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Entropy-based random quantum states

Harry J. D. Miller

TL;DR

This work introduces an entropy-based approach to sampling random quantum states by leveraging the Bogoliubov-Kubo-Mori (BKM) metric, a geometric generalization tied to von Neumann entropy. It derives the metric-induced volume form and the associated eigenvalue density, revealing a sampling procedure linked to the Muttalib–Borodin ensemble and yielding a new random-density ensemble with higher purity than HS or BH ensembles. The paper provides a Page-like entropy estimate for the BKM ensemble, demonstrates concentration of entropy, and offers the X–Y sampling algorithm that reproduces the BKM statistics; these results enable an uninformative prior for Bayesian quantum state tomography, particularly in high-purity regimes, and offer a tool to study typical entanglement in finite-depth quantum circuits. It also outlines future directions, including cost analyses, thermodynamic connections, and extensions to infinite-dimensional systems.

Abstract

In quantum information geometry, the curvature of von-Neumann entropy and relative entropy induce a natural metric on the space of mixed quantum states. Here we use this information metric to construct a random matrix ensemble for states and investigate its key statistical properties such the eigenvalue density and probability distribution of entropy. We present an algorithm for generating these entropy-based random density matrices by sampling a class of bipartite pure states, thus providing a new recipe for random state generation that differs from the well established Hilbert-Schmidt and Bures-Hall ensemble approaches. We find that a distinguishing feature of the ensemble is its larger purity and increased volume towards the boundary of full-rank states. The entropy-based ensemble can thus be used as a uninformative prior for Bayesian quantum state tomography in high purity regimes, and as a tool for quantifying typical entanglement in finite depth quantum circuits.

Entropy-based random quantum states

TL;DR

This work introduces an entropy-based approach to sampling random quantum states by leveraging the Bogoliubov-Kubo-Mori (BKM) metric, a geometric generalization tied to von Neumann entropy. It derives the metric-induced volume form and the associated eigenvalue density, revealing a sampling procedure linked to the Muttalib–Borodin ensemble and yielding a new random-density ensemble with higher purity than HS or BH ensembles. The paper provides a Page-like entropy estimate for the BKM ensemble, demonstrates concentration of entropy, and offers the X–Y sampling algorithm that reproduces the BKM statistics; these results enable an uninformative prior for Bayesian quantum state tomography, particularly in high-purity regimes, and offer a tool to study typical entanglement in finite-depth quantum circuits. It also outlines future directions, including cost analyses, thermodynamic connections, and extensions to infinite-dimensional systems.

Abstract

In quantum information geometry, the curvature of von-Neumann entropy and relative entropy induce a natural metric on the space of mixed quantum states. Here we use this information metric to construct a random matrix ensemble for states and investigate its key statistical properties such the eigenvalue density and probability distribution of entropy. We present an algorithm for generating these entropy-based random density matrices by sampling a class of bipartite pure states, thus providing a new recipe for random state generation that differs from the well established Hilbert-Schmidt and Bures-Hall ensemble approaches. We find that a distinguishing feature of the ensemble is its larger purity and increased volume towards the boundary of full-rank states. The entropy-based ensemble can thus be used as a uninformative prior for Bayesian quantum state tomography in high purity regimes, and as a tool for quantifying typical entanglement in finite depth quantum circuits.

Paper Structure

This paper contains 8 sections, 38 equations, 2 figures.

Figures (2)

  • Figure 1: (a) Plot of the asymptotic marginal eigenvalue density for the BKM ensemble \ref{['eq:lambert']}, compared with the equivalent distribution for Hilbert--Schmidt states \ref{['eq:HS']} and Bures--Hall states \ref{['eq:BH']}. (b) Plot of the average von Neumann entropy $\langle S\rangle$ as a function of dimension $N$ for the BKM ensemble (black) and Bures--Hall ensemble (red), along with the maximum entropy $\ln N$ (blue).
  • Figure 2: Probability density function of standardised von-Neumann entropy compared with a Gaussian fitting for dimension $N=70$ and $10^5$ samples. Inset: standard deviation in entropy $\sigma[S]$ as a function of $N$.