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Subject: Re: QUESTION STABILITY_KEYWORD?
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From: Paul Momoh 

<<<<<<<<<<<<<<<<<,,
Good morning,
I initially performed a stability job (STABLE) on a DFT (B3LYP) job. I
got the message RHF-> UHF instability. I then performed another
stabilty test (using Stable=repopt). The instability was subsequently
corrected (I got a lower abs energy). Where/how can I get the
corrected coordinates and/or multiplicity and/or method used for the
corrected structure?
>>>>>>>>>>>>>>>>>>>>>>

	  By 'corrected' structure you probably mean the structure 
obtained from geometry optimization with the stable wavefunction. 

		 If you have the reoptimized wavefunction saved in your checkpoint
file you can easily start a geometry optimization job with 
unrestricted B3LYP this way


# ub3lyp/(basis set) guess=read opt 

   Provided that the ub3lyp solution does not converge back to 
rb3lyp during the course of geometry optimization your job
may pick up a different structure. In some cases if the structure
has spatial symmetry it may be necessary to specify scf=nosymm
to prevent the collapse of the unrestricted solution back to 
the unstable restricted solution. 

  Whether the obtained structure is correct or not may or may 
not be contingent on the stability of the wavefunction. 

Wai-To Chan




From chemistry-request@ccl.net Thu Jul 22 08:51:43 2004
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Subject: RE: force constants of diatomics in GAUSSIAN-03
Date: Thu, 22 Jul 2004 09:56:56 -0400
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Thread-Topic: force constants of diatomics in GAUSSIAN-03
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From: "Shobe, David" <dshobe$at$sud-chemieinc.com>
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A few loose ends here (now that my interest has been kindled).  To aid the discussion, let's call R the ratio of [the force constant with respect to Gaussian's mass-weighted definition of a unit step] to [the force constant with respect to interatomic distance].

	fc Gaus	fc dist	R
HF	10.66		9.70		1.10
HCl	5.22		4.80		1.09
HBr	4.19		4.10		1.02
HI	3.23		3.20		1.01
CO	41.34		18.60		2.22
NO	39.29		15.30		2.57


1. One thing that puzzled me was the difference between the H-X molecules for which Gaussian and the web site http://hyperphysics.phy-astr.gsu.edu/hbase/molecule/vibspe.html R is close to 1, and on the other hand NO and CO where R is much larger. 

Given your explanation [first attached message], it seems that the mass ratio of the two atoms is the important thing here, and that the ratio R between the mass-weighted comes between two limits.  The upper limit is the homonuclear case with R=2.  The lower limit occurs with an infinite mass ratio, in which case R=1 because the normal-mode step is purely the movement of the light atom.

2. But if that's true, why is R>2 for CO and NO?  

3. What definition does GAMESS(US) use for the unit step [second attached message]?  It doesn't agree with either Gaussian or the web site!

--David Shobe, Ph.D., M.L.S.
S|d-Chemie, Inc.
phone (502) 634-7409
fax (502) 634-7724

Don't bother flaming me: I'm behind a firewall.



-----Original Message-----
From: Computational Chemistry List [mailto:chemistry-request$at$ccl.net]On
Behalf Of Michael Frisch
Sent: Wednesday, July 21, 2004 10:24 AM
To: chemistry$at$ccl.net
Subject: CCL:force constants of diatomics in GAUSSIAN-03


On Wed, Jul 21, 2004 at 03:15:48PM +0400, Dmitry Rozmanov wrote:
Dmitry Rozmanov wrote
> If this is the case, then I guess this is just a wrong way of doing things 
> and the force constants got by Gaussian are not correct at all. There is a
> definition of the thing and there is no two way of calculation.
> 
> ---Dmitry.
> 

This is nonsense.  The details are in a white paper on our web site,
but the key point is that the force constant is the second derivative
with respect to a normal mode displacement and the units for the
normal mode, or equivalently the convention for what consititues a
unit step, are arbitrary.

