From DURRAN@chem.surrey.ac.uk  Thu Apr  6 06:27:13 1995
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To: chemistry@ccl.net
From: Michael <DURRAN@chem.surrey.ac.uk>
Organization: Chemistry Department, Uni of Surrey
Date:         Thu, 6 Apr 1995 11:20:09 GMT
Subject:      Basis sets
Priority: normal
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I would be grateful if anybody could provide information /  references
concerning the availability of the following basis sets :

4-31+G
4-31G*

Thanks 

Mike 

chp1dd@central.surrey.ac.uk

From martin@link.sunet.se  Thu Apr  6 08:12:12 1995
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From: martin@link.sunet.se (Martin Norin, Dept. Biochem., Royal Inst. Technol., Stockholm, tel. +46-8-7907512, e-mail; martin@physchem.kth.se)
To: "chemistry@ccl.net"@kth.sunet.se
Subject: GRID program as scoring function



Dear colleauges,

I've heard that the GRID program (Goodford et al.) may be used in scoring
ligands bound at receptor sites (any protein cavities).

Any comments or pointers to references are welcome. I'll summarize 
replies to the CCL.

Best Regards

Martin Norin\
Pharmacia Biopharmaceuticals              e-mail:martin.norin@sto.pharmacia.se
Dept. Struct. Biochem.
S-11247 Stockholm
Sweden

From darryl@om3.ch.umist.ac.uk  Thu Apr  6 09:12:13 1995
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Date: Thu, 6 Apr 1995 14:24:46 +0100 (BST)
From: Darryl Ellson <darryl@om3.ch.umist.ac.uk>
Subject: Program for coupling constants.
To: chemistry@ccl.net
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I am enquiring whether anyone has knowledge of the MELDF program, and 
whether it may be used for the calculation of isotropic and anisotropic 
coupling constants. I would also be grateful if anyone could inform me of 
any other program they have experience of for the calculation of coupling 
constants.


		Many Thanks.

			Darryl A. Ellson


~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~
   Darryl A. Ellson - Dept. Chemistry, UMIST, Manchester. M60 1QD
              Molecular Simulation & Design Laboratory
	    Tel: 061-236-3311 x4476    Fax: 061-236-7677
                E-mail: darryl@trigger.ch.umist.ac.uk

~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~




From kamal@univ-orleans.fr  Thu Apr  6 09:14:51 1995
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Date: Thu, 06 Apr 1995 13:55:59 +0100
To: chemistry@ccl.net
From: kamal@univ-orleans.fr (Kamal Azzaoui)
Subject: Log P (o/w) of octanol !


Dear netters

We are working in the field of quantitative structure-chromatographic
retention relationships (QSSR) and ,
among various physico-chemical descriptors, we used the calculated Log P
(o/w)( With Ghose and Crippen=92s parameters).

One of our products is Octanol.

It is very easy to calculate the Log P of Octanol ( we found 2.54), this
value is a by evidence a descriptor of the structure , but we have a
=91philosophic=92 problem:

What is the physical meaning of Log P(o/w) of Octanol?
Subsidiary question: What is the Log P of water?

All suggestions are welcome !!=20

thanks

Kamal=20
------------------------------------------------------------------
        Kamal AZZAOUI                                   =20

   LCBA. Universit=E9 d'Orl=E9ans.
     BP 6759.
   45067 Orl=E9ans cedex 2
        France
   Tel: 38-41-70-42
   email: kamal@centre.univ-orleans.fr
------------------------------------------------------------------


From virtual@quantum.larc.nasa.gov  Thu Apr  6 09:17:15 1995
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Date: Thu, 6 Apr 95 09:08:46 -0400
From: "Don H. Phillips" <virtual@quantum.larc.nasa.gov>
To: CHEMISTRY@ccl.net
Subject: Instability


In reply to <9504051643.AA09878@vangogh.chem.uab.edu>
Gavin:

>...... We found that there is a
> triplet state that is lower in energy than the singlet at HF levels of
> theory, but singlet is lower for MP2 and DFT levels of theory.

