From chemistry-request@server.ccl.net  Thu Jul  6 00:02:10 2000
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From: "Tapas Kar" <tapaskar@siu.edu>
To: "art'" <Arturas.Ziemys@vaidila.vdu.lt>
Cc: <chemistry@ccl.net>
References: <200007050652.IAA03759@wacx73.chemie.uni-wuerzburg.de> <3963A64B.3F25AC8A@vaidila.vdu.lt>
Subject: Re: CCL:G94 Cube file
Date: Wed, 5 Jul 2000 22:59:45 -0500
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Chem3D can read and draw nice picture of MOs, densities etc.
__________________________________
Tapas Kar
Department of Chemistry
1245 Lincoln Dr #146F
Southern Illinois University
Carbondale, IL 62901-4409

Tel: 618-453-6485 (Office)/6433(Lab)
Fax:618-453-6408

Email: tapaskar@siu.edu
          tapas@risky3.thchem.siu.edu


----- Original Message -----
From: art' <Arturas.Ziemys@vaidila.vdu.lt>
Cc: <chemistry@ccl.net>
Sent: Wednesday, July 05, 2000 4:19 PM
Subject: CCL:G94 Cube file


> Hi, CCLers,
>
> There is lack of formation about CUBE in the help of Gaussian.
> These are files with data of MO or density information in 3D lattice. What
kind of
> soft can visualise Cube files? How they should be interpreted or analized?
> Any information concerning that is wellcome.
>
> I will summurise
>
> A.Ziemys
> *Vytautas Magnus Universitu            Ins. of Biochemistry
>   Dept. of Biology                             Lab. of Enzymatic chemistry
>   Vileikos 8                                       Mokslininku 12
>   LT-3035, Kaunas                           Vilnius
>   Lithuania                                         Lithuania
>
>
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>
>
>
>


From chemistry-request@server.ccl.net  Wed Jul  5 23:51:51 2000
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From: David Santo Orcero <irbis@df.ibilce.unesp.br>
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To: Iraj Daizadeh <iraj.daizadeh@genxy.com>
cc: chemistry@ccl.net
Subject: Re: CCL:comutational precision: removing round-off errors.
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 Hello!

> If one takes 625 and divides this number by, lets say, 5 on a computer
> one may get one of
> two numbers that look like: 125.000000000000000001 and
> 124.4999999999999999 .
> 
> Is this true? and, if so, how does one remove possible rounding errors

 Yes, it is true.

 And there is no solution, sorry. Here is why:


 Numbers in floating point format are something like:


 Number= (-1)^sign * (1.mantisa) * base ^ (exponent - kexp)


 
 Mantisa can be in other format, but uses to be as (1.mantisa); after
a calculus, the number is LRed to its first digit is 1 (on binary format).
Thus, that 1 doesn't need to be almacenated on the memory of the computer.
This is called "normalized floating point". Nearly all computers uses
this.

 Base uses to be 2; kexp, as far as I renember, 127 in IEEE754 32 bits
and 1023 in IEEE754 64bits.

 0 is not representable. For this, it is used a special kind of 
representation, that allows representate +Inf, -Inf and NaN. It
allows also +0 and -0, but this is another story...

 Then, you will have a number representated as:

(sign, mantisa, exponent)


 As you see, not all numbers are exactly representated. Some
numbers that are simple on decimal representation, on floating
point would need infinite precision.


 The propagation of the error by the non-exact nature of
floating point numbers is really complex, and for really short integration
steps can be 1 or 2 order of magnitude higher that the
error for the truncation of the Taylor's serie by the integration
algorithm.


 Sorry for my bad english. Sorry also by the bad news. ;-) I hope that
this message helps.

 Yours:

David





From chemistry-request@server.ccl.net  Thu Jul  6 02:30:25 2000
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Date: Thu, 6 Jul 2000 11:23:07 +0530 (IST)
From: "R.B.Sunoj" <srb@orgchem.iisc.ernet.in>
To: info@gaussian.com
cc: CHEMISTRY@ccl.net
Subject: CIS calculation
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Hello,

I was trying to do a CIS calculation with a 6-31+G* basis set using G-94.
Unfortunately I always end up in getting the following job termination!.
Please have a look at it and give your valuable suggestions. I will be
happy to summarise the responses.

Tail of the out put
---------------------

 Standard basis: 6-31+G(d) (6D, 7F)
 There are   187 symmetry adapted basis functions of A   symmetry.
 Crude estimate of integral set expansion from redundant integrals=1.000.
 Integral buffers will be    131072 words long.
 Raffenetti 1 integral format.
 Two-electron integral symmetry is turned on.
   187 basis functions      320 primitive gaussians
    32 alpha electrons       32 beta electrons
       nuclear repulsion energy       400.4330949861 Hartrees.
 One-electron integrals computed using PRISM.
 There are   3 eigenvalues of the overlap less than 1.0D-05
 The smallest eigenvalue of the overlap matrix is  3.606D-06
 Projected INDO Guess.
 Requested convergence on RMS density matrix=1.00D-08 within  64 cycles.
 Requested convergence on MAX density matrix=1.00D-06.
 Integral accuracy reduced to 1.0D-05 until final iterations.
 Initial convergence to 1.0D-05 achieved.  Increase integral accuracy.
 SCF Done:  E(RHF) =  -382.484431956     A.U. after   20 cycles
             Convg  =    0.5149D-08             -V/T =  2.0024
             S**2   =   0.0000
 Range of M.O.s used for correlation:    10   187
 NBasis=   187 NAE=    32 NBE=    32 NFC=     9 NFV=     0
 NROrb=    178 NOA=    23 NOB=    23 NVA=   155 NVB=   155

 **** Warning!!: The largest alpha MO coeffient is  0.16393177D+03

 Semi-Direct transformation.
 ModeAB=           4 MOrb=            23 LenV=       3211000
 LASXX=     16662856 LTotXX=    16662856 LenRXX=    33769037
 LTotAB=    17106181 MaxLAS=    69753572 LenRXY=           0
 NonZer=    50431893 LenScr=    78858840 LnRSAI=    69753572
 LnScr1=   107841358 MaxDsk=   671088640 Total=    290222807
 SrtSym=           T
fsync failed in NtrExt1.

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

with best wishes,
Sunoj

===========================
R. B. Sunoj
Dept of Organic Chemistry
Indian Institute of Science
Bangalore 560 012
===========================


From chemistry-request@server.ccl.net  Thu Jul  6 04:47:32 2000
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Date: Thu, 6 Jul 2000 10:49:34 +0200
To: CHEMISTRY@ccl.net
From: Marcel Swart <m.swart@chem.rug.nl>
Subject: Re: CCL:geometry with an applied electrical field?
Content-Type: text/plain; charset="us-ascii" ; format="flowed"

>Dear CCLers!
>
>Does anyone know what quantumchemical program is able to optimize a
>geometry with an applied electrical field? All programs that I have
>used until now allow only single point calculations with an E-field.
>
>Thanks in advance,

HONDO although not as fancy as the major programs, does the trick.

Since GAMESS and HONDO originally come from the same program,
I guess you could also try to use GAMESS, since this is maybe somewhat easier
to obtain.

