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From: Karine Miqueu <Karine.Miqueu@univ-pau.fr>
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Dear CCL readers,

     I'm studying deshydrogenation process and I'm interesting 
in knowing how the H2 molecule can be eliminated (differents reactions 
conceivable).
I would like to find all the minima and transition states for a such 
elimination.
Does anyone know theoretical publications' references about deshydrogenation 
or deshydrohalogenation of compounds (example: ethylene ...,cis or trans 
elimination, leaving of H. or H2)?
 

Thanks in advance

Miqueu Karinne
Ph. D. Student

email: Karine.Miqueu@univ-pau.fr

From chemistry-request@www.ccl.net  Thu Feb  4 05:30:18 1999
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Date: Thu, 4 Feb 1999 10:32:21 +0000
From: Michael Nolan <mnolan@nmrc.ucc.ie>
To: ccl <chemistry@www.ccl.net>
Subject: density matrix renormalisation group methods
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Dear CCLers...

We are looking at studying conjugated polymers for application in 
photvoltaic devices.
I have seen the density matrix renormalisation group (DMRG) method used 
for calculation of excitations and non-linear optical properties.

Does anyone have (i) any experience with using DMRG and (ii) knowledge
as to where there might be an available code? (A web search is none
too useful...)

Thank you in advance

Michael
-- 
**************************************************************************
Mr. Michael Nolan	
Materials Modelling Section, Advanced Materials and Technologies Group
National Microelectronics Research Centre  	
Lee Maltings, Prospect Row				   	
Cork
IRELAND

mail: mnolan@nmrc.ucc.ie

Tel:   + 353 21 90 4113

http://nmrc.ucc.ie/projects/ape/
http://nmrc.ucc.ie/groups/AMT/modellingRes.html

EMRS Call for papers:
http://nmrc.ucc.ie/groups/AMT/SympMain.html
****************************************************************************


From chemistry-request@www.ccl.net  Thu Feb  4 06:46:23 1999
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Dear Ron and Allen

For a very inexpensive windows based package look at Molecules 3D from
molecular arts corporation. Some contact information on them follows.
Unfortunately their WWW page (http://www.molecules.com) does not seem
to be functioning.

---------------------------------------------------------
Molecular Arts Corporation       | <info@molecules.com>
Hanover Corporate Centre         | CompuServe: 71644,3626
1532 E. Katella Ave., Suite 1000 | Voice: (714) 634-8100
Anaheim, California 92805, USA   | FAX: (714) 634-1999
---------------------------------------------------------



> Ron A. Rumley- Van Gurp writes:
>
> >We are looking for software (Linux/Windows95/98 or NT) that can draw Lewis
> >structures of organic molecules, depicting all electron lone  pairs as well
> >as bonding pairs. Is there any computer program  available that generates
> >such structures semi-automatically?
>

--

  Dr Mark J Forster Ph.D.
  Principal Scientist
  Informatics Laboratory
  National Institute for Biological Standards and Control
  Blanche Lane, South Mimms,
  Hertfordshire EN6 3QG, United Kingdom.

  Tel  +44 (0)1707 654753
  FAX  +44 (0)1707 646730
  E-mail  mforster@nibsc.ac.uk



From chemistry-request@www.ccl.net  Thu Feb  4 07:29:59 1999
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Hello all!

    I was wondering if there are any references which affirm or disprove the
following idea:

    Proline isomerases, because they make proline unstable by isomerizing it
between the trans
    and cis conformation, can exhibit a protolytic effect (i.e., cause the break
down of
    proline-rich proteins).

Does anyone know if this is "true", or the correct (or more appropriate) forum to
ask this question in?

    Thanks,
            Ray Crawford.


From chemistry-request@www.ccl.net  Thu Feb  4 07:34:43 1999
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Date: Thu, 04 Feb 1999 12:33:22 +0000
From: Krzysztof Radacki <krys.radacki@ac.rwth-aachen.de>
Subject: Freq in G94
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Dear CCLers,
I have question concerning log from IR calculation in G94.
Below is part of this log:
> Low frequencies ---  -82.8125   -5.2461   -0.0021    0.0021    0.0064    7.1252
> Low frequencies ---   10.1830   65.1288   69.2516
> ******    1 imaginary frequencies (negative signs) ****** 
> Harmonic frequencies (cm**-1), IR intensities (KM/Mole),
> Raman scattering activities (A**4/AMU), Raman depolarization ratios,
> reduced masses (AMU), force constants (mDyne/A) and normal coordinates:
>                     1                      2                      3
>                    A"                     A"                     A'
> Frequencies --   -82.7948                65.1108                69.2511
> Red. masses --     1.0165                 1.0212                 1.1460
> Frc consts  --     0.0041                 0.0026                 0.0032
> IR Inten    --     0.0003                 0.0653                 0.8054
> Raman Activ --     0.0000                 0.0000                 0.0000
> Depolar     --     0.0000                 0.0000                 0.0000
 First frequency is 1A"= -82.7948, and I can also see it in first line
that I gave:
"Low frequencies ---  -82.8125" The second is 65.1108 cm^-1, so my
question what
are this "-5.2461   -0.0021    0.0021    0.0064    7.1252    10.1830" 

In other calculation I can see:
> Low frequencies ---   -9.2092   -8.3593    0.0015    0.0037    0.0040   12.9934
> Low frequencies ---   77.1880   77.8672   96.0089
> Harmonic frequencies (cm**-1), IR intensities (KM/Mole),
> Raman scattering activities (A**4/AMU), Raman depolarization ratios,
> reduced masses (AMU), force constants (mDyne/A) and normal coordinates:
>                     1                      2                      3
>                    A'                     A"                     A'
> Frequencies --    77.1868                77.8275                96.0065
> Red. masses --     1.4137                 1.0145                 1.7426
> Frc consts  --     0.0050                 0.0036                 0.0095
> IR Inten    --     0.8422                 0.2056                 0.2503
> Raman Activ --     0.0000                 0.0000                 0.0000
> Depolar     --     0.0000                 0.0000                 0.0000
And the same question, what are in this case first 7 values?

