In photoproduction experiments, a large number of final states yielding various resonance contributions are accessible. To extract resonance parameters via partial-wave analysis not only the measurement of differential cross-sections is necessary, but also the determination of polarization observables. At the electron accelerator ELSA (Bonn) the coherent bremsstrahlung method was used to generate a linearly polarized photon beam. Using the CBELSA/TAPS detector setup, the beam asymmetry Sigma in the reaction gamma p -< p pi(0) eta was determined as a function of various masses and angles for photon energies between 970MeV and 1650MeV
The first measurements of the beam-target-helicity-asymmetries E and G in the photoproduction of ω-m...
Photoproduction of neutral pions has been studied with the CBELSA/TAPS detector for photon energies ...
Photoproduction of neutral pions has been studied with the CBELSA/TAPS detector for photon energies ...
In photoproduction experiments, a large number of final states yielding various resonance contributi...
In photoproduction experiments, a large number of final states yielding various resonance contributi...
In photoproduction experiments, a large number of final states yielding various resonance contributi...
In photoproduction experiments, a large number of final states yielding various resonance contributi...
In photoproduction experiments, a large number of final states yielding various resonance contributi...
In photoproduction experiments, a large number of final states yielding various resonance contributi...
In photoproduction experiments, a large number of final states yielding various resonance contributi...
In photoproduction experiments, a large number of final states yielding various resonance contributi...
The beam asymmetry, Σ , was measured at ELSA in the reaction $ \boldsymbol\gamma$ p → ηp using linea...
Photoproduction of neutral pions has been studied with the CBELSA/TAPS detector for photon energies ...
AbstractThe first measurements of the beam-target-helicity-asymmetries E and G in the photoproductio...
Photoproduction of neutral pions has been studied with the CBELSA/TAPS detector for photon energies ...
The first measurements of the beam-target-helicity-asymmetries E and G in the photoproduction of ω-m...
Photoproduction of neutral pions has been studied with the CBELSA/TAPS detector for photon energies ...
Photoproduction of neutral pions has been studied with the CBELSA/TAPS detector for photon energies ...
In photoproduction experiments, a large number of final states yielding various resonance contributi...
In photoproduction experiments, a large number of final states yielding various resonance contributi...
In photoproduction experiments, a large number of final states yielding various resonance contributi...
In photoproduction experiments, a large number of final states yielding various resonance contributi...
In photoproduction experiments, a large number of final states yielding various resonance contributi...
In photoproduction experiments, a large number of final states yielding various resonance contributi...
In photoproduction experiments, a large number of final states yielding various resonance contributi...
In photoproduction experiments, a large number of final states yielding various resonance contributi...
The beam asymmetry, Σ , was measured at ELSA in the reaction $ \boldsymbol\gamma$ p → ηp using linea...
Photoproduction of neutral pions has been studied with the CBELSA/TAPS detector for photon energies ...
AbstractThe first measurements of the beam-target-helicity-asymmetries E and G in the photoproductio...
Photoproduction of neutral pions has been studied with the CBELSA/TAPS detector for photon energies ...
The first measurements of the beam-target-helicity-asymmetries E and G in the photoproduction of ω-m...
Photoproduction of neutral pions has been studied with the CBELSA/TAPS detector for photon energies ...
Photoproduction of neutral pions has been studied with the CBELSA/TAPS detector for photon energies ...