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From: sergiusz kwasniewski <sergiusz.kwasniewski@luc.ac.be>
Subject: Re: CCL:excitation energies

Hi,

for the semi-empirical techniques, I've been using the whole space (Energy
criterium is 1000 eV), while for the ab initio methods the basis set is
6-311G(d,p) within the FC approximation...

But I'm concerned about the low energy part of the spectrum, and then the
criterium inside the semi-empirical techniques doesn't change much the
appearence of the spectrum.

Did anyone encounter these inconsistencies? (More information about this,
was inside my last mail) Thanks in advance

Sergiusz

At 11:57 AM 4/26/99 -0300, Sergio Emanuel Galembeck wrote:
>Dear Sergiusz,
>
>    What basis are you using? I don't have experience
>on RHF/CIS, but the results depends on basis sets
>and on the choice of active space.
>
>    Best regards,
>
>                Sergio
>
>PS: Please, sumarize the answers.
>
>==============================================
>Sergio Emanuel Galembeck
>e-mail: segalemb@usp.br
>===============================================


		     _________________________________________________

			Sergiusz Kwasniewski
			LUC SBG/TS
			Universitaire Campus Gebouw D
			3590 Diepenbeek
			BELGIUM
			tel(direct): 011/268315
			fax	   : 011/268301
			email      : sergiusz.kwasniewski@luc.ac.be
		     _________________________________________________

From chemistry-request@server.ccl.net  Tue Apr 27 10:07:22 1999
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Subject: CD spectra
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Dear Netters,

On probing into the details of calculating CD spectra, I 
came across a program (package), called BDZDO/MCDSPD,
which makes the starting CNDO/S-CI calculations and then
the calculation of the rotational strengths etc, and 
the final spectra. 

Could anybody tell me about the origin/availability of this
application (or a corresponding similar one)?

best regards

Dr Tamas E. Gunda


************************************************************************
   Dr Tamas E. Gunda                   phone: (+36-52) 316666-2479
   Research Group of Antibiotics       fax  : (+36-52) 310936
   L. Kossuth University               e-mail: tamasgunda@tigris.klte.hu
   POBox 36                            http://dragon.klte.hu/~gundat               
   H-4010 Debrecen
   Hungary
************************************************************************
From chemistry-request@server.ccl.net  Mon Apr 26 19:58:13 1999
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Subject: 5th International Conference on Chemical Structures - Final Program
Date: Mon, 26 Apr 1999 16:55:26 -0700


I APOLOGIZE FOR DUPLICATE POSTINGS.

The Fifth International Conference on Chemical Structures is only a few
weeks away (June 6 - 10).  The Organizing Committee has put together an
exciting program which is attached to this message.  Those of you who
participated in one of the earlier conferences know that this is one of the
important venues for Chemical Information practitioners.  In case you make a
last-minute decision to participate please register as soon as possible as
we are running out of rooms at the center.  You can find information about
registration on our web site at
http://ChemWeb.com/conference/5iccs/5iccs.html.  


From chemistry-request@server.ccl.net  Mon Apr 26 20:05:25 1999
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From: "Qiang" <fuq@ucla.edu>
To: <chemistry@server.ccl.net>
Subject: G98 Frequency
Date: Mon, 26 Apr 1999 16:56:34 -0700

Hi,

I am trying to calculate the frquencies of a cluster In7P8H21 with G98W. =
The structure was optimized with DFT (PW91PW91) with 6-31G** for P and =
H; ECP(LANL2DZ) for In.  When it came to frequency calculation, I got an =
error message:=20

**** Warning!! The samllest alpha delta epsilon is 0.80370032D-01

The link then died.

Could any one (especially the experts from Gaussian, Inc) give me some =
suggestion about the problem?

Thank you very much

Qiang

From chemistry-request@server.ccl.net  Tue Apr 27 01:09:12 1999
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Subject: Rolling H charges into their heavy atoms?
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Hello people,

I wanted some opinions from those well versed in the field about a practice
I've seen mentioned in some docking studies with proteins (an area in which
I'm interested).  Most PDB files have no H's mapped.  Since the ESP is
important in those studies, having some good estimate for the partial
nuclear charges is naturally important.  It appears that one can either add
the H's onto the existing structure or take a well-calculated amino acid
structure (using an ab initio program) and additively "roll" the nonpolar H
charges into their respective heavy nuclei.  In this case, those which might
H-bond seem to be treated separately (added to the structure), which makes
sense to me.  

