mowindow
Enable the selective perturbation (SP) approach introduced in the context of RT-TDSCF in Kadek et al. PCCP 17, 22566 (2015) but applicable to CPP calculations as well. SP enables to represent the perturbation and response operators only in selected molecular orbitals, allowing thus to eliminate nonphysical excitations that are artifacts of the finite basis representation in core-level spectroscopies.
- Input block
Extended variant
mowindow:
occupied: [intial-mo-index] - [final-mo-index]
virtual: [intial-mo-index] - [final-mo-index]
none
mowindow:
occupied: 4-6
mowindow:
occupied: 7-10
virtual: 15-46
Note
- By default, the entire orbital spectrum is considered.
- Occupied and virtual orbitals must be within their respective range. The range for occupied orbitals is from 1 to HOMO, whereas the range for virtual orbitals is from HOMO+1 to the total number of MOs.
Tip
- SP turns out to be particularly useful for X-ray spectroscopies, where excitations occur only from specific core-shell orbitals. Here, we recommed to select for perturbation only the core-shell occupied MOs.
transition-analysis
Enable the transition density matrix analysis (TDMA) introduced in the context of RT-TDSCF in Repisky et al. JCTC 11, 980 (2015) but applicable to CPP calculations as well. TDMA enables to perform the orbital analysis of spectral transitions in RT-TDSCF simulations.
- Input block
Extended variant
transition-analysis:
occupied: [intial-mo-index] - [final-mo-index]
virtual: [intial-mo-index] - [final-mo-index]
threshold: [real]
none
transition-analysis:
occupied: 8-10
virtual: 11-25
threshold: 1.0e-5
Note
- By default, TDMA is disabled.
- Occupied and virtual orbitals must be within their respective range. The range for occupied orbitals is from 1 to HOMO, whereas the range for virtual orbitals is from HOMO+1 to the total number of MOs.
Tip
- Since TDMA may lead to an extensive data printout, we recommend to select only those orbitals relevant for the spectroscopy of interest.
xc
Specify details associated with the evaluation of the exchange–correlation (xc) kernel.
- Input block
Short variant
xc:
[functional]
Extended variant
xc:
functional: [functional]
noncollinearity: [string]
xc:
functional : from-scf
noncollinearity : v2019
xc: XALDA
xc:
functional : XALDA
noncollinearity : v2005
Warning
- The use of ALDA or XALDA options is not recommended, because they usually approximate the full xc kernel. Their use is only recommended when comparing the calculated data to implementations in other quantum chemistry programs, where those approximations can not be avoided.
maxiterations
Define the maximum number of micro-iterations for the solver.
- Input line
- Default
maxiterations:
[integer]
maxiterations: 30
maxiterations: 50
checkpoint
Define the frequency of data checkpointing during the iterations.
- Input line
- Default
checkpoint:
[integer]
checkpoint: 5
checkpoint: 10
convergence
Define the convergence threshold for the CPP solver.
- Input line
- Default
convergence:
[real]
convergence: 0.0001
convergence: 1.0e-5
Note
- The quantity tested for convergence is the norm of the residue vector divided by the norm of the solution vector.
frequencies
Specify the (angular) frequencies at which to solve the (damped) linear reponse equation.
- Input line
- Default
frequencies:
[real1 integer x real2]
frequencies: 0.0
frequencies: 0.0 50x0.07
frequencies: 0.2 0.5 0.6 1.00
frequencies: 0.2 0.5 0.6
Note
- The units for the frequencies are specified by the keyword units.
damping
Specify the damping parameter for the damped linear reponse equation.
- Input line
- Default
damping:
[real]
damping: 0.0
damoing: 0.1
Note
- The units for the damping parameter are specified by the keyword units.
Latest Publications
Book chapter on relativistic real-time electron dynamics
Book chapter on relativistic theory of EPR and (p)NMR
Useful Links
Our Contacts
Department of Chemistry
UiT The Arctic University of Norway
Tromsø, NO-9037 Norway
Email: info@respectprogram.eu