| dc.contributor.author | Witthauer, L. | |
| dc.contributor.author | Dieterle, M. | |
| dc.contributor.author | Abt, S. | |
| dc.contributor.author | Achenbach, P. | |
| dc.contributor.author | Afzal, F. | |
| dc.contributor.author | Ahmed, Z. | |
| dc.contributor.author | Annand, J. R. M. | |
| dc.contributor.author | Arends, H. J. | |
| dc.contributor.author | Bashkanov, M. | |
| dc.contributor.author | Beck, R. | |
| dc.contributor.author | Biroth, M. | |
| dc.contributor.author | Borisov, N. S. | |
| dc.contributor.author | Braghieri, A. | |
| dc.contributor.author | Briscoe, W. J. | |
| dc.contributor.author | Cividini, F. | |
| dc.contributor.author | Costanza, S. | |
| dc.contributor.author | Collicott, C. | |
| dc.contributor.author | Denig, A. | |
| dc.contributor.author | Downie, E. J. | |
| dc.contributor.author | Drexler, P. | |
| dc.contributor.author | Ferretti-Bondy, M. I. | |
| dc.contributor.author | Gardner, S. | |
| dc.contributor.author | Garni, S. | |
| dc.date.accessioned | 2018-02-08T07:05:22Z | |
| dc.date.available | 2018-02-08T07:05:22Z | |
| dc.date.issued | 2016-09-22 | |
| dc.identifier.citation | Physical Review Letters, 117, 132502 | en_US |
| dc.identifier.issn | 0031-9007 | |
| dc.identifier.uri | https://journals.aps.org/prl/pdf/10.1103/PhysRevLett.117.132502 | |
| dc.identifier.uri | http://repository.seku.ac.ke/handle/123456789/3832 | |
| dc.description | DOI:https://doi.org/10.1103/PhysRevLett.117.132502 | en_US |
| dc.description.abstract | The double polarization observable E and the helicity dependent cross sections σ1/2 and σ3/2 were measured for η photoproduction from quasifree protons and neutrons. The circularly polarized tagged photon beam of the A2 experiment at the Mainz MAMI accelerator was used in combination with a longitudinally polarized deuterated butanol target. The almost 4π detector setup of the Crystal Ball and TAPS is ideally suited to detect the recoil nucleons and the decay photons from η→2γ and η→3π0. The results show that the narrow structure previously observed in η photoproduction from the neutron is only apparent in σ1/2 and hence, most likely related to a spin-1/2 amplitude. Nucleon resonances that contribute to this partial wave in η production are only N1/2− (S11) and N 1/2+ (P11). Furthermore, the extracted Legendre coefficients of the angular distributions for σ1/2 are in good agreement with recent reaction model predictions assuming a narrow resonance in the P11 wave as the origin of this structure. | en_US |
| dc.language.iso | en | en_US |
| dc.publisher | American Physical Society | en_US |
| dc.subject | photon: beam | en_US |
| dc.subject | polarization: longitudinal | en_US |
| dc.subject | cross section | en_US |
| dc.subject | helicity: dependence | en_US |
| dc.subject | eta: photoproduction | en_US |
| dc.subject | tagged beam | en_US |
| dc.subject | nucleon: recoil | en_US |
| dc.subject | photon: decay | en_US |
| dc.subject | angular distribution | en_US |
| dc.subject | nucleon resonance | en_US |
| dc.subject | narrow resonance | en_US |
| dc.subject | partial wave analysis | en_US |
| dc.subject | bremsstrahlung | en_US |
| dc.subject | deuterium: liquid | en_US |
| dc.subject | Crystal Ball | en_US |
| dc.subject | Mainz Linac | en_US |
| dc.subject | p | en_US |
| dc.subject | n | en_US |
| dc.subject | experimental results | en_US |
| dc.title | Insight into the Narrow Structure in η Photoproduction on the Neutron from Helicity-Dependent Cross Sections | en_US |
| dc.type | Article | en_US |