The Tianshan Radio Experiment for Neutrino Detection

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Presentation transcript:

The Tianshan Radio Experiment for Neutrino Detection a Sino-French project for the radio-detection of Extensive Air Showers induced by neutrinos. Olivier Martineau-Huynh, NAOC & CNRS-IN2P3 – Sept.15, 2012, Lijiang – 21CMA workshop

Why neutrino astronomy? g cosmic rays No deflection (≠ cosmic rays) and no attenuation (≠ elm radiation): great probe for astronomy & cosmology Signature for hadronic processes: clean messengers. After elm radiation and cosmic rays, 3rd window on the Universe… Vast perspectives ahead. «X-ray scanner of the Universe» G. Gelmini et al., Scientific American 302, 2010.

Cosmic neutrinos: experimental status Km3 neutrino telescopes: ANTARES-KM3NET (deep sea, France) & AMANDA – IceCube (ice, Antartica). Sensitivity ~ high range of predictions IAU2012: 2 candidates in 2 years of data (bckgd: 0.14) Neutrino astronomy within reach! But will requires larger detection potential. Could radio detection be the solution? ICECUBE

Radio detection of Extensive Air Showers 1- Principles & context

Radio detection of UHE cosmic particles Bgeo  High energy particles generate Extensive Air Showers in the atmosphere. Lorentz force on charged particles in the EAS by the Earth magnetic field (Kahn & Lerche, 1965): electromagnetic emission (geosynchrotron) F = qvBgeo e+ e- Coherent effect detectable radio emission

Radio detection of EAS: experimental status Measurement of EAS direction of origin, energy, nature of primary (LOPES & CODALEMA, 2004-2010) Well adaptated to giant arrays: easiness of deployment, stable (passive detectors), low cost (<10kRMB/unit). Only 2 established setups (LOPES & CODALEMA) <30 antennas: low stat (<1000 showers) Slave-triggered to standards EAS detectors Full understanding of EAS radio signal ? Self-triggering? The TREND prototype phase was initiated in 2008 in order to first adress these issues, with neutrino detection as the long-term perspective.

Radio detection of Extensive Air Showers 2- The TREND prototype phase

The TREND collaboration China: CAS NAOC: Pr. WU XiangPing, DENG JianRong, GU JunHua, Thomas Saugrin (now in Nantes) IHEP: HU HongBo, LIU Zhen’An, … France: CNRS-IN2P3 LPNHE: Olivier Martineau-Huynh SUBATECH: Pascal Lautridou, Olivier Ravel, … LPC: Valentin Niess CC: Fabio Hernandez

Tianshan Radio Experiment Neutrino Experiment @ Ulastai, XinJiang Very clean radio environnement above 20MHz. AM emitters TREND @ Ulastai AM emitters FM emitters Nançay RadioObservatory

North The 21cm array 21CMA infrastructures, equipments and staff fully available for TREND! Very fast deployment & very modest cost for the development phase. 4 km West East DAQ 3 km South

First EAS identification with autonomous radio array TREND prototype N 250 m 2009 : Prototype of 6 log-periodic antennas. Test of EM signal arrival direction econstruction. Test of EAS identification. 100 m Proof of feasability of the TREND concept 2010 : 15 log-periodic antennas + 3 particle detectors. independant trigger & independant analysis of antenna & scintillator data. Hybrid antenna/scintillator coincidences found. First EAS identification with autonomous radio array 800 m (see Ardouin et al., Astropart Phys 34, 2011 <arXiv:1007.4359>) 400 m

The TREND-50 setup ~3 km ~1.5 km² 50 butterfly antennas deployed in summer 2010, making TREND the largest EAS radio-array for EAS detection in the world. Stable operation since March 2011. 240 live days of acquisition (75% of possible time) so far. On average 80% of array up during this period. ~3 km ~1.5 km²

focused ground pattern EAS identification EAS signal: Isolated events, focused ground pattern & plane wavefront Algorithm to select EAS candidates among radio events Time & direction distrib Wave front Ground pattern & amplitude profile Shower axis

EAS identification One TREND EAS radio-candidate Background signal: focused pattern & spherical wavefront (close source) Extended pattern & plane wavefront (distant source) Algorithm to select EAS candidates among radio events Time & direction distrib Wave front Ground pattern & amplitude profile

TREND-50 results (preliminary) 104 live days analyzed. 33 EAS candidates identified with q<65°. Significant North-South assymetry. North |Eew|= |v˄Bgeo |.x Bgeo TREND efficency map to EAS still to be computed, but already experimental skymap distribution compatible with geosynchrotron effect |Eew|= |v˄Bgeo |. x East Bgeo South

To Do Within coming months (weeks): Acquire more data. Extend analysis to larger zenith angles. Complete analysis of remaining 140 days of data. Refine cuts for EAS selection. Increased statistics, down to large zenith angles (80° ?) Perform statistical study of EAS candidates (skymap & evolution with E, lateral profile & evolution with q & E, …) This work will complete the prototype phase of TREND and validate the concept of autonomous detection & identification of EAS with radio antennas.

Neutrino detection with TREND

UHE neutrino detection ~horizontal shower t nt Chalenges: rate of neutrino showers (~ few per year ) background rejection (~few per second)

CODALEA double polar antenna Background rejection Rejection factor has to be >107. Ground pattern/wavefront cuts hardly applicable for horizontal showers. Key parameter could be polarization: E  Bgeo & E  direction of propagation (at 1st order). Prototype setup to be installed at Ulastai: Double polar antennas + vertical scintillators for CR validation CODALEA double polar antenna … available for TREND

Neutrino event rate Giant array required (>>100km²). Size & layout to be determined through end-to-end MC simulation. Already completed: Neutrino interaction in rock, tau energy loss, tau decay and shower generation, antenna response & trigger. Radio signal generation on the way. x En = 1018 eV Averaged over f TREND site topology Flat site Upward going Downward going Mountains correspond to additionnal target: flux doubles vs flat site. Mountains also screen standard CR showers. Mountains = very attractive sites for detection: Increased efficency Better geometry

TREND sensitivity … How large can we go? 1’000 km²? 10’000 km²? What does it cost to build the world most sensitive neutrino telescope? Size of the array is the key parameter (provided backround rejection is OK). … How large can we go? 1’000 km²? 10’000 km²? technical capacity: OK in principle. Installation cost :~ few106 RMBs. Site?

Ulastai 25’000 km² of lowly populated mountains are within reach…