D. Still-FNAL/Tevatron HALO '03 Tevatron Collider II Halo Removal System Dean Still Fermilab Tevatron Department 5/21/2003 Motives for the Collider Run.

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Presentation transcript:

D. Still-FNAL/Tevatron HALO '03 Tevatron Collider II Halo Removal System Dean Still Fermilab Tevatron Department 5/21/2003 Motives for the Collider Run II Collimator Halo Removal System upgrade. Halo Removal System Overview. Run II experience of halo removal and attempts to manage halo background losses at the IP’s – CDF and D0.

D. Still-FNAL/Tevatron HALO '03 Collimator System Upgrades for Run-II Wanted to move to commercial hardware to replace in house motion controls. –Collimators are faster and more reliable. –Each Collimator would be able to do feedback processing. Wanted to move to a more automated system to reduce shot setup time and integrate controls with the Collider Sequencer. –Goal was to shot setup Halo Removal times of about 5 min. Wanted to move to a 2 stage collimator halo removal system. –Build 4 new targets and 8 new secondary collimators.

D. Still-FNAL/Tevatron HALO '03 Collimator System Upgrade Designs for Collider II New design for the collimator system came from: Tevatron Run-II Beam Collimation System A.I Drozhdin and N.V. Mokhov This paper along with the experience from Run-I was the basis for designing the controls and sequence of motion for the Tevatron collimator system.

D. Still-FNAL/Tevatron HALO '03 2 Stage Collimator System ~5   Scattered trajectories

D. Still-FNAL/Tevatron HALO '03 Tevatron Collimator Layout 12 collimators total: 4 Targets 8 Secondary collimators Arranged in 4 sets: 2 proton sets 2 pbar sets Proton Set 1 D49 Tar, E03 & F172 2 nd Proton Set 2 D171Tar, D173 & A0 Pbar Set 1 F49 Tar, F48 & D172 Pbar Set 2 F173 Tar, F171 & E02

D. Still-FNAL/Tevatron HALO '03 Collider II 1.5m Collimator

D. Still-FNAL/Tevatron HALO '03 Collider II Target with 5mm Tungsten wing.

D. Still-FNAL/Tevatron HALO '03 Collider II 1.5m E0 Secondary Collimators.

D. Still-FNAL/Tevatron HALO '03 Tunnel Layout of Collimator Local Loss Monitors Local Loss Monitors used for pbar losses Protons Local Loss Monitors used for proton losses F171 Collimator F172 Collimator F173 Target F17 Spool F17 Dipole F17 Kicker

D. Still-FNAL/Tevatron HALO '03 Collimator Controls Hardware

D. Still-FNAL/Tevatron HALO '03 Overview of New Software Fast Processing : Loss Monitor & Intensity Feedback. X0Xi N*  Front End OAC Application Global Orchestration: Employs states and collimator moving map. Configure/view, Initiate Process: Can use sequencer initiate scraping.

D. Still-FNAL/Tevatron HALO '03 The left side portrays the details of the movement for D49H1 target for Begin Halo Removal. C10 - Controlling one Collimator

D. Still-FNAL/Tevatron HALO '03 Tevatron Shot Setup Process Inject 36 final protons Open Helix & Inject 9 Trans of 4 Pbar bunches Accelerate Goto Lowbeta Remove Halo

D. Still-FNAL/Tevatron HALO '03 Example of D49 movement during Halo Removal Process Fine Scrape process: Scrapes.4% of proton beam Find the edge of the beam Initial Move No feedback Before Halo removal CDF proton loss After Halo Removal CDF proton loss Retracted ~ 40mils or 1mm

D. Still-FNAL/Tevatron HALO '03 Proton & Pbar Targets moving during Halo Removal Proton bunched beam intensity Pbar bunched beam intensity F49 local BLM D49 local BLM

D. Still-FNAL/Tevatron HALO '03 Merit of Halo Removal Efficiency D49 Target position F172 Hor Coll. position CDF proton Halo counter CDF pbar halo counter CDF proton halo loss reduced by factor of 9 CDF pbar halo loss reduced by a factor of 28 D0 proton halo loss reduced by a factor of 1 D0 pbar halo loss reduced by a factor of 100

D. Still-FNAL/Tevatron HALO '03 CDF & D0 Proton Halo Loss vs. Proton Intensity D0 Proton Halo Loss CDF Proton Halo Loss

D. Still-FNAL/Tevatron HALO '03 CDF & D0 Pbar Halo Loss vs. Pbar Intensity D0 Pbar Halo Loss CDF Pbar Halo Loss

D. Still-FNAL/Tevatron HALO '03 F172 Horizontal Retraction Scan (with D49 target in) Into the beam CDF proton halo loss F17 local loss monitor

D. Still-FNAL/Tevatron HALO '03 Halo losses and collimator angle Beam 1.5m collimator Good if < 10 mils difference from upstream to downstream. Live with >10 and <30 mils difference from upstream to downstream. Bad if > 30 mils difference from upstream to downstream.

D. Still-FNAL/Tevatron HALO '03 Typical halo losses during store 2549 D0 proton halo D0 pbar halo CDF pbar halo CDF proton halo

D. Still-FNAL/Tevatron HALO '03 Collider Run II History of Experiences DateEvents June 2001Used Automatic Halo removal system for first time Aug 2001CDF experiencing power supply failure to crates on. CDF sees “spikes” on proton halo losses and muon chambers. Dec – Jan 2001Tevatron quenches on abort due to DC beam. “Spikes” on CDF proton halo loss persist. Jan-June 2002Experience proton halo loss growth during stores due to poor F11 vacuum. Feb 2003CDF added shielding at proton end of detector. Tevatron removed C0 Lambertson- known aperture limit. March 2003Rash of A0 abort kicker prefires lead to addition of A48 collimator.

D. Still-FNAL/Tevatron HALO '03 Retracting F172H effects losses in Muon chambers at CDF Retreact F172 collimator Muon Chamber Loss

D. Still-FNAL/Tevatron HALO '03 DC Beam at Collisions A4 DC beam monitor 36 proton bunches Abort Gap

D. Still-FNAL/Tevatron HALO '03 TEL getting rid of DC beam TEL ON DC BEAM Intensity CDF Proton Halo loss Proton Bunched Beam

D. Still-FNAL/Tevatron HALO '03 Effects of reducing spikes on proton halo losses with TEL TEL ON DC Beam Intensity CDF Muon Losses CDF proton halo loss

D. Still-FNAL/Tevatron HALO '03 CDF Proton Halo loss “spikes” correlated to horizontal orbit motion CDF proton halo Loss counter Out of single BPM Processed to provide Orbit motion. Hor and Ver

D. Still-FNAL/Tevatron HALO '03 Addition of A48 Collimator to Protect against A0 abort kicker prefires Add.5 m Collimator at A48 to shield against prefires A11V collimator Already in place A0 proton abort kickers Date# Prefires Run I4/ / Run II3/2001- present 7

D. Still-FNAL/Tevatron HALO '03 In Closing: The design and implementation of the collider II halo removal system has worked well as far as reliability, speed, ease of use and status mechanics of conducting halo removal. The efficiency of reducing halo loss seems to be reasonable except for proton losses at D0 which requires more understanding. Only 1 proton and pbar collimator sets are used for halo removal. The other sets do not have much effect. The collimators require “aligning” once in awhile to reduce losses from beam not parallel to collimator. The TEL is an operational must in order to maintain spikes in CDF proton halo losses and remove DC beam accumulated in the abort gaps through out the length of a store. Attempts are being made to understand and improve overall vacuum. An additional.5 m collimator will be installed at A48 in order to reduce