• High Power Laser Science and Engineering
  • Vol. 4, Issue 2, 02000e13 (2016)
Mario Ferianis, Enrico Allaria, Eugenio Ferrari, Giulio Gaio, Giuseppe Penco, Fabio Rossi, and Marco Veronese
Author Affiliations
  • Elettra-Sincrotrone Trieste S.C.p.A., Italy
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    DOI: 10.1017/hpl.2016.6 Cite this Article Set citation alerts
    Mario Ferianis, Enrico Allaria, Eugenio Ferrari, Giulio Gaio, Giuseppe Penco, Fabio Rossi, Marco Veronese. How the optical timing system, the longitudinal diagnostics and the associated feedback systems provide femtosecond stable operation at the FERMI free electron laser[J]. High Power Laser Science and Engineering, 2016, 4(2): 02000e13 Copy Citation Text show less
    Block diagram of the FERMI timing system.
    Fig. 1. Block diagram of the FERMI timing system.
    Block diagram of the pulsed optical timing system.
    Fig. 2. Block diagram of the pulsed optical timing system.
    OOL stability measurement of a 150 m pulsed stabilized link (loopback mode). The residual relative drift between the link output and the local splitter port is equal to $5.3~\text{fs}_{\text{RMS}}$.
    Fig. 3. OOL stability measurement of a 150 m pulsed stabilized link (loopback mode). The residual relative drift between the link output and the local splitter port is equal to $5.3~\text{fs}_{\text{RMS}}$.
    Acquisition showing the typical trend of the arrival time at the BAM station, installed after the first bunch compressor. The feedback based on the arrival time was not active.
    Fig. 4. Acquisition showing the typical trend of the arrival time at the BAM station, installed after the first bunch compressor. The feedback based on the arrival time was not active.
    Layout of the BLM.
    Fig. 5. Layout of the BLM.
    Single electron spectral dependence of the radiation emitted from the fourth dipole of BC1; the edge radiation (blue) is dominated by the velocity term and the synchrotron radiation (green) is dominated by the acceleration term.
    Fig. 6. Single electron spectral dependence of the radiation emitted from the fourth dipole of BC1; the edge radiation (blue) is dominated by the velocity term and the synchrotron radiation (green) is dominated by the acceleration term.
    Spectral dependence of the transmission of the optical system.
    Fig. 7. Spectral dependence of the transmission of the optical system.
    Pyrodetector signal versus LINAC 1 RF phase.
    Fig. 8. Pyrodetector signal versus LINAC 1 RF phase.
    Schematic representation of the BAM[34].
    Fig. 9. Schematic representation of the BAM[34].
    Block diagram of the BAM front end.
    Fig. 10. Block diagram of the BAM front end.
    Block diagram of the BAM back end.
    Fig. 11. Block diagram of the BAM back end.
    Estimation of the BAM resolution. By splitting in quadrature the contributions of two independent BAM stations, the width of the shot-to-shot correlations shows an upper estimation for the resolution in 8 fs RMS (bunch charge $=$ 500 pC).
    Fig. 12. Estimation of the BAM resolution. By splitting in quadrature the contributions of two independent BAM stations, the width of the shot-to-shot correlations shows an upper estimation for the resolution in 8 fs RMS (bunch charge $=$ 500 pC).
    Layout of FERMI longitudinal feedbacks.
    Fig. 13. Layout of FERMI longitudinal feedbacks.
    Spectra of the two BAMs with BC1 BAM feedback, OFF and ON.
    Fig. 14. Spectra of the two BAMs with BC1 BAM feedback, OFF and ON.
    Spectra of the bunch arrival (top) and energy (bottom) sensor feedbacks, with bunch arrival feedback configured with low or high loop gain.
    Fig. 15. Spectra of the bunch arrival (top) and energy (bottom) sensor feedbacks, with bunch arrival feedback configured with low or high loop gain.
    Spectra of the BC1 compression factor (top) and the FEL output power (bottom) when compression feedback is switched OFF and ON.
    Fig. 16. Spectra of the BC1 compression factor (top) and the FEL output power (bottom) when compression feedback is switched OFF and ON.
    700 pC-bunch longitudinal phase space imaged on a YAG screen placed in the energy spectrometer at the end of the LINAC; the head of the bunch is on the left.
    Fig. 17. 700 pC-bunch longitudinal phase space imaged on a YAG screen placed in the energy spectrometer at the end of the LINAC; the head of the bunch is on the left.
    Time-sliced current (red line) and energy spread (blue line) along the bunch obtained from the longitudinal phase space reported in Figure 6.1, relative to a 700 pC bunch. The head of the bunch is on the left.
    Fig. 18. Time-sliced current (red line) and energy spread (blue line) along the bunch obtained from the longitudinal phase space reported in Figure 6.1, relative to a 700 pC bunch. The head of the bunch is on the left.
    Mario Ferianis, Enrico Allaria, Eugenio Ferrari, Giulio Gaio, Giuseppe Penco, Fabio Rossi, Marco Veronese. How the optical timing system, the longitudinal diagnostics and the associated feedback systems provide femtosecond stable operation at the FERMI free electron laser[J]. High Power Laser Science and Engineering, 2016, 4(2): 02000e13
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