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Date: Fri, 9 May 1997 09:47:38 +0100 (BST)
From: Michael Nolan <maiden@RedBrick.DCU.IE>
To: chemistry@www.ccl.net
Subject: Re: mn and cr complexes (Summary: part 1)
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Hi CCL!!

thanks again to all those who replied to my pathetic problems with the
aforementioned complexes.

I am posting the summary in two parts, because I got a lot of answers. The
first is this extremely helpful reply from Prof. Guest.

The answer to most of problems was so simple:
(i) increase the number of cycles allowed!
(ii) changing the LEVEL keyword in GAMESS-UK helped enormously.

I also found that starting with a short M-C bond length (1.75 A) helped
The replies also opened my eyes to how tough TM complexes can be. I knew
that there could be problems because of the d-orbitals, but now I know
better.
It seems also that a correlated method should be used. Our HF results are
giving a different ordering of the HOMO-1, HOMO, LUMO and LUMO+1 orbitals
to that from Hoffmann et al (JACS 1976, 98, 7546 i think) and Byers and
Hall's work (Organometallics 1987).

Anyway, thanks to everyone again.

Michael
Der Kobold hat gesprochen
******************************************************************************
Michael Nolan (nearly BSc.)             Dublin City University (quantum
chem.)
41 Woodview                             Chemistry + German Year 4
Lucan
Co. Dublin
Ireland / Republic of Ireland / ROI / Eire

Email: Maiden@redbrick.dcu.ie
******************************************************************************


  
Date: Wed, 30 Apr 1997 22:32:14 +0100
From: "M.F.Guest" <M.F.Guest@dl.ac.uk>
To: Maiden@RedBrick.DCU.IE
Cc: gamess_uk_support@dl.ac.uk, wab@dl.ac.uk
Subject: Re: mn complexes

Dear Michael,

> I am trying to run ab-initio calculations on Mn(CO)3 and Cr(CO)3, using
> GAMESS-UK.

First, let me say that I am sorry you are having so many problems
trying to get these SCF transition metal complexes sorted out. If you
email me the associated input data sets and key sections of the O/P
files, I will run these for you and help resolve the source of the
problems you are encountering. I've run well over 150 TM complexes
using the code, and am very confident that I can resolve the matters
that are causing grief.

First, a couple of general guidelines.  Convergence problems of the
type you have encountered ("excessive iterations", oscillating energies
etc) can arise for a number of different reasons, and with the
information to hand its difficult to provide a definitive answer to
what is happening, but the following may help:

1. oscillations in the energy can often be resolved by increasing the
value of the "level shifter" used in the calculation over and above the
defaults. Thus, assuming you are on the correct initial configuration
(see below for more on that), then presenting the data sequence

          level 5 20 2
          maxcyc 100

will often help. You need to drive the calculation into the regime
where the DIIS convergence scheme is called into play, from which point
hopefully progress will be a lot better.

2. Bear in mind that running with "RUNTYPE OPXYZ" will require a
stricter convergence of the SCF calculation (10**-7 rather than 10**-5
in the "tester"), and you may just be running out of cycles (the
default 50). Without seeing the O/P it is difficult to be more precise
on this, although if the energy is oscillating that is clearly not the
problem.

3. There is no guarantee that the initial SCF configuration is
"correct", particularly for TM complexes where their may be a multitude
of low lying excited states, and in cases of high symmetry (as in your
examples). In the absence of any better starting point, you should use
the default "guess" option (vectors atoms). If you have successfully
converged a related compound with similar geometry or basis, then you
should use these vectors as a source of input to start the SCF. Thus if
you have the Mn(CO)3 vectors on say the dumpfile mnco3.ed3, then use
these to start the Cr(CO)3 calculation, using the directive

    vectors getq ed4 1 1

where I'm assuming that mnco3.ed3 is assigned to the calculation
using the LFN ED4 (perhaps via the setenv environment setting

    setenv ed4 mnco3.ed3

and that the converged Mn(CO)3 vectors reside in section 1.  This will
definitely help.

4. Note that if you inadvertently "split" the degeneracy of the
starting SCF orbitals then you will not recover (you can check this by
looking at the final set of eigen values). The energy may well crash
below that expected when for example degenerate e orbitals are symmetry
broken, and you must try and avoid that by ensuring the starting mos
exhibit the correct degeneracies.

Looking at the specific points you raised:

> 1) RHF/3-21G (3-21G on all atoms) for Mn(CO)3 this is successful, for
> Cr(CO)3 I get excessive number of iterations and an oscillation of the
> energy.

Use the converged  Mn(CO)3 vectors as input to the Cr(CO)3 calculation
as noted above, using "level 3.0 25 2.0"

> 2) RHF, 6-21G on C and O, 3-21G on Mn.  for Mn(CO)3, this is successful

> 3) RHF with minimal basis ECP on all atoms for Mn(CO)3 and Cr(CO)3.
> This gives a ludicrously low energy (about -70a.u.), oscillations in the
> energy and excessive number of iterations
> I have inputted a z-matrix, cartesian coordinates from X-ray diffraction
> studies (using both OPTXYZ keyword and the cartesian coordinates to
> z-matrix conversion) and the idealised geometry above  and I get the same
> result with them all - excessive number of iterations etc..

