From chemistry-request@server.ccl.net  Thu May 27 06:54:13 1999
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Date: Thu, 27 May 1999 11:46:33 +0100
Message-Id: <16730.9905271046@hpf.ch.man.ac.uk>
From: "Nathaniel (noj) Malcolm" <mbdtsnm@mchhpf.ch.man.ac.uk>
To: wtian@uoguelph.ca
Cc: chemistry@ccl.net, jgoddard@uoguelph.ca, huwata@chem.ucla.edu
In-Reply-To: <Pine.HPP.3.95.990525102912.22228E-100000@ccshst01> (message from
	WeiQuan Tian on Tue, 25 May 1999 10:30:14 -0400 (EDT))
Subject: Re: CCL:CASMP2(10,10) Problems (fwd)
Reply-To: Noj.Malcolm@man.ac.uk
X-Beard: Beard v5.3
X-Child: Bethany

 WeiQuan,
just a note of caution, the G98 CASSCF +MP2 is NOT the CASPT2 method
of Roos et al., its the OVB-MP2 method .........

noj

-- 
Dr. Noj Malcolm			
Theory Group, (but only until may 31st)			
Dept. of Chemistry,		
University of Manchester,	
Oxford Road,			
Manchester.			
M13 9PL

e-mail noj.malcolm@man.ac.uk                  


From chemistry-request@server.ccl.net  Thu May 27 09:57:24 1999
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Subject: Re: CCL:Average conformation;  was, A question
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Hi,

	If there is a best way to find some sort of molecular average, I
would think it would be a weighted average, where the weights are those
predicted by a Boltzmann distribution.  If the MD simulation was done
well, this should be what you get from equally weighted MD trajectories.

                                Dave Young
                                youngd2@mail.auburn.edu

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

          Live long and maintain marketable job skills.

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


On Wed, 26 May 1999, Peter Shenkin wrote:

> Hi,
> 
> You could get the "average" conformation by doing an rms superposition
> of all conformations on the first and averaging coordinates, or by
> doing a more sophisticated multiconformer superposition and then
> averaging coordinates.  Simon Kearsley has published a multiple
> conformation superposition method.  So have we, in our XCluster
> paper (J. Comp. Chem., v15, pp899-916, 1994).  Ours involves looking
> at all pairwise superpositions.
> 
> However you do the superposition, the "average" conformation, defined
> as above, might not be terribly useful.  For instance, if half the
> conformations have a +60-degree torsion and the other half have a
> -60-degree torsion, the average might have a 0-degree torsion, and
> thus would not resemble any conformation in the ensemble.  OTOH,
> this might be what you want for some applications.
> 
> It is sometimes more useful to use the "most representative" structure;
> this is the actual structure from the data set that has the smallest
> rms interatomic displacement from the average structure.  It's like
> using the number from a list of numbers which is closest to the
> average, rather than using the average itself.
> 
> In XCluster, we first try to find meaningful clusters (maybe there
> would be two, one with the +60 and one with the -60 torsion). Then
> we write out the the most representative structure from each
> cluster.  Or we can write out the average structure, if that's
> what you really want.
> 
> Hope this helps,
> -P.
> 
> On Wed, 26 May 1999, Richard Wood wrote:
> 
> > Hi all on the CCL
> >    I have a question for you.  I have run 16 molecular dynamics 
> > simulations of the same molecule, each one using a different set of 
> > initial velocities.  From these MD simulations, I have calculated various 
> > properties and obtained their averages.  I have found the lowest PE for 
> > each MD sim and the corresponding conformation.  My question is this: is 
> > there any way that I can generate an "average" conformation that would 
> > give me these "average" properties?
> > 
> > I will post all replies.
> > 
> > Richard
> > 
> > 
> > 
> > 
> > 
> > 
> 
> --
> ********* Peter S. Shenkin; Schrodinger, Inc.; (201)433-2014 x111 *********
> *********** shenkin@schrodinger.com; http://www.schrodinger.com ***********
> 
> -= This is automatically added to each message by mailing script =-
> CHEMISTRY@ccl.net -- To Everybody    |   CHEMISTRY-REQUEST@ccl.net -- To Admins
> MAILSERV@ccl.net -- HELP CHEMISTRY or HELP SEARCH
> CHEMISTRY-SEARCH@ccl.net -- archive search    |    Gopher: gopher.ccl.net 70
> Ftp: ftp.ccl.net  |  WWW: http://www.ccl.net/chemistry/   | Jan: jkl@ccl.net
> 
> 
> 
> 
> 
> 

From chemistry-request@server.ccl.net  Thu May 27 10:07:37 1999
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Date: Thu, 27 May 1999 10:08:40 -0400 (EDT)
From: Peter Shenkin <shenkin@schrodinger.com>
To: David Young <youngd2@mail.auburn.edu>
cc: computational chemistry list <chemistry@ccl.net>
Subject: Re: CCL:Average conformation;  was, A question
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Hi,

Yes, for a conf search, what you say makes some sense.  

