N_FROZEN_CORE
N_FROZEN_CORE
Controls the number of frozen core orbitals.
TYPE:
INTEGER/STRING
DEFAULT:
0
No frozen core orbitals.
OPTIONS:
FC
Frozen core approximation.
Freeze core orbitals.
RECOMMENDATION:
There is no computational advantage to using frozen core for CIS, and
analytical derivatives are only available when no orbitals are frozen. It is
helpful when calculating CIS(D) corrections (see Sec. 7.10).
N_FROZEN_VIRTUAL
N_FROZEN_VIRTUAL
Controls the number of frozen virtual orbitals.
TYPE:
INTEGER
DEFAULT:
0
No frozen virtual orbitals.
OPTIONS:
Freeze virtual orbitals.
RECOMMENDATION:
There is no computational advantage to using frozen virtuals for CIS, and
analytical derivatives are only available when no orbitals are frozen.
MAX_CIS_CYCLES
MAX_CIS_CYCLES
Maximum number of CIS iterative cycles allowed.
TYPE:
INTEGER
DEFAULT:
30
OPTIONS:
User-defined number of cycles.
RECOMMENDATION:
Default is usually sufficient.
MAX_CIS_SUBSPACE
MAX_CIS_SUBSPACE
Maximum number of subspace vectors allowed in the CIS iterations
TYPE:
INTEGER
DEFAULT:
As many as required to converge all roots
OPTIONS:
User-defined number of subspace vectors
RECOMMENDATION:
The default is usually appropriate, unless a large number of states are
requested for a large molecule. The total memory required to store the
subspace vectors is bounded above by , where and represent the
number of occupied and virtual orbitals, respectively. can be reduced to
save memory, at the cost of a larger number of CIS iterations. Convergence may
be impaired if is not much larger than CIS_N_ROOTS.
CIS_CONVERGENCE
CIS_CONVERGENCE
CIS is considered converged when error is less than
TYPE:
INTEGER
DEFAULT:
6
CIS convergence threshold 10
OPTIONS:
Corresponding to
RECOMMENDATION:
None
CIS_DYNAMIC_MEM
CIS_DYNAMIC_MEM
Controls whether to use static or dynamic memory in CIS and TDDFT calculations.
TYPE:
LOGICAL
DEFAULT:
FALSE
OPTIONS:
FALSE
Partly use static memory
TRUE
Fully use dynamic memory
RECOMMENDATION:
The default control requires static memory (MEM_STATIC) sufficient
to hold an array whose size grows by
at each CIS iteration, where
is the number of unconverged roots ( CIS_N_ROOTS).
For a large calculation, one has to specify a large value for MEM_STATIC,
which is not recommended (see Chapter 2). Therefore, it is
recommended to use dynamic memory for large calculations.
CIS_RELAXED_DENSITY
CIS_RELAXED_DENSITY
Use the relaxed CIS density for attachment/detachment density analysis as well
as for for the general excited-state analysis of Section 10.2.9.
TYPE:
LOGICAL
DEFAULT:
FALSE
OPTIONS:
FALSE
Do not use the relaxed CIS density in analysis.
TRUE
Use the relaxed CIS density in analysis.
RECOMMENDATION:
None
CIS_GUESS_DISK
CIS_GUESS_DISK
Read the CIS guess from disk (previous calculation).
TYPE:
LOGICAL
DEFAULT:
FALSE
OPTIONS:
FALSE
Create a new guess.
TRUE
Read the guess from disk.
RECOMMENDATION:
Requires a guess from previous calculation.
CIS_GUESS_DISK_TYPE
CIS_GUESS_DISK_TYPE
Determines the type of guesses to be read from disk
TYPE:
INTEGER
DEFAULT:
Nil
OPTIONS:
0
Read triplets only
1
Read triplets and singlets
2
Read singlets only
RECOMMENDATION:
Must be specified if CIS_GUESS_DISK is TRUE.
STS_MOM
STS_MOM
Control calculation of the transition moments between excited states in
CIS and TDDFT calculations (including spin-flip variants).
TYPE:
LOGICAL
DEFAULT:
FALSE
OPTIONS:
FALSE
Do not calculate state-to-state transition moments.
TRUE
Do calculate state-to-state transition moments.
RECOMMENDATION:
When set to true requests the state-to-state dipole transition moments for
all pairs of excited states and for each excited state with the ground
state. This is not available for restricted open-shell wavefunctions.
CIS_MOMENTS
CIS_MOMENTS
Controls calculation of excited-state (CIS or TDDFT) multipole moments.
TYPE:
LOGICAL
DEFAULT:
FALSE
OPTIONS:
FALSE
Do not calculate excited-state moments.
TRUE
Calculate moments for each excited state.
RECOMMENDATION:
Set to TRUE if excited-state moments are desired. (This is a trivial
additional calculation.) The MULTIPOLE_ORDER controls how many
multipole moments are printed. This option is not available for spin-flip methods.