thanks in advance for any helpfull explanation


       Krzys Radacki

_________________________----------------------------------------------------
 -------------------------   e-mail:      
Krys.Radacki@ac.RWTH-Aachen.DE  ---
 -------------------------   ICQ   :      
19021591                        ---

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

From chemistry-request@www.ccl.net  Thu Feb  4 09:56:06 1999
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Date: Thu, 4 Feb 1999 12:55:37 -0200 (BDB)
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Reply-To: ramon kleber da rocha <rkrocha@dedalus.lcc.ufmg.br>
To: Computational Chemistry Mailing List <chemistry@www.ccl.net>
Cc: ramon kleber da rocha <rkrocha@dedalus.lcc.ufmg.br>
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	Hi CCLers
	About a couple of months ago I posted a query about DIBUG mailing
list. Here is my original post:

--------
	Does anybody have any news about DIBUG (Discover Insight Biosym
Users Group) mailing list? 
	I have been tried to find something about it on WWW without
success. In fact the last new I found was about two years ago.
	Best regards.
--------
	
	And here is the only reply I have received:

--------
Date: Thu, 10 Dec 1998 19:57:51 -0800 (PST)
From: Fenglou Mao <mao@csb0.IPC.PKU.EDU.CN>
To: ramon kleber da rocha <rkrocha@dedalus.lcc.ufmg.br>
Subject: Re: CCL:DIBUG Mailing list

Can you tell me the mailing list address when you get it?
Thank you!

Sincerely Yours,

FengLou Mao
*******************************
ADD:Mr. FengLou Mao
    Peking University
    BeiJing
    P.R.China
Tel:86-10-62751490
Fax:86-10-62751725
--------

	I can conclude that DIBUG mailing list is over.
________________________________________________________________________________
Ramon Kleber da Rocha, MSc.                               VOICE +55-31-499-5765
e-mail rkrocha@dedalus.lcc.ufmg.br                        FAX   +55-31-499-5700

Laboratorio de QSAR e Modelagem Molecular
Nucleo de Estudos em Quimica Medicinal - NEQUIM -
http://www.qui.ufmg.br/~nequim
Departamento de Quimica - Instituto de Ciencias Exatas
Universidade Federal de Minas Gerais
Av. Presidente Antonio Carlos, 6627 Campus Pampulha
CEP 31-270-901 - Belo Horizonte - Minas Gerais - Brasil
________________________________________________________________________________

	
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From chemistry-request@www.ccl.net  Wed Feb  3 05:52:54 1999
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From: Ricardo Nunez <rnunez@dali.eis.uva.es>
Reply-To: Ricardo Nunez <rnunez@dali.eis.uva.es>
To: TOPPER ROBERT <topper@cooper.edu>
cc: CHEMISTRY@www.ccl.net
Subject: Re: CCL:optical activity prediction
In-Reply-To: <199901291711.AA09473@zeus.cooper.edu>
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Dear all,
	Our group have developed a method to calculate the
optical activity from molecular geometry, I give you some
references:

J. Mol. Struct., vol. 354, (1995) 81-87
J. Mol. Struct., vol. 442, (1998) 135-143
J. Mol. Struct., vol. 447, (1998) 127-133


Ricardo Nunez Miguel
rnunez@sorolla.eis.uva.es
Departamneto de Quimica Organica
ETS de Ingenieros Industriales
Universidad de Valladolid
Spain



On Fri, 29 Jan 1999, TOPPER ROBERT wrote:

> Hello all,
> 
> An organic chemists with whom I collaborate has asked me
> whether it is possible to predict the optical activity
> of a mixture of enantiomers, even semiquantitatively.
> (i.e., is the optical activity "big" or "small" for
> a given enantiomeric excess, or e.e.).
> 
> My own search of the Internet has failed to turn up anything.
> Can anyone give us any suggestions? 
> 
> Thanks very much!
> 
> best,
> rqt
> 
> *****************************************************************************
> Prof. Robert Q. Topper                  email:   topper@cooper.edu
> Department of Chemistry                 phone:   (212) 353-4378
> The Cooper Union                        fax:     (212) 353-4341
> 51 Astor Place                          subway:  take the 6 to Astor Place 
> New York, NY 10003                               and you're there!
>                  http://www.cooper.edu/engineering/chemechem/
> *****************************************************************************
> The Cooper Union for the Advancement of Science and Art is a tuition-free
> college in Greenwich Village, at Cooper Square and Astor Place.
> *****************************************************************************
> 
> 
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> 




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From: Ricardo Nunez <rnunez@dali.eis.uva.es>
Reply-To: Ricardo Nunez <rnunez@dali.eis.uva.es>
To: TOPPER ROBERT <topper@cooper.edu>
cc: CHEMISTRY@www.ccl.net
Subject: Re: CCL:optical activity prediction
In-Reply-To: <199901291711.AA09473@zeus.cooper.edu>
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Dear all,
	Our group have developed a method to calculate the
optical activity from molecular geometry, I give you some
references:

J. Mol. Struct., vol. 354, (1995) 81-87
J. Mol. Struct., vol. 442, (1998) 135-143
J. Mol. Struct., vol. 447, (1998) 127-133


Ricardo Nunez Miguel
rnunez@sorolla.eis.uva.es
Departamneto de Quimica Organica
ETS de Ingenieros Industriales
Universidad de Valladolid
Spain



On Fri, 29 Jan 1999, TOPPER ROBERT wrote:

