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Body-fixed wavepackets

For an atom-diatom collision the initial wavepacket, in body-fixed coordinates, is defined as [47,133]... [Pg.275]

The first part of the review deals with aspects of photodissociation theory and the second, with reactive scattering theory. Three appendix sections are devoted to important technical details of photodissociation theory, namely, the detailed form of the parity-adapted body-fixed scattering wavefunction needed to analyze the asymptotic wavefunction in photodissociation theory, the definition of the initial wavepacket in photodissociation theory and its relationship to the initial bound-state wavepacket, and finally the theory of differential state-specific photo-fragmentation cross sections. Many of the details developed in these appendix sections are also relevant to the theory of reactive scattering. [Pg.283]

The wavepacket dynamics were carried out using the Lanczos method with real wavepackets [121] employing Jacobi coordinates to describe the relative positions of the three nuclei in the body fixed plane. As mentioned the novel results... [Pg.122]

For a complete treatment of a laser-driven molecule, one must solve the many-body, multidimensional time-dependent Schrodinger equation (TDSE). This represents a tremendous task and direct wavepacket simulations of nuclear and electronic motions under an intense laser pulse is presently restricted to a few bodies (at most three or four) and/or to a model of low dimensionality [27]. For a more general treatment, an approximate separation of variables between electrons (fast subsystem) and nuclei (slow subsystem) is customarily made, in the spirit of the BO approximation. To lay out the ideas underlying this approximation as adapted to field-driven molecular dynamics, we will consider from now on a molecule consisting of Nn nuclei (labeled a, p,...) and Ne electrons (labeled /, j,...), with position vectors Ro, and r respectively, defined in the center of mass (rotating) body-fixed coordinate system, in a classical field E(f) of the form Eof t) cos cot). The full semiclassical length gauge Hamiltonian is written, for a system of electrons and nuclei, as [4]... [Pg.55]

On the left hand side is the space-fixed wavefunction. The Euler angles are the three angles required to rotate the space-fixed axes to the body-fixed axes. The wavepacket r, 7, t) is defined in the body-fixed axis system. [Pg.4]


See other pages where Body-fixed wavepackets is mentioned: [Pg.260]    [Pg.269]    [Pg.156]    [Pg.156]    [Pg.163]    [Pg.260]    [Pg.269]    [Pg.156]    [Pg.156]    [Pg.163]    [Pg.251]    [Pg.259]    [Pg.269]    [Pg.273]    [Pg.275]    [Pg.155]    [Pg.164]    [Pg.371]    [Pg.155]    [Pg.167]    [Pg.371]    [Pg.114]   


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