HiSCORE. M. Tluczykont for the HiSCORE Collaboration

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Measurements of Gamma Rays and Charged Cosmic Rays in the Tunka-Valley in Siberia by Innovative New Technologies HRJRG 303 Sky above Tunka valley HiSCORE Detector Taiga Frozen Irkut river Irkut river HiSCORE M. Tluczykont for the HiSCORE Collaboration Fall meeting of the Astronomische Gesellschaft Splinter on Multi-Messenger Astroparticle Physics, 25.09. 28.09. 2012 1 RX J1713 H.E.S.S. gamma-rays

HiSCORE The Hundred*i Square-km Cosmic ORigin Explorer Cosmic-rays: 100 TeV < EC R < 1 EeV Gamma-rays: Eγ > 10 TeV, up to PeV, ultra-high energy regime Particle physics: beyond LHC range Concept: non-imaging air Cherenkov technique Large area: up to few 100 km² Large Field of view: ~ 0.6 sr 2 2011AdSpR..48.1935T, astro-ph/1108.5880 http://wwwiexp.desy.de/groups/astroparticle/score/ http://tunka-hrjrg.desy.de/ http://de.wikipedia.org/wiki/hiscore

Why do we need a large area? Energetic events are rare. 3

Physics motivations 4

ara ys Physics motivations spectroscopy Anisotropies G am m Gamma-ray spectra Highest and morphology acceleration energies Diffuse Gamma-ray Diffuse emission Emission (Galaxy, local supercluster) C os m Cosmic-ray Origin of cosmic Origin of rays cosmic rays Nonstandard Propagation Propagation Cosmic-ray Anisotropy Sub-knee pre-ankle Spectral fine-structure NucleonNucleon interaction Particle acceleration Dark matter Particle physics 5 ic -r ay s

Cosmic rays HiSCORE Adapted from Donato & Medina-Tanco 2008 Spectrum&composition in transition range Galactic / extragalactic origin 6

Cosmic ray origin Adapted from Donato & Medina-Tanco 2008 Gammas from Galactic Cosmic rays: Eγ ~ ECR/10 7

Tevatron sky TeV Cosmic rays Eγ > 100 GeV 8

Pevatron sky TeV Cosmic rays Eγ > 100 TeV? Where are the cosmic ray pevatrons? 9

The Pevatron energy range? 10

Opening the Pevatron range Extend energy range! very large area 11

Opening the Pevatron range Extend energy range! very large area @ 100 TeV: hard hadronic spectra vs. soft leptonic spectra = cosmic ray signature 12

Accessing the pevatron sky: large area The HiSCORE detector 13

The HiSCORE detector How to achieve large effective area? Imaging air Cherenkov telescopes: O(1000) channels / km² Non-imaging air Cherenkov technique: O(100) channels / km² 14 Picture: Serge Brunier

The HiSCORE detector How to achieve large effective area? Imaging air Cherenkov telescopes: O(1000) channels / km² Non-imaging air Cherenkov technique: O(100) channels / km² Air shower Cherenkov light cone 15 Picture: Serge Brunier

The HiSCORE detector Lateral Cherenkov Photon Distribution How to achieve large effective area? Imaging air Cherenkov telescopes: O(1000) channels / km² Non-imaging air Cherenkov technique: O(100) channels / km² Air shower Cherenkov light cone 16 Picture: Serge Brunier

Lateral Cherenkov Photon Distribution 17

Lateral Cherenkov Photon Distribution Want large area Want a few stations In inner light pool ~100 200 m spacing 18

Lateral Cherenkov Photon Distribution Want large area Want a few stations In inner light pool ~100 200 m spacing Low photon density: Need large collector area 0.5 m² per station 19

The HiSCORE detector Picture: Serge Brunier m 150 20

The HiSCORE detector Picture: Serge Brunier m 150 21

The HiSCORE detector >0.5 m² station area: E thr Readout: GHz sampling <1ns time synch. Picture: Serge Brunier m 150 22

Physics potential of HiSCORE (gamma-ray astronomy) 23

Opening the Pevatron range 24

Opening the Pevatron range CTA 25

Opening the Pevatron range 26

Opening the Pevatron range 27

Potential HiSCORE detections H.E.S.S. (Veritas) 28

Tunka site exposure map Tunka site exposure map Field of view: π steradian 29

Tunka site exposure map HiSCORE scan, 1 year H.E.S.S. SCAN First H.E.S.S. Galactic plane scan 30 Tunka site exposure map Field of view: π steradian

HiSCORE current status and plans 31

Tunka valley Hamburg Tunka Cosmic ray experiment 1 km² dense array Energy threshold 1015 ev core position resolution ~ 10 m energy resolution ~ 15% Xmax resolution< 25 g cm-2 32

HRJRG-303 Helmholtz Russia Joint Research Group HRJRG-303 Measurements of Gamma Rays and Cosmic Rays in the Tunka-Valley in Siberia by innovative new technologies Low energy (GeV / TeV / PeV): High energy (PeV - EeV): HRJRG-303: Resolve open questions of cosmic rays With innovative methods Cherenkov Radio Cherenkov light cone HiSCORE 33 TunkaRex

HiSCORE prototype @ Tunka HiSCORE prototype installation @ Tunka Top view: light sensors Tunka-133 detector station 34 First HiSCORE Prototype April 2012

HiSCORE prototype @ Tunka S. Epimakhov HiSCORE prototype 35

Time synchronization WhiteRabbit: PTP over synchronuous ethernet Synergies: CTA & HiSCORE same t-synch. geometry Consistent lab & Tunka field-test results: sub-ns resolution T-synchronization Over 2 km ethernet rms ~0.17ns Stability LabTest 50 hrs R. Wischnewski 36

