From chemistry-request@server.ccl.net  Fri Aug 25 04:34:32 2000
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To: Eugene Leitl <eugene.leitl@lrz.uni-muenchen.de>
From: Christoph van =?iso-8859-1?Q?W=FCllen?=  <Christoph.vanWullen@tu-berlin.de>
Subject: Re: CCL:Ahem, shouldn't we do something about it?
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As to the discussion of 'online publishing', my opinion is that if the contributions
are not peer-reviewd (using the same quality standards as in the printed journals),
there is always the risk that there will be some garbage among the contributions. In this
case, not too many scientist will browse the contents.

-- 
+---------------------------------+------------------------------------+
| Prof. Christoph van Wullen      | Tele-Fon   (+49) (0)30 314 27870   |
| Technische Universitat Sekr. C3 | Tele-Fax   (+49) (0)30 314 23727   |
| Strasse des 17. Juni 135        | eMail:                             |
| D-10623 Berlin, Germany         | Christoph.vanWullen@TU-Berlin.DE   |
+---------------------------------+------------------------------------+

From chemistry-request@server.ccl.net  Fri Aug 25 05:20:08 2000
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Subject:  re: Ahem, shouldn't we do something about it?


> As to the discussion of 'online publishing', my opinion is that if the contributions
> are not peer-reviewd (using the same quality standards as in the printed journals),
> there is always the risk that there will be some garbage among the contributions. In this
> case, not too many scientist will browse the contents.

The Chemistry Preprint Server has a ranking mechanism, which allows readers to give a
quality indication. But since these qualification is not only done by people in the same
field of research it is very different from 'refereeing' in the sense it is done with
journals...

This could be circumvented by assining 'research interest' fields to persons and when
this value is the same as for the article, extra weight can be given to the qualification...

Egon

From chemistry-request@server.ccl.net  Fri Aug 25 05:48:45 2000
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Dear friend,
     I have a problem in setting up the model for
enzyme using link edit parm.The charge is not
0.another thing is that i view in rasmol the chain is
broken from various residues especially before or
after HIP residues.If u are using leap i wellcome all
suggestions.
 witj best regards,
sohail.
university sains malaysia.
   

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From chemistry-request@server.ccl.net  Fri Aug 25 06:16:47 2000
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Subject: Re: Ahem, shouldn't we do something about it?
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Hi there,

I didn't follow the start of the discussion, so could somebody clarify
if we talk about preprints of papers that

a) possibly have been published in a journal
b) possibly will be published in a journal
c) are exclusively published on the web (making it an online journal)

The questions associated with a) and b) mainly refer to the publishing
policy of printed journals:

a) Is this allowed? The journal owns the copyright. The author typically
may give away copies, but publishing on the web is a step further. How
do different journals handle this? From the user perspective, it's of
course desirable, because not everybody has a well-stocked library in
the same building (or the same city).

b) Will journals accept something that's already on the web as "original 
and unpublished work"?

c) The advantage is that it's faster than going through the refereeing
and publishing process, and there are (rare) cases where more politics is 
involved than science. But won't it attract mainly the trash that would
never make it past the referees? Archimedes Plutonium and friends (if 
you've ever read sci.physics, you know him)? 

I'm not sure if an open rating system would work either. Chances are 
that it will be hijacked by a few opinionated busybodies, while the 
majority of readers don't find time to submit a rating.

  Herbert


From chemistry-request@server.ccl.net  Fri Aug 25 10:44:58 2000
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Ups, forgot one more response..sorry about that:

Response 10: Leif Norskov
=========================
I think Corel Draw should be able to do it - but not for free.
(check http://www.corel.com/)

/Leif Norskov
 Novo Nordisk A/S
 LNL@novo.dk

___________________________________________________________________________

  Cherif F. Matta		    	  tel. (905) 525-9140 ext. 22502
  Chemistry Department                    fax  (905) 522-2509
  McMaster University                               _______________________ 
  Hamilton, Ontario, CANADA L8S 4M1.                | "Choice not chance
....................................................|  determines one's  
 Member of the Board of Governors of the University |  destiny". Anonymous 
___________________________________________________________________________



From chemistry-request@server.ccl.net  Fri Aug 25 11:26:13 2000
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Subject: Re: CCL:SUMMARY: How to rotate a PostScript file?
From: Eric Bittner <bittner@uh.edu>
To: "C.F. Matta" <mattacf@mcmail.cis.mcmaster.ca>, <CHEMISTRY@ccl.net>
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on 8/25/00 9:44 AM, C.F. Matta at mattacf@mcmail.cis.McMaster.CA wrote:

