From chemistry-request@server.ccl.net Thu Mar 22 00:34:37 2001
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Date: Thu, 22 Mar 2001 23:31:21 +0530
From: Prashant Desai <pradesai@bol.net.in>
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To: Posting Question on CCL <chemistry@ccl.net>
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Can anybody suggest the procedure to prepare the exclude.pdb file,
required for running  'autoMS' in DOCK 4.0.1,  in order to generate dot
surface for the receptor. Also welcome is any practical tips on use of
DOCK.
Thank you in advance.
Prashant Desai
Senior Research Fellow,
Dept. of Pharmaceutical Chemistry
Bombay College of Pharmacy
Kalina
University of Mumbai
India - 400098


From chemistry-request@server.ccl.net Thu Mar 22 00:37:47 2001
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Date: Thu, 22 Mar 2001 12:56:50 +0700 (ICT)
From: Somsak Tonmunphean <somsak@atc.atccu.chula.ac.th>
To: <chemistry@ccl.net>
Subject: Desolvation Free Energy and Inertia Moment 1 size
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Dear CCLers,
	Recently, I read the QSAR articles and found the following three
descriptors, "Desolvation Free Energy for Water (Fh2o)", "Desolvation Free
Energy for Octanol (Foct)", and "Inertia Moment 1 size". The first two
were calculated using the QSAR module in the Cerius 2 software and the
last one was computed using the TSAR software. Since I do not have these
two softwares and could not find their Manuals, I would like to know how
to calculate these three parameters ?? And what are the physical meaning
of these three parameters ??
	Thank you very much in advance for your kind helps.

Your sincerely,
Somsak Tonmunphean, Ph.D. student

Department of Chemistry,
Faculty of Science,
Chulalongkorn University,
Bangkok 10330 Thailand.


From chemistry-request@server.ccl.net Wed Mar 21 14:00:10 2001
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Date: Wed, 21 Mar 2001 13:14:45 -0500
From: Samantha Jenkins <sjenkin@mcmaster.ca>
Organization: McMaster University
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To: chemistry@ccl.net
Subject: Summary  CCL:Basis sets for solid GaAs, GaP and ZnS
References: <3AA3CBBB.4AFB108F@mcmaster.ca> <3AA66AEB.64D6232A@mcmaster.ca>
	 <3AAE69B3.20908@mcmaster.ca> <p04330103b6d5bf91cf7c@[130.220.35.99]>
	 <3AB0E7F6.7050300@mcmaster.ca> <p04330101b6d708b0dc93@[130.220.35.99]>
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 >> Does anyone have any basis sets optimised for  GaAs, GaP and ZnS
 >> suitable for use in CRYSTAL98 calculations?
 >
 >
 > I've been doing some calculations for ZnS, with both the zinc
 > blende/sphalerite and wurtzite structures, using CRYSTAL98. What basis
 > sets are suitable depends on what properties you want to get out of your
 > calculations. I did some geometry optimisations and band structure/DOS
 > calculations on bulk ZnS using the Zn 86-4111/41 basis set supplied with
 > the CRYSTAL98 package (optimised for ZnO) and the S 86-311/1 basis set
 > used by Mian et al for PbS. (Chem. Phys. Lett. 1996, 257, 627-632).
 > These gave suitably accurate results for my needs, particularly when
 > using GGA-DFT or hybrid methods. If they don't work for you, they're
 > probably still a good place to start your own basis set optimisations.
 >
 > I can send you copy of one of my basis set blocks from an input file if
 > you want.
 >
 > Cheers,
 > Rob


Robert Jones wrote:

> Hi Samantha,
> 
> At 11:04 -0500 15/3/01, you wrote:
> 
>>> I can send you copy of one of my basis set blocks from an input file 
>>> if you want.
>>> 
>> Yes please that would be great.
> 
> 
> Below are the Zn and S basis sets, in CRYSTAL98 format, that I've been 
> using for my sphalerite/wurtzite calculations. As stated in my previous 
> message, I didn't derive them myself, they're in the literature. I'm 
> afraid I can't help you with basis sets for Ga, As or P.
> 
> Good luck.
> 
> Cheers,
> Rob
> 
> 
> 30 8  0  0  8  2.0  1.0
>   417016.5        0.00023     60504.2        0.00192     12907.9        
> 0.01101      3375.74       0.04978      1018.11       0.16918       
> 352.55       0.36771      138.19       0.40244       57.851      0.14386 
> 0  1  6  8.0  1.0
>     1079.2       -0.00620      0.00889      256.52      -0.07029      
> 0.06384       85.999     -0.13721      0.22039       34.318      
> 0.26987      0.40560       14.348      0.59918      0.41370        
> 4.7769     0.32239      0.34974 0  1  4  8.0  1.0
>       60.891      0.00679     -0.00895       25.082     -0.08468     
> -0.03333       10.620     -0.34709      0.08119        4.3076     
> 0.40633      0.56518 0  1  1  0.0  1.0
>        1.6868     1.0 1.0
> 0  1  1  0.0  1.0
>        0.62679    1.0 1.0
> 0  1  1  0.0  1.0
>        0.15033    1.0 1.0
> 0  3  4 10.0  1.0
>       57.345      0.02857
>       16.082      0.15686
>        5.3493     0.38663
>        1.7548     0.47766
> 0  3  1  0.0  1.0
>        0.51592    1.0
> 16 6
> 0  0  8  2.0  1.0
>   109211.0        0.0002520
>    16235.206      0.0019934
>     3573.0286     0.0111177
>      943.23811    0.0498945
>      287.26179    0.1661455
>       99.914226   0.3627018
>       38.602137   0.4108787
>       15.531224   0.1457875
> 0  1  6  8.0  1.0
>      281.22171   -0.0057780    0.0081427
>       67.106575  -0.0665855    0.0565570
>       21.794135  -0.1203552    0.2039582
>        8.2097646  0.2741310    0.3973328
>        3.4178289  0.6463829    0.3946313
>        1.5452225  0.2925792    0.1544345
> 0  1  3  8.0  1.0
>        4.3752432 -0.1750000   -0.0613439
>        1.8096201 -0.5938952    0.1272251
>        0.6833985  0.8298996    1.2215893
> 0  1  1  0.0  1.0
>        0.2370     1.0          1.0
> 0  1  1  0.0  1.0
>        0.0814     1.0          1.0
> 0 3 1 0.0 1.0
>        0.30       1.0
> 99 0
> END




