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See refs 24, 25, and 52 for more on the relation between the emission of a single dot and ensemble of dots
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See refs 24, 25, and 52 for more on the relation between the emission of a single dot and ensemble of dots.
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53
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2.
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54
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84906383314
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note
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on/off here represent the standard deviations of the distributions of the corresponding exponents and not the errors in determination of their mean value. We also note that the on time distributions are less close to the power-law decays than the off times, partly due to the exponential cutoffs and partly due to varying intensities in the on-state (cf. Figure 1).
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After our work was completed, a recent study investigated the continuous distribution of emission states from single nanocrystals. Zhang, K.; Chang, H.; Fu, A.; Alivisatos, A. P.; Yang, H. Nano Lett. 2006, 6, 843.
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b/T decreases.
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62
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84906400432
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note
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The observed fluctuations in the on-state intensity of a single dot cannot be accounted for by a combination of background noise, shot noise, and the binning. Indeed, the background noise, which is the same for both on and off-states, is relatively small and lies more or less within one bin in the histograms of Figure 2. The shot noise is due to Poisson statistics of photon emission, and its standard deviation is the square root of the emission mean. With the emission intensity mean in the on-state of the order of 100 photons per bin or more (cf. Figure 2), the shot noise is not wide, relative to the mean. Note that in fact not all the emitted photons are counted, and if the detection efficiency is roughly constant, then the effect of the shot noise is even weaker. Finally, if the intensity trace is dominated by the power-law distributed on and off intervals, then there should be only a small minority of bins inside which state switches, which could produce any averaged intensity value for such a bin, occur.
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