I suspect that your "HF level theory" singlet is closed shell and that
the true ground state is an open shell singlet.  My guess is that the
orbitals involved are (essentially) p orbitals on the terminal oxygen
and the nitrogen, but I haven't done any work on this compound so that's
only a guess. 

Possible approaches to exploring this are:

(1) Carry out an open shell singlet HF calculation.  Use singles and doubles
CI from the open shell reference to improve the description (or open
shell MP4 if available).  Note that, depending upon the relative
importance of the single reference function, this may not yield an
accurate result but it will be improved over what you have now.
An MCSCF treatment to get orbitals and a multiple reference CI or
equivalent coupled cluster calculation would be required for accuracy
if the state isn't described well by a single reference function.

(2) An alternative approach would be to obtain natural orbitals for
the true ground state and base a CI treatment on these orbitals.  The
same caveats as above apply with regard to the suitability of a single
function reference.  The natural orbitals from a UHF treatment of the
lowest triplet state might be a good starting point.  INDO may not provide
a qualitatively correct description of the lowest states.  I would recommend
sticking with ab-initio treatments throughout.

I don't have any experience with Gaussian, which I assume you are using,
or with DFT treatments of open shell singlets, so I am of no help to you
there.  The GAMESS and COLUMBUS packages offer alternatives.  The latter
has a lot of flexibility, but was difficult to use when I last looked.
A recent posting to CCL indicated that there is a more user-friendly
version available somewhere on the net.

It sounds like you have discovered an "interesting" system.  Have fun.

Good luck,
Don

From d3e102@ames.pnl.gov  Thu Apr  6 11:27:16 1995
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Date: Thu, 06 Apr 1995 08:17:57 -0700
From: d3e102@ames.pnl.gov (Dave Feller)
Subject: Ab Initio Benchmark Report
To: chemistry@ccl.net
Message-id: <9504061517.AA11451@ames.pnl.gov>
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All:

The 1995 version of the EMSL Ab Initio Benchmark Report has finally been
clearer and is now available.  It can be found at URL 
http://www.emsl.pnl.gov:2080/ under the "Technical Reports" section.  
PostScript and Microsoft Word (Mac) versions are also available via
anonymous FTP from pnlg.pnl.gov under directory qcbenchmarks.

Hardcopies are being printed, but in order to keep down the printing costs
we are only printing abridged versions of the report.  These abridged
copies will not include the detailed tables of performance data.  People
who have expresses an interest in the report should receive an abridged
copy in the mail in 2 - 3 months.

Dave

David Feller
Environmental Molecular Sciences Laboratory
Battelle Pacific Northwest Labs
Mail Stop K1-96
Battelle Blvd
Richland, WA 99352


From noy@tci002.uibk.ac.at  Thu Apr  6 12:27:16 1995
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From: noy@tci002.uibk.ac.at (Teerakiat Kerdcharoen)
Message-Id: <9504061615.AA29665@tci002.uibk.ac.at>
Subject: ab initio benchmark available !
To: chemistry@ccl.net
Date: Thu, 6 Apr 1995 18:15:31 +0200 (DFT)
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Dear Netters,
	Forgive me if I double this news. I just came across the
ab initio benchmark report worked by Dr. David Feller at EMSL
WWW 

	http://www.emsl.pnl.gov:2080/homes/tms/tmshome.html

	As I remembered, he used to post once that this report
will be available on-line and a lot of people are looking
forward to this benchmark. Now, it is available.
						 best wishes,
						 Teerakiat
----------------------------------------------------------------------------
E-mail:   noy@tci2.uibk.ac.at (University of Innsbruck)
          noy@atc.atccu.chula.ac.th (Bangkok)  (Permanent E-mail address)
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          http://atc.atccu.chula.ac.th/noyhome/    
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Makes a man healthy, wealthy and wise.         -- Benjamin Franklin


