Finite size scaling of bitstring probability distributions for Rydberg arrays

Abstract

We calculate the probabilities $p_{\{n\}}$ of the measured bitstrings $\{n\}$ for the vacuum of Rydberg ladders with $N_q$ atoms. As $N_q$ increases, the $p_{\{n\}}$ decrease but become more dense in the low $p$ region raising the possibility that their smallness could be compensated by their large number. The importance of the low probability states can be estimated from the cumulative probability distribution $\hat{I}\pounds (p_{\hat{I}}›,N_q)$, which is the probability to observe any state having a probability $p\le p_{\hat{I}}›$. For not too large values of $p_{\hat{I}}›$, it is possible to approximately collapse the $\hat{I}\pounds (p_{\hat{I}}›,N_q)$ for successive $N_q$ into a function resembling the Fermi function when plotted as a function of $-\ln (p_{\hat{I}}›)$. We show that the number of shots necessary to reduce $\hat{I}\pounds (p_{\hat{I}}›,N_q)$ to some low enough value grows exponentially with $N_q$. We discuss the implications for calculating observables associated with the vacuum.

9 pages, 9 figures

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