1972
DOI: 10.1103/physrevb.5.2409
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Envelope Modulation in Spin-Echo Experiments

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Cited by 549 publications
(412 citation statements)
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“…The cavity used for the ESEEM experiments was a folded stripline, which could accommodate frozen samples in conventional 3 mm internal diameter quartz EPR tubes [17,18]. ESEEM data were collected at 1.8 K using the stimulated echo technique (90°-r-90°-T-90°) with values of r chosen to suppress modulations arising from weakly coupled protons [19]. Spectra were obtained by Fourier transformation using a modified version of the dead time reconstruction method of Mims [20].…”
Section: Methods Of Pulsed Epr Spectroscopymentioning
confidence: 99%
“…The cavity used for the ESEEM experiments was a folded stripline, which could accommodate frozen samples in conventional 3 mm internal diameter quartz EPR tubes [17,18]. ESEEM data were collected at 1.8 K using the stimulated echo technique (90°-r-90°-T-90°) with values of r chosen to suppress modulations arising from weakly coupled protons [19]. Spectra were obtained by Fourier transformation using a modified version of the dead time reconstruction method of Mims [20].…”
Section: Methods Of Pulsed Epr Spectroscopymentioning
confidence: 99%
“…The hyperfine terms, A iso and A dip , are all divided by the ␥( 1 H)/␥( 2 H) = 6.5 ratio for these simulations, and electric quadrupolar parameters of e 2 qQ = 0.22 MHz and = 0.1 are used for simulations for this nuclear spin I = 1 nucleus. The simulations are carried out via a matrix diagonalization program previously described (Britt et al 1989) based on the density matrix calculations described by Mims (1972). Figure 4a,b shows the data for fixed A dip and varied A iso values.…”
Section: (C) Eseem and Ese-endor Spectral Trendsmentioning
confidence: 99%
“…In parallel, theory was developed for analyzing linewidths and lineshapes in CW EPR spectra in terms of molecular dynamics [8][9][10]. At about the same time a few select groups in the Soviet Union and the USA worked on pulse experiments, using spin echo phenomena to measure electron spin relaxation [11], to detect hyperfine couplings by electron spin echo envelope modulation (ESEEM) techniques [12], to acquire ENDOR spectra in a broader temperature range than with CW methods [13], and to measure distances between electron spins [14]. These developments were pursued by physicists, were heavily focused on methodology, and were hardly recognized by mainstream chemists even by the end of the 1980s when the groundwork was all done.…”
Section: Prefacementioning
confidence: 99%