The dftname Keyword in the Jaguar Input File
density functional, exchange functional, correlation functional
- Overview
- Examples
The dftname keyword is used to specify the density functional, and also turns on the use of DFT in the calculation. The dftname keyword can be given as a standard functional name. The standard names for local, gradient-corrected, hybrid, and long-range-corrected functionals are given in the tables below. The dftname keyword is case-insensitive.
The dftname keyword can also be constructed from a set of functional name strings for exchange and correlation functionals, which are listed in Table 8.
You can modify the dftname keyword by adding a suffix for various corrections:
-
For many of the functionals, dispersion corrections are available, and can be specified by appending the name of the dispersion correction to the functional name, for example,
B3LYP-D3. See Table 1 for an overview of available dispersion corrections.
-
The ulg a posteriori correction of Kim, Choi, and Goddard [92] is available for all functionals and can be specified by appending
-ulgto the functional name. This functional is available for all elements up to Z=103. -
The a posteriori localized orbital correction (LOC) [83-91] is available for the B3LYP functional. It is specified by
B3LYP-LOC. -
The a posteriori correction for dispersion, cation-π, and hydrogen bond interactions [82] is available for the B3LYP functional. It is specified by
B3LYP-MM.
For keywords related to a posteriori corrections, see Other DFT Keywords in the Jaguar Input File.
If you want to evaluate the energy of the final, post-SCF wave function using a particular functional or combination of functionals, you can use the pdftname keyword, which has the same values as the dftname keyword.
- Dispersion Corrections
- Local Density Functionals
- Generalized-Gradient and Meta-GGA Density Functionals
- Hybrid Density Functionals
- Double Hybrid Density Functionals
- Long-Range Corrected Density Functionals
- Composite methods
- Other DFT Functional Keywords
Dispersion Corrections
For many of the functionals, dispersion corrections are available, and can be specified by appending the name of the dispersion correction to the functional name, separated by a dash. For example, to use the B3LYP functional with the D3 dispersion correction, set dftname=B3LYP-D3 in the Jaguar input file. The available dispersion corrections for each functional are listed in the functional keyword tables below.
| Keyword | Description | References |
|---|---|---|
D3
|
Grimme’s two-body dispersion correction | doi:10.1063/1.3382344 |
D3(BJ)
|
D3 correction with a Becke-Johnson damping function | doi:10.1002/jcc.21759 |
D3M
|
Modified D3 correction with revised damping paramaters | doi:10.1021/acs.jpclett.6b00780 |
D3M(BJ)
|
Modified D3 correction with revised damping parameters with a Becke-Johnson damping function | doi:10.1021/acs.jpclett.6b00780 |
D4
|
Successor to the D3 correction, includes charge dependence and three-body effects | doi:10.1063/1.5090222 |
Local Density Functionals
The following density functionals use the local density approximation (LDA). LDA functionals include only the electron density in the exchange-correlation potential.
| Keyword | Description | References |
|---|---|---|
HFS
|
Slater local exchange, also known as Hartree-Fock-Slater | |
XALPHA
|
Xα local exchange | |
SVWN
|
Slater local exchange, Vosko-Wilk-Nusair (VWN) local correlation | doi:10.1139/p80‑159 |
SVWN5
|
Slater local exchange, Vosko-Wilk-Nusair 5 (VWN5) local correlation | doi:10.1139/p80‑159 |
Generalized-Gradient and Meta-GGA Density Functionals
Density functionals using the generalized-gradient approximation (GGA) include the gradient of the electron density in the exchange-correlation potential. Meta-GGA density functionals also include the second derivative (Laplacian) of the electron density.
