The p→qp\to q norm conjecture for Gaussian quantum-limited amplifiers

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Let Aκ\mathcal{A}_\kappa be the one-mode Gaussian quantum-limited amplifier with amplification parameter κ≥1\kappa\ge1, let MM be a positive integer, and let ω^z\hat{\omega}_z denote the thermal Gaussian state parametrized by 0≤z<10\le z<1. For p≥1p\ge1, define the Schatten norm of a positive semidefinite operator A^\hat A by

∥A^∥p=(Tr⁡A^p)1/p.\left\|\hat A\right\|_p=\left(\operatorname{Tr}\hat A^p\right)^{1/p}.

The p→qp\to q norm conjecture. For any κ≥1\kappa\ge1 and any p,q≥1p,q\ge1, every quantum state ρ^\hat\rho satisfies

∥Aκ⊗M(ρ^)∥q∥ρ^∥p≤(sup⁡0≤z<1∥Aκ(ω^z)∥q∥ω^z∥p)M.\frac{\left\|\mathcal{A}_\kappa^{\otimes M}(\hat\rho)\right\|_q}{\left\|\hat\rho\right\|_p} \le \left(\sup_{0\le z<1}\frac{\left\|\mathcal{A}_\kappa(\hat\omega_z)\right\|_q}{\left\|\hat\omega_z\right\|_p}\right)^M.

The conjecture is known for M=1M=1, for p=qp=q and arbitrary MM, and for p=1p=1 and arbitrary MM; in the latter case the supremum is attained by the vacuum, while for p=qp=q it is asymptotically attained as z→1z\to1.

References

Primary source

Giacomo De Palma, “The Wehrl entropy has Gaussian optimizers”, arXiv:1703.02552 (2017).

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