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EMMA Horizontal and Vertical Corrector Study

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Ability to move magnets perpendicular to the beamline in the ... Vertical corrections made using kicker magnets. ... Neil Bliss 3/4/07. MADX Correct' Module ... – PowerPoint PPT presentation

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Title: EMMA Horizontal and Vertical Corrector Study


1
EMMA Horizontal and Vertical Corrector Study
  • David Kelliher
  • ASTEC/CCLRC/RAL
  • 14th April, 2007

2
Introduction
  • Ability to move magnets perpendicular to the
    beamline in the horizontal plane allows
    horizontal corrections to be made.
  • Vertical corrections made using kicker magnets.
  • There will be 2 BPMs per cell, providing both
    horizontal and vertical displacement
    measurements.
  • No BPMs will be placed in those long drifts with
    an RF cavity.

3
BPMs and vertical kicker location
Neil Bliss 3/4/07
4
MADX Correct Module
  • The CORRECT statement makes a complete closed
    orbit or trajectory correction using the computed
    values at the BPMs from the Twiss table.
  • There are three corrections modes MICADO, LSQ,
    SVD. MICADO is used in this study as it tries to
    minimise the number of correctors used.
  • The MICADO algorithm solves a system of linear
    equations
  • Where b is the vector of BPM measurements, q is
    the correction kick vector and A is the beam
    response matrix to a set of kicks. The algorithm
    iteratively minimises the norm of the residual
    vector r using least squares method. At each
    iteration it finds the corrector that most
    effectively lowers r.m.s BPM distortion.

5
Error simulation
  • Errors in the magnet horizontal (?50mm) and
    vertical (?25mm) position simulated by using the
    MADX function EALIGN.
  • Random errors with a Gaussian distribution,
    cut-off point at 2s.
  • MADX was run with many instances of such randomly
    perturbed magnets in order to generate useful
    statistics.

6
Error distribution F magnet
7
BPM location and Horizontal orbit distortion
8
Horizontal tune / Horizontal Orbit distortion
1 seed used to simulate random alignment errors
9
Energy Scan 1 seed
10
10 MeV 50 seeds
11
15 MeV 50 seeds
12
Energy Scan 1 seed
13
Energy Scan 1 seed
14
Variation of Corrector strengths
15
Variation of Corrector strengths
16
Horizontal Correction - Conclusions
  • No optimal position for BPMs can be inferred from
    this study.
  • Outside the vicinity of energies which correspond
    to integral tunes, the difference in orbit
    correction accuracy due to BPM position is of the
    micron order (if all available correctors used).
  • Position of BPMs down to engineering
    considerations.
  • Corrector strengths were allowed to vary in this
    study (not feasible in reality).
  • How to find corrector strengths, constant over
    energy range, which best reduce horizontal orbit
    distortion?

17
Number of correctors and vertical orbit distortion
18
Vertical Tune / Orbit Distortion
1 seed used to simulate random alignment errors
19
1 Corrector Variable Strength
20
1 Corrector Constant Strength
21
2 Correctors Variable Strength
22
2 Correctors Constant Strength
23
Conclusion
  • Due to strongly varying phase advance per cell
    over the energy range, it is difficult to correct
    with constant corrector strength
  • There is no simple way to solve this problem
    using existing MADX routines.
  • A smart interpolation method should be used to
    find the best set of correctors to reduce both
    vertical and horizontal orbit distortion over the
    energy range.
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