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Hypertext Dalton 2.0 manual - Theoretical Chemistry, KTH

Hypertext Dalton 2.0 manual - Theoretical Chemistry, KTH

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CHAPTER 26. LINEAR AND NON-LINEAR RESPONSE FUNCTIONS, RESPONSE271<br />

.PV SO2 Sets A and B in the linear response function to the parity-violating operator and<br />

the two-electron spin–orbit integrals. The .TRPFLG keyword will also be set by this<br />

option.<br />

.QUADMOM Sets A and B to the quadrupole operators.<br />

.QUADXX/XY/XZ/YY/YZ/ZZ Sets A and B to the XX, XY, XZ, YY, YZ, or ZZ component<br />

of the quadrupole operator, respectively.<br />

.RESTLR Restart of response calculation. This can only be used if the operator specified<br />

is the same which was used last in the previous response calculation.<br />

.SOPRSY Calculate both α ij and α ji to test the quadratic accuracy of the calculated property.<br />

Mainly for debugging purposes.<br />

.FERMI Sets A and B to be all spin-dipole operators found on the file AOPROPER, i.e. all<br />

spin-dipole operators requested in the **INTEGRALS input module.<br />

.SPIN-O Sets A and B to spin-orbit operators.<br />

.SPNORX/Y/Z Sets A and B to the X, Y, or Z component of the spin–orbit operator,<br />

respectively.<br />

.THCLR<br />

READ *, THCLR<br />

Relative convergence threshold for all requested linear response functions. Default<br />

is 1.0D-3; note that this number should be at least 10 times bigger than the final<br />

gradient norm in the SCF/MCSCF wave function optimization. The accuracy of<br />

the linear response properties will be quadratic in this threshold; thus the default<br />

corresponds to convergence to approximately 6 digits.<br />

.TRIPLET Defines A and B to be triplet operators. Will also make a simultaneous *LINEAR<br />

.SINGLE RESIDUE calculation to a calculation of triplet excitation energies and transition<br />

moments.<br />

26.1.3 Linear response excitation energies calculation: *LINEAR with .SINGLE<br />

RESIDUE<br />

Single residues of the linear response function is computed. Residues of a linear response<br />

function correspond to transition moments and the associated poles correspond to vertical<br />

electronic excitation energies.

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