| Keyword | Description | Level of Theory | Dispersion Corrections | References |
|---|---|---|---|---|
HFB
|
Slater local exchange, Becke 1988 non-local gradient correction to exchange | GGA | doi:10.1103/PhysRevA.38.3098 | |
HFPW
|
Slater local exchange, Perdew-Wang 1991 GGA‑II nonlocal exchange | GGA | doi:10.1103/PhysRevB.46.6671 | |
BLYP
|
Slater local exchange, Becke 1988 non-local gradient correction; Vosko-Wilk-Nusair (VWN) local correlation, Lee-Yang-Parr local and nonlocal correlation | GGA | D3, D3(BJ), D3M, D3M(BJ), D4 | doi:10.1103/PhysRevA.38.3098
doi:10.1139/p80‑159 doi:10.1103/PhysRevB.37.785 doi:10.1016/0009‑2614(89)87234‑3 |
BPW91
|
Slater local exchange, Becke 1988 nonlocal gradient correction; Perdew-Wang 1991 GGA-II local and nonlocal correlation | GGA | D4 | doi:10.1103/PhysRevA.38.3098
doi:10.1103/PhysRevB.46.6671 |
BP86
|
Slater local exchange, Becke 1988 nonlocal gradient correction; Perdew-Zunger 1981 local correlation, Perdew 1986 gradient correction | GGA | D3, D3(BJ), D3M, D3M(BJ), D4 | doi:10.1103/PhysRevA.38.3098
doi:10.1103/PhysRevB.23.5048 doi:10.1103/PhysRevB.33.8822 doi:10.1103/PhysRevB.33.8822 |
BP86‑VWN5
|
Slater local exchange, Becke 1988 nonlocal gradient correction; Vosko-Wilk-Nusair 5 local correlation, Perdew 1986 gradient correction | GGA | doi:10.1103/PhysRevA.38.3098
doi:10.1139/p80‑159 doi:10.1103/PhysRevB.33.8822 doi:10.1103/PhysRevB.33.8822 |
|
PWPW91
|
Slater local exchange, Perdew-Wang 1991 GGA‑II nonlocal exchange, local and nonlocal correlation | GGA | doi:10.1103/PhysRevB.46.6671 | |
HCTH407
|
Hamprecht-Cohen-Tozer-Handy functional including local and nonlocal exchange and correlation, reparametrized with a training set of 407 molecules by Boese and Handy | GGA | doi:10.1063/1.1347371 | |
PBE
|
Perdew-Burke-Ernzerhof local and nonlocal exchange and correlation | GGA | D3, D3(BJ), D3M, D3M(BJ), D4 | doi:10.1103/PhysRevLett.77.3865
doi:10.1103/PhysRevLett.78.1386 |
M06‑L
|
Zhao and Truhlar gradient-corrected local functional | meta-GGA | D4 | doi:10.1063/1.2370993 |
OLYP
|
Slater local exchange, OPTX nonlocal exchange of Handy and Cohen; Lee-Yang-Parr local and nonlocal correlation | GGA | D3, D3(BJ), D4 | doi:10.1080/00268970010018431
doi:10.1103/PhysRevB.37.785 doi:10.1016/0009‑2614(89)87234‑3 |
GAM
|
Parameterization by Truhlar and coworkers similar to N12, with smoothness constraints to give better accuracy for molecules, particularly transition metal complexes | GGA | doi:10.1021/ct3002656 | |
N12
|
Parameterization by Peverati and Truhlar that combines gradient and density terms in a nonseparable manner, parametrized to give good accuracy for solid-state and molecular energies and structures | GGA | doi:10.1021/ct3002656 | |
MN12‑L
|
Parameterization by Peverati and Truhlar that includes gradient and kinetic energy spin density functionals, with broad applicability | meta-GGA | doi:10.1039/C2CP42025B | |
MN15‑L
|
Reparametrization of the MN12-L functional against a broader database and with constraints to ensure smooth functions of geometry | meta-GGA | doi:10.1021/acs.jctc.5b01082 | |
TPSS
|
Tao, Perdew, Staroverov, and Scuseria functional, defines exchange and correlation | meta-GGA | D4 | doi:10.1103/PhysRevLett.91.146401 |
SCAN
|
Strongly Constrained and Appropriately Normed functional, defines exchange and correlation | meta-GGA | D4 | doi:10.1103/PhysRevLett.115.036402 |
PKZB
|
Perdew, Kurth, Zupan, and Blaha functional, defines exchange and correlation | meta-GGA | doi:10.1103/PhysRevLett.82.2544 | |
SOGGA
|
Zhao and Truhlar second-order GGA exchange, PBE correlation | GGA | doi:10.1063/1.2912068 | |
SOGGA11
|
Peverati, Zhao, and Truhlar improvement on SOGGA, defines exchange and correlation | GGA | doi:10.1021/jz200616w | |
BOP
|
Becke 1988 GGA exchange, BOP one-parameter progressive GGA correlation | GGA | doi:10.1063/1.479012 | |
GLYP
|
Gill 1996 exchange with Lee-Yang-Parr correlation | GGA | D4 | doi:10.1080/002689796173813 |
RPBE
|
Hammer, Hansen, and Norskov modification of PBE exchange | GGA | D4 | doi:10.1103/PhysRevB.59.7413 |
revPBE
|
