From cmartin@london.ks.uiuc.edu  Tue May 16 01:36:59 1995
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Subject: The ab initio basis of DFT and semi-emp methods
To: chemistry@ccl.net
Date: Tue, 16 May 95 0:30:16 CDT
Mailer: Elm [revision: 70.85]


On the subject of DFT, semi-empirical methods, and ab initio theory:

	At first sight it may appear that DFT methods have a stronger
"ab initio" basis than semi-empirical methods, in fact I will argue that
the reverse is actually true because the ab initio basis of semi-empirical
methods are more highly developed and has been more extensively researched
than DFT.  In order to say that there exists an ab initio basis for 
either DFT and/or semi-empirical methods, I argue that there must exist
(1) a formal mathematical theory linking the exact molecular
electronic Schr\"odinger equation and the approximate method
(DFT or Semi-Emp)
(2) an ab initio method which can compute all of the mathematical
parameters (be them matirx elements, functionals, densities, etc)
in the approximate method
(3) tests of the assumptions of the approximate method using the
ab initio techniques described in (2)
(4) [the hardest and most challenging requirement] actual and meaningful
improvements must have been sugested and incoproated into the
approximate methods based on the ab initio tests.

For both Semi-Emp methods and DFT I do not believe that all 4 requirements
have been met, however, I beleive that the ab initio theory of
Semi-Emp methods has been more highly developed than the DFT.

It can be argued that the Hohenberg-Kohn (HK) theorem and
the Kohn-Sham equations provide (1) for DFT, however, I must point out 
that niether of these provide an exact presecription for computing
the density function for an arbitrary molecular system 
the state of DFT theory lies somewhere between requirements (1) and
(2).  I know of of only one paper which describes an ab initio
algorithm for computing the universal density functional using
ab initio techniques for a general molecular system (Karl F. Freed
and Mel Levy, JCP vol 77, page 396 1 July 1982).  Some recent
work by Parr describes ab initio techniques for (3), however;
Parr provides some diagnostic tools for testing the assumptions
of DFT with out actually computing the functionals themselves
(I saw this in a recent talk  Parr and I do not know how well
this is described in his book on DFT). Likewise, other work in the 
literature exists which describes how to express the exact functional
for some model systems (I can not recall all of the work.  I recall
that Bob Harris at U.C. Berkeley has some intersting work in the area.)
If there is other important work in the area plase bring the attention
of the CCL forum.  

In contrast, the theory of semi-empirical methods is more highly
developed as requirements (1)-(3) have been met with the
use of the effective valence shell effective Hamiltonian (Hv) ab initio
method (see, for instance, Charles H. Martin and Karl F. Freed, JPC,
Vol 99, page 2701, 1995, and Karl F. Freed, In Conceptual Trends
In Computational Chemistry; VCH:  New York, 1991; Vol II)
I do not beleive that condition (4) has been fully borne
out by the Hv theory, however, some suggestions have been discussed
by Walter Thiel (Tetrahedron vol 44, page 7393, 1988), and other
semi-empirical methods have been based on related ab initio
theories (Malieru's work, the PCLIO of Peter Fulde)

Neither DFT nor Semi-empirical methods desrve full ab initio status
at this time, however, because neither method may be systematically
corrected with higher levels of theory.  It is this feature
that distinguishes ab initio theory from other approximate
methods as it is always possible, although not always practical,
to systematically extend the methods as close as possible to
the exact solution of the Schr\"odinger equation (or to extend
the Schr\"odinger equation, for that matter) to any desired
accuracy obtainable with current experimental techniques.

I find it most unfortuneate that the ab initio basis of both
Semi-empirical methods and DFT has not been more rigorously
explored; there is tremendous room for advancement in these
areas of research, especially in the area of semi-empirical
methods.  Indeed, the ultimate goal of such research would be 
to obtain ab initio accuarcies with semi-empirical speeds,
a most formidable challenge.






From teck.lim@pembroke.oxford.ac.uk  Tue May 16 05:06:58 1995
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          Tue, 16 May 1995 09:59:48 +0100
Date: Tue, 16 May 1995 09:59:47 +0100 (BST)
From: Teck Lim <teck.lim@pembroke.oxford.ac.uk>
To: ccl <chemistry@ccl.net>
Subject: xdbx source
Message-ID: <Pine.OSF.3.91.950516095318.24458A@sable.ox.ac.uk>
MIME-Version: 1.0
Content-Type: TEXT/PLAIN; charset=US-ASCII


Hi,

  Recently, I posed a query on location of xdbx source for SGI machines.  
Here are the extracts from the replies I received.  Special thanks to Andy, 
David, Walter, Lawrence and Michael.

--------------------------------------------------------------------------
From: "David L. Freeman" <freeman@mozart.chm.uri.edu>/
Walter Koppensteiner <wk@barrel.mdy.univie.ac.at>/
Michael Bass <mbass@amgen.com>/
"Lawrence S. Norris" <lnorris@rookery.acns.nwu.edu>

ftp site...ftp.sgi.com

cd sgi
cd xdbx

There is a tar file there.  I have used this for fortran.  I assume it will
work for C.

