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arXiv:quant-ph/0510148

On Weyl-covariant channels

Motohisa Fukuda, Alexander Semenovich Holevo

Published Oct 19, 2005• 25 citations
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Abstract

Formalism of discrete noncommutative Fourier transform is developed and applied to the study of Weyl-covariant channels. We then extend a result in quant-ph/0509126 concerning a bound of the maximal output 2-norm of a Weyl-covariant channel. A class of channels which attain the bound is introduced, for which the multiplicativity of the maximal output 2-norm is proven. Complementary channels are described which share the multiplicativity properties with the Weyl-covariant channels.

DOI
10.48550/arxiv.quant-ph/0510148

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Formalism of discrete noncommutative Fourier transform is developed and applied to the study of Weyl-covariant channels. We then extend a result in quant-ph/0509126 concerning a bound of the maximal output 2-norm of a Weyl-covariant channel. A class of channels which attain the bound is introduced, for which the multiplicativity of the maximal output 2-norm is proven. Complementary channels are described which share the multiplicativity properties with the Weyl-covariant channels.
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.
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 explore complementarity between output and environment of a quantum channel (or, more generally, CP map), making an observation that the output purity characteristics for complementary CP maps coincide. Hence, validity of the mutiplicativity/additivity conjecture for a class of CP maps implies its validity for complementary maps. The class of CP maps complementary to entanglement-breaking ones is described and is shown to contain diagonal CP maps as a proper subclass, resulting in new class of CP maps (channels) for which the multiplicativity/additivity holds. Covariant and Gaussian channels are discussed briefly in this context.