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Degradation and Recovery of Cavity Performance

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Presentation on theme: "Degradation and Recovery of Cavity Performance"— Presentation transcript:

1 Degradation and Recovery of Cavity Performance
in compact-ERL Injector Cryomodule at KEK Eiji Kako (KEK, Japan) 2012, April 2012, Sept. Eiji Kako (KEK, Japan) Dirty SRF WS at HZB, Sept. 14, 2017

2 Injector-Linac section of compact-ERL
CW RF Power Source Injector-Linac Section Injector Cryomodule Eiji Kako (KEK, Japan) Dirty SRF WS at HZB, Sept. 14, 2017

3 History of cool-down cycles in injector cryomodule
~0.3 mA Stable beam operation ~10 mA ~100 mA Observation of severe x-ray radiation ~1 mA Trial of high RF power pulsed conditioning ~40 pC Eiji Kako (KEK, Japan) Dirty SRF WS at HZB, Sept. 14, 2017

4 Stable beam operation at Vc = 5 MV in May-July, 2013
In this operation, cryogenic system was stopped during night/week-end.  natural warm-up. Presently, only 2K pumping system was stopped during night/week-end.  keep at 4.2 K. Specification: ave. Eacc = 7 MV/m total Vc = 5 MV Eiji Kako (KEK, Japan) Dirty SRF WS at HZB, Sept. 14, 2017

5 Change of x-ray radiation levels in 2013 - 2017
Return to previous level after warm-up Severe increase No change after warm-up Gradual increase after pulsed RF conditioning after pulsed RF conditioning Initial level Eiji Kako (KEK, Japan) Dirty SRF WS at HZB, Sept. 14, 2017

6 Change of x-ray radiation levels in three cavities
DC-Gun side (clean environment) (by individual cavity operation) Photo cathode of Gun Faraday Cup Gate Valve Stopped at moving contamination after pulsed RF conditioning Acceleration of F.E. electrons by Cavity-1 moving contamination Acceleration of F.E. electrons by Cavity-2 after pulsed RF conditioning Main sources of field emission locates in Cavity-3 severe degradation Merger side (dirty environment) degradation start after pulsed RF conditioning Eiji Kako (KEK, Japan) Dirty SRF WS at HZB, Sept. 14, 2017

7 Unexpected vacuum discharge phenomenon (1)
Many bursts of vacuum pressure Gradual increase of x-ray radiation level Vacuum discharge caused by charging-up of Faraday-cup due to field emitted electrons come from injector cavities. Eiji Kako (KEK, Japan) Dirty SRF WS at HZB, Sept. 14, 2017

8 Unexpected vacuum discharge phenomenon (2)
Field emitted electrons from Cavity-1 hit the photocathode. Then, secondary electrons extracted by applied DC voltage of 400 kV, and furtherly accelerated by injector cavity. Finally, high energy electrons collided with a screen monitor and radiate x-rays. Eiji Kako (KEK, Japan) Dirty SRF WS at HZB, Sept. 14, 2017

9 Quench detection : QL-interlock < 0.8 x QL (normal)
High RF power pulsed conditioning CW 25 kW Kly. CW 300 kW Klystron Quench detection : QL-interlock < 0.8 x QL (normal) Eiji Kako (KEK, Japan) Dirty SRF WS at HZB, Sept. 14, 2017

10 Performance recovery by pulsed RF conditioning
Vc= 5MV Vc= 5MV Vc= 3MV Vc= 3MV before before after after Vc= 5MV before Vc= 5MV before Vc= 3MV Vc= 3MV after after Heat load at 2 K was dramatically reduced at 5 MV. Eiji Kako (KEK, Japan) Dirty SRF WS at HZB, Sept. 14, 2017


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