First, is this a reasonable 1st-level understanding of the approaches to
this?  Or have I misunderstood things?

The second approach (rolling charges into the heavy atoms) would certainly
appear to be the easiest to adopt.  Is there good reason Not to do either
approach?  In both I can see an issue of accuracy for a number of obvious
reasons from the QM perspective, but wonder about the validity of this
concern on the broad scale over which these protein interactions occur.  

Any references would also be appreciated.  My apologies if this seems
trivial or mundane ... I'm quite new to all of this, and am learning it near
the back of a dark cave ...  :)  Thanks very much!

Kenward Vaughan
Professor of Chemistry
Bakersfield College
Bakersfield, CA
661-395-4243
kvaughan@bc.cc.ca.us  (work)
-- 
-----------------------------------------------------------
kaynjay@igalaxy.net
-----------------------------------------------------------

--===_372545BD_==--

From chemistry-request@server.ccl.net  Tue Apr 27 01:32:39 1999
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Date: Tue, 27 Apr 1999 08:30:32 +0300
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+======================---------------- --- -- -  -   -     -        .
| Hello everybody,
:
.

Could  anybody  provide  me  examples  of  input files for calculation
UV-Vis spectra using (PC) GAMESS?

Also  I  would  be  great if somebody point me where could I read more
about   calculation  UV-Vis spectra using GAMESS (Internet on-line and
ftp resources are preferable).

Best regards,
 Mike                          mailto:MikePeleah@mail.ru
                                                                     .
... Bring the power of XT to your Pentium-II: use Windows NT.        :
                                                                     |
.        -     -   -  - -- --- ----------------======================+


From chemistry-request@server.ccl.net  Tue Apr 27 04:21:14 1999
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Dear CCLers,
Does anybody know (or have) ZINDO program source code?
I would like to compare this method results with our NDDO
program under development. Closed programs like HyperChem
may not show some important details of calculation.

Regards

V.Khavryutchenko
CompChem group
Kiev
Ukraine

From chemistry-request@server.ccl.net  Tue Apr 27 04:22:39 1999
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From: "Jens Spanget-Larsen" <jsl@virgil.ruc.dk>
Organization: Roskilde Universitetscenter
To: sergiusz kwasniewski <sergiusz.kwasniewski@luc.ac.be>
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Subject: Re: CCL:excitation energies
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Mon, 26 Apr 1999:
sergiusz.kwasniewski@luc.ac.be>

CCL:excitation energies

> Does anyone know something about the difference between the excitation
> energies calculated by RHF CIS and semi-empirical techniques like ZINDO/S
> CIS on organic structures? I've done some calculations on aromatic
> structures, but the spectra are not comparable at all! Is there a reason for
> that behaviour?
> BTW: the semi-empirical calculations are in agreement with experiment.

Dear Sergiusz,

HF CIS calculations are generally in error because of neglect of 
electronic correlation effects.  These effects tend to stabilize 
excited states more than the ground state, and the result is that HF 
CIS frequently predicts excitation energies that are much too large.  
Semiempirical procedures like ZINDO/S are especially parameterized to 
account for the effects of electron correlation (in particular, by 
empirical adjustment of the parameters used to estimate electron 
repulsion terms), and these procedures thus predict transition 
energies of the right order of magnitude, at least for the class of 
compunds and types of transition for which they were parameterized.

By the way, have you tried to apply Time Dependent Density Functional 
Theory (TD DFT) as implemented in Gaussian 98?  For example, TD B3LYP 
does a great job for electronic transitions.

