Prospects for developing new tubes

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Presentation transcript:

Prospects for developing new tubes I. Syratchev, CERN

Theme: RF power sources for the future ‘Big’ science. (It should become ‘Big’, when the number of sources exceeds few hundred) ESS. Conventional single beam klystrons Mostly 704 MHz, ~3msec, 14 Hz. ~50 kW average CLIC MBK (specifications). Frequency: 1.0 GHz Peak RF power: 20 MW Efficiency: >70% Pulse length: up to 150 sec Rep. rate: 50 Hz P average: up to 150 kW ILC MBK (demonstrated). Frequency: 1.3 GHz Peak RF power: 10 MW Efficiency: ~69% Pulse length: up to 1.50 msec Rep. rate: 10 Hz P average: ~150 kW The L-band klystron development is amongst the most strong synergies between CLIC and ILC.

Peak power Efficiency Cost (per MW) Life time What kind of performance we need to improve ? Targeting the higher voltages brings many benefits. But for the long pulses it soon will be limited at about 160-180 kV. The most efficient way out is to use Multi-Beam technology.  Current density New cathode topology/technology CLIC MBK#6 The subjects for the new tubes development  Beam power  High voltage (space charge limited) RF breakdown limited Klystron cluster  Perveance  High voltage (space charge limited) RF circuit topology Depressed collector PPM focusing /SC solenoid Modulator  Peak power CLIC MBK#6 Max. 180 kV  High voltage (space charge limited) Similar scaling for modulator cost We need all of it ! Peak power Efficiency Cost (per MW) Life time

State of art: L-band 10 MW MBK klystrons for ILC. In terms of achieved efficiency at 10 MW peak RF power level, the existing MBK klystrons provides values very close to the 70%, as is specified in CLIC CDR. Minimizing the cost and increasing peak RF power still remain for CLIC as an important objective towards TDR phase

Extending technology: L-band 20 MW MBK klystron for CLIC. We made a study which indicates that the scaling of existing tubes down in frequency may end up in rather powerful (>20 MW) and efficient (>70%) MBK. Currently we are in process of preparing “call for tender” for fabrication of such a tube.

What else people are working at? Cluster X-band (SLAC) Super MBK (KEK) http://accelconf.web.cern.ch/accelconf/pac2009/papers/tu5pfp093.pdf http://indico.cern.ch/confRegistrantsDisplay.py/list?confId=204269 PBGK ABK (CCR) SBK (SLAC) http://www.osti.gov/bridge/servlets/purl/1045838/1045838.pdf http://accelconf.web.cern.ch/accelconf/IPAC10/papers/thpeb066.pdf None of them have clear advantages compared to the existing MBK technology.

Doubly Convergent Multiple-Beam Electron Guns New cathode topology Doubly Convergent Multiple-Beam Electron Guns The multiple beam guns with two stages of compression opens a wide range of opportunities. Even existing MBK designs can be improved in terms of peak power, beam voltage, efficiency and life time. http://ieeexplore.ieee.org/stamp/stamp.jsp?tp=&arnumber=4283375 http://ieeexplore.ieee.org/stamp/stamp.jsp?tp=&arnumber=5452975

Planar RF topology combined with doubly convergent gun. Planar MBK with ‘pencil’ beams. Build and tested in 1961 New guns with double compression, being combined with planar technology might be an attractive solution. It allows integration of the individual (for each beam) drift channels. The use of this technology naturally suggests application of PPM focusing and relatively ‘simple’ fabrication processes, thus substantial cost reduction: http://ieeexplore.ieee.org/stamp/stamp.jsp?tp=&arnumber=1473207&tag=1 ILC–type MBK Planar MBK

Efficiency and klystron RF circuit design Harmonic cavities New method of increasing efficiency in klystrons has been developed and tested. Method is based on the velocity re-distribution of electrons in a bunch prior to its deceleration in the output cavity. IVEC 2013 One also may expect, that spent beam velocity spread can also be reduced, thus depressed collector (if used) will require less stages. Implementation of higher (2nd, 3rd ) harmonic cavities is a well established technique which allows to increase efficiency and reduce the cost (length) of the tube. (see also presentation by Chiara Marrelli)

Efficiency and depressed collector IVEC 2013 A pulsed depressed collector which uses a novel feed-forward energy recovery scheme. It also allows to recover the rise and fall time of the modulator pulse (opens a potential to reduce modulator price). Simulated with 2D-PIC code efficiency using a five-stage, un-optimized collector was as high as 55%.

Predicted Performance 704 MHz MBIOT vs. MBK Predicted Performance Output Power, MW 1.0 1.5 Frequency, MHz 704 Beam Voltage, kV 50 113 51 43.3 Beam Current, A 32 20.8 27.6 32.4 Efficiency, % >65 >71 >73 Gain, dB 22 46 Bandwidth (1dB),MHz 3 4 >4 Hypothetical 6 beams MBK (microperveance / beam=0.4) Hypothetical 12 beams Planar MBK (microperveance / beam=0.3) + R&D VHP-8330A HOM IOT Objectively, MBK performance at this RF power level and frequency can be even better, compared to MBIOT. It does not require dedicated R&D (low risk). It provides high power gain (driver cost) But it might be more expensive. Scaled VKP-8291 MBIOT

Given enough attention and resources, the battle for efficiency (more general for PECL) can gain enough momentum, so that in 5 years we will operate MW(s) RF power stations with overall efficiency above 70%! John Lennon