> 
> Ups, forgot one more response..sorry about that:
> 
> Response 10: Leif Norskov
> =========================
> I think Corel Draw should be able to do it - but not for free.
> (check http://www.corel.com/)
> 
> /Leif Norskov
> Novo Nordisk A/S
> LNL@novo.dk
> 
> ___________________________________________________________________________
> 
> Cherif F. Matta         tel. (905) 525-9140 ext. 22502
> Chemistry Department                    fax  (905) 522-2509
> McMaster University                               _______________________
> Hamilton, Ontario, CANADA L8S 4M1.                | "Choice not chance
>> ....................................................|  determines one's
> Member of the Board of Governors of the University |  destiny". Anonymous
> ___________________________________________________________________________
> 
> 
> 
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> 


Hi, 

two free ways that work:
 you can rotate a PS file by simply editing it. It takes a bit of
trial and error and you sort of have to know what to look for.

use  the graphics package in Latex to write a wrapper that loads the file,
rotates it creates a dvi file with the new figure.  This is really easy.

As a last + costly method
convert them to PDF (using acrobat distiller) and then edit the pdf
file using adobe illustrator.

-Cheers!
ERB

-- 
Prof. Eric R. Bittner
Department of Chemistry
Univ. of Houston
http://eiger.chem.uh.edu/bittner/



From chemistry-request@server.ccl.net  Fri Aug 25 12:51:24 2000
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Date: Fri, 25 Aug 2000 12:55:45 -0400
From: elewars <elewars@trentu.ca>
Subject: SUMMARY DFT ORBITALS, WF
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Friday, 2000 Aug 25

Hello,

here is the summary of replies to my question about orbitals and
wavefunctions in DFT. I got 12 replies:
#1 D. Mathieu, #2 and #3 E. Scerri, #4 E. Proynov, #5 H. van Dam, #6 A.
Bittner, #7 J. Spanget-Larsen, #8 U. Richter, #9 A. Shusterman, #10 K.
Nguyen, #11 J. Smith, #12 R. Jensen. I hope no one has been overlooked.
Thanks very much to all who responded.

I don't think question 3 can really be answered definitively yet. I'll
leave this topic with the thought that an electron density is an
observable (it can be measured), while a wavefunction is a recipe, a
prescription, a Vorschrift--use it in a certain way and you get the
right answers.

THE QUESTION
Sat 2000 Aug 19

Hello,

We know that in pure DFT (in contrast to wavefunction theory) there are
are no orbitals and there is no wavefunction; the Kohn-Sham orbitals of
current practical DFT methods were introduced to make the calculation of

the electron density tractable.

QUESTIONS
(1) An important feature of ab initio (and semiempirical) calculations
is that one can visualize the orbitals, particularly the HOMO and LUMO
(frontier orbitals) and make chemical deductions. In a _pure_ DFT
calculation a question about the shape and energy of these orbitals
would be meaningless, right?

(2) The Fukui function (R. G. Parr and W. Yang, J Am Chem Soc, 1984,
106, 4049) seems to be always discussed in the context of DFT; yet this
function is "a chemical reactivity index in the sense of the
frontier-electron theory of reactivity..." (R. G. Parr and W. Yang,
"Density-Functional Theory of Atoms and Molecules", Oxford, New York,
1989, p. 101). But in pure DFT theory there are no frontier orbitals.
Isn't this strange?

(3)
If, as has been suggested (Parr and Yang, "Density-Funtional Theory...",

p. 53) wave mechanics can be reformulated without the wavefunction
concept, what are we to make of the 80-year-old debate in physics and
philosophy about the meaning of the wavefunction (wavefunction collapse,

Schroedinger's cat, the many-worlds theory of QM, etc, etc, etc; see
e.g. "Einstein, Bohr and the Quantum Dilemma", A. Whitaker, Cambridge
University Press, Cambridge, 1996, and _many_ other books and
papers...). Was this debate a meaningless exercise that would never have

occurred if QM had been originally formulated in terms of electron (or
more generally, particle) density rather than the wavefunction?

Thanks,

E. Lewars
====
THE REPLIES

#1  Didier Mathieu, mathieu@ripault.cea.fr

> In a _pure_ DFT
> calculation a question about the shape and energy of these orbitals
> would be meaningless, right?

While the concept of orbitals is not necessary, it might be possible to
define
orbitals from the density obtained from "pure DFT"and its responses to
changes of
the Hamiltonian. It might then turn out that such orbitals, wile no
physical
observables, can be given some physical meaning a posteriori.

> 1989, p. 101). But in pure DFT theory there are no frontier orbitals.
> Isn't this strange?

Why ? Fukui functions are defined independently of the notion of
orbitals. Thus, I
see them as an natural alternative - whithin DFT - to frontier orbitals
and
perturbation theory in order to interpret chemical reactivity.

> papers...). Was this debate a meaningless exercise that would never
have
> occurred if QM had been originally formulated in terms of electron (or

> more generally, particle) density rather than the wavefunction?

