2006
DOI: 10.1103/physrevb.74.245206
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Transport and recombination through weakly coupled localized spin pairs in semiconductors during coherent spin excitation

Abstract: Semianalytical predictions for the transients of spin-dependent transport and recombination rates through localized states in semiconductors during coherent electron-spin excitation are made for the case of weakly spin-coupled charge-carrier ensembles. The results show that the on-resonant Rabi frequency of electrically or optically detected spin oscillation doubles abruptly as the strength of the resonant microwave field ␥B 1 exceeds the Larmor frequency separation within the pair of charge-carrier states bet… Show more

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Cited by 29 publications
(70 citation statements)
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“…For instance, the study of beat oscillations of charge-carrier spin-Rabi nutation in the conductivity of diode structures based on poly[2-methoxy-5-(2-ethylhexyloxy)-1,4-phenylenevinylene] (MEH-PPV) has been repeated in optical recombination by pODMR spectroscopy through transient detection of photoluminescence intensity changes [41]. This comparison revealed qualitatively identical observations to pEDMR [14] of a pronounced spin-dependent transition rate which displays the same double Gaussian resonance lines, the same Rabi nutation of spin manifolds with s=1/2 as well as distinct beat oscillations, indicative that the observed spin systems belong to weakly coupled pairs with negligible dipolar and exchange coupling [42] [15]. While this experiment unambiguously proves that weakly coupled electron-hole pairs are involved in recombination, and thus luminescence, under the low-temperature conditions where measurements were made, the results do not unambiguously prove that the weakly coupled room-temperature charge carrier spin pairs observed with pulsed EDMR are also of opposite charge and not bipolarons.…”
Section: Introductionsupporting
confidence: 59%
“…For instance, the study of beat oscillations of charge-carrier spin-Rabi nutation in the conductivity of diode structures based on poly[2-methoxy-5-(2-ethylhexyloxy)-1,4-phenylenevinylene] (MEH-PPV) has been repeated in optical recombination by pODMR spectroscopy through transient detection of photoluminescence intensity changes [41]. This comparison revealed qualitatively identical observations to pEDMR [14] of a pronounced spin-dependent transition rate which displays the same double Gaussian resonance lines, the same Rabi nutation of spin manifolds with s=1/2 as well as distinct beat oscillations, indicative that the observed spin systems belong to weakly coupled pairs with negligible dipolar and exchange coupling [42] [15]. While this experiment unambiguously proves that weakly coupled electron-hole pairs are involved in recombination, and thus luminescence, under the low-temperature conditions where measurements were made, the results do not unambiguously prove that the weakly coupled room-temperature charge carrier spin pairs observed with pulsed EDMR are also of opposite charge and not bipolarons.…”
Section: Introductionsupporting
confidence: 59%
“…3(c), we obtain a proportionality factor of γ exp = (1.03 ± 0.08)γ. Since the ratio Ω/γB 1 is greater than 1 for strongly coupled systems [26], the experimentally observed Ω/γB 1 ≈ 1 indicates a weakly coupled spin pair.…”
mentioning
confidence: 99%
“…We note that the transition from a 31 P−P b process 7 at low fields to a P b only mechanism at high fields may be explained by considering the underlying spin dynamics. The strength of an EDMR signal becomes weaker as the ratio ξ = ∆ω γB 1 of the difference of the Larmor frequencies in a pair, ∆ω, to γB 1 drops below 1, with γ being the gyromagnetic ratio 19 . Hence, at low fields EDMR signals are dominated by maximized 31 P−P b signals as ξ > 1 while ξ ≪ 1 for the P b pairs with ∆ω ≪ γB 1 due to the almost identical Landé-factors of two P b centers.…”
mentioning
confidence: 99%