From chemistry-request@ccl.net Wed May 28 23:22:13 2003 -0400
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Reply-To: <mark/at/planaria-software.com>
From: "Mark Thompson" <mark/at/planaria-software.com>
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Subject: bug-fix release for ArgusLab 3.1
Date: Wed, 28 May 2003 20:18:06 -0700
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We've just uploaded a bug-fix release for ArgusLab 3.1

Several users reported the settings file version sometimes being read
incorrectly upon startup.

This release is free for licensed users and can be installed over an
existing ArgusLab 3.1 installation.

To link directly to the download page click on:
http://www.planaria-software.com/download_3_0.htm


=================================
Mark Thompson, Ph.D.
Planaria Software
PO Box 55207
Seattle, WA  98155
FAX: 206-440-3305

ArgusLab is available at:
http://www.arguslab.com
=================================


From chemistry-request@ccl.net Thu May 29 01:19:23 2003
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From: "Mark Thompson" <mark.-at-.planaria-software.com>
To: "Geoff Hutchison" <hutchisn.-at-.chem.northwestern.edu>,
   <sergiusz.kwasniewski.-at-.luc.ac.be>
Cc: <chemistry.-at-.ccl.net>
Subject: CCL: UV spectrum calculation (new question)
Date: Wed, 28 May 2003 22:15:16 -0700
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Geoff,

Great, I'll look at your paper.

I've obtained quite reasonable results with my ZINDO/RPA while specifying
the active space (e.g. 10 occupied, 10 virtual orbitals).  The calculations
do take longer than ZINDO/CIS, but for typical organic molecules of ~50
atoms, it's still just seconds to do the whole calculation on a commodity
PC.  I've obtained good results on the bacteriochlorophyll-b dimer from the
R. viridis xray structure for both UV/vis absorption and rotary strength
with good agreement between length and velocity operators for the transition
moments.  It's remarkable really, that ZINDO mimics a complete basis set in
some sense since the length-velocity operator agreement is exact only in the
limit of a complete basis.

In any case, we're working on our own ZINDO/RPA parameterization and we will
slipstream the parameters into the nearest ArgusLab build when they are
available.

In the meantime, one can run ZINDO/RPA with ArgusLab 3.1 by selecting the
"calculate rotary strengths" button.  This turns on both ZINDO/CIS and
ZINDO/RPA for the spectroscopic calculation of the molecule (the CIS results
are given first in the output and the RPA come after that).

In our 3.5 release (nearing completion), all the spectroscopic results can
be viewed more cleanly with our new property control.  The UV/vis
calculation setup is also cleaner with respect to delineating RPA vs. CIS

Mark

=================================
Mark Thompson, Ph.D.
Planaria Software
PO Box 55207
Seattle, WA  98155
FAX: 206-440-3305

ArgusLab is available at:
http://www.arguslab.com
=================================

> -----Original Message-----
> From: Computational Chemistry List [mailto:chemistry-request.-at-.ccl.net]On
> Behalf Of Geoff Hutchison
> Sent: Wednesday, May 28, 2003 3:50 PM
> To: sergiusz.kwasniewski.-at-.luc.ac.be
> Cc: chemistry.-at-.ccl.net
> Subject: CCL:UV spectrum calculation (new question)
>
>
> > I'm curious how well INDO/S-RPA works against INDO/S-CIS for large
> > systems.
> > I only remember one article by M. Zerner quite a long time ago..
>
> A comparison of ZINDO/RPA vs. ZINDO/CIS on various conjugated oligomers
> is included as part of my larger paper (which also compares HF/CIS,
> HF/RPA, TDDFT/CIS and TDDFT/RPA):
>
> J. Phys. Chem. A (2002) 106(44) p. 10596-10605.
>
> At the time, the only ZINDO/RPA I could put my hands on was contributed
> by Sergei Tretiak and Shaul Mukamel, which didn't let me set an active
> space. (In fact, it uses the Lanczos method for a full active space.) A
> parameterization for RPA calculations or a smaller active space would
> probably help.
>
> > Probably the calculation takes a lot longer (Hamiltonian matrix is
> > four times
> > as big since mixing of particle-hole and hole-particle excitations
> > occurs).
>
> I think with an efficient implementation, it's not really an issue.
> (It's a semiempirical calc. after all!) I never did timing tests, but I
> can relate that up to 60+ heavy atoms, ZINDO/RPA calculations still
> only took something on the order of minutes (on an 800MHz Pentium III,
> so faster times nowadays).
>
> > Are there any problems with numerical instabilities with the
> > implemented RPA scheme in a INDO/S-RPA calculation ?
>
> I'll second Dr. Thompson's comments. I haven't run any extremely
> "strange" molecules, but haven't seen any instabilities.
>
> Cheers,
> -Geoff
>
> --
> -Geoff Hutchison		<hutchisn.-at-.chem.northwestern.edu>
> Ratner/Marks Groups	(847) 491-3295
> Northwestern Chemistry	http://www.chem.northwestern.edu/
>
>
>
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>



From chemistry-request@ccl.net Thu May 29 02:09:21 2003
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From: Wai-To Chan <chan*at*curl.gkcl.yorku.ca>
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Subject: Re: calculating atomic charges with AIMPAC
To: chemistry*at*ccl.net
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<<<<<<<<<<<<<<<<<<<<<<<<<<<<<<<<<
I currently have an undergraduate student who is attempting to compare 
charges of methylated benzene and ferrocene systems using the AIMPAC 
software.  In the case of hexamethyl benzene and the ferrocene analogues he 
is getting very large negative charges on some the ring carbons (-5 to -20) 
and small positive charges on iron (0.5) Can anyone tell me if there is a 
problem with the program or if the ring system can not be treated with this 
method?
>>>>>>>>>>>>>>>>>>>>>>>>>>>>>>>


   I remember reading about the tendency of AIM changes to be larger in magnitude
than expected on the basis of chemical intuition. There is a paper by
Kenneth Wiberg from the early 90s in J. comp. chem. about the comparison of 
several atomic-charge partitioning scheme including Bader's you may find useful. 
You may also consider using the Natural atomic charges method if you want 
faster and less 'surprising' results. 

Wai-To Chan



From chemistry-request@ccl.net Thu May 29 01:58:13 2003
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From: Philip Stortz <madscientist*at*wyoming.com>
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The idea of orbitals seems reasonable, but obviously there have been a lot of simplifications in the
already hugely complex programs written for ccl.  I would also argue, that the programs currently in
use as well as the parameters for each element have been aggressively tweaked to match lab results.
Clearly current ccl code has enough degrees of freedom to model nearly any thing else that's currently
modeled by  subtly changing parameters and/or code.  

CCL programs are useful tools only because of this "tweaking", though any tool is better than no tool
usually.  obviously correlation between calculation and result does not prove a theory "true",
particularly when you have feedback between experiment and model development.  also, most programs do
seem to do better on large systems, probably because of the tendency for errors to cancel each other
to some extent.

one of my favorite examples: there was a period during the late 60's and early seventies when the
length of ladies skirts very, very closely matched sunspot activity, for a whole 11 year cycle!  One
might have concluded that fashion can predict solar activity or vice versa, and developed the
appropriate predicative code, at least until the trend changed.  As i said, it seems to me that modern
ccl code could be modified for nearly any predictive activity and the constant tweaking means that it
must approach consistency with experimental results, no matter whether the original idea has any basis
in "reality" or not.  Reality is in the mind of the beholder, as long as you agree with the majority,
otherwise you still think you understand "reality", but others will think you foolish or insane.
Agreement with experimental data supports a theory, until that experimental data can no longer be
accommodated into the existing model or someone comes up with a simpler or more accurate theory (even
if more complicated, or fundamentally less "real").

Finally, as of last year (I believe it was last year, sorry i don't have a reference), fractional
electrons exist, at least in liquid helium near absolute zero, where they were able to induce i
believe at least 6 different species of charge carrier with different charge to mass ratios.  It
wouldn't surprise me if this partially explains (assuming you take the experimental observation to be
"real") Pi bonds.  And considering it's place on the periodic table (another highly useful but
imperfect tool) i'd suspect this may account for some of the problems modeling lithium compounds.  It
might even relate to superconductivity, which is observed, but still poorly understood i believe.

I only wish there were good code for inorganic crystal electronic spectrum calculations, but that's
not where most people see the money, so the code base hasn't been tweaked in that direction
extensively.  Still, i'd prefer i guide who happens to be right over no guidance at all, it provides
that "comfort" we all seek, and of course a way to shift the blame.  ("it's not my fault we wasted
billions, that was what the program said to do, blame the developers")

elewars wrote:
> 
> 2003 May 28
> 
> Are MOs physically real? This is a meaningful question only if there is some
> experiment or observation that could provide an answer _yes_ or _no_.  Is there,
> at least in principle, such an experiment or observation?
-----------
-- 
Philip Stortz -- To be nobody but yourself when the whole world is trying its best night and day to make you everybody else is to fight the hardest battle any human being will ever fight. -- E.E. Cummings


From chemistry-request@ccl.net Thu May 29 02:05:38 2003
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To help with modeling electronic spectra of crystals, is there a good package out there to build the initial crystal with at least a couple dozen unit cells if i know the crystal structure?  I've tried this with Cache a few years ago, and the drawing tool was not very useful and very painful for building 3d crystals, bonds often wound up in odd places where i didn't mean to put them and it was very hard to view the bonds to see these problems.  Thanks again.

-- 
Philip Stortz -- To be nobody but yourself when the whole world is trying its best night and day to make you everybody else is to fight the hardest battle any human being will ever fight. -- E.E. Cummings


From chemistry-request@ccl.net Thu May 29 02:01:05 2003
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Time for my annual hopeful question, is there currently a program that calculates electronic spectra
of inorganic crystals (and their surfaces) with any accuracy?  I know zindo/indo works good for
organics, but what about for inorganic crystals?  Does mopac do this well, i know fujitsu was working
on it?  I'm hoping someone on this list has had good luck with such problems as it's often hard to
tell from what vendors claim just how good or useful a program may be.  I'm hoping to buy software in
a couple of months that will hopefully let me test fewer samples to find what i'm looking for.  Even
if not absolutely accurate, something that reasonably predicted the change in spectrum from one
inorganic material to another to help steer the research would be very, very helpful.  Thank you in
advance for any help you can provide.

Re: spam problems (listmom), you might look into spamcop.net, they have a fairly good system with a blacklist of
open relays and several addresses that are designed to be spam magnets so they can detect other spam.
I'll use their service myself if i ever start getting more than one or two spams a month, i've been
very lucky as far as spam goes.  I've also aggressively reported spam, which does seem to help (spam
cop will let anyone do that for free).

-- 
Philip Stortz -- To be nobody but yourself when the whole world is trying its best night and day to make you everybody else is to fight the hardest battle any human being will ever fight. -- E.E. Cummings


From chemistry-request@ccl.net Thu May 29 04:36:22 2003
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From: Jamie Platts <Platts~at~Cardiff.ac.uk>
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  Dear Julia - have you checked the quality of the integrations? This is
usually best done with the number reported as "L" (I think the fourth
quantity output by proaimv). This is the value of the Laplacian integrated
over the atomic basin, which should vanish - values of 10^-3 are
borderline OK, lower is obviously better. Also check that the total
populations add up to the no. electrons in your system.

  For a system like ferrocene, with rings (and cages?), you might need to
tweak some of the surface-tracing paramaters - see the top of the
proaimv.f code.

  If this isn't the source of your problem, you could try the integration
methods in Gaussian (disappointing in my experience) or Popelier's
MORPHY, which is generally very robust.

  Hope this helps - Jamie

> I currently have an undergraduate student who is attempting to compare
> charges of methylated benzene and ferrocene systems using the AIMPAC
> software.  In the case of hexamethyl benzene and the ferrocene analogues he
> is getting very large negative charges on some the ring carbons (-5 to -20)
> and small positive charges on iron (0.5) Can anyone tell me if there is a
> problem with the program or if the ring system can not be treated with this
> method?
>
> Thank you,
> Julia Metzker
> University of York
> Department of Chemistry

From chemistry-request@ccl.net Thu May 29 05:56:24 2003
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Subject: CCL: Re:Eigenvalues of hessian
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Dear Daniel,

I think that you should specify more clearly what
system you are calculating (e.g. isolated molecule,
crystal, use of restraints/constraints, etc.)

If you do a full energy minimisation on an isolated
molecule, then you MUST have 3N-6 (or 3N-5 for a
linear molecule) zero frequencies if the frequency
calculation is done from a Hessian matrix calculated 
with Cartesian derivatives, and the system was 
properly minimised.

If the energy surface is flat, you may have to
make the convergence criteria more stringent in order
to reach the minimum more closely.

Each negative (imaginary) frequency implies a maximum
along the corresponding eigenvector, each additional
zero an inflection point.

For crystals the number of non-zero frequencies depends
on how the calculation is done and/or what the space group
of the system is.

If space group symmetry is ignored, 3 (translational)
modes are zero. If space group symmetry is taken into
account, a centro-symmetrical space group will have
no zero frequencies, whereas for the others it depends
on whether the symmetry elements fix the origin along 
each of the 3 axes.

If you are using special features, e.g. rigid groups,
fixing some internal coordinates, etc., there is no 
general rule and the number of zero-frequencies must
be worked out based on the actual number of degrees
of freedom of the system.

If you are using a force field with additional "goodies"
like lone pairs, dummy atoms, or other particles
with undefined mass, the answer depends on how these
artefacts are projected out.

Groeten
Jan Dillen

> Does anybody of you know, why there are more than 3N-6 nonzero
> eigenvalues of the hessian? I am especially interested in the question,
> whether this error is due to the errors made by differentiation or
> whether they are due to an error within the method itself. I usually get
> only 3 zero eigenvalues. No matter if the hessian is calculated on a
> stationary point or not.


From chemistry-request@ccl.net Thu May 29 06:05:45 2003
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From: Marcin Krol <mykrol<<at>>cyf-kr.edu.pl>
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Hello,

I'd like to calclulate dynamic cross-corelation matrices in CHARMM. So
firstly, I oriented all trajectiory frames on the crystal structre (merge
orient keyword). Then I calculated average structure from the oriented
trajectory and defined times series as fluctuation of all CA atoms (each
CA
atoms represents motions of the whole aminoacid). When I had times series
for all CA atoms I started to calculate

<Q(a)*Q(b)>/sqrt<Q(a)**2>*sqrt<Q(b)**2>

where Q(a) is one time series and Q(b) another.
In principle I should get what I want, but the values I obtain are between
0.8-1.0 no matter what time series are chosen. It looks like motions of
all aminoacids in my protein are highly correlated, which is not very
probable. What can be the reason for it? I have oriented the whole
trajectory on the crystal structure so translations and rotations of the
center of mass should be removed.

Thanks in advance for any suggestions how to obtain correct DCCM in CHARMM

Marcin Krol

Below is the charmm script I use.