From chemistry-request@server.ccl.net Wed Mar 21 16:04:05 2001
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From: "Qadir K. Timerghazin" <q_timerg@alcor.concordia.ca>
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Dear CClers,

I am wondering if Atoms-in-Molecule analysis was ever applied to
for electronically excited molecules?

-- 
Best regards,
 Qadir                          mailto:q_timerg@alcor.concordia.ca

****************************************************************************
Qadir K. Timerghazin                 * Kadyr K. Timergazine
Centre for Research                  * Centre de Recherche en
in Molecular Modeling                * de Modélisation Moléculaire
                                     *
Concordia University                 * Université Concordia
1455 De Maisonneuve Blvd St. West,   * 1455 Bvd De Maisonneuve Ouest
Montreal, Quebec,                    * Montréal, Québec,
CANADA H3G 1M8                       * CANADA H3G 1M8
                                     *
Room: 1034-1                         * Salle: 1034-1
Phone: (514) 848 3360                * Tel: (514) 848 3360
****************************************************************************




From chemistry-request@server.ccl.net Wed Mar 21 16:59:25 2001
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Date: Wed, 21 Mar 2001 13:59:25 -0800 (PST)
From: eric hu <erichu_linux@yahoo.com>
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Hi, All

Is anyone using openGL based windowns version of
molscript? 

Eric

__________________________________________________
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From chemistry-request@server.ccl.net Wed Mar 21 19:42:25 2001
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Subject: About CASSCF geometry optimization
Date: Thu, 22 Mar 2001 08:44:16 +0800
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Dear all,

I have a big problem in CASSCF optimization for the MOs change their sequence almost always. So I can hardly go a step forward in the optimaztion. Would you give me some advices on it or suggest me some papers to read.

Best regards,

Chungen Liu


===================================================================
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From chemistry-request@server.ccl.net Wed Mar 21 13:14:15 2001
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	(kresslists@kressworks.com)
Subject: Re: CCL:DCD and software reuse (was Qmol: Molecular viewer for Windows)
References: <062801c0af8d$f9300fe0$b9ac323f@josiah> <200103191755.SAA04714@chinon.cnrs-orleans.fr> <3AB6D022.319959E9@sunesis-pharma.com> <000d01c0b104$efa13940$0300a8c0@quantumnt>

> >After all, if you are not going to commercialize your code, then why not
> make it
> >available to other scientists unconditionally?
> 
> Commercialization means different things to different people.  When someone
> develops code that gives them a 'competitive advantage' in getting grant
> money, they aren't inclined to distribute the code to others.  Isn't that
> another form of 'commercialization'?

That would mean not releasing the code at all. Personally I think that
this is against the principles of science (because others can't check
a computational study if an essential ingredient remains
inaccessible), but that's not the problem we are discussion at the
moment.

The question was why some code is available for a small fee, or for
free but only after signing a license contract, which typically
forbids redistribution. One reason I have heard is that people want to
keep track of all users, in order to mention the popularity of their
product to their sponsors. But I am sure that other counting schemes
can be found (e.g. references to some publication).
-- 
-------------------------------------------------------------------------------
Konrad Hinsen                            | E-Mail: hinsen@cnrs-orleans.fr
Centre de Biophysique Moleculaire (CNRS) | Tel.: +33-2.38.25.56.24
Rue Charles Sadron                       | Fax:  +33-2.38.63.15.17
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From chemistry-request@server.ccl.net Wed Mar 21 22:14:57 2001
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Date: Wed, 21 Mar 2001 21:50:30 -0500 (EST)
From: Artem Masunov <amasunov@blakey.sci.ccny.cuny.edu>
To: <chemistry@ccl.net>
Subject: DFT is over !/? (expert opinion needed)
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 Dear CCLers,
 I just became aware of the recent paper by Clementi et al. (see
the relevant abstracts below).
 It seems to me that the quest for correlation functional is over:
Clementi just did it (without any density, but with 16
empirical parameters).
 He...He, water trimer, and atomization energies to +/- 0.05 kcal/mol
sound pretty convincing.
 What do you think?

