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0347016172
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note
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The hyperfine Hamiltonian depends on the band structure of GaAs because it is proportional to the modulus squared of the electron wavefunction at the Ga and As nuclei; it does not contain the band-structure effective g-factor g*. The bulk GaAs g* of -0.44 [7] has been assumed to calculate the strength of the effective field acting on the electron spin; the same g* must be used to calculate energy shifts arising from that field.
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G.P. Flinn, R.T. Harley, M.J. Snelling, A.C. Tropper, T.M. Kerr, Semicond. Sci. Technol. 5 (1990) 533; M. Krapf, G. Denninger, H. Pascher, G. Weimann, W. Schlapp, Solid State Commun. 78 (1991) 459.
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0026154418
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G.P. Flinn, R.T. Harley, M.J. Snelling, A.C. Tropper, T.M. Kerr, Semicond. Sci. Technol. 5 (1990) 533; M. Krapf, G. Denninger, H. Pascher, G. Weimann, W. Schlapp, Solid State Commun. 78 (1991) 459.
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0346386079
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note
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An additional degree of uncertainty results from possible inaccuracies in the calculated maximum effective nuclear fields [19].
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38
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4143096338
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A.J. Turberfield, S.R. Haynes, P.A. Wright, R.A. Ford, R.G. Clark, J.F. Ryan, J.J. Harris, C.T. Foxon, Phys. Rev. Lett. 65 (1990) 637.
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40
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0347016177
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note
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In [28] the enhancement of the spin-wave energy due to dynamic nuclear polarization was attributed to disorder-activated coupling to large-wavevector spin waves.
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41
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D.R. Leadley, M. van der Burgt, R.J. Nicholas, C.T. Foxon, J.J. Harris, Phys. Rev. B 53 (1996) 2057.
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Harris, J.J.5
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0347016171
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-
note
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BB is used in Eq. (14) then a good fit to the data may be obtained by increasing the photoexcited carrier density assumed. If the same value is used for ε↓ - ζ then it is not possible to map the three sets of measurements to a single curve.
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43
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S.E. Barrett, R. Tycko, L.N. Pfeiffer, K.W. West, Phys. Rev. Lett. 72 (1994) 1368.
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