cepc rf sources system - ias.ust.hk
TRANSCRIPT
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CEPC RF Sources System
Zusheng ZHOU(周祖圣)
Institute of High Energy PhysicsJan. 25, 2017
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Contents
■Design proposal■R&D Progress■Summary
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Design proposal
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Future large accelerators
FCCee, CW, 800MHz, Prf=110MW
ILC, Pulse, 1.3GHz, Prf=88MW
CLIC, Pulse, 1.0GHz, Prf=180MW
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Future large accelerators
CEPC-SppC,CW,650MHz,Prf=100MW
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Current situationFor future large accelerators, just like ILC, FCC and CEPC. It’s
beam power is very high, so high efficiency RF source is muchmore important.
Tetrodes IOTs Conventional klystrons
Solid State PA Magnetrons
DC – 400 MHz (200 – 1500) MHz 300 MHz – 1 GHz DC – 20 GHz GHz range
1 MW 1.2 MW 1.5 MW < 1MW
85% - 90% (class C) 70% 50% 60% 90%
Remark Oscillator, not amplifier!
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Current situationFor future large accelerators, just like ILC, FCC and CEPC. It’s
beam power is very high, so high efficiency RF source is muchmore important.
Tetrodes IOTs Conventional klystrons
Solid State PA Magnetrons
DC – 400 MHz (200 – 1500) MHz 300 MHz – 1 GHz DC – 20 GHz GHz range
1 MW 1.2 MW 1.5 MW < 1MW
85% - 90% (class C) 70% 50% 60% 90%
Remark Oscillator, not amplifier!
RF sources for accelerator are IOT, klystron and solid state amplifier. From cost, frequency limitation and power level, klystron is still the first choice.
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• 2014 saw a breakthrough in klystron theory:– 1981, “congregated bunch” was re-introduced [V.A. Kochetova, 1981]
(later electrons faster when entering the output cavity).
– 2014, “bunch core oscillations” was introduced [A. Yu. Baikov, et al.: “Simulation of conditions for the maximal efficiency of decimeter-wave klystrons”, Technical Physics, 2014]
(controlled periodic velocity modulation)
– 2013, BAC method was invented[I.A. Guzilov, O.Yu. Maslennikov, A.V. Konnov, “A way to increase the efficiency of klystrons”, IVEC 2013]
(Bunch, Align velocities, Collect outsiders)
• These method together promise a significant increase in klystron efficiency(approaching 90%)
• A international collaboration has started. HEIKA – “High EfficiencyInternational Klystron Activity” is evaluating and implementing this“breakthrough”.
Current situation
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Considering klystron lifetime and powerredundancy, 2 cavities will be powered with aCW klystron capable to deliver more than 800kW.
1 klystron power 2 cavities
Parameters Value
Operation frequency 650MHz+/-0.5MHz
RF input power (kW) 280 CW(250)
RF source number 160
Klystron output power (kW) 800 CW
CEPC Collider RF sourcesBaseline
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Klystron key design parameters
Parameters Now FutureCentre frequency (MHz) 650+/-0.5 650+/-0.5
Output power (kW) 800 800Beam voltage (kV) 80 70Beam current (A) 16 15
Efficiency (%) 65 80
CEPC Collider RF sources
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Klystron key design parameters
Parameters Now FutureCentre frequency (MHz) 650+/-0.5 650+/-0.5
Output power (kW) 800 800Beam voltage (kV) 80 70Beam current (A) 16 15
Efficiency (%) 65 80
How to do?
CEPC Collider RF sources
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Klystron key design parameters
Parameters Now FutureCentre frequency (MHz) 650+/-0.5 650+/-0.5
Output power (kW) 800 800Beam voltage (kV) 80 70Beam current (A) 16 15
Efficiency (%) 65 80
How to do?
There are some R&D work supported by IHEP innovation funds.
CEPC Collider RF sources
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R&D Progress
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Klystron Schedule and strategyBecause of klystron efficiency is more than 80%, in order to
fulfill this program, there may have following problems:1) No experience and no related infrastructure on this kind ofklystron;2) Design and simulation are not enough and matured;3) Let’s start from beam tester, classical design and currentlyprogressed design(higher efficiency design).
