From borkent@caos.kun.nl  Wed Jul 10 03:59:30 1996
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From: Hens Borkent <borkent@caos.kun.nl>
Message-Id: <199607100731.JAA00532@cammsg1.caos.kun.nl>
Subject: M: negative freq's.
To: chemistry@www.ccl.net
Date: Wed, 10 Jul 1996 09:31:15 +0200 (MDT)
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Dear CCL-ers,

I mis-sent my reaction last week, but I think it is still
relevant, so I repeat it here:
In case you want to get rid of spurious negative frequencies
(which is often not necessary for the conclusions you draw
>from a calculation) it helps if you visualize the movement
involved (MOLDEN on unix machines, Re_view on PC's).
I have had examples where these frequencies corresponded
to small deviations from symmetry, and it helped to start
with a perfectly symmetrical structure. E.g. I observed
in an sp3-sp3 chain a motion corresponding to rotation
around the central bond, with a negative frequency, after
minimization. It disappeared after changing the dihedral
angles from 179.5 to 179.9999. (and a full minimization
of course, although you can do a step in between in which
you fix the symmetry).

Best regards,
-- 

  *****    J.H. (Hens) Borkent, CAOS/CAMM Center,
 *CAOS *   P.O. Box 9010, 6500 GL Nijmegen, The Netherlands
*   /   *  Tel 0031 24 36 52137  Fax 0031 24 36 52977
 * CAMM*   e-mail: borkent@caos.kun.nl
  *****    http://www.caos.kun.nl/staff/borkent.html

From borkent@caos.kun.nl  Wed Jul 10 04:13:07 1996
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From: Hens Borkent <borkent@caos.kun.nl>
Message-Id: <199607100731.JAA00532@cammsg1.caos.kun.nl>
Subject: M: negative freq's.
To: chemistry@www.ccl.net
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Dear CCL-ers,

I mis-sent my reaction last week, but I think it is still
relevant, so I repeat it here:
In case you want to get rid of spurious negative frequencies
(which is often not necessary for the conclusions you draw
>from a calculation) it helps if you visualize the movement
involved (MOLDEN on unix machines, Re_view on PC's).
I have had examples where these frequencies corresponded
to small deviations from symmetry, and it helped to start
with a perfectly symmetrical structure. E.g. I observed
in an sp3-sp3 chain a motion corresponding to rotation
around the central bond, with a negative frequency, after
minimization. It disappeared after changing the dihedral
angles from 179.5 to 179.9999. (and a full minimization
of course, although you can do a step in between in which
you fix the symmetry).

Best regards,
-- 

  *****    J.H. (Hens) Borkent, CAOS/CAMM Center,
 *CAOS *   P.O. Box 9010, 6500 GL Nijmegen, The Netherlands
*   /   *  Tel 0031 24 36 52137  Fax 0031 24 36 52977
 * CAMM*   e-mail: borkent@caos.kun.nl
  *****    http://www.caos.kun.nl/staff/borkent.html

From ncapron@ccr.jussieu.fr  Wed Jul 10 04:48:05 1996
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Date: Wed, 10 Jul 1996 09:20:03 +0200
From: ncapron@ccr.jussieu.fr (Nathalie CAPRON)
Message-Id: <199607100720.JAA130345@moka.ccr.jussieu.fr>
To: chemistry@www.ccl.net
Subject: About bulk modulus


 Dear all,
 Few weeks ago I sent this following message
 I give you now answers I got :
 Thanks to these persons !
 Good holidays ...........



> Dear all,
> I should need for my study a complete
> ( or near ) list of the calculations carried out on silicon
> which give the theoritical values for the elastic constants
> and especially bulk modulus
> I have already some papers but I am affraid to miss some
> important information.
> Could someone give me the references of these papers ?
> Thank you in advance
> Nathalie Capron


 Laboratoire de Chimie Physique
 Matiere et Rayonnement
 11, rue Pierre et Marie Curie
 75231 Paris Cedex 01
 ncapron@ccr.jussieu.fr

-----------------------------------------------------------------------------------
Hi Nathalie, see for instance:

