CHEM01200604005 A. K. Pathak - Homi Bhabha National Institute
CHEM01200604005 A. K. Pathak - Homi Bhabha National Institute
CHEM01200604005 A. K. Pathak - Homi Bhabha National Institute
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potential energy surface for these clusters and finding a minimum on the surface. The key<br />
issue in this search procedure is to guess a good initial geometry of the cluster, which<br />
might converge during the calculation to a local or the global minimum. It is to be noted<br />
that the adopted procedure for geometry search cannot guarantee to locate the global<br />
minimum. Thus, Monte Carlo based simulated annealing procedures have also been<br />
applied with the effective fragment solvent molecules to find out the global minimum<br />
structure of different size molecular clusters. 36 In this method, molecular coordinates are<br />
displaced by a random amount and the energy of the system has been evaluated at the<br />
new structure. The new structure with lower energy is accepted while structures with<br />
higher energies have been accepted at a probability determined by the Boltzmann factor.<br />
Random structures are generated by carrying out Monte-Carlo steps at a temperature<br />
range of 2000 K to 100 K for more than 8000 steps. 36<br />
In molecular electronic structure methods the energy of a system is calculated<br />
using the self consistent field (SCF) method. For calculation of the energy system many<br />
methods are available. Among them the simplest ab initio method is Hartree-Fock (HF),<br />
which is an electron uncorrelated method.<br />
In all the SCF method the density matrix (P) is guessed initially and is defined for<br />
restricted HF case 37<br />
occupied<br />
P λσ<br />
2 χ λ iχ<br />
σ i<br />
i<br />
= ∑ (5)<br />
where the coefficient ( χ ) comes from the linear combination of the basis set ( ϕ<br />
i<br />
)<br />
N<br />
φ = ∑ χϕ<br />
(6)<br />
j ij i<br />
i=<br />
1<br />
11