From h332262@sirius.cab.u-szeged.hu  Wed Oct 15 03:19:10 1997
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From: Kiss Gergo <h332262@sirius.cab.u-szeged.hu>
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To: chemistry@www.ccl.net
Subject: Molucule sketcher under Linux ,Irix or DECUnix
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Hi everybody,

I am looking for a FREE sketcher(drawer), which can create input files for
quantum chemical software(mopac, gamess,...). It would be important, I
need it bad, but my department can't afford it.
Please Help!!!!!

Kiss Gergo
h332262@sirius.cab.u-szeged.hu


From jochen@pc1.uni-duesseldorf.de  Wed Oct 15 06:30:47 1997
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Date: Wed, 15 Oct 1997 12:26:39 +0200
From: Jochen Kuepper <jochen@pc1.uni-duesseldorf.de>
Message-Id: <9710151026.AA04111@bacchus.pc1.uni-duesseldorf.de>
To: h332262@sirius.cab.u-szeged.hu
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molden from
  http://www.caos.kun.nl/~schaft/molden/molden.html
 =20
  Jochen

-----------------------------------------------------------------------
  Jochen K=FCpper

  Heinrich-Heine-Universit=E4t D=FCsseldorf     =
jochen@uni-duesseldorf.de
  Institut f=FCr Physikalische Chemie I
  Universit=E4tsstrasse 1, Geb 26.43.02.19       phone ++49-211-8113681
  40225 D=FCsseldorf                             fax   ++49-211-8115195
  Germany             http://www-public.rz.uni-duesseldorf.de/~jochen
-----------------------------------------------------------------------

From rummey@chemie.uni-wuerzburg.de  Wed Oct 15 07:30:49 1997
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Date: Wed, 15 Oct 1997 12:16:06 +0100 (MET)
From: Christian Rummey <rummey@chemie.uni-wuerzburg.de>
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To: chemistry@www.ccl.net
Subject: Summary: g94 frequency-output
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Hi!

About a week ago I posted a msg about visaulisation of the g94 frequency 
output. Thanks again to all who replied, and now for the people who asked 
about it: the summary

- 1. Vibration Modes for Windows
I didn't try it until now, possibly can only read gaussian92 output.
available at
ftp://ftp.ccl.net/pub/chemistry/software/MS-WIN3/Vibration_modes_for_Windows/
vibratio.zip

- 2. Viewmol
can only read g92 output (in this version) but Dr. Joerg-R. Hill sent me 
a 'patch' for g94 output. If one needs it, ask me for it.
Sorry, but I'm very busy at the moment, so I didn't try to compile it yet.

file://ftp.ask.uni-karlsruhe.de/pub/education/chemistry/viewmol.source-2.0.3.tar.gz

- 3. AniMol (for Windows)
but the poster didn't tell me where to get it.

- 4. Molwin
Avaikable at the CCL-Archive, needs the long frequency-output from 
gaussian94 (# freq=HPMode MP2/6-31G*)


- 5. xvibs (version 4)
ftp://www.ccl.net/pub/chemistry/software/SOURCES/C/xvibs/
Its output can be read eg by xmol.


That's all.
Sorry I did not have the time for testing yet.

Cheers
CR

 _________________________________________________________________
/                                                                 \
|  Christian Rummey                                               | 
|  Institut fuer Organische Chemie                                |
|  Universitaet Wuerzburg                                         |
|  Computational Chemistry Group                                  |
|                                                                 |
|  Am Hubland        |    email : rummey@chemie.uni-wuerzburg.de  |
|  97074 Wuerzburg   |    voice : +49-(0)931-888-4750             |
|  Germany           |    fax   : +49-(0)931-888-4755             |
\_________________________________________________________________/


From Marc.Prosenc@uni-konstanz.de  Wed Oct 15 10:31:06 1997
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From: Marc.Prosenc@uni-konstanz.de (Marc-Heinrich.Prosenc)
Subject: vibration spectras from force-field calculations
To: CHEMISTRY@www.ccl.net
Date: Wed, 15 Oct 1997 15:31:26 +0200 (CDT)
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dear CCLers,

it would be kind if anyone could tell me if there exist a program that calculates
vibrational spectras from forcefields like MM2 or DISCOVER or HYPERCHEM .... for free ?

do there any public domain routines exist, which are able to refine existing forcefields
like mm2 or amber when the IR-spectrum is given ?


