j. teichert, a. büchner, h. büttig, f. gabriel, p. … 1 radiation source elbe mitglied der...
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17.03.20051
Radiation Source ELBE
Mitglied der Leibniz-GemeinschaftJ. Teichert
Status of superconducting module developmentsuitable for cw operation: ELBE cryostats
J. Teichert, A. Büchner, H. Büttig, F. Gabriel, P. Michel, K. Möller, U. Lehnert, Ch. Schneider,
J. Stephan, A. Winter Forschungszentrum Rossendorf
Zentralabteilung Strahlungsquelle ELBEPF 510119, 01314 [email protected]
Radiation Source ELBE
Mitglied der Leibniz-GemeinschaftJ. Teichert
The radiation source ELBE
MeV Brems-strahlung 10-100 keV
Channeling
FEL 1: 3-22 µm
Neutrons
Positrons
FEL 2: 10-150 µm
KlystronsAcceleratorelectronics
FEL user labs
• First beam in April 2001• Nuclear physics experiments are running since January 2002• Channeling radiation since September 2003• FEL 1 since May 2004 • Second Cryomodule since February 2005
17.03.20053
Radiation Source ELBE
Mitglied der Leibniz-GemeinschaftJ. Teichert
ELBE radio-frequency electron accelerator
Accelerator parameters:40 MeV cw-operation2 modules, each 2 TESLA cavitiesrf frequency: 1.3 GHz10 MeV & 10 kW rf power per cavity average beam current: ≤ 1 mAbunch charge: ≤ 77 pCpulse frequency: 260, 26 … 0.01 MHzvariable pulse trains
74.0,1,250 =βmAkeV7 MeV @ 10 MV/m foroptimum beam capture
17.03.20054
Radiation Source ELBE
Mitglied der Leibniz-GemeinschaftJ. Teichert
ELBE cryomodule design
17.03.20056
Radiation Source ELBE
Mitglied der Leibniz-GemeinschaftJ. Teichert
ELBE cryogenics
Helium plant 220 W @ 1.8 Kp control with cold compressors CC1, CC2
Cryostat pot heater
T1 T2 T3
CC1CC2
C1-2
VSC
1-3
cryostat
Coldbox
Byp
ass
1.8K 16 mbar
4K 1bar
14K 0.1 bar
293K
12
bar
Now: stable operation of the two cryomodules
Problems at beginning:- pressure instability- interference between
p and He level (valve) controlSolutions:
- increased He flow in CC via bypass,- level control with heater in modulesfeed-forward control from gradients
17.03.20057
Radiation Source ELBE
Mitglied der Leibniz-GemeinschaftJ. Teichert
ELBE tuning system
Tuning rangemechanical: ±0.37 mmfrequency: ± 116 kHz
Tuning resolutionmechanical: 3 nmfrequency: 1 Hz
Transfer156 nm/motor turn2.3 steps/nm
Maximum load: 3000 N
“slow” spindle/lever system due to cw fast Lorentz-force compensation not needed
Lorentz-force detuning: 50 Hz @ 7 MV/mcompensation “by hand” during gradient ramp up
17.03.20058
Radiation Source ELBE
Mitglied der Leibniz-GemeinschaftJ. Teichert
RF control
10 kW CPI VKL 7811 ST klystron for each cavity, in cw operation analog low-level rf control, phase & amplitude loop
separate for each cavity:- gradient- phase- power meas. values(tuning)
Safety systemGradient loop error:- detuned cavities- beam loading etc.
microphonicsopen loop: 0.97 deg rmsclosed loop: 0.02 deg rms
17.03.20059
Radiation Source ELBE
Mitglied der Leibniz-GemeinschaftJ. Teichert
ELBE rf power coupler
LN port
coldwindow
Cu antenna
contactsprings
overheated incoupler testswith 8 kW fullreflection
Coupler design for 10 kW cwusing the TTF conical insulator,T.Kimura/HEPL-Stanford & J.Stephan
three-stub waveguide tuner for BW adjustment
RT planar window in waveguideREXOLITHEposition at E-field waist
conical cold window at 70 Kceramics
Coupling is matched for 1 mAbeam current at 10 MV/m
BW = 114 HzQL= 1.2 x 107
17.03.200512
Radiation Source ELBE
Mitglied der Leibniz-GemeinschaftJ. Teichert
ELBE module - cavity properties
Idealkurve einfügen
cavity operation at ELBE: Gradient limit due to strong field emission
ELBE cavities vertical test at DESY before tank welding etc.:Q0 = 2 x 1010, Eacc = 15... 25 MV/m
TESLA cavities
Pdi
ss/ W
Eacc / MVm-1
Reason: welding, assembling, storage, couplers?
17.03.200513
Radiation Source ELBE
Mitglied der Leibniz-GemeinschaftJ. Teichert
ELBE module – energy drift
We observed an energy growth with time after switching ongradient set values and pick-up signals are constant
20 40 60 80 100 120 140 160 180 200 220 240 260
7,3
7,4
7,5
7,6
7,7
7,8
7,9
8,0
8,1
8,2
Energy drift of cavity RC01 after switch on
RC11 off RC11 on (8 MV/m)
beam
ene
rgy
/ MeV
time / min
0 50 100 150 200 250 300
950
1000
1050
1100
1150
1200
1250
1300
energy drift after rf on cavity RC01
slope: 1.1 W/min
rf po
wer
(for
war
d) /
Wtime / min
the source is in the module, it is not rf control,temperature increase with the same time scale,connected with cw operation of TESLA cavities at ELBE?
17.03.200514
Radiation Source ELBE
Mitglied der Leibniz-GemeinschaftJ. Teichert
ELBE cryomodule - summary
• ELBE cryomodules are suitable for cw-operation @ 10 MV/m & 1 mAmost of module parameters better/equal to design specificationscommon He pressure control with cold compressors,separate He level control (heater) in each module,analog phase and amplitude rf control for each cavity,sophisticated coupler/window diagnostics,
• Higher gradients:1. limit due to field emission in cavities, difficult to reach 20 MeV,
extended quality management for next module2. At ELBE: capacity limit of the cryogenic plant,
• Higher current (rf power):1 mA (10 kW) seems near to the limit of the rf power couplers,
• Energy drift:cw-operation causes 1 MeV energy drift within first hours,source is in module (temperature effect) , no rf control
17.03.200515
Radiation Source ELBE
Mitglied der Leibniz-GemeinschaftJ. Teichert
Acknowledgment
FZ Rossendorf:Module design and assembling:J. Stephan, R. Schlenk, B. Wustmann, A. Winter, M. Freitag, A. Noack, B. ReppeLL RF control: F.GabrielRF and couplers: H. Büttig, R. Schurig, A. BüchnerDiagnostics: D. Pröhl, F. Herbrand, R. Jainsch, J. Claussner, A. SchamlottCryogenic system: Ch. Schneider, Ch. Haberstroh, B. HartmannOperation: U. Lehnert, P. Michel, P. Evtoushenko, J. Voigtländer
DESY Hamburg (A. Matheisen ...), HEPL Stanford, ACCEL, TU Dresden