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  • 1985-1989  (5)
  • 1
    Online Resource
    Online Resource
    American Chemical Society (ACS) ; 1985
    In:  The Journal of Physical Chemistry Vol. 89, No. 2 ( 1985-01), p. 214-222
    In: The Journal of Physical Chemistry, American Chemical Society (ACS), Vol. 89, No. 2 ( 1985-01), p. 214-222
    Type of Medium: Online Resource
    ISSN: 0022-3654 , 1541-5740
    RVK:
    Language: English
    Publisher: American Chemical Society (ACS)
    Publication Date: 1985
    detail.hit.zdb_id: 2006064-6
    detail.hit.zdb_id: 3003-X
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  • 2
    Online Resource
    Online Resource
    AIP Publishing ; 1987
    In:  The Journal of Chemical Physics Vol. 86, No. 12 ( 1987-06-15), p. 7025-7034
    In: The Journal of Chemical Physics, AIP Publishing, Vol. 86, No. 12 ( 1987-06-15), p. 7025-7034
    Abstract: An approximate solution to the problem of constructing a pair of diabatic states exists only if certain requirements are fulfilled, for example, when the nonadiabatic coupling results from an interaction between two electronic configurations which are doubly excited with respect to one another. It is then possible to build up a model in which the series expansion of the elements of the Hamiltonian matrix is truncated after the first nonzero term. This leads to several conclusions concerning the nonadiabatic transition probability which differentiate conical intersections from avoided crossings. For the latter, the nonadiabatic coupling matrix elements (which are Lorentzians with an area equal to π/2) reach their maximum at the nuclear geometry for which ΔE (the energy gap between adiabatic surfaces) is a minimum. The loci along which the angle θ of the orthogonal transformation which relates adiabatic and diabatic wave functions keeps a constant value are a set of parallel straight lines which coincides with the loci along which ΔE remains constant. This reference direction in the configuration space corresponds to nuclear trajectories which are unable to bring about a nonadiabatic transition. In the case of avoided crossings, there exists only one nuclear degree of freedom which gives rise to surface hopping. Conical intersections, on the other hand, have two such active degrees of freedom. This creates a qualitative difference between the two cases which makes conical intersections more efficient as funnels than avoided crossings. A two-dimensional extension of the Landau–Zener formula is derived for avoided crossings. It contains a factor of anisotropy. It is possible, at least in favorable cases, to extract approximate diabatic quantities from ab initio calculations and to compare them with the predictions of these models. This has been done for two 2A1 electronic states of the CH+2 ion. The results are found to agree with the predictions of the model, at least in a restricted range of internuclear distances.
    Type of Medium: Online Resource
    ISSN: 0021-9606 , 1089-7690
    Language: English
    Publisher: AIP Publishing
    Publication Date: 1987
    detail.hit.zdb_id: 3113-6
    detail.hit.zdb_id: 1473050-9
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  • 3
    In: Molecular Physics, Informa UK Limited, Vol. 61, No. 4 ( 1987-07), p. 981-997
    Type of Medium: Online Resource
    ISSN: 0026-8976 , 1362-3028
    Language: English
    Publisher: Informa UK Limited
    Publication Date: 1987
    detail.hit.zdb_id: 1491083-4
    SSG: 12
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  • 4
    Online Resource
    Online Resource
    AIP Publishing ; 1987
    In:  The Journal of Chemical Physics Vol. 86, No. 3 ( 1987-02-01), p. 1429-1436
    In: The Journal of Chemical Physics, AIP Publishing, Vol. 86, No. 3 ( 1987-02-01), p. 1429-1436
    Abstract: We consider here two approaches which have been proposed in the literature to obtain diabatic states from ab initio calculations. First, by calculating explicitly the coupling vector g=〈ψ2‖∇ψ1〉 which describes the nonadiabatic interaction between two adiabatic states ψ1 and ψ2. Second, by some extrapolation process of the wave functions obtained at a particular reference point. The coupling vector g is the sum of three contributions: g=gCI+gLCAO+gAO. The first two represent the change in character of the adiabatic states in the region of nonadiabatic coupling due to the variation of the CI and LCAO coefficients, whereas gAO results from the translation of the atomic orbitals with the moving nuclear centers. Criteria have been given to recognize when it is possible to transform a set of CI wave functions into a pair of useful diabatic states. A particularly favorable situation is obtained when the interacting electronic states are doubly excited with respect to each other. Within the two-state approximation, gCI is strictly irrotational and never gives rise to problems. One can expect situations in which this is also true for gLCAO. However, that part of the coupling represented by gAO can never be described as a rotation of two diabatic functions. Nevertheless, the latter contribution can frequently be neglected, at least when the nonadiabatic coupling is strong. The theory of the electron translation factors (ETF’s) provides further insight into the problem and confirms our conclusions.
    Type of Medium: Online Resource
    ISSN: 0021-9606 , 1089-7690
    Language: English
    Publisher: AIP Publishing
    Publication Date: 1987
    detail.hit.zdb_id: 3113-6
    detail.hit.zdb_id: 1473050-9
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  • 5
    Online Resource
    Online Resource
    AIP Publishing ; 1989
    In:  The Journal of Chemical Physics Vol. 91, No. 7 ( 1989-10-01), p. 4155-4168
    In: The Journal of Chemical Physics, AIP Publishing, Vol. 91, No. 7 ( 1989-10-01), p. 4155-4168
    Abstract: The formalism of the resonance states is used to derive approximate expressions of the unimolecular law of decay resulting from a specific excitation. These expressions contain no cross terms and wash out the quantum interferences. We propose a method to relate them to an experimentally observable quantity, viz., the autocorrelation function C(t) obtained as the Fourier transform of a spectral profile, which is available even when the spectrum is poorly resolved. For a specific excitation, the exact initial rate of decay (valid up to the dephasing time T1) is equal to the initial slope of ‖C(t)‖2. The subsequent time evolution can be obtained by averaging ‖C(t)‖2 over its oscillations. This generates a function ‖C(t)‖2av whose area (from time T1 onwards) is directly related to an average decay lifetime. At times t & gt;T1, a good approximation to the average decay curve Pav(t) can be derived by multiplying ‖C(t)‖2av by an appropriate constant. The method is exemplified on various diatomic and triatomic models. As an application to a real system, we study the B̃ 2B2 state of H2O+ which is coupled to the Ã 2A1 state via a conical intersection. State B̃ is found to undergo an ultrafast intramolecular relaxation with a lifetime of (1.6±0.2) 10−14 s.
    Type of Medium: Online Resource
    ISSN: 0021-9606 , 1089-7690
    Language: English
    Publisher: AIP Publishing
    Publication Date: 1989
    detail.hit.zdb_id: 3113-6
    detail.hit.zdb_id: 1473050-9
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