thx in advance


Marc




Marc Heinrich Prosenc
Universitaet Konstanz
78434 Konstanz
Po 5560 M738

Prosenc@dg5.chemie.uni-konstanz.de





From nbbienia@cyf-kr.edu.pl  Wed Oct 15 10:39:33 1997
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Date: Wed, 15 Oct 1997 15:45:21 +0200 (METDST)
From: Leslaw Bieniasz <nbbienia@cyf-kr.edu.pl>
To: chemistry@www.ccl.net
Subject: cheminformatics
Message-ID: <Pine.HPP.3.95.971015154114.9356A-100000@kinga.cyf-kr.edu.pl>
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				Cracow, 15.10.97

Hello,

I am looking for the (published) definition of "cheminformatics"
and for the most recent review papers or other prominent references on 
this subject. I would appreciate any help.

Sincerely,

					L. Bieniasz

*-------------------------------------------------------------------*
|                         Dr. Leslaw Bieniasz,                      | 
| Institute of Physical Chemistry of the Polish Academy of Sciences,| 
| Molten Salts Laboratory, ul. Zagrody 13, 30-318 Cracow, Poland.   | 
|                    tel./fax: +48 (12) 266-03-41                   |
|                      E-mail: nbbienia@cyf-kr.edu.pl               |
|                    Web site: http://www.cyf-kr.edu.pl/~nbbienia   | 
*-------------------------------------------------------------------*


From elewars@alchemy.chem.utoronto.ca  Wed Oct 15 10:44:01 1997
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Date: Wed, 15 Oct 1997 10:23:18 -0400 (EDT)
From: "E. Lewars" <elewars@alchemy.chem.utoronto.ca>
Message-Id: <199710151423.KAA10197@alchemy.chem.utoronto.ca>
To: chemistry@www.ccl.net
Subject: EXTENDED HUECKEL AND ORTHOGONALIZATION


Wed, 1997 Oct 15

>From E. Lewars
To:  CCL
Subj: Extended Huckel Method

Hello,

Regarding the extended Hueckel method as implemented by Roald Hoffmann:
I know that the overlap integrals are calculated and used to construct
the Fock matrix elements (which are proportional to these integrals in
the EHM).   My question is:
in Hoffmann's implementation are the overlap integrals used to calculate an
orthogonalizing matrix to convert (e.g. by Loewdin orthogonalization) the
matrix equation
                    FC = SCe
into standard eigenvalue form
                    F'C' = C'e   i.e   F' = C'eC'^-1

as in ab initio calculations,
        OR  is it simply pretended, as in simple Hueckel theory, that
                    S=I  ?

   I read Hoffmann's 1963 paper in J Chem Phys, but this point does not
seem to be explicity made clear.  Maybe I missed it.

        Thanks


         E. Lewars
=============

From eldbjorg.sofie.heimstad@nilu.no  Wed Oct 15 10:46:56 1997
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From: =?iso-8859-1?Q?Eldbj=F8rg_Sofie_Heimstad?=
	 <eldbjorg.sofie.heimstad@NILU.no>
To: "'chemistry@www.ccl.net'" <chemistry@www.ccl.net>
Subject: Software for 3D-QSAR/QSTR
Date: Wed, 15 Oct 1997 15:35:51 +-100
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Dear members,

I would be very happy if some of you could give me your opinions about =
software packages
which include the methods of SAR, CoMFA, QSAR, QSTR etc. I have some =
information from the internet about the methods, but is more difficult =
to evaluate the different software packages. For instance, is there a =
need for several different software packages to get the most reliable =
effect modelling. I have assumed that the molecular descriptors ( =
electrostatic-, steric-,etc.) should be derived from 3D molecular =
structures, do one separate between the definitions QSAR and 3D-QSAR ?

My background are more or less within molecular mechanics and molecular =
dynamics simulations of enzymes, but I am now looking into the =
enviromental toxicology field.=20

All responses will be appreciated,
Thanks in advance,

#########################################
Eldbj=F8rg S. Heimstad, Dr.scient.=20
NILU Norwegian Institute for Air Research=20
P.O. Box 1245=20
N-9001 Troms=F8, Norway=20

Tel. +47-77 60 69 74
Fax. +47-77 60 69 71=20
E-mail: Eldbjorg.Sofie.Heimstad@nilu.no
#########################################


From gmercier@mail.med.upenn.edu  Wed Oct 15 10:48:19 1997
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From: "Gustavo A. Mercier Jr" <gmercier@mail.med.upenn.edu>
Message-Id: <199710151357.JAA31579@mail.med.upenn.edu>
Subject: moldy: quaternion constraint error
To: chemistry@www.ccl.net
Date: Wed, 15 Oct 1997 09:57:02 -0400 (EDT)
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Hi!

