From tamasgunda@tigris.klte.hu  Fri Mar  7 03:27:42 1997
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From: "tamasgunda@tigris.klte.hu" <Tamas Gunda@www.ccl.net>
To: chemistry@www.ccl.net
Date: Fri, 7 Mar 1997 08:41:45 +1
Subject: Re: CCL:PDB format Documented?
Reply-To: tamasgunda@tigris.klte.hu
Priority: normal
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Nicholas C. DeMello wrote
> 
>    Folks,
> 
>       Can someone point me to documentation in the literature
>         regarding the PDB file format?  I've noticed that
>         several software products have slightly different
>         "PDB" output formats for small molecules.  I'm
>         interested in getting more information on what the
>         standard says... I'm just having trouble finding
>         where that standard is documented :-)
> 
>       Pointers to HTTP sites, journal articles, or other
>         places where the PDB standard is authoritatively
>         described would be appreciated.  Thanks,
> 
Hi,


2-3 years ago I asked for and got the documentation of PDB files from 
Brookhaven itself. Try now the url www.pdb.bnl.gov


Take into consideration, that although the PDB molfile
format itself is a strict one, the informations it contains may be redundant and
not all of the possible fields are necessary to include. In other words, the
chemical symbols and the coordinates of the atoms are a must, as these define
the structure, nearly all the other infos/fields can be neglected. It depends 
on the creator program, what is included and what not in the file, and on the
intelligence of the program using the file, how can it digest the content. For
example, the hydrogens and atom connectivities may be included or not, this is
usually a choice in the creator program. Whether the user program can add
hydrogens and generate connectivities, it is another question. 

For small molecules (not peptides) the atom structural fields must begin with
the token HETATM, and the lines should contain at least the coordinates and the 
atom symbols. Substructure information may be included or not. The 
connectivities are contained by the CONECT lines, but it is not necessary to 
include. The file must be ended with END.      

Tamas Gunda

 

************************************************************************
   Dr Tamas E. Gunda                   phone: (+36-52) 316666 ext 2479
   Research Group of Antibiotics       fax  : (+36-52) 310936
   L. Kossuth University               e-mail: tamasgunda@tigris.klte.hu
   POBox 36                                   
   H-4010 Debrecen
   Hungary
************************************************************************

From vkitzing@sunny.mpimf-heidelberg.mpg.de  Fri Mar  7 05:27:42 1997
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Date: Fri, 7 Mar 1997 10:41:40 +0100
To: <bantingl@cv.port.ac.uk>, chemistry@www.ccl.net
From: vkitzing@sunny.mpimf-heidelberg.mpg.de (Eberhard von Kitzing)
Subject: Re: CCL:HYDRATED METAL IONS


At 15:33 Uhr 06.03.1997, <bantingl@cv.port.ac.uk> wrote:
>I HAVE A COLLEAGUE WORKING ON AN ION CONDUCTING CHANNEL AND IS REQUESTING INFO
>ON 'EFFECTIVE' HYDRATED ION SIZE. ANY TAKERS FOR A SUITABLE REFERENCE ?

The classical reference is:
E. R. Nightingale Jr. (1959). "Phenomenological Theory of Ion Solvation.
Effective Radii of Hydrated Ions." Journal of Physical Chemistry [#361]
63(9) 1381-1387.

One can also use the result of Adams et al and interpolate:
David J. Adams, Terry M. Dwyer and Bertil Hille (1980). "The Permeability
of Endplate Channels to Monovalent and Divalent Metal Cations." The Journal
of General Physiology 75 493-510.

An alternative source for alkali metal ions is:
Dikeos Mario Soumpasis, Michel Robert-Nicoud and Thomas M. Jovin (1987).
"B-Z DNA conformational transition in 1:1 electrolytes: dependence upon
counter-ion size." Letters of the Federation of European Biochemical
Societies [#481] 213(2) 341-344.