In that case, I wonder how these physical concepts would have emerged.
Clearly, the one-particule density is not suitable as it does not
contains all the
information about the system.
However, QM has also been formulated in terms of the density matrix
since the
beginning.
For me, probably for historical reasons, it is easier to grasp many QM
ideas in
terms of the wavefunction, also because some of the basic notions
involve
"interference effects", (sorry for being so conditioned by the
wavefunction
picture) and the phase of the wavefunction might be more suitable than
the
coherences of the density matrix to study them.
On the other hand, in some cases, the influence of the environment on
the quantum
system considered is more naturally introduced in the density matrix
formulation:
for instance when adding the phenomenological relaxation rates T1 and T2
to the
evolution equation in NMR. This sounds more natural than modifying the
Shrodinger
equation through adding a non-hermitian term to the hamiltonian.

Cheers,

Didier.

===
#2  Eric Scerri,  scerri@purdue.edu

But surely the shape of the electron density which would correspond
to these orbitals could still be visualized if necessary, just as
electron density can be in the ab initio wavefunction approaches.

The two approaches are alternative ways of looking at the micro
world.  Whether one chooses to visualize, or not, is always an option
in any theory.  But perhaps you ar asking a more specific question
like what do HOMO and LUMO electron density plots look like?

Please clarify your question (1)

eric scerri


-------------------------------------------------
Eric Scerri PhD,
Visiting Professor,
Department of Chemistry & Biochemistry,
UCLA,
Los Angeles,  CA 90095
USA
---
I replied:
Hello,

I'll summarize the answers, maybe with some comments. But concerning
your answer:
in wavefunction theory we have a series of atomic or molecular orbitals,
psi_1,
psi_2,..., with increasing energy. I think that in a pure density
functional theory
we just have an electron density function, rho(r); not a series of
electron
densities. So there is no electron density rho_1 corresponding to a
certain
orbital , and another density rho_2 corresponding to another orbital,
etc. Just one density function. But maybe I have overlooked
something--so I am
asking the chemical community for their thoughts. And it just occurrs to
me that
one might wonder how this fits in with photoelectron spectroscopy, which
indicates
that molecules have groups of electrons of different energies.

thanks

EL
====
#3  Eric Scerri

I dont know enough about DFT to know the answer to this further
point.  I would guess that it is possible to recover some kind of
shell tructure from DFT.  Please let me know what you discover from
others.  I am also still puzzling over your No 3.

You ask interesting philosophical questions.  Please consider joining
the Philchem list.

  the address can be found on the web pages for the International
Society for the Philosophy of Chemistry after the section on the
recent meeting in Poznan.

====
#4 Emil Proynov,  proynov@chimie.umontreal.ca

Dear Dr Elewards,

I would suggest not to get so upset by those who claim that the
Kohn-Sham (KS) determinantal
wavefunction does not have a physical meaning. The SCF potential, as
defined
in the KS DFT scheme, determines a self-consistent field such that the
KS determinant
minimizes the electron kinetic energy and yields the exact electron
density. It
differs from the Hartree-Fock (HF) self-consistent field in what the
latter is associated
with the HF determinant (minimizes the total energy but does not yield
the
exact electron density). To any meaningful self-consistent field one can

assign SCF one electron orbital picture with a portion of
physical/chemical meaning in it.
To my opinion there is nothing mysterious in the KS SCF field, just to
keep in mind that
it does not originate directly from the Schrodinger equation
but from the Euler equation of the DFT variational task. It is true that
in the latter
one does not deal directly wavefunctions, but all the quantum mechanics
with its
postulates, theorems and paradoxes is hidden there in the
exchange-correlation potential.

You can find different opinions on this in the literature indeed. The
matter is perhaps
more complicated that I am trying to make it with this comment. Just to
note that
an increasing amount of theoretical studies use and refer explicitly to
the KS
SCF orbitals demonstrating their practical utility (see for example: I.
Verdernikova et.al.
Int. J. Quant. Chem. vol.77, 161 (2000)).

Best wishes,

Emil Proynov

+-----------------------------+
| Emil Proynov                |
| proynov@chimie.umontreal.ca |
+-----------------------------+

=====

#5  Hub van Dam,  h.j.j.vandam@dl.ac.uk

(Question 1)
People try that sort of thing, yes. But I am not sure if this really
works in
cases where there is strong static correlation. In other words where you
have a
wavefunction (again) with multi configurations with large coefficients.

(Q2)
Yes, this seems very strange.