I am trying to perform some rigid body dynamic simulations
using MOLDY 2.11b in an SGI box R4000 running IRIX5.3

The system is a manganese metalloporphyrins embeded in
a water box (454 waters). This system was "equilibrated"
using amber4.1 by letting the waters move around the fixed
metalloporphyrin in a 22 ps simulation. Only the nonbonded
interaction was kept. The water model is the TIP3P, a
rigid water model available in amber4.1

I programmed a filter to get the amber output (XYZ)
to the (COM, Rotation quaternion) used in moldy, but
discarded the velocities!

Below is the input to moldy (the control file).
The system file contains the COM and quaternions, plus
the parameters for a L-J potential, and atom-centered
point charges.

**** Problem:
 While heating the system up (starting at 300K gave the
same error) doing 2ps runs at 0K, 50K, 100K, 150K I ran
into the following error:

*F* Quaternion (some #) constrain ... (another number)

Looks like the magnitude of the quanternion is no longer 1.0

**** Question:

What are possible causes...? Any help will be welcomed!

I am already using a step size 0.001ps The scale interval is
0.005ps using Mx-Bz temperature scaling.
I am only doing NVT dynamics.  The box is 27.0488x26.8614x19.3569.
This is the result of the amber4.1 NPT run at 300k using Baerends
thermostat/pressure sink. The density is 1.0087gm/cc

Using defaults the e-walds parameters yields the following:

        Interaction cut-off              = 10.394 A
        Alpha parameter for Ewald sum    = 0.326263 A(-1)
        Reciprocal space cut-off         = 2.21282 A(-1)

 *I* Distant potential correction = -76.180287, Pressure correction = 
-17.982072
 *I* MD cell divided into 1521 subcells (13x13x9)
 *I* Neighbour list contains 488 cells
 *W* System has net electric charge of 1 - correction of 1.45791 
kJmol(-1) added to
 self energy
 *I* Ewald self-energy = 2168.232620 Kj/mol
 *I* 1298 K-vectors included in reciprocal-space sum

-------- Input file ---------------------

title=MnPm/TIPS3 after 22.5 ps; Q's  tweaked; d=1.0087
sys-spec-file=mnpmW.sys
lattice-start=1
nsteps=2000   # 2.0 ps 
step=0.001
save-file=mnpmW4.rst
restart-file=mnpmW3.rst # run at 100K
text-mode-save=0
scale-interval=5
const-temp=0
scale-options=8     # Mx-Bz distribution
temperature=150.0
const-pressure=0
strain-mask=238   # all off diagonals fixed
strict-cutoff=0  # only cell to cell interaction otherwise tooo slow!
surface-dipole=0
average-interval=100
rdf-interval=10   # every 0.05 ps
dump-file=mWdmp
time-unit=4.8888213e-14  # reading kcal/mol; not kJ/mol
end

 -- 
                                      ("`-/")_.-'"``-._
Gustavo A. Mercier,Jr.,MD,PhD         (. . `) -._    )-;-,_() 
Division of Nuclear Medicine          (v_,)'  _  )`-.\  ``-
Dept. of Radiology                    _;- _,-_/ / ((,'
University of Pennsylvania           ((,.-'  ((,/
3400 Spruce St.                  gmercier@mail.med.upenn.edu
Philadelphia, PA 19104         215-662-3069/3091 fax: 215-349-5843



From daizadeh@indigo.ucdavis.edu  Wed Oct 15 11:31:02 1997
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From: "Iraj Daizadeh" <daizadeh@indigo.ucdavis.edu>
Message-Id: <9710150811.ZM20690@indigo.ucdavis.edu>
Date: Wed, 15 Oct 1997 08:11:33 -0700
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To: chemistry@www.ccl.net, daizadeh@indigo.ucdavis.edu
Subject: Molecular Dynamics on Biological Molecules.
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Hello.

