From chemistry-request@www.ccl.net  Fri Feb 12 09:33:15 1999
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             Dear all,

    I received one reply from Reinaldo Piz Diez. Thanks, Reinaldo.

>
>		A given PP gives place to pseudo valence wave functions (vwf) that must
>mimic the all-electron vwf outside a given radius. This radius is tipically
>chosen around the outermost maximum in the all-electron vwf. When that
>radius is chosen relatively small, it is said that the PP is hard because
>you need a great number of functions to describe the pseudo vwf. On the
>other hand, when the radius is larger, the PP is soft since a relatively
>modest number of functions is sufficient to describe the pseudo vwf.
>Moreover, in these cases the "norm-conservation" is impossed to the pseudo
>vwf.
>		In the ultrasoft PP, you basically retain all the advantages of the soft
>PP but now the norm-conservation is removed making the pseudo vwf smoother
>in the core region. 
>		You should have a look at "Planewaves, Pseudopotentials and the LAPW
>Method" by David Singh. You should find a lot of useful references there.   
>		Hope this helps a little.
>		Regards,
>
>						Reinaldo
>	
>
>



From chemistry-request@www.ccl.net  Fri Feb 12 10:25:19 1999
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Dear Colleagues;

	For some work in which I'm engaged I need to generate non-degenerate
(i.e., non-repetitive) sets of integers in the range 1-124.  Does anyone
know of a DOS/Win95-compatible programme that will allow me to do something
like enter the range in which I am interested and which will then produce
sets of non-degenerate integers?

Thanks in advance to all responders,

S. Shapiro
toukie@zui.unizh.ch



From chemistry-request@www.ccl.net  Fri Feb 12 10:33:52 1999
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In the G94 manual, it states that the required input for a SCRF=PCM calculation
is 1) dielectric constant of the solvent and 2) the number of points per sphere.
What is an acceptable value for the number of points per sphere.  Does a larger
number increase comp. time and add better "resolution"?  I'll summarize this
thread.

Thanks in advance.

Douglas E. Stack
Assistant Professor
Department of Chemistry
University of Nebraska at Omaha
Omaha, NE 68182-0109
(402) 554-3647
(402) 544-3647 (fax)
Douglas_Stack@unomaha.edu




From chemistry-request@www.ccl.net  Fri Feb 12 11:08:06 1999
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III CONGRESS OF THE INTERNATIONAL SOCIETY FOR THEORETICAL CHEMICAL
PHYSICS.

MEXICO CITY, UNIVERSIDAD NACIONAL AUTONOMA DE MEXICO (UNAM), NOV. 8-13,
1999.


Miguel Castro (Facultad de Quimica, UNAM, Mexico)
Director of the Congress

Janos Ladik (University of Erlangen, Germany)
Co-director of the Congress


Local Organizing Committee

Carlos Bunge (Instituto de Fisica, UNAM, Mexico)
Gerardo Cisneros (Silicon Graphics, S.A. de C.V.)
Roberto Escudero (Instituto de Investigaciones en Materiales, UNAM,
Mexico)
Luis Enrique Sansores (Instituto de Investigaciones en Materiales, UNAM,
Mexico)


It is with great pleasure that we communicate the first announcement of
the
Third Congress of the International Society for Theoretical Chemical
Physics,
(III-CISTCP), to be held in Mexico City at the National Autonomous
University
of Mexico (UNAM), November 8-13, 1999. As is known, the Society is
interested
in any kind of theory which is applied or can be applied to any chemical

problem. Accordingly, this forthcoming III-CISTCP will address several
research fields going from the development of fundamental (mathematical,

physical, and chemical) aspects up to the application of the proposed
theories
or methodologies to the solution or understanding of some specific
chemical
problems. Contributions (invited talks and poster presentations) will be

published in a special issue of the International Journal of Quantum
Chemistry.

We hope you will be able to attend this meeting and look forward to
seeing you
in Mexico City next year.


