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Possibility of Electron tracking Compton camera for seeking deep universe in MeV gamma-ray band CONTENS 1. MeV Gamma-ray Astronomy 2. Problem of MeV gamma ray observation 3. Electron Tracking Compton Camera 4. Performance of SMILE-II (+Polarization measure) 5. Expected Astrophysics in SMILE-II and III balloon experments. 6. Summary Toru Tanimori Department of Physics, Kyoto Univ., Kyoto, Japan T.Tanimori, H.Kubo, K.Miuchi 2 , J.D.Parker, S.Komura, S.Iwaki, T.Sawano, K.Nakamura1, S.Nakamura, Y.Matsuoka, T.Mizumoto 3 , Y.Mizumura, M.Oda. S.Sonoda, A.Takada, D.Tomono, 1) Department of Physics, Kyoto University, Kyoto, Japan, 2) Department of Physics, Kobe University, Japan, 3 )Research Instit. for Sustainable Humanosphere, Kyoto Univ. 07/10/2013 GRB Meeting @ Ext Univ.Lab.

CONTENS - exul.ru · Noise Rejection of ETCC for BG gamma Case 1: downward gammas (signal) Compton in TPC x Absorption in Sciniti.(high Z) Case2 upward gammas (dominant in BG) Absorption

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Page 1: CONTENS - exul.ru · Noise Rejection of ETCC for BG gamma Case 1: downward gammas (signal) Compton in TPC x Absorption in Sciniti.(high Z) Case2 upward gammas (dominant in BG) Absorption

Possibility of Electron tracking Compton camera for seeking deep universe in MeV gamma-ray band

CONTENS 1. MeV Gamma-ray Astronomy 2. Problem of MeV gamma ray observation 3. Electron Tracking Compton Camera 4. Performance of SMILE-II (+Polarization measure) 5. Expected Astrophysics in SMILE-II and III

balloon experments. 6. Summary

Toru Tanimori Department of Physics, Kyoto Univ., Kyoto, Japan

T.Tanimori, H.Kubo, K.Miuchi2, J.D.Parker, S.Komura, S.Iwaki, T.Sawano, K.Nakamura1, S.Nakamura, Y.Matsuoka, T.Mizumoto3, Y.Mizumura, M.Oda. S.Sonoda, A.Takada, D.Tomono, 1) Department of Physics, Kyoto University, Kyoto, Japan, 2) Department of Physics, Kobe University, Japan, 3 )Research Instit. for Sustainable Humanosphere, Kyoto Univ.

07/10/2013 GRB Meeting @ Ext Univ.Lab.

Page 2: CONTENS - exul.ru · Noise Rejection of ETCC for BG gamma Case 1: downward gammas (signal) Compton in TPC x Absorption in Sciniti.(high Z) Case2 upward gammas (dominant in BG) Absorption

COMPTEL(1-30MeV)

Line g

Nucleosynthesis SNR : Galactic plane :

26Al・60Fe, 511 keV Continuum g

Strong Gravitational Potential Cosmic ray Acceleration Early GRB Terrestrial Gamma-ray bursts

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G.Weidenspointner, et.al. (2001) 0 10 -10 [nsec] -20

dowward

upward COMPTEL

Main reasons of Difficulty

1. Huge BG from gammas from Albedo and satellite and fast neutrons

2. Obscurity of imaging by circular direction

If no background, a fewx10cm2 effective area

=> a few mCrab@106sec

1. Good angular res.(ARM) = good Energy res. 2. Redundancies (TOF, Kinematics, dE/dx ) 3. Measurement of electron direction (SPD)! 4. Low-z material and light weight 5. Short timing gate

V.Schönfelder (2004) Suggestion Low background is most important for next MeV detector

Effective Area ~20cm2@1MeV

Page 4: CONTENS - exul.ru · Noise Rejection of ETCC for BG gamma Case 1: downward gammas (signal) Compton in TPC x Absorption in Sciniti.(high Z) Case2 upward gammas (dominant in BG) Absorption

Advanced Compton Camera

Crab 4s (8hrs) with NLEM meth.

Ge strio with BGO VETO

FoV 3str (BGO 8str)

0.3-1.5MeV Eff.A 6cm2

Simulation 3800 g detection 667 g

B.G. in Crab view~29000(S/N~0.02)

Priority: good energy res.

M. S. Bandstra et al. ApJ 2011

Le Xe TPC 2000

No VETO

0.1-10MeV Expected eff.A~20cm2

Obs. 1-10MeV ~2cm2

expected gamma from Crab ~50ph.

