1983
DOI: 10.1103/physrevlett.50.1309
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Nonlinear Far-Infrared Magnetoabsorption and Optically Detected Magnetoimpurity Effect inn-GaAs

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Cited by 29 publications
(17 citation statements)
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“…Studies of such bipolar spin orientation, where both electrons and holes got excited, gave important insights into the mechanisms of spin relaxation. We show below that by combining the circular photogalvanic effect (CPGE) [10] with saturation (bleaching of absorption) spectroscopy [17][18][19][20][21] we are able to probe spin relaxation for monopolar spin orientation. In contrast to the conventional methods of optical spin orientation, in our measurements only one type of charge carriers (electrons or holes) gets spin oriented and is involved in relaxation processes.…”
mentioning
confidence: 99%
“…Studies of such bipolar spin orientation, where both electrons and holes got excited, gave important insights into the mechanisms of spin relaxation. We show below that by combining the circular photogalvanic effect (CPGE) [10] with saturation (bleaching of absorption) spectroscopy [17][18][19][20][21] we are able to probe spin relaxation for monopolar spin orientation. In contrast to the conventional methods of optical spin orientation, in our measurements only one type of charge carriers (electrons or holes) gets spin oriented and is involved in relaxation processes.…”
mentioning
confidence: 99%
“…The free carrier concentration p, and thus the photoconductive signal AV/V, depends linearly on F for F << Fs and assumes a constant, saturated value, psat = N~i *r--~---in the high intensity limit. This approximation has been 2r~jl used to evaluate resonant impurity photoconductivity in n-GaAs at 4.2 K [3] and was also the basis of interpretation of high power absorption measurements [1,2]. It has been previously shown that at temperatures well below 4.2 K in n-GaAs excited state impact ionization dominates the optically induced free carrier generation.…”
Section: -Imentioning
confidence: 99%
“…(3) gives the typical saturation behaviour aF P :-N~4TlZ 1 + F/Fs (6) which is due to the depleting of the ground state by optical excitations. Here Fs = (2~r~'e/y)-I is the saturation photon flux 1'* density with reyI = 2 ~ T1 + S'T2 the effective relaxation time of optically excited carriers [1,5]. The free carrier concentration p, and thus the photoconductive signal AV/V, depends linearly on F for F << Fs and assumes a constant, saturated value, psat = N~i *r--~---in the high intensity limit.…”
Section: -Imentioning
confidence: 99%
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