From chemistry-request@ccl.net Wed Feb  2 01:27:41 2005
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From: "Telkuni Tsuru" <telkuni #%# venus.dti.ne.jp>
To: <chemistry #%# ccl.net>
Subject: Movement unit for geometry optimization
Date: Wed, 2 Feb 2005 15:24:00 +0900
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Hello, CCLers.

I like to ask the movement unit for geometry optimization.

The books which I have describe the optimization method as follows:
   ... when one can't find optimized structure, one should calculate 
  force constant of atoms as the differentiation of energy, and move 
  each atoms obeying the force direction. ...

Exactly, there are many MO calculating softwares: Gaussian, Mopac, ...
and so on. I wonder what units they use. 0.1[A], 0.05[A] or 0.01[A] ?
  * [A] is angstrom.

If you know the information which concerns with this question, please 
let me know. 
When I receive replies, I will summarize them.



  Sincerely yours,
----------------------------------------------------
        Telkuni Tsuru     telkuni #%# venus.dti.ne.jp




From chemistry-request@ccl.net Wed Feb  2 02:38:01 2005
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Dear:
 I want run opt=z-matrix freq scf=(tight,direct)
 by method mp2/6-311g** for moleculs cycloheptanone
 ,cyclooctanone, Indanone,3,4-dihydro-2H-naphthalene-1-one
,banzocycloheptanone,banzocyclooctane for my project with
 gaussian 98 A.7 I run this method by in put:
 %mem=256mb
  %nosave
  %rwf=rwf1,245mw,rwf2,245mw,rwf3,245mw,rwf4,245mw
  %CHK=E:\2MP2\CYC7 maxdisk=1960mw
 but I can not accept correct answer

 Please write me how I can run and show me a way for this run
and write me correct ratio between memory and N-basis and maxdisk
and how I can recognize correct memory and maxdisk?
 thanks





__________________________________________________
Do You Yahoo!?
Tired of spam?  Yahoo! Mail has the best spam protection around 
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--0-1028815011-1107326278=:287
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<DIV>
<DIV>
<DIV>
<DIV>Dear:<BR>&nbsp;I want run opt=z-matrix freq scf=(tight,direct)<BR>&nbsp;by method mp2/6-311g** for moleculs cycloheptanone<BR>&nbsp;,cyclooctanone, Indanone,3,4-dihydro-2H-naphthalene-1-one<BR>,banzocycloheptanone,banzocyclooctane for my project with<BR>&nbsp;gaussian 98 A.7 I run this method by in put:<BR>&nbsp;%mem=256mb<BR>&nbsp; %nosave<BR>&nbsp; %rwf=rwf1,245mw,rwf2,245mw,rwf3,245mw,rwf4,245mw<BR>&nbsp; %CHK=E:\2MP2\CYC7 maxdisk=1960mw<BR>&nbsp;but I can not accept correct answer<BR><BR>&nbsp;Please write me how I can run and show me a way for this&nbsp;run<BR>and write me correct ratio between memory and N-basis and maxdisk</DIV>
<DIV>and how I can recognize correct memory and maxdisk?<BR>&nbsp;thanks<BR></DIV></DIV></DIV></DIV><p>__________________________________________________<br>Do You Yahoo!?<br>Tired of spam?  Yahoo! Mail has the best spam protection around <br>http://mail.yahoo.com 
--0-1028815011-1107326278=:287--


From chemistry-request@ccl.net Wed Feb  2 06:13:16 2005
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Date: Wed, 02 Feb 2005 11:09:08 +0200
Subject: dft question on sugar
From: Nicola Catozzi <ctzncl /a\ unife.it>
To: <chemistry /a\ ccl.net>
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Hi I want to know if there are someone expert in DFT calculation methods on
carbohydrates? 

My question is: which  is or which are the best functionals for dft that
describe correctly hydrogen bond and weak interaction like van der walls
etc
in sugar moieties?

