1. Conventional e + Source Rotation Target R/D T. Omori (KEK) ANL, IHEP, Hiroshima U, U of Tokyo, KEK, DESY, U of Hamburg, CERN 3-Sep-2015 POSIPOL 2015, Cockcroft Institute, Daresbury On behalf of the Truly Conventional Collaboration Rotation target design study: ongoing with Rigaku

2. (1)Summary of the R/D in 2013-2014, and the first half of 2015. (2) Plan of the R/D in 2015-2016. Today’s Talk R/D of the Slow Rotation Target of the Conventional e+ Source for ILC

3. 20 triplets, rep. = 300 Hz triplet = 3 mini-trains with gaps 44 bunches/mini-train, T b_to_b = 6.15 n sec DR T b_to_b = 6.15 n sec 2640 bunches/train, rep. = 5 Hz T b_to_b = 369 n sec e+ creation go to main linac Time remaining for damping = 137 m sec We create 2640 bunches in 63 m sec Booster Linac 5 GeV NC 300 Hz Drive Linac Several GeV NC 300 Hz Target Amorphous Tungsten Slow Rotation 2640 bunches 60 mini-trains Stretching Conventional e+ Source for ILC Normal Conducting Drive and Booster Linacs in 300 Hz operation NIM A672 (2012) 52—56

4. 20 triplets, rep. = 300 Hz triplet = 3 mini-trains with gaps 44 bunches/mini-train, T b_to_b = 6.15 n sec DR T b_to_b = 6.15 n sec 2640 bunches/train, rep. = 5 Hz T b_to_b = 369 n sec e+ creation go to main linac Time remaining for damping = 137 m sec We create 2640 bunches in 63 m sec Booster Linac 5 GeV NC 300 Hz Drive Linac Several GeV NC 300 Hz Target Amorphous Tungsten Slow Rotation 2640 bunches 60 mini-trains Stretching Conventional e+ Source for ILC Normal Conducting Drive and Booster Linacs in 300 Hz operation NIM A672 (2012) 52—56 Today’s Talk

5. Moving Target ~5m/sec required (1/20 of undulator scheme) 2013/8/30 ILC monthly, Yokoya5 ferromagnetic fluid seal airvacuum rotating target with ferromagnetic seal main issue: vacuum

6. The target R/D in 2013-2014, and the first half of 2015.

7. TEST: Vacuum Leak Rate FY2013 Small (d=10 cm) off-the-shelf rotation target

8. TEST: Vacuum Leak Rate FY2013

9. TEST: Vacuum Leak Rate Conclusion: No problem Leak Rate Measurement: various speed, various temperature no problem (both CN-oil and F-oil) Lake rate was small enough. We can get P< 1x10 -7 Pa, if we put reasonable pumps (several 1000 letters/s) at the upstream of the target. FY2013

10. Takasaki Advanced Radiation Research Institute, JAEA Gamma-ray source: Co 60 1.1 x 10 4 Gy/h Radiation Tolerance Test FY2013 Photo: Dec/2013

11. TEST: Radiation Tolerance FY2013

12. Dec/2013 0.27 M Gy3.2 M Gy 0.27 M Gy3.2 M Gy

13. TEST: Radiation Tolerance FY2013: Conclusion F-oil Dissociation/degradation occurred at low dose, 0.27 MGy. No hope. CN-oil Viscosity increased, but NO dissociation/ degradation occurred. --> We planed more systematic study. Viscosity change as a function of dose. Use irradiated fluid in vacuum seal.

14. d = 40 cm with radiation shield 200 W Fe W FerroFluid Cu 165 85 50 17 5 30 64.5 T. Takahashi (Hiroshima) Dose Estimation FY2014

15. Results Energy Depotit(MeV)/2mm/5×10^5e- S(mm) Z(mm) S Z Peak 1.5MGy/year (2630 bunches/pulse, 5Hz 2e10/bunch 1 year = 10^7s) d = 40 cm with radiation shield T. Takahashi (Hiroshima) Dose Estimation FY2014

16. TEST: Radiation Tolerance FY2014 Takasaki Advanced Radiation Research Institute, JAEA November 2014 10-Nov-2014

17. November 2014 TEST: Radiation Tolerance FY2014 Dose [MGy] Viscosity Viscosity as a function of dose More systematic study for CN oil