> Hello all,
> 
> An organic chemists with whom I collaborate has asked me
> whether it is possible to predict the optical activity
> of a mixture of enantiomers, even semiquantitatively.
> (i.e., is the optical activity "big" or "small" for
> a given enantiomeric excess, or e.e.).
> 
> My own search of the Internet has failed to turn up anything.
> Can anyone give us any suggestions? 
> 
> Thanks very much!
> 
> best,
> rqt
> 
> *****************************************************************************
> Prof. Robert Q. Topper                  email:   topper@cooper.edu
> Department of Chemistry                 phone:   (212) 353-4378
> The Cooper Union                        fax:     (212) 353-4341
> 51 Astor Place                          subway:  take the 6 to Astor Place 
> New York, NY 10003                               and you're there!
>                  http://www.cooper.edu/engineering/chemechem/
> *****************************************************************************
> The Cooper Union for the Advancement of Science and Art is a tuition-free
> college in Greenwich Village, at Cooper Square and Astor Place.
> *****************************************************************************
> 
> 
> -------This is added Automatically by the Software--------
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> 
> 




From chemistry-request@www.ccl.net  Wed Feb  3 08:59:35 1999
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Dear Colleagues;

	About two weeks ago I posted a question to the CCL, and to date the
response has been underwhelming, which is to say that I didn't receive any
replies.  It may well be that the information I seek is not yet available,
though I would be a bit surprised if that were indeed the case.  In any
event, I am reposting this query in the hope that someone will deem to
respond.

	The query is as follows:

       I am seeking published references to neutron diffraction (preferred)
and/or X-ray diffraction (acceptable) data for the following two classes of
compounds:

        (a) simple nitrophenols (with or without an additional alkyl
substituent);

        (b) simple monoalkoxy- or monoaryloxyphenols.

I am also seeking this same data for 

        (c) 2,6-diphenylphenol

If anyone has this information, or access to databases containing this
information, and can dig out the relevant references, I would be very
grateful.

Thanks in advance to all responders,

S. Shapiro
toukie@zui.unizh.ch

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 Dear CCL Readers:

I sent this message last weak and unfortunately anybody reply to my
question, I am very interesting in this topic and I would appreciate
finding someone to know about this.  the message was..

 I am studying  gas chemisorption  on  solid surface and I am
interested  in knowing how the CO2 can be chemisorbed (Different states
of energy, any mechanical theory about that or whatever, and calculus ab
initio)  . If someone can help me whit any kind of information
(publications/refrences) about  this topic I will be very grateful. I
will sumarize the massages.

Thanks in advance.

Alejandro Montoya E.
e-mail: alemoe@catios.udea.edu.co
Ph.D student
University of Antioquia

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<!DOCTYPE HTML PUBLIC "-//W3C//DTD HTML 4.0 Transitional//EN">
<HTML>
&nbsp;
<BR>&nbsp;Dear CCL Readers:
<P>I sent this message last weak and unfortunately anybody reply to my
question, I am very interesting in this topic and I would appreciate finding
someone to know about this.&nbsp; the message was..
<P>&nbsp;I am studying&nbsp; gas chemisorption&nbsp; on&nbsp; solid surface
and I am interested&nbsp; in knowing how the CO<FONT SIZE=-2>2</FONT> can
be chemisorbed (Different states of energy, any mechanical theory about
that or whatever, and calculus ab initio)&nbsp; . If someone can help me
whit any kind of information&nbsp; (publications/refrences) about&nbsp;
this topic I will be very grateful. I will sumarize the massages.
<P>Thanks in advance.
<P>Alejandro Montoya E.
<BR><FONT COLOR="#FF0000">e-mail: alemoe@catios.udea.edu.co</FONT>
<BR>Ph.D student
<BR>University of Antioquia</HTML>

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From chemistry-request@www.ccl.net  Wed Feb  3 11:57:09 1999
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 Dear CCL Readers:

I sent this message last weak and unfortunately anybody reply to my
question, I am very interesting in this topic and I would appreciate
finding someone to know about this.  the message was..

 I am studying  gas chemisorption  on  solid surface and I am
interested  in knowing how the CO2 can be chemisorbed (Different states
of energy, any mechanical theory about that or whatever, and calculus ab
initio)  . If someone can help me whit any kind of information
(publications/refrences) about  this topic I will be very grateful. I
will sumarize the massages.

Thanks in advance.

Alejandro Montoya E.
e-mail: alemoe@catios.udea.edu.co
Ph.D student
University of Antioquia

--------------404EABA60A8DA2084B3678F4
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<!DOCTYPE HTML PUBLIC "-//W3C//DTD HTML 4.0 Transitional//EN">
<HTML>
&nbsp;
<BR>&nbsp;Dear CCL Readers:
<P>I sent this message last weak and unfortunately anybody reply to my
question, I am very interesting in this topic and I would appreciate finding
someone to know about this.&nbsp; the message was..
<P>&nbsp;I am studying&nbsp; gas chemisorption&nbsp; on&nbsp; solid surface
and I am interested&nbsp; in knowing how the CO<FONT SIZE=-2>2</FONT> can
be chemisorbed (Different states of energy, any mechanical theory about
that or whatever, and calculus ab initio)&nbsp; . If someone can help me
whit any kind of information&nbsp; (publications/refrences) about&nbsp;
this topic I will be very grateful. I will sumarize the massages.
<P>Thanks in advance.
<P>Alejandro Montoya E.
<BR><FONT COLOR="#FF0000">e-mail: alemoe@catios.udea.edu.co</FONT>
<BR>Ph.D student
<BR>University of Antioquia</HTML>

--------------404EABA60A8DA2084B3678F4--





From chemistry-request@www.ccl.net  Wed Feb  3 13:54:21 1999
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From: Christoph Maerker <maerker@chris2.u-strasbg.fr>
Message-Id: <199902031854.TAA00344@chris2.u-strasbg.fr>
Subject: summary: problems with G94 volume runs
To: chemistry@www.ccl.net (ccl)
Date: Wed, 3 Feb 1999 19:54:46 +0100 (MET)
Cc: maerker@chris2.u-strasbg.fr (Christoph Maerker)
Organization: Laboratoire de Chimie biophysique, Institut Le Bel,



Universite Louis Pasteur
Postal-Address: 4, rue Blaise Pascal, F- 67000 Strasbourg FRANCE
Phone: +33/3-88-41-53-19
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Dear CClers,

here is the summary for the problems with volume runs in G9x. I have receiv=
ed
three very helpful answers listed below. It was true that the problems
occurred on SGI's. However, the failure seems to come from Gaussian,
not the OS. Larry Cuffe provided a nice patch.

