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Neutrinos as probes of gamma-ray bursts. Hylke Koers. Service de physique théorique, UL Brussels. Based on work in collaboration with: Ralph Wijers (API Amsterdam) Asaf Pe’er (Giacconi fellow, Hubble Space Telescope Science Institute)
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Neutrinos as probes of gamma-ray bursts Hylke Koers Service de physique théorique, UL Brussels Based on work in collaboration with: Ralph Wijers (API Amsterdam) Asaf Pe’er (Giacconi fellow, Hubble Space Telescope Science Institute) Dimitrios Giannios (Max-Planck-Institute for Astrophysics Garching) TexPoint fonts used in EMF. Read the TexPoint manual before you delete this box.:
Outline A gamma-ray burst primer Fireball neutrino cooling Neutrino production in np collisions Neutrino emission from choked GRBs
Motivation Interesting for modelling: unresolved observations and extreme properties Probes of the universe up to z ~ 5, constraining DM and DE Candidate sources of cosmic rays Speculative ideas: constraining Lorentz invariance through arrival times, ... (?) Candidate sources of neutrinos
A GRB primer: observational landmarks • Some observational landmarks: • ’60s: Discovery of very energetic flashes of gamma rays. (military VELA satellites) – distance scale? • >1991: Isotropic distribution found (BATSE all-sky monitor from CGRO) • 1997: Afterglow observations establish cosmological scales (BeppoSAX satellite) • 1998: First identification of a contemporaneous SN – GRB (BeppoSAX / BATSE) • 2004: SWIFT satellite observes shallow decay phase, late energetic flares, and other unexpected phenomena
A GRB primer: prompt emission • Key features of the prompt emission • Irregular lightcurves:“if you’ve seen one GRB...” • Rapid varibility, up to 10-3 sec. • Duration from 10-2 s – 103 s, subdivided intolong GRBs (~20 sec) and short GRBs (~0.2 sec) • Non-thermal spectrum (broken power-law), peaking around ~250 keV; occasionally extending to very high energies (> GeV... TeV?)
A GRB primer: afterglow • Key features of the afterglow • Broad-band spectrum over many decades in energy (radio, optical/IR, X-ray) • Characteristic break energies compatible with synchrotron emission • Slowly declining (typically power-law) lightcurve (sometimes detectable up to years
Initial phase(106.5 cm) Catastrophic event: core-collapse of a massive star (long GRB): Formation of black hole + accretion disk system which launches a fireball Acceleratingphase(108 cm) Fireball accelerates to relativistic velocities G ~ 300by radiation pressure; stops due to energy constraints (baryonic load) Energy dissipation (shock acceleration):gamma-ray burst Coastingphase (1012 cm) Interaction with external environment: afterglow Afterglowphase (1016 cm) A GRB primer: the fireball model Key features Total energy ~ 1052 erg Lorentz factors ~ 300 Collimation Small baryonic load [Cavallo & Rees 1978; Paczynski 1986; Mészáros & Rees 1992, 1993]
n Neutrinos are expected to be very useful probes to gain insight in these issues! A GRB primer: open questions A GRB primer: open questions A GRB primer: open questions • Important (partly) unsolved questions: • How are the jets formed? • What is the nature of the outflow? Dominated by thermal energy (=fireball?) or by electromagnetic energy? • How is shock-acceleration realized? Hylke Koers, Service de Physique Theorique, UL Brussels Hylke Koers, Service de Physique Théorique, UL Brussels
Outline A gamma-ray burst primer Fireball neutrino cooling Neutrino production in np collisions Neutrino emission from choked GRBs Can neutrino cooling stop a developing GRB? [Koers & Wijers, MNRAS, 364, 934, 2005]
n e± n g p Fireball cooling: the fireball fire· ball [‘fIr-”bol]: A tightly coupled plasma of photons, electron-positron pairs and neutrinos(with a small baryonic load) • Environment • Temperature: T ~ 1011 K (20 MeV) • Electrons, positrons: ne ~ 1035 cm-3 • Baryons: nB ~ 1032 cm-3 • Neutrino physics dominated by leptonic • processes Dynamics The fireball expands by radiation pressure to relativistic velocities.
rapid cooling Fireball cooling: neutrino phase diagram Roughly 30% of the initial energy is released as a burst of ~60 MeV neutrinos The fireball is transparant in regions of fast neutrino creation. Here neutrinos just follow the usual hydrodynamic evolution. [HK & Wijers 2005]
Outline A gamma-ray burst primer Fireball neutrino cooling Neutrino production in np collisions Neutrino emission from choked GRBs Can we use neutrinos (or gamma rays) from nucleonic collisions to discriminate between models? [Koers & Giannios, A&A, 471, 395, 2007]
NP decoupling: characteristic radii Accelerating phase Coasting phase Fireball model: AC (magnetic) model:
np gamma rays(fireball only!) prompt GRB (internal shocks) ~100 keV ~10 GeV NP decoupling: neutrinos and gamma rays Fireball (FB) model AC model fluence fromburst at z=0.1 peak energy Both fluence and energy are below IceCube sensitivity!
Outline A gamma-ray burst primer Fireball neutrino cooling Neutrino production in np collisions Neutrino emission from choked GRBs Can neutrino emission indicate the existenceof choked GRBs? [Koers & Wijers, arXiv: 0711.4791]
Choked GRBs: model Hypothesis: suppose that a (large) fraction of supernovae is accompanied by GRB-like outflows that stops below the surface [Mészáros & Waxman 2002] No gamma-ray emission Potential source of neutrinos (largely unconstrained) Motivation: Observed SN – GRB connection Missing ingredient in SN modelling Ubiquity of astrophysical jets
Choked GRBs: protons Scheme: accelerate protons, create mesons,decay to neutrinos Proton shock acceleration VS • Proton energy losses • Synchrotron radiation • Photopion • ... [Razzaque, Mészáros & Waxman 2003, 2004, 2005; Ando & Beacom 2005]
Maximum energy (in jet frame) Choked GRBs: protons
Cooling break Choked GRB: mesons
Cooling break Maximum energy (in jet frame) Choked GRB: mesons
maximum energy Choked GRBs: neutrino spectrum Neutrino spectrum from meson (and muon) decay: cooling break Strong increase in high-energy neutrinos! (at Earth)
Choked GRBs: detection prospects NB: optimistic case of efficient meson injection
Conclusions Neutrino emission is an interesting and promising way to probe the physics of GRBs. However it remains a challenging task to identify concrete realizations of this potential.