18. November 2014 TEST: Radiation Tolerance FY2014 More systematic study for CN oil Dose [MGy] Viscosity Viscosity as a function of dose 4.7 MGy

19. FF seal Ar Vac. Air atmospher RGA Ar(40) O 2 (32) N 2 (28) The seal dosed 4.7 MGy (3 ILC year) is examined with Ar purged chamber. Rotation : 0-600 rpm. No leak was found. (m/q = 28 and 32 are N 2 and O 2 from air) Ar purge seal test PY2014: Radiation Test: We used irradiated CN-oil (4.7 MGy) in a small rotation target. Made vacuum test after Ar-purging.

20. Rotation target design study: ongoing with Rigaku Points: Diameter, material, shape, rotation speed, cooling,,, B-filed on the target disk (Hiroshima), Flux concentrator (IHEP, BINP) FY2014-2015

21. ＩＩ 間接冷 却 Ｉ 直接冷 却 Peter SIEVERS (CERN) Ｉ Direct Cooling Rotation target design study FY2014 ＩＩ Indirect Cooling "monolithic welded water circuit entirely of the same material (Cu)” W-Cu joint metal gaskets remain UHV leak tight?

22. ＩＩ 間接 冷却 Ｉ 直接冷 却 Rigaku Rotation target design study FY2014 Ｉ Direct Cooling ＩＩ Indirect Cooling

23. Temperature Distribution 600rpm Rigaku Rotation target design study FY2014 Ｉ Direct Cooling ＩＩ Indirect Cooling Temperature Distribution Max. 330 ℃ Max. 840 ℃ Conclusion: Indirect cooling is better.

24. AMD is employed is a capture section. The AMD will be a pulse Flux Concentrator. Need to consider the effect of the Flux Concentrator leakage field on the target disk. Seimiya, Kuriki (Hirosima U.), et al. Submitted to PTEP Rotation target design study FY2014 Seimiya & Kuriki (Hirosima U.)

25. (1)The FC B-field is pulse. The pulse is fast. half cycle ~12 micro second (roughly sinusoidal) Dominant (2) The target is rotating. Rotation is slow. ~5 m/s. Small, Negligible (2)/(1) ~ 1/1000 Rotation target design study FY2014 The effect of the FC leakage field on the target.

26. Rotation target design study FY2014 The effect of the FC leakage field on the target. Heat: caused by the eddy current 190 kW : (preliminary, discussions are ongoing) Not negligible (c.f. Heat by EM shower 35 kW) note: assume 2600 bunches, 5 Hz We may need cure. Make many radial slits? Omori’s Presentation at ALCW 2015 Tsukuba

27. Rotation target design study FY2014 The effect of the FC leakage field on the target. Heat: caused by the eddy current 190 kW : (preliminary, discussions are ongoing) Not negligible (c.f. Heat by EM shower 35 kW) note: assume 2600 bunches, 5 Hz We may need cure. Make many radial slits? Omori’s Presentation at ALCW 2015 Tsukuba was NOT correct

28. Flux Concentrator (FC) leakage field on the target disk. Rotation target design study FY2015 Cone diameter is 16 mm (Nose FC) Pavel Martyshkin (BINP) Sun Xianjin (IHEP) also made a study too, based on another design (2014-2015).

29. Flux Concentrator (FC) leakage field on the target disk. Rotation target design study FY2015 Pavel Martyshkin (BINP) B = 1 Tesla at Target Disk Cone diameter is 16 mm (Nose FC) Nose FC type D 16 mm 25 kA 5 Tesla 50-60 mTesla half of sine 25 µs ≈ 10 J/pulse ≈ 140 J/pulse 3.2 kW 41 kW Peak current Peak field Peak transverse field Current shape Current pulse length Target ohmic loss FC ohmic loss Repetition rate 300 pps * Target losses * FC losses * Sun Xianjin (IHEP) also made a study too, based on another design. * When we calculate real average, we need to divide the numbers by three.

