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            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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