(Q3)
The 74 year old debate, autumn next year the Schroedinger equation will
have been
around for 75 years (I haven't heard any plans yet of how people want to

commemorate this anniversary). I would like to think that quantum
mechanics only
obtained a firm foundation with Schroedingers wave-equations. Anyway, I
don't
think this was a meaningless exercise. Although the wavefunction in
itself has no
direct physical interpretation, we still need it to get the probability
density
right. I.e. the probability to find a particle at a certain point in
space behaves
like there is some superposition of waves involved. Trying to formulate
quantum
mechanics in terms of the electron density only, and at the same time
including
these superposition effects correctly is a far from trivial matter (I
think it is
save to say that this problem is unsolved). Therefore I think that
although the
wavefunction has not direct physical interpretation it is far from
"meaningless"
concept.

Kind regards, Huub

--

========================================================================

Huub van Dam                               E-mail: h.j.j.vandam@dl.ac.uk

CCLRC Daresbury Laboratory                  phone: +44-1925-603362
Daresbury, Warrington                         fax: +44-1925-603634
Cheshire, UK
WA4 4AD

======
#6  Eric Bittner,  bittner@uh.edu

No, There is the issue of measurement, interference, causality, etc..
which
you can not simply sweep under the rug by invoking a density.
The debate over the ontology of quantum mechanics continues and is
perhaps
extremely relevant in the advent of quantum computers.  Perhaps if your
only
interested in using quantum theory as an algorithm for making
predictions
about physical reality,  the debate is pointless.  However, if you
really
and truly want to understand the inner workings of nature, it is not.

IF you do choose to only work with the density, rho(x), you are not
representing the full physical picture.
QM is completely formulated in terms of
the density, which evolves under the continuity equation, AND the
quantum
Hamilton-Jacobi equation,

\frac{\partial S}{\partial t} - H(p,q) -
\frac{\hbar^2}{2m}\frac{1}{\sqrt{\rho}}\nabla^2 \sqrt{rho} = 0

where H(p,q) is the Hamiltonian with the canonical substitution p->
\nabla
S/m and the last term is the quantum potential, Q.

If you seek stationary states, i.e. d\rho/dt = 0, then the QHJ  reduces
to
the time-independent Schrodinger equation.

These equations of motion
are easily derived from the Schrodinger eqn. by writing
 psi = R exp(i S/hbar)
and defining the density as rho = |psi|^2.

On the computational side of this:
Bob Wyatt and I have recently developed methods to solve these equations
of
motion using ONLY the trajectories they imply...no wave function, no
basis
functions...only quantum paths.
A pre-print version of one of our papers is included as an attachment
(pdf
format).


-Cheers,
Eric R. Bittner
U. Houston

--
Prof. Eric R. Bittner
Department of Chemistry
Univ. of Houston
==========

#7  Jens Spanget-Larsen,  jsl@virgil.ruc.dk

(Q1)
Or, in other words: "What Do the Kohn-Sham Orbitals and Eigenvalues
Mean?".
Stowasser and Hoffmann address this question in their recent paper -

Ralf Stowasser & Roald Hoffmann: J. Am. Chem. Soc. 121, 3414-3420
(1999).

Yours, Jens >--<

=-=-=-=-=-=-=-=-=-=-=-=-=-=-=-=-=-=-=-=-=-=-=-=-=-=-=-=-=-=-=-=
JENS SPANGET-LARSEN         Phone:  +45 4674 2000  (RUC)
Department of Chemistry             +45 4674 2710  (direct)
Roskilde University (RUC)   Fax:    +45 4674 3011
P.O.Box 260                 E-Mail: JSL@virgil.ruc.dk
DK-4000 Roskilde, Denmark
=========

#8  Uwe Richter,  uwe@nist.gov

Hi,

I'm very interested in answers to this questions. Please could you
summarize
or send me the responses directly? There are some people who even
discuss
virtual KS orbitals.

Thanks,
Uwe
===========

#9  Alan Shusterman,  Alan.Shusterman@directory.reed.edu

These are great questions. I'd be grateful if you would pass along any
answers you receive. Thanks,

-Alan
alan@reed.edu

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

#10  Kiet Nguyen,  Kiet.Nguyen@wpafb.af.mil

Although there is considerable controversy in the literature concerning
the meaning of
Kohn-Sham orbitals,  I think they are far from "meaningless".  This
topic has been carefully
analyzed and reviewed.[1-5]   Parr and Yang stated that "... one should
expect no simple
physical meaning for the Kohn-Sham orbital energies."[3]  However,
using the Janak theorem
which "provides a meaning for the eigenvalues of the Kohn-Sham
equation", they have connected
the HOMO and LUMO energies to the ionization potential and electron
affinity,
respectively.[3]

[1]   E. J. Baerends and O. V. Gritsenko, J. Phys. Chem. A 101 (1997)
5383.
[2]   R. G. Parr and W. Yang, Density Functional Theory of Atoms and
Molecules (University
Press,  Oxford, 1989).
[3]   J. P. Perdew, in: Density Functional Methods in Physics, edited by
R. M. Dreizler and
J. da Providencia New York, 1985), p. 265
[4]   E. J. Baerends and O. V. Gritsenko, J. Phys. Chem. A 101 (1997)
5383.
[5] R. Stowasser and R.  Hoffman, J. Am. Chem. Soc. 121 (1999),  3414.

