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24 THE CLOSED SHELL CCSD PROGRAM 185<br />

24.6.2 Single-reference correlation treatments for N 2 F 2<br />

***,N2F2 CIS GEOMETRY (C2h)<br />

rnn=1.223,ang<br />

!define N-N distance<br />

rnf=1.398,ang<br />

!define N-F distance<br />

alpha=114.5;<br />

!define FNN angle<br />

geometry={N1<br />

N2,N1,rnn<br />

F1,N1,rnf,N2,alpha<br />

F2,N2,rnf,N1,alpha,F1,180}<br />

basis=vtz<br />

!cc-pVTZ basis set<br />

$method=[hf,cisd,ccsd(t),qcisd(t),bccd(t)] !all methods to use<br />

do i=1,#method<br />

!loop over requested methods<br />

$method(i)<br />

!perform calculation for given methods<br />

e(i)=energy<br />

!save energy in variable e<br />

enddo<br />

!end loop over methods<br />

table,method,e<br />

!print a table with results<br />

title,Results for n2f2, basis=$basis !title of table<br />

http://www.molpro.net/info/current/examples/n2f2_ccsd.com<br />

This calculation produces the following table:<br />

Results for n2f2, basis=VTZ<br />

METHOD E E-ESCF<br />

CISD -308.4634948 -0.78283137<br />

BCCD(T) -308.6251173 -0.94445391<br />

CCSD(T) -308.6257931 -0.94512967<br />

QCISD(T) -308.6274755 -0.94681207<br />

24.7 Saving the density matrix<br />

DM[,record.ifil];<br />

The effective first order density matrix is computed an stored in record record on file ifil. This<br />

currently works for closed-shell MP2, QCISD, and QCISD(T). See also NATORB. Note that this<br />

is much more expensive than a simple energy calculation, since the response equations have<br />

to be solved. Note: CCSD first order properties without orbital relaxation contribution can be<br />

computed using<br />

ccsd<br />

expec,dm<br />

The orbital relaxation can be included using<br />

ccsd<br />

core,0<br />

expec,relax,dm<br />

Currently, this works only without core, i.e., CORE,0 is required.

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