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Testing effects of Lorentz invariance violation in the propagation of astroparticles with the Pierre Auger Observatory

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arxiv 2112.06773 v2 pith:YZAGN6OI submitted 2021-12-13 astro-ph.HE

The Pierre Auger Collaboration: P. Abreu , M. Aglietta , J.M. Albury , I. Allekotte , K. Almeida Cheminant , A. Almela , J. Alvarez-Muñiz , R. Alves Batista
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G.A. Anastasi L. Anchordoqui B. Andrada S. Andringa C. Aramo P.R. Araújo Ferreira E. Arnone J. C. Arteaga Velázquez H. Asorey P. Assis G. Avila A.M. Badescu A. Bakalova A. Balaceanu F. Barbato J.A. Bellido C. Berat M.E. Bertaina X. Bertou G. Bhatta P.L. Biermann V. Binet K. Bismark T. Bister J. Biteau J. Blazek C. Bleve J. Blümer M. Boháčová D. Boncioli C. Bonifazi L. Bonneau Arbeletche N. Borodai A.M. Botti J. Brack T. Bretz P.G. Brichetto Orchera F.L. Briechle P. Buchholz A. Bueno S. Buitink M. Buscemi M. Büsken K.S. Caballero-Mora L. Caccianiga F. Canfora I. Caracas R. Caruso A. Castellina F. Catalani G. Cataldi L. Cazon M. Cerda J.A. Chinellato J. Chudoba L. Chytka R.W. Clay A.C. Cobos Cerutti R. Colalillo A. Coleman M.R. Coluccia R. Conceição A. Condorelli G. Consolati F. Contreras F. Convenga D. Correia dos Santos C.E. Covault S. Dasso K. Daumiller B.R. Dawson J.A. Day R.M. de Almeida J. de Jesús S.J. de Jong J.R.T. de Mello Neto I. De Mitri J. de Oliveira D. de Oliveira Franco F. de Palma V. de Souza E. De Vito A. Del Popolo M. del Río O. Deligny L. Deval A. di Matteo M. Dobre C. Dobrigkeit J.C. D'Olivo L.M. Domingues Mendes R.C. dos Anjos M.T. Dova J. Ebr R. Engel I. Epicoco M. Erdmann C.O. Escobar A. Etchegoyen H. Falcke J. Farmer G. Farrar A.C. Fauth N. Fazzini F. Feldbusch F. Fenu B. Fick J.M. Figueira A. Filipčič T. Fitoussi T. Fodran T. Fujii A. Fuster C. Galea C. Galelli B. García A.L. Garcia Vegas H. Gemmeke F. Gesualdi A. Gherghel-Lascu P.L. Ghia U. Giaccari M. Giammarchi J. Glombitza F. Gobbi F. Gollan G. Golup M. Gómez Berisso P.F. Gómez Vitale J.P. Gongora J.M. González N. González I. Goos D. Góra A. Gorgi M. Gottowik T.D. Grubb F. Guarino G.P. Guedes E. Guido S. Hahn P. Hamal M.R. Hampel P. Hansen D. Harari V.M. Harvey A. Haungs T. Hebbeker D. Heck G.C. Hill C. Hojvat J.R. Hörandel P. Horvath M. Hrabovský T. Huege A. Insolia P.G. Isar P. Janecek J.A. Johnsen J. Jurysek A. Kääpä K.H. Kampert N. Karastathis B. Keilhauer A. Khakurdikar V.V. Kizakke Covilakam H.O. Klages M. Kleifges J. Kleinfeller F. Knapp N. Kunka B.L. Lago R.G. Lang N. Langner M.A. Leigui de Oliveira V. Lenok A. Letessier-Selvon I. Lhenry-Yvon D. Lo Presti L. Lopes R. López L. Lu Q. Luce J.P. Lundquist A. Machado Payeras G. Mancarella D. Mandat B.C. Manning J. Manshanden P. Mantsch S. Marafico F.M. Mariani A.G. Mariazzi I.C. Mariş G. Marsella D. Martello S. Martinelli O. Martínez Bravo M. Mastrodicasa H.J. Mathes J. Matthews G. Matthiae E. Mayotte S. Mayotte P.O. Mazur G. Medina-Tanco D. Melo A. Menshikov S. Michal M.I. Micheletti L. Miramonti S. Mollerach F. Montanet L. Morejon C. Morello M. Mostafá A.L. Müller M.A. Muller K. Mulrey R. Mussa M. Muzio W.M. Namasaka A. Nasr-Esfahani L. Nellen G. Nicora M. Niculescu-Oglinzanu M. Niechciol D. Nitz D. Nosek V. Novotny L. Nožka A Nucita L.A. Núñez C. Oliveira M. Palatka J. Pallotta P. Papenbreer G. Parente A. Parra J. Pawlowsky M. Pech J. Pękala R. Pelayo J. Peña-Rodriguez E.E. Pereira Martins J. Perez Armand C. Pérez Bertolli M. Perlin L. Perrone S. Petrera C. Petrucci T. Pierog M. Pimenta V. Pirronello M. Platino B. Pont M. Pothast P. Privitera M. Prouza A. Puyleart S. Querchfeld J. Rautenberg D. Ravignani M. Reininghaus J. Ridky F. Riehn M. Risse V. Rizi W. Rodrigues de Carvalho J. Rodriguez Rojo M.J. Roncoroni S. Rossoni M. Roth E. Roulet A.C. Rovero P. Ruehl A. Saftoiu M. Saharan F. Salamida H. Salazar G. Salina J.D. Sanabria Gomez F. Sánchez E.M. Santos E. Santos F. Sarazin R. Sarmento C. Sarmiento-Cano R. Sato P. Savina C.M. Schäfer V. Scherini H. Schieler M. Schimassek M. Schimp F. Schlüter D. Schmidt O. Scholten H. Schoorlemmer P. Schovánek F.G. Schröder J. Schulte T. Schulz S.J. Sciutto M. Scornavacche A. Segreto S. Sehgal R.C. Shellard G. Sigl G. Silli O. Sima R. Smau R. Šmída P. Sommers J.F. Soriano R. Squartini M. Stadelmaier D. Stanca S. Stanič J. Stasielak P. Stassi A. Streich M. Suárez-Durán T. Sudholz T. Suomijärvi A.D. Supanitsky Z. Szadkowski A. Tapia C. Taricco C. Timmermans O. Tkachenko P. Tobiska C.J. Todero Peixoto B. Tomé Z. Torrès A. Travaini P. Travnicek C. Trimarelli M. Tueros R. Ulrich M. Unger L. Vaclavek M. Vacula J.F. Valdés Galicia L. Valore E. Varela A. Vásquez-Ramírez D. Veberič C. Ventura I.D. Vergara Quispe V. Verzi J. Vicha J. Vink S. Vorobiov H. Wahlberg C. Watanabe A.A. Watson A. Weindl L. Wiencke H. Wilczyński D. Wittkowski B. Wundheiler A. Yushkov O. Zapparrata E. Zas D. Zavrtanik M. Zavrtanik L. Zehrer
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classification astro-ph.HE
keywords deltaconstraintscosmicenergyaugercompositionenergiesgamma
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abstract

