Separation of σL and σT in η electroproduction at the resonance S11 (1535)
References (13)
- et al.
Phys. Lett.
(1974) - et al.
Nucl. Phys.
(1975) Nucl. Phys.
(1972)Nucl. Phys.
(1976)- et al.
Phys. Rev. Lett.
(1973) Phys. Rev.
(1975)
There are more references available in the full text version of this article.
Cited by (28)
Photo- and electro-production of mesons on nucleons and nuclei
2008, Progress in Particle and Nuclear PhysicsCitation Excerpt :Details for the present case are described in [56].
Eta and two pion electroproduction with CLAS
2003, Nuclear Physics AStudy of Non-Strange Baryon Resonances with Meson Photoproduction
2003, Progress in Particle and Nuclear PhysicsAn isobar model for η photo- and electroproduction on the nucleon
2002, Nuclear Physics AElectron and photon induced reactions on nuclei in the nucleon resonance region
2000, Nuclear Physics AResonances and higher twist in polarized lepton-nucleon scattering
2000, Nuclear Physics ACitation Excerpt :The S11 resonance has spin 1/2, so that the helicity amplitude A3/2 is absent. We constrain the parametrization of the amplitude A1/2 by the photo- and electro-production data from Refs. [35–39]. For the D13(1520) the amplitude A1/2 is found to be very small at Q2=0.
- ★
Now at Kurukshetra University, Kurukshetra, India.
Copyright © 1978 Published by Elsevier B.V.