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1 Correction to: J Stat Phys (2014) 154:807–818 https://doi.org/10.1007/s10955-013-0890-x
The original version of this article unfortunately contained an error and it has been corrected with this erratum. We consider in [5, p. 810 and Theorem 2.2] the following results which we here put together.
Theorem 1
The functions
are operator monotone (thus operator concave) for \( 0< p\le 1 \) and operator convex for \( 1\le p\le 2. \)
The first part \( (0< p\le 1) \) is proved on page 810. Note that the statement is different from Ando [1, Corollary 4.3]. The second part \( (1\le p\le 2) \) is our [5, Theorem 2.2]. The perspective of an operator concave (convex) function is again an operator concave (convex) function of two variables, cf. [3, Theorem 1.1]. By applying [4, Theorem 1.1] these results entail that for arbitrary K the trace functions
are concave for \( 0< p\le 1 \) and convex for \( 1\le p\le 2. \) We then try to use these results to recover Carlen-Lieb’s theorems in [2].
Theorem 2
(Carlen-Lieb) The trace functions
are concave for \( 0<p\le 1 \) and convex for \( 1\le p\le 2. \)
We do this by claiming the identity
where the left hand side is obtained by setting \( K=I \) (the identity operator) in (1). By replacing A with \( A^{1/p} \) and B with \( B^{1/p} \) this would then entail that
for positive definite matrices. This however is wrong. Victoria Chayes informed me in a private communication that for \( p=1/4 \) the difference
and the difference therefore vanishes if and only if A and B commute.
The failed identity in (3) is of no consequence here since we already know that Carlen-Lieb’s theorem is true.
Later in the paper [5, Theorem 3.1] we prove that the functions of two variables
are operator concave for \( 0<p\le 1, \) and this implies that the trace functions
are concave for arbitrary K. We then put \( K=I \) and try to use an identity similar to (3) to obtain [5, Theorem 3.2] which claims that the trace functions
are concave in positive definite matrices. This claim is no longer verified. In fact, numerical calculations indicate that the trace functions in (4) are concave only for \( p=1/2 \) and not concave for \( 0<p<1/2 \) and \( 1/2<p<1. \)
References
Ando, T.: Concavity of certain maps of positive definite matrices and applications to Hadamard products. Linear Algebra Appl. 26, 203–241 (1979)
Carlen, E.A., Lieb, E.H.: A Minkowsky type trace inequality and strong subadditivity of quantum entropy II: convexity and concavity. Lett. Math. Phys. 83, 107–126 (2008)
Effros, E., Hansen, F.: Non-commutative perspectives. Ann. Funct. Anal. 2, 74–79 (2014)
Hansen, F.: Extensions of Lieb’s concavity theorem. J. Stat. Phys. 124, 87–101 (2006)
Hansen, F.: Trace functions with applications in quantum physics. J. Stat. Phys. 154, 807–818 (2014)
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Hansen, F. Correction to: Trace Functions with Applications in Quantum Physics. J Stat Phys 188, 14 (2022). https://doi.org/10.1007/s10955-022-02929-z
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DOI: https://doi.org/10.1007/s10955-022-02929-z