-- 
------------------------------------------------
drs. Marcel Swart

Theoretical Chemistry (MSC)
Molecular Dynamics (GBB)

Rijksuniversiteit Groningen
Chemistry Department
Nijenborgh 4
9747 AG Groningen
The Netherlands

tel : +31 - (0)50 - 3634377
fax : +31 - (0)50 - 3634441

E-mail : m.swart@chem.rug.nl
WWW: http://theochem.chem.rug.nl/~marcel/
------------------------------------------------

From chemistry-request@server.ccl.net  Thu Jul  6 05:02:30 2000
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Date: Thu, 06 Jul 2000 10:58:49 -0700
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Subject: SUMMURY: G94 Cube file
References: <200007050652.IAA03759@wacx73.chemie.uni-wuerzburg.de> <3963A64B.3F25AC8A@vaidila.vdu.lt> <001c01bfe6fe$9f1b2060$5363e683@thchem.siu.edu>
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Hi CCLers,

Thank you all, who repyed so quickly. gOpenMol was the most mention free
software for visualisation of Cube files.
Here is all answers:

************************************************
Tapas Kar wrote:

> Chem3D can read and draw nice picture of MOs, densities etc.
> __________________________________
> Tapas Kar
> Department of Chemistry
> 1245 Lincoln Dr #146F
> Southern Illinois University
> Carbondale, IL 62901-4409
>
> Tel: 618-453-6485 (Office)/6433(Lab)
> Fax:618-453-6408
>
> Email: tapaskar@siu.edu
>           tapas@risky3.thchem.siu.edu

***********************************************
You can see GOPENMOL package at
http://www.csc.fi/~laaksone/gopenmol/gopenmol.html

  Andrea Giovanni Alparone
  PhD
  Universita di Catania
  Dipartimento di Scienze C
***********************************************
The next version of MOLEKEL http://igc.ethz.ch/molekel/ will be able to
visualize gaussian cube files. The new release will be based on OpenGL
and not IRIX GL anymore, those will be much more flexible according
platforms. The release is planed for this fall.

Stefan

--
Dr. Stefan Portmann
Laboratory of Physical Chemistry
ETH-Zurich
Universitaetsstr. 65
CH-8092 Zurich
Switzerland

Phone: +41 (0) 1 632 57 82
Fax:   +41 (0) 1 632 16 15
e-mail: portmann@igc.phys.chem.ethz.ch
WWW: http://igc.ethz.ch/portmann
***********************************************
ou can read and visualise this data for example with molden, gaussview,
gOpenMol.

I prefer gOpenMol.

Have a look at http://www.gaussian.com/00000430.htm
and http://www.csc.fi/~laaksone/gopenmol/gopenmol.html
and http://www.caos.kun.nl/~schaft/molden/molden.html

  Stefan Konietzny
  Dipl.-Chem.
  Heinrich-Heine-Universit?t D?sseldorf
  Institut f?r Anorganische Chemie und
  Strukturchemie II
                                      <Stefan.Konietzny@uni-duesseldorf.de>
                                      Conference Software Address
                                      Default
***********************************************
hello
you can use OpenDX (www.opendx.org), the cube files generated
by g94 are easily adapted to DX format, this is a .dx data
file , the `#' commented lines are those on the original g94 cube file.

 #SCF Total Density
 #   8   -6.658018   -6.512752   -6.658017
 #  86    0.190134    0.000000    0.000000
 #  70    0.000000    0.190134    0.000000
 #  86    0.000000    0.000000    0.190134
 #   6    6.000000    0.000000    0.000000    0.000000
 #   6    6.000000    0.000000    0.000000    2.813980
 #   6    6.000000    2.813980    0.000000    2.813980
 #   6    6.000000    2.813980    0.000000    0.000001
 #   8    8.000000   -1.687280    0.000000   -1.687281
 #   8    8.000000   -1.687282    0.000000    4.501260
 #   8    8.000000    4.501261    0.000000    4.501261
 #   8    8.000000    4.501260    0.000000   -1.687282
object 0 class gridpositions counts 86 70 86
origin -6.658018   -6.512752   -6.658017
delta   0.190134    0.000000    0.000000
delta   0.000000    0.190134    0.000000
delta   0.000000    0.000000    0.190134

object 1 class gridconnections counts 86 70 86
#attribute "element type" string "cubes"
attribute "ref" string "positions"

object 2 class array type float rank 0 items 517720 data follows
  1.65385E-08  2.05079E-08  2.53339E-08  3.11707E-08  3.81895E-08  4.65774E-08
[...517720 cube data points...]
attribute "dep" string "positions"

object "density" class field
component "positions" value 0
component "connections" value 1
component "data" value 2
end
***********************************************
The program Molden can visualize Gaussian Cube files.
have a look at URL:

http://www.cmbi.kun.nl/~schaft/molden/mapped.html

It discusses how to create an isodensity surface colorcoded with the
electrostatic potential. It also explains how to generate the gaussian
cube files and how to use them with molden.
Molden can render the outcome as postscript, vrml, povray and OpenGL
(you need the molden helper program moldenogl for that:

http://www.cmbi.kun.nl/~schaft/molden/opengl.html
For more information have a look at the Molden Home Page:
http://www.cmbi.kun.nl/~schaft/molden/molden.html
You can download the software at our anonymous ftp site:
ftp.cmbi.kun.nl, /pub/molgraph/molden/molden3.6.tar.Z

Best Regards,
Gijs Schaftenaar
Author of Molden
***********************************************
Dear Arturas,

There is at least a solution at no cost: GOpenMol. This software is freely
available at the following address:

http://laaksonen.csc.fi/gopenmol/gopenmol.html

It works under MS Windows 95/98/NT, and offers many possibilities, apart from
the nice visualization of Gaussian cube files (through conversion to the
corresponding .plt files, which is accomplished from one of the menu options)
Of course, there are also commercial possibilities. Apart from GaussView, the
graphical interface to Gaussian, from Gaussian Inc., the last versions of
Chem3D, from Cambridge Software, are able to read directly Gaussian cube
files,
leading to nice representations of MOs, Electrostatic Potentials, Total
Densities, Spin densities, etc.

Regards,

Jose I. Garcia
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
Dr. Jose Ignacio Garcia-Laureiro
Depto. Quimica Organica. Instituto de Ciencia de Materiales de Aragon
Facultad de Ciencias (edificio D). Universidad de Zaragoza-CSIC
c/ Pedro Cerbuna, 12. E-50009 Zaragoza (Spain)
Phone: +34 976762271       e-mail: jig@posta.unizar.es
Fax:   +34 976762077
+++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
***********************************************
The gOpenMol-package is one free and good option for drawing the 3D
isosurfaces (and a lot more) from gaussian cube files. The program is
available for most platforms. See
http://www.csc.fi/~laaksone/gopenmol/gopenmol.html

Cheers,

Atte

        atte.sillanpaa@oulu.fi          +358 (0)8 553 1681 (work), KE 368
        Dept. of Physical Chemistry     +358 (0)40 592 7369 (gsm)
        Po-BOX 3000
        FIN-90014 University of Oulu
        FINLAND
                  |   Entropy requires no maintenance.   |
***********************************************
   There is extensive discussion of the format of the Cubes generated by G94
in the G94 User's Reference starting on page 54 along with skeleton Fortran
code to read one.

