Abstract

The discovery of anions in the interstellar medium has shown that they are very reactive species. This gave them great importance in the modeling of the chemical and astrophysical evolution of the interstellar medium. The detection of the first anion C6H− followed by the other anions C4H−, C8H− and CN− in the interstellar medium has encouraged research on other detectable anions. The C2H− anion was observed for the first time in the circumstellar envelope of IRC+10216 and in TMC-1. In these cold and low-density regions, precise modeling of the chemical and physical conditions of the observed emission lines requires knowledge of the radiative and collisional excitation rates. We present here the first new two-dimensional Potential Energy Surface (PES) for C2H–H2 interaction. Rotational excitation of the anion by collision with para-H2(jH2 = 0) is investigated. The PES is obtained in the super-molecular approach based on a single and double excitation coupled cluster method with perturbative contributions from triple excitations (CCSD(T)). In all our calculations, all atoms were described using the augmented correlation-consistent triple zeta (aug-cc-pVTZ) basis sets and bond f unctions. Fully-quantum close-coupling calculations of inelastic integral cross sections are done on a grid of collision energies large enough to ensure converged state-to-state rate coefficients for the 16 first rotational levels of C2H− and for temperatures ranging from 5 to 120 K. For this collisional system, rate coefficients exhibit a strong propensity in favor of even Δj transitions.

Highlights

  • In the last two decades, anions have been intensively studied

  • We report in this work a rst collisional study of C2HÀ with para-H2(jH2 1⁄4 0) at low temperatures trying to understand the particular behavior of negatively charged species during collisions and how they compare with neutral forms[27,47] and the C2HÀ anion in collision with He.[48]

  • The calculations are based on a new, highly correlated 2D Potential Energy Surface (PES) calculated at the RCCSD(T) level using large AVTZ basis sets and a bend functions

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Summary

Introduction

In the last two decades, anions have been intensively studied. These studies were framed by observations in the laboratory[1,2,3] and some astrophysical observations.[2,4,5,6] Among these species, mention is made of carbon chain anions C2nHÀ.[6]. Several observations in the laboratories have justi ed the detection of the C2HÀ anion. Cernicharo et al.[15,25] detected the 1–0 transition of the C2HÀ anion and calculated the abundance ratio C2H/C2HÀ 1⁄4 12.5. We report in this work a rst collisional study of C2HÀ with para-H2(jH2 1⁄4 0) at low temperatures trying to understand the particular behavior of negatively charged species during collisions and how they compare with neutral forms[27,47] and the C2HÀ anion in collision with He.[48] we will present details of the ab initio calculations of the C2H–para-H2 potential Energy Surface (PES).In Section 3, some theoretical.

Potential Energy Surface
Dynamical calculation
Integral cross sections
Rate coefficients
Comparison with C2H–He collisions
Summary and conclusion
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