1972
DOI: 10.1021/j100652a024
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Paramagnetic relaxation study of spatial distribution of trapped radicals in .gamma.-irradiated alkaline ice and organic glasses at 4.2.deg.K

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Cited by 13 publications
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“…(5)') under the adiabatic stow passage (5) conditions; where H I/z is the HI at which the EPR signal intensity is one-half of that in the absence of saturation. A parameter "a" which is necessary to determine T: can also be obtained from the saturation curve: (6) where H1u and HIL are the microwave HI at which the signal has decreased to 1/2 of its maximum amplitude in the saturated region and unsaturated region, respectively. The equation was derived by Zhidkov et al'?…”
Section: Theorymentioning
confidence: 99%
“…(5)') under the adiabatic stow passage (5) conditions; where H I/z is the HI at which the EPR signal intensity is one-half of that in the absence of saturation. A parameter "a" which is necessary to determine T: can also be obtained from the saturation curve: (6) where H1u and HIL are the microwave HI at which the signal has decreased to 1/2 of its maximum amplitude in the saturated region and unsaturated region, respectively. The equation was derived by Zhidkov et al'?…”
Section: Theorymentioning
confidence: 99%
“…(2) Does the electron spin resonance relaxation time (TiT2)1''2 of the radicals decrease with increasing dose in surements have been used to determine upper limits of the electron spur dimensions in several glasses6 and of the radical spur dimensions in 2-methyltetrahydrofuran (MTHF). 7 The latter suggest that the radical spur is smaller than the electron spur.…”
Section: Introductionmentioning
confidence: 99%