Zhang and Yang one-parameter modification of the PBE exchange | GGA | D4 | doi:10.1103/PhysRevLett.80.890 |
revTPSS
|
Revised version of the TPSS exchange functional, defines exchange and correlation | meta-GGA | D4 | doi:10.1103/PhysRevLett.103.026403 |
KT2
|
GGA functional designed specifically for shielding constant calculations, defines exchange and correlation | GGA | doi:10.1063/1.1590634 | |
MGGA‑MS0
|
Sun, Bing, and Ruzsinszky Meta-GGA exchange derived from examining dependence on kinetic energy density, regTPSS correlation | meta-GGA | doi:10.1063/1.4742312 | |
MGGA‑MS1
|
MGGA-MS0 with modified empirical parameters, regTPSS correlation | meta-GGA | doi:10.1063/1.4789414 | |
MGGA‑MS2
|
MGGA-MS0 with modified empirical parameters, regTPSS correlation | meta-GGA | doi:10.1063/1.4789414 | |
rSCAN
|
Regularized Strongly Constrained and Appropriately Normed functional, defines exchange and correlation | meta-GGA | D4 | doi:10.1063/1.5094646 |
r2SCAN
|
Regularized-restored Strongly Constrained and Appropriately Normed functional, defines exchange and correlation | meta-GGA | D3(BJ), D4 | doi:10.1021/acs.jpclett.0c02405 |
B2PLYP
|
Grimme and Neese Double Hybrid GGA functional | GGA | doi:10.1063/1.2148954 | |
B2GPPLYP
|
Reparametrization of B2PLYP, trained to be 'General Purpose' (GP) | GGA | doi:10.1021/jp801805p | |
DSD‑BLYP
|
Kozuch, Gruzman, and Martin Double Hybrid modification of the BLYP GGA functional | GGA | doi:10.1021/jp1070852 | |
DSD‑PBEP86
|
Double hybrid pairing PBE exchange with the GGA P86 correlation functional | GGA | doi:10.1039/C1CP22592H | |
PWPB95
|
Double hybrid combining PWP exchange with the Meta-GGA B95 correlation functional | meta-GGA | doi:10.1021/ct100466k | |
B2K‑PLYP
|
Double hybrid functional parametrized for good performance for kinetics | GGA | doi:10.1021/jp710179r | |
B2T‑PLYP
|
Double hybrid functional parametrized for good performance for thermodynamics | GGA | doi:10.1021/jp710179r | |
DSD‑PBEB95
|
Double hybrid pairing PBE exchange with the Meta-GGA B95 correlation functional | meta-GGA | doi:10.1002/jcc.23391 | |
MPW2PLYP
|
Double hybrid derived from B2PLYP by replacing B88 exchange with mPW exchange | meta-GGA | doi:10.1039/B608478H | |
SCS‑B2GPPLYP
|
Spin component scaled variant of B2GPPLYP | GGA | doi:10.1021/acs.jctc.1c00535 | |
SCS‑PBE‑QIDH
|
Spin component scaled variant of PBE-QIDH | GGA | doi:10.1021/acs.jctc.1c00535 | |
SOS‑B2GPPLYP
|
Scaled opposite spin variant of B2GPPLYP | GGA | doi:10.1021/acs.jctc.1c00535 | |
SOS‑PBE‑QIDH
|
Scaled opposite spin variant of PBE-QIDH | GGA | doi:10.1021/acs.jctc.1c00535 | |
PBE‑QIDH
|
Quadratic Integrand Double Hybrid (QIDH) derived from PBE | GGA | doi:10.1063/1.4890314 | |
PBE0‑DH
|
Double Hybrid (QIDH) derived from PBE0 | GGA | doi:10.1063/1.3604569 |
Hybrid Density Functionals
Hybrid density functionals are GGA or meta-GGA functionals that also include a part of Hartree-Fock (HF) exchange in their exchange-correlation potential.
| Keyword | Description | Level of Theory | Dispersion Corrections | References |
|---|---|---|---|---|
PBE0
|
Adamo and Barone functional based on PBE. 0.25 HF exchange, 0.75 PBE non-local exchange; Perdew-Burke-Ernzerhof local and nonlocal correlation | GGA/hybrid | D3, D3(BJ), D3M, D3M(BJ), D4 | doi:10.1063/1.478522
doi:10.1103/PhysRevLett.77.3865 doi:10.1103/PhysRevLett.78.1386 |
B3LYP
|
HF and Slater local exchange, Becke 1988 non-local gradient correction; Vosko-Wilk-Nusair local correlation, Lee-Yang-Parr local and nonlocal correlation | GGA/hybrid | D3, D3(BJ), D3M, D3M(BJ), D4 | doi:10.1103/PhysRevA.38.3098
doi:10.1139/p80‑159 doi:10.1103/PhysRevB.37.785 doi:10.1016/0009‑2614(89)87234‑3 |
B3PW91
|
HF and Slater local exchange, Becke 1988 nonlocal gradient correction; Perdew-Wang 1991 GGA-II local and nonlocal correlation | GGA/hybrid | D3, D3(BJ), D4 | doi:10.1103/PhysRevA.38.3098
doi:10.1103/PhysRevB.46.6671 |
B3P86
|
HF and Slater local exchange, Becke 1988 nonlocal gradient correction; Vosko-Wilk-Nusair local correlation, Perdew 1986 gradient correction | GGA/hybrid | D4 | doi:10.1103/PhysRevA.38.3098
