National Institute of Standards and Technology
Computational Chemistry Comparison and Benchmark DataBase
Release 22May 2022
NIST Standard Reference Database 101
IIntroduction
IIExperimental data
IIICalculated data
IVData comparisons
VCost comparisons
VIInput and output files
VIITutorials and Units
VIIILinks to other sites
IXFeedback
XOlder CCCBDB versions
XIIGeometries
XIII Vibrations
XIVReaction data
XVEntropy data
XVIBibliographic data
XVIIIon data
XVIIIBad calculations
XIXIndex of properties
XXH-bond dimers
XXIOddities

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III.F.2.

Completed calculations for CH3NHCH3 (Dimethylamine)

Methods and basis sets for which an energy has been calculated. "e" indicates just an energy has been calculated. "o" indicates an optimized geometry. "v" indicates vibrational frequencies. "s" followed by a number indicates completed calculations for different states (for example s1ov). "c" followed by a number indicates completed calculations for different conformations (for example c2ov).
See the Calculated Energies page (section III.A.1) for more calculated properties.
Methods with predefined basis sets
semi-empirical AM1 o
PM3 ov
composite G1 e
G2MP2 e
G2 e
G3 e
G3B3 e
G3MP2 e
G4 e
CBS-Q e

Methods with standard basis sets
STO-3G 3-21G 3-21G* 6-31G 6-31G* 6-31G** 6-31+G** 6-311G* 6-311G** 6-31G(2df,p) 6-311+G(3df,2p) TZVP cc-pVDZ cc-pVTZ cc-pVQZ aug-cc-pVDZ aug-cc-pVTZ cc-pV(T+d)Z Sadlej_pVTZ daug-cc-pVTZ
hartree fock HF ov ov ov ov ov ov ov ov ov ov ov ov ov ov ov ov ov ov ov ov
density functional BLYP ov ov ov ov ov ov ov ov ov ov     ov ov   ov   ov    
B1B95 ov ov ov ov ov ov ov ov ov ov     ov ov   ov ov ov    
B3LYP ov ov ov ov ov ov ov ov ov ov ov ov ov ov   ov ov ov ov  
B3LYPultrafine         ov   ov             ov     ov      
B3PW91 ov ov ov ov ov ov ov ov ov ov     ov ov   ov ov ov    
mPW1PW91 ov ov ov ov ov ov ov ov ov ov     ov ov   ov   ov    
M06-2X     ov   ov         ov ov     ov     ov      
PBEPBE ov ov ov ov ov ov ov ov ov ov ov   ov ov   ov ov ov ov  
PBEPBEultrafine         ov                              
PBE1PBE         ov                              
HSEh1PBE   ov     ov   ov             ov            
TPSSh         ov   ov     ov       ov            
wB97X-D     ov   ov   ov   ov     ov ov ov     ov      
B97D3   ov     ov   ov   ov   ov ov   ov     ov     ov
STO-3G 3-21G 3-21G* 6-31G 6-31G* 6-31G** 6-31+G** 6-311G* 6-311G** 6-31G(2df,p) 6-311+G(3df,2p) TZVP cc-pVDZ cc-pVTZ cc-pVQZ aug-cc-pVDZ aug-cc-pVTZ cc-pV(T+d)Z Sadlej_pVTZ daug-cc-pVTZ
Moller Plesset perturbation MP2 ov ov ov ov ov ov ov ov ov ov   ov ov ov   ov ov ov ov  
MP2=FULL   ov     ov ov ov ov ov ov     ov ov     ov   ov  
MP3         ov   o                          
MP3=FULL         ov   ov                          
MP4         ov                              
B2PLYP         ov         ov       ov     ov      
B2PLYP=FULLultrafine         ov               ov ov     ov      
Configuration interaction CID         ov                              
CISD   ov     ov ov                            
STO-3G 3-21G 3-21G* 6-31G 6-31G* 6-31G** 6-31+G** 6-311G* 6-311G** 6-31G(2df,p) 6-311+G(3df,2p) TZVP cc-pVDZ cc-pVTZ cc-pVQZ aug-cc-pVDZ aug-cc-pVTZ cc-pV(T+d)Z Sadlej_pVTZ daug-cc-pVTZ
Quadratic configuration interaction QCISD   ov     ov ov ov ov   ov     ov ov     o      
QCISD(T)         ov                              
Coupled Cluster CCD         ov               ov              
CCSD         ov         ov       ov     o      
CCSD=FULL         ov         ov       ov     o      
CCSD(T)         ov ov                            
STO-3G 3-21G 3-21G* 6-31G 6-31G* 6-31G** 6-31+G** 6-311G* 6-311G** 6-31G(2df,p) 6-311+G(3df,2p) TZVP cc-pVDZ cc-pVTZ cc-pVQZ aug-cc-pVDZ aug-cc-pVTZ cc-pV(T+d)Z Sadlej_pVTZ daug-cc-pVTZ

Methods with effective core potentials (select basis sets)
CEP-31G CEP-31G* CEP-121G CEP-121G* LANL2DZ SDD cc-pVTZ-PP aug-cc-pVTZ-PP Def2TZVPP
hartree fock HF ov ov ov ov ov ov     ov
density functional B1B95 ov ov              
B3LYP ov ov ov ov ov ov     ov
PBEPBE                 ov
Moller Plesset perturbation MP2 ov ov ov ov ov ov     ov

Single point energy calculations (select basis sets)
6-311+G(3df,2p) cc-pVDZ cc-pVTZ aug-cc-pVDZ aug-cc-pVTZ cc-pV(T+d)Z
Moller Plesset perturbation MP2FC// HF/6-31G* e e e e e e
MP2FC// B3LYP/6-31G* e e e e e e
MP2FC// MP2FC/6-31G*   e e e e e
MP4// HF/6-31G* e e e     e
MP4// B3LYP/6-31G*   e e     e
MP4// MP2/6-31G*     e     e
Coupled Cluster CCSD// HF/6-31G* e e e e   e
CCSD(T)// HF/6-31G* e e e e   e
CCSD// B3LYP/6-31G*   e e     e
CCSD(T)// B3LYP/6-31G*   e e     e
CCSD(T)//B3LYP/6-31G(2df,p)     e     e
CCSD// MP2FC/6-31G*   e e e e e
CCSD(T)// MP2FC/6-31G*   e e e e e

Barriers to internal rotation or inversion


Methods with predefined basis sets
semi-empirical AM1 s1c1t2
PM3 s1c1t2

Methods with standard basis sets
3-21G 6-31G* 6-31+G** cc-pVTZ
hartree fock HF s1c1t2 s1c1t2 s1c1t2 s1c1t2
density functional B3LYP s1c1t2 s1c1t2 s1c1t2 s1c1t2
3-21G 6-31G* 6-31+G** cc-pVTZ
Moller Plesset perturbation MP2 s1c1t2 s1c1t2 s1c1t2 s1c1t2
3-21G 6-31G* 6-31+G** cc-pVTZ
For descriptions of the methods (AM1, HF, MP2, ...) and basis sets (3-21G, 3-21G*, 6-31G, ...) see the glossary in section I.C. Predefined means the basis set used is determined by the method.