From BGoodin@UNEX.ucla.edu  Thu Apr  6 15:57:19 1995
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From: "Goodin, Bill" <BGoodin@UNEX.ucla.edu>
To: "'List-Biomaterials'" <biomat-l@hearn.nic.surfnet.nl>,
        List-Biotechnology <biotech@umdd.umd.edu>,
        List-Biotechnology business <biz-biotech@netcom.com>,
        "'List-Computational chem2'" <chem-com@mailbase.ac.uk>,
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        "'List-Chemical engineering'" <cheme-l@psuvm.psu.edu>,
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To: List-Materials <materi-l@taunivm.tau.ac.il>,
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Cc: "Goodin, Bill" <BGoodin@UNEX.ucla.edu>
Subject: UCLA short course on "Computational Chemistry for Materials and  Drug
	Design"
Date: Thu, 06 Apr 95 12:19:00 PDT
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Encoding: 48 TEXT
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On August 14-17, 1995, UCLA Extension will present the short course,
"Computational Chemistry for Materials and Drug Design", on the UCLA
campus in Los Angeles.

The instructors are Richard Judson, PhD, Senior Member of the
Technical Staff, Sandia National Laboratories; Tony Hopfinger, PhD,
Professor, Department of Medicinal Chemistry and Pharmacognosy,
University of Illinois at Chicago; and Michael Colvin, PhD, Senior Member
of the Technical Staff, Sandia National Laboratories.

This course provides a broad introduction to computational molecular
modeling.  A variety of methods are discussed which range from statistical
methods based on experimental data to high-level ab initio quantum
chemical calculations.  The course stresses how different methods can be 
appropriately applied in a variety of situations.  These methods include
molecular dynamics, quantum chemistry, and statistical methods such as
QSAR (Quantitative Structure Activity Relationships).  Lectures also 
introduce homology-based protein modeling and general-purpose optimization
methods used across a range of computational chemistry methods.

The course combines descriptions of methods with applications to specific
areas, including predictions of physical properties of molecules 
(solubilities,
conformations, pKa, diffusion coefficients, etc.), predictions of binding
properties of drugs (binding geometries and energetics), and statistical
prediction of various properties from experimental data.  Methods are
illustrated with case studies, and the course also addresses the use of
available commercial modeling software both in lectures and hands-on
sessions.

Specific topics include: Molecular Modeling, Computer Lab Session,
Quantum Chemistry, Case Study, Continuum Solvent Models, Case
Study, Polarizable Treatment of Metals, Computer Lab Session,
Quantitative Structure Activity Relationship (QSAR), Molecular Diversity
and Computer -Assisted Molecular Design, Case Study, Computer Lab
Session, Applications of Computational Methods to Polymeric Materials
Design, Commonly Used Optimization Methods in Chemical Calculations,
Protein Homology Modeling, and Commercially Available Modeling
Software.

For additional information and a complete course description, please
contact Marcus Hennessy at:

(310) 825-1047
(310) 206-2815  fax
mhenness@unex.ucla.edu

From moret@far.ruu.nl  Thu Apr  6 16:27:21 1995
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	(16.6/16.2) id AA17003; Thu, 6 Apr 95 22:18:18 +0200
From: "E.E.Moret" <moret@far.ruu.nl>
Subject: Why is trimethoprim selective for bacterial DHFR??
To: chemistry@ruucmc.far.ruu.nl
Date: Thu, 6 Apr 95 22:18:17 METDST
Name: Ed Moret
Organisation: Utrecht University
Phone: 030 - 536979
Mailer: Elm [revision: 66.25]



Dear colleagues,

The following question is of a rather detailed nature. Still, in view of
the omnipresence of DHFR research in the modelling literature of the last
decade, I think many of you can help us out.

Trimethoprim (TMP) is a valuable antibacterial compound used 
in pharmacotherapy. Its value is based on its 10000 times higher affinity
for bacterial over human Dihydrofolate Reductase (DHFR). 
It is a classical example in medicinal chemistry and drug design.

