From sschulz@weasel.chemie.fu-berlin.de  Wed Sep 10 09:23:16 1997
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Date: Wed, 10 Sep 1997 14:27:21 +0200 (METDST)
From: Stefan Schulz <sschulz@chemie.fu-berlin.de>
To: chemistry@www.ccl.net
Subject: CIS question for GAUSSIAN94
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Hi,

I am trying to do some very simple GAUSSIAN94 CIS/6-311++G(d,p) calculations for the 
first excited state of NaNH3 (C3V - symmetry) which has 
spin multiplicity 2 and spatial symmetry E.
My input looks like this:

#P CIS(NSTATES=3,ROOT=1)/6-311++G(d,p)
UNITS=(ANG,DEG) GFINPUT IOP(6/7=3)

sodium-ammonia excited states

0 2
Na
N  Na R
H1 N  R1 Na THETA
H2 N  R1 Na THETA  H1  120.0
H3 N  R1 Na THETA  H1 -120.0

R        2.59296852
R1       1.01379999
THETA  108.25124277

Although everything seems to work fine there are two points in the 
following lines of output which still give me some trouble:

1) What does this mean: Convergence on expansion vectors, NOT on wavefunctions!

2) Why is Gaussian unable to determine the spin multiplicity of the excited states?
   (Both spin and spacial symmetry are determined correctly for the ground state : 2-A1)

Can anybody give me some advice on these problems ???

I will be grateful for any advice or hint on this problem.
I have already checked www.gaussian.com 

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OUPUT SECTION (excerpt):
=========================

 Convergence on expansion vectors, NOT on wavefunctions!
 ***********************************************************************
 Excited states from <AA,BB:AA,BB> singles matrix:
 ***********************************************************************

 1PDM for each excited state written to RWF  633
 Ground to excited state Transition electric dipole moments (Au):
       state          X           Y           Z          Osc.
         1        -0.2376     -2.8373      0.0000      0.2988
         2        -2.8373      0.2376      0.0000      0.2988
         3         0.0000      0.0000     -2.4685      0.2590
 Ground to excited state transition velocity dipole Moments (Au):
       state          X           Y           Z          Osc.
         1         0.0098      0.1175      0.0000      0.1675
         2         0.1175     -0.0098      0.0000      0.1675
         3         0.0000      0.0000      0.1468      0.2252
 Ground to excited state transition magnetic dipole Moments (Au):
       state          X           Y           Z
         1        -0.6525      0.0546      0.0000
         2         0.0546      0.6525      0.0000
         3         0.0000      0.0000      0.0000
 Ground to excited state transition densities written to RWF  633

 Excitation energies and oscillator strengths:

 Excited State   1:   ?Spin  -E      1.5046 eV  824.04 nm  f=0.2988
     11A -> 14A        0.70608
     11A -> 17A        0.66651
     11A -> 23A       -0.20883
 This state for optimization and/or second-order correction.
 Total Energy, E(Cis) =  -218.013605359
 Copying the Cisingles density for this state as the 1-particle RhoCI density.

 Excited State   2:   ?Spin  -E      1.5046 eV  824.04 nm  f=0.2988
     11A -> 13A        0.70608
     11A -> 16A        0.66651
     11A -> 22A       -0.20883

 Excited State   3:   ?Spin  -A1     1.7348 eV  714.69 nm  f=0.2590
     11A -> 12A        0.79583
     11A -> 18A        0.57207
     11A -> 19A       -0.10003
     11A -> 24A        0.13997
 






From kotelyan@plmsc.psu.edu  Wed Sep 10 10:23:19 1997
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Date: Wed, 10 Sep 1997 10:08:01 -0400 (EDT)
From: Mike Kotelyanskii <kotelyan@planck.plmsc.psu.edu>
To: CHEMISTRY@www.ccl.net
Subject: Inorganic crystal structures
In-Reply-To: <199709092312.TAA15185@helix.nih.gov>
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Is anybody aware of the database, or other source of the crystal 
structures (lattice symmetry groups, lattice parameters, moduli??)
of the inorganic compounds like SiC, aluminium, zinc and other oxides,
particularly, III-V groups elements and compounds, 
Thank you
Michael

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Michael J. Kotelyanskii				Phone (814) 863 43 81
Polymer Science Program				FAX   (814) 865 29 17
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Engineering                                     kotelyan@plmsc.psu.edu
Pennsylvania State University
University Park, PA 16802, USA
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From berriz@chasma.harvard.edu  Wed Sep 10 11:23:16 1997
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From: berriz@chasma.harvard.edu (Gabriel Berriz)
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To: chemistry@www.ccl.net
Subject: [Q] for users of PSC's T3E





Dear netters,

I have an account on the Cray T3E at the Pittsburgh Supercomputer
Center, which I use remotely from my office in Cambridge, MA.  I would
like to communicate with other *remote* users (preferably not
affiliated with the PSC) about their experiences with this system.  I
am very concerned about the exceedingly slow performance of crucial
interactive X-window tools such as Cray's multiprocess debugger
TotalView.  I'm trying to determine whether the problems I'm having
are widespread or unique to my setup, and if the former, whether other
users have found acceptable workarounds.