======================================================================

Eberhard von Kitzing

Max-Planck-Institut fuer Medizinische Forschung
Jahnstr. 29
D 69115 Heidelberg
Germanny

email: vkitzing@sunny.mpimf-heidelberg.mpg.de
WWW: http://sunny.mpimf-heidelberg.mpg.de/people/vkitzing/Eberhard.html



From mebel@linsgi.iams.sinica.edu.tw  Fri Mar  7 06:27:41 1997
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Date: Wed, 7 Mar 2001 19:21:30 -0800 (PST)
From: "A. Mebel" <mebel@linsgi.iams.sinica.edu.tw>
To: chemistry@www.ccl.net
Subject: HONDO
Message-ID: <Pine.SGI.3.91.1010307191921.18237A-100000@linsgi.iams.sinica.edu.tw>
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  Dear CCLers:
  Can someone give me the e-mail address of the HONDO team where I can by 
a license for this program?
  Thank you very much in advance.

                            Alexander Mebel

From brain@amethyst.Chemie.Uni-Dortmund.de  Fri Mar  7 10:27:45 1997
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From: brain@amethyst.Chemie.Uni-Dortmund.de (Christoph Schwittek)
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Subject: electrochemistry
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A more practical question:

What time does it take for a molecule to be reduced by a catode in
solution? How is this time related to the typical timescale of diffusion
and to the time the electronic relaxation of the filled orbitals?
(Is the latter important at all, what is the timescale?)

Can anybody help me?

C.Schwittek


From rew@qc.ag-berlin.mpg.de  Fri Mar  7 11:27:54 1997
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From: rew@qc.ag-berlin.mpg.de (Rene Windiks)
Message-Id: <9703071611.AA15713@oberon.qc.ag-berlin.mpg.de>
Subject: Symmetry in DSOLID
To: chemistry@www.ccl.net
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Dear all,

since short time I using DSolid (DMOL for
periodic structures) to calculate crystals
with large unit cells.  The structures have
symmetry.  So it should be better exploiting
symmetry.  In the manual is written, that
DSolid treats crystalline systems as having P1
symmetry.
I asked the author of this program, B. Delley,
and he answered that the program is able exploiting
symmetry, but not by default.  Unfortunately,
he did not tell me how.

Does somebody know, how one takes symmetry into
consideration in DSolid ?  Has this something to
do with the SYMDEC file?  Is it similar as in 
DMOL?

Best wishes,

Rene Windiks

-- 
____________________________________________
Chemical Institute 
Quantum Chemistry Working Group
Humboldt University Berlin
Leader: Prof. J. Sauer

*   Rene Windiks

Jaegerstr. 10/11
D-10117 Berlin
Germany
Tel. +49-30-20192-306
Fax. +49-30-20192-302
e-mail: rew@qc.ag-berlin.mpg.de
____________________________________________

From daizadeh@indigo.ucdavis.edu  Fri Mar  7 11:33:18 1997
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From: "Iraj Daizadeh" <daizadeh@indigo.ucdavis.edu>
Message-Id: <9703070822.ZM22369@indigo.ucdavis.edu>
Date: Fri, 7 Mar 1997 08:22:15 -0800
In-Reply-To: "nick.c" <online@mactech.com>
        "CCL:PDB format Documented?" (Mar  6,  4:07pm)
References: <v03007801af450bdc3e40@[128.97.76.42]>
X-Mailer: Z-Mail (3.2.0 26oct94 MediaMail)
To: CHEMISTRY@www.ccl.net
Subject: Re: CCL:PDB format Documented?
Mime-Version: 1.0
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Hello.

The following url reference facilitated my understanding
of the PDB format:

http://www.pdb.bnl.gov/Format.doc/formatdoc.html#RTFToC56

Good Luck.

Iraj Daizadeh
Department of Chemistry
University of California
Davis, CA 95616

P.S.  This file existed circa. 07/95 hopefully it's still there.


