Transcript Slide 1
Collimator Functionality, Performance and First View on Set-up and Optimization R. Assmann AB/ABP, CERN Part of discussions on commissioning of machine protection related system: B. Dehning, B. Goddard, M. Lamont, J. Wenninger, R. Schmidt External Review of the LHC Collimation Project June 30th - July 2nd 2004 R. Assmann Outline • Functionality of the LHC collimator • Performance estimates • Set-up and optimization • Conclusion R. Assmann The LHC Type Collimator If we say collimator: R. Assmann We mean a collimator with two parallel jaws! Each jaw controllable in position and angle! Functionality Side view at one end Calibration: Inside vs outside gap etc Microphonic sensor Temperature sensor Reference Reference Motor Motor Gap opening (LVDT) Resolver R. Assmann Resolver Gap position (LVDT) Not shown: IN, OUT, ANTI-COLL switches! Functionality Side view at one end Calibration: Inside vs outside gap etc Microphonic sensor Temperature sensor Reference Reference Motor Motor Gap opening (LVDT) Resolver R. Assmann Gap position (LVDT) Resolver Basic control in-/output Basic input: Motor setting: jaw position at each end Readings: Control position and angle of each jaw independently! For each motor: Local resolver reading For each end of the jaw: Monitoring: R. Assmann Gap width Gap position Temperature, switches, micro-phonic sensors For set-up We can guarantee a gap in mm to several 10’s of mm! However, we must set to beam s, e.g. 6 s for primary collimators! Understand beta function at collimator! Must be known to 20% anyway for aperture before serious commissioning J. Wenninger! Collimator gaps can be set to better ± 0.6 s from basic aperture tolerances! Major task for collimation set-up: R. Assmann Centering of gap around the beam! Inefficiency and Allowable Intensity Allowed intensity Quench threshold (7.6 ×106 p/m/s @ 7 TeV) N pmax Rq Ldil /c Beam lifetime (e.g. 0.2 h minimum) R. Assmann Dilution Length (50 m) (Luminosity) Cleaning inefficiency = Number of escaping p (>10s) Number of impacting p (6s) How to get collimators going for phase 1 Start at low intensity: Need for less cleaning efficiency! No collimation Pilot bunch Single-stage collimation ~ 500 bunches (inj) ~ 20 bunches (top) b-cleaning: 2 primary coll. momentum cleaning: 1 primary coll. Help with local tertiary coll. Limited two-stage collimation Intermediate intensities Bring on secondary coll. b-cleaning: ~ 7 TCS momentum cleaning: ~ 4 TCS Full two-stage cleaning R. Assmann Up to 50% of nom. intensity b-cleaning: 11 TCS momentum cleaning: 4 TCS Components for the Collimation System (Phase 1) Label Number per beam Material Jaw length [m] Collimators Primary betatron Secondary betatron TCP TCSG 3 11 CC CC 0.2 1.0 Primary momentum Secondary momentum TCP TCSG 1 4 CC CC 0.2 1.0 TCT 6 Cu/W 1.0 TCHS TCHS 2 1 tbd tbd tbd tbd TCLI TCLP TCLA 2 2 (8) CC Cu/W Cu/W 1.0 1.0 1.0 Tertiary triplets Focus of review Most difficult! Number of objects: 80 + 13 spares Scrapers Betatron Momentum Absorbers Injection errors Luminosity debris Cleaning showers R. Assmann Per beam: 25 collimators 3 scrapers 12 absorbers Collimators / Scrapers / Absorbers Components of the collimation system are distinguished by their function: Collimators: Elastic and inelastic interactions of beam protons. Precise devices with two jaws, used for efficient beam cleaning. Small gaps and stringent tolerances. Scrapers: Used for beam shaping and diagnostics. Thin one-sided objects. Absorbers: Absorb mis-kicked beam or products of proton-induced showers. Movable absorbers can be quite similar in design to collimators, but mostly with high-Z jaws. Larger gaps and relaxed tolerances. Precise set-up and optimization in first line affects collimators! R. Assmann Set-up of single collimator BLM Beam BLM R. Assmann Set-up of single collimator 1-by-1 procedure: 1. Lower intensity 1 stage cleaning is sufficient. 2. Scraping of beam to ~ 3 s 3. Move in single jaw. One edge after the other. 4. Second jaw the same way. 5. Collimator to reference position (record) and then out. 6. Next collimator… No problem of cross-talk (do both beams at same time). Need good BLM system (B. Dehning, B. Holzer) adjusted to set-up. R. Assmann Set-up of single collimator BLM Beam Shower BLM R. Assmann Set-up of single collimator BLM Beam Shower BLM R. Assmann Set-up of single collimator BLM Beam Shower BLM R. Assmann Set-up of single collimator BLM Beam Shower BLM R. Assmann Set-up of single collimator BLM Beam Calibrated center and width of gap, if beam extension is known (e.g. after scraping). Advance with experience! Rely on good BLM system... R. Assmann BLM Advance procedures Put all collimators to same normalized setting! Assume we want to center gaps... R. Assmann Advance procedures Grow beam emittance... Shower R. Assmann Advance procedures Grow beam emittance... Shower R. Assmann Advance procedures Grow beam emittance... Shower R. Assmann Advance procedures Grow beam emittance... Shower R. Assmann Advance procedures Grow beam emittance... Shower R. Assmann Advance procedures Grow beam emittance... Shower R. Assmann Advanced procedures • In principle we could optimize many collimators at once. • Efficient procedures should be prepared! • Can also imagine long orbit bumps through collimation insertions with equal settings similar to emiitance growth procedure! • Do at lower intensity, where one-stage cleaning is sufficient (20 nom. bunches at 7 TeV, more at injection). • Maybe less for machine protection!? • Detailed simulations for these set-up procedures will be done required and achievable tolerances (~0.1s or 20 mm)!? • SPS: Test for single collimator set-up! R. Assmann Fine tuning of performance • Best cleaning efficiency to avoid quenches! • Look at places where losses are highest! Critical BLM’s! • Use critical BLM’s for empirical optimization of collimator settings (within limits): Trial and error procedure! • Similar to regular machine tuining (orbit, ...). Just watch out not to get the collimators damaged: Limits on tuning range (several s?). R. Assmann Loss Maps Around the Ring: Injection Tertiary halo Aperture model for 27,000 m LHC with 0.1 m longitudinal resolution: ~ 270,000 loss points! S. Redaelli G. Robert-Demolaize Q6 downstream of betatron cleaning: first SC magnet Acceptable!? Understand effect of azimuth on quench. Help further with absorbers in IR7! R. Assmann Loss Maps Around the Ring: Collision Peaks in all triplets: Tertiary halo Cure with tertiary collimators! Work is ongoing... Massive computing effort: 9 × 106 p tracked over 100 turns through each LHC element! 27,000 loss points checked in aperture! So far only tertiary halo: Include also secondary halo. IR8: Initial optics with b* = 1 m R. Assmann Future data generated from SIXTRACK! Conclusion • Preliminary thoughts on set-up and optimization. • Evolutionary process: no collimation – 1 stage – limited 2 stage – full 2 stage. Help by tertiary collimators! • Time scale of months/years not all collimators needed for day 1. Learn while the LHC performance is being pushed! • Set-up of single collimator: Standard procedure exists and is used successfully at other laboratories (adjust position and angle)! Test with LHC collimator in the LHC! • Advanced procedures: Should work to efficiently set up many collimators! • All of this will be simulated in detail! • Goal: Procedures ready and implemented for LHC start-up in 2007! Then make them work... R. Assmann