Two recent developments with Gamma Ray Burst Classification. And their implications for GLAST. Eric Charles. Glast Science Lunch Nov.

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Two recent developments with Gamma Ray Burst Classification And their implications for GLAST Eric Charles Glast Science Lunch Nov. 2, 2006

Outline Numerology, taxonomy and phrenology of GRBs Salient facts for GLAST Rates, spectra, variability, performance Previous observations MeV GeV GRM models and phenomenology (phrenology?) Recent developments Dichotomy in SHB/LSB environment LSB: SFR. Consistent w/ SNe collapse SHB: Older galaxies. Could favor binary merger model. Non-observation of SNe in long bursts Implications for GRB classification w/ GLAST data Conclusions

GLAST Performance I: LAT Angular Resolution (per γ) For typical observation angle F = 40 : A eff (40 ) ~ 0.75 A eff (0 ) thin thick Effective Area all layers At 30 (100) MeV single photon Angular resolution ~ 10 (3 ) PSF occupies 0.09 sr (0.0086 sr) http://www-glast.slac.stanford.edu/software/is/glast_lat_performance.htm

GLAST Performance II: GBM LAT FoV GBM FoV FoV = 9.5 sr ~200 GRBs/year, > 50 in LAT FoV GBM A eff ~ 100cm 1% of LAT A eff For E -1 ~ E -2 Sensitivity ~ LAT NaI crystals (12) BGO crystals (2)

Salient features of GRBs I: Light curves Highly variable. Spikes 1ms and shorter: LAT single g resolution ~ 0.5 us LAT deadtime ~ 27 us GBM deadtime ~ 3 us EGRET deadtime ~ 200 ms Diverse: no characteristic shape (Individual spikes are more similar) Bimodal duration distribution: ~ 0.2 s (short) ~ 20 s (long) Canonical 2s division for long/short Caveat: I suspect some effort went into finding set of 12 bursts that all look different from each other. Tricky combinatorial problem. Probably solved with visual search.

Salient features of GRBs II: spectra Peak of SED falls right in the Middle of GBM band Spectra are well fit with broken power law Low E (α ~ 1), High E (β ~ 2), Peak Energy E p = E 0 (2+α) E 0 is power law break

Salient features of GRBs III: classification Spectral LAG in long bursts LONG SHORT Short bursts tend to also be harder. Short-Hard Burst (SHB) v. Long Soft Bursts (LSB) Norris 2002, Norris & Bonnel 2006

Some more GRB Key features Agreed features: Collimated, relativistic Long/short dichotomy Decaying afterglows/ re-flaring Cosmological redshifts Band spectrum E p ~ 40 KeV 1 MeV Some SNe association Energy reservoir ~ SNe scale Disputed features: Jet opening angle value Energy transport mechanism HE γ emission mechanism Source of high variability, large Δt / t Observation angle Bulk Lorentz factor (Γ ~ 30-1000) Circumburst environment/ fields Cephid type relations (standard candles?) Polarziation Degree SNe association

GLAST Performance III: Projections 200 Burst/ yr in GBM 100 Burst/ yr in LAT (70 w > 10 counts) About 20% of Swift bursts in LAT FOV Handful of brigh bursts w/ 10s of γ above 1 GeV Extrapolation from BATSE data. Given the large (up to 5 decade) extrapolation and model dependence plot should be Tens of thousands of burst photons Plot from N. Omodei s talk @ San Servolo, June 2006

GLAST Performance IV: Backgrounds 10-2 Hz 10-3 Hz LAT regime Only the tails of the T 90 distribution get to 10 2-10 3 s Timescale for random EGB photons in LAT GRB PSF is 10 2-10 3 s Prompt emission is nearly background free Observing delayed emission on timescale of hours requires background subtraction/ statistics Likewise, observing several bursts

Egret observations I: High energy component Taking composite spectra of several GRB show no sign of HE cutoff Caveat: diversity of GRBs could Introduce artifact in this type of analysis Composite spectrum of 5 EGRET Bursts Dingus et al. 1997 Evidence of HE component in GRB 941017 No evidence of cutoff M.M. Gonzalez et. al. Nature 2003

