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From: "Shobe, Dave" <dshobe@sud-chemieinc.com>
Subject: RE: Can change of 0.02-0.05 Angstrams in bond to change radically
	system
To: "'art''" <Arturas.Ziemys@vaidila.vdu.lt>, "'CCL'" <chemistry@ccl.net>
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In transition metal complexes the answer is "yes, sort of."  :-)   A small
change in bond length can lead to a change in the ground electronic state.
It's also very easy in ab initio calculations of transition metal complexes
for the wavefunction not to end up in the ground state.  There is an analogy
between calculation of the wavefunction and optimization of the geometry
(both involve varying parameters to minimize an energy), and it's possible
to end up at a "stationary point" which is a local but not the global
minimum.  It's also possible to end up with a wave function which is
analogous to a transition state or higher-order saddle point.  Gaussian has
a keyword "stable" to check for this.

--David Shobe
SØd-Chemie Inc.
phone (502) 634-7409
fax     (502) 634-7724
email  dshobe@sud-chemieinc.com

Any opinions herein are not necessarily representative of SØd-Chemie.

-----Original Message-----
From: art' [mailto:Arturas.Ziemys@vaidila.vdu.lt]
Sent: Monday, August 28, 2000 7:39 AM
Cc: Computational Chemistry List
Subject: CCL:Can change of 0.02-0.05 Angstrams in bond to change
radically system


Hi, CCLers,

Can change of 0.02-0.05 Angstrams in bond length to change radically MO
system ?

I've got a serial of calculations whith growing one bond length in heme
system. For
some of calculated points the structure of HOMO were very diffrent from the
point
of view of contribution coefficients  of atoms.

Is it possible? Any opinion is wellcome.

By the way, interesting fatc that in the bond growth length by 0.3
Angstrams, there
alternating Single Point calculations, where convergence speed changes by
3-5 times
>...( for example .. - 25 -155 -40 -122 -50 -90 - ...). As I mentioned, the
step is
around 0.02 Angstrams. Is it not strange ??????

A.Ziemys


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From chemistry-request@server.ccl.net  Mon Aug 28 18:38:34 2000
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From: "Thoms, Travis" <TThoms@cra.canon.com>
To: "Computational Chemistry List (E-mail)" <CHEMISTRY@ccl.net>
Subject: Summary of HOMO-LUMO calculation suggestions Was: A Novice and HO
	MO-LUMO bandgap calculations
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Greetings and thank you for all of your responses,

Here are the general conclusions that I have drawn from your posts; I will
have the actual posts follow.

1.  For realistic UV-Vis absorption calculations, ZINDO/s is the way to go.
(Hyperchem does have ZINDO)
2.  Most semi-empirical methods greatly overestimate the energy level of the
LUMO.
3.  Calculating the HOMO-LUMO bandgap is difficult, since the assumption by
the model is that the molecule is neutral and at its ground state.  Once an
electron was removed from the HOMO or added to the LUMO coulombic
interactions would change the energy level, and this interaction is not
taken into effect.
4.For a more accurate feeling of band gap interactions, ab-initio methods
(namely DFT, with which I am not familiar) are probably most helpful.  (Can
anyone recommend a DFT program?)
5.  Initial geometry optimization is important

Thanks again,

T.Thoms

Message 1:

pm3 and even hartree-fock methods are poor for describing virtual
(unoccupied) states. try a method with electron correlation (mpx or ci).

Message 2:
Equating a molecular orbital energy difference to an electronic excitation
energy is wrong, primarily for two reasons:

1)
The energy required to promote an electron from orbital i to orbital j (say,

>from the HOMO to the LUMO) is not at all equal to the orbital energy
difference 
e(j) - e(i). The promotion energy E(i-->j) can be expressed as  

  E(i-->j) = e(j) - e(i) - v(i,j)

where the term -v(i,j) represents the interaction between a hole in orbital
i
and an electron in orbital j.  This term may be relatively small if the two
molecular orbitals are spatially separated, but in general, v(i,j) amounts
to
several electron volts and is by no means negligible.