doi:10.1139/p80‑159 doi:10.1103/PhysRevB.33.8822 doi:10.1103/PhysRevB.33.8822 |
BHANDH
|
0.5 HF exchange, 0.5 Slater local exchange.
Note: The definition of this functional was changed in the 2020-4 release, to be made consistent with other QM programs. To reproduce the previous definition, use dftname=user-defined
and set
x_hf=0.5 x_slater=0.5
in the
xcfunc
section of the input file.
|
doi:10.1063/1.464304 | ||
BHANDHLYP
|
0.5 HF exchange, 0.5 Slater local exchange, Becke 1988 nonlocal gradient correction; Lee-Yang-Parr local and nonlocal correlation.
Note: The definition of this functional was changed in the 2020-4 release, to be made consistent with other QM programs. To reproduce the previous definition, use dftname=user-defined
and set
x_hf=0.5 x_slater=0.5 c_lyp=0.5
in the
xcfunc
section of the input file.
|
GGA/hybrid | doi:10.1063/1.464304
doi:10.1103/PhysRevA.38.3098 doi:10.1103/PhysRevB.37.785 doi:10.1016/0009‑2614(89)87234‑3 |
|
B97
|
Becke 1997 hybrid functional | GGA/hybrid | doi:10.1063/1.475007 | |
B97‑D
|
Modified Becke 1997 functional with Grimme long-range dispersion correction, useful for noncovalent interactions | GGA/hybrid | doi:10.1063/1.475007
doi:10.1063/1.3382344 |
|
B97‑1
|
Reparametrization of Becke 1997 hybrid functional by Hamprecht, Cohen, Tozer, and Handy | GGA/hybrid | doi:10.1063/1.475007
doi:10.1063/1.477267 |
|
B98
|
Becke 1998 hybrid including Laplacian of the density and kinetic energy density terms | GGA/hybrid | doi:10.1063/1.476722 | |
SB98
|
Schmider and Becke reparametrization of Becke 1998 functional | GGA/hybrid | doi:10.1063/1.477481
doi:10.1063/1.476438 |
|
MPW1K
|
Reoptimization of mPW1PW91 for prediction of barrier heights, by Lynch, Fast, Harris, and Truhlar | GGA/hybrid | doi:10.1021/jp000497z | |
MPWB1K
|
Zhao and Truhlar 2004 functional, optimized for reaction barriers and reaction energies | meta-GGA/hybrid | D3, D4 | doi:10.1021/jp048147q |
B1B95
|
Becke 1996 hybrid functional with 0.28 HF exchange | meta-GGA/hybrid | D3, D3(BJ), D4 | doi:10.1063/1.470829 |
BB1K
|
Zhao, Lynch and Truhlar reparametrization of Becke 1996 hybrid functional for kinetics (reaction barriers), with 0.42 HF exchange | meta-GGA/hybrid | doi:10.1021/jp049908s | |
X3LYP
|
Xu and Goddard extension of B3LYP to include Perdew-Wang 1991 exchange gradient correction, with exchange parametrized to fit Gaussian exchange density | GGA/hybrid | D4 | doi:10.1103/PhysRevB.46.6671
doi:10.1073/pnas.0308730100 |
MPW1PW91
|
Hybrid with modification of Perdew-Wang exchange gradient correction by Adamo and Barone, 0.25 HF exchange, 0.75 Slater local exchange, Perdew-Wang 1991 gradient correction; correlation: Perdew-Wang 1991 GGA-II local and nonlocal correlation | GGA/hybrid | D4 | doi:10.1103/PhysRevB.46.6671
doi:10.1063/1.475428 |
PWB6K
|
Zhao and Truhlar reoptimization of MPWB1K functional for simultaneous accuracy of bond energies, barrier heights, and nonbonded interactions | meta-GGA/hybrid | doi:10.1021/jp049908s | |
PW6B95
|
Zhao and Truhlar reoptimization of MPW1B95 functional for simultaneous accuracy of bond energies, barrier heights, and nonbonded interactions | meta-GGA/hybrid | D3, D3(BJ), D4 | doi:10.1021/jp049908s |
M05
|
Zhao, Schultz, and Truhlar hybrid parametrized for broad accuracy, including noncovalent interactions, kinetics, and interactions with metals | meta-GGA/hybrid | D3 | doi:10.1063/1.2126975
doi:10.1021/ct0502763 |
M05‑2X
|