Doug Stack gave the hint to Gaussian test input file test232.com.
I ran it both with G94 and G98 on the same SGI; G94 (RevE.2) gave the zero=
=20
volume as reported before, but G98 (RevA.6) gave non-zero volumes, although
different from those listed in the test232.log file.

I tried other platforms as well (HP-UX and Linux), and got always different
results. I do not list the numbers, because everybody can do it on his own=
=20
hardware within seconds. There seems to be considerable numerical noise in=
=20
the MC procedure applied, rendering the results machine-dependent.

The recommended radii are less affected, whereas the volumes are. Thus, tho=
se
who are interested in the cavity radii and subsequent scrf=3Ddipole runs sh=
ould do
all computations on the VERY same machine !

Regards,
Christoph Maerker

PS The answers are listed according to the authors' last names.

=3D=3D=3D=3D=3D=3D=3D=3D=3D=3D=3D=3D=3D=3D=3D=3D=3D=3D=3D=3D=3D=3D=3D=3D=3D=
=3D=3D=3D=3D=3D=3D=3D=3D=3D=3D=3D=3D=3D=3D=3D=3D=3D=3D=3D=3D=3D=3D=3D=3D=3D
From: "Dale A. Braden" <genghis@darkwing.uoregon.edu>
Subject: Re: CCL:problem with G94 volume runs

Dear Christoph,

Are you running G94 on an SGI?  I had this problem also, and the folks at
Gaussian told me that it was due to a bug in the random number generator
in the SGI operating system.  It appears in some versions of IRIX but not
others.  Gaussian did not give me any fix for it, either, so I was forced
to calculate volumes on another platform.

Best wishes,

Dale

Dale Braden
Department of Chemistry
University of Oregon
Eugene, OR 97403-1253
genghis@darkwing.uoregon.edu

=3D=3D=3D=3D=3D=3D=3D=3D=3D=3D=3D=3D=3D=3D=3D=3D=3D=3D=3D=3D=3D=3D=3D=3D=3D=
=3D=3D=3D=3D=3D=3D=3D=3D=3D=3D=3D=3D=3D=3D=3D=3D=3D=3D=3D=3D=3D=3D=3D=3D=3D=
=3D=3D=3D=3D=3D
From: larry@melanie.ucd.ie (Larry Cuffe)
Subject: Re: SGI problems

Here is the code with a reference for the random number generator at the end
good luck and if there are any problems dont hesitate to contact me.
Larry Cuffe


  The version running on the SGI failed to compute molecular volumes correc=
tly. This computation is made in L604 which performs a Monte Carlo integrat=
ion over a box containing the molecule in this process points within the vo=
lume of the box are sampled a=
t a number of points and the electron density is calculated. If the electro=
n density is above a threshold value it is deemed to be part of the molecul=
e  At the end of this process the volume of the box is multiplied by the ra=
tio of occupied to empty poin=
ts and this is taken to be the molecular volume.  On the SGI machine comput=
ed molecular volumes returned by the program corresponded to either total o=
r zero occupancy.  This problem was traced back to problems with the random=
 number generator which is ca=
lled as a machine dependant function Gran() from the module of machine depe=
ndent utilities mdutil.f  This source file was edited and the call to the m=
achine dependent routine was replaced by a random number generator based on=
 the!
 proposals
    of S. D. Stearns.1.
The code for the relevent changes is detailed below.

Calling Routine in l604.f

*Deck GnMCPt
      Subroutine GnMCPt(IOut,IPrint,MaxPt,NPt,NDone,XO,YO,ZO,X1,Y1,Z1,
     $  XYZ)
      Implicit Real*8 (A-H,O-Z)
C
C     Generate the list of points for Monte-Carlo calculation
C
      Dimension XYZ(MaxPt,3)
      Save One
      Data One/1.0d0/
 1000 Format(' Points from I=3D',I10,' through I=3D',I10)
 1010 Format(' IPt=3D',I10,' XYZ=3D',3F12.6)
C
      IFirst =3D NDone + 1
      ILast =3D NDOne + NPt
      Lim =3D NPt / 2
      Do 10 I =3D 1, Lim
   10   XYZ(I,1) =3D XO + GRan(0)*X1
      Do 20 I =3D 1, Lim
   20   XYZ(I,2) =3D YO + GRan(0)*Y1
      Do 30 I =3D 1, Lim
   30   XYZ(I,3) =3D ZO + GRan(0)*Z1
      Do 40 I =3D (Lim+1), NPt
   40   XYZ(I,1) =3D XO + (One-GRan(0))*X1
      Do 50 I =3D (Lim+1), NPt
   50   XYZ(I,2) =3D YO + (One-GRan(0))*Y1
      Do 60 I =3D (Lim+1), NPt
   60   XYZ(I,3) =3D ZO + (One-GRan(0))*Z1
C
      If(IPrint.ge.3) then
        Write(IOut,1000) IFirst,ILast               =20
        Write(IOut,1010) (I,(XYZ(I,J),J=3D1,3),I=3D1,NPt)
        endif
      Return
      End