Our group has just bought 2 DEC 500 au (low-end workstations) running DEC UNIX
4.0c and we are trying to find computational chemistry software packages that
can calculate classical dynamics of motion for large (circa. 2000+atoms)
biological molecules.  It would be nice if the programs could implement a
Nose/Hoover thermostat and equipped with a variety of force fields such as
amber, ESFF, cff91, etc...  Futhermore, the programs (which may be free or
commercial) must be able to write out trajectories to some sort of archive file
in ascii form for our own calculations.  I will summarize the results as is
customary.

Thanks in advance for all contributions.

Iraj.

-- 
Iraj Daizadeh
Department of Chemistry
University of California
One Shields Ave.
Davis, CA  95616-5295
Phone:  916.754.8695
Fax:    916.752.8995
email:  daizadeh@indigo.ucdavis.edu

From yliu@mail.wesleyan.edu  Wed Oct 15 12:30:57 1997
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Date: Wed, 15 Oct 1997 11:41:39 -0400
To: chemistry@www.ccl.net
From: Yongxing Liu <yliu@wesleyan.edu>
Subject: Summary: Assign Atomic Types for Small Molecules.
Cc: dbeveridge@mail.wesleyan.edu


Dear CCLers, 

Thanks again for all who answered my questions. This a summary.

**** The Original Question****

I am looking for rules based on SMILES to assign molecular mechanic atomic
types( e.g. for OPLS all atom model) to a variety kinds of small organic
molecules and molecular ions(total about 300 molecules).  By doing that I
can assign atomic charges and VDW radii for each molecule atom. Would any
one please give me any information about where can I find these rules and
programs(free source code) to do this ? Or are there any alternative ways
to assign MM atomic charges and VDW radii for small organic molecules
automatically? 

**** Comments to the question ****

My goal is to assign OPLS-AA/AMBER charges and VDW radius to each atom for
my 300 molecules training set. I tried HyperChem and Insight-Buider.
HyperChem can assign AMBER types to all my moelcules, but AMBER do not have
charge parameters for all my small molecules(Unless you do the ab initio
calculation which I can not afford for all my 300 molecules). I also do not
want to write OPLS rules for InsightII Builder.  

*** Answers from Professor DOUGH ****

BABEL does conversion of simple SMILES to MM2/MM3 file formats - you should
search for it to find the places it can be obtained.

*** Answers From Professor  TJ O'Donnell ***

We published a paper on a method to assign atom types using
SMARTS, an extension of SMILES to define molecular substrucutres,
which of course include atoms.
I believe this is what you were looking for.
We have sets of SMARTS for a variety of atom-type sets,
e.g. AMBER, GRIN/GRID, etc., but not for OPLS.
The actual implementation uses an old (no longer supported)
Daylight program GCL and we have not modified the program
to work with newer Daylight versions.  However, the SMARTS
strings defining the atomic environments are entirely
compatible with recent versions of Daylight SMARTS.

A General Approach for Atom-Type Assignment and the Interconversion of
Molecular Structure
Files, TJ O'Donnell, et. al., J. Comput. Chem., 12, 209-213 (1991). 

*** Answers From Professor Richard Gillilan ***

Although FFAssign is not yet available for general use, I am interested
in any intrepid early users who would be willing put the code to a good
test (not too many please). Currently the code should reproduce all 
the charge assignments in Halgren's papers and supplementary 
material except two or three cases documented in the README (soon to 
be fixed). Many of the exotic chemical types have not been tested yet.

 The assignments are being tested against available published results
 and should agree with all values in Halgren's papers (please notify 
 me if you find exceptions). I have not yet compaired absolute energy
 values against those in commercial implementations (soon, maybe). 

Interested persons should
contact me (Richard Gillilan) richard@tc.cornell.edu
---------------
               >>>> FFAssign Version 0.0 <<<<

          Copyright (C) 1997 Cornell Theory Center

 FFAssign is an independent implementation of the MMFF94 force field
 written at the Cornell Theory Center. The Theory Center's Parallel 
 Processing Resource for Biomedical Scientists is supported by the National 
 Center for Research Resources of the NIH under grant # P41 RR04293. 

What does FFAssign do?

