From chemistry-request@ccl.net Thu May 29 16:32:07 2003
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Date: Thu, 29 May 2003 13:32:07 -0700 (PDT)
From: Guosheng Wu <wu_guosheng2002{at}yahoo.com>
Subject: CCL: Orbitals
To: Sengen Sun <sengensun{at}yahoo.com>
Cc: chemistry{at}ccl.net
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A few words about Orbitals and QM.

If Einstein was one of those who first discovered Quantum Mechanics,
he might have had different opinion about it, which partly would 
make it easy for many others to accept it earlier than later.

It is just because QM is so great and he was also so great...

There seems no conceptual or logical conflicts about QM.

It's just about wave_like_properties described with MO(Molecular Orbital)
or WF(wavefunction), no matter how sophisticated it may be, 
and properties from it(propability, energies...) by something like 
<WF|operator|WF>. Put time into the operator and elsewhere properly
if one is interested in the properties of dynamics.

By the way, it seems to me MO is mostly seen as just an essentially 
same concept as WF. "MO" is still used at least in this list, just like 
any piece of a language, or the formation of a physical road ... 

As a mathematical problem for a MODEL system, it had certainly 
been solved accurately by QM, in the scope of atoms & electrons in the vacum.

For the real world problems, most people and many in this list are just 
playing with Applied Maths & computers to get something useful in some
areas of chemistry, materials or biology. 

That's it, like Direc ever said.

Guosheng

--- Sengen Sun <sengensun{at}yahoo.com> wrote:
> 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 16:38:51 2003
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Date: Thu, 29 May 2003 17:52:59 -0300
From: Sidney Ramos de Santana <sidney$at$dqf.ufpe.br>
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To: CCL List <chemistry$at$ccl.net>
Subject: Dalton 1.2 Problem: wave function not converged!
Content-Type: multipart/mixed;
 boundary="------------080901090907070203060208"

This is a multi-part message in MIME format.
--------------080901090907070203060208
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Dear CCL Users,

I have been trying to perform a Shieldings and Spin-Spin Couplins Constants
calculations with Dalton 1.2 for Pt[(SnCl3)4]3-.
I am using ECP but I don't have sucessful.
Please see below:

Basis Set Section:
------------------------
 label    atoms   charge   prim    cont     basis  
  ----------------------------------------------------------------------
   Pt         1      18      46      32      
[9s5p3d1f|3s4p2d1f]                         
...
   Sn         1       4      17      13      
[3s3p1d|2s2p1d]                             
...
   Cl         1       7      17      13      
[3s3p1d|2s2p1d]                             
  ----------------------------------------------------------------------
  total:     21     143     386     292
  ----------------------------------------------------------------------

Sirius Section:
-------------------
 *** Optimization control WARNING: MCSCF not converged ***
     Maximum number of iterations or backsteps reached:
     Number of macro iterations used            5
        Maximum                                15
     Number of micro iterations used           47
        Maximum                               180
     Number of back steps this macro            6
        Maximum                                 5
     Total number of CPU seconds used    195396.71

 WARNING: wave function not converged

End of File:
----------------
- DALTON aborted because wave function not converged!

  --- SEVERE ERROR, PROGRAM WILL BE ABORTED ---
     Date and time (SUN)    : Mon May 26 22:47:46 2003
     Host name              : samba                                  

 Reason: DALTON aborted because wave function not converged

 >>>> Total CPU  time used in DALTON:  74 hours 48 minutes 59 seconds
 >>>> Total wall time used in DALTON:  77 hours 50 minutes 53 seconds

Anybody Can Help me ?
What can I do ?