Since this is somewhat off-topic, please e-mail me directly.

Thank you.

Gabriel Berriz
berriz@chasma.harvard.edu

From duca@tigger.cc.uic.edu  Wed Sep 10 13:23:20 1997
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From: Jose Santiago Duca <duca@tigger.cc.uic.edu>
To: CHEMISTRY@www.ccl.net
Subject: about review_3
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Hi, this short e-mail is to find out about the web address where to find
the review_3 software (or newer) because I lost it.
Thank you in advance,

Jose S. Duca, PhD

QSAR and Molecular Modeling Laboratory

Dept. of Medicinal Chemistry and Pharmacognosy
College of Pharmacy
University of Illinois at Chicago
833 South Wood St. (M/C 781)
Chicago, IL  60612-7231

Voice: (312)996-6004     Fax: (312)996-7107


From roberson@kemibm.kemi.aau.dk  Wed Sep 10 13:49:44 1997
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To: CHEMISTRY@www.ccl.net
Subject:  SGI Octane workstation



Wise Ones,

    We are looking into the purchase of a workstation for running gaussian,
with the intention of studying transition-metal catalysed organic reactions.
We have our eyes on the SGI Octane workstation with two R10000 chips, 128MB
RAM, and 4GB disk.

    I would appreciate e-mail from anyone who has experience with this machine,
regarding whether the basic configuration is adequate for the sort of 
calculations we wish to perform or whether upgrades will be advisable.

						MJR


From angel@fluor.quimica.uniovi.es  Wed Sep 10 15:23:20 1997
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	<angel@fluor.quimica.uniovi.es>
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Dear CCLers,

           I am interested in obtaining reasonable analytical  periodic
           electron densities  of  simple metals (Li,  Ca, etc)  in
order to apply
           Bader's formalism to pure metallic crystals. However, it
seems
           quite difficult  to find any solid state physics code that
uses some
           flavor of Plane Wave  expansion.  Could anyone inform me
about
           any (freeware,  shareware, etc) code  or package meeting my
needs?

--

         \|/
        |^.^|
----OOO--\_/--OOO------------------------------------------------------
                                      | Oh, The cheapness of mindless
    Angel Martin Pendas               | calculation in modern age
    Professor of Chemistry            |
    Dpto. Quimica Fisica y Analitica. | Roger Penrose,
    Univ. de Oviedo                   | The Emperor's new mind
    33006 Oviedo. SPAIN               |
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            angel@carbono.quimica.uniovi.es
     voice: (int) 34 8 5103037
       fax: (int) 34 8 5103125
       www: http://www.uniovi.es/~quimica.fisica/qcg/amp/amp.html
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From norge@karin.fmq.uh.edu.cu  Wed Sep 10 19:23:20 1997
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Date: Wed, 10 Sep 1997 16:10:22 -0400 (CDT)
From: Norge Cruz Hernández <norge@karin.fmq.uh.edu.cu>
To: chemistry@www.ccl.net
Subject: Help in Mathematics. 
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Hi,

I am trying to solve an optimization problem.
It is the core of my quantum chemistry research.

The problem is the following  :
 Min.  F(X1,X2,...Xn,Y1,Y2,....Yn) 
 
Constrained :
         X1*X1+Y1*Y1=X1
         X2*X2+Y2*Y2=X2
          ..............................
         Xn*Xn+Yn*Yn=Xn
       
and 
         2*(X1+X2+X3+     Xn) = Ne

I used  The gradient projection method. It was a good method when the 
number n was not very large, but when n is very large it is not 
possible.  

Would you give me any idea ? ? ?  

Your help will be very important for me.


Best regard 
Norge



From norge@karin.fmq.uh.edu.cu  Wed Sep 10 19:41:12 1997
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From: Norge Cruz Hernández <norge@karin.fmq.uh.edu.cu>
To: chemistry@www.ccl.net
Subject: CCl: Help in Mathematics.
Message-ID: <Pine.LNX.3.91.970910161232.8587B-100000@karin.fmq.uh.edu.cu>
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Hi,

I am trying to solve an optimization problem.
It is the core of my quantum chemistry research.

The problem is the following  :
 Min.  F(X1,X2,...Xn,Y1,Y2,....Yn) 
 
Constrained :
         X1*X1+Y1*Y1=X1
         X2*X2+Y2*Y2=X2
          ..............................
         Xn*Xn+Yn*Yn=Xn
       
and 
         2*(X1+X2+X3+     Xn) = Ne

I used  The gradient projection method. It was a good method when the 
number n was not very large, but when n is very large it is not 
possible.  

Would you give me any idea ? ? ?  

Your help will be very important for me.


Best regard 
Norge