-------------------------------------------------------------------------
From: Mr Andrew D Allen <chp1aa@surrey.ac.uk>

   We do have xdbx!!! though, I've tar'ed and compressed
it and put it onto our ftp server.

        ftp 131.227.110.69  -> /pub/INCOMING/xdbx.tar.Z

---------------------------------------------------------------------------
best regards - tecksin



From HRUSAK@jh-inst.cas.cz  Tue May 16 05:22:01 1995
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From: "Dr. Jan Hrusak" <HRUSAK@jh-inst.cas.cz>
Organization:  Institute of Physical Chemistry
To: chemistry@ccl.net
Date:          Tue, 16 May 1995 10:54:11 +0100
Subject:       Is ab initio semiempirical ?
Return-Receipt-To: "Dr. Jan Hrusak" <HRUSAK@jh-inst.cas.cz>
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In general I do not like such philosophical discussions,  but on the other 
hand I would like to stress my opinion to this particular problem. I 
think there is no reason for DFT to enter a claim to be called ab 
initio. Since in my wiev just very few ab initio calculations are 
realy  "first principle" calculations. First of all, ab initio is 
just an approximation to solution of the Schroedinger equation.
There is usually an (arbitrary or not) chosen a  basis set (parameter set?) 
for a given atom. Further, in many of the ab initio codes not 
all the integrals are evaluated in course of the calculation. 
(neglecting small int., cuttoff criteria are set etc.)
Thus "ab initio" in a strong sense is just an terminus 
technicus describing a given technique, which is more or less non 
empirical.

Jan




----------------------------------------------------------------------------
Dr. Jan Hrusak                               ###############################
J. Heyrovsky Institute of Physical Chemistry ## MEMOR ESTO CONGREGATIONIS ##
Academy of Sciences of the Czech Republic    ##   TVAE QVAM POSSEDISTI    ##
Dolejskova 3, CZ-182 23 Prague 8             ##         AB INITIO         ##
Czech Republic                               ###############################
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
Phone: (0042 2) 66 05 3436                    FAX: (0042 2) 858 2307
                     E-Mail: hrusak@jh-inst.cas.cz
----------------------------------------------------------------------------


From hs@helix.mdy.univie.ac.at  Tue May 16 08:37:03 1995
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From: "Hellfried Schreiber" <hs@helix.mdy.univie.ac.at>
Message-Id: <9505161423.ZM28387@helix.mdy.univie.ac.at>
Date: Tue, 16 May 1995 14:23:51 -0600
X-Mailer: Z-Mail (3.2.0 26oct94 MediaMail)
To: chemistry@ccl.net
Subject: CONFERENCE ANNOUNCEMENT
Mime-Version: 1.0
Content-Type: text/plain; charset=us-ascii




    >> INTERNATIONAL CONFERENCE ON MOLECULAR STRUCTURAL BIOLOGY <<

             Organized by the Austrian Chemical Society

              Vienna (Austria), September 17-20, 1995


TOPICS:

      1) The Impact of Molecular Biology on Structural Biology
      2) Biomolecular Structure Determination
                  a) X-Ray Diffraction
                  b) NMR Spectroscopy
      3) Dynamics and Function of Biomolecules
      4) Computational Methods
      5) Protein Engineering and Design


The scientific programme is designed to cover a broad range of disciplines in
molecular structural biology. Topics will be presented in the form of plenary
lectures, posters, discussions and exhibitions.


Sunday, (17.9)
-----------------------------------------------------------------------------
    Registration
    Welcome Cocktail
    Honory Lecture by H.Neurath


Monday, (18.9)
-----------------------------------------------------------------------------

1. The impact of Molecular Biology on Structural Biology

	C.Cantor (USA) "Application of Streptavidin and
		Genetically Engineered Variants"
	T.Blundell (GB) "Protein Super Families: Genome
		Analyses and Drug Discovery"

2. Biomolecular Structure Determination

   a) X-Ray Crystallography

	R.Huber (D) "Proteolytic Enzymes and Their Natural
		Inhibitors - New Functions and New Structures
		and No End in Sight"
	M.Walkinshaw (CH) "Structures and Biological
		Implications of Series of Cyclophilin-Cyclosporin
		Crystal Complexes"
	I.Schlichting (D) "Ligand Binding in Heme Proteins
		Studied by Kinetic X-Ray Crystallography"

Tuesday (19.9.)
-----------------------------------------------------------------------------

   b) NMR Spectroscopy

	O.Jardetzky (USA) "Flexibility and Function in a DNA
		Binding Protein - the Trp-Repressor of E.Coli"
	P.Roesch (D) "The Structure of Iron-Sulfur Proteins
		in Solution"
	C.Dobson (GB) "The Structural Basis of Protein Folding"

