From chemistry-request@ccl.net Mon Jul 12 23:15:41 2004
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From: <victor_anisimov-.at.-comcast.net>
To: <hinsen-.at.-cnrs-orleans.fr>, "Shobe, David" <dshobe-.at.-sud-chemieinc.com>
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Subject: CCL:time-dependent and time-independent QM
Date: Tue, 13 Jul 2004 00:25:47 -0400
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----- Original Message ----- 
From: <hinsen-.at.-cnrs-orleans.fr>
To: "Shobe, David" <dshobe-.at.-sud-chemieinc.com>
Cc: "CCL computational chemistry list (E-mail)" <chemistry-.at.-ccl.net>
Sent: Monday, July 12, 2004 4:52 PM
Subject: CCL:time-dependent and time-independent QM


> On 12.07.2004, at 22:14, Shobe, David wrote:
> 
> > Where does the part where measuring a property of the system "resets"  
> > the quantum state of the system come in?   That's always been  
> > mysterious:
> 
> That depends on who you ask, I think that discussion is still  
> open-ended. The "collapse of the wave function" is part of the original  
> Copenhagen interpretation of the meaning of the wave function. However,  
> there are other interpretations. As the term "interpretation" implies,  
> the choice of one does not change the maths - the equations and wave  
> functions remain the same.
> 
> The real problem in that discussion is that "measurement" needs to be  
> defined. In a pure quantum world, there are particles interacting, all  
> subject to the same laws, and the whole universe is governed by a  
> single huge wave function. No measurements, no problems. Various  
> definitions of measurements have been proposed, but none has yet been  
> found to be without problems. Some say that measuring implies human  
> consciousness - hence the paradox known as "Schrvdinger's cat". Others  
> say that measurement is an interaction with a classical object, but  
> that would imply that quantum mechanics needs to be defined in terms of  
> its own limiting case, classical mechanics.

Perhaps the term "measurement" is already satisfactorily defined in quantum 
mechanics. The "measurement" of a physical property, which is an operator |p|,
e.g. impulse, is a mean value <W|p|W> where W is wavefunction of the
system. Thus we know how to perform "measurement". The quantum problem, 
which is associated with the process  of "measurement" is related to the fact that 
those operators, which do not commute, like energy |E| and impulse |p| yield different 
results depending of their order. Thus, |E*p| operator is different from its |p*E| 
counterpart and being applied to wavefunction they would yield different results. This 
leads to the well-known statement that one can not measure energy and impulse at 
the same time. Commuting operators, like energy and dipole moment do not show 
such restriction.

Supposedly this has little to do with "interpretation" but this is rather a mathematical 
apparatus of quantum mechanics that can be either confirmed or rejected by
experiment. So far we know only confirmations.

With kind regards,
Victor

--
Victor Anisimov
School of Pharmacy
University of Maryland



From chemistry-request@ccl.net Tue Jul 13 09:44:55 2004
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Date: Tue, 13 Jul 2004 17:50:56 +0300 (IDT)
From: Pinchas Aped <aped_at_mail.biu.ac.il>
To: chemistry_at_ccl.net
Subject: CCL: using SCF=QC in G03 on Linux system
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Dear All:

      We have recently installed Gaussian 03 on an Intel-based system with
Linux (RedHat 9.0). Most job types ran successfully, but when we tried to
use SCF=QC the job aborted after a few seconds without any error message.
has anyone experienced such problems with Gaussian on Linux systems? (the
same job ran to completion on AIX and IRIX systems).

      Thanks in advance

      Pinchas Aped


------------------------------------------------------------------------
Dr. Pinchas Aped                      Tel.:   (+972-3) 531-7683
Department of Chemistry               FAX :   (+972-3) 535-1250
Bar-Ilan University                   E-Mail: aped_at_mail.biu.ac.il
52900 Ramat-Gan, ISRAEL               WWW:    http://www.biu.ac.il/~aped
------------------------------------------------------------------------


From chemistry-request@ccl.net Tue Jul 13 11:16:50 2004
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Date: Tue, 13 Jul 2004 12:19:41 -0400
From: Rick Venable <rvenable!at!pollux.cber.nih.gov>
To: Anil Korkut <ak2048!at!columbia.edu>
cc: chemistry!at!ccl.net
Subject: Re: CCL:normal modes problem/CHARMM
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There's a forum at www.charmm.org which adresses Minimization and Normal
Modes, etc.