For polyatomic molecules, one typically diagonalizes the force
constant matrix in mass-weighted coordinates, so the natural unit step
is a normalized displacement in these coordinates.  This approach is
general and applicable to any polyatomic molecule.  In the particular
case of H2 with the molecule along the x-axis, this normalized step
would be (1/sqrt(2),0,0,1/sqrt(2),0,0) in the 6 cartesian coordinates.
This unit step changes the H-H distance by sqrt(2).  For the particular
case of diatomic molecules when people calculate by hand, they use the
distance between atoms as the coordinate, which simpler for diatomics
but doesn't apply to polyatomics.  In that coordinate system, a unit
displacement changes the distance by 1 rather than sqrt(2), so the force
constants (second derivatives of the energy) differ by a factor of 2.
The corresponding reduced masses for the mode also differ by a factor
of two and the frequency is the same.  

For the diatomic, the "by hand" coordinates give a reduced mass for
the mode which is the same as the overall reduced mass for the
molecule.  For a general polyatomic molecule, the reduced mass
corresponding to a particular mode is not an observable quantity and
is not defined until one adopts a convention for the (arbitrary) size
of a unit normal mode displacement.

Mike Frisch





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Earlier, Dmitry Rozmanov wrote:

This is what Gaussian says:

  Harmonic frequencies (cm**-1), IR intensities (KM/Mole), Raman scattering
  activities (A**4/AMU), depolarization ratios for plane and unpolarized
  incident light, reduced masses (AMU), force constants (mDyne/A),
  and normal coordinates:
                      1
                     SG
  Frequencies --  2117.8243
  Red. masses --    14.8673
  Frc consts  --    39.2882
  IR Inten    --    86.4086
  Atom AN      X      Y      Z
    1   7     0.00   0.00   0.75
    2   8     0.00   0.00  -0.66

This is what GAMESS (US) says:

-------------------------------------------------------------------------------
          INTRINSIC VIBRATIONAL FREQUENCIES AND FORCE CONSTANTS
  FREQUENCIES AND FORCE CONSTANTS IN PARENTHESES SCALED BY 1.000 AND 1.000, RESP.
  -------------------------------------------------------------------------------
  INTERNAL COORDINATE        INTRINSIC FREQUENCIES
                                  (CM**-1)
  --------------------------------------------------

  STR.  2  1               2117.8       (2117.8    )

  --------------------------------------------------------------------
  INTERNAL COORDINATE                INTRINSIC FORCE CONSTANTS
                             (HARTREES/BOHR**2)        (MDYN/ANG)
  --------------------------------------------------------------------

  STR.  2  1                  1.2673  (  1.2673)     19.731  ( 19.731)


You see, the frequencies are perfectly the same and the units are the same.

However, I was pointed to a document which describes some pecularities of how 
Gaussian treats the reduced masses. I saw it before and I cannot still get how 
the same value with definite units can be different with two ways of calculation 
anyway.

Here is the link:
http://www.gaussian.com/g_whitepap/vib.htm#SECTION00036000000000000000

If this is the case, then I guess this is just a wrong way of doing things and 
the force constants got by Gaussian are not correct at all. There is a 
definition of the thing and there is no two way of calculation.

---Dmitry.

Per-Ola Norrby wrote:
>     Hi Dmitry
> 
>> I do no agree here. In fact I can do the same calculation with GAMESS 
>> (US) easily and get the meaningful result with the same method 
>> (ROHF/6-31G):
> 
> 
>     OK, I think you have two problems.  First, if GAMESS and G98 differ 
> that much, it's probably because you located two different states.  Have 
> you compared the total energies of the molecules, and the orbital 
> output?  I had a look in Jaguar, using C2v symmetry (I have to stay with 
> Abelian subgroups).  In that notation, the 2a1 state is high in energy, 
> whereas the 2b1 and 2b2 states are degenerate.  Watch out for this type 
> of situation!  The final wavefunction is completely dependent on the 
> first guess, it's very possible that Gaussian and GAMESS locate 
> different states (you can modify it in Gaussian using the GUESS 
> keyword).  And you can be quite sure that the 2b1 and 2b2 states will 
> not be correctly represented by a simple ROHF.
> 
>     I get my output as frequencies.  For the 2a1 state (the wrong one, 
> since it's high in energy), I get 943 cm-1, whereas 2b1 gives 2278 
> cm-1.  My guess is that GAMESS actually is the culprit here, locating 
> the high-energy state and thus giving a reasonable frequency for the 
> completely wrong reason.  You'd expect that an ROHF solution for a 
> problem that is inherently multideterminant would be expected to give a 
> too high force constant, like Gaussian is doing.
> 
>     And I know the problems of applying MCSCF to "real" situations, I'm 
> currently working with CASPT2 on some metal complexes.  Sometimes you 
> have to, when you run into problems that not even B3LYP or CCSD(T) can 
> handle...
> 
>     Regards,
> 
>     Per-Ola



