Formation of eta-prime(958)-mesic nuclei by (p,d) reaction
arXiv:1211.2506 · doi:10.1103/PhysRevC.87.045201
Abstract
We calculate theoretically the formation spectra of eta'(958)-nucleus systems in the (p,d) reaction for the investigation of the in-medium modification of the eta' mass. We show the comprehensive numerical calculations based on a simple form of the eta' optical potential in nuclei with various potential depths. We conclude that one finds an evidence of possible attractive interaction between eta' and nucleus as peak structure appearing around the eta' threshold in light nuclei such as 11C when the attractive potential is stronger than 100 MeV and the absorption width is of order of 40 MeV or less. Spectroscopy of the (p,d) reaction is expected to be performed experimentally at existing facilities, such as GSI. We also estimate the contributions from the omega and phi mesons, which have masses close to the eta' meson, concluding that the observation of the peak structure of the eta'-mesic nuclei is not disturbed although their contributions may not be small.
8 pages, 8 figures
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Cited by in corpus (13)
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- Measurement of excitation spectra in the C reaction near the emission threshold
- Determination of the real part of the η'-Nb optical potential
- Chiral symmetry restoration at high matter density observed in pionic atoms
- Momentum dependence of the imaginary part of the - and -nucleus optical potential
- Experimental constraints on the -nucleus real potential
- meson under partial restoration of chiral symmetry in nuclear medium
- Structure of double pionic atoms
- Formation of eta'(958) Meson Bound States by the 6Li(gamma,d) reaction
- The interaction from the correlation function
- Search for the 4He-eta bound state in dd->(4He-eta)_{bound}->3He n pi0 and dd->(4He-eta)_{bound}->3He p pi- reactions with the WASA-at-COSY facility
- Feasibility of the observation of mesic nuclei in the semi-exclusive C() reaction
- Pseudoscalar mesons from a PNJL model at zero temperature