Accelerating Cavities

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Accelerating Cavities for the Damping Ring (DR) Tetsuo ABE For KEKB RF/ARES Cavity Group (T. Abe, T. Kageyama, H. Sakai, Y. Takeuchi, and K. Yoshino) The 16 th KEKB Accelerator Review Meeting February 8, 2011

Old RF Model shown in the 15 th KEKB Accelerator Review Meeting, February 16 (2010) (Normal View) R Q Q V c 0 150 29000 (IACS90%) 0.5 MV Loss Factor : 1.9 [V/pC] (Transparent View) Bullet shaped HOM Absorbers (SiC; Hexoloy) Tuner Input Coupler (Used one from APS) SiC Duct (Cerasic B) Pumping Port Taper( 150< > 40) with L=400mm 1

[Basic Conditions] A) Frequency: 508.887MHz (= thefreq. of themr) B) Based on KEKB MR/ARES, but without S cav and C cav C) Connection to 40 beam ducts ( taper near the cavity) D) Max. Total Vc: 05 0.5 2MV Against microwave instabilities from CSR effects Should be larger enough than the current design value: 1.4MV [Main Topics] ving) (S Space conser (Changes after Feb. 2010) 1. 3 Cavities (max) with 0.7MV/cav in the RF section (~5m long) 2. SiC tiles for all the Higher Order Mode (HOM) dampers 3. Grooved Beam Pipe (GBP) made common between the neighboring cavities 4. Connection between the cavity and GBP 5. HOM Impedances for Coupled Bunch Instabilities (CBIs) 6. RF absorption power in each HOM damper 7. Coupled oscillations of the accelerating (ACC) mode 2

Specification of the Vc and Wall Loss of the DR Cavity Based on the results of the HPT of the ARES Prototype performed in the KEK/AR Tunnel (1997) Vc Wall Loss Wall Temperature [MV/cav] Power [kw] (calc.) [degc] KEKB Design 0.50 60 50 Max. Continuous o 070 0.70 133 74 Max. Instantaneous 0.82 193 94 (Appendix A) Note: The DR cavity has been designed with the same basic structure as the ARES/A-Cav on the basis of its successful experiences. (Appendix B) 3

New RF Model ver.2011 02 08 02 08 Pumping Ports 3 cavities with 0.7MV/cav GBP common between the neighboring i cavities HOM dampers with SiC tiles SiC tiles on the duct work similarly to SiC ducts. Loss Factor : 2.5 [V/pC] (Dimensions in mm) Tuner Input Couplers (from KEKB MR) Taper End SiC tiles 1100 72 400 Taper 30 Flange 300 256 200 Bellows Taper End 5324 2662 110 GV 4

Two Types of Components 1. Cavity 2. GBP with SiC tiles Connection: Welding for vacuum sealing RF shield inside We do not use flanges because of No space for bellows Non-circular duct (GBP) Thermal stress by the ACC mode 5

Connection between the Cavity and GBP A-Cav C-Cav S-Cav Lip welding for vacuum sealing, like: 5 cycles of Welding Cutting are possible. Vacuum Metal O or C ring 340mm between C-Cav and S-Cav of ARES Finger-type RF shield, like: Safe for low beam currents, such as 70mA 30mm in the flange for KEK/PF; Courtesy of T. Honda. 6

HOM Absorbers The basic HOM damped structure is the same as that of the KEKB-MR/ARES cavity, but the HOM absorbers are all SiC tiles: t20mm x 48 mm x 48mm. Bullet-shaped SiC absorbers used for the KEKB-MR/ARES SiC tiles used in the GBP of the KEKB-MR/ARES (Electric Field) SiC tiles are: - brazed on a copper plate. - water-cooled via the copper plate. Power Capability: ~1 kw/set (@1.3GHz) TM Mode TE Mode Absorbing both TM & TE modes 7

Longitudinal Impedance of the RF section: and CBI Estimated from Finite-Difference Time-Domain parallel computations of GdfidL with the PC cluster (256 cores & 512GB memory) CBI threshold for Total Vc: 1.4MV Growth Time > 20ms > 5ms (rad. damping time) 8