Sidney Ramos
Graduate Program of Materials Science
CCEN - DQF - UFPE - Brazil

--------------080901090907070203060208
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 name="complex1.dal"
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**DALTON INPUT
.RUN PROPERTIES
.DIRECT
**WAVE FUNCTION
.HF
**PROPERTIES
.SHIELD
.SPIN-S
*SPIN-S
.ABUNDA
  0.10
.SELECT
  5
  1  3  4  5  6
*END OF INPUT



--------------080901090907070203060208
Content-Type: text/plain;
 name="complex1.mol"
Content-Transfer-Encoding: 7bit
Content-Disposition: inline;
 filename="complex1.mol"

BASIS
ECP
NMR parameters - Geom. Optimized 
12345678901234567890123456789012345678901234567890
    3             -3
       78.    1
 Pt         -0.000033   -0.000283   -0.000186
       50.    5
 Sn         -0.000080   -1.570825   -2.048043
 Sn         -0.000039   -0.990691    2.382968
 Sn          0.000162    2.558780   -0.334569
 Sn          2.554395    0.001166   -0.000422
 Sn         -2.554461    0.001405   -0.000410
       17.   15
 Cl         -3.802978   -1.942611    0.750175
 Cl         -3.799062    0.326369   -2.061309
 Cl         -3.798572    1.625239    1.309935
 Cl          3.802841   -1.942389    0.751459
 Cl          3.798619    1.625839    1.308775
 Cl          3.798953    0.324672   -2.061577
 Cl          0.001018   -3.426703    2.638517
 Cl         -1.772298   -0.579453    4.015542
 Cl          1.771227   -0.577884    4.016225
 Cl         -1.772125   -3.191337   -2.504964
 Cl          1.770880   -3.192816   -2.503934
 Cl          0.000995   -0.577499   -4.286911
 Cl          0.001882    3.998926    1.646483
 Cl         -1.772925    3.765926   -1.506748
 Cl          1.771766    3.765506   -1.509414



--------------080901090907070203060208--



From chemistry-request@ccl.net Thu May 29 17:29:55 2003
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Dear CCL Users,

I compiled the Shell-Dynamo 2.1 with G77(Gnu Compiler)
and with IFC(Intel Fortran Compiler).
I have been trying to perform a calculation of diffusion constants
of Ions in a oxifluoride glass.
In this program I am using Buckigham potential and the initial
coordinates of the ions in the simulation box was been filling
randomicly, because I choosed the option "fillbox random".
This initial coordinates in the program compiled with G77
are generating by "ranf" intrinsic function, and in the IFC are
generating by "random_number" intrinsic function using
"date_and_time" intrinsic function to generate a seed.
In the both cases the initial configuration generated was the worst
possible. This way, I will need a very, very big step numbers in
this MD simulation.
So, this question for you:
What is the best to generate randomicly an initial
coordinates  of the ions the simulation box:
an intrinsic function of Compiler to generate random
number (if yes, why?) or an algorithm(if yes, why) ?

Sidney Ramos
Graduate Program of Materials Science
DQF - CCEN - UFPE



From chemistry-request@ccl.net Fri May 30 02:29:17 2003
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Subject: CCL:RE: Eigenvalues of hessian
Date: Fri, 30 May 2003 08:28:41 +0200
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From: "Dillen Jan <jlmd:at:sun.ac.za>" <JLMD:at:sun.ac.za>
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> 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. 

Dear Daniel,

The fact that frequencies are equal to the square
root of the diagonalised mass-weighted Hessian
matrix is a result obtained from solving the following 
equations of motions:

	F = m.a = - H.dx

where 'm' is a diagonal mass matrix, 'a' the acceleration,
'H' the Hessian, and 'dx' are the displacement coordinates.
The 'H.dx' appears if one assumes that (1) the potential energy
can be written as a harmonic function of the displacement
coordinates and (2) that the gradient vanishes, i.e.

	U = U(0) + 1/2 (dx)^T.H.dx

(1) is called the harmonic approximation and (2) implies
a stationary point. Hence "frequencies" which are not
calculated at a stationary point do not necessarily have
zero translational and rotational components.