    There are a number of programs which can read this GaussViewW, PCModel
and Chem3D under Windows.  GaussView under Unix and Cerius 2 may still have
this capability.  You can also read these in a number of generic isodensity
codes by modifying the header information.  Check our Web site www.gaussian.com
under the applications showcase and the details for a number of options are
discussed.
--

  Douglas J. Fox
  Director of Technical Support
  help@gaussian.com
***********************************************

Have a nice day
A.Ziemys




From chemistry-request@server.ccl.net  Thu Jul  6 06:04:17 2000
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From: uccatvm <uccatvm@UCL.ac.uk>
Message-Id: <14897.200007061004@socrates-a.ucl.ac.uk>
Subject: Re: CCL:d-aug-cc-pVDZ for sulphur
To: chemistry@ccl.net (CCL)
Date: Thu, 6 Jul 2000 11:04:03 +0100 (BST)
In-Reply-To: <006f01bfe6df$d164c180$2fa1f8cf@cimav.edu.mx> from "Dr. Daniel Glossman" at Jul 06, 2000 09:49:00 AM
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Dear Daniel,

> Where can I find the coefficients of the d-aug-cc-pVDZ basis
> set for sulphur?  I have checked the EMSL data base but that
> basis set for sulphur is lacking.

The d-aug-cc-pVnZ sets can be easily derived from the aug-cc-pVnZ
sets by addition of an extra diffuse function for each angular
momentum symmetry present in the set (in your case: s,p,d). The 
exponents of the additional functions are given by alpha*beta (for
d-aug-cc-pVnZ), alpha*beta*beta (for t-aug-cc-pVnZ), etc.. Alpha 
is the exponent of the diffuse function in the aug-cc-pVnZ, and beta
is the ratio of the exponents of the two most diffuse functions in
this set (beta < 1). 

See Woon and Dunning, J.Chem.Phys. 103, 4572 (1995).

And also:
Van Mourik, Wilson, and Dunning, Mol.Phys. 96, 529 (1999) Appendix.

HTH,

Tanja
-- 
  ====================================================================
     Tanja van Mourik                                                
                                      phone                               
     University College London        work:   +44 (0)20-7679-4665   
     Christopher Ingold Laboratories  home:   +44 (0)1895-259-312    
     20 Gordon Street                 e-mail                         
     London WC1H 0AJ                  work: T.vanMourik@ucl.ac.uk 
     United Kingdom                   home: tanja@netcomuk.co.uk     
  ====================================================================

From chemistry-request@server.ccl.net  Thu Jul  6 11:53:04 2000
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From: "Tapas Kar" <tapaskar@siu.edu>
To: "R.B.Sunoj" <srb@orgchem.iisc.ernet.in>, <info@gaussian.com>
Cc: <CHEMISTRY@ccl.net>
References: <Pine.LNX.4.04.10007061114190.10878-100000@helix.orgchem.iisc.ernet.in>
Subject: Re: CCL:CIS calculation
Date: Thu, 6 Jul 2000 10:50:31 -0500
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Try with Cis=direct and MAXDISK=xxMB. The error is due to disk space
limitation.
Depending on your disk put xx values.
__________________________________
Tapas Kar
Department of Chemistry
1245 Lincoln Dr #146F
Southern Illinois University
Carbondale, IL 62901-4409

Tel: 618-453-6485 (Office)/6433(Lab)
Fax:618-453-6408

Email: tapaskar@siu.edu
          tapas@risky3.thchem.siu.edu


----- Original Message -----
From: R.B.Sunoj <srb@orgchem.iisc.ernet.in>
To: <info@gaussian.com>
Cc: <CHEMISTRY@ccl.net>
Sent: Thursday, July 06, 2000 12:53 AM
Subject: CCL:CIS calculation


>
> Hello,
>
> I was trying to do a CIS calculation with a 6-31+G* basis set using G-94.
> Unfortunately I always end up in getting the following job termination!.
> Please have a look at it and give your valuable suggestions. I will be
> happy to summarise the responses.
>
> Tail of the out put
> ---------------------
>
>  Standard basis: 6-31+G(d) (6D, 7F)
>  There are   187 symmetry adapted basis functions of A   symmetry.
>  Crude estimate of integral set expansion from redundant integrals=1.000.
>  Integral buffers will be    131072 words long.
>  Raffenetti 1 integral format.
>  Two-electron integral symmetry is turned on.
>    187 basis functions      320 primitive gaussians
>     32 alpha electrons       32 beta electrons
>        nuclear repulsion energy       400.4330949861 Hartrees.
>  One-electron integrals computed using PRISM.
>  There are   3 eigenvalues of the overlap less than 1.0D-05
>  The smallest eigenvalue of the overlap matrix is  3.606D-06
>  Projected INDO Guess.
>  Requested convergence on RMS density matrix=1.00D-08 within  64 cycles.
>  Requested convergence on MAX density matrix=1.00D-06.
>  Integral accuracy reduced to 1.0D-05 until final iterations.
>  Initial convergence to 1.0D-05 achieved.  Increase integral accuracy.
>  SCF Done:  E(RHF) =  -382.484431956     A.U. after   20 cycles
>              Convg  =    0.5149D-08             -V/T =  2.0024
>              S**2   =   0.0000
>  Range of M.O.s used for correlation:    10   187
>  NBasis=   187 NAE=    32 NBE=    32 NFC=     9 NFV=     0
>  NROrb=    178 NOA=    23 NOB=    23 NVA=   155 NVB=   155
>
>  **** Warning!!: The largest alpha MO coeffient is  0.16393177D+03
>
>  Semi-Direct transformation.
>  ModeAB=           4 MOrb=            23 LenV=       3211000
>  LASXX=     16662856 LTotXX=    16662856 LenRXX=    33769037
>  LTotAB=    17106181 MaxLAS=    69753572 LenRXY=           0
>  NonZer=    50431893 LenScr=    78858840 LnRSAI=    69753572
>  LnScr1=   107841358 MaxDsk=   671088640 Total=    290222807
>  SrtSym=           T
> fsync failed in NtrExt1.
>
> -------------------------------------------------------------
>
> with best wishes,
> Sunoj
>
> ===========================
> R. B. Sunoj
> Dept of Organic Chemistry
> Indian Institute of Science
> Bangalore 560 012
> ===========================
>
>
> -= This is automatically added to each message by mailing script =-
> CHEMISTRY@ccl.net -- To Everybody    |   CHEMISTRY-REQUEST@ccl.net -- To
Admins
> MAILSERV@ccl.net -- HELP CHEMISTRY or HELP SEARCH
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70
> Ftp: ftp.ccl.net  |  WWW: http://www.ccl.net/chemistry/   | Jan:
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>
>
>
>
>


From chemistry-request@server.ccl.net  Thu Jul  6 13:09:14 2000
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Date: Thu, 06 Jul 2000 13:13:21 -0400
From: elewars <elewars@trentu.ca>
Subject: WORDS LOCAL AND NONLOCAL:SUMMARY
To: chemistry@ccl.net
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Thurs, 2000 July 6

Thanks very much to all who responded to my question. The answers,
#1--8, are summarized below. I hope I haven't overlooked anyone.

EL
----

Original question:
Wednesday, 2000 June 21

Hello,

Does any one know why DFT functionals without gradient corrections are
called _local_, while gradient-corrected functionals are called
_nonlocal_? I am not asking about the theory behind these, but why these

terms are used. I know that nonlocal has a certain meaning in quantum
physics; does it have some special meaning in connection with
mathematical functions or functionals?  The term nonlocal applied to
gradient-corrected functional has been said to be mathematically wrong
(A. St-Amant, Reviews in Computational chemistry, vol. 7, chapter 5,
1996; p. 223).