 FFAssign reads in a molecular coordinate file (in either of
 two formats) and assigns empirical forcefield parameters
 based on the chemical types encountered and supplies efficient
 basic simulation functionality suitable for inclusion in 
 user-written (C++) applications. Output files generated are
 also compatible with Trevor Hart's RESEARCH docking program.
 FFAssign is a FULL implementation of the Merck Molecular Force 
 Field (MMFF94) based on the published work of T.A. Halgren:

 T.A. Halgren. "Merck Molecular Force Field. I. Basis, Form, Scope,
 Parameterization, and Performance of MMFF94
 Journal of Computational Chemistry", Vol 17 Nos 5,6  pp 490-519 (1996)

(See also parts II-V in the same Journal and supplementary material)

*** Conclusion ***

The above answers are very helpful to me. Based on the answers, I will write
a program suitable for my purpose.



 






Yongxing Liu
Department of Chemistry
Wesleyan University
Middletown CT 06459

E-mail yliu@wesleyan.edu
Telephone: 860-685-2777(Office)
           860-343-7330(Home)
           860-685-7467(Home)
Fax:       860-685-2211
Http://linus.chem.wesleyan.edu/yliu/ 


From sichelj@UMoncton.ca  Wed Oct 15 14:30:51 1997
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Date: Wed, 15 Oct 1997 15:04:26 -0300 (ADT)
From: "J. Sichel" <sichelj@UMoncton.ca>
Subject: Re: CCL:EXTENDED HUECKEL AND ORTHOGONALIZATION
To: "E. Lewars" <elewars@alchemy.chem.utoronto.ca>
Cc: chemistry@www.ccl.net
In-Reply-To: <199710151423.KAA10197@alchemy.chem.utoronto.ca>
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Yes, Hoffmann's EH method uses explicit Lowdin orthogonalization; I 
remember working through a copy of his computer code as a graduate 
student in 1964!

As for his 1963 JCP paper, he does say (p.1399) that "the complete set of 
Eq.(2) [the secular equations] is solved with _two_ matrix diagonalizations."
If S = 1 were assumed, only one diagonalization would be required.

John Sichel
Dept de chimie et biochimie
Universite de Moncton, NB, Canada

On Wed, 15 Oct 1997, E. Lewars wrote:

> Regarding the extended Hueckel method as implemented by Roald Hoffmann:
> I know that the overlap integrals are calculated and used to construct
> the Fock matrix elements (which are proportional to these integrals in
> the EHM).   My question is:
> in Hoffmann's implementation are the overlap integrals used to calculate an
> orthogonalizing matrix to convert (e.g. by Loewdin orthogonalization) the
> matrix equation
>                     FC = SCe
> into standard eigenvalue form
>                     F'C' = C'e   i.e   F' = C'eC'^-1
> 
> as in ab initio calculations,
>         OR  is it simply pretended, as in simple Hueckel theory, that
>                     S=I  ?
> 
>    I read Hoffmann's 1963 paper in J Chem Phys, but this point does not
> seem to be explicity made clear.  Maybe I missed it.
> 
>         Thanks
>          E. Lewars


From bruno@antas.agraria.uniss.it  Wed Oct 15 14:35:53 1997
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Date: Wed, 15 Oct 1997 20:00:22 +0100 (NFT)
From: "Dr. Bruno Manunza" <bruno@antas.agraria.uniss.it>
To: Iraj Daizadeh <daizadeh@indigo.ucdavis.edu>
Cc: chemistry@www.ccl.net, daizadeh@indigo.ucdavis.edu,
        molecular-dynamics-news@mailbase.ac.uk
Subject: Re: Molecular Dynamics on Biological Molecules.
In-Reply-To: <9710150811.ZM20690@indigo.ucdavis.edu>
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On Wed, 15 Oct 1997, Iraj Daizadeh wrote:

> Hello.
> 
> Our group has just bought 2 DEC 500 au (low-end workstations) running DEC UNIX
> 4.0c and we are trying to find computational chemistry software packages that
> can calculate classical dynamics of motion for large (circa. 2000+atoms)
> biological molecules.  It would be nice if the programs could implement a
> Nose/Hoover thermostat and equipped with a variety of force fields such as
> amber, ESFF, cff91, etc...  Futhermore, the programs (which may be free or
> commercial) must be able to write out trajectories to some sort of archive file
> in ascii form for our own calculations.  I will summarize the results as is
> customary.
> 
> Thanks in advance for all contributions.
> 
> Iraj.