Now I9m using b3lyp but it under estimate that kind of forces in my
experiments...while hf overestimate these effects.
 
thanks

By 

Nicola  
======================================================
*  Dott. Nicola Catozzi                              *
*  Department of Chemistry - University of Ferrara   *
*  Via Borsari, 46 - 44100 Ferrara (Italy)           *
*  Tel. +39.0532291177; Fax +39.0532291167           *
*  E-mail  ctzncl /a\ unife.it                           *
======================================================





From chemistry-request@ccl.net Wed Feb  2 06:24:31 2005
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Date: Wed, 02 Feb 2005 10:20:51 +0100
From: Stefan Bromley <s.bromley/at/qf.ub.es>
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Subject: Re: orbital and reality
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Dear all,

I have been following the evolution of the discussion on the reality of 
orbitals with interest. I think it is important, however, to be careful 
to distinguish claims about the possible physical reality of the orbital 
model and the possible physical reality of actual wavefunctions.

Malcolm Davis for example writes:
"Folks have tried to show that there is some "normal" reality underlying 
QM that we just cannot measure.  Such "Hidden Variable" theories have 
been ruled out by "Bell's Inequality" and the "Aspect" experiments.  So, 
wave functions are as real as it gets".

This is a very common misconception and is one I hope that does not 
pervade throughout the whole of the CCL community. Bell's inequality and 
the Aspect experiments rule out only *local* hidden variable theories. 
Based on the work of de Broglie, David Bohm in the 1950s developed an 
example of a theory not ruled out by the Bell inequality (A suggested 
interpretation of the quantum theory in terms of "hidden" variables. I & 
II. D. Bohm, Phys. Rev. 85, 166-193, 1952). In fact Bell's inequality 
came about largely through contemplation of Bohm's work - in particular 
its non-local aspect. Importantly, Bohm's theory, by the necessity of 
its construction, it is exacty equivalent in its predictions to standard 
quantum mechanics. The extra given by such a theory is many-fold in 
terms of physical insight but arguably little in terms of  present day 
measurement. You can find a large resource of literature on the theory 
(see e.g. The Quantum Theory of Motion: An account of the de 
Broglie-Bohm Causal Interpretation of Quantum Mechanics by Peter 
Holland, Cambridge University Press 1995). In this theory (or 
interpretation) the wavefunction is a real field which gives rise to a 
quantum potential acting on a real particle (e.g. an electron) which 
follows a *non-classical* trajectory in real space.

I do not wish to go into the merits or physical validity of such an 
interpretation but just to note that it is perfectly possible to have a 
quantum theory where wavefunctions and electrons do have "an underlying" 
physical reality.

It is, perhaps, of further note that Bohm's causal interpretation of 
quantum mechanics based on the wavefunction as a guiding field to 
particles has lead to some recent advances in the 
modelling/interpretation of scattering and tunnelling processes and 
Quantum Field theory (see e.g. O. V. Prezhdo et al. Phys.Rev. Lett. 86, 3521, 2001, C. L. Lopreore 
et al. Phys. Rev. Lett. 82, 5190, 1999,  A. S. Sanz et al. Phys. Rev. B 
69, 11513, 2004, Phys. Rev. Lett. 93, 090402, 2004)

Best regards,

Stefan Bromley

   





From chemistry-request@ccl.net Wed Feb  2 11:37:44 2005
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Message-ID: <4200E86C.6080508 -()- fen.bilkent.edu.tr>
Date: Wed, 02 Feb 2005 16:49:16 +0200
From: Ulrike Salzner <salzner -()- fen.bilkent.edu.tr>
Organization: Bilkent University
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Hello,
I have money for a couple of PCs and there is a choice between dual CPU 
Intel server mainboards with two 2.8 GHz Xeon processors and a single 
CPU mainboard with one 3.2 GHz Pentium IV processor. The Server with two 
CPUs would coast a bit more than twice as much ($1960) than the a 
machine with one CPU ($875). I could just buy twice as many single CPUs 
machines to get the same number of processors. What would give me a 
better throughput for calculations mainly with G03? Is the Xeon 
processor worth the cost for this purpose or would I waste money?

