N. Kheswa

activity

20172022

most citedIsospin Mixing and the Cubic Isobaric Multiplet Mass Equation in the Lowest T = 2, A = 32 Quintet

4 citations · 7 across the 2 of their papers we have counts for

collaborators

3 papers

nucl-ex2020

Fine Structure of the Isovector Giant Dipole Resonance in $^{142 - 150}$ Nd and $^{152}$ Sm

L. M. Donaldson, J. Carter, P. von Neumann-Cosel +35

Background: Inelastic proton scattering at energies of a few hundred MeV and very-forward angles including $0^{\circ}$ has been established as a tool to study electric-dipole strengt…

nucl-ex2018

Second T = 3/2 state in $^{9}$ B and the isobaric multiplet mass equation

N. J. Mukwevho, B. M. Rebeiro, D. J. Marín-Lámbarri +17

Recent high-precision mass measurements and shell model calculations~[Phys. Rev. Lett. {\bf 108}, 212501 (2012)] have challenged a longstanding explanation for the requirement of a…

nucl-ex2017

Re-examining the $^{26}$ Mg( $α, α^{'}$ ) $^{26}$ Mg reaction - probing astrophysically important states in $^{26}$ Mg

P. Adsley, J. W. Brümmer, K. C. W. Li +10

Background: The $^{22}$ Ne( $α, n$ ) $^{25}$ Mg reaction is one of the neutron sources for the $s$ -process in massive stars. The properties of levels in $^{26}$ Mg above the $α$ -particle…

Fine Structure of the Isovector Giant Dipole Resonance in 142−150Nd and 152Sm

Second T = 3/2 state in 9B and the isobaric multiplet mass equation

Re-examining the 26Mg(α,α′)26Mg reaction - probing astrophysically important states in 26Mg

Fine Structure of the Isovector Giant Dipole Resonance in $^{142 - 150}$ Nd and $^{152}$ Sm

Second T = 3/2 state in $^{9}$ B and the isobaric multiplet mass equation

Re-examining the $^{26}$ Mg( $α, α^{'}$ ) $^{26}$ Mg reaction - probing astrophysically important states in $^{26}$ Mg