Dear Iraj, there are several programs doing the things you want. I just 
recall DLPOLY from Daresbury (free after signing a licence), and Amber 
(commercial). You'll find links to the above and several others looking 
throught our software page at http://antas.agraria.uniss.it
go there an then click the Computational Chemistry Software link.
You'll find some info also in the molmod page

Hope it helps
regards
Bruno


Dr Bruno Manunza
DISAABA (Dept. of Agricultural Environm. Sci)
University of Sassari
V.le Italia 39
07100 Sassari, ITALY
phone: 39 79 229215
fax:   39 79 229276
e-mail: bruno@antas.agraria.uniss.it
e-mail: bruno@tharros.dipchim.uniss.it
e-mail: gx6bot81@cray.cineca.it
web: http://antas.agraria.uniss.it



From schrecke@t12.lanl.gov  Wed Oct 15 16:31:01 1997
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Date: Wed, 15 Oct 1997 13:43:50 -0700
To: CHEMISTRY@www.ccl.net (CCL)
From: schrecke@t12.lanl.gov (Georg Schreckenbach)
Subject: summary: DFT MO energies


Dear CCL readers,

last week, I posted a question about DFT MO energies,
and how they are different in hybrid methods vs. GGA or LDA.
I got a few interesting replies -- thanx to those who took the
time to write! If anybody wants to comment further, please
do so, either to me, or to the CCL. I have posted this summary
also at my webpages, cf.
http://www.t12.lanl.gov/~schrecke/research.DIR/CCL_DFTMOEnergies.html

-----------------------------------------------
Original question:

Date: Fri, 10 Oct 1997 10:59:01 -0700
Subject:DFT MO energies

Dear CCL readers,

is anybody aware of papers that study DFT orbital energies?
More precisely, I would like to learn how those orbital energies
(Kohn-Sham eigenvalues) are different in hybrid methods like
B3LYP as compared to GGAs like BP86 or PW91, or also as
compared to the LDA. If there are systematic differences (which
I am sure is the case) then I would like to know how they can
be understood.
    There was recently some discussion on the
list about the possible physical meaning of the Kohn-Sham
eigenvalues. While this is an interesting subject in itself,
it is, this time, *not* my question.

-----------------------------------------------
Reply by Jon Rienstra <rienstra@xerxes.ccqc.uga.edu>

In general, the hybrid methods are to some degree sucessful in
incorporating some of the HF electron self-interaction cancellation, and
in many cases succeed in giving negative HOMO energies, even in anions.
GGA's on the other hand often give positive HOMO energies (esp in anions),
and much recent debate has focused on whether or not this is
problematic.
=46or more details see:
See Galbraith and Schaefer, J. Chem. Phys. 105, 1996 p. 862
and
Rosch and Trickey, J. Chem. Phys. 106, 1997 p. 8940

-----------------------------------------------
Reply by P. A. Politzer <PAPCM@jazz.ucc.uno.edu>

Dear Dr. Schreckenbach,
We have recently finished a comparison of Hartree-Fock and various DFT
Kohn-Sham orbital energies.  There are indeed some interesting patters.
The paper has been submitted to Theoretical Chemical Accounts.  I will
be glad to send you a preprint.     Best regards,   Peter Politzer

-----------------------------------------------
Reply by Ulrike Salzner <salzner@feryal.fen.bilkent.edu.tr>
(this one was also posted to the CCL)

Dear Georg,
I have testet DFT orbital energies for some small and medium sized
organic systems with pi-bonds (acetylene oligomers, thiophene monomer
through trimer, pyrrole and similar systems). There are significant
differences between LSDA and hybrid methods. The paper will soon appear
in the Journal of Computational Chemistry.

 To summarize: The IPs (negative HOMO energies) are closer to experiment
with hybrid functionals than at LSDA. The P86 correlation functional
seems to work better than the LYP correlation functional. All IPs with
DFT are smaller than experimental values (about 0.5 - 1 eV) and smaller than
at HF with the same basis set which are quite close to experiment. In my
limited data set it looks like there is little depenedence of the quality
of IP on the size of the system.

 The negative LUMO energies used as EAs are by far superior with all DFT
methods than with HF. LSDA works slightly better than hybrid
functionals. Again the P86 correlation functional works better than LYP.
I obtained the "experimental EAs" using experimental IPs and excitation
energies. So they have to be treated with some caution. It looks like the
agreement improves as the systems get larger. But the data are more than
insecure.

