From chemistry-request@server.ccl.net  Fri Mar 24 01:04:00 2000
Received: from biol2.bio.nagoya-u.ac.jp ([133.6.127.8])
	by server.ccl.net (8.8.7/8.8.7) with ESMTP id BAA02461
	for <chemistry@ccl.net>; Fri, 24 Mar 2000 01:03:59 -0500
Received: from [133.6.127.65] (jupiter [133.6.127.65])
	by biol2.bio.nagoya-u.ac.jp (8.9.2/8.9.2) with SMTP id NAA23701;
	Fri, 24 Mar 2000 13:57:09 +0900 (JST)
Date: Fri, 24 Mar 2000 13:57:09 +0900 (JST)
Message-Id: <200003240457.NAA23701@biol2.bio.nagoya-u.ac.jp>
To: "Yanni Wang" <wangyn@Kvac.UU.SE>
From: shinoda@biol2.bio.nagoya-u.ac.jp (Kazuki Shinoda)
Subject: Re: Re: CCL:Program to convert CHARMM force field file to AMBER
 format
Cc: chemistry@ccl.net
MIME-Version: 1.0
Content-Type: text/plain; charset=iso-2022-jp
X-Mailer: Eudora-J(1.3.8.5-J13)

Dear Yanni,

I am sorry for lating to summarize.
Unforturnately, however, I have got no replies from anyone about
my question yet. So I cannot inform you of any information.
Sorry, again.

Best regards,

Kazuki

>
>Dear Kazuki,
>
>     You have ever submitted the following question on CCL. Would you like to
>summarize the answers you got?
>
>     Best regards!
>
>
>On Jan 25,  8:57pm, Kazuki Shinoda wrote:
> > Subject: CCL:Program to convert CHARMM force field file to AMBER format
> > Dear CCLers,
> >
> > Does anyone have a program to convert CHARMM format
> > force field file to AMBER format ?
> >
> > Best regard,
> >
> > Kazuki
> >


================================================
 Kazuki Shinoda, MC2
 Division of Biological Science, Graduate school of Science
 Nagoya University, Chikusa, Nagoya 464-8602, Japan

 E-mail : shinoda@biol2.bio.nagoya-u.ac.jp
 URL:      http://bio.nagoya-u.ac.jp:8001/~kazuki/kazuki.html
================================================


From chemistry-request@server.ccl.net  Fri Mar 24 04:43:01 2000
Received: from uvaix7e1.comp.UVic.CA (root@uvaix7e1.comp.UVic.CA [142.104.5.107])
	by server.ccl.net (8.8.7/8.8.7) with ESMTP id EAA03454
	for <CHEMISTRY@ccl.net>; Fri, 24 Mar 2000 04:43:00 -0500
Received: from p17-62.dialup.UVic.CA (p17-62.dialup.UVic.CA [142.104.17.62])
	by uvaix7e1.comp.UVic.CA (8.9.3/8.9.3) with SMTP id AAA179604
	for <CHEMISTRY@ccl.net>; Fri, 24 Mar 2000 00:38:35 -0800
From: Roy Jensen <royj@uvic.ca>
To: CHEMISTRY@ccl.net
Subject: SUMMARY: Dipole Moment from PES scan
Date: Fri, 24 Mar 2000 00:38:40 -0800
Message-ID: <00amdsg1uke0d2giaq9esggmu0qk3ul407@4ax.com>
X-Mailer: Forte Agent 1.7/32.534
MIME-Version: 1.0
Content-Type: text/plain; charset=us-ascii
Content-Transfer-Encoding: 8bit
X-MIME-Autoconverted: from quoted-printable to 8bit by server.ccl.net id EAA03455

My original question was:

> Is there a way of getting Gaussian 94 to output the multipole moments
> at each step of a relaxed or rigid PES scan?
> Gaussian 98 is available but I have not used it.

