Summary Session Advanced Collimation CARE-HHH-APD BEAM'07 R. Assmann.

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Presentation transcript:

Summary Session Advanced Collimation CARE-HHH-APD BEAM'07 R. Assmann

Agenda

RWA, 1/10/2007 The Staged LHC Path Energy density at collimators (nominal 7 TeV) Stored energy in beams Number of LHC collimators State-of-the-art in SC colliders (TEVATRON, HERA, …) 1 MJ/mm 2 2 MJ Phase 1 LHC collimation 400 MJ/mm MJ88 Nominal LHC 1 GJ/mm MJ122 Ultimate & upgrade scenarios ~2 GJ/mm MJ≤ 138 Limit (avoid damage/quench) ~50 kJ/mm 2 ~10-30 mJ/cm 3 Factor > 1000 energy density Equivalent 80 kg TNT explosive

RWA, 1/10/2007 The LHC Upgrade Scenarios Scenario Protons stored Energy stored Energy in 200 ns ** Peak luminosity Phase 1 collimation 1.4 × MJ 0.4 MJ 0.55 m0.4 × Nominal3.2 × MJ 1.0 MJ 0.55 m1.0 × Ultimate4.8 × MJ 2.2 MJ 0.50 m2.3 × Scenario I4.8 × MJ 2.2 MJ 0.08 m15.5 × Scenario II6.9 × MJ 2.3 MJ 0.25 m10.7 × Improve stability and efficiency! Address collimator robustness or upgrade beam dump!

RWA, 1/10/2007 Collimation Issues for LHC Upgrade I Higher stored energy (higher peak losses, higher annual losses, higher activation): beam stability –Better or same beam stability (upgrade must not reduce beam stability – should be a decision criterion). spreading of losses –Better spreading of losses  Operational procedures to avoid local hot spots. collimation efficiency –Improved collimation efficiency  White paper, LARP, FP7 work. radiation hardness of collimators –Improved radiation hardness of collimators  White paper, LARP, FP7 work. power absorption –Improved power absorption  White paper, LARP, FP7 work. local protection or more radiation-hard warm magnets –Improved local protection or more radiation-hard warm magnets  Experience will show whether needed (less leakage with phase 2). shielding of electronics –Improved shielding of electronics  Experience will show whether needed. –Radiation impact –Radiation impact study. beam dump and protection devices –Upgrade of beam dump and protection devices. super-conducting link cable in IR3 –Upgrade of super-conducting link cable in IR3.

RWA, 1/10/2007 Collimation Issues for LHC Upgrade II Higher beam intensity (intensity dependent effects from collimator- driven LHC impedance): chromaticity –Operation with increased chromaticity. transverse feedback –Upgrade of transverse feedback. collimator gaps opened –Operational collimator gaps opened, if efficiency/protection/halo allows to do this. conducting collimator jaw material –Better conducting collimator jaw material  White paper, LARP, FP7 work. Higher shock beam impact from irregular dumps: LHC beam dump –Upgrade of the LHC beam dump to reduce amount of escaping beam. collimator robustness –Address collimator robustness  White paper, LARP, FP7 work.

RWA, 1/10/2007 Collimation Issues for LHC Upgrade III Layout, aperture and optics changes in experimental insertions: –Local collimation and protection tertiary collimation –Local collimation and protection must be re-evaluated in detail such that tertiary collimation (effect on background) is kept functional. rebuild tertiary collimators –Probably need to rebuild tertiary collimators for ATLAS and CMS. simulation of multi-turn halo losses in local aperture, power loads, machine protection and energy deposition –Full simulation of multi-turn halo losses in local aperture, power loads, machine protection and energy deposition is absolutely essential. halo dynamics with potentially increased off-momentum beta- beat –Full study of halo dynamics with potentially increased off-momentum beta- beat. local triplet masks also for the incoming beam –Collimation request: local triplet masks also for the incoming beam (best possible protection and cleaning)! Important not to underestimate the overall effects from local changes in the experimental insertions!

RWA, 1/10/2007 Future Plans extrapolation in stored energy by factor 100Powerful LHC collimation system is being installed. Should allow extrapolation in stored energy by factor 100. limited due to beam loss and collimationNevertheless, it can well be that nominal and ultimate LHC intensities already are limited due to beam loss and collimation. phase 2 collimationWork already ongoing or being prepared for phase 2 collimation with support from CERN white paper, LARP and FP7 (if approved): –Better efficiency –Better radiation hardness –Better power absorption –Better conducting jaws –More robust jaws or in-situ handling of damage –Improved operational setup with jaw-internal diagnostics No magic bullet  Several improvements together will get us ready for LHC upgrade scenarios!