In ligand modelling, the DHFR and methotrexate (MTX) complex (for example
4dfr.pdb) has been the de facto standard example for testing new programs
like Ludi, Leapfrog, Apex-3D, MCSS, Grow and others.
The X-ray structure of TMP with vertebrate or bacterial DHFR has never 
been deposited at the PDB. 

The selectivity of TMP for bacterial DHFR is believed to be based on a 
somewhat different binding mode, caused by decreased accessibility of 
the hydrophobic pocket, as compared to vertebrate DHFR. Although it is possible
to generate a complex with energy minimisation and docking algorithms, the
giant effect of these subtle changes remains mysterious to me. 
Although our docking method seems to work fine, given the precise
prediction of the crystal structure positions of MTX and DHF, the interaction
energies for TMP in human and bacterial DHFR are roughly the same. 
Some workers have pointed to changes in a histidines protonation state 
and its effect on the co-factor NADPH. Other workers have pointed out 
the importance of buried water molecules. Some workers have pointed at 
the protonation state of an aspartate or glutamate residue. 
A mutative loss of a valine in human DHFR compared to E.Coli DHFR seems to 
explain the loss of one hydrogen bond. The crystallographers describe the 
hydrophobic pocket in vertebrate DHFR as being too wide. A cooperative
binding effect of NADPH has been experimentally determined.

I still do not grasp what interactions are missing in vertebrate DHFR. 
What prevents TMP from adopting the conformation found in bacterial
DHFR? What are the extra interactions in bacterial DHFR which account for
the 10000-fold difference, roughly equal to 23 kJ/mole or 2 to 3 salt bridges?
(No flames on my estimates please; the difference is HUGE and complete
therapy is based on this)

Among you, there should be numerous workers who have studied this complex. 
What do you think is the main determinant for this selectivity?

With best regards,
Ed Moret
--
-------------------------------------------------------------------------
E.E. Moret	(@more@)			    E.E.Moret@far.ruu.nl
Computational Medicinal Chemistry/Department of Pharmaceutical Chemistry
Faculty of Pharmacy/Utrecht University/the Netherlands
Telephone	(31-30)536979/536958        Facsimile      (31-30)516674
-------------------------------------------------------------------------

From paul@simulate.chem.vt.edu  Thu Apr  6 17:27:19 1995
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From: paul@simulate.chem.vt.edu (Paul Gregory)
Message-Id: <9504062123.AA14973@simulate.chem.vt.edu>
Subject: Re: CCL:heterogeneous nucleation
To: rmiller@hplato.hpl.hp.com (Robert Miller)
Date: Thu, 6 Apr 1995 17:23:49 +22300129 (EDT)
Cc: chemistry@ccl.net (complist)
In-Reply-To: <9504060155.AA21824@hplato.hpl.hp.com> from "Robert Miller" at Apr 5, 95 06:55:09 pm
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> 
> Colleagues;
> Have any of you attempted to simulate vapor nucleation?
> Do any of you have thoughts on the topic?
> I will post a summary of any and all replies.
> --
> Sincerely, 
> Robert Miller, PhD
> Hewlett-Packard Laboratories
> e-mail: rmiller@hplato.hpl.hp.com

I published a paper on homogeneous nucleation.  The reference is:

V.P. Gregory and J.C. Schug, "Clustering of Lennard-Jones Particles Below the
Critical Temperature", 1993, Molecular Physics, 78, 407.

The abstract follows:

    The clustering properties of sub-critical 3D Lennard-Jones particles have
been determined by Monte Carlo computer simulation.  The goal was to study
liquid formation, which results in the definition of a cluster that is based on
the radial distribution function of the LJ liquid.  The cluster distribution
was compared with that predicted by classical nucleation theory and analyzed
with the cluster distribution scaling law.  It was found that the surface
tension must vary with cluster size in order for classical theory to fit the
simulation data.  Also, the scaling law was determined to have limited
usefullness over the range of system densities and was most applicable to lower
densities and higher temperatures.  The density profile revealed that the
clusters did not have well defined surfaces and were liquid-like in the
interior.  The fractal dimension was calculated from the radius of gyration and
found to agree with the accepted value.  The presence of a phase transition was
determined from the cluster energy plots.