Again, a no. of reasons why this could happen, with a splitting
in degeneracy of the input MOs a likely candidate. You have to damp
the oscillations with "level"

> 4) RHF as above, but ECP-double zeta (ECPDZ) on all atoms same result
> 5) RHF, min. basis ECP and ECPDZ on Mn, 3-21G and 6-31G on C and O
> see number 4.
> I assume the fact that Mn(CO)3 is positively charged has nothing to do
> with it (it is a closed shell).
> I know that 3-21G and 6-31G are not good for transition metals, yet I got
> reasonable results using these (MOs and charge distribution).
> Does anyone have any ideas for how I can use ECPs (we are limited to
> about 1.2GB) or anything else to get these calculations to run (we do
> not yet have DFT).  

As I said at the outset, I've run a lot of TM ECP calculations without
experiencing the sort of problems you have encountered.  You could try
just siting the ECP on the TM to start with; are these calculations
using the Hay and Wadt ECP's, or those due to Stevens et al. I've found
the latter a lot better, and would suggest you try these.

> As an aside, I keep getting an error message when
> converting from cartesian coordinates to z-matrix. Has anyone else had
> this?

I seem to remember seeing an example like this posted to the GAMESS-UK
support list. If you have not received any feedback let me be the first
to apologise; Allan Beveridge, who was appointed to deal with this type
of query left his position a month or so ago, and we are a bit thin on
the ground in trying to deal with enquiries, installations etc. Again,
if you send me a data set where this problem manifests itself, I will
try and sort it out.

> sorry for bothering you and thank you in advance

Hopefully we can get your problems resolved asap. Please send me what
you consider to be relevant information (key data sets etc), and we'll
progress matters very rapidly. I trust that when all these problems are
resolved, that you will broadcast the successful outcome to the CCL.

Best regards

Martyn

******************************************************************
* Martyn F. Guest                                                *
* Computing for Science               email:  m.f.guest@dl.ac.uk *
* c/o CCLRC Daresbury Laboratory      FAX  :  +44 (0)1925 603634 *
* Warrington                          voice:  +44 (0)1925 603247 * 
* Cheshire WA4 4AD                                               *
* England, UK                                                    *
******************************************************************


From slo1@bnfl.co.uk  Fri May  9 07:42:10 1997
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Dear all,

this message is for members of the Royal Society of Chemistry in the UK.

Recently the Industrial Division of the Royal Society of Chemistry has
undergone some reorganisation moving from being organised at a regional
level to organisation based on subject groups. Several groups such as
specialty chemicals and pharmaceuticals are already in existence to
represent members interests in those industrial sectors.

A group has now been formed to bring together researchers and practitioners
in atomistic modelling techniques mostly from an industrial perspective but
also welcoming interested academic members. The group is called Molecular
Modelling Group and is located within the RSC's industrial division.

There will be an inauguration meeting at the RSC's lecture theatre in
Burlington Place (off Saville Row) London on Monday 16 June. Speakers will
represent a number of industrial companies including ICI, Courtaulds,
Unilever and BASF. This will be a one day meeting, with free buffet lunch.

Any enquiries about the meeting or the subject group please contact me at
one of the addresses below.

RSCconf@bnfl.co.uk
slo1@bnfl.co.uk



*********************************************
The opinions expressed above are those of 
Scott Owens...... So don't complain to BNFL if
you don't like them, because they probably 
don't like them either.
**********************************************

Dr. Scott Owens,
Company Research Laboratory,
BNFL,
B516, Springfields works,
Salwick,
Preston,
PR4 0XJ,
UK.

Phone:   +44 (0)1772 763914
Fax:     +44 (0)1772 762470
e-mail slo1@bnfl.co.uk

*********************************************

From pis_diez@nahuel.biol.unlp.edu.ar  Fri May  9 10:42:00 1997
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To: chemistry@www.ccl.net
From: pis_diez@nahuel.biol.unlp.edu.ar (Reinaldo Pis Diez)
Subject: G94, dft, and vshift 


        Dear netters,

                I've just read the mail sent by Michael Nolan and the answer
he received from  Martyn Guest concerning convergence problems in TM systems. 
                When one uses dft methods in TM systems the oscillating
energy problem is very often found. It is solved by using vshift in G94
calculations for example. But the final electronic configuration doesn't
correspond to the true ground state because some empty orbitals have lower
energy than some occupied ones. This can be solved by rerunning the
calculation using guess=read and eliminating vshift. Now, what does it
happen in a geometry optimisation where vshift must be on to achieve
convergence, but the orbitals don't correspond to the ground state? Can I
trust the optimised geometry and then rerun a single point calculation
without vshift to get the correct ground state?
                I'd appreciate any comments and will summarize to the net.
                Regards,