	O.H. Nielsen and R.M. Martin, Phys.Rev. B 32, 3792(1985)
	D.J. Chadi and R.M.Martin, Sol.State.Comm. 19, 643(1976)

and references therein.
			Bye,
-- 
                        Leonardo De Maria                  
          SISSA                  |      Universita di Trieste 
    Scuola Internazionale        |   Dipartimento di Fisica Teorica 
  Superiore di Studi Avanzati    |       Strada Costiera 11
   via Beirut 2-4, Grignano      |       Miramare-Grignano
      I-34014 - Trieste          |       I-34014 - Trieste
   tel:    +39 40 3787506        |   tel:     +39 40 224265
   fax:           3787528        |   fax:            224601  
e-mail:demaria@neumann.sissa.it  | e-mail : demaria@vstst0.ts.infn.it

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


    Hello Nathalie;

    Here are some references about Si calculations.  I think they
contain info about the bulk modulus and also other elastic constants:

E. R. Cowley, Phys. Rev. Lett. 60 (1988) 2379
B. W. Dodson, Phys. Rev. B 35 (1987) 2795

M. T. Yin and M. L. Cohen, Phys. Rev. B 24 (1981) 2303
M. T. Yin and M. L. Cohen, Phys. Rev. B 26 (1982) 5668
M. T. Yin and M. L. Cohen, Phys. Rev. B 29 (1984) 6996


    Regards,
               Rene Fournier     fournier@physics.unlv.edu

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



Tres chere Nathalie,

J'ai entre les mains un excellent article concernqnt l'oxyde de Ti. C'est
quelque peu different de ton systeme d'etude, mais toute la procedure de calcul
de bulk modulus et autre snt reportes dans cet article. Cela peut t'aider.

"Structural and electronic properties of titanium dioxide", K. M. Glassford et
J. R. Chelikowsky, Physical Review B, vol 46, N 3, p.1284-1298, 1992.

Frederic Bouyer

-- 
__________________________________________________________________________

Frederic Bouyer
Groupe Chimie Corrosion - RNE-EMA
EDF-DER Les Renardieres              Tel:   (33) 1-60-73-69-65
Route de Sens, Ecuelles, BP1         Fax:   (33) 1-60-73-68-89    
77250 MORET-SUR-LOING - FRANCE       Email: Frederic.Bouyer@der.edfgdf.fr
__________________________________________________________________________

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

From wieland@btm2d1.mat.uni-bayreuth.de  Wed Jul 10 06:13:06 1996
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Mime-Version: 1.0
Date: Wed, 10 Jul 96 10:04:43 +0200
To: MOL-DIVERSITY@LISTSERV.ARIZONA.EDU, chemistry@www.ccl.net
Subject: Summary: Toplogical indices and active sites
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Dear netters,

last week I posted a question about the connections between topological indices,
similarity, screening and drug design. There were 9 summarizable replies most of 
which were rather lengthy. In order to avoid filling your mail boxes with too much
trash, this is just an announcement about the availability of the summary.
You can get it from:

   http://www.mathe2.uni-bayreuth.de/thomas/summary.html

or I send it to you as e-mail on your request.
My deep thanks go to all who responded. I think we should keep the track on this
issue.

Best regards,

Thomas Wieland



From guillem@gauss.uib.es  Wed Jul 10 06:17:41 1996
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Date: Wed, 10 Jul 1996 11:31:23 +0100
From: "Guillem A. Sunyer" <guillem@gauss.uib.es>
Organization: Departament de Quimica, Universitat de les Illes Balears
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Subject: unit cell generation
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Dear Netters,

I post the following query on behalf of my colleague Dr. Pablo
Ballester:

Dear CCL members,

        I will like to know if someone is aware of a program able to
generate a
unit cell from X-ray data (internal coordinates, a b c values, angles ,
number of molecules per unit cell etc.) that is,  drawing a box
representing
the cell and also the molecules inside it. I will summarize to the net
if
there is interest.

Please e-mail me directly.