On Mar 6,  4:07pm, nick.c wrote:
> Subject: CCL:PDB format Documented?
>
>
>    Folks,
>
>       Can someone point me to documentation in the literature
>         regarding the PDB file format?  I've noticed that
>         several software products have slightly different
>         "PDB" output formats for small molecules.  I'm
>         interested in getting more information on what the
>         standard says... I'm just having trouble finding
>         where that standard is documented :-)
>
>       Pointers to HTTP sites, journal articles, or other
>         places where the PDB standard is authoritatively
>         described would be appreciated.  Thanks,
>
>
>
>
>
> ____Nicholas C. DeMello, Ph.D.________________________________________
>
>    Online at MacTech Magazine, the Journal of Macintosh Programming
>      http://www.MacTech.com/
>                                        _/   _/  _/  _/_/_/   _/   _/
>   Chemistry: Nick@chem.UCLA.edu       _/_/ _/  _/  _/   _/  _/_/_/
>     MacTech: Online@MacTech.com      _/ _/_/  _/  _/       _/ _/
>        http://www.chem.ucla.edu/~nick/   _/  _/   _/_/_/  _/   _/
>
>
>
>
> -------This is added Automatically by the Software--------
> -- Original Sender Envelope Address: online@mactech.com
> -- Original Sender From: Address: online@mactech.com
> CHEMISTRY@www.ccl.net: Everybody | CHEMISTRY-REQUEST@www.ccl.net: Coordinator
> MAILSERV@www.ccl.net: HELP CHEMISTRY or HELP SEARCH | Gopher: www.ccl.net 73
> Anon. ftp: www.ccl.net   | CHEMISTRY-SEARCH@www.ccl.net -- archive search
>              Web: http://www.ccl.net/chemistry.html
>-- End of excerpt from nick.c



From youngd2@mallard.duc.auburn.edu  Fri Mar  7 11:36:40 1997
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From: youngd2@mail.auburn.edu
Message-Id: <199703071616.KAA03874@wood.mail.auburn.edu>
To: CHEMISTRY@www.ccl.net
Subject: Chem Topic: Excited States



Hello all,

	I have written the following short essay for my users and am 
posting it here for your enjoyment and comments.  Please let me know
if I missed any important techniques.

	My compilation of chemical topics can be accessed via the web 
at URL http://www.auburn.edu/~youngd2/topics/contents.html

                                Dave Young
                                youngd2@mail.auburn.edu

---------------------------------------------------------------------------

                       Calculating Electronic Excited States

   				   David Young

			Division of University Computing
                       		 144 Parker Hall
                      	        Auburn University
                       		Auburn, AL 36849


INTRODUCTION

	This is an introduction to the techniques used for the calculation
of electronic excited states of molecules (sometimes called eximers).  
Specifically, these are methods for obtaining wave functions for the
excited states of a molecule from which energies and other molecular properties 
(such as dipole moments) can be calculated.  These calculations are an 
important tool for the analysis of spectroscopy, reaction mechanisms
and other excited state phenomena.

	These same techniques may also be necessary to find the ground state
wave function.  Determining the ground state electron configuration can
be particularly difficult for compounds with very low energy excited states.

	This document is concerned only with ab initio calculations.  These
are calculations in which only the theory of quantum mechanics is applied
with no experimental data used in the calculation.  Some of these techniques
are also applicable to certain classes of semiempirical calculations.

	This write up is not intended to be a detailed description. 
It is meant to be a short introduction with a discussion of strengths and
weaknesses of various methods.  This should also serve as a check list
of available methods when faced with computational difficulties.  References
are provided for more detailed discussions information.


SPIN STATES

	Ab initio programs attempt to compute the lowest energy state of
a specified multiplicity.  Thus calculations for different spin states 
will give a lowest energy state and a few of the excited states.  This 
is most often done to determine singlet - triplet gaps in organic molecules.


CIS

	A single excitation configuration interaction (CIS) calculation is
probably the most common way to get excited state energies.  This is because
it is one of the easiest calculations to perform.

	A configuration interaction calculation uses molecular orbitals
that have been optimized typically with a Hartree-Fock (HF) calculation. 
Generalized Valence Bond (GVB) and multi-configuration self consistent
field (MCSCF) calculations can also be used as a starting point for
a configuration interaction calculation.

	A CIS calculation starts with this initial set of orbitals and 
moves one electron to one of the virtual orbitals from the original 
calculation.  This gives a description of one of the excited states of
the molecule, but does not change the quality of the description of the
ground state as double excitation CIs do.  This gives a wave function of 
somewhat lesser quality than the original calculation since the orbitals 
have been optimized for the ground state.  Often this results in the ground 
state energy being a bit low relative to the other states.

	A CIS calculation is not extremely accurate.  However, it has the
advantage of being able to compute many excited state energies easily.


