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Fig. 1. Schematic drawing of SwissFEL. The picture, slightly modified, was taken from [7]. The total length of this machine is 740 m. The photocathode laser beam, injected at the left, delivers sub-10 ps pulses on a CsTe2 cathode. The FEL emits fs-scale x-ray pulses at the end. Their drift and jitter in space, energy and time has to be minimized.

Journal: Optics Express

Article Title: Arrival time fluctuation of the SwissFEL photocathode laser: characterization by a single color balanced cross correlator

doi: 10.1364/oe.444679

Figure Lengend Snippet: Fig. 1. Schematic drawing of SwissFEL. The picture, slightly modified, was taken from [7]. The total length of this machine is 740 m. The photocathode laser beam, injected at the left, delivers sub-10 ps pulses on a CsTe2 cathode. The FEL emits fs-scale x-ray pulses at the end. Their drift and jitter in space, energy and time has to be minimized.

Article Snippet: This can cause the amplifier laser jitter and drift easily exceed that of the oscillator whereas within the titanium sapphire laser user community the contribution of drift and jitter from the amplifier is usually neglected (for comparison: drift and jitter between oscillator and amplifier of the SwissFEL experimental titanium sapphire lasers (oscillator: Vitara, amplifier: Legend, both from Coherent Inc., parameters: repetition rate: 100 Hz, max. energy/pulse: 27 mJ, pulse width: 30 fs, one regenerative amplifier (12 passes), two one pass post-amplifiers [12]) amount to 0.8 fs/mbar/m (drift) and 5 fs rms (jitter)).

Techniques: Modification, Injection