Kiet A. Nguyen
AFRL/MLPJ
Laser Hardened Materials Branch
Wright-Patterson AFB, OH  45433
Phone (937) 255-6671, Ext 3178
FAX   (937) 255-1128

==========

#11  Jack Smith,  Smithja@ucarb.com

(We know that in pure DFT...no wavefunction)
At least not explicitly.  One-electron orbitals are not required for
wavefunction theory either.  I would say that the two approaches
converge
when you reduce it to N-electron density matrices (probably even at the
2-electron density matrix level).

(The KS orbitals...electron density tractable)
Particularly to make the kinetic energy part tractable.  Orbitals also
made
wavefunction theory more tractable by introducing the
pseudo-one-particle
SCF equations, which further allowed for the formulation of the Roothan
equations (for a basis set expansion approach).

> My feeling is that Natural Orbitals from a CI calculation
(eigenvectors of
> 1-particle density matrix) should correspond to KS orbitals with
> fractional occupations.  Is there an analog to Natural Geminals (from
the
> 2-particle density matrix) in DFT?



(In a pure DFT calc., a question about the shape and energy of these
orbitals would be meaningless, right?)
Orbitals, yes; orbital densities, no.  The density differences between
the
neutral system and its various ionic states are in principle observable
quantities (assuming you can get xray diffraction data for the ions).
Under
Koopmans' approximation these density differences should be the same as
the
orbital-derived densities.  And the orbital energies should correspond
to
the ionization (electron attachment) energies.  A similar correspondence
can
be defined for orbital density differences among different excited
states.
One thing that's missing from a pure density picture is the concept of
overlap and orthogonality, which depend on the sign of the underlying
one-electron orbitals (wavefunctions).  Overlap is a key component of
frontier orbital theory.  Should it be?  Is there a pure density analog?



(The Fukui function.. But in a pure DFT theory these are no orbitals.
Isn't this strange?)
But there ARE frontier orbital DENSITIES.  The +/- Fukui functions
should
correspond to the orbital densities mentioned above for whole electron
changes (N +/-n).  However, in an "open" sysem (in a Grand Canonical
sense)
where fractional electrons can come and go, the Fukui function can also
be
defined for infinitessimal changes in electron number - a continuous
functional of the number of electrons.  Thus, derivatives in the density
wrt
electron number can be defined even at N electrons.  The corresponding
derivative in energy would be the chemical potential, and the second
derivative would be the hardness -- with no need to define a HOMO or
LUMO
and use crude finite difference approximations (along with Koopmans'
approximation).

> (3)
> If, as has been suggested (Parr and Yang, "Density-Funtional
Theory...",
> p. 53) wave mechanics can be reformulated without the wavefunction
> concept, what are we to make of the 80-year-old debate in physics and
> philosophy about the meaning of the wavefunction (wavefunction
collapse,
> Schroedinger's cat, the many-worlds theory of QM, etc, etc, etc; see
> e.g. "Einstein, Bohr and the Quantum Dilemma", A. Whitaker, Cambridge
> University Press, Cambridge, 1996, and _many_ other books and
> papers...). Was this debate a meaningless exercise that would never
have
> occurred if QM had been originally formulated in terms of electron (or

> more generally, particle) density rather than the wavefunction?
>
It just means that all the debate is focused on the form of energy
functional itself, the exchange and correlation parts in particular,
rather
than the wavefunction.  One still has to explain the particle-wave
duality
of the electron beam experiments.  The outcome is still probabilistic
(non-deterministic for a given electron) whether you speak in terms of
electron density or a wavefunction.  The concepts of exchange and
correlation are still very much "quantum" phenomena, whether you
encapsulate
in a quantum-constrained probabilistic wavefunction and a classical
Hamiltonian (energy) operator, or in a classical-like probabilistic
electron
density and a quantum-constrained energy functional.

DFT-KS and HF only converge when HF exchange is used, no correlation
term is
included, AND the Grand Canonical (GC) form of the density operator is
used.
DFT-KS and MC-SCF converge as the MC-SCF approach a full CI and the
correlation functional approaches the "exact" expression, but again only
if
the GC form of the density operator is used.  An interesting middle
ground
would be a Natural Orbital iteration on a small CI, or a VB wavefunction

using non-orthogonal orbitals, or GC UHF using localized fractionally
occupied nearly-orthogonal orbitals.  (As you might tell, I'm a an
advocate
of the latter - which should have a correspondence with DFT-KS, given
the
right functional).

