From Jennie.Weston@org.chemie.uni-giessen.de  Thu Nov  7 05:11:47 1996
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From: Jennie.Weston@org.chemie.uni-giessen.de (Jennie Weston)
Message-Id: <9611070904.AA13739@maier.org.chemie.uni-giessen.de>
Subject: Re: CCL:G94 nbo problem THANKS+SOLN
To: CHEMISTRY@www.ccl.net
Date: Thu, 7 Nov 1996 10:04:45 +0100 (CET)
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Dear Everybody,

Thanks for the helpful comments 
Doug Fox at gaussian had the soln. (Thanks Doug...)
Some Unix systems eat the $ symbol(IBM RS600) if it is standing in column 1.
Gives really nice errors. 
Soln. put some white space before the $nbo or $del commands in gaussian
input files.

> 
>   Jennie,
> 
>   check out g94/tests/com/test166.com for a more extensive example.  The
> basic input is POP=NBODEL which looks for the required NBO input at the
> end just as you have it except put the $ in column 2 to make sure Unix
> does not consume it.
> 
> > Hello everybody,
> > 
> > I have a little problem with the nbo implementation in gaussian94.
> > According to the NBO manual, in order to do matrix element deletions,
> > i need to use a non-standard gaussian input stream. Well, i have an
> > nbo manual version 3.0, which describes the implementation in gaussian88.
> > The code has changed a little since then........
> > I managed to get the manual's example working for a normal nbo analysis,
> > but when it enters the link to calculate the matrix deletion, my job
> > dies wanting a g94-5262.nbo file. Does any Guru out there know how to
> > induce the program to write this file? Or is there a simpler way to do
> > this? A working example file would be AWFULLY nice.......
> > 

From hinsen@ibs.ibs.fr  Thu Nov  7 05:23:32 1996
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From: Konrad Hinsen <hinsen@ibs.ibs.fr>
To: walt@panix.com
Cc: echamot@xnet.com, rochus@felix.anorg.chemie.tu-muenchen.de,
        chemistry@www.ccl.net
In-Reply-To: <Pine.SUN.3.94.961106142715.15909B-100000@panix3.panix.com>
	(message from Walter Polkosnik on Wed, 6 Nov 1996 14:33:30 -0500
	(EST))
Subject: Re: CCL:MD/MM combination


> What I was trying to point out (perhaps in a very roundabout way) is that
> defining 'temperature' in this way for an MD situation is a problem (and it
> seems like all MD simply uses ideal gas results). This 'temperature' is not
> simply related to the real physical temperature.

I still don't see the problem, much less where "ideal gas" results are
used. Of course defining temperature via the equipartition theorem is
something else than using the proper definition, and it makes sense
only under certain assumptions (equilibrium, sufficiently large
system, etc.)  that are perhaps not fulfilled and that many users are
not aware of. But then that is true for many other subtle problems
related to MD. For example, conventional wisdom says that the time
step is small enough if the energy is reasonably well conserved, even
if high frequencies are not sufficiently sampled and other conserved
quantities (momentum, angular momentum) show a constant drift.

I do agree, of course, that such topics should be discussed and
analyzed, and that users of MD should be aware of the huge range
of assumptions they are implicitly making.

-- 
-------------------------------------------------------------------------------
Konrad Hinsen                          | E-Mail: hinsen@ibs.ibs.fr
Laboratoire de Dynamique Moleculaire   | Tel.: +33-76.88.99.28
Institut de Biologie Structurale       | Fax:  +33-76.88.54.94
41, av. des Martyrs                    | Deutsch/Esperanto/English/
38027 Grenoble Cedex 1, France         | Nederlands/Francais
-------------------------------------------------------------------------------

From hutschka@quantix.u-strasbg.fr  Thu Nov  7 08:11:48 1996
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To: chemistry@www.ccl.net
Subject: SUMARY:MP2 density in CHK file.
Cc: hutschka@quantix.u-strasbg.fr
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Hello,

Here is the sumary about my question to the CCL:

THE QUESTION:

I am using gaussian92 to fit atomic charges with potential
derived methods.
To save computer time the electronic density can be read
from the checkpoint file to avoid to calculate it several time
if you want to use it for different calculations.
By default, the HF density is saved in the CHK file.
Since I want to use the MP2 density, could somebody tell me if
there is a way to save the MP2 density in the CHK file and if
so, how to do it ??
More is it possible to save both the HF and the MP2 densities in the
same CHK file??

