LIU Day 2014 – M.Bodendorfer - LEIR model. LEIR model A plan for understanding/upgrading the LEIR performance limitations M.Bodendorfer BE/ABP & LEIR.

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Presentation transcript:

LIU Day 2014 – M.Bodendorfer - LEIR model

LEIR model A plan for understanding/upgrading the LEIR performance limitations M.Bodendorfer BE/ABP & LEIR team

LIU Day 2014 – M.Bodendorfer - LEIR model 3 LEIR performance, 2013 and LIU Ions Why upgrade? All HI LHC experiments want by 2035: 10nb -1 ParameterUnitLEIR 2013 run LEIR Baseline upgrade LEIR Full upgrade Pb charge state [-]54+ Output Energy[GeV/u] In/Out Bρ[Tm]1.138 / 4.8 Inject. to next machine [-]1 Bunches/ring [-]2 Charge at flat bottomCharges~6.0x x x10 11 Total extracted chargeCharges~5.4x x x10 10 From: PERFORMANCE OF THE INJECTORS WITH IONS AFTER LS1 D. Manglunki for the LIU-Ions team, CERN, Geneva, Switzerland, 2013

LIU Day 2014 – M.Bodendorfer - LEIR model 4 LEIR NOMINAL cycle 6 injections. First at 215ms, then spaced 200ms. 200μs long. 2880ms capture in H2, 1780ms Up to 50% beam loss (Coasting beam) B-field Start of Beam loss BHN current [100A]

LIU Day 2014 – M.Bodendorfer - LEIR model 5 Finding a solution for LEIR What we have found so far: 1.Working point on 4 th order resonance 2.Transverse instability at RF capture 3.Positive chromaticity in the vertical plane 4.Beam loss associated to RF-capture rather than magnetic Ramp Proposed MDs series dedicated to each of the above findings in 2014, 2015.

LIU Day 2014 – M.Bodendorfer - LEIR model 6 1. LEIR working point Design tune: Q H =1.82, Q V =2.72 Q x - Q y = -1 2Q x - Q y = 1 4Q y = 11 Q x + 3Q y = 10 3Q y = 8 2Q x + 2Q y = 9

LIU Day 2014 – M.Bodendorfer - LEIR model 7 Before: -20ms After: +20ms Beam loss continues 1815ms Beam loss starts here 2. LEIR Instability at RF capture and ramp Pickups output:

LIU Day 2014 – M.Bodendorfer - LEIR model ✗ Bad fit RF capture Displayed ✗ 3. Tune and chromaticity measurement after RF-capture

LIU Day 2014 – M.Bodendorfer - LEIR model Good fit RF capture Displayed ✓ Good fit (LSQR quadratic) ✓ 3. Tune and chromaticity measurement after RF-capture

LIU Day 2014 – M.Bodendorfer - LEIR model Horizontal chromaticity < 0 (after RF capt.) (Horizontal design chromaticy = -1) Good fit Fit slop (Linear chromaticity) Residual of fit Intensity

LIU Day 2014 – M.Bodendorfer - LEIR model Vertical chromaticity > 0 (after RF capt.) (Vertical design chromaticy = -1) Good fit Fit slope (Linear chromaticity) Residual of fits Intensity

LIU Day 2014 – M.Bodendorfer - LEIR model Disentangling beam loss from magnetic ramp Start mag. ramp Beam loss with advanced RF-capture Beam dump Start of Beam loss Advanced by 300ms BHN current [100A] RF beam bunching  Higher peak density increases space-charge  Individual particle tune shift  Individual particles cross resonance  Loss

LIU Day 2014 – M.Bodendorfer - LEIR model 13 Clues from measurements: 1.Working point on 4 th order resonance 2.Transverse instability at RF capture 3.Positive chromaticity in the vertical plane 4.Beam loss associated to RF-capture rather than mag. ramp Summary of observations BHN current [100A]

LIU Day 2014 – M.Bodendorfer - LEIR model 14 Measurement clue and suggested MD: 1.Working point on 4 th order resonance 1.Explore other regions of the tune space (Q y > 2.75) 2.Investigate chromaticity for new tune regions MD suggestions

LIU Day 2014 – M.Bodendorfer - LEIR model 15 Measuremene clue and suggested MD: 1.Working point on 4 th order resonance 2.Transverse instability at RF capture 1.Study effect of the transverse damper 2.Investigate origin of instability with transv. damper off MD suggestions

LIU Day 2014 – M.Bodendorfer - LEIR model 16 Measuremene clue and suggested MD: 1.Working point on 4 th order resonance 2.Transverse instability at RF capture 3.Positive chromaticity in the vertical plane 1.Chrom. < 0 for both planes 2.Qmeter software from PS MD suggestions

LIU Day 2014 – M.Bodendorfer - LEIR model 17 Measuremene clue and suggested MD: 1.Working point on 4 th order resonance 2.Transverse instability at RF capture 3.Positive chromaticity in the vertical plane 4.Beam loss associated to RF-capture rather than magnetic ramp 1.Try RF-capture with different beam parameters (bunch length and transverse emittances) to check the impact of space-charge. 2.Study the effect of electron cooling and acceleration. MD suggestions

LIU Day 2014 – M.Bodendorfer - LEIR model 18 Conclusion & Summary Further reading: Plans for the upgrade of CERN’s Heavy Ion Complex, D. Manglunki et al., CERN-ACC-Note LINAC3 tank2 phase change and LEIR performance, M. Bodendorfer, R. Scrivens, CERN-ATS-Note Chromaticity in LEIR performance, M. Bodendorfer & LEIR team, CERN-ACC-Note Longitudinal emittance reduction in LEIR of ion beams for LHC, M. E. Angoletta, M. Bodendorfer, A. Findlay. S. Hancock, D. Manglunki, upcoming So far we have: found working point on/close to resonance found transverse instability found wrong chromaticity Pb 54+ beam loss associated to RF-capture rather than the magnetic ramp The Plan: Dedicated MD series for each finding. Further disentangling of space-charge, transverse instability and resonant beam loss. Refine the optics model of LEIR.

LIU Day 2014 – M.Bodendorfer - LEIR model THANK YOU FOR YOUR ATTENTION!