Victoria J. Wright | Searcharxiv

arXiv2024

Indistinguishability in general probabilistic theories

The existence of indistinguishable quantum particles provides an explanation for various physical phenomena we observe in nature. We lay out a path for the study of indistinguishable particles in general probabilistic theories (GPTs) via two frameworks: the traditional GPT framework and the diagrammatic framework of process theories. In the first approach we define different types of indistinguishable particle by the orbits of symmetric states under transformations. In the diagrammatic approach, we find a decomposition of the symmetrised state space using two key constructions from category theory: the biproduct completion and the Karoubi envelope. In both cases for pairs of indistinguishable particles in quantum theory we recover bosons and fermions.

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arXiv2024

Maximal intrinsic randomness of a quantum state

One of the most counterintuitive aspects of quantum theory is its claim that there is 'intrinsic' randomness in the physical world. Quantum information science has greatly progressed in the study of intrinsic, or secret, quantum randomness in the past decade. With much emphasis on device-independent and semi-device-independent bounds, one of the most basic questions has escaped attention: how much intrinsic randomness can be extracted from a given state $ρ$, and what measurements achieve this bound? We answer this question for three different randomness quantifiers: the conditional min-entropy, the conditional von Neumann entropy and the conditional max-entropy. For the first, we solve the min-max problem of finding the projective measurement that minimises the maximal guessing probability of an eavesdropper. The result is that one can guarantee an amount of conditional min-entropy $H^*_{\textrm{min}}=-\log_2 P_{\textrm{guess}}^{*}(ρ)$ with $P_{\textrm{guess}}^{*}(ρ)=\frac{1}{d}(\textrm{tr} \sqrtρ)^2$ by performing suitable projective measurements. For the conditional von Neumann entropy, we find that the maximal value is $H^{*}= \log_{2}d-S(ρ)$, with $S(ρ)$ the von Neumann entropy of $ρ$, while for the conditional max-entropy, we find the maximal value $H^{*}_\textrm{max}=\log_{2}d + \log_{2}λ_{\textrm{max}}(ρ)$, where $λ_{\textrm{max}}(ρ)$ is the largest eigenvalue of $ρ$. Optimal values for $H^{*}_{\textrm{min}}$, $H^{*}$ and $H^{*}_\textrm{max}$ are achieved by measuring in any basis that is unbiased to the eigenbasis of $ρ$, as well as by other, less intuitive, measurements.

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