Here is an alternative reasoning. The potential energy
should not change if the molecule is translated, i.e.

	dU/dX = 0

with 'X' are the coordinates of the centre of mass. However,

	dU/dX = sum (dU/dx) (dx/dX)

where 'x' are atomic coordinates. More complex expressions
appear for the second derivatives. Obviously, dX/dx is
not zero (and hence also dx/dX), so dU/dx must be zero in 
order to have dU/dX = 0, i.e. a stationary point. (or
if the sum of these terms happens to be exactly zero)

Hope this helps.

Groeten
Jan Dillen


 


From chemistry-request@ccl.net Fri May 30 08:07:56 2003
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To: chemistry-.at.-ccl.net
Subject: CCL: Orbitals


Hey,

Just to throw oil on fire....

Of course orbitals (molecular, atomic...) are not "real", because they
just result from the mathematical construction of our theory. They are
not unique, and so on...
But is the many electrons wave function (Y) more "real"?
   Parentheses:
Ok, I know that wave function are not real, only the square (YY*) has a
physical meaning. But I prefer to speak about wave function, knowing
that 
the observable density is deduced from this wave function.
   End Parentheses.
What I mean is that:
    - The exact Hamiltonien (fully relativistic, not B-O,...) is
generally 
not used (not known?).
Then the exact solutions we have are just solution of an approximate
Hamiltonien, and thus can not describe exactly the physical phenomenon.
    - The exact solutions of the (even approximate) Hamiltonien are not
known.
What we get, is just a more or less acceptable representation of
"reality".
Does that mean that everything we get with Hartree-Fock method is
garbage?
The answer is no, because a lot of the "physic" of the system is
included 
in the theory, but it could be improved...

Does someone remember (or know) why we use orbitals in the first time?
I think that it is because they can be exact solutions of approximate
Hamiltonien! If, in a model representation of the world surrounding us, 
we consider that all electrons of a system can move more or less 
independently from one another, then orbitals are "real" in the sense 
that they allow us to describe the world with a given level of accuracy.
Of course it is not perfect. 
I really do think that canonical orbitals are "real" because they come 
> from a theory that has the major physical factor in it (symmetry,
nuclear
attraction, kinetic energy, average coulombic interaction...). Thus, if
one improve the one-electron Hamiltonien (for example  with Kohn-Sham
method) that gives the canonical orbitals, then orbitals will be more 
"real" in the sense that they will predict or explain more accurately 
the world...


Well, that was just my 2 eurocents.

PS: In reply to E. Lewars, I will even say that virtual orbitals are
"real"
 because they allow us to explain spectroscopy (n -> Pi* transition in
H2CO
 for example)


                                      ...Xav

Pr. Xavier Assfeld             Xavier.Assfeld-.at.-lctn.uhp-nancy.fr
Laboratoire de Chimie thiorique     (T) 33 3 83 68 43 74
Universiti Henri Poincari           (F) 33 3 83 68 43 71
F-54506 Nancy B.P. 239              http://www.lctn.uhp-nancy.fr



From chemistry-request@ccl.net Fri May 30 00:40:42 2003
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Dr. Noodleman, I hate to quibble with what you've written, since you've
expressed things so clearly, and I agree with most of what you say, but...

> 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).


I think of orbitals as somewhat LESS real than "Lewis bond structures"
since in most cases the latter can be uniquely derived from topological
analysis of the (real) electron-density, i.e. from the gradient paths and
critical points thereof, whereas individual one-electron orbitals for
many-electron systems, however useful they might be, are quite arbitrary;
orbitals are solutions to a mathematical equation for a model system and
will differ depending upon the model employed (Huckel, Hartree-Fock,
Kohn-Sham, natural orbitals).

With all due respect to the stalwarts of quantum mechanics, it makes little
sense today to use terms like "physical reality" which cannot be defined
with the degree of rigor we expect in science, without employing circular
logic. And how to define "think" and "I" without invoking open systems and
wavefunction collapse? Why, I'll be glad if we can all agree on the meaning
of the word "is"!