Pablo Ballester

+++++++++++++++++++++++++++++++++++++++++
+  Pablo Ballester, Associate Professor +
+  Universitat de les Illes Balears     +
+  Departamento de Quimica              +
+  07071-Palma de Mallorca, SPAIN       +
+  phone: 34 71 173265                  +
+  fax:   34 71 173426                  +
+  E-mail: dqupbb0@ps.uib.es            +
+++++++++++++++++++++++++++++++++++++++++

-- 
Dr Guillermo A. Suner; Dep. de Quimica, UNIVERSITAT DE LES ILLES BALEARS
E-07071-Palma de Mallorca, SPAIN.
E-mail: guillem@gauss.uib.es    Tel: + 34 71 173498  Fax: + 34 71 173426 
WWW URL: http://www.uib.es/depart/dqu/dquo/suner.html

From tmmec@fcindy5.NCIFCRF.GOV  Wed Jul 10 06:19:48 1996
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Date: Wed, 10 Jul 1996 06:10:42 -0700
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                          TMMeC CALL FOR PAPERS


 A final agreement  has been  reached between TMMeC and Elsevier Publishers for
 the  joint  publication of articles  in TMMeC  and THEOCHEM. The  text  of the 
 agreement can be found in the WWW pages of TMMeC and THEOCHEM. We believe that
 this mechanism of  publication  will greatly  reduce the  lag between referees
 acceptance and the public access of a paper.

 An open  discussion  will  follow  the publication  of a paper, thus  bringing
 together the  advantages of  a traditional  journal and those of an electronic
 conference. Please read the Publication Policy  in TMMeC  for more  details on
 this mechanism of publication.

 TMMeC  is  a  non-commercial  Web  publication  developed  by  the  Montevideo
 Theoretical  Chemistry  Lab, Universidad de la Republica, Montevideo, Uruguay.

 TMMeC  is  a  distributed  resource. Please  choose the mirror nearest to your
 place to access TMMeC pages.


 TMMeC Mirrors: http://bilbo.edu.uy/agora/Mirrors.html
                http://uqbar.ncifcrf.gov/agora/Mirrors.html

 THEOCHEM:      http://www.elsevier.nl/section/chemical/theochem/


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



From wallenborn@phys.chem.ethz.ch  Wed Jul 10 06:21:58 1996
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Hi there,

I have a problem with the slapaf input (molcas 3.0). 
It's the following:

I'm trying to do a casscf geometry optimization in
molcas (i don't feel like doing it in g94 with a different
basis set and transferring the resulting geometry to molcas,
although this would be my last resort). My dummy problem is
formaldehyde, the route seward-scf-alaska-slapaf (as in the
scfgrad script. I left out the rasscf because the problem
is not connected with it).

Input files are:

-----seward.input-----
 &SEWARD &END
Title 
 formaldehyde
Square
Symmetry
x y
Basis set
C.ANO-S...3s2p1d.
 C                 .0000000000         .0000000000       -1.0143690059
End of basis
Basis set
O.ANO-S...3s2p1d.
 O                 .00000000         .0000000000        1.2925328919
End of basis
Basis set
H.ANO-S...2s1p.
 H                .0000000000        1.7657335076       -2.1270245501
End of basis
End of input
-----scf.input-----
 &SCF &END
Title
 formaldehyde
Occupied
 5 1 2 0
Ivo
End of input
-----alaska.input-----
 &ALASKA &END
End of Input
-----slapaf.input-----
 &SLAPAF &END
Internal coordinates
r1 = Bond C O
r2 = Bond C H
r3 = Bond C H(y)
a1 = Angle O C H
a2 = Angle O C H(y)
d1 = Dihedral H O C H(y)
Vary
r1 
r2 
r3 
a1 
a2 
d1 
End of internal
Iterations
20
Print
1
111 99
End of Input
-----end-----

the Iterations and Print statements are taken from the worked
example in the Molcas documentation (which works, actually).
They shouldn't be a problem.

Everything works fine until slapaf. It exits with the output
-----slapaf.output-----
[snip]

 ********************************************
 * Values of primitive internal coordinates *
 ********************************************
 
 R1       : Bond Length=    2.3069/ bohr
 R2       : Bond Length=    2.0871/ bohr
 R3       : Bond Length=    2.0871/ bohr
 A1       : Angle=  122.2166/degree,     2.1331/rad
 A2       : Angle=  122.2166/degree,     2.1331/rad
  Warning: dihedral angle close to end of range
 D1       : Dihedral Angle=  180.0000/degree,    3.1416/rad
 
 
 *********************************************
 * Value of internal coordinates / au or rad *
 *********************************************
 
