Results from Observations of AGNs with the H·E·S·S· Telescope System and Future Plans Michael Punch for the H·E·S·S· Collaboration PhysiqueCorpusculaire et Cosmologie, IN2P3/CNRS, Coll`ege deFrance, 11 Place Marcelin Berthelot, F-75231 Paris Cedex 05, France 5 0 0 Abstract. The H·E·S·S· (High Energy Stereoscopic System) Phase-I is comprised of 2 four Imaging Atmospheric Cherenkov Telescopes (IACTs) for observation of galactic n and cosmic sources of Very High Energy (VHE) gamma rays, with a significant im- a provementin sensitivity andadetection threshold below that ofpreviousIACTs. Ob- J servationsofActiveGalacticNuclei(AGNs)sincethestartofoperationsinJune2002 0 are presented, in particular for PKS2155-304 and Mkn421, along plans for Phase-II. 1 1 1 The H·E·S·S· Telescope System v 5 The H·E·S·S· detector for observation of > 100 GeV γ-rays has been operating 5 ◦ ◦ 1 sinceJune,2002intheKhomashighlandsofNamibia(23 S,15 E,1.8kma.s.l.). 1 It captures the Cherenkov light emitted by cascades of particles in the atmo- 0 sphereinitiatedbyaγ-rayorchargedcosmicrayincidentontheatmosphere.The 5 Cherenkov pulses (λ 350nm) are brief (few ns), faint, and illuminate a light- 0 ∼ pool of diameter 250 m on the ground for vertical cascades. The Cherenkov h/ imagesoftheseca∼scades,roughlycometaryinshapewithanangularextentofa p few mrad,canbe seenby a detector anywhereinthe light-poolequipped witha - o sufficiently fast and sensitive camera. This permits the estimation of the nature r of the initiating particle (signal γ-ray or background cosmic-ray) and the mea- t s surementofitsangularoriginandenergy.TheAtmosphericCherenkovtechnique a 2 intrinsically has a large ( 50000m ) collection area, though with a small field : v of view (few degrees). Ob∼servations must take place on clear, moonless nights. i X Thedetector,initsPhase-I,consistsoffourIACTsinasquareofside120m. 2 Each telescope mount has a tessellated mirror of 107m area with a camera in r a the focal plane at 15m. The camera contains 960 photo-multipliers (PMs) with ◦ ◦ 0.16 pixel-size, 5 field of view. The read-out electronics, all contained within thecamera,istriggeredwhenthesignalfromanumberofPMsexceedsatrigger threshold in an effective 1.3 ns trigger window. The PM signals, which are ∼ stored in an analogue memory while awaiting the trigger, are then read out, digitized, and integrated within a 16ns window. The results are then sent from the camera’s data-acquisition system to the control room via optical fibres. SoonafterthesecondtelescopebecameoperationalinJanuary2003,a‘Stereo’ centraltrigger was implemented (June 2003),by which events are only retained ifmultiple telescopesseethe samecascade.This decreasesthe dead-time forthe individual telescopes, allowing the trigger threshold to be decreased (thus de- creasing detector’s energy threshold), while the multiple images of eachcascade 2 Michael Punch for theH·E·S·S· Collaboration provide a increase in the background-rejection capability and the angular and energy resolution of the system. The Phase-IofH·E·S·S·was completedinDecember,2003,with the addition ofthefourthtelescope,sincewhichtimethesystemhasbeenoperatingatitsfull sensitivity.Theenergythresholdofthesystemis 120GeV forsourcescloseto ∼ Zenith after background rejection cuts ( 400 GeV for single-telescope mode) ∼ ◦ ◦ with an angular resolution improved to 0.06 (from 0.1 ) and allowing spectral measurements with an energy resolution of 15%. Observations of the Crab ≃ nebula have confirmed the system’s performance, with a rate of 10.8 γ/minute andadetectionsignificanceof26.6σ/√hr,whichwhenextrapolatedforasources close to Zenith give a 1 Crab-level sensitivity (5σ detection) in only 30 seconds (1% Crab in 25 hrs). See [1,2] for further details. 2 Observations of AGNs with H·E·S·S· SincethefirstoperationoftheH·E·S·S·detector,manygalacticandextragalactic sources have been studied. The observation of AGNs at the highest energies is a probe of the emission mechanisms in the jets of these sources, and studies of the their multi-wavelength spectral energy distributions (SEDs) and correlated variability over wavelength enable emission models (leptonic or hadronic) to be tested. In addition, as these VHE photons interact with the intergalactic Infra- Red(IIR)background(togiveanelectron-positronpair)andarethusabsorbed, they can also serve as a probe of this background (resulting mainly from early star formation) which is difficult to measure by direct means. However, this absorptionlimits the distanceatwhichwecansee AGNsto aredshift0.5atthe H·E·S·S·detectorthresholdenergy.ThelargedetectionareaofH·E·S·S·allowsus to measure spectralandtemporalcharacteristicson hourtimescales (depending on the strength of flares) for the sources seen. Amongtheextra-galactictargets(withobservingtimeuptoSummer,2004in parentheses)are:PKS2155-304(92h),PKS2005-489(52h),M87(32h),NGC253 (34h). Here we present results from two AGNs: PKS2155-304and Mkn421. 