Abstract

We perform a systematic study of the α\alpha-particle excitation from its ground state 01+0_1^+ to the 02+0_2^+ resonance. The so-called monopole transition form factor is investigated via an electron scattering experiment in a broad Q2Q^2-range (from 0.50.5 to 5.05.0 fm−2^{-2}). The precision of the new data dramatically superseeds that of older sets of data, each covering only a portion of the Q2Q^2-range. The new data allow the determination of two coefficients in a low-momentum expansion leading to a new puzzle. By confronting experiment to state-of-the-art theoretical calculations we observe that modern nuclear forces, including those derived within chiral effective field theory which are well tested on a variety of observables, fail to reproduce the excitation of the α\alpha-particle

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