Zhao, Schultz, and Truhlar hybrid with larger HF exchange component, similar to M05 but parametrized for nonmetals | meta-GGA/hybrid | D3 | doi:10.1063/1.2126975
doi:10.1021/ct0502763 |
M06
|
Zhao and Truhlar functional, parametrized with metallic systems, for organometallic and inorganic chemistry and noncovalent interactions | meta-GGA/hybrid | D3, D4 | doi:10.1007/s00214‑007‑0310‑x |
M06‑2X
|
Zhao and Truhlar functional, parametrized for nonmetals, for main-group thermochemistry, kinetics, noncovalent interactions, and electronic excitation energies to valence and Rydberg states | meta-GGA/hybrid | D3 | doi:10.1007/s00214‑007‑0310‑x |
M06‑HF
|
Zhao and Truhlar functional with full HF exchange and M06 local functionals that eliminates long-range self-interaction | meta-GGA/hybrid | D3 | doi:10.1021/jp066479k |
O3LYP
|
HF and Slater local exchange, OPTX nonlocal exchange of Handy and Cohen; Lee-Yang-Parr local and nonlocal correlation | GGA/hybrid | D4 | doi:10.1080/00268970010018431
doi:10.1103/PhysRevB.37.785 doi:10.1016/0009‑2614(89)87234‑3 |
M08‑HX
|
Zhao and Truhlar functional, constraining the reduced density gradient to exact exchange and correlation functional forms through second order, parametrized on a broad range of properties | meta-GGA/hybrid | doi:10.1021/ct800246v | |
M08‑SO
|
Zhao and Truhlar functional, similar to M08-HX | meta-GGA/hybrid | doi:10.1021/ct800246v | |
MN15
|
Nonseparable gradient approximation from Truhlar and coworkers, with emphasis on multireference systems, barrier heights, noncovalent interactions and excitation energies | doi:10.1039/C6SC00705H | ||
TPSSh
|
10% HF exchange + 90% TPSS exchange + TPSS correlation | meta-GGA/hybrid | D4 | doi:10.1063/1.1626543 |
SCAN0
|
25% HF exchange + 75% SCAN exchange + SCAN correlation | meta-GGA/hybrid | doi:10.1063/1.4940734 | |
revTPSSh
|
Revised version of the TPSSh exchange functional, defines exchange and correlation | meta-GGA/hybrid | D4 | doi:10.1021/ct100488v |
SOGGA11‑X
|
Peverati and Truhlar 21-parameter functional with 40.15% HF exchange, defines exchange and correlation | GGA/hybrid | doi:10.1063/1.3663871 | |
MGGA‑MS2h
|
9% HF exchange, 91% MGGA-MS2 exchange, regTPSS correlation | meta-GGA/hybrid | doi:10.1063/1.4789414 |
Double Hybrid Density Functionals
| Keyword | Description | Level of Theory | Dispersion Corrections | References |
|---|---|---|---|---|
B2PLYP
|
Grimme and Neese Double Hybrid GGA functional | GGA | doi:10.1063/1.2148954 | |
B2GPPLYP
|
Reparametrization of B2PLYP, trained to be 'General Purpose' (GP) | GGA | doi:10.1021/jp801805p | |
DSD‑BLYP
|
Kozuch, Gruzman, and Martin Double Hybrid modification of the BLYP GGA functional | GGA | doi:10.1021/jp1070852 | |
DSD‑PBEP86
|
Double hybrid pairing PBE exchange with the GGA P86 correlation functional | GGA | doi:10.1039/C1CP22592H | |
PWPB95
|
Double hybrid combining PWP exchange with the Meta-GGA B95 correlation functional | meta-GGA | doi:10.1021/ct100466k | |
B2K‑PLYP
|
Double hybrid functional parametrized for good performance for kinetics | GGA | doi:10.1021/jp710179r | |
B2T‑PLYP
|
Double hybrid functional parametrized for good performance for thermodynamics | GGA | doi:10.1021/jp710179r | |
DSD‑PBEB95
|
Double hybrid pairing PBE exchange with the Meta-GGA B95 correlation functional | meta-GGA | doi:10.1002/jcc.23391 | |
MPW2PLYP
|
Double hybrid derived from B2PLYP by replacing B88 exchange with mPW exchange | meta-GGA | doi:10.1039/B608478H | |
RSX‑0DH
|