Original Code in mdutil.f

*Deck GRan
      Function GRan(IDummy)
      implicit real*8(a-h,o-z)
C
C     Working-Precision random number.
C
      Logical Called
      Integer ITime
#ifdef IBM_RS6K
#define USE_DRAND48
#endif
#ifdef _I386_
#define USE_DRAND48
#endif
#ifdef _SGI_
#define USE_RAND
      External Time
#endif
#ifdef _PMAX_
#define USE_RAND
      Real*4 Rand
#endif
#ifdef __CONVEX__
#define GRAN0_DONE
      Real*4 Secnds, R4Zero, Rand
      Save R4Zero
      Data R4Zero/0.0/
#endif
#ifdef __HPPA
#define GRAN0_DONE
$NOSTANDARD SYSTEM
      Real*4 R4Zero
      Integer ISeed
      Data R4Zero/0.0/
#endif
#ifdef IBM_PC
#define GRAN0_DONE
      Integer*2 I2Time(2), I2, J2
      Real*4 URand
      Equivalence (I2Time(1),ITime)
#endif
#ifndef GRAN0_DONE
      Integer Time
#endif
      Save Called, ITime
      Data Called/.False.
C
      If(Called) then
#ifdef __CONVEX__
#define GRAN1_DONE
        ITIME=3DIrand(ITime)
        GRan =3D Rand(ITime)
#endif
#ifdef __HPPA
#define GRAN1_DONE
        GRan =3D RAN(ISeed)
#endif
#ifdef IBM_PC
#define GRAN1_DONE
        GRan =3D URand(ITime)
#endif
#ifdef ALPHA_VMS
#define GRAN1_DONE
        Gran =3D getran()
#endif
#ifdef _SGI_
        ITime =3D Time()
        Call SRand(ITime)
#endif
#ifdef USE_RAND
#define GRAN1_DONE
        Gran =3D Rand()
#endif
#ifdef USE_DRAND48
#define GRAN1_DONE
        Gran =3D DRand48()
#endif
#ifndef GRAN1_DONE
        GRan =3D DRand(0)
#endif
      else
        Called =3D .True.
#ifdef __CONVEX__
#define GRAN2_DONE
        ITime =3D Int(20.0*Secnds(R4Zero))
        ITime =3D IRand(ITime)
#endif
#ifdef __HPPA
#define GRAN2_DONE
        ISeed =3D Int(20.0*Secnds(R4Zero))
#endif
#ifdef IBM_PC
#define GRAN2_DONE
        Call GetTim(I2,J2,I2Time(2),I2Time(1))
#endif
#ifdef ALPHA_OSF1
#define GRAN2_DONE
        ITime =3D Time()
        Call SRand(ITime)
#endif
#ifdef ALPHA_VMS
#define GRAN2_DONE
        GRan =3D getrans()
#endif
#ifndef GRAN2_DONE
        ITime =3D Time()
#endif
#ifdef __CONVEX__
#define GRAN3_DONE
        GRan =3D Rand(ITime)
#endif
#ifdef __HPPA
#define GRAN3_DONE
        GRan =3D Ran(ISeed)
#endif
#ifdef IBM_PC
#define GRAN3_DONE
        Gran =3D URand(ITime)
#endif
#ifdef ALPHA_VMS
#define GRAN3_DONE
#endif
#ifdef USE_DRAND48
#define GRAN3_DONE
        Call GSR48(ITime)
        Gran =3D DRand48()
#endif
#ifdef USE_RAND
#define GRAN3_DONE
        Call SRand(ITime)
        Gran =3D Rand()
#endif
#ifndef GRAN3_DONE
        GRan =3D DRand(ITime)
#endif
        endIf
      Return
      End

modified code=20

*Deck GRan
      Function GRan(IDummy)
      implicit real*8(a-h,o-z)
C
C     Working-Precision random number.
C     modified LPC 8 sept 98
      Logical Called
      Integer ITime
      Integer SEED
      Save SEED
      REAL*8 RANDX
      SEED=3D2045*SEED + 1
      SEED =3D SEED - (SEED/1048576)*1048576
      RANDX =3D REAL(SEED + 1)/1048577.0
      GRan=3DRANDX
      return
      end

1 S. D. Stearns, "A Portable Random Number Generator for Use in Signal Proc=
essing", Sandia Laboratory Technical Report (1981).

=3D=3D=3D=3D=3D=3D=3D=3D=3D=3D=3D=3D=3D=3D=3D=3D=3D=3D=3D=3D=3D=3D=3D=3D=3D=
=3D=3D=3D
From: Douglas_Stack/CAS/UNO/UNEBR@unomail.unomaha.edu

I've had this same problem w/ G94 running on an SGI Onynx sever (multiple
processors).  I ran a couple of test jobs that applied to the type of
calculations I was doing.  The test for molecular volume is test232.com, wh=
en I
performed this test, I did not get the same output as test232.log!  The
test232.log from Gaussian gives:

 Molar volume =3D  456.410 bohr**3/mol ( 40.729 cm**3/mol)
 Recommended a0 for SCRF calculation =3D  3.28 angstrom (  6.20 bohr)


My test232.log output was:

 Molar volume =3D 2389.438 bohr**3/mol (213.231 cm**3/mol)
 Recommended a0 for SCRF calculation =3D  5.33 angstrom ( 10.07 bohr)

This the only case where I've seen the output from a local job I've run
differing from the output of the Gaussian test file.

I obtained my a0 for SCRF calculations by importing the molecules into Spar=
tan,
creating an density isosurface at the 0.01 level, and having Spartan tell m=
e the
volume of that surface.  With the volume, I worked back to the radius, adde=
d 0.5
A and used that number in SCRF.

If Doug Fox see this tread, maybe he can give some insight to this problem.

