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84863867682
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As seen from Fig. 3 the PL polarization changes its sign, i.e., becomes positive, at small B when the optical excitation is weak. The origin of this positive polarization can be understood from an analysis of the PL kinetics. The PL polarization is positive right after the excitation (Ref.) and then approaches a negative value whose magnitude is small at weak excitation when the relaxation of the electron-spin polarization becomes competitive with the excitation.
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As seen from Fig. 3 the PL polarization changes its sign, i.e., becomes positive, at small B when the optical excitation is weak. The origin of this positive polarization can be understood from an analysis of the PL kinetics. The PL polarization is positive right after the excitation (Ref.) and then approaches a negative value whose magnitude is small at weak excitation when the relaxation of the electron-spin polarization becomes competitive with the excitation.
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84863859243
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Absorption of the photon results in creation of an electron-hole pair which relaxes in energy and is coupled with the resident electron in a trion. During this process the wave function and the energy of the resident electron is considerably changed. We assume that it is the process, which allows one to overcome the problem of the energy conservation in the process of transfer of angular momentum from electron to nuclear spins.
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Absorption of the photon results in creation of an electron-hole pair which relaxes in energy and is coupled with the resident electron in a trion. During this process the wave function and the energy of the resident electron is considerably changed. We assume that it is the process, which allows one to overcome the problem of the energy conservation in the process of transfer of angular momentum from electron to nuclear spins.
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84863859221
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Experimentally, the HWHM of the polarization dip depends on the excitation conditions, in particular, on the excitation density and the laser excitation mode (pulsed or continuous wave). For determining Bfρ in this work we used the same conditions as for studying the DNP field.
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Experimentally, the HWHM of the polarization dip depends on the excitation conditions, in particular, on the excitation density and the laser excitation mode (pulsed or continuous wave). For determining Bfρ in this work we used the same conditions as for studying the DNP field.
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