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GZK cutoff distortion due to the energy error distribution shape
Institution:1. Instituto Física, Universidade de São Paulo, SP, Brazil;2. Space Science Laboratory, University of California, Berkeley, CA 94720, United States;3. Lawrence Berkeley National Laboratory, Space Sciences Laboratory and Department of Physics, University of California, Berkeley, CA 94720, United States;1. School of Physics, Peking University, Beijing 100871, China;2. Center for High Energy Physics, Peking University, Beijing 100871, China;3. Collaborative Innovation Center of Quantum Matter, Beijing, China;1. AMME-LECAP EA4528 International Laboratory, Institut des Matériaux de Rouen, Université et INSA de Rouen, BP12, 76801 Saint Etienne du Rouvray Cedex, France;2. Institute for Chemical and Physical Processes, CNR, Largo Pontecorvo 3, 56127 Pisa, Italy;1. Laboratory of Cyto-Molecular Genetics, Department of Anatomy, AIIMS, New Delhi 110029, India;2. National Drug Dependence Treatment Center, Department of Psychiatry, AIIMS, New Delhi 110029, India;1. Graduate Program in Electrical Engineering, Department of Electrical Engineering, Faculty of Engineering, Chiang Mai University, Chiang Mai, Thailand;2. Department of Electrical Engineering, Faculty of Engineering, Chiang Mai University, Chiang Mai, Thailand
Abstract:The development of an ultra high energy air shower has an intrinsic energy fluctuation due both to the first interaction point and to the cascade development. Here we show that for a given primary energy this fluctuation has a lognormal distribution and thus observations will estimate the primary energy with a lognormal error distribution. We analyze the UHECR energy spectrum convolved with the lognormal energy error and demonstrate that the shape of the error distribution will interfere significantly with the ability to observe features in the spectrum. If the standard deviation of the lognormal error distribution is equal or larger than 0.25, both the shape and the normalization of the measured energy spectra will be modified significantly. As a consequence, the GZK cutoff might be sufficiently smeared as not to be seen (without very high statistics). This result is independent of the power law of the cosmological flux. As a conclusion we show that in order to establish the presence or not of the GZK feature, not only more data are needed but also that the shape of the energy error distribution has to be known well. The high energy tail and the sigma of the approximate lognormal distribution of the error in estimating the energy must be at the minimum set by the physics of showers.
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