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1–3 Nov 2011
Ruxin conference center
Asia/Shanghai timezone
We are going to have inauguration ceremony at 11:00 on 1st of November and all are invited to join the ceremony.

The parity-transfer reaction $(^{16}{\rm O},^{16}{\rm F})$ for studies of pionic $0^-$ mode

3 Nov 2011, 12:00
30m
Ruxin conference center

Ruxin conference center

Xueyuan road 37#, Haidian district, 100191, Beijing, China

Speaker

Dr Masanori Dozono (Riken Nishina Center)

Description

The spin-isospin excitation modes in nuclei have been instrumental for the understanding of nuclear structure for the several decades. Spin-dipole (SD) $(L=1,S=1,J^{\pi}=0^{-},1^{-},2^{-})$ excitations have been under extensive theoretical studies. Isovector $0^{-}$ excitations are of particular interest since they carry the simplest pion-like quantum number. The distribution of $0^{-}$ states is expected to reflect pion-like correlations in nuclei. Recently, the effects of tensor correlations on the $0^{-}$ excitations have been investigated by using a self-consistent HF+RPA calculations~\cite{bai2010,bai2011}. From the calculations, It is found that the tensor correlations produce a strong hardening (shifting toward higher excitation energy) effect on the collective $0^{-}$ resonance, and the effect is very sensitive to the magnitude of tensor strength. Therefore, from the study of $0^{-}$ states, we are able to pin down the tensor correlation effects. In spite of its importance, experimental information on $0^{-}$ states is very limited. We propose a new probe, a parity-transfer reaction $(^{16}{\rm O},^{16}{\rm F})$ for the $0^{-}$ study. The parity-transfer reaction uses $0^{+} \rightarrow 0^{-}$ transition as a probe to $0^{-}$ states in nuclei. This reaction has advantages over other reactions used so far. In order to confirm its effectiveness, we study the $0^-$ distribution in $^{12}{¥rm B}$ by using the $^{12}{¥rm C}(^{16}{\rm O},^{16}{\rm F})$ reaction at 250MeV/u. The excitation energy of $^{12}{¥rm B}$ are deduced by means of the missing-mass spectroscopy by using the SHARAQ spectrometer~¥cite{uesaka2008}. The outgoing $^{16}{¥rm F}$ are identified by using the invariant-mass of the decayed $p$ + $^{15}{¥rm O}$ pairs, which are measured at the low-momentum side of the first dipole magnet and the focal plane of the SHARAQ spectrometer. \bibitem{bai2010} C.~L.~Bai {\it et al.}, Phys. Rev. Lett. {\bf 105}, 072501 (2010). \bibitem{bai2011} C.~L.~Bai {\it et al.}, Phys. Rev. C {¥bf 83}, 054316 (2011). \bibitem{uesaka2008} T.~Uesaka {\it et al.}, Nucl. Instrum. Meth. In Phys. Res. {\bf B266}, 4218 (2008).

Primary author

Dr Masanori Dozono (Riken Nishina Center)

Presentation materials