Beamline 0 is directly downstream of the linac and serves to transport the beam from the linac to any one of the three experimental beamlines. Beamline 0 is modeled using MAD. Shown below is a summary of the MAD simulation results.
This beam line currently serves the Plasma Acceleration,
Current Filamentation Instability and Compton
scattering experiments. A summary of the MAD
simulation results is shown below.
MAD input deck | Output of optical functions | Beamline control system panel (PDF)
ATF beamline 2 previously served the IFEL experiment, the
SASE experiment and the High-Gain Harmonic-Generation
experiment. It now serves the Plasma Wakefield
Acceleration experiment. Beamline 2 is modeled using MAD,
whose input deck may be found here. A summary of the MAD
simulated optical functions for the PWFA experiment is shown
below.
MAD input deck | Raw simulation output | Control system panel (PDF)