MEIC Ion Linac and Pre-Booster Design Bela Erdelyi Department of Physics, Northern Illinois University, and Physics Division, Argonne National Laboratory Review 09/2010 Page 1 Acknowledgements • Joint Work of • Bela Erdelyi (NIU/ANL) • Shashikant Manikonda (ANL) • Peter Ostroumov (ANL) • Sumana Abeyratne (NIU student) • With assistance from JLab staff (Y. Derbenev, Y. Zhang, G. Krafft, etc.) Review 09/2010 Page 2 ELIC Conceptual Layout Three compact rings: • 3 to 11 GeV electron • Up to 12 GeV/c proton (warm) • Up to 60 GeV/c proton (cold) Review 09/2010 Page 3 Ion Linac for ELIC • Pulsed linac • Short Normal Conducting section: RFQ and IH structure • Followed by Superconducting section that contains • Stripper for heavy ions at 12 MeV/u Review 09/2010 Page 4 Basic Parameters of the Linac • Linac layout RFQ IH QWR IS MEBT Normal conducting QWR HWR Stripper Superconducting Parameter 1 2 3 4 5 6 7 8 9 DSR Ion species Ion species for the reference design Kinetic energy of lead ions Maximum beam current averaged over the pulse Pulse repetition rate Pulse length Maximum beam pulsed power Fundamental frequency Total length Review 09/2010 Value From Hydrogen to Lead Pb 100 MeV/u 2 mA 10 Hz 0.25 msec 680 kW 80 MHz 115 150 m 208 Page 5 Superconducting Cavities • Developed for the RIA/FRIB project QWR Review 09/2010 HWR DSR Page 6 4 4 3.5 3.5 3 3 2.5 Voltage (MV) Voltage (MV) Voltage Gain per Cavity for Protons and Lead Ions 2 1.5 1 2.5 2 1.5 1 0.5 0.5 0 0.1 0.2 0.3 0.4 b Review 09/2010 0.5 0.6 0 0.1 0.2 0.3 b Page 7 0.4 0.5 QWR and HWR production at ANL • QWR, f=109 MHz, b=0.15 • HWR, f=172 MHz, b=0.26 Review 09/2010 Page 8 Cryomodule assembly at ANL beam Review 09/2010 Page 9 Accumulator/Pre-Booster Concept • • Purpose: • Inject from linac • Accumulate ions • Accelerate them • Extract and send to large booster Concepts: • Figure-8 shape for ease of spin transport, manipulation and preservation • Modular design, with (quasi)independent module design optimization • FODO arcs for simplicity and ease of implementation of optics correction schemes • No dispersion suppressors • Injection insertion • Doublet/Triplet straights for long dispersion-less drifts • Matching/tuning modules in between Review 09/2010 Page 10 Constraints • • • • • • • • • Figure-8 shaped; circumference ~250 m Maximum bending field: 1.5 T Maximum quadrupole gradient: 20 T/m Momentum compaction smaller than 1/25 Maximum beta functions less than 35 m Maximum full beam size less than 2.5 cm and 1 cm vertically in dipoles 5m m long dispersion-less sections for RF cavities, electron cooling collimation and extraction Sizable (normalized) dispersion for/at injection Working point chosen such that tune footprint does not cross low order resonances (tunability) Review 09/2010 Page 11 Injection • Protons (and light ions) • Stripping injection • Heavy ions • Repeated multi-turn injection • Transverse (horizontal and possibly also vertical) and longitudinal painting • Electron cooling for stacking/accumulation Review 09/2010 Page 12 Heavy-Ion Injection Review 09/2010 Page 13 Acceleration • h=1 • RF swing necessary is [0.4,2] MHz • 15 kV per cavity • 50kV/turn => 3-4 cavities • 56000 