TOPICS


 1. Chemical Reactions and Catalysis
 2. Theoretical and Experimental Studies in Material Science
 3. Applications of Relativistic Theories and Quantum
    Electrodynamics to Chemical Problems
 4. Density Functional Theory
 5. Correlation in Molecules and Solids
 6. New Mathematical Techniques for Chemical Problems
 7. Non linear Phenomena
 8. Theory of Molecular and Polymeric Properties



CONFIRMED INVITED SPEAKERS

 R. J. Bartlett (Univ. of Florida, QTP, USA)
 D. M. Bishop (University of Ottawa, Ottawa, Canada)
 D. Buckingham  (Cambridge, England)
 C. F. Bunge     (Instituto de Fisica, UNAM, Mexico)
 R. Carbo (Univ. of Girona, Espana)
 M. Castro    (Facultad de Quimica, UNAM, Mexico)
 B. Champagne (FUNDP, Namur, Belgium)
 J. Cizek (Univ. of Waterloo, Ontario, Canada)
 E. Clementi (Universite L. Pasteur, Strasbourg, France)
 T. Collins   (Oklahoma State University, OKL, USA)
 J. Delhalle  (F.N.D.P., Namur, Belgium)
 D. Dixon (Pacific Northwestern Laboratories, USA)
 R. Escudero  (Instituto de Materiales, UNAM, Mexico)
 W. Foerner (King Fahd Univ.of Petroleum and Minerals, Dhahran, Saudi
Arabia)
 H. Frauenfelder  (Los Alamos National Laboratory, USA)
 I. Grant     (Mathematical Institute, Oxford, England)
 E. K. U. Gross (University of Wurzburg, Germany)
 N. Handy  (Univ. of Cambridge, England)
 I. Kaplan    (Instituto de Fisica, UNAM, Mexico)
 J. Keller  (Faculty of Chemistry, UNAM, Mexico)
 B. Kirtman (Univ. of California, Sta. Barbara, USA)
 W. Kohn   (Univ. of California at Santa Barbara, USA)
 J. Ladik     (Univ. of Erlangen, Germany)
 R. Lefebvre (Lab. de Photophysique Moleculaire, Orsay, Paris, France)
 M. Levy   (Tulane University, New Orleans, USA)
 P. O. Lowdin (University of Florida, USA, and Uppsala University,
Sweden)
 N. March     (Oxford, England)
 D. A. Micha (U. of Florida, QTP, USA)
 W. Miller (Univ. of California, Berkeley, USA)
 J. B. Nicholas (PNNL, EMSL, Richland, WA, USA)
 W. Nieuwpoort  (Univ. of Groningen, Netherlands)
 D. M. Nicholson (Oak Ridge National Laboratory, USA)
 H. Nakatsuji  (Univ. of Kyoto, Japan)
 T. Petrosky  (Instituts Int. Physique et de Chimie, Bruxelles, Belgium)

 J. Paldus  (Univ. of Waterloo, Ontario, Canada)
 P. Saalfrank (Free Univ. of Berlin, Germany)
 D. R. Salahub   (Univ. of Montreal, Canada)
 L. E. Sansores (Instituto de Materiales, UNAM, Mexico)
 D. F. Scofield (Sterling Diagnostic I., Inc., Newark, DE, USA)
 L. Skala (Univ. of Harles, Prague)
 S. Suhai (Cancer Research Center, Heidelberg, Germany)
 S. B. Trickey   (Univ. of Florida, QTP, USA)
 C. Valdemoro  (CSIC, Madrid, Espana)
 V. Van Doren (University of Antwerpen, Belgium)
 A. J. C. Varandas  (Univ. of Coiombra, Coiombra, Portuga)
 L. Wolniewicz  (Univ. of Torun, Poland)
 M. Zaider (Columbia University, N. York, USA)
 T. P. Zivkovic   (Ruder Boskovic Institute, Zagreb, Croatia)



  REGISTRATION FEE

 $350 (until May 1, 1999), $450 (afterwards).
 $250 (for members, until May 1, 1999), $350 (for members, afterwards).
 $200 (for students, until May 1, 1999), $300 (for students,
afterwards).


WE WILL APPRECIATE VERY MUCH THE RETURN, EITHER BY ORDINARY OR BY
ELECTRONIC MAIL, OF THE FOLLOWING INFORMATION.


 NAME: _________________________________________________________


 ADDRESS:_______________________________________________________


 PHONE:_________________________________________________________


 FAX: __________________________________________________________



 E-MAIL:________________________________________________________




  _______      I intend to come to the Congress.

  _______      I am undecided to come to the Congress,
               but please keep me informed.

  _______      I intend not to come to the Congress.




--
Luis Enrique Sansores
Instituto de Investigaciones en Materiales, UNAM
Apartado Postal 70-360
Mexico D.F. 01020
Mexico
Tel: (52)(5) 622-4637   Fax: (52)(5) 616-1251
e-mail: sansores@servidor.unam.mx       lesc@casper.iimatercu.unam.mx





