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Page 1: Gamma-ray Bursts and Particle Acceleration

Gamma-ray Bursts andParticle Acceleration

Katsuaki Asano(Tokyo Institute of Technology)

S.Inoue ( NAOJ ) , P.Meszaros ( PSU )

Page 2: Gamma-ray Bursts and Particle Acceleration

Physical Condition in a Shell

R

ΔR=R/Γ2

Photons: Luminosity L

erg/s 10L ,300 cm,10 5214 R

In the comoving frame Energy Density: Magnetic Field:

erg/cc 1034

722

cRL

U

G 860081.0 UB

Page 3: Gamma-ray Bursts and Particle Acceleration

Time ScalesLet us consider a proton of 1019eV

In the comoving frame,7

2

19

106.3eV10

cmp

Dynamical Time Scale: sec 11/ cR

Acceleration Time Scale: sec 4.02

eBc

cm

cR pL

Cooling Time Scale: sec 18006

22

3

Bm

cm

eT

p

Page 4: Gamma-ray Bursts and Particle Acceleration

How to find evidence of proton acceleration?

Page 5: Gamma-ray Bursts and Particle Acceleration

Neutrinos

Page 6: Gamma-ray Bursts and Particle Acceleration

Neutrinos

Waxman and bahcall 1997, 1998

p+ γ→n+π +

π +→ μ + +νμ

μ + → e + + νμ + νe

log [

E N

(E)]

1052erg x 100=500R=5 1014 cmB=0.1eat 1Gpcby 105 km2 detector

Kaon-decay

Pion-decay

Muon-decay

16 17 18 19 20-4

-3

-2

-1

0

1

2

3

4

5

-4

-3

-2

-1

0

1

2

3

4

5

Next talk -> Murase

Asano & Nagataki 2006

Page 7: Gamma-ray Bursts and Particle Acceleration

PhotonsSee e.g. Meszaros 2006, Dermer & Atoyan 2006

Page 8: Gamma-ray Bursts and Particle Acceleration

GRB spectrum

???

Page 9: Gamma-ray Bursts and Particle Acceleration

To catch the sign of proton acceleration

• GLAST will be Launched May in this year.• It will observe 10 MeV - 300 GeV photons.

Page 10: Gamma-ray Bursts and Particle Acceleration

TeV Photons

HESS

MAGIC

CANGAROO-III

Page 11: Gamma-ray Bursts and Particle Acceleration

Proton Cascade

p+ γ→n+π +

      → p+π0

Asano 2005

Page 12: Gamma-ray Bursts and Particle Acceleration

I.C.

E (eV)

E2N(E) [erg/cm2]

104 105 106 107 108 10910-5

10-4

10-3

Distortion due to proton cascade

s 1.1

100

erg 1051

t

E sh

Lepton distribution

E

Primary Electrons

Pairs from Cascade

fB=1.0

e-SY

Our Monte Carlo Simulation

Asano & Inoue 2007

Up=UefB=UB/Ue

Page 13: Gamma-ray Bursts and Particle Acceleration

I.C.

E (eV)

E2N(E) [erg/cm2]

104 105 106 107 108 109 101010-5

10-4

10-3

Deviation due to Inv. Comp.

s 33.0

100

erg 1050

t

E sh

fB=0.1

No sign of protonacceleration

Asano & Inoue 2007

e-SY

Page 14: Gamma-ray Bursts and Particle Acceleration

I.C.

E (eV)

E2N(E) [erg/cm2]

104 105 106 107 108 109 101010-5

10-4

10-3

Double break

s 12.0

300

erg 1051

t

E sh

fB=1.0

Characteristic Spectrum due to Protons

e-SY

Page 15: Gamma-ray Bursts and Particle Acceleration

I.C.

