CCL:Summary of the question: Does optimized structure depend on the input?



 Dear all CCLers:
 Last Friday, I posted the question of whether the optimized structure
 depends on the input. I recieved a number of reponses from you guys.
 Thanks are due to all of you who promptly responsed my qusetion.
 Following are the answers:
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 From TANG # - at - # kitten.chem.uh.eduMon Apr 10 09:51:49 1995
 There is no optimization method to my knowledge that can GUARRANTEE to
 reach a global minimum.  Searching a global minimum becomes more
 difficult with increase of the number of variables.  For small molecules,
 chemical (or any) intuition is at times the only guide for searching what
 is desired.  For instance, when dealing with TiCl_6 complex, it's good
 to try Oh symmetric geometry first.  The "best" way other than the
 Good luck.
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 From: David Close <R29CLOSE # - at - # ETSU.EAST-TENN-ST.EDU>
   Part of what you say is true.  But part of the answer depends on the
 types of problems your are dealing with.  A good example of a local
 minimum would be trying to do a calculation on an isolated molecule.
 As torsion angles vary there are going to be geometries encountered
 where strong intra-molecular hydrogen bonds form.  Often times the
 calculation stops at this local minima.  However in a more realistic
 situation, the atoms forming the intra-molecular bond are most likely
 tied up with H-bonds to neighboring molecules.  But few of us can
 afford the computer time to add very many neighboring molecules.  One
 trick here is to use small neighboring molecules like waters of hydra-
 tion.  But there are many other things that one can do.  First of all,
 what systems are you studying, and what are you trying to learn?
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 From lim # - at - # rani.chem.yale.eduMon Apr 10 09:52:30 1995
 Most geometry optimization algorithms find a nearby local minimum,
 as opposed to a global minimum. In general, it is not an easy task
 to find out the global minimum of a molecule, especially when the
 molecule becomes larger. But there are mothods for locating global
 minima. The simulated annealing method is one example.
 However, in general, we don't know how many conformers there will
 be in a given molecule. So we try to find out as many (low-energy)
 conformers as possible in a conformational space.
 This is called 'conformational searching'.
 There are two major categories in the conformational searching:
 1) deterministic method
 2) stochastic method
 Method 1) is used in small to medium systems and method 2) in
 medium to large systems.
 You can get more information from A. R. Leach "A Survey of Methods for
 Searching the Conformational Space of Small and Medium-Sized Molecules"
 in Reviews in Computational Chemistry, Ed. K. B. Lipkowitz and D. B. Boyd,
 Vol. 2, VCH, 1991.
 -Dongchul Lim
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 From sbl # - at - # linus.herl.epa.govMon Apr 10 09:52:42 1995
 To  the best of my knowledge there is no direct way to find a global
 minima apart from a reasonably exhaustive search for all degrees of
 freedom. The approaches may include systematic conformational searches ro
 random sampling of conformational space using a molecular mechanics
 force  field level  of theory followed by a more  focused search using
 semi-empirical methods (for poorly  parameterized chemical species) and
 ab initio calculations at selected local minima to  verify the global
 minima at  a  given level of theory.
   You should talk  with Alex Tropsha  with  the Pharmacy School  Modelling
 Laboratory,   tropsha # - at - # gibbs.oit.unc.edu.
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 From ccl # - at - # cric.chemres.huMon Apr 10 09:52:54 1995
 As far as I know, there are numerous tricks, methods and practical recipes,
 but neither has strict guaranties that you will find the global minimum and
 not only a local one.
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 From montero # - at - # coch01.chm.tu-dresden.deMon Apr 10 09:53:27 1995
 G92, as all other geometry optimizing theoretical procedures, looks
 for minimal energy in a function of the nuclear coordinates. This func-
 tion is the electronic hamiltonian of the molecule. If you start from
 a geometry very near or very far from the absolute minimum, the result
 could be a partial minimum. Gradients are calculated analiticaly, and
 very accurate input data can give a first gradient displacement going
 farther than the right amount. In such a case, a van der Waals minimum
 could be attained (in a predisociative state, for example) in place
 of the equilibrium geometry. A too distorted input can conduct to
 unpredicatable results.
 It is a matter of experience and doing it many times. If not, theore-
 tical chemistry research is meaningless, because programs and computers
 are doing all things.
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 From elewars # - at - # alchemy.chem.utoronto.caMon Apr 10 09:53:42 1995
 Shubin Liu (shubin # - at - # email.unc.edu) asked how one can be sure he has
 found the
 global, rather than merely a local, minimum.  I think there is no short answer
 to this question.  If you are looking at something like water or methane, where
 everyone knows in a general way what the answer looks like, there is no
 ambiguity (what's the n-fold analog of an ambiguity?), and you might even
 dispense with the frequency job which is usually considered prudent to
 characterize a stationary state.  But note that even very simple molecules can
 have PES's with >1 minimum.