No. detection

priority: Large effective Area large

. Aprile et al(2004)

Page 5: CONTENS - exul.ru · Noise Rejection of ETCC for BG gamma Case 1: downward gammas (signal) Compton in TPC x Absorption in Sciniti.(high Z) Case2 upward gammas (dominant in BG) Absorption

Electron Tracking Compton Camera(ETCC)

Goal: High sensitivity for Continuum gammas

with > 10~50 better than COMPTEL

Strong BG rejection & clear imaging are needed

1. Electron tracking for imaging,

Kinematics(a)+dE/dx (multi redundancies)

2. Large FoV. ~3str

3. No Veto counters & light weight

50cm-cubic 3atm CF4 gas ~110cm2@1MeV

α

2 events 1 2 3

5 10 100

Page 6: CONTENS - exul.ru · Noise Rejection of ETCC for BG gamma Case 1: downward gammas (signal) Compton in TPC x Absorption in Sciniti.(high Z) Case2 upward gammas (dominant in BG) Absorption

10cm-cube m-TPC & ETCC

E

e

proton

electron

400mm

m-PIC

Micro Pixel Chamber

Timing Projection Chamber (TPC)

TPC

GSO

Pixel

3x3 array

11%@ 662 keV(FWHM)

GSO:Crystal

SPD ~160o

Page 7: CONTENS - exul.ru · Noise Rejection of ETCC for BG gamma Case 1: downward gammas (signal) Compton in TPC x Absorption in Sciniti.(high Z) Case2 upward gammas (dominant in BG) Absorption

All Trigger # 2.3x105 (3hours) Signal ~420(down going) +500(up) Simulation ~400 (diffuse cosmic)

Diffuse Cosmic g

Takda et al.ApJ (2011)

2006 Sep.

Sub-MeV g-ray Imaging Loaded-on-balloon Exp. (SMILE-I)

Event Selection

Neutron background

Page 8: CONTENS - exul.ru · Noise Rejection of ETCC for BG gamma Case 1: downward gammas (signal) Compton in TPC x Absorption in Sciniti.(high Z) Case2 upward gammas (dominant in BG) Absorption

Noise Rejection of ETCC for BG gamma Case 1: downward gammas (signal) Compton in TPC x Absorption in Sciniti.(high Z)

Case2 upward gammas (dominant in BG) Absorption in Scinti (high-Z) >> Compton in Scinti

Scinti (1 Radiation Length) 1/8 (SMILE-I)

Scinti (2 RL) ~1/50

Self Veto System ! Case 3 & Case 4 (two gammas)

Rejection by geometrical and kinematical cuts !

TPC

PSAs

PS

As

downward g

g’

upward g

g’

g’’

Case 1 Case 2

Case 3

Remained BG in SMILE-1 20% of real signal (Diffuse Cosmic-gamma)

Expected remained BG in SMILE-II only a few % of Diffuse Cosmic-gamma

Due to improved SPD, ARM and dE/dx

Case 4

Ryan, J. M., NewAR, 48, 199 (2004).

Leakage BG Suppress by

SPD

Page 9: CONTENS - exul.ru · Noise Rejection of ETCC for BG gamma Case 1: downward gammas (signal) Compton in TPC x Absorption in Sciniti.(high Z) Case2 upward gammas (dominant in BG) Absorption

① Physical process • Recoil e stopping in TPC • Scattered gamma absorbing

②Reconstruction Inefficiency ~10% in SMILE-I TPC

Crab Observation : ~104s observation 5σ detection

If Recont. Eff. -> 100%

SMILE-II

(30 cm)3 TPC x 20 times of SMILE-I Reconst. Eff. ⇒ X 10 Angular Res. 16o=>5.3o

Effective area : 1 cm2 DARM 10o

Diffuse gamma ⇒ point sources

But SMILE-I= : 1~2 mm2

X100times Improvement

reconstructed photo-peak

Eff

icie

ncy

1%

0.1%

0.01%

0.001%

10 cm2

1 cm2

0.1 cm2

0.01 cm2

Effective Area

GSO

GS

O TPC

GS

O

30cm

SMILE-II

MILE-I

Page 10: CONTENS - exul.ru · Noise Rejection of ETCC for BG gamma Case 1: downward gammas (signal) Compton in TPC x Absorption in Sciniti.(high Z) Case2 upward gammas (dominant in BG) Absorption