 R1            2.3069
 R2            2.0871
 R3            2.0871
 A1            2.1331
 A2            2.1331
 D1            3.1416
 
 ESV2105S  DGEICD   FACTORIZATION FAILED DUE TO NEAR ZERO PIVOT NUMBER
(4).                                                        
 EXECUTION TERMINATING DUE TO ERROR COUNT FOR ERROR NUMBER  2105
 MESSAGE SUMMARY: MESSAGE NUMBER - COUNT
                      2103          1
                      2105          1
-----end of slapaf.output-----


I have no idea what causes this behaviour. I thought that
the near 180 deg dihedral was responsible, and substituted
a third angle for it. Also i tried to avoid using symmetry in 
the input, as in the manual's worked example (enediyne), where
no two internal coordinates are connected to each other by
a symmetry operation. The result was the same. NEAR ZERO PIVOT NUMBER.

The molcas homepage (garm.teokem.lu.se) has not been reachable 
since yesterday, so i can't get information from there.


Er, help?






-- 
-ernst wallenborn.

i'm not a bug.
i'm an undocumented feature.

From tp@elptrs7.rug.ac.be  Wed Jul 10 06:24:11 1996
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Date: Wed, 10 Jul 1996 12:07:01 +0200 (DFT)
From: "Park, Tae-Yun" <tp@elptrs7.rug.ac.be>
To: Computational Chemistry List <chemistry@www.ccl.net>
Subject: Searching transition state with MOPAC; part2
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Dear all,

I've received a lot of helpful messages from many CCLers, 
concerning my earlier questions on how to get the structure 
of transition state of the reaction,


 
   H              H     H                       H H H
   |               \   /                        | | |
 H-C(+)       +     C=C     ---->(TS?)---->   H-C-C-C(+)
   |               /   \                        | | |
   H              H     H                       H H H

 gas-phase                                     gas-phase
   methyl         ethylene                   primary propyl
carbenium ion                                 carbenium ion



Thanks a lot! I greatly appreciate all the messages concerning 
this problem. 

Most of the messages pointed out that I made a mistake to prepare
the input file for SADDLE calculation; all the atom should be in
the same order between reactants and product z-matrix field.

I made second try with a corrected input file as follows;


************************************************************** 

SADDLE DENSITY GRAPH XYZ CHARGE=1 PRECISE
Me--->p methylation activated complex

C    0.000000  0    0.000000  0    0.000000  0    0   0   0
C    8.471619  1    0.000000  0    0.000000  0    1   0   0
C    1.325912  1  162.328125  1    0.000000  0    2   1   0
H    1.108597  1   65.592545  1 -150.347214  1    1   2   3
H    1.113968  1  120.001495  1 -151.401566  1    1   4   2
H    1.108612  1  119.996246  1 -179.367538  1    1   4   5
H    1.098282  1  122.722214  1   57.159393  1    2   3   1
H    1.098328  1  122.715210  1  179.999634  1    2   3   7
H    1.098267  1  122.715210  1   -0.316483  1    3   2   7
H    1.098206  1  122.715210  1 -179.684021  1    3   2   7
0    0.000000  0    0.000000  0    0.000000  0    0   0   0
C     .000000  0     .000000  0     .000000  0    0   0   0
C    1.506600  1     .000000  0     .000000  0    1   0   0
C    1.418947  1  116.688263  1     .000000  0    2   1   0
H    1.118077  1  111.116249  1  -59.952415  1    1   2   3
H    1.119762  1  109.783371  1 -179.449097  1    1   2   3
H    1.118210  1  111.069687  1   61.123405  1    1   2   3
H    1.150598  1  110.672989  1  174.990601  1    2   1   4
H    1.150955  1  110.650314  1   64.874481  1    2   1   4
H    1.109621  1  121.247902  1 -179.729874  1    3   2   1
H    1.110257  1  121.556961  1     .300391  1    3   2   1
0     .000000  0     .000000  0     .000000  0    0   0   0

**************************************************************

This time MOPAC produced a structure of transition state which 
is almost the same as that of reactants, that is, there was 
almost no change between reactants and transition state.

I've tried to refine the transition state with the key words,
"TS", "SIGMA", and "NLLSQ" separately, which gives no change
either.

