S. Ahn

activity

20242026

collaborators

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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-ex2024

Cluster structure of 3 $I^\pm$ +p states in $^{13}$ N

J. Bishop, G. V. Rogachev, S. Ahn +16

Background: Cluster states in $^{13}$ N are extremely difficult to measure due to the unavailability of $^{9}$ B+ $I^\pm$ elastic scattering data. Purpose: Using $I^^{2}$ -delayed charged-par…

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

Cluster structure of 3I^±+p states in 13N

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

Cluster structure of 3 $I^\pm$ +p states in $^{13}$ N