Regards,
Artem

-- 

     __    ___________       Artem.Masunov@USA.net; Tel 212-650-7792
    /  \  /  __   __  \     Computational Biophysical Chemistry Group
   /    \/\  \ \  \ \  \        Chemistry Dept, City College, CUNY
  /  /\  \ \  \ \  \ \  \    J-1325, Convent Ave, New York, NY 10031
 /  ____  \ \  \ \  \ \  \ -------http://www.biosys.net/artem----------
/__/\ _/\ _\ \ _\ \ _\ \ _\ FORGIVE MY NONSENSE AS I ALSO FORGIVE THOSE
\ _\/  \/__/\ __/\ __/\ __/ WHO THINK THEY TALK SENSE  --  ROBERT FROST


---------- Forwarded message ----------

Revision and extension of the HF-CC method
Clementi E, Corongiu G
JOURNAL OF MOLECULAR STRUCTURE-THEOCHEM
493: 1-20 DEC 15 1999

Abstract:
The Hartree-Fock-correlation correction (HF-CC) molecular model is a
recent post-HF perturbation model which decomposes the correlation
correction into atomic and molecular components. In this work, the HF-CC
model is modified with attention to weak and very weak interactions, and
validated by computing the atomisation energy of 112 test molecules: 104
closed shell, from diatomic to naphthalene, and 8 radicals. The
atomisation energies, computed at six successive approximations by
optimising an increasing number of empirical parameters have mean
deviations of 13.82, 11.90, 6.32, 4.57, 0.54 and 0.05 kcal/mol,
respectively, relative to experiments. The method is successfully extended
to weak interactions testing the dimer and trimer of water and the
complexes H2O-X with X = Li+, Na+, K+, F-, Cl-. The feasibility to predict
very weak interactions is tested with computations of van der Waals
energies: at the computed minimum. He-2, Ne-2 and Ar-2 have inter nuclear
distances and interaction energies in agreement with laboratory data.
Finally, the total molecular binding energy is decomposed into computed
bond energies that are comparable to the available experimental bond
energies.


Soft Coulomb hole method applied to theoretical equilibrium geometries of
singlet diatomic molecules
A. Hernández-Laguna and L. Alfonso-Méndez
Estación Experimental del Zaidín (CSIC), C/Prof. Albareda 1, 18008
Granada, Spain
P. Otto
University Erlangen-Nürnberg, Egerlandstraße 3, D-91055 Erlangen, Germany

It has been demonstrated that the soft Coulomb hole method is a reliable
and efficient approach to calculate the electron correlation energy for
atoms and molecules. In this method the perturbation operator
–exp(–ar)/r12 is introduced, where  determines the size of the Coulomb
hole. The set of parameters for  has been redetermined to calculate
equilibrium bond distances. Calculations have been performed for 41 homo-
and heteronuclear singlet diatomic molecules and ions (X 1+), including
atoms of the second and third periods of the periodic table. The soft
Coulomb hole correlation energies are compared to the corresponding
empirical correlation energies. In general, calculated equilibrium bond
distances are in better agreement with the experimental values than
Hartree-Fock and Møller-Plesset-2 results. With respect to
Møller-Plesset-3, the soft Coulomb hole method gives slightly larger
values for the average deviations, except for the homonuclear series

Molecular correlation energy with the HF-CC method
Clementi E, Corongiu G
CHEMICAL PHYSICS LETTERS
282 (5-6): 335-346 JAN 23 1998

Abstract:
The 'HF-CC' model is extended from atomic to molecular systems. An
analysis of the total and binding energy components points out mechanisms
of molecular binding and a strategy to compute the latter via a
partitioning of the correlation energy into atomic and molecular
components. The HF-CC model is size consistent and basis set independent.
We considered 41 molecules at optimised geometry with basis sets near to
the Hartree-Fock limit. The average atomisation energy is 69.65% of the
experimental data (average error is 147.59 kcal/mol) from Hartree-Fock and
becomes 95.10%, 97.68%, and 99.52% (average errors become 31.79 kcal/mol,
10.54 kcal/mol, and 2.36 kcal/mol, respectively) for the HF-CC model with
either one parameter (for the H atom), or one parameter per each atomic
species, or one parameter per each class of an atomic species; the
Becke-Perdue BP-86 density functional yields 94.45% with an average error
of 20.43 kcal/mol.