It really does depend on just what you want to do with the result.

	-P.

On Thu, 27 May 1999, David Young wrote:

> 
> Hi,
> 
> 	If there is a best way to find some sort of molecular average, I
> would think it would be a weighted average, where the weights are those
> predicted by a Boltzmann distribution.  If the MD simulation was done
> well, this should be what you get from equally weighted MD trajectories.
> 
>                                 Dave Young
>                                 youngd2@mail.auburn.edu
> 
> ------------------------------------------------------------------------
> 
>           Live long and maintain marketable job skills.
> 
> ------------------------------------------------------------------------
> 
> 
> On Wed, 26 May 1999, Peter Shenkin wrote:
> 
> > Hi,
> > 
> > You could get the "average" conformation by doing an rms superposition
> > of all conformations on the first and averaging coordinates, or by
> > doing a more sophisticated multiconformer superposition and then
> > averaging coordinates.  Simon Kearsley has published a multiple
> > conformation superposition method.  So have we, in our XCluster
> > paper (J. Comp. Chem., v15, pp899-916, 1994).  Ours involves looking
> > at all pairwise superpositions.
> > 
> > However you do the superposition, the "average" conformation, defined
> > as above, might not be terribly useful.  For instance, if half the
> > conformations have a +60-degree torsion and the other half have a
> > -60-degree torsion, the average might have a 0-degree torsion, and
> > thus would not resemble any conformation in the ensemble.  OTOH,
> > this might be what you want for some applications.
> > 
> > It is sometimes more useful to use the "most representative" structure;
> > this is the actual structure from the data set that has the smallest
> > rms interatomic displacement from the average structure.  It's like
> > using the number from a list of numbers which is closest to the
> > average, rather than using the average itself.
> > 
> > In XCluster, we first try to find meaningful clusters (maybe there
> > would be two, one with the +60 and one with the -60 torsion). Then
> > we write out the the most representative structure from each
> > cluster.  Or we can write out the average structure, if that's
> > what you really want.
> > 
> > Hope this helps,
> > -P.
> > 
> > On Wed, 26 May 1999, Richard Wood wrote:
> > 
> > > Hi all on the CCL
> > >    I have a question for you.  I have run 16 molecular dynamics 
> > > simulations of the same molecule, each one using a different set of 
> > > initial velocities.  From these MD simulations, I have calculated various 
> > > properties and obtained their averages.  I have found the lowest PE for 
> > > each MD sim and the corresponding conformation.  My question is this: is 
> > > there any way that I can generate an "average" conformation that would 
> > > give me these "average" properties?
> > > 
> > > I will post all replies.
> > > 
> > > Richard
> > > 
> > > 
> > > 
> > > 
> > > 
> > > 
> > 
> > --
> > ********* Peter S. Shenkin; Schrodinger, Inc.; (201)433-2014 x111 *********
> > *********** shenkin@schrodinger.com; http://www.schrodinger.com ***********
> > 
> > -= This is automatically added to each message by mailing script =-
> > CHEMISTRY@ccl.net -- To Everybody    |   CHEMISTRY-REQUEST@ccl.net -- To Admins
> > MAILSERV@ccl.net -- HELP CHEMISTRY or HELP SEARCH
> > CHEMISTRY-SEARCH@ccl.net -- archive search    |    Gopher: gopher.ccl.net 70
> > Ftp: ftp.ccl.net  |  WWW: http://www.ccl.net/chemistry/   | Jan: jkl@ccl.net
> > 
> > 
> > 
> > 
> > 
> > 
> 

--
********* Peter S. Shenkin; Schrodinger, Inc.; (201)433-2014 x111 *********
*********** shenkin@schrodinger.com; http://www.schrodinger.com ***********

From chemistry-request@server.ccl.net  Thu May 27 12:18:11 1999
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From: sergiusz kwasniewski <sergiusz.kwasniewski@luc.ac.be>
Subject: summary: excitation energies

Hi all,

a couple of weeks ago I asked the following question:
_____________________________________________________

---0---

CCL:excitation energies

> Does anyone know something about the difference between the excitation
> energies calculated by RHF CIS and semi-empirical techniques like ZINDO/S
> CIS on organic structures? I've done some calculations on aromatic
> structures, but the spectra are not comparable at all! Is there a reason for
> that behaviour?

