Abstract
In this paper, we examine the average Rényi entropy \(S_{\alpha }\) of a subsystem A when the whole composite system AB is a random pure state. We assume that the Hilbert space dimensions of A and AB are m and mn, respectively. First, we compute the average Rényi entropy analytically for \(m = \alpha = 2\). We compare this analytical result with the approximate average Rényi entropy, which is shown to be very close. For general case, we compute the average of the approximate Rényi entropy \({\widetilde{S}}_{\alpha } (m,n)\) analytically. When \(1 \ll n\), \({\widetilde{S}}_{\alpha } (m,n)\) reduces to \(\ln m - \frac{\alpha }{2 n} (m - m^{-1})\), which is in agreement with the asymptotic expression of the average von Neumann entropy. Based on the analytic result of \({\widetilde{S}}_{\alpha } (m,n)\), we plot the \(\ln m\)-dependence of the Rényi information derived from \({\widetilde{S}}_{\alpha } (m,n)\). It is remarkable to note that the nearly vanishing region of the information becomes shorten with increasing \(\alpha \) and eventually disappears in the limit of \(\alpha \rightarrow \infty \). The physical implication of the result is briefly discussed.
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The datasets generated during and/or analyzed during the current study are available from the corresponding author on reasonable request.
Notes
Eq. (2.2) is called a density of the eigenvalues of the Wishart matrix.
Furthermore, F(m, n) depends on the \(j^{th}\) term of some recurrence relations, where j is a function of m and n. This term is expressed with the aid of few special functions such as Lerch transcendent
$$\begin{aligned} \Phi (z,s,a) = \sum _{k=0}^{\infty } \frac{z^k}{(k + a)^s}. \end{aligned}$$
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This work was supported by the National Research Foundation of Korea (NRF) grant funded by the Korea government (MSIT) (No. 2021R1A2C1094580).
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Kim, M., Hwang, MR., Jung, E. et al. Average Rényi entropy of a subsystem in random pure state. Quantum Inf Process 23, 37 (2024). https://doi.org/10.1007/s11128-023-04249-x
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DOI: https://doi.org/10.1007/s11128-023-04249-x