Bulletin of the American Physical Society
6th Joint Meeting of the APS Division of Nuclear Physics and the Physical Society of Japan
Sunday–Friday, November 26–December 1 2023; Hawaii, the Big Island
Session 3WAA: New Results and Prospects of Time Projection Chambers for Low-energy Nuclear Physics I
9:00 AM–10:30 AM,
Monday, November 27, 2023
Hilton Waikoloa Village
Room: Kings 1
Chair: Wolfgang Mittig, Facility for Rare Isotope Beams, Michigan State University, East Lansing, MI
Abstract: 3WAA.00002 : Overview of the RI beam experiments at RCNP and recent results of the MAIKo active target
9:30 AM–10:00 AM
Presenter:
Tatsuya Furuno
(Department of Physics, Osaka University)
Authors:
Tatsuya Furuno
(Department of Physics, Osaka University)
Hooi Jin Ong
(Institute of Modern Physics, Chinese Academy of Sciences)
The missing mass spectroscopy is attractive for RI beam experiments because it can be applied to the excited states even above the particle-decay thresholds. However, this spectroscopy at forward angles at the center of the mass frame is extremely difficult because it requires the detection of low-energy recoil particles. Active-target time projection chambers (TPC) overcome this challenge by utilizing the detector gas also as the target material and lower the detection threshold.
We developed an active target named MAIKo at RCNP [6]. The MAIKo TPC has a sensitive volume of 10 x 10 x 15 cm3. Recently, we successfully measured alpha elastic and inelastic scattering on 10C beam at 68 MeV/u. The nucleon density distribution of the 10C ground state and the effective interaction between the alpha particles and 10C were determined from the differential cross section of the elastic scattering. From the cross section of the inelastic scattering to the first 2+ state, we determined neutron quadrupole transition matrix element Mn to discuss the Z=6 magicity [7]. We are continuing the analysis of the highly excited states to search for alpha cluster states in 10C. The MAIKo has been upgraded to MAIKo+ with 20 times larger detection volume.
Having demonstrated the possibilities of the active target method, we are planning a campaign project at RCNP using the world's largest active target system AT-TPC from Michigan State University [8]. The AT-TPC will be operated with C3D8 gas to measure the 17C(d,p)18C, 17N(d,3He) 13,15B(d,3He)12,14Be, and 12C+12C reactions.
In the present talk, we will introduce the recent results from the RCNP RI beam experiments and measurements with the MAIKo active target.
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