Balloon-borne experiment for deep sky survey of MeV gamma rays - - PowerPoint PPT Presentation

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Balloon-borne experiment for deep sky survey of MeV gamma rays - - PowerPoint PPT Presentation

Balloon-borne experiment for deep sky survey of MeV gamma rays using an Electron-Tracking Compton Camera S. Komura , T. Tanimori, H. Kubo, A.Takada, S. Iwaki, Y. Matsuoka, S. Miyamoto, T. Mizumoto, Y. Mizumura, K. Nakamura, S. Nakamura, M. Oda,


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SLIDE 1

Balloon-borne experiment for deep sky survey of MeV gamma rays using an Electron-Tracking Compton Camera

  • S. Komura, T. Tanimori, H. Kubo, A.Takada, S. Iwaki, Y. Matsuoka, S. Miyamoto,
  • T. Mizumoto, Y. Mizumura, K. Nakamura, S. Nakamura, M. Oda, J. D. Parker,
  • S. Sonoda, T. Takemura, D.Tomono (Kyoto Univ.) K. Miuchi (Kobe Univ.),
  • T. Sawano (Kanazawa Univ.), S. Kurosawa (Tohoku Univ.)

Sub-MeV gamma-ray Imaging Loaded-on-balloon Experiment Now planning SMILE-II (1 day flight) Crab Nebula, Cygnus X-1 SMILE-III (1 month flight) ・ more faint sources ・ polarization measurements

SMILE-I (Sep., 2006 ) gas-TPC Pixel Scintillators

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SLIDE 2

Contents

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  • 1. Status and problems in MeV gamma-ray astronomy
  • 2. How to challenge by using ETCC
  • 3. Current and near-future ETCC

 Performances  Polarization measurement

 Summary

34th ICRC Hague, 4 August 2015

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SLIDE 3

Status of MeV gamma-ray astronomy

34th ICRC Hague, 4 August 2015 3

~30 objects/10 years COMPTEL 1-30 MeV map ~3000 objects/4 years

  • F. Acero+ (ApJS, 2015)

Fermi > 1 GeV map

  • V. Schönfelder+ (A&AS, 2000)

NASA/DOE/ Fermi LAT Collaboration

MeV gamma-ray region is unexplored frontier!

❏ Nucleosynthesis in SNR ❏ Particle acceleration in AGN ❏ Early universe probe with GRB etc.

Interesting science

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SLIDE 4

Problems

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 Unclearness of Imaging

wide-spread Point Spread Function (PSF)

needs of optimization algorithm as like ML-EM

COMPTEL did not measure direction of recoil electron.

=> Imaging by superposition of event circles

34th ICRC Hague, 4 August 2015

Radioactivation of detectors by cosmic rays BG rejection in COMPTEL was not sufficient. => ~ 1/3 of the expected sensitivity

  • G. Weidenspointner+ (A&A, 2001)

TOF between two detectors

 Huge backgrounds in space

Reliable PSF and Powerful BG rejection are needed.

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SLIDE 5

Electron-Tracking Compton Camera (ETCC)

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gas-TPC 3D-track

& energy

Pixel Scintillators position & energy

  • Well-defined PSF without ML-EM
  • Powerful BG rejection using dE/dx
  • No shield => Wide field of view ~ 6sr

Conventional method Electron Tracking method SPD

34th ICRC Hague, 4 August 2015

By measuring electron tracks, ETCC overcome the problems !

