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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

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