                                                                        Reinaldo
            


From chan@uni-muenster.de  Fri May  9 10:59:11 1997
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Date: Fri, 9 May 1997 15:42:13 +0200 (MES)
From: "Jerry C.C. Chan" <chan@uni-muenster.de>
To: chemistry@www.ccl.net
Subject: Chemical Softness by DFT 2
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Hi Netters,

	Last week I posted a question concerning the determination of
chemical hardness (or softness) of the metal centre of a TM complexes. 
Maybe the way I asked the question was not specific enough, I just
received two mails asking for the summary.  So I try to write down my
thinking explicitly and hope that someone in the net, who could not
tolerate the naiveness or even mistakes of my post, would kindly comment
on it.  I will summarize. 
 
I want to determine the chemical hardness of the metal centre of a charged
TM complexes.  The method that comes to my mind is to do a HF calculation 
and get the MO spectrum.  Based on the Koopmans' theorem the hardness of 
the complexes would be (E_LUMO - E_HOMO)/2.

Even my thinking is correct, HF calculation seems to be unreliable for TM 
complexes and correlated methods are usually very expensive.  Therefore 
last time I enquired the possibility of using DFT methods as an 
alternative although Koopman's theorem does not hold for KS orbitals.

By the way, I have heard that Fukui function is somehow related to the
chemical hardness but I don't have the recipe.  

Many thanks,
Jerry


******************************************************************
* Universitaet Muenster 		phone: 0049-251-83-29156 *
* Institut fuer Physikalische Chemie	fax:   0049-251-83-29159 *
* Schlossplatz 4-7						 *
* D-48149 Muenster						 *
* Germany							 *
******************************************************************



From Y0H8797@ACS.TAMU.EDU  Fri May  9 12:42:01 1997
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Date: Fri, 9 May 1997 11:08:10 -0500 (CDT)
From: YONG HUANG <Y0H8797@ACS.TAMU.EDU>
To: CHEMISTRY@www.ccl.net
Message-Id: <970509110810.20497cf1@ACS.TAMU.EDU>
Subject: Question to think about during a break


Here's a simple question. Is a NaCl molecule (yes, molecule, maybe in gas phase 
or in a computational chemist's space) a radical? How's the spin density
distribution look like if it is? This has nothing to do with my research. Just 
a question.

Yong

From cmartin@curie.syr.edu  Fri May  9 15:42:07 1997
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From: Charles Martin <cmartin@curie.syr.edu>
To: YONG HUANG <Y0H8797@ACS.TAMU.EDU>
Cc: CHEMISTRY@www.ccl.net
Subject: CCL:Question to think about during a break
In-Reply-To: <970509110810.20497cf1@ACS.TAMU.EDU>
References: <970509110810.20497cf1@ACS.TAMU.EDU>



 > Here's a simple question. Is a NaCl molecule (yes, molecule, maybe in gas phase 
 > or in a computational chemist's space) a radical? How's the spin density
 > distribution look like if it is? This has nothing to do with my research. Just 
 > a question.
 > 

	Similar question has been addressed by Steve Berry at the 
University of Chicago a long time ago (at least on some Halide
molecules).  The ground state changes character from covalent to 
ionic as the bond is stretched (i.e the typical problem addressed in
Landau-Zener hopping).    This is a very difficult problem 
with traditional ab initio methods because most ab initio methods 
can not treat curve crossings like this properly.  

	Chuck Martin

-- 
========================================================
 ||     Charles H. Martin                            ||
 ||     2-004 Center for Science and Technology      ||
 ||     W. M. Keck Center for Molecular Electronics  ||
 ||     Department of Chemistry                      ||
 ||     Syracuse University                          ||
 ||     Syracuse, NY  13244                          ||
--------------------------------------------------------
 ||     cmartin@cat.syr.edu                          ||
 ||     cmartin@rainbow.uchicago.edu                 ||
 ||     CELL   (315) 415-2093                        ||
 ||     OFFICE (315) 443-3754                        ||
 ||     LAB    (315) 443-5928                        ||
 ||     FAX    (315) 443-4070                        ||
========================================================

From Y0H8797@ACS.TAMU.EDU  Fri May  9 22:42:07 1997
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Date: Fri, 9 May 1997 20:46:10 -0500 (CDT)
From: YONG HUANG <Y0H8797@ACS.TAMU.EDU>
To: CHEMISTRY@www.ccl.net
Message-Id: <970509204610.204a086b@ACS.TAMU.EDU>
Subject: NaCl a radical?


I guess I didn't make it clear why this is a legitimate question. The reason I 
ask wheather NaCl is a radical is because a Na atom is closed shell, so Na+ is 
open shell. Na+Cl- is open shell. If you think NaCl is a Na atom plus a Cl atom
without electron transfer, then a Cl atom is open shell so NaCl is still open
shell.

Yong

