26 June 2022 to 1 July 2022
University of Santiago de Compostela
Europe/Madrid timezone

Decomposition of the fusion cross section in breakup reactions

Not scheduled
20m
Facultad de Ciencias de la Comunicación (University of Santiago de Compostela)

Facultad de Ciencias de la Comunicación

University of Santiago de Compostela

Campus Norte, Av. de Castelao, s/n, 15782 Santiago de Compostela, Spain
Oral contribution WED2

Speaker

Hasan Maridi (Heavy Ion Laboratory, University of Warsaw)

Description

The nuclear fusion cross section has been a quantity of interest since the advent of nuclear physics [1]. Its dependence on the combination of projectile and target, as well as incident energy, has been studied in great detail. More recently, interest has turned to the effects on the cross section of the breakup of weakly bound projectiles, which brings the possibility of incomplete fusion, where only a part of the projectile fuses with the target [2-5].

Two recent papers have performed a fairly thorough phenomenological analysis of the various contributions to the complete and incomplete fusion cross sections [6,7]. Using the reaction formalism of Ichimura, Austern and Vincent [8,9] and excluding the effects of inelastic excitation, we confirm the basic characteristics of their analysis. When taking into account the breakup of a weakly bound projectile into two fragments, the reaction cross section can be decomposed into a breakup cross section, two incomplete fusion cross sections, in which one or the other fragment fuses with the target, and a complete fusion cross section. The complete fusion cross section, in turn, can be decomposed into a cross section for fusion of the complete projectile with the target, as well as two cross sections describing the ordered sequential fusion of the two fragments with the target. Here, we analyze the energy and target dependence of these cross sections for the simple case of deuteron-induced reactions [10,11]. In closing, we briefly discuss how the formalism could be extended to treat three-body projectile breakup reactions, in particular, the case two-neutron halo nuclei [12].

[1] N. Bohr, Nature 137, 344 (1936).
[2] L.F. Canto, P.R.S. Gomes, R. Donangelo, M.S. Hussein, Phys. Rep. 424 (2006) 1; Phys. Rep. 596 (2015) 1.
[3] J. J. Kolata, V. Guimarães, and E. F. Aguilera, Eur. Phys. J. A 52, 123 (2016).
[4] P. R. S. Gomes, D. R. Mendes Junior, L. F. Canto, J. Lubian, and P. N. de Faria, Few Body
Syst. 57, 205 (2016).
[5] Jin Lei, Antonio M. Moro, Phys. Rev. Lett. 122, 042503 (2019).
[6] J. Rangel, M. Cortes, J. Lubian, and L. F. Canto, Phys. Lett. B 803, 135337 (2020).
[7] M. R. Cortes, J. Rangel, J. L. Ferreira, J. Lubian, and L. F. Canto, Phys. Rev. C 102, 064628 (2020).
[8] M. Ichimura, N. Austern, C. M. Vincent, Phys. Rev. C 32, 431 (1985).
[9] N. Austern, Y. Iseri, M. Kamimura, M. Kawai, G. Rawitscher, M. Yahiro, Phys. Rep. 154, 125 (1987).
[10] Jin Lei, Antonio M. Moro, Phys. Rev. C 92, 044616 (2015); 061602(R) (2015).
[11] B. V. Carlson, R. Capote and M. Sin, Few Body Systems 57, 307 (2016).
[12] B. V. Carlson, T. Frederico, M.S. Hussein, Phys. Lett. B 767, 53 (2017).

Topic Theory

Authors

Brett V Carlson Prof. Tobias Frederico (Instituto Tecnológico de Aeronáutica) Prof. Luiz Felipe Canto (Universidade Federal do Rio de Janeiro)

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