CCL:G: AW: G: AW: CIS Optimization for the First Singlet Excited State



Dear Markus,
 
It is a local minimum.
 
After you found the excited state with symmetry constraint, did you reoptimize your system into a C1 symmtery?
 
Thanks,
Sue

"Markus Thut markus.thut..iac.unibe.ch" <owner-chemistry a ccl.net> wrote:
Dear Sue
 
It is certainly true that this mixing of the LUMO and LUMO+1 is the problem causing the mixing of the two transitions. Usually such mixings occur at transition states. Is it a transition state or just a local minima?
 
The systems we observed such interchanges are _not_ symmetric either. Thus, we forced them to be. Maybe you are able to do something similar.
 
The _calcall_ calculates the forces at each point in the optimization. Thus, the minimization algorithm can easily step into the direction of the largest force contribution. This speeds up convergence (or makes it possible for shallow potentials), but strongly slows down your calculations. So use it just in case you have convergence problems.
 
 Cheers
 
Markus
 
 

Von: owner-chemistry[A]ccl.net [mailto:owner-chemistry[A]ccl.net]
Gesendet: Dienstag, 20. November 2007 04
:04
An: Thut, Markus
Betreff: CCL:G: AW: CIS Optimization for the First Singlet Excited State
 
Dear Markus
Thank you very much for your suggestion.
 
The compound that I have studied do not have any symmetry. In my case, the LUMO and LUMO+1 is mixed. That might caused the problem for the interchange of the excited states.
 
The basis set that I used is 6-31g* for all atoms. Is the optimization more easiler to get converged with Calcall keyword?
 
Best regards,
Sue
 


"Markus Thut markus.thut[-]iac.unibe.ch" <owner-chemistry|-|ccl.net> wrote:

Sent to CCL by: "Markus Thut" [markus.thut+/-iac.unibe.ch]
Dear Sue

We usedd to encounter this problem too. What we found is that

i) upon interchange of the excited states, the electronic character of the
two states interchange. Thus, a "major" change in geometry occurs upon this
change. Please check the evolution of your optimized molecule.

ii) Usually, such interchanges occur due to symmetry-breaking optimization
steps. Sometimes, you can prevent interchanges by restricting the
optimization to e.g. Cs instead of C1, even though the cluster/molecule you
are optimizing is presumably C1.

iii) if you have a symmetry wich allows optimizations for a' or a"
transitions, try to optimize for the desired transition (you can do this in
TURBOMOLE, I'm not sure about Gaussian03). In this case, you should get a
minima for the a' and on for the a" transition. Comparing these two
geometries, you should find the structural change responsible for the
interchange of the two states. We found, for example thath for
hydroxyquinolines, such an interchage is induced by a significant change of
the angle of the quinone-N.

iv) there might be some problems with your basis set (inducing structural
changes and so on), maybe you first choose a standard basis set?

v) try the CalcAll parameter for the opt command.

Cheers,

Markus


> -----Ursprüngliche Nachricht-----
> Von: owner-chemistry .. ccl.net [mailto:owner-chemistry .. ccl.net]
> Gesendet: Samstag, 17. November 2007 03:05
> An: Thut, Markus
> Betreff: CCL: CIS Optimization for the First Singlet Excited State
>
>
> Sent to CCL by: "Sue L" [chsue2004 ~~ yahoo.com]
> Hi all,
>
> I have performed a CIS optimization for the first singlet excited state
> with the keywords #n cis(root=1,direct) gen opt
>
> However, the optimization cannot be converged. I found that in the middle
> of the optimization, the first- and second- excited state swapped, as
> indicated in the section of Excitation energies and oscillator strength
> (as below).
>
> ---------
> Excited State 1: Singlet-A 3.7320 eV 332.22 nm f=0.1634
> 93 -> 94 0.67286
> This state for optimization and/or second-order correction.
> Copying the excited state density for this state as the 1-particle RhoCI
> density.
>
> Excited State 2: Singlet-A 5.5654 eV 222.78 nm f=0.2648
> 91 -> 94 -0.12140
> 91 -> 96 -0.14274
> 92 -> 94 0.46889
> 92 -> 95 -0.14756
> 93 -> 95 -0.35249
> ---------
>
> ---------
> Excited State 1: Singlet-A 5.5227 eV 224.50 nm f=0.2035
> 91 -> 94 -0.11890
> 91 -> 95 -0.11553
> 91 -> 96 -0.13341
> 92 -> 94 0.46589
> 92 -> 95 -0.17450
> 93 -> 95 -0.35340
> This state for optimization and/or second-order correction.
> Copying the excited state density for this state as the 1-particle RhoCI
> density.
>
> Excited State 2: Singlet-A 4.0937 eV 302.86 nm f=0.1943
> 92 -> 95 -0.11059
> 93 -> 94 0.66385
> --------
>
> Could anyone know what the problem is?
>
> Thank you very much.
>
> Sue
>
>
>
>
>> > > > > >
>
>
> > >
> =>
>


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