T.Tanimori et al., ApJ (2015) accepted, arXiv: 1507.03850 [astro-ph.IM]

Recoil electron p + n

Particle ID by dE/dx

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SLIDE 6

Current and near-future performance

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1 m

SMILE-II Flight model TPC Scinti. Pressure vessel

Gas Ar-based @1atm Gas volume 30 cm-cubic Track sampling 800 μm Scintillator GSO:Ce 1 Radiation length Energy resolution 10%@662 keV (FWHM) Field of View ~ 6 sr

Effective Area

 40 cm-cubic  CF4 gas @3atm  3 R.L. scintillator

Points: measured Lines : simulated

PSF: angle containing half of all photons

SMILE-II, III 7-15º Near future ~ 1º  more precise track sampling

34th ICRC Hague, 4 August 2015

Effective Area

[keV]

SPD < 10º SPD 30-100º

(energy dependence)

SMILE-III SMILE-II

Points: measured Lines : simulated

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SLIDE 7

Detection sensitivity

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 SMILE-II : Crab nebula > 5σ (middle latitude, @ 40 km, 4 hours)  SMILE-III : 10 times better sensitivity (polar region, @ 40 km, 1 month)

~10 celestial objects, extragalactic and galactic plane survey

 Satellite : reach 1 mCrab sensitivity (50 cm-cubic ETCC x 4)

34th ICRC Hague, 4 August 2015

(5 years) (4.5 years)

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SLIDE 8

as a Polarimeter

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linearly polarized γ-ray min max

Azimuthal angle Φ [deg]

Counts [a.u.]

Asymmetric distribution of the scattered photons

Modulation Factor

= 𝑛𝑏𝑦−𝑛𝑗𝑜

𝑛𝑏𝑦+𝑛𝑗𝑜

[%]

~ 0.6@200 keV, ~ 0.5@500 keV

(Geant4 simulation) Minimum detectable polarization (MDP)

A Effective area [cm2] M Modulation Factor T Observation time [sec] S Signal [cm-2 sec-1] B Background [sec-1]

Sensitivity is limited by the background rate. 𝛤 ≫ 𝛣𝑇 M𝐸𝑄 ∝ 𝐶 𝐵𝑇 ETCC has a large advantage  Powerful background rejection  Imaging with wide FOV ~ 6sr

  • 200 -100 0 100 200

1.5 1 0.5

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SLIDE 9

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 M ~ 0.6@130 keV  Polarization angle ≒ Rotation angle

Beam test

~ 96% polarized 123-148 keV

rotation [deg.] M Polarization angle [deg.]

0.57 0.3±1.3

  • 22.5

0.59

  • 22±1.0
  • 45

0.60

  • 44±0.7
  • 90

0.57

  • 90±1.1
  • 180

0.60

  • 2.3±1.1

Modulation Factor is consistent with the simulation results.

34th ICRC Hague, 4 August 2015

0 deg.

  • 22.5 deg.
  • 45 deg.
  • 90 deg.
  • 180 deg.

Azimuthal angle [degree] Counts [a.u.]

  • 200 -100 0 100 200

2 1 2 1 2 1 2 1 2 1

Al target ON Al target OFF Subtracted

Peak ~ 130 keV

Energy [keV]

50 100 150 200 250

1 10-2 10-4

Counts [/sec/keV]

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SLIDE 10

Summary

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  • SMILE-II ETCC ~ 1 cm2 @ 200 keV

 detectable Crab nebula with > 5σ level

(middle latitude, 4 hours at 40 km)

  • Future Plan: SMILE-III ETCC (~10 times better sensitivity)

 ~ 10 celestial objects (polar region, 1 month at 40 km)  Polarization sensitivity : 3σ MDP Crab nebula ~ 15 %, Cyg X-1 ~ 20 % (half-day flight) GRBs ~ 6% for 10-6 erg/cm2 s (2-3 GRBs/month) ~ 20% for 10-7 erg/cm2 s (~10 GRBs/month)

  • Future Plan: SMILE-satellite (~ 1mCrab sensitivity in 106 sec)

❏ Well-defined PSF without ML-EM ❏ Powerful background rejection by dE/dx

34th ICRC Hague, 4 August 2015

ETCC has the potential to overcome the problems in MeV band.

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SLIDE 11

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Thank you for your attention!

Details are discussed in T.Tanimori+2015 accepted for publication in ApJ. [arXiv: 1507.03850] Report of polarization measurement will be submitted within the year.