3. Dynamics and Function of Biomolecules

	J.Lakowicz (USA) "Fluorescence Spectroscopic Studies
		of the Structure and Dynamics of Biomolecules"
	W.Kuehlbrandt (D) "Structure Determination of Membrane
		Proteins by High-Resolution Electron Microscopy"
        H.Frauenfelder (USA) "Dynamics and Function of Biomolecules"

Wednesday (20.9.)
-----------------------------------------------------------------------------

4. Computational Methods

	M.Karplus (USA) "Simulations of Protein Folding From the
		Native to the Denatured State and Back Again"
	J.Skolnick (USA) "A Hierarchial Approach to the Prediction
		of Protein Structures"
	H.-J.Boehm (D) "New Computational Tools for Structure
		Based Drug Design"

5. Protein Engineering and Design

	A.Fersht (GB) "Pathways of Protein Folding"
	L.Presta (USA) "Protein Engineering of Immunoglobulins and
		Immunoglobulin-Like Domains"
        M.Mutter (CH) "De Novo Protein Design"

CALL FOR POSTERS
-----------------

	All those intending to participate in the conference are invited
to submit posters presenting original work.
Abstracts prepared according to the instructions given below should arrive

			NOT LATER THAN JUNE 30th, 1995.

The authors will be informed about the provisional acceptance in July, 1995.
The presentation of the posters will be finally approved and thus the
contribution included in the Book of Abstracts when at least one of the
registers before August 1st, 1995. Contributors of outstanding posters will
be chosen by the scientific committee to give a 20 minute lecture.

Head of Scientific Committee:         P.Schuster


EXHIBITON:
---------

       An exhibition of instruments, accessories, software, literature and
other items is planned. Companies interested in displaying their products
are kindly requested to contact the conference secretariat.


INDUSTRIAL SATELLITE MEETING:
-----------------------------
       A half day industrial symposium is planned. Those companies
who are interested in presenting up-to-date results obtained on their
products in the form of 20 minute lectures are kindly requested to
contact the conference secretariat.



Registration Fees (before August 1):  Regular Participant   4000 ATS
                                      GOeCH Member          3500 ATS
                                      Student               2000 ATS

The registration fee includes the Book of Abstracts, the welcome cocktail
and buffet, the invitation to the Viennese Rathaus, a ticket for the piano
concert, coffee breaks and tram tickets.


If your are interested in a folder of the second announcement including a
registration form and the social program, please contact:

      A.Kungl
      Gesellschaft Oesterreichischer Chemiker
      AG Biophysikalische Chemie
      Nibelungengasse 11
      A-1010 Wien, Austria
      Tel.: (43) 1 587249
      FAX.: (43) 1 587966
      e-mail: msb95@helix.mdy.univie.ac.at



-- 


+-----------------------------------------------------------------------------+
|                                                                             |
|                           Hellfried Schreiber, Ph.D.                        |
|                                                                             |
+---------------------------------------+-------------------------------------+
|                                       |                                     |
|  Institute for Theoretical Chemistry  |                                     |
|  Theoretical Biochemistry Group       |   Mail:  hs@helix.mdy.univie.ac.at  |
|  Waehrigerstrasse 17                  |   Voice: +43 1 40480 - 618          |
|  A-1090 Wien, Austria, Europe         |   FAX:   +43 1 4028525              |
|                                       |                                     |
+-----------------------------------------------------------------------------+

From ivarm@boc.ic.ee  Tue May 16 09:22:10 1995
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	by www.ccl.net (8.6.10/930601.1506) id JAA04828; Tue, 16 May 1995 09:08:34 -0400
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	id aa12400; Tue, 16 May 95 16:12:39 estonia
From: "Ivar Martin" <ivarm@boc.ic.ee>
Date: Tue, 16 May 95 16:00:56 EST
Message-Id: <5667.ivarm@boc.ic.ee_POPMail/PC_3.2.2>
Reply-To: <ivarm@boc.ic.ee>
X-POPmail-Charset: English
To: chemistry@ccl.net
Subject: Imaginary frequency and rate constant?


Hello!

     As it is expected, MOPAC calculates one and only one negative
vibrational frequency at TS. The value lies (-300 - -150 cm-1). Now, is it 
correct to use this frequency as pre-exponent factor (frequency factor) in 
Arrhenius rate constant equation? The reaction I study is C-C single bond
forming (or splitting) reaction.

If there will be interest, I'll give the summary to list.


Thanks,
_______________________________
Dr. Ivar Martin
Department of Bioorganic Chemistry           tel: +372 2 526510
Institute of Chemistry                       fax: +372 2 536371
Akadeemia tee 15 EE0026                   e-mail: ivarm@boc.ic.ee
Tallinn, ESTONIA

From dimitris@3dp.com  Tue May 16 10:37:05 1995
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From: "Dimitris Agrafiotis" <dimitris@3dp.com>
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Date: Tue, 16 May 1995 10:27:25 -0400
X-Mailer: Z-Mail (3.1.0 22feb94 MediaMail)
To: dvm@extreme.chem.rpi.edu
Subject: Delaware Valley Modeling Club Meeting
Cc: chemistry@ccl.net, krystek@bms.com
Content-Type: text/plain; charset=us-ascii
Mime-Version: 1.0


Dear DVM'ers,

The next meeting of the Delaware Valley Molecular Modeling Club will be
held on May 31, 1995, at 6.30 pm. The subject will be diversity profiling
for combinatorial libraries, and the meeting will be hosted by 3-Dimensional
Pharmaceuticals in Exton, PA.