TPC 3

0cm

6x6 PSAs

3x6

PS

As

30cm

Total weight 300kg Power ~350W

136c

m

106cm

30cm-cube-ETCC

Improvement of Tracking in SMILE-II

Imaging of 3D tracks

prot

on

electr

on 2cm

Bargg peak (Stop position)

Scattering

Page 11: CONTENS - exul.ru · Noise Rejection of ETCC for BG gamma Case 1: downward gammas (signal) Compton in TPC x Absorption in Sciniti.(high Z) Case2 upward gammas (dominant in BG) Absorption

Source

ETCC

Imaging in 30cm ETCC

fkin

fgeo

~ 2

m

Zenith Angle

fgeo:calculated f

fgeo

fkin

data

Scattering Angle φ

e-

Scatterd g

Page 12: CONTENS - exul.ru · Noise Rejection of ETCC for BG gamma Case 1: downward gammas (signal) Compton in TPC x Absorption in Sciniti.(high Z) Case2 upward gammas (dominant in BG) Absorption

Noise reduction by Energy loss rate dE/dx (dE/dX)

e-

cosmic μ

e-

φgeo

φkin

φkin

φgeo

dE/dX

Simulation for recoil electron SMILE-I

Page 13: CONTENS - exul.ru · Noise Rejection of ETCC for BG gamma Case 1: downward gammas (signal) Compton in TPC x Absorption in Sciniti.(high Z) Case2 upward gammas (dominant in BG) Absorption

Gamma + Noise

Gamma ray Event selection in ETCC

dE/dX

dE/dX Cut Energy Cut

137Cs

BG

Continuum Gamma

⇒ Continuum fully gamma events selected by dE/dx cut

662keV Gamma

6m

Page 14: CONTENS - exul.ru · Noise Rejection of ETCC for BG gamma Case 1: downward gammas (signal) Compton in TPC x Absorption in Sciniti.(high Z) Case2 upward gammas (dominant in BG) Absorption

Angular Resolution in 30cm cubicETCC

Angular Resolution(FWHM)@662keV

5.3 deg. 93 deg.

GSO(simulation)

LaBr3(simulation)

Energy Resolytion (FWHM)

18 %@ 166 keV 11 %@ 662 keV

SPD = 93o <doube of multiple scattering (UC group using 10um pixel CCD

SPD ~200o <100keV electron (D.H.Chivers et al.,2010 IEEE)

Page 15: CONTENS - exul.ru · Noise Rejection of ETCC for BG gamma Case 1: downward gammas (signal) Compton in TPC x Absorption in Sciniti.(high Z) Case2 upward gammas (dominant in BG) Absorption

Imaging Improvement by SPD

:Advanced

(SPD=200°)

⇒ (~4times better contrast image

RI

Ryan, J. M., NewAR, 48, 199 (2004).

137Cs×3 3.2MBq 0.85MBq 0.74MBq

Legacy

Page 16: CONTENS - exul.ru · Noise Rejection of ETCC for BG gamma Case 1: downward gammas (signal) Compton in TPC x Absorption in Sciniti.(high Z) Case2 upward gammas (dominant in BG) Absorption

2013/9/22

Some Back Projection Image

15°

30deg.

60deg.

30° 60°(~3str) 137Cs(~0.85MBq)

6m

Multi energy souces

Field of View

⇒ FoV ~3str

Page 17: CONTENS - exul.ru · Noise Rejection of ETCC for BG gamma Case 1: downward gammas (signal) Compton in TPC x Absorption in Sciniti.(high Z) Case2 upward gammas (dominant in BG) Absorption

Detection Efficiency & Effective Area

Further improvement

⇒CF4 + 3atm Eff. Area ~10cm2 + double of Scintillator -> Total ~20 cm2 @ SMILE-II

Simulated Effective Area

Present Eff. Area~1cm2

Compton electrons in TPC ->100% detection

SMILE-I(10cm)

SMILE-II(10cm proto.)

