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Active polarimeter simulation Suguru Shimizu Osaka University . 1, 2007 RC TREK Collaboration meeting at Saskatchewan
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Active polarimeter simulation

Jan 15, 2016

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Sep. 1, 2007 JPARC TREK Collaboration meeting at Saskatchewan. Active polarimeter simulation. Suguru Shimizu Osaka University. Assembly of Active polarimeter. Identification of muon stopping point/ decay vertex Measurement of positron energy E e + and angle q e + - PowerPoint PPT Presentation
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Page 1: Active polarimeter simulation

Active polarimeter simulation

Suguru Shimizu

Osaka University

Sep. 1, 2007JPARC TREK Collaboration meeting at Saskatchewan

Page 2: Active polarimeter simulation

Assembly of Active polarimeter Identification of muon stopping point/ decay vertex Measurement of positron energy Ee+ and angle e+ Large positron acceptance of nearly 4 Higher sensitivity Lower BG in positron spectra

Parallel plate stopper withGap MWPC Number of plates 31 Plate material Al, Mg or alloy Plate thickness ~ 2 mm Plate gap ~ 8 mm Ave. density 0.24 Al

stop efficiency ~ 85%

Small systematics for L/R positron Fit for 0 fwd/bwd measurement

Plates are ground  potential

Page 3: Active polarimeter simulation

Muon stopping distribution in the stopper

t/d = const.

d=2 mm

d=8 mm d (mm)

d = 8 mm

t=2 mm

t = 0. 5 mm

(g/cm3)

= 0.2Al

= 0.54 g/cm3

stop > 85% for t = 2 mm d =8 mm

Stopping prob. is determined by effective density.

Page 4: Active polarimeter simulation

Readout assembly for gap MWPC

• Requirements to the gap MWPC0 fwd/bwd analysis:

e+ timing resolution is not important because time integrated analysis is applied.

0 left/right analysis:e+ timing resolution is very important because we have to measure PT precession ( ~ 200ns c

ycle).

• Readout: anode readout from both endsy and z directions: anode wire hit patternradial direction: wire charge ratio. 5mm anode wire pitch corresponds to 50 ns Max. drift ti

me.(wire pitch is one of important parameters)

Page 5: Active polarimeter simulation

Readout methods for active polarimeter• We need time and charge information from each wire

• Multi-hit TDC and ADC are necessary because of 10 sec gate

→ QT-converter with pipeline TDC

Analog sum of 12 gaps →Data size was reduced to 1/12

In case of 5mm pitch, total number of channel is 2400.

prop. to Q multi-hit TDC Leading and trading edge should be read.

Page 6: Active polarimeter simulation

Tracking in gap MWPC tracking

trajectory is measured from wires which coincide with trigger timing. Drift time analysis is feasible.

e+ tracking e+ energy and direction should be obtained in order to increase the experimental sensitivity (FOM)

stopping position stopping position is determined from and e+ tracks as their intersection point.

Page 7: Active polarimeter simulation

Simple analysis using MC simulation data

Identification probability is > 98%.

Blue: + cellRed: e+ cell

+ stopping plate was determined by + cell and e+ cell.

Page 8: Active polarimeter simulation

Preliminary results of e+ angular resolution• Angular resolution for e+ track

+ stopping position: no ambiguitye+ track: obtained by MWPC information.

r=0cm

r=1cm

r=0.5 cm

e+ angular dist. (true-mea.) (deg)

=5 degree was obtained.

Page 9: Active polarimeter simulation

Future plan   (design of the polarimeter)

• Drift time in muon cell. Drift chamber analysis for muon track.

• Multi-cell hit by e+ are analyzed. The e+ track can be determined more precisely.

• Realistic position resolution in radial direction.• Test bench test using cosmic ray?