VERITAS Observations of Starburst Galaxies. The Discovery of VHE Gamma Rays from a Starburst Galaxy

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VERITAS Observations of Starburst Galaxies The Discovery of VHE Gamma Rays from a Starburst Galaxy Wystan Benbow for the VERITAS Collaboration 1 Harvard-Smithsonian Center for Astrophysics 1 see R.A. Ong et al. (these proceedings) or http://veritas.sao.arizona.edu/conferences/authors?icrc2009 31 st International Cosmic Ray Conference; July 7-15, 2009; Lodz, Poland

VERITAS: A Cherenkov Telescope Array Arizona: ~32º N, ~111º W, 1268 m a.s.l. Four identical telescopes: Mirror Area: ~106 m2; 350 mirrors 109 m Fall 2006 85 m T3 85 m T4 Camera: 499 pixels (0.15º) & 3.5º FoV f/d ~ 1.0; D = 12 m; f = 12 m 35 m March 2007 Readout: Dual-gain; 500 MHz FADC 3-level trigger: ~10% dead time; ~300 Hz Since January 2006 T2 Moving T1 in Summer 2009 Data: ~750 h / year + 35% in moonlight Metrics: Studies from ~100 GeV to ~30 TeV Detect (5σ) 1% Crab source in <50 h @zenith Angular resolution: r68 < 0.1º Energy resolution: ~15% 8. 1 m Wystan Benbow, VERITAS Discovery of VHE γ-rays from M82, 31st ICRC (Lodz) T1

M 82: A Starburst Galaxy M 82 is the prototype starburst galaxy δ ~ 70º => Culminates at θ ~ 40º D = ~3.9 Mpc towards Ursa Major: EBL a non-issue Diameter ~1ʼ => Point-like for VHE γ-ray studies Central SMBH: <3 x 107 Msun; No evidence of an AGN Johannes Schedler (Panther Observatory) M 82 interacting with group of galaxies Over hundreds of millions of years At least 1 major interaction with larger spiral M 81 Tidal forces => Active starburst region Diameter ~ 1000 light years HST => Contains >200 massive star clusters 104-106 Msun; brighter than most in Local Group NASA, ESA, The Hubble Heritage Team, (STScI / AURA) Wystan Benbow, VERITAS Discovery of VHE γ-rays from M82, 31st ICRC (Lodz)

The Starburst Region of M 82 High star formation rate: ~10x Milky Way High supernova rate: ~0.1 to ~0.3 / year Cosmic-ray (CR) origin? 100-year old question Preferred theory: SNR & wind-zones of massive stars High CR density: ~100x Milky Way Inferred from intense radio-synchrotron emission Chandra High gas density: ~150 particles / cm3 CR hadrons + gas => pions => γ-rays CR electrons + ambient photons => γ-rays >60% of EGRET γ-rays from CR HEGRA & Whipple: VHE flux <10% Crab

VERITAS Discovery of VHE Gamma-rays VERITAS (2007-09): ~137 h live time Only in astronomical darkness; Mean θ ~ 39º Bad weather data removed (via FIR data) Standard VERITAS analysis + hard cuts Eth ~ 700 GeV; NB: Sensitivity less at θ ~ 39º Cuts a priori optimized using Crab at θ ~ 40º For detection of weak, hard-spectrum sources Theoretical expectation for M 82 Standard practice, but 3 trials: std & soft cuts Point-like excess of 91 γ; 5.0σ pre-trials Post-trials significance of 4.8σ Chance probability of 7.7 x 10-7

M 82: A Steady VHE Flux Among weakest-ever VHE sources F(>700 GeV)=(3.7 ± 0.8stat ± 0.7syst) x 10-13 cm -2 s -1 0.9% of Crab Nebula (>700 GeV) Gamma-ray rate: 0.7 / hour No variations in monthly flux χ 2 = 11.5, 9 d.o.f.; P(χ 2 ) = 0.24 Factor of a few variations not ruled out Steady signal accumulation