My 2 cents' worth.

- Jack

-=-=-=-=-=-=-=-=-=-=-=-=-=-=-=-=-=-=-=-=-=-=-=-=-=-=-
 Jack A. Smith             ||
 Union Carbide             || Phone:  (304) 747-5797
 Catalyst Skill Center     || FAX:    (304) 747-4672
 P.O. Box 8361             ||
 S. Charleston, WV  25303  || smithja@ucarb.com
-=-=-=-=-=-=-=-=-=-=-=-=-=-=-=-=-=-=-=-=-=-=-=-=-=-=-

=====

#12  Roy Jensen,  royj@uvic.ca

Have you had any response to your questions. I would be very
interested to hear the results. Please post a summary to the CCL.

Roy Jensen
===================
================
=========










From chemistry-request@server.ccl.net  Fri Aug 25 10:22:46 2000
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Date: Fri, 25 Aug 2000 10:22:33 -0400 (EDT)
From: "C.F. Matta" <mattacf@mcmail.cis.McMaster.CA>
To: CHEMISTRY@ccl.net
Subject: SUMMARY: How to rotate a PostScript file?
In-Reply-To: <Pine.SOL.4.21.0008211048370.26463-100000@mcmail.cis.McMaster.CA>
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Hello,

I would like to thank all those who kindly responded to my question: 
         "how to rotate a postscript file": 
Rajendra Zope, Thomas Heine, Antonio Buljan, T. Daniel Crawford, Heidi
M. Muchall, Xavier Fradera, David van der Spoel, Michael Braunschweig,
Antonio Marquez Cruz.  Thank you all.

Here are their individual responses in the order received:

Response 1:  Rajendra Zope 
==========================
From: Rajendra Zope <zope@drfmc.ceng.cea.fr>

I am also in need of a package which can merge two or more  postscript
files into a single file. Please kindly notify me or summarize the
responses to your querry.

Rajendra Zope
---------------------------------------------------------------------------
Rajendra Zope                       e-mail: rzope@cea.fr
 DRFMC/SI2A                          e-mail: zope@drfmc.ceng.cea.fr
 CEA-Grenoble                        Tel: 04 76 88 45 04
 17, rue des Martyrs                 FAX: 04 76 88 51 60
 F-38054 Grenoble Cedex 9
 FRANCE
--------------------------------------------------------------------

Response 2: Thomas Heine
========================
From: Thomas Heine <Thomas.Heine@chiphy.unige.ch>

90 rotate
(rotates by 90 degrees)
100 100 translate
(translates in x/y direction which you will need to fix it to the place}
Make sure to put it behind the bounding box (the stuff with the %)

Thomas

Response 3:  Antonio Buljan
============================
From: Dr. Antonio Buljan <abuljan@udec.cl>

the command is rotate alpha,
where alpha is the angle.
Now, alpha can be positive or negative.
If you don't can do it, send the postscript file and I can fix it.
I have some experience with this matter.

Antonio

Response 4:  T. Daniel Crawford
===============================
From: T. Daniel Crawford <crawdad@vt.edu>

You could try (1) converting the PS file to a PNM using the pstopnm
utility,
(2) using pnmrotate to rotate the new image, and then (3) use pnmtops to
convert back to a PS file.  All three of these utilities are available
on RedHat Linux systems, but I don't recall where to find them for other
systems.  A web search might help you there.

-Daniel
--
T. Daniel Crawford                           Department of Chemistry
crawdad@vt.edu                          Virginia Polytechnic Institute and
www.chem.vt.edu/chem-dept/crawford              State University

Response 5:  Heidi M. Muchall
=============================
From: Dr. Heidi M. Muchall <muchall@alcor.concordia.ca>

just put 90 rotate for a counterclockwise rotation of 90 deg. or -90
rotate
for clockwise. Any other angle will work, too. You might have to adjust
the
translate values, too. How's it going at Mac?
Heidi
*************************************************************
Dr. Heidi M. Muchall     | e-mail: muchall@alcor.concordia.ca
Assistant Professor      |
Department of Chemistry  |
  and Biochemistry       |
Concordia University     | phone: (514) 848-3342
Montreal, Quebec H3G 1M8 |
Canada                   | fax: (514) 848-2868
*************************************************************

Response 6: Xavier Fradera
========================== 
From: Xavier Fradera <iqcxfl@xamba.udg.es>

you could also try using Gsview. I'm not sure about it, but I think it
allows you to read a postscript file, change its orientation (i.e.,
portrait to landscape) and save it. Have a look at:
http://www.cs.wisc.edu/~ghost/

Xavier.

Response 7: David van der Spoel
===============================
From: David van der Spoel <spoel@xray.bmc.uu.se>

put:
rotate angle
in front of the real code.

