overview of beam delivery system final focus optics collimator final doublet extraction/dump others...
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![Page 1: Overview of Beam Delivery System Final Focus Optics Collimator Final Doublet Extraction/Dump Others S.Kuroda ( KEK ) MDI meeting at SLAC 1/6/2005](https://reader036.vdocuments.net/reader036/viewer/2022070415/56649d395503460f94a12f31/html5/thumbnails/1.jpg)
Overview of Beam Delivery System
• Final Focus Optics• Collimator• Final Doublet• Extraction/Dump• Others
S.Kuroda ( KEK )
MDI meeting at SLAC 1/6/2005
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Final Focus Optics1. Beam size blow-up due to energy spread( chromatic effect ) Generally is large for FF. ( =103~104, mainly from final Q)2. Chromaticity correction introducing SX.3. SX also introduces geometric aberration(GA). Need another SX and special optics for the GA cancellation
Two Cancellation Scheme “Traditional” :GA cancelled by -I optics between SXs “Local Correction” : corrected locally
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Traditional Optics
TESLA TDR
correction by SX far upstream of IP Transfer matrix of -I between SXs = ’=0 at IP
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Local Correction Optics
[J.Payet, O.Napoly]
NLC BDS
[A.Seryi et al]
New TESLA BDS
corrected locallyGA must be corrected by optics 2nd order correction also required
c=0 Long drift space for dump
Collimator in FFSOCT tail folding works good
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Summary of Optics
‘Traditional Optics’ ‘Local Correction Optics’
• Easy to understand
• Tested at FFTB
• Wide momentum band width
• Expandability to high energy
• Compact beam line
Recent design tendency is ‘Local Correction Optics’
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CollimatorMachine( Detector ) ProtectionBackground to Detector SR of Beam Halo at Final Q
Collimation with spoiler+absorber Energy Collimation Betatron CollimationNon-linear field in beam line Simulation is required for performance check
[TESLA]
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Energy Collimation
SR protection x+Lp = (+L ’)< r
Detector protection Background study
High dispersion & low beta section
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Betatron Collimation
High beta & dispersion free sectionNeed iterative collimation for action variable cut in phase space(Optional use) Periodic Optics with = 45° emittance measurement
2J
L cos Lsin
2J L 2 L2
SR by e of (x, p) at distance L x+Lp=
(in action-angle var.)< aperture
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Performance of Collimator
Better collimation performance in NLC/CLIC(beta+collimation+local correction FF is better than (+beta)collimation+traditional FF ?
[A.Drozhdin et al]
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Other Machine Protection Magnetic Energy Spoiler(MES) OCT+skew SX Large beam kicked by OCT horizontally large x in skew SX x-y coupling & beam blow-up
Fast Extraction Line Long bunch spacing in Cold machinemuch enough time to detect error and fire kicker
[TESLA]
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Other Issue for Collimator
Spoiler & Absorber Wake field Heat load survivability/life time
Muon collimationsurvivable spoiler [A.Seryi]
Fast emergency extractionline is necessary
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Final Doublet
Normal Electric Magnet• Established technology• Heat loadcooling
Crossing angle c & L* is the critical parameters for designOutgoing beam go inside or outside of the bore
[T.Mihara,O.Napoly 1st ILCWS]
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Super-conducting Magnet• High gradient/Low power consumption• Large bore radius ( common with outgoing beam )• Vibration? He flow in cryostat
Various type of SC magnets are proposed
LHC
Small bore/double aperture
Compact SC magnet
Flat inner tube
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Permanent Magnet
• High gradient w/o power consumption • Compact/small bore • Fine tuning for temperature/ rad. Damage
Adjusting for big E change( e.g. Z-pole ) Hybrid Field compensation mover
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Summary for Final Doublet
EM SC PM
• Established technology
• Power consumption
cooling
• High gradient
• Large bore( generally )
• Vibration?
• High gradient • Compact/small bore • Adjustability / tunability
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Beam Extraction/Dump • Charged beam extraction
Boundary condition by c and L* Diagnostic section 1) Energy 2) Polarization …… Chicane for photon separation 2nd focusing point for Laser collision Machine protection by beamstrahlung • Dump for beamstrahlung? • Background( neutron ) study from the extraction/dump ……•
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TESLA Extraction
Head-on schemeIrradiation of septum magnetNo beam diagnostic after collision is considered
optics
Beam size when no collision
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GLC ExtractionGeometry
optics
7mrad crossingSuperconducting final Q is assumed (out-going particle goes inside of Q )Diagnostic section is considered.
Transmission and background study need more to do
[K.Kubo]
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Extraction for 20mrad crossing
2nd focal point in vertical chicane for beam diagnosisGood transmission for disrupted beam
[Y.Nosochkov]
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Others• Straw-man layout for ILC BDS
Yuri’s ILC 20 mrad dump lines
IR120 mrad
IR22 mrad
Andrei’s 20 mrad ILC FF (x 4)
NLC BSYdump lines
11 mrad NLC-styleBig Bends
200 m drifts
IP separation:150 m (Z), 22 m (X)
Design done except Pre-IP E-spectrometer FEXL Extraction for 2mrad
[M.Woodley]
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• Solenoid Field Compensation
LD model, = 20 mrad
LD model, = 0
Solenoid field at FD beam size blow-up( independent on crossing angle )
With antisolenoids and linear knobs, y = 0.9%
Total field with and w/o antisolenoids
Anti-solenoids provide good compensation, and it is considered as a part of detectorMore effective with skew Q
[Y. Nosochkov, A. Seryi]
Anti-solenoid compensation