INITIAL GUESS

	If the initial guess for a calculation is very close to an
excited state wave function, the calculation may converge to that
excited state.  This is typically done by doing an initial calculation
then using it's wave function with some of the orbitals switched as
the initial guess for another calculation.  

	The advantage of this method is that the orbitals have been 
optimized for the excited state.  

	The disadvantage is that there is no guarantee that it will work.  
If there is no energy barrier between the initial guess and the ground state 
wave function, the entire calculation will converge back to the ground state.
The convergence path may take the calculation to an undesired state in
any case.

	A second disadvantage of this technique applies if the state is the 
same symmetry as a lower energy state.  There is no guarantee that the
state obtained is completely orthogonal to the ground state.  This means
that the wave function obtained may be some mix of the lower energy
state and a higher energy state.  In practice, this type of calculation
only converges to a higher state if a fairly reasonable description of
the excited state wave function is obtained.  Mixing tends to be a significant 
concern if the orbital energies are very close together or the system is very 
sensitive to correlation effects.


BLOCK DIAGONAL HAMILTONIANS

	Most ab initio calculations use symmetry adapted molecular orbitals.
Under this scheme, the Hamiltonian matrix is block diagonal meaning that 
every molecular orbital will behave according to the symmetry of one of the 
irreducible representations of the point group.  No orbitals will be described
by a mixing of different irreducible representations.

	Some programs such as COLUMBUS, DMOL and GAMESS actually set up a 
separate matrix for each irriducible representation and solve them separately.
Such programs give the user the option of defining how many electrons
are of each irreducible representation.  This defines the symmetry of the
wave function.  In this case the resulting wave function is the lowest
energy wave function of a particular symmetry.  

	This is a very good way to get excited states which differ in 
symmetry from the ground state and are the lowest energy state within that 
symmetry.


HIGHER ROOTS OF A CI

	For configuration interaction calculations of double excitations
or higher, it is possible to solve the CI super-matrix for the second root,
third root, fourth root, etc.  

	This is a very reliable way to get a high quality wave function for 
the first few excited states.  For higher excited states, CPU times become 
very large since more iterations are generally needed to converge the
CI calculation.


NEGLECTING A BASIS FUNCTION

	Some programs, such as COLUMBUS, allow a calculation to be done 
with some orbitals completely neglected from the calculation.  For example,
in a transition metal compound you could work with four d functions so that
the calculation would have no way to occupy the function that was left out.

	This is a reliable way to get an excited state wave function even
when it is not the lowest energy wave function of that symmetry.  However
it might take a bit of work to construct the input file depending upon the 
individual program.


IMPOSING ORTHOGONALITY - DFT TECHNIQUES

	Traditionally, excited states have not been one of the strong
points of density functional theory.  This is due to the difficulty
in ensuring orthogonality to the ground state wave function when 
no wave functions are being used in the calculation.

	The easiest excited states to find using density functional 
theory techniques are those which are the lowest state of a given 
symmetry thus using a ground state calculation.

	A promising techniques is one which uses a variational bound
for the average of the first M states of a molecule.

	A few other options have been examined.  However, there is not
yet a large enough volume of work applying DFT to excited states to
predict the reliability of any of these techniques.


IMPOSING ORTHOGONALITY - QMC TECHNIQUES

	Quantum Monte Carlo (QMC) methods are computations which use a
statistical integration to calculate integrals which could not be 
evaluated analytically.  These calculations can be extremely accurate,
but often at the expense of enormous CPU times.

	There are a number of methods for getting excited state energies
>from QMC calculations.  These methods will only be mentioned here and
are explained more fully in the text by Hammond, Lester and Reynolds 
referenced at the end of this document.

	Computations done in imaginary time can yield an excited state
energy by a transformation of the energy decay curve.

	If an accurate description of the ground state is already available,
an excited state description can be obtained by forcing the wave function
to be orthogonal to the ground state wave function.

	Diffusion and Green's function QMC calculations are often done
using a fixed node approximation.  Within this scheme, the nodal surfaces
used define the state that is obtained as well as ensuring an antisymmetric 
wave function.

