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Pion capture and transport system for PRISM M. Yoshida Osaka Univ. 2005/8/28 NuFACT06 at UCI

Pion capture and transport system for PRISM M. Yoshida Osaka Univ. 2005/8/28 NuFACT06 at UCI

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Page 1: Pion capture and transport system for PRISM M. Yoshida Osaka Univ. 2005/8/28 NuFACT06 at UCI

Pion capture and transport system for PRISM

M. YoshidaOsaka Univ.

2005/8/28NuFACT06 at UCI

Page 2: Pion capture and transport system for PRISM M. Yoshida Osaka Univ. 2005/8/28 NuFACT06 at UCI

PRISM/PRIME project

Phase Rotated Intense Slow Muon source Collect 68MeV/c -

pion production, capture and transport system

proton beam

Phase rotator

PRIME detector

Page 3: Pion capture and transport system for PRISM M. Yoshida Osaka Univ. 2005/8/28 NuFACT06 at UCI

Concepts of pion capture/transport system for PRISM Capture low-energy pions produced in Graphite targ

et with 6T solenoid field Low-Z material

to avoid absorption in the target Collect backward pions from the target

Direction of emitted low energy pions is almost isotropic helps to reduce radiation heating on cold mass (avoid high e

nergy hadrons) Tilt target by 10 deg. to implement proton beam pipe Energy deposit on superconducting coil of capture solenoi

d < 100W Al-stabilized SC coil to reduce cold mass

Transport pions+muons in long 2T solenoid channel Bent solenoid channel

Target should be off-site from experimental area Reduce background by wiping out higher energy particles

The first trial of conceptual design has been done.

Page 4: Pion capture and transport system for PRISM M. Yoshida Osaka Univ. 2005/8/28 NuFACT06 at UCI

Heat load estimationMARS Simulation

MARS15(04) Primary beam

40GeV size =1.0cm 1014 protons/sec

Target Graphite (1.7g/cm3) radius=2cm

Magnetic field uniform 6Tesla Solenoid inner R=15cm

Coil Al-stabilized superconducting

Coil 71%Al + 11%NbTi + 14%Cu + 4%G10-tape

density 3.1 g/cm3

15cm

5cm

protons

140cm

Tungsten shield

Page 5: Pion capture and transport system for PRISM M. Yoshida Osaka Univ. 2005/8/28 NuFACT06 at UCI

Coil: 89 WShield: 41 kW

Heat load on coil

0

100

200

300

400

500

600

20 25 30 35Shield thickness (cm)

Ener

gy d

epos

it (W

) 0cm-5cm0cm-10cm0cm-15cm

Choosethickness of shield = 30cmthickness of coil = 12cm 17 A/mm2

target length = 60cm

80cm-long graphite target

Page 6: Pion capture and transport system for PRISM M. Yoshida Osaka Univ. 2005/8/28 NuFACT06 at UCI

Spatial distribution of deposit energy

0

2

4

6

8

10

12

14

16

0 50 100 150

z pos (cm)

depo

sit (W

) 090180270

0

90

270

180

Page 7: Pion capture and transport system for PRISM M. Yoshida Osaka Univ. 2005/8/28 NuFACT06 at UCI

Geometry of Pion Capture System

1400

600

300

90050

0

3600

100

To transport solenoid

300

mag

netic

fie

ld [

Tes

la]

Page 8: Pion capture and transport system for PRISM M. Yoshida Osaka Univ. 2005/8/28 NuFACT06 at UCI

, distributions @3m

25cm20cm

15cm10cm

Total momentum (GeV/c)

Pt

Radius squared (cm2)

0.058 -+-/POT @3-meter downstream traget

Page 9: Pion capture and transport system for PRISM M. Yoshida Osaka Univ. 2005/8/28 NuFACT06 at UCI

Transport solenoid channel

Transport pions and muons in 2T solenoid

Bent towards experimental area put radiation shield along proton

beam line

Page 10: Pion capture and transport system for PRISM M. Yoshida Osaka Univ. 2005/8/28 NuFACT06 at UCI

arc radius : 4000 mmbend angle : 90 deg.Bs : 2 TBy : 0.05 T

coil inner raduis : 350 mm(inner wall : 50mm)coil thickness : 50.0 mmcoil length : 629.0 mmcurrent : 36.5 A/mm^2step angle : 10 deg.

10 deg.

4 meters

Parameters of transport solenoid

A. Sato

Page 11: Pion capture and transport system for PRISM M. Yoshida Osaka Univ. 2005/8/28 NuFACT06 at UCI

Before BS

total

After BS

total

Transport loss in bent solenoid

7%

A. Sato

G4BeamLineSimulation

Page 12: Pion capture and transport system for PRISM M. Yoshida Osaka Univ. 2005/8/28 NuFACT06 at UCI

Summary

Conceptual design of pion capture solenoid and transport bent solenoid has been performed for PRISM

Heat load on coils of capture solenoid can be less than 100W as 40 GeV proton beam injected, assuming 0.6MW beam power.

Design works for the solenoid magnets are being started in collaboration with KEK

To improve pion yield Reduce beam spot size on target Field gradient around the target

acceptance would increase by mirroring forward pions To fit to FFAG acceptance (H: 40 mm-rad, V:6.5 mm-rad)

optimize field profile in the capture system to reduce muon emittance. (keep higher field?)

Page 13: Pion capture and transport system for PRISM M. Yoshida Osaka Univ. 2005/8/28 NuFACT06 at UCI
Page 14: Pion capture and transport system for PRISM M. Yoshida Osaka Univ. 2005/8/28 NuFACT06 at UCI

Horizontal position/direction distribution at exit of transport solenoid

Smooth curve bend in 3 steps

Page 15: Pion capture and transport system for PRISM M. Yoshida Osaka Univ. 2005/8/28 NuFACT06 at UCI

Injection Point: s=7m

Capture Matching Bent Post