Range separated exchange (RSX) PBE0 Double Hybrid (0DH) derived from PBE0 | GGA | doi:10.1063/1.5097164 | |
RSX‑QIDH
|
Range separated exchange (RSX) Quadratic Integrand Double Hybrid (QIDH) derived from PBE | GGA | doi:10.1063/1.5097164 | |
wB2GPPLYP
|
Range separated variant of B2GPPLYP | GGA | doi:10.1021/acs.jctc.9b00013 | |
wB2PLYP
|
Range separated variant of B2PLYP | GGA | doi:10.1021/acs.jctc.9b00013 | |
wB88PP86
|
Range separated Becke88 exchange with P86 correlation | GGA | doi:10.1021/acs.jctc.1c00535 | |
wPBEPP86
|
Range separated PBE exchange with P86 correlation | GGA | doi:10.1021/acs.jctc.1c00535 | |
SCS‑B2GPPLYP
|
Spin component scaled variant of B2GPPLYP | GGA | doi:10.1021/acs.jctc.1c00535 | |
SCS‑PBE‑QIDH
|
Spin component scaled variant of PBE-QIDH | GGA | doi:10.1021/acs.jctc.1c00535 | |
SCS‑RSX‑QIDH
|
Spin component scaled variant of RSX-QIDH | GGA | doi:10.1021/acs.jctc.1c00535 | |
SCS‑wB2GPPLYP
|
Spin component scaled variant of wB2GPPLYP | GGA | doi:10.1021/acs.jctc.1c00535 | |
SCS‑wB88PP86
|
Spin component scaled variant of wB88PP86 | GGA | doi:10.1021/acs.jctc.1c00535 | |
SCS‑wPBEPP86
|
Spin component scaled variant of wPBEPP86 | GGA | doi:10.1021/acs.jctc.1c00535 | |
SOS‑B2GPPLYP
|
Scaled opposite spin variant of B2GPPLYP | GGA | doi:10.1021/acs.jctc.1c00535 | |
SOS‑PBE‑QIDH
|
Scaled opposite spin variant of PBE-QIDH | GGA | doi:10.1021/acs.jctc.1c00535 | |
SOS‑RSX‑QIDH
|
Scaled opposite spin variant of RSX-QIDH | GGA | doi:10.1021/acs.jctc.1c00535 | |
SOS‑wB2GPPLYP
|
Scaled opposite spin variant of wB2GPPLYP | GGA | doi:10.1021/acs.jctc.1c00535 | |
SOS‑wB88PP86
|
Scaled opposite spin variant of wB88PP86 | GGA | doi:10.1021/acs.jctc.1c00535 | |
SOS‑wPBEPP86
|
Scaled opposite spin variant of wPBEPP86 | GGA | doi:10.1021/acs.jctc.1c00535 | |
PBE‑QIDH
|
Quadratic Integrand Double Hybrid (QIDH) derived from PBE | GGA | doi:10.1063/1.4890314 | |
PBE0‑DH
|
Double Hybrid (QIDH) derived from PBE0 | GGA | doi:10.1063/1.3604569 |
Long-Range Corrected Density Functionals
Long-range corrected functionals include long-range Hartree-Fock exchange in their exchange-correlation potentials. You can set the value for the range separation parameter w with the lrc-omega keyword, in bohr-1. The names of the modified versions of the exchange are prefixed with SR- or LR-.
| Keyword | Description | Level of Theory | Dispersion Corrections | References |
|---|---|---|---|---|
LRC‑BLYP
|
Yanai, Tew, and Handy functional, short-range exchange Becke 88, long-range HF exchange; ω=0.33; LYP correlation | GGA | D4 | doi:10.1103/PhysRevA.38.3098
doi:10.1103/PhysRevB.37.785 doi:10.1016/0009‑2614(89)87234‑3 doi:10.1016/j.cplett.2004.06.011 |
CAM‑B3LYP
|
Yanai, Tew, and Handy functional, short-range exchange 0.19 HF, 0.81 Becke 88, long-range exchange 0.65 HF, 0.35 Becke 88; ω=0.33; LYP correlation | GGA/hybrid | D3, D3(BJ), D4 | doi:10.1103/PhysRevA.38.3098
doi:10.1103/PhysRevB.37.785 doi:10.1016/0009‑2614(89)87234‑3 doi:10.1016/j.cplett.2004.06.011 |
uPBE
|
PBE functional, short range exchange PBE, long range HF exchange; ω=0.30; PBE correlation | GGA | doi:10.1103/PhysRevLett.77.3865
doi:10.1103/PhysRevLett.78.1386 |
|
uPBE0
|
PBE hybrid, short range exchange 0.25 HF, 0.75 PBE, long range HF exchange; ω=0.30; PBE correlation | GGA/hybrid | doi:10.1103/PhysRevLett.77.3865
doi:10.1103/PhysRevLett.78.1386 |
|
wPBE
|
Vydrov and Scuseria functional, short range exchange SR-PBE, long range HF exchange; ω=0.30 (NWChem value); PBE correlation.