SMILE-II(30cm FM) without side PSAs

Similar effective area to COMPTEL But 3str FoV, Low background, Clear Imaging in SMILE-II

Eff. Area~1cm2

Page 18: CONTENS - exul.ru · Noise Rejection of ETCC for BG gamma Case 1: downward gammas (signal) Compton in TPC x Absorption in Sciniti.(high Z) Case2 upward gammas (dominant in BG) Absorption

Weak source detection such as Crab

RI:22Na

Zenith = 26 deg.

z = 2095[mm]

31 kBq

511 keV±10%

# Event= 1.2x103 (26h)

S/N = 0.019

a few times stronger source

than crab for SMILE-II

Advanced Compton Image

10.8σ @ 5.4h

Livetime vs . Significance

Livetime [h]

Sig

nific

ance [

σ]

22Na

BG

2013/9/22

Spectrum after dE/dx

Preliminary

Page 19: CONTENS - exul.ru · Noise Rejection of ETCC for BG gamma Case 1: downward gammas (signal) Compton in TPC x Absorption in Sciniti.(high Z) Case2 upward gammas (dominant in BG) Absorption

Modulation Factor in SMILE-II in Simulation

#Event Max Min MF

Un polarized 5.33e5

0o, 100% 4.69e5 1.4 0.35 0.60

45o, 100% 4.83e5 1.45 0.35 0.61

Un-polarized, Cos θ < 0.7 0o, 100%, Cos θ < 0.7 45o, 100%, Cos θ < 0.7

MF = (max-min)/(max+min)

Page 20: CONTENS - exul.ru · Noise Rejection of ETCC for BG gamma Case 1: downward gammas (signal) Compton in TPC x Absorption in Sciniti.(high Z) Case2 upward gammas (dominant in BG) Absorption

天文学会

(@東北大学)

2013/09/11 (水)

SMILE-II (in USA) Collaboration with Goddard 30cmETCC with 1~4cm2 Detection Crab ,CygX-1 at >5s Polarization

SMILE-Ⅲ(Polar region) upgrade to 10-20cm2

Deep Survey for galactic plane

106 sec, 3σ detection

Preliminary

SMILE-satellite

SMILE-III

New Balloon Exp. (SMILE-II & III)

SMILE-Satellite 40cm-ETCC (>40cm2)x4

SMILE-II

Eff.Area 2cm2

Japan

Crab

Kiruna

Page 21: CONTENS - exul.ru · Noise Rejection of ETCC for BG gamma Case 1: downward gammas (signal) Compton in TPC x Absorption in Sciniti.(high Z) Case2 upward gammas (dominant in BG) Absorption

Crab & CygX-1 fluxes ( SMILE-II)

Crab polarization above 200keV (Integral/IBIS) P=0.46+0.3-0.19 (Integral/SPD) P=0.4+10-10% Cyg X-1 above 400keV P=67+30-30% IBIS M=0.3 SPI were not calibrated on the ground as a polarimeter.

Cyg X-1

Crab flux

E>100keV, 1cm2 ETCC 1300 gamma /10hrs from Crab

BG 6500 gamma /10hrs MPD=28/M % 4cm2 MPD=12/M

10cm2 28/3.3=8.5/M %

M:modulation factor M > 0.6 expected for ETCC (Low background compared to IBIS due to real imaging )

Page 22: CONTENS - exul.ru · Noise Rejection of ETCC for BG gamma Case 1: downward gammas (signal) Compton in TPC x Absorption in Sciniti.(high Z) Case2 upward gammas (dominant in BG) Absorption

Precise measurement of MeV CMB

• 0.1-10MeV Dominant contribution is unclear

Seyfert or FSRQ?

• SMILE-II Polar flight

• Due to its large FoV (4str) , background rejection, and point-like gamma-ray direction measure, precise measurement of the map of MeV CMB will be possible.

(CBR)

(from Y.Inoue)

(Y.Inoue氏の資料より)

Page 23: CONTENS - exul.ru · Noise Rejection of ETCC for BG gamma Case 1: downward gammas (signal) Compton in TPC x Absorption in Sciniti.(high Z) Case2 upward gammas (dominant in BG) Absorption

Polar Flight (~106 sec) ⇒ >106 events ⇒ precise spectrum of CMB

Anisotropy ⇒ >105 events is enough for separation of

Seyfert and FSRQ with 5s

N > 104~5

N > 2×104~5

For >3σ detection of Anistoropy

10 Y. Inoue

Page 24: CONTENS - exul.ru · Noise Rejection of ETCC for BG gamma Case 1: downward gammas (signal) Compton in TPC x Absorption in Sciniti.(high Z) Case2 upward gammas (dominant in BG) Absorption

GRB Cosmology

From Dr. Suwa

POP-III

Flu

ence

POP-III

40cm-cube ETCC • 10-8erg/cm2s 1g(>100keV)@10cm2

for GRB of 10-9erg/cm2s (900Msolar)

Eff.Area 50cm2

• 103s 500g B.G. 40g in 4x4o S/N ~20s

• 105s 5x104g B.G> 4x103g S/N =680s

• 5s detection during 105s -> ~300g

<100Msolar Super long bursts OK!

