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Vosko, Wilk, Nusair

We have used the multisublattice generalization of the coherent potential approximation (CPA) in conjunction with the Linear-MufRn-Tin-Orbital (LMTO) method in the atomic sphere approximation (ASA). The LMTO-ASA is based on the work of Andersen and co-workers and the combined technique allows us to treat all phases on equal footing. To treat itinerant magnetism we have employed for the local spin density approximation (LSDA) the Vosko-Wilk-Nusair parameterization". [Pg.14]

SVWN Model. (Slater, Vosko, Wilk, Nusair) A Density Functional Model which involves the Local Density Approximation. [Pg.769]

VWN5 A Vosko, Wilk, Nusair correlation functional... [Pg.556]

The LDA exchange-correlation potential used in this study was not the common Vosko, Wilk, Nusair parameterization of the Ceperley-Adler data for the uniform electron gas but the potential of Heidin and Lundqvist.68... [Pg.167]

Figure 2-6. Comparison of calculated and experimental vertical excitation energies of Be and H20. TDDFT is based on the Slater-Vosko-Wilk-Nusair functional. See Ref. [110] for details... Figure 2-6. Comparison of calculated and experimental vertical excitation energies of Be and H20. TDDFT is based on the Slater-Vosko-Wilk-Nusair functional. See Ref. [110] for details...
The extension of TDDFT and Tamm-Dancoff TDDFT to crystalline polymers is straightforward within the formalisms of Section 2.2.2. Figure 2-7 summarizes the results of TDDFT calculations of the photoconduction, photoemission, and optical absorption thresholds (energy gap, ionization energy, and excitation energy) of polyethylene as a function of basis set [50], The Slater-Vosko-Wilk-Nusair functional [116, 117] is used, but the following conclusion is unaltered... [Pg.49]

Figure 2-7. TDDFT (the Slater-Vosko-Wilk-Nusair functional) predictions of the photoconduction (fundamental gap), photoemission (ionization), and optical absorption (excitation) energies of polyethylene [50]... Figure 2-7. TDDFT (the Slater-Vosko-Wilk-Nusair functional) predictions of the photoconduction (fundamental gap), photoemission (ionization), and optical absorption (excitation) energies of polyethylene [50]...
Figure 2-8. Convergence of the excitation energy to the lowest-lying singlet exciton computed by CIS and TDDFT using the Slater-Vosko-Wilk-Nusair functional with the STO-3G basis set as a function of the number of wave vector sampling points (K) [50]. The error is defined as the absolute difference from the K = 100 results. The converged (K = 100) result with TDDFT is very close to the fundamental energy gap... Figure 2-8. Convergence of the excitation energy to the lowest-lying singlet exciton computed by CIS and TDDFT using the Slater-Vosko-Wilk-Nusair functional with the STO-3G basis set as a function of the number of wave vector sampling points (K) [50]. The error is defined as the absolute difference from the K = 100 results. The converged (K = 100) result with TDDFT is very close to the fundamental energy gap...
VWN(Vosko, Wilk, Nusair)(12) p / +correl. PZ(Perdew, Zunger) (1J) electron gas exchange and correlation from accurate Quantum Monte Carlo calcs, of Ceperley and Alder (14)... [Pg.10]

Hedin- Lundqvist, HL, exchange-correlation potential [37], which is equivalent to our earlier use [130] of the von Barth-Hedin potential, vBH, [38] with parameter values as used by Hedin and Lundqvist. Calculations were also performed using the Xa form, with a = 0.7 [4] and the Vosko-Wilk-Nusair form of Vxc [41]. A somewhat lower total energy was obtained by inclusion of the 3d, and in particular the 3p and 3d, basis functions, compared with the results obtained using the minimal basis set. [Pg.33]

To confirm the minimum point of the total energy profile with respect to the U=0 distance, other exchange - correlation potentials were also examined a local density functional by Vosko-Wilk-Nusair (VWN) (14) and a nonlocal... [Pg.329]

The one-electron Kohn-Sham equations were solved using the Vosko-Wilk-Nusair (VWN) functional [27] to obtain the local potential. Gradient correlations for the exchange (Becke fimctional) [28] and correlation (Perdew functional) [29] energy terms were included self-consistently. ADF represents molecular orbitals as linear combinations of Slater-type atomic orbitals. The double- basis set was employed and all calculations were spin unrestricted. Integration accuracies of 10 -10 and 10 were used during the single-point and vibrational frequency calculations, respectively. The cluster size chosen for Ag or any bimetallic was... [Pg.267]

Here j SDA timkind of accurate pure DFT LSDA non-gradient-corrected exchange functional alluded to in section 7.2.3.4b, is the KS-orbital-based HF exchange energy functional of Eq. (7.30), is the Becke 88 exchange functional mentioned above, is the Vosko, Wilk, Nusair function (VWN, or Slater VWN, SVWN... [Pg.399]

GGA functionals. Slater (S) exchange [68] and Vosko-Wilk-Nusair (VWN) correlation [74] LDA functionals, and the HF exchange integral with three parameters ... [Pg.530]

VOSKO-WILK-NUSAIR EXCHANGE CORRELATION CAN. J. PHYS. 58,1200(1980)... [Pg.233]


See other pages where Vosko, Wilk, Nusair is mentioned: [Pg.125]    [Pg.472]    [Pg.556]    [Pg.462]    [Pg.19]    [Pg.211]    [Pg.147]    [Pg.345]    [Pg.4]    [Pg.36]    [Pg.212]    [Pg.358]    [Pg.52]    [Pg.351]    [Pg.221]    [Pg.798]    [Pg.442]    [Pg.225]    [Pg.232]    [Pg.253]    [Pg.212]    [Pg.17]    [Pg.714]    [Pg.96]    [Pg.125]   
See also in sourсe #XX -- [ Pg.582 , Pg.586 ]

See also in sourсe #XX -- [ Pg.560 , Pg.565 ]




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