I received two responses. The response from Doug Fox at Gaussian
proved to be definitive. Contrary to his hints at the difficulty, it
wasn't that bad to implement! It would be nice if Gaussian, Inc. would
leave up the online manual for the previous versions of Gaussian...it
was hard to find the IOPs for Gaussian 94; they do not appear to be
the same as in Gaussian 98.

Roy Jensen


******************************************************************************
gaussian.com!fox@gaussian.com (Doug Fox) wrote:

  Dr. Jensen,

   There is no trivial way to request this.  The structure of G94 and
G98 computes the energy and checks if it is "optimized" and then loops
back to update the structure.  The population analysis is a separate
program and it is not trivial to have it jump into the population
analysis only at optimized points.  It is on the list of requested
features but it is not present even in G98.

   For a rigid scan you can make a nonstandard route which does the
population analysis at every point.  The basis non-standard route is,

 1/38=1/1,8;
 2/17=6,18=5/2;
 3/11=9,25=1,30=1/1,2,3;
 4//1;
 5/5=2,38=4/2;
 6/7=2,8=2,9=2,10=2,18=1,28=1/1;
 1//8(1);
 99/9=1/99;
 2//2;
 3/11=9,25=1,30=1/1,2,3;
 4/5=5,16=2/1;
 5/5=2,38=4/2;
 1//8(-4);
 99/9=1/99;

and if you modify the final three lines as follows

 5/5=2,38=4/2;
 6/7=2,8=2,9=2,10=2,18=1,28=1/1;
 1//8(-5);
 99/9=1/99;

you will get population analysis and multipole moments at each step.

   Best to start with the output from testrt for the case you want to
get the basis set and other options set correctly.  Then run a job
like

# NonStd
 1/38=1/1,8;
 2/17=6,18=5/2;
 3/11=9,25=1,30=1/1,2,3;
 4//1;
 5/5=2,38=4/2;
 6/7=2,8=2,9=2,10=2,18=1,28=1/1;
 1//8(1);
 99/9=1/99;
 2//2;
 3/11=9,25=1,30=1/1,2,3;
 4/5=5,16=2/1;
 5/5=2,38=4/2;
 6/7=2,8=2,9=2,10=2,18=1,28=1/1;
 1//8(-5);

Your title  and structure input follow.

  Check the G94 Programmer's Reference for details on the print
options for l601 to tailor the output to get fewer features you don't
want.


******************************************************************************
straka@chem.helsinki.fi (Michal Straka) wrote:

Hi,
I had the same problem
I used Pop=Full
but it gives an huge out file.
I needed just one so I didn't bother,


<NOTE: this did not work when I tried it. Roy Jensen>

From chemistry-request@server.ccl.net  Fri Mar 24 05:16:11 2000
Received: from sunu450.rz.ruhr-uni-bochum.de (sunu450.rz.ruhr-uni-bochum.de [134.147.64.5])
	by server.ccl.net (8.8.7/8.8.7) with SMTP id FAA03736
	for <Chemistry@CCL.net>; Fri, 24 Mar 2000 05:16:10 -0500
Received: (qmail 29788 invoked from network); 24 Mar 2000 09:11:49 -0000
Received: from cvw.orch.ruhr-uni-bochum.de (HELO ?134.147.110.57?) (134.147.110.57)
  by mailhost.rz.ruhr-uni-bochum.de with SMTP; 24 Mar 2000 09:11:49 -0000
Mime-Version: 1.0
X-Sender: wuellcbd@mailhost.rz.ruhr-uni-bochum.de
Message-Id: <a04310100b500e15420d4@[134.147.110.57]>
In-Reply-To: <862568AB.00469176.00@unomail.unomaha.edu>
References: <862568AB.00469176.00@unomail.unomaha.edu>
Date: Fri, 24 Mar 2000 10:11:39 +0100
To: Douglas_Stack/CAS/UNO/UNEBR@unomail.unomaha.edu
From: Christoph van =?iso-8859-1?Q?W=FCllen?=  <Christoph.van.Wuellen@Ruhr-Uni-Bochum.De>
Subject: Re: CCL:Cluster information and Linux Alpha
Cc: Chemistry@CCL.net
Content-Type: text/plain; charset="us-ascii" ; format="flowed"