HARTREE-FOCK SOFT COULOMB HOLE TO ESTIMATE CORRELATION ENERGIES IN ATOMS,
MOLECULES AND POLYMERS
OTTO, P;REIF, H;HERNANDEZLAGUNA, A
THEOCHEM-JOURNAL OF MOLECULAR STRUCTURE
340: 51-62 SEP 20 1995

Abstract:
We have shown that the empirical correction introduced into the
Hartree-Fock method to calculate correlation energies for atoms and
therefore to remove the error caused by the so-called Coulomb hole can be
extended from atoms to molecules and polymers. A reformulation was
required of the necessary parameter representation. The reparametrization
has been performed staying as close as possible to the original
expressions for atoms reported by Chakravorty and Clementi (S.J.
Chakravorty and E. Clementi, Phys. Rev. A, 39 (1989) 2290). In addition to
their work, where the correlation energy has been calculated with the
self-consistent Hartree-Fock wavefunction and the correction integrals, we
have performed investigations, including the perturbation operator in the
Fock operator, so that the total energy also contains the correlation
energy. The applications of this approach to atoms and molecules show that
the total electron correlation energies and ionization potentials
calculated as differences of total energies can be obtained very
satisfactorily. On the basis of the reported calculations it turns out
that one obtains better agreement with reference values of more
sophisticated calculations when the correction integrals are used to build
up the Fock matrix. Furthermore we have found that the magnitude of the
correlation energy depends only weakly on the size of the basis sets,
which makes this empirical method very attractive for its application to
large molecular and polymeric systems.


COULOMB-HOLE-HARTREE-FOCK FUNCTIONAL FOR MOLECULAR-SYSTEMS
CLEMENTI E, HOFMANN DWM
THEOCHEM-JOURNAL OF MOLECULAR STRUCTURE
330: 17-31 JAN 10 1995

Abstract:
We have extended to molecules a density functional previously parametrized
for atomic computations. The Coulomb-hole-Hartree-Fock functional,
introduced by Clementi in 1963, estimated the dynamic correlation energy
by the computation of a Hartree-Fock type single-determinant wavefunction,
where the Hartree-Fock potential was augmented with an effective potential
term, related to a hard Coulomb hole enclosing each electron. The method
was later revised by S. Chakravorty and E. Clementi, Phys, Rev. A, 38
(1989) 2290, so that a Yukawa-type soft Coulomb hole replaced the previous
hard hole. Atomic correlation energies, computed for atoms with Z = 2 to
54, as well as for a number of excited states, validated the method. In
this work we have parametrized for molecules a function which controls the
width of the soft Coulomb hole by fitting the first and second atomic
ionization potentials of atoms with 1 less than or equal to Z less than or
equal to 18 and the binding energies of a few diatomic molecules. The
parametrization was successfully validated by computing the dissociation
energy for a number of molecules. A few-determinant version of the
Coulomb-Hartree-Fock method (CHF-N) necessary to account for the
non-dynamic correlation correction and to ensure proper dissociation
products, is briefly discussed with reference to a previous proposal by
G.C. Lie and E. Clementi, J. Chem. Phys., 60 (1974) 1275 and 60 (1974)
1288.


EXTENSION OF THE COULOMB-HOLE-HARTREE-FOCK THEORY TO MOLECULES
DEWINDT L, HOFMAN DWM, PISANI L, CLEMENTI E
INTERNATIONAL JOURNAL OF QUANTUM CHEMISTRY
53 (2): 131-147 JAN 15 1995

Abstract:
The Coulomb-Hole-Hartree-Fock method introduced by E. Clementi in the
early 1960s and reparametrized more recently by S. Chakraworty and E.
Clementi to compute the correlated electronic energy in atomic systems, is
here extended to compute molecules. The new parametrization is obtained
empirically by fitting first and second atomic ionization potentials from
He to Ca and a few diatomic molecules. The present formulation makes use
of either one or more determinants in order to ensure proper dissociation
products, following the early proposal of G. C. Lie and E. Clementi in the
context of density functional computations for molecular systems. The new
formulation is tested against the dissociation energies of a large number
of molecules and it is found satisfactory.

COULOMB-HOLE-HARTREE-FOCK FUNCTIONAL
CLEMENTI E, HOFMANN DWM
INTERNATIONAL JOURNAL OF QUANTUM CHEMISTRY
52 (4): 849-865 NOV 5 1994

Abstract:
We have extended to molecules a density functional previously parametrized
for atomic computations. The Coulomb-hole-Hartree-Fock functional,
introduced by Clementi in 1963, estimates the dynamical correlation energy
by the computations of a Hartree-Fock-type single-determinant wave
function, where the Hartree-Fock potential was augmented with an effective
potential term, related to a hard Coulomb hole enclosing each electron.
The method was later revisited by S. Chakravorty and E. Clementi [Phys.
Rev. A 39, 2290 (1989)], where a Yukawa-type soft Coulomb hole replaced
the previous hard hole; atomic correlation energies, computed for atoms
with Z = 2 to Z = 54 as well as for a number of excited states, validated
the method. In this article, we parametrized a function, which controls
the width of the soft Coulomb hole, by fitting the first and second atomic
ionization potentials of the atoms with 1 less-than-or-equal-to Z
less-than-or-equal-to 18. The parametrization has been preliminarily
validated by computing the dissociation energy for a number of molecules.
A few-determinant version of the Coulomb-hole-Hartree-Fock method,
necessary to account for the nondynamic correlation corrections, is
briefly discussed.