PLEASE let me know if you are going to attend, to help us make the necessary
catering arrangements.

See you all in a couple of weeks.


-----------
DIRECTTIONS:
-----------

            3-Dimensional Pharmaceuticals, Inc.
            Eagleview Corporate Center
            665 Stockton Drive, Suite 104
            Exton, PA 19341


1) From Philadelphia:

Take the Schuykill Expressway (I-76) to Rt. 202 South. Continue South on
Rt. 202 to Rt. 30 West. Continue on Rt. 30 West to Rt. 100 North. You will
make a right onto 100 North. Continue North on 100 until you see the exit
for the Pennsylvania Turnpike and continue with directions below.

2) From the Pennsylvania Turnpike (Exit 23), and Rt. 100 North:

Go 1/2 mile to traffic light. Just north of the light, take jughandle to
the right for entrance to Eagleview Boulevard West. You will cross Rt. 100.
Follow Eagleview Blvd. 1/4 mile to second right (Pennsylvania Drive).
Go Right on Pennsylvania Drive for 3/10 mile to Rice Blvd. on left.
Go left on Rice Blvd. for 1/10 mile to Stockton Drive (firth right).
Go right on Stockton Drive to second building on right (3rd lot entrance).


-- 
Dimitris K. Agrafiotis, PhD             | e-mail: dimitris@3dp.com
3-Dimensional Pharmaceuticals, Inc.     | tel:    (610) 458-6045
665 Stockton Drive, Suite 104           | fax:    (610) 458-8249
Exton, PA 19341



From jkl@ccl.net  Tue May 16 11:37:08 1995
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	by www.ccl.net (8.6.10/930601.1506) id LAA09101; Tue, 16 May 1995 11:36:46 -0400
Date: Tue, 16 May 1995 11:36:46 -0400
From: Jan Labanowski <jkl@ccl.net>
Message-Id: <199505161536.LAA09101@www.ccl.net>
To: chemistry@ccl.net
Subject: Re: Molecular Graphics and Animation Workshop - Please Post
Forwarding: Mail from 'jeanne@tc.cornell.edu (Jeanne C. Butler)'
     dated: Tue, 16 May 1995 09:44:43 -0400



MOLECULAR GRAPHICS AND ANIMATION WORKSHOP

The Cornell Theory Center will hold a workshop June 29-July 1, 1995,
focusing on the use of computer graphics in molecular and biological
sciences. The workshop will cover the principles of molecular graphics
using the IBM Visualization Data Explorer (DX) software in combination with
a publicly available chemistry module suite (CM) that was written at CTC.
In cooperation with the Division of Biological Sciences, participants will
have access to a state-of-the-art interactive graphics workstation
facility, complete with stereo-viewing equipment and hardware rendering.

Although some previous UNIX and DX experience is	desirable, the workshop
will include an introduction to both.  Participants are encouraged to bring
their own data sets. Consulting staff will be available to assist
researchers in their visualization projects.  The first morning of the
workshop will be held on the seventh floor (rm 708) of the Engineering and
Theory Center Building on Hoy Road on the Cornell University campus in
Ithaca, New York. The reception desk can be reached at (607) 254-8686 from
8:00 a.m. to 5:00 p.m. The remainder of the workshop will be held at
Stimson Hall in the Laboratory of Computer Graphics (rm G04) and in the
 CTC Visualization facility (rm 653). Saturday morning will be open lab
time for final video productions and virtual reality experiments.

COVERED IN THE WORKSHOP:
-theory and use of the basic molecular graphics constructs (CPK, stick
models, ribbon representations, and molecular surfaces)

-visualization of electrostatic fields, quantum mechanics, and dynamics

-three-dimensional reconstructions from microscopy

-advanced rendering (volumetric rendering, constructive solid geometry, and
texture maps)

-animation techniques using DX

-virtual reality using the DX-to-CAVE module

So that each participant will have access to a workstation, class size
will be limited to ten. Short lectures and video  presentations will be
interspersed with generous periods of lab time. Participants will be
provided with examples from a wide variety of research projects, which they
can copy and modify to fit their own research problems. Also available will
be CTC computing and data facilities, including a high-quality color
printer and a growing virtual reality environment.

HOTEL ACCOMMODATIONS:
Attendees are responsible for their own hotel reservations and meals. Paid
parking is available on campus, but walking or public transportation are
recommended.

