The UHECR dipole and quadrupole in the latest data from the original Auger and TA surface detectors

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    • uploaded July 5, 2021

    Discussion timeslot (ZOOM-Meeting): 15. July 2021 - 12:00
    ZOOM-Meeting URL: https://desy.zoom.us/j/92210078166
    ZOOM-Meeting ID: 92210078166
    ZOOM-Meeting Passcode: ICRC2021
    Corresponding Session: https://icrc2021-venue.desy.de/channel/06-CR-Anisotropies-CRI/118
    Live-Stream URL: https://icrc2021-venue.desy.de/livestream/Discussion-03/4

    Abstract:
    The sources of ultra-high-energy cosmic rays are still unknown, but assuming standard physics, they are expected to lie within a few hundred megaparsecs from us. Indeed, over cosmological distances cosmic rays lose energy to interactions with background photons, at a rate depending on their mass number and energy and properties of photonuclear interactions and photon backgrounds. The universe is not homogeneous at such scales, hence the distribution of cosmic-ray arrival directions is expected to reflect the inhomogeneities in the distribution of galaxies, the shorter the energy loss lengths, the stronger the expected anisotropies. Galactic and intergalactic magnetic fields can blur and distort the picture, but the magnitudes of the largest-scale anisotropies, namely the dipole and quadrupole moments, are the most robust to their effects. Measuring them with no bias regardless of any higher-order multipoles is not possible except with full-sky coverage. In this work, we achieve this in three energy ranges (approximately 8–16 EeV, 16–32 EeV, and 32– EeV) by combining surface-detector data collected at the Pierre Auger Observatory and the Telescope Array until 2019, before the completion of the upgrades of the arrays with new scintillation detectors. The results will be presented at the conference.'

    Authors: Peter Tinyakov | For the Telescope Array and Pierre Auger collaborations
    Collaboration: Telescope ArrayAuger

    Indico-ID: 1048
    Proceeding URL: https://pos.sissa.it/395/375

    Tags:
    Presenter:

    Peter Tinyakov


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