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Measurements performed on different singly charged dots reveal very similar electron Knight fields Be ∼10mT. In case of positively charged dots Be corresponds to the effect of the photoexcited electron of the trion while in negatively charged dots Knight field is induced by the residual charge
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Measurements performed on different singly charged dots reveal very similar electron Knight fields B e ∼ 10 mT. In case of positively charged dots B e corresponds to the effect of the photoexcited electron of the trion while in negatively charged dots Knight field is induced by the residual charge.
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The effect of the electron field on nuclei is significant only if electron-spin lifetime T1e exceeds the precession period of the nuclear spin 1/ νL, determined by Larmor frequency which is νL 9 (17 )MHz/T for indium (phosphorus). The exact value of T1e in InP dots at different fields is not available. It is known however that for large enough magnetic field T1e can be on a millisecond time scale (Ref.). We thus assume that T1e 1/ νL for Bz 0.5T and the effective field experienced by nuclei equals to the instant value of Be
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The effect of the electron field on nuclei is significant only if electron-spin lifetime T1e exceeds the precession period of the nuclear spin 1/ νL, determined by Larmor frequency which is νL 9 (17 )MHz/T for indium (phosphorus). The exact value of T1e in InP dots at different fields is not available. It is known however that for large enough magnetic field T1e can be on a millisecond time scale (Ref.). We thus assume that T1e 1/ νL for Bz 0.5T and the effective field experienced by nuclei equals to the instant value of Be.
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