Dark current measurement at KEK M. Gerbaux, S. Döbert, T. Higo, S. Matsumoto, K. Yokoyama.

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Presentation transcript:

Dark current measurement at KEK M. Gerbaux, S. Döbert, T. Higo, S. Matsumoto, K. Yokoyama

Courtesy of T. Higo FC-Mid FC-UP FC-DN Magnet Accelerating structure (T18) 75cm 195cm FC-DNFC-UPFC-MidAM Experimental setup Spectrometer FC

Field enhancement factor measurement

pA fluctuations Data manually recorded during a very stable running period at (64.0  0.3) MW Input power fluctuation < 0.5 % Sampling rate ≈ 1.2 Hz

Dark current spectra measurement Pulse length : 252 ns Horizontal error bars : spectrometer resolution (Δslit/ρ) Vertical error bars : pA-meter fluctuations

Dark current spectra measurement Pulse length : 252 ns Always the same low-energy cut off (≈3.5 MeV)  low energy e - lost in the pipe ? Spectrum maximum around 5 MeV Often exhibits a double peak structure that tends to smooth while decreasing the gradient (  dark current originating mainly from 2 cells at high power ?).

T18_VG2.4_Disk_#2 Dark current spectra measured 18 June 2009 Dependence on powerDependence on width Higo Courtesy of T. Higo 64 MW  108 MV/m 55 MW  100 MV/m 70 MW  113 MV/m

Conclusion Nice test bench, very stable running which makes the measurements easy. An automation of the pA-meter read-out would make the measurement even easier and more precise. Change in the spectra shape since March to be investigated. Possible measurement of the dark current spectrum upstream ?

La réserve du chef

Dark current spectra measurement Pulse length : 252 ns

Courtesy of Toshi Higo FC-Mid FC-UP FC-DN Magnet Accelerating structure (T18) 75cm 195cm FC-DNFC-UPFC-MidAM Experimental setup Spectrometer FC Acoustic sensors (1 / cell)