	Matrix QMC procedures similar to configuration interaction 
treatments have been devised in an attempt to calculate many states
concurrently.  These methods are not yet well developed as evidenced
by oscillatory behavior in the excited state energies.
 

FURTHER INFORMATION

There are many books on the principles of quantum mechanics and every
physical chemistry text has an introductory treatment.  The
work which I am listing here is a two volume set with each chapter
broken into a basic and advanced sections making it excellent for
both intermediate and advanced users.
C. Cohen-Tannoudji, B. Diu, F. Laloe "Quantum Mechanics Volumes I & II" 
Wiley-Interscience (1977)

For an introduction to quantum chemistry see
D. A. McQuarrie "Quantum Chemistry" University Science Books (1983)

A graduate level text on quantum chemistry is
I. N. Levine "Quantum Chemistry" Prentice Hall (1991)

For quantum Monte Carlo methods, order the following book using 
ISBN 981-02-0322-5 because the title is listed incorrectly in 
'Books in Print'.
B. L. Hammond, W. A. Lester, Jr., P. J. Reynolds "Monte Carlo Methods
in Ab Initio Quantum Chemistry" World Scientific (1994)

For density functional theory see
R. G. Parr, W. Yang "Density-Functional Theory of Atoms and Molecules"
Oxford (1989)

There is a comprehensive listing of all available molecular modeling
software and structural databanks, free or not, in appendix 2 of
"Reviews in Computational Chemistry Volume 6" 
Ed. K. B. Lipkowitz and D. B. Boyd, VCH (1995)

---------------------------------------------------------------------------


From tvd@msi.com  Fri Mar  7 14:27:46 1997
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Date: Fri, 7 Mar 1997 10:50:28 -0800
From: tvd@msi.com (Ton van Daelen)
Message-Id: <199703071850.KAA15447@iris69.msi.com>
To: CHEMISTRY@www.ccl.net
Subject: ACS seminar on Cerius2 software developer's kit



To all software developers out there...

Molecular Simulations is organizing a seminar on the 
Cerius2 Software Developer's Kit. The seminar is free 
of charge, but please sign up soon as space is limited.

With best regards - Ton van Daelen

----------------------------------------------

Cerius2 Software Developer's Kit Seminar
ACS San Fransisco
Rm 276, Moscone Convention Center
9:00am-11:00am, April 14, 1997


 During the ACS meeting in San Francisco
 MSI is organizing a seminar on the Cerius2
 software developer's toolkit (C2.SDK).
 C2.SDK allows you to plug your own
 chemistry applications into MSI's Cerius2
 modeling environment. You can link in
 existing software or develop entirely new
 applications. You concentrate on the
 scientific side of your program and C2.SDK
 takes care of the molecular graphics, window
 management, and data visualization.

 C2.SDK is used to develop scientific
 applications that solve research problems in
 fields including polymer science, rational
 drug design, combinatorial chemistry,
 catalysis, chemical reactions, and protein
 chemistry. The C2.SDK toolkit consists of a
 rich API set dealing with all aspects of
 interfacing chemistry codes, including GUI
 design, structure visualization, graphing, and
 volumetric display. Applications can be
 written in FORTRAN, C, or C++.

 The seminar will also discuss imminent SDK
 extensions that allow you to run applications
 through the internet, or an intranet, from a
 web browser interface on your desktop
 computer (PC, or MAC).

 In addition, we will demonstrate the use of
 C2.Tcl, the scripting language for the Cerius2
 interface, for simple customization of routine
 modeling operations. C2.Tcl is based on the
 standard tcl scripting language, it lets you put
 together a simple application with its own
 graphical user interface in a matter of
 minutes. C2.Tcl aids in all aspects of
 molecular modeling, in particular in drug
 design and protein analysis.

