Time operator for a quantum many-body system with SU(1,1) dynamical symmetry

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dc.creatorAndric, I.
dc.creatorMartinis, M.
dc.date2003-02-14
dc.date.accessioned2026-07-07T06:06:09Z
dc.date.available2026-07-07T06:06:09Z
dc.descriptionThe time operator canonically conjugated to the Hamiltonian of $N$ interacting particles on the line is constructed using SU(1,1) as a dynamical symmetry. This hidden conformal symmetry enables us to make a group theoretic analysis of the time operator in terms of SU(1,1) generators. At distances very far from the interacting region the time operator is represented as a generalization of the quantum "time-of-arrival" operator.
dc.description6 pages, LaTeX
dc.identifierhttps://arxiv.org/abs/quant-ph/0302116
dc.identifierhttp://arxiv.org/abs/quant-ph/0302116
dc.identifier.urihttp://salesiana.dossiersoluciones.com/handle/123456789/90878
dc.subjectQuantum Physics
dc.titleTime operator for a quantum many-body system with SU(1,1) dynamical symmetry
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