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(1)

Recent Results from

the CANGAROO Observations

Kyoshi Nishijima

Department of Physics, Tokai University

(2)

Observation Technique of Gamma-Rays

„ E≥300 GeV

‹ IACT(Imaging Air Cherenkov Telescope)

‹ Large collection area

‹ Whiple, CANGAROO, HEGRA, ・・・

‹ Array of heliostats (→50 GeV)

Š CELESTE, STACEE, ・・・

„ E≤30 GeV

‹ Satellite

Š OSO-3, SAS-2, COS-B, EGRET, ・・・

Š AGILE, GLAST (→ 100GeV)

Whipple STACEE

EGRET

(3)

Satellite vs

Ground-based gamma-ray telescope

Base Satellite Ground

Gamma- ray

detection

Direct

(pair creation) Indirect

(atmospheric Cherenkov) Energy < 30 GeV

( 100 GeV)

>300 GeV ( 50 GeV) Pros High S/N

Large FOV

Large area Good ⊿θ Cons Small area

High cost

Low S/N (CR bkgd.) (but imaging

overcomes this!) Small FOV

(4)

4

Imaging Air Cherenkov Technique

Seff = 108109cm2

(5)

Image Parameters

(Simulation)

D.J. Fegan, J.Phys.G, 1997

(6)

CANGAROO Collaboration

Collaboration of Australia and Nippon for a GAmma Ray Observatory in the Outback

z University of Adelaide

z Australian National University

z Ibaraki University

z Ibaraki Prefectual University

z Kanagawa University

z Konan University

z Kyoto University

z Nagoya University

z National Astronomical Observatory of Japan

z Osaka city University

z Institute of Physical and Chemical Research

z Shinshu University

z Institute for Space and Aeronautical Science

z Tokai University

z University of Tokyo

z Tokyo Institute of Tehnology

z Yamagata University

z Yamanashi Gakuin University

(7)

CANGAROO-II 10m Telescope

1992-1998 3.8 m 10m telescope

Focal length 8m

Parabola 80cm CFRP

mirrors 114 (57m2) Number of

PMTs

552 (1/2”) FOV ~ 3° (4° )

Electronics TDC & ADC Point image

size 0.20° (FWHM)

(<0.15° )

Mar2000- 10 m

May1999- Feb2000

7 m

(8)

Why VHE Gamma-Rays ?

Origin of cosmic rays

Characteristics of cosmic ray sources Physics of particle accerelation

Something new....

(9)

Energetics of Cosmic Rays

(<1016 eV) Required Energy Supply

~1040 erg/s

~ 106~7 yrs, ρCR ~ 1 eV/cm) Unique Candidate

SNR Emax ~ 1015 eV

Extra Galactic Origin (>1018 eV) Emax~1020 eV

Spectrum Index   

-2.5 ~ -3.0

Shock Acceleration  

Composition : Mainly Protons

Origin of Cosmic Rays

(10)

TeV Gamma-Ray Processes

Uphoton

2 T max I.C. 3

4

dt

dE = σ

2 3

4 2 2

T max Sync

B dt

dE = σ

6 .

1

E

2 .

2

E

2 .

2

E

2 .

2

E

2 .

2

E E1.6

(11)

Why VHE Gamma-Rays ?

Origin of cosmic rays

Characteristics of cosmic ray sources Physics of particle acceleration

Something new....

(12)

TeV Gamma-Ray Sources

Galactic Objects

„ Pulsar/nebula: Young pulsar + synchrotron nebula Crab pulsar, PSR1706-44, Vela pulsar,( PSRB1509-58)

„ SNR:Synchrotron X-rayemission,

SN1006 , RX J1713.7-3946, Cas A ,(RCW86, RX J0852-4622)

„ Other candidates: G.C., Micro qusar, pulsar/Be star binary

Extragalactic objects

„ AGN: nearby blazars (z <0.1)

Mkn421, Mkn501, PKS2155-304, 1ES1426+428,

1ES2344+514, 1ES1959+650 , (PKS2005-489, EXO055625-3838.6)

„ Starburst galaxy: NGC253

„ Other candidates: Merging cluster of Galaxy

(13)

Crab nebula:

unpulsed spectrum

Aharonian & Atoyan, astro-ph/9803091 / Heidelberg WS, 2000

synchrotron

IC

SSC(Synchrotron Self Compton) B=(170±30)µG (Aharonian et al. 2000)

Emax 1016eV (De Jager & Harding 1992)

important tested and calibration source

(14)

PSR1706-44: Differential flux

Chandra ACIS

PSR 1706-44

ATCA image

zPeriod :102 ms

zDistance :1.8 kpc

zAge :1.7×104 yr

zSpin-down energy loss : 3.4×1036 erg/s

Differential Flux

10 arcsec

= 0.087 pc

E-3.0

vary around 1 TeV ? steep above 1TeV

IC scattering due to electrons ?

