High-field ENDOR and the sign of the hyperfine coupling
High-field ENDOR and the sign of the hyperfine coupling
复制标题
DOI:
10.1007/bf03162408
复制
发表时间:
2001-01-01
影响因子:
1
通讯作者:
Goldfarb, D
中科院分区:
文献类型:
--
作者:
Epel, B;Manikandan, P;Goldfarb, D
Two different approaches for assigning electron nuclear double resonance (ENDOR) signals to their respective Ms manifolds by a controlled generation of asymmetric ENDOR spectra, are described and applied to a number of systems. This assignment then allows a straightforward determination of the sign of the hyperfine coupling. Both approaches rely on a high thermal polarization that is easily achieved at high fields and low temperatures. For high-spin systems, such as S = 5/2 the assignment is afforded by the selective inversion of the \-3/2> --> \-1/2) electron paramagnetic resonance (EPR) transition which is highly populated as compared to its symmetric counterpart, the \1/2> --> \3/2> EPR transition, and therefore is easily identified. For S = 1/2 the determination of the sign of the hyperfine coupling becomes possible when the cross- and nuclear-spin relaxation rates are much slower than the electron-spin relaxation rate and variable mixing time pulse ENDOR is used to measure the spectrum. Under these conditions the signals of the Ms = 1/2 (cc) manifold become negative when the mixing time is on order of the electron-spin relaxation time, whereas those of the M-s = -1/2 (beta) manifold remain positive. Under partial saturation of the nuclear transitions and short mixing time the opposite behavior is observed. Pulse W-band H-1 ENDOR experiments demonstrating these approaches were applied and the sips of the hyperfine couplings of the water ligands in Mn(H2O)(2+)(6), the H-alpha and H-beta histidine protons in the Cu(histidine)(2) complex, the imidazole protons in Cu(imidazole)(2+)(6) and the cysteine beta-protons in nitrous oxide reductase were determined.