E (eV)

E2N(E) [erg/cm2]

Proton

Muon

Pion

104 106 108 1010 101210-6

10-5

10-4

10-3

Proton and muon synchrotron

s 033.0

1000

erg 1052

t

E sh

fB=30.0

e-SY

Page 16: Gamma-ray Bursts and Particle Acceleration

Proton acceleration efficiency

eV10@ 19

We need 6-8 1043 ergs/Mpc3/yr to explain UHECRs

epacc UU /ξ

See e.g. Murase, Ioka, Nagataki, Nakamura 2008

We may need Up/Ue>20. If GRB rate is 0.05 Gpc-3/yr, Up/Ue>100

We have assumed Up=Ue so far, but…

Page 17: Gamma-ray Bursts and Particle Acceleration

GRB rate

Page 18: Gamma-ray Bursts and Particle Acceleration

Much more protons are accelerated?

me/mp

Particle Number Distribution

Electron Proton

Energy (Arbitrary)0.0001 0.01 1 100

1e-06

0.0001

0.01

1 Acceleration

Larmor radius∝EJust behind the shock front

Page 19: Gamma-ray Bursts and Particle Acceleration

Much more protonsf() erg/cm2

Proton x10, p=2.5,Esh=1051 erg, t=0.1 s,=300, fB=1.0

Sync-e+ e-

IC-e+ e-

Sync-Sync-

[eV]100 103 106 109 1012

10-5

10-4

10-3

10-2

Asano, Inoue, & Meszaros in prep.

Proton=10 x Electron

Page 20: Gamma-ray Bursts and Particle Acceleration

Much more protonsf() erg/cm2

Proton x100, p=2.5,Esh=1051 erg, t=0.1 s,=300, fB=1.0

Sync-e+ e-

IC-e+ e- Sync-

IC-p

[eV]100 102 104 106 108 1010

10-4

10-3

10-2

Proton=100 x Electron

Photons from Proton cascade dominate.

See also Asano & Takahara 2003

Page 21: Gamma-ray Bursts and Particle Acceleration

Very Hard GRB

Kaneko et al. 2008

GLAST will find more such bursts ?

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Esh-dependence

[eV]

f() [erg/cm2] Up/Ue=10, UB/Ue=1, t=0.1 s, =300

Esh=1049 erg

Esh=1050 erg

Esh=1051 erg

102 104 106 108 1010 101210-9

10-8

10-7

10-6

10-5

Page 23: Gamma-ray Bursts and Particle Acceleration

Up-dependence

[eV]

f() [erg/cm2] Esh=1051 erg, UB/Ue=1, t=0.1 s, =300

Up/Ue=10

Up/Ue=30

Up/Ue=100

102 104 106 108 101010-6

10-5

10-4

Page 24: Gamma-ray Bursts and Particle Acceleration

Γ-dependence

[eV]

f() [erg/cm2] Esh=1051 erg, Up/Ue=30, t=0.1 s, UB/Ue=1

103 106 109 101210-7

10-6

10-5

10-4

Page 25: Gamma-ray Bursts and Particle Acceleration

Hypernova

•Very bright supernova•Some associate GRBs•Progenitors may be massive stars (WR type?).•A stellar wind environment may exist around progenitors

Ejecta from hypernovae may be sources of 1017-1018eV CRs. (Wang et al. 2007)

Page 26: Gamma-ray Bursts and Particle Acceleration

Hypernovae are Sources of 1018 eV Cosmic Rays ?

1020eV

SNR ?

AGN? GRB?銀河団 ?

??

Wang et al. 2007

Page 27: Gamma-ray Bursts and Particle Acceleration

Particle Acceleration in Winds

Faster, Energetically lower

Page 28: Gamma-ray Bursts and Particle Acceleration

[eV]

f() [erg/cm2]

Initial p (dashed)

Final p/n (solid)

(solid)(dashed)

p-SY

p-IC

Hypernova

100 105 1010 1015 102010-12

10-10

10-8

10-6

Secondary ParticlesAsano & Meszaros 2008

@100Mpc

~ 4 days integration

Page 29: Gamma-ray Bursts and Particle Acceleration

Secondary Photons

[eV]

f() [erg/cm2]

GLAST

-decay

p-SY-SY

e-SY

MAGIC

XMM-NewtonRegenerated Photon

100 105 1010 101510-9

10-8

10-7

10-6

~ 4 days integration

Page 30: Gamma-ray Bursts and Particle Acceleration

Regenerated Photons

GRBGamma-ray

IR background photons

e+ e-

CMB photons

Inv. Comp.

Razzaque et al. 2004

Page 31: Gamma-ray Bursts and Particle Acceleration

Summary

• GeV-TeV emissions due to protons in GRBs• Too much protons change spectra drastically• Secondary emission from hyeprnovae

– X-ray due to cascade from muon decay– GeV emission from proton synchrotron– “Delayed” TeV emission