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   [We apologize should you receive multiple copies of this CFP.]

----------------------------------------------------------------------
    9th International Conference on Neural Information Processing 
                         (ICONIP'02)
    4th Asia-Pacific Conference on Simulated Evolution And Learning 
                          (SEAL'02)
   International Conference on Fuzzy Systems and Knowledge Discovery 
                          (FSKD'02)
----------------------------------------------------------------------
        November 18 - 22, 2002, Orchid Country Club, Singapore
                 http://www.ntu.edu.sg/home/nef      
                       
                         Organized by:
           School of Electrical and Electronic Engineering
             Nanyang Technological University, Singapore

                         Sponsored by:
                Asia-Pacific Neural Network Assembly
                  SEAL & FSKD Steering Committees
                         Lee Foundation

                      In Co-Operation with:
                   IEEE Neural Network Council
               International Neural Network Society 
                  European Neural Network Society 
                            SPIE 

               ----------------------------------
               CALL FOR PAPERS, SPONSORSHIPS, AND 
                   SPECIAL SESSION PROPOSALS
               ----------------------------------

ICONIP'02, SEAL'02, and FSKD'02 will be jointly held in Orchid Country
Club, Singapore from November 18 to 22, 2002. The conferences will 
not only feature the most up-to-date research results in neural 
information processing, evolutionary computation, fuzzy systems, and 
knowledge discovery, but also promote cross-fertilization over these 
exciting and yet closely-related areas. Registration to any one of the 
conferences will entitle a participant to the technical sessions and 
the proceedings of all three conferences, as well as the conference 
banquet, buffet lunches, and tours to two of the major attractions in 
Singapore, i.e., Night Safari and Sentosa Resort Island. Many well-
known researchers will present keynote speeches, panel discussions, 
invited lectures, and tutorials.

About Singapore
---------------
Located at one of the most important crossroads of the world, 
Singapore is truly a place where East and West come together. Here you 
will find Chinese, Indian, and Malay communities living together, 
their long established cultures forming a unique backdrop to a clean 
and modern garden city. English is spoken everywhere and is the common 
business language of all. Few places on earth promise such a delight 
for the palate, with gourmet cuisine from over 30 countries. Exotic 
resorts in neighboring countries are only a short bus/ferry ride away.

Orchid Country Club (OCC)
-------------------------
The venue for this year's conferences is at one of Singapore's 
premier country club, a 25-minute bus ride from the city. Away from 
the hustle and bustle of downtown Singapore, the tranquil setting of 
the resort is ideal for serious technical discussions with an 
accommodating space and ambience for relaxation. Not to miss out on 
the splendor of downtown Singapore, the organizer has also secured 
good quality and affordable accommodation in the heart of the city 
with pre-arranged transport to/from the OCC. For golf enthusiasts, 
OCC is equipped with the largest computerized driving range in South 
East Asia and boasts of a 27-hole golf course with facilities for 
night golfing, ideal for relaxation after each day of technical 
discussions. Visit the OCC website at http://www.orchidclub.com

Night Safari and Sentosa Resort Island 
--------------------------------------
It is said that a visit to Singapore is not complete without making 
a trip to two of the Republic's famous attractions. The only one of 
its kind in the world, the Night Safari provides a setting for 
visitors to experience what it is like to observe animals in their 
nocturnal habitat. The island of Sentosa offers some unique 
attractions and a visit there will also provide a glimpse and 
imagery of Singapore's past and present. Visits to these two 
attractions will be included as recreation for the joint conference.
(Websites: http://www.zoo.com.sg/safari/, http://www.sentosa.com.sg)

Submission of Papers 
--------------------
Authors are invited to submit electronic files (postscript, pdf or 
Word format) through the conference home page. Papers should be 
double-column and use 10 pt Times Roman or similar fonts. The final
version of a paper should not exceed 5 pages in length. A selected 
number of accepted papers will be expanded and revised for possible 
inclusion in edited books and peer-reviewed journals, such as 
"Soft Computing" and "Knowledge and Information Systems: An 
International Journal" by Springer-Verlag.