The asterisks indicate a formatting problem, not a 'blank' normal mode,
but they should be near zero in any event.

I strongly suggest checking the output logs of your minimization and
normal mode calc for warning and error messages; there is a problem.

I'd use a lot less SD min, maybe just 100-200 steps to relieve bad
contacts.

Also, try a smaller and simpler test case.


On Mon, 12 Jul 2004, Anil Korkut wrote:
> I am doing an NMA calculation for a protein with 3000 atoms using
> charmm simulation package.
>
> I minimized my structure to a gradient of 1e-6 with 2000 steps of sttepest
> descent followed by about 8000 steps of ABNR.
>
> I know that the first six normal modes should have zero frequency.
>
> However, I got no frequency values for the first two normal modes!!!!
>
> The translational and rotational modes start at mode 3 and the vibrational
> modes start at mode 9 instead of 7.
>
> The frequency values are
> VIBRAN> PRINT NORM MODE 1 THRU 16 DIPO
>
> NORMAL MODES
>
> 1********** 2********** 3 -0.01 4 -0.01 5 0.00
> 6 0.00 7 0.00 8 0.01 9 1.51 10 1.76
> 11 2.40 12 3.03 13 3.40 14 3.76 15 4.05
> 16 4.29
>
>
> I have done the same calculation with a different force field (opls-ua)
> using TINKER and results were as expected (i.e. no blank modes, no
> negative
> eigenvalues)
>
> The nomal mode 7 from tinker has very similar freq. value to normal mode 9
> > from charmm.
>
> I also used BPTI as a sample protein and the same problem exists.
>
> Does anyone have any idea what is going wrong here?
>
> I can post my script, if anyone is interested.
>
> Thanks
>
> ______________________________________________________________
> Anil Korkut
> Dept of Biochemistry and Mol. Biophysics
> Columbia University,
> 630 West 168th St, BB204
> New York, NY 10032
> office ph (212) 305 1846
> ______________________________________________________________
>
>
> -= This is automatically added to each message by the mailing script =-
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>
>
>
>
>
>

=+=+=+=+=+=+=+=+=+=+=+=+=+=+=+=+=+=+=
Rick Venable           29/500
FDA/CBER/OVRR Biophysics Lab
1401 Rockville Pike    HFM-419
Rockville, MD  20852-1448  U.S.A.
(301) 496-1905   Rick_Venable!at!nih.gov
ALT email:  rvenable!at!speakeasy.org
-------------------------------------
"Don't blame me, I voted for Kang."
                         Homer
=+=+=+=+=+=+=+=+=+=+=+=+=+=+=+=+=+=+=

From chemistry-request@ccl.net Tue Jul 13 07:33:29 2004
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From: "Xavier ASSFELD" <Xavier.Assfeld|at|lctn.uhp-nancy.fr>
To: <victor_anisimov|at|comcast.net>, <hinsen|at|cnrs-orleans.fr>,
   "Shobe, David" <dshobe|at|sud-chemieinc.com>
Cc: "CCL computational chemistry list \(E-mail\)" <chemistry|at|ccl.net>
Subject: RE: time-dependent and time-independent QM
Date: Tue, 13 Jul 2004 14:36:42 +0200
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X> -----Message d'origine-----
X> De : Computational Chemistry List [mailto:chemistry-request|at|ccl.net]De
X> la part de victor_anisimov|at|comcast.net
X> Envoyi : mar. 13 juillet 2004 06:26
X> @ : hinsen|at|cnrs-orleans.fr; Shobe, David
X> Cc : CCL computational chemistry list (E-mail)
X> Objet : CCL:time-dependent and time-independent QM
X>
X> Perhaps the term "measurement" is already satisfactorily defined
X> in quantum
X> mechanics. The "measurement" of a physical property, which is an
X> operator |p|,
X> e.g. impulse, is a mean value <W|p|W> where W is wavefunction of the
X> system. Thus we know how to perform "measurement". The quantum problem,
X> which is associated with the process  of "measurement" is
X> related to the fact that
X> those operators, which do not commute, like energy |E| and
X> impulse |p| yield different
X> results depending of their order. Thus, |E*p| operator is
X> different from its |p*E|
X> counterpart and being applied to wavefunction they would yield
X> different results. This
X> leads to the well-known statement that one can not measure
X> energy and impulse at
X> the same time. Commuting operators, like energy and dipole
X> moment do not show
X> such restriction.
X>