Plans 2012: further prototype deployments 2013: engineering array (~60 stations) 37 Proof-of principle & optimization Potentially first physics: strong pevatrons ~2015: 10 km² 100 km² Low-energy core (8'' 12'' PMTs) Optimized layout: graded? Possible combination with imaging technique Better overlap with Gamma: CTA C.R.: direct measurements

Summary & outlook HiSCORE goals: Ultra-high energy gamma-ray survey: pevatron search Cosmic ray physics from 100 TeV to 1 EeV Particle physics beyond LHC energy range Prototype activities ongoing @ Tunka (also planned later: PAO) Engineering array (1 km²), HiSCORE-EA: Start 2013 st Potential for 1 physics results 10 km² 100 km² ~2014 Southern site? 38

Recent news article: http://physicsworld.com/cws/article/news/2012/sep/19/huge-cosmic-ray-observatory-set-for-siberia Upcoming publication: Tluczykont et al. 2012, The HiSCORE detector Submitted to Astroparticle physics 39

Opening the Pevatron range 40

Backup slides 41

Tunka site exposure map Det ect or axi st iltin g HiSCORE scan normal mode 42

Tunka site exposure map Det ect or axi st iltin g H.E.S.S. SCAN HiSCORE scan normal mode 43

Simulation & Reconstruction 44

Simulation & reconstruction CORSIKA + IACT *.iact sim_score iact-package Full detector sim *.ascii *.root reco_score 45

Reconstruction HiSCORE event display 500 TeV gamma-ray Simulation 46

Reconstruction Extract PMT signal parameters Preliminary shower core position (cog) Preliminary direction (time plane fit) Improved core position: light distribution function (LDF) fitting Improved direction: arrival time model Fit of signal widths Simulated Cherenkov signal 47

Direction reconstruction >3 stations: model fit adapted from Stamatescu et al. 2008, Parametrization of time-delay dt at detector position 48

Direction reconstruction >3 stations: model fit adapted from Stamatescu et al. 2008, Parametrization of time-delay dt at detector position r: Distance from shower core to detector Shower height in km Slope of atmospheric refractive index Zenith angle 49

Reconstruction 50 Direction: photon arrival time model Energy: Value of LDF @ 220 m Particle type: Shower depth and Signal rise-time

Direction reconstruction 51

Energy reconstruction Particle energy: Q220 = Value of LDF at 220m Q220 52

Energy reconstruction 53 Particle energy: Q220 = Value of LDF at 220m

Shower depth reconstruction Time model method: one free parameter in arrival time model LDF method: Depth from LDF slope, Q50/Q220 Width method: Depth from signal width 54

Shower depth 55 Depth of shower maximum

Shower depth bias Systematic bias LDF & widths : sensitive to whole shower Large overestimation for heavy particles (long tails) Timing : sensitive to specific point (edge time) Small overestimation for heavy particles 56

Particle separation 57

Particle separation (1) Lighter particles develop Higher up in atmosphere 58

Particle separation (2) Systematic difference Between width and timing Depths 59

Particle separation (3) Systematic difference Cherenkov signal rise times 60

Layout studies Different altitudes Different PMT sizes Combination with other techniques (scintillator, imaging) 61

HRJRG-303 Helmholtz Russia Joint Research Group Measurements of Gamma Rays and Charged Cosmic Rays in the Tunka-Valley in Siberia by Innovative New Technologies 04/2012 04/2015 G. Rubtsov, I. Tkatchev (INR) A. Konstantinov, L. Kuzmichev (MSU) R. Vasilyev, N. Budnev (ISU) R. Wischnewski, C. Spiering (DESY) F. Schröder, A. Haungs (KIT) M. Tluczykont, D. Horns (U. Hamburg) 62 HiSCORE and Radio detectors @ Tunka Innovation Proof-of-principle Synergies

References [HS1] [HS2] [HS3] [HS4] [HS5] [HS6] M. Tluczykont, D. Hampf, D. Horns, et al. (2011), Adv. Sp. Res. 48, 1935 D. Hampf (2012), PhD thesis, University of Hamburg M. Tluczykont, T. Kneiske, D. Hampf & D. Horns (2009), Proc. of the ICRC 2009, arxiv e-print (arxiv:0909.0445v1) D. Hampf, M. Tluczykont & D. Horns (2009), Proc. of the ICRC 2009, arxiv e-print (arxiv:0909.0663v1) M. Tluczykont, D. Hampf, D. Horns, et al., HiSCORE, in prep. D. Hampf, M. Tluczykont, D. Horns, HiSCORE reco, in prep. [Tunka133] Berezhnev S F, Besson D, Korobchenko A V et al. 2012 The Tunka-133 EAS Cherenkov light array: status of 2011 NIM A DOI : 10.1016/j.nima.2011.12.091 Preprint astro-ph.he/1201.2122 [Hec1998] [Ber2008] [Hen1994] [Hör2003] [Abd2007] 63 D. Heck, J. Knapp, J.N. Capdevielle, G. Schatz, and T. Thouw, Report FZKA 6019 (1998), http://www-ik.fzk.de/~heck/publications K. Bernlöhr (2008), astrop-ph preprint, arxiv:0808.2253 V. Henke (1994), Diploma thesis, University of Hamburg J.R. Hörandel, Astropart. Phys., 19, 193 (2003) Abdo A A, Allen B, Berley D et al. 2007 Astrophys. J. 658 L33 L36