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Constraints for stellar electron-capture rates on ⁸⁶Kr via the ⁸⁶Kr(t,³He+γ)⁸⁶Br reaction and the implications for core-collapse supernovae

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arxiv 1908.03985 v1 pith:NXVQQKEI submitted 2019-08-12 nucl-ex astro-ph.HEastro-ph.SRnucl-th

Constraints for stellar electron-capture rates on ⁸⁶Kr via the ⁸⁶Kr(t,³He+γ)⁸⁶Br reaction and the implications for core-collapse supernovae

classification nucl-ex astro-ph.HEastro-ph.SRnucl-th
keywords rateselectron-capturesimulationsapproximationsingle-stateaboveaccurateastrophysical
verification ladder T0 review T1 audit T2 compute T3 formal T4 reserved
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In the late stages of stellar core-collapse, prior to core bounce, electron captures on medium-heavy nuclei drive deleptonization and simulations require the use of accurate reaction rates. Nuclei with neutron number near $N=50$, just above atomic number $Z=28$, play an important role, but rates used in astrophysical simulations rely primarily on a relatively simple single-state approximation. In order to improve the accuracy of astrophysical simulations, experimental data are needed to test the electron-capture rates and to guide the development of better theoretical models. This work presents the results of the $^{86}$Kr($t$,$^{3}$He+$\gamma$) experiment at the NSCL, from which an upper limit for the Gamow-Teller strength up to an excitation energy in $^{86}$Br of 5 MeV is extracted. The derived upper limit for the electron-capture rate on $^{86}$Kr indicates that the rate estimated through the single-state approximation is too high and that rates based on Gamow-Teller strengths estimated in shell-model and QRPA calculations are more accurate. The QRPA calculations tested in this manner were used for estimating the electron capture rates for 78 isotopes near $N=50$ and above $Z=28$. The impact of using these new electron-capture rates in simulations of supernovae instead of the rates based on the single-state approximation is investigated, indicating a significant reduction in the deleptonization that affects multi-messenger signals, such as the emission of neutrinos and gravitational waves.

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