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Beamline Simulation Data and Control Panel Displays
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.
- Beamline control system panel (PDF)
- Transport line control system panel (PDF)
- MAD input deck
- Raw output
![beamline 0](https://www.bnl.gov/atf/images/beamline0.png)
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)
![beamline 1 output](https://www.bnl.gov/atf/images/beamline1.png)
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)
![beamline 2](https://www.bnl.gov/atf/images/beamline2.png)