The IceCube Neutrino Telescope Project overview and Status EHE Physics Example: Detection of GZK neutrinos TAUP2003 Shigeru Yoshida, Chiba University.

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Presentation transcript:

The IceCube Neutrino Telescope Project overview and Status EHE Physics Example: Detection of GZK neutrinos TAUP2003 Shigeru Yoshida, Chiba University

The IceCube collaboration Chiba University, Chiba, Japan Clark Atlanta University, Atlanta, GA DESY-Zeuthen, Zeuthen, Germany Imperial College, UK Institute for Advanced Study, Princeton, NJ Lawrence Berkeley National Laboratory, Berkeley, CA Pennsylvania State University, Philadelphia, PA South Pole Station, Antarctica Southern University and A & M College, Baton Rouge, LA Stockholm Universitet, Stockholm, Sweden Universit ä t, Mainz, Germany Universit ä t Wuppertal, Wuppertal, Germany Universit é Libre de Bruxeelles, Bruxelles, Belgium Universit é de Mons-Hainaut, Mons, Belgium University of Alabama, Tuscaloosa, AL University of California-Barkeley, Berkeley, CA University of Delaware, Newark, DE University of Kansas, Lawrence, KS University of Maryland, College Park, MD University of Wisconsin-Madison, Madison, WI University of Wisconsi-RiverFalls, River Falls, WI Universidad Simon Bolivar, Caracas, Venezuela Uppsala Universitet, Uppsala, Sweden Vriie Universiteit Brussel, Brussels, Belgium

South Pole Dark sector AMANDA IceCube Dome Skiway

IceCube 1400 m 2400 m AMANDA South Pole IceTop Skiway 80 Strings 4800 PMT Instrumented volume: 1 km3 (1 Gt) IceCube is designed to detect neutrinos of all flavors at energies from 10 7 eV (SN) to eV

E µ =10 TeV ≈ 90 hitsE µ =6 PeV ≈ 1000 hits How our events look like The typical light cylinder generated by a muon of 100 GeV is 20 m, 1PeV 400 m, 1EeV it is about 600 to 700 m.

DAQ design: Digital Optical Module - PMT pulses are digitized in the Ice Design parameters: Time resolution:≤ 5 nsec (system level) Dynamic range: 200 photoelectrons/15 nsec (Integrated dynamic range: > 2000 photoelectrons) (1.p.e. /10ns ~  10^7G ~8mV 50  4V saturation  500p.e. Digitization depth: 4 µsec. Noise rate in situ: ≤500 Hz Tube trig.rate by muons 20Hz 33 cm DOM

Capture Waveform information (MC) ATWD 300MHz 14 bits. 3 different gains (x15 x3 x0.5) Capture inter. 426nsec 10 bits FADC for long duration pulse. E=10 PeV µsec Events / 10 nsec String 1 String 2 String 3 String 4 String 5 

Photomultiplier: Hamamatsu R (10 ”, 10-stage, 1E+08 gain) Selection criteria -40 °C) Noise < 300 Hz (SN, bandwidth) Gain > 5E7 at 2kV (nom. 1E7 + margin) P/V > 2.0 (Charge res.; in- situ gain calibration) Notes: Only Hamamatsu PMT meets excellent low noise rates! Tested three flavors of R7081.

Digital Optical Module (DOM) Main Board Test Card

SPE Discriminator Scan – PMT Pulses Input (71DB)

The big reel for the hotwater drill

Energy Spectrum Diffuse Search Blue: after downgoing muon rejection Red: after cut on N hit to improve sensitivity EdN/dE=10 -7 GeV/cm 2 sec sr Emax 10 8 GeV

cos  A eff / km 2 Effective area vs. zenith angle after rejection of background from downgoing atmospheric muons Effective area of IceCube Note: Should be further improved by utilizing waveform information