 For more information about C2.SDK and C2.Tcl:

 http://www.msi.com/support/sdk/

 The seminar is offered free of charge.
 Because space is limited, attendance is by
 registration only. The deadline for
 advanced registration is April 7. You can
 sign up at the following URL:

 http://www.acs.org/meetings/sanfran/exhwksp.html

  Ton van Daelen  	Product Manager Software Developer's Kit
           
       __o                                 	E: tvd@msi.com
     _`\<,_       	Molecular Simulations	P: -1-619-546-5329
    (*)/ (*)    	9685 Scranton Road	F: -1-619-458-0136
  /\/\/\/\/\/\    	San Diego, CA 92121	W: http://www.msi.com

Check out What's New in SDK on the SDK web pages at http://www.msi.com/support/sdk/

From ccl@www.ccl.net  Thu Mar  6 05:44:12 1997
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	id AA06949; Thu, 6 Mar 97 11:15:40 +0100
Date: Thu, 6 Mar 1997 11:15:39 +0100 (MET)
From: Cezary Czaplewski <czarek@rutyl.chem.univ.gda.pl>
Subject: Re: CCL: G94 on LINUX
To: R29CLOSE@ETSU.ETSU-TN.EDU
Cc: chemistry@ccl.net
In-Reply-To: <199702281901.OAA24055@bedrock.ccl.net>
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On Fri, 28 Feb 1997 R29CLOSE@ETSU.ETSU-TN.EDU wrote:

> 
>   It seems that I have a faulty memory chip.  My computer, a Gateway
> P6 has 64 Mbytes of new memory.  The machine says all is ok on boot-
> up.  But I have random problems with the C-compiler quitting.
> So maybe there is a memory problem.  Gaussian suggested removing
> or switching memory.  Now it appear I can compile the program
> with only 2x16 Mbytes of memory.

There is also a possibility that memory is not completely bad but just too 
slow. I had similar problems - compilation of large code crashing with 
Signal 11. I have changed just one parameter in chipset features setup - 
"DRAM Write CAS  Width" from 2T to 3T and now everything is OK.


				Cezary Czaplewski
                                Faculty of Chemistry
                                University of Gdansk
									


From l504@cacr.ioc.ac.ru  Thu Mar  6 18:27:40 1997
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From: "Sergey Nogaev" <l504@cacr.ioc.ac.ru>
Date: Fri, 7 Mar 97 02:48:59 +0400
Message-Id: <10142.l504@cacr.ioc.ac.ru>
X-POPmail-Charset: IBM 8-Bit
To: chemistry@www.ccl.net
Subject: Studies on ozone




Dear Collegues,
We have just started the studies on ozone interaction with
different molecules, mainly F- and Cl-containing, using
quantum chemical methods. This is in connection with 
stratospheric ozone depletion problem. 
I would be happy if somebody share his/her experience
in this field.
Any references on this subject are appreciated.
Sincerely,
          Sergey Nogaev, Institute of Chemical Physics, Russia.


From wagenert@Mailer.Uni-Marburg.DE  Fri Mar  7 05:34:02 1997
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From: Thomas Wagener <wagenert@Mailer.Uni-Marburg.DE>
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To: Computational Chemistry List <CHEMISTRY@www.ccl.net>
Subject: Fixing Electronic Configuration in Atoms
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Hi,

since I would like to add an polarization f-funtion to an ECP basis set of
palladium I am trying to get the DFT atomic energies for the 1S, 3D and 3F
configuration. The singlet state is no trouble at all as well as the 3D
state which comes out automatically if I force the multiplicity to be a
triplet but I am not able to fix the electronic configuration to the 3F
configuration.
Any attempt with guess=alter has failed so far though the program claims 
to switch the correct orbitals. So, is there any way to force Gaussian to
optimize a fixed electronic configuration?

TIA
	Thomas  

- "You are wrong! 2+2=5.8354! Please adjust your equipment accordingly."
			The Computer (your friend)

*****************************************************************************
* Thomas Wagener                   *  Tel: ++49-(0)6421-285561              *
* FB Chemie                        *                                        *
* Phillips-Universitaet Marburg    *  Email: wagenert@mailer.uni-marburg.de *
*                                  *                                        *
* 35032 Marburg                    *                                        *
* Germany                          *                                        *
*****************************************************************************



From BISETTYK@wpogate.mlsultan.ac.za  Fri Mar  7 06:37:37 1997
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From: "KRISHNA BISETTY" <BISETTYK@wpogate.mlsultan.ac.za>
To: chemistry@www.ccl.net
Date: Fri, 07 Mar 1997 12:45:00 +200
Subject: Request-Modeling Biopolymers
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Dear Netters,

I am carrying out computational studies on some small peptide molecules
as test cases in terms of reproducibility, and presently using the PC version
of HyperChem.