30. Rotation target design study FY2014 The effect of the FC leakage field on the target. Heat: caused by the eddy current 190 kW : (preliminary, discussions are ongoing) Not negligible (c.f. Heat by EM shower 35 kW) note: assume 2600 bunches, 5 Hz Omori’s Presentation at ALCW 2015 Tsukuba was NOT correct Nose FC type D 16 mm 25 kA 5 Tesla 50-60 mTesla half of sine 25 µs ≈ 10 J/pulse ≈ 140 J/pulse 3.2 kW 41 kW Nose FC Cone diameter 16 mm FY2015 * When we calculate real average, we need to divide the numbers by three. Peak current Peak field Peak transverse field Current shape Current pulse length Target ohmic loss FC ohmic loss Repetition rate 300 pps * Target losses * FC losses *

31. Rotation target design study FY2014 The effect of the FC leakage field on the target. Heat: caused by the eddy current 190 kW : (preliminary, discussions are ongoing) Not negligible (c.f. Heat by EM shower 35 kW) note: assume 2600 bunches, 5 Hz Omori’s Presentation at ALCW 2015 Tsukuba was NOT correct Nose FC type D 16 mm 25 kA 5 Tesla 50-60 mTesla half of sine 25 µs ≈ 10 J/pulse ≈ 140 J/pulse 3.2 kW 41 kW Nose FC Cone diameter 16 mm 190 kW Old Estimation ALCW 2015 Tsukuba New Estimation 1 kW average FY2015 * When we calculate real average, we need to divide the numbers by three. Peak current Peak field Peak transverse field Current shape Current pulse length Target ohmic loss FC ohmic loss Repetition rate 300 pps * Target losses * FC losses * 1/200

32. Force 1 ： Attraction/Repulsion Forces Rotation target design study FY2014 The effect of the FC leakage field on the target. Omori’s Presentation at ALCW 2015 Tsukuba Force 2 ： Breaking Force Forces: caused by the interaction between the magnetic field and the eddy current 2000N (200 kgw): repulsive in the first half (first 6  s) 2000N (200 kgw): attractive in the next half (next 6  s) 6x10 -3 Ns (0.6 gws) : repulsive in the first half 6x10 -3 Ns (0.6 gws) : attractive in the next half Forces Impulses Impulses are small, and integration is ZERO. Conclusion: No problem. ZERO. (force acting at the right (up) side and the force acting at the left (down) side cancels each other.) Conclusion: No problem.

33. Force 1 ： Attraction/Repulsion Forces Rotation target design study FY2014 The effect of the FC leakage field on the target. Omori’s Presentation at ALCW 2015 Tsukuba Force 2 ： Breaking Force Forces: caused by the interaction between the magnetic field and the eddy current 2000N (200 kgw): repulsive in the first half (first 6  s) 2000N (200 kgw): attractive in the next half (next 6  s) 6x10 -3 Ns (0.6 gws) : repulsive in the first half 6x10 -3 Ns (0.6 gws) : attractive in the next half Forces Impulses Impulses are small, and integration is ZERO. Conclusion: No problem. ZERO. (force acting at the right (up) side and the force acting at the left (down) side cancels each other.) Conclusion: No problem. were NOT correct

34. Force 1 ： Attraction/Repulsion Forces Rotation target design study FY2014 The effect of the FC leakage field on the target. Omori’s Presentation at ALCW 2015 Tsukuba Force 2 ： Breaking Force Forces: caused by the interaction between the magnetic field and the eddy current 2000N (200 kgw): repulsive in the first half (first 6  s) 2000N (200 kgw): attractive in the next half (next 6  s) 6x10 -3 Ns (0.6 gws) : repulsive in the first half 6x10 -3 Ns (0.6 gws) : attractive in the next half Forces Impulses Impulses are small, and integration is ZERO. Conclusion: No problem. ZERO. (force acting at the right (up) side and the force acting at the left (down) side cancels each other.) Conclusion: No problem. were NOT correct Current estimation 1/200 Conclusions remain: NO problem

35. Rotation target design study FY2014-2015 The effect of the FC leakage field on the target. Forces: Small in both braking and attractive/repulsive forces. Conclusion: No problem. Heating: 1 kW (3.2 kW in 63 msec). It is 1/30 of the heat by beam. Conclusion: No problem.