Special Sessions
----------------
The conferences will feature special sessions on specialized topics 
to encourage in-depth discussions. To propose a special session, email
the session title, name of the conference under which the special 
session will be oragnized, contact information of the organizer(s), 
and a short description on the theme and topics covered by the 
session to Xin Yao, Special Sessions Chair (x.yao@cs.bham.ac.uk), 
with a copy to Lipo Wang, General Chair (Cc: elpwang@ntu.edu.sg).  

Sponsorship
-----------
The conferences will offer product vendors a sponsorship package 
and/or an opportunity to interact with conference participants. 
Product demonstration and exhibition can also be arranged. For more 
information, please visit the conference website or contact 
Tong Seng Quah, Sponsorship/Exhibition Chair (itsquah@ntu.edu.sg), 
with a copy to Lipo Wang, General Chair (Cc: elpwang@ntu.edu.sg).

Keynote Speakers 
----------------
Shun-ichi Amari, RIKEN Brain Science Institute, Japan
David Fogel, Natural Selection, Inc., USA
Mitsuo Kawato, ATR, Japan
Xin Yao, The University of Birmingham, UK
Lotfi A. Zadeh, University of California, USA

Important Dates
---------------
	Paper/Summary Deadline     :   April 30, 2002
	Notification of Acceptance :   July 15, 2002
	Final Paper/ Registration  :   August 15, 2002

Registration Fee
----------------
The registration fee for regular participants before August 15, 2002
is S$680 (approximately US$370 as at February 6, 2002), which includes
the proceedings, lunches, banquet, and tours.

Honorary Conference Chairs
--------------------------
	Shun-ichi Amari, Japan
	Hans-Paul Schwefel, Germany
	Lotfi A. Zadeh, USA

International Advisory Board
----------------------------
	Sung-Yang Bang, Korea 
	Meng Hwa Er, Singapore  
	David B. Fogel, USA  
	Toshio Fukuda, Japan  
	A. Galushkin, Russia
	Tom Gedeon, Australia  
	Zhenya He, China  
	Mo Jamshidi, USA
	Nikola Kasabov, New Zealand  
	Sun-Yuan Kung, USA  
	Tong Heng Lee, Singapore  
	Erkki Oja, Finland 
	Nikhil R. Pal, India 
	Enrique H. Ruspini,USA 
	Harcharan Singh, Singapore  
	Ah Chung Tsoi, Australia  
	Shiro Usui, Toyohashi, Japan
	Lei Xu, China  
	Benjamin W. Wah, USA  
	Donald C. Wunsch II, USA
	Xindong Wu, USA 
	Youshou Wu, China 
	Yixin Zhong, China  
	Jacek M. Zurada, USA

Advisor
-------
	Alex C. Kot, Singapore

General Chair
-------------
	Lipo Wang, Singapore

Program Co-Chairs
-----------------
	ICONIP'02: 	
		Kunihiko Fukushima, Japan
		Soo-Young Lee, Korea
		Jagath C. Rajapakse, Singapore
	SEAL'02: 	
		Takeshi Furuhashi, Japan
		Jong-Hwan Kim, Korea
		Kay Chen Tan, Singapore
	FSKD'02: 	
		Saman Halgamuge, Australia
	Special Sessions:    
		Xin Yao, UK

Finance Chair
-------------
	Charoensak Charayaphan, Singapore

Local Arrangement Chair
-----------------------
	Meng Hiot Lim, Singapore

Proceedings Chair
-----------------
	Farook Sattar, Singapore

Publicity Chair
---------------
	Chunru Wan, Singapore

Sponsorship/Exhibition Chair
----------------------------
	Tong Seng Quah, Singapore

Tutorial Chair
--------------
	P. N. Suganthan, Singapore

For More Information 
--------------------
Please visit the conference home page or contact:
	Lipo Wang, ICONIP'02-SEAL'02-FSKD'02 General Chair
	School of Electrical and Electronic Engineering
	Nanyang Technological University
	Block S2, 50 Nanyang Avenue, Singapore 639798
	Email: elpwang@ntu.edu.sg
	Phone: +65 790 6372

Conference Secretariat 
----------------------
	ICONIP'02-SEAL'02-FSKD'02 Secretariat
	Conference Management Center/CCE, NTU
	Administration Annex Building #04-06
	42 Nanyang Avenue, Singapore 639815
	Email: nef@ntu.edu.sg
	Fax:   +65 793 0997



From chemistry-request@server.ccl.net Mon Feb 11 02:59:44 2002
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Date: Sun, 10 Feb 2002 23:59:23 -0800 (PST)
From: "J. Zheng" <jzheng73@u.washington.edu>
To: chemistry@ccl.net
Subject: charmm force derivation
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Dear CCLer:

  Do you know where I can find the force derivation of Bond, Angle,
Torsion, and Improper based on CHARMM equation?

