Abstract

We present state-selective electron capture cross sections in collision between Be4+ and ground state hydrogen atom. The n- and nl-selective electron capture cross sections are calculated by a three-body classical trajectory Monte Carlo method (CTMC) and by a classical simulation schema mimicking quantum features of the collision system. The quantum behavior is taken into account with the correction term in the Hamiltonian as was proposed by Kirschbaum and Wilets (Phys Rev A 21:834, 1980). Calculations are carried out in the projectile energy range of 1–1000 keV/amu. We found that our model for Be4+ + H(1s) system remarkably improves the obtained state-selective electron capture cross sections, especially at lower projectile energies. Our results are very close and are in good agreement with the previously obtained quantum–mechanical results. Moreover, our model with simplicity can time efficiently carry out simulations where maybe the quantum mechanical ones become complicated, therefore, our model should be an alternative way to calculate accurate cross sections and maybe can replace the quantum–mechanical methods.

Highlights

  • We present state-selective electron capture cross sections in collision between ­Be4+ and ground state hydrogen atom

  • The calculation of the principle quantum number, n, dependent cross sections has been studied by Jorge et al.[15] by solving the time-dependent Schrödinger equation with the GridTDSE package (GTDSE) numerically in the broad energy range between 1 keV/amu and 500 keV/amu

  • We treat the collision dynamics classically using a three-body classical trajectory Monte Carlo (CTMC) and a three-body quasi classical Monte Carlo (QCTMC) model when the Heisenberg correction term is added to the standard classical trajectory Monte Carlo method (CTMC) model via model p­ otential[16,17,18,19,20,21]

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Summary

Introduction

We present state-selective electron capture cross sections in collision between ­Be4+ and ground state hydrogen atom.

Results
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