Thanks

E. Lewars
=====
Answers:

Andrew T. Pudzianowski, andrew.pudzianowski@bms.com
#1


Dr. Lewars -
                    The term "local" comes from the local density
approximation
(LDA) in DFT, where it's assumed that the electron density at any given
point in a
molecule is the same as that in an electron gas, a system which has been
solved
exactly. The LDA provides correlation and is more accurate than the
Hartree-Fock
approximation in many cases, but it tends to "overbind" systems, i.e.,
it leads to
overestimates of bond energies and complexation energies. The LDA is
particularly
bad in describing H-bonded systems.
     The term "nonlocal" has been used to refer to anything that goes
beyond the
LDA, including gradient-corrected functionals. Some of these have
"local"
components derived from the electron gas description, but I don't know
if that's
what's objectionable about the use of "nonlocal" terminology with these
functionals.
                                                              Regards,
                                                       Andrew
Pudzianowski

---------
#2
Huub van Dam, h.j.j.vandam@dl.ac.uk

The term nonlocal originates from the fact that in addition to the local

terms you have gradient terms which say something about how the
functional
behaves in the immediate vicinity of the point where you're at. E.g.
compare gradient corrected functionals with a first order Taylor
expansion.


The reason I wouldn't use the term nonlocal is because of the word
"vicinity". In practice the gradient corrected functionals are still so
local that any long range correlation effect (e.g. dispersion) isn't
accounted for at all. So in fact these functionals are much more local
than
the name nonlocal suggests. So if you really don't want to write
"gradient
corrected" all the time than the term "semi-local" wouldn't be too bad
(although strictly mathematically that is probably wrong as well,
because
even gradient corrected functionals contain only quantities evaluated at
1
particular point even though it is a density and the norm of the
gradient).

------------------------
#3
Thomas Bligaard Pedersen,  bligaard@fysik.dtu.dk

Hello,

Locality in physics is often related to closeness in the time-space
continuum -
that a theory should yield its results without taking information into
account
that is not accessible due to information travelling only at the speed
of light or
slower. Accepting general relativity to be an axiom, means that all
correct
theories of nature should be local, which is not yet the case for
quantum
mechanics.

This meaning of locality would then principally be of interest in TDFT,
but nobody
would really care about it, as it is related to extremely small
corrections of
general relativity, while it is plentily difficult to include all
special
relativistic terms.

For many years the most used functionals in solid state physics were LDA
and LSDA.
That's probably why everything else going beyond the LSDA got to be
called
non-local, including the GGAs which are mathematically local.
Interestingly Walter
Kohn calls GGAs quasi-local when he speaks about them.

Best regards

Thomas B. Pedersen

-------
#4
Lou Noodleman  lou@scripps.edu

Dear Dr. Lewars,
Yes, words can cause big problems. DFT functionals without gradient
corrections are called local, precisely because there are no gradient
terms (and gradient terms in some sense sample the surroundings of
a given point); gradient-corrected functionals are called nonlocal
for exactly this reason. There is some confusion attending this,
since in quantum chemistry, "nonlocal" is also used for situations
where each orbital sees a different exchange potential (or exchange-
correlation potential). The latter meaning is true for Hartree-Fock (and
also
probably in a number of explicitly correlated methods like
MC-SCF and CI methods), but not in DFT methods either LDA or gradient-
corrected (GGA) methods. Hybrid Hartree-Fock-DFT methods like B3LYP
should be like Hartree-Fock, nonlocal in that each orbital sees a
different exchange-correlation potential in the one-electron SCF
equations.
Nonlocal terms cause the worse scaling behavior of Hartree-Fock (n**4)
versus
DFT (n**3) as a function of the number of active electrons in the
molecule.
However, there are fitting tricks (and threshold tricks)
 that can help to control this worse
scaling behavior in ab initio methods (as implemented in local MP2
methods
in Jaguar), and also there are other tricks in Turbomole (I hear).
A general rule in quantum chemistry is: "be sure you know how a
technical
term is being used in a particular context, what the author really
means."
Further, realize that the same term can be used to mean different things

by different people in different contexts. For example, "correlation"
can
mean whatever is left out of Hartree-Fock
(but is this spin restricted or unrestricted or broken symmetry?), but
there
are other equally valid frameworks.
 "Fermi correlation" has a statistical meaning (see McWeeney), and in my

view, "correlation" as defined in a statistical context as in the theory

of reduced density matrices has a much deeper meaning than the usual
"correction to Hartree-Fock" meaning.
Lou Noodleman
Molecular Biology TPC15
The Scripps Research Institute
La Jolla, CA 92037
.
-------------------
#5
Ross Dickson, rdickson@molecularmining.com


I believe the term "local" derives from the "local density
approximation"
(LDA), of Kohn & Sham (1965, Phys. Rev. A 1133).  Although the idea
is theirs, I can't say for certain that the term originated with them
also,
as I haven't the paper easily at hand.  I further suspect that the term
"non-local" arose as a casual or inexact means of distinguishing the
non-(local density approximation) functionals from the at-the-time
dominant LDA.

(I hope TeX notation is clear enough for this.)
A consequence of the Hohenberg-Kohn theorem is that
    e_{xc}(x) = e_{xc}[\rho]:
The exchange-correlation energy density at a point x is a _functional_
of the charge density at all points.  The local density approximation
amounts to supposing that
    e_{xc}(x) = e_{xc}(\rho(x)),
i.e. that the exchange-correlation energy density at a point x can be
adequately approximated by a _function_ of the charge density at that
point x.  It's local in the very concrete sense of "doesn't depend on
anything far away in coordinate space."

The various degrees of gradient correction can be characterized as
    e_{xc}(x) = e_{xc}(\rho(x), \rho'(x), \rho''(x), ...)
and so on:  You're still using a function, not a functional, for e_{xc},

but employing more and more derivatives of the charge density as
arguments (signified by ', '', etc.)  This, I think, is why Alain
St.-Amant
suggested that "non-local" is a bad term for this family of functionals,

and I am inclined to agree.  One is still working with the charge
density in the locality of the point at which one is evaluating the
energy
density (or the exchange-correlation potential), even though one is no
longer using the local density approximation.


Cheers,
Ross Dickson,
no longer a quantum chemist...

-----------
#6
Per-Ola Norrby, peo@dfh.dk

       Hi,

        I think the term "local" in this context means that the value
of the function in a mathematical point depends on that point only.
The gradient is by definition the difference between the function
values for two points separated by an infinitesimal distance.  That
is, the gradient and any functional depending on it can never be
exactly "local".  In principle, there could also be other types of
"non-local" functionals, but I believe that the gradient correction
is the first "non-local" fix that anybody ever introduces.  I'm not
aware of any non-local functional without gradient correction, but
there could well be.

        Caveat: I'm a chemist, so my language is probably not
mathematically correct...

        Per-Ola Norrby
--

^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^
  *  Per-Ola Norrby, Associate Professor
  *  The Royal Danish School of Pharmacy, Dept. of Med. Chem.
  *  Universitetsparken 2, DK 2100 Copenhagen, Denmark
  *  Tel.   +45-35306506, fax +45-35306040
  *  Email: peo@dfh.dk (preferred), peo@compchem.dfh.dk
  *  WWW:   http://compchem.dfh.dk/PeO/
-------------------
#7
Herbert Fruchtl, fruechtl@fecit.co.uk

There is a mathematical theorem  which states that if you know all
derivatives of an 'analytical function' (i.e. one that can be expressed
in a power series) in one point, you know the function in its complete
definition range.

Nonlocal functionals depend not only on the value of the density, but
also its derivatives (mostly only the first one, the gradient). The
gradient contains information about the surrounding area, not only the
point you look at. So the expression nonlocal my be not very intuitive,
but I don't think it's wrong.

