From jan.hrusak@jh-inst.cas.cz Thu Apr 30 05:11 EDT 1998
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From: Jan Hrusak <jan.hrusak@jh-inst.cas.cz>
To: "'CHEMISTRY-REQUEST@www.ccl.net'" <CHEMISTRY-REQUEST@www.ccl.net>,
        "'Jan Hrusak'" <hrusak@jh-inst.cas.cz>
Subject: RE: QCISD energy lower than QCISD(T) energy!
Date: Thu, 30 Apr 1998 11:12:58 +-200
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I would like to add also my contribution to the recent discussion on 
QCISD/QCISD(T). I have been using these methods for a quite long
time. They became very popular due to the implementation into all
(or almost all) of the QC programs. The wide use of the QCI methods 
is also due to the implementation and particular success of the G1/G2
methods. For many (gas phase) experimentalists the numbers produced by
using the GAUSSIAN G2 keyword are a kind of final answer if the experimental 
data are not listed in standard data compilations. I am not saying, that G2
does not produce "good" numbers in most of the cases. However, examples
documented (L. Radom) where even G2 energies are quite unreasonable. 
This could be atributed to the multireference character of the WF,
wrong orbitals (T1 not close to 0), and/or to a simple failure of the QCISD 
method. The QCI is in the limit (i.e. T1=O) equal to the 
coupled cluster method (CC). For T1~0 the CC method is more stable than 
QCI. However, one should always check the T1 and T2 amplitudes and the
T1 norm. Recently, we have investigated one of the cases where QCI gives
unreasonable results while CC is still OK. (JCP 106 (1997) 7185) These 
cases demonstrate themself in big T1 (T2) amlitudes (and positive energy 
contributions of the pertubative triples in QCI). The QCISD gives seemingly
correct results for the structure, energy, freqs etc. but the QCISD density 
(dipole moments!!) are qualitativelly wrong. QCISD(T) breaks down completely.
In most of the QC programs the QCISD ist only marginaly more expensive
than the corresponding CCSD and thus I do not see any reason for using
the QCI method. In addition, in cases where the WF is not a strict single
reference one the convergency of CCSD is superior to QCISD.

Jan Hrusak




From korkin@act.sps.mot.com  Fri May  1 18:28:12 1998
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From: Anatoli Korkin <korkin@act.sps.mot.com>
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Date: Fri, 1 May 1998 14:50:34 -0700 (MST)
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To: CHEMISTRY@www.ccl.net
Subject: Project based mailing list: molecular mideling of silicon nitrdide films deposition, structure and properties
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Dear Colleagues,
 
For one of our projects we are going to organize an e.mail based
"discussion club". You are invited to join us if you are interested
in the topic and feel able to contribute in discussions based
on your experience and research in this field. The project concerns gas
phase, surface and solid state chemistry (theoretical and experimental) 
of silicon nitride film preparation, namely chemical vapor deposition and
related phenomena. The detailed molecular mechanism is of interest, as well
as relations between "chemistry" and film properties at a molecular/atomic
level.
 
This "discussion forum" will start as my own personal e.mail group.
Depending on the response, it  may be kept in this form or converted
to a separate automatically running mailing list. Additional tools,
e.g. databases, web pages, electronic and "real life" workshops may
be organized based upon how much interest, information and funding are
available.

Although we do not require any particular application/subscription form,
you are welcome to send some information about yourself and your area
of research. All questions and comments are welcome. Most frequently
asked questions and answers will be posted to everyone who expresses
interest in  participating in the topic discussions. Feel free to forward
this message to your colleagues, who may be interested to participate.

You should understand that any information you submit will be freely
distributed to others who have expressed an interest in this email
based information exchange.  Therefore, no confidential information 
should be submitted.  By participating you agree that any information 
you submit will be considered in the public domain, even if marked as
confidential, and that this information may be distributed to other 
members of this mailing group.
 
Sincerely,
 
Anatoli Korkin

From kallies@serv.chem.uni-potsdam.de  Thu Apr 30 09:27:55 1998
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Date: Thu, 30 Apr 1998 14:45:25 +0200
From: Bernd Kallies <kallies@serv.chem.uni-potsdam.de>
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Subject: parm94 and glycam93 in AMBER
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We are currently dealing with molecular mechanics calculations on
proteins coupled with oligosaccharides. We decided to use an AMBER force
field together with GLYCAM. The original GLYCAM paper (Woods et al, JPC
1995) said that this parameter set (called glycam93 in the AMBER
program) was developed in agreement with the old AMBER force field
(Weiner et al, JACS 1984, called parm91), but it might also be used with
the new developed AMBER parameters (Cornell et al, JACS 1995, called
parm94) because of the similar philosophy of assignment of atomic
charges (both parm94 and glycam93 use RESP charges from HF/6-31G*,
whereas parm91 used HF/STO-3G).
Regarding to the coupling of glycam93 and parm94 we have several
questions:
1. Does anybody know if these parameter sets should be coupled in
principle?
2. If one can do so, which scaling factor of 1-4 nonbonding interactions
should be used (0.5 as for parm91 and as used in Woods' paper for
parameterization, or 0.83 as for parm94)?
3. The Woods paper refers to some parameters in the GLYCAM force field
which were adopted from the parm91 parameter set. Should these
parameters be used from parm91 also for the coupling with the parm94 set
or should they be replaced by the new parm94 parameters, which are a bit
different?

Thank you for your assistance.

Bernd Kallies

--
Dr. Bernd Kallies
University Potsdam
Institute for Physical and Theoretical Chemistry
Am Neuen Palais 10
14469 Potsdam
GERMANY
e-mail: kallies@serv.chem.uni-potsdam.de
WWW   : http://www.chem.uni-potsdam.de/~kallies/kallies.htm
Tel   : [+49] (0)331 / 977-1313
Fax   : [+49] (0)331 / 977-1315




