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ZERO-FIELD ELECTRON MAGNETIC RESONANCE SPECTRA OF COPPER CARBOXYLATES

机译:羧酸铜的零场电子磁共振谱

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The design of a new zero-field electron magnetic resonance spectrometer including cryogenic capabilities and a new tuning mechanism for sweeping over approximately two octaves is described, The tuning mechanism is based on a one-loop, two-gap resonator mounted on quartz rods in such a manner that rotating the rods changes the width of the gap and the resonant frequency of the resonator, The spectrometer was used to measure the zero-field emr spectra of several copper carboxylate dimers at 90 K and 70 K. The parallel hyperfine structure was well resolved in all of the spectra and this allowed accurate determination of D, E, and A(parallel to). A(perpendicular to) was found to be poorly defined in general and least square refinements attached large errors to this term in the spin Hamiltonian. The zero-field terms in the spin Hamiltonian at 90 K were determined to be D=9.828 GHz, E=83 MH2, A(parallel to)=217 MHz for [Cu(CH3CO2)(2)(CO(NH2)(2))](2) . 2H(2)O; D=9,985 GHz, E = 43 MHz, A(parallel to) = 221 MHz for [Cu(C2H5CO2)(2) (H2O)](2); D= 10.107 GHz, E = 49 MHz, A(parallel to) = 218 MHz for [Cu(C2H5CO2)(2)(CO(NH2)(2))](2); D=9.979 GHz, E = 192 MHz, (parallel to) = 223 MHz for [Cu(C6H5CO2)(2)(C6M5CO2H)](2). A model which assumes A(perpendicular to)=0 is discussed in detail as it was found that all of the features observed in the spectra could be interpreted using simple explicit expressions derived from the model. (C) 1997 American Institute of Physics. [References: 32]
机译:描述了一种新型的具有低温能力的零场电子磁共振波谱仪的设计,以及一种用于扫过大约两个八度音阶的新调谐机构的设计。该调谐机构基于一个安装在石英棒上的单环,两间隙谐振器。通过旋转棒改变间隙的宽度和谐振器的谐振频率,该光谱仪用于测量90 K和70 K上几个羧酸铜二聚体的零场emr光谱。在所有光谱中均得到分离,从而可以精确测定D,E和A(平行于)。在一般的自旋哈密顿量中,发现A(垂直于)定义不充分,最小二乘精化对该术语附加了较大的误差。对于[Cu(CH3CO2)(2)(CO(NH2)(2),确定为90 K的自旋哈密顿量的零场项为D = 9.828 GHz,E = 83 MH2,A(平行)= 217 MHz ))](2)。 2H(2)O;对于[Cu(C 2 H 5 CO 2)(2)(H 2 O)](2),D = 9,985 GHz,E = 43 MHz,A(平行)= 221 MHz;对于[Cu(C 2 H 5 CO 2)(2)(CO(NH 2)(2))](2),D = 10.107GHz,E = 49MHz,A(平行)= 218MHz;对于[Cu(C6H5CO2)(2)(C6M5CO2H)](2),D = 9.979 GHz,E = 192 MHz,(平行)= 223 MHz。详细地讨论了假设A(垂直于)= 0的模型,因为发现可以使用从模型得出的简单显式来解释光谱中观察到的所有特征。 (C)1997美国物理研究所。 [参考:32]

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