HTH,

  Herbert

--------------
#8
Bert te Velde, tevelde@scm.com

Hi,

The 'local' functionals all use (only) the value rho(r), i.e. the
density in a particular point in space. The formula for the
density-functional potential (and/or) the energy-density in a given
point in space is a more or less simple formula of rho(r), the charge
density in the same point.

The term 'non-local' has been used to stress that the (original)
non-local gradient corrections used not only rho(r) but also its
derivatives, so you could see it as implying that not only the local
value of the density went into the formula but also (implicitly,
through the derivatives) values at other (nearby) points in space:
non only the LOCAL value of rho.

Critics of the phrase 'non-local' refer to the fact that the
potential (or energy-function) is not in itself a non-local function:
it still is a 'simple' function v(r), respectively e(r).
Consequently, the term 'nonlocal' has gradually disappeared and has
been replaced by the more appropriate phrase 'gradient-corrected', or
'generalized gradient approximation (GGA)'.

Best regards
Bert
============
=========












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Date: Thu, 06 Jul 2000 13:35:36 -0400
From: elewars <elewars@trentu.ca>
Subject: X-ALPHA, DFT TODAY:SUMMARY
To: chemistry@ccl.net
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Thurs 2000 July 6

Here is a summary of the answers to my X-alpha question. I thank all who
responded (#1--#4).

Question:

> > Monday 2000 June 12
> >
> > Hello,
> >
> > the Xalpha method, developed by John slater (1951) mainly for solids
and
> > atoms, and used till at least the early 1970's , was perhaps the
first
> > really useful DFT method. For molecules it has now been replaced by
> > Kohn-Sham-based approaches to DFT.
> >
> > (1) Is the Xalpha method still used for solids/crystals (e.g. by
> > solid-state physicists?). If not, what replaced it?
> > (2) In modern molecular DFT, probably the most popular method is
> > B3LYP/6-31G*. What seems to be the second most widely-used?
> >
> > Thanks
> > E. Lewars
====

Answers
#1
Dr Robert J. Doerksen, rjd@bastille.cchem.berkely.edu

> Dear Dr. Lewars,
>
>         I just have a small comment on (1):
>         You may be amused by the article Dennis Salahub wrote giving a

> retrospective on the X-Alpha method, in Theoretical Chemistry
Accounts,
> in their 20th century highlights issue:
>
> Dennis R. Salahub: From X<alpha>-scattered wave to end-of-the-century
> applications of density functional theory in chemistry.  Perspective
on
> "Chemical bonding of a molecular transition-metal ion in a crystalline

> environment" (Johnson KH, Smith FC Jr (1972) Phys Rev B 5: 831-843)
>
> That's in:       Theor Chem Acc 103 (2000) 3/4, 311-312
>
> Cheers,
>
>   Robert
>
> Dr. Robert J. Doerksen
*************************************************
> Head-Gordon Group
*
> Department of Chemistry                        work phone (510)
642-9304
> University of California                              fax (510)
643-6232
> Berkeley, CA, USA  94720         e-mail:
rjd@bastille.cchem.berkeley.edu
> **** webpage:
http://www.cchem.berkeley.edu/~mhggrp/doerksen/rjdhome.htm

---
#2
Per-Ola Norrby, peo@dfh.dk

         Hi,
>
> >(2) In modern molecular DFT, probably the most popular method is
> >B3LYP/6-31G*. What seems to be the second most widely-used?
>
>         I'd vote for BP86.  It's been around longer, is almost as
> accurate, and substantially faster (at least in some codes...).
>
>         /Per-Ola
> --
>
> ^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^
>   *  Per-Ola Norrby, Associate Professor
>   *  The Royal Danish School of Pharmacy, Dept. of Med. Chem.
>   *  Universitetsparken 2, DK 2100 Copenhagen, Denmark
>   *  Tel.   +45-35306506, fax +45-35306040
>   *  Email: peo@dfh.dk (preferred), peo@compchem.dfh.dk
>   *  WWW:   http://compchem.dfh.dk/PeO/

------------
#3
Thomas Heine, Thomas.Heine@chiphy.unige.ch

> (1) mainly LDA, later on GGA was used as well
> (2) B3LYP is the mostly used by chemists, it is almost never used by
> physicists, since (i) they don't like HF exchange since it makes the
> programs very slow, (ii) it just works well for lighter elements.
> Perdew-Wang 96, PW91 and the newer PBE is used quite often, I think in
a
> competitive amount with old-fashioned LDA (e.g. VWN).
>
> Thomas
> University of Geneva
>
> PS: Let me know what others tell you

---------
#4
Thomas Bligaard Petersen, bligaard@fysik.dtu.dk


 Hello,
>
> I propose a response to question 1:
>
> The Xalpha was also replaced by the Kohn-Sham approch. In solid state
physics the
> LDA (of Kohn-Sham) was the most used exchange-correlation functional.
The role was
> taken over by the LSDA (Gunnarson and Lundquist) that describes
magnetic systems
> better. These are still used, and especially in more theoretical part
of solid
> state theory, as they are some of the only true ab-initio approches in
DFT. For
> applications the PW91 (Perdew-Wang) has become very important, as it
corrects some
> important deficiencies of the LDA. The PBE (Perdew-Burke-Ernzerhofer)
removes
> some problems of oscillating xc-potential in the PW91, whereby the
numerical
> behaviour of the calculations are somewhat improved. Other then that
it yields
> results very similar to PW91, and has more or less replaced the use of
PW91 today.
> The B3LYP yields quite bad results in solids, this is probably related
to the
> Hartree-Fock approch having some problems here. In the future orbital
dependent
> potentials are probably going to have growing importance in solid
state physics,
> but the selfconsistent implementation of these functionals are not yet
in common
> use, even if the functionals appear to give vastly improved results
for some
> systems. One such functional is the PKZB meta-GGA
(Perdew-Kurth-Zupan-Blaha).
>
> In short the LSDA and the PBE are the most used today.

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


From chemistry-request@server.ccl.net  Thu Jul  6 04:15:00 2000
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Hello,

Is there some open source code (or part of code) allowing
to locate automatically where can occur possible variation of
torsion angles in a given molecule ?  Fortran preferably. Thanks.

--
Armel Le Bail
http://www.cristal.org/




From chemistry-request@server.ccl.net  Thu Jul  6 04:40:46 2000
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Date: Thu, 6 Jul 2000 10:42:49 +0200
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Subject: Re: CCL:comutational precision: removing round-off errors.
Content-Type: text/plain; charset="us-ascii" ; format="flowed"

>Hello.
>
>If one takes 625 and divides this number by, lets say, 5 on a computer
>one may get one of
>two numbers that look like: 125.000000000000000001 and
>124.4999999999999999 .
>
>Is this true? and, if so, how does one remove possible rounding errors
>produced when
>this occurs during lets say integration....

This is true, but depends on the machine on which you run the program.
However, if you use FORTRAN90, you have somewhat control of the error.
If you use selected_real_kind(15,70) to define the kind of all reals,
you can check if that kind is available on that machine.
The 15,70 means 15 decimals precision, and exponent up to power 70.



