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Three-Hilbert-Space Formulation of Quantum Mechanics

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    SYSNO ASEP0329440
    Document TypeJ - Journal Article
    R&D Document TypeJournal Article
    Subsidiary JČlánek ve WOS
    TitleThree-Hilbert-Space Formulation of Quantum Mechanics
    Author(s) Znojil, Miloslav (UJF-V) RID, ORCID, SAI
    Source TitleSymmetry, Integrability and Geometry: Methods and Applications. - : Natsional'na Akademiya Nauk Ukrainy - ISSN 1815-0659
    Roč. 5, - (2009), 001/1-001/19
    Number of pages19 s.
    Action7th Workshop on Quantum Physics with Non-Hermitian Operators
    Event date29.06.2007-11.07.2007
    VEvent locationBenasque
    CountryES - Spain
    Event typeWRD
    Languageeng - English
    CountryUA - Ukraine
    Keywordsformulation of Quantum Mechanics ; cryptohermitian operators of observables ; triplet of the representations of the Hilbert space of states
    Subject RIVBE - Theoretical Physics
    R&D ProjectsGA202/07/1307 GA ČR - Czech Science Foundation (CSF)
    LC06002 GA MŠMT - Ministry of Education, Youth and Sports (MEYS)
    CEZAV0Z10480505 - UJF-V (2005-2011)
    UT WOS000267267900001
    DOI10.3842/SIGMA.2009.001
    AnnotationIn paper [Znojil M., Phys. Rev. D 78 (2008), 085003, 5 pages, arXiv: 0809.2874] the two-Hilbert-space (2HS, a.k.a. cryptohermitian) formulation of Quantum Mechanics has been revisited. In the present continuation of this study (with the spaces in question denoted as H-(auxiliary) and H-(standard)) we spot a weak point of the 2HS formalism which lies in the double role played by H-(auxiliary). As long as this confluence of roles may (and did!) lead to confusion in the literature, we propose an amended, three-Hilbert-space (3HS) reformulation of the same theory. As a byproduct of our analysis of the formalism we offer an amendment of the Dirac's bra-ket notation and we also show how its use clarifies the concept of covariance in time-dependent cases. Via an elementary example we finally explain why in certain quantum systems the generator H-(gen) of the time-evolution of the wave functions may differ from their Hamiltonian H.
    WorkplaceNuclear Physics Institute
    ContactMarkéta Sommerová, sommerova@ujf.cas.cz, Tel.: 266 173 228
    Year of Publishing2010
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