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Summary of Accelerator System (WG2) 김김김 김김김김김

Summary of Accelerator System (WG2) 김귀년 경북대학교. Presentations for WG2 -Polarized Electron Source for ILC in Korea - ( 김귀년 ( 경북대 ), 박성주 (PAL)) - ILC

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Page 1: Summary of Accelerator System (WG2) 김귀년 경북대학교. Presentations for WG2 -Polarized Electron Source for ILC in Korea - ( 김귀년 ( 경북대 ), 박성주 (PAL)) - ILC

Summary of Accelerator System (WG2)

김귀년 경북대학교

Page 2: Summary of Accelerator System (WG2) 김귀년 경북대학교. Presentations for WG2 -Polarized Electron Source for ILC in Korea - ( 김귀년 ( 경북대 ), 박성주 (PAL)) - ILC

Presentations for WG2

-Polarized Electron Source for ILC in Korea

- ( 김귀년 ( 경북대 ), 박성주 (PAL))

- ILC Bunch Compressor 의 현황과 계획

- ( 손동철 , 김유종 ( 경북대 ) )

- Beam dynamics on Damping Rings and Beam-Beam Interaction

- ( 김은산 (PAL))

-General Idea on ILC Beam Diagnostics

- ( 황정연 (PAL))

-ILC 를 위한 PAL 에서의 facility 제안

- ( 손동철 ( 경북대 ))

Page 3: Summary of Accelerator System (WG2) 김귀년 경북대학교. Presentations for WG2 -Polarized Electron Source for ILC in Korea - ( 김귀년 ( 경북대 ), 박성주 (PAL)) - ILC

pre-linac

Damping ring

Bunch compressor

linac

Beam delivery

Interaction region

Source

Page 4: Summary of Accelerator System (WG2) 김귀년 경북대학교. Presentations for WG2 -Polarized Electron Source for ILC in Korea - ( 김귀년 ( 경북대 ), 박성주 (PAL)) - ILC

Specifications for ILC polarized electron source

Parameters units TESLA-TDR NLC/GLC

US-COLDGun bunch charge nC (#e-)4.5 (2.8×1010)Polarization % > 80Bunch length ns 2 0.7Cathode bias voltage kV -120Beam radius mm 12# bunches / pulse 2820 192Bunch spacing ns 337 1.4Pulse length µs 950 0.27Repetition rate Hz 5 120

1. Polarized Electron Source

Page 5: Summary of Accelerator System (WG2) 김귀년 경북대학교. Presentations for WG2 -Polarized Electron Source for ILC in Korea - ( 김귀년 ( 경북대 ), 박성주 (PAL)) - ILC

Korea’s Capabilities Relevant to ILC Injcetors

1. PES Test Stand• GaAs-NEA Photocathode Production• Compact Mott Polarimeter• Electrostatic Bend• PEGGY Source (provided by the SLAC)

2. PAL XFEL Injector• GTS (Gun Test Stand)

– BNL Gun-IV-type 1.6-Cell RF Gun– Ti:Sapphire Laser– Dedicated RF Source– Beam Diagnostics

• PPI (Pohang Photo-Injector)

Page 6: Summary of Accelerator System (WG2) 김귀년 경북대학교. Presentations for WG2 -Polarized Electron Source for ILC in Korea - ( 김귀년 ( 경북대 ), 박성주 (PAL)) - ILC

4. Special facilities for klystron fabrication• XHV Baking Station• Various Furnaces• HP Microwave Test-Lab

5. Infra-Structures• Chemical Cleaning Shop, Plating Facility, Welding Shop, 3D CM

M,…• Magnetic Field Measurement Facilities• Full-line of Microwave Equipments

6. High-Quality Manpowers• Beam-Dynamics Experts• Mechanical Engineers• High-Power Electrical Engineers• RF Engineers (LL & HL)• XHV Experts• were involved in the PLS construction, now in the PAL XFEL pr

oject

Korea’s Capabilities Relevant to ILC Injcetors- Continued -

Page 7: Summary of Accelerator System (WG2) 김귀년 경북대학교. Presentations for WG2 -Polarized Electron Source for ILC in Korea - ( 김귀년 ( 경북대 ), 박성주 (PAL)) - ILC

2. Newly Proposed Bunch Compressor for ILC by Y. Kim

Final parameters

E = 6.0 GeV = 2.173%z = 300 m nx= 8.7 m, ny= 0.02 m

z = 6.00 mm 673 m 300 m

ACC1 ACC2 ACC4

Q=3.2 nC e-beam

23.4 MV/m-45 deg

24.8 MV/m170.0 deg

ACC5 ACC6ACC3BC1

E = 5.689 GeV ~ 2.4%R56 = 236 mm = 5.3 deg

E = 6.0 GeV ~ 2.174%R56 ~ 17 mm ~ 1.4 deg

BC2

13.3 MV/m-21.5 deg

Up to main linac : ELEGANT with CSR, ISR, and geometric short-range wakefields.but without space charge

Initial parameters

E = 5.0 GeV = 0.13% (small !)z = 6.0 mm nx= 8.0 m, ny= 0.02 m

1/8.9 1/2.2

Damping Ring

ACC39

Oral Talk at 1st ILC Workshop, KEK, Japan

Page 8: Summary of Accelerator System (WG2) 김귀년 경북대학교. Presentations for WG2 -Polarized Electron Source for ILC in Korea - ( 김귀년 ( 경북대 ), 박성주 (PAL)) - ILC

