C. Wheldon

collaborators

3 papers

nucl-ex2026

Differential cross sections for $^{12} C (n, I^\pm_{0})$ , $^{16} O (n, I^\pm_{0})$ and $^{16} O (n, I^\pm_{1, 2, 3})$ 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 $^{12} C (n, I^\pm_{0})$ , $^{16} O (n, I^\pm_{0})$ and $^{16} O (n, I^\pm_{1, 2, 3})$ differential cross sections are important for several differen…

nucl-ex2025

Potential absence of observed $I ¨ ^{2}$ linear-chain structures in $^{14}$ O via $^{10}$ C( $I^\pm, I^\pm$ ) resonant scattering

J. Bishop, A. Hollands, Tz. Kokolova +14

Background: The preference for light nuclear systems to coagulate into $I^\pm$ -particle clusters has been well-studied. The possibility of a linear chain configuration of $I^\pm$ -particl…

nucl-ex2025

Unbound neutron $ν 0 d_{3/2}$ strength in $^{17}$ C and the N=16 shell gap

J. Lois-Fuentes, B. FernÃ¡ndez-DomÃnguez, F. Delaunay +61

Significant continuum strength has been observed to be populated in $^{17}$ C produced in the d( $^{16}$ C,p) reaction at a beam energy of 17.2~MeV/nucleon. The strength appears at gr…

Differential cross sections for 12C(n,I^±0​), 16O(n,I^±0​) and 16O(n,I^±1,2,3​) between En​ = 7.2 and 10 MeV with an active-target Time Projection Chamber

Potential absence of observed I¨2 linear-chain structures in 14O via 10C(I^±,I^±) resonant scattering

Unbound neutron ν0d3/2​ strength in 17C and the N=16 shell gap

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

Potential absence of observed $I ¨ ^{2}$ linear-chain structures in $^{14}$ O via $^{10}$ C( $I^\pm, I^\pm$ ) resonant scattering

Unbound neutron $ν 0 d_{3/2}$ strength in $^{17}$ C and the N=16 shell gap