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REACTIVE ELECTRON/MOLECULE COLLISIONS: FROM MECHANISMS TO NEW STATE-TO-STATE CROSS SECTIONS AND RATE COEFFICIENTS

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REACTIVE ELECTRON/MOLECULE COLLISIONS: FROM MECHANISMS TO NEW STATE-TO-STATE CROSS SECTIONS AND RATE COEFFICIENTS J. Zs. Mezei

(a,b)1

, E. Djuissi

(b)

, A. Abdoulanziz

(b)

, F. Iacob

(c)

, N. Pop

(d)

, D. Talbi

(e)

, V. Laporta

(f)

,

M. Ayouz

(g)

, V. Kokoouline

(h)

and I. F. Schneider

(b)

(a) Institute for Nuclear Research, Hungarian Academy of Sciences, H-4001 Debrecen, Hungary

(b) LOMC, CNRS, Normandie Université, Le Havre, 76056 Le Havre, France

(c) West University of Timisoara, 300223 Timisoara, Romania

(d) Politehnica University of Timisoara, 300223 Timisoara, Romania

(e) LUPM, CNRS, Université de Montpellier, 34095 Montpellier, France

(f) P. Las.M.I.Lab. Nanotec, CNR, 70126 Bari, Italy

(g) LGPM, CNRS, CentralSupelec, Univ. Paris Saclay, 91190 Gif-sur-Yvette, France

(h) University of Central Florida, Orlando, 32816 Orlando, Florida, USA

Electron-impact dissociative recombination, ro-vibrational (de)excitation and dissociative excitation of molecular cations are at the heart of molecular reactivity in the cold ionised media [1], being major molecular ion destruction reactions, and producing often atomic species in metastable states, un-accessible through optical excitation.

These processes involve super-excited molecular states undergoing pre-dissociation and autoionization, having thus strong resonant character. We use methods based on Multichannel Quantum Defect Theory and R-Matrix Theory [2], capable to account for the strong mixing between ionization and dissociative channels, open - direct mechanism - and closed - indirect mechanism, via capture into prominent Rydberg resonances [3] correlating to the ground and excited ionic states, and for rotational effects. These features will be illustrated for several cations of high astrophysical and planetary relevance such as H2+ [3], CO+ [4], SH+ [5], CH+ [2,6], N2+ [7], ArH+[8], CH2NH2+[9].

Results for reactions similar to (1) but involving the neutral target CO2 [10] will be also displayed.

Comparisons with other existing theoretical and experimental results will be given.

References

[1] I. F. Schneider, O. Dulieu, and J. Robert (editors) 2015 Eur. Phys. J. Web of Conf. 84.

[2] J. Zs. Mezei et al, ACS Earth. Space.Chem. 3, 2376 (2019).

[3] M. D. Epee Epee et al, MNRAS 455, 276 (2016).

[4] Y. Moulane et al, A&A 615, A53 (2018).

[5] J. Zs. Mezei et al, J. Chem. Phys. 146, 204109 (2017).

[6] K. Chakrabarti et al, J. Phys. B. 51, 104002 (2018).

[7] D. A. Little et al, Phys. Rev. A 90, 052705 (2014).

[8] A. Abdoulanziz et al, MNRAS 479, 2415 (2018).

[9] C. H. Yuen et al, MNRAS 484, 659 (2019).

[10] V. Laporta et al, Phys. Rev. A 91, 012701 (2015).

1 mezei.zsolt@atomki.mta.hu

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