2)
The wavefunction |i-->j> of an excited electronic configuration is not 
in general a good approximation to an eigenfunction of the many-electronic
Hamilton operator H.  Generally, matrix elements corresponding to
<i-->j|H|k-->l> are not close to zero.  Hence, excited configurations tend
to
interact, and a proper description must include Configuration Interaction,
(CI).
 Of particular importance is the first order CI between near-degenerate
configurations of the same symmetry, f.inst. for alternant hydrocarbons
(like 
styrene) where it gives rise to "plus" and "minus" states. - Inclusion of 
multiply excited configurations (like i,k-->j,l etc.) in the CI formally 
accounts for electronic correlation effects, thus leading to a description 
going beyond the orbital picture.  However, semiempirical CI-procedures
(PPP, 
CNDO/S, INDO/S, ZINDO, etc.) usually limit the CI expansion to singly
excited 
configurations, and account for correlation effects by empirical adjustment
of 
parameters in the models.

In summary, if you want to predict electronic excitation energies for 
conjugated organic molecules with HyperChem, try ZINDO/S with CI.
Application 
of ZINDO/S should be explained in the HyperChem user's manual. - Good Luck! 

Message 3:
Try ZINDO, and especially the spectroscopic stuff.
These are generally very good.

Message 4:
HOMO-LUMO gap energies overestimate the actual excited state energies 
(and frequently by quite something).  At best the gap is useful for 
some trends, but don't expect any miracles from it.  The simplest way 
to imagine this is that both the HOMO and the LUMO change in going 
>from 2 resp. 0 electrons in it, to a situation with 1 electron in 
each, and that the interaction between the different orbitals also 
changes upon this change in occupancy (so e.g. the electron may not 
'fully' end up in the LUMO, but also 'to some degree' in higher 
orbitals).  In short: the HOMO-LUMO excitation picture is somewhat 
too simple, and this is independent of the programs used.
A recent readable review is one by B.O. Roos in Acc. Chem. Res. 
(either this or last year).

Somewhat better to significantly better (depending on the case) 
results can be obtained by either parametrized semiempirical methods 
(ZINDO is one of them, INDO/s another; isn't either of them in 
Hyperchem?), or by heavy-duty ab initio calculations (such as TD-DFT 
or CASSCF).  Depending on your aims, you will have to choose between 
them.

Message 5:

Try with MOPAC AM1 just to compare MOPAC AM1 and PM3.
I have compared these two methods on one molecular system.
In this case band-gaps very comparable with eachother, but heats of
formation
were different.

I am sure someone will tell you that QM (quantum mechanics) and/or DFT are
better methods
to use, but of course these methods are much more timeconsuming.

See if you find this web-site interesting:
9.7 Comparison of Calc'd and Observed for MNDO, AM1, and PM3 - Next: Notes
on the Table Up: 9. Accuracy of Methods Previous: 9.6 Faults and Errors 9.7
Comparison of Calc'd and Observed for MNDO, AM1, and PM3 :
http://www.psgvb.com/Mopac/html/node657.html

Have a nice day,

Message 6:

I suspect that you are running standard INDO/1S of Zerner, et.al.  Errors of
30-100
NM in Lmax are common......

Quality geometries often help correlations of Lmax(computed) against
experiment,
but the correlation does _not_ have slope of 1 and intercept of 0.
Intercept is
ofted ~ 70-100 NM, depending on the size of the molecule..

Message 7:

PM3 cannot reproduce the real band gap because PM3 can not handle exact
value of LUMO energy. Also PM3 was not parameterized to estimate the UV
spectra. You may use DFT program for evaluating HOMO/LUMO gap, and ZIDO/S
is known to be very powerful to calculate UV absorption spectra. 


Message 8:

Your problem is a common one. I encourage you to search the CCL archives for
this year and the last you to find extensive and more sophisticated
discussions of this problem. 
As you observed, HOMO-LUMO bandgaps are never a good measure of actual
excitation energies. There are many reasons why, but here is one way to look
at it. 
The HOMO energy is a measure of how hard it is to remove an electron from
the neutral molecule, and the LUMO energy (taken with a large grain of salt)
is a measure of how hard it is to add an electron to the neutral molecule. 
Excitation, by contrast, can be thought of as removal of an electron from
the neutral molecule (giving a radical cation), followed by return of the
electron to an unoccupied orbital of the RADICAL CATION. It is much easier
to add an electron to a radical cation than it is to add an electron to a
neutral molecule, so excitation energies are much smaller than HOMO-LUMO
bandgaps. 
Message 9:
A simple HOMO-LUMO picture for UV Vis spectra (especially for conjugated
species
is fundamentally incorrent).  Something liek PM3 can only be successfully
used for
ground state geometries and there to0 (PM3 being a semi-empirical method),
you
could encounter problems.

