Observation of GRBs at tens of GeV with a full-coverage air shower array at 5000-6000 m elevation Zhaoyang Feng (Speaker), Yiqing Guo, Yi Zhang, Hong Lu, Hongbo Hu Institute of High Energy Physics, CAS, Beijing, China Tianlu Chen Tibet University, Lhasa, China ICRC2011, Beijing, China 1 Gamma-ray bursts: the most violent explosions in the universe Compact Star Merger Massive Star Core Collapse 2 The GRB field Still a relatively young field, many open questions: --Classification(how many physically distinct types?) --Progenitors(massive stars vs. compact stars; others?) --Central engine( black hole, magnetar, quark star?) --Ejecta composition (baryonic vs.magnetic?) --Energy dissipation mechanism (shock vs.magnetic reconnection) --Particle acceleraton & radiaton mechanisms (synchrotron, inverse Compton,quasi-thermal) --Afterglow physics (medium interaction vs. long-term engine activity) Due to their elusive feature, GRBs are still not fully observationally uncovered in all the temporal and spectral regimes Major advance is made whenever a new temporal or spectral window is unveiled ---Bing Zhang 3 Why Study GRBs at Very High Energy (GeV-TeV)? A new temporal window Need to understand acceleration mechanisms , energetics, and therefore constrain the progenitors and jet feeding mechanism Constrain local environment characteristics: Doppler factor, seed populations, photon density, B field, acceleration and cooling timescales, … Understanding progenitor then leads to an understanding of cosmology & stellar evolution required to support progenitor population Extragalactic background light induced absorption (EBL absorption) of high energy photons Potential ultra high energy cosmic ray sources Limits on Lorentz Invariance Violation 4 Gamma-Ray Telescopes Pair Production Telescopes EGRET/Fermi Atmospheric Cherenkov Telescopes HESS/VERITAS/MAGIC Particle Detection Arrays Milagro/HAWC 0.1 - 100 GeV Space-Based (small area) Background free Large Aperture/High Duty Cycle 50 GeV - 100 TeV Large Area Excellent background rejection 100 GeV - 100 TeV Large Area Good background rejection Large Aperture & Duty Cycle Small acceptance: difficult to extend to high energies Small FOV, small duty circle, not fast slew speed Low altitude, High threshold 5 Let’s go to 5000-6000 m altitude, with Lower energy threshold Better energy resolution Better angular resolution Cosmological GAmma rays Observatory (CGAO) Observation of GRBs at tens of GeV 6 Candidate sites( please refer to next talk #1348) • • A site survey team (7 physicists) investigating 7 candidate sites at June 2011. Two excellent sites are found Pumajiangtang Township (~5100m): suitable for HAWC-like detector Sheka(4300-5400m): Weather is good for IACTs YangBaJing Sheka Pumajiangta ng Township 7 HAWC-like CGAO @5100m(Pumajiangtang Township) Preliminary configuration in MC study: Instrumented Area: 150m*150m = 22,500m2 841 PMTs (29x29) Single layer with 4m depth 5.0m spacing Trigger Condition: Nhit > 10 Trigger ~42 kHz 4m 5m Sincerely thank HAWC collaboration for allowing us to use HAWC simulation and reconstruction code 8 Effective Area Very preliminary! 5100m CGAO: ~ 5-6x effective area VS 4100m ~ 100x effective area VS Fermi-LAT @40GeV ~ 1000x effective area VS Fermi-LAT @80GeV 9 Sensitivity as function of spectral index and cutoff Very preliminary! Simulated GRB: T = 1 s Zenith = 20 deg Power law spectrum with energy cutoff 10 Sensitivity with different Z Very preliminary! 11 Another possibility: CGAO (IACTs) at Sheka (4300m-5400m), A new 5@5 project ? Traditional IACTs, Magic, HESS,…, but with very fast slew speed: 5-10o/s? or GAW, Gamma Air Watch – a new generation of IACTs with large field of view? 12 In summary, we proposed a “Cosmological GAmma rays Observatory ” Observation of GRBs at tens of GeV at 50006000 m elevation in Tibet * Nature of GRBs (central engine, radiation mechanisms, et al.) * Ultra high energy cosmic ray sources * Cosmology, EBL absorption * Lorentz Invariance Violation ... Also an excellent telescope for detection and study of gamma ray sources 13 Thank you! 14 Fermi-LAT GRB catalog • • • • • • • PRELIMINARY ~30 GRB have been seen by LAT above 100 MeV; Both long (>2 sec) and short (<2 sec) bursts have been seen; Some bursts are only visible in LAT Low Energy events; Most of the bursts show highenergy emission afterglow and delayed high-energy onset; Constraint: lower limit of bulk Lorentz factor of the colliding shells: ~1000; Some bursts have an extra spectral component (a different mechanism at high energy?); These short, distant and bright flashes can be used as tools to probe basic physics… 15 15 GeV GRBs observation EGRET: detected 4 GeV photos. For GRB940217, 2 photons with energies 3 GeV, and one photon with energy 18 GeV 90 minutes later. Fermi-LAT: detected 32 GRBs in three years’ run, six of which have gamma-rays with energies up to tens of GeV. Ground-based experiments: Tibet ASgamma experiment, ARGO-YBJ ,Milagro,Pierre Auger Observatory, Wipple, MAGIC, HESS, VERITAS without positive result. only the prototype of Milagro (Milagrito) reported a possible detection of signals associated with GRB970417 with 3 confidence level. 16 Limits on Lorentz Invariance Violation Some QG models violate Lorentz invariance: vph(Eph) ≠ c 2 n E ph E ph E ph 1 n E ph 2 2 2 c pph E ph 1 ... , v c 1 ph M QG,1c 2 M QG,2c 2 pph 2 M QG,n c 2 A high-energy photon Eh would arrive after (or possibly before in some models) a low-energy photon El emitted together GRB080916C: highest energy photon (13 GeV) arrived 16.5 s after low-energy photons started arriving (=the GRB trigger) a conservative lower limit: MQG,1 > (1.50±0.20)×1018 GeV/c2 Pulsar GRB (Kaaret 99) (Ellis 06) 15 16 1015 1.8x10 0.9x10 1016 AGN (Biller 98) GRB AGN (Boggs 04) (Albert 08) 4x1016 1017 1.8x1017 0.2x1018 GRB080916C 1018 1.5x1018 Planck mass min MQG (GeV/c2) 1019 1.2x1019 (Jacob & Piran 2008) n = 1,2 for linear and quadratic Lorentz invariance violation, respectively 17 Moderate Angular and energy Resolution Very preliminary! Energy resolution is under studied 18
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