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SLAC HEP Activities: NLC and PEPII Support

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Marco Venturini, John Byrd, Daniel Lee, Kurt Kennedy. DoE HEP Review. February 2004 ... LBNL leads the Damping Ring studies. Lattice design and dynamics studies ... – PowerPoint PPT presentation

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Title: SLAC HEP Activities: NLC and PEPII Support


1
SLAC HEP ActivitiesNLC and PEP-II Support
  • Andy Wolski, Christoph Steier,Marco Venturini,
    John Byrd,Daniel Lee, Kurt Kennedy
  • DoE HEP Review
  • February 2004

2
LBNL collaborates closely with SLAC on HEP
projects
  • Linear Collider
  • LBNL leads the Damping Ring studies
  • Lattice design and dynamics studies
  • Studies of collective effects (electron cloud
    etc.)
  • Oversight of technical and engineering issues
  • Contribution to experimental program at KEK-ATF
  • Contributes to activities of US Linear Collider
    Steering Group
  • LBNL represented on Accelerator Subcommittee
  • Contributed to review of US-sited LC options
  • Providing information for ITRP
  • PEP-II
  • Improving present performance through lattice
    studies
  • Validation of interaction region optics model
  • Optics studies/analysis of closed orbit response
    matrix
  • Planning for luminosity upgrade (21034 by July
    2006)
  • Low-? lattice designs to benefit from reduced ?
  • RF system upgrade to allow stable beam at higher
    currents

3
NLC DR lattices revised in 2003 raised
instability thresholds
  • Previous lattice design was reworked to increase
    momentum compaction (by reducing dipole field)
    and lengthen the bunch.
  • Reduced strength of dipole field compensated by
    additional20 m of wiggler to preserve damping
    time.
  • Wiggler has strong nonlinear effects
  • Detailed model needed to estimate impact on beam
    dynamics.
  • 60 kW mean injected beam power requires 100
    injection efficiency.
  • Highly stable operation at high beam current
    needed
  • Detailed studies of collective effects have begun.

4
Developed new techniques for modeling wiggler
effects
  • Problem of modeling wiggler effects breaks down
    into two parts
  • Accurate representation of 3D wiggler field is
    needed.
  • Effect of wiggler field on beam dynamics must be
    determined.
  • Cylindrical mode expansion provides fast and
    accurate field fitting.
  • Ideas for fast symplectic integration are being
    explored.
  • Continuing collaboration with Cornell to
    benchmark new techniques
  • Effects of new wigglers on dynamics in CESR-c to
    be studied.

Field profile of CESR-c 8 pole wiggler.
Error using a 3D multipole field representation
through azimuthal 14-pole term.
5
Nonlinearities cause large tune shifts with
amplitude
Frequency map in tune space
Vertical tune shift
Horizontal tune shift
  • Large tune shift spreads beam particles through
    a number of resonances
  • Control tune shift as a way to make motion more
    regular? Improve dynamic aperture?

6
Octupoles can be effective in controlling tune
shifts
  • Use two families of octupoles distributed through
    wiggler sections.
  • Aim for a dynamic aperture of 15 injected beam
    size.

Dynamic aperture in co-ordinate space. 15
injected beam size is approximately 12 mm 3.8
mm.
Qx2Qy
Dynamic aperture in tune space, using octupoles
to control the tune shifts.
7
The wiggler also makes electron cloud more severe
Simulated cloud density in TESLA wiggler.
  • Electrons accelerated by positron beam generate
    high numbers of secondaries by impact with wall
    of vacuum chamber.
  • Magnetic fields can confine the electrons and
    lead to high densities.
  • Electron cloud drives beam instabilities.
  • Collaboration with SLAC to research possibility
    of preventing build-up of the cloud using low
    secondary yield coatings.

Cloud density vs chamber SEY in TESLA wiggler.
TiN coatings produced at LBNL for analysis at
SLAC.
Simulation results from Mauro Pivi (SLAC).
TiN coating on Al
Gold coating on stainless
8
Resistive wall wake field drives single bunch
instability
  • Threshold appears at a few times nominal bunch
    charge.
  • Including other sources of impedance will lower
    the threshold.

Longitudinal phase space at nominal, 8 nominal,
and 12 nominal bunch charge.
Growth of quadrupole mode amplitude with bunch
charge.
9
Resistive wall also drives multibunch instability
  • Tracking simulations to determine growth rates
    include radiation damping and resistive wall wake
    field
  • Bunch-by-bunch feedback can be used to suppress
    unstable modes.

t 0 ms
t 10 ms
10
Recent experimental results at ATF support IBS
theory
  • Results obtained by KEK-ATF group using low
    emittance beam.
  • Record low emittance of 4 pm, meets specification
    for NLC DRs.
  • LBNL/SLAC contributed through studies of
    beam-based alignment.
  • Reliable measurements obtained using advanced
    diagnostics.
  • Calculations for present NLC damping ring lattice
    indicate IBS emittance growth will be within
    tolerable limits.

Variation of bunch length, horizontal and
vertical emittance with bunch intensity in
KEK-ATF under various coupling conditions.
Calculations of IBS bunch length and emittance
growth in the NLC MDRs. The red dashed lines
show the design specifications.
11
Quality of work on DRs recognized by NLC MAC
  • From NLC MAC Report June 2003
  • The Committee would like to congratulate the
    damping ring team for the excellent work and the
    important recent achievements.
  • The Committee is pleased with the good progress
    the Berkeley group has made with the design of
    the new lattice.
  • From NLC MAC Report December 2003
  • Study of the damping ring physics has made
    considerable progress since the last review.
  • The stated plans for continued study of damping
    ring physics appear to be very complete The
    Committee believes it is entirely appropriate to
    place heavy emphasis on minimizing the production
    of secondary electrons by finding a suitable
    coating for the chamber interior.
  • Recent results of emittance measurements at ATF
    are particularly impressive and important.

