N. J. Mukwevho

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-ex2022★ 3 cited

Proton capture on $^{30}$ P in novae: On the existence of states at $6.40$ MeV and $6.65$ MeV in $^{31}$ S

M. Kamil, S. Triambak, G. C. Ball +10

We use a high resolution $^{32} S (d, t)$ measurement to investigate the claimed existence of a 6401(3) keV state in $^{31}$ S that may affect the $^{30} P (p, γ)$ nuclear rea…

nucl-ex2022★ 4 cited

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

M. Kamil, S. Triambak, A. Magilligan +24

The isobaric multiplet mass equation (IMME) is known to break down in the first T = 2, A = 32 isospin quintet. In this work we combine high-resolution experimental data with state-…

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…

Proton capture on 30P in novae: On the existence of states at 6.40 MeV and 6.65 MeV in 31S

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

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

Proton capture on $^{30}$ P in novae: On the existence of states at $6.40$ MeV and $6.65$ MeV in $^{31}$ S

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