Expected g in S-ETCC for GRB @z=20 & Eiso=1052 erg -> >several x100 ph.

Page 25: CONTENS - exul.ru · Noise Rejection of ETCC for BG gamma Case 1: downward gammas (signal) Compton in TPC x Absorption in Sciniti.(high Z) Case2 upward gammas (dominant in BG) Absorption

GRB Polarization observational Situation

1. GRB 021206: 80+-20% (Coburn & Boggs 03) but, claim from Rutledge & Fox 2004; Wigger et al. 04;)

2. . GRB 930131, GRB 960924: > 30% (Willis et al. 05)

3. GRB 041219a: 96+-40% (Kalemci et al. 07; McGlynn et al. 07)]

4. GAPS

Page 26: CONTENS - exul.ru · Noise Rejection of ETCC for BG gamma Case 1: downward gammas (signal) Compton in TPC x Absorption in Sciniti.(high Z) Case2 upward gammas (dominant in BG) Absorption

GRB detection in SMILE-III • ETCC M>0.6 GRB signal >>BG FoV 3str

• SMILE- 30cmETCC Eff. Area 20cm2@200 keV

GRB 10-6erg/cm2s ~160 photon/s T90=40s 160x40s ~6000

MDP = 5.5/M % (3s) (M>0.6 ) 10% polarization OK!

For, 30% polarization -> 10-5erg/cm2s- GRB

a few GRBs (10-6erg/cm2s) ~10 (10-5erg/cm2s) with one-month

• Satellite ETCC~100㎝2 (Sensitivity~1mCrab@106sec)

10-7erg/cm2s GRB MDP =5.5/M % (>100 GRB/year)

10-6erg/cm2s GRB MPD= 3/M % (several 10 GRB/year)

Page 27: CONTENS - exul.ru · Noise Rejection of ETCC for BG gamma Case 1: downward gammas (signal) Compton in TPC x Absorption in Sciniti.(high Z) Case2 upward gammas (dominant in BG) Absorption

Galactic lines of SMILE-III

Polar Flight (SMILE-II 10 cm2, 106 sec) ⇒ > 103~104 event/pixel More detailed map of 511keV due to point-like direction of gamma rays In addition, survey for galactic plane ⇒ possible detection of new sources due to low background and point-like directional imaging of ETCC

L. Bouchet+ (2010)

0.003 0.0025 0.002 0.0015 Photons/cm2/sec

30°

30°

511keV map (INTEGRAL)

1 pixel = 5°×5°

0.85 MBq 0.74 MBq

3.2 MBq

0 1 2 3 -1 -2 -3 -3

-2

-1

0

1

2

3 137Cs×3 @ 2m

X [m]

~30°

Simple back projection image More fine imaging is obtained by using MLEM

511keV, 1804keV(Al-26), 4MeV (C-12)

Page 28: CONTENS - exul.ru · Noise Rejection of ETCC for BG gamma Case 1: downward gammas (signal) Compton in TPC x Absorption in Sciniti.(high Z) Case2 upward gammas (dominant in BG) Absorption

Vela Pulsar

Ar 1 atm

M.S.Stickman et al. ApJ. 1996

CF4 3 atm Syfert II galaxy

Page 29: CONTENS - exul.ru · Noise Rejection of ETCC for BG gamma Case 1: downward gammas (signal) Compton in TPC x Absorption in Sciniti.(high Z) Case2 upward gammas (dominant in BG) Absorption

ETCC have obtained both strong background rejection abilities and

high contrast imaging by direction of recoil electron.

ETCC has nearly one order better sensitivity than usual CC with

similar effective area.

ETCC also is a good polarimeter with MF>0.6 in sub-MeV region.

SMILE-II having 1-4cm2 @0.3MeV effective area will be planned in

USA in 2014, 15 for the observation of Crab and Cyg.X-1 with one-

day flight. (>5shigma detection, and Polarization)

SMILE-II will be improved to SMIEL-III having > 10cm2 ( several

times better sensitivity of COMPTEL) in 2016.

In the long duration flight around the Polar cap, SMILE-III will

measure ~10 Celestial objects, MeV-Cosmic Background and several

GRBs with polarization.