# Master Lovas-Andai and Equivalent Formulas Verifying the $\frac{8}{33}$   Two-Qubit Hilbert-Schmidt Separability Probability and Companion   Rational-Valued Conjectures

**Authors:** Paul B. Slater

arXiv: 1701.01973 · 2018-02-28

## TL;DR

This paper investigates and verifies the Hilbert-Schmidt two-qubit separability probability of 8/33 using Lovas-Andai and Slater frameworks, deriving a master formula and confirming conjectures through advanced algebraic methods.

## Contribution

It establishes a unified Lovas-Andai master formula for separability functions across different dimensions and confirms the 8/33 probability conjecture with new analytical and computational techniques.

## Key findings

- Confirmed the 8/33 two-qubit separability probability.
- Derived a general Lovas-Andai master formula for separability functions.
- Established equivalence of different formulas using holonomic recurrence relations.

## Abstract

We begin by investigating relationships between two forms of Hilbert-Schmidt two-re[al]bit and two-qubit "separability functions"--those recently advanced by Lovas and Andai (J. Phys. A 50 [2017] 295303), and those earlier presented by Slater (J. Phys. A 40 [2007] 14279). In the Lovas-Andai framework, the independent variable $\varepsilon \in [0,1]$ is the ratio $\sigma(V)$ of the singular values of the $2 \times 2$ matrix $V=D_2^{1/2} D_1^{-1/2}$ formed from the two $2 \times 2$ diagonal blocks ($D_1, D_2$) of a $4 \times 4$ density matrix $D$. In the Slater setting, the independent variable $\mu$ is the diagonal-entry ratio $\sqrt{\frac{\rho_{11} \rho_{44}}{\rho_{22} \rho_{33}}}$--with, of central importance, $\mu=\varepsilon$ or $\mu=\frac{1}{\varepsilon}$ when both $D_1$ and $D_2$ are themselves diagonal. Lovas and Andai established that their two-rebit "separability function" $\tilde{\chi}_1 (\varepsilon )$ ($\approx \varepsilon$) yields the previously conjectured Hilbert-Schmidt separability probability of $\frac{29}{64}$. We are able, in the Slater framework (using cylindrical algebraic decompositions [CAD] to enforce positivity constraints), to reproduce this result. Further, we newly find its two-qubit (yielding $\frac{8}{33}$), two-quater[nionic]-bit (yielding $\frac{26}{323}$) and "two-octo[nionic]-bit" (yielding $\frac{44482}{4091349}$) counterparts. Then, we find a Lovas-Andai "master formula", $\tilde{\chi_d}(\varepsilon)= \frac{\varepsilon ^d \Gamma (d+1)^3 \,_3\tilde{F}_2\left(-\frac{d}{2},\frac{d}{2},d;\frac{d}{2}+1,\frac{3d}{2}+1;\varepsilon ^2\right)}{\Gamma \left(\frac{d}{2}+1\right)^2}$ encompassing both even and odd values of $d$. C. Koutschan, then, using his HolonomicFunctions program, develops an order-4 recurrence satisfied by the predictions of the several formulas, establishing their equivalence.

## Full text

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## Figures

29 figures with captions in the complete paper: https://tomesphere.com/paper/1701.01973/full.md

## References

58 references — full list in the complete paper: https://tomesphere.com/paper/1701.01973/full.md

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Source: https://tomesphere.com/paper/1701.01973