(15)

PSR1706: Multiwavelength Spectrum

New

Sync IC

TeV gamma-ray flux is difficult to be explained by Sync-IC model (2.7K CMB) in the nebula.

Energy (eV)

E2 ×I(E)(erg cm-2 s-1 ) ●CANGAROO ☆COMPTEL

Radio(VLA) RXTE

*Optical(VLT) ★OSSE

*Optical nebula ■EGRET pulsed

Chandra pulsarEGRET unpulsed Chandra nebula

IC with 2.7K CMB B=3µG

B=0.15µG Sync.

X-ray sync. peak energy:

higher than 10 keV Expected IC peak energy:

higher than our results

(16)

Period [sec]

E (erg/s)/4pd (cm)2.

PSRJ1420-6048

Thompson, Heidelberg WS, 2000

PSRB1706-44 PSRB1509-58

Crab

Vela

Chandra ACIS(2000),

〜60arcsec=0.15pc Vela

Chandra ACIS(2000),

〜200arcsec=4.3pc PSR1509-58 ASCA image

10 arcmin.

pulsed

unpulsed

TeV Gamma-ray sources of pulsars and candidates

Roberts,Romani,Johnston (2001) ApJ 561: L187—L190.

(17)

Supernova Remnant: SN1006

z Radio:Shell, with two bright arcs

z X-ray:Thermal shell, with non-thermal limb-brightened arcs

z Distance:Optical spectra and proper motion indicate 1.7-3.1 kpc, modeling spectra gives 1.8±0.3 kpc

Shock structure

Chandra ACIS T. Naito

(18)

Observation by ASCA/SIS : SN1006

Non-thermal emission from NE rim existence of high energy electrons up to 100 TeV the possibility of TeV Gamma-Ray Emission

Several Peaks:

Thermal Emission

`Power-law

Synchrotron Rad.

Koyama et al.1995

(19)

Chandra ACIS

Significance map: SN1006

We succeeded in detection of TeV signals

from the northeast rim. 10m result.

PSF ~0.25 deg radius.

3.8m result.

(20)

Multi-band Spectrum & Fitting:SN1006

S = -2.2 B ~ 4μG Emax ~50TeV

Durham

TeV emission : IC scattering of CMB photons by high energy electrons.

Naito et al. Astron. Nach. 320, 1999

There is no evidence of proton acceleration.

(21)

Supernova Remnat: RXJ1713.7-3946

Radio Image @843MHz

Galactic plane CO Image

Slane et al, ApJ, 525,1999

Adjacent clouds

& HII region

Density in SNR

<<1atom/cm-3

Discovered in ROSAT All Sky Survey

(22)

Observation by ASCA/SIS : RX J1713.7-3946 (G347.3-0.5)

Synch. X-ray Emission (ASCA)

Existence of multi TeV

Electrons

Tomida, Ph.D., 1999 Slane et al, ApJ, 525,1999

z Radio:Faint emission

z X-ray:Non-thermal, with limb-brightened, with central sources

z Distance:Association with molecular clouds, and HII region, suggests 6 kpc

(23)

TeV gamma-rays expected from

synchrotron inverse Compton model:

RX J1713.7-3946

Synchrotron Rad.

3µG

Ellison et al 2001

5µG 10µG 2µG

20µG I.C.

1TeV Naito et al 2001(CANGAROO)

3.8m

(24)

Spectrum & Significance map:

RX J1713.7-3946

8 .

2

E

X-ray TeVγ Infrared Steeper sub-TeV spectrum than

expected from IC model

(25)

Multiwavelength spectrum : RX J1713.7-3946

π0 decay Bremsstrahlung

I.C.

TeV spectral shape does not show a good fit with simple IC model

Detected gamma-rays are produced by π0 decay rather than IC.

Nature 416(2002) 823

Sync.

Proton acceleration?

(26)

Non-thermal shell type SNRs

RX J0852-4622

Dist >1kpc?

RCW86

Dist. a few Kpc Type II

Slane et al. 2001

ASCA Results

Bamba et al. 2000

(27)

AGN: Mkn 421 Variability and Multiwavelength Observation

Time scale < a few hours   R<10-4 pc (10RSch radii of a 108 Solar mass black hole)

Correlation with an X-ray variability

The X-ray and the TeV photons arise from the same emission region, likely from the same population of

synchrotron radiating electrons

the SSC mechanism is at least partially if not dominantly at work in the γ-ray production

Gaidos et al., Nature, 383, 1996

Takahashi et al. ApJ 542, 2000

(28)

AGN: Mkn 421

multiwavelength spectrum

Takahashi et al. ApJ 542, 2000

Synchrotron

+ inverse Compton model works well

e± origin Proton model

still possible synchrotron inverse Compton

One-zone SSC model δ=14, B=0.14G

(29)

CANGAROO Observation of Mkn421 in 2001

Observation:10 nights during extremely

strong flare periods Large zenith angle observation:(70 °) Energy threshold :

10TeV effective area: more than ten times larger than the case of

vertical showers

(30)

Attenuation of TeV Gamma-rays with CIB

Energy spectrum in multi TeV ⇔ absorption of TeV gamma-rays due to cosmic infrared photon background(CIB)

E>10TeV gamma-rays from Mkn421 ⇒ suppressed

interaction with mid- to far-infrared photons

(31)

Energy spectrum: Mkn421

TeV cm

TeV ph E dE

dN stat syst

syst

stat / /sec/

10 10 )

3 . 0 9

. 0 3 . 3

( 2

) 3 . 0 0

. 4 ( 13

. .

