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PRISM RF Ultra High Field Gradient RF for Bunch Rotation

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High Purity. Pion Contamination 10-18. Low E - ~105MeV e- Stop Experiment ... Accelerates Slow Muon and Decelerates Fast Muon by a RF Field in PRISM-FFAG ring. ... – PowerPoint PPT presentation

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Title: PRISM RF Ultra High Field Gradient RF for Bunch Rotation


1
PRISM RFUltra High Field Gradient RF for Bunch
Rotation
  • Y.KURIYAMA
  • OSAKA UNIV.

2
Contents
  • Introduction of PRISM
  • PRISM RF Techniques
  • RF System RD
  • Summary

3
Introduction of PRISM (1)
Phase Rotated Intense Slow Muon Source
105MeV e-
  • Search for Lepton Flavor Violation
  • B(µ-N?e-N) lt 10-18
  • High Intensity
  • Intence 101112 µ/sec
  • Beam Repetitaion 1001000Hz
  • Muon Kiematic Energy 20MeV(68MeV/c)
  • High Quality
  • Muon Energy Spread 0.51.0MeV
  • High Purity
  • Pion Contamination lt 10-18

Low E µ-
Stop µ Experiment
4
Introduction of PRISM (2)
  • PRISM consists of
  • Pion Capture System
  • Pion Decay and Muon Transport System
  • Phase Rotation System

5
To Obtain a Muon Beam with Low Momentum Spread,
  • Several Ideas
  • -Cooling in Synchrotron
  • -Linac Option
  • etc.
  • But Short Life Time of Muon,
  • Solution
  • Bunch Rotation in a FFAG!

6
Phase Rotation
  • Accelerates Slow Muon and Decelerates Fast Muon
    by a RF Field in PRISM-FFAG ring.
  • Due to Muon Life Time, Bunch Rotation should be
    completed in 1µs(5turns).

High Gradient RF System is required.
7
Spec. for PRISM RF
  • High Field Gradient (gt200kV/m)
  • Muon has shrot life time
  • Low Frequency RF (45MHz)
  • Muons of low energy spread longitudinally
  • Difficulty to get High Voltage at Low Frequency
  • Saw tooth like RF shape
  • Low-Q cavity to allow Higher Harmonics
  • Magnetic Alloy Core (Finemet) is employed

8
High Field Gradient
High Gap Voltage (3) Short Cavity (2) Very
High Gradient for very short moment (10ms)
9
To Obtain High Voltage at Low Frequency.
  • Magnetic Alloy
  • High Field Gradient ( -200kV/m) might be possible
    by an optimum design.
  • Ceramic Cavity
  • Very high field gradient might be possible.
  • Need RD

10
Magnetic Cores for Cavity
Ferrites
Requirements for PRISM BV/OS400Gauss
Magnetic Alloys
11
MA Core for PRISM
1.7m
12
Parameters of MA Cavity
13
Saw Tooth RF Shape
5ns Muon width at given momentum
RF 5MHz, 250kV/m
?p/p3
Geant3 Simulation by A.Sato
Not a sinusoidal but a saw tooth shape is needed.
14
PRISM RF RD
  • FY2003
  • Production of AMP, Power Supply etc.
  • FY2004
  • AMP Commissioning by a test cavity _at_ RCNP,
    Osaka-U.
  • Design production of 33 cm Cavity

????
Test Cavity
15
Test RF System
AMP
Cavity
Power Supply
M-Experimental Hall, RCNP,Osaka-Univ.
Core
16
RF System RD
  • 43 kV/gap using 700O test cavity
  • Design goal (60A RF current) of AMP was achieved.
  • 33 cm cavity will be gt900O
  • Very compact design for AMP and APS.

86.6kV
17
PRISM Cavity Design
AMP
AMP
Cavity
Cavity
APS
APS
Beam Pipe
Beam Pipe
33cm
Side View
  • 1 Gap will be produced in this FY04.

By C. Ohmori, Y. Kuriyama
18
Summary
  • RD for PRISM RF has been started in RCNP,
    Osaka-U.
  • AMP, PS, D-AMP and MA Cores have been produced.
  • AMP has been tested using a test cavity and
    achieved 43 kV at 5MHz.
  • Ultra High Field Gradient Cavity will be
  • produced in FY2004.
  • Test of Ultra High Field Gradient in FY2005.
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