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arXiv:quant-ph/0606040

On the additivity conjecture for the Weyl channels being covariant with respect to the maximum commutative group of unitaries

Grigori Gennadievich Amosov

Published Jun 6, 2006• 0 citations
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Abstract

Some new examples of quantum channels for which the infimum of the output entropy is additive under taking a tensor product of channels are given.
DOI
10.48550/arxiv.quant-ph/0606040

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We investigate the Weyl channels being covariant with respect to the maximum commutative group of unitary operators. This class includes the quantum depolarizing channel and the “two-Pauli” channel as well. Then, we show that our estimation of the output entropy for a tensor product of the phase damping channel and the identity channel based upon the decreasing property of the relative entropy allows to prove the additivity conjecture for the minimal output entropy for the quantum depolarizing channel in any prime dimension and for the two-Pauli channel in the qubit case.
We estimate the von Neumann entropy infimum for the output of the Weyl channels being covariant with respect to the maximum commutative group. In qubit case, such the class includes the quantum depolarizing channel and the "two-Pauli" channel as well. For the dimesion d=2d=2d=2 our approach allows to prove the additivity conjecture for the Holevo-Schumacher-Westmoreland bound. Our method is based upon using the decreasing property of the relative entropy. Earlier we had shown that the method gives the proof of the additivity conjecture for the quantum depolarizing channel in any dimension.
Following the method introduced in quant-ph/0408004 and quant-ph/0605177 we prove that the additivity conjecture for the Holevo-Schumacher-Westmoreland bound of the output of a quantum channel holds for the channels of the form Phi(x)=sumlimitsm=02(rmWm,0xWm,0∗+p1Wm,1xWm,1∗+p2Wm,2xWm,2∗)\\Phi (x)=\\sum \\limits _{m=0}^{2}(r_{m}W_{m,0}xW_{m,0}^{*}+p_{1}W_{m,1}xW_{m,1}^{*}+p_{2}W_{m,2}x W_{m,2}^{*})Phi(x)=sumlimitsm=02​(rm​Wm,0​xWm,0∗​+p1​Wm,1​xWm,1∗​+p2​Wm,2​xWm,2∗​). Here xxx runs the set of states sigma(H)\\sigma (H)sigma(H) in the Hilbert space H,dimH=3,H, dimH=3,H,dimH=3, Wm,nW_{m,n}Wm,n​ are the Weyl operators satisfying the relation Wm,nWm′,n′=efrac2pii(m′n−mn′)3Wm+m′,n+n′,0lem,nle2,W_{m,n}W_{m',n'}=e^{\\frac {2\\pi i(m'n-mn')}{3}}W_{m+m',n+n'}, 0\\le m,n\\le 2,Wm,n​Wm′,n′​=efrac2pii(m′n−mn′)3Wm+m′,n+n′​,0lem,nle2, and 0lerm,p1,p2le1,sumlimitsm=02rm+3(p1+p2)=10\\le r_{m},p_{1},p_{2}\\le 1, \\sum \\limits _{m=0}^{2}r_{m}+3(p_{1}+p_{2})=10lerm​,p1​,p2​le1,sumlimitsm=02​rm​+3(p1​+p2​)=1. This class includes the quantum depolarizing channel as well as a number of the other channels being covariant with respect to the maximum commutative group of unitaries.