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From chemistry-request@ccl.net Thu Jul 22 00:48:33 2004
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From: "Telkuni Tsuru" <telkuni..at..venus.dti.ne.jp>
To: <chemistry..at..ccl.net>
Subject: CCL:Fluorescence from Intercalated Dye
Date: Thu, 22 Jul 2004 14:53:48 +0900
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  Hello, CCLers.

I like to ask my interpretation for the fluorescence from the intercalated dye.
All responses, I will appreciate and summarize them.

I'm studying the fluorescence intensity magnification of the intercalated dye
> from the viewpoint of molecular orbital theory. My question is about the
mechanism of this magnification, and I need your comment for my 
interpretation.

  For example, when a dye EtBr(Ethidium Bromide) intercalated into the
  stacked DNA(*) or RNA bases (it is just like a sandwich !), the fluorescence
  intensity is magnified.
  (*) Bases are paired and stacked 

I've read books, papers, and web documents, but I'm yet to understand the
correct theoretical and molecular orbital effect from stacked bases.

Now, I guess the scheme between the stacked bases and dye as follows:
  The dye had intercalated.
  --> MOs of dye are changed by each base.
  --> Degree-of-freedom of dye electron is increased, so the charge separation
      become easier.
  --> Quantum yield for fluorescence is increased, then the fluorescence 
      intensity is magnified.

  ... Is this scheme true? Comment please.


  Thanks in advance,


--------------------------------------------------------
          Telkuni Tsuru        telkuni..at..venus.dti.ne.jp
                        Tekcel corp.
--------------------------------------------------------



From chemistry-request@ccl.net Thu Jul 22 15:25:27 2004
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Date: Thu, 22 Jul 2004 13:31:54 -0700
From: Oliver Hucke <ohucke<<at>>u.washington.edu>
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To: CCL <chemistry<<at>>ccl.net>
Subject: CCL:binding energy of Zn2+ ligands - SUMMARY
References: <40C8AAC8.4090008<<at>>u.washington.edu>
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Dear CCL'ers,

some time ago I sent the request shown below concerning the influence of 
ligand basicity on the binding affinity to a zinc ion.

I received two replies pointing me to interesting papers.
Many thanks to Ida Ma and Miquel Sola!

Oliver

-----------------------my request-------------------------------------
> I am looking for literature describing the influence of the basicity of 
> metal ion ligands (ideally Zn2+ ligands) on the binding energy.
> 
> For example, I would expect the binding energy for an imidazole to be 
> more favorable than for an imidazole with an electron withdrawing 
> substituent, let's say an -SO2-group.
> 
> Can somebody point me to articles on this matter?
> 
----------------------the replies-------------------------------------

   Our group has been working on the gas phase cation-ligand affinities 
(both expt and theory), in particular for K+ and Ag+, and recently 
published a paper for potassium cation affinities in Chem. Eur. J. 2003, 
9, 3383 - 3396, which maybe of interest to you.

   For Zn2+, Ohanessian and Hoppillard been working on the it but I 
think the focus is more on amino acids currently, rather than small 
model organic ligands.  For general cation-ligand interaction, pls 
consult work from Peter Armentrout and Mary Rodger's group.  Their work, 
and some other key references in the area, can be found in the reference 
section in the our paper above.

---

You may find interesting the following papers:

M. Sol`, A. Lledss, M. Duran and J. Bertran, Inorg. Chem. 30 (1991) 
2523-2527.
M. Sol`, J. L. Andris, M. Duran, A. Lledss and J. Bertran, Theor. Chim. 
Acta 91 (1995) 333-351

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

-- 
_______________________________________________________________

Oliver Hucke, Dr.
                               Health Sciences Building - K418C
University of Washington      1959 NE Pacific St.
Dept. of Biochemistry         phone: (206) 685 7046
Box 357742                    fax  : (206) 685 7002
Seattle, WA 98195-7742        email: ohucke<<at>>u.washington.edu
_______________________________________________________________



