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Entropy exchange

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In quantum mechanics, and especially quantum information processing, the entropy exchange of a quantum operation ϕ {\displaystyle \phi \,} acting on the density matrix ρ Q {\displaystyle \rho _{Q}\,} of a system Q {\displaystyle Q\,} is defined as

S ( ρ , ϕ ) S [ Q , R ] = S ( ρ Q R ) {\displaystyle S(\rho ,\phi )\equiv S=S(\rho _{QR}')}

where S ( ρ Q R ) {\displaystyle S(\rho _{QR}')\,} is the von Neumann entropy of the system Q {\displaystyle Q\,} and a fictitious purifying auxiliary system R {\displaystyle R\,} after they are operated on by ϕ {\displaystyle \phi \,} . Here,

ρ Q R = | Q R Q R | , {\displaystyle \rho _{QR}=|QR\rangle \langle QR|\quad ,}
T r R [ ρ Q R ] = ρ Q , {\displaystyle \mathrm {Tr} _{R}=\rho _{Q}\quad ,}

and

ρ Q R = ( ϕ Q 1 R ) [ ρ Q R ] , {\displaystyle \rho _{QR}'=(\phi _{Q}\otimes 1_{R})\quad ,}

where in the above equation ( ϕ Q 1 R ) {\displaystyle (\phi _{Q}\otimes 1_{R})} acts on Q {\displaystyle Q} leaving R {\displaystyle R} unchanged.

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