Identification of alpha cluster states analogous to the 12 C Hoyle state in heavier alphaconjugate nuclei can provide tests of the existence of alpha condensates in nuclei. Such states are predicted for 16 O, 20 Ne, 24 Mg,28 Si etc. at excitation energies slightly above the multi-alpha particle decay threshold, but have not yet been experimentally identified. The Thick Target Inverse Kinematics (TTIK) technique can be used to study the breakup of excited self-conjugate nuclei into many alpha particles. The reaction 20 Ne+α was studied using a 20 Ne beam at 12 MeV/nucleon from the K150 cyclotron at Texas A&M University. The TTIK method was used to study both single α-particle emission and multiple α-particle decays. Events with alpha multiplicity up to four were analyzed. The analysis of the three α -particle emission data allowed the identification of the Hoyle state and other 12 C excited states decaying into three alpha particles. The results are shown and compared with other data available in the literature. Although the statistics for events with alpha multiplicity four is low, the data show a structure at about 15.2 MeV that could indicate the existence in 16 O of a state analogous to the 12 C Hoyle state. This structure is confirmed by the re-analysis of alpha multiplicity four events from a previous experiment performed at 9.7 MeV/nucleon with a similar setup but lower granularity. Moreover, the reconstructed excitation energy of 24 Mg for these events peaks at around 34 MeV, very close to the predicted excitation energy for an excited state analogous to the 12 C Hoyle state in 24 Mg.
Introduction:The alpha cluster structure of nuclei with an equal number of protons and neutrons (alpha conjugate nuclei) was categorized in 1968 by Ikeda [1] to explain some excited states not reproduced by the shell model. Since then many studies have been performed, but alpha clustering is still not completely understood especially in the medium-light and heavy systems. In the last ten years a lot of theoretical effort has been focused on the study of 0 + states built on alpha-particle cores in self-conjugate nuclei at excitation energies slightly above the multi-alpha particle decay threshold. Those states are described as diluted gases of alpha particles occupying the same 0 + orbital. They are characterized by a larger radius compared to the normal bound states so that the interaction between alpha particles is reduced. Therefore, these states can be considered as the best candidates for Bose-Einstein condensates of alpha particles in the atomic nucleus. Examples of such states are the ground state of 8 Be and the famous 12 C Hoyle state. Analogous states are predicted for 16 O, 20 Ne, 24 Mg, 28 Si etc. at excitation energies slightly above the multi-alpha particle decay threshold, but have not yet been experimentally identified [2,3].