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31 EXPLICITLY CORRELATED METHODS 228<br />

default,vdz/jkfit }<br />

hf<br />

{lt-df-lcc2<br />

!ground state CC2<br />

!five lowest triplet states, dipole moments for four lowest, density saved:<br />

eom,-6.1,triplet=1,singlet=0,propes=-5.1,densave=5000.2<br />

eomprint,popul=-1,loceom=-1 } !minimize the output<br />

!ground state density, file h2o0_density.cube:<br />

{cube,h2o0,,80,80,80<br />

density,5000.2,cc2 }<br />

!difference excited state density, file h2o1_density.cube:<br />

{cube,h2o1,,80,80,80<br />

density,5000.2,diff,state=2.1 }<br />

31 EXPLICITLY CORRELATED METHODS<br />

Explicitly correlated calculations provide a dramatic improvement of the basis set convergence<br />

of MP2 and CCSD correlation energies. Such calculations can be performed using the commands<br />

of the form<br />

command, options<br />

where command can be one of the following:<br />

MP2-F12 Closed-shell canonical MP2-F12. By default, the fixed amplitude<br />

ansatz (FIX, see below) is used, but other ansätze are also possible.<br />

The F12-corrections is computed using density fitting, and then added<br />

to the MP2 correlation energy obtained without density fitting.<br />

DF-MP2-F12<br />

DF-LMP2-F12<br />

DF-RMP2-F12<br />

CCSD-F12<br />

CCSD-F12c<br />

CCSD(T)-F12<br />

As MP2-F12, but the DF-MP2 correlation energy is used. This is less<br />

expensive than MP2-F12.<br />

Closed-shell DF-MP2-F12 with localized orbitals. Any method and<br />

ansatz as described in J. Chem. Phys. 126, 164102 (2007) can be used<br />

(cf. secions 31.2,31.7).<br />

Spin-restricted open-shell DF-RMP2-F12 using ansatz 3C. Any method<br />

as described in J. Chem. Phys. 128, 154103 (2008) can be used (cf.<br />

sections 31.2,31.7).<br />

Closed-shell CCSD-F12 approximations as described in J. Chem. Phys.<br />

127, 221106 (2007). By default, the fixed amplitude ansatz is used<br />

and the CCSD-F12A and CCSD-F12B energies are computed. Optionally,<br />

the command can be appended by A or B, and then only<br />

the corresponding energy is computed. For more details see section<br />

31.10.<br />

Closed-shell CCSD(F12*) approximation as proposed by Hättig, Tew<br />

and Köhn. In Molpro this is denoted f12c. As compared to CCSD-<br />

F12a/b it requires additional computational effort. Since in some parts<br />

the implementation is brute-force without paging algorithms, large<br />

memory may be required. In most cases there is no gain in accuracy<br />

as compared to f12b and therefore the use of this method is normally<br />

not recommended. Currently CCSD-F12c is not available for openshell<br />

cases.<br />

Same as CCSD-F12, but perturbative triples are added.

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