K. Brandenburg

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-ex2024

Direct cross-section measurement of the weak r-process 88Sr(α,n)91Zr reaction in ν-driven winds of core collapse supernovae

C. Fougères, M. L. Avila, H. Jayatissa +15

About half of the heavy elements beyond iron are known to be produced by the rapid neutron capture process, known as r-process. However, the astrophysical site producing the r-proc…

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

Direct cross-section measurement of the weak r-process 88Sr(α,n)91Zr reaction in ν-driven winds of core collapse supernovae

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