Just my 2 eurocents,
I think that the problem of measuring something of a quantum system is
related to the superposition state. A quantum system can be in a
superposition of eigenstate, e.g. a hydrigen atom can be in state Y = c1*1s
+c2*2s. When you measure in which state the hydrogen atom is, you will find
c1*c1 times the energy of the 1s state and c2*c2 times the energy of the 2s
state. You'll never find c1*c1*E1+c2*c2*E2 value! When you measure the
energy the wavefunction is "reduced" to only one eigenstate.
Hope that I throw oil on fire...
Yours

X> Supposedly this has little to do with "interpretation" but this
X> is rather a mathematical
X> apparatus of quantum mechanics that can be either confirmed or
X> rejected by
X> experiment. So far we know only confirmations.
X>
X> With kind regards,
X> Victor
X>
X> --
X> Victor Anisimov
X> School of Pharmacy
X> University of Maryland
X>
X>
X>
X> -= This is automatically added to each message by the mailing script =-
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X> Subject: line
X> and send your message to:  CHEMISTRY|at|ccl.net
X>
X> Send your subscription/unsubscription requests to:
X> CHEMISTRY-REQUEST|at|ccl.net
X> HOME Page: http://www.ccl.net   | Jobs Page: http://www.ccl.net/jobs
X>
X> If your mail is bouncing from CCL.NET domain send it to the maintainer:
X> Jan Labanowski,  jlabanow|at|nd.edu (read about it on CCL Home Page)
X> -+-+-+-+-+-+-+-+-+-+-+-+-+-+-+-+-+-+-+-+-+-+-+-+-+-+-+-+-+-+-+-+-+-+-+-+
X>
X>
X>
X>
X>



                                      ...Xav

Pr. Xavier Assfeld                  Xavier.Assfeld|at|lctn.uhp-nancy.fr
Laboratoire de Chimie thiorique     (T) 33 3 83 68 43 82
Universiti Henri Poincari           (F) 33 3 83 68 43 71
F-54506 Nancy B.P. 239              http://www.lctn.uhp-nancy.fr




From chemistry-request@ccl.net Tue Jul 13 02:13:10 2004
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From: hinsen|at|cnrs-orleans.fr
Subject: Re: CCL:time-dependent and time-independent QM
Date: Tue, 13 Jul 2004 09:19:53 +0200
To: CCL computational chemistry list (E-mail) <chemistry|at|ccl.net>
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On 13.07.2004, at 06:25, <victor_anisimov|at|comcast.net> wrote:

> Perhaps the term "measurement" is already satisfactorily defined in  
> quantum
> mechanics. The "measurement" of a physical property, which is an  
> operator |p|,
> e.g. impulse, is a mean value <W|p|W> where W is wavefunction of the
> system. Thus we know how to perform "measurement". The quantum

Then what is the physical procedure to obtain the mean value?  
Measurement is a physical operation, not a mathematical one.

> Supposedly this has little to do with "interpretation" but this is  
> rather a mathematical
> apparatus of quantum mechanics that can be either confirmed or  
> rejected by experiment. So far we know only confirmations.

It is true that quantum mechanics is largely confirmed by experiment,  
but that doesn't resolve the question of the definition of measurement.  
The different interpretations that have been proposed for the wave  
function make no difference for the experiments that have been devised  
so far, otherwise the issue might have been settled by now.

I suspect that ultimately the problem is an artificial one, that  
"measurement" is an unnecessary idealization that doesn't fit the  
quantum world. Any experimental setup can be described by quantum  
mechanics, even though the maths may be too complicated to do the  
computations explicitly. An apparatus suitable for "measurement" is  
simply one whose states are sufficiently distinct to permit observation  
by human sensory organs.

------------------------------------------------------------------------ 
-------
Konrad Hinsen
Laboratoire Leon Brillouin, CEA Saclay,
91191 Gif-sur-Yvette Cedex, France
Tel.: +33-1 69 08 79 25
Fax: +33-1 69 08 82 61
E-Mail: hinsen|at|llb.saclay.cea.fr
------------------------------------------------------------------------ 
-------



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Date: Tue, 13 Jul 2004 13:35:28 +0200 (CEST)
From: Torsten Becker <torsten.becker_at_iwr.uni-heidelberg.de>
To: chemistry_at_ccl.net
Subject: Re: CCL:time-dependent and time-independent QM
In-Reply-To: <002201c46891$7bb1e820$549c8b45@test>
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On Tue, 13 Jul 2004 victor_anisimov_at_comcast.net wrote:
> 
> Perhaps the term "measurement" is already satisfactorily defined in quantum 
> mechanics. The "measurement" of a physical property, which is an operator |p|,
> e.g. impulse, is a mean value <W|p|W> where W is wavefunction of the
> system. Thus we know how to perform "measurement". 