Why is the result like this?  Could anyone PLEASE tell me how 
can I go further to obtain a reliable structure of the 
transition state??

Thank you VERY MUCH in advance.



				Sincerely,

				     Park, TAE-YUN    
=-=-=-=-=-=-=-=-=-=-=-=-=-=-=-=-=-=-=-=-=-=-=-=-=-=-=-=-=
State University of Ghent
Laboratorium voor Petrochemische Techniek
Krijgslaan 281, Blok S5  
9000 Gent, Belgium	  
TEL:+(32)-0(9)-264-4527
FAX:+(32)-0(9)-264-4999
e-mail: tp@elptrs7.rug.ac.be
=-=-=-=-=-=-=-=-=-=-=-=-=-=-=-=-=-=-=-=-=-=-=-=-=-=-=-=-=



From MEDVEN@olimp.irb.hr  Wed Jul 10 09:13:10 1996
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Date: Wed, 10 Jul 1996 14:40:41 +0200 (IST)
From: ZELJKA MEDVEN <MEDVEN@olimp.irb.hr>
Subject: QM calculations on hydrogen bonds
To: chemistry@www.ccl.net
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Dear netters,
Is any of you aware of semiempirical or ab initio calculations
on hydrogen bonds involving nucleic acid bases or any other 
nitrogen containing aromatics?
I would appreciate any reference.

                       Sincerely,
                                     Zeljka
           
******************************************************************************
M.Sc. Zeljka Medven                           Area code: 385-1
Department of Chemistry                       Phone:     456-1089
Rugjer Boskovic Institute                     Fax:       272-648
POB 1016, HR-10001 Zagreb, Croatia            e-mail:    medven@olimp.irb.hr
******************************************************************************



From Frederic.Bouyer@der.edfgdf.fr  Wed Jul 10 12:13:10 1996
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From: "Frederic Bouyer" <Frederic.Bouyer@der.edfgdf.fr>
Message-Id: <9607101726.ZM1688@ret45ab.der.edf.fr>
Date: Wed, 10 Jul 1996 17:26:43 -0600
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To: chemistry@www.ccl.net
Subject: Semi-empirical codes for solids ?
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Dear Netters,

I search a software (a semi-empirical one) that can treat solid phase and
compute frequencies.
I saw that MOSOL can deal with solids (special thanks to Ratty), but there is
only H, Be, B, C, N, O, F, Al, Si, P, S,  Cl, Ge, Br, Sn, and I. But I would
like to have Li, Fe, Sn, Cr, O, Zr elements. Is it possible to have MOSOL with
these elements included, or are there other packages that offer such
capabilities ?

Frederic Bouyer

From KANTERS@urvax.urich.edu  Wed Jul 10 12:18:18 1996
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 10 Jul 1996 12:05:29 -0400 (EDT)
Date: Wed, 10 Jul 1996 12:05:29 -0400 (EDT)
From: "Rene P.F. Kanters" <kanters@urvax.urich.edu>
Subject: XMol on SGI IRIS 6.2
To: CHEMISTRY@www.ccl.net
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Dear CCL'er:

We just upgraded our SGI's from IRIS 5.3 to 6.2 and XMol can not run 
anymore (since it relies on COFF files that are not supported anymore).

Does anybody know about a free-ware SGI IRIS 6.2 compatible application 
that can animate multistep XYZ files?

Rene Kanters
Chemistry Project Specialist
Chemistry Department
University of Richmond, VA 23173

phone (804) 287-6873
email kanters@urvax.urich.edu
www   http://www.science.urich.edu/~kanters



From janr@tiger.chem.uw.edu.pl  Wed Jul 10 13:13:16 1996
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Date: Wed, 10 Jul 1996 18:53:46 +0200
From: janr@tiger.chem.uw.edu.pl (Jan Radomski)
Message-Id: <9607101653.AA11448@tiger.chem.uw.edu.pl>
To: CHEMISTRY@www.ccl.net
Subject: Q: 3D --> IsisDraw 2D mol_file conversion?
Cc: janr@tiger.chem.uw.edu.pl



Dear Netters,

is there any utility allowing conversion from 3D structural
data of molecule to the MDL's IsisDraw 2D molfile format?
Or am I missing something obvious?

