1974
DOI: 10.1016/0009-2614(74)85112-2
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Theory of time-resolved resonance scattering

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Cited by 83 publications
(9 citation statements)
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“…A more general relationship between line shape and 'lifetime' has recently been discussed by a number of authors (Friedman and Hochstrasser 1974a;Mukamel and Jortner 1975;Nitzan, A., 1974, private communication;Berg et al 1974) where o is the angular frequency, i.e. a reduced energy variable in units of h, and where the lifetime is determined by the time dependence of Pl(t), the probability that at time t the system is in the state 1 prepared by a light source whose output characteristics are defined by the amplitude function When the amplitude functions S(t) and S(o) conform to [3], the output of the excitation source will be said to be transform limited APE -LIFETIME RELATIONSHIP 2069 (Bradley and New 19742 ;von der Linde 19723) with intensity functions I(t) = IS(t)12 and f(o) = IS(o)12 in the time and frequency domains re~pectively.~ It is easily established that it is immaterial whether total energy is obtained by integration over the entire intensity function in the time domain or in the frequency d~m a i n .~ 111.…”
Section: The Line Shape -Lifetime Relationshipmentioning
confidence: 95%
“…A more general relationship between line shape and 'lifetime' has recently been discussed by a number of authors (Friedman and Hochstrasser 1974a;Mukamel and Jortner 1975;Nitzan, A., 1974, private communication;Berg et al 1974) where o is the angular frequency, i.e. a reduced energy variable in units of h, and where the lifetime is determined by the time dependence of Pl(t), the probability that at time t the system is in the state 1 prepared by a light source whose output characteristics are defined by the amplitude function When the amplitude functions S(t) and S(o) conform to [3], the output of the excitation source will be said to be transform limited APE -LIFETIME RELATIONSHIP 2069 (Bradley and New 19742 ;von der Linde 19723) with intensity functions I(t) = IS(t)12 and f(o) = IS(o)12 in the time and frequency domains re~pectively.~ It is easily established that it is immaterial whether total energy is obtained by integration over the entire intensity function in the time domain or in the frequency d~m a i n .~ 111.…”
Section: The Line Shape -Lifetime Relationshipmentioning
confidence: 95%
“…При удалении от резонанса появляется НРС с малой длительностью ~τ имп амплитуда которого падает с увеличением отстройки, но «эффективность» (т. е. специально определенный квантовый выход) возрастает, и кинетика свечения в целом может выглядеть биэкспоненциальной. Численные расчеты [84][85][86] показывают, что при больших отстрой-ках и Δω ког амплитуда НРС достаточно велика для выделения быстрой компоненты на фоне медленной.…”
Section: 4unclassified
“…Time It is well known that there exists a time delay between the time at which a laser pulse reaches its maximum intensity and the time at which the fluorescence intensity induced by the laser pulse has maximum intensity, which is related to such properties as the lifetime r of the excited state from which the fluorescence transition originates and the cross section of the absorption transition from ground to excited state (18,19). Thus, for equal absorption cross sections, one finds that the build up of fluorescence of a short-lived excited state occurs more rapidly than that of a longer-lived fluorescence process.…”
Section: Chl a In Benzene Solutionmentioning
confidence: 99%