-Best Western University Inn (<1 mile)
East Hill Plaza
Ithaca
607/272-6100
FAX: 607/272-1518

-Collegetown Motor Lodge (walking distance)
312 College Avenue
Ithaca
607/273-3542
800/745-3542

-Sheraton Inn (<3miles)
One Sheraton Drive
Ithaca
607/257-2000
FAX: 607/257-3998

-Statler Hotel (1 block from Theory Center)
Cornell University campus
607/257-2500
FAX: 607/257-6432

TO APPLY:
Due to restricted space, registration for this workshop is limited. The
completed application form, along with payment, must be received by Friday,
June 9, 1995. Applications will be accepted after this date only if
openings still remain. The workshop fee includes all workshop materials.
Local researchers may charge the registration fee to the appropriate
Cornell University account number. Applications that do not include payment
cannot be accepted. Payment checks will be returned promptly to applicants
not accepted due to over-enrollment.  Notification will be mailed on June
12, 1995.

PAYMENT SCALE, PAYABLE TO CORNELL UNIVERSITY:
Academic participants: $70
Corporate Research Institute members: $250
Other corporate participants: $350

------------REGISTRATION FORM------------------

This registration form and payment must be received by June 9, 1995.

SEND TO:
Jeanne Butler
Cornell Theory Center
427 Engineering and Theory Center Building
Ithaca, NY 14853-3801 (607) 254-8813
jeanne@tc.cornell.edu

REGISTRATION FORM

Name__

Institution__

Address__

City, State, Zip__

Telephone__

Fax__

Preferred electronic mail address__

Do you have a current CTC account: __no __yes;  my userid is__

Do you have a pending allocation request: __no __yes

Social Security #:____-_____-_____ to set up new supercomputer accounts.
(Submission of social security numbers is voluntary and will not affect
eligibility for access to CTC facilities. However, SSNs are an integral
part of the National Science Foundation's information system and assist in
managing the Supercomputer Centers program. SSN solicited under NSF Act of
1950, as amended.)

Special needs (e.g., mobility impaired)__

Account number to charge (Cornell applicants only)__

Academic discipline (e.g., biological sciences, geosciences, chemical eng.)__

Status (check all that apply)

Academic
__Undergraduate
__Graduate
__Postdoctoral
__Faculty
__Smart Node Consultant/Advisor
__Other:

Corporate/Commercial
__Research
__Other:

ETHNIC ORIGIN (OPTIONAL)
__African American
__Caucasian
__Asian American
__Hispanic American
__Native American
__Alaskan Native
__Other:

If possible, please list the various types and formats of data you are
likely to bring to the workshop (optional). This will help ensure that we
can read your data into the graphics programs. (e.g., molecular structures
in Brookhaven Protein Databank format, or electron densities from Gaussian,
or confocal microscope images from our own lab [can send sample] ). ___

If nonstandard format, please contact richard@tc.cornell.edu.

*All trade names referred to are trademarks or registered trademarks of
their respective companies.





----------- End Forwarded Message -----------


From shep@appsdiv.cray.com  Tue May 16 15:07:06 1995
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Date: Tue, 16 May 95 14:04:58 CDT
From: shep@appsdiv.cray.com (Shepard Smithline)
Message-Id: <9505161904.AA04563@ss1.cray.com>
To: chemistry@ccl.net
Subject: similarity



Dear Netters,

A while back I posted  some questions regarding similarity.  Below
is the original question and the responses I received.  Thanks to
all who responded.

Shep Smithline

__________________________________________________

Original Posting:

Dear Netters,

I have some questions for the similarity gurus out there.

(i)   What are the commonly used (public or commercial) similarity
      programs?

(ii)  What are their major features?

     For example:

     Do they allow a test structure to rotate or translate relative
     to a reference structure or can the internal geometry change?
     Do they perform any additional analyis once the indexes are computed? 

(iii) What sort of data do they use to compute the similarity?

      For example:

      Do they compute indexes based only on volume or shape?
      Do they use charges or other quantum mechanically derived
      data to compute an index?

Please foward responses directly to me. I will summarize to the net.

Thanks,

Shep Smithline

_______________________________________________________________________

Responses:



Dear Shep
I have a method of similarity searching based on the method of "icosahedral
matching".  The algorithm is described in reference (1). It was taken up by
workers at Organon Oss (reference 2) who developed a 3D database seaching 
program called SPERM. Subsequently and independently I amplified the original
method into a series of programs all of which use the library of subroutines
but the different programs do different things:-

THREEDOM 	3D-database searching
COMPARISONS 	Compares a single structures with many structures
CORRELATE	Compares structures in one series with those in another series 
		(the two series may be the same)

The feature of icosahedral matching is that it makes use of the symmetry
of the icosahedral group to increase the efficiency of the matching process
(over brute-force methods) by the factor of 60 (120 if mirror image searching
is included).  

The programs use the ideas of Dean (reference 3) on gnomonic projections to
handle the properties being compared. These properties can either be shape
(e.g. distances from points on an encompasing sphere to the nearest atoms)
or electronic (potentials at points on the encompasing sphere), and in 
principal other properties could be used (e.g. hydrophobicity).