From chemistry-request@ccl.net Thu Jul 22 23:03:33 2004
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Date: Fri, 23 Jul 2004 12:10:09 +0800 (HKT)
Subject: Evaluate the electrostatic interaction of intramolecules
From: "GAO Yi" <chgy=at=ust.hk>
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Hi,

I want to evaluate the electrostatic interaction contributions of the
intramolecule,  such as an alanine residue. My method is to divided the
intramolecular N-C(alpha) and O=C-C(alpha) bonds, and use hydrogen atoms
instead of the alpha-carbon atoms. But these artificial H-atoms are too
close to represent the real situation. Could you give me any suggestions
to evaluate the electrostatic interactions of such intramolecular hydrogen
bonding?

Best,

Yi Gao
Department of Chemistry,
The HongKong University of Science and Technology, HK



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	 <gauss(at)slater.chemie.uni-mainz.de>,
   Kimihiko Hirao
	 <hirao(at)qcl.t.u-tokyo.ac.jp>,
   Mark Gordon <mark(at)si.fi.ameslab.gov>, Michael Frisch <frisch(at)gaussian.com>,
   Mike Colvin <colvin2(at)llnl.gov>, NeSC <gill(at)nesc.ac.uk>,
   "Noble, CJ (Cliff)" <C.J.Noble(at)dl.ac.uk>,
   Open Babel <openbabel-discuss(at)lists.sourceforge.net>,
   Peter Gill
	 <peter.gill(at)nottingham.ac.uk>,
   Peter Taylor <p.r.taylor(at)warwick.ac.uk>,
   Reinhart Ahlrichs <reinhart.ahlrichs(at)chemie.uni-karlsruhe.de>,
   Richard Friesner <rich(at)chem.columbia.edu>,
   Robert Harrison
	 <harrisonrj(at)ornl.gov>,
   Roland Lindh <roland.lindh(at)chemphys.lu.se>, Sam French <sam(at)ri.ac.uk>,
   Stefano Evangelisti
	 <stefano(at)irsamc.ups-tlse.fr>,
   Stuart Cant <rsc10(at)eng.cam.ac.uk>,
   "Temmerman, WM (Walter)" <W.M.Temmerman(at)dl.ac.uk>,
   "Tyer, RP (Rick)"
	 <R.P.Tyer(at)dl.ac.uk>,
   Walter Thiel <thiel(at)mpi-muelheim.mpg.de>,
   "Wander, A (Adrian)" <A.Wander(at)dl.ac.uk>
Subject: Towards a Common Data and Command Representation for Quantum Chem
	istry
Date: Fri, 23 Jul 2004 13:54:33 +0100
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Towards a Common Data and Command Representation for Quantum Chemistry - the
eCCP1 Project.

The eCCP1 project is a collaboration between CCP1 (Quantum Chemistry) of the
UK CCPs (http://www.ccp.ac.uk/) and the CLRC Daresbury Laboratory's
e-Science Centre (http://www.e-science.clrc.ac.uk). The project aims to
develop, with broad consensus, mechanisms to facilitate the interoperation
of quantum chemistry and other codes, allowing, for example, a plug-and-play
approach to techniques such as QM/MM, or tools such as graphical user
interfaces. The eCCP1 project also builds on developments in Grid technology
and other e-science activities to enable effective use of Grid resources by
the quantum chemistry community.

A specific first object for the eCCP1 project is to track and develop, where
necessary, emerging standards in computational chemistry data and command
representation, with the aim of producing a common widely-accepted format
for quantum chemistry data. The project is beginning to gather the
requirements for the data and meta-data models and associated tools from the
international quantum chemistry community. If you have an interest in this
area, I would encourage you to participate at this early stage, as any
comments/suggestions that you may have could impact on our decisions and
would be very gratefully received. Some information has already been
collected via meetings such as those at NeSC 'Toward a Common Data and
Command Representation for Quantum Chemistry'
(http://www.nesc.ac.uk/esi/events/394/) and 'CCP/e-Science Workshop'
(http://www.nesc.ac.uk/esi/events/298/). It is also planned to start
discussions on the eCCP TWiki site (http://grids.ac.uk/eccp) and email list
(eccp-data(at)forge.nesc.ac.uk). 