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Klystron Schedule and strategy(2)
(1) Beam tester
(2) #1 prototype
(3) #2 prototype
Merits• Saving the money• Saving the time• Possible to try 2 or 3
designs
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1.57E+03V/mm
Gun region beam trajectory simulation with Egun
-81.5kV 0kV
EGUN simulation result:
Area compression ratio : 4.4Perveance: 0.647μPCathode current density:0.39A/cm2~0.43A/cm2Max. electric field : 2.520kV/mm
Electrode E fied density optimization with Possion
-57kV 2.52E+03V/mm
Cathode current density
R&D-Electron gun
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DGUN simulation resultsDGUN simulation result :Beam Diameter=17.8mmCurrent=15.12 APerveance= 1.43 μA/V3/2
Vc =-81.5kV
VMA=-48.0kV
1.77 kV/mm
on Anode
3.94 kV/mm
on BFE
2.51 kV/mm
on M.Anode
54 mm35.6 mm
0
4
2
6
5 10 15 25 30 35
Cathode R(mm)
Cu
rre
nt
Den
sit
y
(mA
/mm
2)
20
R&D-Electron gun
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Beam Diameter=17.7mmCurrent=14.88 APerveance= 1.41 μA/V3/2
CST simulation results
R&D-Electron gun
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Type DGUN EGUN CST
Current(A) 15.12 14.88 14.88
Beam DIA(mm) 17.8 17.7 17.7
Perveance(μA/V3/2) 1.43 1.41 1.41
Simulation results comparison
Vc =-81.5kV, VMA=-48.0kV
R&D-Electron gun
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Amplitude of magnetic field Bz on axis
Simulation results comparison
R&D-Electron gun
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Ripple rate = 8.0%R&D-Beam trajectory
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R&D-Beam trajectory
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Gun assembly with Drift Tube and Collector
0 500 1000 1500 2000 2500 400035003000Z (mm)
Solenoid
R&D-Beam trajectory
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HV Gun Envelop for Electron Gun
R&D-Electron gun
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5 fundamental cavities and 1 2nd harmonic cavity, 1 d simulationresult shows 74.55% efficiency.
R&D-RF interaction
AJ disk design Mechanical design
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8 cavities and BAC method, 1 d simulation result shows 79.41%efficiency.
R&D-RF interaction
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8 cavities, BAC method and low pervence gun, 1 d simulationresult shows 85% efficiency.
R&D-RF interaction
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We are doing more simulations in detail using other 2d and 3dcodes. The final parameters of cavities will be given and then startto mechanical design with company engineers.
R&D-RF interaction
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Simulation and optimization
Window and coupler cooling system design
Window multipactoreffector analysis
Window coupler simulation and
mechanical design
High power test stand
construction
R&D-Output window
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multipactor effector simulation
99.5% Al2O3 and OFC multipactor effector
CST and MULTIPACT code simulation results
R&D-Output window
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Structure optimization
With 800kW power and 650MHzfrequency, S parameters and VSWRmeet demands.
R&D-Output window
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HFSS and CST electromagnet filed and thermal simulations
Electromagnet filed simulation
HFSS and CST simulations are in complete agreement
R&D-Output window
Thermal analysis simulation
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Collector shape and beam dissipation optimization
Analytic design Numerical design
Collector Length 2147mm 1912mm
Collector radius 210mm 210mm
Total Beam power 1231kW 1230kW
Capability of power density in collector 150W/cm2 150W/cm2
Max power density in collector 197W/cm2 207W/cm2
J collector optimization using universal beam spread curve collector optimization using EGUN code
Crosscheck of beam trajectory with EGUN and MAGIC
R&D-Collector
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Groove dimensions optimization
Groove number
Groove dimensions(a:b)
Total water flow rate
Water pressure loss for ideal smooth surface
180 1:2 1400kg/min 2.34E+4 Pa
Contour of temperature and water pressure loss
R&D-Collector
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Collector Thermal analysis
Groove structure for 2 meter tapered collector in Ansys-CFX
contour of temperature on inner surface of copper domain contour of temperature of water domain
R&D-Collector
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Geometry of collector tapered part
AB
CD
E
Section A B C D E
groove number 180 150 120 60 40
2030mm
Collector geometry of tapered part
R&D-Collector
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Final design
R&D-Collector
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IHEP is taking bids now.
R&D-Beam tester
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We form a joint institute with local government and Company:GLVAC Industrial Technology Research Institute of High PowerDevices.
R&D-Current status
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Summary The design of the electron gun and collector has been
completed;
RF Section for classical design klystron is completed;
Mechanical design for beam tester is also completed;
IHEP is taking bids for fabrication of beam tester;
Mechanical design for classical design klystron is about tobegin.
RF Section for high efficiency design klystron is almostcompleted.
Fabrication for high efficiency klystron will be discussed.
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Thanks for your attention!