[molpro-user] Calculation of L_z and L^2
Robert Polly
polly at kit.edu
Wed Jan 21 12:37:17 GMT 2015
Dear MOLPRO community,
I try to calculate the expectation values of <l_z> and <l^2> as
described in the manual:
6.13 One-electron operators and expectation values (GEXPEC)
http://www.molpro.net/info/2012.1/doc/manual/node68.html
In order to get familiar with the calculation of the expectation values
of the operators
I modified the test input listed in the manual:
***,h2o properties
geometry={o;h1,o,r;h2,o,r,h1,theta} !Z-matrix geometry input
r=1 ang !bond length
theta=104 !bond angle
gexpec,dm,sm,qm !compute dipole and quarupole moments
$methods=[hf,multi,ci] !do hf, casscf, mrci
do i=1,#methods !loop over methods
$methods(i) !run energy calculation
e(i)=energy
dip(i)=dmz !save dipole moment in variable dip
quadxx(i)=qmxx !save quadrupole momemts
quadyy(i)=qmyy
quadzz(i)=qmzz
smxx(i)=xx !save second momemts
smyy(i)=yy
smzz(i)=zz
enddo
table,methods,dip,smxx,smyy,smzz !print table of first and second moments
table,methods,e,quadxx,quadyy,quadzz !print table of quadrupole moments
I added LOP and LOP2 to either gexpec or added explicitly
{$methods(i); expec,lop,lop2},
but did not have any success!
For LOP2 I got the error message:
_Invalid operator on EXPEC directive: LOP2 (2-electron operator)__._
For LOP I got the output
OPERATOR LOP FOR CENTER 0 COORDINATES: 0.000000 0.000000
0.000000
but
show, l*
did not show any variable calculated!
Any help from your side would be greatly appreciated,
cheers,
Robert
--
*********************************************************************
Karlsruher Institut für Technologie (KIT)
Institut fuer Nukleare Entsorgung
Dr. Robert Polly
Quantenchemie
Institut fuer Nukleare Entsorgung (INE), Campus Nord, Gebaeude 712,
Postfach 3640, 76021 Karlsruhe, Germany
0049-(0)721-608-24396
email: polly at kit.edu
www: http://www.fzk.de/ine
KIT - Universität des Landes Baden-Württemberg und
nationales Großforschungszentrum in der Helmholtz-Gemeinschaft
*********************************************************************
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