------------
V. Paul Gregory, PhD
Department of Chemistry                    Internet: paul@simulate.chem.vt.edu
Virginia Tech                        ,/\        IBM RISC System/6000 Model 350
Blacksburg, Virginia               ,/   `\/`'\
            24061-0212         ,/\/          /
                             ,/             <_          ._.
                            /                 `\       / /
                 ,/\_     _/'                   `-`-\  |/
              ,/'    `_'_'  *  Blacksburg          \_> '
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          +----------------------------------------------+


From butch@sunlc2.chem.uga.edu  Thu Apr  6 19:27:24 1995
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Date: Thu, 6 Apr 1995 19:26:32 -0400
From: Butch Carreira <butch@sunlc2.chem.uga.edu>
Message-Id: <199504062326.TAA04981@sunlc2.chem.uga.edu>
To: chemistry@ccl.net
Subject: Log P (o/w) of octanol
X-Sun-Charset: US-ASCII



Dear Kamal,


> Date: Thu, 06 Apr 1995 13:55:59 +0100
> To: chemistry@ccl.net
> From: kamal@univ-orleans.fr (Kamal Azzaoui)
> Subject: CCL:Log P (o/w) of octanol !
> Sender: Computational Chemistry List <chemistry-request@ccl.net>
> Errors-To: ccl@ccl.net
> Precedence: bulk
> 
> Dear netters
> 
> We are working in the field of quantitative structure-chromatographic
> retention relationships (QSSR) and ,
> among various physico-chemical descriptors, we used the calculated Log P
> (o/w)( With Ghose and Crippen=92s parameters).
> 
> One of our products is Octanol.
> 
> It is very easy to calculate the Log P of Octanol ( we found 2.54), this
> value is a by evidence a descriptor of the structure , but we have a
>philosophic problem:
> 
> What is the physical meaning of Log P(o/w) of Octanol?
> Subsidiary question: What is the Log P of water?
 
The answer is this:
 
Log P(o/w) for a solute is the difference in the log activities of 
that solute in water and octanol solvents. The log activity of octanol
in octanol is 0.0 (~0.04 or so if you take into account that it is really
wetted octanol). However, the log activity for octanol in water is about
4.0. If you express the log P using a moles/l reference rather than a mole
fraction reference (the usual) then the difference in the log of the 
molecularites of the solvents must be taken into account, for o/w this 
is ~0.82. So the log P would be 4.0-0.8 or around 3.1-3.2.

The same scheme will hold for the log P(o/w) of water.

Hope that helps.

Butch Carreira
====================================================================
Butch Carreira                             butch@sunlc2.chem.uga.edu
Department of Chemistry                    (706) 542-2050 or 2051
The University of Georgia                  (706) 542-9454 FAX
Athens, GA  30602


From tony@schroeder.newcastle.edu.au  Thu Apr  6 20:12:22 1995
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Date: Fri, 7 Apr 1995 11:02:27 +1100 (E  )
From: Tony Dyson <tony@schroeder.newcastle.edu.au>
To: Computational Chemistry List <chemistry@ccl.net>
Subject: Gaussian & VAX/VMS
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I don't see VAX/VMS amongst the list of current or proposed platforms for 
Gaussian94. Why is this so? We ourselves use the unix version, but the 
fact that a VMS version is not promised has meant that our associates in 
the Chemistry department are refusing to share the cost of the license 
upgrade this time. Does anyone know why Gaussian seems to be moving off 
VMS platforms?

	Tony

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

  Mr. Anthony J. Dyson		tony@schroeder.newcastle.edu.au
  Dept. of Physics		phone: +49 21 5425
  University of Newcastle	fax:   +49 21 6907
  Callaghan, Australia, 2308

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


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Date: Thu, 06 Apr 1995 21:58:44 -0300
Subject: Summary of internal coordinates --> normal coordinates
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Dear Netters,

Many thanks to people who replied to my query about converting 
internal coordinates to the normal coordinates.  Here is a summary 
of replies I have received.