Lorentz invariance violation (LIV) is often described by dispersion relations of the form $E_i^2=m_i^2+p_i^2+\delta_{i,n} E^{2+n}$ with delta different based on particle type $i$, with energy $E$, momentum $p$ and rest mass $m$. Kinematics and energy thresholds of interactions are modified once the LIV terms become comparable to the squared masses of the particles involved. Thus, the strongest constraints on the LIV coefficients $\delta_{i,n}$ tend to come from the highest energies. At sufficiently high energies, photons produced by cosmic ray interactions as they propagate through the Universe could be subluminal and unattenuated over cosmological distances. Cosmic ray interactions can also be modified and lead to detectable fingerprints in the energy spectrum and mass composition observed on Earth. The data collected at the Pierre Auger Observatory are therefore possibly sensitive to both the electromagnetic and hadronic sectors of LIV. In this article, we explore these two sectors by comparing the energy spectrum and the composition of cosmic rays and the upper limits on the photon flux from the Pierre Auger Observatory with simulations including LIV. Constraints on LIV parameters depend strongly on the mass composition of cosmic rays at the highest energies. For the electromagnetic sector, while no constraints can be obtained in the absence of protons beyond $10^{19}$ eV, we obtain $\delta_{\gamma,0} > -10^{-21}$, $\delta_{\gamma,1} > -10^{-40}$ eV$^{-1}$ and $\delta_{\gamma,2} > -10^{-58}$ eV$^{-2}$ in the case of a subdominant proton component up to $10^{20}$ eV. For the hadronic sector, we study the best description of the data as a function of LIV coefficients and we derive constraints in the hadronic sector such as $\delta_{\mathrm{had},0} < 10^{-19}$, $\delta_{\mathrm{had},1} < 10^{-38}$ eV$^{-1}$ and $\delta_{\mathrm{had},2}< 10^{-57}$ eV$^{-2}$ at 5$\sigma$ CL.

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Cited by 2 Pith papers

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  1. Constraining Lorentz invariance violation from the depth of air-shower maximum

    astro-ph.HE 2026-08 conditional novelty 6.0 of 10

    A simulation-based toy analysis of Auger Xmax data yields M_LIV > 1.5e21 GeV (95% CL) for subluminal photon-sector Lorentz invariance violation, subject to simplified detector and composition assumptions.

  2. Bounds on Lorentz invariance violation from muon fluctuations at the Pierre Auger Observatory

    astro-ph.HE 2026-02 conditional novelty 6.0 of 10

    Muon-count fluctuations in Auger air showers exclude first-order Lorentz invariance violation in the hadronic sector down to η ≈ −1.3×10⁻⁶ at the highest confidence level reported.

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