Dr. N. Sukumar
http://www.drugmining.com/
Visiting Scientist
Rensselaer Department of Chemistry and
Wadsworth Center, New York State Dept.of Health



From chemistry-request@ccl.net Fri May 30 01:02:18 2003
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Date: 29 May 2003 22:02:13 PDT
From: Alan.Shusterman-.at.-directory.reed.edu (Alan Shusterman)
Subject: CCL: Orbitals and Reality
To: chemistry-.at.-ccl.net
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This discussion has taken some very unexpected and interesting twists. I want to put in my 2 cents regarding two interesting ideas that have appeared today...

1. Orbitals may only be mathematical constructs, but since they explain so much (scattering expts, PES, Woodward-Hoffman rules, aromaticity, etc.), they *feel* real and ought to be accepted as such

2. All of our theories contain approximations, so we are not justified in calling anything "real" that we calculate

Response to 1. I think this proposal has emotional appeal, and therein lies the problem. Take Woodward-Hoffman rules. They are just one of the many ways to explain what goes on in a pericyclic transition state. Or, take aromaticity. The traditional pi MO explanation of aromaticity was successfully challenged over a decade ago. Finally, take PES spectra - one can find PES spectra that fit MO energy sequences nicely and others that don't.

Knowing the limitations of, and alternatives to, MO-based rationales does not make MOs less useful, but it should temper one's emotional attachment to them. The fact that MOs display interesting properties does not make them real. Conversely, the fact that they are only mathematical constructs does not prevent them from being interesting or useful.

Response to 2. Lou Noodleman points out the many layers of approximation embedded in ab initio computations. I think his argument may be a red herring, however.

When we calculate energy, we calculate an *estimate* (subject to one or more of the approximations Lou listed) of an observable quantity. It's true that if we remove an approximation (Born-Oppenheimer, lack of relativistic effects, etc.) we must change the methodology used to estimate the molecular energy, but we continue to estimate *molecular energy*.  Furthermore, we can compare our estimate to experiment, and learn about the significance of these approximations.

The situation is different for wavefunctions and MOs. First, these are mathematical constructs that can't be compared to any observable quantities except by introducing a theory or rationale that says "wavefunction/MO property Z should correlate with observable X". Second, and more important for this discussion, MOs only appear when we assume independent electron behavior (which is the most extreme approximation that we can make).

This seems to make MOs rather special - you can write wavefunctions that cannot be factored into MOs. They do not simply adjust their values, like the molecular energy does, as approximations are added or removed.

(I hope this won't look like hair-splitting when I read this tomorrow morning)

-Alan

====

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



From chemistry-request@ccl.net Fri May 30 05:08:32 2003
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Dear all,

Can anybody point me to a (preferably free are reasonably priced)
software that can do docking between a given surface structure
and a range of organic molecules/polymers ? 

Can any of the programs that are used for bio-receptor/ligand
or protein-protein interactions (such as dock, autodock flexx, etc)
be used for this purpose ?

thanks in advance for any help!
cheers,
Michael


==========================================================================
"Emotions are alien to me.  I'm a scientist."
(Spock, "This Side of Paradise", stardate 3417.3)

--------------------------------------------------------------------------
Michael Brunsteiner
Centre for Theoretical and Computational Chemistry
University College London
mailto:m.brunsteiner.-at-.ucl.ac.uk
http://www.ucl.ac.uk/~uccambr/
--------------------------------------------------------------------------


From chemistry-request@ccl.net Fri May 30 03:51:42 2003
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Date: Fri, 30 May 2003 09:12:27 +0200
From: Sebastien Laugaro <laugaro.-at-.ccr.jussieu.fr>
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Hy,

I work on Gaussian and I have a problem. In fact, when I use 
B3LYP/6-31G* OPT  TEST Int(Grid=35110) , I have a error message :
'Convergence Failure. Error Termination'. When I use the same file and
HF/STO-3G OPT TEST Int(Grid=35110), I have no problem.
Can you help me to resolve my problem.
Thank you.
                                                                       
