Abstract

Given a convex function φφ and two hermitian matrices AA and BB, Lewin and Sabin study in [M. Lewin, J. Sabin, {\it A Family of Monotone Quantum Relative Entropies}, Lett. Math. Phys. \textbf{104} (2014), 691-705.] the relative entropy defined by H(A,B)=Tr[φ(A)−φ(B)−φ′(B)(A−B)]\mathcal{H}(A,B)=\text{Tr} [ φ(A) - φ(B) - φ'(B)(A-B) ]. Amongst other things, they prove that the so-defined quantity is monotone if and only if φ′φ' is operator monotone. The monotonicity is then used to properly define H(A,B)\mathcal{H}(A,B) for self-adjoint bounded operators acting on an infinite-dimensional Hilbert space by a limiting procedure. More precisely, for an increasing sequence of finite-dimensional projections {Pn}n=1∞\lbrace P_n \rbrace_{n=1}^{\infty} with Pn→1P_n \to 1 strongly, the limit lim⁡n→∞H(PnAPn,PnBPn)\lim_{n \to \infty} \mathcal{H}(P_n A P_n, P_n B P_n) is shown to exist and to be independent of the sequence of projections {Pn}n=1∞\lbrace P_n \rbrace_{n=1}^{\infty}. The question whether this sequence converges to its "obvious" limit, namely Tr[φ(A)−φ(B)−φ′(B)(A−B)]\text{Tr} [ φ(A)- φ(B) - φ'(B)(A-B) ], has been left open. We answer this question in principle affirmatively and show that lim⁡n→∞H(PnAPn,PnBPn)=Tr[φ(A)−φ(B)−ddαφ(αA+(1−α)B)∣α=0]\lim_{n \to \infty} \mathcal{H}(P_n A P_n, P_n B P_n) = \text{Tr}[ φ(A) - φ(B) - \frac{\text{d}}{\text{d} α} φ( αA + (1-α)B )|_{α= 0} ]. If the operators AA and BB are regular enough, that is (A−B)(A-B), φ(A)−φ(B)φ(A)-φ(B) and φ′(B)(A−B)φ'(B)(A-B) are trace-class, the identity Tr[φ(A)−φ(B)−ddαφ(αA+(1−α)B)∣α=0]=Tr[φ(A)−φ(B)−φ′(B)(A−B)]\text{Tr}[ φ(A) - φ(B) - \frac{\text{d}}{\text{d} α} φ( αA + (1-α)B )|_{α= 0} ] = \text{Tr} [ φ(A)- φ(B) - φ'(B)(A-B) ] holds.

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