As to the possiblity to combine Alpha/Intel Clusters, note this 
statement coming from the vendors of LINDA:

"However, Gaussian does not  currently allow heterogenous execution.
When the folks at Gaussian quoted "Linda for a heterogenous network"
they are talking about a Linda distribution that runs independent
problems on different networks."
-- 
---------------------------+------------------------------------------------
Christoph van Wullen       | Fon (University):  +49 234 32 26485
Theoretical Chemistry      | Fax (University):  +49 234 32 14109
Ruhr-Universitaet          | Fon/Fax (private): +49 234 33 22 75
D-44780 Bochum, Germany    | eMail: Christoph.van.Wuellen@Ruhr-Uni-Bochum.de
---------------------------+------------------------------------------------

From chemistry-request@server.ccl.net  Thu Mar 23 18:32:06 2000
Received: from Mercury.acs.unt.edu (mercury.acs.unt.edu [129.120.220.1])
	by server.ccl.net (8.8.7/8.8.7) with ESMTP id SAA00862
	for <CHEMISTRY@server.ccl.net>; Thu, 23 Mar 2000 18:32:05 -0500
Received: from jove.acs.unt.edu (10759@jove.acs.unt.edu [129.120.220.41])
	by Mercury.acs.unt.edu (8.8.8/8.8.8) with ESMTP id QAA21403;
	Thu, 23 Mar 2000 16:27:48 -0600 (CST)
Received: from localhost (tdp0006@localhost)
	by jove.acs.unt.edu (8.8.8/8.8.8) with ESMTP id QAA17424;
	Thu, 23 Mar 2000 16:25:41 -0600 (CST)
Date: Thu, 23 Mar 2000 16:25:40 -0600 (CST)
From: TREVOR D POWER <tdp0006@unt.edu>
To: Dave Price <d.w.price@reading.ac.uk>
cc: Comp Chem Mailing List <CHEMISTRY@server.ccl.net>
Subject: Re: CCL:MM vdW potential function derivation
In-Reply-To: <38D8EBD8.6381D052@reading.ac.uk>
Message-ID: <Pine.GSO.4.05.10003231618220.16440-100000@jove.acs.unt.edu>
MIME-Version: 1.0
Content-Type: TEXT/PLAIN; charset=US-ASCII

 You will want to take a look at:

Norrby, P.-O.; Liljefors, T. J. Comp. Chem. (1998) 19,10 1146-1166

There is quite a lot in there about force field development.

Cheers,
Dr. David Power
Department of Chemistry
University of North Texas
NT Station, Box 305070
Denton, TX 76203-5070
USA
tdp0006@unt.edu







On Wed, 22 Mar 2000, Dave Price wrote:

> Dear CCLers,
> 	I am trying to parameterise a system for use in molecular
> mechanics/molecular dynamics/monte carlo calculations.  I have seen
> little in the literature about this (eg electron gas method, 
> HF/DFT calcs for torsional angles), has anyone published a comprehensive
> review or have any very useful programs for this sort of thing?
> I will summarise any answers I get if there is an interest.
> (Please don't tell me to use the universal force-field).
> 	Cheers,
> 		Dave
> 
> -- 
> ------------------------------------------------------------------------
> 
> Dr. David W. Price,       Tel: +44 (0)118 9875123  extn 7415
> Department of Chemistry,  Fax: +44 (0)118 9316331
> University of Reading,    mailto:d.w.price@reading.ac.uk
> Whiteknights, 
> READING                http://www.chem.rdg.ac.uk/g50/mmrg/dave/dave.html
> RG6 6AD 
> U.K.
>  
> ------------------------------------------------------------------------
> 
> 
> -= This is automatically added to each message by mailing script =-
> CHEMISTRY@ccl.net -- To Everybody    |   CHEMISTRY-REQUEST@ccl.net -- To Admins
> MAILSERV@ccl.net -- HELP CHEMISTRY or HELP SEARCH
> CHEMISTRY-SEARCH@ccl.net -- archive search    |    Gopher: gopher.ccl.net 70
> Ftp: ftp.ccl.net  |  WWW: http://www.ccl.net/chemistry/   | Jan: jkl@ccl.net
> 
> 
> 
> 
> 
> 