  It is really pain to derive this equation by myself. I think it woule be
better to share this equations with those who codes program on molecular
modeling.

  I will appreciate your helping.

  Good day.

  Jie


-----------------------------------------------
|  JIE ZHENG                          	      |
|  Department of Chemical Engineering	      |
|  University of Washington		      |
|  Seattle, WA 98105, USA   		      |
-----------------------------------------------
|  Tel:  (206) 616-6510 (o)		      |
| Email: jzheng73@u.washington.edu	      |
| Webpg: students.washington.edu/jzheng73     |
-----------------------------------------------


From chemistry-request@server.ccl.net Mon Feb 11 02:34:05 2002
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From: Per-Ola Norrby <pon@kemi.dtu.dk>
Subject: Summary: High level for TMs
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	Dear CCLers,

	I've now had some responses to my question about high level
calculations on transition metals.  Not unexpectedly, if you need
accuracy, you pay for it...

	Several answers led to further corresponendence, but I'm
only summarizing the original answers here.  Many thanks to:

Frank Jensen
N.O.J. Malcolm
Stefan Grimme
Markus Reiher
Max C. Holthausen
Luigi Cavallo

	To summarize, we still have no good alternative to DFT for
medium size systems (>10 atoms), and it cannot be a priori trusted
for all transition metals.  Most responders agree that we can still
trust DFT for geometries, and then use better methods for single
point energies.  There is some verification for this statement;
for example, I've seen a chapter by Diedenhofen, Wagener, and Frenking
in "Computational Organometallic Chemistry" (Ed: Tom Cundari).
However, I'd want to see more before I believe it's valid for all
TMs.  Thanks also to Max C. Holthausen for a book reference
(see below); comparing to good experimental gas phase data is still
the best way to validate our methods...

	For near degenerate systems, CC or similar alternatives is
not the answer, especially not with small bases.  In my own case,
I'll try to go the way of CASSCF and CASPT2 (thanks to Björn Roos
for getting me started on this), but it is not the final answer.
I'm still looking for a method that can give me trustworthy relative
energies of different spin states for complexes with 10-20 atoms
(a full coordination shell around a TM), preferably in solvent.
Tweaking the DFT for each system might be the answer, but I still
need accurate data for coordinatively saturated TMs to apply this
method.  Maybe Max is right, that you can do this for coordinatively
unsaturated systems and then use the modified DFT for larger
complexes?  I'll try.

	Thanks to all who responded,

	Per-Ola

------------Original message-------------------------------------

	I'd like to get some opinions on high level calculations on 
first row transition metal complexes, in particular for complexes 
with near-degenerate states.  Furthermore, I'm interested in 
complexes used for homogeneous catalysis, so even very smal models 
frequently have 10-20 heavy atoms and as many hydrogens in addition 
to the metal.

	I've used various types of DFT, both pure and hybrid, for 
these types of systems for several years now.  However, I've seen 
several indications recently that the relative energies of different 
spin surfaces can be wrong by up to 100 kJ/mol.  This is, of course, 
unacceptable.  I very much like the pragmatic fix proposed by Reiher 
et al, Theor. Chem. Acc. 107 (2001) 48-55, where they reparameterize 
the amount of exact exchange in B3LYP for organometallic complexes. 
However, having been burned once, I don't want to assume that one 
fixed parameterization is going to be valid for all first row 
transition metals.  Thus, to apply this approach I need very good 
reference data for some experimentally inaccessible complexes.  I'll 
have to obtain them computationally, but what level to use? 
Alternatively, I may not go for the modified DFT, but then I still 
need a theoretical level I can access, which will give me good 
relative energies (and the geometries, but maybe DFT can do this..?).