               Sebastien.
                                                                        
              laugaro.-at-.ccr.jussieu.fr



From chemistry-request@ccl.net Fri May 30 10:50:37 2003
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Date: Fri, 30 May 2003 16:41:48 +0200
From: "Nicolas Ferre'" <ferre^at^unisi.it>
Subject: CCL: QM/MM cutoffs
Sender: ferre^at^unisi.it
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Hi folks,

I'm currently implementing a simple QM/MM molecular dynamics approach,
but I have some doubts about the right way of dealing with the
electrostatic interactions between the quantum distribution and the
classical point charges. Using periodic boundary conditions and the
minimum image convention, I have to define a cutoff distance : a
site-site interaction is discarded if the site-site distance is greater
than this value. OK for a classical simulation.
Now if part of the system is treated quantum mechanically, the
definition of some QM sites is non-obvious : the QM wavefunction is
delocalized on the whole QM subsystem.
The simplest idea would be to select the center of mass of the QM
subsystem as a unique site only to choose MM point charges interacting
with the QM subsystem, but if the QM molecular shape is not spherical,
this solution is not convenient (a QM atom located at one end of the QM
subsystem could not interact with the closest images of some MM point
charges).
Thus I'd like to hear about your solutions/experiences/references to
solve this problem, taking in mind that I don't want to approximate (for
the moment) the QM electronic distribution (no fitted multipoles ...) I
know about Ewald sums for QM/MM interactions but I'd prefer to start
with a rather simplest approach.

Best regards,

Nicolas

-- 
~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~
Nicolas FERRE' (PhD)
				 phone/fax : +39-0577-234278
Dipartimento di Chimica
Universita` di Siena             mailto:ferre^at^unisi.it
via Aldo Moro
53100 SIENA (Italia)             http://ccmaol1.chim.unisi.it/
~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~

From chemistry-request@ccl.net Fri May 30 11:39:49 2003
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Date: Fri, 30 May 2003 11:27:21 -0400 (EDT)
From: Rene Fournier - 1999-07-07 <renef)at(yorku.ca>
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To: chemistry)at(ccl.net
Subject: Orbitals
In-Reply-To: <200305301206.OAA26570)at(host20.lctn.uhp-nancy.fr>
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I agree with Lou Noodleman's point that we have many mathematical
models with different degrees of rigor to approach reality
without ever quite reaching it (sounds like calculus...).
And I do like orbitals, especially Kohn-Sham orbitals, a lot.
But I think there's a difference between, say, an approximate 
electron density -- far from reality because it is inaccurate --
and a set of orbitals -- far from reality because we're not sure
exactly what kind of measurements they should be compared to.

That being said, theoretical arguments and comparisons to
experiments support the view that KS orbital energies are good
approximations to relaxed vertical ionization potentials
(Chong, Gritsenko, Baerends, J Chem Phys 116 (2002) 1760),
that differences of virtual and occupied KS orbital energies
are good approximations to excitation energies (A Savin,
CJ Umrigar, X Gonze, Chem Phys Lett 288 (1998) 391), that
KS orbitals give good approximations to spherically averaged
momentum distributions obtained by electron momentum spectroscopy
(P Duffy, DP Chong, ME Casida, DR Salahub, Phys Rev A 50 (1994)
4707;  S Hamel, P Duffy, ME Casida, DR Salahub Journal of Electron
Spectroscopy and Related Phenomena (2002?)).  To me, KS orbitals
are meaningful, and are useful for quantitative comparisons even
though it's not 100% clear what they should be compared with.
Whether they are "real" in some particular philosophical system
is not as important for me...  but it's still interesting!  :)

-- Rene Fournier.
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| Rene Fournier                 | Office:  303 Petrie              |
| Chemistry Dpt, York University| Phone: (416) 736 2100 Ext. 30687 |
| 4700 Keele Street,  Toronto   | FAX:   (416)-736-5936            |
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From chemistry-request@ccl.net Fri May 30 19:00:38 2003
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Date: Fri, 30 May 2003 19:00:43 -0400 (EDT)
From: Avijit Ghosh <avijit/at/physics.drexel.edu>
To: chemistry/at/ccl.net
Subject: Re: CCL:Orbitals
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	Hi all, let me first qualify this as I am far removed from
quantum dynamics/electronic structure/semiclassical physics and
am just putting some thoughts in as someone who has been listening
to the discussion w/ great interest.