From chemistry-request@server.ccl.net  Fri Mar 24 05:49:46 2000
Received: from fsuj20.rz.uni-jena.de (fsuj20.rz.uni-jena.de [141.35.1.18])
	by server.ccl.net (8.8.7/8.8.7) with ESMTP id FAA03920
	for <chemistry@ccl.net>; Fri, 24 Mar 2000 05:49:45 -0500
Received: from pc04.chemie.uni-jena.de (pc04.chemie.uni-jena.de [141.35.29.60])
	by fsuj20.rz.uni-jena.de (8.9.1a/8.9.1) with ESMTP id KAA20394
	for <chemistry@ccl.net>; Fri, 24 Mar 2000 10:45:21 +0100 (MET)
Received: from pc04.chemie.uni-jena.de by pc04.chemie.uni-jena.de (8.8.8/1.1.22.3/02Dec99-0338PM)
	id KAA0000015794; Fri, 24 Mar 2000 10:45:21 +0100 (MET)
Sender: goeller@pc04.chemie.uni-jena.de
Message-ID: <38DB3930.10AA9EE2@pc04.chemie.uni-jena.de>
Date: Fri, 24 Mar 2000 10:45:20 +0100
From: Andreas Goeller <goeller@pc04.chemie.uni-jena.de>
X-Mailer: Mozilla 4.5 [en] (X11; I; OSF1 V4.0 alpha)
X-Accept-Language: German, de, en
MIME-Version: 1.0
To: "chemistry@ccl.net" <chemistry@ccl.net>
Subject: Summary: UV/vis visualisation
Content-Type: text/plain; charset=iso-8859-1
Content-Transfer-Encoding: 8bit

Dear all,

here's the summary of my question about simulating UV/vis spectra:


________________________________________________________________________
*The original question:
*from semiempirical calculations I get transition energies (say, in
*wavenumbers, lam) and oscillator strengths (osc), i.e. a line spectrum.
*The osc are proportional to the surface below one extinction curve. I
*can model this curve approximately by using a Gauss curve f(x), and by
*summation over all curves (g(x)) I get something comparable to an
*experimental spectrum. The function is
*
*g(x)= sum_i(osc_i*(fx_i))
*f(x)= 1/(sigma*sqrt(2*pi))*exp(-0.5*((x-x0)/sigma)**2)
*
*Can anybody give me a hint about reasonable choices for sigma, the
*standard deviation? The smaller sigma, the steeper the curve. 
*
_________________________________________________________________________

>>>>>>>>>>>>>>>>>>>>>>

There seems to be no quantitative relationship one can use. There are
empirical factors that work. 

>>>>>>>>>>>>>>>>>>>>>>


_________________________________________________________________________
From:"Paul N. Day MLPJ CON" <daypn@Picard.ml.wpafb.af.mil>

It seems like with the normalization coefficient you have put
on f(x), you will always get f(x)=1.  I think you want to model
the absorption spectrum with a gaussian such as

epsilon=epsilon(max)*exp(-0.5*((x-x0)/sigma)**2)

where epsilon(max) is the extinction coeficient at the line maximum
with frequency x0.  Then when you integrate this over x and multiply
by the appropriate constant (4.33e-9 in customary units), you will get 
the oscillator strength.
sigma is related to the linewidth at half-max, gamma, by

sigma = 0.5*gamma/sqrt(2*ln2)

It seems like the usual practice is to choose an arbitrary value for
the line-width based on experiment.  In a paper by Albota, et al
(Science 281, 1653(1998)), for the calculations they use 0.1 eV for 
the linewidth.  The linewidth is related to the decay rate of the
state and is affected by temperature, solvent, etc.  I do not know
of a rigorous theoretical method for getting the linewidth, but I
would be interested in hearing about any that you hear about.