What you describe here is not a measurement. 
Given a measurable quantity represented by an Operator P, the outcome of a 
measurement will be one of the Eigenvalues p_i of P, not the mean value  
<W|P|W>. 
If |W_i> is an Eigenvector of P with Eigenvalue p_i, then <W|W_i> gives 
you the probability that your measurement yields p_i. 
Only after plenty of single measurements you can access  the mean value.

The 'measurement problem' in the Copenhagen Interpretation, as Konrad 
Hinsen wrote already, means that the measuring apparatus is not included 
in the system describtion given by the wavefunction |W>. In the 
Copenhageninterpretation the measuring apparatus is described in the 
framework of classical physics and measuring a system leads to a collaps 
of its wavefunction. 
'Collapse of the wavefunction` means that after a measurement that 
yielded p_i, the system is no longer in the state |W> but it 'collapsed' 
into the state |W_i>.

> The quantum problem, 
> which is associated with the process  of "measurement" is related to the fact that 
> those operators, which do not commute, like energy |E| and impulse |p| yield different 
> results depending of their order. 

Energy and momentum usually do commute. They have to, otherwise energy and 
momentum would not both be conserved in physical processes. 
So the operator P usually commutes with the Hamiltonian H.

There are of course non-commuting operators like position and momentum and 
indeed that's the jist of QM. But it is not related to the measurement 
problem. 


************************************************************************
Torsten Becker                        Computational Molecular Biophysics   
                                      IWR, Universitaet Heidelberg 
+49-6221-54-8808 (office)             Im Neuenheimer Feld 368 
+49-0177-7273406 (mobile)             D-69120 Heidelberg; Germany

torsten.becker_at_iwr.uni-heidelberg.de ***********************************  



From chemistry-request@ccl.net Tue Jul 13 11:42:52 2004
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From: Ian Hovell <HOVELL:at:cetem.gov.br>
To: "'chemistry'" <chemistry:at:ccl.net>
Subject: CCL:Summary Choice of computer for G03
Date: Tue, 13 Jul 2004 13:48:17 -0300
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As promised here is a summary to the following question

>I'm looking for the ideal computer for running G03. I was wondering what
>people on the list, when buying a new computer dedicated to Gaussian03,
>would go fo? Would people go for cpu speed, cache memory, RAM or hard disk.
>Where would the emphasise be? And what OS would you opt for. I'm sure these
>questions have been asked for before so if any body can point me to a URL
>they know, okay.
>Thanks for your help and time.

The answers;

I don't believe you will get definite answers to your question. I've seen
people on this list using computers of all kinds, single or multi
processors, Linux, Windows, Mac, etc... running Gaussian. Maybe the most
important question is what kind of simulations do you want to do on this
computer?

Of course, I'd go for the best computer possible, ant that means best CPU,
with large cache,  maximum RAM and a large HD. Especially, if you plan on
doing ab-initio calculations on large molecules, you will need lots of HD
space, and maybe consider a 62 bit processor.

As for OS, I'd definetely go for Linux, unless you choose a multi-processor
computer for which Linux isn't available.

HTH,
          Gustavo Seabra.

