References quoted in the XUNDL dataset: 9C 9BE(13O,9C):XUNDL-4

2 references found.

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2019HO14

Phys.Rev. C 100, 054618 (2019)

J.Hooker, G.V.Rogachev, E.Koshchiy, S.Ahn, M.Barbui, V.Z.Goldberg, C.Hunt, H.Jayatissa, E.C.Pollacco, B.T.Roeder, A.Saastamoinen, S.Upadhyayula

Structure of ⁹C through proton resonance scattering with the Texas Active Target detector

NUCLEAR REACTIONS ¹H(⁸B, p)⁹C^*, E=60.8 MeV, [secondary ⁸B beam from ⁶Li(³He, n)⁸B, E=13.2 MeV/nucleon primary reaction, and using the Momentum Achromat Recoil Spectrometer (MARS) at the Cyclotron Institute of Texas A and M University]; measured charged products, ⁸B spectrum, Ep, (⁸Be)p-coin, angular distributions using TexAT time projection chamber (TPC) and CsI(Tl) scintillators. ⁹C; deduced levels, resonances, J, π, phase shifts, widths using R-matrix analysis. Comparison with previous experimental data, and with ab initio calculations in literature.

doi: 10.1103/PhysRevC.100.054618

2023CH47

Phys.Rev. C 108, 044318 (2023)

R.J.Charity, L.G.Sobotka

Invariant-mass spectroscopy in projectile fragmentation reactions

NUCLEAR REACTIONS ⁹Be(¹³O, X)⁹N/¹⁰N/¹¹N/⁹C/¹⁰C/¹²O, E=65.4 MeV/nucleon; ⁹Be(⁹C, X), (⁹C, ⁹C), E=68 MeV/nucleon; measured charged particles from reaction products decay channels; deduced invariant mass spectra, resonances. ^9,10,11N, ^9,10C, ¹²O; deduced levels, J, π, widths of the resonances. Discussed application of the invariant-mass method to the study of the reaction products located furthest beyond the proton drip line. Experiments carried out at NSCL-MSU facility using A1900 fragment separator and High Resolution Array of Si-CsI(Tl) telescopes (HiRA).

doi: 10.1103/PhysRevC.108.044318