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Excited-state spectroscopy on a nearly closed quantum dot via charge detection
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9.This expression is obtained by multiplying the probability that the dot is empty, with a sine-wave of frequency (as is done in the lock-in amplifier), and averaging the resulting signal over one period. is given by during the high stage of the pulse, and by during the low stage.
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11.The expected Zeeman splitting of the triplet state is not resolved here.
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