Groeten, David.
________________________________________________________________________
Dr. David van der Spoel         Biomedical center, Dept. of Biochemistry
s-mail: Husargatan 3, Box 576,  75123 Uppsala, Sweden
e-mail: spoel@xray.bmc.uu.se    www: http://zorn.bmc.uu.se/~spoel
phone:  46 18 471 4205          fax: 46 18 511 755
+++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++

Response 8: Michael Braunschweig
================================
From: michael braunschweig <charly@citrin.chemie.uni-dortmund.de>

try the "rotation" package in latex. including the two ps files als
pictures you can rotate them and create a new one.

michael braunschweig
department of chemistry
university of dortmund
germany

Response 9: Antonio Marquez Cruz
================================
From: Antonio Marquez Cruz <marquez@cica.es>

my $0.02 contribution:

the command to rotate a file is

x rotate

where "x" is the rotation angle (positive as well as negative angles can
be used). Try different values until you get the best fit of your two
files. You may need also to translate your files at the same time.

Dr. Antonio M. Marquez
Dpt. of Physical Chemistry                      Dpto. de Quimica Fisica
University of Seville                           Universidad de Sevilla
E-41012 Seville (SPAIN)                         41012-Sevilla
Phone:  34-95-4557177                           FAX: 34-95-4557174

====================================================================

Cherif F. Matta

___________________________________________________________________________

  Cherif F. Matta		    	  tel. (905) 525-9140 ext. 22502
  Chemistry Department                    fax  (905) 522-2509
  McMaster University                               _______________________ 
  Hamilton, Ontario, CANADA L8S 4M1.                | "Choice not chance
....................................................|  determines one's  
 Member of the Board of Governors of the University |  destiny". Anonymous 
___________________________________________________________________________




From chemistry-request@server.ccl.net  Fri Aug 25 10:34:48 2000
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Date: Fri, 25 Aug 2000 09:34:36 -0500
Subject: On line preprint/reprint server.
From: Eric Bittner <bittner@uh.edu>
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I've been following the discussion regarding a Chemistry Online
preprint/reprint service.
This already exists in the physics community and has been extremely
successful and basically self reviewed.
The URL is http://xxx.lanl.gov/
Sure, there is a lot of bolognia and you have to filter some of this out.
But, it's a great way to
get the really latest and greatest results and opinions.  It's heavily
theoretical (eq. quant-ph ) but there is certainly a healthy portion of
experimental papers.  Moreover, some of the best physics discussions I've
seen have been posted on this server.
Moreover, Phys. Rev. will consider postings to the LANL server as
submissions if the author chooses to do inform PR of the posting.
In fact, I have found that in some cases I have gotten *better* reviews
(i.e. more critical) of preprints I've posted to LANL...often better and
more critical than journal reviewers. (plus it's either in the open forum or
by email.  In either case, you know who your critics are.)

Also, I've never seen "Archimedes Plutonium" or Mills (of Blacklight
Power.com) post any thing on the server. I'd love to see Mills post his
"hydrino" theory on the server.

My $0.02
ERB

-- 
Prof. Eric R. Bittner
Department of Chemistry
Univ. of Houston
http://eiger.chem.uh.edu/bittner/




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Bachrach, Steven writes:
 > 
 > First, NOTHING kept anyone from starting such an effort at any time in the
 > past. In fact, the Chemistry Preprint Server form ChemWeb is NOT the first
 > such effort in chemistry. Way back in 1994 and 1995 (ancient history on the
 > web), a Chemical Physics preprint server was enacted originating from Brown
 > University utilizing the same code as the LANL preprint server. This effort
 > was essentailly a failure as few authors submitted.

I have a suspicion that the choice of the canonical publishing format
used for http://xxx.lanl.gov (LaTeX), albeit being natural to
physicists and mathematicians and convenient, since allowing
automatical generation of multiple formats on the fly (necessary for
future portability), was too intimidating for the typical chemist.

AdobeAcrobat files (the de facto standard in online publishing) can be
difficult to index/search, and I've noticed that some .pdf files do
break GhostScript (a suite of applications created around a free
PostScript interpreter) rendering. No robust OpenSource crossplatform
reader is thus so far available, making .pdf a risky standard to
adapt. (As far as I can tell .pdf prepared via the ps2pdf route
renders ok with AdobeAcrobat). A scientific publishing standard has to
be noncommercial, to guarantee its long-term readability. This can
only be defined by a few-person independant commitee, who will also
have to supply a demo implementation.
 
