J. Derkin

most cited

^{57}

β

-delayed proton emission establishes the

^{56}

r p

-process waiting point bypass

5 citations · 5 across the 1 of their papers we have counts for

collaborators

2 papers

nucl-ex2026

Differential cross sections for $^{12} C (n, α_{0})$ , $^{16} O (n, α_{0})$ and $^{16} O (n, α_{1, 2, 3})$ between $E_{n}$ = 7.2 and 10 MeV with an active-target Time Projection Chamber

J. Bishop, C. E. Parker, R. Smith +24

Data for the $^{12} C (n, α_{0})$ , $^{16} O (n, α_{0})$ and $^{16} O (n, α_{1, 2, 3})$ differential cross sections are important for several different a…

nucl-ex2022★ 5 cited

$^{57}$ Zn $β$ -delayed proton emission establishes the $^{56}$ Ni $r p$ -process waiting point bypass

M. Saxena, W. -J Ong, Z. Meisel +32

We measured the $^{57}$ Zn $β$ -delayed proton ( $β$ p) and $γ$ emission at the National Superconducting Cyclotron Laboratory. We find a $^{57}$ Zn half-life of 43.6 $\pm$ 0.2 ms, $β$ p…

Differential cross sections for 12C(n,α0​), 16O(n,α0​) and 16O(n,α1,2,3​) between En​ = 7.2 and 10 MeV with an active-target Time Projection Chamber

57Zn β-delayed proton emission establishes the 56Ni rp-process waiting point bypass

Differential cross sections for $^{12} C (n, α_{0})$ , $^{16} O (n, α_{0})$ and $^{16} O (n, α_{1, 2, 3})$ between $E_{n}$ = 7.2 and 10 MeV with an active-target Time Projection Chamber

$^{57}$ Zn $β$ -delayed proton emission establishes the $^{56}$ Ni $r p$ -process waiting point bypass