Coincident events Energy range: ~3 x eV Two functions veto and calibration cosmic-ray physics few to thousands of muons per event Measure: Shower size at surface High energy muon component in ice Large solid angle One IceTop station per hole ~ 0.5 sr for C-R physics with “contained” trajectories Larger aperture as veto IceTop

E 2 dN /dE ~10 -8 GeV/cm 2 s sr (diffuse) E 2 dN /dE ~7x10 -9 GeV/cm 2 s (Point source) 200 bursts in coincidence (GRBs – WB flux) In three years operation … TAUP 2003 For 5  detection

Construction: 11/ /2009 AMANDA SPASE-2 South Pole Dome Skiway 100 m Grid North Next season: Buildup of the Drill and IceTop prototypes Co-operation of AMANDA-IceCube From the 1 st year

Project status Startup phase has been approved by the U.S. NSB and funds have been allocated. 100 DOMs are produced and being tested this year. Assembling of the drill/IceTop prototypes is carried out at the pole this season. Full Construction start in 04/05; takes 6 years to complete. Then 16 strings per season, increased rate may be possible. TAUP 2003

GZK EHE detection What is the GZK mechanism? EHE  Propagation in the Earth Expected intensities at the IceCube depth Atmospheric  – background Event rate TAUP 2003

GZK Neutrino Production K 411 photons / cm x cm 2 γ p n p π + μ + ν e + ν γ E = eV E 0.8 x eV ~ Conventional Mechanism of EHE neutrinos!!

TAUP 2003 Yoshida and Teshima 1993 Yoshida, Dai, Jui, Sommers 1997 Note: The oscillations convert e,  to e, , 

e e      e/     Weak Incoming Products Weak Cascades Decay Weak Pair/decay Bremss Pair PhotoNucl. Decay Pair Pair Bremss Decay Weak Decay

TAUP 2003 Tau(Neutrinos) from    Suppression By  decay Muon(Neutrinos) from   Nadir Angle

1.4 km 1km Upward Ice Rock ν ± π γ ν + e - e 1km Downward ν γ γ + e - e lepton

TAUP 2003 Upward-goingDownward going!! Atmospheric muon! – a major backgrond But so steep spectrum

TAUP 2003 Down-going events dominate… 1400 m 2800 m 11000m UpDown Atmospheric  is strongly attenuated…

Flux as a function of energy deposit in km 3 dE/dX~  E  E~  XbE

TAUP 2003 Intensity of EHE  and  GZK m=4 Z max =4 I  (E>10PeV)I  (E>10PeV) RATE [/yr/ km 2 ] Down Up I  (E>10PeV) Energy Deposit I  (E>10PeV) Energy Deposit Down m=7 Z max =5 Down Atm  [cm -2 sec -1 ]

TAUP 2003 Conclusion  appeared in 10 PeV- EeV are our prime target on GZK detection. 1/100-1/500 of primary  intensity! Downward  and  make main contributions in PeV -EeV Energy Estimation would be a key for the bg reduction Because atmospheric  spectrum ~ E -3.7 GZK is DETECTABLE by IceCube events/year (BG 0.05 events/year) IceCube has great capability for TeV-PeV -induced muons taking advantage of long range in the clear ice. For EHE like the GZK….

Backup slides

Theoretical bounds and future atmospheric  W&B MPR DUMAND test string FREJUS NT-200 MACRO  NT-200+ AMANDA-II IceCube AMANDA-97 AMANDA-00 opaque for neutrons Mannheim, Protheroe and Rachen (2000) – Waxman, Bahcall (1999)  derived from known limits on extragalactic protons +  -ray flux neutrons can escape

UHE (EeV or even higher) Neutrino Events Arriving Extremely Horizontally Needs Detailed Estimation Limited Solid Angle Window (  N A ) -1 ~ 600 (  / cm 2 ) -1 (  /2.6g cm -3 ) -1 [km] Involving the interactions generating electromagnetic/hadron cascades NN  X e + e - TAUP 2003

 /  propagation in Earth

1.4 km 1km Upward Ice Rock ν ± π γ ν + e - e 1km lepton ν

N