The gamma-ray strength function of $^{89}$Y and $^{90}$Y
In this work, we present new data on the $^{89}$Y($γ$,n) cross section studied with a quasi-monochromatic photon beam produced at the NewSUBARU synchrotron radiation facility in Japan contributing torwards resolving a long standing discrepancy between existing measurements of this cross section. Results for $γ$-ray strength function below threshold obtained by applying the Oslo method to $^{89}$Y($p,p'γ$)$^{89}$Y coincidences combined with the $^{89}$Y($γ$,n) data this providing experimental data for the $γ$-ray strength function of $^{89}$Y for $γ$ energies in the range of $\approx 1.6$ Mev to $\approx$ 20 MeV. A low-energy enhancement is seen for $γ$-rays below $\approx 2.5$ MeV. Shell-model calculations indicate that this feature is caused by strong, low-energy $M1$ transitions at high excitation energies. The nuclear level density and $γ$-ray strength function have been extracted from $^{89}$Y($d,p γ$)$^{90}$Y coincidences using the Oslo method. Using the ($γ,n$) and ($d,pγ$) data as experimental constraints, we have calculated the $^{89}$Y($n,γ$)$^{90}$Y cross section with the TALYS reaction code. Our results have been compared with directly measured (n,$γ$) cross sections and evaluations. The $N=50$ isotope $^{89}$Y is an important bottleneck in the s-process and the magnitude of the $^{89}$Y(n,$γ)$ cross section is key to understanding how s-process stars produce heavy isotopes.