On Wed, 21 Mar 2001, Vitaly Rassolov wrote:

> Artem,
>
> The main stuff in JCP_corrop.pdf article.  There is a bit on problems of
> new operator in H2 molecule in the other article.  Peter Gill is working
> on a similar approach now, but as far as I know, his publications are
> still in the pipeline.
>
> Cheers,
> _______
>
> Vitaly Rassolov                      rassolov@chem.nwu.edu
> Chemistry Department                 tel. (847) 491-3423
> Northwestern University              fax  (847) 491-7713
>
> On Wed, 21 Mar 2001, Artem Masunov wrote:
>
> > Privet Vitaly!
> >  I was a little disappointed to learn that you terminated you project on
> > r12 operators. Did you ever publish the stuff presented at Sanibel 2 yrs
> > ago?
> >  If not, can you at least send me that abstract with the relevant
> > references (I am sure you searched for the refs)?
> >  I would greatly appreciate that.
> >
> > Artem
> >
> > --
> >
> >      __    ___________       Artem.Masunov@USA.net; Tel 212-650-7792
> >     /  \  /  __   __  \     Computational Biophysical Chemistry Group
> >    /    \/\  \ \  \ \  \        Chemistry Dept, City College, CUNY
> >   /  /\  \ \  \ \  \ \  \    J-1325, Convent Ave, New York, NY 10031
> >  /  ____  \ \  \ \  \ \  \ -------http://www.biosys.net/artem----------
> > /__/\ _/\ _\ \ _\ \ _\ \ _\ FORGIVE MY NONSENSE AS I ALSO FORGIVE THOSE
> > \ _\/  \/__/\ __/\ __/\ __/ WHO THINK THEY TALK SENSE  --  ROBERT FROST
> >
> >
> >
>

-- 

     __    ___________       Artem.Masunov@USA.net; Tel 212-650-7792
    /  \  /  __   __  \     Computational Biophysical Chemistry Group
   /    \/\  \ \  \ \  \        Chemistry Dept, City College, CUNY
  /  /\  \ \  \ \  \ \  \    J-1325, Convent Ave, New York, NY 10031
 /  ____  \ \  \ \  \ \  \ -------http://www.biosys.net/artem----------
/__/\ _/\ _\ \ _\ \ _\ \ _\ FORGIVE MY NONSENSE AS I ALSO FORGIVE THOSE
\ _\/  \/__/\ __/\ __/\ __/ WHO THINK THEY TALK SENSE  --  ROBERT FROST






From chemistry-request@server.ccl.net Thu Mar 22 04:39:56 2001
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Date: Thu, 22 Mar 2001 11:39:54 +0200 (EET)
From: John Kerkines <jkerkin@cc.uoa.gr>
To: chemistry@ccl.net
Subject: Scalar relativistic corrections for CCSD(T)?
Message-ID: <Pine.GSO.3.96.1010322113830.4313A-100000@nikias.cc.uoa.gr>
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Hi everybody,

Does anybody know of a program that can perform scalar relativistic
corrections to an RCCSD(T) wavefunction?

Best Regards,
John


From chemistry-request@server.ccl.net Thu Mar 22 10:46:27 2001
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To: CHEMISTRY@ccl.net
Subject: Translations


Hi all, i am looking for translation lists of chemical term from one langauge
to a second. I would prefere lists from which i *may* (copyright) extract
translations. The result of the extraction will be used to generate
a new multi-lingual translation list (freely available from 
http://www.sci.kun.nl/woc/translation/).

Note that the language i am interested in are *not* limited to those mentioned
on the website.

thanx in advance.

Egon Willighagen

From chemistry-request@server.ccl.net Thu Mar 22 03:47:47 2001
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From: "Dr. Sudhir A. Kulkarni" <sudhirk@mahindrabt.com>
Organization: Mahindra British Telecom Limited
To: chemistry@ccl.net
Subject: Slow drug delivery via polymers


Hello,
    I am looking for references and pointers to theoretical/molecular
modeling studies on polymer supported drug delivery systems.
    Thanks in advance.

Sudhir

Dr. Sudhir A. Kulkarni
Mahindra British Telecom Limited
sudhirk@MahindraBT.com



From chemistry-request@server.ccl.net Thu Mar 22 04:44:51 2001
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From: Adrian Mulholland <Adrian.Mulholland@bristol.ac.uk>
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Reply-To: Adrian.Mulholland@bristol.ac.uk
To: chemistry@ccl.net
cc: mike smith <mike_smith07@yahoo.com>
Subject: Re: CCL:experiment of H-bond strength in solution
In-Reply-To: <3AB52348.A090BE15@usc.edu>
Message-ID: <SIMEON.10103220920.B@chth044.bris.ac.uk>
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Dan Herschlag has done some interesting experimental work 
on H-bonds in solution, see e.g.