Reference implementation tools will be available at NeSCForge
(http://forge.nesc.ac.uk/projects/eccp) and data and meta-data models will
available at the eCCP TWiki site. The models will be made available as UML
and XML schema. Detailed discussions will take place on the mail list and
overview documents will be maintained at the TWiki site. These overviews
will include details of the components of the models and software tools and
issues associated with each. An initial document, based on the data-type
discussions at the NeSC meeting, can now be found at the site. The TWiki
documents will be editable by anyone who has registered at the site and been
given edit access permissions (please see the site main page for guidance). 

This project is about producing something which is practically useful for
quantum chemistry and based on the desires of the quantum chemistry
community, so if you have an interest, please get involved.

For more information on the eCCP1 project, please refer to the eCCP TWiki
site (http://grids.ac.uk/eccp).

Very best wishes,

Philip Couch.

--

Dr Philip Couch,
A46,
CCLRC Daresbury Laboratory,
Daresbury,
Warrington,
Cheshire,
WA4 4AD,
UK.

E-mail: p.a.couch(at)dl.ac.uk



From chemistry-request@ccl.net Thu Jul 22 12:03:37 2004
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Date: Thu, 22 Jul 2004 12:10:02 -0500
From: Jay Ponder <ponder/at/dasher.wustl.edu>
Organization: Biochemistry, Washington University Medical School
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Dear Computational Chemistry List,

A new release of the TINKER Molecular Modeling Package, version 4.2,
is available from the Ponder Lab web site at http://dasher.wustl.edu/
or via anonymous ftp from dasher.wustl.edu in the /pub/tinker area.
We encourage all current TINKER users to upgrade to the new version.

TINKER 4.2 is a modular, general package for molecular mechanics and
dynamics with some special features, facilities and parameter sets for
biopolymers. It currently supports several force fields, including
Amber (ff94, ff96, ff98 and ff99), CHARMM (19 and 27), Allinger MM
(MM2-1991 and MM3-2000), OPLS (OPLS-UA, OPLS-AA and OPLS-AA/L), Liam
Dang's polarizable potentials and our own AMOEBA polarizable atomic
multipole force field. The software contains many advanced algorithms
for energy minimization, molecular dynamics, distance geometry and
global search, including some methods that are not readily available
elsewhere.

Included with TINKER 4.2 are new and updated force field parameter
sets. In particular, this version contains the first public release
of the full AMOEBA polarizable atomic multipole protein force field
(AMOEBAPRO). Several additional AMOEBA parameters for small molecules
are also available, and others will be added shortly.

In addition, release of TINKER version 4.2 coincides with an updated
version of the Force Field Explorer (FFE) visualization program and
GUI for the TINKER package. This new FFE contains major improvements
over previous releases in stability, speed, features, and integration
with TINKER. FFE is currently supported on the Linux, Windows and
Mac OSX 10.3 platforms.

Also new with TINKER 4.2 are downloadable self-extracting installation
packages that install ready-to-use TINKER and FFE versions on Linux,
Windows or Mac OSX 10.3 systems.

As before, TINKER and Force Field Explorer are available with full
source code, a User's Guide, and several examples and molecule files.
Directions are supplied for building the package on most commonly
used CPU/OS combinations. Prebuilt command line executables limited
to a maximum of 10000 atoms are also provided.

Please see the web site above for further information. We ask those
who make significant use of TINKER to complete, sign, and return by
regular mail the license form available on our web site. We keep all
the returned forms and use them to help justify further development
of the package.

Comments, questions and suggestions for improvements should be sent
to ponder/at/dasher.wustl.edu. We are particularly eager to get feedback
> from people who are considering using TINKER and Force Field Explorer
in an instructional setting.

                        Best wishes, Jay Ponder

-- 
Jay W. Ponder                          Phone:  (314) 362-4195
Biochemistry, Campus Box 8231          Fax:    (314) 362-7183
Washington University Medical School
660 South Euclid Avenue                Email:  ponder/at/dasher.wustl.edu
St. Louis, Missouri 63110  USA         WWW:    http://dasher.wustl.edu/



From chemistry-request@ccl.net Thu Jul 22 09:06:05 2004
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Subject: RE: 2 questions
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From: "Shobe, David" <dshobe=at=sud-chemieinc.com>
To: <Stanislav.Ivan=at=unibas.ch>,
   "CCL computational chemistry list (E-mail)" <chemistry=at=ccl.net>
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1. You can continue a TS calculation with "opt=(ts,readfc) geom=check"; if you think the force constants are inaccurate you can use "opt=(ts,calcfc) geom=check" instead.