However, I would be grateful if someone could please recommend other
suitable packages for both molecular mechanics and semi-empirical
applications.

We are investigating CHARMM and the pc version of Spartan. Any
hints???

Thanking you in advance.

Best wishes,


---------------------------------------------------------------------------------------------
Vincent Bisetty
Department of Chemistry
ML Sultan Technikon
Durban
South Africa
BisettyK@wpo.MLSULTAN. ac.za

-------------------------------------------------------------------------------------------------


From info@chemcomp.com  Fri Mar  7 16:27:50 1997
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Chemical Computing Group, Inc. has posted a text on the CCL Commercial
Software List announcing the release of it's new Molecular Operating
Environment (MOE).

We encourage you to read about the latest advance in computational
chemistry software by visiting:

          gopher://www.ccl.net/11/software/info-on-software/

or by visiting our website:

          http://www.chemcomp.com


Thank you,

Bill Hayden
Vice President
CHEMICAL COMPUTING GROUP, INC.

From cmartin@curie.syr.edu  Fri Mar  7 16:36:02 1997
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From: Charles Martin <cmartin@curie.syr.edu>
To: youngd2@mail.auburn.edu
Cc: CHEMISTRY@www.ccl.net
Subject: CCL:Chem Topic: Excited States
In-Reply-To: <199703071616.KAA03874@wood.mail.auburn.edu>
References: <199703071616.KAA03874@wood.mail.auburn.edu>


 > 
 > 	I have written the following short essay for my users and am 
 > posting it here for your enjoyment and comments.  Please let me know
 > if I missed any important techniques.
 > 
	What about many-body theories?  These include
effective operator theory, many-body green's functions, 
etc.  

	Chuck Martin

-- 
========================================================
 ||     Charles H. Martin                            ||
 ||     2-004 Center for Science and Technology      ||
 ||     W. M. Keck Center for Molecular Electronics  ||
 ||     Department of Chemistry                      ||
 ||     Syracuse University                          ||
 ||     Syracuse, NY  13244                          ||
--------------------------------------------------------
 ||     cmartin@cat.syr.edu                          ||
 ||     cmartin@rainbow.uchicago.edu                 ||
 ||     CELL   (315) 415-2093                        ||
 ||     OFFICE (315) 443-3754                        ||
 ||     LAB    (315) 443-5928                        ||
 ||     FAX    (315) 443-4070                        ||
========================================================

From csg.admin@amgen.com  Fri Mar  7 16:40:14 1997
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Subject: CCL-ACS seminar on Cerius2 
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Mail*Link=AE SMTP               CCL:ACS seminar on Cerius2 software devel=
oper's kit


To all software developers out there...

Molecular Simulations is organizing a seminar on the=20
Cerius2 Software Developer's Kit. The seminar is free=20
of charge, but please sign up soon as space is limited.

With best regards - Ton van Daelen

----------------------------------------------

Cerius2 Software Developer's Kit Seminar
ACS San Fransisco
Rm 276, Moscone Convention Center
9:00am-11:00am, April 14, 1997


 During the ACS meeting in San Francisco
 MSI is organizing a seminar on the Cerius2
 software developer's toolkit (C2.SDK).
 C2.SDK allows you to plug your own
 chemistry applications into MSI's Cerius2
 modeling environment. You can link in
 existing software or develop entirely new
 applications. You concentrate on the
 scientific side of your program and C2.SDK
 takes care of the molecular graphics, window
 management, and data visualization.

 C2.SDK is used to develop scientific
 applications that solve research problems in
 fields including polymer science, rational
 drug design, combinatorial chemistry,
 catalysis, chemical reactions, and protein
 chemistry. The C2.SDK toolkit consists of a
 rich API set dealing with all aspects of
 interfacing chemistry codes, including GUI
 design, structure visualization, graphing, and
 volumetric display. Applications can be
 written in FORTRAN, C, or C++.

 The seminar will also discuss imminent SDK
 extensions that allow you to run applications
 through the internet, or an intranet, from a
 web browser interface on your desktop
 computer (PC, or MAC).