Thanks,
Paul
_________________________________________________________________________
From: Demetrio Antonio da Silva Filho - doutorado <dasf@ifi.unicamp.br>

I do the same as you to fit the UV-Vis peaks that we get from QC
calculations ( I have a fortran CODE do to that and I can send the code
to
you if you want).
The value of sigma depends on the resolution of the article that you
have
to compare your results. I have an article which the experimental
resolution was 10nm. So I use the same!
Hope it helps!
Demetrio Filho
_________________________________________________________________________
From: Sérgio Emanuel Galembeck <segalemb@usp.br>


    Some years ago I simulate some spectra of organic substances using a
Gaussian, and I considered sigma an empirical parameter that are ajusted
in
order to reproduce experimental spectra.
    There some softwares that calculate a Gaussian using absorption and
oscillator stenghts, as
synspec.

_________________________________________________________________________
From: Scott McMillan <smcmilla@nwu.edu>

I've looked into this issue.  I also use Gaussians for each individual 
excitation.  In my case, I looked at the half-width of Gaussians fit to
the 
experimental spectrum and used something similar to that.  I found that
a 
half-width between 500 and 1000 cm-1 works well.  If you have
experimental 
spectra, you could also trying fitting the half-widths although you
could have 
a lot of fitting parameters.  I don't know of a way to determine the
width of 
the Gaussians a priori.  Please send me a summary of the responses to
your 
question. Thanks.

_________________________________________________________________________
From: Stefan Grimme <grimmes@uni-muenster.de>

to my expierience, the band width at 1/e height is about
0.3-0.5 eV for larger molecules if measured in solution.



>>>>>>>>>>>>>>>>>>>>>>>

I mailed back to Demetrio:


>it would be nice if I could have your source for reasons of comparison.
>What exactly do you mean with sigma=10nm. The std. dev. or the line
>width?


and got the answer:

______________________________________________________________________________
10nm is my  dd, and it's your  (sigma)^2

To run the the code, after compilation, you should have an archive
called fort.1 with the energy in one column and the dipole oscilator
strenght in the other. The archive fort.2, that will be created after
running
the program, will contains the spectrum with gaussians.
Hope it helps!
Demetrio FIlho



f(x)= 1/(sigma*sqrt(2*pi))*exp(-0.5*((x-x0)/sigma)**2)

Here is the code!

        implicit real*8(a-h,o-z)
        dimension energy(600),weight(600)
c       energy(i) e' a energia da transicao em eV ou comprimento de onda
c               em nanometros
c       weight(i) e' a forca de oscilador
c       dd e' a largura da gaussiana em eV ou nanometros
c       nn the number of transitions to be read
        read(1,*)nn,dd
       READ(1,*)( energy(I),weight(i),i=1,NN)
       eini=energy(1)-100.d0
        emax=energy(nn)+100.d0
       de=1.d0
       e=eini
       pi=3.1415927d0
       den=dsqrt(2.d0*pi)*dd
        dd=dd*dd
       npoint=(emax-eini)/de
       do i=1,npoint
       f=0.d0
         do j=1,nn
        w=weight(j)
        ene=energy(j)
         if(dabs(e-ene).le.500.d0) f=f+w*exp(-0.5*(e-ene)**2/dd)
         enddo
       f=f/den
       write(2,*)e,f
       e=e+de
       enddo
        stop
        end





