1987
DOI: 10.1016/0022-2364(87)90340-4
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Echo envelope modulation with quadrupole interaction

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Cited by 4 publications
(5 citation statements)
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“…The observation that echo modulation depth decreases with larger quadrupole interaction was discussed by Rowan, who showed that when the quadrupole interaction is much stronger than the electron nuclear hyperfine interaction, the nuclear spin quantum axis is determined by the direction of the quadrupole interaction and is not changed appreciably by electron spin flips induced by the microwave pulses. Therefore there is little nuclear spin state coherent superposition induced by the microwave pulse and therefore little echo envelope modulation results.…”
Section: Discussionmentioning
confidence: 98%
“…The observation that echo modulation depth decreases with larger quadrupole interaction was discussed by Rowan, who showed that when the quadrupole interaction is much stronger than the electron nuclear hyperfine interaction, the nuclear spin quantum axis is determined by the direction of the quadrupole interaction and is not changed appreciably by electron spin flips induced by the microwave pulses. Therefore there is little nuclear spin state coherent superposition induced by the microwave pulse and therefore little echo envelope modulation results.…”
Section: Discussionmentioning
confidence: 98%
“…42 Simulation of ESEEM recordings was performed using the density operator (DO) formalism as described previously. 43 The general strategy consisted of evaluation of the DO matrix, F ˆ, which is initially equal to that of the thermal equilibrium DO, F ˆ0, and then evolves during the subsequent periods of pulse action and the pulse-free evolution, terminating at the final instant of echo detection…”
Section: Methodsmentioning
confidence: 99%
“…They were programmed and executed using the EasySpin toolbox for the Matlab program package . Simulation of ESEEM recordings was performed using the density operator (DO) formalism as described previously . The general strategy consisted of evaluation of the DO matrix, ρ̂, which is initially equal to that of the thermal equilibrium DO, ρ̂ 0 , and then evolves during the subsequent periods of pulse action and the pulse-free evolution, terminating at the final instant of echo detection ρ ^ SSE = U ^ SSE · ρ ^ 0 · U ^ SSE 1 Here ρ̂ 0 = Z ·exp(− h ℋ̂/ kT ) with Z −1 = Tr{exp(− h ℋ̂/ kT )}.…”
Section: Methodsmentioning
confidence: 99%
“…A 14 N eeqQ value of 2.0 MHz (η ) 0) was chosen on the basis of an azide solution NMR study (44,45). For the modest isotropic coupling employed here (lower than the "exact cancellation" matching condition that gives favorable 14 N modulation) (46), the effect of the nonzero nqi is to broaden and decrease the amplitude of the 14 N peaks (47). Peaks were observed in the undamped simulation (not shown), but after the exponential damping function was applied, the simulated frequency-domain spectrum was quite featureless, matching the experimental observation.…”
Section: Resultsmentioning
confidence: 99%