emulsion detector for future neutrino research possibility of the technology

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Emulsion Detector for Future Neutrino Research Possibility of the Technology NAKAMURA M. (NAGOYA Univ.)

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Emulsion Detector for Future Neutrino Research Possibility of the Technology. NAKAMURA M. (NAGOYA Univ.). CONTENTS. Emulsion Detector Overview New Study. Emulsion Spectrometer Emulsion in Magnetic field Expected scanning power in near future. Intrinsic position resolution. - PowerPoint PPT Presentation

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Page 1: Emulsion Detector  for Future Neutrino Research  Possibility of the Technology

Emulsion Detector for Future Neutrino Research

Possibility of the Technology

NAKAMURA M. (NAGOYA Univ.)

Page 2: Emulsion Detector  for Future Neutrino Research  Possibility of the Technology

CONTENTS

• Emulsion Detector Overview

• New Study. Emulsion Spectrometer

Emulsion in Magnetic field

• Expected scanning power in near future

Page 3: Emulsion Detector  for Future Neutrino Research  Possibility of the Technology

Cross sectional view of an emulsion layer

30grains/100mgrain diameter ~ 0.6m

Ag grain after development

dx

= 0.06m

Compton Electron

Fog

M.I.P. Track

100m

M.I.P. Track

Intrinsic position resolution

One Emulsion Layer = vector chamber with 60nm position resolution

& ~1mrad Angular resolution (100micron layer)

Page 4: Emulsion Detector  for Future Neutrino Research  Possibility of the Technology

Achievement in OPERA R&D

• Nuclear Emulsion Films

Suited for Mass production ~ 100,000m2

Uniform quality

Refresh function   R&D by

Nagoya Univ. & Fujifilm

• Fast Scanning systems

in Japan & Europe

125mm

100mm

Page 5: Emulsion Detector  for Future Neutrino Research  Possibility of the Technology

Refresh

Cosmic-rays

Emulsion film accumulates all signals during its live time

:No dead time.

Compton electrons by γ rays of natural radio activity

Before Refresh After Refresh

We can reset the accumulated images by Refreshing.

Before use or re-use

Page 6: Emulsion Detector  for Future Neutrino Research  Possibility of the Technology

OPERA ECC Brick

10cm

12.5cm8cm

8kg:  Portable Unit for 2~10kton detectors

Page 7: Emulsion Detector  for Future Neutrino Research  Possibility of the Technology

Tau detection :

DONUT -> OPERA

Topological decay detection:

Kinematical analysis: Momentum measurement by Multiple Coulomb Scatterings (or Emulsion Spectrometer) Electron ID by shower detection Particle ID by dE/dX measurement

Decay search

τ

Fe

film

Page 8: Emulsion Detector  for Future Neutrino Research  Possibility of the Technology

dE/dX measurement

Pb Film

P=1.2GeV/c

Hadron+

@KEK/PS

dE/dX

dE/dX = measurement

~number of grains

P

Page 9: Emulsion Detector  for Future Neutrino Research  Possibility of the Technology

dE/dX measurement : TEST exp at KEK0.4 GeV/c 0.5 GeV/c 0.6 GeV/c

0.74 GeV/c 0.87 GeV/c 1.14 GeV/c 2.0 GeV/c

P P P

PP

P

π π π

π π π

D

D D D D

P&π

Entry 1610 tracks Entry 1345 tracks Entry 1175 tracks Entry 1206 tracks

Entry 996 tracks Entry 1310 tracks Entry 1278 tracks

• Using only 5 ~ 6 films.• VPH, measured by the system, is ~propotional to dE/dX.

VPH

Page 10: Emulsion Detector  for Future Neutrino Research  Possibility of the Technology

P

π

P andπ

Using 5 ~ 6 films.VPH, measured by the system, is ~propotional to dE/dX. Error bar is 1σof the distribution. At 2 GeV/c , proton and pion are not separated in 5 or 6 OPERA films.VPH of proton below 0.6GeV/c is saturated.

