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31 EXPLICITLY CORRELATED METHODS 237<br />

NOZ=1<br />

NOX=1<br />

FIX=1<br />

FIX=2<br />

FIXCAN=1<br />

FIXCAN=-1<br />

CABS=1<br />

ORTHO CABS=1<br />

THRABS=thrabs<br />

THRCABS=thrcabs<br />

Neglect Z terms (only 3B and 3C).<br />

Neglect X terms (only 3A and 3B).<br />

Use diagonal ansatz with fixed coefficient approximation (orbital invariant).<br />

Use diagonal ansatz with fixed coefficient approximation. Evaluate<br />

only first order energy expression, not the Hylleraas functional. Very<br />

fast but less accurate and reliable!<br />

Use diagonal ansatz with fixed coefficient approximation and canonical<br />

orbitals. A non-iterative method is used to evaluate the energy.<br />

This is equivalent to FIX=1,CANONICAL=1 and is most efficient.<br />

As FIXCAN=1, but equations are solved iteratively (test purpose only).<br />

Use CABS (default). If CABS=0 is given, CABS is disabled. However,<br />

if RI BASIS=OPTRI, the orbital and OPTRI basis sets are automatically<br />

merged, and then exactly the same results as with CABS=1<br />

are obtained.<br />

Construct CABS basis from orthogonal MOs and ABS basis rather<br />

than AO and RI basis.<br />

Threshold for smallest eigenvalue of S in auxiliary ABS (only used<br />

with ORTHO CABS=1; default=THRCABS).<br />

Threshold for smallest eigenvalue of S in CABS (default 1.d-8).<br />

THRCABS REL=thrcabs rel Relative CABS threshold (default 1.d-9). The actual threshold<br />

is max(thrcabs,eigmax*thrcabs rel, where eigmax is the<br />

largest eigenvalue of the overlap matrix.<br />

PRINT=level<br />

DEBUG=level<br />

SOLVE=0<br />

SOLVE=1<br />

SOLVE=2<br />

SOLVE=3<br />

CANONICAL=1<br />

DOMSEL=1<br />

Print parameter. PRINT=1 give information about all computed integrals<br />

and the iterations.<br />

Can be used to obtain extended debug print.<br />

Use a most efficient pair-specific fully iterative method (default).<br />

Use simple fully iterative method.<br />

Use pair specific iterative method (more expensive).<br />

Use pair specific non iterative method (most expensive, only with<br />

canonical orbitals).<br />

Use canonical orbitals and full domains.<br />

Use full domains and localized orbitals (unless CANONICAL=1 is<br />

given).<br />

SCALE TRIP=1 Scale triples energy as explained in section 31.10.<br />

SINGLES<br />

CORE SINGLES<br />

EXTGEN<br />

For instance<br />

If set to one, include CABS singles correction (default=1)<br />

If set to one, include CABS singles correction for core orbitals (default=0)<br />

For open-shell systems: If 1 (default,recommended), include all occupied<br />

valence orbital pairs for mn in Tmn, i j independent of spin (as<br />

described in J. Chem. Phys. 130, 054104 (2009), section II.E). If 0,<br />

use only pairs mn where the spins of i and m, and j and n are equal.<br />

ANSATZ=3C,fix=1,hybrid=1,canonical=1

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