(-1), and D-x = 0.0053 cm(-1). The appearance of the structure is a result of a decrease in the number of magnetic dimers due to a rapid thermal depopulation of the triplet state when kT < 2J(0). A detailed analysis of this process allowed us to determine intralayer exchange coupling between dimers which amounts to J(2) = 0.041 cm(-1) at 100 K and decreases on cooling following triplet density rho(T) = [1 + 1/3 exp(-2J(0)/kt)](-1)) behavior. Hyperfine splitting is not resolved down to 4.2 K, and the relatively narrow lines indicate a strong mobility of the still remaining triplet excitons. The line width decreases on cooling down to about 100 K, and then a strong broadening appears resulting in the fine structure splitting. Contributions from the narrowing effect, triplet state density, and temperature variations of the zero-field splitting have been separated in Delta B-rho rho(T). A decrease in the zero-field splitting occurs on heating and, in the temperature range 4.2-100 K, is phenomenologically described by the equation D(T) = D-0(1 - aT - bT(-2)). [References: 36]
机译:Co(en)(3)CuCl5的低温EPR光谱。在X波段研究了H2O单晶。晶体包含反铁磁耦合的Cu2Cl84-二聚体层,单峰-三重态分裂2J(0)= -14.8 cm(-1),由抗磁性Co(en)(3)分子分隔。由邻近位置的EPR线的合并效应确定的位于相邻层中的二聚体之间的超交换耦合在室温下为J(1)= 0.00712 cm(-1),在100 K以下时降低为0.00325 cm(-1),并且那么温度是独立的。在15 K以下,使用以下零场分裂参数解析S = 1的精细结构线:Dz = -0.0200 cm(-1),Dy = 0.0147 cm(-1)和Dx = 0.0053 cm(-1) 。该结构的出现是由于当kT <2J(0)时三重态的快速热减少导致的磁性二聚体数量减少的结果。对该过程的详细分析使我们能够确定二聚体之间的层内交换耦合,在100 K时,其耦合量为J(2)= 0.041 cm(-1),在三重态密度rho(T)= [1 + 1/3之后,冷却时降低exp(-2J(0)/ kt)](-1))行为。直到4.2 K都无法解析超精细分裂,并且相对较窄的线表示仍然存在的三重态激子具有很强的迁移能力。线宽在冷却至约100 K时减小,然后出现强烈的展宽,从而导致精细的结构分裂。在Delta B-rho rho(T)中分离了来自变窄效应,三重态密度和零场分裂温度变化的贡献。零场分裂的减少在加热时发生,并且在温度范围4.2-100 K上,从现象学上用等式D(T)= D-0(1- aT-bT(-2))描述。 [参考:36]

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