Note: The value used in the original publication is ω=0.4. |
GGA | D3, D3(BJ), D3M, D3M(BJ) | doi:10.1103/PhysRevLett.77.3865
doi:10.1103/PhysRevLett.78.1386 doi:10.1063/1.2409292 |
wPBEH
|
Rohrdanz, Martins, and Herbert hybrid, short range exchange 0.20 HF, 0.80 PBE, long range HF exchange; ω=0.20; PBE correlation | GGA/hybrid | doi:10.1103/PhysRevLett.77.3865
doi:10.1103/PhysRevLett.78.1386 doi:10.1063/1.3073302 |
|
HSE03
|
Heyd, Scuseria, and Ernzerhof hybrid, short range exchange 0.25 HF, 0.75 PBE, long range HF exchange; ω=0.33 (NWChem value); PBE correlation.
Note: For the value used in the original publication, see the Erratum: doi:10.1063/1.2204597 |
GGA | D4 | doi:10.1103/PhysRevLett.77.3865
doi:10.1103/PhysRevLett.78.1386 doi:10.1063/1.156406 |
HSE06
|
Heyd, Scuseria, and Ernzerhof hybrid, short range exchange 0.25 HF, 0.75 PBE; long range HF exchange; ω=0.11; PBE correlation | GGA | D4 | doi:10.1103/PhysRevLett.77.3865
doi:10.1103/PhysRevLett.78.1386 doi:10.1063/1.2404663 |
M11
|
Peverati and Truhlar hybrid, short range exchange: 0.428 M11 and HF, long-range HF exchange; ω=0.25; M11 correlation | meta-GGA/hybrid | doi:10.1021/jz201170d | |
M11‑L
|
Peverati and Truhlar non-hybrid, short range exchange M11; long-range exchange M11; ω=0.25; M11-L correlation | meta-GGA | doi:10.1021/jz201525m | |
wB97
|
Chai and Head-Gordon functional, short range exchange Becke 97; long-range HF exchange; ω=0.4; Becke 97 correlation | GGA/hybrid | D4 | doi:10.1063/1.475007
doi:10.1063/1.2834918 |
wB97X
|
Chai and Head-Gordon hybrid, short range exchange 0.16 Becke 97, HF; long-range HF exchange; ω=0.3; Becke 97 correlation.
Note: wB97X-D3(BJ) calculations use the wB97X-V kernel with a D3(BJ) correction, while xB97X-D4 calculations use the original wB97X kernel and its corresponding D4 correction. |
GGA/hybrid | D3, D3(BJ), D4 | doi:10.1063/1.475007
doi:10.1063/1.2834918 |
wB97X‑D
|
Chai and Head-Gordon hybrid with Grimme long-range dispersion correction, short range exchange 0.22 Becke 97, HF; long-range HF exchange; ω=0.2; Becke 97 correlation | GGA/hybrid | doi:10.1063/1.475007
doi:10.1039/B810189B |
|
BNL
|
Baer, Neuhauser, and Livshits functional. Short-range exchange: 90% SR-Savin; long-range exchange: HF; ω =0.3; LYP correlation | GGA | doi:10.1103/PhysRevLett.94.043002
doi:10.1039/B617919C |
|
MN12‑SX
|
MN12-L functional with 0.25 HF short-range exchange, 0 long-range HF exchange (screened exchange) | meta-GGA/hybrid | D4 | doi:10.1039/C2CP42576A |
wB97M‑V
|
Mardirossian and Head-Gordon combinatorially optimized, range-separated hybrid with VV10 nonlocal correlation | meta-GGA/hybrid | doi:10.1063/1.4952647 | |
wB97X‑V
|
Mardirossian and Head-Gordon 10 parameter range-separated hybrid with VV10 nonlocal correlation | GGA/hybrid | doi:10.1039/c3cp54374a | |
RSX‑0DH
|
Range separated exchange (RSX) PBE0 Double Hybrid (0DH) derived from PBE0 | GGA | doi:10.1063/1.5097164 | |
RSX‑QIDH
|
Range separated exchange (RSX) Quadratic Integrand Double Hybrid (QIDH) derived from PBE | GGA | doi:10.1063/1.5097164 | |
wB2GPPLYP
|
Range separated variant of B2GPPLYP | GGA | doi:10.1021/acs.jctc.9b00013 | |
wB2PLYP
|
Range separated variant of B2PLYP | GGA | doi:10.1021/acs.jctc.9b00013 | |
wB88PP86
|
Range separated Becke88 exchange with P86 correlation | GGA | doi:10.1021/acs.jctc.1c00535 | |
