6533b85dfe1ef96bd12bf0b9

RESEARCH PRODUCT

Breakup channels forC12triple-αcontinuum states

Björn JonsonS. P. FoxGöran Hugo NymanA. NieminenF.c. BarkerC. Aa. DigetC. Aa. DigetHenrik B. JeppesenMaría José García BorgeHeikki PenttiläA. JokinenPeter DendoovenOlof TengbladH. O. U. FynboJ. ÄYstöJussi HuikariV. F. E. PucknellK. WilhelmsenS. HyldegaardY. WangB. R. FultonTommi EronenR. BoutamiK. RiisagerSami Rinta-antilaIain MooreAnu Kankainen

subject

PhysicsNuclear and High Energy PhysicsAngular momentumExcited stateNuclear TheoryContinuum (design consultancy)Carbon-12Alpha particleAtomic physicsNuclear ExperimentSpin (physics)Ground stateBreakup

description

The triple-alpha-particle breakup of states in the triple-alpha continuum of C-12 has been investigated by way of coincident detection of all three alpha particles of the breakup. The states have been fed in the beta decay of N-12 and B-12, and the alpha particles measured using a setup that covers all of the triple-alpha phase space. Contributions from the breakup through the Be-8(0(+)) ground state as well as other channels-interpreted as breakup through excited energies in Be-8-have been identified. Spins and parities of C-12 triple-alpha continuum states are deduced from the measured phase-space distributions for breakup through Be-8 above the ground state by comparison to a fully symmetrized sequential R-matrix description of the breakup. At around 10 MeV in C-12, the breakup is found to be dominated by 0(+) strength breaking up through the ghost of the Be-8(0(+)) ground state with L = 0 angular momentum between the first emitted alpha particle and the intermediate Be-8 nucleus. For C-12 energies above the 12.7 MeV 1(+) state, however, L = 2 breakup of a C-12 2(+) state through the Be-8(2(+)) excited state dominates. Furthermore, the possibility of a 2(+) excited state in the 9-12 MeV region of C-12 is investigated.

https://doi.org/10.1103/physrevc.80.034316