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PSI3 can perform ab initio computations employing
basis sets of up to 32768 contracted Gaussian-type functions of
virtually arbitrary orbital quantum number.
PSI3 can recognize and exploit the largest Abelian subgroup of the
point group describing the full symmetry of the molecule.
Table 2 displays the range of theoretical
methods available in PSI3.
Table 2:
Summary of theoretical methods available in PSI3.
| Method |
Energy |
Gradient |
Hessian |
| RHF SCF |
Y |
Y |
Y |
| ROHF SCF |
Y |
Y |
N |
| UHF SCF |
Y |
N |
N |
| HF DBOC |
Y |
N |
N |
| CIS/RPA/TDHF |
Y |
N |
N |
| TCSCF |
Y |
Y |
N |
| CASSCF |
Y |
Y |
N |
| RASSCF |
Y |
Y |
N |
| RAS-CI |
Y |
N |
N |
| RAS-CI DBOC |
Y |
N |
N |
| RHF MP2 |
Y |
Y |
N |
| UHF/ROHF MP2 |
Y |
N |
N |
| RHF MP2-R12 |
Y |
N |
N |
| RHF/UHF/ROHF CCSD |
Y |
Y |
N |
| RHF/UHF/ROHF CCSD(T) |
Y |
Y |
N |
| RHF/UHF/ROHF EOM-CCSD |
Y |
Y |
N |
CCSD(T) gradients implemented only via an experimental
code. A more efficient and robust implementation will appear in the next
release.
Geometry optimization (currently restricted to true minima on the potential
energy surface) can be performed using either analytic gradients
or energy points. Likewise, vibrational frequencies can be
computed using analytic second derivatives, by finite
differences of analytic gradients, or finite differences of energies.
PSI3 can also compute an extensive list of one-electron properties.
Next: Technical Support
Up: Introduction
Previous: Supported Architectures
Contents
T. Daniel Crawford
2009-02-16