The following answers where provided to me:
___________________________________________


---1---

From: "Jens Spanget-Larsen" <jsl@virgil.ruc.dk>
Organization: Roskilde Universitetscenter
To: sergiusz kwasniewski <sergiusz.kwasniewski@luc.ac.be>
Date: Tue, 27 Apr 1999 10:20:45 +0100
Subject: Re: CCL:excitation energies
CC: chemistry@ccl.net

Dear Sergiusz,

HF CIS calculations are generally in error because of neglect of 
electronic correlation effects.  These effects tend to stabilize 
excited states more than the ground state, and the result is that HF 
CIS frequently predicts excitation energies that are much too large.  
Semiempirical procedures like ZINDO/S are especially parameterized to 
account for the effects of electron correlation (in particular, by 
empirical adjustment of the parameters used to estimate electron 
repulsion terms), and these procedures thus predict transition 
energies of the right order of magnitude, at least for the class of 
compunds and types of transition for which they were parameterized.
By the way, have you tried to apply Time Dependent Density Functional 
Theory (TD DFT) as implemented in Gaussian 98?  For example, TD B3LYP 
does a great job for electronic transitions.
Yours, Jens >--<                             
=-=-=-=-=-=-=-=-=-=-=-=-=-=-=-=-=-=-=-=-=-=-=-=-=-=-=-=-=-=-=-=
JENS SPANGET-LARSEN         Phone:  +45 4674 2000  (RUC)
Department of Chemistry             +45 4674 2710  (direct)
Roskilde University (RUC)   Fax:    +45 4674 3011 
P.O.Box 260                 E-Mail: JSL@virgil.ruc.dk
DK-4000 Roskilde, Denmark   http://www.rub.ruc.dk/dis/chem/psos/
=-=-=-=-=-=-=-=-=-=-=-=-=-=-=-=-=-=-=-=-=-=-=-=-=-=-=-=-=-=-=-=

---2---

Hi,

for the semi-empirical techniques, I've been using the whole space (Energy
criterium is 1000 eV), while for the ab initio methods the basis set is
6-311G(d,p) within the FC approximation...

But I'm concerned about the low energy part of the spectrum, and then the
criterium inside the semi-empirical techniques doesn't change much the
appearence of the spectrum.

Did anyone encounter these inconsistencies? (More information about this,
was inside my last mail) Thanks in advance

Sergiusz

At 11:57 AM 4/26/99 -0300, Sergio Emanuel Galembeck wrote:
>Dear Sergiusz,
>    What basis are you using? I don't have experience
>on RHF/CIS, but the results depends on basis sets
>and on the choice of active space.
>    Best regards,
>                Sergio
>PS: Please, sumarize the answers.
>==============================================
>Sergio Emanuel Galembeck
>e-mail: segalemb@usp.br
>===============================================


		     _________________________________________________

			Sergiusz Kwasniewski
			LUC SBG/TS
			Universitaire Campus Gebouw D
			3590 Diepenbeek
			BELGIUM
			tel(direct): 011/268315
			fax	   : 011/268301
			email      : sergiusz.kwasniewski@luc.ac.be
		     _________________________________________________

From chemistry-request@server.ccl.net  Thu May 27 12:50:07 1999
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Sorry if this has already been posted. I'm, temporarily off the list
but thought this would be of real interest. The IBM Data Explorer
visualization software that we have used for a number of years
has officially gone open source and can be obtained free from
the web site (OpenDX.org). 

 Richard Gillilan
 Cornell Theory Center

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

The long awaited announcement is now public. Source code will officially
be
released in two days.
http://www.ibm.com/dx

As a founding member of the OpenDX.org, I'm happy to answer any
questions
that aren't answered on the website(s).

Cheers,

Chris Pelkie
Scientific Visualization Producer
Cornell Theory Center
618 Rhodes Hall
Cornell University
Ithaca, NY 14853-3801
chrisp@tc.cornell.edu
From chemistry-request@server.ccl.net  Thu May 27 14:24:46 1999
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Hi, CCLers:

        I tried to download Ahlrich's VTZ basis set from
tchibm3.chemie.uni-karlsruhe.de which they allowed anonymous logging.
Unfortunately, the anonymous is rejected.  The VTZ basis set also does
not list on his 1992 JCP paper.   Any help would be appreciated!!