	 I think orbitals used as "basis set expansions" as in many 
electronic structure calculations might be considered a mathematical trick 
to solve a differential equation and  there should be treated as 
mathematical constructs since they are being treated as such.

	However there are several issues here.

	(1) If I take the term orbital to mean the "wave function"
 of a  single e-, is it "real"? I would say no as the wave function is
a thing that exists in complex space and is not as such observable
property. In this sense the "many e-" wavefunction is not 
observable either, so that statement I think has less to do w/ "orbitals" 
but more to do w/ wavefunctions as the thing that one "operates" on
to get observables.

	(2) Does the single e- wavefunction density have any
meaning? Let me decompose this a bit. To me the fact that
organic chemists can "hybridize" orbitals (aka "handwaving
quantum mechanics") is a testament to the contribution of
e-e- correlation as actually not being that much at least
for the first part of the periodic table. In fact that  elements have 
the properties that they do is also a testament to this.

	Let me rephrase this w/ a model, suppose epsilon_0 for e-e- 
interactions only  were some other value. That is we could scale down the 
correlation function, at arbitrarily small scaling (i.e large epsilon_0) 
the "orbital" approximation (as observable single e- densities)

By construction the "orbital" approximation is closer to "reality" as
I scale my hamiltonian. That is the wavefunction would become a product 
of single e- wavefunctions,  even though technically I can not *ever* 
write the wavefunction as a  product of single e- wavefunctions  as long 
as I have even an arbitrarily small amount of e-e- correlation.

	I think that the assertion of orbitals "existing" is just an 
assertion of  that e-e- is 0.5 % of the answer allowing the organic 
chemists to  "write" the wavefunction as a product of single e- 
wavefunctions. It seems to me that if one is allowed to posit the total 
electronic wavefunction density has a "reality" on its own and 
corresponding  measurements and eigenstates  (i.e. decoupling the 
nuclear/electronic  kinetic terms  ala born oppenheimer) as having
a reality, then one in the same manner should be allowed to posit orbitals 
as having a "reality" since it seems to me to be the same approximation
just on a different part of the hamiltonian.

	

	-avi


Asst. Prof. Avijit Ghosh
Dept of Physics
Drexel University
	




From chemistry-request@ccl.net Fri May 30 14:23:54 2003
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From: "Zeinalipour-Yazdi Constantinos" <czeinalip_at_hotmail.com>
To: "Computational Chemistry list" <chemistry_at_ccl.net>
Subject: CCL: STM simulation package
Date: Sat, 31 May 2003 11:14:13 -0700
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Dear CCLer's,

I am trying to find a software that can simulate the STM image of a DFT =
calculation using HF/B3LYP. I am currently using GAMESS/US as my =
computational tool.=20

Best regards, Constantinos.

Zeinalipour-Yazdi Constantinos
PhD student
Department of Chemistry
San Diego State University
University of California, San Diego

