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Geant Simulation of Muon Cooling Rings

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Geant Simulation of Muon Cooling Rings. Amit Klier. University of California Riverside ... Runge-Kutta changed to include changing electric fields (eg RF cavities) ... – PowerPoint PPT presentation

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Title: Geant Simulation of Muon Cooling Rings


1
Geant Simulation of Muon Cooling Rings
  • Amit Klier
  • University of California Riverside

2
Outline
  • A short reminder from Nufact03
  • The RFOFO ring
  • Geometry
  • Software improvements
  • Simulation results
  • The small dipole ring
  • Geometry
  • Software improvements
  • Some Results

3
Muc_Geant
  • Modified, data-driven Geant3 application for
    simulating muon cooling
  • Electric fields added
  • Runge-Kutta changed to include changing electric
    fields (eg RF cavities)
  • Realistic magnetic fields can be read from
    external field maps

4
From Nuact03
Tetra ring simulated
Rajendran Raja Nufact 03
5
The RFOFO ring
  • A few code changes w.r.t. Tetra
  • Realistic magnetic field maps read-in (R.
    Godang, S. Bracker MC-Note 271)

6
The RFOFO ring
Full Geant simulation A. Klier MC-Note 298
7
The ring geometry
  • 33 m circumference
  • 12 cells (2.75m)
  • A wedge absorber
  • opening angle 110,
  • pointing upwards
  • 6 RF cavities
  • 28.75 cm long,
  • iris radius 25 cm
  • flat E field in z direction
  • 2 tilted solenoids
  • inner/outer r 77/88 cm
  • tilt angle 3
  • Only for display here

8
Closed orbits in a single cell
Solid line the reference orbit
200 MeV
270 MeV
227 MeV
250 MeV
250 MeV
227 MeV
E 200 MeV
E 270 MeV
9
Software improvements
  • ICOOL input/output format used, ecalc9 can be
    used to calculate emittance
  • Use initial time of particle at entry
  • Use virtual detectors

10
Cooling of a muon beam
11
Comparison with ICOOL
Transmission
6-D emittance
12
More comparisons
Results after 10 turns
Merit factor
Trans. W/O decay Trans. With decay Merit Factor
Balbekov (MC-264) 70 56 55
ICOOL (Fernow) -- 58 66
Geant 72 57 70
13
Change beam entry angle
14
The small dipole ring
Weak (edge) focusing (ideally) scaling Filled
with 10 Atm. hydrogen gas _at_ 77K
Dipole field 2 T
For P?200 MeV/c, the radius should be 60 cm
15
Field map (from S. Kahn)
By in a single quadrant
By at R60 cm
Return yoke
16
Reference orbit
  • Scale B down to 90
  • closed orbit
  • P171.25 MeV/c
  • Rmin56.32 cm
  • (x0 in virtual detectors)

Rmin
RF cavity (active region)
Virtual detector plane
17
Ellipses
Stable up to y13 cm
Y plane symmetry imposed
18
Acceptance of the ring
A blob
Py19 MeV/c
y8.5 cm
Px34 MeV/c
More natural decrease with no x-z plane
symmetry
x6.5 cm
19
Cooling with no scattering
Xinitial6 cm
Yinitial8 cm
tinitial 1.5 ns
Xcentral0.04 cm
Ycentral0 cm
tcentral0 ns
PXinitial30 MeV/c
PYinitial17.5 MeV/c
Einitial213 MeV
PXcentral0.12 MeV/c
PYcentral0 MeV/c
Ecentral201.8 MeV
20
Software improvements
  • More flexibility less hard-coding, more
    external parameters
  • Field map reading code used to be RFOFO-specific,
    now more general
  • More RF parameters
  • Cavities in small dipole ring are off-center
  • So far, only perfect pillbox (or flat field..)
    cavity are simulated
  • Flexibility different frequencies, gradients,
    types can be used in the same channel

21
To do
  • Simulate the small dipole ring with a beam
  • Introduce more realistic features
  • Injection
  • Detectors

22
(No Transcript)
23
Additional Slides
24
Comparison with ICOOL
Transverse emittance
Longitudinal emittance
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