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First Tracking Studies of Phase Rotation Using a Scaling FFAG

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A. Sato was kind enough to give me the OPERA field map of the PRISM magnet. ... First simulations in ICOOL with the coarse grid and without cavities. ... – PowerPoint PPT presentation

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Title: First Tracking Studies of Phase Rotation Using a Scaling FFAG


1
First Tracking Studies of Phase Rotation Using a
Scaling FFAG
Ajit Kurup BENE06 14th November
2
Introduction
  • A. Sato was kind enough to give me the OPERA
    field map of the PRISM magnet.
  • Averaged the field map to use with ICOOL.
  • First simulations in ICOOL with the coarse grid
    and without cavities.
  • Obtain closed orbit and look at dynamic aperture.
  • Include cavities and look at phase rotation.
  • Use simple saw-tooth waveform for the rf with a
    gap size of 0.33m.
  • Scale up B-field map for neutrino factory
    scenario.

3
PRISM
The PRISM cavities are designed for 150-200 kV/m
at 5MHz. A simplified waveform is used in these
simulations.
For a 0.33m gap
4
Field Map
  • PRISM field map
  • r from 565 to 735cm (step1cm)
  • z from 0 to 17cm (step1cm)
  • ? from -18o to 0o (step0.1o)
  • Averaged field map
  • r from 567.5 to 732.5cm (step5cm)
  • z from 0 to 17cm (step1cm)
  • ? from -17o to 0o (step1o)

5
Dynamic Aperture
  • Generated a beam evenly spaced in x, px, y and py
    for different momenta.
  • xx0(-0.5m0.8m) in 0.1m steps, yy0 0.15m in
    0.03m steps
  • pxpx00.02GeV/c in 0.005GeV/c steps
  • pypy00.005GeV/c in 0.001GeV/c steps
  • P P00.04GeV/c in 0.01GeV/c steps
  • x0, y0, px0, py0 and P068MeV/c are the coords of
    the closed orbit particle.

For 10 turns of the ring
6
Gaussian Beam Tracking
  • Generated a Gaussian beam (with no correlations)
    of 1000 muons using
  • ?x0.05, ?y0.025, ?px0.001 and ?py0.001
  • P is fixed at 68MeV/c

For 3 cells
7
Phase Rotation
  • Generated a Gaussian beam (with no correlations)
    of 1000 muons using
  • ?x0.05, ?y0.025, ?z0.0001, ?px0.001,
    ?py0.001 and ?pz0.034

For 7 turns of the ring
8
Neutrino Factory Scenario
  • Required momentum range is now 200 MeV/c 100
    MeV/c
  • Scale field map by 200/68 2.94
  • Keep everything else the same to start off with.
  • First use a Gaussian generated beam then use beam
    from a mercury target simulation.

9
Dynamic Aperture
  • Generated a beam evenly spaced in x, px, y and py
    for different momenta.
  • xx0(-0.5m0.8m) in 0.1m steps, yy0 0.15m in
    0.03m steps
  • pxpx00.05GeV/c in 0.01GeV/c steps
  • pypy00.012GeV/c in 0.002GeV/c steps
  • P P0(-0.15 0.2)GeV/c in 0.05GeV/c steps
  • x0, y0, px0, py0 and P00.2GeV/c are the coords
    of the closed orbit particle.

For 10 turns of the ring
10
Gaussian Beam Tracking
  • Generated a Gaussian beam (with no correlations)
    of 1000 muons using
  • ?x0.05, ?y0.025, ?px0.01 and ?py0.005
  • P is fixed at 200MeV/c

For 3 cells
11
Phase Rotation
  • Generated a Gaussian beam (with no correlations)
    of 1000 muons using
  • ?x0.05, ?y0.025, ?z0.0001, ?px0.01 and
    ?py0.005 and ?pz0.1
  • RF same as for the PRISM case.

For 7 turns of the ring
12
Phase Rotation(2)
  • Generated a Gaussian beam (with no correlations)
    of 1000 muons using
  • ?x0.05, ?y0.025, ?z0.0001, ?px0.01 and
    ?py0.005 and ?pz0.1
  • RF same as for the PRISM case but now gap size is
    0.033m.

For 7 turns of the ring
13
Phase Rotation (3)
  • 10GeV protons on a mercury target MARS14
    simulation.
  • Produced by H. Kirk and includes capture
    solenoid.
  • No muons survived 7 turns.

Selection Criteria No. of positive muons in input file
none 978
0.16ltplt0.24 GeV/c 177
pxlt0.02 GeV/c 154
pylt0.01 GeV/c 86
all 1
This muon only survives 4.5 turns.
14
Conclusions and Plan
  • Simulation method looks ok, results consistent
    with PRISM results.
  • Transverse momentum spread of the input beam
    needs to be improved for the neutrino factory
    scenario.
  • Redo simulations with a less coarse field map.
  • Can get p20 for neutrino factory but need to
    increase rf gradient, also can go to higher
    frequency. Otherwise itll take longer for the
    rotation.
  • Investigate injection and effect of alignment
    errors.
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