Gavin Tsai

From chemistry-request@server.ccl.net  Thu May 27 14:39:10 1999
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Date: Thu, 27 May 1999 14:35:43 -0400 (EDT)
From: Jan Labanowski <jkl@ccl.net>
To: Gavin Tsai <hxt10@po.cwru.edu>
cc: CHEMISTRY@ccl.net
Subject: Re: Ahlrich's VTZ basis set
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On Thu, 27 May 1999, Gavin Tsai wrote:

> Hi, CCLers:
> 
>         I tried to download Ahlrich's VTZ basis set from
> tchibm3.chemie.uni-karlsruhe.de which they allowed anonymous logging.
> Unfortunately, the anonymous is rejected.  The VTZ basis set also does
> not list on his 1992 JCP paper.   Any help would be appreciated!!
> 
> Gavin Tsai
> 


Check the venerable {:-)} CCL archives:
   http://www.ccl.net/cca/data/basis-sets/

Jan
jkl@ccl.net

Jan K. Labanowski            |    phone: 614-292-9279,  FAX: 614-292-7168
Ohio Supercomputer Center    |    Internet: jkl@ccl.net 
1224 Kinnear Rd,             |    http://www.ccl.net/chemistry.html
Columbus, OH 43212-1163      |    http://www.ccl.net/

From chemistry-request@server.ccl.net  Thu May 27 15:37:48 1999
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Richard Gillilan <richard@tc.cornell.edu> said:
> The IBM Data Explorer visualization software that we have used
> for a number of years has officially gone open source and can
> be obtained free from the web site (OpenDX.org). 

And if anyone is interested, here are instructions for getting
the source to compile on IRIX 6.5 using the 7.2 C/C++ compiler.

1) download the source (and examples) from
      http://www.research.ibm.com/dx/download/

2) The configuration code uses the value of SHELL rather than
/bin/sh, so if you have a non-sh compatible shell (like tcsh)
you are best off starting 'sh' then doing
   SHELL=/bin/sh
   export SHELL

3) If you want to use SGI's C++ compiler over GNU, you also need
to set the CXX environment variable to "CC", as in
   CXX=CC
   export CXX

4) Configure by running "./configure"

5) The default 'make' on SGIs isn't very good.  Use "smake" or
GNU make ("gmake" or "gnumake") instead.  This can best be
done by adding

  #!/usr/sbin/smake

to the top of the newly created Makefile.  The normal make will
restart with the #! indicated make if given.

This is needed for compiling dx because otherwise every time
you run "make" it will try to recompile some of the files.  This
is annoying because it will try to recompile even when using
"make install" after the system has been built.

6) The file "src/exec/libdx/memory.c" didn't compile because of
the code:
===
#ifdef SYSTYPE_SVR4
            if (inv->inv_class==INV_MEMORY && inv->inv_type==INV_MAIN) {
                physmem = (uint)((double)inv->inv_state / 1024. / 1024.);
                break;
            }
#else
            if (inv->class==INV_MEMORY && inv->type==INV_MAIN) {
                physmem = (uint)((double)inv->inv_state / 1024. / 1024.);
                break;
            }
#endif  /* SVR4 */
===

It is supposed to use the first block but instead uses the second.
Easiest fix is to replace #ifdef with #ifndef .

7) Once the "#!" was added, "make" it.

8) Become root and "make install".  There is a problem with the
code -- some of it assumes data files are in "/usr/lpp/dx" instead
of "/usr/local/dx" and it will complain about missing files during
startup.  The only fix I know so far is to make a symbolic link,
as in

  cd /usr
  ln -s local lpp

9) Some of the help files are sym linked to themselves.

val> pwd
/usr/local/dx/help
val> ls -l GarHelpDir BMHelpDir
lrwxr-xr-x    1 root     sys           28 May 27 10:48 BMHelpDir ->
  /usr/local/dx/help/MBHelpDir
lrwxr-xr-x    1 root     sys           29 May 27 10:48 GarHelpDir ->
  /usr/local/dx/help/GarHelpDir

There is no fix for this, but it hasn't been a problem (yet?).

10) To use the sample files, set the environment variable DXDATA
to point to your dxsamples-4.0/data directory.

11) Start the program by running "/usr/local/dx/bin_sgi/startupui".

There may be other ways to start it, but I'm not sure what they
are.  Also, looking at the memory usage with "gmemusage", at least
some of the time DX wants up to 400 MB of memory.  If you run
"dxui" directly, it seems to keep that memory need, but starting
>from the startupui makes that need be only transient.  I don't
understand the behaviour, but it may be because dxui isn't meant
to be started directly.

Then take a look at some of the Chemistry extensions developed
by Richard Gililan and others at the Theory Center, under

    http://www.tc.cornell.edu/DX/


						Andrew Dalke
						dalke@bioreason.com
