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Status of HAGAR B S Acharya (on behalf of HAGAR collaboration)
Tata Institute of fundamental Research (on behalf of HAGAR collaboration) IIA, TIFR, SINP, BARC 5th WAPP , Dec 14-16, 2010
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Advantages of setting up Atmospheric Cherenkov
experiment at high altitude Higher Cherenkov photon density at higher altitude Lower atmospheric attenuation of Cherenkov photons Lower energy threshold at higher altitudes Interesting physics issues: more sources can be observed, cutoffs in spectra of Active Galactic Nuclei, pulsars Overlapping observations with FERMI Phase 1: HAGAR (IIA+TIFR) 7 element WS array (non-imaging); Now operating Phase 2: 21 m Dia MACE (BARC) imaging Tel. Expected in 2011 Phase 3: MACE-II Stereo imaging; 2012+
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Latitude: 32° 46΄ 46˝ N Longitude : 78° 57΄ 51˝ E Altitude : 4300 m
IAO, Hanle N HEGRO, Pachmarhi Latitude: 32° 46΄ 46˝ N Longitude : 78° 57΄ 51˝ E Altitude : 4300 m
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First HAGAR Telescope at Hanle
2005 First HAGAR Telescope at Hanle
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Data acquisition and Telescope control
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All 7 telescopes were commissioned Array is operating
HAGAR All 7 telescopes were commissioned Array is operating Latitude: 32° 46΄ 46˝ N Longitude : 78° 57΄ 51˝ E Altitude : 4300 m 7
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Status of HAGAR HAGAR array was operational in Sept 2008.
After few engineering runs regular observations were started since October 2008 (Shutdown 3 months in , 2 months , aiming for 0 months in onwards) Upgrade/Modifications to various sub-systems of HAGAR were also undertaken in addition to data analysis -These upgrades were partly planned & partly from feed back from data collected. Instrument upgrade Calibrations (NSB monitoring, Relative Time offsets…) Software (DAQ & Telescope control) Data analysis methods/procedure
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Instrument Development
Mechanical – lid for Telescope (IIA) Alignment (vertical position & mirror orientation ) HV control- SY1527LC was bought Trigger system (Version 0 Version 3) Monitoring – Night Sky, Low Voltage Data acquisition system Acqiris Flash ADC parallel system, Data Format, Prog. Disc. ,Delay Gen, Offset measurement Towards Automation for remote operation
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Coming soon - HTL version #3
HAGAR Trigger Logic Custom designed for HAGAR trigger logic Trigger and Chance trigger sections Accepts 7 NIM inputs for trigger and 7 diff ECL inputs for Chance Any N fold or selected combinations jumper options common to both sections supports GATE to QDC,Latch, RTC latch in, TDC start, Vetoed & un vetoed trigger, chance trigger, Clear Veto in signal vetoes the Trigger section Version #1 – April 2009 Version #2 – April 2010 Coming soon - HTL version #3
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8 Channel Programmable Digital Delay Generator
Delays output by programmed delay wrt to leading edge of input -- AD9500 Inputs are NIM type and Maskable Outputs are NIM , (diff ECL or diff LVDS : FRC16) and Maskable Common external input or SW trigger input Common Trigger out Single Channel prototype worked fine. 8 Ch module has problems – interference PCB is being redesigned – added ground layers
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8 Chl Programmable Discriminator Module
The Discriminator threshold is programmable 8 channel analog inputs. Front panel width control Front panel common test point for measure of set Thresholds of 8 channels selected by Thumbwheel CAMAC interface Since July 13,2010 Sharma et al., Jour of Institute of Engg, Jan 2010.
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Calibrations/Monitoring…..
