Events in our system are self-managed.  Group and event managers are encouraged to review privacy and security settings, and adjust them if needed.  If you need assistance please contact Indico Support - contact Help at bottom of page. https://learn.getindico.io/categories/managing/

15–18 Feb 2024
Mt. Bromont
Canada/Eastern timezone

Measurement of 59Cu(p,alpha)56Ni Reaction Rate to Constrain the Flow of nu p-Process

15 Feb 2024, 20:15
15m
Salon AB (Hotel Chateau Bromont)

Salon AB

Hotel Chateau Bromont

Contributed Oral Nuclear Physics Evening 1 - Feb. 15, 2024

Speaker

Mr Nikhil Bhati (Saint Mary's University)

Description

In the universe, most matter is mainly composed of light elements like hydrogen and helium, which were synthesised shortly after the Big Bang. Elements beyond iron are produced through neutron capture via the r-process or the s-process. However, these processes can’t explain the existence of several neutron-deficient elements, called p-nuclei, especially $^{92,94}$Mo and $^{96,98}$Ru. The $ \nu$p-process which happens during the Core-Collapse SuperNovae (CCSNe) explosion and the rp-process in type-I X-ray bursts (XRBs) have been suggested as potential sites to produce these nuclei. In both processes, the ability to synthesise heavy elements depends on the competition between $^{59}$Cu(p,$ \gamma $)$^{60}$Zn and $^{59}$Cu(p,$ \alpha $)$^{56}$Ni reactions, where the latter hinders the flow to the higher mass region, this is the Ni-Cu cycle. The upper-temperature limit for effective $\nu$p-process strongly depends on the $^{59}$Cu(p,$ \alpha $)$^{56}$Ni reaction rate. CCSNe ejects the nucleosynthesis products to the interstellar medium whereas the ashes of XRBs do not become part of the interstellar medium, XRBs are therefore an unlikely source of heavy nuclei. However, the Ni-Cu cycle directly affects the energy generation and, consequently, the shape of the XRB light curves. There is presently no direct experimental information on these reaction rates, at temperatures relevant for CCSNe and XRBs. A first direct measurement of $^{59}$Cu(p,$ \alpha $)$^{56}$Ni reaction cross-section at a higher energy (E$_{c.m.}$ = 6 MeV) was reported recently. This work will report an experiment to directly measure this reaction cross-section at E$_{c.m.}$ = 4.64 MeV, which is relevant to the temperature range for $\nu$p-process. Therefore, it is important to measure the $^{59}$Cu(p,$ \alpha $)$^{56}$Ni reaction rate to understand the Ni-Cu cycle in the $\nu$p-process and XRBs.

Your current academic level, PhD student
Your Email nikhil.bhati@smu.ca
Affiliation Saint Mary's University
Supervisor Prof. Rituparna Kanungo
Supervisor Email rituparna.kanungo@smu.ca

Primary author

Mr Nikhil Bhati (Saint Mary's University)

Co-authors

Prof. Rituparna Kanungo (Saint Mary's University) Dr Jaspreet Randhawa (Saint Mary's University, Halifax) Mx Iris Collaboration

Presentation materials