Heavy Ion Radiolysis of the Chiral Terpene α-pinene

Author:

de Barros A L F12ORCID,Ricca A34,Bychkova A2,da Costa C A P2,Costa J W1,Boduch P2,Rothard H2,da Silveira E F5ORCID,Domaracka A2

Affiliation:

1. Departamento de Física, Centro Federal de Educação Tecnológica Celso Suckow da Fonseca , Av. Maracanã 229, 20271-110 Rio de Janeiro, RJ , Brazil

2. Centre de Recherche sur les Ions, les Matériaux et la Photonique Normandie Univ, ENSICAEN, UNICAEN, CEA, CNRS, CIMAP , F-14000 Caen , France

3. Carl Sagan Center, SETI Institute , 339 Bernardo Ave., Suite 200, Mountain View, CA 94043 , USA

4. NASA Ames Research Center , Mail Stop 245-6, Moffett Field, CA 94035-1000 , USA

5. Departamento de Física, Pontifícia Universidade Católica do Rio de Janeiro , Rua Marquês de São Vicente 225, 22451-900, Rio de Janeiro, RJ , Brazil

Abstract

ABSTRACT Radiolysis of α-pinene by 61.3 MeV 84Kr15 + ions was analysed with the scope to simulate the effects of heavy ion cosmic ray bombardment on chiral molecules in the interstellar medium. The α-pinene ice samples were irradiated at 10 K and their chemical evolution was monitored by mid-infrared Fourier transform (FTIR) spectroscopy to characterize the reaction products and to determine the extent of racemization. The integrated band strengths have been obtained for all the neutral α-pinene vibrational bands using the experimental band integrated absorbances and the theoretical absolute intensities calculated along the column densities. In the current heavy ion bombardment experiments, small molecules were formed and the precursor, α-pinene, was destroyed instead of being racemized. Twelve hydrocarbons were produced (final fluence of 2.0 × 1012 ions cm−2): methane (CH4), acetylene (C2H2), ethylene (C2H4), propylene (C3H6), propane (C3H8), n-butane (C4H10), butene (C4H8), propyne (C3H4), benzene (C6H6), ethane (C2H6), vinylacetylene (C4H4), and 2-methyl-1,3-butadiene or isoprene (C5H8). The highest formation cross-section (∼ 40 × 10−15 cm2) was observed for the C3H4 and the lowest was for C3H8 (∼ 3 × 10−15 cm2). The radiochemical yields for these molecules follow the same trends as those of their cross-sections. The atom budget calculation confirms that all the expected products have been generated during the radiolysis and supports the conclusion that the proposed A values are accurate. The α-pinene sputtering yield for this ion beam was found to be Y0  = 1.84 × 106 molecules per impact.

Funder

CAPES

CNPq

FAPERJ

Publisher

Oxford University Press (OUP)

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