Transverse Impedances of the RF section: and CBI Estimated from Finite-Difference Time-Domain parallel computations of GdfidL with the PC cluster (256 cores & 512GB memory) (Tuner Position: 30mm inside) CBI threshold for Total Vc: 1.4MV Growth Time > 30ms > 10ms (rad. damping time) 9

Power of RF Absorption in Each Set of SiC Tiles HOM Power from the Long-Range Wakefield Estimated from the time-domain computation of GdfidL (smax=1000m) with the conditions: - Bunch charge: 8nC - Bunch length: 6mm Scalar sum over four bunches - Beam offset: 2mm (X,Y) ~15W ~15W ~14W ~58W ~19W ~58W 14W ~58W ~18W ~52W ~21W ~20W ~18W ~16W ~16W ~15W << (Power Capability: 1kW/set) 10

Heating Value by the ACC Mode for SiC Tiles Eigenmode Analysis Using CST-MWS With 40 MeshLines/WaveLength Til Tail of fthe Electric ti Fild Field of fthe ACC mode (magnification) Electric Field of the ACC mode (6 SiC tiles are approximated by one plate.) 11

Heating Value by the ACC Mode Simulation Results ( All-SiC means these 4 plates(=sets).) For the mechanically innermost position P ( All SiC) loss (Wall) P loss P ( Wall) loss 0.1% 133kW for 0.7MV/cav ( All SiC ) P loss 133 W Heating value < 100W/set << Power Capability: 1kW/set 12

Coupled Oscillations of the ACC Mode Electric Field Coupled Oscillations of the ACC Mode might be non-negligible via the TE mode. TM mode Cutoff: 1.51 GHz TE mode Cutoff: 588 MHz Close to the ACC-mode Frequency: 508.9MHz 13

Step 1: Two Cavity System Electric Short or Magnetic Short Conditions: - Lossfree approximation - Cavity interval: 956mm - 6 SiC tiles approximated by one plate Compute Mode Frequencies using CST-MWS and GdfidL. 14

Two Cavity System f acc Q 509MHz 30000 << 20kHz 0 15

Step 2: Periodic Structure One Unit Periodic Boundary Condition with a phase shift: 0 or 180 deg 16

Periodic Structure f acc Q 509MHz 30000 << 20kHz 0 17

Two-Cavity System Periodic Structure The Coupled Oscillations of the ACC Mode are negligible. 18

Schedule JFY Cavity No. to be made Remarks 2011 0 HPT to be done by May 2012; (prototype) Could be a spare. 2012 1 Feedback from the HPT of the Cavity No.0 2013 2 Get ready for the commissioning with the two cavities. 201X 3 If needed 19

Starting the commissioning with two cavities: Dummy GBP Total Vc: 1.4MV Total Vc: 2MV Install the 3 rd Cavity if needed 20

Summary The design of the accelerating structure for the DR has been modified for the total Vc: 2MV(max). Based on the KEKB MR/ARES Three cavities with 0.7MV/cav GBP made common between the neighboring cavities SiC tiles are used for all the HOM dampers. Based on the established technology used for KEKB MR/ARES (RF absorption power)/set < 180W << PowerCapability: 1kW/set CBIs driven by the HOM impedances Longitudinal lgrowth thtime > 20 ms > 5 ms (rad. damping time) Transverse Growth Time > 30 ms > 10 ms (rad. damping time) Coupled Oscillations of the ACC mode: negligible OK 21

Fin. 22

Appendix A Assumptions for estimating wall temperatures of the DR cavity - Cooling-water flow: 200 L/min - Cooling-water temperature: 30 degc - Cooling-water velocity: 2.0 m/s - Hydraulic equivalent diameter of the cooling-water channel: 9.1e-3 m - Reynolds number: :224(t 2.2e4 (turbulence) bl - Heat-transfer coefficient from the channel to the water: 8.9e3 W/m^2/K - Thermal conductivity of copper: 4.0e2 W/m/K 23

Appendix B Accelerator Resonantly coupled with Energy Storage 3-cavity system stabilized with the /2-mode operation consists of HOM damped accelerating cavity (A cav), Energy storage cavity with TE013 (S cav), Coupling cavity (C cav) with a parasitic mode damper. We use only this for the DR. Perpendicular to the beam axis Along the beam axis 24