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Experimental Constraint on Stellar Electron-Capture Rates from the {}⁸⁸Sr(t,{}³He+γ){}⁸⁸Rb reaction at 115 MeV/u

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arxiv 1906.05934 v1 pith:4ZYORMTU submitted 2019-06-13 nucl-ex astro-ph.SR

Experimental Constraint on Stellar Electron-Capture Rates from the {}⁸⁸Sr(t,{}³He+γ){}⁸⁸Rb reaction at 115 MeV/u

classification nucl-ex astro-ph.SR
keywords rateselectron-capturetextapproximationeffectsgammastrengthbelow
verification ladder T0 review T1 audit T2 compute T3 formal T4 reserved
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The Gamow-Teller strength distribution from ${}^{88}$Sr was extracted from a $(t,{}^{3}\text{He}+\gamma)$ experiment at 115 MeV/$u$ to constrain estimates for the electron-capture rates on nuclei around $N=50$, between and including $^{78}$Ni and $^{88}$Sr, which are important for the late evolution of core-collapse supernovae. The observed strength below an excitation energy of 8 MeV was consistent with zero and below 10 MeV amounted to $0.1\pm0.05$. Except for a very-weak transition that could come from the 2.231-MeV $1^{+}$ state, no $\gamma$ lines that could be associated with the decay of known $1^{+}$ states were identified. The derived electron-capture rate from the measured strength distribution is more than an order of magnitude smaller than rates based on the single-state approximation presently used in astrophysical simulations for most nuclei near $N=50$. Rates based on shell-model and quasiparticle random-phase approximation calculations that account for Pauli blocking and core-polarization effects provide better estimates than the single-state approximation, although a relatively strong transition to the first $1^{+}$ state in $^{88}$Rb is not observed in the data. Pauli unblocking effects due to high stellar temperatures could partially counter the low electron-capture rates. The new data serves as a zero-temperature benchmark for constraining models used to estimate such effects.

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