Best regards,
Jan Radomski

From vangreve@univ-orleans.fr  Wed Jul 10 13:20:54 1996
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Message-ID: <31E3E2D4.397D@univ-orleans.fr>
Date: Wed, 10 Jul 1996 19:05:24 +0200
From: Eric VANGREVELINGHE <vangreve@univ-orleans.fr>
Organization: ICOA
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Subject: Software to calculate ionic mobility
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Dear Netters,

	I am looking for a program which can compute the
mobility of ionic compound.

	I don't know if it's exist but any help will be
appreciated.

			Thanks in advance


_____________________________________________________________

Eric VANGREVELINGHE   --------  Graduate Student in Chemistry
	                                     ___    _  
e-mail: vangreve@univ-orleans.fr             `T\_ww/|@,_ _  
http://web.univ-orleans.fr/ICOA       ~  ~~~  =(_)\___[/(_)`>

I.C.O.A.	Institut de Chimie Organique et Analytique
URA 499-UFR Sciences  BP 6759  45067 ORLEANS Cedex 2   FRANCE
tel: (33) 38 49 45 77 			fax: (33) 38 41 72 81
_____________________________________________________________

From chpajt@bath.ac.uk  Wed Jul 10 15:13:12 1996
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Date: Wed, 10 Jul 1996 19:14:20 +0100 (BST)
From: A J Turner <chpajt@bath.ac.uk>
To: A J Turner <chpajt@bath.ac.uk>
cc: CHEMISTRY@www.ccl.net
Subject: Re M imaginary frequencies
In-Reply-To: <31E3E2D4.397D@univ-orleans.fr>
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Hi!

There are a few points that are maybe worth thinking about. 

1: Mopac is not stable under restarts - in my experiance.  Ie if you have
and EF job that ran half way and was restarted , then  compare to a
complete run - the answers will not be the same. This sometime erroniously
results in to jobs giveing different answers - and you think - err why did
that happen!

2: The hessian update does seem to fail sometime on EF.  I often use
hess=3 recalc=3 or recalc=1.  Most people say this is excessive - but I
find it kills off these imaginary frequencies.

3:  I once accedantally started EF on a transition state - absolutelyy
100% on the torsion barrier - eay for a z-matrix.  I said that this was a
minimum!  IE - it cn fail in this way.

4: My version of mopac 6.0 has ddmin  - something odd here.

Anyhow - hess=3 recalc=3 or recalc=1 has never ever failed me yet.

Good luck

Alex



 -------------------------------------------------------------------
|Alexander J Turner         |A.J.Turner@bath.ac.uk                  |
|Post Graduate              |http://www.bath.ac.uk/~chpajt/home.html|
|School of Chemistry        |+144 1225 8262826 ext 5137             |
|University of Bath         |                                       |
|Bath, Avon, U.K.           |Field: QM/MM modeling                  |
 ------------------------------------------------------------------- 



From Steve.Bowlus@sandoz.com  Wed Jul 10 16:13:12 1996
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To: <CHEMISTRY@www.ccl.net>
Subject: Mopac: Summary: Structure of excited states
Date: Wed, 10 Jul 1996 21:07:24 +0200


My thanks to those who replied to my query on optimizing structures of excited
states in Mopac.  This appears to be less straightforward than I expected. .
 .ah, well, fools rush in. . .

Below are the replies I received, subjected to some (unmarked) snipping:

>>Andreas Parusel, Vienna (andreas@majestix.msp.univie.ac.at):

I read your posting in the ccl about excited states. I am working also with
these problems in the VAMP package, but I do have the same problems.

As fas as I know, you have to change the structure of the MOLECULE a bit ( for
my large molecules for ex. -Ph --> -CH3) then it works better.
Sometimes it works if you coose another converger ... PULAY or IIS ... you
could try this.
Or you have to optimize the excited state with GNORM=20 f. ex. and lowering the
gradient step by step ...  this are all possibilities that work sometimes but
not always!

>>Dr. Jose Ignacio Garcia-Laureiro (jig@qorg.unizar.es):

In general, geometric optimizations at the CI level are MUCH more time
demanding than "normal" ones, but I realize that 10 cpu hours on an
Indigo2 is too much... You may take a look to the following reference:

M.J.S. Dewar, S. Olivella, J.J.P. Stewart
J. Am. Chem. Soc., 108 (1986) 5771-5779

These authors recommend to start with an UHF geometry optimization, which
is as fast as an normal RHF one, but leads to a better starting point for
a further CI optimization.