1. To remove trans and rot of the center of mass

open crystal struture
read crystal structure

coor copy comp

open input traj files

open output traj files

merge firstu 41 nunit 24 skip 500 outputu 71 nfile 200 sele segid (name of
my protein) end orient sele type CA end

(so I should get a new traj files which contain only protein atoms and
frames are oriented on crystal structure CA atoms)

2. Caluculate DCCM

open crystal structure
read crystal structure

open oriented traj files

coor dyna comp firsu 41 nunit 5

correl maxt 1050 maxseries 433 maxatoms 433 cutnb 2.

set res 1

label enterdccm
	enter a@res fluc r sele resi @res .and. type CA end
 	traj first 41 nunit 5

	incr res by 1
if res lt 433 goto eneterdccm

set res 1

label one
      set res

      label two

  	   mantime a@res fluct a@resn

           incr resn by 1
       if resn lt 433 goto two

       incr res by 1

if res lt 433 goto one

stop
end



From chemistry-request@ccl.net Thu May 29 06:49:52 2003
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Date: Thu, 29 May 2003 03:49:51 -0700 (PDT)
From: Noriaki Ikuta <noriaki_ikuta<<at>>yahoo.com>
Subject: CCL: ic50 values in dtp aids dataset
To: chemistry<<at>>ccl.net
Cc: noriaki_ikuta<<at>>yahoo.com
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I have three questions regarding the DTP AIDS
Antiviral Screening dataset.
http://dtp.nci.nih.gov/docs/aids/aids_data.html

i) The explanation for the IC50 is "concentration of
compound that inhibits the growth of uninfected cells
by 50%" I do not understand this. I throught it would
be of interest to inhibit the virus or at least the
growth of infected cells?

ii) How is the conclusion active/inactive drawn from
those IC50 values? 
I have included a few example entries with ConcUnit =
M in the mail.

HiConc - the highest concentration used in the dose
response
Flag -  when different experiments are averaged,
        "=" indicated that all the experiments reached
IC50
        ">" indicates that at least one of the
          experiments don't actually reach an EC50
          and the highest tested concentration is 
          used for the value of IC50 
IC50 - concentration of compound that inhibits the
growth of uninfected cells by 50%
Conclusion - CA active, CM moderately active, CI
inactive

NSC	Log10HiConc	Flag	Log10IC50	Conclusion
646607	-5.4	>	-5.42	CA
646607	-4.5	=	-5.29	CA
646607	-3.7	=	-5.79	CA
646609	-4.5	=	-5.78	CA
646609	-3.7	=	-5.61	CA
646610	-4.5	=	-5.77	CA
646610	-3.7	=	-5.88	CA
639762	-3.7	=	-4.75	CM
639762	-3.6	=	-4.88	CM
639763	-4.4	=	-4.63	CM
639765	-3.9	=	-4.69	CM
639766	-4.6	>	-4.79	CM
626162	-3.7	<	-7.2	CI
629266	-3.7	<	-7.2	CI
630958	-3.9	=	-4.74	CI
630959	-3.2	=	-3.85	CI
639915	-4.7	>	-4.7	CI
639975	-3.9	>	-5.05	CI
640064	-5	>	-5	CI
640064	-3.7	>	-3.7	CI


iii) Are there papers available explaining this
dataset in depth?


Noriaki 

__________________________________
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Yahoo! Calendar - Free online calendar with sync to Outlook(TM).
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From chemistry-request@ccl.net Thu May 29 05:59:42 2003
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Subject: RE: Eigenvalues of hessian
From: "Daniel R. Rohr" <rohrd<<at>>students.uni-marburg.de>
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Hi CCLer

 Maybe I should clearify my question:
I do know that in the Hessians calculated, there is usually translation
and rotation. I want to avoid speaking of frequencies, because we are
talking about Hessians which are not necessarily calculated at
stationary points. That#s why I talk of the eigenvalues.
In an excat method there should be exactly 3N-6 nonzeroeigenvalues and 6
exact zeros. ANY method I tested (HF, DFT and MP2) with ANY Program I
tested (Gaussian, Turbomole, Jaguar) gives me 3N nonzero Eigenvalues.
The question is now. Why are there too many nonzero Eigenvalues? In my
eyes there are two possible reasons:

1. The method is ok but there are errors made in the derivations of the
method. Maybe neglecting terms in the differentiation. Or maybe
asumptions that hold true only for stationary points.

2. The method is not ok. This means that I do get different Energies for
different orientations of my molecule (As is the case in DFT)

Of course it is also possible that there is a mixture of both. I would
like to know which error is the bigger one? And maybe get a reference
for this question.

Another point which I do not understand:
Some answers state that there is only little translation and rotation
since the frequencies are close to zero. Is the absolute value of an
eigenvalue a measure for the quantity (whaterver that means) of its
eigenvector???? And if that is the case why is there "more" translation
and rotation at nonstationary points? I get "frequencies" (this is
eigenvalues of the Hessian) between 400 and 850 cm^-1 for Water with HF
6-31G** (Gaussian calculation):

Low frequencies --- -410.8545   -0.0007   -0.0006    0.0017  489.4045
853.6142
 Low frequencies --- 1891.8502 3808.4304 3946.8117

These are of course the frequencies calculated BEFORE projection of
translation and rotation.

I hope you can help me on that

Daniel Rohr


Hi Daniel,

Your question is a bit tricky in that the answer depends on the method
you
are using.
 
If you are calculating Hartree-Fock or MP2 hessians then I think you
should
get 6 zero eigenvalues and 3N-6 non-zero eigenvalues at a stationary
point.
Even if the hessian is obtained by numerical differentiation of
gradients
this should come out allright, otherwise the code is broken.

If you are doing a DFT calculation life typically gets a bit more
complicated. If the DFT hessian is implemented as a proper second
derivative
of the energy expression with respect to the nuclear coordinates you
should
still get 6 zero eigenvalues. However this requires that the code takes
the
2nd derivatives of the Becke weights (A.D. Becke, J.Chem.Phys. 88 (1988)
2547-2553) into account as well. Some codes don't bother calculating
these
terms in which case the strict translational invariance of the hessian
is
violated. This typically expresses itself in 3 additional non-zero but
small
valued eigenvalues. 

If you are calculating the vibrational modes by numerical
differentiation of
DFT gradients then there may still be a problem if your molecule has
symmetry. Many quantum chemistry packages will reorientate your molecule
such that the main axes of ineratia coincide with the Cartesian axes of
your
coordinate system. This means that different points in the numerical
differentiation algorithm may be calculated at different orientations.
However, the DFT quadratures are not always invariant for rotations. For
example if you want to do calculations on H2 and you are going to use 6
points per H atom all placed on the Cartesian axes than the energy
you'll
get for the following two orientations will not be the same even if the
bond
distance is:

    H  H
    |   \
    H    H

Again this will lead to additional non-zero but small eigenvalues. In
this
case it may help to switch the use of symmetry off, so that all points
are
calculated in exactly the same orientation. 

As you have given very little details about exactly which calculation
you
are doing I can not say for sure which of the above reasons is the most
like
cause. However I think it is most likely one of these and with some
experimentation and a good look at the documentation for your program
you
should be able to find out what is happening.

Best wishes,

   Huub van Dam

-----Original Message-----
From: Daniel R. Rohr
To: ccl
Sent: 5/28/03 3:20 PM
Subject: CCL:Eigenvalues of hessian

Hi CCLers

 Does anybody of you know, why there are more than 3N-6 nonzero
eigenvalues of the hessian? I am especially interested in the question,
whether this error is due to the errors made by differentiation or
whether they are due to an error within the method itself. I usually get
only 3 zero eigenvalues. No matter if the hessian is calculated on a
stationary point or not.

Thanks for your help

Daniel Rohr

-- 
-----------------------------------------------------------------------
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                                                Philipps-Universitdt
 Tel.: +49-6421-28-25686                        Hans-Meerwein-Stra_e
 Fax.: +49-6421-28-25566                        D-35043 Marburg
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From chemistry-request@ccl.net Thu May 29 04:12:10 2003
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To: "'Guosheng Wu'" <wu_guosheng2002=at=yahoo.com>, <chemistry=at=ccl.net>
Subject: RE: orbitals
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* * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * *
Jangbae Kim
Researcher                                                  
Bio-Organic Science Division
Korea Research Institute of Chemical Technology (KRICT)
 
P.O.Box 107,  Yuseong, Taejeon,
305-600, Korea
TEL : +82-42-860-7067
FAX : +82-42-861-0307
E-mail : jbkim=at=krict.re.kr
* * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * *


> -----Original Message-----
> From: Computational Chemistry List [mailto:chemistry-request=at=ccl.net] On
> Behalf Of Guosheng Wu
> Sent: Thursday, May 29, 2003 7:46 AM
> To: chemistry=at=ccl.net
> Subject: CCL:orbitals
> 
> --- Rene Fournier - 1999-07-07 <renef=at=yorku.ca> wrote:
> >    Leif Laaksonen makes an important point: only observables
> > are "real" in QM.  So the question arises: is it possible to
> > define orbitals as QM observables.  It entirely depends on
> > how you define the word "orbital".  If one says orbitals are
> > one-electron functions and nothing more, then of course orbitals
> > can be made to be QM observables.  For example, just integrate
> > an exact squared wavefunction over all electron coordinates
> > but one to get the electron density, then take the square
> > root, multiply by a phase factor and you get "density orbitals".
> > [G Hunter, Int J Quantum Chem 9 (1975) 237].   They may not be
> > very useful as orbitals, but they are "real" in the sense of
> > QM observables.
> 
> It's not clear for me how you define "QM observable"?
> 
> MO is certainly not "observable", if "observable" is defined as something
> can be measured directly or indirectly by an experiment. For example,
> electronic density, ionization energy, and so on.
> 
> The issue is related with the phase factor you mentioned:
>   From experimental data, one can get |MO|^2 at a certain position,
>   but here "MO" is not unique: MO = |MO|*[cos(theta)+i*sin(theta)],
>   where "theta" can be any arbitary value.
> This may be traced back to the Uncertainty Principles.
> 
> Similarly to my original post, 0, 1, 2,... are countable (defined as
> non-negative integers). However, if one do the square of 1, +1 and -1
> will come out, not unique --- 2 directions in the 1-D space;
> Do the square of -1, we get +i and -i, 2 direction in the 2-D space...
> It seems we can safely say that -1 & i are not countable!?
> 
> By the way, does it really matter if "MO" is observable or not in any
> sense?
> Maybe useful for teaching.
> 
> Guosheng
> 
> 
> > --- Rene Fournier - 1999-07-07 <renef=at=yorku.ca> wrote:
> > >    Leif Laaksonen makes an important point: only observables
> > > are "real" in QM.  So the question arises: is it possible to
> > > define orbitals as QM observables.  It entirely depends on
> > > how you define the word "orbital".  If one says orbitals are
> > > one-electron functions and nothing more, then of course orbitals
> > > can be made to be QM observables.  For example, just integrate
> > > an exact squared wavefunction over all electron coordinates
> > > but one to get the electron density, then take the square
> > > root, multiply by a phase factor and you get "density orbitals".
> > > [G Hunter, Int J Quantum Chem 9 (1975) 237].   They may not be
> > > very useful as orbitals, but they are "real" in the sense of
> > > QM observables.
> > >     Orbitals are always defined as one-electron functions,
> > > but THAT does not make them "unreal".  The electron density
> > > is a one electron function and very real for any N-electron
> > > system, not only for the H atom.
> > >     One "ab initio" way to define orbitals is to start from
> > > exact wavefunctions and calculate the overlap of a N-electron
> > > wavefunction (neutral) and the ground and various excited
> > > states a (N-1)-electron wavefunction (ion) (Dyson orbitals are
> > > defined in such a way I think).  I'm sure there are definitions
> > > that will make such orbitals unique, but does that make them
> > > QM observables?  I don't think so, but I'd like to hear from
> > > the CCL community on that.  There are other ways to define orbitals
> > > > from exact wavefunctions, I'm sure: are any of them QM observables?
> > >     As for Kohn-Sham orbitals, they may not be real individually
> > > but the N lowest energy ones squared and summed give the true
> > > electron density (an observable) and the negative of the KS HOMO
> > > energy is exactly equal to the first IP (another observable) so
> > > there are at least some bits of reality built in KS orbitals!
> > >
> > > Here's some relevant articles:
> > >
> > > 1) Kohn, Becke, Parr, J Phys Chem 100 (1996) 12974
> > > 2) "Kohn-Sham Orbitals and Orbital Energies: Fictitious Constructs but
> > >    Good Approximations All the Same"
> > >    by S. Hamel, P. Duffy, M.E. Casida, and D.R. Salahub
> > >    Journal of Electron Spectroscopy and Related Phenomena (2002?)
> > > 3) Chong, Gritsenko, Baerends, J Chem Phys 116 (2002) 1760
> > >
> > > --------------------------------------------------------------------
> > > | Rene Fournier                 | Office:  303 Petrie              |
> > > | Chemistry Dpt, York University| Phone: (416) 736 2100 Ext. 30687 |
> > > | 4700 Keele Street,  Toronto   | FAX:   (416)-736-5936            |
> > > | Ontario, CANADA   M3J 1P3     | e-mail: renef=at=yorku.ca           |
> > > --------------------------------------------------------------------
> > > |                http://www.chem.yorku.ca/profs/renef/             |
> > > --------------------------------------------------------------------
> > >
> > >
> > >
> > >
> > >
> > >
> > >
> > >
> > >
> > >
> >
> >
> > __________________________________
> > Do you Yahoo!?
> > Yahoo! Calendar - Free online calendar with sync to Outlook(TM).
> > http://calendar.yahoo.com
> >
> 
> 
> __________________________________
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> 
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From chemistry-request@ccl.net Thu May 29 08:56:31 2003
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From: "Shobe, Dave" <dshobe{at}sud-chemieinc.com>
To: "'CCL'" <chemistry{at}ccl.net>
Subject: RE: calculating atomic charges with AIMPAC
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But a charge of -20 almost certainly is the result of assigning the
electrons of one atom's basin to another atom.  Something which occurs as a
result of the program failing to find the boundary between them.  

At any rate, I would try a 2nd AIM calculation program if one is available,
before giving up.  E.g., I often find Gaussian's AIM code halts with a
(usually cryptic) error message, but for the same molecule AIM2000 may
complete the calculation with no problem.



-----Original Message-----
From: Wai-To Chan [mailto:chan{at}curl.gkcl.yorku.ca]
Sent: Thursday, May 29, 2003 2:09 AM
To: chemistry{at}ccl.net
Subject: CCL:calculating atomic charges with AIMPAC


<<<<<<<<<<<<<<<<<<<<<<<<<<<<<<<<<
I currently have an undergraduate student who is attempting to compare 
charges of methylated benzene and ferrocene systems using the AIMPAC 
software.  In the case of hexamethyl benzene and the ferrocene analogues he 
is getting very large negative charges on some the ring carbons (-5 to -20) 
and small positive charges on iron (0.5) Can anyone tell me if there is a 
problem with the program or if the ring system can not be treated with this 
method?
>>>>>>>>>>>>>>>>>>>>>>>>>>>>>>>


   I remember reading about the tendency of AIM changes to be larger in
magnitude
than expected on the basis of chemical intuition. There is a paper by
Kenneth Wiberg from the early 90s in J. comp. chem. about the comparison of 
several atomic-charge partitioning scheme including Bader's you may find
useful. 
You may also consider using the Natural atomic charges method if you want 
faster and less 'surprising' results. 

