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High-Energy Gamma-Rays and Physical Implication for GRBs in Fermi Era

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Presentation on theme: "High-Energy Gamma-Rays and Physical Implication for GRBs in Fermi Era"— Presentation transcript:

1 High-Energy Gamma-Rays and Physical Implication for GRBs in Fermi Era
Katsuaki Asano (Tokyo Institute of Technology)

2 Particle Acceleration
Outline Introduction Limit on LIV Jet Acceleration Particle Acceleration

3 Gamma-Ray Burst The most luminous explosion in the universe
erg/s Reference: Sun erg/s X-ray star 1038 erg/s Supernova, Galaxy 1043 erg/s AGN 1046 erg/s SGR 1047 erg/s Light Curve

4 GRB rate Supernova rate ~ 2.4x105 Gpc-3yr-1 (60% II, 30% Ia,
10% type Ib/c) Hypernova ~500 Gpc-3yr-1 GRB (Jet corrected) ~20 Gpc-3yr-1 ~1 detection/day

5 Standard Picture ISM External Shock Internal Shock

6 Afterglow Racusin et al. 2009 Nardini et al. 2009

7 Evidence of Collimated Jet
Sideway Expansion Jet Break Stanek et al. 2000 Apparent Energy >1053erg ->Actual Energy erg?

8 The most distant object ever confirmed
GRB z=8.2, t=0.6 billion yrs LyαEmitter z=6.964, t=0.78 bill. yrs

9 Open Problems Emission Mechanism (Synchrotron?)
High Efficiency Spectrum Central Engine (Death of Massive Star?) Progenitor Energy Release Jet Acceleration & Collimation Afterglow (External Shock?) Spectrum & Time Evolution

10 2008/6/11

11 GRB C; Spectra Classical Energy Range

12 Famous Fermi/LAT GRBs GRB 080825C GRB 080916C GRB 081024B GRB 090510
First LAT GRB, delay for>100MeV GRB C Eiso=8.8x1054 z=4.35, delay GRB B First short LAT GRB, delay GRB z=0.903, delay?, extra component GRB B Eiso=4x1054 z=1.822 , extra component

13 Constraints on Lorentz Invariant Violation

14 Measuring the Speed of Light
GRBs: Bright Distant Objects with Emissions of Wide Energy Ranges -> Ideal to measure the difference of “c”! Loop quantum gravity? NYTimes ’09 Oct. 28

15 Motivation How to reconcile gravitation with quantum mechanics?
-> Classical symmetric properties will be sacrificed? (Spontaneously? Effectively in 4-D?) Effective Field Theory (Colladay & Kostelecky 1998) CPT violating CPT conserving Photon velocity CPT symmetry kills the term.

16 Quantum Gravity Test 高エネルギー光子が遅れてくる? ? (LHC BH??)
Smaller MQG -> large time delay?

17 GRB 090510 Short GRB Precursor Delay z=0.903 (traveling 7.3 Bill. yrs)
8keV-260keV 260keV-5MeV z=0.903 (traveling 7.3 Bill. yrs) Eiso=1053erg >100MeV >1GeV 31GeV, 3.4GeV

18 “c” is the same with 18 digits!
?? cm/s depends on E? At least MQG,1>Mpl !

19 CTA We can expect 1000 photons @ 10 GeV from a GRB. 10 GeV pulse shape
~keV pulse shape Much stronger constraint

20 Ultra-relativistic… Jet Acceleration

21 GRB 080916C Long GRB Delay z=4.35 Eiso=8.8x1054erg ~5xMsunc2 13GeV
8keV-260keV GRB C 260keV-5MeV Long GRB Delay z=4.35 Eiso=8.8x1054erg >100MeV ~5xMsunc2 >1GeV 13GeV 3GeV

22 Compactness Problem If gamma-rays are emitted isotropically, GeV photons cannot escape because electron-positron pairs should be created via photon-photon collision. →Inconsistent with obs. In the comoving frame… If the sources are ultra-relativistic… (We have observed blue-shifted photons) X-ray No high energy photons

23 Minimum Lorentz factor
GRB > 1200 GRB C > 900

24 Fireball Acceleration
Radiation dominated plasma; huge amount of electron-positron pairs and photons, and small amount of protons. Adiabatic Expansion; Thermal Energy -> Bulk Kinetic Energy Fireball Evolution: is required.

25 Central Engine How to deposit energy without much baryons?
Neutrino pair annihilation? Collimated energy injection can evacuate baryons and make a fireball. Macfadyen & Woosley

26 Lack of Thermal Emission
The fireball becomes optically thin as it expands. -> Thermal Photons GRB C GRB090102 Optical polarization is reported. -> Strongly Magnetized Plasma? Zhang & Pe’er 2009

27 Poynting Flux Dominated Jet?
Magnetic Energy dominates the bulk kinetic energy -> can be relativistic. MHD turbulences (MRI) enhance the magnetic field. Weak points: Hard to produce shocks Hard to induce magnetic reconnection How to convert kinetic energy into photons?? McKinney & Blandford 2009

28 Ultra High Energy Cosmic Rays
Particle Acceleration

29 Ultra High Energy Cosmic Ray (UHECR)
Where is the accelerator?? (Strong magnetic field or large size to confine particles) n(E)∝E-3 Energy distribution >1020eV Ref: 7 TeV by LHC AGN? (low number density)

30 Highest Accelerator=GRB?
We need ergs/Mpc3/yr to explain UHECRs See e.g. Murase et al. 2008 We may need Up/Ue>20. If GRB rate is 0.05 Gpc-3/yr, Up/Ue>100 Hidden Energy?

31 GRB ; Spectra Band+ Extra PL

32 Extra Component=Afterglow?
2009 GRB

33 GeV-MeV correlate? Abdo et al Supporting material

34 Signature of Proton Acceleration?
Hadronic Cascade p+γ→p(n)+π0(π+) p+γ→p+ e+ + e- π0→γ+γ, π+→μ+ +νμ μ+ →e+ + νμ + νe Synchrotron from π+ ,μ+, e± Inverse Compton from π+ ,μ+, e± γ+γ→ e+ + e- Synchrotron Self Absorption

35 Cascade due to photopion production
Asano, Guiriec & Meszaros 2009 Cascade due to photopion production gg-absorption R=1014 cm G=1500 Band component 3.4GeV Synchrotron and Inverse Compton due to secondary electron-positron pairs

36 Proton Synchrotron R=1014 cm Even in this case,
secondary pairs contribute

37 Proton Dominated GRBs Favorable for ultra high-energy cosmic ray production Asano, Inoue & Meszaros 2009 GRB 10keV 1MeV 1GeV The extra component: Hard spectrum: Index -1.6 Comparable flux to the Band flux 10 keV

38 Neutrinos from GRB 090510 “Bright” Neutrino
We may need >10-2 erg/cm2 to detect with IceCube.

39 GRB B

40 Conclusion LIV with n=1 may be excluded.
Lorentz factor of GRB Jets > 1000. Possible signature of UHECR production. New Theoretical Challenge: Delayed onset of GeV Emission GRB C GRB


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