The icosahedral matching algorithm takes care of the business of rotating 
one of the pair of structures being matched with respect to the other.  It does
not incorporate any translational operation.

Because the icosahedral matching process does not take into account the 
overall size of structures being compared, it is necessary in database 
searching to apply some prefiltering, to avoid comparing grossly disimilar 
structures.  Accordingly there are two other programs:- PREFILTERS and 
QUICKSCAN. The first of these will produce an index file for the database for
the parameters:- volume, size of largest axis, and ellipticities (i.e. ratios 
of three principal axes), for all structures in the database.  The second 
program will extract just those structures from the database which meet 
criteria of similarity (+/- percentages of volume, axis size, ellipticity)
to the target structure). These extracted structures are then submitted to the
program THREEDOM.

All of these programs are available from QCPE as part of the INTERCHEM package
for quite modest fees.

References:
(1) P. Bladon J. Mol. Graphics, 1989,7,130-137.
(2) V. J. van Geerestein, N. C. Perry, P. D. J. Grotenhuis, and C. A. G.
    Haasnoot, Tetrahedron Computer Methodology, 1990, 3, 595-613; N. C. Perry 
    and V. J. van Geerestein, J. Chem. Inf. Comput. Sci., 1992, 32, 607-616.
(3) P.-L. Chau and P. M. Dean, J. Mol. Graphics, 1987,5,97; P. M. Dean and 
    P.-L. Chau, J. Mol. Graphics, 1987,5,152; P. M. Dean and P. Callow, J.
    Mol. Graphics, 1987,5,159; P. M. Dean, P. Callow, and P.-L. Chau, J
    Mol. Graphics, 1988,6,28.

Yours sincerely

Peter Bladon

Phone/Fax +44-(0)141-776-1718
email cbas25@vaxa.strath.ac.uk

_________________________________________________________



Shep,

You should be aware of the Oxford Molecular package Asp, this is an
implementation of the Carbo method of similarity calculation as developed
by Dr. Graham Richards et al in Oxford University.  The method relies on
the calculation of property overlap integrals and uses either a grid-based
method, or a gaussian approximation.  The latter is significantly faster,
and yields indices which are comparable with the grid calculations.  The
'property' is either shape, charge, lipophilicity or any other
user-supplied potential that may be calculated from atom-centred values.

Similarity indices may be calculated either for;

1) fixed orientations,
2) rigid rotation/translation
3) flexible (bonds).

In all cases the 'lead' molecule is fixed and the comparison is optimised.

The software runs on SGI, IBM and HP workstations, and presents the user
with a spreadsheet-based GUI.  Alternatively, Asp may be run via the OM
product Tsar, which is an integrated package (molecular spreadsheet) for
QSAR analysis.

Further details may be obtained from any OM office, or via the OM WWW pages at;

http://www.oxmol.co.uk/

Hope this helps,

Rob Scoffin
===========


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___________________________________________________________________


Dear Shepard,

What kind of similarity are you referring to?
Similarity can be structurally based, such as an RMSD.
Or, similarity can refer to an aggregate representation of a molecule
comprising the number and types of functional groups, presence absence
of rings, etc. 

As I am mopre familiar with the latter, Daylight which develops and
markets the MedChem suite of programs is indeed the best for the
latter. Hope this helps...

-mark


******************************************************
*                                                    *
*                                                    *
* Mark A. Zottola                                    *
* markz@dna.chem.duke.edu                            *
* Department of Chemistry                            *
* Duke University                                    *
* Durham, NC 27704                                   *
*                                                    *
*                                                    *
* The fault, dear Brutus, lies not with ourselves,   *
* but rather within our CPUs.                        *  
* (with apologies to Shakespeare                     *
*                                                    *
*                                                    *
******************************************************




________________________________________________________________

Hello,

I read your request for similarity methods and I would like to 'submit' the 
following information about a superposition method developed in the group of 
Prof. J. Kroon at Utrecht. The method is to be published soon. 

-------------------------------------------------------------------------------



* QUASIMODI
* Molecular superposition by means of simulated diffraction patterns.
* Patterson (electron) density superposition.


QUASIMODI is a superposition program using similarity index calculation by means 
of simulated crystallographical data. Optimization of overlap is performed in 
Fourier space; the constraint of overlap is Patterson (electron) density (which 
automatically includes steric and electronic factors).

As for now, the input requires atomic coordinate data for two molecules (.mol, 
.res files). Internal rotations are not incorporated, so a fixed conformation is 
to be supplied. A job file specifies the optimizations to be performed.

Resolution of the Patterson (electron) density description is defined by the 
user.

Further use is made of quantum-chemical data which are incorporated in the 
program (taken from SHELX).