Wai-To Chan



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charset=3Diso-8859-1">
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<TITLE>RE: calculating atomic charges with AIMPAC</TITLE>
</HEAD>
<BODY>

<P><FONT SIZE=3D2>But a charge of -20 almost certainly is the result of =
assigning the electrons of one atom's basin to another atom.&nbsp; =
Something which occurs as a result of the program failing to find the =
boundary between them.&nbsp; </FONT></P>

<P><FONT SIZE=3D2>At any rate, I would try a 2nd AIM calculation =
program if one is available, before giving up.&nbsp; E.g., I often find =
Gaussian's AIM code halts with a (usually cryptic) error message, but =
for the same molecule AIM2000 may complete the calculation with no =
problem.</FONT></P>
<BR>
<BR>

<P><FONT SIZE=3D2>-----Original Message-----</FONT>
<BR><FONT SIZE=3D2>From: Wai-To Chan [<A =
HREF=3D"mailto:chan{at}curl.gkcl.yorku.ca">mailto:chan{at}curl.gkcl.yorku.ca</=
A>]</FONT>
<BR><FONT SIZE=3D2>Sent: Thursday, May 29, 2003 2:09 AM</FONT>
<BR><FONT SIZE=3D2>To: chemistry{at}ccl.net</FONT>
<BR><FONT SIZE=3D2>Subject: CCL:calculating atomic charges with =
AIMPAC</FONT>
</P>
<BR>

<P><FONT =
SIZE=3D2>&lt;&lt;&lt;&lt;&lt;&lt;&lt;&lt;&lt;&lt;&lt;&lt;&lt;&lt;&lt;&lt=
;&lt;&lt;&lt;&lt;&lt;&lt;&lt;&lt;&lt;&lt;&lt;&lt;&lt;&lt;&lt;&lt;&lt;</F=
ONT>
<BR><FONT SIZE=3D2>I currently have an undergraduate student who is =
attempting to compare </FONT>
<BR><FONT SIZE=3D2>charges of methylated benzene and ferrocene systems =
using the AIMPAC </FONT>
<BR><FONT SIZE=3D2>software.&nbsp; In the case of hexamethyl benzene =
and the ferrocene analogues he </FONT>
<BR><FONT SIZE=3D2>is getting very large negative charges on some the =
ring carbons (-5 to -20) </FONT>
<BR><FONT SIZE=3D2>and small positive charges on iron (0.5) Can anyone =
tell me if there is a </FONT>
<BR><FONT SIZE=3D2>problem with the program or if the ring system can =
not be treated with this </FONT>
<BR><FONT SIZE=3D2>method?</FONT>
<BR><FONT =
SIZE=3D2>&gt;&gt;&gt;&gt;&gt;&gt;&gt;&gt;&gt;&gt;&gt;&gt;&gt;&gt;&gt;&gt=
;&gt;&gt;&gt;&gt;&gt;&gt;&gt;&gt;&gt;&gt;&gt;&gt;&gt;&gt;&gt;</FONT>
</P>
<BR>

<P><FONT SIZE=3D2>&nbsp;&nbsp; I remember reading about the tendency of =
AIM changes to be larger in magnitude</FONT>
<BR><FONT SIZE=3D2>than expected on the basis of chemical intuition. =
There is a paper by</FONT>
<BR><FONT SIZE=3D2>Kenneth Wiberg from the early 90s in J. comp. chem. =
about the comparison of </FONT>
<BR><FONT SIZE=3D2>several atomic-charge partitioning scheme including =
Bader's you may find useful. </FONT>
<BR><FONT SIZE=3D2>You may also consider using the Natural atomic =
charges method if you want </FONT>
<BR><FONT SIZE=3D2>faster and less 'surprising' results. </FONT>
</P>

<P><FONT SIZE=3D2>Wai-To Chan</FONT>
</P>
<BR>
<BR>

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From chemistry-request@ccl.net Thu May 29 08:46:35 2003
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From: "Shobe, Dave" <dshobe{at}sud-chemieinc.com>
To: "'Renxiao Wang'" <renxiao{at}med.umich.edu>, chemistry{at}ccl.net
Subject: RE: A question on heat of formation
Date: Thu, 29 May 2003 08:44:17 -0400
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Most people do the following.  They find the lowest-energy =
conformations of
the molecules involved, and use the energy at those geometries to =
calculate
delta-H.  The computational chemist should of course use any prudent,
reasonable means to ensure that these are indeed the *global* =
conformational
minima.

However...

I think to really "do it right" one has to calculate all the low-lying
conformations and determine the relative statistical-mechanical =
populations
of each conformation, and from that the average enthalpy per molecule =
(or
per mole). =20

Usually there are enough other sources of error that the correct =
procedure
has little advantage over the first approach, at least for enthalpy.  =
But
the corresponding "correct" procedure is often done for entropy, where
population of low-lying conformational isomers can make a significant
difference in the outcome.

--David Shobe
S=FCd-Chemie Inc.
phone (502) 634-7409
fax     (502) 634-7724
email  dshobe{at}sud-chemieinc.com

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




-----Original Message-----
From: Renxiao Wang [mailto:renxiao{at}med.umich.edu]
Sent: Wednesday, May 28, 2003 8:19 PM
To: chemistry{at}ccl.net
Subject: CCL:A question on heat of formation


Hi, CCLers!

Should the heat of formations of two enantiomers of a chiral compound =
be
identical? I think the answer is yes. Please point out some references
for this.=20

A disturbing fact is that, no matter you use QM or MM to calculate the
heat of formation for a given molecule, the number is
conformation-depentdent. I guess this is because of the steric energy
part is conformation-dependent. So, if I really want to compare the
stability of two molecules using heat of formation, how may I calculate
it right?

Best regards,

Renxiao Wang
renxiao{at}med.umich.edu



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<TITLE>RE: A question on heat of formation</TITLE>
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<P><FONT SIZE=3D2>Most people do the following.&nbsp; They find the =
lowest-energy conformations of the molecules involved, and use the =
energy at those geometries to calculate delta-H.&nbsp; The =
computational chemist should of course use any prudent, reasonable =
means to ensure that these are indeed the *global* conformational =
minima.</FONT></P>

<P><FONT SIZE=3D2>However...</FONT>
</P>

<P><FONT SIZE=3D2>I think to really &quot;do it right&quot; one has to =
calculate all the low-lying conformations and determine the relative =
statistical-mechanical populations of each conformation, and from that =
the average enthalpy per molecule (or per mole).&nbsp; </FONT></P>

<P><FONT SIZE=3D2>Usually there are enough other sources of error that =
the correct procedure has little advantage over the first approach, at =
least for enthalpy.&nbsp; But the corresponding &quot;correct&quot; =
procedure is often done for entropy, where population of low-lying =
conformational isomers can make a significant difference in the =
outcome.</FONT></P>

<P><FONT SIZE=3D2>--David Shobe</FONT>
<BR><FONT SIZE=3D2>S=FCd-Chemie Inc.</FONT>
<BR><FONT SIZE=3D2>phone (502) 634-7409</FONT>
<BR><FONT SIZE=3D2>fax&nbsp;&nbsp;&nbsp;&nbsp; (502) 634-7724</FONT>
<BR><FONT SIZE=3D2>email&nbsp; dshobe{at}sud-chemieinc.com</FONT>
</P>

<P><FONT SIZE=3D2>Don't bother flaming me: I'm behind a =
firewall.</FONT>
</P>
<BR>
<BR>
<BR>

<P><FONT SIZE=3D2>-----Original Message-----</FONT>
<BR><FONT SIZE=3D2>From: Renxiao Wang [<A =
HREF=3D"mailto:renxiao{at}med.umich.edu">mailto:renxiao{at}med.umich.edu</A>]<=
/FONT>
<BR><FONT SIZE=3D2>Sent: Wednesday, May 28, 2003 8:19 PM</FONT>
<BR><FONT SIZE=3D2>To: chemistry{at}ccl.net</FONT>
<BR><FONT SIZE=3D2>Subject: CCL:A question on heat of formation</FONT>
</P>
<BR>

<P><FONT SIZE=3D2>Hi, CCLers!</FONT>
</P>

<P><FONT SIZE=3D2>Should the heat of formations of two enantiomers of a =
chiral compound be</FONT>
<BR><FONT SIZE=3D2>identical? I think the answer is yes. Please point =
out some references</FONT>
<BR><FONT SIZE=3D2>for this. </FONT>
</P>

<P><FONT SIZE=3D2>A disturbing fact is that, no matter you use QM or MM =
to calculate the</FONT>
<BR><FONT SIZE=3D2>heat of formation for a given molecule, the number =
is</FONT>
<BR><FONT SIZE=3D2>conformation-depentdent. I guess this is because of =
the steric energy</FONT>
<BR><FONT SIZE=3D2>part is conformation-dependent. So, if I really want =
to compare the</FONT>
<BR><FONT SIZE=3D2>stability of two molecules using heat of formation, =
how may I calculate</FONT>
<BR><FONT SIZE=3D2>it right?</FONT>
</P>

<P><FONT SIZE=3D2>Best regards,</FONT>
</P>

<P><FONT SIZE=3D2>Renxiao Wang</FONT>
<BR><FONT SIZE=3D2>renxiao{at}med.umich.edu</FONT>
</P>
<BR>
<BR>

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From chemistry-request@ccl.net Thu May 29 09:45:33 2003
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Message-Id: <200305291345.h4TDjXgC007456{at}server.ccl.net>
From: "Paul Hawkins" <phawkins{at}tripos.com>
To: "Noriaki Ikuta" <noriaki_ikuta{at}yahoo.com>
Cc: <chemistry{at}ccl.net>
Date: Thu, 29 May 2003 09:44:44 -0400
Subject: RE: ic50 values in dtp aids dataset
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Noriaki,

I suspect the statement

"concentration of
compound that inhibits the growth of uninfected cells
by 50%"

is a typo. IC50 is the concentration of a compound required to reduce the
readout of the assay by 50%, whether you are measuring enzyme activity,
receptor activation or cell growth/division.
The classification into the different activity classes is somewhat
arbitrary. Generally speaking a compound having an IC50 greater than 10^-5
is not considered active as the doses required to achieve those
concentrations in an animal (let alone a human) would be huge. For
comparison most anti-HIV drugs on the market now have IC50's in this sort of
assay around 10^-6 and have IC50's against their target receptor (the
protease or reverse transcriptase mostly) in the 10^-9 range.
There may also be a known correlation between IC50's in this assay and doses
required to cause remission of infection in an animal model of HIV in humans
and again the maximum acceptable dose may translate to an IC50 in this assay
of 10^-5.
I am unaware of any papers on this dataset in particular though a good many
studies have used this dataset for various purposes.

One word of warning Log10HiConc should always be around 10x greater than the
IC50 so as the Log10HiConc approaches the reported IC50 the IC50 result
becomes less and less reliable.

Paul Hawkins
Applications Scientist
Tripos Inc
1699 South Hanley Road
St. Louis MO 63144

Ph: 617-899-4151
E-mail: phawkins{at}tripos.com

www.tripos.com

-----Original Message-----
From: Computational Chemistry List [mailto:chemistry-request{at}ccl.net]On
Behalf Of Noriaki Ikuta
Sent: Thursday, May 29, 2003 6:50 AM
To: chemistry{at}ccl.net
Cc: noriaki_ikuta{at}yahoo.com
Subject: CCL:ic50 values in dtp aids dataset



I have three questions regarding the DTP AIDS
Antiviral Screening dataset.
http://dtp.nci.nih.gov/docs/aids/aids_data.html

i) The explanation for the IC50 is "concentration of
compound that inhibits the growth of uninfected cells
by 50%" I do not understand this. I throught it would
be of interest to inhibit the virus or at least the
growth of infected cells?

ii) How is the conclusion active/inactive drawn from
those IC50 values?
I have included a few example entries with ConcUnit =
M in the mail.

HiConc - the highest concentration used in the dose
response
Flag -  when different experiments are averaged,
        "=" indicated that all the experiments reached
IC50
        ">" indicates that at least one of the
          experiments don't actually reach an EC50
          and the highest tested concentration is
          used for the value of IC50
IC50 - concentration of compound that inhibits the
growth of uninfected cells by 50%
Conclusion - CA active, CM moderately active, CI
inactive

NSC	Log10HiConc	Flag	Log10IC50	Conclusion
646607	-5.4	>	-5.42	CA
646607	-4.5	=	-5.29	CA
646607	-3.7	=	-5.79	CA
646609	-4.5	=	-5.78	CA
646609	-3.7	=	-5.61	CA
646610	-4.5	=	-5.77	CA
646610	-3.7	=	-5.88	CA
639762	-3.7	=	-4.75	CM
639762	-3.6	=	-4.88	CM
639763	-4.4	=	-4.63	CM
639765	-3.9	=	-4.69	CM
639766	-4.6	>	-4.79	CM
626162	-3.7	<	-7.2	CI
629266	-3.7	<	-7.2	CI
630958	-3.9	=	-4.74	CI
630959	-3.2	=	-3.85	CI
639915	-4.7	>	-4.7	CI
639975	-3.9	>	-5.05	CI
640064	-5	>	-5	CI
640064	-3.7	>	-3.7	CI


iii) Are there papers available explaining this
dataset in depth?


Noriaki

__________________________________
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From chemistry-request@ccl.net Thu May 29 09:57:54 2003
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From: "Shobe, Dave" <dshobe{at}sud-chemieinc.com>
To: "'Daniel R. Rohr'" <rohrd{at}students.uni-marburg.de>,
   ccl
	 <chemistry{at}ccl.net>
Subject: RE: Eigenvalues of hessian
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What I said earlier was made on the assumption of being at a =
stationalry
point. =20

I have always heard that a freq calculation is unreliable at =
non-stationary
points, but I don't remember (and perhaps I never knew) the reason for =
this
warning. =20

--David Shobe
S=FCd-Chemie Inc.
phone (502) 634-7409
fax     (502) 634-7724
email  dshobe{at}sud-chemieinc.com

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



-----Original Message-----
From: Daniel R. Rohr [mailto:rohrd{at}students.uni-marburg.de]
Sent: Thursday, May 29, 2003 5:54 AM
To: ccl
Subject: CCL:Eigenvalues of hessian


Hi CCLer

 Maybe I should clearify my question:
I do know that in the Hessians calculated, there is usually translation
and rotation. I want to avoid speaking of frequencies, because we are
talking about Hessians which are not necessarily calculated at
stationary points. That#s why I talk of the eigenvalues.
In an excat method there should be exactly 3N-6 nonzeroeigenvalues and =
6
exact zeros. ANY method I tested (HF, DFT and MP2) with ANY Program I
tested (Gaussian, Turbomole, Jaguar) gives me 3N nonzero Eigenvalues.
The question is now. Why are there too many nonzero Eigenvalues? In my
eyes there are two possible reasons:

1. The method is ok but there are errors made in the derivations of the
method. Maybe neglecting terms in the differentiation. Or maybe
asumptions that hold true only for stationary points.

2. The method is not ok. This means that I do get different Energies =
for
different orientations of my molecule (As is the case in DFT)

Of course it is also possible that there is a mixture of both. I would
like to know which error is the bigger one? And maybe get a reference
for this question.

Another point which I do not understand:
Some answers state that there is only little translation and rotation
since the frequencies are close to zero. Is the absolute value of an
eigenvalue a measure for the quantity (whaterver that means) of its
eigenvector???? And if that is the case why is there "more" translation
and rotation at nonstationary points? I get "frequencies" (this is
eigenvalues of the Hessian) between 400 and 850 cm^-1 for Water with HF
6-31G** (Gaussian calculation):

Low frequencies --- -410.8545   -0.0007   -0.0006    0.0017  489.4045
853.6142
 Low frequencies --- 1891.8502 3808.4304 3946.8117

These are of course the frequencies calculated BEFORE projection of
translation and rotation.