Regards,

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  Wed Feb  3 19:35:02 1999
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Reply-To: <hayden@chemcomp.com>
From: "Bill Hayden" <hayden@chemcomp.com>
To: "John Marelius" <john@alpha2.bmc.uu.se>, <chemistry@www.ccl.net>
Subject: RE: Re: Alpha based computers in computational chemistry
Date: Wed, 3 Feb 1999 19:31:54 -0500
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Our software, MOE - the Molecular Operating Environment, is the only
platform independent software on the market.  It covers the full spectrum of
drug discovery and runs on SGI, Sun, WinNT, Win 95 and, of particular
interest to your questions, DEC Alpha NT.

I invite you to visit our site at:  http://www.chemcomp.com

Bill


Hayden@chemcomp.com


-----Original Message-----
From:	chemistry-request@www.ccl.net [mailto:chemistry-request@www.ccl.net]
On Behalf Of John Marelius
Sent:	February 2, 1999 5:40 AM
To:	chemistry@www.ccl.net
Subject:	CCL:Re: Alpha based computers in computational chemistry


On Fri, 29 Jan 1999 shelley.jc@pg.com wrote:

>
> Hello,
>     In the context of individual research laboratories looking for
> workstations or low to mid-range compute servers, are alpha based
computers
> used much in computational chemistry laboratories and if so how?

In the group I work in we use Alpha workstations with WindowsNT for
computational chemistry, mostly running our own molecular dynamics
software. The Alpha + WindowsNT combination has proven to be a powerful
combination of a high-performance number-cruncher and a desktop computer
for word processing (MS Office etc) in one box.
We find systems based on the Alpha processor not only to be the fastest
but also to give the highest performance/price ratio. Systems based on the
new generation of Alpha chips ("21264") are starting to become available,
promising another large jump in performance.

WindowsNT still has some drawbacks as a compute server operating system.
* A third-party batch queue package is needed.
* It's not a (simultaneous) multi-user system although remote login by
telnet is possible (although sometimes problematic) by means of additional
software.

John Marelius

+-----------------------------------------------------------------+
|          John Marelius                                          |
|          Dept. of Molecular Biology, Uppsala University         |
| E-mail:  john@alpha2.bmc.uu.se                                  |
| address: Box 590, S-751 24 Uppsala, Sweden                      |
+-----------------------------------------------------------------+




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Polar has been moved to
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*************************************************
* Dr Weiguang Huang,   BS, MS, PhD, MACS *
* 124 Eastern Avenue, Kingsford   *
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* Phone: 61 2 96620516 (h), 0413 008 019 *
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From chemistry-request@www.ccl.net  Thu Feb  4 13:08:43 1999
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Dear CCL's,

I'm currently working on an implementation of an uniform electric field
in VAMP (a semiempirical program package similar to MOPAC or AMPAC).
This feature is included as an undocumented option in MOPAC, but
comments in the source are missing...

Can anybody give me some references about theory or actual
implementation of an electric field within semiempirical MO theory ?

Any suggestions will be appreciated !!

Anselm Horn

--
_______________________________________________________________________
Anselm Horn, Dipl. Chem. Univ.          Anselm.Horn@ccc.uni-erlangen.de
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From: "Stephen R. Heller" <srheller@nal.usda.gov>
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        chminf-l@listserv.indiana.edu, orgchem@extreme.chem.rpi.edu
Subject: Software for Review
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4  February, 1999

Subject:  Computer Software for Review

	As the Software Review Editor for the ACS Journal of Chemical 
Information and Computer Science (JCICS) I often get software for review 
in the journal.   I have three (3) new software products. I am looking 
for  people who are willing to review these software products.  In return 
for the review which is published in JCICS you get to keep the software 
or database.  The review should be completed in 1-3 months.  The length 
of the review is 4-10 double spaced typed pages.  Sample reviews can be 
found in most of the recent issues of JCICS.

	Please try to give me some (short) reason to choose you over 
another person. 

	I have tried this approach for about the past seven years and it 
is working reasonably well. (REMINDER: For those who haven't finished 
your reviews of software sent months and months ago, this last sentence 
does not apply to you!)  As a result, I am continuing this new method to 
find reviewers using this e-mail/user group system.  I reserve the right 
to abandon this if it is a problem, or inappropriate.  I will not notify 
people if I have found a reviewer.  If you don't hear from me within a 
few days I have chosen someone else to review the particular package.

	As I get many, many, (too many) replies to this message, please 
do not respond after 8 February, 1999 (Monday), as I am sure the software 
will be gone by then.

	I can be reached on Internet (SRHELLER@NIST.GOV).

	PLEASE BE SURE TO INCLUDE AN STREET ADDRESS, PHONE, and FAX 
NUMBER!!!	 (I often send the software by Federal Express.)  Without 
this information I WILL NOT consider your request.


	Steve Heller


The packages I now have are:



1. ACD/Boiling Point 3.6 software from ACD Labs (www.acdlabs.com).  

2. ACD/ChemFinder 3.6 software from ACD Labs (www.acdlabs.com)

3. Elsevier Active Library on Corrosion, version 2.0 on CD-ROM.


Steve Heller, Guest Researcher
NIST/SRD, Mail Stop: 820/113
820 Diamond Avenue, Room 101
Gaithersburg, MD 20899-2310 USA
Phone: 301-975-3338    FAX: 301-926-0416
E-mail:  srheller@nist.gov
WWW:     www.hellers.com/~steve


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Date: Thu, 4 Feb 1999 15:24:42 -0500 (EST)
From: Steve Heller <chem@feldmann.nist.gov>
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Subject: Chemisty & the Internet Meeting 
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The ChemInt'99 draft program is now available at the conference web site:
www.chemint.org.  The list of all invited speakers and virtually all panel
members is now complete and listed in the program.  ChemInt'99 will be
held in at Georgetown University in Washington DC on September 25-27,
1999.  Poster talks/papers submissions will be accepted only via the web
site starting in the spring.