Shan, S., Loh, S., Herschlag, D. 'The Energetics of 
Hydrogen Bonds in Model Systems: Implications for Enzymatic 
Catalysis', Science 272, 97-101 (1996)


Shan, S., Herschlag, D. 'The change in hydrogen bond 
strength accompanying charge rearrangement: Implications 
for enzymatic catalysis' Proc. Natl. Acad. Sci. USA 93, 
14474-14479 (1996)

Shan, S., Herschlag, D. 'Energetic Effects of Multiple 
Hydrogen Bonds. Implications for Enzymatic Catalysis', 
J.Am.Chem.Soc. 118, 5515-5518

Shan, S. and Herschlag, D. (1998) 'Hydrogen Bonding in 
Enzymatic Catalysis: Analysis of Energetic Contributions.' 
In Methods in Enzymology , Vol. 308, Schramm, V.L. and 
Purich, D.L., eds. Academic Press, San Diego, pp. 246-276.

Adrian
----------------------
Adrian Mulholland

School of Chemistry        Phone: 0117-928-9097
University of Bristol      Fax:   0117-925-1295
Bristol BS8 1TS            Adrian.Mulholland@bris.ac.uk



From chemistry-request@server.ccl.net Thu Mar 22 04:48:02 2001
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Date: Thu, 22 Mar 2001 15:17:56 +0530 (IST)
From: "Students of Dr. S. R. Gadre" <tcg@chem.unipune.ernet.in>
To: chemistry@ccl.net
Subject: AM1/PECI in MOPAC query
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Dear all, 
 where can i get a free downloadable MOPAC version which has a PECI(pair
electron configuration interaction) option....
bala



From chemistry-request@server.ccl.net Thu Mar 22 07:15:06 2001
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Date: Thu, 22 Mar 2001 20:16:34 +0800 (CST)
From: "Fan Jianmiao" <jim_fan@263.net>
To: CHEMISTRY@ccl.net
Subject: setup a cluster and avoid g98 error link 9999
X-Priority: 3
X-Originating-IP: [61.132.182.2]

Dear CCLers:

     I want to get some help on how to establish a cluster and how to avoid 
the error of gaussian 98 link 9999.

     Our lab needs a cluster running gaussian to get a better calculating 
envirement. But we haven't enough money, we want to buy some PC and form a 
small cluster. But now I don't know the price of Gaussian in parallel(can it 
sell to china?) and whether there is any other programs needed. Currently we 
have buy four PCs(each is equipted with 2 processors of pIII933 and 768M
SDRAM) and a network switcher. But I haven't installed any software for 
paralleling yet. I wonder, how shall I make up the system?

     Another problem is how to avoid the error of g98 link 9999. This error
is very common in our work. Usually we change the iop parameter, but it works
not alwaysly. We found if the start geometry is not very good then maybe this 
problem will be conquered. And if the start geometry is similler to the finial
, it will not come to a normail termination then. Why?  Puzzling problem!
I often saw this infomation on my screen:
" Error termination request processed by link 9999.
  Error termination via Lnk1e in /usr/g98/l9999.exe.
  Job cpu time:  1 days  1 hours 39 minutes  8.0 seconds.
  File lengths (MBytes):  RWF=  824 Int=    0 D2E=    0 Chk=    7 Scr=    1"

What shall I do after I failed changing the iop parameter?If the geometry should
not be wrong, how can I manage to overcome it?

    If there's anyone can give me some suggestion or comments on it, I would 
be very appreciated. 

    Thanks for all in advance.
With My Best Regards,

Sincerely yours,
Jim Fan

~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~
Fan Jianmiao(Jim_Fan)
Department of Chemistry
East Campus,USTC
Hefei,Anhui,230026,P.R.China

Tel:86-551-3654322(dorm) E-Mail:jim_fan@263.net
    86-551-3606640(lab)  Http://mail.ustc.edu.cn/~fan/

~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~
_____________________________________________
ÄÚÈÝ£º³¬¼¶ÓòÃû.Web¿ªÊ¼×¢²á£¬180Ôª/Äê£¬»¹ÓÐ¶ÔÓ¦ÖÐÎÄÓòÃûµÈ£¬
link: http://cn.tf?263b


From chemistry-request@server.ccl.net Thu Mar 22 07:19:29 2001
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From: Stefan Grimme <grimmes@uni-muenster.de>
Organization: Universitaet Muenster, Organisch-Chemisches Institut
To: chemistry@ccl.net
Subject: Re: CCL:DFT is over !/? (expert opinion needed)
Date: Thu, 22 Mar 2001 13:16:51 +0100
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> Dear CCLers,
>  I just became aware of the recent paper by Clementi et al. (see
> the relevant abstracts below).
>  It seems to me that the quest for correlation functional is over:
> Clementi just did it (without any density, but with 16
> empirical parameters).
>  He...He, water trimer, and atomization energies to +/- 0.05 kcal/mol
> sound pretty convincing.
>  What do you think?