I hope you can help me on that

Daniel Rohr


Hi Daniel,

Your question is a bit tricky in that the answer depends on the method
you
are using.
=20
If you are calculating Hartree-Fock or MP2 hessians then I think you
should
get 6 zero eigenvalues and 3N-6 non-zero eigenvalues at a stationary
point.
Even if the hessian is obtained by numerical differentiation of
gradients
this should come out allright, otherwise the code is broken.

If you are doing a DFT calculation life typically gets a bit more
complicated. If the DFT hessian is implemented as a proper second
derivative
of the energy expression with respect to the nuclear coordinates you
should
still get 6 zero eigenvalues. However this requires that the code takes
the
2nd derivatives of the Becke weights (A.D. Becke, J.Chem.Phys. 88 =
(1988)
2547-2553) into account as well. Some codes don't bother calculating
these
terms in which case the strict translational invariance of the hessian
is
violated. This typically expresses itself in 3 additional non-zero but
small
valued eigenvalues.=20

If you are calculating the vibrational modes by numerical
differentiation of
DFT gradients then there may still be a problem if your molecule has
symmetry. Many quantum chemistry packages will reorientate your =
molecule
such that the main axes of ineratia coincide with the Cartesian axes of
your
coordinate system. This means that different points in the numerical
differentiation algorithm may be calculated at different orientations.
However, the DFT quadratures are not always invariant for rotations. =
For
example if you want to do calculations on H2 and you are going to use 6
points per H atom all placed on the Cartesian axes than the energy
you'll
get for the following two orientations will not be the same even if the
bond
distance is:

    H  H
    |   \
    H    H

Again this will lead to additional non-zero but small eigenvalues. In
this
case it may help to switch the use of symmetry off, so that all points
are
calculated in exactly the same orientation.=20

As you have given very little details about exactly which calculation
you
are doing I can not say for sure which of the above reasons is the most
like
cause. However I think it is most likely one of these and with some
experimentation and a good look at the documentation for your program
you
should be able to find out what is happening.

Best wishes,

   Huub van Dam

-----Original Message-----
From: Daniel R. Rohr
To: ccl
Sent: 5/28/03 3:20 PM
Subject: CCL:Eigenvalues of hessian

Hi CCLers

 Does anybody of you know, why there are more than 3N-6 nonzero
eigenvalues of the hessian? I am especially interested in the question,
whether this error is due to the errors made by differentiation or
whether they are due to an error within the method itself. I usually =
get
only 3 zero eigenvalues. No matter if the hessian is calculated on a
stationary point or not.

Thanks for your help

Daniel Rohr

--=20
-----------------------------------------------------------------------
 Daniel Rohr                                    Fachbereich Chemie der
                                                Philipps-Universitdt
 Tel.: +49-6421-28-25686                        Hans-Meerwein-Stra_e
 Fax.: +49-6421-28-25566                        D-35043 Marburg
 eMail: rohrd{at}stud-mailer.uni-marburg.de        Germany
-----------------------------------------------------------------------




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--=20
-----------------------------------------------------------------------
 Daniel Rohr                                    Fachbereich Chemie der
                                                Philipps-Universitdt
 Tel.: +49-6421-28-25686                        Hans-Meerwein-Stra_e
 Fax.: +49-6421-28-25566                        D-35043 Marburg
 eMail: rohrd{at}stud-mailer.uni-marburg.de        Germany
-----------------------------------------------------------------------




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<TITLE>RE: Eigenvalues of hessian</TITLE>
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<P><FONT SIZE=3D2>What I said earlier was made on the assumption of =
being at a stationalry point.&nbsp; </FONT>
</P>

<P><FONT SIZE=3D2>I have always heard that a freq calculation is =
unreliable at non-stationary points, but I don't remember (and perhaps =
I never knew) the reason for this warning.&nbsp; </FONT></P>

<P><FONT SIZE=3D2>--David Shobe</FONT>
<BR><FONT SIZE=3D2>S=FCd-Chemie Inc.</FONT>
<BR><FONT SIZE=3D2>phone (502) 634-7409</FONT>
<BR><FONT SIZE=3D2>fax&nbsp;&nbsp;&nbsp;&nbsp; (502) 634-7724</FONT>
<BR><FONT SIZE=3D2>email&nbsp; dshobe{at}sud-chemieinc.com</FONT>
</P>

<P><FONT SIZE=3D2>Don't bother flaming me: I'm behind a =
firewall.</FONT>
</P>
<BR>
<BR>

<P><FONT SIZE=3D2>-----Original Message-----</FONT>
<BR><FONT SIZE=3D2>From: Daniel R. Rohr [<A =
HREF=3D"mailto:rohrd{at}students.uni-marburg.de">mailto:rohrd{at}students.uni-=
marburg.de</A>]</FONT>
<BR><FONT SIZE=3D2>Sent: Thursday, May 29, 2003 5:54 AM</FONT>
<BR><FONT SIZE=3D2>To: ccl</FONT>
<BR><FONT SIZE=3D2>Subject: CCL:Eigenvalues of hessian</FONT>
</P>
<BR>

<P><FONT SIZE=3D2>Hi CCLer</FONT>
</P>

<P><FONT SIZE=3D2>&nbsp;Maybe I should clearify my question:</FONT>
<BR><FONT SIZE=3D2>I do know that in the Hessians calculated, there is =
usually translation</FONT>
<BR><FONT SIZE=3D2>and rotation. I want to avoid speaking of =
frequencies, because we are</FONT>
<BR><FONT SIZE=3D2>talking about Hessians which are not necessarily =
calculated at</FONT>
<BR><FONT SIZE=3D2>stationary points. That#s why I talk of the =
eigenvalues.</FONT>
<BR><FONT SIZE=3D2>In an excat method there should be exactly 3N-6 =
nonzeroeigenvalues and 6</FONT>
<BR><FONT SIZE=3D2>exact zeros. ANY method I tested (HF, DFT and MP2) =
with ANY Program I</FONT>
<BR><FONT SIZE=3D2>tested (Gaussian, Turbomole, Jaguar) gives me 3N =
nonzero Eigenvalues.</FONT>
<BR><FONT SIZE=3D2>The question is now. Why are there too many nonzero =
Eigenvalues? In my</FONT>
<BR><FONT SIZE=3D2>eyes there are two possible reasons:</FONT>
</P>

<P><FONT SIZE=3D2>1. The method is ok but there are errors made in the =
derivations of the</FONT>
<BR><FONT SIZE=3D2>method. Maybe neglecting terms in the =
differentiation. Or maybe</FONT>
<BR><FONT SIZE=3D2>asumptions that hold true only for stationary =
points.</FONT>
</P>

<P><FONT SIZE=3D2>2. The method is not ok. This means that I do get =
different Energies for</FONT>
<BR><FONT SIZE=3D2>different orientations of my molecule (As is the =
case in DFT)</FONT>
</P>

<P><FONT SIZE=3D2>Of course it is also possible that there is a mixture =
of both. I would</FONT>
<BR><FONT SIZE=3D2>like to know which error is the bigger one? And =
maybe get a reference</FONT>
<BR><FONT SIZE=3D2>for this question.</FONT>
</P>

<P><FONT SIZE=3D2>Another point which I do not understand:</FONT>
<BR><FONT SIZE=3D2>Some answers state that there is only little =
translation and rotation</FONT>
<BR><FONT SIZE=3D2>since the frequencies are close to zero. Is the =
absolute value of an</FONT>
<BR><FONT SIZE=3D2>eigenvalue a measure for the quantity (whaterver =
that means) of its</FONT>
<BR><FONT SIZE=3D2>eigenvector???? And if that is the case why is there =
&quot;more&quot; translation</FONT>
<BR><FONT SIZE=3D2>and rotation at nonstationary points? I get =
&quot;frequencies&quot; (this is</FONT>
<BR><FONT SIZE=3D2>eigenvalues of the Hessian) between 400 and 850 =
cm^-1 for Water with HF</FONT>
<BR><FONT SIZE=3D2>6-31G** (Gaussian calculation):</FONT>
</P>

<P><FONT SIZE=3D2>Low frequencies --- -410.8545&nbsp;&nbsp; =
-0.0007&nbsp;&nbsp; -0.0006&nbsp;&nbsp;&nbsp; 0.0017&nbsp; =
489.4045</FONT>
<BR><FONT SIZE=3D2>853.6142</FONT>
<BR><FONT SIZE=3D2>&nbsp;Low frequencies --- 1891.8502 3808.4304 =
3946.8117</FONT>
</P>

<P><FONT SIZE=3D2>These are of course the frequencies calculated BEFORE =
projection of</FONT>
<BR><FONT SIZE=3D2>translation and rotation.</FONT>
</P>

<P><FONT SIZE=3D2>I hope you can help me on that</FONT>
</P>

<P><FONT SIZE=3D2>Daniel Rohr</FONT>
</P>
<BR>

<P><FONT SIZE=3D2>Hi Daniel,</FONT>
</P>

<P><FONT SIZE=3D2>Your question is a bit tricky in that the answer =
depends on the method</FONT>
<BR><FONT SIZE=3D2>you</FONT>
<BR><FONT SIZE=3D2>are using.</FONT>
<BR><FONT SIZE=3D2>&nbsp;</FONT>
<BR><FONT SIZE=3D2>If you are calculating Hartree-Fock or MP2 hessians =
then I think you</FONT>
<BR><FONT SIZE=3D2>should</FONT>
<BR><FONT SIZE=3D2>get 6 zero eigenvalues and 3N-6 non-zero eigenvalues =
at a stationary</FONT>
<BR><FONT SIZE=3D2>point.</FONT>
<BR><FONT SIZE=3D2>Even if the hessian is obtained by numerical =
differentiation of</FONT>
<BR><FONT SIZE=3D2>gradients</FONT>
<BR><FONT SIZE=3D2>this should come out allright, otherwise the code is =
broken.</FONT>
</P>

<P><FONT SIZE=3D2>If you are doing a DFT calculation life typically =
gets a bit more</FONT>
<BR><FONT SIZE=3D2>complicated. If the DFT hessian is implemented as a =
proper second</FONT>
<BR><FONT SIZE=3D2>derivative</FONT>
<BR><FONT SIZE=3D2>of the energy expression with respect to the nuclear =
coordinates you</FONT>
<BR><FONT SIZE=3D2>should</FONT>
<BR><FONT SIZE=3D2>still get 6 zero eigenvalues. However this requires =
that the code takes</FONT>
<BR><FONT SIZE=3D2>the</FONT>
<BR><FONT SIZE=3D2>2nd derivatives of the Becke weights (A.D. Becke, =
J.Chem.Phys. 88 (1988)</FONT>
<BR><FONT SIZE=3D2>2547-2553) into account as well. Some codes don't =
bother calculating</FONT>
<BR><FONT SIZE=3D2>these</FONT>
<BR><FONT SIZE=3D2>terms in which case the strict translational =
invariance of the hessian</FONT>
<BR><FONT SIZE=3D2>is</FONT>
<BR><FONT SIZE=3D2>violated. This typically expresses itself in 3 =
additional non-zero but</FONT>
<BR><FONT SIZE=3D2>small</FONT>
<BR><FONT SIZE=3D2>valued eigenvalues. </FONT>
</P>

<P><FONT SIZE=3D2>If you are calculating the vibrational modes by =
numerical</FONT>
<BR><FONT SIZE=3D2>differentiation of</FONT>
<BR><FONT SIZE=3D2>DFT gradients then there may still be a problem if =
your molecule has</FONT>
<BR><FONT SIZE=3D2>symmetry. Many quantum chemistry packages will =
reorientate your molecule</FONT>
<BR><FONT SIZE=3D2>such that the main axes of ineratia coincide with =
the Cartesian axes of</FONT>
<BR><FONT SIZE=3D2>your</FONT>
<BR><FONT SIZE=3D2>coordinate system. This means that different points =
in the numerical</FONT>
<BR><FONT SIZE=3D2>differentiation algorithm may be calculated at =
different orientations.</FONT>
<BR><FONT SIZE=3D2>However, the DFT quadratures are not always =
invariant for rotations. For</FONT>
<BR><FONT SIZE=3D2>example if you want to do calculations on H2 and you =
are going to use 6</FONT>
<BR><FONT SIZE=3D2>points per H atom all placed on the Cartesian axes =
than the energy</FONT>
<BR><FONT SIZE=3D2>you'll</FONT>
<BR><FONT SIZE=3D2>get for the following two orientations will not be =
the same even if the</FONT>
<BR><FONT SIZE=3D2>bond</FONT>
<BR><FONT SIZE=3D2>distance is:</FONT>
</P>

<P><FONT SIZE=3D2>&nbsp;&nbsp;&nbsp; H&nbsp; H</FONT>
<BR><FONT SIZE=3D2>&nbsp;&nbsp;&nbsp; |&nbsp;&nbsp; \</FONT>
<BR><FONT SIZE=3D2>&nbsp;&nbsp;&nbsp; H&nbsp;&nbsp;&nbsp; H</FONT>
</P>

<P><FONT SIZE=3D2>Again this will lead to additional non-zero but small =
eigenvalues. In</FONT>
<BR><FONT SIZE=3D2>this</FONT>
<BR><FONT SIZE=3D2>case it may help to switch the use of symmetry off, =
so that all points</FONT>
<BR><FONT SIZE=3D2>are</FONT>
<BR><FONT SIZE=3D2>calculated in exactly the same orientation. </FONT>
</P>

<P><FONT SIZE=3D2>As you have given very little details about exactly =
which calculation</FONT>
<BR><FONT SIZE=3D2>you</FONT>
<BR><FONT SIZE=3D2>are doing I can not say for sure which of the above =
reasons is the most</FONT>
<BR><FONT SIZE=3D2>like</FONT>
<BR><FONT SIZE=3D2>cause. However I think it is most likely one of =
these and with some</FONT>
<BR><FONT SIZE=3D2>experimentation and a good look at the documentation =
for your program</FONT>
<BR><FONT SIZE=3D2>you</FONT>
<BR><FONT SIZE=3D2>should be able to find out what is happening.</FONT>
</P>

<P><FONT SIZE=3D2>Best wishes,</FONT>
</P>

<P><FONT SIZE=3D2>&nbsp;&nbsp; Huub van Dam</FONT>
</P>

<P><FONT SIZE=3D2>-----Original Message-----</FONT>
<BR><FONT SIZE=3D2>From: Daniel R. Rohr</FONT>
<BR><FONT SIZE=3D2>To: ccl</FONT>
<BR><FONT SIZE=3D2>Sent: 5/28/03 3:20 PM</FONT>
<BR><FONT SIZE=3D2>Subject: CCL:Eigenvalues of hessian</FONT>
</P>

<P><FONT SIZE=3D2>Hi CCLers</FONT>
</P>

<P><FONT SIZE=3D2>&nbsp;Does anybody of you know, why there are more =
than 3N-6 nonzero</FONT>
<BR><FONT SIZE=3D2>eigenvalues of the hessian? I am especially =
interested in the question,</FONT>
<BR><FONT SIZE=3D2>whether this error is due to the errors made by =
differentiation or</FONT>
<BR><FONT SIZE=3D2>whether they are due to an error within the method =
itself. I usually get</FONT>
<BR><FONT SIZE=3D2>only 3 zero eigenvalues. No matter if the hessian is =
calculated on a</FONT>
<BR><FONT SIZE=3D2>stationary point or not.</FONT>
</P>

<P><FONT SIZE=3D2>Thanks for your help</FONT>
</P>

<P><FONT SIZE=3D2>Daniel Rohr</FONT>
</P>

<P><FONT SIZE=3D2>-- </FONT>
<BR><FONT =
SIZE=3D2>---------------------------------------------------------------=
--------</FONT>
<BR><FONT SIZE=3D2>&nbsp;Daniel =
Rohr&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&n=
bsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&n=
bsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp; =
Fachbereich Chemie der</FONT>
<BR><FONT =
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sp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nb=
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sp; Philipps-Universitdt</FONT>
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<BR>
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<P><FONT SIZE=3D2>-- </FONT>
<BR><FONT =
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--------</FONT>
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Rohr&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&n=
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From chemistry-request@ccl.net Thu May 29 10:15:03 2003
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Date: Thu, 29 May 2003 10:18:15 -0400
From: elewars <elewars{at}trentu.ca>
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To: Leif Laaksonen <leif.laaksonen{at}csc.fi>, chemistry{at}ccl.net
Subject: Re: CCL:Orbitals
References: <003801c32546$68145fd0$bb1c7b0a@ISOSIRRI>
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2003 May 29

Hello,

So you are saying that there is a one-to-one correspondence between physically real things X and
QM operators X^ , the average value of the thing X for a system being the integral of the system's
wavefunction over the operator. So orbitals are real only if there is, mathematically, an orbital
operator PSI^--which there is not (?). Good point.