Lab phone : (619)-594-2002

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<STYLE></STYLE>
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<DIV><FONT face=3DArial size=3D2>Dear CCLer's,</FONT></DIV>
<DIV>&nbsp;</DIV>
<DIV><FONT face=3DArial size=3D2>I am trying to find a software =
that&nbsp;can=20
simulate the STM image of a DFT calculation using HF/B3LYP. I am =
currently using=20
GAMESS/US as my computational tool. </FONT></DIV>
<DIV>&nbsp;</DIV>
<DIV><FONT face=3DArial size=3D2>Best regards, =
Constantinos.</FONT></DIV>
<DIV>&nbsp;</DIV>
<DIV><FONT face=3DArial size=3D2>Zeinalipour-Yazdi Constantinos<BR>PhD=20
student<BR>Department of Chemistry<BR>San Diego State =
University<BR>University=20
of California, San Diego</FONT></DIV>
<DIV><FONT face=3DArial size=3D2><BR>Lab phone :=20
(619)-594-2002</FONT></DIV></BODY></HTML>

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From chemistry-request@ccl.net Fri May 30 19:07:54 2003
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To: ccl <chemistry_at_ccl.net>
From: Eric Scerri <scerri_at_chem.ucla.edu>
Subject: orbitals
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As somebody working in philosophy of science and more specifically 
philosophy of chemistry I have found the recent discussion very 
interesting.

Although I may not have fully digested every subtle nuance and 
technicality concerning orbitals that has been voiced in recent days 
I believe I may still be able to contribute to one major aspect of 
the discussion.

This is on the question of usefulness and reality.

There is a long-standing debate in philosophy of science going back 
for hundreds of years which in modern terminology is referred to as 
the realism versus anti-realism debate.

Very briefly realists believe that we can attribute physical reality 
to scientific terms that are used in successful scientific theories 
regardless of whether or not these terms can be observed.  Indeed 
most realists believe that we should attribute physical reality to 
unobservable terms or entities like quarks.

Modern realism arose as a reaction against logical positivism whereby 
every scientific term would need to be grounded in observation.  The 
failure of the program of logical positivism (Carnap, Schlick, Nagel, 
Reichenbach etc.) came about for many reasons among them being the 
inability to draw a sharp distinction between theoretical and 
observational terms.

But logical positivism has not died away altogether and there is a 
sense in which it survives in the modern anti-realism view of 
scientific theories.  According to this view, of which Bas van 
Fraassen is the leading proponent, observability remains an important 
criterion.  If a scientific term or entity cannot or has not been 
observed then we have no warrant for assigning physical reality to 
it.  No matter how useful a scientific theory or scientific term 
might be this does not warrant us in the further belief that this 
theory or particular scientific term might have physical reality.  As 
I mentioned in an earlier posting there have been many terms that 
were temporarily useful in now defunct theories.  For example 
phlogiston was initially quite useful and successful in explaining 
many chemical facts.  Some people may even have believed that this 
meant that phlogiston was a real physical entity and yet as everybody 
knows it turned out to be a mistake.

Of course I am not suggesting that orbitals will necessarily turn out 
be be a mistake, except in the general sense that all scientific 
theories and approaches are eventually refuted.  This view, called 
the pessimistic meta-induction, provides a rather powerful argument 
against regarding any scientific theory realistically and similarly 
any scientific terms from current theories.


Finally, it should also be recalled that the most widely held 
interpretation of quantum mechanics, the Copenhagen interpretation, 
is essentially an anti-realistic interpretation regardless of what 
people like Einstein and David Bohm may have wanted.  So it is a 
little puzzling to discover that some quantum chemists are prepared 
to go beyond this general philosophical framework when it comes to 
one particular term within quantum chemistry and to attribute 
physical reality to orbitals.


regards,

eric scerri
-- 


Dr. Eric Scerri ,
UCLA,
Department of Chemistry & Biochemistry,
607 Charles E. Young Drive East,
Los Angeles,  CA 90095-1569
USA

E-mail :   scerri_at_chem.ucla.edu
tel:  310 206 7443
fax:  310 206 2061
Web Page:    http://www.chem.ucla.edu/dept/Faculty/scerri/index.html

Editor  of  Foundations of Chemistry
http://www.kluweronline.com/issn/1386-4238

Also see International Society for the Philosophy of Chemistry
http://www.georgetown.edu/earleyj/ISPC.html