According to this, DFT corrects for the main deficiency of HF theory and
brings the LUMO down. I reasoned that this must have to do with the error
in the Coulomb terms in HF which seems to be absent in DFT. I was pleased
to see that Baerends et al. came to a similar conclusion in their feature
article in J. Phys. Chem.

 The main error in DFT seems to be due to the IP and not to the EA. Taking t=
he
difference between the two, I got very nice excitation energies. These
improve as the systems get larger. The agreement is pretty poor for
monomers but with trimers of purrole and thiophene the excitation
energies become good.

I also tried what happens when the weight of the HF exchange is
increased. I got the best HOMO-LUMO gaps with 30% HF exchange instead of
20%. Geometries were not changed by this. For ethylene I increased the HF
exchange stepwise up to 100%. There is no convergence. With 100% HF
exchange the gap is as bad as with HF but the orbital levels are shifted
compared to those at HF. So all this fudging is empirical and can - at
least for now - not be put on solid theoretical ground.

As for my personel interest in the band gaps of conducting polymers this
is good enough. Needless to say that I had major problems to publish
this. It took 1 1/2 years and one reviewer said it was not interesting
enough for rapid publication.  But the first paper is in press now as
mentioned above. There will be two more papers extending these findings
to band gaps of polymers by extrapolation. These are submitted to J.
Phys. Chem. and Synth. Met. Maybe in two years you can read them.

By the way. You're right I am German. I keep writing in English so more
people can read it.

 Cheers,

Dr. Ulrike Salzner

-----------------------------------------------
Reply by Heinz Schiffer <schiffer@h1tw0036.hoechst.com>

Hi George,
see table III in : Garnet K.-L. Chan, David J. Tozer, and
Nicholas C. Handy, Correlation potentials and functionals
in Hartree-Fock-Kohn-Sham theory, J. Chem. Phys. 107(5) (1997) 1536-1543
Ciao
Heinz
-----------------------------------------------
(End of summary)

Best regards, Georg

--
Dr. Georg Schreckenbach           Tel:     (USA)-505-667 7605
Theoretical Chemistry T-12        FAX:     (USA)-505-665 3909
M.S. B268, Los Alamos National      E-mail:  schrecke@t12.lanl.gov
Laboratory, Los Alamos, New Mexico, 87545, USA
Internet:    http://www.t12.lanl.gov/~schrecke/



From rvenable@deimos.cber.nih.gov  Wed Oct 15 18:34:15 1997
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Date: Wed, 15 Oct 1997 17:54:09 -0400 (EDT)
From: Rick Venable <rvenable@deimos.cber.nih.gov>
To: Iraj Daizadeh <daizadeh@indigo.ucdavis.edu>
Cc: chemistry@www.ccl.net, molecular-dynamics-news@mailbase.ac.uk
Subject: Re: CCL:Molecular Dynamics on Biological Molecules.
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On Wed, 15 Oct 1997, Iraj Daizadeh wrote:
> Our group has just bought 2 DEC 500 au (low-end workstations) running DEC UNIX
> 4.0c and we are trying to find computational chemistry software packages that
> can calculate classical dynamics of motion for large (circa. 2000+atoms)
> biological molecules.  It would be nice if the programs could implement a
> Nose/Hoover thermostat and equipped with a variety of force fields such as
> amber, ESFF, cff91, etc...  Futhermore, the programs (which may be free or
> commercial) must be able to write out trajectories to some sort of archive file
> in ascii form for our own calculations.  I will summarize the results as is
> customary.

I know that the DEC Alpha is one of the platforms supported by the
academic version of CHARMM; it does have Nose/Hoover, can easily handle
30,000 atoms or more, and individual coordinate frames from a trajectory
can be easily written in the CHARMM ASCII format, or in PDB format.  It's
not so great at supporting other force fields, for a variety of reasons
(some technical).  The academic version is available for a modest fee via
the Karplus group at Harvard;  for more info see

	http://yuri.harvard.edu

--
Rick Venable                  =====\     |=|    "Eschew Obfuscation"
FDA/CBER Biophysics Lab       |____/     |=|
Bethesda, MD  U.S.A.          |   \    / |=|  ( Not an official statement or
rvenable@deimos.cber.nih.gov  |    \  /  |=|    position of the FDA; for that,
http://nmr1.cber.nih.gov/           \/   |=|    see   http://www.fda.gov  )