The main lecturers for the meeting will be:

Alan Arnold, University College (UNSW)
Steven Bachrach, Northern Illinois University
Robert Bovenschulte, ACS
Stephen Boyer, IBM
Karl Harrison, Oxford University
Clemens Jochum, Deutsche Bank
Gary Mallard, NIST
Tom Pierce, Rohm & Haas
Jerome Reichman, Vanderbilt
Achim Zielesny, Bayer AG
Steven S. Zumdahl, University of Illinois at Urbana-Champaign


The corporate sponsors for the meeting are:
ChemWeb and the Internet Journal of Chemistry


Technical Sponsors are:

ACS CINF Division 
ACS COMP Division
The Chemical Structure Association (CSA)
Georgetown University - Department of Chemistry
International Union of Pure and Applied Chemistry (IUPAC) (pending)
Japan Association for International Chemical Information (JAICI)
Special Libraries Association (SLA) Chemistry Division
Royal Society of Chemistry (RSC)

A list of current exhibitors is on the web site.


This note is also to remind people that webcasting (video/audio)
and/or slides for more tha a dozen  of the Chemistry and the Internet
(ChemInt'98) meeting talks, held in Irvine CA in September, are also
available on the ChemInt web site (www.chemint.org).  A 42 page report on
the meeting by Wendy Warr is also available.



Steve Heller


Steve Heller, Guest Researcher
NIST/SRD, Mail Stop: 820/113
820 Diamond Avenue, Room 101
Gaithersburg, MD 20899-2310 USA
E-mail:  chem@feldmann.nist.gov





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To: chemistry@www.ccl.net
Subject: Histogram method, redux





Thanks for the replies to my earlier query about the histogram method.
I have attempted to read some of the references suggested (given
below, for those interested, along with other references requested),
but I must confess that I can barely understand them.  Before spending
any more time trying to make sense of them, it would be wise to
determine whether these methods would actually serve my purposes.  So
here I give a schematic description of the problem I'm dealing with,
in the hope that someone may be able to tell me whether the "multiple
histogram method" would be of any use.

Consider a model of protein folding dynamics, with the following
features:

1. The folding is perfectly two-state, the two states being designated
U (unfolded) and F (folded).  Moreover, the two states are well
separated in terms of energy; i.e., if we were able to produce an
energy histogram at the folding transition temperature (Tf), the
distribution would be distinctly bimodal, with a largely unpopulated
region separating the peaks corresponding to F and U.

2. Let t_F(T) and t_U(T) be the mean passage times for the folding
(U->F) and the unfolding (F->U) transitions, respectively, as
functions of the temperature T.

3. We distinguish three temperature regimes I < II < III.  In regime
I, for all practical purposes, t_U(T) is infinite, while t_F(T) is
"reasonably small".  Conversely, in regime III, t_F(T) is practically
infinite, while t_U(T) is small.

4. In regime II, a narrow neighborhood of the folding transition
temperature Tf, both t_F(T) and t_U(T) are roughly equal, and both are
extremely large (of the order of 2-3 CPU-weeks on our workstations).

(Of course, no sharp boundaries separate these three temperature
regimes; t_F(T) and t_U(T) grow rapidly, as one approaches regime II
from regime I and III, respectively.)

5. Because of the slowing down described in 4, it is extremely
difficult to determine Tf.

The single histogram method (which I described in my original post)
would require a single run near Tf, long enough to sample both the F
and U states in a way that actually reflects their relative
probabilities.  For the reason mentioned in (4) and (5) this is
impractical, which seems to rule out this method.

But it was suggested by a few responders to my earlier post that the
*multiple* histogram method may be useful in this case.  The only way
I can see to apply this method is by producing two histograms, one at
temperature T1 in regime I to sample F, and one at temperature T3 in
regime III to sample U.  Then, if we "absorb" the temperature into the
definition of the Hamiltonian (as Ferrenberg and Swendsen do, see
reference below), then this could be construed a case of having two
"Hamiltonians", H/(k*T1) and H/(k*T2), (where H is the actual
Hamiltonian, in the standard nomeclature).  Then I would use the
method of Bennett (see reference below) to obtain a free energy
difference between these two states (as a function of T).  Is this
correct?

(The method of Ferrenberg and Swendsen is a generalization of
Bennett's method to more than two histograms, if I've understood them
correctly).

These multiple histogram methods require a certain amount of overlap
between the histograms, which leads, for the system described above,
to a somewhat paradoxical situation: the greater the overlap between
the two states (meaning that neither P(U;T)/P(F;T) nor P(F;T)/P(U;T)
is too small), the closer the simulation temperatures have to be to
Tf, and therefore the longer it would take to adequately sample the
phase space (as remarked in (4) above).  This suggests that the
multiple histogram method would not be very useful either.  Am I
right?

Thanks for your patience.  Below are the references mentioned above.
Regards,

KJ


Papers that report using the histogram method:

@ARTICLE{klimov-thirumalai98,
		AUTHOR	= {D. K. Klimov and M. R. Betancourt and
		D. Thirumalai},
		TITLE	= {Virtual atom representation of hydrogen
		bonds in minimal off-lattice models of alpha helices:
		effect on stability, cooperativity and kinetics},
		JOURNAL	= {Folding and Design},
		VOLUME	= 3,
		NUMBER	= 6,
		PAGES	= {481--496},
		YEAR	= 1998
		}

@ARTICLE{guo-brooks97,
		AUTHOR  = {Zhuyan Guo and Charles L. {Brooks~III}},
		TITLE   = {Thermodynamics of Protein Folding:  A Statistical
		Mechanical Study of a Small All-$\beta$ Protein},
		JOURNAL	= {Biopolymers},
		VOLUME	= 42,
		PAGES	= {745--757},
		YEAR	= 1997
		}

