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Free, publicly-accessible full text available January 1, 2026
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Bahini, A; von_Neumann-Cosel, P; Carter, J; Usman, IT; Arsenyev, NN; Severyukhin, AP; Litvinova, E; Fearick, RW; Neveling, R; Adsley, P; et al (, Nuclear Physics A)Free, publicly-accessible full text available July 1, 2026
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Markova, M.; Larsen, A_C; von_Neumann-Cosel, P.; Litvinova, E.; Choplin, A.; Goriely, S.; Martinet, S.; Siess, L.; Guttormsen, M.; Pogliano, F.; et al (, Physical Review C)
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Bahini, A.; von_Neumann-Cosel, P.; Carter, J.; Usman, I_T; Arsenyev, N_N; Severyukhin, A_P; Litvinova, E.; Fearick, R_W; Neveling, R.; Adsley, P.; et al (, Physical Review C)
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Deary, J; Scheck, M; Schwengner, R; O’Donnell, D; Bemmerer, D; Beyer, R; Hensel, Th; Junghans, A R; Kögler, T; Müller, S E; et al (, The European Physical Journal A)Abstract The electricE1 and magneticM1 dipole responses of the$$N=Z$$ nucleus$$^{24}$$ Mg were investigated in an inelastic photon scattering experiment. The 13.0 MeV electrons, which were used to produce the unpolarised bremsstrahlung in the entrance channel of the$$^{24}$$ Mg($$\gamma ,\gamma ^{\prime }$$ ) reaction, were delivered by the ELBE accelerator of the Helmholtz-Zentrum Dresden-Rossendorf. The collimated bremsstrahlung photons excited one$$J^{\pi }=1^-$$ , four$$J^{\pi }=1^+$$ , and six$$J^{\pi }=2^+$$ states in$$^{24}$$ Mg. De-excitation$$\gamma $$ rays were detected using the four high-purity germanium detectors of the$$\gamma $$ ELBE setup, which is dedicated to nuclear resonance fluorescence experiments. In the energy region up to 13.0 MeV a total$$B(M1)\uparrow = 2.7(3)~\mu _N^2$$ is observed, but this$$N=Z$$ nucleus exhibits only marginalE1 strength of less than$$\sum B(E1)\uparrow \le 0.61 \times 10^{-3}$$ e$$^2 \, $$ fm$$^2$$ . The$$B(\varPi 1, 1^{\pi }_i \rightarrow 2^+_1)/B(\varPi 1, 1^{\pi }_i \rightarrow 0^+_{gs})$$ branching ratios in combination with the expected results from the Alaga rules demonstrate thatKis a good approximative quantum number for$$^{24}$$ Mg. The use of the known$$\rho ^2(E0, 0^+_2 \rightarrow 0^+_{gs})$$ strength and the measured$$B(M1, 1^+ \rightarrow 0^+_2)/B(M1, 1^+ \rightarrow 0^+_{gs})$$ branching ratio of the 10.712 MeV$$1^+$$ level allows, in a two-state mixing model, an extraction of the difference$$\varDelta \beta _2^2$$ between the prolate ground-state structure and shape-coexisting superdeformed structure built upon the 6432-keV$$0^+_2$$ level.more » « less
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