From chemistry-request@www.ccl.net  Fri Feb 12 19:47:48 1999
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From: "Kalju Kahn" <kalju@bioorganic.ucsb.edu>
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Dear CCLers,

I realize there has been some controversy about basis set
superposition error (BSSE), and that the current consensus
favors the view that full counterpoise procedure (CP) of
Boys and Bernardini is a good way to correct for BSSE.
(e.g. van Duijneveldt et. al. in Chem. Rev, 1994, 94, 1873-1885)

My question concerns application of BSSE correction via CP
to bimolecular reactions. Let's take gas phase SN2
displacement as an example. Here we have a two reactants, A and B,
forming first a bimolecular "reactants complex" (RC), followed by
transition state (TS):
          A + B -> (A...B)[RC] -> A-B[TS]
The activation barrier can be defined as an energy difference
between TS and RC. What is the correct way to calculate this
energy difference? (Assuming Born-Oppenheimer approximation,
and dealing with size-consistent methods, e.g. HF level of theory)

My own answer would be:
 If one accepts a view that energies of both RC and TS
 (relative to isolated reactants) are affected by BSSE,
 one should correct both according to the CP scheme, and now:
 E_act = E(TS,TS_basis_in_TS_geometry)-E(RC,RC_basis_in_RC_geometry)-
        E(A,TS_basis_in_TS_geometry) -E(B,TS_basis_in_TS_geometry)+
        E(A,RC_basis_in_RC_geometry) +E(B,RC_basis_in_RC_geometry)

 Obviously, the number of basis functions in TS_basis and RC_basis
 is the same, but the geometrical position of ghost orbitals relative
 to partner molecule are different in TS_geometry and RC_geometry.
 So, the last four terms do not cancel out.

This seems a right way to account for BSSE, but the above method
was quoted as "misinterpretation of the BSSE concept" by Dr. J. A. Sordo
in "Comment on "Ab initio investigation of internal rotation in the
ethylene-sulfur dioxide dimer"" (J. Chem. Phys., 106(14), 6204).

Could somebody kindly explain me how do I misinterpret the BSSE
concept here? Or do we need to be concerned about BSSE when
calculating ab initio activation barriers?

Thanks a lot, Kalju

P.S. I will summarize your responses.

P.S.2. Happy Valentine's Day!

******************************************************************
Kalju Kahn				kalju@bioorganic.ucsb.edu
Chemistry Department			tel: (805)-893-7158
University of California Santa Barbara
Santa Barbara, CA 93106
##################################################################


From chemistry-request@www.ccl.net  Sat Feb 13 03:39:03 1999
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 13 Feb 1999 09:39:01 MET
Date: Sat, 13 Feb 1999 09:39:01 +0100 (MET)
Subject: PCM jobs with Gaussian 98
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Hello !

I'd like to optimize an hexaaquo rhodium (III) complex including solvent 
effects but I don't know if I have to use a PCM standard job or a 
SCI-PCM job with the Gaussian 98 software. Does anyone have 
experience in this domain ?

There are many parameters to set in this kind of job; what are the best 
ones (number of tesserae, scaling factor, etc) ?

Thanks for the preciously help !


Best regards at all. 


D. De Vito (University of Geneva, Physical Chemistry Dept).




From chemistry-request@www.ccl.net  Sat Feb 13 18:02:16 1999
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Does anyone have a pointer to a simple method for histogramming a
distribution of rotations - that is, a parametrization of SO(3) that leads
to 'cubic' bins of equal volume?

Wolfgang Huber
IBM Almaden




From chemistry-request@www.ccl.net  Mon Feb 15 02:40:30 1999
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Date: Mon, 15 Feb 1999 09:40:29 +0200
From: Maija Lahtela <mlahtela@csc.fi>
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Dear CCLers,

  I am trying to do NBO (Natural Bond Orbital) analysis within 
Gaussian98 ( options for calculation b3lyp/6-311+g* scf=tight pop=nboread
IOP(3/59=9)). In the middle of calculations following warning appear:
 
WARNING:  1 low occupancy (<1.9990e) core orbital  found on  P 3
           1 low occupancy (<1.9990e) core orbital  found on  C 5

 WARNING:  Population inversion found on atom  P 3
           Population inversion found on atom  O 4
           Population inversion found on atom  C 5
           Population inversion found on atom  C 6
           Population inversion found on atom  C 7
           Population inversion found on atom  C 8
           Population inversion found on atom  C 9
           Population inversion found on atom  C10
           Population inversion found on atom  O11
           Population inversion found on atom  S13


