Kick of neutron stars as a possible mechanism for gamma-ray bursts Yong-Feng Huang Department of...
-
date post
21-Dec-2015 -
Category
Documents
-
view
214 -
download
0
Transcript of Kick of neutron stars as a possible mechanism for gamma-ray bursts Yong-Feng Huang Department of...
Kick of neutron stars as a possible mechanism for
gamma-ray bursts
Yong-Feng Huang
Department of Astronomy, Nanjing University
Fishman et al. 1994
1. Background --- GRBs
Short bursts of -rays from the sky (Klebesadel et al. 1973) 。
Durations: ms --- ks
Basic features of GRBs
-- spatial features
-- detection rate:
-- temporal features
-- spectral features
• Profiles Complicated
• Durations 5 ms ─ 10 s ─ 5×103 s
• Variability 0.1ms ─1ms ,
• No repetition
1-2 events per day by CGRO/BATSE
• Photon Energy 0.1 ─ 1 MeV ─ 20 GeV
• Non-thermal:
N(E) E∝ -α
• High Energy Tail:
no cutoff above 1 MeV
• Fluence:
10-5 ─ 10-7 ergs /cm2
logIsotropicLack of weak GRBs
Breakthrough in 1997: afterglows discovered
X-ray afterglow of GRB 970228: discovered by BeppoSAX 。Optical, radio afterglow also observed
GRBs are at cosmological distances
Optical afterglow Groot et al., IAUC 6584 X-ray afterglow Costa et al. 1997, Nature
• Hundreds of GRBs localized • Optical afterglows: ~40 % • Redshift measured: ~20 % • Radio afterglows: ~10 % ( Error bars: 0.001’’ )
Basic features of afterglows
GRBs located:960720 970111 970228 970402 970508 970616 970815 970828 971024 971214 971227 980302 980326 980329 980425 980515 980519 980613 980703 981220 981226 990123 990217 990506 990510 990712 991208 991216 000301c 000630 000630 000418 … …
F t ∝ –1 ─ t –2
Kann 2008
the Fireball Model
Inter-StellarMedium
初始火球
~108 kmγ~1000
internalshocks
External shocks
~1011 kmγ>>1R~10 km
E>1052 ergsM<10-5 Msun
Afterglows
However, what is the central engine?
GRB主暴
2. Central engines of GRBs
Observational constraints:1. Isotropic energy release: 1049 --- 1054 ergs 2. Event rate: ~10-6/galaxy/yr3. Low baryon contamination
~10-5Msun per 1052 ergs, gamma ~ 100 -- 10004. Duration: short ms -- ks5. Fast variability variation timescale as small as: ms6. Long-term activities Energy injections, flares: 1000 s – 10000 s
Central enginesCollapse of massive stars Collision of Compact stars Phase transition of NS to Strange star Kick of neutron stars (Cen 1999; Dar 1999; Huang et al. 2003) Other mechanisms
3. GRBs from NS kicks
Jet energy:
Momentum conservation:NSNSflow / VMcE
Radiation energy:
ergs104~05.0,3.0 54iso E
Assume: NS kick is associated with the launch of a jet.
And the jet is ultra-relativistic.
(Cen 1999; Dar 1999; Huang et al. 2003)
Kick mechanism
(i) Hydrodynamically driven kick mechanism kick time scale: ~0.1 s (Lai et al. 2001)
difficult to produce high speed NS (> 500km/s) (Janka & Muller 1994)
(ii) Neutrino-driven kick mechanism asymmetric neutrino emission induced by strong B difficult to produce high speed NS (need B > 1016 G) (Lai et al. 2001)
(iii) Electromagnetic radiation-driven kicks EM radiation from a rotating off-centered magnetic dipole
(Lai et al. 2001)
Event rate
Observational constraints:GRB event rate: ~10-6/galaxy/yr
SN rate: 1/30 – 1/50 /yr/galaxy
NS birth rate: ~10-2 /yr /galaxy
High speed NS birth rate: ~10-4 – 10-3 /yr/galaxy
Beam corrected GRB rate: ~10-7 – 10-6 /yr/galaxy
Baryon contamination
Observational constraints:Low baryon contamination
~10-5Msun per 1052 ergs, gamma ~ 100 – 1000
Naturally expected in the EM radiation-driven kicks
emitted particles are mainly electrons/positrons
Duration
Observational constraints:Duration: short
ms -- ks
Electromagnetic radiation-driven kicks
millisecond magnetar can do the job
(Usov 1992)
Fast variability
Observational constraints:Fast variability
variation timescale as small as: ms
Guaranteed by NS spin
may produce a precessing jet
Long-term activities
Observational constraints:Long-term activities
Energy injections, flares: 1000 s – 10000 s
Dipole radiation of the pulsar
Dai 2004
Short GRBs
Long GRBs: duration ~ 20 s
Short GRBs: duration ~ 0.2 s
For a NS, when P < Pcr ~ 0.5 – 1.6 ms, instability arises inside the star, and gravitational radiation plays the major role in slowing down the NS. Then the spin-down timescale is:
Conclusions
Observational constraints:1. Isotropic energy release: 1049 --- 1054 ergs 2. Event rate: ~10-6/galaxy/yr3. Low baryon contamination
~10-5Msun per 1052 ergs, gamma ~ 100 -- 10004. Duration: short ms -- ks5. Fast variability variation timescale as small as: ms6. Long-term activities Energy injections, flares: 1000 s – 10000 s
Thank you !