Dear Artem,
I recently had the opportunity to talk with Clementi about his approach
and I also read a recent preprint (I think the one you mentioned). I'm not
really convinced that the Coulomb-hole approach with a lot of parameters 
represents a reasonable quantum chemical approch. The main points of my
criticism are as follows:

1. The dispersive interactions are modelled by an empirical formula
which means that the approach is not more than a combination of
force field technology and QM in that respect, i.e. its a new version of QM/MM.

2. The Coulomb-hole (CH) improves on the HF atomization energies but does
NOT improve the relative energies which we are most interested in (Clementi
strongly emphasizes on atomisation energies but forgot to look to the relative
energies!). Simple organic reaction energies are even WORSE with the CH-HF
method compared to HF. Even the simplest DFT's perform better in that respect.

3. An important part of the new CH-HF formalism is based on Mulliken
charges and bond orders. We all know the problems associated with this
approach (strong basis set dependence) and I therefore expect that
each basis set would need its own parametrization (this problem has not
been discussed in the paper I know).

4. Some time ago we tested a simpler (meaning a smaller number of parameters)
version of CH-HF for He and H-. The result was that the radial densities were
even worse than those from HF when compared with almost exact densities. 
My impression was that the basic correlation effects are NOT included
accurately, even not in a qualitative manner. Again, DFT improves upon HF, at
least qualitatively. Thus, I don't expect any improvement for properties with
the CH-HF method (I think this question is important and Clementi has to
investiagte this. We know that DFT does not only improve energies but also
properties like dipole moments etc.; the reason is simply that the DFT
densities are on the whole better than HF densities).

In summary I think the approach is worth while testing it but I don't think
that "the quest for correlation functional is over".
Stefan

_________________________________________________________
Prof. Dr. Stefan Grimme
Organisch-Chemisches Institut (Abt. Theoretische Chemie)
Westfaelische Wilhelms-Universitaet, Corrensstrasse 40
D-48149 Muenster, Tel (+49)-251-83 36512/33241/36515(Fax)
Email:grimmes@uni-muenster.de
http://www.uni-muenster.de/Chemie/OC/research/grimme/
_________________________________________________________
Positions available for carrying out doctoral or 
postdoctoral studies in chemistry in Münster: 
http://www.uni-muenster.de/Chemie/OC/positions/
_________________________________________________________



From chemistry-request@server.ccl.net Thu Mar 22 12:17:41 2001
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Date: Thu, 22 Mar 2001 11:17:39 -0600
From: John Stone <johns@ks.uiuc.edu>
To: deva@XRAY.bmc.uu.se, chemistry@ccl.net
Subject: Re: Orthographics projections in VMD
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Hi,
  We just got back from presenting a paper on some of our recent
VMD work at Siggraph I3D, so we missed this topic while we were
out of town.  Anyway, we are working on improving the renderer
export code in VMD so that it can produce orthographic views in
POV-Ray, Raster3D, Tachyon, and other programs.  There is some
tricky stuff we have to unravel to make this work well, but I'm
hoping we'll get this in one of the upcoming beta versions soon.  

Thanks for using VMD!
  John Stone
  vmd@ks.uiuc.edu

-- 
NIH Resource for Macromolecular Modeling and Bioinformatics
Beckman Institute for Advanced Science and Technology
University of Illinois, 405 N. Mathews Ave, Urbana, IL 61801
Email: johns@ks.uiuc.edu                 Phone: 217-244-3349              
  WWW: http://www.ks.uiuc.edu/~johns/      Fax: 217-244-6078

From chemistry-request@server.ccl.net Thu Mar 22 11:04:46 2001
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Date: Thu, 22 Mar 2001 10:07:24 -0600
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Hi,

I would like to ask if any one have had this kind of error
message before and what it means. I was running a freqency
calculation with Gussian 98, A.6 version.  It is 31 atoms (2
metal, C, N, O, H and S) and 272 basis functions.  Although it
is high spin, the calculation reached the SCF convergency and
give spin conatmination ok. The following is the error message I
got:

----
 Leave Link 1110 at Thu Mar 22 04:22:25 2001, MaxMem=    6291456
cpu:   29102.6
 (Enter /usr/local/g98/l1002.exe)
 Minotr:  UHF wavefunction.
          Direct CPHF calculation.
          Solving linear equations simultaneously.
          Requested convergence is 1.0D-08 RMS, and 1.0D-07
maximum.
          Secondary convergence is 1.0D-12 RMS, and 1.0D-12
maximum.
          Differentiating once with respect to electric field.
                with respect to dipole field.
          Differentiating once with respect to nuclear
coordinates.
          NewPWx=T KeepS1=F KeepF1=F KeepIn=F MapXYZ=F.
          MDV=  6291456
          Using IRadAn=       2.
 Error #1 in AlGdDF.
 Error termination via Lnk1e in /usr/local/g98/l1002.exe.
 Job cpu time:  0 days 14 hours 20 minutes 59.7 seconds.
 File lengths (MBytes):  RWF=  135 Int=    0 D2E=    0 Chk=    2
Scr=    1
----


Any suggestions will be high appreciated.

