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ESRF interest & commitment to (ultra-) fast science with X-rays Kees Scheidt Diagnostics group, Machine division. ESRF interest & commitment to (ultra-) fast science with X-rays. Thorough tests of the quasi-isochronous Storage Ring in 1995 :
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ESRF interest & commitment to (ultra-) fast science with X-rays Kees Scheidt Diagnostics group, Machine division
ESRF interest & commitment to (ultra-) fast science with X-rays • Thorough tests of the quasi-isochronous Storage Ring in 1995 : • inadequate since incompatible with high-intensity demands • so : typical bunch length remains ~100ps (fwhm) at 5mA single bunch • Operation of various filling patterns to satisfy the whole user • community, including specialized time-resolved beamlines 3) Development of X-ray time resolved detector for sub-pico second time resolved diffraction experiments
ultra-fast X-ray diffraction experiments that use the pump-probe technique with : a 100femtoSec Laser light pump pulse and a 100picoSec X-ray probe pulse the ultimate time resolution depends on : 1) intrinsic time resolution of the Streak Camera for X-rays 2) the quality of synchronization Objective : 1) sub-picoSec time resolution 2) high quality data by accumulation over many shots
the Streak-Tube : improved version of commercial model (Photonis)
5mm 10 picosec
Critical laser issues : • Amplitude stability • Contrast (or pre-pulse • energy variations)
Sensitivity for hard X-rays is low due to poor DQE of photo-cathodes decreasing DQE for increasing Energy best : Cesium-Iodide (100) low : Potassium-Iodide (10) Potassium-Bromide poor : Gold (1)
Conclusion (1): • Optical synchronization by a GaAs photo-switch between a • femtosec-laser and a Streak-Camera attains values <100fs when : • Laser energy >25uJ per pulse • Laser stability 0.25% rms • Laser contrast >104 In these conditions (obtained after delicate adjustments) the time resolution of the system in accumulation mode is determined by the tube’s intrinsic time resolution, at ~500fs fwhm for UV light The exact time resolution for hard X-rays was never assessed since various attempts to produce a sub-pico sec event in an appropriate Pump-Probe experiments were without success.
Conclusion (2): • The accumulating Jitter-Free X-ray streak camera • for sub-pico sec pump-probe experiments was Not a scientific success • due to : • The difficulty of conceiving an appropriate experiment • The required delicate adjustments on laser, photo-switch • and streak-camera making it not user-friendly • The particular limitations of a Streak-Tube detector: • No real space-dimension • b) Low sensitive photo-cathode material