par Kondo, Takeo;Utsunomiya, Hiroaki;Goriely, Stéphane 
;Daoutidis, Ioannis ;Iwamoto, C.;Akimune, H;Okamoto, Yoshio;Yamagata, Tamio;Kamata, Masaki;Itoh, Osamu;Toyokawa, Hiroyuki;Lui, Yiu-Wing;Harada, H.;Kitatani, Fumito;Hilaire, Stéphane;Koning, Arjan J.
Référence Physical review. C. Nuclear physics, 86, page (014316)
Publication Publié, 2012-07-17
;Daoutidis, Ioannis ;Iwamoto, C.;Akimune, H;Okamoto, Yoshio;Yamagata, Tamio;Kamata, Masaki;Itoh, Osamu;Toyokawa, Hiroyuki;Lui, Yiu-Wing;Harada, H.;Kitatani, Fumito;Hilaire, Stéphane;Koning, Arjan J.Référence Physical review. C. Nuclear physics, 86, page (014316)
Publication Publié, 2012-07-17
Article révisé par les pairs
| Résumé : | Using quasimonochromatic laser-Compton scattering γ rays, total photoneutron cross sections were measured for 206 ,207 ,208Pb near neutron threshold with a high-efficiency 4π neutron detector. Partial E1 and M1 photoneutron cross sections along with total cross sections were determined for 207 ,208Pb at four energies near threshold by measuring anisotropies in photoneutron emission with linearly polarized γ rays. The E1 strength dominates over the M1 strength in the neutron channel where E1 photoneutron cross sections show extra strength of the pygmy dipole resonance in 207 ,208Pb near the neutron threshold corresponding to 0.32%-0.42% of the Thomas-Reiche-Kuhn sum rule. Several μN2 units of B(M1)→ strength were observed in 207 ,208Pb just above neutron threshold, which correspond to an M1 cross section less than 10% of the total photoneutron cross section. © 2012 American Physical Society. |
