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The quantum information manifold for ε-bounded forms
Let H 0 ≥ I be a self-adjoint operator and let V be a form-small perturbation such that ▪, where ϵ ϵ (0, 1 2 ) and R 0 = H −1 0. Suppose that there exists a positive β < 1 such that Z 0 ≔ Tr e −β H 0 < ∞. Let Z ≔ Tr e −( H 0+ V) . Then we show that the free energy Ψ = log Z is an analytic func...
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Published in: | Reports on mathematical physics 2000-12, Vol.46 (3), p.325-335 |
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Main Authors: | , |
Format: | Article |
Language: | English |
Citations: | Items that this one cites Items that cite this one |
Online Access: | Get full text |
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Summary: | Let
H
0 ≥
I be a self-adjoint operator and let
V be a form-small perturbation such that
▪, where ϵ ϵ (0,
1
2
) and
R
0 =
H
−1
0. Suppose that there exists a positive β < 1 such that
Z
0 ≔ Tr
e
−β
H
0
< ∞. Let
Z ≔ Tr
e
−(
H
0+
V)
. Then we show that the free energy Ψ = log Z is an analytic function of
V in the sense of Fréchet, and that the family of density operators defined in this way is an analytic manifold. |
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ISSN: | 0034-4877 1879-0674 |
DOI: | 10.1016/S0034-4877(00)90003-X |