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Extraction line design constraints and choices

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and polarimeter) a considerable complication [removal would reduce cost and ease ... Beam shape at the SF of polarimeter. e.g. NbTi for 500 GeV. Baseline ... – PowerPoint PPT presentation

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Title: Extraction line design constraints and choices


1
Extraction line design constraints and choices
  • Rob Appleby
  • The Cockcroft Institute and the University of
    Manchester
  • Small crossing angle layout workshop
  • LAL, Orsay, France
  • 19th October 2006

2
What do I mean?
  • Small (and zero) crossing angle layouts are very
    challenging, due to
  • Beam conditions
  • Hardware and layout constraints
  • We have some experience of the small crossing
    angle design evolution, which Ill review
  • The fundamental challenges
  • Progress and problems with the Snowmass
    extraction line, developed by the 2mrad task
    force
  • An attempt at modularising the extraction line
    optics (because we need to change the optics
    considerably)

3
Purpose of the extraction line
  • The extraction line is the post-collision
    beamline of the machine, which must satisfy the
    following conditions
  • Transport the disrupted beam to the beam main
    beam dump for disposal
  • Transport the nominal beam to the beam dump (with
    the use of beam sweeping magnets)
  • Transport the beamstrahlung photons to a suitable
    photon dump
  • All the beam transport must occur with controlled
    and safe losses in magnetic elements and
    collimators
  • Provide post-IP diagnostics (? Stripped down
    version)
  • Provide sufficient separation between the
    incoming and outgoing beams
  • Allow satisfactory final focus optics in the
    event of shared magnets for incoming and outgoing
    beams

4
The old baseline
The baseline is now 14mrad/14mrad (14mrad was
derived from the 20mrad and is technological
easier and cheaper than the 2mrad)
5
Why is it difficult?
  • The beamstrahlung tail (large energy spread) and
    large angular divergence of the beam causes
    over-focusing and stronger deflections ( 1/E)
    increasing beam size and power losses (Large
    power means even small losses are bad)
  • The shared large-aperture magnets with the final
    focus are strong, causing strong focusing and
    large non-linear dispersion of the outgoing,
    off-axis beam
  • Beam size means diagnostics at SF difficult
  • Diagnostic and beam separation constraints
    require horizontal bending, which is difficult to
    manage due to beam energy spread
  • The small crossing angle gives a small beam
    separation, causing magnet design problems
  • Beamstrahlung shares the same aperture as the
    beam in the early part of the line, requiring
    large magnet apertures

6
Snowmass layout
  • Developed by 2mrad task force
  • Final doublet is shared, and a drift gives beam
    separation before first extraction line
    quadrupole
  • Extraction line magnets and collimators optimised
    to reduce beam size
  • Bore sizes derived from beam fit margin
  • Resulting apertures are largecostly
  • Vertical collimation chicane and collimators in
    early part of line to remove extreme
    beamstrahlung tail
  • Power losses too high in regions of parameter
    space
  • Key parameter is location of first extraction
    line quadrupolemove closer and reduce aperture
    at expenses of beam separation?
  • Diagnostics (energy spec. and polarimeter) a
    considerable complication removal would reduce
    cost and ease design
  • Beam transport properties bad for high
    beamstrahlung parameter

7
Modular approachin the final doublet region
FD region
FFS magnet
2 mrad
l3.5m
6 mrad
12cm
18m
? optical transfer
Two F-quads
to beam diagnostics
Close 1st order dispersion, but could optimise
for beam size
(consistent with ILC parameters group parameter
space)
8
Optics abstraction
X collimator
Y collimator
transverse Separation (120mm)
to dump
FQs bend
Quadruplet
Bendback
Polarimeter
FD
IP
e.g. NbTi for 500 GeV
dxdpx0
focus to sf ?ilt100, ?i0)
parallel to IP
R22-0.5?
SF (dy4cm)
  • Optimise layout for beam size transport?
  • Concerns are
  • Transport of higher order dispersion
  • Beam shape at the SF of polarimeter

9
Baseline latticeBeta functions
10
Baseline latticeDispersion
11
Reversed structureBeta functions
12
Conclusions
  • The small (and zero) extraction line designs
    provide considerable technical challenges to beam
    and magnet physicists
  • The Snowmass layout leaves several issues
    unresolved, including cost and technical
    feasibility
  • An attempt at a new optics was presented, with
    several attractive features. The magnet apertures
    will need careful study
  • Removing the diagnostics will considerably reduce
    complexity and cost
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