	So, what level can we trust for this?  CCSD(T) has been 
proposed, but it's expensive, and we all know that it requires a 
large basis set, certainly much better than the double-zeta valence 
that is often used.  And it is still only a perturbation method, so 
if the underlying HF is way off, no amount of perturbation will fix 
it.  However, I'd like to try it out if I can find a program that is 
reasonably efficient.  I've heard rumors of linear scaling CCSD(T) or 
equivalent methods, does anyone know of an available implementation 
that will allow a calculation with ca 500 basis functions?

	How about MC methods?  I'm trying out CASPT2, but what else is there?

	BTW, don't suggest any MP-method (MP2, LMP2,...).  I've tried 
them for a couple of test cases, and the errors are much larger than 
with DFT.

	As a side issue, any suggestions of what type of experimental 
data to compare to?  There are a couple of cases where population 
distributions among near-degenerate states can be measured, but this 
is not general enough, I also want to be able to predict cases where 
the energy difference is large.

	All the best

	Per-Ola
----------Response from Frank Jensen---------------------------
	Per-Ola,
	DALTON er maaske en mulighed for CC-beregninger. Den kan
koere integral-direkte beregninger, bl.a. paa linux maskiner.
Det er gratis, check ICC-hjemmesiden for en www-adresse.

	Frank
----------Response from N.O.J. Malcolm-------------------------
per-ola,

you might want to try something along the lines of an experiment we
tried (simply for first row TM excitation energies), very quick and
dirty.

see:

"A simple scaling for combining multiconfigurational wavefunctions with
density functionals"
Malcolm NOJ, McDouall JJW
CHEMICAL PHYSICS LETTERS
282 (2): 121-127 JAN 9 1998

noj
----------Response from Stefan Grimme--------------------------
Dear Per-Ola,
we have developed a simplified MR-MP2 scheme without CASSCF step
running in parallel on a cheap linux PC-cluster. We are just testing
energetics of simple TM compounds. If you are interested I can provide
you with some numbers (we just started and are not so far yet). In principle
our implementation works for 500-800 basis functions.
Stefan Grimme
---(I asked for a reference on this, and got it, thank's Stefan)---
S. Grimme und M. Waletzke, Multi-reference M¯ller-Plesset
theory: computational strategies for large molecules, Phys. Chem. Chem.
Phys., 2, (2000), 2075-2081.
(its also available via our homepage)
However, this paper mainly deals with excited states and also
the parallel stuff is not described there.
----------Response from Markus Reiher--------------------------
Dear Per-Ola,

after I read your email postet at CHEMISTRY@ccl.net
I thought it might be useful to write you the latest
experiences with our reparametrized B3LYP functional.

My diploma student worked out how B3LYP* performs for the G2 test
set and for transition metal complexes of the first period.
It turned out that B3LYP* is as good as B3LYP for the
thermochemistry of the G2 test test. Furthermore, the
effects we found are transferable to other transition
metals. But there are some pathological cases, for which
the deficiencies which we detected are most prominent, which
means, that one must be very careful with DFT calculations.
These difficult cases are compounds with Mn, Fe, Co, Ni
in weak ligand fields. We prepared a second paper on this
which is submitted to JCP.

However, if states of different multiplicity are really close,
DFT will certainly not get things right. Therefore, we are
after these cases with multireference MP2 methods which are
capable of any electronic situation (CCSD(T) is too unreliable
as you often have multi-determinant ground states for transition
metal complexes).
Experimental data is hard to obtain and I believe that
highly accurate ab initio calculations done for a representative
of those molecules which shall be studied by DFT is the
best way to calibrate DFT.

Best regards

Markus
----------Response from Max C. Holthausen----------------------
Dear Per-Ola,

	you'll find an an excellent compilation of gas-phase ion data for small
TM systems in the book "Organometallic Ion Chemistry" edited by Ben
Freiser (Kluwer 1996) p284 ff.

