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Beam losses in the CLIC drive beam: specification of acceptable level and how to handle them ACE 2010 02 04 Michael Jonker
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Beam losses in the CLIC drive beam: specification of acceptable level and how to handle them

Feb 14, 2016

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Beam losses in the CLIC drive beam: specification of acceptable level and how to handle them. ACE 2010 02 04 Michael Jonker. Beam loss detection and Radiation issues. (in the main tunnel). BLM system primary purpose: detection of onset of slow losses. - PowerPoint PPT Presentation
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Page 1: Beam losses in the CLIC drive beam:  specification of acceptable level and how to handle them

Beam losses in the CLIC drive beam: specification of acceptable level and how

to handle them

ACE 2010 02 04Michael Jonker

Page 2: Beam losses in the CLIC drive beam:  specification of acceptable level and how to handle them

Beam loss detection and Radiation issues. (in the main tunnel)

BLM system primary purpose: detection of onset of slow losses.

Operational beam loss background levels:• Tails on the beam entering the main linac and decelerators• Interaction with residual beam gaz.Loss levels limits• From Beam Physics: 0.1 % main beam, 0.1% each drive train• From Radiation damage over the lifetime of CLIC (1MGy/year see following slides)Hence, these limits will define the required vacuum performance• Resolution at operational background levels 20 % ?

Dangerous level of beam loss when 10-2 of DB or 10-4 of MB is lost on an single aperture restriction. (Rough estimate needs further detailed simulations)

Extended range for catastrophic (fast) losses: diagnostics only. (i.e. to better understand what happened, if ever something should happen)

Page 3: Beam losses in the CLIC drive beam:  specification of acceptable level and how to handle them

Effect of beam in matterNote: in energy density in cupper for Melting : 400 J g-1, Structural yield 62 J g-1

Material C Al Cu W

LEP Beam (100GeV, 445 nC)Energy Density @ shower core [J g-1] 0.64 1.68 22 112Energy Density @ IB 0.1 mm2 [J g-1] 778 719 624 510

CLIC Main Pulse (1.5 TeV, 186 nC, @ collimators)Energy Density @ shower core [J g-1] 3 9 122 614

Energy Density @ IB 40 mm2[J g-1] 8.3 105 7.7 105 6.7 105 5.4 105 2.2 103 /bunch

CLIC Main Pulse (2.8 GeV, 204 nC @ DR septum) Energy Density @ shower core [J g-1] 0.01 0.03 0.34 1.6

Energy Density @ IB 125 mm2 [J g-1] 2.3 105 2.2 105 1.8 105 1.5 105 600 /bunch

CLIC Drive Train (2.4 GeV, 24545 nC)Energy Density @ shower core [J g-1] 1.34 3.08 40 187

Energy Density @ IB 1 mm2 [J g-1] 4293 3964 3444 2810

Page 4: Beam losses in the CLIC drive beam:  specification of acceptable level and how to handle them

03.12.2009 CLIC OMPWG

Beam losses (DB 2.4 GeV)

2.4 GeV Lost before QP

1.5 TeV Lost in QP

Page 5: Beam losses in the CLIC drive beam:  specification of acceptable level and how to handle them

S. Mallows, T. Otto, CLIC Two-Beam Module Review, September 2009

Page 6: Beam losses in the CLIC drive beam:  specification of acceptable level and how to handle them

03.12.2009 CLIC OMPWG

Permitted fractional loss model (New model, Drive beam)

Loss point Beam dynamics

Old estimate

New Estimate

in QP 1.25 E-6 1.0 E-7 1.6 E-6before QP 1.25 E-6 -- 2.1 E-6in PET 1.25 E-6

Loss point Beam dynamics

Old estimate

New Estimate

in QP 1.25 E-6 4.7 E-7 1.9 E-5before QP 1.25 E-6 -- 2.0 E-5in PET 1.25 E-6 4.8 E-5

2.4 GeV

0.24 GeV

Based on radiation limits of magnets during 10 years x 6 month operation.Regular magnet design (no rad hard)

Page 7: Beam losses in the CLIC drive beam:  specification of acceptable level and how to handle them

Type of failures• Failures causing slow onset of losses

– Magnet system– Vacuum system (performance defined by tolerable operational losses)

– Slow drifts (alignment, temperature, …)Next pulse permit and safe by design(2 ms)

• Failures causing fast losses (“in-flight” failures)

– RF breakdown (effects on the beam under study)– Kicker misfiring (turn around kickers !)– Klystron trips (not applicable for DB)

Protection by fixed masks (Impedance?)