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2006.12.19 3rd ATF2 project meeting Permanent Magnet Updates Y. Iwashita, M. Ichikawa, Y. Tajima, M.Kumada, C.M. Spencer Kyoto University, NIRS, SLAC Contents:

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Presentation on theme: "2006.12.19 3rd ATF2 project meeting Permanent Magnet Updates Y. Iwashita, M. Ichikawa, Y. Tajima, M.Kumada, C.M. Spencer Kyoto University, NIRS, SLAC Contents:"— Presentation transcript:

1 2006.12.19 3rd ATF2 project meeting Permanent Magnet Updates Y. Iwashita, M. Ichikawa, Y. Tajima, M.Kumada, C.M. Spencer Kyoto University, NIRS, SLAC Contents: Brief review of PMQ study Longitudinal distribution 14mrad Octupole

2 2006.12.19 3rd ATF2 project meeting PMQ with saturated iron pole B=2Br (1-r 1 /r 2 ) cos 2 (π/M) sin(2π/M) /(2π/M)

3 2006.12.19 3rd ATF2 project meeting First prototype (fixed field)

4 2006.12.19 3rd ATF2 project meeting Adjustable Permanent Magnet Quadrupole Permanent Magnet (NEOMAX38AH)

5 2006.12.19 3rd ATF2 project meeting Prototype Magnet PMQ assembling

6 2006.12.19 3rd ATF2 project meeting Photos

7 2006.12.19 3rd ATF2 project meeting Magnetic Center Movement Magnetic Center moves by tens of micron when the strength was changed.

8 2006.12.19 3rd ATF2 project meeting Effect of Solenoid solenoid coil back coilmagnetic shield Integrated strength is reduced by Solenoid field because PMQ has pole (vanadium permendur). Back coil and/or some shield is needed.

9 2006.12.19 3rd ATF2 project meeting Demagnetization by Radiation Continuous 1mo.(2.6Ms) operation may cause about 0.01[%] of (reversible?) demagnetization on NEOMAX 32EH.

10 2006.12.19 3rd ATF2 project meeting Recent Modification Demonstrate a higher field gradient by reducing the bore size from ø20mm down to ø15mm. Temperature compensation of the inner ring; 1 mm (left) and 1.6 mm (right) MS-1 trapezoidal plates are seen in a 2cm space between magnets.

11 Longitudinal Distribution Vertical component By measured by a Group3 Tesla meter. dz = 2mm, z = 0 ~ 380mm dx, dy = ±2mm

12 Longitudinal Distribution All ON All OFF Almost flat: Gmax ~ 190 T/m Gmin ~ 29 T/m

13 SWL = 4cmSWL = 8cm Gradient is high at ON region. Magnet gaps of the inner ring affects the distribution.

14 Magnetic field centroid Cases of only 8cm (entrance) ON or only 4cm (exit) ON shows the maximum and minimum. Centroid location as a function of SWL mm 50 -50

15 SWL GL value is proportional to the SWL: GLmax ~ 38 T GLmin ~ 5.9T GL value

16 2006.12.19 3rd ATF2 project meeting Configurations for Various Crossing Angles Incoming Beam Table II PMQ parameters for various crossing angles.

17 2006.12.19 3rd ATF2 project meeting Difficult: less adjustability and stray field at extraction line Direct extension

18 2006.12.19 3rd ATF2 project meeting Side by Side Quad D for incoming F for outgoing Strength can be reduced by opening the gap.

19 2006.12.19 3rd ATF2 project meeting Side by Side Quad Both D Strength can be reduced by opening the gap.

20 2006.12.19 3rd ATF2 project meeting 70T/m @ ø30mm Octupole components tolerable? Both D Strength can be reduced by opening the gap. Side by Side Quad

21 2006.12.19 3rd ATF2 project meeting PMO (octupole)

22 2006.12.19 3rd ATF2 project meeting Two-piece configuration to dismount.

23 2006.12.19 3rd ATF2 project meeting Summary Almost done with the first adjustable model. Baseline changed to 14 mrad... Fabricate third model — may be tested in ATF2 Side by Side usable? Octupole for halo folding?


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