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Multiconfigurational time-dependent Hartree MCTDH approach

The three-pulse EOM-PMA can be formulated not only in terms of density matrices and master equations but also in terms of wavefunctions and Schrodinger equations [29]. The EOM-PMA can therefore be straightforwardly incorporated into computer programs which provide the time evolution of the density matrix or the wavefunction of material systems. Besides the multilevel Redlield theory, the EOM-PMA can be combined with the Lindblad master equation [49], the surrogate Hamiltonian approach [49], the stochastic Liouville equation [18], the quantum Fokker-Planck equation [18], and the density matrix [50] or the wavefunction [14] multiconfigurational time-dependent Hartree (MCTDH) methods. When using the... [Pg.470]


See other pages where Multiconfigurational time-dependent Hartree MCTDH approach is mentioned: [Pg.200]    [Pg.200]    [Pg.34]    [Pg.185]    [Pg.241]    [Pg.48]    [Pg.483]    [Pg.47]    [Pg.333]    [Pg.1192]    [Pg.103]   


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Multiconfiguration

Multiconfiguration time-dependent

Multiconfiguration time-dependent Hartree

Multiconfigurational approaches

Multiconfigurational time-dependent Hartree

Multiconfigurational time-dependent Hartree MCTDH)

Time-dependent Hartree

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