Jian Wang
Department of Chemistry
Dalhousie University
Halifax, Nova Scotia
Canada B3H 4J3
Tel: (902)-494-7921
Fax: (902)-494-1310


---------- Original Question ----------

Dear Netters,

I am looking for a code to calculate the matrix which converts the
internal coordinates to the normal mode coordinates.  I can get the
force constant matrix with respect to the internal coordinates, but
I need a code to calculate the G matrix, which is necessary for the
diagonization of the FG matrix.  From there I will be able to
obtain the transformation matrix.

Thanks in advance.

Jian Wang


------------ Replies -------

From:   IN%"cas@softshell.com"  "Craig Shelley"
==============================

I will be gone the week of March 20th.  I will be back on the 27th.  If you need
support or other information before then, e-mail development@softshell.com, call
our office at 303-242-7502, or fax at 303-242-6469.

Thanks,

Craig A Shelley

From:   IN%"youkha@biosym.com"
==============================

If you already have code that calculates normal modes in cartesian
X = Lx Q

and to determine the "B matrix"

R = B X ...

(a program that does the former does the latter if the force constants are expresse
d in internal
space)

then the Lr matrix you are looking for is

Lr = B * Lx

where R = int coords
      X  cartesian coords
      Q  normal coords

this is much simpler. programs at QCPE exist for these things.
see the book of Wilson on that topic

**************************************************************************
Dr. Philippe Youkharibache                      e-mail: youkha@biosym.com
Biosym Technologies Inc.
9685 Scranton Road                              tel: (619) 546 5562
San Diego, CA 92121                             fax: (619) 458 0136
**************************************************************************



From:   IN%"GOVENDEM@che.und.ac.za"  "Magan Govender - PG"
==============================

Dear Sir,

I have some codes available, and shall be
happy to forward them to you, on request.

Greatings from South Africa

M.G. Govender
Centre for Theoretical and Computational Chemistry
Dept of Chemistry
University of Natal
King George V Avenue
Durban
South Africa

M.G. Govender's second reply:
==============================

Dear Sir,

The program we are using does a complete vibrational
calc. of the secular equation, it is called Vibra by Dr. STeele.
We also have ASYM20, by Ian Mills , obtained from QCPE. A also have a
code from SPectro, author Handy, and Willets, I can send you this
code, and lastly there is a program obtainable via ftp
iqm.unicamp.br, in the chem or pub dir, which is called BGF and NCA,
similar to ASyM20. Anyway I shall forward you the code soon which is
in fortran. The address of Dr STeele is aslc801@vmsfe.ulcc.ac.uk.

regards
Magan


From:   IN%"nowak@ibm320.chemie.th-merseburg.de"
==============================

Dear Jian Wang
If you have the B matrix which transform the cartesian force constant matrix
to the internal force constant matrix you can build the G matrix by
G=B M**-1 B#.
Where B# is the transpose of the B matrix and M**-1 is the inverse of
the M matrix. M is a diagonal matrix of tripels of the mass.
The product FG is a nonsymmetric matrix. The simplest way to get
 the eigenvalue and eigenvectors is to bring the matrix to
 a hessenberg matrix then you can get the eigenvalue and eigenvectors by the
 qr methode.
 I wrote  a FORTRAN program which can build the internal force constants matrix
 from the cartesian force constant matrix. Futhermore it will calculate the G
 matrix and frequences. There is also a procedure which bild the B matrix.
 If you are interested in my program please send me a e-mail.
 If you are loocking for some literature for this topic:

Califano Vibrational States
JOHN WILLEY & SONS 1976
T.Miyazawa J. Chem. Phys. 1958 29 P.246
R.J.Malriot J. Chem. Phys. 1955 23 P.30

Futhermore I am intrested in your way to get the internal force constant matrix.
Thanks in advance.
Thomas Nowak
e-mail nowak@ibm320.chemie.th-merseburg.de


--------------  End of Replies ---------