Yours, Jens >--<
                             
=-=-=-=-=-=-=-=-=-=-=-=-=-=-=-=-=-=-=-=-=-=-=-=-=-=-=-=-=-=-=-=
JENS SPANGET-LARSEN         Phone:  +45 4674 2000  (RUC)
Department of Chemistry             +45 4674 2710  (direct)
Roskilde University (RUC)   Fax:    +45 4674 3011 
P.O.Box 260                 E-Mail: JSL@virgil.ruc.dk
DK-4000 Roskilde, Denmark   http://www.rub.ruc.dk/dis/chem/psos/
=-=-=-=-=-=-=-=-=-=-=-=-=-=-=-=-=-=-=-=-=-=-=-=-=-=-=-=-=-=-=-=
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From: kozelka@citi2.fr (JirKa Kozelka)
Message-Id: <199904271340.PAA06275@bisance.citi2.fr>
Subject: Summary:HOMO-LUMO gap in Pt(II)
To: chemistry@www.ccl.net
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Some days ago, I sent to CCL a question concerning the HOMO-LUMO gap in Pt(II)
complexes. I should perhaps have specified that I was not primarily interested
in excitation energies (at least for the moment), but wanted to use the
HOMO-LUMO-gap as a check whether the calculations were reasonable.
I have obtained a series of quick responses which are given below.
I would like to express my thanks to all contributors for their interesting
comments.

**********************
Initial Question:

Dear CCL-members,

I have carried out a number of SCF calculations on Pt(II) complexes with
chloride, amine, and phosphine ligands, using Gaussian 94 and 98, with
different basis sets, and find consistently HOMO-LUMO gaps of 0.3-0.4
Hartrees, i.e., 65000-90000 cm-1. This is roughly 3 times the excitation
energies of spin-allowed d-d bands seen in
solutions of these species. The difference seems too big to me to be
explained by electron relaxation. I would very much appreciate comments
and/or explications on/of this apparent discrepancy.
We have seen that the bond lengths and dipole moment coming from HF
calculations are quite wrong for these compounds, and one has to apply 
correlated methods to get these quantities right. But can it be that the
difference in energies of the HF HOMO/LUMO one-electron orbitals is so
far from the excitation energy?

I shall summarize the answers.

Thanks,

Jirka Kozelka
**************************
Answers:
***************************
Hello, Jirka.

Recently we have been involved in the theoretical calculation of band gaps of
ionic crystals. They are certainly a type of materials different from those you
are considering, but perhaps the main findings could be relevant to you. We
have found that inclusion of electron relaxation (by means of a DeltaSCF
procedure, that is separate calculations on the ground and excited states an
difference of total energies) changes the magnitude of the band gap by more
than 3 eV in some cases (aprox. 0.1 hartrees). The effect of correlation on
the band gap was also accusated (2-3 eV), and crucial in order to achieve a
good agreement with experimental results.

If you are interested, you can download copies of our works from
http://xxx.lanl.gov/abs/cond-mat/9809176/
http://xxx.lanl.gov/abs/cond-mat/9901145/

best wishes,

        Andres Aguado.

****************************
I would be very much surprised if you (for Pt compounds) would obtain 
better results. Generally, the IP's (Excitation energies and EA's) in heavy 
metal compounds are very much influenced by relativistic effects. You 
probably used RECP's which include the mass-velocity and Darwin
terms (being derived on DHF atomic calculations) and thus you could 
argue that the relativistic effects are partially included. However, the 
correlation energy in Heavy-Metal systems is by far more important as
it is for "regular" organic systems. Especially, the correlation contribution 
to the relativistic (de)stabilization is usually responsible for more than 50% 
of the energy (IP, E(ex), BDE, etc.). If you are interested in qualitative 
numbers and if you are willing to accept errors of ~0.5 eV you may try
some of the DFT methods, which are in connection with a proper RECP 
quite "cheap" and were proven to offer reasonable results. The Kohn-Sham
orbitals will give you an estimate (not theoretically justified) for the numbers
 you are looking for. On the other hand you may suffer from the inappropriate
description of the "exchange-correlation" which quite often leads to larger
errors (wrong ground states of the atoms) and for sure you miss the 
important spin-orbit effect. 
 
Best regards 
Jan Hrusak
****************************
If one examines excited states using CI theory one sees that  the
diagonal of the CI matrix is E(lumo)-E(homo) - [exchange and coulombic
terms expressed in an Molecular Orbital basis]...  A decent theory book
would probably tell you exactly what the correction terms are.

