1981
DOI: 10.1063/1.2914770
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Theory and Applications of Electron Spin Resonance and Spin Exchange: Principles and Applications in Chemistry and Biology

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Cited by 43 publications
(94 citation statements)
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“…If the radical is tumbling rapidly in solution, the three components are ofequal intensity, are separated by the isotropic hyperfine coupling, Ai.0, and are centered -at the isotropic g value, giso0 However, if the motion is slowed, then the lines broaden as the anisotropy of the magnetic parameters of the radical is no longer averaged. r4N hyperfine couplings in Xr radicals are generally axial (AX = AY = A±, AZ = All) and strongly anisotropic (All >» AL); g values also are axial (gx = gy = g, gZ = g11) (19). The result of this is that the spectrum of the immobilized radical is dominated by z components, giving a characteristic spectrum of the kind observed here.…”
Section: Resultssupporting
confidence: 52%
“…If the radical is tumbling rapidly in solution, the three components are ofequal intensity, are separated by the isotropic hyperfine coupling, Ai.0, and are centered -at the isotropic g value, giso0 However, if the motion is slowed, then the lines broaden as the anisotropy of the magnetic parameters of the radical is no longer averaged. r4N hyperfine couplings in Xr radicals are generally axial (AX = AY = A±, AZ = All) and strongly anisotropic (All >» AL); g values also are axial (gx = gy = g, gZ = g11) (19). The result of this is that the spectrum of the immobilized radical is dominated by z components, giving a characteristic spectrum of the kind observed here.…”
Section: Resultssupporting
confidence: 52%
“…Furthermore, we have found that the shift of the centroid of the 42 mT with respect to the main position of the E' γ central line is ∆g=0.0071±0.0005, and that of the 49 mT with respect to the E' α is ∆g=0.0096±0.0005. Second order hyperfine interaction corrections [20] predict a shift of ∆g≅0.0072 for the 42 mT and of ∆g≅0.0099 for the 49 mT doublets, in quite good agreements with the experimental values. The different shift observed for the two hyperfine doublets being due to the dependence of the second order corrections on the square of the hyperfine splitting.…”
supporting
confidence: 72%
“…The corresponding ESR frequencies are collected in (4) From the transition probabilities for the allowed (Ia) and forbidden (I,) ESR transitions, which are given by the expressions in (6) with sin ' p, = B/w, and sin 'pg = B/wg, it follows that the "forbidden" transitions can only take place if the quantity B [see (3)] differs from zero.…”
Section: Conventional Esr Spectroscopymentioning
confidence: 99%
“…[1][2][3][4] The electronic Zeeman operator PEz includes the interaction of the electron spin with the external field B,. As the Zeeman energy can also be affected by orbital magnetic moments, the term PEz often yields information about excited electronic states and about the symmetry of the environment of a paramagnetic center.…”
Section: Conventional Esr Spectroscopymentioning
confidence: 99%