EL
======

Leif Laaksonen wrote:

> Hi,
>
> I might remember wrong from my primary courses in quantum chemistry
> that only obsrvables are the expectation values from the wave
> function!
>
> This means that while the wave function (|P>) as such is not
> observable the expectation value of property X is (<P|X|P>).
>
> Regards,
>
> -leif
>
> -----Original Message-----
> From: Computational Chemistry List [mailto:chemistry-request{at}ccl.net] On Behalf Of Guosheng Wu
> Sent: Wednesday, May 28, 2003 7:46 PM
> To: chemistry{at}ccl.net
> Subject: CCL:Orbitals
>
> > > > --- elewars <elewars{at}trentu.ca> wrote:
> > > > > 2003 May 28
> > > > >
> > > > > Are MOs physically real? This is a meaningful question only if there is some
> > > > > experiment or observation that could provide an answer _yes_ or _no_.  Is there,
> > > > > at least in principle, such an experiment or observation?
>
> > > Guosheng Wu wrote:
> > >
> > > > MO is just a useful mathematical tool for quantum chemistry/physics, and
> > > > it seems to me itself does not have much physical meaning.
> > > >
> > > > However, many properties from MOs are meaningful and can be observed
> > > > by exmperiments: such as the square of absolute MOs (|MO|^2) corresponding
> > > > to the electronic density. Things like |MO|^2 of d-orbitals were published
> > > > in a Science article last one or a few years.
>
> > --- elewars <elewars{at}trentu.ca> wrote:
> > > Hello,
> > >
> > > Thanks for your ideas. If photoel. spectra (and Koopmans theorem--in this case the
> > > second MO is at the ionization limit) really measure the energy difference of two MOs,
> > > then MOs exist!
> > >
> > > In any case, it is an interesting discussion.
> > >
> > > EL
> > > =====
>
> The properties from |MO|^2 exist does not really mean MO exists.
>
> When we know some properties from x^2 exist and can be measured,
> this does not mean x exists and can be measured.
>
> For example, what does the complex number(i) mean in the real world?
> Measurable? Not really, but obviously it's a useful mathematical tool
> for lots of applications. Certainly (i^2=-1) means something. Right?
>
> Related issue for absolute energy: energy difference is measurable
> by many kind of experiments, but not for the absolute energy.
>
> This may lead to some kind of philosophical problem, if one has
> such a taste.
>
> Guosheng
>
> __________________________________
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From chemistry-request@ccl.net Thu May 29 11:29:19 2003
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Date: Thu, 29 May 2003 08:28:26 -0700
To: Philip Stortz <madscientist:at:wyoming.com>
From: David Gallagher <dgallagher:at:cachesoftware.com>
Subject: Re: CCL:Crystal building tools
Cc: chemistry:at:ccl.net
In-Reply-To: <3ED5A324.B8CC04AE:at:wyoming.com>
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Hi Phil,

For building crystals there is a special crystal builder in CAChe complete 
with all 230 space groups. Indeed, the drawing tool was never intended to 
build crystal structures. The crystal builder, which was recently updated 
to handle larger systems, requires only the space group, cell parameters, 
and fractional coordinates, then you can specify as many unit cells as you 
wish. If you send us your crystal data, we'll build the crystal for you and 
send it back in the format you specify.

David Gallagher, Fujitsu.


At 12:05 AM 5/29/2003 -0600, Philip Stortz wrote:
>To help with modeling electronic spectra of crystals, is there a good 
>package out there to build the initial crystal with at least a couple 
>dozen unit cells if i know the crystal structure?  I've tried this with 
>Cache a few years ago, and the drawing tool was not very useful and very 
>painful for building 3d crystals, bonds often wound up in odd places where 
>i didn't mean to put them and it was very hard to view the bonds to see 
>these problems.  Thanks again.
>
>--
>Philip Stortz -- To be nobody but yourself when the whole world is trying 
>its best night and day to make you everybody else is to fight the hardest 
>battle any human being will ever fight. -- E.E. Cummings
>
>
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From chemistry-request@ccl.net Thu May 29 11:16:47 2003
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Date: Thu, 29 May 2003 11:16:39 -0400
From: "Qadir K.Timerghazin" <Qadir.Timerghazin:at:CERMM.Concordia.CA>
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Message-ID: <96266648750.20030529111639:at:cermm.concordia.ca>
To: "'CCL'" <chemistry:at:ccl.net>
Subject: Re: CCL:calculating atomic charges with AIMPAC
In-Reply-To: <5CF08BBFE6DE97478C1E76E654CAF90801BC0BF1:at:lvlxch02.ntdomain.americas.sc-world.com>
References: 
 <5CF08BBFE6DE97478C1E76E654CAF90801BC0BF1:at:lvlxch02.ntdomain.americas.sc-world.com>
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Which integration algorithm are you using?
PROAIM is much faster than PROMEGA, but if something goes wrong, I
recommend to compare the results with PROMEGA.
And, of course, always check if your integrated L values are small
enough (at least 10e-3)

-- 
     Qadir                      mailto:Qadir.Timerghazin:at:CERMM.Concordia.CA

SD> But a charge of -20 almost certainly is the result of assigning the
SD> electrons of one atom's basin to another atom.  Something which occurs as a
SD> result of the program failing to find the boundary between them.  

SD> At any rate, I would try a 2nd AIM calculation program if one is available,
SD> before giving up.  E.g., I often find Gaussian's AIM code halts with a
SD> (usually cryptic) error message, but for the same molecule AIM2000 may
SD> complete the calculation with no problem.



SD> -----Original Message-----
SD> From: Wai-To Chan [mailto:chan:at:curl.gkcl.yorku.ca]
SD> Sent: Thursday, May 29, 2003 2:09 AM
SD> To: chemistry:at:ccl.net
SD> Subject: CCL:calculating atomic charges with AIMPAC


SD> <<<<<<<<<<<<<<<<<<<<<<<<<<<<<<<<<
SD> I currently have an undergraduate student who is attempting to compare 
SD> charges of methylated benzene and ferrocene systems using the AIMPAC 
SD> software.  In the case of hexamethyl benzene and the ferrocene analogues he 
SD> is getting very large negative charges on some the ring carbons (-5 to -20) 
SD> and small positive charges on iron (0.5) Can anyone tell me if there is a 
SD> problem with the program or if the ring system can not be treated with this 
SD> method?
>>>>>>>>>>>>>>>>>>>>>>>>>>>>>>>>


SD>    I remember reading about the tendency of AIM changes to be larger in
SD> magnitude
SD> than expected on the basis of chemical intuition. There is a paper by
SD> Kenneth Wiberg from the early 90s in J. comp. chem. about the comparison of 
SD> several atomic-charge partitioning scheme including Bader's you may find
SD> useful. 
SD> You may also consider using the Natural atomic charges method if you want 
SD> faster and less 'surprising' results. 

SD> Wai-To Chan



SD> To send e-mail to subscribers of CCL put the string CCL: on your Subject:
SD> line

SD> Send your subscription/unsubscription requests to: CHEMISTRY-REQUEST:at:ccl.net



****************************************************************************
Qadir K. Timerghazin                 * Kadyr K. Timergazine
Centre for Research                  * Centre de Recherche en
in Molecular Modeling                * Modilisation Moliculaire
                                     *
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From chemistry-request@ccl.net Thu May 29 11:09:27 2003
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Subject: Re: CCL:Electronic Spectra of inorganic crystals
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To: Philip Stortz <madscientist:at:wyoming.com>
From: Geoff Hutchison <hutchisn:at:chem.northwestern.edu>
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On Thursday, May 29, 2003, at 01:00  AM, Philip Stortz wrote:

> Time for my annual hopeful question, is there currently a program that 
> calculates electronic spectra of inorganic crystals (and their 
> surfaces) with any accuracy?

I have little experience in these calculations, but do collaborate with 
a solid-state physics group that calculates semiconductor band 
structures all the time. The state-of-the-art AFAIK, are 
"screened-exchange" DFT band codes, or GW calculations. These produce 
band structues and optical properties of crystals and "slabs" at 
surfaces to a high degree of accuracy.

(Hmm, I probably have papers on those somewhere around here, so please 
ask if you want more details. Or do a search on "Prof. Arthur Freeman" 
at Northwestern, and you'll turn up this group.)

But you also said "trends" were OK, in which case, most DFT band 
structure codes should do what you want with no problem (e.g. DMol3, 
which I've used, FLAPW, or Wein2K, etc.) The band gap is usually given 
in eV directly from the calculation.

Regards,
-Geoff

--
-Geoff Hutchison		<hutchisn:at:chem.northwestern.edu>
Ratner/Marks Groups	(847) 491-3295
Northwestern Chemistry	http://www.chem.northwestern.edu/



From chemistry-request@ccl.net Thu May 29 12:04:39 2003
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From: "Shobe, Dave" <dshobe(at)sud-chemieinc.com>
To: "'Guosheng Wu'" <wu_guosheng2002(at)yahoo.com>,
   "'Renxiao Wang'"
	 <renxiao(at)med.umich.edu>, "'CCL'" <chemistry(at)ccl.net>
Subject: RE: CCL:A question on heat of formation
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---Guosheng Wu wrote:
> It seems to me, dH has not much to do with propabilities of all
conformations,
> which is essentially entropy contribution.=20

There is a small effect on enthalpy, for temperatures above zero =
Kelvin.
Most people ignore it, since there are more important sources of error. =
 But
I think the NIST/JANAF tables do take this effect into account.  It may
affect dH/dT more than it affects dH itself.

--David Shobe
S=FCd-Chemie Inc.
phone (502) 634-7409
fax     (502) 634-7724
email  dshobe(at)sud-chemieinc.com

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



-----Original Message-----
From: Guosheng Wu [mailto:wu_guosheng2002(at)yahoo.com]
Sent: Thursday, May 29, 2003 11:20 AM
To: Shobe, Dave; 'Renxiao Wang'
Subject: Re: CCL:A question on heat of formation


Were you talking about free energy(dG), instead of heat of formation =
(dH)?

It seems to me, dH has not much to do with propabilities of all
conformations,
which is essentially entropy contribution.=20

BTW, John Pople and others had a few papers on Gn theory to get very =
high
quality
heat of formation for a small molecule, by ab initio plus scaling
strategy... but
obviously not interested to most of the Med. Chem. community.=20

Guosheng

--- "Shobe, Dave" <dshobe(at)sud-chemieinc.com> wrote:
> Most people do the following.  They find the lowest-energy =
conformations
of
> the molecules involved, and use the energy at those geometries to
calculate
> delta-H.  The computational chemist should of course use any prudent,
> reasonable means to ensure that these are indeed the *global*
conformational
> minima.
>=20
> However...
>=20
> I think to really "do it right" one has to calculate all the =
low-lying
> conformations and determine the relative statistical-mechanical
populations
> of each conformation, and from that the average enthalpy per molecule =
(or
> per mole). =20
>=20
> Usually there are enough other sources of error that the correct =
procedure
> has little advantage over the first approach, at least for enthalpy.  =
But
> the corresponding "correct" procedure is often done for entropy, =
where
> population of low-lying conformational isomers can make a significant
> difference in the outcome.
>=20
> --David Shobe
> S=FCd-Chemie Inc.
> phone (502) 634-7409
> fax     (502) 634-7724
> email  dshobe(at)sud-chemieinc.com
>=20
> Don't bother flaming me: I'm behind a firewall.
>=20
>=20
>=20
>=20
> -----Original Message-----
> From: Renxiao Wang [mailto:renxiao(at)med.umich.edu]
> Sent: Wednesday, May 28, 2003 8:19 PM
> To: chemistry(at)ccl.net
> Subject: CCL:A question on heat of formation
>=20
>=20
> Hi, CCLers!
>=20
> Should the heat of formations of two enantiomers of a chiral compound =
be
> identical? I think the answer is yes. Please point out some =
references
> for this.=20
>=20
> A disturbing fact is that, no matter you use QM or MM to calculate =
the
> heat of formation for a given molecule, the number is
> conformation-depentdent. I guess this is because of the steric energy
> part is conformation-dependent. So, if I really want to compare the
> stability of two molecules using heat of formation, how may I =
calculate
> it right?
>=20
> Best regards,
>=20
> Renxiao Wang
> renxiao(at)med.umich.edu
>=20
>=20
>=20
> -=3D This is automatically added to each message by mailing script =
=3D-
> To send e-mail to subscribers of CCL put the string CCL: on your =
Subject:
> line
>=20
> Send your subscription/unsubscription requests to:
CHEMISTRY-REQUEST(at)ccl.net
>=20
> HOME Page: http://www.ccl.net   | Jobs Page: http://www.ccl.net/jobs=20
>=20
>=20
>=20
>=20
>=20
>=20
>=20


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<TITLE>RE: CCL:A question on heat of formation</TITLE>
</HEAD>
<BODY>
<BR>

<P><FONT SIZE=3D2>---Guosheng Wu wrote:</FONT>
<BR><FONT SIZE=3D2>&gt; It seems to me, dH has not much to do with =
propabilities of all conformations,</FONT>
<BR><FONT SIZE=3D2>&gt; which is essentially entropy contribution. =
</FONT>
</P>

<P><FONT SIZE=3D2>There is a small effect on enthalpy, for temperatures =
above zero Kelvin.&nbsp; Most people ignore it, since there are more =
important sources of error.&nbsp; But I think the NIST/JANAF tables do =
take this effect into account.&nbsp; It may affect dH/dT more than it =
affects dH itself.</FONT></P>

<P><FONT SIZE=3D2>--David Shobe</FONT>
<BR><FONT SIZE=3D2>S=FCd-Chemie Inc.</FONT>
<BR><FONT SIZE=3D2>phone (502) 634-7409</FONT>
<BR><FONT SIZE=3D2>fax&nbsp;&nbsp;&nbsp;&nbsp; (502) 634-7724</FONT>
<BR><FONT SIZE=3D2>email&nbsp; dshobe(at)sud-chemieinc.com</FONT>
</P>

<P><FONT SIZE=3D2>Don't bother flaming me: I'm behind a =
firewall.</FONT>
</P>
<BR>
<BR>