Particle ID by dE/dx Measurement

K

dE/dx(MeV ・ cm2/g)

Momentum(GeV/c)

VPH

e

KEK Beam Test Preliminary

Page 11: Emulsion Detector  for Future Neutrino Research  Possibility of the Technology

50GeV electrons + muons

Electron ID

Test Exp. @ CERN

Page 12: Emulsion Detector  for Future Neutrino Research  Possibility of the Technology

Electron energy measurement

MC Data

)(E

4.0~

GeV

@ a few GeVEnergy determination by calorimetric method( in study)

Test exp. @ CERN

Page 13: Emulsion Detector  for Future Neutrino Research  Possibility of the Technology

Emulsion in Magnetic Field

• Charge Sign determination + increase sensitivity + increase BG-rejection power

o scanning load (mention later) o cost??

• We have experience in CHORUS/ET(Emulsion Tracker)

Page 14: Emulsion Detector  for Future Neutrino Research  Possibility of the Technology

Structure for MC study

Stainless steel or Lead Film

Air Gap

DONUT/OPERA type target + Emulsion spectrometer

B

~ 3Xo ~10Xo

Assumption: accuracy of film by film alignment =10 micron (conservative).(Ex. 20mm gap structure gives 0.5mrad angular resolution.)

mu

Page 15: Emulsion Detector  for Future Neutrino Research  Possibility of the Technology

Charge determination (0.5T) MC

P(GeV/ c) Eff. 20mm Eff. 30mm1 99.93% 99.96%2 99.95% 99.97%3 99.94% 99.67%4 99.90% 99.98%5 99.83% 99.96%6 99.58% 99.97%7 98.98% 99.97%8 97.97% 99.96%9 96.78% 99.97%

10 95.32% 99.95%

10mm Gap

20mm Gap

>=30mm Gap

Page 16: Emulsion Detector  for Future Neutrino Research  Possibility of the Technology

Momentum resolution(0.5T) MC

10mm Gap

20mm Gap

30mm Gap

40mm Gap

50mm Gap

Page 17: Emulsion Detector  for Future Neutrino Research  Possibility of the Technology

P(GeV/ c) Eff. 20mm Eff. 30mm1 99.980% 99.994%2 99.983% 99.993%3 99.979% 99.993%4 99.981% 99.992%5 99.973% 99.998%6 99.978% 99.996%7 99.981% 99.994%8 99.976% 99.990%9 99.966% 99.995%

10 99.947% 99.994%

Charge determination (1.0T) MC

10mm Gap

>=20mm Gap

Page 18: Emulsion Detector  for Future Neutrino Research  Possibility of the Technology

Momentum resolution(1.0T) MC

10mm Gap

20mm Gap

30mm Gap

40mm Gap50mm Gap

Page 19: Emulsion Detector  for Future Neutrino Research  Possibility of the Technology

Summary of the MC study• Emulsion Spectrometer ( B 0.5T,Gap > 20mm, ≧

Total Length~10cm) has power to determine sign & momentum efficiently.

• Further MC study: Investigate the Possibility to open the sensitivity

for hadronic and electric decay mode. Sensitivity >~ x 3 (like OPERA)

• Technological R&D : Unique track connection How to keep air gap Test exp.

Page 20: Emulsion Detector  for Future Neutrino Research  Possibility of the Technology

Emulsion Film Read-out

Page 21: Emulsion Detector  for Future Neutrino Research  Possibility of the Technology

Emulsion Readout History

• E531, E653, etc . (~1994) – Semi-automatic scanning

• CHORUS phase I– Track selector, New TS (1994~)

• DONUT, CHORUS phase II– UTS (1998~) Net scan (angle: |<0.4).

• OPERA

Automatic Automatic ScanningScanning

Page 22: Emulsion Detector  for Future Neutrino Research  Possibility of the Technology

Bottle necks in the Read-out System

Speed of Image Data taking

Movement of Z Stage

Field of View :

Objective Lens

Movement of X-Y stage

Page 23: Emulsion Detector  for Future Neutrino Research  Possibility of the Technology

Overcome the Bottle necks

Stage moves at constant velocity

Synchronized motion to cancel relative velo.

