2020
DOI: 10.1007/s00723-020-01263-5
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Parallel-Mode EPR of Atomic Hydrogen Encapsulated in POSS Cages

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Cited by 6 publications
(7 citation statements)
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“…The hyperfine coupling constant A of the encapsulated D atom is slightly larger than that of H as can be seen from the ratios f = A / A vac , where A vac = 1420.4057 and 218.2562 MHz are the vacuum coupling constants of hydrogen and deuterium, respectively. This result is in line with previous studies and has been attributed to both static and dynamic effects. , The parameters of Table are in very good agreement with those obtained in a recent dual-mode EPR study …”
Section: Resultssupporting
confidence: 92%
See 1 more Smart Citation
“…The hyperfine coupling constant A of the encapsulated D atom is slightly larger than that of H as can be seen from the ratios f = A / A vac , where A vac = 1420.4057 and 218.2562 MHz are the vacuum coupling constants of hydrogen and deuterium, respectively. This result is in line with previous studies and has been attributed to both static and dynamic effects. , The parameters of Table are in very good agreement with those obtained in a recent dual-mode EPR study …”
Section: Resultssupporting
confidence: 92%
“…12,13 The parameters of Table 1 are in very good agreement with those obtained in a recent dual-mode EPR study. 25 The spin−lattice relaxation time, T 1 , is very sensitive to magnetic impurities, and under aerobic conditions a short value of 1 μs is measured at room temperature. To avoid relaxation enhancement effects from paramagnetic oxygen, the EPR quartz tube was filled with helium gas with the method described previously.…”
Section: ■ Results and Discussionmentioning
confidence: 99%
“…Weil initially predicted the allowed transitions for the S = 1/2, I = 1/2 hydrogen atom (aiso = 1420 MHz), along with their intensities. 25 Later, Mitrikas et al 27 directly measured both the perpendicular and parallel-mode EPR spectra of the H atom encapsulated in polyhedral oligomeric silsesquioxane cages ( 1 H@h72Q8M8) and observed a hyperfine coupling of A = 1416.58 MHz, in excellent agreement with Weil's proposal. The parallel-mode EPR of the H atom is fairly weak and it is noted that the intensity of both the perpendicular and parallel-mode EPR transitions are determined by the time dependent perturbation solution of the magnetic dipole transition spin-Hamiltonian operator.…”
Section: Introductionsupporting
confidence: 54%
“…More simply stated, the intensity of the parallel-mode EPR is proportional to the degree of state-mixing, which is greatest in the low field regime. Mitrikas et al 27 recognized the potential of parallel-mode EPR spectroscopy to other S = 1/2 systems and reported the predicted perpendicular and parallel-mode EPR spectra of Bi:Si.…”
Section: Introductionmentioning
confidence: 99%
“…Weil initially predicted the allowed transitions for the S = 1/2, I = 1/2 hydrogen atom ( a iso = 1420 MHz), along with their intensities . Later, Mitrikas et al directly measured both the perpendicular- and parallel-mode EPR spectra of the H atom encapsulated in polyhedral oligomeric silsesquioxane cages ( 1 H@ h 72 Q 8 M 8 ) and observed a hyperfine coupling of A = 1416.58 MHz, in excellent agreement with Weil’s proposal. The parallel-mode EPR of the H atom is fairly weak, and it is noted that the intensity of both the perpendicular- and parallel-mode EPR transitions is determined by the time-dependent perturbation solution of the magnetic dipole transition spin-Hamiltonian operator.…”
Section: Introductionmentioning
confidence: 63%