<P><FONT SIZE=3D2>-----Original Message-----</FONT>
<BR><FONT SIZE=3D2>From: Guosheng Wu [<A =
HREF=3D"mailto:wu_guosheng2002(at)yahoo.com">mailto:wu_guosheng2002@yahoo.c=
om</A>]</FONT>
<BR><FONT SIZE=3D2>Sent: Thursday, May 29, 2003 11:20 AM</FONT>
<BR><FONT SIZE=3D2>To: Shobe, Dave; 'Renxiao Wang'</FONT>
<BR><FONT SIZE=3D2>Subject: Re: CCL:A question on heat of =
formation</FONT>
</P>
<BR>

<P><FONT SIZE=3D2>Were you talking about free energy(dG), instead of =
heat of formation (dH)?</FONT>
</P>

<P><FONT SIZE=3D2>It seems to me, dH has not much to do with =
propabilities of all conformations,</FONT>
<BR><FONT SIZE=3D2>which is essentially entropy contribution. </FONT>
</P>

<P><FONT SIZE=3D2>BTW, John Pople and others had a few papers on Gn =
theory to get very high quality</FONT>
<BR><FONT SIZE=3D2>heat of formation for a small molecule, by ab initio =
plus scaling strategy... but</FONT>
<BR><FONT SIZE=3D2>obviously not interested to most of the Med. Chem. =
community. </FONT>
</P>

<P><FONT SIZE=3D2>Guosheng</FONT>
</P>

<P><FONT SIZE=3D2>--- &quot;Shobe, Dave&quot; =
&lt;dshobe(at)sud-chemieinc.com&gt; wrote:</FONT>
<BR><FONT SIZE=3D2>&gt; Most people do the following.&nbsp; They find =
the lowest-energy conformations of</FONT>
<BR><FONT SIZE=3D2>&gt; the molecules involved, and use the energy at =
those geometries to calculate</FONT>
<BR><FONT SIZE=3D2>&gt; delta-H.&nbsp; The computational chemist should =
of course use any prudent,</FONT>
<BR><FONT SIZE=3D2>&gt; reasonable means to ensure that these are =
indeed the *global* conformational</FONT>
<BR><FONT SIZE=3D2>&gt; minima.</FONT>
<BR><FONT SIZE=3D2>&gt; </FONT>
<BR><FONT SIZE=3D2>&gt; However...</FONT>
<BR><FONT SIZE=3D2>&gt; </FONT>
<BR><FONT SIZE=3D2>&gt; I think to really &quot;do it right&quot; one =
has to calculate all the low-lying</FONT>
<BR><FONT SIZE=3D2>&gt; conformations and determine the relative =
statistical-mechanical populations</FONT>
<BR><FONT SIZE=3D2>&gt; of each conformation, and from that the average =
enthalpy per molecule (or</FONT>
<BR><FONT SIZE=3D2>&gt; per mole).&nbsp; </FONT>
<BR><FONT SIZE=3D2>&gt; </FONT>
<BR><FONT SIZE=3D2>&gt; Usually there are enough other sources of error =
that the correct procedure</FONT>
<BR><FONT SIZE=3D2>&gt; has little advantage over the first approach, =
at least for enthalpy.&nbsp; But</FONT>
<BR><FONT SIZE=3D2>&gt; the corresponding &quot;correct&quot; procedure =
is often done for entropy, where</FONT>
<BR><FONT SIZE=3D2>&gt; population of low-lying conformational isomers =
can make a significant</FONT>
<BR><FONT SIZE=3D2>&gt; difference in the outcome.</FONT>
<BR><FONT SIZE=3D2>&gt; </FONT>
<BR><FONT SIZE=3D2>&gt; --David Shobe</FONT>
<BR><FONT SIZE=3D2>&gt; S=FCd-Chemie Inc.</FONT>
<BR><FONT SIZE=3D2>&gt; phone (502) 634-7409</FONT>
<BR><FONT SIZE=3D2>&gt; fax&nbsp;&nbsp;&nbsp;&nbsp; (502) =
634-7724</FONT>
<BR><FONT SIZE=3D2>&gt; email&nbsp; dshobe(at)sud-chemieinc.com</FONT>
<BR><FONT SIZE=3D2>&gt; </FONT>
<BR><FONT SIZE=3D2>&gt; Don't bother flaming me: I'm behind a =
firewall.</FONT>
<BR><FONT SIZE=3D2>&gt; </FONT>
<BR><FONT SIZE=3D2>&gt; </FONT>
<BR><FONT SIZE=3D2>&gt; </FONT>
<BR><FONT SIZE=3D2>&gt; </FONT>
<BR><FONT SIZE=3D2>&gt; -----Original Message-----</FONT>
<BR><FONT SIZE=3D2>&gt; From: Renxiao Wang [<A =
HREF=3D"mailto:renxiao(at)med.umich.edu">mailto:renxiao(at)med.umich.edu</A>]<=
/FONT>
<BR><FONT SIZE=3D2>&gt; Sent: Wednesday, May 28, 2003 8:19 PM</FONT>
<BR><FONT SIZE=3D2>&gt; To: chemistry(at)ccl.net</FONT>
<BR><FONT SIZE=3D2>&gt; Subject: CCL:A question on heat of =
formation</FONT>
<BR><FONT SIZE=3D2>&gt; </FONT>
<BR><FONT SIZE=3D2>&gt; </FONT>
<BR><FONT SIZE=3D2>&gt; Hi, CCLers!</FONT>
<BR><FONT SIZE=3D2>&gt; </FONT>
<BR><FONT SIZE=3D2>&gt; Should the heat of formations of two =
enantiomers of a chiral compound be</FONT>
<BR><FONT SIZE=3D2>&gt; identical? I think the answer is yes. Please =
point out some references</FONT>
<BR><FONT SIZE=3D2>&gt; for this. </FONT>
<BR><FONT SIZE=3D2>&gt; </FONT>
<BR><FONT SIZE=3D2>&gt; A disturbing fact is that, no matter you use QM =
or MM to calculate the</FONT>
<BR><FONT SIZE=3D2>&gt; heat of formation for a given molecule, the =
number is</FONT>
<BR><FONT SIZE=3D2>&gt; conformation-depentdent. I guess this is =
because of the steric energy</FONT>
<BR><FONT SIZE=3D2>&gt; part is conformation-dependent. So, if I really =
want to compare the</FONT>
<BR><FONT SIZE=3D2>&gt; stability of two molecules using heat of =
formation, how may I calculate</FONT>
<BR><FONT SIZE=3D2>&gt; it right?</FONT>
<BR><FONT SIZE=3D2>&gt; </FONT>
<BR><FONT SIZE=3D2>&gt; Best regards,</FONT>
<BR><FONT SIZE=3D2>&gt; </FONT>
<BR><FONT SIZE=3D2>&gt; Renxiao Wang</FONT>
<BR><FONT SIZE=3D2>&gt; renxiao(at)med.umich.edu</FONT>
<BR><FONT SIZE=3D2>&gt; </FONT>
<BR><FONT SIZE=3D2>&gt; </FONT>
<BR><FONT SIZE=3D2>&gt; </FONT>
<BR><FONT SIZE=3D2>&gt; -=3D This is automatically added to each =
message by mailing script =3D-</FONT>
<BR><FONT SIZE=3D2>&gt; To send e-mail to subscribers of CCL put the =
string CCL: on your Subject:</FONT>
<BR><FONT SIZE=3D2>&gt; line</FONT>
<BR><FONT SIZE=3D2>&gt; </FONT>
<BR><FONT SIZE=3D2>&gt; Send your subscription/unsubscription requests =
to: CHEMISTRY-REQUEST(at)ccl.net</FONT>
<BR><FONT SIZE=3D2>&gt; </FONT>
<BR><FONT SIZE=3D2>&gt; HOME Page: <A HREF=3D"http://www.ccl.net" =
TARGET=3D"_blank">http://www.ccl.net</A>&nbsp;&nbsp; | Jobs Page: <A =
HREF=3D"http://www.ccl.net/jobs" =
TARGET=3D"_blank">http://www.ccl.net/jobs</A> </FONT>
<BR><FONT SIZE=3D2>&gt; </FONT>
<BR><FONT SIZE=3D2>&gt; </FONT>
<BR><FONT SIZE=3D2>&gt; </FONT>
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<BR><FONT SIZE=3D2>&gt; </FONT>
<BR><FONT SIZE=3D2>&gt; </FONT>
<BR><FONT SIZE=3D2>&gt; </FONT>
</P>
<BR>

<P><FONT SIZE=3D2>__________________________________</FONT>
<BR><FONT SIZE=3D2>Do you Yahoo!?</FONT>
<BR><FONT SIZE=3D2>Yahoo! Calendar - Free online calendar with sync to =
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From chemistry-request@ccl.net Thu May 29 11:49:20 2003
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Subject: Optimization in Gamess and in Gaussian
Message-ID: <1054223354.3ed62bfae75de(at)webmail.u-picardie.fr>
Date: Thu, 29 May 2003 17:49:14 +0200 (CEST)
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Dear All,

I am interested in better understanding the optimization procedure implemented 
in Gamess & Gaussian. In Gaussian, the optimization accuracy is controlled by 
the OPT keyword. Gaussian checks four parameters: the "Maximum Force", "RMS 
Force", "Maximum Displacement" and "RMS Displacement". From the numerous tests 
I ran using Gaussian, the "Maximum Displacement" and "RMS Displacement" 
thresholds are far MORE difficult to reach than the "Maximum Force" and "RMS 
Force" ones. Thus, after some optimization steps, the "Maximum Force" and "RMS 
Force" thresholds are usually satisfied. On the contrary, to satisfy the 2 
other ones (related to the "Displacement"), this demands a certain numbers of 
additional optimization steps...

- In GAMESS, the optimization is controlled by the OPTTOL keyword. The 
optimization is stopped when the "Maximum gradient" and the "RMS gradient" are 
below the demanded threshold value. It means (to me) that the "Maximum 
Displacement" and the "RMS Displacement" are NOT checked by GAMESS. Am I right ?

- Since the two "Displacement" thresholds are the MOST difficult criterions to 
be satisfied in Gaussian and as they are NOT checked by GAMESS (from what I 
understand), what are the implications of such differences in the optimization 
accuracy in GAMESS ?

Thank you very much, best regards, Francois




From chemistry-request@ccl.net Thu May 29 13:00:37 2003
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Date: Thu, 29 May 2003 18:00:29 +0100
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From: "Dr. Julia Metzker" <jm45|at|york.ac.uk>
Subject: calculating atomic charges with AIMPAC
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In reading the responses to my previous enquiry I decided I should probably 
include some more information.  The student working on this project has 
used G98 to generate the wavefunction file and is using the PROAIMV method 
of calculating the charges for methyl substituted benzenes and 
ferrocenes.  He has used an all electron basis  set in all of the 
calculation.  He has had success in all cases for benzene except hexamethyl 
benzene where he gets very large negative charges on some of the methyl 
carbons and methyl hydrogens.  I have looked at his wfn file and it indeed 
shows 45 doubly occupied molecular orbitals as expected.  I have also 
noticed that the N value (which I am assuming is the number of electrons 
associated with the atom) ranges from 6.5-7.5 for the atoms with large 
negative charges. and the L value is relatively large (10^-1 to `0 ^-2)  I 
have not yet tried the PROMEGA option.


I have two questions, really.

Can anyone tell me what the various information in the crt file means

and is there a simple way to figure out what is causing the very large charges?


The total charge does not add up to 0 as expected.  It is equal to -35.

I have included the relevant responses to my last email below

Thank you,
Julia Metzker



Dear Dr. Metzker,

It looks like you need to tightens the integration parameters in
"PROAIMV" and use the "PROMEGA" option (which seldom fails, but
slower of course) rather the usual option of "PROAIM" within the input
files (.inp).

To have an idea of the magnitudes of the charged on a Titanocene
moiety, perhaps you may wish to have a look at:

Bader RFW, Matta CF. Bonding to titanium. Inorg. Chem. 2001;40:5603-5611.

Best of luck,

Sincerely,

   Cherif

   -----------------------------------------
   Chirif F. Matta, Ph.D.
   Chemistry Department, University of Toronto,
   Toronto, Ontario, Canada M5S 3H6.
   Telephone:      (416) 978 - 3625
   Fax:            (416) 978 - 7580
   Web Site: http://chem.utoronto.ca/~cmatta/
   ------------------------------------------


I don't have any experience doing AIMPAC calcs, but I've read plenty of 
papers describing the calcs.

The charges on C seem unrealistic. The sum of the atomic charges must be 
the same as the molecular charge. If you have a neutral molecule that 
contains some highly negatively charged atoms, it must also contain some 
highly positively charged atoms. You didn't mention the latter, so I 
suspect that something was set up incorrectly.

Good luck,

-Alan

====
Alan Shusterman
Department of Chemistry
Reed College
Portland, OR

Hello,
Though I do not know which method you are using to get the wavefunction,
I would blame first to the quality of the wavefunction than to the aimpac
program. Check the boundaries of the carbon atoms to see if the atomic
basin is what you expect to be.
Hope it helps

_-_-_-_-_-_-_-_-_-_-_-_-

    Carlos Silva Lspez
  Dept. Qummica Organica
   Universidade de Vigo
   Phone:0034 986812226
-_-_-_-_-_-_-_-_-_-_-_-_


Hi,

   I just read your email on the CCL. My first question is what software are
you using to calculate the charges, proaimv, gaussian's implementation or
Kunig's AIM200?. The second question is how did you generate the wave
funcion, hf, dft, basis set. Best,

f

   Fernando Martmn,
      Plexxikon
      91 Bolivar Drive, Suite A
      Berkeley, CA 94710, USA
      510.647.4014 (phone)  510.548.8014 (fax)

Dear Julia,

These types of systems can be problematic if the topology of the density is
complex.  For example, are you certain that you've successfully identified the
ring and cage critical points in the ferrocene case (particularly) and assigned
them to the associated bond and ring critical points, 
respectively?  Problems in
this area can lead to the "overintegration" problems that you've described.

Curt Breneman
RPI Chemistry



--- You wrote:
The charges actually do not add to 0, indicating a problem somewhere, but I 
don't know where.
--- end of quote ---

This is definitely a problem if your molecules are neutral.

First, double-check the original wavefn/energy calculation. Perhaps the 
total charge was defined incorrectly.

Second, check your basis set. It is quite common to use effective core 
potentials (ECP) with organometallic compounds like ferrocene. If you used 
an ECP basis set, you have effectively deleted some or all of the core 
electrons from your wavefn. When you use this wavefn to calculate atomic 
charges you might get unrealistic results (but I would expect to see large 
*positive* charges due to the missing electrons, and not large negative 
charges).

Third, see if the wavefn and orbital occupancy info is being transferred 
correctly to AIMPAC. Perhaps AIMPAC thinks the wrong number of orbitals are 
populated?

Good luck,

-Alan

====

Alan Shusterman
Department of Chemistry
Reed College
3203 S.E. Woodstock Blvd.
Portland, OR 97202-8199
503-517-7699

   Dear Julia - have you checked the quality of the integrations? This is
usually best done with the number reported as "L" (I think the fourth
quantity output by proaimv). This is the value of the Laplacian integrated
over the atomic basin, which should vanish - values of 10^-3 are
borderline OK, lower is obviously better. Also check that the total
populations add up to the no. electrons in your system.

   For a system like ferrocene, with rings (and cages?), you might need to
tweak some of the surface-tracing paramaters - see the top of the
proaimv.f code.