Agenda

Beam’ October 2007LARP Phase II Collimation - T. Markiewicz LHC Phase II Base Concept physical constraints current jaw design beam beam spacing: geometrical constraint Length available 1.47 m flange - flange Jaw translation mechanism and collimator support base: LHC Phase I >10 kW per jaw Steady State heat dissipation (material dependent) Cu coolant supply tubes twist to allow jaw rotation Hub area Glidcop Cu Mo Cantilever Mo both ends Helical cooling channels 25mm below surface 20 facets

Beam’ October 2007LARP Phase II Collimation - T. Markiewicz Up Beam end beam side view Spiral style backing springs reside inside “Sheath” (sheath not shown) Thin sheet metal RF “Curtain” Round to Square Transition Transition “Socket” Spherical profile “Fingers”

Beam’ October 2007LARP Phase II Collimation - T. Markiewicz Final Wind of First 200mm Copper Mandrel

Beam’ October 2007LARP Phase II Collimation - T. Markiewicz Braze Test #3: Vacuum tests 3rd Jaw Braze Test Assembly has been vacuum baked at 300 degrees C for 32 hours. Results in slightly lower pressure. Inclusion of longitudinal grooves in the inner length of jaws for better outgasing Test Chamber setup similar to previous test. OldNew Baseline3.2E-9 Torr2.4E-9 Torr?? w/ jaw assy.3.7E-9 Torr3.4E-9 Torr Presumed jaw assy. pressure 4.5E-10 Torr10E-10 Torr?? LHC requirement 7.5E-10 Torr

Beam’ October 2007LARP Phase II Collimation - T. Markiewicz LARP Collimator Delivery Schedule DoneBraze test #1 (short piece) & coil winding procedures/hardware Prep heaters, chillers, measurement sensors & fixtures, DAQ & lab Section Braze test #2 (200mm Cu) and examine –apply lessons Braze test #3 (200mm Cu) – apply lessons learned Fab/braze 930mm shaft, mandrel, coil & jaw pieces st full length jaw ready for thermal tests Fab 4 shaft supports with bearings & rotation mechanism Fab 2 nd 930mm jaw as above with final materials (Glidcop) and equip with rf features, cooling features, motors, etc. Modify 1 st jaw or fab a 3 rd jaw identical to 2 nd jaw, as above Mount 2 jaws in vacuum vessel with external alignment features full length jaws with full motion control in vacuum tank available for mechanical & vacuum tests in all orientations (“RC1”) Modify RC1 as required to meet requirements Final prototype (“RC2”) fully operational with final materials, LHC control system-compatible, prototype shipped to CERN to beam test

Agenda

1 October 2007Reflection on bent crystals p Beam propagation Sensitive equipment Primary halo (p) Absorber  Primary halo directly extracted!  Much less secondary and tertiary halos  Larger gap in the secondary collimators e  Shower Crystal Crystal collimation Beam Core …but not enough data available yet to substantiate the idea… E. Tsyganov & A. Taratin (1991)

1 October 2007Reflection on bent crystals Particle-crystal interaction Possible processes:  multiple scattering  channeling  volume capture  de-channeling  volume reflection d U Volume reflection Prediction in 1985-’87 by A.M.Taratin and S.A.Vorobiev, First observations in 2006 (IHEP - PNPI - CERN)

1 October 2007Reflection on bent crystals Rotation angle (µrad ) Angular profile (µrad) 1 -“amorphous” orientation 2 -channeling 3 -de-channeling 4 -volume capture 5 -volume reflection Angular beam profile as a function of the crystal orientation The particle density decreases from red to blue The angular profile is the change of beam direction induced by the crystal The rotation angle is angle of the crystal respect to beam direction

1 October 2007Reflection on bent crystals High statistics Best alignment  Volume reflection angle 53  rad  Efficiency  90 % Steps to align the five crystals Multi Reflection on Quasi-Mosaic Crystals (2)

1 October 2007Reflection on bent crystals Conclusion  High efficient reflection (and channeling) observed in single pass interaction of high-energy protons with bent crystals (0.5 to 10 mm long)  Single reflection on a Si bent crystal deflects > 98 % of the incoming 400 Gev p beam by an angle 12÷14  rad  Multi-reflections on a sequence of aligned crystals to enhance the reflection angle successfully tested with two and five consecutive crystals.  Axial channeling observed (scattering enhancement) Very promising results for application in crystal collimation

Agenda

Discussion LHC(+) collimation issues: –Risk associated with radiation damage to CFC material. –Expected limitations for intensity, beam loss rates and LHC performance. –SNS experience supports criticality of collimation (already facing loss limitations). –Diffusion models and size of impact parameter are crucial. SLAC/LARP phase 2 work: –Material choice for phase 2: Glidcop. –Risk when bending cooling pipes must take radiation effects into account. –Extent of expected jaw damage after beam impact. Crystals: –Acceptance of crystals in particle angle. –Complements conventional collimation – surface effects at crystal. –Radiation-hardness of crystals. –Experimental program (CERN, FNAL, …). Electron lens: –Will still need efficient collimators, does not replace them. –What increase in impact parameter at collimators. –Can efficiently smooth out loss spikes (solution for possible major LHC issue). –Inherently safe with collimators still in place.

Conclusion Beam loss and collimation issues are challenging and are inspiring new solutions… Lively session with plenty of discussion past 6pm. –Thanks to the speakers and the audience for this! The story on collimation at LHC and other high power accelerators (SNS, FAIR, …) is just starting: –Lot´s of lessons will be learnt from the beam with the phase 1 LHC collimation system. –SNS experience shows this: several loss issues addressed there with high priority. –Plenty of new ideas and concepts available for getting full performance reach of the LHC  not just ideas… –The advanced ideas are being tested and made to work through hardware prototyping (SLAC/LARP) and beam tests (FNAL/LARP, CERN, crystal collaboration). Future work funded through CERN white paper, FP7 and LARP. Session showed that collaboration is really fruitful…