2. I don't know this myself, but the question of how to add explicit hydrogens to a heavy-atom-only structure comes up a lot on this list, so I'm sure you'll get a useful asnwer from someone.

--David Shobe, Ph.D., M.L.S.
S|d-Chemie, Inc.
phone (502) 634-7409
fax (502) 634-7724

Don't bother flaming me: I'm behind a firewall.



-----Original Message-----
From: Computational Chemistry List [mailto:chemistry-request=at=ccl.net]On
Behalf Of Stanislav.Ivan=at=unibas.ch
Sent: Wednesday, July 21, 2004 5:56 AM
To: chemistry=at=ccl.net
Subject: CCL:2 questions


Dear ccl'ers,
I have 2 questions regarding g03:
1. is it possible to restart previous TS calculation ?
2. how to define explicit (hydrogen) atoms in g03 ?

Thank you.


--
Stanislav Ivan
Universitdt Basel
Departement Chemie
St.Johanns-Ring 19
4056 Basel
Switzerland

Tel.: (+41) (61) 267 11 44
Email: stanislav.ivan=at=unibas.ch

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From chemistry-request@ccl.net Thu Jul 22 01:41:34 2004
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Date: Thu, 22 Jul 2004 09:00:53 +0200
From: Alessandro Contini <alessandro.contini=at=unimi.it>
Subject: Re: CCL:2 questions
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Dear Ivan,
yes, TS calculations can be restarted with the opt=(ts,restart) keyword. It 
could be a good idea using opt=(ts,restart,noeigentest,rcfc) set of keywords 
in order to avoid the interruption of the calculation whenever more than one 
negative eigenvalue are found.
For the point 2 do you mean expliciting H in SCRF calculations? if yes you 
could use scrf=(pcm,read) and put radii=model (wher model could be uff, 
bondi, pauling, etc.) at the end of molecule specifications.

Hope this help, reguards

Alessandro

 
Alle 11:55, mercoledl 21 luglio 2004, Stanislav.Ivan=at=unibas.ch ha scritto:
> Dear ccl'ers,
> I have 2 questions regarding g03:
> 1. is it possible to restart previous TS calculation ?
> 2. how to define explicit (hydrogen) atoms in g03 ?
>
> Thank you.
>
>
> --
> Stanislav Ivan
> Universitdt Basel
> Departement Chemie
> St.Johanns-Ring 19
> 4056 Basel
> Switzerland
>
> Tel.: (+41) (61) 267 11 44
> Email: stanislav.ivan=at=unibas.ch
>
> ----------------------------------------------------------------
> This message was sent using IMP, the Internet Messaging Program.
>
>
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> Jan Labanowski,  jlabanow=at=nd.edu (read about it on CCL Home Page)
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-- 
Alessandro Contini, Ph.D.
Istituto di Chimica Organica "Alessandro Marchesini"
Universit` degli Studi di Milano, Facolt` di Farmacia
Via Venezian, 21 20133 Milano 
Tel. +390250314480 Fax. +390250314476
e-mail alessandro.contini=at=unimi.it





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Date: Thu, 22 Jul 2004 12:20:01 -0700
From: "Black, Gary D" <gary.black/at/pnl.gov>
Subject: CCL:Extensible Computational Chemistry Environment
To: chemistry/at/ccl.net
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Dear Colleagues,

The Extensible Computational Chemistry Environment, ECCE (pronounced
etch-ay), is a freely available suite of graphical user interface
applications with underlying data management support. Many features for
setup, submission, monitoring, and visualization of output from NWChem
(http://www.emsl.pnl.gov/docs/nwchem), Gaussian 03, Gaussian 98, and
Amica (http://gdanitz.hec.utah.edu/amica) electronic structure
calculations are available.  ECCE was first released in 1997 as a core
component of the Environmental Molecular Sciences Laboratory (EMSL) at
Pacific Northwest National Laboratory.  The ECCE project team of
computer scientists and computational chemists continue to provide new
functionality and operational support.  Version 3.2.1 of ECCE has
recently been released and runs on Linux platforms with Intel Pentium
and Itanium compatible processors, SGI workstations, and Sun
workstations.  Distributions of both the full ECCE software suite and
just the three-dimensional direct manipulation Molecule Builder are
available.  New computational codes and features of existing codes not
currently supported can be integrated into Ecce by users through a code
registration capability.