Monitoring – Night Sky, Low Voltage NSB Measurement (with Prog. Disc many measurements possible) 12 Measurements in Novemebr 2010 13 measurements in July 2010 – (1.17+/-0.22 )E8 ph/cm2/s/sr 3 measurements in July (0.82 +/-0.14)E8 ph/cm2/s/sr Hagar PMT- Nov 2008 – (1.91+/-0.05)E8 ph/cm2/s/sr (Refer to Note by BBSingh, Nawang, Phunchok) SKY quality meter – July 2010 Internal note by BBSingh et al. 2010 Low Voltage monitoring system –μcontroller based Internal note by Sandeep kumar et al., 2010
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Software Upgrade Telescope control and orientation
Modified algorithm for Vertical position and near vertical position. New bright star scans overall pointing accuracy ~0.2 deg. Data acquisition system Acqiris Flash ADC ; a parallel DAQ system, Data Format New hardware - for eg. Prog. Disc. Missing events at high trigger rates are understood. For details refer to Note by Kiran Gothe et al Internal note by B K Nagesh et al. 2010
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Centre represents focal point of each mirror and Markers represent observed positions of the star
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DATA (Sept 08 to Sept 2010) source ON (hrs) OFF(hrs) Crab 82.6 73.5
Geminga 59.4 41.4 Mkn 421 74.9 87.8 Mkn 501 48.8 52.5 1ES 51.7 56.9 3C454 13.3 12.1 MGRO 12.6 11.9 LSI (X-ray Binary) 8.3 7.7 PSR007+73 2.4 2.8 M87 2.0 2.7 Dark region (fake source) 79.18 Calibration (Fixed angle) 35.1
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Monte Carlo Simulation of Extensive Air Showers
CORSIKA package used for simulations of extensive air showers initiated by -rays and cosmic ray particles CORSIKA simulates interactions and decays of hadrons, air nuclei, muons, electrons and photons in atmosphere Tracks down all the particles and photons in the shower to observation level Simulates Cherenkov emission caused by relativistic charged particles in shower Simulation of HAGAR array response to Cherenkov light using our own code e+ / e- + / - hadrons
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CORSIKA Inputs : Cosmic rays : within 3 around vertical
Primary type and energy Arrival angle of primary -rays : vertical Cosmic rays : within 3 around vertical Impact parameter : m Altitude of observation level and geomagnetic field Hanle altitude : 4.3 kms Telescope array geometry Wavelength range : nm Wavelength dependent absorptions of Cherenkov photons : atmospheric absorption, mirror reflectivity, photo-tube quantum efficiency : peak 24% at 400 nm Output : Arrival time, direction and position of Cherenkov photons hitting telescopes
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Details of Spectral Shapes Used for Simulations
For -rays : (20 GeV – 5 TeV) J(E) = 3.2 (E TeV) m-2 s-1 TeV-1 For protons : (50 GeV – 5 TeV) J(E) = (E TeV)-2.7 m-2 s-1 sr-1 TeV-1 For particles : (100 GeV – 10TeV) J(E) = (E TeV)-2.7 m-2 s-1 sr-1 TeV-1 For electrons : ( 50 GeV – 5 TeV) J(E) = (E GeV)-3.3 m-2 s-1 sr-1 GeV-1 19
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Simulation of Detector Response
Site and instrument related parameters Night sky background : 2 108 ph cm-2 s-1 sr-1 Field of view : 3 FWHM Phototube response : Gain = 1.5 106 Pulse shape : Gaussian with rise time 2 ns and width 3.3 ns Attenuation of pulse in coaxial cables : 30 m LMR-Ultraflex-400, 55m RG213 Pulse amplification : factor of 10 Discriminator thresholds : ~220 mV for telescope pulses Trigger generation criteria : at least 4 telescope pulses out of 7 crossing threshold 20
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Simulated Sample Vertically incident showers Species
Energy range (GeV) No. of showers No. of triggers Duration (s) -rays 3,40,000 4,080 37,064 protons 23,89,810 ~60 lakhs 2,543 ~6000 266.0 ~660 particles 1,00,000 52.7 electrons 2,697 Inclined showers 15 deg : -rays – 2,00,000 showers protons – 2,00,000 showers 30 deg : -rays – 2,00,000 showers protons – 2,00,000 showers
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Performance Parameters of HAGAR
Trigger condition No. of events Energy threshold (GeV) Rate (/min) Collection area (m2) 3 Tel. 6113 180 9.9 5104 4 Tel. 4080 210 6.6 4104 5 Tel. 2591 240 4.2 3104 6 Tel. 1621 2.6 2104 7 Tel. 961 300 1.6 1104 Performance parameters for inclined showers will be available soon
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Performance Parameters of HAGAR
Trigger rate : Protons 9.6 Hz, including particles and electrons 13.0 Hz Observed trigger rate = 14 Hz Simulations to be repeated for other trigger rates Hz varying PMT gain and NSB Energy Threshold :
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Sensitivity
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Simulations are compared with Data
to validate the Monte Carlo Simulations and decide cuts on data for signal extraction Comparison of trigger rates Comparison of rate-threshold curves: night sky pulse height spectrum TDC : comparison of Space angle distributions QDC : comparison of total ADC charge – to be taken up FADC: comparison – just started
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Arrival Direction Profiles
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The Crab field-of-view of HAGAR
Blue star Mag= 3 3°17'
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Data Analysis Methods Dark regions: PRELIMINARY
Time offsets (TZERO) – trigger dependant Cuts on data based on zenith angle and azimuth ON-Off Normalisation region Normalisation scheme QDC data - Acqiris data – Flash ADC data PRELIMINARY (April-May 2009) Data Analysis Methods 85 % cut
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Preliminary Results Crab nebula :
Estimate of Crab flux from HAGAR is consistent with other experiments
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Some earlier results on Crab
First simultaneous detection of PeV energy burst from the Crab Nebula - B. S. Acharya, M. V. S. Rao, K. Sivaprasad, B. V. Sreekantan & P. R. Vishwanath Here we report the simultaneous detection on 23 February 1989, by experiments in the Kolar Gold Fields A very high energy -ray burst from the Crab pulsar P. N. Bhat, P. V. Ramanamurthy, B. V. Sreekantan & P. R. Vishwanth Tata Institute of Fundamental Research, Homi Bhabha Marg, Bombay , India The Crab pulsar, ..In our recent observations, we identified a 15-min interval on 23 January 1985 during which pulsed TeV -rays were detected at a 5.1 sigma level at the same phase as the radio main pulse.