Systematic Checks All hardware operating normally, no moonlight data & dark NSB region Hard cuts : Enormous images (>200 PE); bright star effects mitigated; very low background (S/N ~ 1/3) Result verified (5.2σ) by independent analysis/calibration/simulation package(s) Alternate background estimation: Ring method => 5.1σ on-source Also ~5σ using a binned maximum-likelihood method Reflected-region BG method always has 11 off-source regions Significance distribution is Gaussian (mean 0, σ = 1) No bias in long data set: Stack extragalactic non-blazar data With the same analysis: Combined excess of -4 events (-0.2σ) in ~121 h of live-time (no moonlight data) Not due to brightness of M 82 (V=9.3) when integrated over its extent => V ~ 8.2 Two V < 9 stars in FOV: Excesses of 1.1σ & 0.8σ at their locations (>0.7º from M 82) Not due to dodgy behavior in a telescope: Signal still present when each tel. is individually excluded

The VHE Gamma-Ray Spectrum Fit Range: 875 GeV to ~5 TeV Model of Persic et al. 2008 Fit to dn/de ~ (E / TeV) -Γ χ 2 = 0.1, 1 NDF; P(χ 2) = 0.7 Γ= 2.5 ± 0.6 VHE flux close to predictions Incl. both leptonic & hadronic channels Pohl 1994 Model of de Cea del Pozo et al. 2009 Völk et al. 1996 Persic et al. 2008 de Cea del Pozo et al. 2009

Some Quick Interpretation Leptons or hadrons? We canʼt say, yet... Hadronic channel: Protons + Matter => Pions => γ-rays; but also => Pions => Secondary Electrons Use radio emission from secondary electrons to limit γ-ray flux from CR hadrons @ 20 GeV Extrapolate VERITAS spectrum downwards: Γ = 2.5 => Flux ~2x higher; Γ = 2.3 => OK Either the true gamma-ray spectrum from 10 GeV to 1 TeV is harder than the VERITAS measurement, or the VHE flux is not predominantly from CR hadrons Leptonic channel: CR electrons + ambient photons => X-rays & γ-rays via IC scattering Use non-thermal X-ray flux => limit number of electrons @ 1 GeV, but need 10 TeV electrons for VHE Theory & comparison to CR-induced X-ray flux to VHE flux => IC spectrum: Γ ~ 2 from 100 kev to 100 GeV Electron energy losses (IC & synchrotron) => Steepening + cut-off in IC spectrum above some energy If Fermi sees a cut-off, the particles responsible for VHE γ-rays could be identified Dark Matter annihilation? In concentrations near the central SMBH, or from formation of an identified IMBH HESS didnʼt see DM-related γ-rays from the GC, or from IMBHʼs in Galactic Plane & M 82 is far more distant!

Conclusions Enormous VERITAS exposure on M 82: ~137 h quality-selected live time over 2 years VERITAS has detected M 82 (91 γ, 4.8σ post-trials, P ~ 7.7 x 10-7 ); The observed flux is steady: F(>700 GeV) = (3.7 ± 0.8stat ± 0.7syst) x 10-13 cm -2 s -1 ; ~0.9% Crab Luminosity is ~2 x 10 32 W; Approximately 0.03% of the optical luminosity The observed photon spectrum has large errors: Γ = 2.5 ± 0.6stat ± 0.2syst 1st VHE γ-ray detection of an object that is not clearly related to an AGN Measurement of CRs outside the galaxy => Help solve 100-yr old mystery of CR origin VHE detection confirms a long standing prediction of the theory of CR acceleration in SNR Detection helps address a number of scientific questions: Role of CRs: in driving large-scale galactic winds; in feedback of star formation on the structure of galaxies Whether smaller shocks (e.g. in SNR) are the predominant CR acceleration sites? or, if CR acceleration occurs on larger scales (>30 ly) in a more distributed fashion?