At present the RASCI1 and RASCI2 implementations employ different keywords (which will be reconciled in a future version). This subsection applies to RASCI1 (spin adapted algorithm using exact integrals).
The use of the RAS-CI1 methodology is controlled by setting the $rem variable CORRELATION to RASCI and EXCHANGE should be set to HF. The RASCI1 implementation is only compatible with even numbers of electrons and restricted orbitals, i.e., UNRESTRICTED = FALSE.
The minimum input also requires specifying the desired (non-zero) value for RAS_ROOTS, the number of electrons in the “active” RAS2 space and the number of orbitals in RAS1 and RAS2 subspaces.
RAS_ROOTS
RAS_ROOTS
Sets the number of RAS-CI roots to be computed.
TYPE:
INTEGER
DEFAULT:
None
OPTIONS:
Compute RAS-CI states
RECOMMENDATION:
None. Only works with RASCI.
RAS_ELEC
RAS_ELEC
Sets the number of electrons in RAS2 (active electrons).
TYPE:
INTEGER
DEFAULT:
None
OPTIONS:
User-defined integer,
RECOMMENDATION:
None. Only works with RASCI.
RAS_ELEC_ALPHA
RAS_ELEC_ALPHA
Sets the number of spin- electrons in RAS2 (active electrons).
TYPE:
INTEGER
DEFAULT:
None
OPTIONS:
User-defined integer,
RECOMMENDATION:
None. Only works with RASCI.
RAS_ELEC_BETA
RAS_ELEC_BETA
Sets the number of spin- electrons in RAS2 (active electrons).
TYPE:
INTEGER
DEFAULT:
None
OPTIONS:
User-defined integer,
RECOMMENDATION:
None. Only works with RASCI.
RAS_ACT
RAS_ACT
Sets the number of orbitals in RAS2 (active orbitals).
TYPE:
INTEGER
DEFAULT:
None
OPTIONS:
User-defined integer,
RECOMMENDATION:
None. Only works with RASCI.
RAS_OCC
RAS_OCC
Sets the number of orbitals in RAS1
TYPE:
INTEGER
DEFAULT:
0
OPTIONS:
User-defined integer,
RECOMMENDATION:
These are the initial doubly occupied orbitals (RAS1) before
including type of excitations.
The RAS1 space starts from the lowest orbital up to RAS_OCC,
i.e. no frozen orbitals option available yet. Only works with RASCI.
RAS_DO_HOLE
RAS_DO_HOLE
Controls the presence of hole excitations in the RAS-CI wave function.
TYPE:
LOGICAL
DEFAULT:
TRUE
OPTIONS:
TRUE
Include hole configurations (RAS1 to RAS2 excitations)
FALSE
Do not include hole configurations
RECOMMENDATION:
None. Only works with RASCI.
RAS_DO_PART
RAS_DO_PART
Controls the presence of particle excitations in the RAS-CI wave function.
TYPE:
LOGICAL
DEFAULT:
TRUE
OPTIONS:
TRUE
Include particle configurations (RAS2 to RAS3 excitations)
FALSE
Do not include particle configurations
RECOMMENDATION:
None. Only works with RASCI.
RAS_AMPL_PRINT
RAS_AMPL_PRINT
Defines the absolute threshold () for the CI amplitudes to be printed.
TYPE:
INTEGER
DEFAULT:
10
0.1 minimum absolute amplitude
OPTIONS:
User-defined integer,
RECOMMENDATION:
None. Only works with RASCI.
RAS_ACT_ORB
RAS_ACT_ORB
Sets the user-selected active orbitals (RAS2 orbitals).
TYPE:
INTEGER ARRAY
DEFAULT:
From RAS_OCC+1 to RAS_OCC+RAS_ACT
OPTIONS:
The number of orbitals must be equal to the RAS_ACT variable
RECOMMENDATION:
None. Only works with RASCI.
RAS_NATORB
RAS_NATORB
Controls the computation of the natural orbital occupancies.
TYPE:
LOGICAL
DEFAULT:
FALSE
OPTIONS:
TRUE
Compute natural orbital occupancies for all states
FALSE
Do not compute natural orbital occupancies
RECOMMENDATION:
None. Only works with RASCI.
RAS_NATORB_STATE
RAS_NATORB_STATE
Saves the natural orbitals of the -th RASCI computed state into the .fchk file.
TYPE:
INTEGER
DEFAULT:
0
OPTIONS:
Saves the natural orbitals for the -th state
RECOMMENDATION:
None. Only works with RASCI and if GUI = 2.
RAS_GUESS_CS
RAS_GUESS_CS
Controls the number of closed shell guess configurations in RAS-CI.
TYPE:
INTEGER
DEFAULT:
0
OPTIONS:
Imposes to start with closed shell guesses
RECOMMENDATION:
Only relevant for the computation of singlet states. Only works with RASCI.
RAS_SPIN_MULT
RAS_SPIN_MULT
Specifies the spin multiplicity of the roots to be computed
TYPE:
INTEGER
DEFAULT:
1
Singlet states
OPTIONS:
0
Compute any spin multiplicity
User-defined integer,
RECOMMENDATION:
RAS_SPIN_MULT option is only available for systems, that is, with the same number of
and electrons.
RAS_PT2
RAS_PT2
Perform second-order perturbative correction to RAS-CI energy
TYPE:
LOGICAL
DEFAULT:
FALSE
OPTIONS:
TRUE
Compute RASCI(2) energy corrections
FALSE
Do not compute RASCI(2) energy corrections
RECOMMENDATION:
None. Only works with RASCI.
