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Linear Response TD-DFT

To obtain excitation energies and properties within the time-dependent Kohn-Sham framework, it is possible to propagate in time the time-dependent electron density, through the solution of Eq. (4.60), and then extract energies and oscillator strengths from a Fourier analysis of the results [98-102]. Alternatively, the excited-state properties can be determined through the linear response theory. This is an efficient approach which avoids the direct solution of the time-dependent Kohn-Sham equations and is often used in practical applications. [Pg.200]

As shown in Sec. 1.2.3, if we consider a small time-dependent external perturbation Vgxt(r, we can write the linear variation of the electron density as (in the Fourier domain)  [Pg.200]

Equations (4.66) and (4.67) can be finally written in the more compact form  [Pg.201]

Equation (4.73) has the same form as that of the random-phase approximation (or TD-HF) problem and its solutions were extensively studied in literature [103], [Pg.202]

This work was funded by the ERG Starting Grant FP7 Project DEDOM, Grant Agreement No. 207441. [Pg.203]


See other pages where Linear Response TD-DFT is mentioned: [Pg.454]    [Pg.46]    [Pg.200]   


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