Toward a Test Facility for an ERL Circulator

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Toward a Test Facility for an ERL Circulator Ring Based e-Cooler MEIC Electron Cooler

Toward a Test Facility for an ERL Circulator Ring Based e-Cooler MEIC Electron Cooler Test Facility Planning Retreat January 31, 2012

Charge of the Retreat • Examine the feasibility of utilizing JLab FEL Facility for

Charge of the Retreat • Examine the feasibility of utilizing JLab FEL Facility for a test bad of ERL-Circulator-Ring e-cooler • Determine the goals of this test facility • Formulate plausible test scenarios • Determine the required pre-R&D • Draft a plan for this test facility

What We Want to Test/Demonstrate/Study? • Production of high current/bunch intensity, high repetition beam

What We Want to Test/Demonstrate/Study? • Production of high current/bunch intensity, high repetition beam • Energy recovery of a high current electron beam after its extended stay in a circulator ring; • Operation of a circulator ring including injection and ejection of the beam bunches, and advanced filling schemes; • Quality of the beam bunch during a large number of circulations in a ring • Collective beam effects (space charge, CSR)

e-Cooler Test Facility Diagnostic element Fast kicker Cooling channel solenoid lattice Fast kicker

e-Cooler Test Facility Diagnostic element Fast kicker Cooling channel solenoid lattice Fast kicker

Scaling Down Parameters: How Much? For a convincing demonstration • • • Beam current

Scaling Down Parameters: How Much? For a convincing demonstration • • • Beam current in circulator ring: 1. 5 A 15 m. A ? Charge per bunch: 2 n. C 0. 4 n. C ? ERL beam current: 15 m. A ? Fast kicker: 1. 33 ns (750 MHz) 20 ns (50 MHz) ? Turns of circulation: 10 to 30 turns ?

Beam Parameters MEIC FEL Test Facility 88 – 165 11 – 54 Energy range

Beam Parameters MEIC FEL Test Facility 88 – 165 11 – 54 Energy range Me. V 11 – 54 Beam current in circulator cooler ring m. A 1500 150 Bunch repetition in circulator cooler ring MHz 748. 5 50 Bunch spacing in circulator cooler ring m 0. 4 6 Circumference of circulator cooler ring m 120 90 300 15 Bunches in circulator cooler ring Charge per bunch n. C 2 0. 135 0. 4 Electrons/bunch 1010 1. 25 0. 084 0. 25 bunch revolutions in circulator cooler ring 100 to 300 10 to 30 Current in ERL m. A 15 to 5 9. 1 15 Bunch repetition in ERL MHz 2. 5 to 7. 5 0. 58 – 74. 85 5 to 1. 67 RMS Bunch length cm 1 -3 0. 005 (160 fs) 1 Energy spread 10 -4 1 -3 40 10 Beam radius in solenoid mm ~1

Test Scenarios • • Test high bunch charge injector (DC gun? SRF gun? )

Test Scenarios • • Test high bunch charge injector (DC gun? SRF gun? ) Test high current ERL without/with circulator ring? Test kicker/filling scheme of a circulator ring? Test beam stability/collective effects in circulator ring?

Additional Hardware & pre-R&D • Magnetic lattice for the circulator ring • Fast kickers

Additional Hardware & pre-R&D • Magnetic lattice for the circulator ring • Fast kickers • Beam diagnostic instruments • High bunch intensity electron source • ERL for high bunch intensity beam (? ) • (not very fast) kicker • Design and simulation

Timeline • • Total time: 2 years (? ) Design/simulation/pre-R&D: 1. 5 year commissioning:

Timeline • • Total time: 2 years (? ) Design/simulation/pre-R&D: 1. 5 year commissioning: 2 months Running experiments: 4 months

High Brightness SRF Photo Injector Gun

High Brightness SRF Photo Injector Gun

A Polarized Ring-Ring MEIC at JLab Large booster to collider ring Large booster (warm)

A Polarized Ring-Ring MEIC at JLab Large booster to collider ring Large booster (warm) transfer beamline (up to 20 Ge. V/c) Pre-booster (up to 3 Ge. V) Ion source SRF linac Ion collider ring (cold) (up to 100 Ge. V/c) Three Figure 8 rings stacked vertically Medium energy IP with horizontal crab crossing Electron ring (3 to 11 Ge. V) Injector 12 Ge. V CEBAF Future energy/luminosity upgrade possible (250 Ge. V proton, 100 Ge. V/u ion, 1035 cm-2 s-1)

Optimized Location of Cooling Channel 20 m id no e l o ) m

Optimized Location of Cooling Channel 20 m id no e l o ) m (15 S injector SRF Short circulating beam-line Center of Figure-8 Eliminating a long circulating beam-line could • cut cooling time by half, or • reduce the cooling electron current by half, or • reduce the number of circulating by half dumper

Cooling in Ion Collider Ring • Initial cooling after ions injected into the collider

Cooling in Ion Collider Ring • Initial cooling after ions injected into the collider ring for reduction of longitudinal emittance before acceleration • After boost & re-bunching, cooling for reaching design values of beam parameters • Continuous cooling during collision for suppressing IBS, maintaining luminosity lifetime Initial after boost Colliding Mode Ge. V/Me. V 15 / 8. 15 60 / 32. 67 A 0. 5 / 1. 5 Particles/Bunch 1010 0. 416 / 2 Bunch length mm (coasted) 10 / 20~30 Momentum spread 10 -4 10 / 2 5/2 3/2 Hori. & vert. emittance, norm. µm 4/4 Energy proton/electron beam current Laslett’s tune shift (proton) 0. 002 In collision mode of MEIC, 60 Ge. V proton formula Long. Hori. IBS Piwinski s 66 86 IBS Martini (Beta. Cool) s 50 100 Cooling Derbenev s ~24 0. 35 / 0. 07 0. 005 0. 06 Beta. Cool Simulations Vert. 1923 emittance IBS growth time

Monitoring Bunch Evolution in Circulator Ring Cooling channel solenoid lattice Kicking bunches out after

Monitoring Bunch Evolution in Circulator Ring Cooling channel solenoid lattice Kicking bunches out after n-th turn Fast kicker Diagnostic element

Energy Me. V 80 -200 Charge/bunch p. C 135 Average current m. A 10

Energy Me. V 80 -200 Charge/bunch p. C 135 Average current m. A 10 Peak current A 270 Beam power MW 2 % 0. 5 µm-rad <30 Energy spread Normalized emittance