John McKelvey
*************************
Hi !
 
I just read your message on the CCL-list.
Unfortunately I am no expert in HOMO-LUMO gaps, but I would
be curious if you also tried to use completely uncontracted
basis functions for you calculations too ?

If your compounds are closed shell systems, we could try to
recompute it with my own HF-code for comparitive purposes only.

Best greetings
Siegfried
***************************
Jirka,
   With any SCF method, the LUMO energy of a gas phase molecule will always
be exactly 0.0 hartree at the basis set limit.  Thus, in effect, you can
obtain the LUMO energy that you desire by "wisely" choosing your basis set.
Only the total energies (kinetic, e-N, N-N, e-e) have physical significance.

Preston MacDougall
***************************
Dear Jirka, the HOMO/LUMO gap can not be directly correlated with the
excitation energies!

In case of close shell molecule, the excitation energy E* from HOMO to
LUMO  is expressed by

E*= E(LUMO) - E(HOMO) - J(HOMO,LUMO) + 2 K(HOMO,LUMO)

where J and K are coulomb and exchange integrals and E's are eigenvalues.
(no CI is also assumed)

Since for d orbitals J(HOMO,LUMO) is quite large (~10 eV), the excitation
energies are significantly lower than HOMO/LUMO gap.

Serge Gorelsky
******************************
Hi Jirka,

as a method I would recommend LDA (SVWN) rather than HF or MP2. LDA 
(no gradient corrections) gives much better geometries.

Concerning the HOMO-LUMO gap, I assume you will get very good and 
sound comments to it - much better than I can give. But I recall that 
HOMO-LUMO gap does correspond to transitions and the HOMO-LUMO gap is 
by a factor of about 2 larger. 

If you do not get other answers I will look up the reference for you.

Generally I am very interested in what kind of Pt complexes you are 
interested in and what properties you investigate.

Our homepage is just under constructions, but do give you a feel of 
what we doing you might want to have a look at our test-version.

http://nitrogen.cem.uct.ac.za/achim/indexpgm.htm (no WWW !!)

Best regards

Achim
***************************
I'm not sure if this helps much, but HF theory tends to yeild a HOMO-LUMO
which is too big.  LDA on the other hand yeilds a HOMO-LUMO which is too small.
And B3LYP tends to yeild a HOMO-LUMO which is just right.  I'd give it a try.   
 

All the best, Matt
Matt Challacombe
*************************
Jirka:

Many years ago I did all the excitation energies for the chloride systems by
appropriatly populating the d orbitals and the excitation energies are in
reasonable accord with the experiments.

Mo Krauss
*********************
Dear Jirka,

modeling a complex in solution by SCF calculations in the gas phase 
contains two errors: You neglect correlation and solvent effects.

Normally reaction energies are more sensitive to correlation than the 
geometry. I would not be surprised if this holds for HOMO-LUMO gaps too. 
By the way, DFT methods include correlation effects and are only slightly 
more expensive than HF calculations.

The HOMO -> LUMO transition is accompanied by a change of the charge 
distribution. Since the solvent can be polarized by the solute, your 
ground and excited state energies are lowered (by different amounts) 
in the presence of a solvent. 

There are two methods for inclusion of solvents, explicitly including 
the solvent molecules into the calculation (expensive!) and using a 
polarizable continuum as a model for the solvent (cheaper). 

Stefan
______________________________________________________________________
Dr. Stefan Fau
******************************
Dear Jirka
The HOMO-LUMO gap calculated with the HF method, is almost allways far from the
observed excitation energy.. There are several other methods which are suitable
for  this kind of calculations  e.g CIS (C.I. sinnglets calculations).
Even semiempirical methods (suitably parametrized) usually give  HOMO-LUMO gaps
which are closer to the observed ones.

C. Garoufalis
University of Patras, Dept of Physics
****************
   Dear Jirka,

   Have you compared the experimental excitation energies 
to those came from CIS calculations? They should be much 
more precise since CIS is developed for this aim, and in fact,
this is the cheepest ab initio tool to perform such a calculation. 
Using Gaussian, you may even take the solvent effects into account.
I would suggest to try this.