This is the first time ECCE has been widely announced to the
computational chemistry community beyond NWChem users and EMSL
collaborators.  More information about ECCE is available at our website,
http://ecce.emsl.pnl.gov.  Instructions for registering to download the
free software are found at
http://ecce.emsl.pnl.gov/using/download.shtml.  You may subscribe to an
email list for new ECCE release announcements at
http://ecce.emsl.pnl.gov/support/mailing_list.shtml.  Please send any
questions to our support address, ecce-support/at/emsl.pnl.gov.

Gary Black
ECCE project lead, on behalf of the ECCE team


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<P><FONT FACE=3D"Times New Roman">Dear Colleagues,</FONT>
</P>

<P><FONT FACE=3D"Times New Roman">The Extensible Computational Chemistry =
Environment, ECCE (pronounced etch-ay), is a freely available suite of =
graphical user interface applications with underlying data management =
support. Many features for setup, submission, monitoring, and =
visualization of output from NWChem (</FONT><A =
HREF=3D"http://www.emsl.pnl.gov/docs/nwchem"><U><FONT COLOR=3D"#0000FF" =
FACE=3D"Times New =
Roman">http://www.emsl.pnl.gov/docs/nwchem</FONT></U></A><FONT =
FACE=3D"Times New Roman">), Gaussian 03, Gaussian 98, and Amica =
(</FONT><A HREF=3D"http://gdanitz.hec.utah.edu/amica"><U><FONT =
COLOR=3D"#0000FF" FACE=3D"Times New =
Roman">http://gdanitz.hec.utah.edu/amica</FONT></U></A><FONT =
FACE=3D"Times New Roman">) electronic structure calculations are =
available.&nbsp; ECCE was first released in 1997 as a core component of =
the Environmental Molecular Sciences Laboratory (EMSL) at Pacific =
Northwest National Laboratory.&nbsp; The ECCE project team of computer =
scientists and computational chemists continue to provide new =
functionality and operational support.&nbsp; Version 3.2.1 of ECCE has =
recently been released and runs on Linux platforms with Intel Pentium =
and Itanium compatible processors, SGI workstations, and Sun =
workstations.&nbsp; Distributions of both the full ECCE software suite =
and just the three-dimensional direct manipulation Molecule Builder are =
available.&nbsp; New computational codes and features of existing codes =
not currently supported can be integrated into Ecce by users through a =
code registration capability.</FONT></P>

<P><FONT FACE=3D"Times New Roman">This is the first time ECCE has been =
widely announced to the computational chemistry community beyond NWChem =
users and EMSL collaborators.&nbsp; More information about ECCE is =
available at our website, </FONT><A =
HREF=3D"http://ecce.emsl.pnl.gov"><U><FONT COLOR=3D"#0000FF" =
FACE=3D"Times New Roman">http://ecce.emsl.pnl.gov</FONT></U></A><FONT =
FACE=3D"Times New Roman">.&nbsp; Instructions for registering to =
download the free software are found at </FONT><A =
HREF=3D"http://ecce.emsl.pnl.gov/using/download.shtml"><U><FONT =
COLOR=3D"#0000FF" FACE=3D"Times New =
Roman">http://ecce.emsl.pnl.gov/using/download.shtml</FONT></U></A><FONT =
FACE=3D"Times New Roman">.&nbsp; You may subscribe to an email list for =
new ECCE release announcements at </FONT><A =
HREF=3D"http://ecce.emsl.pnl.gov/support/mailing_list.shtml"><U><FONT =
COLOR=3D"#0000FF" FACE=3D"Times New =
Roman">http://ecce.emsl.pnl.gov/support/mailing_list.shtml</FONT></U></A>=
<FONT FACE=3D"Times New Roman">.&nbsp; Please send any questions to our =
support address, ecce-support/at/emsl.pnl.gov.</FONT></P>

<P><FONT FACE=3D"Times New Roman">Gary Black</FONT>

<BR><FONT FACE=3D"Times New Roman">ECCE project lead, on behalf of the =
ECCE team</FONT>
</P>

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