3. Possible things for damping ring design of ILC-ASIA

• Optics• * Lattice design ( suggested dogbone and small DR ) • * Effects of edge field of wigglers on dynamic aperture• * Tune survey • * Optics/dispersion correction with space charge• * Tolerances for the emittance

• Tracking simulations• * Emittance growth and particle loss due to space charge.• * Effects of wakes in damping rings• * Multi-bunch instabilities due to superconducting RF cavities• * Electron cloud instabilities and ion instability.• * Wiggler effects on beam parameters

Page 9: Summary of Accelerator System (WG2) 김귀년 경북대학교. Presentations for WG2 -Polarized Electron Source for ILC in Korea - ( 김귀년 ( 경북대 ), 박성주 (PAL)) - ILC

Quantity of ILC Quantity of ILC MonitorsMonitors

BPMBeam

Profile(size)

Bunch Length

Beam sources

500 40 10

Linac 2200 24 ?

Damping Ring

1000 8 10

Beam Delivery system

300 ? 8

Page 10: Summary of Accelerator System (WG2) 김귀년 경북대학교. Presentations for WG2 -Polarized Electron Source for ILC in Korea - ( 김귀년 ( 경북대 ), 박성주 (PAL)) - ILC

Most critical measurements for Linear Collider

nanometer beam position measurement near IP (σz ~ 1000 - 5 nm)

-best cavity BPM (cBPM) ~ 25 nm

-best stripline BPMs (sBPM) ~ 1 μm

nanometer beam size measurement at IP

- best laser wire scan ~100 nm

- best metal wire scan ~ 5 μm

- laser interference slit scan ~ 50 nm (Shinta

ke)

resolution limited by wavelength

fs bunch length measurement

- electro-optic/ CSR, CTR/ rf deflector ~30 fs

Various techniques for PAL XFEL will be also applicable for ILC

Requirements and Status of ILC DiagnosticsRequirements and Status of ILC Diagnostics4. Beam Diagnostics

Page 11: Summary of Accelerator System (WG2) 김귀년 경북대학교. Presentations for WG2 -Polarized Electron Source for ILC in Korea - ( 김귀년 ( 경북대 ), 박성주 (PAL)) - ILC

Major parameters

Injector BC Undulator Remarks

Beam Energy 150 MeV 442 MeV 3,000 MeV  

Beam Charge 1.0 nC 1.0 nC 1.0 nC0.1% 1 pC

Bunch Length

900 μ m (3 ps) 110 μ m (300 fs) 25 μ m (80 fs)σz rms

3μ m (10fs)

Beam Size (135, 125) μ m (115, 100) μ m (68, 62) μ m (σx, σy)

5μ m

Beam Emittance 1.0 μ m 1.0 μ m ~1.0 μ m 10%

Beam position

∓ 10 μ m ∓ 10 μ m ∓ 2 μ m  

Beam parameters for PAL-XFEL Beam parameters for PAL-XFEL diagnosticsdiagnostics

Page 12: Summary of Accelerator System (WG2) 김귀년 경북대학교. Presentations for WG2 -Polarized Electron Source for ILC in Korea - ( 김귀년 ( 경북대 ), 박성주 (PAL)) - ILC

포항가속기연구소 선형가속기 남서쪽 부지

• 1) 선형충돌가속기 편극전자 /양전자 빔원 및 빔압축장치 시험 시설 (LC-PEPS: Linear Collider Polarized Electron and Positron Sources)

• 2) 고에너지입자검출기 빔 시험 시설 및 초전도가속관 제작 시험 시설 (HEP-BTF: High Energy Particle Detector Beam Test Facility) – ▶ 고에너지 전자 빔 및

기타 제 2 차 입자 시험 빔– ▶ 초전도가속관 제작 및

시험 시설

Page 13: Summary of Accelerator System (WG2) 김귀년 경북대학교. Presentations for WG2 -Polarized Electron Source for ILC in Korea - ( 김귀년 ( 경북대 ), 박성주 (PAL)) - ILC

Conventional vs. Gamma Based Positron Source

Target

Photons 10-20 MeV

Electrons 0.1-10 GeV

Primary Beam Capture Optics

thin target: 0.4 X0

thick target: 4-6 X0

Page 14: Summary of Accelerator System (WG2) 김귀년 경북대학교. Presentations for WG2 -Polarized Electron Source for ILC in Korea - ( 김귀년 ( 경북대 ), 박성주 (PAL)) - ILC

Pohang Accelerator Lab.

Laser Compton Scattering Beam Line using Pohang Linac

Page 15: Summary of Accelerator System (WG2) 김귀년 경북대학교. Presentations for WG2 -Polarized Electron Source for ILC in Korea - ( 김귀년 ( 경북대 ), 박성주 (PAL)) - ILC

Summary of WG2

1.Polarized Electron Source:

2. Damping Ring

3. Bunch Compressor:

4. Beam diagnosticsdiagnostics

5. Test Facility for ILC at PAL5. Test Facility for ILC at PAL