 In addition, we will demonstrate the use of
 C2.Tcl, the scripting language for the Cerius2
 interface, for simple customization of routine
 modeling operations. C2.Tcl is based on the
 standard tcl scripting language, it lets you put
 together a simple application with its own
 graphical user interface in a matter of
 minutes. C2.Tcl aids in all aspects of
 molecular modeling, in particular in drug
 design and protein analysis.

 For more information about C2.SDK and C2.Tcl:

 http://www.msi.com/support/sdk/

 The seminar is offered free of charge.
 Because space is limited, attendance is by
 registration only. The deadline for
 advanced registration is April 7. You can
 sign up at the following URL:

 http://www.acs.org/meetings/sanfran/exhwksp.html

  Ton van Daelen  	Product Manager Software Developer's Kit
          =20
       __o                                 	E: tvd@msi.com
     _`\<,_       	Molecular Simulations	P: -1-619-546-5329
    (*)/ (*)    	9685 Scranton Road	F: -1-619-458-0136
  /\/\/\/\/\/\    	San Diego, CA 92121	W: http://www.msi.com

Check out What's New in SDK on the SDK web pages at http://www.msi.com/su=
pport/sdk/

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From bruce@cosy.utmb.edu  Fri Mar  7 18:27:49 1997
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	 id QAA07916; Fri, 7 Mar 1997 16:47:47 -0600
From: "Bruce A. Luxon" <bruce@cosy.utmb.edu>
Message-Id: <9703071647.ZM7914@cosy.utmb.edu>
Date: Fri, 7 Mar 1997 16:47:39 -0600
Organization: Sealy Center for Structural Biology
Reply-To: bruce@nmr.utmb.edu
X-Phone: (409) 747-6802
X-Mailer: Z-Mail (3.2.0 26oct94 MediaMail)
To: CHEMISTRY@www.ccl.net, str-nmr@net.bio.NET
Subject: NMR SOFTWARE UPDATE:  MORASS 2.3 
Mime-Version: 1.0
Content-Type: text/plain; charset=us-ascii



NMR SOFTWARE ANNOUNCEMENT:

MORASS 2.3 is now available for downloading with improved handling of
proteins, RNA and DNA over previous versions.

MORASS - Multiple Overhauser Relaxation AnalysiS and Simulation - uses
a full hybrid matrix eigenvalue/eigenvector solution to the Bloch equations
to derive cross-relaxation rates and interproton distances for determining
the NMR solution structures of DNA/RNA and proteins.

MORASS is available free for academic use from the research laboratories
of Prof. David Gorenstein.  Distribution is available from:

  http://www.nmr.utmb.edu/ provides downloading & information via the WWW.

  nmr.utmb.edu in /pub/morass for standard ftp anonymous protocol.

For more information contact: Bruce Luxon  bruce@nmr.utmb.edu


-- 

*=-=-=-=-=-=-=-=-=-=-=-=-=-=-=-=-=-=-=-=-=-=-=-=-=-=-=-=-=-=-=-=-=-=-=-=-=-*
*  Bruce A. Luxon, Ph.D                                                    *
*  Assistant Professor                                                     *
*  Sealy Center for Structural Biology                                     U
*  Dept. of Human Biological Chemistry & Genetics                          T
*  University of Texas Medical Branch                                      M
*  Galveston, TX   77555-1157                                              B
*                                                                          *
*  (409)747-6802; Fax (409)747-6850              http://www.hbcg.utmb.edu/ *
*  bruce@nmr.utmb.edu                            http://www.nmr.utmb.edu/  *
*=-=-=-=-=-=-=-=-=-=-=-=-=-=-=-=-=-=-=-=-=-=-=-=-=-=-=-=-=-=-=-=-=-=-=-=-=-*

From matteo@pauli.mbi.ucla.edu  Fri Mar  7 21:27:51 1997
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From: Matteo Pellegrini <matteo@pauli.mbi.ucla.edu>
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Dear netters,
    
    Would anyone tell me which package is able to calculate CD 
related properties (rotatory strength) for peptides?

    
   Sincerely

   Matteo Pellegrini
   matteo@galileo.mbi.ucla.edu

