2007
DOI: 10.1007/s00440-007-0073-2
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Hypercontractivity for a quantum Ornstein–Uhlenbeck semigroup

Abstract: We prove hypercontractivity for a quantum Ornstein-Uhlenbeck semigroup on the entire algebra B(h) of bounded operators on a separable Hilbert space h. We exploit the particular structure of the spectrum together with hypercontractivity of the corresponding birth and death process and a proper decomposition of the domain. Then we deduce a logarithmic Sobolev inequality for the semigroup and gain an elementary estimate of the best constant.

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Cited by 22 publications
(31 citation statements)
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“…For any 1 < q < p and any 0 < λ < 1 the p → q norm of E λ is infinite and is asymptotically achieved by thermal Gaussian states with infinite temperature: 6) and the claim follows. One-mode quatum Gaussian channels have Gaussian maximizers 21…”
Section: )mentioning
confidence: 85%
See 1 more Smart Citation
“…For any 1 < q < p and any 0 < λ < 1 the p → q norm of E λ is infinite and is asymptotically achieved by thermal Gaussian states with infinite temperature: 6) and the claim follows. One-mode quatum Gaussian channels have Gaussian maximizers 21…”
Section: )mentioning
confidence: 85%
“…Proof. IfX has rank 1, we have from Lemma 3.8 6) and the claim follows since S a X = 0. IfX has rank at least 2, then S a X > 0 and the claim follows from Theorem 3.1 with 0 < z < 1 chosen such that S a (ω z ) = S a X .…”
Section: )mentioning
confidence: 88%
“…We remark that it would significantly strengthen known results about the qOU semigroup. Specifically, Carbone et al [26] established that the qOU semigroup is hypercontractive. In [26,Proposition 4.2], the following inequality was shown for the Log-Sobolev-2 constant 1 α 2 of L µ,λ :…”
Section: Application To the Ornstein-uhlenbeck Semigroupmentioning
confidence: 99%
“…for any integrable, continuously differentiable function f , which has an integrable partial derivative ∂ x j f , where z j denotes the j th component of the vector z ∈ Z. Secondly, for any square integrable function h on R 2n , we have that 5) which is the classical Plancherel identity. We also employ the well-known polarization identity:…”
Section: Proofs Of Theorem and Theoremmentioning
confidence: 99%