Stimulated by the quantum generalization of the canonical representation theory for Gaussian processes in \cite{AHH}, we first give the representations (not necessarily canonical) of two stationary Gaussian processes $X$ and $Y$ by means of white noises $q_t$ and $p_t$ with no assumptions on their commutator. We then assume that $q_t+ip_t$ annihilates the vacuum state and prove that the representations are the joint Boson Fock ones if and only if $X$ and $Y$ have a scalar commutator.

Accardi, L., Hibino, Y. (2002). Canonical representation of stationary quantum Gaussian processes. INFINITE DIMENSIONAL ANALYSIS QUANTUM PROBABILITY AND RELATED TOPICS, 5(3), 1-8 [10.1142/S0219025702000869].

Canonical representation of stationary quantum Gaussian processes

ACCARDI, LUIGI;
2002-01-01

Abstract

Stimulated by the quantum generalization of the canonical representation theory for Gaussian processes in \cite{AHH}, we first give the representations (not necessarily canonical) of two stationary Gaussian processes $X$ and $Y$ by means of white noises $q_t$ and $p_t$ with no assumptions on their commutator. We then assume that $q_t+ip_t$ annihilates the vacuum state and prove that the representations are the joint Boson Fock ones if and only if $X$ and $Y$ have a scalar commutator.
2002
Pubblicato
Rilevanza internazionale
Articolo
Esperti anonimi
Settore MAT/06 - PROBABILITA' E STATISTICA MATEMATICA
English
Accardi, L., Hibino, Y. (2002). Canonical representation of stationary quantum Gaussian processes. INFINITE DIMENSIONAL ANALYSIS QUANTUM PROBABILITY AND RELATED TOPICS, 5(3), 1-8 [10.1142/S0219025702000869].
Accardi, L; Hibino, Y
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Utilizza questo identificativo per citare o creare un link a questo documento: https://hdl.handle.net/2108/82871
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