Cosmogenic background simulations for neutrinoless double beta decay with the DARWIN observatory at various underground sites

Author:

,Adrover M.,Althueser L.,Andrieu B.,Angelino E.,Angevaare J. R.,Antunovic B.,Aprile E.,Babicz M.,Bajpai D.,Barberio E.,Baudis L.,Bazyk M.,Bell N.,Bellagamba L.,Biondi R.,Biondi Y.,Bismark A.,Boehm C.,Breskin A.,Brookes E. J.,Brown A.,Bruno G.,Budnik R.,Capelli C.,Cardoso J. M. R.,Chauvin A.,Cimental Chavez A. P.,Colijn A. P.,Conrad J.,Cuenca-García J. J.ORCID,D’Andrea V.,Decowski M. P.,Deisting A.,Di Gangi P.,Diglio S.,Doerenkamp M.,Drexlin G.,Eitel K.,Elykov A.,Engel R.,Farrell S.,Ferella A. D.,Ferrari C.,Fischer H.,Flierman M.,Fulgione W.,Gaemers P.,Gaior R.,Galloway M.,Garroum N.,Ghosh S.,Girard F.,Glade-Beucke R.,Glück F.,Grandi L.,Grigat J.,Größle R.,Guan H.,Guida M.,Hammann R.,Hannen V.,Hansmann-Menzemer S.,Hargittai N.,Hasegawa T.,Hils C.,Higuera A.,Hiraoka K.,Hoetzsch L.,Iacovacci M.,Itow Y.,Jakob J.,Jörg F.,Kara M.,Kavrigin P.,Kazama S.,Keller M.,Kilminster B.,Kleifges M.,Kobayashi M.,Kopec A.,von Krosigk B.,Kuger F.,Landsman H.,Lang R. F.,Li I.,Li S.,Liang S.,Lindemann S.,Lindner M.,Lombardi F.,Loizeau J.,Luce T.,Ma Y.,Macolino C.,Mahlstedt J.,Mancuso A.,Marrodán Undagoitia T.,Lopes J. A. M.,Marignetti F.,Martens K.,Masbou J.,Mastroianni S.,Milutinovic S.,Miuchi K.,Miyata R.,Molinario A.,Monteiro C. M. B.,Morå K.,Morteau E.,Mosbacher Y.,Müller J.,Murra M.,Newstead J. L.,Ni K.,Oberlack U. G.,Ostrovskiy I.,Paetsch B.,Pandurovic M.,Pellegrini Q.,Peres R.,Pienaar J.,Pierre M.,Piotter M.,Plante G.,Pollmann T. R.,Principe L.,Qi J.,Qin J.,Rajado Silva M.,Ramírez García D.,Razeto A.,Sakamoto S.,Sanchez L.,Sanchez-Lucas P.,dos Santos J. M. F.,Sartorelli G.,Scaffidi A.,Schulte P.,Schultz-Coulon H.-C.,Schulze Eißing H.,Schumann M.,Scotto Lavina L.,Selvi M.,Semeria F.,Shagin P.,Sharma S.,Shen W.,Silva M.,Simgen H.,Singh R.,Solmaz M.,Stanley O.,Steidl M.,Tan P.-L.,Terliuk A.,Thers D.,Thümmler T.,Tönnies F.,Toschi F.,Trinchero G.,Trotta R.,Tunnell C.,Urquijo P.,Valerius K.,Vecchi S.,Vetter S.,Volta G.,Vorkapic D.,Wang W.,Weerman K. M.,Weinheimer C.,Weiss M.,Wenz D.,Wittweg C.,Wolf J.,Wolf T.,Wu V. H. S.,Wurm M.,Xing Y.,Yamashita M.,Ye J.,Zavattini G.,Zuber K.

Abstract

AbstractXenon dual-phase time projections chambers (TPCs) have proven to be a successful technology in studying physical phenomena that require low-background conditions. With $$40\,\textrm{t}$$ 40 t of liquid xenon (LXe) in the TPC baseline design, DARWIN will have a high sensitivity for the detection of particle dark matter, neutrinoless double beta decay ($$0\upnu \upbeta \upbeta $$ 0 ν β β ), and axion-like particles (ALPs). Although cosmic muons are a source of background that cannot be entirely eliminated, they may be greatly diminished by placing the detector deep underground. In this study, we used Monte Carlo simulations to model the cosmogenic background expected for the DARWIN observatory at four underground laboratories: Laboratori Nazionali del Gran Sasso (LNGS), Sanford Underground Research Facility (SURF), Laboratoire Souterrain de Modane (LSM) and SNOLAB. We present here the results of simulations performed to determine the production rate of $${}^{137}$$ 137 Xe, the most crucial isotope in the search for $$0\upnu \upbeta \upbeta $$ 0 ν β β of $${}^{136}$$ 136 Xe. Additionally, we explore the contribution that other muon-induced spallation products, such as other unstable xenon isotopes and tritium, may have on the cosmogenic background.

Funder

US National Science Foundation

Dutch Science Council

H2020 European Research Council

Horizon 2020 Framework Programme

Ministry of Education, Science and Technological Development of the Republic of Serbia

Deutsche Forschungsgemeinschaft

GRK-2149

PortugueseFCT

Max-Planck-Gesellschaft

H2020 Marie Skłodowska-Curie Actions

Science and Technology Facilities Council

Publisher

Springer Science and Business Media LLC

Subject

Physics and Astronomy (miscellaneous),Engineering (miscellaneous)

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