Automated optimization is performed starting from 12 starting geometries which 
are generated by the program. The output contains a list of optimized rotation 
and translation parameters for a number of overlays which give rise to maxima in 
the similarity parameter space. 
Optimized parameters are given with respect to the input geometry. Root Mean 
Squared deviations with respect to the input coordinate data (or a user-supplied 
molecule) can be determined.
Output of the optimized geometries is possible.

Calculation times are rather fast: 
Twelve optimizations are performed in 5-10 minutes at intermediate resolution 
(twelve low resolution calculations are performed within two minutes).
The twelve starting optimizations cover the parameter space to be searched well 
(in practice it is seen that the number of optimal overlays, i.e. the number of 
-local- maxima in similarity index parameter space is less than 12).


Submission of the program to QCPE will follow.

---

I hope this is of any use to you. 
Kind regards,

Willem Nissink






________________________________________________________________
J.W.M. Nissink                 |              
Utrecht University             |    E-Mail:           
Department of Analytical       |    W.Nissink@ams.chem.ruu.nl
Molecular Spectrometry         |    
P.O. Box 80.083                |    S-mail:             
3508 TB Utrecht                |    Poortstraat 14 bis         
The Netherlands                |    3572 HJ  Utrecht            
Tel. +31.30.536817 / 537500    |    Holland
Fax. +31.30.518219             |    
________________________________________________________________



Shep,

	Thought I'd take the opportunity to describe some new stuff I've done
(we're shipping it with Spartan V4.0)...

(i)   What are the commonly used (public or commercial) similarity
      programs?
(ii)  What are their major features?

	Spartan now has a similarity/superposition tool - it aligns a series of
molecules against a user-specified template by maximizing the similarity of 3D
grid-based functions surrounding each molecule.  These can be classical
"functions" like volume or electrostatic potential from formal charge or
quantum-based functions like density, electrostatic potential, etc.  In
addition, the user can import functions calculated outside of Spartan.  It's a
simplex-based optimizer, since that seems to be pretty successful in spanning
problem space (and is less dependent on initial guesses for alignment).
 Naturally, the code can be used as a similarity measure as well.  It does not
allow for internal motion (although it can be mated with conformational
analysis to "emulate" flexible fitting).

	We also have a form of Hopfinger's molecular shape analysis - it will
report the volumes, pairwise volumes and volume similarities for a series of
molecules.

Hope this helps!

Joe


(iii) What sort of data do they use to compute the similarity?

	The MSA code uses a MC/numerical integration scheme to calculate
volume/shared volume.  The similarity/superposition module uses 3D grid-based
functions - as simple as y/n values for VdW-sphere volume to as complex as the
user can calculate.  It uses Spartan's graphics module to calculate the grids
(which permits difference grids, etc) and can import grids from outside
Spartan.
There are a range of error functions (RMS, correlation, Carbo, etc).



-- 

------------------------------------------------------------------------
Joe Leonard
Wavefunction Inc.
18401 Von Karman, Suite 370
Irvine, CA  92715                       I am a professional...
714-955-2120                                    do not attempt this at home.
714-955-2118 fax
jle@wavefun.com

_____________________________________________________________


Shep,
	The topic of structural similarity is fairly old and diverse now.
Here is an ever so quick low down:

1.	2D methods
	The earliest are topological, and the following are some of the 
	approaches:
	-	Fragment keys for substructure search (Pfizer, Willett)
	-	Atom-pair enumeration (Lederle)
	-	'Torsional descriptors' (Lederle)
	-	Maximal common subgraph (Willett)
	-	Topological indices (?)

	The best summary is Willett, "Similarity and Clustering in
	Chemical Information systems," RSP, 1987. 

2.	3D methods
	-	Grid or field overlay (Richards), w/ or w/o conformational 
		flexibility
	-	Projection ('Sperm')
	-	Atom-triplet enumeration (Lederle, CAS)
	-	Atom-triplet enumeration, with fancy indexing (IBM's "FLASH")
	-	Distance matrix comparison (Willett)
	-	3D Maximal Common Subgraph (Willett)
	-	... And lots more than that...

Enjoy -- Tom Moock, MDLI

______________________________________________________________________




Dear Dr. Smithline

Here is an answer to your query about 'similarity'.  I hope you will summarize
and post the answers you get.

>i)   What are the commonly used (public or commercial) similarity
>      programs?
---- I don't know how many of the programs themselves are available, but do you realize
how many different methods are available ? There are indeeed very many, ranging
>from topological indices ( Randic, Balaban, Keir & Hall and many others ), surface
topology and homology groups of algebraic topology ( Mezey ), graph theoretical
methods ( Randic, Bayada ), quantum mechanical methods ( Carbo, Richards et al.,
Cioslowoski, Allen & Cooper and others ) and surface shape descriptors ( Bywater et al.,and various researchers at Scripps: Duncan, Olson, Getzoff, Max). You will find all
the references to these methods in a forthcoming book :


"~Quantitative Measurement of Molecular Similarity using Shape Descriptors~" in
R. Carb\'{o} (~Ed.~), "~Molecular Similarity and Reactivity~: from Quantum
Chemistry to Phenomenological Approaches~", Kluwer Verlag, 1994. 