36. Thermal Analysis: Target Model and Cooling Condition Model : 500 mm diameter rotation target Rim (φ500-φ366×14t) W + Central Cu Disk (water flow inside) Rotation: 200 - 600rpm Water temperature at inlet: 25 o C Software; ANSYS CFX Model 39 FY2014-2015

37. CW beam analysis 38kW (35kW+3kW ( * ) ) CW Common condition Cooling water: 30 l /min, Temp. at inlet: 25 ℃ Pulse beam analysis 114.1 kW(111.1kW+3kW) 63 ms 0 kW ( 0kW+0kW) 137 ms Thermal Analysis: We did both CW beam analysis (for simplicity) and pulse beam analysis (more realistic). beam FC beam FC FY2014-2015 FY2015 New We assume 2600 bunches/pulse in all analysis. * Note 3 kW is not correct should be 1 kW

38. 200rpm Max.; 322 ℃ 600rpm Max.; 298 ℃ 400rpm Max.; 304 ℃ 等温度平面 ; 295 ℃ Temperature in various rotation speeds: 38kW(CW analysis) Nb=2600

39. Copyright © 2013 — Rigaku Corporation and its Global Subsidiaries. All Rights Reserved. Temperature in various rotation speeds: 38kW(CW analysis) Nb=2600

40. Direction (arrows) Min Principal Stress (Compression) → - 3e+8Pa Max Principal Stress (Expansion) → 2e+8Pa 高温部の応力を正確に得る為に非定常解析が必要 Stress: rotation speed 200 rpm, 38kW(CW analysis) Nb=2600

41. Pulse beam analysis t=0 (beam start) to 50 turns After 5 turns After 20 turns After 50 turns Pulse beam analysis 114.1kW(111.1kW+3kW) 63ms On 0 kW (0+0) 137ms Off Nb=2600

42. Pulse beam analysis t=0 (beam start) to 50 turns After 5 turns After 20 turns After 50 turns Pulse beam analysis 114.1kW(111.1kW+3kW) 63ms On 0 kW (0+0) 137ms Off 200 rpm seems NO GOOD

43. Rotation = 200 rpm, R_hit = 240 mm, C_hit = 1507 mm, V_ tangential = 5023 mm/s,  C(63ms)=316 mm,  C(137ms) = 688 mm (2) Beam OFF t: 63 -> 200 ms (3) Beam ON t: 200 -> 263 ms (5) Beam ON t: 400 -> 463 ms (6) Beam OFF t: 463 -> 600 m (4) Beam OFF t: 263 -> 400 ms (1) Beam ON t: 0 -> 63 ms

44. Simulated by Rigaku Pulse beam analysis: Comparison of 200 rpm and 180 rpm 200 rpm180 rpm after 150 turns after 100 turns Max Temp = 391 o C Max Temp = 343 o C 180 rpm is BETTER than 200 rpm. At 180 rpm: Temperature more UNIFORM and LOWER maximum value. Nb=2600

45. Simulated by Rigaku Pulse Beam Simulation Energy Flow (kW) - 35 kW 114 kW 0 kW At the point of beam hit At the boundary of Cu-Water t = 0 After 100 turns Rotation speed = 180 rpm From “t=0” to “after 100 turns”. Time Nb=2600

46. Simulated by Rigaku Energy Flow (kW) - 38 kW 114 kW 0 kW At the point of beam hit At the boundary of Cu-Water t = 0 After 300 turns Pulse Beam Simulation Rotation speed = 180 rpm From “t=0” to “after 300 turns”. Time Nb=2600

47. Simulated by Rigaku Temperature ( o C) 120 oC 360 o C At the point of beam hit At the boundary of W-Cu after 250 turns After 300 turns Room Temp. Temp of water 87 o C Pulse Beam Simulation Rotation speed = 180 rpm From “t=200 turns” to “after 300 turns”. Time Nb=2600

48. Summary of the R/D in Past Two Years: FY2013-FY2014

49. FY2013: Leak Rate measurement We took leak rate data by using a small (d=10cm) rotation target off the shelf. Conclusion: Leak Rate is small enough. FY2013-2014: Radiation Test: We made radiation test of ferrofluid at Takasaki Lab. Conclusion: F-oil: No hope. CN-oil: No problem up to 4.7 MGy (about 3 ILC years). FY2014-2015: Target Design Study. We made design study the the company, Rigaku. We now have a nearly final technical design.