 > [...]
 > Third, there is no question that Chemweb is a subsidiary of Elsevier.
 > However, I question exactly what has been given to the Elsevier monopoly
 > here. When an author places an article into the preprint archive, the author
 > assigns no rights to Chemweb. The author retains the copyright and all
 > rights associated with the article. Elsevier cannot charge for access to the
 > article or reproduce it in any form without the express written consent of
 > the author. Chemweb (or Elsevier if you prefer) acts as the conduit for
 > access. Fairly subtle ad placement is the only source of income for Chemweb
 > for providing this service. (In the interest of full disclosure, I am on the
 > advisory board for the CPS.)

I'd rather not give a single commercial body opportunity to establish
itself as the de facto standard. Once a user base has been created,
things will impercerceptibly start to change, commercial interests
attempting to lock users into place, and to keep them there by
balkanizing what for user's sake should remain a single
community. Proprietary "standards" will be introduced, users will have
to register themselves to allow tracking for marketing purposes, in
absence of open mirrors, content is entirely at the publisher's mercy
constituting a single-point failure, etc.
 
The issue is much too important to be trusted to a single commercial
vendor, however benign. As I understand, some of Elsevier's business
practices are being frowned upon in the librarian/user
community. Somehow, I do not believe that Elsevier's motives this time
are entirely lily-white.

 > Lastly, my conclusion form the plenary session on online preprints was that
 > many people are unaware of what a preprint server is and what its
 > implications really are. Unquestionably, education of the chemical community
 > IS the first priority towards making any serious change to our publication
 > system. I concur with Steve Berry who argued at the plenary session that we
 > should be trying many different experiments, learning along the way,
 > adopting good things and throwing out those that fail. I view the CPS as
 > being one of the necessary experiments and hope that many more experiemnts
 > in publication (not just preprint severvices) will follow in the near
 > future.

The question of peer-review in regards to e-preprint servers has come
up in this thread. Both issues are independant of each other. A
peer-review authority, whether commercial or free (as I understand
peer reviewers are typically not being reimbursed for their pains) can
of course digitally sign pointers to the documents in the public
e-preprint archive, or store digitally signed peer-reviewed documents
verbatim on their own server.

I think it should be very possible to attract a minimal number of
volunteer developers and have a sufficient number of administered
storage and bandwidth donated for an alternative e-preprint
server. Maybe it's time to move this to sourceforge.


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there is always some garbage, particularly on the web.  i'd rather read
other opinions/research results and decide for myself.  some garbage
even gets through peer review.  there could still be a mechanism
to block papers from people who consistently post garbage, and
who don't have any credentials.  it would also be nice to have
a brief summary of the authors credentials, even if not
verified.  it's been my experience that there are allot
of politics involved with most of the science journals.


Christoph van Wüllen wrote:
> 
> As to the discussion of 'online publishing', my opinion is that if the
contributions
> are not peer-reviewd (using the same quality standards as in the printed journals),
> there is always the risk that there will be some garbage among the contributions.
In this
> case, not too many scientist will browse the contents.
-- 
"..a cynic is just a romantic who got mugged watching sausage being made last night" Klima and the
Belmonts ("negations," 1964)


From chemistry-request@server.ccl.net  Fri Aug 25 14:57:33 2000
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Date: Fri, 25 Aug 2000 11:27:37 -0700
From: "Jason K. Perry" <jkp@firstprinciples.com>
Subject: Ahem, shouldn't we do something about it?
To: chemistry@ccl.net
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I'm a regular follower of the xxx.lanl.gov/cond-mat high temperature
superconductivity e-print server (check out
http://xxx.lanl.gov/list/cond-mat.supr-con/recent).  The server has
become a vital part of research in this particular field, where peer
review is extremely slow (publication of theory papers routinely takes
more than one year and is often subject to politics).  There are no
forums for ranking or commenting on the papers.  It's just a fast
delivery service for preprints.  This, of course, is its biggest
advantage.

Some of the papers on this site have been uploaded after being accepted
for publication in a journal, but most are uploaded in conjuction with
journal submission. Physical Review even allows transfer of a paper
directly from the Los Alamos server when submitting for publication
on-line.  The APS is definitely way ahead of the ACS in this arena.

While I recognize that peer review is an important process for catching
errors, and the papers on this site should be approached carefully, in
general I like being able to judge for myself if a paper has merit or
not.  I definitely appreciate having access to the most cutting edge
work in the field.

I'm not sure yet how this might play out in chemistry.  Research topics
are much more diverse than in physics, and the review process is not
quite as bad.  This suggests the demand for an e-print server may be
less.  Still, I would like to see a server devoted to computational
chemistry.  Something in conjuction with CCL would be ideal...

    Jason Perry

--
..................................................................
Jason K. Perry, Ph.D.
First Principles Research, Inc.
8391 Beverly Blvd., #171, Los Angeles, CA 90048
phone (323) 465-9572
FAX (323) 465-2805
http://www.firstprinciples.com
..................................................................