******************************************************************

THE ANSWERS:

******************************************************************
From Seiji Mori
e-mail: smori@utsc3.chem.s.u-tokyo.ac.jp
****************************************

By default, even in the MP2 calculations, SCF density was shown in the
output file and
stored in chkpoint file.
To show and store MP2 density to checkpoint file, you need to add the option ,
"density=MP2" or "density=current", that is OK.

> More is it possible to save both the HF and the MP2 densities in the
> same CHK file??

Of course, you can split to two jobs (SCF and MP2 density calculations) but
I do not know .

*******************************************************************
From Jean-Marie Teuler
e-mail: teuler@idris.fr

In French..

Je vous reponds directement concernant votre question concernant les matrices
de densite.

En effet, par defaut c'est la matrice de densite HF qui est stockee dans le
checkpoint.
- Si vous specifiez DENSITY=MP2, ce sera la matrice MP2.
- Si vous specifiez DENSITY=ALL, les deux matrices seront stockees et vous
pourrez selectionner celle que vous voulez utiliser avec ce meme mot-cle
DENSITY.

*********************************************************************
From Michael Schimeczek
e-mail: schimi@sg1506.chemie.uni-marburg.de
*******************************************

first of all, I am using Gaussian94 not 92, so I'm not sure if the results
will be the same, but here we go:

First, to check if the resulting checkpoint file really contains the desired
data, use the program formchk, which resides in the gaussian executable
directory. It reads in your checkpoint file and writes a formatted
checkpointfile (name.fchk) that you can easily read.

Then, use the keyword DENSITY in the route card.
The options are: HF, MP2, ALL, CURRENT, and several others for CI etc.
Normally, the HF density will be used as default for pop analysis (and also for
writing to the checkpoint), but if you specify DENSITY=CURRENT, the density
belonging to the method you are using is taken.
Gaussian94 then writes both HF and MP2 densities to the chkfile (if you did an
MP2 calculation).

Hope this helps (and works for G92, too!)

**********************************************************************
From Douglas J. Fox
e-mail: help@gaussian.com
*************************

   If you run G92 with MP2 DENSITY=3DCurrent, both the HF and MP2 density
are saved.  You can then use DENSITY=3D(CHECK,MP2) to recover the MP2
density or DENSITY=3DCHECK to get the HF density.

**********************************************************************

Thanks to all for your help.

=============================================================================
¤  François HUTSCHKA                 Ph.D. Student in Quantum Chemistry     ¤
¤                                                                           ¤
¤  Laboratoire de Chimie Quantique                                          ¤
¤  UPR 139 du CNRS                                                          ¤
¤  4, rue Blaise Pascal              Phone:  (33).03.88.41.60.32            ¤
¤  67000 STRASBOURG                  Fax:    (33).03.88.61.20.85            ¤
¤  FRANCE                            E-Mail: hutschka@quantix.u-strasbg.fr  ¤
=============================================================================


From dsmith@CTCnet.Net  Thu Nov  7 10:11:57 1996
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Subject: need IR frequencies/intensities


Dear All:
        Because we just moved our offices, I do not have access to my usual
sources of information, so I would appreciate an answer to the following
simple question.

        Can someone provide me with the EXPERIMENTAL IR frequencies and
intensities for nitromethane and nitrobenzene?  I am particularly interested
in the frequencies related to the nitro group.

Doug
--
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From dsmith@CTCnet.Net  Thu Nov  7 10:24:38 1996
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The DASGroup, Inc. has moved.  Our new address and contact information are
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--
Dr. Douglas A. Smith, President and CEO     |  voice: (814) 255-7859
The DASGroup, Inc.                          |    fax: (814) 255-3517
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From val@nmr1.ioc.ac.ru  Thu Nov  7 12:11:52 1996
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Date: Tue, 7 Nov 95 19:58:35 +0300
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Subject: All atom Force Field



Dear CCL'ers,

I am looking for  programs (preferably  freeware or shareware) with 
full periodic table force fields: all atom type version of the YETI force 
field, Universal Force Field, DREIDING-style scheme and other.

I will summarize.

Thank you.

Sincerely,
Valentin.