Also, in the former days of spectroscopy, semiempirical methods 
were used for predicting electron excitation and ionisation energies.
If everything else fails, i would -at least- try some of them.
Most of them is parametrized on experimental data (IPs, etc.)
Many programs that are dealing with semiempirical calculations
allows you to carry out CIS calculations on semiempirical SCF, as well.
For very large systems -in my opinion- this is the only way.

Hope this helps.
Best wishes,

Tamas Karpati
Technical University of Budapest, Hungary
********************
I sent a reply to Serge:

Dear Serge,

>From Jorgensen's book "Absorption Spectra and Chemical Bonding in
Complexes", I once calculated the change in interelectron repulsion for
the d-d transitions in square-planar complexes. For the spin-allowed dz2
to dx2-y2 transition, for instance, I obtained 
E* = E(LUMO) - E(HOMO) - 4B -C.
Taking for the Racah parameter B Jorgensen's value of 600 cm-1 and C =
4B, I get a correction term 4B + C = 4800 cm-1 which is somewhat more
than 0.5 eV. Even if I take larger estimates for B, like , e.g., 822
cm-1 obtained by Vanquickenborne & Ceulemans (Inorg.Chem.,20, 796,1981),
I do not obtain more than 1 eV. That is why I neglected the
interelectron repulsion while posing my question. Your estimate is
perhaps valid for some metal ions with more contracted orbitals? I would
like to know how you have obtained it. Thank you anyway for responding
so quickly.

Greetings,

Jirka
******************
...and got the following comment back:

well, this expression is not valid if E(LUMO) and E(HOMO) are "true"
HF eigenvalues.

Racah papameters are small because they characterize "nonspherical"
effects in interelectronic repulsion.

J(d,d) integral is much bigger than B and C and in 8-15 eV for practically
all transition metals.
Serge Gorelsky
*******************



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From: "Mike McBrien" <bellycrawl@hotmail.com>
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Subject: Re: CCL:Estimation of vapour pressure of organic liquids and solids
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Hello, Merethe.

Advanced Chemistry Development makes a BP/Vapour Pressure/Flash Point 
Calculation product.  It bases the calculation of these values on:

- an internal database of about 10000 compounds
- estimated Molar Volume of the compound
- a proprietary algorithm that estimates the value of BP/VP/Flash 
Point/ Enthalpy of Vapourisation.

There is more information at:

http://www.acdlabs.com/products/bp/

Best regards,

Mike.




>From: "Merethe Sjovoll" <msj@fskru5.hre.hydro.com>
>To: chemistry@www.ccl.net
>Subject: CCL:Estimation of vapour pressure of organic liquids and 
solids
>Date: Thu, 22 Apr 1999 10:14:29 -0600
>
>Hi everybody,
>
>is there a way of estimating in a crude way the vapour pressure of 
organic
>liquids and solids? I have a whole bunch of molecules and I don't 
need absolute
>values, just look for tendencies. So I imagine some calculation 
formula which
>perhaps contains temperature, possibly boiling point and melting 
point, or
>perhaps dipole moment, molecular weight etc. (easily accessible 
quanities).
>
>Is this wishful thinking?
>
>Best regards
>
>Merethe Sjovoll
>
>-- 
>
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Subject: Workshop: DEVELOPING AND USING PC CLUSTERS AS A BIOMEDICAL RESEARCH TOOL
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DEVELOPING AND USING PC CLUSTERS AS A BIOMEDICAL RESEARCH TOOL

Workshop Dates: June 17-19, 1999.  Application deadline:  May 20, 1999

This workshop is designed to assist biomedical researchers who are
interested in establishing a PC cluster for use by their laboratory.
The workshop will address software and hardware topics encountered in
the process of building, operating and managing a PC cluster. In addition,
software development issues will also be described. Topics of discussion
will include: "What do you need to consider when creating an operating
environment?" "How to select System Software?" "How to Administer the
Cluster?" "What applications are appropriate?" and "How to get the best
performance for your money?"

Full details, including on-line applications and financial support, may
be found on the PSC Web site:

    http://www.psc.edu/biomed/workshops/workshops.html
	 
The Pittsburgh Supercomputing Center's Biomedical Initiative is an NIH
Supported Resource Center.