2.1 The AGN PKS 2155-304 PKS 2155-304 is the brightest AGN in the Southern Hemisphere, and has been wellstudiedin manyenergybands overthe last20years.Ithas beenpreviously detected at VHE energies [3]. With a redshift of z =0.117 it is one of the most distant VHE blazars, and therefore of interest not only for studies of this class of object, but also for IIR studies. Initial observations were taken over all the installation phase of H·E·S·S· Phase-I from July 2002 to October 2003, with an evolving detector threshold and sensitivity. Clear detections (> 5σ) are seen in each night’s observations, and an overall signal of 44.9σ in 63.1 h of this mixed data, with 1.2 γ/min, ∼ 10-60% Crab level, with variability on time-scales of months, days, and hours. H·E·S·S· AGN Results and FuturePlans 3 Theenergyspectraarecharacterizedbyasteeppowerlawwithatime-averaged photon index of α= 3.31 0.06. − ± Owing to a particularly high level seen by H·E·S·S· in October, 2003, we triggered our RXTE “target of opportunity” proposal on this source, enabling quasi-simultaneousobservationstobetakenbetweenthetwoinstruments.Short- termvariations(<30min)areseeninboththesedatasets,andmulti-wavelength correlations will be published in a forthcoming paper. A H·E·S·S· multi-wavelength campaign with the PCA instrument on board the Rossi X-ray Timing Explorer (RXTE) has been successfully completed in August,2004,withthe fullfour-telescopePhase-Iarray,andthereforefullsensi- tivity,andthesedataareunderanalysis.Thisintensestudyofthissourceshould yield insights into its inner workings. 2.2 The AGN Mkn 421 Mkn421wasthefirstextra-galacticsourcedetectedatVHEenergies[4].Itisthe closestsuchsource(atz =0.03)andsoislittleaffectedbyIIRabsorption.With a declination δ 38◦, it is still accessible to H·E·S·S·, though culminating at a Zenith angle ab∼ove 60◦. Under these conditions, observations with the H·E·S·S· detectorhaveahigherthreshold,butacompensatorylargereffectivearea(asthe light-poolisgeometricallylargerforshowersdevelopingatagreateratmospheric slant distance), and so gives access to the highest energies of the spectrum. In April of this year, a great increase in activity from this source was seen by the all-sky monitor aboard RXTE, reaching an historically-high level of 110mCrab in mid-April. A multi-wavelength campaign was therefore triggered onthis source,including other IACTs, radioandoptical telescopes,andRXTE. TheH·E·S·S·observations,atanaverageZenithangleof62◦,providedavery clear signal in April, with 66σ in 9.71 h of data, yielding 5.1 γ/min, and ∼ an estimated 1-2 Crab level. The flux clearly increases from the January level (6σ in 2.12 h, 0.8 γ/min, 10-50% Crab level), and was also seen by other ∼ IACTs in the Northern hemisphere (Whipple, MAGIC). Shorter-termvariations and correlations with other energy domains are currently under study. 3 Future Plans for expansion to H·E·S·S· Phase-II Plans for Phase-II of the experiment are comprised of a large telescope in the centre of the current Phase-I providinga loweredthreshold and increasedsensi- tivity.Thiswillprovideaccesstoanumberofastrophysicalphenomenæ,suchas thespectralcut-offsinpulsars,microquasars,GRBs,anddarkmatterintheform of WIMPs. As concerns this paper, AGNs can be observedup to redshift of 2-3 with H·E·S·S· Phase-2 (vs. 0.5 with H·E·S·S·), provided that they are sufficiently bright,astheopticaldepthduetoabsorptionintheintergalacticinfra-redback- groundissmalleratlowerenergies.WithdetectionsofalargernumberofAGNs at varying redshifts, the effect of IIR absorption may be disentangled from the intrinsic spectra of the sources. 4 Michael Punch for theH·E·S·S· Collaboration Technical plans for this very-large telescope are well advanced. The mount and dish structure (30m Ø) are well within the capabilities of industry, since much larger radio-telescopeshave been built. The camera,using the same tech- nology as Phase-I, with some improvements in order to decrease the dead-time ◦ ◦ and readout speed, will have 2000 pixels of size 0.05 ( 3 field of view). An ∼ ∼ improved Analogue Memory ASIC (Application-Specific Integrated Circuit) is being prototyped, and the associatedcamera and read-outelectronics are being designed, based on the experience gained with the Phase-I. In operation with the four telescopes of Phase-I, Monte Carlo simulations indicate that, in coincidence mode the ‘4+1’ system would have a detection threshold of 50GeV with fine-grained and photon-rich image in the central ∼ telescope providing improvedbackgroundrejection and angular and energy res- olution.Instand-alonemode,athresholdaslowas15 25GeVmaybeachieved, − though with lower background-rejectioncapability. 4 Conclusions Phase-I of H·E·S·S· has already provided many interesting new results, of which some of those from extra-galactic sources are presented here. Based on the ex- perience gained with H·E·S·S· Phase-I, a Phase-II extension consisting of a very largeCherenkovImaging Telescope is being designed, which will providean un- precedentedly low threshold IACT, while greatly increasing the sensitivity at current energies. H·E·S·S· Phase-I will continue to provide exciting new results in the future, while the Phase-II is being designed and installed. References 1. W.Hofmann et al., Proc. 28th ICRC (Tsukuba) 2811 (2003) 2. P.Vincent et al., Proc. 28th ICRC (Tsukuba) 2887 (2003) 3. P.Chadwick et al., Astrophysical Journal 513, 161 (1999) 4. M. Punch et al., Nature 358, 477 (1992) Fig.1. Photo of the current four-telescope H·E·S·S· Phase-I array, with an artist’s impression of the Phase-II 30m Ø telescope in the centreof thearray superimposed.