New analysis of experimental data for the second hexad {(050), (130), (210), (012), (031), (111)} of H2/16O molecule interacting states

    Результат исследований: Материалы для журналаСтатья

    8 Цитирования (Scopus)

    Выдержка

    A new theoretical model of an effective Hamiltonian for non-rigid H2X-type molecules, based on the generating function approach, is applied to the experimental energy levels of the second hexad of interacting states of H2O. The experimental energy levels for J ≤ 11 and J ≤ 15 of the 5 vibrational states {(130), (210), (111), (012), (031)} are fitted with an average discrepancy r.m.s. = 12.0 x 10-3 cm-1 and r.m.s. = 14.4 x 10-3 cm-1, respectively. The influence of interactions of the mentioned pentad with (050) and (060) vibration states is discussed.

    Язык оригиналаАнглийский
    Страницы (с-по)39-51
    Число страниц13
    ЖурналJournal of Molecular Structure
    Том449
    Номер выпуска1
    DOI
    СостояниеОпубликовано - 4 авг 1998

    Отпечаток

    Vibration
    Electron energy levels
    Theoretical Models
    energy levels
    Hamiltonians
    Molecules
    vibrational states
    molecules
    vibration
    interactions

    ASJC Scopus subject areas

    • Structural Biology
    • Organic Chemistry
    • Physical and Theoretical Chemistry
    • Spectroscopy
    • Atomic and Molecular Physics, and Optics

    Цитировать

    New analysis of experimental data for the second hexad {(050), (130), (210), (012), (031), (111)} of H2/16O molecule interacting states. / Starikov, V. I.; Mikhaïlenko, Semen Nikolaevich.

    В: Journal of Molecular Structure, Том 449, № 1, 04.08.1998, стр. 39-51.

    Результат исследований: Материалы для журналаСтатья

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    abstract = "A new theoretical model of an effective Hamiltonian for non-rigid H2X-type molecules, based on the generating function approach, is applied to the experimental energy levels of the second hexad of interacting states of H2O. The experimental energy levels for J ≤ 11 and J ≤ 15 of the 5 vibrational states {(130), (210), (111), (012), (031)} are fitted with an average discrepancy r.m.s. = 12.0 x 10-3 cm-1 and r.m.s. = 14.4 x 10-3 cm-1, respectively. The influence of interactions of the mentioned pentad with (050) and (060) vibration states is discussed.",
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