I am not sure I understand what happend. Can somebody 
give me some hints or comments on that?
Thank you for your help in advance

Sincerely Yours,
Maija Lahtela-Kakkonen

***************************************
Maija Lahtela-Kakkonen
Researcher
CSC-Center for Scientific Computing
P.O.Box 405
FIN-02101 ESPOO FINLAND
TEL 358-9-4572079
FAX 358-9-4572302
E-MAIL mlahtela@csc.fi
***************************************


From chemistry-request@www.ccl.net  Mon Feb 15 05:34:01 1999
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From: "Malgorzata Baranska, p.253, tel. 265" <baranska@Trurl.ch.uj.edu.pl>
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Dear CCLers,
I have a question concerning Gaussian 94.
I had it installed on Pentium 200MHz, 64 Mb RAM.
I have modified my computer to Pentium II 350 MHz, 128 Mb RAM and 
installed Gaussian 94 again, but in spite succesful installation the 
program does not calculate. I can only prepare my input, but when it 
starts calculation I get information about mistake (Win 386, #2069).
Where is the problem? I have heard that this program can calculate 
even on Pentium II 400 MHz, 128 Mb RAM. 
I would be grateful for any suggestion.
M.Baranska

From chemistry-request@www.ccl.net  Mon Feb 15 13:13:31 1999
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To: chemistry@www.ccl.net, chemistry-request@www.ccl.net
Subject: Wavelet Transform.
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Hello.

I am insearchof a wavelet transform program in C for a UNIX (sgi irix 6.5)
box to study time-series data; viz. a single column of floats (reals).

Any thoughts would be appreciated.

Thanks in advance

Iraj.

Iraj Daizadeh, Ph. D.
Harvard University
Department of Cellular and Molecular Biology
The Biological Laboratories, Box #140
16 Divinity Avenue
Cambridge, MA 02138
Phone: (617) 495-0783
       (617) 495-0560
Fax:   (617) 496-4313
Email: daizadeh@fas.harvard.edu


From chemistry-request@www.ccl.net  Mon Feb 15 14:57:43 1999
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Hello!  Please help me.  I need information
about the determination of the dielectric
constant of a solvent mixture (e.g. DMF,
DMSO, acetnitrile and water, maybe 0-40%
solvent in water).  Some of these solvents
canhave ion-pairing interactions.  I
believe that the weighted average dielectic
of the two solvents is not a good enough
approximation.

Can anyone advise me - point me to the
right sources.

Thanks very much,

Mary Jo Ondrechen

From chemistry-request@www.ccl.net  Mon Feb 15 17:16:20 1999
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Date: Mon, 15 Feb 1999 16:21:13 -0600 (CST)
From: Tapas Kar <tapas@risky3.thchem.siu.edu>
To: "Comp. Chem. List" <chemistry@www.ccl.net>
Subject: Most efficient box within $40K
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Hi
 I am looking for expert's recommendation to buy a new box which
will be fully dedicated to Gaussian98/Gamess etc jobs and which should
be able to handle efficiently large calculations (e.g., more than 100 
atomic systems). Our budget is about $40K.
Tapas

--------------------------------------------
Tapas Kar, Ph. D                           
Asst. Scientist/Asst. Professor (Adjunct)                            
Forestry Bldg 118
Department of Chemistry
Southern Illinois University at Carbondale
Illinois 62901-4409

Fax: (618) 453 6408
Tel: (618) 453 6433(Lab) 6485(Office)
--------------------------------------------     


From chemistry-request@www.ccl.net  Mon Feb 15 23:02:02 1999
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Date: Tue, 16 Feb 1999 04:07:50 +0000 (   )
From: Somsak Tonmunphean <somsak@atc.atccu.chula.ac.th>
To: chemistry@www.ccl.net
Subject: Initial Temperature in Simulated Annealing ??
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Dear CCLers,
	I'm interesting to do the docking calculation with Autodock
program which uses Monte Carlo Simulated Annealing (SA) to explore
conformational state. However, I have one question about an initial
temperature in Simulated Annealing (SA). Since the SA is the process in
which the temperature of a molten substance is gradually reduced until it
crystalize, this mean I have to heat the substance until it melt ?? In a
case that my molecule has Carbon atom (m.p. above 3727 degree celcius), do
I have to set the temperature to above 3727 degree celcius ??
	Thank you in advence for your kind help.

Yours sincerely,
Somsak Tonmunphean
Department of Chemistry, Faculty of Science,
Chulalongkorn University, Bangkok 10330 Thailand.




