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Completed calculations for B4H10 (Tetraborane(10))

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 dnf
PM3 dnf
composite G1 e
G2MP2 e
G2 e
G3 e
G3B3 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 aug-cc-pVQZ daug-cc-pVTZ
hartree fock HF o ov ov ov ov ov ov ov ov ov   ov ov ov ov ov ov ov ov
density functional LSDA ov ov ov ov ov ov ov ov ov ov   ov ov ov   ov ov    
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   o ov    
B3LYP ov ov ov ov ov ov ov ov ov ov   ov ov ov ov ov ov ov  
B3LYPultrafine   ov     ov ov ov ov       ov ov ov   ov ov    
B3PW91 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 ov    
M06-2X ov ov ov ov ov ov ov ov ov ov ov ov ov ov   ov ov    
PBEPBE ov ov ov ov ov ov ov ov ov ov   ov ov ov   ov ov    
PBEPBEultrafine   ov     ov ov ov ov       ov ov ov   ov ov    
PBE1PBE ov ov ov ov ov ov ov ov ov ov   ov ov ov   ov ov    
HSEh1PBE ov ov ov ov ov ov ov ov ov ov   ov ov ov   ov ov    
TPSSh   ov ov ov ov ov ov ov       ov ov ov   ov ov    
B97D3                     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 aug-cc-pVQZ daug-cc-pVTZ
Moller Plesset perturbation MP2 ov ov ov ov ov ov ov ov ov ov   ov ov ov ov ov ov o  
MP2=FULL ov ov ov ov ov ov ov ov ov ov   ov ov ov ov ov ov o  
MP3         ov   ov         ov ov o          
MP3=FULL         ov   ov         ov ov o          
MP4   ov     ov       ov     ov ov ov   ov o    
MP4=FULL   ov     ov       ov       ov ov   ov o    
B2PLYP ov ov ov ov ov ov ov ov ov ov   ov ov ov   ov o    
B2PLYP=FULL ov ov ov ov ov ov ov ov ov ov   ov ov ov   ov ov    
B2PLYP=FULLultrafine         ov               ov ov     ov    
Configuration interaction CID   ov ov ov ov     ov                      
CISD   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 aug-cc-pVQZ daug-cc-pVTZ
Quadratic configuration interaction QCISD   ov ov ov ov ov ov ov ov ov   ov ov ov   dnf o    
QCISD(T)         ov             ov ov ov   ov o    
QCISD(T)=FULL         ov   ov           ov ov   ov o    
Coupled Cluster CCD   ov ov ov ov ov ov ov ov ov   ov ov o   ov o    
CCSD         ov         ov   ov ov ov   ov o    
CCSD=FULL         ov         ov   ov ov dnf dnf ov dnf    
CCSD(T)         ov             ov ov ov   o o    
CCSD(T)=FULL         ov             ov ov o   ov o    
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 aug-cc-pVQZ 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 B3LYP ov ov ov ov ov ov     ov
PBEPBE                 ov
Moller Plesset perturbation MP2 ov ov ov ov ov ov     ov
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.