	My two cent: The best you can probably do for this type of species is
full valence CAS-based MRCI (ACPF,AQCC). CASPT2 fails miserably in many
instances, and this is not only due to those 'intruder states' -
perturbation theory it is after all! MRCI has to be done with
substantially expanded basis sets in order to hope to predict meaningful
numbers (cc-pVT/QZ on first row elements, for the 3d metals
Bauschlicher's or Pou-Amerigo's ANOs including the full set of
polarization functions - see the EMSL Web site, the latter is referred
to as ROOS augmented triple zeta ANO). For late 3d metals you would
often need to include 4p orbitals in the active space next to 3d and 4s
and the valence space of the organic moiety. If you can keep the active
space consistent (i.e. empty 4s is not flipping out and 4d is flipping
into the active space or something painstaking like that) you would need
to start with a small basis and active space and improving both up to
the point where the observable of interest (binding energy, say)
converges. If you do not show this convergence, your post-HF result is
no better than any B3LYP/TZ2P calculation! You would need to check all
potentially meaningful spin states (e.g. Fe(H2O)+ in quartet and sextet
multiplicity). For Cu you need to include relativistic effects - one can
hope it's sufficiently done including darwin and mass velocity terms
only. Geometries can probably done at B3LYP/TZP (ECP), also BP/TZP (ECP)
seems to work fine (the latter not for energies!) - but this is an issue
for benchmarking, too. Definitely, studies like those of Bauschlicher
(and Siegbahn for 4d species) some years back, but with larger basis
sets and large reference expansions for MRCI, would be very important to
provide a solid database for checking experimental data and to fit
functionals. But this is hard work for more than one brave theorist.

	What you're up to is something that interests me for quite a while now.
I do think that parametrizing DFT on small, coordinatively unsaturated
TM complexes can be very successful, but most certainly not simply by
modifying the exact exchange admixture in Gaussian's B3LYP, as has been
done by Hess's group. E.g., some years ago I have modified that
parameter to about 35% in order to better describe the whole set of
M-C2H4+ and MCH3+ binding energies for first row metals. Then, however,
I found M=CH2+ being described worse than with the original 20% and I
never published that. I remember a polish group presenting a poster at
the Paris DFT conference presenting a parameter of 30% HF admixture
obtained by parametrizing some organic systems. In several recent
studies Fritz Schaefer finds BHHLYP superior over B3LYP, if memory
serves me right. This is to say: the 15% Reiher et al are coming up with
might do a good job for their set of systems, certainly not for others.
A general improvement of functional performance can most likely not be
accomplished by such simple modifications, based on scarce data. Basis
set quality plays a significant role as well. The compensation of errors
by admixing more or less of the very diffuse HF exchange hole to some
functional flavor is not likely to solve funadmental problems for TMs!

	However, proper physics can probably be incorporated to some extent by
parametrizing a functional, fitting ALL PARTS contributing to the
exchange-correlation hole! As far as I know, this has not been done on
the basis of "hard" transition metal data (I would think of an expansion
of Handy's recent work as promising). The reason is that there is no
such thing as the G2 set for TM systems (save atomic energies, which are
precisely known, probably a good set to start with). Some geometrical
data would be needed as well. Just these days I am thinking of
restarting research along theses lines, as a new PhD student will enter
my little group - he said he wants to do some real calculations, not
that B3LYP/lanl2dz he has done before ... if I can catch his interest
the first step would be creation of MRCI binding energy tables. Maybe
you have vacant resources as well ...

	Best regards,
	Max
----------Response from Luigi Cavallo--------------------------
      Dear Per-Ola,

my compliments for your post. I think you dared to say something that a
lot of people thinks but usually are rather scary to say. Pure or hybrid
DFT is often used uncritically (and I am in the number), just because it
is a "standard" tool, and reviewers usually don't complain. Particularly
if you use B3LYP.

As for the case that "burned" you, I think you refer to the Mn-salen
stuff. Well, I think I could have been on your place, indeed. It was just
a lucky case that I used BP86, and that BP86 proved to be less wrong than
B3LYP (at a level higher of ccsd(t) BP86 could be even worse than B3LYP).

I do agree that ccsd(t) is not the optimal solution. Recently, I've done
quite a few of those calculations with roughly 250 basis functions, 35
atoms H included, closed shell. On the average, the single point took.....
10 days!   (G98 is the program) So, unless you have huge cpu-power and HD
(yes, with ccsd(t) scratch space is another big issue), ccsd(t) is not the
tool to make "ordinary" chemistry.

After that much cpu-time I feel unsatisfied for the reasons you wrote.
Relatively poor basis set, perturbative approach, etc etc.

The alternative is to make MC calculations, as you wrote, and MOLCAS
> from the group in Lund should perform nicely. But I don't have
any experience there.

I would appreciate if you could summarize the "best" answers you got.