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HAGAR data on MKN 421 in Feb 2010(Prelimiary)
Mjd Rate/min /- 3.7 /-3.7 /-3.7 Total duration ~550 mins excess number of on source events = Mean gamma rate = /- 1.0 / minute
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HAGAR (preliminary) + others
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FERMI Detected Pulsars
COSB/SAS2:02 CGRO:07 FERMI:54+ 54+ Pulsars 08 are millisecond Pulsars and Old (Char age ~ 106 kyr) All millisecond pulsars have their radio counterparts. Outof 54 Pulsars, 37 are visible for HAGAR telescopes. (Declination angle -35 deg to 80) 24 gamma ray pulsars have been detected by Fermi-LAT in the blind search. 31 Pulsars are young and isolated. 21 Pulsars are with spectral index in the range 0.5 – 1.5 12 Pulsars with E_dot > 100x1034 ergs/sec.
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Crab Pulsar Results Duration=76 hours
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Crab Pulsar Results Duration=76 hours
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Crab Pulsar Results P1+P2 P1+P2 P1 P2
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Geminga Pulsar Results
Duration=49 hours
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Geminga Pulsar Results
P1+P2 P1 P2
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Pair selection along with run selection
More accuracy in data selection Doing space angle analysis after HA selection only Rejection factor known → efficiency of our cuts Not “disturbed” by bad events which are not in the common HA range Easier to compare with simulation BUT: - Hardware threshold different in ON and OFF - How to balance changes in HV → gains of PMTs...?
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Acqiris 8-bit flash ADCs
Tel. 1 Acqiris 8-bit flash ADCs DC271A – 1GHz (since spring 2009) Tel. 2 Tel. 3 Run cb518_280909 DC271A – 1GHz) Tel. 4 Tel. 5 Tel. 6 Tel. 7 Trigger 1000 ns samples - 128 counts ~ (- 8) mV
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Pedestal from 40 first nanoseconds from Flash ADCs
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Conceptual design of the MACE telescope
Conceptual design of the MACE telescope
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Major Atmospheric Cherenkov Experiment (MACE)
Future Prospects Major Atmospheric Cherenkov Experiment (MACE) Second stage of HIGRO collaboration (IIA, BARC, SINP and TIFR) Initially single imaging telescope of dia 21 m cluster of 832 PMTs with pixel resolution of 0.1 (0o.2) covering FOV of 4 4 at the focus lower energy threshold of 20 GeV Sensitivity : 5 Crab in 13 minutes > 200 GeV 43 minutes > 55 GeV located near HAGAR : common events first light expected in 2011 Will be augmented by one more similar element by 2013 to enable stereoscopic operations
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Astrophysical Sciences Division
MACE Simulations Preliminary Results Nilay Bhatt on behalf of Simulation Team : Abhas Mitra Subir Bhattacharyya Nilay Bhatt Astrophysical Sciences Division BARC, Mumbai HIGRO Collaboration Meeting, 01 – 03 December 2010 50 50
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Cosmic Ray SImulation for KASCADE
Important Input parameter: Primary Spectral Index : 1.8 Atmosphere Model US standard (planar) Cerenkov Waveband 240 – 650 nm Observation level 4217 m asl Magnetic Field (Hanle) Bx = T, Bz = T No. of Scatters 10 Gamma Proton Electron Alpha Energies (GeV) 1 – 104 10 – 104 5 – 104 Scatter Rad.(m) 400 500 Viewcone Angle -- 4o 5o # showers ~ 106 Zenith Angles 0o , 20o , 40o , 60o
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Differential Rate & Energy threshold Estimate
19 GeV 4 NNP, 5 p.e. 40 GeV
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Differential Rate & Energy Threshold Estimate
For Protons : For Electrons: For Alpha : 4 NNP, 5 p.e.
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Differential Rate Estimate
( Effect of the single pixel threshold ) 4 NNP, 5 p.e. 54
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Total/Integral Event Rates
5 p.e. Primary Rates (Hz) Gamma 11.86 Electron 37.13 Alpha 137.7 Proton 818.8 Total 1005.5
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Thank you
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