@              Valentin P. Ananikov  (Post-Graduate Student)    @      
 @    NMR Laboratory                                             @
  @    N.D. Zelinsky Institute of Organic Chemistry               @
   @    Leninsky Prospect 47                                       @
    @    Moscow  117913                                             @
     @    Russia                                                     @


From ryszard@msi.com  Thu Nov  7 13:11:52 1996
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Date: Thu, 7 Nov 1996 12:58:08 -0500 (EST)
From: Ryszard Czerminski <ryszard@msi.com>
To: Konrad Hinsen <hinsen@ibs.ibs.fr>
Cc: walt@panix.com, echamot@xnet.com, rochus@felix.anorg.chemie.tu-muenchen.de,
        chemistry@www.ccl.net
Subject: Re: CCL:MD/MM combination
In-Reply-To: <199611071007.LAA13033@ibs.ibs.fr>
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Few formulas from text book
(D. A. McQuarrie "Statistical Thermodynamics") :

In microcanonical ensemble ( H(p,q) = E = const)
partition function is defined as the volume of
phase space accessible at constant energy E

$$
   \Omega(E) = \int\limits_{H(p,q)=E} dp dq
$$

and thermodynamical temperature is defined by

$$
    {1 \over kT} = {\Bigl( {{\partial \Omega(E)} \over
                   {\partial E}} \Bigr)}_{N,V}
$$

(which is just different way of writing 1/T= dS/dE, since
S = k ln $\Omega$) so in order to calculate it, it is
necessary to be able to calculate partition function $\Omega(E)$
which is formidable challenge for any system a little
bit more complicated then ideal gases
and harmonic oscillators (not to mention big protein in water with
ions, etc...).

Interesting question remains how much proper thermodynamic
temperature differs from "temperature" calculated from an average kinetic
energy using equipartition theorem with all its limitations discussed so far.

 ..................................
Ryszard Czerminski
Molecular Simulations Incorporated
8 New England Executive Park
Burlington, MA 01803-5297
tel: (617)229-8875 x 217 or 229-9800
fax: (617)229-9899
e-mail: ryszard@msi.com


From debay93k@ibmmail.com  Thu Nov  7 15:11:54 1996
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Subject: job opportunity at BAYER/Wuppertal                                                                                           



                           Start of Attached Message
                           =========================

































































                    Computational Chemist at Bayer

In our German Pharmaceutical Research Centre at Wuppertal an opportunity
has arisen for a computational chemist to join our Structural Research Group.

Our Profile:
Bayer is a recognized research-based healthcare company headquartered in
Leverkusen/Germany. [For more details please refer to http://www.bayer-ag.de]

Your Task:
The successful candidate will collaborate in a multidisciplinary team
responsible for Structural Analysis (including High Field NMR and X-Ray
Analysis) and Molecular Modelling in close cooperation with medicinal
chemists and pharmacologists. State-of-the art equipment for computational
chemistry is available as well as almost complete access to virtually all
TRIPOS and MSI/Biosym software modules.

Your Profile:
We are currently seeking a PhD research scientist (Computational Chemist)
with significant professional expertise in at least one of the following
areas:

    -   use and/or development of molecular modelling methods for proteins,
        protein/small molecule interaction or indirect drug design techniques.
    -   Use of De novo Drug Design and/or Structure Activity Relationship
        methodology
    -   usage of 2D/3D-Databases and calculated molecular properties in
        course of drug finding process, high throughput screening analysis
        and/or structure and property-based design of libraries for automated
        synthesis.
    -   bio-informatics or biochemistry including homology modelling of
        proteins

Working experience in a pharmaceutical company's molecular modelling group
will be an advantage. The successful applicant must have a good working
knowledge of chemistry. UNIX experience and C-programming skills are
desirable. Demonstrable expertise and experience in available commercial
modelling software packages (e.g. the TRIPOS and MSI suite of programs) will
be an advantage too.

-------------------------------------------------------------------------------
Contact Address:
If your background and personal experience fits to this profile,  please apply
with full CV to:

    Bayer AG
    Mr. G. Ritter
    Personalmarketing
    Hauptstr. 119
    D51368 Leverkusen
------------------------------------------------------------------------------

In urgent cases please contact:

Axel Jensen,  PhD
Pharmaceutical Research Centre
PH-RSR
D42096 Wuppertal
Germany
email: DEBAY93K@IBMMAIL.COM