Ian, I have grown fond of Mac's again, since OS X is the only operating
system where I can do both professional development in C and Python
alongside Word - all without an emulator and/or dual booting.  The prices
for dual processors are comparable to what Dell has, if not a little cheaper
(list prices, YMMV).
Whatever you get, there are a number of things to consider:
1)	People forget that there are things like memory bandwidth and
disk/IO bandwidth.  Thus, they purchase the fastest processor(s) they can,
and wonder why their jobs don't run as fast as they'd expected.  I'd plan
for 1 job per 1 or 2 processors for maximum efficiency.  If you have to use
integral files, I'd investigate fast disks, SCSI, etc.
2)	Compilers make a HUGE difference.  gcc/g77 are way slower than
machine-specific compilers (Intel/PC or IBM/Mac).  While it costs a little
$$, getting 20-50% faster run-time is a cheap upgrade.  Some compilers also
have difficulties with some parallel libraries, or don't offer them - check
with Gaussian if there's any good or bad purchases.
3)	The safe recommendation is that one should get as much memory and
disk as possible.  See (1) for kinds and/or speeds of disk.  Regarding
cache, I don't know how particular portions of Gaussian relate to cache
hits/misses - they should know this.  Of course, running more than a single
job on the box is quite a bit worse re: cache than differences with a single
job.  And I think people now feel that machines should NEVER page (some turn
off the option in Linux), so lots and lots of RAM is required.
4)	Do you want to be your own system manager?  Do you have access to
one who is competent?  If not, maybe Linux will be a bother - nothing's real
good out of the box as I understand things.  I run off-the-shell OS X to
success.
5)	Do you need any kind of compatibility with PC/Mac/Linux/...?  Does
the machine have to have a graphics head or is it merely a server - the
latter is WAY easier to configure and maintain.  I'm not sure how PC's
communicate with
Mac/Linux/Unix, but the latter three seem to talk to each other well.
Hope this helps...
Joe

I've used various versions of Gaussian on various machines at supercomputing
centers for many years (at least 18 years).  My current favorite machine is
SGI's itantuim/altix machine.  It is shared memory so gaussian speed-up is
nearly linear (at least up to 8 processors, as many as I have tried), and
the 64 bit system makes file size limitations no longer an issue.  I have
been able to optimizations/frequency calculations on molecules with nearly
150 atoms, including Re atoms, using good quality DFT methods, as well as
MP2 calculations that choked other machines I have used.
Steve Williams

I hope that helps
Ian Hovell 


From chemistry-request@ccl.net Tue Jul 13 06:04:01 2004
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Subject: CCL: your favorite threads?
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Hi,

I ran into an old CCL "a bit more on molecular computational chemistry",

http://www.ccl.net/cgi-bin/ccl/message.cgi?2002+11+11+002

Another one was, "CCL:orbitals"

http://server.ccl.net/cgi-bin/ccl/message.cgi?2003+05+28+022

They are interesting.


Wonder what are your favorite thread(s)? Has this SUMMARY been done before?

-- 

Regards,

Yao-Ying Chien
 
Department of Crop and Soil Sciences
Michigan State University
Plant and Soil Sciences Building, Rm A526
East Lansing, MI 48824-1325

Office: (517)355-0271x249
SGI lab: (517)355-0271x253
Fax:	(517)355-0270
email: chieny/at/msu.edu	


From chemistry-request@ccl.net Tue Jul 13 15:25:39 2004
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Date: Tue, 13 Jul 2004 13:31:33 -0700 (PDT)
From: "O. Hucke" <ohucke$at$u.washington.edu>
To: chemistry$at$ccl.net
Subject: SAR database software
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Dear CCLers,

we are looking for a (ideally free, of course) database software for the
storage and the work with SAR data. Ideally the program should be able to
o store 3D structures of inhibitors
o perform substructure searches
o provide a web interface for online access (?)

Any hints are highly appreciated.

Thanks,

Oliver

_________________________

Oliver Hucke, Dr.

University of Washington
Dept. of Biochemistry
Seattle, WA 98195
_________________________


From chemistry-request@ccl.net Tue Jul 13 21:43:26 2004
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Date: Wed, 14 Jul 2004 10:49:30 +0800 (CST)
From: =?gb2312?q?Jinsong=20Zhao?= <zh_jinsong_at_yahoo.com.cn>
Subject: CCL: Orient molecule in GRID
To: CCL <chemistry_at_ccl.net>
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Dear all,

I have a set of molecule, I hope to do molecular interaction field
(MIF) analysis using GRID21 (Molecular Discovery Ltd.). I hope to do a
CoMFA like analysis, i.e., performing PLS analysis on the MIF data,
thus molecular orientation or molecular alignment is very important in
such situation. 

However, I don't know how to control the molecular orientation in
GRID21 and give a reasonable box arround the molecule.

Any suggestions will be really appreciated. Thanks in advance.

Regards,

Jinsong

=====
(Mr.) Jinsong Zhao
Ph.D. Candidate
School of the Environment
Nanjing University
No.22 Hankou Road, Najing 210093
P.R. China
E-mail: zh_jinsong_at_yahoo.com.cn

_________________________________________________________
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