. . 9 . 0

8 .

0 ±

+

×

±

±

=

Energy spectrum steeper than that observed E<10TeV However, marginally significant excess (4σ) observed at E>20TeV ⇒ Cut off energy:〜8TeV

assuming power law

ApJ. 579 (2002) L9

(32)

PKS2155-304 Energy Spectrum (preliminary)

CANGAROO has not succeeded in detection of VHE gamma-rays from other blazars.

- Durham group reported the detection from PKS2155-304 in 1997 correlated with a strong X-ray flare

- This is the only TeV blazar detected in southern sky

- We have observed, but only upper limits are obtained

Integral Flux (cm-2 sec-1 )

(33)

NGC253

distance : 2.5 Mpc

Enhanced star formation rate High SN rate : 0.1 - 0.3/yr

Higher CR production by factor 10-100

The emission region is:

- much broader than the PSF of our telescope

- somewhat larger than the optical image of the galaxy.

Gamma-ray signals (0.5TeV) are detected at a high

confidence level(>10σ)

(34)

NGC253: differential flux

( ) 12 3.85 0.46

10 1 71

. 0 85 . 2

±

×

±

= TeV

E dE

dF

b b E

E e

E ae E

dE

dF 1.5 /

0

0 /

⎟⎟

⎜⎜

=

(1)

(2) Crab

(2)

(1)

(a=6×10-5, E0=200MeV, b=0.25±0.01) (2) New TeV gamma-ray source !

Submitted for publication

(35)

Summary of Galactic Sources

„ Pulsar/nebula

Š Unpulsed TeV gamma-ray emission from young pulsars with synchrotron nebula are detected.

Š Crab, Vela, PSR1706-44

Š seem to be well explained by IC with CMB or SSC by e± ?

„ SNR

Š Shell type SNRs with non-thermal X-ray emission are detected in TeV region.

Š SN1006, RXJ1713.7-3946, Cas A

Š seem to be well explained by IC with CMB by e± , or by π0 decay produced by proton(Cosmic Ray Origin) ?

„ Other candidates

Š G.C., Micro qusar, pulsar/Be star binary....

(36)

Summary of Extragalactic Sources

AGN (still not well-understood!)

„ 6 nearby blazar, HBLs, Strongly time variable,

„ Mrk421, Mkn501, PKS2155-304, 1ES1426+428, 1ES2344+514, 1ES1959+650

„ Leptonic models are preferred

„ SSC(Synchrotron Self Compton) model ? EC(External Compton) model ? accretion disk ?, BLR clouds?

„ Hadoronic models are not ruled out

„ photo-meson production ? photo-pair production ? proton synchrotron ?

Starburst Galaxy

„ NGC253:the first normal spiral galaxy other than our own where TeV cosmic rays exit

Other candidates

„ EGRET unID, GRBs, SUSY particles, Merging clusters,G.C., Diffuse, ..., and more ?

(37)

Summary of VHE Gamma-ray Astronomy

Experimentally, great progress has been made last decade.

Source count is increasing steadily, however it is still a handful.

We need more sources and better data.

With the advent of CANGAROO-III, HESS,

MAGIC, (VERITAS), we are entering a new era for observations

Broadband simultaneous observations are essential!

(38)

CANGAROO-III

(Stereo Observation)

Array of four 10m telescopes(~2004) Full Imaging:

„ Angular Res. : ~0.1 deg.

„ Energy Threshold: ~100GeV

  

(39)

Third generation ground-based

IACTs

CANGAROO-III 4×10m, Australia, 2000-

VERITAS

7×10m, Arizona, 2004-

HESS 4×12m, Namibia, 2002-

MAGIC

1×17m, Canary Island, 2001-

(40)

Summary of VHE Gamma-ray Astronomy

Experimentally, great progress has been made last decade.

Source count is increasing steadily, however it is still a handful.

We need more sources and better data.

With the advent of CANGAROO-III, HESS,

MAGIC and (VERITAS), we are entering a new era for observations.

Broadband (simultaneous) observations are essential!

(41)

TeV sky 2000

(42)
(43)

Sensitivity of future detectors

(44)

Third EGRET catalog

R.C. Hartman et al., ApJS, 1999

Referensi

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