When you say band-gap I presume you are refering to excitattion energies.
What
kind of systems ar eyou using (# of heavy atoms etc)?


Fore spectra you need to use what are known as CI (configuration
interaction)
methods and for a molecule like styrene you need at least double CI.

Hyperchem should include ZINDO.  Have you tried that?

Message 10:
As far as I know, semi-empirical methods like PM3 overestimate the energy of
LUMO orbitals. There are techniques to reduce this effect but I think, since
you are dealing with small molecules, that the most effective way to get
better
results is to use some ab initio method. HyperChem 6 allows you to do that
at
some extent.




From chemistry-request@server.ccl.net  Tue Aug 29 07:27:52 2000
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Date: Tue, 29 Aug 2000 13:27:38 +0200 (MDT)
From: Harald Svedung <svedung@phc.chalmers.se>
To: chemistry@server.ccl.net
Subject: F2 Ne potential
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Hi all of you,

I'm about to take a look at rovibrational energy transfer in F2-Ne 
collisions. Does anyone have a subroutine implementing the potential in:

K. W. Chan, T. D. Power, J. Jai-nhiknan and S. M. Cybulski, J. Chem. 
Phys. 110 860-869 (1999)

preferably giving the intermolecular potential energy as a function of 
the interatomic distances.

Many thanks in advance!

:-)
/Harald


Harald Svedung (Ph.Lic.)                phone:          +46-31-7722816
Department of Chemistry                 fax:            +46-31-167194
Physical Chemistry                      home phone:     +46-31-240897, +46-709223206	
Goeteborg University                    home e-mail:    harald.svedung@svedung.pp.se
SE-412 96 Goeteborg, Sweden             www.che.chalmers.se/~svedung/	


From chemistry-request@server.ccl.net  Tue Aug 29 09:55:23 2000
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Hi all, 

Does anyone know where I can get a copy of the fortran source of the

program written by Bartels used in the parameterization procedure of
semiempirical methods ?



Thank you in advance,



--

Gerd Bruno

www.dqf.ufpe.br

From chemistry-request@server.ccl.net  Tue Aug 29 09:07:22 2000
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Date: Tue, 29 Aug 2000 21:04:27 +0800
From: Yubo Fan <yubofan@guomai.sh.cn>
Subject: ECP for Lanthanides?
To: CHEMISTRY@ccl.net
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Hi,

I am going to deal with some reaction concerning Lanthanides. And I
found a reference (M. Kaupp, P.v.R. Schleyer, M. Dolg, H. Stoll, J. Am.
Chem. Soc. 1992, 114, 8202), in which some particular ECP basis sets
were used. These ECPs treat [Kr]_4d10_4fx as fixed core. Could you
please tell me where can I get these basis sets. If I muse edit the G98
files for these basis sets based on references, how should I do.

I will summarize.

Thanks in advance

Y. Fan

--
=============================================================
Yubo Fan                         Email: yubofan@guomai.sh.cn
Organic Synthesis Lab
The Department of Chemistry
Fudan University                 Phone: 8621-65648139
No. 220 Handan Road              Fax:   8621-65641740
Shanghai, 200433
P. R. China
=============================================================





From chemistry-request@server.ccl.net  Tue Aug 29 09:07:22 2000
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Date: Tue, 29 Aug 2000 20:56:31 +0800
From: Yubo Fan <yubofan@guomai.sh.cn>
Subject: Is the scale available for B3LYP/LanL2DZ FREQ calculation?
To: CHEMISTRY@ccl.net
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Organization: Fudan University
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Hi, everyone,

I tried some metal clusters' G98 jobs in these days. I cannot find the
frequency scales for LanL2DZ basis set. Could somebody have the scale
for B3LYP/LanL2DZ? If possible, please tell me the reference.

Thanks in advance.

Y. Fan

--
=============================================================
Yubo Fan                         Email: yubofan@guomai.sh.cn
Organic Synthesis Lab
The Department of Chemistry
Fudan University                 Phone: 8621-65648139
No. 220 Handan Road              Fax:   8621-65641740
Shanghai, 200433
P. R. China
=============================================================






From chemistry-request@server.ccl.net  Tue Aug 29 14:27:03 2000
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Dear Colleagues,

Can someone help me with papers/reviews on carbon in transitional metal
oxide films deposited on silicon using organometallic precursors.
Where is carbon located before and after annealing, e.g. substitutional
or interstitial? In MeOx film, in silicon or at the interface? Does it have
thermodynamic  or kinetic stability? Any information which can help to
conduct investigation will be  kindly appreciated :-)

I am temporary NOT at CCL: many trips to avoid the heat in Phoenix :-)
Nice chats at the list can easily overload a mailbox in a few weeks
of absence.