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Dear all

I've got the following message error when linking the g98 on a Linux RedHat
machine:

g77   -O2 -march=pentiumpro -malign-double -m486 -fexpensive-optimizations -O3
-ffast-math -funroll-loops  -c ml0.f
rm -f ml0.f ml0.c
make[1]: Leaving directory `/home/perico/g98'
g77    -O2 -march=pentiumpro -malign-double -m486 -fexpensive-optimizations -O3
-ffast-math -funroll-loops  -o g98 ml0.o   util.so
util.so: undefined reference to `wait_'
util.so: undefined reference to `fork_'
collect2: ld returned 1 exit status
make: *** [g98] Error 1
endif

It seems that it can't resolve a couple of functions which however are defined in
the mdutil.c file. Are they essential? Any suggestions?

thank you in advance

Pedro
--
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Reply-To: Malcolm Gillies <M.B.Gillies@pharm.uu.nl>
Subject: Summary: OpenGL on Linux and Insight/Sybyl
In-reply-to: <200007030955.LAA12754@cmcind.pharm.uu.nl>
Date: Thu, 06 Jul 2000 12:49:21 +0200
From: Malcolm Gillies <gillies@cmcind.pharm.uu.nl>

I've compiled a (slightly edited) list of replies to my question, as
well as some ensuing discussions.

Thank you to everyone who responded.

The general impression I gained is that hardware accelerated OpenGL
on Linux has similar performance to SGI for many molecular graphics
applications, and that people who are using it are quite satisfied.
In particular, various in-house and non-commercial programs are
reported to work well.

Unfortunately, noone seems to have succeeded in getting MSI Insight
(aka Biosym InsightII) working with a remote Linux OpenGL display.
At first glance, this appears to be a minor problem with Insight
recognizing the remote display type correctly, but there may also be
other more subtle difficulties to overcome. I'd be interested to know
MSI's response to this problem.

I received one clear report that Sybyl can be used in the way I
propose, though apparently there is a problem with object selection.
Given that Tripos are supporting configurations using a PC X server
with OpenGL (e.g.  Exceed 3D), I would expect that fixes or
workarounds shouldn't be too difficult.

I didn't hear from anyone who is using the new SGI Visual
Workstations.
--
Malcolm Gillies <M.B.Gillies@pharm.uu.nl>
PhD student, computational medicinal chemistry
Dept Medicinal Chemistry, Faculty of Pharmacy,
Utrecht University, The Netherlands
------- Messages

Date:         Mon, 03 Jul 2000 11:55:21 +0200
From:         Malcolm Gillies
Subject:      CCL:OpenGL on Linux and Insight/Sybyl - any experiences?
Message-Id:   <200007030955.LAA12754@cmcind.pharm.uu.nl>

I'm interested in hearing about any experiences using Linux with an
X server supporting OpenGL/GLX as a remote display for modelling
programs such as MSI Insight or Tripos Sybyl.

In particular, I'd like to hear if the following kind of setup is
workable in practise:

* Insight running on SGI
* Linux 2.2.* kernel on x86
* Nvidia video card (GeForce 256/GeForce 2 GTS/Quadro)
* Nvidia OpenGL Linux reference drivers and Xfree86

But I'm also interested in information on other video cards, drivers,
or the new SGI Visual Workstations (VPro graphics) under Linux.

If this sort of configuration is practical, then it could be a cheap way
of expanding a modelling lab with extra workstations for light use by
students, etc.

------- Message 2

Date:         Mon, 03 Jul 2000 14:29:59 +0200
From:         Sigismondo Boschi
Message-Id:   <39608747.8A7F4472@cineca.it>

Dear Malcolm,

I have installed the glx module for the Matrox G400. It is a module
in development, for Xfree 3.x You can find it and information about
it at http://www.matroxusers.com/

It works quite fine interfacing MSI cerius2 (InsightII does not
recognize it giving the error "Couldn't get initial visual in
app_init_display" indeed!  Xvision for windows does the same) running
both on IBM rs6000 (SP) and Origin2000. The main lack is the "depth
cueing". For the rest it works fine, very fast rendering atoms and
isosurfaces, comparable with an SGI O2. The PC is a PentiumIII
450MHz, Linux Redhat 6.1, XFree86 3.3.5, matrox G400 single-head
16MB.  Also other software runs fine: gaussview and gOpenMol for
example.

Checking now the site "matroxusers" I have found they have included
the DRI driver (direct rendering interface) also for this board in
the very new Xfree86 4.0.1. More information at
http://www.xfree86.org and in particular
http://www.xfree86.org/4.0.1/RELNOTES.html

Actually I have not tried it: I have found it just now. I will let
you know if in the next days I will be able to try it.

Please, post the summary to CCL!  Thanks

Kind regards

   Sigismondo

-- 
 -------------------------------------------------------------------------
|Sigismondo Boschi, Ph.D.                |tel: +39 051 6171559            |
|CINECA (High Performance Systems)       |fax: +39 051 6137273 - 6132198  |
|via Magnanelli, 6/3                     |                                |
|40033 Casalecchio di Reno (BO) ITALY    |WWW: http://www.cineca.it       |
 -------------------------------------------------------------------------

------- Message 3

Date:         Mon, 03 Jul 2000 09:27:47 -0400
From:         "Bienstock.Rachelle"
Message-Id:   <4D693F933DD8D311A18C00E018B0057652C825@trollope.niehs.nih.gov>

Malcolm:

Although I am by no means an expert in this area, it was my
impression that the MSI Insight software package currently available
will not run on Linux.  First, because it is commercial software
package, you are only given the executibles which are currently only
sold and available as compiled code under Irix.  MSI is working on a
commerical version which will be available for Linix.  You may want
to consult with MSI to see when this will be available.

Rachelle

------- Message 4

Date:         Mon, 03 Jul 2000 09:54:06 -0400
From:         "Bienstock.Rachelle"
Message-Id:   <4D693F933DD8D311A18C00E018B0057652C827@trollope.niehs.nih.gov>

> I'm aware that neither Insight nor Sybyl will run on Linux. What I'm
> actually proposing is that the software continue to run on an SGI
> machine, but with a remote Linux X server as display.

Yes, I guess it should work.  Actually, I know at several
universities they have been running the MSI Insight software using
the Hummingbird Exceed software on the PC as an X-terminal emulator.

------- Message 5

Date:         Mon, 03 Jul 2000 10:07:00 -0400
From:         "Bienstock.Rachelle"
Message-Id:   <4D693F933DD8D311A18C00E018B0057652C828@trollope.niehs.nih.gov>

> Right, the crux of the question is if they are using -opengl graphics or
> -axxess X graphics; the latter has been possible for some time, but comes
> at the cost of much more primitive graphics.
> 
> Do you know if they are using a version of Exceed which supports OpenGL
> graphics (I think it's called Exceed 3D)?

You know,I believe it was using the Axxess X graphics. At one time I
had thought of setting this up (to run the software at home on my PC)
and received lots of replies from people who were using the Insight
II software this way with Exceed.

If you search the Comp. Chem. archives you may find some info.
Everyone told me though that the software ran so slowly that it was
almost to the point of being unusuable- i.e.  rotating large
molecules etc.

------- Message 6

Date:         Mon, 03 Jul 2000 09:40:34 -0400
From:         Zsolt Zsoldos
Message-Id:   <396097D2.4F791EB0@simbiosys.ca>

Dear Malcolm,

My experience is not with Nvidia card, so I cannot comment on its
performance.  However, we have an SGI Indigo2 Impact and a number of
Linux computers. One of the Linux machines have an ELSA Gloria L/MX
graphics card and we use it with the XiG 3D Accelerated-X OpenGL
driver and X server combination (see http://www.xig.com/). This
combination on a 2.2.5-15smp kernel 2x350MHz Pentium II computer can
provide a very comparable performance to the Impact.  We use it with
our own modelling package, not Insight or Sybyl as we are a
computational chemistry software company ourselves. We use standard
OpenGL/GLX graphics in our software which runs on both the SGI and
the Linux-PC.  We use it in every combination (running the software
on either platform with both local and remote display) and each
combination works fine for the OpenGL graphics. On the other hand, we
experience some color mapping problems with non-OpenGL graphics
(menubars, button colors etc) wen running on Linux and remote
displaying on SGI.  But this might be to do with the Java Swing
library.

