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Completed calculations for GeBr4 (Germanium tetrabromide)

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 ov
PM3 ov
composite G3 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 aug-cc-pVDZ aug-cc-pVTZ
hartree fock HF 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 ov ov
B1B95 ov 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
B3LYPultrafine   ov     ov ov ov ov   ov ov ov ov ov ov ov
B3PW91 ov 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 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 ov
PBEPBEultrafine   ov     ov 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 ov
HSEh1PBE ov 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 ov ov ov ov
wB97X-D ov ov ov ov ov ov ov ov ov ov ov ov ov ov ov ov
B97D3 ov ov ov ov ov ov ov 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 aug-cc-pVDZ aug-cc-pVTZ
Moller Plesset perturbation MP2                     o          
MP2=FULL ov ov ov ov ov ov ov ov ov ov ov ov ov ov ov ov
B2PLYP ov ov ov ov ov ov ov ov ov ov o ov ov ov ov ov
B2PLYP=FULL ov ov ov ov ov ov ov ov ov ov ov ov ov ov ov ov
B2PLYP=FULLultrafine ov ov ov ov ov ov ov ov ov ov ov ov ov ov ov o
Configuration interaction CID   ov ov ov ov     ov     ov   ov ov    
CISD   ov ov ov ov     ov     ov   ov ov    
Quadratic configuration interaction QCISD(T)         ov     ov     o ov ov o ov o
Coupled Cluster CCSD         ov ov ov ov ov ov ov ov ov ov ov o
CCSD(T)         ov ov ov ov ov ov ov ov ov ov 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 aug-cc-pVDZ aug-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
density functional LSDA             ov    
BLYP             ov   ov
B1B95             ov   ov
B3LYP ov   ov   ov ov ov   ov
B3LYPultrafine             ov   ov
B3PW91             ov   ov
mPW1PW91             ov   ov
M06-2X             ov   ov
PBEPBE             ov   ov
PBEPBEultrafine             ov   ov
PBE1PBE             ov   ov
HSEh1PBE             ov   ov
TPSSh             ov   ov
wB97X-D ov   ov   ov ov ov   ov
B97D3             ov   ov
Moller Plesset perturbation MP2=FULL             ov   ov
B2PLYP             ov   ov
B2PLYP=FULL             ov   ov
B2PLYP=FULLultrafine             ov   ov
Configuration interaction CID             ov    
CISD             ov   ov
Quadratic configuration interaction QCISD(T)             ov   ov
Coupled Cluster CCSD             ov   ov
CCSD(T)             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.