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Re: SA-CASSCF(4,4) two configuration in an one state and XMCQDPT.....

Alex Granovsky
gran@classic.chem.msu.su


Dear Pasha,

I would be glad to help. Could you please be a bit more specific formulating the problem itself?

Kind regards,
Alex Granovsky


On Tue Oct 4 '11 6:44am, Solntsev Pasha wrote
---------------------------------------------
>Dear colleagues.

>I am working on aromatic system related to porphyrin. So, i decided to check unsubstituted porphyrin by CASSCF/XMCQDPT(CASSCF(4,4)/6-311G(d,p)//b3lyp/6-311G(d,p)). I need only 1st and 2nd excited states. Their formation can be described by four orbital approach. Indeed, such approximation quite reasonable, because HOMO,HOMO-1 are separated from another HOMO's by big enough energy gap. All intense transitions in UV-Vis spectra rise from transitions HOMO->LUMO/LUMO+1, HOMO-1->LUMO/LUMO+1. In literature, people used CASPT2(4,4) method and showed such active space can be used for porphyrins (actually 4,4 is the smallest active space for such mycrocycles). So i did SS-CASSCF(4,4)+ntrack and caught all single electron excitations (4 for such active space). After optimization my 1st state was ground state and all single electron excited states were states from 2 to 5. Afterwards, i performed SA-CASSCF(4,4) over 5 lowest states ($drt wstate(1)=1,1,1,1,1 $end ) and got interesting picture(all configuration with zerro's coefficients were removed):

>STATE #    1  ENERGY =    -983.487159757
>
>
>
>      CSF      COEF    OCCUPANCY (IGNORING CORE)

>      ---      ----    --------- --------- -----

>        1   -0.961493  2200

>        4    0.113581  2002

>        6    0.072134  0202

>        9   -0.185355  1111

>       11    0.022668  1111

>       15    0.096837  2020

>       17    0.103561  0220

>       20   -0.049553  0022
>
>
>
> STATE #    2  ENERGY =    -983.360422516
>
>
>
>      CSF      COEF    OCCUPANCY (IGNORING CORE)

>      ---      ----    --------- --------- -----

>        3    0.660764  1201

>        7   -0.735886  2110

>       14    0.094658  0112

>       18   -0.113585  1021
>
>
> STATE #    3  ENERGY =    -983.352359738
>
>
>
>      CSF      COEF    OCCUPANCY (IGNORING CORE)

>      ---      ----    --------- --------- -----

>        2    0.752067  2101

>        8    0.646632  1210

>       13    0.105209  1012

>       19    0.072064  0121
>
>
> STATE #    4  ENERGY =    -983.286322394
>
>
>
>      CSF      COEF    OCCUPANCY (IGNORING CORE)

>      ---      ----    --------- --------- -----

>        3    0.708619  1201

>        7    0.627084  2110

>       14    0.216679  0112

>       18    0.240156  1021
>
>
> STATE #    5  ENERGY =    -983.285640465
>
>
>
>      CSF      COEF    OCCUPANCY (IGNORING CORE)

>      ---      ----    --------- --------- -----

>        2    0.611178  2101

>        8   -0.722176  1210

>       13    0.227594  1012

>       19   -0.230485  0121
>
>
>
>As we can see for state #2
>  3    0.660764  1201
>  7   -0.735886  2110

>two excitations have almost same contribution. The same thing with another states too.

>I performed also XMCQDPT with different size of the H_ef but only first state from CAS-CI corresponds to first state in MCQDPT reference:
>
>
> *** MC-XQDPT2 ENERGIES ***

