mitglied der helmholtz-gemeinschaft jochen teichert [email protected] hzdr wp10 srf task 7 scrf...
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Mitglied der Helmholtz-GemeinschaftJochen Teichert [email protected] www.hzdr.de HZDR
WP10 SRFTask 7 SCRF Gun at ELBE
Subtask 7.3
Evaluation of Critical R&D Issues of SRF Guns
J. Teichert, A. Arnold, T. Kamps, P. Murcek, R. NietubycJ. Rudolph, S. Schubert
EuCard - SRF2011Institute de Physique Nucleaire d´Orsay
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Use of semiconductor photo cathodes like Cs2Te requires a permanentvacuum of 10-9 mbar during preparation, transport, storage and operation
Ø10 mm Cs2Tecone forpositioning &thermal contact
pressure springbayonet fixing
this cathode has until April 2011: 950 h beam time 35 C extracted charge
FLASH/DESYProc. EPAC2006
Subtask 7.3 - Photocathodes
cathode #250310Mo: 25/5/2010 – in use
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Subtask 7.3 - Photocathodes
Quantum efficiency measurement, cathode #250310Mo, April 2011, in SRF gun
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Subtask 7.3 - Photocathodes
Dark current measured in Faraday cup 0.5 m in front of gunwith pulsed RF, peak field until 21.6 MV/m
8 MV/m acc. Gradient= 21.6 MV/m peak field= 4 MeV kinetic energy
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dark current picture on YAG screen
calculation of V. Volkov (HZB/BINP)
emission
point escape
E/Ebeam
calculation measured
1 yes 75 % 90-95 %
2 no 15 %
3 no 20 %
4 yes 60 % 81-87 %
5 no 45 %
6 yes 30 %
7 no 75 %
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Subtask 7.3 - Photocathodes
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• SRF Gun cavity performanceMax. 16 MV/m peak field= 6 MV/m acc. gradient= 3 MeV beam energy
Subtask 7.3 - Photocathodes
• Measurement of Q0 versus Epeak since 2007 no degradation due to NC photo cathodes
• excellent life time of photo cathodes in SRF gun
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Subtask 7.3 - Photocathodes
Test of superconducting Pb photo cathodes in the ELBE SRF gunActivity started after discussion at the Daresbury meeting April 2010J. Teichert (HZDR), S. Schubert, T. Kamps (HZB), R. Nietubyc (IPJ Swierk)
- Fabrication of Niobium plugs at FZD (3 samples) and polishing, - Inspection at HZB and polishing of one plug (34) @ Pilz Optics- deposition of Pb layer at IPJ - Inspection at HZB – with SEM/EDX for layer homogeneity and pollution- QE measurements and QE maps at HZDR (in preparation system)- Test of Pb cathodes in SRF gun at HZDR- Inspection after use at HZB
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Subtask 7.3 - Photocathodes
SEM images of Pb layer on cathode 32
SEM/EDX studies by S. Schubert, HZB
Nb plug
Pb layer
Status:
next: load into the transport chamber with the next set of photo cathodes
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beam loss > 2.5 % in dogleg
(beam loss monitor)
Subtask 7.3 Achromatic beam transport and phase matching
Transmission measurement
Maximum bunch charge injectedand accelerated in ELBE: 120 pC @ 50 kHz (6 µA);with 100% transmission: 60 pC @ 125 kHz
Dogleg acceptance needs low energy spread,
Correlated energy spread can becompensated in module 1
Optimum Gun Parameters?
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Subtask 7.3 Longitudinal phase space measurement
• Method of measurement: phase scan technique
C2 phase variation energy spectrum
11 12
12 22
11
22
( )
( )
t
E
rms bunch length ps
rms energy spread keV
longitudinal beam ellipse
2 2(1) (0) TC CR R
cavity transport matrix
22 2
1 0
sin( ) 1CRF C C
RV
:
cos( )2 2
cavity energy boost
VC C
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Longitudinal phase space measurement
2 222 12 2 2 11 2 2(1) (0) 2 (0) sin( ) (0)( sin( ))E C C C CV V
from parabola fit
rms longitudinal emittance
211 22 12long
bunch length
correlation
energy width
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10°5°-7° 0°
30°15° 25°20°
Subtask 7.3 Longitudinal phase space measurement
Beam energy (pc): 18.6 MeV, Gradient C1: 6.8 MV/m, gradient C: 8.4 MV/mGun gradient: 6.0 MV/m, Ekin = 3 MeVReprate: 125 kHz CW, 1.3 µA average current, bunch charge: 10 pC
Phase space measured at cavity C2 as function of SRF gun laser phase
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Subtask 7.3 Longitudinal phase space measurement
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14Phys. Rev. ST Accel. Beams 14, 024801 (2011)
Subtask 7.3 publications
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Subtask 7.3
Summary
• Demonstration of succesfull operation and long lifetime of normal conducting photo cathodes in SC RF guns• First successful measurements using the ELBE accelerator - slice emittance measurements - longitudinal phase space• Start the collaboration work in photo cathodes with Pb-cathodes comparison of results exchange for characterization standard design for SRF gun cathodes at HZB and HZDR
• Next work - continuation of dark current studies - after 13 MHz laser upgrade: high average current operation (1mA) - publication