@ARTICLE{berriz-shakhnovich97,
		AUTHOR	= {Gabriel F. Berriz and Alexander M. Gutin and
		Eugene I. Shakhnovich},
		TITLE	= {Cooperativity and Stability in a {L}angevin Model
		of Proteinlike Folding},
		JOURNAL	= {Journal of Chemical Physics},
		VOLUME	= 106,
		NUMBER	= 22,
		PAGES	= {9276--9285},
		YEAR	= 1997
		}

@ARTICLE{socci-onuchic95,
		AUTHOR	= {Nicholas D. Socci and Jos\'{e} N. Onuchic},
		TITLE	= {Kinetics and thermodynamic analysis of
		proteinlike heteropolymers: Monte Carlo histogram
		technique},
		JOURNAL	= {Journal of Chemical Physics},
		VOLUME	= 103,
		NUMBER	= 11,
		PAGES	= {4732--4744},
		YEAR	= 1995
		}

@ARTICLE{sali-karplus94,
		AUTHOR  = {Andrej \u{S}ali and Eugene Shakhnovich and
		Martin Karplus},
		TITLE   = {How Does a Protein Fold?},
		JOURNAL	= {Nature},
		VOLUME	= 369,
		PAGES	= {248--251},
		YEAR    = 1994
		}


Methodological papers:

@ARTICLE{bennett76,
		AUTHOR  = {Charles H. Bennett},
		TITLE   = {Efficient Estimation of Free Energy Differences
		from {M}onte {C}arlo Data},
		JOURNAL = {Journal of Computational Physics},
		VOLUME  = 22,
		PAGES   = {245--268},
		YEAR    = 1976
		}

@ARTICLE{ferrenberg-swendsen88,
		AUTHOR  = {Alan M. Ferrenberg and Robert H. Swendsen},
		TITLE   = {New {M}onte {C}arlo Technique for Studying
		Phase Transitions},
		JOURNAL = {Physical Review Letters},
		VOLUME  = 61,
		NUMBER  = 23,
		PAGES   = {2635--2638},
		YEAR    = 1988
		}

@ARTICLE{ferrenberg-swendsen89,
		AUTHOR  = {Alan M. Ferrenberg and Robert H. Swendsen},
		TITLE   = {Optimized {M}onte {C}arlo Data Analysis},
		JOURNAL = {Physical Review Letters},
		VOLUME  = 63,
		NUMBER  = 12,
		PAGES   = {1195--1198},
		YEAR    = 1989
		}

@ARTICLE{kumar-rosenberg92
		AUTHOR	= {Shankar Kumar and Djamal Bouzida and
		Robert H. Swendsen and Peter A. Kollman and
		John M. Rosenberg},
		TITLE	= {The Weighted Histogram Analysis Method for
		Free-Energy Calculations on Biomolecules.
		{I}. {T}he Method},
		JOURNAL	= {Journal of Computational Chemistry},
		VOLUME	= 13,
		NUMBER	= 8,
		PAGES	= {1011--1021},
		YEAR	= 1992
		}

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Date: Thu, 04 Feb 1999 22:07:58 +0100
From: Krzysztof Radacki <Krys.Radacki@ac.rwth-aachen.de>
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Dear CCLers,
I would like to thank all people who answerd my question.
Below is one of first answers I get ( from Frank Jensen):
>These are the 6 modes corresponding to overall translation
>and rotation of the molecule. The three 0.00xx modes are the T-modes,
>which should be identically zero, but are not due to numerical
>inaccuracies. The other 3 are the R-modes, which also should be
>zero, but are not since the gradient is not exactly zero. The
>second set of frequencies are obtained by diagonalizing the
>force constant matrix after explicit removal of these 6
>T+R modes.
Once more thank you all.

Regards
      Krzys Radacki
 _________________________----------------------------------------------------
 -------------------------   e-mail:       Krys.Radacki@ac.RWTH-Aachen.DE  ---

----------------------------------------------------------------------------
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Subject: RE: G:Histogram method, redux
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I will try once more to explain with the magnetism analogy (as used by
Ferrenberg and Swendsen).
		
			Magnetism			Protein folding
You tune		Temp & Field (T,Hm)		Temp &
"FoldingField" (T,Hfold)
MC measures		Energy & Magnetization (E,m)	Energy & Degree
of folding (E,f)

In the magnetic system below Tc the free energy F(m) becomes bimodal
with minima at +m and -m.  The MC time required to jump from the +m to
-m grows exponentially with (Tc-T), so it is hopeless to measure the
relative probability of the two states at low T.  You need a way to get
around this.  
	For the multi histogram method we have to options for data
collection, 1) sweep various T values and store energy histograms H(E),
m(e), m^2(e) etc. (as do Ferrenberg and Swendsen) or 2) sweep H values
and store H(m), E(m), E^2(m) etc.  Joining histograms H(E) provides
information on the relative probabilities of the various energy states
P(E), not the probabilities of magnetization states.  For the latter you
need to build up H(m), which is most efficiently done sweeping the
external field that couples to m in the Hamiltonian, Hm.
	Enough magnetism.  For protein folding the story is similar,
joining H(E) histograms does not help you determine H(f). f=degree of
folding).  You need to define a folding parameter (doesn't sound too
hard) and add a term Hfold*f to your Hamiltonian.  Hfold now  "pushes"
your system towards folded (Hfold>0) and unfolded (Hfold<0) states.  In
the end you calculate P(f) (or the log) using the multi histogram method
for a value of Hfold=0, so the fact that Hfold is unphysical is
irrelvant to the final number, it just forces the metropolis algorithm
to sample states that are extremly low probability when Hfold=0.
________________________
                                                  
Jan N. Reimers (Ph.D.)
Manager, Materials Research 
NEC Moli Energy (Canada) Ltd.
________________________ 



