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Measurement of the cosmic ray hadron spectrum up to 30 TeV at mountain altitude: the primary proton spectrum
The flux of cosmic ray hadrons at the atmospheric depth of 820 g cm −2 has been measured by means of the EAS-TOP hadron calorimeter (Campo Imperatore, National Gran Sasso Laboratories, 2005 m a.s.l.). The hadron spectrum is well described by a single power law: S h (E h )=(2.25±0.21±0.34 sys )×10 −7...
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Published in: | Astroparticle physics 2003-06, Vol.19 (3), p.329-338 |
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Main Authors: | , , , , , , , , , , , , , , , , , , , , , , , , , |
Format: | Article |
Language: | English |
Subjects: | |
Citations: | Items that this one cites Items that cite this one |
Online Access: | Get full text |
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Summary: | The flux of cosmic ray hadrons at the atmospheric depth of 820 g
cm
−2 has been measured by means of the EAS-TOP hadron calorimeter (Campo Imperatore, National Gran Sasso Laboratories, 2005 m a.s.l.).
The hadron spectrum is well described by a single power law:
S
h
(E
h
)=(2.25±0.21±0.34
sys
)×10
−7
E
h
1000
(−2.79±0.05)
m
−2
s
−1
sr
−1
GeV
−1
overthe energy range 30 GeV–30 TeV. The procedure and the accuracy of the measurement are discussed.
The primary proton spectrum is derived from the data by using the CORSIKA/QGSJET code to compute the local hadron flux as a function of the primary proton spectrum and to calculate and subtract the heavy nuclei contribution (basing on direct measurements). Over a wide energy range
E
0=0.5–50 TeV its best fit is given by a single power law:
S(E
0)=(9.8±1.1±1.6
sys
)×10
−5
E
0
1000
(−2.80±0.06)
m
−2
s
−1
sr
−1
GeV
−1
The validity of the CORSIKA/QGSJET code for such application has been checked using the EAS-TOP and KASCADE experimental data by reproducing the ratio of the measured hadron fluxes at the two experimental depths (820 and 1030 g
cm
−2 respectively) at better than 10% in the considered energy range. |
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ISSN: | 0927-6505 1873-2852 |
DOI: | 10.1016/S0927-6505(03)00103-8 |