Thanks a lot in advance,

Anatoli
r40757@email.sps.mot.com


From chemistry-request@server.ccl.net  Tue Aug 29 14:33:21 2000
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Dear CCLers,

Last week, the Computers in Chemistry Division (COMP) held 
the first ever Emerging Technology Symposium at the 
American Chemical Society National Meeting, Washington, DC.

Seven speakers competed for a prize of $1000, sponsored by 
Schroedinger, Inc.

We are happy to announce the winner, who received a cash 
prize at the meeting:  Prof. Amiram Goldblum (Hebrew 
University of Jerusalem) spoke on work by himself and his 
student Meir Glick.  The talk was entitled "A novel 
stochastic algorithm for structure predictions in proteins 
and for biomolecular interactions."

The following six speakers received a complimentary volume of 
"Reviews in Computational Chemistry":

Melissa L. Plount Price (Yale University)
Matthew R. Lee (University of California, San Francisco)
Randy J. Zauhar (University of the Sciences in Philadelphia)
Shiang-Tai Lin (University of Delaware)
Thomas F. Hendrickson (Agouron Pharmaceuticals)
Joao M. Aires-de-Sousa (New University of Lisbon, Portugal)

Congratulations to Amiram and everyone else who participated.

The seven talks were judged by a Panel of Experts consisting of 
Prof. Curt Breneman, Dr. George R. Famini, Dr. Charles H. Reynolds, 
Dr. Peter S. Shenkin, Dr. David C. Spellmeyer, and Dr. Terry R. Stouch.

Thanks, Don

Donald B. Boyd, Ph.D.
Editor, Journal of Molecular Graphics and Modelling
	(publication of the ACS COMP division and MGMS)
	http://chem.iupui.edu/~boyd/jmgm.html
Indiana University-Purdue University at Indianapolis
E-mail boyd@chem.iupui.edu


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Would anyone be willing to explain the essential difference between 
Richard Bader's approch to quantum chemistry and more conventional ab 
inito work?

Also if possible, how does this approach relate to mainstream DFT work?

regards,

From chemistry-request@server.ccl.net  Tue Aug 29 15:46:50 2000
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From: "Donahue, Mike" <MDonahue@atinc.com>
To: "'CHEMISTRY@ccl.net'" <CHEMISTRY@ccl.net>
Subject: virtual IMS
Date: Tue, 29 Aug 2000 15:44:31 -0400
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Hi anybody interested,

Is there software currently available that can mimic reactions typical of an
IMS(Ion Mobility Spectrometer)?

Any info would be greeatly appreciated.

Thanks,
Mike Donahue


From chemistry-request@server.ccl.net  Tue Aug 29 16:08:13 2000
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From: Don Steiger <dsteiger@bioeng.ucsd.edu>
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Subject: Dielectric of NON bulk water.


Does anybody know of any crude formulas (or methods) for estimating the 
dielectric of a "small" number of water molecules.  I am looking for something
that is just a little better than always defaulting to 80.

Thanks,


Don

dsteiger@be-research.ucsd.edu

From chemistry-request@server.ccl.net  Tue Aug 29 17:27:53 2000
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From: "Alexei Khalizov" <khalizov@chemistry.mcgill.ca>
Organization: Chemistry Dept., McGill University
To: chemistry@ccl.net
Date: Tue, 29 Aug 2000 17:27:53 -0400
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Subject: QCISD()/CCSD() and T1Diag
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Dear CCLers,

I would greatly appreciate receiving any help regarding the next two 
questions on QCISD/CCSD keyword and T1Diag command in 
G98W:

(i) I found that upon any modifications applied with QCISD/CCSD 
keywords, e.g.:

#P QCISD/6-31G* QCISD(MaxCycle=40) 
  or 
#P QCISD/6-31G* QCISD(T1Diag)

Gaussian performs calculation using Brueckner doubles. Why 
does it do this? How should one treat the energies obtained in 
such calculations?