12
PEP-II Luminosity gt 21034 cm-2s-1 by July 2006
  • Recently achieved 7.41033 cm-2s-1
  • CDR (1993) specified 31033 cm-2s-1 30 fb-1 per
    calendar year.
  • Total delivered so far 173 fb-1.
  • Luminosity improvement will be achieved by a
    variety of means
  • Better reliability.
  • Better control over lattice / tuning for optimum
    IP parameters.
  • Increased current (bunch charge and number of
    bunches).
  • Modified IR to reduce ?
  • Modified lattices / increased RF to reduce the
    bunch length.
  • At SLACs request, LBNL is already contributing
    to
  • Support of existing systems, e.g. bunch-by-bunch
    feedback.
  • Modeling of present lattices to improve
    tunability.
  • Studies of options for low ? lattices to reduce
    bunch length.
  • and we are exploring other opportunities to
    support PEP-II
  • Review of RF options and work needed to allow
    stable beam with higher beam current and RF
    voltage.

13
Expertise with proven modeling techniques applied
to PEP-II
  • LOCO developed by J. Safranek (now at SSRL)
    applied successfully to many machines, including
    the ALS.
  • Measure a closed orbit response matrix, and
    adjust parameters in a lattice model to reproduce
    the measured matrix.
  • An effective technique for identifying optics
    errors (focusing, coupling).
  • Now being applied to PEP-II, with some
    challenges
  • Interaction region has complex design.
  • Large quantity of data involved (matrices with
    108 components).

Measured response matrix in HER.
Measured - fitted model response matrix.
14
Phase advance in fitted model agrees well with
direct measurement
15
Fitted model identifies focusing and coupling
errors in HER
16
Zero crossing angle makes modeling IR complicated
  • PEP-II Interaction Region presently modeled as
    sliced solenoid.
  • gt100 slices of length 5 cm.
  • Design trajectory through solenoid modeled by
    individual misalignments on solenoid slices and
    vertical kicks.
  • Quadrupole and dipole fields inserted as kicks
    between slices.

17
Simplifying the IR model requires new maps
  • An accurate model of the IR is essential for
    optimizing luminosity.
  • Fitting IR magnet parameters to measured data
    would be helped by using a simplified (not
    sliced) model.
  • MARYLIE is being used to integrate the trajectory
    through a detailed field model, and to verify the
    maps being used.

Horizontal trajectory through IR.
Vertical trajectory through IR.
18
A new LER lattice reducing ? is challenging
  • Reasonable low ? solution for HER achieved by
    raising phase advance in arcs from 60º per cell
    to 90º per cell.
  • Present LER arcs have 90º phase advance per cell.
  • Raising phase advance to 120º in LER reduces ?
    30, and has a severe effect on the dynamic
    aperture.
  • Other options require new magnets, for example
  • One option is to add a new quadrupole every two
    arc cells.
  • Momentum compaction can be reduced from 12.410-4
    to 4.810-4
  • Natural emittance also reduced (from 24 nm to 16
    nm).

Present LER arc cell.
Possible new LER arc cell.
19
Low ? LER may be possible with hardware changes
  • Studies in simplified lattice show reasonable
    dynamic aperture.
  • 3-fold symmetry, constructed from modified arcs.
  • No errors included.
  • Next step is to include IR and adjacent
    straights.
  • Other options are still being explored, for
    example
  • Low ? insert based on long dipole chicane.

10?x
10??
20
Increasing beam current requires RF upgrade
  • In heavily beam-loaded large rings, the
    fundamental mode of the accelerating cavities
    becomes the dominant driver of beam
    instabilities.
  • RF feedback is used to reduce beam impedance by
    factor 100.
  • Existing system is at the edge of stability.
  • RF trips are the primary reason for beam loss.

21
LBNL has significant expertise in relevant RF
systems
  • Increased luminosity calls for
  • Factor of 2 increase in the beam currents.
  • Factor of 2 increase in the RF voltage.
  • Reduction in momentum compaction.
  • All the above increase the strain on the
    low-level RF.
  • LBNL has strong skills in critical areas
  • LBNL is providing RF systems for SNS.
  • LBNL can contribute accelerator physics expertise
    for modeling and experimental studies for RF
    systems in PEP-II upgrade.
  • Issues identified for possible initial studies
  • Evaluate options for high power RF upgrades.
  • Redesign of low-level RF system using modern
    technology.

22
Summary
  • Quality of work and progress with NLC Damping
    Ring studies is recognized by NLC Collaboration
    and MAC.
  • Work on wiggler has led to development of
    advanced techniques for modeling field and
    dynamics.
  • Collaboration with ALS group has led to
    implementation of powerful techniques for
    studying nonlinear dynamics.
  • Electron cloud is recognized as one of the most
    serious issues for the damping rings, and a clear
    path has been defined for RD leading to a
    solution.
  • A significant contribution is being made towards
    improving PEP-II luminosity.
  • Expertise in use of modeling techniques is being
    applied to improve tuning and optics of present
    lattices.
  • Strengths in nonlinear design and optimization
    are being used to find solutions for lower
    momentum compaction lattices, to benefit from
    reduced ? at the interaction point.
  • Skills in RF technology are a good match to
    critical systems in the luminosity upgrade.
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