50. Plan of the R/D in FY2015-FY2016

51. (1) We will make a prototype in two years (FY2015-2016). (2) The prototype is full-size, d=500 mm. (3) Full-size means that target wheel has the same radius, the same weight, the same moment as those of the real target. The locations of the vacuum seal and bearing in the prototype are as same as those in the real one. (4) The prototype is not totally as same as the real one. The prototype has no water channels in it. We don’t use W for disk. (5) We will use irradiated ferromagnetic fluid in the prototype. (6) We will make continuous running test (~1 year?) and will prove that vacuum always stay good level. Outline of the Plan in Next Two Years

52. The loads on the vacuum seal and the bearing are determined by the weight and the moment of the target disk. So we will make full size prototype. The purpose is vacuum test. It is not necessary to use W for the disk. We don’t use W for cost saving. Water channels will be unimplemented. It is cost saving. Target rotation is slow, water circulation is within the past experience of the company. We have no need to demonstrate. Points of the prototype

53. Backup

55. 5 cm 30 cm 90 cm Set#5 Set#6 Set#7 Set#9 Set#10  -Ray Source Co 60 Out 48 h Out 168 h Out 240 h Out 360 h 1.30x10 4 Gy/h Nov/12 Wed Nov/17 Mon Nov/20 Thu Nov/25 Tue 0.607x10 4 Gy/h 0.205x10 4 Gy/h Set#4 0.098 MGy 1.0 MGy 3.1 MGy 1.5 MGy 4.7 MGy 2.1 MGy Bottle Stand#1 Bottle Stand#2 Bottle Stand#3 Put in All Bottles 0 h Nov/10 Mon 16 days of Exposure bottle: ferromagnetic fluid bottle: base oil 1 R = 8.77 mGy Set#8 0.49 MGy November 2014 TEST: Radiation Tolerance FY2014 More systematic study for CN oil

56. November 2014 TEST: Radiation Tolerance FY2014 More systematic study for CN oil

57. Copyright © 2013 — Rigaku Corporation and its Global Subsidiaries. All Rights Reserved. Max: 0.14mm Displacement: rotation speed 200 rpm, 38kW(CW analysis)

58. 最大主応力分布 各部位と温度 @600rpm 高温部 ; 840 ℃ 切り込み先端部 ;140 ℃ 内径部 ; 65 ℃ 温度分布 Rigaku Rotation target design study FY2014 Ｉ Direct Cooling

59. 冷却水の流線温度分布 → Max. 330 ℃ 結論：間接冷却で OK Rigaku Rotation target design study FY2014 ＩＩ Indirect Cooling Conclusion: Indirect cooling is better.

60. Mar 2015 TEST: Radiation Tolerance FY2014 Irradiation to the small (d=10 cm) off-the-shelf rotation target 0.6 M Gy irradiation on the motor. corresponds 1 ILC year Radiation test fo the moter: After irradiation, we made rotation and vacuum test. NO problem

61. Ar-purging Magnet Ferrofulid seal Seal against Ar Seal against Water Seal against Air

62. H26 年度 : 設計検討 PY2014: Radiation Test: We used irradiated CN-oil (4.7 MGy) in a small rotation target. Made vacuum test after Ar-purging.

63. PY2014: Radiation Test: Vacuum spike was observed. Vacuum test

64. Ar purge seal test FF seal Ar Vac. Air atmospher RGA Ar(40) O 2 (32) N 2 (28) The seal dosed 4.7 MGy (3 ILC year) is examined with Ar purged chamber. Rotation : 0-600 rpm. No leak was found. (m/q = 28 and 32 are N 2 and O 2 from air)

65. Issue of Slow Rotation Target Issue: Can we sustain ultra-high vacuum?

66. Issue of Slow Rotation Target Issue: Can we sustain ultra-high vacumme? undulator source ： Vacuum test of rotation seal

68. Beam before DR <-- the 100 ns gap is required to cure an e- cloud problem in e+ DR. =132 bunches

69. Beam before DR Injection: usual kicker ( ~ 1 us) no stacking is necessary <-- the 100 ns gap is required to cure an e- cloud problem in e+ DR. =132 bunches