   If this isn't the source of your problem, you could try the integration
methods in Gaussian (disappointing in my experience) or Popelier's
MORPHY, which is generally very robust.

   Hope this helps - Jamie




From chemistry-request@ccl.net Thu May 29 13:34:30 2003
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Date: Thu, 29 May 2003 19:34:01 +0200 (METDST)
From: Victor Lua~na <pueyo<<at>>pinon.ccu.uniovi.es>
Subject: Re:  CCL:'electron density' vs 'electronic configurations'...
To: chemistry<<at>>ccl.net, owner-chemistry<<at>>ccl.net
Cc: pueyo<<at>>pinon.ccu.uniovi.es
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> From: Roy Jensen <royj<<at>>uvic.ca>
> Date: Mon, 26 May 2003 00:47:58 -0700
> The following came up recently and we could not come to a conclusion.
>
> One premise behind DFT is that a _single_ electron density completely
> describes each electronic state of a system. In ab initio systems,
> _all_ electronic configurations contribute to the wavefunction for
> each electronic state of a system. Is this an artifact of the
> approximations in ab initio calculations? Alternatively, if described
> exactly, is an exact ab initio wavefunction still composed of all the
> electronic configurations?

I find some confussion in this description, so perhaps I am not
understanding your question. DFT is founded on the Hohenberg-Kohn (HK)
theorem, according to which, for a non-degenerated ground state, the
exact energy can be obtained as a functional of the exact electron
density.  Thus the emphasis on the ground state electron density.
However, every different electronic state has a different electron
density (notice that the Born-Oppenheimer approximation is assumed
here).

>From a full CI perspective, the wavefunction of a given electronic state
will be given as a linear combination of a large number of Slater
determinants, each corresponding to a configuration (i.e. to a
electronic state under the approximation of independent electrons).
Therefore, the single electron density of an electronic state depends
(contains information) on the coupling of all the electron-independent
configurations entering the CI.

> On a second point, would it be correct to say that DFT _variationally_
> optimizes the electron density to determine the minimum energy of the
> system?

There are *many* DFT techniques. Perhaps the most commonly found (at
least in the molecular world) go back to the orbital description and
solve the Kohn-Sham equations. KS equations are not an outcome of the
variational principle. However, they are variational in the sense that,
once an exchange and correlation functional has been fixed, improving
the flexibility of the basis set will diminish the energy and converge
to the best solution that could have been obtained from that basis set.
Notice, however, that in most DFT methods neither the energy nor the
electron density is obtained by solving a variational equation.

    Regards,
                Victor Lua~na

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From chemistry-request@ccl.net Thu May 29 13:57:08 2003
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Date: Thu, 29 May 2003 19:56:58 +0200 (METDST)
From: Victor Lua~na <pueyo|at|pinon.ccu.uniovi.es>
Subject: Re:  CCL:calculating atomic charges with AIMPAC
To: chemistry|at|ccl.net, owner-chemistry|at|ccl.net
Cc: pueyo|at|pinon.ccu.uniovi.es
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> From: "Dr. Julia Metzker" <jm45|at|york.ac.uk>
> Date: Wed, 28 May 2003 15:13:03 +0100
> Subject: CCL:calculating atomic charges with AIMPAC
>
> I currently have an undergraduate student who is attempting to compare 
> charges of methylated benzene and ferrocene systems using the AIMPAC 
> software.  In the case of hexamethyl benzene and the ferrocene analogues he 
> is getting very large negative charges on some the ring carbons (-5 to -20) 
> and small positive charges on iron (0.5) Can anyone tell me if there is a 
> problem with the program or if the ring system can not be treated with this 
> method?

The charge integrated on the basin of a carbon atom goes from -5 to
-20 electrons??? That looks as big mistake. Either, the wavefunction
is not converged and it is made mostly of noise or the integration has
completely failed in AIMPAC. I suggest you first examining the actual
topology of the electron density. EXTREME is pretty fast and you can
easily discard any wrong-looking wavefunction. If everythhing looks
right you can try the *two* different integration techniques included
within AIMPAC. See the documentation of PROAIM. Notice that the laplacian,
L(r), should integrate to zero within a basin. An integral of 1e-4 a.u.
is reasonable given the finite precision of numerical integrations.
A value larger than some 1e-3 a.u. should make you suspect an error.

      Regards,
                Victor Lua~na

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From chemistry-request@ccl.net Thu May 29 14:17:31 2003
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Date: Thu, 29 May 2003 20:17:18 +0200 (METDST)
From: Victor Lua~na <pueyo|at|pinon.ccu.uniovi.es>
Subject: Re:  CCL:calculating atomic charges with AIMPAC
To: chemistry|at|ccl.net, owner-chemistry|at|ccl.net
Cc: pueyo|at|pinon.ccu.uniovi.es
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> From owner-chemistry|at|ccl.net Thu May 29 08:35:48 2003
> From: Wai-To Chan <chan|at|curl.gkcl.yorku.ca>
> Date: Thu, 29 May 2003 02:09:19 -0400 (EDT)
> Subject: CCL:calculating atomic charges with AIMPAC
> <<<<<<<<<<<<<<<<<<<<<<<<<<<<<<<<<
> I currently have an undergraduate student who is attempting to compare 
> charges of methylated benzene and ferrocene systems using the AIMPAC 
> software.  In the case of hexamethyl benzene and the ferrocene analogues he 
> is getting very large negative charges on some the ring carbons (-5 to -20) 
> and small positive charges on iron (0.5) Can anyone tell me if there is a 
> problem with the program or if the ring system can not be treated with this 
> method?
> >>>>>>>>>>>>>>>>>>>>>>>>>>>>>>>
> I remember reading about the tendency of AIM changes to be larger in magnitude
> than expected on the basis of chemical intuition. There is a paper by
> Kenneth Wiberg from the early 90s in J. comp. chem. about the comparison of 
> several atomic-charge partitioning scheme including Bader's you may find useful. 
> You may also consider using the Natural atomic charges method if you want 
> faster and less 'surprising' results. 

What "chemical intuition"? The one that comes from looking for many years
to Mulliken populations in gaussian outputs? That is not science, it is
prejudgment. Whatever interpretation we want to give to them, Bader charges
are unique and well defined properties of the electron density of the
molecule or solid under study. Both experimental and good theoretical
electron densities agree on the calculated Bader charges of hundreths of
compounds well characterized so far. On the other hand, Bader charges
are not enough to analyze the electron densities. The whole multipolar
series (charges are nothing but the zero order poles) should be considered
instead. Several recent works by Popelier, for instance, would made a
good reading in this respect.

In any case, the charges quoted in the original question look like if
the wavefunction is wrong by some reason. Perhaps a calculation
not converged.

   Regards,
             Victor Lua~na
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From chemistry-request@ccl.net Thu May 29 13:40:17 2003
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From: Paul.Mathias|at|aspentech.com
To: dshobe|at|sud-chemieinc.com, wu_guosheng2002|at|yahoo.com, renxiao|at|med.umich.edu,
   chemistry|at|ccl.net
Subject: RE: A question on heat of formation
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The NIST-JANAF tables are primarily based upon experimental data.
Computational predictions are sratting to be used, but the contribution =
is
-- yet -- very small.
=20
Paul Mathias

-----Original Message-----
From: Shobe, Dave [mailto:dshobe|at|sud-chemieinc.com]
Sent: Thursday, May 29, 2003 12:02 PM
To: 'Guosheng Wu'; 'Renxiao Wang'; 'CCL'
Subject: CCL:A question on heat of formation




---Guosheng Wu wrote:=20
> It seems to me, dH has not much to do with propabilities of all
conformations,=20
> which is essentially entropy contribution.=20

There is a small effect on enthalpy, for temperatures above zero =
Kelvin.
Most people ignore it, since there are more important sources of error. =
 But
I think the NIST/JANAF tables do take this effect into account.  It may
affect dH/dT more than it affects dH itself.

--David Shobe=20
S=FCd-Chemie Inc.=20
phone (502) 634-7409=20
fax     (502) 634-7724=20
email  dshobe|at|sud-chemieinc.com=20

Don't bother flaming me: I'm behind a firewall.=20



-----Original Message-----=20
From: Guosheng Wu [ mailto:wu_guosheng2002|at|yahoo.com
<mailto:wu_guosheng2002|at|yahoo.com> ]=20
Sent: Thursday, May 29, 2003 11:20 AM=20
To: Shobe, Dave; 'Renxiao Wang'=20
Subject: Re: CCL:A question on heat of formation=20


Were you talking about free energy(dG), instead of heat of formation =
(dH)?=20

It seems to me, dH has not much to do with propabilities of all
conformations,=20
which is essentially entropy contribution.=20

BTW, John Pople and others had a few papers on Gn theory to get very =
high
quality=20
heat of formation for a small molecule, by ab initio plus scaling
strategy... but=20
obviously not interested to most of the Med. Chem. community.=20

Guosheng=20

--- "Shobe, Dave" <dshobe|at|sud-chemieinc.com> wrote:=20
> Most people do the following.  They find the lowest-energy =
conformations
of=20
> the molecules involved, and use the energy at those geometries to
calculate=20
> delta-H.  The computational chemist should of course use any prudent, =

> reasonable means to ensure that these are indeed the *global*
conformational=20
> minima.=20
>=20
> However...=20
>=20
> I think to really "do it right" one has to calculate all the =
low-lying=20
> conformations and determine the relative statistical-mechanical
populations=20
> of each conformation, and from that the average enthalpy per molecule =
(or=20
> per mole). =20
>=20
> Usually there are enough other sources of error that the correct =
procedure

> has little advantage over the first approach, at least for enthalpy.  =
But=20
> the corresponding "correct" procedure is often done for entropy, =
where=20
> population of low-lying conformational isomers can make a significant =

> difference in the outcome.=20
>=20
> --David Shobe=20
> S=FCd-Chemie Inc.=20
> phone (502) 634-7409=20
> fax     (502) 634-7724=20
> email  dshobe|at|sud-chemieinc.com=20
>=20
> Don't bother flaming me: I'm behind a firewall.=20
>=20
>=20
>=20
>=20
> -----Original Message-----=20
> From: Renxiao Wang [ mailto:renxiao|at|med.umich.edu
<mailto:renxiao|at|med.umich.edu> ]=20
> Sent: Wednesday, May 28, 2003 8:19 PM=20
> To: chemistry|at|ccl.net=20
> Subject: CCL:A question on heat of formation=20
>=20
>=20
> Hi, CCLers!=20
>=20
> Should the heat of formations of two enantiomers of a chiral compound =
be=20
> identical? I think the answer is yes. Please point out some =
references=20
> for this.=20
>=20
> A disturbing fact is that, no matter you use QM or MM to calculate =
the=20
> heat of formation for a given molecule, the number is=20
> conformation-depentdent. I guess this is because of the steric energy =

> part is conformation-dependent. So, if I really want to compare the=20
> stability of two molecules using heat of formation, how may I =
calculate=20
> it right?=20
>=20
> Best regards,=20
>=20
> Renxiao Wang=20
> renxiao|at|med.umich.edu=20
>=20
>=20
>=20
> -=3D This is automatically added to each message by mailing script =
=3D-=20
> To send e-mail to subscribers of CCL put the string CCL: on your =
Subject:=20
> line=20
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<!DOCTYPE HTML PUBLIC "-//W3C//DTD HTML 4.0 Transitional//EN">
<HTML><HEAD>
<META HTTP-EQUIV=3D"Content-Type" CONTENT=3D"text/html; =
charset=3Diso-8859-1">
<TITLE>RE: CCL:A question on heat of formation</TITLE>

<META content=3D"MSHTML 5.50.4522.1800" name=3DGENERATOR></HEAD>
<BODY>
<DIV><SPAN class=3D430453417-29052003><FONT face=3DArial =
color=3D#0000ff size=3D2>The=20
NIST-JANAF tables are primarily based upon experimental data.&nbsp;=20
Computational predictions are sratting to be used, but the contribution =
is --=20
yet -- very small.</FONT></SPAN></DIV>
<DIV><SPAN class=3D430453417-29052003><FONT face=3DArial =
color=3D#0000ff=20
size=3D2></FONT></SPAN>&nbsp;</DIV>
<DIV><SPAN class=3D430453417-29052003><FONT face=3DArial =
color=3D#0000ff size=3D2>Paul=20
Mathias</FONT></SPAN></DIV>
<BLOCKQUOTE dir=3Dltr style=3D"MARGIN-RIGHT: 0px">
  <DIV class=3DOutlookMessageHeader dir=3Dltr align=3Dleft><FONT =
face=3DTahoma=20
  size=3D2>-----Original Message-----<BR><B>From:</B> Shobe, Dave=20
  [mailto:dshobe|at|sud-chemieinc.com]<BR><B>Sent:</B> Thursday, May 29, =
2003 12:02=20
  PM<BR><B>To:</B> 'Guosheng Wu'; 'Renxiao Wang'; =
'CCL'<BR><B>Subject:</B> CCL:A=20
  question on heat of formation<BR><BR></FONT></DIV><BR>
  <P><FONT size=3D2>---Guosheng Wu wrote:</FONT> <BR><FONT =
size=3D2>&gt; It seems to=20
  me, dH has not much to do with propabilities of all =
conformations,</FONT>=20
  <BR><FONT size=3D2>&gt; which is essentially entropy contribution. =
</FONT></P>
  <P><FONT size=3D2>There is a small effect on enthalpy, for =
temperatures above=20
  zero Kelvin.&nbsp; Most people ignore it, since there are more =
important=20
  sources of error.&nbsp; But I think the NIST/JANAF tables do take =
this effect=20
  into account.&nbsp; It may affect dH/dT more than it affects dH=20
  itself.</FONT></P>
  <P><FONT size=3D2>--David Shobe</FONT> <BR><FONT =
size=3D2>S=FCd-Chemie Inc.</FONT>=20
  <BR><FONT size=3D2>phone (502) 634-7409</FONT> <BR><FONT=20
  size=3D2>fax&nbsp;&nbsp;&nbsp;&nbsp; (502) 634-7724</FONT> <BR><FONT=20
  size=3D2>email&nbsp; dshobe|at|sud-chemieinc.com</FONT> </P>
  <P><FONT size=3D2>Don't bother flaming me: I'm behind a =
firewall.</FONT>=20
  </P><BR><BR>
  <P><FONT size=3D2>-----Original Message-----</FONT> <BR><FONT =
size=3D2>From:=20
  Guosheng Wu [<A=20
  =
href=3D"mailto:wu_guosheng2002|at|yahoo.com">mailto:wu_guosheng2002@yahoo.c=
om</A>]</FONT>=20
  <BR><FONT size=3D2>Sent: Thursday, May 29, 2003 11:20 AM</FONT> =
<BR><FONT=20
  size=3D2>To: Shobe, Dave; 'Renxiao Wang'</FONT> <BR><FONT =
size=3D2>Subject: Re:=20
  CCL:A question on heat of formation</FONT> </P><BR>
  <P><FONT size=3D2>Were you talking about free energy(dG), instead of =
heat of=20
  formation (dH)?</FONT> </P>
  <P><FONT size=3D2>It seems to me, dH has not much to do with =
propabilities of=20
  all conformations,</FONT> <BR><FONT size=3D2>which is essentially =
entropy=20
  contribution. </FONT></P>
  <P><FONT size=3D2>BTW, John Pople and others had a few papers on Gn =
theory to=20
  get very high quality</FONT> <BR><FONT size=3D2>heat of formation for =
a small=20
  molecule, by ab initio plus scaling strategy... but</FONT> <BR><FONT=20
  size=3D2>obviously not interested to most of the Med. Chem. =
community.=20
  </FONT></P>
  <P><FONT size=3D2>Guosheng</FONT> </P>
  <P><FONT size=3D2>--- "Shobe, Dave" &lt;dshobe|at|sud-chemieinc.com&gt;=20
  wrote:</FONT> <BR><FONT size=3D2>&gt; Most people do the =
following.&nbsp; They=20
  find the lowest-energy conformations of</FONT> <BR><FONT =
size=3D2>&gt; the=20
  molecules involved, and use the energy at those geometries to =
calculate</FONT>=20
  <BR><FONT size=3D2>&gt; delta-H.&nbsp; The computational chemist =
should of=20
  course use any prudent,</FONT> <BR><FONT size=3D2>&gt; reasonable =
means to=20
  ensure that these are indeed the *global* conformational</FONT> =
<BR><FONT=20
  size=3D2>&gt; minima.</FONT> <BR><FONT size=3D2>&gt; </FONT><BR><FONT =
size=3D2>&gt;=20
  However...</FONT> <BR><FONT size=3D2>&gt; </FONT><BR><FONT size=3D2>&g=
t; I think=20
  to really "do it right" one has to calculate all the low-lying</FONT> =

