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III.F.2.

Completed calculations for NO3+ (nitrogen trioxide cation)

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 c1ov
PM3 c1ov c2o
composite G1 c1e c2e
G2MP2 c1e c2e
G2 c1e c2e
G3 c1e c2e
G3B3 c1e c2e
G4 c1e c2e
CBS-Q c1e c2e

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) TZVP cc-pVDZ cc-pVTZ cc-pVQZ aug-cc-pVDZ aug-cc-pVTZ aug-cc-pVQZ
hartree fock HF c1ov c2ov c1ov c2ov c1ov c2ov c1ov c2ov c1ov c2o c1ov c2o c1ov c2o c1ov c2o c1ov c2o c1ov c2o c1ov c2o c1ov c2o c1ov c2o c1ov c2o c1ov c2o c1ov c2o c1ov c2o
ROHF c1ov c2ov c1ov c2ov c1ov c2ov c2ov c1ov c2o c1ov c2o c1ov c2o c1ov c2o c1ov c2o c1ov c2o   c1ov c2o c1ov c2o c1ov c2o c1ov c2o c1ov c2o c1ov c2o
density functional LSDA c1ov c2ov c1ov c2ov c1ov c2ov c1ov c2ov c1ov c2ov c1ov c2ov c1ov c2ov c1ov c2ov c1ov c2ov c1ov c2ov c1ov c1ov c2ov c1ov c2ov c1ov c2ov c1ov c2ov c1ov c2ov c1ov c2ov
SVWN   c1ov     c1ov c1ov c1ov c1ov c1ov c1ov   c1ov c1ov   c1ov c1ov  
BLYP c1ov c2ov c1ov c2ov c1ov c2ov c1ov c2ov c1ov c2ov c1ov c2ov c1ov c2ov c1ov c2ov c1ov c2ov c1ov c2ov c1ov c1ov c2ov c1ov c2ov        
B1B95 c1o c2o c1o c2o c1o c2o c1ov c2ov c1ov c2ov c1ov c2ov c1ov c2ov c1ov c2ov c1ov c2ov c1ov c2ov c1ov c1ov c2ov c1ov c2ov c1ov c2ov c1ov c2ov c1ov c2ov c1ov c2ov
B3LYP c1o c2o c1o c2o c1o c2o c1ov c2ov c1ov c2ov c1ov c2ov c1ov c2ov c1ov c2ov c1ov c2ov c1ov c2ov c1ov c2ov c1ov c2ov c1ov c2ov c1ov c2ov c1ov c2ov c1ov c2ov c1ov c2ov
B3LYPultrafine         c1ov c2dnfv             c1ov c1ov   c1ov c1ov c2ov  
B3PW91 c1o c2o c1o c2o c1o c2o c1ov c2ov c1ov c2ov c1ov c2ov c1ov c2ov c1ov c2ov c1ov c2ov c1ov c2ov c1ov c1ov c2ov c1ov c2ov        
mPW1PW91 c1o c2o c1o c2o c1o c2o c1ov c2ov c1ov c2ov c1ov c2ov c1ov c2ov c1ov c2ov c1ov c2ov c1ov c2ov c1ov c1ov c2ov c1ov c2ov   c1ov c1ov  
M06-2X c1ov c1ov c1ov c1ov c1ov c1ov c1ov c1ov c1ov c1ov c1ov c1ov c1ov   c1ov c1ov  
PBEPBE c1ov c2ov c1ov c2ov c1ov c2ov c1ov c2ov c1ov c2ov c1ov c2ov c1ov c2ov c1ov c2ov c1ov c2ov c1ov c2ov c1ov c1ov c2ov c1ov c2ov c1ov c2ov c1ov c1ov c1ov c2ov
PBEPBEultrafine         c1ov             c1ov c1ov   c1ov c1ov  
PBE1PBE c1ov c1ov c1ov c1ov c1ov c1ov c1ov c1ov c1ov c1ov c1ov c1ov c1ov   c1ov c1ov  
HSEh1PBE c1ov c1ov c1ov c1ov c1ov c1ov c1ov c1ov c1ov c1ov c1ov c1ov c1ov   c1ov c1ov  
TPSSh         c1ov c2ov   c1ov c2ov                    
Moller Plesset perturbation MP2 c1o c2ov c1ov c2ov c1ov c2ov c1ov c2ov c1ov c2ov c1ov c2ov c1ov c2ov c1ov c2ov c1ov c2ov c1ov c2ov c1ov c2ov c1ov c2ov c1ov c2ov   c1ov c2ov c1ov  
MP2=FULL c1o c2ov c1ov c2ov c1ov c2ov c1ov c2ov c1ov c2ov c1ov c2ov c1ov c2ov c1ov c2ov c1ov c2ov c1ov c2ov c1ov c1ov c2ov c1ov c2ov   c1ov c1ov  
ROMP2 c1o c2o c1ov c2ov c1ov c2ov c1ov c2ov c1ov c2o c1ov c2o c1ov c2o c1ov c1ov c1ov   c1ov     c1ov c1ov  
MP3         c1ov c2ov   c1o c2o                    
MP3=FULL         c1ov c2ov   c1ov c2ov                    
MP4   c1ov c2o     c1ov c2o       c1ov c2o   c1ov c1ov c1ov   c1ov c1ov  
MP4=FULL   c1ov     c1ov       c1ov     c1ov c1ov   c1ov c1ov  
Configuration interaction CID   c1ov c2ov c1ov c2ov c1ov c2ov c1ov c2ov     c1ov c2dnfv                  
CISD   c1ov c2ov c1ov c2ov c1ov c2ov c1ov c2dnfv     c1ov c2ov                  
Quadratic configuration interaction QCISD   c1ov c2o c1ov c2o c1o c2o c1ov c2o c1ov c2o c1ov c2o c1ov c2o c1ov c2o c1ov c1ov c1ov c2o c1ov   c1ov c1ov  
QCISD(T)         c1ov c2o           c1ov c1ov c2o c1ov c2o   c1ov c2o c1ov  
Coupled Cluster CCD   c1ov c2ov c1ov c2ov c1ov c2ov c1ov c2ov c1ov c2ov c1ov c2ov c1ov c2ov c1ov c2ov c1ov c1ov c1ov c2ov c1ov   c1ov c2ov c1ov  
CCSD         c1o c2o           c1ov c1ov c1ov   c1ov c1ov  
CCSD=FULL         c1ov           c1ov c1ov c1ov   c1ov c1ov  
CCSD(T)         c1ov c2o           c1ov c1ov c2o c1ov c2o   c1ov c2o c1ov  
CCSD(T)=FULL         c1ov           c1ov c1ov c1ov   c1ov c1ov  

Methods with effective core potentials (select basis sets)
CEP-31G CEP-31G* CEP-121G CEP-121G* LANL2DZ SDD
hartree fock HF c1ov c2ov c1ov c2o c1ov c2ov c1ov c2o c1ov c2ov c1ov c2ov
density functional B3LYP c1ov c2ov c1ov c2dnfv c1ov c2ov c1ov c2ov c1ov c2ov c1ov c2ov
Moller Plesset perturbation MP2 c1ov c2ov c1ov c2ov c1ov c2ov c1ov c2ov c1ov c2ov c1ov c2ov

Single point energy calculations (select basis sets)
aug-cc-pVTZ
Moller Plesset perturbation MP2FC// MP2FC/6-31G* c2e
Coupled Cluster CCSD// MP2FC/6-31G* c2e
CCSD(T)// MP2FC/6-31G* c2e
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.