     If you are working with proteins I suspect that at the current state of
 the art you may as well forget about nailing down the global minimum.  Somewhere
 between water and a peptide you can worry about finding the global min. If, as
 is usually the case, the various possible minima you are concerned about arise
 from conformational possibilities, the systematic way to look for the global
 one is with a conformational search program as implemented in several commercial
 packages, e.g. Spartan.  If you have no hangups about gambling, there is at
 least
 one stochastic search program, PCGlobal, from Serena Software, which randomly
 generates a slew of input structures, hopefully including some you may not have
 thought of.  If your molecule is not too big you could do the job by hand,
 using input structures corresponding to all reasonable-looking possibilities
 for minima; your computational chemistry program should slide each one into
 the nearest minimum for the level you're using; if size doesn't make it
 impractical then do a freq job to see if the lowest-E stationary point is
 really a min.
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 From FOX # - at - # cmchem.chem.cmu.eduMon Apr 10 09:53:50 1995
   There are a number of possibilities raised by your question about how
 the Gaussian input can give rise to a local minimum,
   1) You could have symmetry constrained the input and the true minimum
      does not have the initial symmetry
   2) You could have started near a local minimum and the global minimum
      is separated by a barrier.
   3) You supplied a Z-matrix which does not span the full conformational
      space, either by restricting some internal coordinates, i.e. having
      too few coordinates, or by supplying a set with a redundancy so that
      it effectively has too few variables.
   Only the third would get close to being an input error.  The first two
 qualify as constrained solutions and local solutions respectively.  Check
 to see that your input spans the full conformational space with the
 keyword FOPT in place of OPT. It does not change the algorithm, simply
 adds a check that the coordinate supplied are linearly independent and
 sufficient in number to span the space.
   If you have symmetry constraing
 then the frequency result will guide you in reducing the symmetry and
 displacing toward the true minimum.  If you simply have located a local
 minimum try SCAN'ing the surface, possibly with a lower cost method, to
 locate other potential minima.
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 From GOVENDEM # - at - # che.und.ac.zaMon Apr 10 09:54:01 1995
 To obtain a global minimum, the entire PES
 has to be scanned, and not a region..this is
 however difficult in some cases where there
 is little experimental support.
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 From bouyer # - at - # ext.jussieu.frMon Apr 10 09:54:12 1995
 About local and global minimum, there is a simple answer:
 we cannot be sure of the minimum is local or global. All optimizer converge
 to an local minimum.
 To be sure of a global one, try others geometries (a little distorted) and
 calculate the energy.
 Within gaussian, there is a keyword (I don't remember, perhaps SCAN, see
 the documentation) that scan the potential energy surface. So gaussian can
 do that for you.
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 From noy # - at - # tci002.uibk.ac.atMon Apr 10 09:54:19 1995
 	Gaussian 92 will locate to the next (closet) minima using
 various methods, steepest descent, conjugated gradient and so on.
 Therefore, you are right that the optimized geometrical structure
 definitely depends on the initial input.
 	To my limit knowledge, there is no ultimate method to locate
 the global minimum, especially when the potential hypersurface
 is rather complicated. The most promising method in the modern
 days is "simulated annealing" [1] with the help of statistical
 mechanics,
 molecular dynamics and Monte Carlo simulations to find the global
 minimum. The idea is to search all the energetically possible
 areas as much as possible by increasing temperature so that
 molecular complexe can wander over the energy barrier (Gaussian
 can't do that since it always goes downhill) and then gradually
 decrease the temperature to allow the molecular complex to relax
 to the lowest minimum. Statistical mechanics tools are used to
 search the possible potential hypersurface. Somebody believes
 that this is the ONLY gauranteed method to find the global minimum.[2,3]
 The method is applied in connection with DFT and HF theory for mimization
 of geometry and wave-function paremeters on the fly. This approach
 is so-called Car-Parinello molecular dynamics [4] (see review in
 [5]) which successfully works with solid-state but now extends
 to organic chemistry [6].
 Reference
 =========
 1. S. Kirkpatrick, C. D. Gelatt Jr. and M. P. Vecchi, Science 220: 4598 (1983)
 2. P. J. M. van Laarhoven and E. H. L. Aarts, Simulated Annealing:
    Theory and Applications (Reidel, Dordrecht, 1987).
 3. B. Hartke and E. A. Carter, J. Chem. Phys. 97: 6569 (1992).
 4. R. Car and M. Parinello, Phys. Rev. Letters 55: 2473 (1985).
 5. D. K. Remler and P. A. Madden, Mol. Phys. 70: 921 (1990).
 6. U. C. Singh and P. A. Kollman, J. Comput. Chem. 7: 718 (1986).
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 Best regards,
 Shubin
 .............................................................................
 Shubin Liu
 Department of Chemistry			    Email: shubin # - at - # email.unc.edu
 University of North Carolina		           sliu # - at - # mulliken.chem.unc.edu
 Chapel Hill, NC 27599-3290		    Tel  : (919) 962-0150(O)
 USA                                                (919) 914-6923(H)
 .............................................................................