Abstract
The underlying physics triggering core collapse supernovae is not fully understood but observations of material ejected during such events helps to solve this puzzle. In particular, several satellite based γ-ray observations of the isotope 44Ti have been reported recently. Conveniently, the amount of this isotope in stellar ejecta is thought to depend critically on the explosion mechanism. The most influential reaction to the amount of 44Ti in supernovae is Ti44(α,p)V47. Here we report on a direct study of this reaction conducted at the REX-ISOLDE facility, CERN. The experiment was performed with a 44Ti beam at Elab=2.16 MeV/u, corresponding to an energy distribution, for reacting α-particles, centred on Ecm=4.15 with a 1σ width of 0.23 MeV. This is, for the first time, well within the Gamow window for core collapse supernovae. The material from which the 44Ti beam was extracted originates from highly irradiated components of the SINQ spallation neutron source of the Paul Scherrer Institute. No yield above background was observed, enabling an upper limit for the rate of this reaction to be determined. This result is below expectation, suggesting that the Ti44(α,p)V47 reaction proceeds more slowly than previously thought. Implications for astrophysical events, and remnant age, are discussed.
Highlights
The underlying physics triggering core collapse supernovae is not fully understood but observations of material ejected during such events helps to solve this puzzle
The radionuclide 44Ti is one of the very few cosmogenic nuclei to be observed in our Galaxy, and in particular from remnants of core collapse supernovae (CCSNe)
In this Letter we report on a recent experiment conducted at CERN aimed at providing the first direct measurement of the
Summary
The underlying physics triggering core collapse supernovae is not fully understood but observations of material ejected during such events helps to solve this puzzle. The recoil nuclei were analysed and the cross section for the 44Ti(α, p)47V reaction extracted at various centre of mass energies, between 5.7 and 9.0 MeV, with the different energies reached by using appropriate thicknesses of titanium degrader foil.
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