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Detecting UHE cosmic-rays and neutrinos hitting the Moon

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Presentation on theme: "Detecting UHE cosmic-rays and neutrinos hitting the Moon"— Presentation transcript:

1 Detecting UHE cosmic-rays and neutrinos hitting the Moon
The νMoon project: Detecting UHE cosmic-rays and neutrinos hitting the Moon νMoon Collaboration: J. Bacelar (KVI) R.Braun (ASTRON) G. de Bruyn (ASTRON) H. Falcke (ASTRON) O. Scholten (KVI) B. Stappers (ASTRON) R. Strom (ASTRON)

2 Neutrino detection needs large detector volumes!
Use the moon …

3 Cosmic Ray Westerbork antennas 100 MHz Radio Waves

4 Particle hits Moon (radius=1700 km; area = 6×106 km2):
Interacts: protons within meters, V Askaryan effect -> Coherent Cherenkov emission Shower development -> including LPM effect Transmission through Moon material λr= 15[m] /  [GHz] = 7m (at 2.2 GHz) Transmissivity across Moon surface – vacuum boundary eV eV Moon n= Vacuum Cosmic particle interaction θc ≈ 560 Vacuum Moon n= Spread emitted power density in a gaussian of width Δθc≈λ/ℓ Hadronic component: Δθc= 2.5 (3/) = (at 2.2 GHz) EM component Δθc= 2.5 (3/)( / E)1/3 = θc ≈ 560 θc 2.2 GHz

5 Particle hits Moon (radius=1700 km; area = 6×106 km2):
Interacts: protons within meters, V Askaryan effect -> Coherent Cherenkov emission Shower development -> including LPM effect Transmission through Moon material λr= 15[m] /  [GHz] = 150 m (at 0.1 GHz) Transmissivity across Moon surface – vacuum boundary eV eV Moon n= Vacuum Cosmic particle interaction θc ≈ 560 Spread emitted power density in a gaussian of width Δθc≈λ/ℓ Hadronic component: Δθc= 2.5 (3/) = (at 0.1 GHz) EM component Δθc= 2.5 (3/)( / E)1/3 = 0.50 θc 100 MHz

6 Where can one do this experiment at 150 MHz ?
GMRT in India (30 dishes 45m diameter) Problem: Data acquisition, Ionosphere, Interference,separation between telescopes WSRT Westerbork – available at present (14 dishes 25 m diameter) Use “PUMA II” backend for pulsar observations LOFAR – available in the future Dedicated mode for moon experiment

7 Westerbork (WSRT) Experiment
Basic Properties: 14 x 25 m diameter dishes 12 dishes phased-up 110 hour observation time 40 M samples/sec (PuMa II) Full Polarization information MHz band 8 dual-pol bands of 20 MHz 3×1020 eV would give 15 σ peak (req.) 2 separate 4’ × 6° pencil beams covering 50% of moon Westerbork Synthesis Radio Telescope

8 Westerbork (WSRT) Experiment
4 freq. bands 4 freq. bands Westerbork Synthesis Radio Telescope

9 Schedule Pilot experiment at WSRT, followed by campaign at LOFAR
First: Director’s time at WSRT 2005, 14th June 17:00-19:00 several different daq. Options tried (PuMa I) 2005, 8th July 07:00-09: measurements at 117 and 162 MHz (PuMa I) 2006, 20th Feb :00-06:00 measurement with PuMaII 2006: νMoon approved as Long-Term Project First 110 hrs granted, starting July 15, 2006 A total of 510 hrs requested for subsequent years Currently observed 24 hrs / 12 hrs of useful data

10 Spectrum before & after interference excision
Processing Pipeline Spectrum before & after interference excision 18 TB raw data per 6 hr slot Excision of narrow-band interference De-Dispersion of ionosphere with GPS TEC values Indentification of peaks 100:1 to 180 GB

11 First Data Products: Noise Distribution & Power Spectra
Simulation of data for 15 events within 1 hour data taking Noise is Gaussian down to 10-7 10 s of data

12 Scholten et al. (NuMoon Collab.) 2006, Astropart. Phys., in press
Expected Sensitivity Cosmic Rays Neutrinos TDs GZK ν´s Scholten et al. (NuMoon Collab.) 2006, Astropart. Phys., in press

13 Summary Low-Frequency radio observations are ideal to study super-GZK particles. Westerbork experiment has just begun Data pipeline is working 100 hrs granted, 500 hrs expected in total Search for pulses is next … Very interesting first limit within one year!? LOFAR will improve limits(?) even more


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