> -----------------------------------------------------------------------

>   STATE                       1ST ORDER                       2ND ORDER

>     1     E(MCSCF)=     -983.4871597547     E(MP2)=     -986.9200228420

>     2     E(MCSCF)=     -983.2674851340     E(MP2)=     -986.7845079006

>     3     E(MCSCF)=     -983.2459151152     E(MP2)=     -986.7769659778

>     4     E(MCSCF)=     -983.2049480922     E(MP2)=     -986.7676948438

>     5     E(MCSCF)=     -983.1927574918     E(MP2)=     -986.7429440001

>     6     E(MCSCF)=     -983.1590205258     E(MP2)=     -986.7369602361

>     7     E(MCSCF)=     -983.0694701169     E(MP2)=     -986.6898412033

>     8     E(MCSCF)=     -982.8072824406     E(MP2)=     -986.5873781504

> EIGENVECTORS OF THE EFFECTIVE HAMILTONIAN
>
>
>
>                      1          2          3          4          5
>
>
>
>               -986.920023-986.784508-986.776966-986.767695-986.742944
>
>
>
>    1            -0.994895  -0.067638   0.033741   0.014361   0.032678

>    2            -0.067492   0.708971  -0.294819  -0.530914   0.158499

>    3             0.038811   0.159120   0.755152  -0.237075   0.492123

>    4            -0.030986   0.638493   0.157087   0.438907  -0.478557

>    5             0.018530   0.016946  -0.563000   0.081181   0.443499

>    6             0.004953  -0.211512   0.001229  -0.675617  -0.548424

>    7             0.034252  -0.118795  -0.004363   0.076785   0.041466

>    8             0.040266  -0.025619  -0.004813   0.011612   0.058562
>
>
>
>                      6          7          8
>
>
>
>               -986.736960-986.689841-986.587378
>
>
>
>    1             0.040499  -0.026339  -0.029372

>    2            -0.270110  -0.161009   0.003527

>    3             0.320243   0.031284   0.031555

>    4             0.379967  -0.019337  -0.016894

>    5             0.678936   0.128538   0.040542

>    6             0.444792   0.005797  -0.011659

>    7             0.129239  -0.953704   0.225448

>    8             0.054535  -0.214298  -0.972233

> EIGENVALUES OF THE NON-SYMMETRIC EFFECTIVE HAMILTONIAN
>
>
>
>     1     -986.91955413898560000000 + I *        0.00000000000000000000

>     2     -986.78419407332210000000 + I *        0.00000000000000000000

>     3     -986.77622935041040000000 + I *        0.00000000000000000000

>     4     -986.76715735894640000000 + I *        0.00000000000000000000

>     5     -986.74307507596620000000 + I *        0.00000000000000000000

>     6     -986.73745642166250000000 + I *        0.00000000000000000000

>     7     -986.68459320897090000000 + I *        0.00000000000000000000

>     8     -986.59405552588180000000 + I *        0.00000000000000000000

>OVERLAP NORM MATRIX OF NON-ORTHOGONAL EIGENVECTORS
>
>
>
>             1           2           3           4           5
>
>
>
>    1    1.0000000   0.0033939   0.0162086   0.0031617   0.0031535

>    2    0.0033939   1.0000000   0.2549902   0.1426137   0.0648010

>    3    0.0162086   0.2549902   1.0000000   0.1192571   0.0789034

>    4    0.0031617   0.1426137   0.1192571   1.0000000   0.2513337

>    5    0.0031535   0.0648010   0.0789034   0.2513337   1.0000000

>    6    0.0038417   0.0901892   0.0600024   0.2513302   0.4293901

>    7    0.0375041   0.0049329   0.1179925   0.0041655   0.0068307

>    8    0.0448358   0.0165570   0.1067129   0.0007353   0.0019392
>
>
>
>             6           7           8
>
>
>
>    1    0.0038417   0.0375041   0.0448358

>    2    0.0901892   0.0049329   0.0165570

>    3    0.0600024   0.1179925   0.1067129

>    4    0.2513302   0.0041655   0.0007353

>    5    0.4293901   0.0068307   0.0019392

>    6    1.0000000   0.0078361   0.0617392

>    7    0.0078361   1.0000000   0.4620405

>    8    0.0617392   0.4620405   1.0000000
>
>
>I also played with $xmcqdpt  wstate(1) and avecoe(1) arrays. I used same as for $drt wstate(1)=1,1,1,1,1 $end but also default value for wstate from xmcqdpt.

>Could you please to help me solve this problem.

>If you need any extra information just let me know. I have a lot of different files related to this problem.

>Best,

>Pavel.
>
>
>
>
>


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