Abstract

Pseudopotential calculations of the ground state energies of the Lanthanum neutral atom, first and second corresponding cations by means of the variational Monte Carlo (VMC) and the diffusion Monte Carlo (DMC) methods are performed. The first and the second ionization potentials have been calculated for Lanthanum. The obtained results are satisfactory and comparable with the available experimental data. Studying the DMC energy of the La atom at different time steps, gave us a time step error of the order 0.0019 Hartree for the smallest time step, τ = 0.0001 Hartree-1, and -0.0104 Hartree for the largest time step, τ = 0.01 Hartree-1. This paper demonstrates the ability of extending the QMC method for lanthanides and obtaining highly accurate results.

Highlights

  • Quantum Monte Carlo (QMC) is a powerful technique by which one can perform computational electronic structure calculations with high accuracy

  • One of the advantages of the QMC technique is that its computational efforts scales with N3 where N is the number of electrons in the system

  • Quantum Monte Carlo methods have been extensively described in the literatures [9,10,11], so we give here a brief description of the two methods, the variational and diffusion Monte Carlo methods

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Summary

Introduction

Quantum Monte Carlo (QMC) is a powerful technique by which one can perform computational electronic structure calculations with high accuracy. One of the advantages of the QMC technique is that its computational efforts scales with N3 where N is the number of electrons in the system. Accurate calculations for extremely light atoms using QMC methods are performed by a large number of researchers [1,2,3,4]. By means of VMC and DMC methods, we have done calculations for the ground state energies of La atom and its charged cations with the hope “achieving high accuracy”. To allow the QMC calculations of this heavy atom, pseudopotential valence-only calculations have been performed, since the presence of the inert core electrons introduces a large fluctuation in the energies and this reduces the computational efficiency. Atomic units are used throughout this work unless otherwise indicated

Computational Methods
H T R T R
Results and Discussion

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