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 CH3COCH2CH3 (2-Butanone)

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 PM3 c1o c2ov
composite G1 c1e
G2MP2 c1e
G2 c1e c2e
G3 c1e
G3B3 c1e
G3MP2 c1e
G4 c1e
CBS-Q c1e

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 aug-cc-pVDZ aug-cc-pVTZ cc-pV(T+d)Z daug-cc-pVTZ
hartree fock HF c1ov c1ov c1ov c1ov c1ov c1ov c1ov c2ov c2ov c2ov c2ov c1ov c1o c2ov c1ov c1ov c2ov c2ov c1ov c1ov c2ov
density functional BLYP c2ov c2ov c2ov c2ov c1o c2ov c2ov c2ov c2ov c2ov     c2ov c2ov c2ov   c2ov  
B1B95 c2ov c2ov c2ov c2ov c2ov c2ov c2ov c2ov c2ov c2ov     c2ov c2ov c2ov c1o c2ov  
B3LYP c2ov c2ov c2ov c2ov c2ov c2ov c2ov c2ov c2ov c1o c2ov c1o c2ov c2ov c2ov c2ov c1o c2ov  
B3LYPultrafine         c2ov                 c1ov   c1o    
B3PW91 c2ov c2ov c2ov c2ov c2ov c2ov c2ov c2ov c2ov c2ov     c2ov c2ov c2ov   c2ov  
mPW1PW91 c2ov c2ov c2ov c2ov c2ov c2ov c2ov c2ov c2ov c2ov     c2ov c2ov c2ov   c2ov  
M06-2X     c1o c2ov   c1o           c1o              
PBEPBE c2ov c2ov         c2ov c2ov c2ov   c1ov c2ov     c2ov     c2ov  
PBEPBEultrafine         c1ov                          
PBE1PBE         c1o                          
HSEh1PBE   c1o     c1o   c1o             c1o        
TPSSh         c1o   c1o     c1ov c2ov       c1o        
wB97X-D     c1o c2o   c1o c2o   c1o c2o   c1o c2o     c1o c2o c1o c2o c1o c2o   c1o c2o    
B97D3   c1o c2o     c1o c2o   c1o c2o   c1o c2o   c1o c2o c1o c2o   c1o c2o   c1o c2o   c1o
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 aug-cc-pVDZ aug-cc-pVTZ cc-pV(T+d)Z daug-cc-pVTZ
Moller Plesset perturbation MP2 c1ov c1ov c1ov c1ov c1ov c2ov c1ov c2ov c1o c2o c2ov c1ov   c1o c2ov c1ov c1o c2ov c2ov c1o c2ov  
MP2=FULL   c2ov c2ov c2ov c1ov c2ov c2ov c2ov c2ov c2ov       c2ov c1ov c2ov     c2ov  
MP3         c2ov   c1o                      
MP3=FULL         c1ov   c1o                      
MP4         c2o                          
B2PLYP         c1ov                 c1o        
B2PLYP=FULLultrafine         c1ov               c1ov c1ov   c1o    
Configuration interaction CID         c2ov                          
CISD         c2ov                          
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 aug-cc-pVDZ aug-cc-pVTZ cc-pV(T+d)Z daug-cc-pVTZ
Quadratic configuration interaction QCISD   c2ov c2ov c2ov c2ov c2ov   c2ov c2ov       c2ov          
Coupled Cluster CCD   c2ov c2ov c2ov c1ov c2ov c2ov   c2ov         c2ov          
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 aug-cc-pVDZ aug-cc-pVTZ cc-pV(T+d)Z 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 c2ov c2ov c2ov c2ov c2ov c2ov     c1ov c2ov
density functional B1B95 c2ov                
B3LYP c2ov c2ov c2ov c2ov c2ov c2ov     c1o c2ov
PBEPBE                 c1o c2o
Moller Plesset perturbation MP2 c2ov c2ov c2ov c2ov c2ov c2ov     c1o c2o

Single point energy calculations (select basis sets)
6-311+G(3df,2p) cc-pVDZ aug-cc-pVDZ aug-cc-pVTZ
Moller Plesset perturbation MP2FC// HF/6-31G* c1e c1e    
MP2FC// MP2FC/6-31G*     c1e c1e
Coupled Cluster CCSD(T)// HF/6-31G*   c1e    
CCSD// MP2FC/6-31G*       c1e
CCSD(T)// MP2FC/6-31G* c1e     c1e

Barriers to internal rotation or inversion


Methods with predefined basis sets
semi-empirical AM1 s1c1t1
PM3 s1c1t1

Methods with standard basis sets
3-21G 6-31G* 6-31+G** cc-pVTZ
hartree fock HF s1c1t1 s1c1t1 s1c1t1 s1c1t1
density functional B3LYP s1c1t1 s1c1t1 s1c1t1  
3-21G 6-31G* 6-31+G** cc-pVTZ
Moller Plesset perturbation MP2 s1c1t1 s1c1t1 s1c1t1  
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.