Thanks for advice,
Ulrike Salzner
salzner -()- bilkent.edu.tr

Associate Professor
Department of Chemistry
Bilkent University





From chemistry-request@ccl.net Wed Feb  2 16:48:50 2005
Message-ID: <1107380928.42014ac0be7cd _(a)_ webmail.nd.edu>
Date: Wed,  2 Feb 2005 16:48:48 -0500
From: Jan K Labanowski <jlabanow _(a)_ nd.edu>
To: chemistry _(a)_ ccl.net
Subject: Call for Papers - Large Scale Molecular Dynamics, Nanoscale, and Mesoscale Modeling and Simulation: Bridging the Gap


----- Forwarded message from rbross _(a)_ mmm.com -----
 Date: Wed, 2 Feb 2005 14:15:21 -0600
 From: rbross _(a)_ mmm.com
 Reply-To: rbross _(a)_ mmm.com
 Subject: Call for Papers - Large Scale Molecular Dynamics, Nanoscale,
          and Mesoscale Modeling and Simulation: Bridging the Gap
 To: jlabanow _(a)_ nd.edu


                              CALL FOR PAPERS

   Large Scale Molecular Dynamics, Nanoscale, and Mesoscale Modeling and
                       Simulation: Bridging the Gap

     230th National American Chemical Society Meeting, Washington, DC
                        August 28-September 1, 2005

             Sponsored by the Computers in Chemistry Division
              Co-sponsored by the Physical Chemistry Division


With increasing accuracy and applicability of molecular modeling tools, the
challenge is beginning to shift to addressing how molecular modeling can
help engineer materials and processes at the macro-scale. The properties at
the macro-scale not only depend on the molecular arrangement, but often on
how the nanoscale arrangements of these molecules themselves cluster. Thus,
molecular design of macroscale properties requires increased understanding
of molecular scale, nano-scale, meso-scale and macro-scale phenomena.

This symposium will focus on applications and methodology development in
integrating the nano, meso and larger length scale regions. Applied
large-scale atomistic molecular dynamics simulations, mesoscale
simulations, and additional course grain methodology studies with focus on
structure-property behavior as well as kinetic processes are requested.
Applications in nanotechnology, biology, inorganic materials, catalysis,
polymers, pharmaceuticals and additional life and materials science areas
are encouraged. Contributions are solicited from academic, industrial, and
the governmental research sectors.

A poster session is planned in addition to oral presentations. A panel
discussion of modeling and simulation in this area is also planned. In
addition, the organizers plan to publish a proceedings pending interest
> from contributing authors.  A social event for contributing authors during
the ACS meeting is also planned.

Please submit abstracts to either Sanat Mohanty or Rick Ross (email below)
at your earliest convenience to aid in session planning.  Please also
directly submit abstracts to the American Chemical Society via the official
on-line abstract submissions system when it becomes available on Feb. 28 to
officially have your presentation entered for the meeting.*   Final
deadline for electronic submission of abstracts is April 25th.  For
additional information on the symposium, please contact Sanat Mohanty or
Rick Ross.

Symposium Organizing Committee:

Sanat Mohanty and Rick Ross
201-2E-23, Corporate Research Materials Laboratory
3M Company, St. Paul, MN 55144
smohanty _(a)_ mmm.com; rbross _(a)_ mmm.com

* see http://oasys.acs.org/ for abstract submission access and guidelines.


From chemistry-request@ccl.net Wed Feb  2 19:03:21 2005
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From: Schrodinger Announcements <announce #%# schrodinger.com>
To: CCL <chemistry #%# ccl.net>
Subject: Schrodinger announces the release of two new products
Date: Wed, 02 Feb 2005 17:38:49 -0500
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Schrodinger announces the release of two new products: Phase, a
high-performance program for ligand-based drug design; and Strike,
powerful new software for statistical modeling and QSAR. Phase is an
easily mastered pharmacophore modeling program, while Strike integrates
a chemically aware statistics package into Schrodinger's modeling
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Along with these two new products are new releases of all of
Schrodinger's software, including Glide, Prime, MacroModel, Jaguar,
Maestro, and more. To find out more about the new releases, please go to
http://www.schrodinger.com.