All the best, and meet you soon at some congress,

luigi




-- 

^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^
Per-Ola Norrby, Assoc. Professor, http://compchem.dfh.dk/PeO/
Technical University of Denmark, Dept. of Chem., Org. Chem.
Building 201, Kemitorvet, DK-2800 Kgs. Lyngby, Denmark
Email: pon@kemi.dtu.dk  tel +45-45252123,  fax +45-45933968


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From: Jim Phillips <jim@ks.uiuc.edu>
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cc: chemistry@ccl.net
Subject: Re: CCL:charmm force derivation
In-Reply-To: <Pine.A41.4.44.0202102356590.106350-100000@dante28.u.washington.edu>
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Hi,

You can borrow code from NAMD.  http://www.ks.uiuc.edu/Research/namd/

"Licensee may redistribute without restriction works with up to 1/2 of
their non-comment source code derived from at most 1/10 of the non-comment
source code developed by Illinois and contained in the Software, provided
that the above directions for notice and acknowledgement are observed."

-Jim


On Sun, 10 Feb 2002, J. Zheng wrote:

>
> Dear CCLer:
>
>   Do you know where I can find the force derivation of Bond, Angle,
> Torsion, and Improper based on CHARMM equation?
>
>   It is really pain to derive this equation by myself. I think it woule be
> better to share this equations with those who codes program on molecular
> modeling.
>
>   I will appreciate your helping.
>
>   Good day.
>
>   Jie
>
>
> -----------------------------------------------
> |  JIE ZHENG                          	      |
> |  Department of Chemical Engineering	      |
> |  University of Washington		      |
> |  Seattle, WA 98105, USA   		      |
> -----------------------------------------------
> |  Tel:  (206) 616-6510 (o)		      |
> | Email: jzheng73@u.washington.edu	      |
> | Webpg: students.washington.edu/jzheng73     |
> -----------------------------------------------
>
>
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From chemistry-request@server.ccl.net Mon Feb 11 11:58:47 2002
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Date: Mon, 11 Feb 2002 17:55:05 +0100
From: "Nicolas Ferre'" <ferre@unisi.it>
Subject: Tinker: reduction factors
Sender: ferre@unisi.it
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To the Tinker's users.

I'm coding some stuff into Tinker3.9 and I'd like to know what are the
"reduction factors" applied to the cartesian coordinates of atoms in the
van der waals and electrostatic interactions parts.

Thanks for your help and/or references.

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

From chemistry-request@server.ccl.net Mon Feb 11 14:44:45 2002
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Date: Mon, 11 Feb 2002 14:44:21 -0500 (EST)
From: "Robert Q. Topper" <topper@cooper.edu>
To: chemistry@ccl.net
Cc: TOPPER ROBERT <topper@cooper.edu>
Subject: ECCC8 Starts March 4!
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Dear colleagues,

I hope that you all will register for, and participate in,
ECCC8 - the 8th Electronic Computational Chemistry Conference -
which begins on Monday, March 4, 2002 and will take place entirely
on the web at http://eccc8.cooper.edu.

We have ended up with a solid 36 papers in this year's conference. 
20 different countries are represented, with contributions
> from North America, South America, Europe, Australia and Asia.
There is a marvelous diversity of topics as well, with
abstracts touching on many different aspects of 
computational and theoretical chemistry and biology.

It promises to be a particularly interesting meeting, and I
am positive that you will find it worthwhile. Registration takes
less than 5 minutes and it is free. After March 4, registration will be
required in order to view the abstracts and presentations
as well as to participate in online discussions. However, everyone
may view the abstracts without registering until March 4.

Best regards to all - Robert

*****************************************************************************
8th ELECTRONIC COMPUTATIONAL CHEMISTRY CONFERENCE MARCH 2002
http://eccc8.cooper.edu
*****************************************************************************
Robert Q. Topper, Ph.D.                 email:   topper@cooper.edu
Associate Professor of Chemistry        phone:   (212) 353-4378
School of Engineering                   fax:     (212) 353-4341
The Cooper Union for the Advancement   
of Science and Art                      subway:  take the 6 to Astor Place
51 Astor Place                                   or the N/R to 8th street
New York, NY 10003                               and you're there!
*****************************************************************************
                 http://www.cooper.edu/engineering/chemechem/
*****************************************************************************