The mentioned XiG X server provides drivers for a large number of 3D
accelerated OpenGL cards, including the cheap Permedia2 based cards,
like Diamond FireGL 10 00Pro.  Those definitely provide a very cheap
alternative to SGI with usable performance.

I hope you find this information useful.  I'd be very interested to
see a summary of the replies you get, especially if you hear anything
about the SGI Visual Workstations graphics under Linux.

Best regards,
Zsolt

- -- 
Zsolt Zsoldos, PhD.                                         
Simbiosys Inc.                    phone: 1 - 416 - 741-4263
135 Queen's Plate Dr., Unit 355     fax: 1 - 416 - 741-5084
Toronto, Ont, M9W 6V1, Canada      http://www.simbiosys.ca/

------- Message 7

Date:         Mon, 03 Jul 2000 10:56:56 -0300
From:         antonio luiz oliveira de noronha
Message-Id:   <Pine.A32.3.96.1000703105252.5151A-100000@dedalus.lcc.ufmg.br>
In-Reply-To:  <200007030955.LAA12754@cmcind.pharm.uu.nl>

Mr. Gillies
	In my lab we use Linux MANDRAKE 7.1 and we had in our
workstations TRIPOS/SYBYL and MSI/INSIGHTII. Both work fine with the
linux box. Our video card is pretty simple, it's a Trident with 2 M.
Also, vwe only use the PCs with linux as terminals, but work very
fine!

Best Regards!!

 ___________________________________________________________________
|                                                                   |
|Antonio Luiz Oliveira de Noronha                                   |
|Medicinal Chemistry of Organotin Compounds                         |
|NEQUIM - Medicinal Chemistry Group                                 |
|Chemistry Departament - DQ                                         |
|UFMG - Federal University of Minas Gerais - Brazil                 |
|Av. Antonio Carlos, 6627 - Campus Pampulha                         | 
|CEP 31270-901 - Belo Horizonte - MG - Brazil                       |
|VOICE +55 31 499 5765   -   FAX +55 31 499 5700                    |
|___________________________________________________________________|

------- Message 8

Date:         Mon, 03 Jul 2000 16:03:16 -0300
From:         antonio luiz oliveira de noronha
Message-Id:   <Pine.A32.3.96.1000703160145.12817A-100000@dedalus.lcc.ufmg.br>

Mr. Gillies

	I check it. Yup, the INSIGHT does not work, but the SYBYL
works fine, using the x graphics.

Regards!!

------- Message 9

Date:         Mon, 03 Jul 2000 15:58:52 +0200
From:         Ezequiel Quintana Morales
Message-Id:   <39609C1C.E1DE1154@iiq.cartuja.csic.es>

Hi,

We use on a daily basis, linux boxes as terminals of SGI's running
Sybyl. We use SuSE Linux starting from 6.2 to 6.4, and Nvidia TNT2
or GeForce 256 DDR video cards. For us that is the best option (the
cheapest).

They all run fine (GeForce better, :-)). The configuration is very
simple and y ou only need to load the iris fonts into the linux
machines. However, we have found that running Sybyl in OGLX mode,
the selection on screen of objects can hung the SGI. In XDEV mode
there is no problem.

Hope this help. If you want more details, please let me know.

Regards,
Ezequiel

- --------------------------------------------------------------------
Dr. Ezequiel Quintana Morales
Instituto de Investigaciones Quimicas
Centro de Investigaciones Cientificas Isla de la Cartuja
c/ Americo Vespucio, s/n
41092 Sevilla
Tel: + 34 95 4489564           Fax: + 34 95 4460565
- --------------------------------------------------------------------


------- Message 10

Date:         Mon, 03 Jul 2000 17:59:12 +0200
From:         Ezequiel Quintana Morales
Message-Id:   <3960B850.EF602CF6@iiq.cartuja.csic.es>

Malcolm,

> I guess you are using the Nvidia reference Linux driver. Is it
> reasonably stable?

I don't use the nvidia driver but the one that come with the SuSE
distribution. I tried several: Utah-glx and nvidia drivers but SuSE
in collaboration with UTAH-glx has one which works fine and it's
easier to install (just from the CD).

> > They all run fine (GeForce better, :-)). The configuration is very
> > simple and y ou only need to load the iris fonts into the linux
> > machines. However, we have foun d that running Sybyl in OGLX mode,
> > the selection on screen of objects can hung th e SGI. In XDEV mode
> > there is no problem.
> 
> That's interesting. So the SGI hangs, rather than the X server on
> the Linux machine?
> 
> I was hoping that things would work stably in OGLX mode.

I don't know if you has used Sybyl too much, but it's a very tricky
software. If you select objects using the dialog boxes everything is
ok, but if you need to point with the mouse on the screen Sybyl
crashes and most of the times hangs the computer (OGLX mode).

For TRIAD (NMR module of Sybyl), the best configuration I had tested
is XDM/Fvwm2(or mwm), but never KDM/KDE, and if you want a working
rubber band you need to have activated Num Lock.

> If possible, could you tell me which software versions you are using?
> 
> - Sybyl

6.6

> - Xfree86

3.3.6 (but 3.3.5 and 4.0 are also ok)

> - Nvidia drivers

As I told you before I use the drives which come with SuSE 6.2 and 6.4
(6.1 doesn't have them and I haven't tried 6.3).
For SuSE 6.2 they are:
   glxriva-1.0.8
   mesa-3.0.48
For SuSE 6.4:
   glx-000229-20
   mesa-3.1.35

------- Message 11

Date:         Tue, 04 Jul 2000 11:15:20 +0200
From:         Ezequiel Quintana Morales
Message-Id:   <3961AB28.727ADB3C@iiq.cartuja.csic.es>

Malcolm,

> I had the impression that the SuSE drivers only support the
> Riva 128/128ZX/TNT/TNT2 graphic boards of NVIDIA, and not the GeForce?

SuSE 6.4 supports also GeForce 256, GeForce 256 DDR and Quadro.

------- Message 13

Date:         Mon, 03 Jul 2000 16:24:44 +0100
From:         "BAYARD Francois"
Organisation: COMS
Message-Id:   <6920061747@mulliken.cpe.fr>

I am also very interested by this topic.
(I use sybyl)

Thanks to forward the answers you will collect.