As to programs that are available, you should ask Oxford Molecular about the program
ASP. The shape descriptor programs developed by myself and colleagues will be
available one day, but don't expect that to happen too soon, ask me again in about
6 months from now. But in the meanwhile, you might want to read these papers :

S. Leicester, J. Finney & R. Bywater J. Mol. Graph. (1988) 6 104-108
S. Leicester, J. Finney & R. Bywater J. Mathematical Chemistry (1994) 16 315-341
S. Leicester, J. Finney & R. Bywater J. Mathematical Chemistry (1994) 16 343-365

Good luck !

Robert Bywater

Novo Nordisk A/S
DK-2880 Bagsvaerd
Denmark


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I believe that it was one of Prof. Dewar's remarks that practically all HF was 
'semi-empirical' in a number of senses: ultimately that it had to pe compared to
reality at some point, which meant for STO-nG calculations one would fudge 
around explaining why the computations were so bad.

I'm not one to say whether such comments are truth or propaganda, nor can I say 
whether DFT has forms which are 'ab-initio enough' to be ab-initio. However, one
can parameterize mm2 methods to reproduce HF or MP energies, and no-one would 
believe that those methods are 'ab-initio', even though from a black-box view 
they might be. Likewise, from a black-box view the fact that DFT spews out HF or
MP quality results does not mean that the calculations are ab-initio.

Personally, I don't care much for the need to distinguish the two in any other 
way than to say that semi-empirical methods are fudged to make them look better.
Given a 'good' ab-initio method, it would seem foolish to not fudge the 
parameterization a little to 'represent nature' better, either subsequent to the
calculation with pages and pages of text to explain what the difference between 
theory and experiment is, or before the calcualtion with pages and pages of text
to explain why this parameter or that functional makes the calculation mirror 
reality better.

Matthew Harbowy
'my views have nothing to do with lipton'

______________________________ Reply Separator _________________________________
Subject: CCL:Are methods based on DFT ab initio?
Author:  chemistry-request@ccl.net at INTERNET
Date:    05/15/95 9:25 PM
     
     <snip>
     
Does this make HFS a semi-empirical theory?  I think not:  There is 
one and only one adjustable parameter, and the functional should be 
equally applicable in any part of any molecule.  If you insisted on 
calling such a scheme semi-empirical, then you'd have to call Hartree- 
Fock frequencies adjusted by the famous 10% factor semi-empirical as 
well.  (If you already do, that's fine with me.  You're a purer man 
than I am, Gunga Din.)  In a semi-empirical method, parameters are 
chosen for *each atom*, and if you don't have parameters for cesium, 
you simply cannot do semi-empirical calculations on cesium chloride. 
But once you have this one DFT parameter -- or even two or three -- 
you can do calculations anywhere on the periodic table (modulo 
relativity).
     
Now there have been calculations carried out in which this HFS alpha 
parameter *was* different for each atomic environment (the so-called 
muffin-tin method), and those I *would* call semi-empirical.  But
that does not represent the main body of present-day density functional 
theory.
     
There are certainly more recent examples of density functionals 
containing one or more fitted parameters; my former boss Axel Becke 
frequently ends up with one unknown left over when he's inventing a new 
functional.  Nevertheless, in every case I know of the result after the 
fitting has been a density functional intended to be universally 
applicable.  What we are pursuing, after all, is Hohenberg's and Kohn's 
universal functional of the density -- you only need, in principle, one 
functional and you can then calculate all nondegenerate ground states. 
If we try to derive this functional from physics, we are working "from 
first principles" -- or "ab initio".
     
The other sense in which I can imagine DFT being characterized as 
"semi-empirical" is the manner in which the recent proliferation of 
functionals has been greeted by the user community.  I've seen more 
papers and talks and posters than I can count that had the nature of 
"try six different density functionals and see which one gives the best 
results for my systems."  If some thought then goes into the 
relationship between the underlying physics of the functionals and their 
performance, this is quite reasonable.  But if the lowest average 
deviation from experiment -- sometimes by a vanishingly small margin -- 
is then taken as the only reason for choosing functional X over 
functional Y for further studies on analogs of these systems, then we 
are at some risk of passing straight through semi-empirical methods into 
pure empiricism, and neither DFT nor semi-empirical specialists might 
care to claim such work as characteristic of their field. (Although I 
should confess I'm prone to this disease myself. Mea culpa.)
     
In conclusion, I don't really care what DFT is called except inasmuch 
as naming affects understanding.  I myself try not to use language 
which classes DFT as either ab initio or semi-empirical, because those 
terms have accreted fairly specialized meanings over the last twenty 
years and DFT really doesn't fit comfortably into either.
     
     
Cheers,
Ross M. Dickson, Ph.D. (dickson@zinc.chem.ucalgary.ca) 
Chemistry Dept., The University of Calgary, Alberta, Canada.
     
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