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    Experimentally constrained 165,166Ho(n,γ)^{165,166}\text{Ho}(n,\gamma) rates and implications for the ss process

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    The γ\gamma-ray strength function and the nuclear level density of 167^{167}Ho have been extracted using the Oslo method from a 164Dy(α,pγ)167^{164}\text{Dy}(\alpha,p\gamma)^{167}Ho experiment carried out at the Oslo Cyclotron Laboratory. The level density displays a shape that is compatible with %can be approximated with the constant temperature model in the quasicontinuum, while the strength function shows structures indicating the presence of both a scissors and a pygmy dipole resonance. Using our present results as well as data from a previous 163Dy(α,pγ)166^{163}\text{Dy}(\alpha,p\gamma)^{166}Ho experiment, the 165Ho(n,γ)^{165}\text{Ho}(n,\gamma) and 166Ho(n,γ)^{166}\text{Ho}(n,\gamma) MACS uncertainties have been constrained. The possible influence of the low-lying, long-lived 6~keV isomer 166^{166}Ho in the ss process is investigated in the context of a 2~M⊙M_\odot, [Fe/H]=-0.5 AGB star. We show that the newly obtained 165Ho(n,γ)^{165}\text{Ho}(n,\gamma) MACS affects the final 165^{165}Ho abundance, while the 166Ho(n,γ)^{166}\text{Ho}(n,\gamma) MACS only impacts the enrichment of 166,167^{166,167}Er to a limited degree due to the relatively rapid β\beta decay of the thermalized 166^{166}Ho at typical ss-process temperatures.Comment: 11 pages, submitted to Physical Reviews
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