Francois BAYARD 

Laboratoire COMS - CNRS/CPE UMR 9986
Bat F308  CPE LYON 
43 Bd du 11 Novembre 1918 - BP2077
F-69616 VILLEURBANNE CEDEX - FRANCE       
- -------------------------------
                              http://www.cpe.fr/lcoms
tel    (+33) 4 72 43 18 08  fax    (+33) 4 72 43 17 95

------- Message 15

Date:         Mon, 03 Jul 2000 17:25:25 -0500
From:         John Stone
Message-Id:   <20000703172524.C26538@geneseo.ks.uiuc.edu>


Hi Malcolm,
  I saw your post on CCL asking about hardware accelerated OpenGL on
Linux.  We've recently been woking with using the NVidia TNT2,
GeForce 256, and Geforce 2 GTS boards with Linux and XFree 4.0, and
have had some great results.  We are running VMD, our own molecular
visualization tool, which you may have already seen or heard of:
http://www.ks.uiuc.edu/Research/vmd/

Running VMD, a 700MHz Athlon with a GeForce 2 GTS easily doubles an
Onyx2 InfiniteReality2 on rendering speed with a 4,000 atom molecule
displaying in VDW representation.  The GeForce board isn't quite as
fast on lines, and it doesn't have the same hardware antialiasing
that our Onyx2 does, but for $300 US, there's no reason to question
the utility of having a GeForce... :-)

We've also run VMD with some of the other PC video boards that
support hardware 3-D on XFree 4.0, but I'd have to say that the only
ones worth looking at are the NVidia GeForce 2 GTS boards...  For
$300 US, you can get a linux box setup that'll roast most of the SGI
boxes that are out there, certainly so for the kinds of rendering
done in molecular graphics.  There are still a number things that the
SGI machines are better at, but rendering molecules isn't one of
them.  The only thing I can think of that the current generation
NVidia boards lack, that we want to have in our lab, are stereo sync
outputs for use with the CrystalEyes stereo glasses.  Fortunately,
there are some new low-end LCD stereo glasses coming out for PCs that
work with almost any video board, it'll only be a matter of time
before we see support for them in XFree/Linux....

Anyway, if you have questions about Linux and XFree 4.x, or on
getting/using VMD, let us know, and we can help you out.

  John Stone

- -- 

Theoretical Biophysics Group                             
Beckman Institute              http://www.ks.uiuc.edu/~johns/
University of Illinois         Phone:  (217) 244-3349
405 N. Mathews  Ave              FAX:  (217) 244-6078 
Urbana, IL 61801, USA          Unix Is Good For You!!!

------- Message 16

Date:         Tue, 04 Jul 2000 10:30:08 +0200
From:         Stefan Konietzny
Message-Id:   <3961A090.B5F8B6C8@uni-duesseldorf.de>

Hi Malcolm,

if it need not to be Linux, you should also try the Hummingbird
Exceed 3D X-Server for Windows.  They send you an evaluation copy
when you ask for.  Of course it's not free, but it worked really fine
with my ErazorIII (TNT2) Card. Most of those programs on our
origin2000 that where denoted "for SGI Workstation only" worked fine
on my PC-Display.  The Linux solution is cheaper, but the Windows
solution is still much cheaper than to buy several SGI's.

Don't blame me for giving the advise to use Windows :-), i'm a Linux
user, but the Exceed-X-Server worked better on my PC than the 3.3.6
plus the appropriate extensions from Nvidia.

Have fun, Stefan.

------- Message 17

Date:         Tue, 04 Jul 2000 13:43:10 +0200
From:         Stefan Konietzny
Message-Id:   <3961CDCE.F3FA2C68@uni-duesseldorf.de>

Hi Malcolm,

it was Gaussview in OpenGl mode, Cerius2 and InsightII.  It's a few
weeks ago, so i'm not really sure any more.  Further on all those
little programs that our sysop put in the toolchest with the comment
"for SGI only", that are 3D plots of CPU usage etc.

If you like to use Insight without OpenGL in the meantime try (is it
InsightII?) to start it with the --axxess option; that forces the
program not to use OpenGL but usual X-Graphics.

Stefan.

------- End of Forwarded Messages



From chemistry-request@server.ccl.net  Thu Jul  6 08:14:57 2000
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Date: Thu, 6 Jul 2000 14:13:59 +0200 (CEST)
From: Jochen Kuepper <Jochen@pc1.uni-duesseldorf.de>
To: Iraj Daizadeh <iraj.daizadeh@genxy.com>
Cc: chemistry@ccl.net
Subject: CCL:comutational precision: removing round-off errors.
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Iraj Daizadeh writes:
 > If one takes 625 and divides this number by, lets say, 5 on a computer
 > one may get one of
 > two numbers that look like: 125.000000000000000001 and
 > 124.4999999999999999 .
 > 
 > Is this true? 

Yes.

 > and, if so, how does one remove possible rounding errors
 > produced when
 > this occurs during lets say integration....

Look up a numerics book on floating point numbers. Some good and free
docs are lying around the net ;-)

Jochen
-- 
Heinrich-Heine-Universität, Institut für Physikalische Chemie I
Universitätsstr. 1, Geb. 26.43 Raum 02.29
40225 Düsseldorf, Germany                phone ++49-211-8113681
http://www.Jochen-Kuepper.de               fax ++49-211-8115195


From chemistry-request@server.ccl.net  Thu Jul  6 09:41:31 2000
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From: "Fulton CR (Charles)" <fultoncr@ucarb.com>
To: "'CCL'" <chemistry@ccl.net>
Cc: "'Krzysztof Radacki'" <krys.radacki@ac.rwth-aachen.de>
Subject: RE: Problem with stability of linux
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What motherboard and processors are you using? Have you tried using the
latest stable kernel (2.2.16)? 

Link to Linux-SMP FAQ - http://www.irisa.fr/prive/dmentre/smp-howto/ ,
specifically look at what kernel compile options you need to have your
.config. (mtrr, etc). There is some great information in the howto/faq. 

Hardware could be the problem.. (are you overclocking, etc?)  

-Charlie


------------------------------------------------------------------------
"Open your source and they will come" - various. 

Charles Fulton
Catalyst Skill Center
Union Carbide Corporation
S. Charleston, WV.  phone: (304) 747-3175 email: fultoncr@ucarb.com


> ----------
> From: 	Krzysztof Radacki[SMTP:krys.radacki@ac.rwth-aachen.de]
> Sent: 	Monday, July 03, 2000 1:08 PM
> To: 	chemistry@ccl.net
> Subject: 	CCL:Problem with stability of linux
> 
> 
> Hi,
> I got some problems with the linux-box on which I work.
> Real often the maschine hang during gaussian calculations
> in SMP-modus with following message (just example):
> ====
> Unable to handle kernel NULL pointer dereference at virtual adress
> 00000018
> current -> tss.cr3 = 0e0a6000, %cr3 = 0e0a6000
> *pde = 00000000
> Oops = 0000
> CPU = 1
> EIP = 0010: [<c0111478>]
> EFLAGS: 00010207
> ax: a7553000 ebx: daad4000 ecx: 00000000 edx: c023c000
> esi: 00000000 edi: 00000000 edp: daad5fbe esp: daad5f9c
> de: 0018  ec: 0018  sw: 0019
> Process l502.exe (pid:727, process nr:7, stackpage: daad5f9c
> Stack: 00000000....... some lines
> CallTrace : [<c0...>]
> Code: 8b 41 18 c1 f8 d1 03 41 1c 89 41 18
> 8b 49 34 81 f9 00 c0 23
> ======
> The questions: why  and what should I do again   :)
> Is it problem of software (I've change the kernel and I can't see any =
> difference),
> is it SMP-hardware or maybe memory? How can I test it?
> 
> regards
> Krzys Radacki
> 
> 
> -= This is automatically added to each message by mailing script =-
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> 
> 


From chemistry-request@server.ccl.net  Thu Jul  6 22:20:35 2000
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Hi,
I was wondering if anyone had surplus gaussian 94 user manuals 
that they no longer required, and wanted to sell (or give away).  As 
more groups at our University are becoming interested in 
computational chemistry, our copy is going walkabout a lot!!  The 
$US 70 price to buy another copy seems rediculous.  If anyone 
can help, please email me.
Thanks very much,
Tim


-------------------------------
Tim Robinson
Vikings Group
Department of Chemistry
University of Otago
03 479 7929
timr@alkali.otago.ac.nz


