TY - JOUR
T1 - Nuclear reactions of 19,20C on a liquid hydrogen target measured with the superconducting TOF spectrometer
AU - Yamaguchi, T.
AU - Tanaka, K.
AU - Suzuki, T.
AU - Ozawa, A.
AU - Ohtsubo, T.
AU - Aiba, T.
AU - Aoi, N.
AU - Baba, H.
AU - Fukuda, M.
AU - Hashizume, Y.
AU - Inafuku, K.
AU - Iwasa, N.
AU - Izumikawa, T.
AU - Kobayashi, K.
AU - Komuro, M.
AU - Kondo, Y.
AU - Kubo, T.
AU - Kurokawa, M.
AU - Matsuyama, T.
AU - Michimasa, S.
AU - Motobayashi, T.
AU - Nakabayashi, T.
AU - Nakajima, S.
AU - Nakamura, T.
AU - Sakurai, H.
AU - Shinoda, R.
AU - Shinohara, M.
AU - Suzuki, H.
AU - Takechi, M.
AU - Takeshita, E.
AU - Takeuchi, S.
AU - Togano, Y.
AU - Yamada, K.
AU - Yasuno, T.
AU - Yoshitake, M.
PY - 2011/8/1
Y1 - 2011/8/1
N2 - Reaction cross sections with various kinds of breakup channels for neutron-rich carbon isotopes 18-20C and for 9Be impinging on a liquid hydrogen target were investigated at 40 MeV/nucleon. The nuclides of interest were produced via projectile fragmentation from a 63 MeV/nucleon 40Ar beam and were separated in flight at the RIKEN projectile fragment separator (RIPS). The combination of the large-acceptance superconducting TOF spectrometer, TOMBEE (TOF Mass analyzer for exotic BEam Experiment), with a liquid hydrogen target, CRYPTA (CRYogenic ProTon and Alpha target system), enables simultaneous measurements of several reaction channels: the reaction cross sections (σR), individual elemental fragmentation cross sections (σΔZ), charge-changing cross sections (σcc), neutron-removal cross sections (σΔxn), and charge-pickup cross sections (σΔZ+1) for 19,20C; σΔZ, σΔxn, and σΔZ+1 for 18C; and σR for 9Be. The present σR of 9Be on proton, σR=397±23 mb, measured in the inverse kinematics, was consistent with the previous measurements using proton beams at different laboratories. The σR of 19C and 20C on proton were determined to be σR=754±22 mb and σR=791±34 mb, respectively. Taking into account the beam energy and target dependence of σR, the present σR are found to be considerably enhanced compared with those measured at around 1 GeV/nucleon. The σΔZ+1 appears to increase with the mass number of the projectiles, and it significantly contributes to σR in the present energy range. The finite-range optical-limit and few-body Glauber model analyses were performed for σR to study the nuclear matter density distributions and to derive the relative strength of the s-wave components of the valence neutrons in 19C and 20C. A neutron halo structure of 19C is confirmed with an s-wave dominance of the valence neutron when the effect of the charge-pickup reaction is taken into account. The large σΔn of 19C and σΔ2n of 20C also support the decoupled structures of 18C+n and 18C+2n, respectively. The σcc of 19C and 20C agree with each other within their experimental uncertainties, which might indicate a similar proton density distribution in 19C and 20C. The σΔZ decreases monotonically without the even-odd effect as the number of removed protons increases.
AB - Reaction cross sections with various kinds of breakup channels for neutron-rich carbon isotopes 18-20C and for 9Be impinging on a liquid hydrogen target were investigated at 40 MeV/nucleon. The nuclides of interest were produced via projectile fragmentation from a 63 MeV/nucleon 40Ar beam and were separated in flight at the RIKEN projectile fragment separator (RIPS). The combination of the large-acceptance superconducting TOF spectrometer, TOMBEE (TOF Mass analyzer for exotic BEam Experiment), with a liquid hydrogen target, CRYPTA (CRYogenic ProTon and Alpha target system), enables simultaneous measurements of several reaction channels: the reaction cross sections (σR), individual elemental fragmentation cross sections (σΔZ), charge-changing cross sections (σcc), neutron-removal cross sections (σΔxn), and charge-pickup cross sections (σΔZ+1) for 19,20C; σΔZ, σΔxn, and σΔZ+1 for 18C; and σR for 9Be. The present σR of 9Be on proton, σR=397±23 mb, measured in the inverse kinematics, was consistent with the previous measurements using proton beams at different laboratories. The σR of 19C and 20C on proton were determined to be σR=754±22 mb and σR=791±34 mb, respectively. Taking into account the beam energy and target dependence of σR, the present σR are found to be considerably enhanced compared with those measured at around 1 GeV/nucleon. The σΔZ+1 appears to increase with the mass number of the projectiles, and it significantly contributes to σR in the present energy range. The finite-range optical-limit and few-body Glauber model analyses were performed for σR to study the nuclear matter density distributions and to derive the relative strength of the s-wave components of the valence neutrons in 19C and 20C. A neutron halo structure of 19C is confirmed with an s-wave dominance of the valence neutron when the effect of the charge-pickup reaction is taken into account. The large σΔn of 19C and σΔ2n of 20C also support the decoupled structures of 18C+n and 18C+2n, respectively. The σcc of 19C and 20C agree with each other within their experimental uncertainties, which might indicate a similar proton density distribution in 19C and 20C. The σΔZ decreases monotonically without the even-odd effect as the number of removed protons increases.
KW - Calculated
KW - Liquid hydrogen target and secondary radioactive beams
KW - Measured
KW - Nuclear reactions
KW - Transmission method with TOMBEE spectrometer and CRYPTA target
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U2 - 10.1016/j.nuclphysa.2011.05.095
DO - 10.1016/j.nuclphysa.2011.05.095
M3 - Article
AN - SCOPUS:79960637774
SN - 0375-9474
VL - 864
SP - 1
EP - 37
JO - Nuclear Physics A
JF - Nuclear Physics A
IS - 1
ER -