Ultra High Speed Imager with Real Time processing

• Ultra High Speed Imager– 120 fps -> 3000 fps

• Image taking by follow shot– X-Y stage : Non-stop – Objective lens: Driven by piezo electr

ic devices ( fres>2kHz ) .

• Enlarging size of Field of View– Effective FOV: 100m×100m-> 140m×140m

1cm2/h -> 60cm2/h

Page 24: Emulsion Detector  for Future Neutrino Research  Possibility of the Technology

SUTS + Old stage

Page 25: Emulsion Detector  for Future Neutrino Research  Possibility of the Technology

0.008

0.25

3

60

0.001

0.01

0.1

1

10

100

TS(TTL) NTS(CPLD) UTS(FPGA) S-UTS

Scanning System Historyviews/sec(1view=120×90 m2)

Evolution of the Scanning Power

Our code name (device technology)

CHORUS DONUT OPERA

Page 26: Emulsion Detector  for Future Neutrino Research  Possibility of the Technology

Expected evolution of the Scanning Power in near future

• Enlarge a Field of View × (1.25)2 reduce objective mag. × 50 -> × 40

• Speed up Image data taking ×4 Ultra High Speed Camera 3kfps->12kfps.

400cm2/hours/system. (~1m2/day/system)

Page 27: Emulsion Detector  for Future Neutrino Research  Possibility of the Technology

How many events?Scanning Power

1 m2/day/system~ 100events/day/system

( OPERA like ECC 1event/brick ~100cm2/event)

~25,000events/year/system

Normally one lab has ~10 system

~250,000 events/year/lab.

Events in Neutrino Factory

160,000 events/kton

(L=3000km,1021mu+ decays)

Page 28: Emulsion Detector  for Future Neutrino Research  Possibility of the Technology

Event selection for 10kton

• 10kton Total event: 1,600,000

= 1,600,000/250,000

~ 6 Lab ・ year

   Loose-selection is Acceptable.

• During the RUN : Extract and Analyze wrong sign muon events.

End of the RUN : Extract all bricks which have tagged neutrino interactions in it.

Page 29: Emulsion Detector  for Future Neutrino Research  Possibility of the Technology

L3 Magnet 0.5T

OPERA 1SM 850t Or Modified ATLAS TROID

Page 30: Emulsion Detector  for Future Neutrino Research  Possibility of the Technology

Related Works

• OPERA Exposure will start at the middle of 2006. Scanning in many Labs (Japan, Italy, France, Swiss….)• PEANUT Test exp. at NUMI near detector site. Start neutrino exposure at Aug. 2005. Plan: Test of “ ECC in Magnet” with Permanent magnet (2006).

Page 31: Emulsion Detector  for Future Neutrino Research  Possibility of the Technology

OPERA 1st Super Module

2nd Super Module

Page 32: Emulsion Detector  for Future Neutrino Research  Possibility of the Technology

PEANUT Detector :DONUT SFT+ Mini Brick Wall

MINOS Near detector as mu ID

Page 33: Emulsion Detector  for Future Neutrino Research  Possibility of the Technology

Location of Neutrino interactions in ECC brick

1. Pick up tracks in the most downstream plate

Neutrino

2. Follow tracks to the interaction veretex

Page 34: Emulsion Detector  for Future Neutrino Research  Possibility of the Technology

P measurement using Multiple Scattering

rms

rms 1

n n : number of measurements

For example: 10 GeV/c has rms deflection of 0.3m

Kinematical AnalysisMomentum

measurement

Page 35: Emulsion Detector  for Future Neutrino Research  Possibility of the Technology

Momentum measurement

Low dE/dX

Higher dE/dX

Consistent with Pion

Consistent with Proton

P measurement using Multiple Scattering

Expected Value for pion

Expected Value for proton

Resolution p