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| Both sides previous revision Previous revision Next revision | Previous revision | ||
| kohn-sham_random-phase_approximation [2025/07/30 22:05] – [RPAX2 program] hesselmann | kohn-sham_random-phase_approximation [2025/07/30 22:26] (current) – [Kohn-Sham random-phase approximation] hesselmann | ||
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| ====== Kohn-Sham random-phase approximation ====== | ====== Kohn-Sham random-phase approximation ====== | ||
| + | This chapter describes three different programs that are related to Kohn-Sham based RPA correlation methods. The first one is the density fitting RPA program of Heßelmann et al. described in section [[Kohn-Sham random-phase approximation# | ||
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| + | All of the different codes are capable to perform standard RPA correlation energy calculations, | ||
| ===== Density fitting RPA programs ===== | ===== Density fitting RPA programs ===== | ||
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| Spin-unrestricted calculations can be done using the **URPAX2** program. In this case the orbitals from a preceeding unrestricted Kohn-Sham calculation have to be passed to the program (via the '' | Spin-unrestricted calculations can be done using the **URPAX2** program. In this case the orbitals from a preceeding unrestricted Kohn-Sham calculation have to be passed to the program (via the '' | ||
| - | ===== ACFDT program | + | ==== ACFDT program ==== |
| The ACFDT (adiabatic connection fluctuation-dissipation theorem) method is an alternative approach to derive the RPA. If used in conjunction with local adiabatic exchange-correlation kernels, the method can also describe electron-electron interaction contributions beyond the RPA. Currently, the ALDA xc-kernel can be used in the program (ACFDT(ALDA) method), see also Ref. [4]. The **ACFDT** program has the following options: | The ACFDT (adiabatic connection fluctuation-dissipation theorem) method is an alternative approach to derive the RPA. If used in conjunction with local adiabatic exchange-correlation kernels, the method can also describe electron-electron interaction contributions beyond the RPA. Currently, the ALDA xc-kernel can be used in the program (ACFDT(ALDA) method), see also Ref. [4]. The **ACFDT** program has the following options: | ||
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| - | ===== RIRPA program | + | ===== Self consistent RPA programs ===== |
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| + | ==== RIRPA program ==== | ||
| The RIRPA and URIRPA programs allow non-self-consistent spin-restricted and spin-unrestricted resolution of identity (RI) random phase approximation (RPA) [1-3] and σ-functional [4-6] calculations. These methods should be used in conjunction with conventional Kohn-Sham (KS) density functional theory (DFT) calculations, | The RIRPA and URIRPA programs allow non-self-consistent spin-restricted and spin-unrestricted resolution of identity (RI) random phase approximation (RPA) [1-3] and σ-functional [4-6] calculations. These methods should be used in conjunction with conventional Kohn-Sham (KS) density functional theory (DFT) calculations, | ||
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| * **verb** determines the level of verbosity in the output file, integer values of 0, 1, 3 provide different levels of verbosity (default ’0’) | * **verb** determines the level of verbosity in the output file, integer values of 0, 1, 3 provide different levels of verbosity (default ’0’) | ||
| - | ===== SCEXX program | + | ==== SCEXX program ==== |
| The '' | The '' | ||
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| {{: | {{: | ||
| - | ===== SCRPA program | + | ==== SCRPA program ==== |
| The '' | The '' | ||