RAS_PT2_PARTITION
RAS_PT2_PARTITION
Specifies the partitioning scheme in RASCI(2)
TYPE:
INTEGER
DEFAULT:
1
Davidson-Kapuy (DK) partitioning
OPTIONS:
2
Epstein-Nesbet (EN) partitioning
0
Do both DK and EN partitionings
RECOMMENDATION:
Only for RASCI if RAS_PT2 is set to true.
RAS_PT2_VSHIFT
RAS_PT2_VSHIFT
Defines the energy level shift () in RASCI(2)
TYPE:
INTEGER
DEFAULT:
0
OPTIONS:
User-defined integer
RECOMMENDATION:
Only for RASCI if RAS_PT2 is set to true.
RAS_SRDFT
RAS_SRDFT
Perform short-range density functional RAS-CI calculation
TYPE:
LOGICAL
DEFAULT:
FALSE
OPTIONS:
TRUE
Compute RASCI-DFT states and energies
FALSE
Do not perform a RASCI-DFT calculation
RECOMMENDATION:
None. Only works with RASCI.
RAS_SRDFT_EXC and RAS_SRDFT_COR need to be set.
RAS_SRDFT_EXC
RAS_SRDFT_EXC
Define short-range exchange functional
TYPE:
STRING
DEFAULT:
No default
OPTIONS:
NAME
Use RAS_SRDFT_EXC = NAME, where NAME is
one of the short-range exchange functionals listed in
Section 5.3.3
RECOMMENDATION:
None. Only works with RASCI.
RAS_SRDFT_COR
RAS_SRDFT_COR
Define short-range correlation functional
TYPE:
STRING
DEFAULT:
No default
OPTIONS:
NAME
Use RAS_SRDFT_COR = NAME, where NAME is
one of the short-range correlation functionals listed in Section 5.3.4
RECOMMENDATION:
None. Only works with RASCI.
RAS_OMEGA
RAS_OMEGA
Sets the Coulomb range-separation parameter within the RAS-CI-DFT method.
TYPE:
INTEGER
DEFAULT:
400
( bohr)
OPTIONS:
Corresponding to , in units of bohr
RECOMMENDATION:
None. Range-separation parameter is typical indicated by or . Only works with RASCI.
RAS_SRDFT_DAMP
RAS_SRDFT_DAMP
Sets damping factor () in the RAS-CI-DFT method.
TYPE:
REAL
DEFAULT:
0.5
()
OPTIONS:
Damping factor
RECOMMENDATION:
Modify in case of convergence issues along the RAS-CI-DFT iterations. Only works with RASCI
RAS_SRDFT_SA_ROOTS
RAS_SRDFT_SA_ROOTS
Sets the list of roots used to build the state averaged reference density in RAS-CI-srDFT.
TYPE:
INTEGER ARRAY
DEFAULT:
All computed states
OPTIONS:
List of states.
RECOMMENDATION:
None. Only works with RASCI
RAS_NFRAG
RAS_NFRAG
If activates the excitation analysis in RASCI
TYPE:
INTEGER
DEFAULT:
0
OPTIONS:
Number of fragments to be considered
RECOMMENDATION:
Only for RASCI. The printed information level is controlled by RAS_PRINT
RAS_NFRAG_ATOMS
RAS_NFRAG_ATOMS
Sets the number of atoms in each fragment.
TYPE:
INTEGER ARRAY
DEFAULT:
None
OPTIONS:
The sum of the numbers must be equal to the total number
of atoms in the systems
RECOMMENDATION:
None. Only works with RASCI.
RAS_FRAG_SETS
RAS_FRAG_SETS
Defines the number of orbitals in each disjoint set to perform orbital localization.
TYPE:
INTEGER ARRAY
DEFAULT:
[NOcc,NAct,NVir]
Number of orbitals within RAS1, RAS2 and RAS3 spaces
OPTIONS:
Defines sets of canonical MOs to be localized into fragments
RECOMMENDATION:
Setting within RAS1, RAS2 and RAS3 spaces alleviates the computational
cost of the localization procedure. It might also result in improved fragment
orbitals. Only works with RASCI.
CALC_SOC
CALC_SOC
Controls whether to calculate the SOC constants for EOM-CC, RAS-CI, ADC, TDDFT/TDA and TDDFT.
TYPE:
INTEGER/LOGICAL
DEFAULT:
FALSE
OPTIONS:
FALSE
Do not perform the SOC calculation.
TRUE
Perform the SOC calculation.
RECOMMENDATION:
Although TRUE/FALSE values will work, EOM-CC code has more variants of SOC evaluations. For details, consult with EOM section.
RAS_SOC_2E
RAS_SOC_2E
Controls whether to compute two-electron mean-field contribution to RAS-CI SOC.
TYPE:
LOGICAL
DEFAULT:
TRUE
OPTIONS:
FALSE
Do not compute two-electron mean-field contribution.
TRUE
Compute two-electron mean-field contribution.
RECOMMENDATION:
None.
RAS_SOC_SYM_DENS
RAS_SOC_SYM_DENS
Controls whether to perform averaging of and densities.
TYPE:
LOGICAL
DEFAULT:
FALSE
OPTIONS:
FALSE
Do not average and densities .
TRUE
Average and densities.
RECOMMENDATION:
None.