Title: PowerPoint Prsentation des FZ Rossendorf
1Status of the Superconducting RF Photo-injector
Development
Jochen Teichert for the BESSY, DESY, MBI, FZD
collaboration Forschungszentrum
Dresden-Rossendorf Institut für
Strahlenphysik Strahlungsquelle ELBE PF 510119,
01314 Dresden J.Teichert_at_fzd.de
2Outline
- Introduction
- Application Parameters
- Photocathode
- Niobium Cavity
- Cryomodude
- Emittance Compensation
- Laser Diagnostic Beamline
3Introduction Radiation Source ELBE
- 40 MeV, 1 mA CW superconducting linac
- thermionic injector (250 kV DC), pulse frequency
of 13 MHz (260, 26, MHz)
4Introduction Superconducting RF Photoinjector
- Advantage
- low emittance like NC RF photoinjector high
average current (CW) -
- Use at ELBE
- - high charge (1 nC) high current for neutron
physics - - improvement of beam quality for FELs , etc.
- - future laser acceleration, Compton x-ray
source, ERL - Prototype test bench for future use at other
accelerators
5Introduction SRF Gun Parameters
6Introduction
Specific SRF Photoinjector Problems and Open
Questions
- Cavity contamination by particles sputtered from
cathode (fast Q degradation, low gradient).
- Operation of the photo cathode itself at
- cryogenic temperature.
- Specific geometry of the SC cavity (cathode
- insert).Can we reach the high gradient?
- Its not possible to do the emittance
compensation - like in a NC RF gun.
7Photo Cathode NC Cathode in SC Cavity
- Photocathodes ?
- - superconducting
- Nb, Pb
- outside
- Peking Univ.
- DC-SRF gun
- Cs2Te
- highest currents
- diamond
- amplifier
successful Rossendorf ½ - cell gun with NC
cathode D. Janssen et al., NIM-A, Vol.
507(2003)314
- Heat input 5 W
dielectric loss 15 W laser power
1 W - isolated from Nb cavity - liquid N2
cooling - SC Nb choke filter prevents rf flow
8Photo Cathode Cooling System
LN2 reservoir
cathode cooler
cathode
Test bench for thermal conduction measurements,
with electrical heater 20 W - about 40 deg
temperature increase at cathode - delivers 20 mW
radiation power to cavity
9Photo Cathode Cs2Te layer deposition
- New clean room (Class 1000)
- Ultra high vacuum (P lt 10-9 mbar )
- 4 evaporators for Cs Te
- 2 deposition rate sensors
- Measurement of Q.E.
- 262nm laser
- Q.E. during deposition
- life time, Q.E. distribution scan
- Controlled by computer
10Photo Cathode Exchange and Storage
11Cavity - Design
Nb RRR 300 cavity Eacc 25 MV/m in TESLA cells,
Q01x1010 (TESLA 500 specification) 110 mT
maximum magnetic surface field Epeak (TESLA
cells) 50 MV/m Epeak (half-cell) 30
MV/m Ecathode 20 MV/m (retreated cathode)
12Cavity Treatment
Cavity from ACCEL
- RF measurements, mechanical inspection, warm
tuning - Chemical etching inside (BCP 100 µm clean
water rinsing) - Chemical etching outside (gt20 µm clean water
rinsing) - Annealing and H2 outgasing in UHV oven at 800 C
- Warm tuning
- Chemical etching inside (final BCP 20 µm
clean water rinsing) - Drying in class 10 clean room air 12 h
- Assembly of auxiliaries
- Vacuum leak check
- High pressure rinsing
- Drying in class 10 clean room air 12 h
- Installation of antenna for vertical RF test
- RF Measurement _at_ 1.8 K
Preparation for vertical test
13Cavity Vertical Tests
Tests in the vertical cryostat (1.8 K) at DESY
14Cavity Treatment Vertical Tests
4th vertical test measurement of the 4 modes
electric axis field Ez of the for modes
performance limit comes from half -cell
15Cavity Treatment
He Tank welding final preparation _at_ ACCEL
- Helium tank welding
- Field profile measurments
- Vacuum leak checks
- Chemical etching inside (final BCP 20 µm
clean water rinsing) - Drying in class 10 clean room air 12 h
- Assembly of auxiliaries
- Vacuum leak check
- High pressure rinsing
- Drying in class 10 clean room air 12 h
- Vacuum leak check
- To Rossendorf for cryomodule assembly
16Cryomodule test assembly N2 cooldown (Nov. 06)
Cavity alignment test in April 2007
17Emittance Compensation
Studies with - retracted cathode - shaped
cathode - downstream solenoid field later TE
mode in cavity (JanssenVolkov)
details in the talk of Friedrich Staufenbiel
18 Laser System
- 500 kHz laser for High-charge mode
- Max. frequency 0.5 MHz
- Lower frequencies for alignment
- Pulse duration 1215 ps
- Laser material NdYLF, pumped by 8 fiber-coupled
diodes - Optical layout
- Oscillator (13 MHz)
- Regenerative amplifier
- Short-pulse laser for 13 MHz
- Frequency 13 MHz only
- Mechanical chopper to reduce this frequency
- Expected pulse duration 2 ps (UV)
- Laser material YbKGW or YbYAG
- Layout Power Oscillator, Additive-pulse
modelocked
Developed by MBI Berlin, see talk of Ingo Will
19 Diagnostics Beamline
Developed by BESSY Berlin, Test installation on
the roof of the ELBE cave
20Installation Commissioning
- Just finished
- clean room assembling of main coupler/
- pickups / flanges / both cavity tuners
- adjust choke filter and pre-stressing
- of the tuners by measuring
- passband frequencies
- HOM tuning to suppress out coupling
- of fundamental mode
21Installation Commissioning
- Next
- Assembly of the cryomdule
- Cleaning and white assembly
- of cathode transfer system
- Delivery installation of the
- 500 kHz laser system
- Installation of cryomodule
- transfersystem in the next
- ELBE shutdown in June/July
- -Installation of diagnostics beamline
- in the autumn ELBE shutdown
22Summary
- A SRF photoinjector will be installed at the
ELBE linac - in summer 2007 for 1 mA cw operation
- It will improve the beam quality for users
- (higher bunch charge, lower transverse
emittance) - It will be a test bench for SRF injector studies
- In the SRF gun cavity design, cleaning and
clean room handling - should be better considered
-
23Thank you for your attention
Collaboration BESSY, Berlin DESY, Hamburg
Zeuthen Max-Born-Institut, Berlin TJNAF, Newport
News University of Peking BINP, Novosibirsk CERN,
Geneva INFN, Frascati CCLRC Daresbury ACCEL GmbH,
Bergisch Gladbach Technische Universität
Dresden IfE-Automatisierung GmbH,
Dresden Ingenieurkontor Stephan, Dresden
The ELBE crew (in the Radebeul vineyards, near
Dresden)
Acknowledgements We acknowledge the support of
the European Community-Research Infrastructure
Activity under the FP6 Structuring the European
Research Area programme (CARE, contract number
RII3-CT-2003-506395) and the support of the
German Federal Ministry of Education and
Research grant 05 ES4BR1/8.
24Appendix
25Appendix