2007
DOI: 10.1109/tns.2007.895505
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Using RPC Detectors as Cosmic Rays Monitor

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Cited by 5 publications
(7 citation statements)
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“…Among the different detection systems available—emulsions (Tanaka et al 2007b), resistive plate chambers (De Asmundis et al 2007), micromegas (Giomataris et al 2006), scintillators (Pla‐Dalmau et al 2001)—matrices made with scintillator strips are favoured by the teams doing experiments on volcanoes (Uchida et al 2009; Gibert et al 2010). This choice was also guided by the strong experience acquired by several authors of the present paper who participate to the OPERA experiment (Acquafredda et al 2009).…”
Section: An Example Of Muon Telescopementioning
confidence: 99%
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“…Among the different detection systems available—emulsions (Tanaka et al 2007b), resistive plate chambers (De Asmundis et al 2007), micromegas (Giomataris et al 2006), scintillators (Pla‐Dalmau et al 2001)—matrices made with scintillator strips are favoured by the teams doing experiments on volcanoes (Uchida et al 2009; Gibert et al 2010). This choice was also guided by the strong experience acquired by several authors of the present paper who participate to the OPERA experiment (Acquafredda et al 2009).…”
Section: An Example Of Muon Telescopementioning
confidence: 99%
“…Excepted in very particular situations where artificial sources of muons could be used to perform imaging of geological objects (see Nagamine 2003, for a discussion about such a possibility), all experiments performed to date used muons of cosmic origin, belonging to the so-called secondary cosmic rays. The latter are produced high in the atmosphere (typically 15 km) through interactions between primary cosmic rays, coming from outer space (mainly protons-82.4 per cent-and α particles-11.5 per cent when normalized in number of nucleons per GeV per nucleon, see Table 1.1 in Gaisser 1990) and atmospheric molecules (Gaisser 1990;Crozon 2005). When measured at the sea level, charged cosmic rays are mainly (63 per cent) composed of muons with a mean energy E 0 ≈ 4 GeV near the zenith (Gaisser 1990).…”
Section: The Muon Spectrummentioning
confidence: 99%
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“…Different detection techniques are available: emulsions (Tanaka et al, 2007), resistive plate chambers (De Asmundis et al, 2007), micromegas (Giomataris et al, 2006), scintillators (Pla-Dalmau et al, 2001). We retained the scintillator bars option to build the detection matrices since plastic scintillators are known to be robust, light, low-cost detectors particularly well suited to field conditions and actually used for most studies on volcanoes (Tanaka et al, 2005;Marteau et al, 2011).…”
Section: Scintillator Barsmentioning
confidence: 99%
“…Different detection techniques are available: emulsions (Tanaka et al, 2007), resistive plate chambers (De Asmundis et al, 2007), micromegas (Giomataris et al, 2006), scintillators (Pla-Dalmau et al, 2001. We retained the scintillator bars option to build the detection matrices since plastic scintillators are known to be robust, light, low-cost detectors particularly well suited to field conditions and actually used for most studies on volcanoes (Tanaka et al, 2005;Marteau et al, 2011).…”
Section: Scintillator Barsmentioning
confidence: 99%