Acoustic And Radio EEV Neurtrino Detection Activities by Rolf Nahnhauer, Sebastian Boser

By Rolf Nahnhauer, Sebastian Boser

The world Workshop in Zeuthen was once the 1st to mix largely the fields of acoustic and radio detection thoughts for high-energetic particle cascades from cosmic neutrino interactions. The articles during this quantity contain the newest learn paintings which used to be offered by means of over 50 audio system from 10 nations. The broad assurance contains: theoretical predictions on fluxes and the prospects of latest recommendations, theoretical and experimental effects on course fabric homes, the basics of interactions and cascade simulation, and present experimental effects and the latest neutrino flux limits. The publication additionally considers destiny plans and experiments for either radio and acoustic equipment with the purpose of giving the reader an up to date review of this speedily constructing box.

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Rev. D 72 (2005) 023001. Z. Fodor, S. D. Katz, A. Ringwald and H. Tu, JCAP 0311 (2003) 015. B. Eberle, A. Ringwald, T. J. Weiler and Y. Y. Y. Wong, DESY 05-165. E. Waxman and J. N. Bahcall, Phys. Rev. D 59 (1999) 023002. M. , J. Phys. G 18 (1992) 423. M. Takeda et al. ], Phys. Rev. Lett. 81 (1998) 1163; Astropart. Phys. jp/AGASA/ 20. D. J. Bird et al. [Fly's Eye Collaboration], Phys. Rev. Lett. 71 3401 (1993); Astrophys. J. 424, 491 (1994); Astrophys. J. 441, 144 (1995). 21. T. Abu-Zayyad et al.

32 59 21 39 36 The error value shows a standard deviation of a distribution in the measured values. The deviation comes mainly from imperfect shape of the cylinder, mechanical setting at the center of the cavity with caps and the moisture at the surface of the samples. The humidity under 50 % is required at the measurement and the preservation of the samples. Long-term storage in the higher humidity increases the radio wave absorption and some samples showed a recovery of the attenuation length keeping low humidity for quite a while.

For semi-rigid Haverhill cable, only attenuation was measured as a function of frequency with a network analyzer. The phase response was ignored due to a short relative length of the cable used. The resulting time-domain response of LPDA-cable system as used in the experiment is shown in Fig. 2. 3. Analysis The voltage recorded by the scope can be expressed as V(t) = EAsk(t) i o hLPDA{t) For LPDA, far-field requirement reduces to d > A/4. e. the cable transfer function expressed in the time domain, and o is a convolution operator.

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