wPBEPP86
|
Range separated PBE exchange with P86 correlation | GGA | doi:10.1021/acs.jctc.1c00535 | |
SCS‑RSX‑QIDH
|
Spin component scaled variant of RSX-QIDH | GGA | doi:10.1021/acs.jctc.1c00535 | |
SCS‑wB2GPPLYP
|
Spin component scaled variant of wB2GPPLYP | GGA | doi:10.1021/acs.jctc.1c00535 | |
SCS‑wB88PP86
|
Spin component scaled variant of wB88PP86 | GGA | doi:10.1021/acs.jctc.1c00535 | |
SCS‑wPBEPP86
|
Spin component scaled variant of wPBEPP86 | GGA | doi:10.1021/acs.jctc.1c00535 | |
SOS‑RSX‑QIDH
|
Scaled opposite spin variant of RSX-QIDH | GGA | doi:10.1021/acs.jctc.1c00535 | |
SOS‑wB2GPPLYP
|
Scaled opposite spin variant of wB2GPPLYP | GGA | doi:10.1021/acs.jctc.1c00535 | |
SOS‑wB88PP86
|
Scaled opposite spin variant of wB88PP86 | GGA | doi:10.1021/acs.jctc.1c00535 | |
SOS‑wPBEPP86
|
Scaled opposite spin variant of wPBEPP86 | GGA | doi:10.1021/acs.jctc.1c00535 |
Composite methods
The following density functionals are composite methods which use a pre-defined basis set and apply pre-defined corrections. These pre-defined parameters are described in the Description column.
| Keyword | Description | Level of Theory | References |
|---|---|---|---|
B97‑3c
|
Grimme and coworkers composite method combining reparametrized B97 with short range basis (SRB) and D3(BJ) dispersion corrections. Uses def2-mTZVP basis. | GGA | doi:10.1063/1.5012601 |
r2SCAN‑3c
|
Grimme and coworkers composite method combining r2SCAN with geometric counterpoise (gCP) and D4 dispersion corrections. Uses def2-mTZVPP basis. | meta-GGA | doi:10.1063/5.0040021 |
wB97X‑3c
|
Grimme and coworkers composite method which replaces the VV10 kernel of wB97X-V with the D4 dispersion correction. Uses vDZP basis. | GGA/hybrid | doi:10.1063/5.0133026 |
PBEH‑3c
|
Grimme and coworkers composite method combining reparametrized PBEh with geometric counterpoise (gCP) and D3(BJ) dispersion corrections. Uses def2-mSVP basis. | GGA/hybrid | doi:10.1063/1.4927476 |
HF‑3c
|
Grimme and coworkers composite method combining Hartree-Fock with short range basis (SRB), geometric counterpoise (gCP), and D3(BJ) dispersion corrections. Uses MINIX basis. | doi:10.1002/jcc.23317 |
Other DFT Functional Keywords
You can combine the functional name strings listed in Table 8 to construct the dftname keyword. For example, dftname=bp86 specifies the BP86 functional, and is a combination of b for exchange and p86 for correlation. This is a way of combining functionals to form a particular combination, though you can’t specify the coefficients. If you also want to modify the various coefficients of the exchange and correlation functionals, see The xcfunc Section of the Jaguar Input File.
| Name String | Functional Description |
|---|---|
|
|
Slater local exchange |
|
|
Xα local exchange |
|
|
Becke 1988 nonlocal exchange, Slater local exchange |
|
|
Gill's gradient-corrected exchange functional [302] |
|
|
Perdew-Wang 1991 GGA-II nonlocal exchange, Slater local exchange |
|
|
Vosko-Wilk-Nusair local correlation |
|
|
Vosko-Wilk-Nusair 5 local correlation |
|
|
Perdew-Zunger 1981 local correlation |
|
|
Perdew-Zunger 1981 local correlation, Perdew 1986 nonlocal gradient correction |
|
|
Perdew-Wang GGA‑II 1991 local and nonlocal correlation |
|
|
Lee-Yang-Parr local and nonlocal correlation |