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Volumn 79, Issue 12, 2009, Pages

Electron-spin relaxation in bulk III-V semiconductors from a fully microscopic kinetic spin Bloch equation approach

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EID: 65549135019     PISSN: 10980121     EISSN: 1550235X     Source Type: Journal    
DOI: 10.1103/PhysRevB.79.125206     Document Type: Article
Times cited : (112)

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    • The spin-orbit parameter is also checked by comparing with the experimental results in Ref.. A best fitting gives γD =99.2eV3 in InAs which is 2.3 times as large as that in Ref.. This only enhances the DP spin relaxation by 5.5 times and strengthens our conclusion that the DP mechanism is more efficient (6 times) than the EY mechanism in InAs. It is noted that the fitted γD =99.2eV 3 is comparable with the value γD =105eV 3 calculated in 10.1063/1.1290143
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    • Boggess, T.F.1    Olesberg, J.T.2    Yu, C.3    Flatté, M.E.4    Lau, W.H.5
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    • 65549125663 scopus 로고    scopus 로고
    • The spin-orbit parameter γD in GaAs fitted from experiments is 2.9 times smaller than that in Table 1. Even for such a γD, the spin relaxation due to the DP mechanism is still much more efficient (20 times) than that due to the EY mechanism [see also Appendix].
    • The spin-orbit parameter γD in GaAs fitted from experiments is 2.9 times smaller than that in Table 1. Even for such a γD, the spin relaxation due to the DP mechanism is still much more efficient (20 times) than that due to the EY mechanism [see also Appendix].
  • 118
  • 120
    • 65549084073 scopus 로고    scopus 로고
    • Note that the SOC parameter we used in this section (γD =23.9eV 3) is larger than the value (γD =8.2eV 3) fitted from experimental data (see Appendix). However, as the DP spin relaxation is more than two orders of magnitude larger than the BAP spin relaxation, the choice of the γD does not change the conclusion that the BAP mechanism is unimportant.
    • Note that the SOC parameter we used in this section (γD =23.9eV 3) is larger than the value (γD =8.2eV 3) fitted from experimental data (see Appendix). However, as the DP spin relaxation is more than two orders of magnitude larger than the BAP spin relaxation, the choice of the γD does not change the conclusion that the BAP mechanism is unimportant.
  • 121
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    • Further calculation indicates that the results from Eq. 28 deviate more from the calculation via the KSBEs at small spin polarization as the Pauli blocking of spin-flip scattering is more pronounced when both spin bands are nearly equally populated.
    • Further calculation indicates that the results from Eq. 28 deviate more from the calculation via the KSBEs at small spin polarization as the Pauli blocking of spin-flip scattering is more pronounced when both spin bands are nearly equally populated.
  • 122
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    • According to Eq. 27, the effect of the Coulomb HF term can be estimated by τs (P) = τs (P=0) [1+ (V q0 ne P τ) 2] where V q0 describes the average Coulomb interaction with q0, ne, P being the average momentum, the electron density, and the initial spin polarization, respectively. Thus the effect of the Coulomb HF term is more pronounced for larger ne, P and weaker scattering (i.e., larger τ). Moreover, increase in the temperature would reduce the effect as q0 becomes larger and V q0 becomes smaller.
    • According to Eq. 27, the effect of the Coulomb HF term can be estimated by τs (P) = τs (P=0) [1+ (V q0 ne P τ) 2] where V q0 describes the average Coulomb interaction with q0, ne, P being the average momentum, the electron density, and the initial spin polarization, respectively. Thus the effect of the Coulomb HF term is more pronounced for larger ne, P and weaker scattering (i.e., larger τ). Moreover, increase in the temperature would reduce the effect as q0 becomes larger and V q0 becomes smaller.
  • 123
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    • The EY mechanism is checked to be unimportant in the parameter region we studied for both p-GaAs and p-GaSb.
    • The EY mechanism is checked to be unimportant in the parameter region we studied for both p-GaAs and p-GaSb.
  • 124
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    • The initial spin polarization dependence of the SRT is weak due to the fact that the impurity density is larger than the electron density according to the analysis in Sec. 3 3.
    • The initial spin polarization dependence of the SRT is weak due to the fact that the impurity density is larger than the electron density according to the analysis in Sec. 3 3.
  • 127
    • 56349143869 scopus 로고    scopus 로고
    • 10.1063/1.3018600
    • J. Y. Fu and M. W. Wu, J. Appl. Phys. 104, 093712 (2008). 10.1063/1.3018600
    • (2008) J. Appl. Phys. , vol.104 , pp. 093712
    • Fu, J.Y.1    Wu, M.W.2
  • 128
    • 21244505446 scopus 로고    scopus 로고
    • Spin relaxation in ZnO has attracted much interest recently. Experiment indicates very long spin relaxation time [10.1063/1.1946204] and the electrical control of spin lifetime was also achieved
    • Spin relaxation in ZnO has attracted much interest recently. Experiment indicates very long spin relaxation time [S. Ghosh, V. Sih, W. H. Lau, D. D. Awschalom, S.-Y. Bae, S. Wang, S. Vaidya, and G. Chapline, Appl. Phys. Lett. 86, 232507 (2005) 10.1063/1.1946204] and the electrical control of spin lifetime was also achieved
    • (2005) Appl. Phys. Lett. , vol.86 , pp. 232507
    • Ghosh, S.1    Sih, V.2    Lau, W.H.3    Awschalom, D.D.4    S.-Y. Bae5    Wang, S.6    Vaidya, S.7    Chapline, G.8
  • 130
    • 63249123143 scopus 로고    scopus 로고
    • a theoretical study including both the localized and conduction electrons with the Wurzite-structure-induced Rashba-like SOC considered was performed [10.1103/PhysRevB.79.115204
    • a theoretical study including both the localized and conduction electrons with the Wurzite-structure-induced Rashba-like SOC considered was performed [N. J. Harmon, W. O. Putikka, and R. Joynt, Phys. Rev. B 79, 115204 (2009)]. 10.1103/PhysRevB.79.115204
    • (2009) Phys. Rev. B , vol.79 , pp. 115204
    • Harmon, N.J.1    Putikka, W.O.2    Joynt, R.3
  • 132
    • 65549112717 scopus 로고    scopus 로고
    • Ph.D. thesis, University of Science and Technology of China
    • J. L. Cheng, Ph.D. thesis, University of Science and Technology of China, 2007.
    • (2007)
    • Cheng, J.L.1


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