>>Dr. Peter Gedeck (gedeck@organik.uni-erlangen.de):

As far as I think SHIFT only damp SCF oscillations and does not change
the behaviour of the EF geometry optimization. You should try setting DMAX
to a smaller value. This restricts the maximum step size of the geometry
optimization and might thus damp the oscillations. Also try different
geometry optimizers.

Another problem that can occur is a crossing of excited states during the
course of the geometry optimization. If such a crossing occurs the
calculated gradients suddenly belong to a different state than in the
steps before and you can imagine that this way your calculation must
fail. A possible way to reduce the problem here is to define the
multiplicity of the state you want to optimize. E.g use:
   root=1 singlet    for the S0 state
   root=2 singlet    for the S1 state
   root=1 triplet    for the T1 state
This way at least we get rid of the problem of crossing singlet and
triplet states.

It might be that some of the keywords are not correct because I usually
use VAMP and not Mopac but there are definitly similar keywords.

>>Lutfur Khundkar (LKHUNKR@NEU.EDU):

     I have tried a few excited state calculations using MOPAC 6 using OS/2 on a
486D50. My molecules were relatively small, but what I would consider medium to
large for semiempirical calculations, specially geometry optimizations. I have
worked with about 16 heavy and 12  H atoms. There are some special keywords
(SINGLET and TRIPLET) that you can use to restrict yuour basis set. However,
geomtry optimizations do take a long time.From what I understand from talking to
a few people, C.I.=2 is not really a useful choice --- unless you are interested
in very approximate numbers. My own experience with a limited set of molecules
has been that even the energies that you get seem to depend on the level of CI.
I find that CI=4 (single geometry SCF calculations) and less gives results that
are reasonably similar, but CI=5 makes a significant difference to the energies
and relative ordering of states (I use dipole moments to "identify" my states
--- its an approximate handle for me, since thats what I am interested in). I
remember seeing a post to this list several months back about MECI in Mopac that
discussed an alternative to using the preset CI keyword. You can define your
microstates to be used in MECI by Mopac, although this does not address your
initial concern about how long it takes to get a converged calcualtion.


From boyd@chem.iupui.edu  Wed Jul 10 18:13:13 1996
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 10 Jul 1996 16:33:36 -0500
Date: Wed, 10 Jul 1996 16:22:55 -0500
From: Boyd <boyd@chem.iupui.edu>
Subject: Gordon Conference on Computational Chemistry
To: OSC CCL <chemistry@www.ccl.net>
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CCLers:
Last week, the 6th biennial Gordon Research Conference on 
Computational Chemistry was held in New Hampton, New 
Hampshire.  At the conference, which was chaired this year by 
Dr. Tom Halgren (Merck), elections were held for the future 
guidance of the conference.  By policy, the chair of this 
conference alternate between someone from academia and 
someone from industry.  Last week the conferees elected Dr. 
Terry Stouch to be Vice Chair.  So when the conference next 
meets in the summer of 1998, Dr. Jeffry Madura will be Chair.  In 
the year 2000, Terry will be Chair.

For information about these future conferences, contact:

Jeffry D. Madura, Ph.D.
Department of Chemistry
University of South Alabama
Mobile, AL 36688 USA
Phone: 334-460-7430  -  FAX: 334-460-7359
E-mail: jmadura@jaguar1.usouthal.edu

Terry R. Stouch, Ph.D.
Room H3812, Department of Macromolecular Modeling 
Bristol-Myers Squibb Pharmaceutical Research Institute
P.O. Box 4000, Princeton, NJ 08543-4000 USA
Phone: 609-252-5442  -  FAX: 609-252-6030
E-mail: stouch@bms.com


On behalf of everyone at the conference, we thank Tom Halgren 
for his superb organization of a most stimulating meeting, truly 
at the cutting edge of science.

Donald B. Boyd, Ph.D.
Member of the Steering Committee of Past Chairs
Indiana University-Purdue University at Indianapolis
E-mail: boyd@chem.iupui.edu