turns for 200MeV -> 3 GeV • Less than 80 ms acceleration time Review 09/2010 Page 14 Extraction • Conventional fast extraction Review 09/2010 Page 15 Layout ARC 1 Injection Insertion section ARC 3 ARC 2 Beam from LINAC RF cavity Solenoid for Electron Cooling Review 09/2010 Page 16 Review 09/2010 Page 17 Arc 2 Straight 2 Arc 3 Straight 1 Arc 1 Injection Linear Optics Optical modules ARC1&2 FODO STRAIGHT TRIPLET Review 09/2010 ARC3 FODO INJECTION INSERT Page 18 Tunability Review 09/2010 Page 19 Main Parameters Units Value 1 Circumference m 302 2 Angle at crossing deg 44 3 Number of dispersive FODO cells (Type I) 6 4 Number of dispersive FODO cells (Type II) 8 5 Number of triplet cells 18 6 Number of matching cells (2 types) 4 7 Minimum drift length between magnets cm 50 8 Drift length in the injection insertion m 5.0 9 Drift lengths between triplets (for RF, extraction, collimation and electron cooling) m 5.3 10 Beta maximum in X m 33 11 Beta maximum in Y m 36 12 Maximum beam size cm 2.3 12 Maximum vertical beam size in the dipole magnets cm 0.6 13 Maximum dispersion (x|delta_KE) m 3.3 14 Normalized dispersion value at injection insert m½ 2.1 15 Tune in X 7.92 16 Tune in Y 7.24 17 Gamma of particle 4.22 18 Gamma at transition energy 5.6 19 Momentum compaction 3.2E-2 Review 09/2010 Page 20 Magnets Quantity 1 2 3 Quadrupole Magnets Dipole Magnets (Type I) Dipole Magnets (Type II) Review 09/2010 Parameters Units Value Length cm 40 Half aperture cm 5 Maximum pole tip field T 1.5 Minimum pole tip field T 0.15 Strength T 1.41 Radius m 9.0 Vertical aperture cm 3.0 Angle deg 11.6 Length m 1.83 Strength T 1.41 Radius m 9.0 Vertical aperture cm 3.0 Angle deg 14.0 Length m 2.19 113 16 18 Page 21 Summary and Work in Progress • Presented a preliminary design of the linac and the accumulator/pre-booster, which satisfy the constraints while providing superior performance • • • • Fine tuning first order optics Space charge limits on current and emittance Spin and spin-orbit resonance analysis Dynamic aperture estimation Review 09/2010 Page 22 BACKUP SLIDES Review 09/2010 Page 23 Cavity subsystems • 4 kW capacitive coupler • Adjustable • 1 cold/warm windows • Pneumatic slow tuner • Piezoelectric tuner (PZT) • ~90 Hz window • 35 m displacement LN in beam Ceramic disk LN out PZT has been tested with excellent performance Review 09/2010 Page 24 Proton beam • Setting 1: • • • • Mass= 1, Charge= 1, Kinetic Energy = 3000 MeV Electric rigidity (χe) = 3.71E+9 V Magnetic Rigidity (χm) = 12.74 Tm Proton beam Emittance in x and y = 16 π mm·mrad • x=± 4mm y=± 4mm , • a=±4mrad b = ±4mrad • Kinetic Energy Dispersion (δKE/KE )= 1E-4 • Setting 2: • • • • Mass= 1, Charge= 1, Kinetic Energy = 200 MeV Electric rigidity (χe) = 3.68E+8 V Magnetic Rigidity (χm) = 2.14 Tm Proton beam Emittance in x and y = 140π mm·mrad • x=± 4mm y=± 4mm , • a=±35mrad b = ±35mrad • Kinetic Energy Dispersion (δKE/KE )= 1E-2 Review 09/2010 Page29-31 25July,2010 25 Main Parameters (1) • Energy range • Protons: from 200 MeV (β=0.57, γ=1.21) @ injection to 3 GeV (β=0.97, γ=4.2) at extraction • Lead ions: if fully stripped, from 80 MeV/u (β=0.39, γ=1.08) @ injection to 1.18 GeV/u (β=0.9, γ=2.26) @ extraction • Circumference • An integer multiple of it must be ~900-1000 m => ~250-300 m Review 09/2010 Page 26 Main parameters (2) • • Revolution times/frequencies • Protons @ injection: • {0.883753 μs,1.13154 MHz} if C=150m • {0.515181 μs,1.94107 MHz} if C=300m • Protons @ extraction: • {1.76751 μs,0.565769 MHz} if C=150m • {1.03036 μs,0.970533 MHz} if C=300m • Pb @ injection: • {1.29609 μs,0.771552 MHz} if C=150m • {0.557907 μs,1.79241 MHz} if C=300m • Pb @ extraction: • {2.59218 μs,0.385776 MHz} if C=150m • {1.11581 μs,0.896207 MHz} if C=300m If acceleration done with h=1 • RF swing necessary is [0.38,1.95] MHz Review 09/2010 Page 27 Cooling times • Assuming: • 3 m long cooling section • 300 mA electron current • 2.5 cm beam radius • ± 5 mrad beam divergence • ±0.004 momentum dispersion • Cooling for 3 time constants Transverse cooling time: ~ 130 ms Longitudinal cooling time: ~ 67 ms Cooling electron energies: • @ injection: { 0.55394 MeV, γ=2.0840 } • @ extraction: { 1.15511 MeV, γ=3.2605 } Review 09/2010 Page 28 Lead Charge Distributions • @ injection • Q (0) Q (1) Q (2) • 0 4% 70% • @ extraction • Q (0) Q (1) • 83% 17% Review 09/2010 Q (3) 22% Q (4) 3% Page 29 Intensities • Protons • If assuming 1A current, depending on circumference and injection/extraction: => N_p ~ [ 3 , 11 ] x 1012 • Lead ions • Under similar circumstances: => N_Pb ~ N_p / Q Review 09/2010 Page 30 Pre-Booster Cycle Time • Assuming 5x1010 lead ions need to be accumulated • One linac pulse delivers ~2x108 ions (assumed @ ~50% efficiency) • 50 linac pulses, 250 μs each • Total time = 50x 250 μs +50x130 ms+2x80 ms ≈ 7 s Review 09/2010 Page 31 Shorter Version Layout Review 09/2010 Page29-31 32July,2010 Shorter Version Lattice functions Review 09/2010 Page29-31 33July,2010 Shorter Version Parameters Units Value 1 Total length m 254 2 Angle at crossing deg 60 3 Number of dispersive FODO cells (Type I) 6 4 Number of dispersive FODO cells (Type II) 8 5 Number of triplet cells 12 6 Number of matching cells 4 7 Minimum drift length between magnets cm 50 8 Drift lengths in the insertion region m 5.0 9 Drift lengths between triplets (for RF, collimation and electron cooling) m 5.0 10 Beta maximum in X m 32 11 Beta maximum in Y m 32 12 Maximum beam size cm 2.5 12 Maximum beam size in the dipole magnets cm 0.6 13 Maximum Dispersion (x|delta_KE) 2.5 14 Normalized dispersion value at injection (x|δ_KE)/√β 1.41 15 Tune in X 7.24 16 Tune in Y 6.60 17 Gamma of particle 4.22 18 Gamma at Transition Energy 4.7 19 Momentum compaction factor 4.4E-2 Review 09/2010 Page29-31 34July,2010 Shorter Version Magnets Quantity 1 2 3 4 Quadrupole Magnet Dipole Magnet (Type I) Dipole Magnet (Type II) Dipole Magnet (Type III) Review 09/2010 Parameters Units Value Length cm 40 Half aperture cm 5 95 Maximum pole tip T field 1.5 Minimum pole tip T field 0.16 Strength T 1.41 Radius m 9 Vertical aperture cm 3 Angle deg 14 Length m 2.19 Strength T 1.41 Radius m 9 Vertical aperture cm 3 Angle deg 12.9 Length m 2.04 Strength T 1.41 Radius m 9 Vertical aperture cm 3 Angle deg 14.9 Length m 2.35 12 18 18 Page 35 New Layout with 5 quads in each matching section (302m) Review 09/2010 Page 36