(ii) Does Gaussian calculate the value of T1/Q1 diagnostic or I have 
to do it myself? How can I do it (part of the output is presented 
below)? There is no explanation in Gaussian manual/help about it. I 
have read the quoted papers, but it didn't help me much.

Sincerely yours,
Dr. Alexei Khalizov

------------------------------------------------
 Doing CCD using Brueckner orbitals...
 RMS singles vector = 7.71D-06
 which is small enough for convergence.
 Time for triples=      154.00 seconds.
 T4(BD)= -0.27566640D-01
 BD(T)= -0.10024046695D+04
 Leave Link  916 at Sun Apr 30 19:41:58 2000, MaxMem=    
8388608 cpu:     254.0
 (Enter C:\G98W\l915.exe)
 UMP5:  MDV=   8388608.
 Brueckner Doubles with Triples and Quadruples (BD(TQ))
 
=================================================
=====
 Saving the triples amplitudes on disk, using   58994116 words of 
disk space.
 Time for triples=      170.00 seconds.
 Disk space used for TT scratch files  :     62365056 words
 E5TTaaa =   0.81839768D-04
 E5TTaab =  -0.13959555D-03
 E5TTabb =  -0.24724111D-03
 E5TTbbb =   0.86337162D-04
 E5TT     =  -0.21865973D-03
 E5TQ2    =   0.61318769D-02
 EQQ2     =  -0.38569674D-02
 DE5   =   0.20562497883D-02 BD(TQ)    =  -0.10024026133D+04
-------------------------------------------------------



-------------------------
Dr. Alexei Khalizov
Department of Chemistry
McGill University,
801 Sherbrooke St. W.,
Montreal, Quebec, CANADA,
H3A 2K6

Phone: (514) 398-6920
Fax: (514) 398-2382

From chemistry-request@server.ccl.net  Tue Aug 29 18:15:12 2000
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Date: Tue, 29 Aug 2000 17:15:08 -0500 (CDT)
From: TREVOR D POWER <tdp0006@unt.edu>
To: chemistry@server.ccl.net
Subject: Re: CCL:F2 Ne potential
In-Reply-To: <Pine.A32.3.91.1000829132649.11664B-100000@fkrs2.phc.chalmers.se>
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Harald,
 
   You can get the program for calculating two-dimensional 
surfaces, that is for a given value of r, but you will have 
to figure out something better than what we used for a three-
dimensional surface. Since our dynamical calculations were 
very approximate, the error made by using a 3D surface described
in the paper was not a crucial factor. However, if one wants to
do more accurate calculations a better representation of the 3D 
surface is needed. 

Regards,
Trevor D. Power
NT Station, Box 305070
Department of Chemistry
University of North Texas
Denton, TX 76203-5070
tdp0006@unt.edu

On Tue, 29 Aug 2000, Harald Svedung wrote:

> Hi all of you,
> 
> I'm about to take a look at rovibrational energy transfer in F2-Ne 
> collisions. Does anyone have a subroutine implementing the potential in:
> 
> K. W. Chan, T. D. Power, J. Jai-nhiknan and S. M. Cybulski, J. Chem. 
> Phys. 110 860-869 (1999)
> 
> preferably giving the intermolecular potential energy as a function of 
> the interatomic distances.
> 
> Many thanks in advance!
> 
> :-)
> /Harald
> 
> 
> Harald Svedung (Ph.Lic.)                phone:          +46-31-7722816
> Department of Chemistry                 fax:            +46-31-167194
> Physical Chemistry                      home phone:     +46-31-240897, +46-709223206	
> Goeteborg University                    home e-mail:    harald.svedung@svedung.pp.se
> SE-412 96 Goeteborg, Sweden             www.che.chalmers.se/~svedung/	
> 
> 
> -= This is automatically added to each message by mailing script =-
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> 
> 
> 
> 



From chemistry-request@server.ccl.net  Tue Aug 29 23:19:27 2000
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References: <39A1B113.59576DBD@ksu.edu> <003901c00c46$44ecfd80$933a5392@ciencias.uchile.cl>
Subject: one question
Date: Tue, 29 Aug 2000 16:49:25 +0800

hi. CCLers,
 
When I run AMBER5.0, I face a problem as follows:
 
Reading &cntrl namelist w/ portable lib
 
old-style input no longer supported
 
Since I just begin to use this program, please tell me what
happaned.Thx!