-- 
                                Andreas Goeller

---------------------------------------------------------------
   Dr. Andreas Goeller       Institut fuer Physikalische Chemie
                               Friedrich-Schiller-Universitaet
                                       Lessingstr. 10
phone: +49(0)-3641-948352               D-07743 Jena
  fax: +49(0)-3641-948302 (secretary)     Germany
email: goeller@pc04.chemie.uni-jena.de
http://www.uni-jena.de/chemie/photo/goeller/goeller.html
---------------------------------------------------------------
   Dr. Andreas Goeller   ehemals Computer Chemie Centrum

email: goeller@organik.uni-erlangen.de
http://www.organik.uni-erlangen.de/clark/goeller/goeller.html
---------------------------------------------------------------


From chemistry-request@server.ccl.net  Fri Mar 24 11:28:12 2000
Received: from tca7.dl.ac.uk (tca7.dl.ac.uk [193.62.112.105])
	by server.ccl.net (8.8.7/8.8.7) with SMTP id LAA06317
	for <chemistry@ccl.net>; Fri, 24 Mar 2000 11:28:11 -0500
Received: from localhost by tca7.dl.ac.uk; (5.65v4.0/1.1.8.2/06Oct95-0132PM)
	id AA00990; Fri, 24 Mar 2000 15:10:58 GMT
Sender: hgs@dl.ac.uk
Message-Id: <38DB8581.207618C9@dl.ac.uk>
Date: Fri, 24 Mar 2000 15:10:58 +0000
From: Georg Schreckenbach <h.g.schreckenbach@dl.ac.uk>
Reply-To: h.g.schreckenbach@dl.ac.uk
Organization: CLRC Daresbury Laboratory
X-Mailer: Mozilla 4.05 [en] (X11; I; OSF1 V4.0 alpha)
Mime-Version: 1.0
To: Computational Chemistry List <chemistry@ccl.net>
Subject: frequency calculations for metal complexes
Content-Type: text/plain; charset=us-ascii
Content-Transfer-Encoding: 7bit

Hi,

having been off-line for a while, I just came across an old
(mid Feb. or so) summary in the CCL archives. I thought
that I should add a little comment. The old summary is about
the use of ECP basis sets for metal complexes. In this
summary, somebody claims that one cannot calculate
frequencies for metal complexes if an ECP basis set is used.
This is definitely not correct anymore since, e.g., Gaussian98 has
analytical second derivatives for ECPs. Thus, frequency
calculations are, indeed, possible in these cases! (and I have
done a lot of them lately ...)

Best regards, Georg



From chemistry-request@server.ccl.net  Fri Mar 24 11:28:57 2000
Received: from tca7.dl.ac.uk (tca7.dl.ac.uk [193.62.112.105])
	by server.ccl.net (8.8.7/8.8.7) with SMTP id LAA06329
	for <chemistry@ccl.net>; Fri, 24 Mar 2000 11:28:53 -0500
Received: from localhost by tca7.dl.ac.uk; (5.65v4.0/1.1.8.2/06Oct95-0132PM)
	id AA00994; Fri, 24 Mar 2000 15:11:45 GMT
Sender: hgs@dl.ac.uk
Message-Id: <38DB85B0.25A42697@dl.ac.uk>
Date: Fri, 24 Mar 2000 15:11:45 +0000
From: Georg Schreckenbach <h.g.schreckenbach@dl.ac.uk>
Reply-To: h.g.schreckenbach@dl.ac.uk
Organization: CLRC Daresbury Laboratory
X-Mailer: Mozilla 4.05 [en] (X11; I; OSF1 V4.0 alpha)
Mime-Version: 1.0
To: Computational Chemistry List <chemistry@ccl.net>
Subject: all-electron Gaussian basis for actinides
Content-Type: text/plain; charset=us-ascii
Content-Transfer-Encoding: 7bit

Dear everybody,

does anyone know of ALL-ELECTRON Gaussian basis sets for
actinide elements, published or unpublished? I'd be particularly
interested in the early actinides, Th thru' Am, say.

