17
Hot Relics in GRB Photosphere and GeV Photon Delay Kunihito Ioka (KEK)

Hot Relics in GRB Photosphere and GeV Photon Delay Kunihito Ioka (KEK)

Embed Size (px)

Citation preview

Page 1: Hot Relics in GRB Photosphere and GeV Photon Delay Kunihito Ioka (KEK)

Hot Relics in GRB Photosphere and GeV Photon Delay

Kunihito Ioka (KEK)

Page 2: Hot Relics in GRB Photosphere and GeV Photon Delay Kunihito Ioka (KEK)

Contents

Very High Lorentz Factor (VHLF)Gmax can be up to ~106 (> Gmax,conv~103)

Internal Shock Synchrotron⇒ Power-law component over >7 decades

c tdelay ~ Baryon Load Radius~ Progenitor Radius ~ 1010cm

Neutrino – GeV g Anti-Correlation

Page 3: Hot Relics in GRB Photosphere and GeV Photon Delay Kunihito Ioka (KEK)

Fermi Revolution

Abdo+ 09Ohno’s talk

MeV

GeV

GeV onset delay gg→e+e-

⇒ G>103

~1 sec

Page 4: Hot Relics in GRB Photosphere and GeV Photon Delay Kunihito Ioka (KEK)

Fermi Revolution

Abdo+ 09Ohno’s talk

GRB 090902B

GRB 090510

Band component+ Power Law

Band ~ Black body-like⇒ Photosphere emission

GeVkeV

Hurley+94Gonzaletz+03

Page 5: Hot Relics in GRB Photosphere and GeV Photon Delay Kunihito Ioka (KEK)

Photosphere-Internal-External Shock Model

Photo-sphere

InternalShock

ExternalShock

νFν

νkeV MeV GeV

Toma, Wu & MeszarosKumar & Barniol Duran 09Ghisellini+09, Wang+09Corsi+09, Gao+10

Variable Long-lived

Page 6: Hot Relics in GRB Photosphere and GeV Photon Delay Kunihito Ioka (KEK)

Amati/Yonetoku Relation

L T∝ 2

L = 4πr02aT0

4

Tobs ~ T0

L T∝ 4

Yonetoku+KI 03[Ghirlanda’s talk]

A Distance Indicator

Page 7: Hot Relics in GRB Photosphere and GeV Photon Delay Kunihito Ioka (KEK)

Fireball Dissipation

ln r

L = 4πrb2aTb

4

Tb ∝ rb−1 2L1 4

r0 rb

G

rshrph

Tobs

Gm

For Yonetoku Rel.

rb ∝Γm−1 ∝ L−1 2

Rees & Meszaros 05Thompson+ 07Ghisellini+ 07Ryde & Pe’er 09KI+07

Page 8: Hot Relics in GRB Photosphere and GeV Photon Delay Kunihito Ioka (KEK)

Radiation

in Comoving

Proton

Energy Densityafter Shock

pp collision thick pp collision thin

Accelerated to Very High

Radiation Dominated

Γm

′ U γ ~ ′ U p>> ′ U p,rest

Γc ~ Γm2

~ 104 −106( )

′ γ p ~ Γm

~ 102 −103( )

(A) Ekinetic << Eγ ⇐ E internal( )

(B) Eγ ~ Ekinetic ⇐ E internal( )

~ Hot Relicsin Cosmology

Page 9: Hot Relics in GRB Photosphere and GeV Photon Delay Kunihito Ioka (KEK)

Conventional Fireball

Gmax~103

Meszaros & ReesShemi & PiranPaczynskiGoodman

Baryon-LessBaryon-Rich

Page 10: Hot Relics in GRB Photosphere and GeV Photon Delay Kunihito Ioka (KEK)

Reheated Fireball

Gmax~106!

KIin prep.

Baryon-LessBaryon-Rich

Page 11: Hot Relics in GRB Photosphere and GeV Photon Delay Kunihito Ioka (KEK)

Internal Shock Synchrotron

KIin prep.

Page 12: Hot Relics in GRB Photosphere and GeV Photon Delay Kunihito Ioka (KEK)

For Moderate GToma+10

G~103

Page 13: Hot Relics in GRB Photosphere and GeV Photon Delay Kunihito Ioka (KEK)

Max Synchrotron Energy

′ t acc = ′ t cool

νmaxcool =

mec2

αΓ ~ 500 GeV

Γ

104

⎝ ⎜

⎠ ⎟

′ t acc = ′ t dyn

νmaxdyn ~ 1 GeV

Γ

6 ×104

⎝ ⎜

⎠ ⎟−6

GRB 090926 Break??

A target for CTA

Very High Lorentz Factor (VHLF) case

Wang+ 09Piran & Nakar 10Barniol Duran & Kumar 10

KI in prep.

Page 14: Hot Relics in GRB Photosphere and GeV Photon Delay Kunihito Ioka (KEK)

GeV Onset Delay

pp Collision Thick Thin⇒[Baryon-rich Barion-less]⇒

Page 15: Hot Relics in GRB Photosphere and GeV Photon Delay Kunihito Ioka (KEK)

νFν

νFν

νFν

Time

MeV g

GeV g

TeV n

Time

Time

η

Time

ηk1

pp thin

pp thick

pp→p→nen~Gm

2mpc2>0.1TeV

TeV n – GeV g Anti-Correlation

Baryon-less

Baryon-rich

Page 16: Hot Relics in GRB Photosphere and GeV Photon Delay Kunihito Ioka (KEK)

Summary

Very High Lorentz Factor (VHLF)Gmax can be up to ~106 (> Gmax,conv~103)

Internal Shock Synchrotron⇒ Power-law component over >7 decades

c tdelay ~ [rm=rpp~L-1/5] ~ Rstar ~ 1010cm

Neutrino – GeV g Anti-Correlation

Page 17: Hot Relics in GRB Photosphere and GeV Photon Delay Kunihito Ioka (KEK)

Two-Mass Collision

Coasting Gc~Gm2

Mass=ErGr/Gm2<10− 8M ( available at Rstar)

E rΓr + Mc 2 = Γm Mc 2 + Em( )Γm

E r Γr2 −1 = Γm Mc 2 + Em( ) Γm

2 −1

Energy

Momentum

⇒ Γm ~E rΓr

2Mc 2∝ L1 2

E r

Γr

< Mc 2 < E rΓr

⎝ ⎜

⎠ ⎟

YonetokuRelation

Em ~ Γm Mc 2 Before dissipation,rela. matter E ~ radiation E