Egret observations II: photons 2 photons @ 3 GeV 2 photons @ 3 GeV Photons @ 10 2 MeV Photons @ 10 2 MeV Do observe photons co-incident w/ bursts However Egret GRB observations only marginally quantitative Particularly hampered for short bursts 1) Deadtime for pointing photons is similar to short burst time of 200ms 2) Short bursts are fainter, need more active area Delayed emission observed, but statistics too low to say much beyond that Summary: GLAST results will quickly re-define HE emission picture

Taxonomy of GRB models Type Progenitor Source of HE γ Emission Model Cannonballs Proton Synch. SNe related Hadronic pp,pn,pγ Long Bursts Not SNe related EM Flux Leptonic shocks Internal External Larger variety of observations of long bursts. Forward Reverse Short bursts Compact Merger Magnetar Diverse Theories Main point of this slide is to show wealth of models

GRB model predictions for GLAST Entire slide stolen from H. Tajima s glast science lunch talk in 2004. Could have taken slide from any of many talks. Point is that w/ Glast w/ get a first quantitative look at important energy band for GRB

GLAST input on key questions Unification schemes ie. viewing angle dependence, standard energy reservoir GLAST good for model testing Bulk Lorentz factor Glast measures cut-off in MeV-GeV spectra Time Variability Glast has Δt resolution down to ~30us Temporal localization of MeV-GeV emission Energy transport Significant number of photons in MeV-GeV range Measure position/ ration of SED peaks Constrains energy fraction ε B ε e High energy power law fits Constrains emitter energy distribution

Long Burst Host Galaxy Associations Long-soft bursts localized to SF galaxies No observed offset from galaxy core Bloom et al., ApJ,2002

First Short Burst Host Associations Prochaska+05 Gorosabel+05, Fox+05, Pedersen+05, Covino+05, Berger+05, Soderberg+06, Levan+06 Swift detection of rapidly decaying afterglow (~300s) of short (40ms) GRB 050509b Allowed host association Gehrels et. al. 2005

Gathering evidence of different progenitors Properties of Short-Hard Burst hosts redshift host classification SFR (Myr -1 ) burst offset [kpc] 050509B 0.225 E < 0.1 39 ± 13 050709 0.160 Irr/late-type dwarf > 0.3 3.5 ± 1.3 050724 0.258 early (E+S0) < 0.05 2.4 ± 0.9 050813 0.722 (1.7?) E? < 0.2 33.2 ± 17.6 Diverse star forming rates. But lower than for long bursts Offset from galaxy centers. Bloom+05, Gorosabel+05; Gehrels+05, Prochaska+05

Missing SNe in LSB GRB 060505 060614 Non-observation of SNe in long bursts to less that 0.01 of standard SN GRB z t 90 notes 060505 0.089 4s faint burst 060614 0.125 102s hard to soft evolution astro-ph/0608313. Fynbo et.al.

But were they really long-soft bursts? 060505 060614 GRB 060614 Canonical 2s is: 1) Bandpass dependent 2) Minimum of N(T 90 ), not 50% probability point Further analysis of SNe missing bursts raises issues w/ classification Short pulse Long flaring New family astro-ph/0610635. Gehrels et.al.

Points about GRB classification w/ GLAST Clear evidence for at least two types of GRB progenitors Duration, spectral index, host galaxy type, afterglow Accurate taxonomy required for obvious reasons Model building/testing work better without outliers to explain Using GRB for cosmology require accurate inputs Low statistics, measurements can be badly pulled by outliers Any information that GLAST can add to taxonomy question is useful Study GLAST specific burst classifications Many GLAST bursts w/ no prompt SWIFT data Provide x-correlation for those bursts which do 25-35% of GBM bursts have significant number of LAT γs What can LAT γs add to GRB classification?

Lessons from Phrenology Be cautious in the interpretation of bumps

Conclusions Recent results have refined (or challenged) existed GRB taxonomy Localization of Short-Hard burst to halo of older, elliptical galaxies favor compact binary merger models over SNe Missing SNe in two recent bursts prompt re-examination of Long/Short burst differentiation GLAST will be have much to add to this discussion GBM covers critical 8 KeV 30 MeV range Measuring peak of prompt spectra past 1MeV Sensitivity in 5MeV 100 GeV range commensurate w/ Swift Constrains emission mechanism model May provide good discrimination between burst types Improved time resolution may add information about HE emission Will need to re-examine GRB classification in light of GLAST data before running off to measure dark energy