Energy upper bound for structurally stable $N$-passive states

Passive states are special configurations of a quantum system which exhibit no energy decrement at the end of an arbitrary cyclic driving of the model Hamiltonian. When applied to an increasing number of copies of the initial density matrix, the requirement of passivity induces a hierarchical orderi...

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Main Authors: Raffaele Salvia, Vittorio Giovannetti
Format: Article
Language:English
Published: Verein zur Förderung des Open Access Publizierens in den Quantenwissenschaften 2020-05-01
Series:Quantum
Online Access:https://quantum-journal.org/papers/q-2020-05-28-274/pdf/
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spelling doaj-f761aeb7a99c49348f3ecacc5ce7a8a62020-11-25T02:50:40ZengVerein zur Förderung des Open Access Publizierens in den QuantenwissenschaftenQuantum2521-327X2020-05-01427410.22331/q-2020-05-28-27410.22331/q-2020-05-28-274Energy upper bound for structurally stable $N$-passive statesRaffaele SalviaVittorio GiovannettiPassive states are special configurations of a quantum system which exhibit no energy decrement at the end of an arbitrary cyclic driving of the model Hamiltonian. When applied to an increasing number of copies of the initial density matrix, the requirement of passivity induces a hierarchical ordering which, in the asymptotic limit of infinitely many elements, pinpoints ground states and thermal Gibbs states. In particular, for large values of $N$ the energy content of a $N$-passive state which is also structurally stable (i.e. capable to maintain its passivity status under small perturbations of the model Hamiltonian), is expected to be close to the corresponding value of the thermal Gibbs state which has the same entropy. In the present paper we provide a quantitative assessment of this fact, by producing an upper bound for the energy of an arbitrary $N$-passive, structurally stable state which only depends on the spectral properties of the Hamiltonian of the system. We also show the condition under which our inequality can be saturated. A generalization of the bound is finally presented that, for sufficiently large $N$, applies to states which are $N$-passive, but not necessarily structurally stable.https://quantum-journal.org/papers/q-2020-05-28-274/pdf/
collection DOAJ
language English
format Article
sources DOAJ
author Raffaele Salvia
Vittorio Giovannetti
spellingShingle Raffaele Salvia
Vittorio Giovannetti
Energy upper bound for structurally stable $N$-passive states
Quantum
author_facet Raffaele Salvia
Vittorio Giovannetti
author_sort Raffaele Salvia
title Energy upper bound for structurally stable $N$-passive states
title_short Energy upper bound for structurally stable $N$-passive states
title_full Energy upper bound for structurally stable $N$-passive states
title_fullStr Energy upper bound for structurally stable $N$-passive states
title_full_unstemmed Energy upper bound for structurally stable $N$-passive states
title_sort energy upper bound for structurally stable $n$-passive states
publisher Verein zur Förderung des Open Access Publizierens in den Quantenwissenschaften
series Quantum
issn 2521-327X
publishDate 2020-05-01
description Passive states are special configurations of a quantum system which exhibit no energy decrement at the end of an arbitrary cyclic driving of the model Hamiltonian. When applied to an increasing number of copies of the initial density matrix, the requirement of passivity induces a hierarchical ordering which, in the asymptotic limit of infinitely many elements, pinpoints ground states and thermal Gibbs states. In particular, for large values of $N$ the energy content of a $N$-passive state which is also structurally stable (i.e. capable to maintain its passivity status under small perturbations of the model Hamiltonian), is expected to be close to the corresponding value of the thermal Gibbs state which has the same entropy. In the present paper we provide a quantitative assessment of this fact, by producing an upper bound for the energy of an arbitrary $N$-passive, structurally stable state which only depends on the spectral properties of the Hamiltonian of the system. We also show the condition under which our inequality can be saturated. A generalization of the bound is finally presented that, for sufficiently large $N$, applies to states which are $N$-passive, but not necessarily structurally stable.
url https://quantum-journal.org/papers/q-2020-05-28-274/pdf/
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