I have already searched the CCL archives and the EMSL basis set
repository but with no success. I know, of course, that one would
normally use ECPs or related methods for these heavy elements.
(... and there are a couple of ECP basis sets in the EMSL library ...)
I also know that the ADF program provides all-electron
SLATER basis sets for these elements.

Would it, perhaps, be possible to use the basis sets that were
developed for four-component relativistic methods? If so, would
they have to be modified? (I suppose so ... e.g. take the large
component only?) Where are they to be found?

I'll summarize as usual.

Thank you, and best regards,

Georg




From chemistry-request@server.ccl.net  Fri Mar 24 12:12:01 2000
Received: from yeager5.chem.tamu.edu (yeager5.chem.tamu.edu [165.91.176.73])
	by server.ccl.net (8.8.7/8.8.7) with ESMTP id MAA06620
	for <chemistry@ccl.net>; Fri, 24 Mar 2000 12:12:01 -0500
Received: (from noj@localhost) by yeager5.chem.tamu.edu (980427.SGI.8.8.8/980728.SGI.AUTOCF) id RAA28678; Fri, 24 Mar 2000 17:07:45 +0100 ("MET)
Date: Fri, 24 Mar 2000 17:07:45 +0100 ("MET)
Message-Id: <200003241607.RAA28678@yeager5.chem.tamu.edu>
From: noj malcolm <noj@yeager5.chem.tamu.edu>
To: h.g.schreckenbach@dl.ac.uk
CC: chemistry@ccl.net
In-reply-to: <38DB85B0.25A42697@dl.ac.uk> (message from Georg Schreckenbach on
	Fri, 24 Mar 2000 15:11:45 +0000)
Subject: Re: CCL:all-electron Gaussian basis for actinides
Reply-To: noj@yeager5.chem.tamu.edu
X-Beard: Beard v5.3
X-Child: Bethany

Georg,
	you will find some references in a recent paper by Tilson,
Shepard, Naleway, Wagner and Ermler (JCP 112#5 (2000) p2292)

the basis sets employed seem to be private communications
unfortunately, but you may get soemwhere by getting in touch with the
authors.

noj

-- 
--------------------------------------------------------------------------
Dr. N.O.J. Malcolm			 e-mail:noj@yeager5.chem.tamu.edu
Department of Chemistry
Texas A&M University
College Station
TX 77845
U.S.A
--------------------------------------------------------------------------

From chemistry-request@server.ccl.net  Fri Mar 24 14:10:08 2000
Received: from NPD1.NPD.UFPE.BR (npd1.npd.ufpe.br [150.161.6.2])
	by server.ccl.net (8.8.7/8.8.7) with ESMTP id OAA07338
	for <chemistry@ccl.net>; Fri, 24 Mar 2000 14:09:56 -0500
Received: from mail.npd.ufpe.br ([150.161.40.38])
 by npd.ufpe.br (PMDF V5.1-4 #20469)
 with ESMTP id <01JNF0O8KOZK000EWI@npd.ufpe.br> for chemistry@ccl.net; Fri,
 24 Mar 2000 16:01:51 GMT-3
Date: Fri, 24 Mar 2000 16:12:32 -0300
From: Patricia Farias <pmaf@frevo.npd.ufpe.br>
Subject: SOCC/trans.dipole moments (Br2)
Sender: pati@[150.161.40.38]
To: chemistry@ccl.net
Message-id: <38DBBE20.45609034@mail.npd.ufpe.br>
Organization: UFPE
MIME-version: 1.0
X-Mailer: Mozilla 4.7 [en] (X11; I; Linux 2.2.5-23cl i686)
Content-type: text/plain; charset=us-ascii
Content-transfer-encoding: 7bit
X-Accept-Language: en

    Dear CCL members,

    My research field involves Potodissociation Dynamics (theoretical
work) and I would be very grateful if someone could provide me the
following experimental data concerning Br2 (molecular bromine):
-transition dipole moments
-spin orbit coupling constants

Thanks for any help

Patricia Farias
DQF-UFPE
Recife-Brasil



