Time-dependent density-functional theory calculations: Difference between revisions
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# ground-state calculation | # ground-state calculation | ||
# optical absorption calculation | # optical absorption calculation | ||
For example, an optical absorption calculation of bulk Si can be performed using a dielectric-dependent hybrid-functional described in Ref. {{cite|chen2018nonempirical}} | For example, an optical absorption calculation of bulk Si can be performed using a dielectric-dependent hybrid-functional described in Ref. {{cite|chen2018nonempirical}}{{cite|cui2018doubly}}{{cite|liu2019assessing}}. | ||
{{TAG|SYSTEM}} = Si | {{TAG|SYSTEM}} = Si | ||
Revision as of 17:42, 7 February 2024
VASP offers a powerful module for performing time-dependent density-functional theory (TDDFT) or time-dependent Hartree-Fock (TDHF) calculations by solving the Casida equation . This approach can be used for obtaining the frequency-dependent dielectric function with the excitonic effects and can be based on the ground-state electronic structure in the DFT, hybrid-functional or even GW approximations.
Solving Casida equation
The algorithm for solving the Casida equation can be selected by setting ALGO = TDHF. This approach is very similar to BSE but differs in the way the screening of the Coulomb potential is approximated. The TDHF approach uses the exchange-correlation kernel , whereas BSE requires the from a preceding GW calculation. Thus, in order to perform a TDHF calculation, one only needs to provide the ground-state orbitals (WAVECAR) and the derivatives of the orbitals with respect to (WAVEDER).
| Mind: Unlike BSE, TDHF calculations do not require , i.e., Wxxxx.tmp |
In summary, both TDHF and BSE approaches require a preceding ground-state calculation, however, the TDHF does not need the preceding GW and can be performed with the DFT or hybrid-functional orbitals and energies.
Time-dependent Hartree-Fock
The TDHF calculations can be performed in two steps:
- ground-state calculation
- optical absorption calculation
For example, an optical absorption calculation of bulk Si can be performed using a dielectric-dependent hybrid-functional described in Ref. [1][2][3].
SYSTEM = Si ISMEAR = 0 SIGMA = 0.05 NBANDS = 16 ! or any larger desired value ALGO = D ! Damped algorithm often required for HF type calculations, ALGO = Normal might work as well LHFCALC = .TRUE. LMODELHF = .TRUE. AEXX = 0.083 HFSCREEN = 1.22 LOPTICS = .TRUE. ! can also be done in an additional intermediate step
In the second step, the dielectric function is evaluated by solving the Casida equation
SYSTEM = Si ISMEAR = 0 SIGMA = 0.05 NBANDS = 16 ALGO = TDHF IBSE = 0 NBANDSO = 4 ! number of occupied bands NBANDSV = 8 ! number of unoccupied bands LHARTREE = .TRUE. LADDER = .TRUE. LFXC = .TRUE. LMODELHF = .TRUE. AEXX = 0.083 HFSCREEN = 1.22
THDF calculations can be performed for non-spin-polarized, spin-polarized, and noncollinear cases, as well as the case with spin-orbit coupling. There is, however, one caveat. The local exchange-correlation kernel is approximated by the density-density part only. This makes predictions for spin-polarized systems less accurate than for non-spin-polarized systems.
Time-dependent DFT calculation
The TDDFT calculation using the PBE exchange-correlation kernel can be performed by disabling the ladder diagrams LADDER = .FALSE., i.e., only the PBE exchange-correlation kernel is present in the Hamiltonian.
SYSTEM = Si ISMEAR = 0 SIGMA = 0.05 NBANDS = 16 ALGO = TDHF IBSE = 0 NBANDSO = 4 ! determines how many occupied bands are used NBANDSV = 8 ! determines how many unoccupied (virtual) bands are used LFXC = .TRUE. LHARTREE = .TRUE. LADDER = .FALSE.
| Mind: In TDDFT calculation, where the ladder diagrams are not included (LADDER=.FALSE.) or the fraction of exact exchange in the kernel is zero (AEXX=0), the resulting dielectric function lacks the excitonic effects. |
VASP tries to use sensible defaults, but it is highly recommended to check the OUTCAR file and make sure that the right bands are included. The tag OMEGAMAX specifies the maximum excitation energy of included electron-hole pairs and the pairs with the one-electron energy difference beyond this limit are not included in the Hamiltonian.
The calculated frequency-dependent dielectric function, transition energies and oscillator strength values are stored in the vasprun.xml file.
Calculations beyond Tamm-Dancoff approximation
Calculations beyond Tamm-Dancoff approximation can be performed in the same manner as in the BSE.
Calculations at finite wavevectors
Calculations at finite wavevectors can be performed in the same manner as in the BSE.
References
- ↑ W. Chen, G. Miceli, G.M. Rignanese, and A. Pasquarello, Nonempirical dielectric-dependent hybrid functional with range separation for semiconductors and insulators, Phys. Rev. Mater. 2, 073803 (2018).
- ↑ Z.H. Cui, Y.C. Wang, M.Y. Zhang, X. Xu, and H. Jiang, Doubly Screened Hybrid Functional: An Accurate First-Principles Approach for Both Narrow- and Wide-Gap Semiconductors J. Phys. Chem. Lett., 9, 2338-2345 (2018).
- ↑ P. Liu, C. Franchini, M. Marsman, and G. Kresse, Assessing model-dielectric-dependent hybrid functionals on the antiferromagnetic transition-metal monoxides MnO, FeO, CoO, and NiO, J. Phys.: Condens. Matter 32, 015502 (2020).