Thanks in advance.

Huajun

From chemistry-request@server.ccl.net Thu Mar 22 11:40:59 2001
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Subject: BABEL & sybyl format

        Dear All,

I converted PDB structures to the SYBYL format using BABEL.
The obtained SYBYL structures are not recognized by InsightII (MSI) when I
try to load it (using the SYBYL format).

Is it possible to created SYBYL format with BABEL compatible with InsightII ?

Thanks, Best regards    
Francois
 --
F.-Y. Dupradeau            
http://www.u-picardie.fr/UPIC/UPJV/recherche/labos/bpd/fyd.htm


From chemistry-request@server.ccl.net Thu Mar 22 11:25:50 2001
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Date: Thu, 22 Mar 2001 11:17:46 -0500
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To: Konrad Hinsen <hinsen@cnrs-orleans.fr>
cc: kresslists@kressworks.com, chemistry@ccl.net
Subject: Re: CCL:DCD and software reuse (was Qmol: Molecular viewer for
 Windows)
In-Reply-To: <200103211808.TAA07627@chinon.cnrs-orleans.fr>
Message-ID: <Pine.SGI.4.21.0103221103390.77152-100000@gandalf.cber.nih.gov>
MIME-Version: 1.0
Content-Type: TEXT/PLAIN; charset=US-ASCII

>> Commercialization means different things to different people.  When
>> someone develops code that gives them a 'competitive advantage' in
>> getting grant money, they aren't inclined to distribute the code to
>> others.  Isn't that another form of 'commercialization'?

On Wed, 21 Mar 2001, Konrad Hinsen wrote:
> The question was why some code is available for a small fee, or for
> free but only after signing a license contract, which typically
> forbids redistribution. One reason I have heard is that people want
> to keep track of all users, in order to mention the popularity of
> their product to their sponsors. But I am sure that other counting
> schemes can be found (e.g. references to some publication).

In the case of CHARMM, it is commercialization in the more classic
sense; the existence of CHARMm as a product from MSI has placed
contractual limits on the redistribution of the academic source code.  
This can hamper independent development projects which might wish to be
able to read and write CHARMM-DCD files (which we call CHARMM binary
trajectories).  Note that code divergence may mean that XPLOR-DCD,
CHARMm-DCD, and CHARMM-DCD formats may not be completely identical.

In particular, CHARMM simulations run with features such as 4D dynamics,
free energy perturbation, or fragment replicas may produce trajectory
files which only CHARMM could read.


=+=+=+=+=+=+=+=+=+=+=+=+=+=+=+=+=+=+=
Rick Venable
FDA/CBER/OVRR Biophysics Lab
1401 Rockville Pike    HFM-419
Rockville, MD  20852-1448  U.S.A.
(301) 496-1905   Rick_Venable@nih.gov
ALT email:  rvenable@speakeasy.org
=+=+=+=+=+=+=+=+=+=+=+=+=+=+=+=+=+=+=




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Date: Thu, 22 Mar 2001 07:51:00 -0500
To: chemistry@ccl.net
From: Jeff Nauss <jnauss@msi.com>
Subject: MSI Advanced Customer Training Workshops in Houston, Texas, May 15-18
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Molecular Simulations Inc. will be holding a pair of 2-day workshops at the 
University of Houston, Houston, Texas, May 15-18.  These are advanced 
workshops for InsightII users.

On May 15-16, the "Homology-Based Protein Design" training will be offered. 
This workshop is relevant to any of our customers who are interested in 
predicting protein structure and who would like to make more effective use 
of modeling in their work. During the two-day workshop, the process of 
producing a three-dimensional model from an amino acid sequence will be 
covered step-by-step.  Both manual and automatic methodologies will be 
discussed.  Prerequisites for this course are the "Introduction to Life 
Science Modeling with InsightII" workshop or extensive experience with 
InsightII.

Following the homology workshop will be the "Structure-Based Drug design in 
InsightII Workshop" on May 17-18.  This workshop is for advanced users who 
are interested in docking, structure-based ligand design, conformer 
generation, and molecular comparison techniques in the Insight II user 
interface environment. The focus for the workshop is on receptor based 
analysis of ligand binding and interactions using force field techniques 
rather than high-throughput screening.

Fees for each 2-day course are $1000 commercial, $500 government, and $400 
academic.  However, register for both courses and receive a 25% discount 
for the second course.

Further detailed information about this and other MSI training workshops, 
as well as on-line course registration, can be found at MSI's website 
(http://www.msi.com/about/events/training).  Please do not hesitate to 
contact us should you have any questions.

Thank you very much.

                                 Jeffrey L. Nauss
                                 858-799-5555

                 Chris Arzt
                                 858-799-5340





--
Jeffrey L. Nauss, PhD		Phone: (858) 799-5555
Customer Training Programs	Fax: (858) 458-0136
Molecular Simulations Inc.	E-mail: jnauss@msi.com
9685 Scranton Road		http://www.msi.com/about/events/training
San Diego, CA 92121-3752