  <BR><FONT size=3D2>&gt; conformations and determine the relative=20
  statistical-mechanical populations</FONT> <BR><FONT size=3D2>&gt; of =
each=20
  conformation, and from that the average enthalpy per molecule =
(or</FONT>=20
  <BR><FONT size=3D2>&gt; per mole).&nbsp; </FONT><BR><FONT =
size=3D2>&gt;=20
  </FONT><BR><FONT size=3D2>&gt; Usually there are enough other sources =
of error=20
  that the correct procedure</FONT> <BR><FONT size=3D2>&gt; has little =
advantage=20
  over the first approach, at least for enthalpy.&nbsp; But</FONT> =
<BR><FONT=20
  size=3D2>&gt; the corresponding "correct" procedure is often done for =
entropy,=20
  where</FONT> <BR><FONT size=3D2>&gt; population of low-lying =
conformational=20
  isomers can make a significant</FONT> <BR><FONT size=3D2>&gt; =
difference in the=20
  outcome.</FONT> <BR><FONT size=3D2>&gt; </FONT><BR><FONT =
size=3D2>&gt; --David=20
  Shobe</FONT> <BR><FONT size=3D2>&gt; S=FCd-Chemie Inc.</FONT> =
<BR><FONT=20
  size=3D2>&gt; phone (502) 634-7409</FONT> <BR><FONT size=3D2>&gt;=20
  fax&nbsp;&nbsp;&nbsp;&nbsp; (502) 634-7724</FONT> <BR><FONT =
size=3D2>&gt;=20
  email&nbsp; dshobe|at|sud-chemieinc.com</FONT> <BR><FONT size=3D2>&gt;=20
  </FONT><BR><FONT size=3D2>&gt; Don't bother flaming me: I'm behind a=20
  firewall.</FONT> <BR><FONT size=3D2>&gt; </FONT><BR><FONT =
size=3D2>&gt;=20
  </FONT><BR><FONT size=3D2>&gt; </FONT><BR><FONT size=3D2>&gt; =
</FONT><BR><FONT=20
  size=3D2>&gt; -----Original Message-----</FONT> <BR><FONT =
size=3D2>&gt; From:=20
  Renxiao Wang [<A=20
  =
href=3D"mailto:renxiao|at|med.umich.edu">mailto:renxiao|at|med.umich.edu</A>]<=
/FONT>=20
  <BR><FONT size=3D2>&gt; Sent: Wednesday, May 28, 2003 8:19 PM</FONT> =
<BR><FONT=20
  size=3D2>&gt; To: chemistry|at|ccl.net</FONT> <BR><FONT size=3D2>&gt; =
Subject: CCL:A=20
  question on heat of formation</FONT> <BR><FONT size=3D2>&gt; =
</FONT><BR><FONT=20
  size=3D2>&gt; </FONT><BR><FONT size=3D2>&gt; Hi, CCLers!</FONT> =
<BR><FONT=20
  size=3D2>&gt; </FONT><BR><FONT size=3D2>&gt; Should the heat of =
formations of two=20
  enantiomers of a chiral compound be</FONT> <BR><FONT size=3D2>&gt; =
identical? I=20
  think the answer is yes. Please point out some references</FONT> =
<BR><FONT=20
  size=3D2>&gt; for this. </FONT><BR><FONT size=3D2>&gt; =
</FONT><BR><FONT=20
  size=3D2>&gt; A disturbing fact is that, no matter you use QM or MM =
to calculate=20
  the</FONT> <BR><FONT size=3D2>&gt; heat of formation for a given =
molecule, the=20
  number is</FONT> <BR><FONT size=3D2>&gt; conformation-depentdent. I =
guess this=20
  is because of the steric energy</FONT> <BR><FONT size=3D2>&gt; part =
is=20
  conformation-dependent. So, if I really want to compare the</FONT> =
<BR><FONT=20
  size=3D2>&gt; stability of two molecules using heat of formation, how =
may I=20
  calculate</FONT> <BR><FONT size=3D2>&gt; it right?</FONT> <BR><FONT =
size=3D2>&gt;=20
  </FONT><BR><FONT size=3D2>&gt; Best regards,</FONT> <BR><FONT =
size=3D2>&gt;=20
  </FONT><BR><FONT size=3D2>&gt; Renxiao Wang</FONT> <BR><FONT =
size=3D2>&gt;=20
  renxiao|at|med.umich.edu</FONT> <BR><FONT size=3D2>&gt; </FONT><BR><FONT =

  size=3D2>&gt; </FONT><BR><FONT size=3D2>&gt; </FONT><BR><FONT =
size=3D2>&gt; -=3D This=20
  is automatically added to each message by mailing script =3D-</FONT> =
<BR><FONT=20
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From chemistry-request@ccl.net Thu May 29 13:21:27 2003
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Date: Thu, 29 May 2003 10:21:26 -0700 (PDT)
From: Sengen Sun <sengensun|at|yahoo.com>
Subject: Re: CCL:Orbitals
To: chemistry|at|ccl.net
MIME-Version: 1.0
Content-Type: text/plain; charset=us-ascii

E. Lewars wrote:

 If MOs have no physical reality for multielectron
species, why (a) is Koopmans' theorem useful, why (b)
do photoelectron spectra match the predictions of MO
energy-level diagrams, and why (c) does the Hueckel
4n+2 rule, which is based on MO diagrams, work? 

These are extremely interesting questions to me. They
are very difficult to be answered, as implied by two
very prominent theoretical physicists in the last
century   Gell-Mann and Feynman: 
http://www.prometheus.demon.co.uk/02/02kumar.htm

I agree with Scerri, Spanget-Larsen, and many others
that MOs have no physical reality. But I don t think
that we, as suggested by Feynman, should stop asking
why MOs are so powerful for predictions in chemistry.
If we stop thinking, we would accept the control of
the universe by something of no physical reality; And
we would not be able to achieve a real understanding
of chemistry and the universe; And we would have
conceptual or logical conflicts... 


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From chemistry-request@ccl.net Thu May 29 14:42:00 2003
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Date: Thu, 29 May 2003 11:42:00 -0700 (PDT)
From: Noriaki Ikuta <noriaki_ikuta|at|yahoo.com>
Subject: RE: ic50 values in dtp aids dataset
To: Paul Hawkins <phawkins|at|tripos.com>
Cc: chemistry|at|ccl.net
MIME-Version: 1.0
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Paul Hawkins thank you for your respond.

But it seems to be imposible the categorise the compounds based on the
provided IC50 values. The ranges do significantly overlapp.
	
categy	mean	min	max	#cmpds (several outliers are left out)
CA	-4.5	-7.0	-2.5	705
CM	-4.0	-7.4	-2.7	1360
CI	-4.0	-10.0	-1.9	36289
NA	-4.4	-7.3	-3.0	294

Note on reliability:
The expression "Log10HiConc - Log10IC50 > 1.0" is only met in roughly 18%
of the cases. How useful are those IC50 values at all?

Noriaki


--- Paul Hawkins <phawkins|at|tripos.com> wrote:
> Noriaki,
> 
> I suspect the statement
> 
> "concentration of compound that inhibits the growth of uninfecte
> cells by 50%"
> 
> is a typo. IC50 is the concentration of a compound required to reduce
> the
> readout of the assay by 50%, whether you are measuring enzyme activity,
> receptor activation or cell growth/division.
> The classification into the different activity classes is somewhat
> arbitrary. Generally speaking a compound having an IC50 greater than
> 10^-5
> is not considered active as the doses required to achieve those
> concentrations in an animal (let alone a human) would be huge. For
> comparison most anti-HIV drugs on the market now have IC50's in this
> sort of
> assay around 10^-6 and have IC50's against their target receptor (the
> protease or reverse transcriptase mostly) in the 10^-9 range.
> There may also be a known correlation between IC50's in this assay and
> doses
> required to cause remission of infection in an animal model of HIV in
> humans
> and again the maximum acceptable dose may translate to an IC50 in this
> assay
> of 10^-5.
> I am unaware of any papers on this dataset in particular though a good
> many
> studies have used this dataset for various purposes.
> 
> One word of warning Log10HiConc should always be around 10x greater than
> the
> IC50 so as the Log10HiConc approaches the reported IC50 the IC50 result
> becomes less and less reliable.
> 
> Paul Hawkins
> Applications Scientist
> Tripos Inc
> 1699 South Hanley Road
> St. Louis MO 63144
> 
> Ph: 617-899-4151
> E-mail: phawkins|at|tripos.com
> 
> www.tripos.com
> 


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From chemistry-request@ccl.net Thu May 29 15:16:56 2003
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Date: Thu, 29 May 2003 12:13:55 -0700 (PDT)
From: Lou Noodleman <lou.-at-.scripps.edu>
Message-Id: <200305291913.h4TJDtO13881.-at-.degas.scripps.edu>
To: chemistry.-at-.ccl.net
Subject: Orbitals and Reality
Cc: lou.-at-.scripps.edu, tlovell.-at-.scripps.edu, wengehan.-at-.scripps.edu,
   ithink.-at-.san.rr.com, sharples.-at-.scripps.edu, himo.-at-.TheoChem.kth.se
X-Sun-Charset: US-ASCII

Dear Dr. Fournier and Group at CCL,
At the risk of getting into deep metaphysics, I want to make a few
simple observations about this issue of the reality of orbitals.
I have found some of the discussion surprising.
"Are orbitals real?" No, orbitals are a model (equivalently, a representation
of reality). Only "reality", "the things out there that we deal with" are
real. Orbitals are " a map" of that reality, or more precisely, they are
part of a family of theories of a certain level of accuracy.
Are "many electron wavefunctions real"? No, when properly used, they may
provide a more accurate representation of the real world, than wavefunctions
based on a single set of orbitals. However, the information and more
importantly, connections and generalizations to other systems may be more
difficult to obtain. Is the solution to the many electron Schrodinger
equation real? No, for example, what if the Born-Oppenheimer separation
fails separating the nuclear wavefunction from the geometry dependent
electronic wavefunction? What about the problems of dealing with the
quantum mechanics of open systems? What about relativistic effects and
their many subtleties? I do give higher priority at least as a touchstone
to QM observables like electron density, which are measurable for example,
> from high precision X-ray structures of well defined systems. But these are
neither exact nor precise even in principle, given coupling to nuclear motion
which is quantum mechanical, and in some cases not separable.
Also, the world is an open system, with all the problems that gives.
Since the world and all of its interconnected parts have an infinite number
of facets, we will never know reality, but it is fun to understand something
about some of the pieces and their linkages.
Concerning orbitals, beyond their other uses, I recall from earlier work of
Chris Brion that in e-2e inelastic scattering experiments, something
very much like orbitals can be mapped out. In photoelectron spectroscopy,
the multiple peaks in final electron kinetic energy for a given photon energy
can usually be correlated with orbitals (but sometimes this collapses
(see L. Cederbaum's work))
 and for optical spectra, orbital analysis can
be done in Time Dependent DFT, as shown by Rich Martin at Los Alamos.
Concepts have value even when they are not perfect, and no concept is
perfect (see Ralph Waldo Emerson).
In general, I think of orbitals as somewhat real, less than electron densities,
or atoms,
but more than Lewis bond structures (at least, most of the time).
> From a philosophical viewpoint, nothing that I have said is very new.
"The gods did not reveal from the beginning
All things to us; but in the course of time,
Through seeking, men find that which is better.
But as for certain truth, no man has known it.
Nor will he know it."
Xenophanes (6th Century B.C.)
(quoted from Marion, "Classical Electromagnetic Radiation",1965).
Also, Newton's quotation, better known among scientists, is as valid
today as it was for him over 300 years ago. We forget the past at our peril.

Lou Noodleman
Department of Molecular Biology, TPC15
The Scripps Research Institute
La Jolla, CA
.



From chemistry-request@ccl.net Thu May 29 16:11:43 2003
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From: alewand$at$medusa.bioc.aecom.yu.edu
To: chemistry$at$ccl.net
Subject: TS optimization with restraints in G98
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I 'm making optimization of transition state structure with
restraints imposed especially along reaction coordinate.

I got some converged structures on semiepmirical level with only 
one negative frequency (probably on DFT 
it will be more difficult to converge) but I still consider if approach is 
correct. 
Thank you for every regards concerning this calculation.

Andrzej



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From: James Robinson <prsjjr$at$bath.ac.uk>
To: chemistry$at$ccl.net
Subject: RE: Orbitals and Reality
Date: Thu, 29 May 2003 21:00:20 +0100
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If we do not find anything very pleasant, at least we shall find something new.. Volatire.

Is the basis of aromaticity and Woodward-Hoffman rules to be placed in a bin?

I remember that some scientist captured an image of the letters IBM some years ago, written by aligning individual atoms (Switzerland I think)

I wondered what the image was, what it meant. MOs themselves may be nothing more than the result of applied mathematics, however, I have difficulty in understanding a plausible alternative to describe the wave-nature of electrons.

James, Bath. 




From chemistry-request@ccl.net Thu May 29 18:16:03 2003
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Subject: Re: CCL:Orbitals and Reality
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I'm enjoying this discussion about MO. I should say that Molecular Orbitals
are not Real, but Complex. It is a mathematical tool that represents the
electronic structure of the matter.

Please correct me if this is wrong.


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From: Damian A Scherlis Perel <damians-.at.-MIT.EDU>
To: <chemistry-.at.-ccl.net>
Subject: CCL: CASSCF and basis set superposition
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 Dear all,

 I am performing a series of multireference calculations on
 dimers. In order to apply the basis set superposition correction
 I must do the calculations also on the monomer, which has as
 many basis functions but one half the number of
 electrons. On the other hand, while the dimer is a closed
 shell system, the monomer is a radical. My concern is the
 relation between the active spaces to be picked for the dimer
 and the monomer so that the energy difference may be obtained.
 For instance, let's say the active space is 8-electrons 6-orbitals
 (8,6) in the closed shell dimer, what should it be in the
 open shell monomer?

 Thanks so much,
                    damian

 ------------------------
 Damian Scherlis
 Department of Materials Science & Engineering
 Massachusetts Institute of Technology
 damians-.at.-mit.edu
 617 253 6026


