References quoted in the XUNDL dataset: 6LI 6LI(10B,X):XUNDL-11

3 references found.

Clicking on a keynumber will list datasets that reference the given article.


1977KE09

Phys.Rev. C15, 1726 (1977)

K.W.Kemper, G.E.Moore, R.J.Puigh, R.L.White

Spectroscopic Information from the 9Be(7Li, 6He)10B and 9Be(7Li, 6Li)10Be Reactions

NUCLEAR REACTIONS 9Be(7Li, 7Li), E=30 MeV; 10B(6Li, 6Li), E=34 MeV; measured σ(θ); deduced optical model parameters. 9Be(7Li, 6He), E=34 MeV; measured σ(θ); deduced spin transfer. 9Be(7Li, 6Li), E=34 MeV; measured σ(θ). 10B, 10Be levels deduced S. Finite range DWBA analysis.

doi: 10.1103/PhysRevC.15.1726


2007RU13

Eur.Phys.J. A 33, 317 (2007)

A.T.Rudchik, V.O.Romanyshyn, E.I.Koshchy, A.Budzanowski, K.W.Kemper, K.Rusek, V.D.Chesnokova, J.Choinski, B.Czech, L.Glowacka, S.Kliczewski, V.M.Kyryanchuk, S.Yu.Mezhevych, A.V.Mokhnach, O.A.Momotyuk, O.A.Ponkratenko, R.Siudak, I.Skwirczynska, A.Szczurek

Isotopic effects in the 7Li + 10, 11B elastic and inelastic scattering

NUCLEAR REACTIONS 7Li(10B, 10B), E=51 MeV; measured elastic scattering σ and angular distributions. 10B(7Li, 7Li), E=24, 39 MeV; 11B(7Li, 7Li), E=34 MeV; analyzed elastic scattering σ using optical model and coupled channel method.

doi: 10.1140/epja/i2007-10483-5


2022RU05

Phys.Rev. C 106, 014615 (2022)

A.T.Rudchik, A.A.Rudchik, O.O.Chepurnov, K.W.Kemper, N.Keeley, K.Rusek, E.I.Koshchy, S.Kliczewski, S.Yu.Mezhevych, V.M.Pirnak, O.A.Ponkratenko, R.Siudak, H.M.Maridi, A.P.Ilyin, B.V.Mishchenko, Yu.M.Stepanenko, V.V.Uleshchenko, Yu.O.Shyrma, K.A.Chercas, B.Zalewski

Comparison of 10B + 6Li and 10B + 7Li elastic scattering: The role of ground state reorientation and breakup

NUCLEAR REACTIONS 6Li(10B, 10B), E=51 MeV; measured reaction products, angular distributions; deduced σ(θ), parameters of the optical model potentials, influence of the resonant states on the σ(E) of the α+d breakup. 7Li(10B, 10B), E=51 MeV; analyzed σ(E) and angular distributions from 2007RU13; deduced parameters of the optical model potentials, influence of the resonant states on the σ(E) of the α+t breakup. Comparison to coupled discretized continuum channel (CDCC) calculations. Setup consisting of solid state silicon detectors and gas-filled ionization chamber at U-200P cyclotron of the Heavy Ion Laboratory of the University of Warsaw.

doi: 10.1103/PhysRevC.106.014615