Probing the scalar WIMP-pion coupling with the first LUX-ZEPLIN data

Author:

,Aalbers J.,Akerib D. S.,Al Musalhi A. K.,Alder F.,Amarasinghe C. S.,Ames A.,Anderson T. J.,Angelides N.,Araújo H. M.,Armstrong J. E.,Arthurs M.,Baker A.,Balashov S.,Bang J.,Barillier E. E.,Bargemann J. W.,Beattie K.,Benson T.,Bhatti A.,Biekert A.,Biesiadzinski T. P.,Birch H. J.,Bishop E. J.,Blockinger G. M.,Boxer B.ORCID,Brew C. A. J.,Brás P.,Burdin S.,Buuck M.,Carmona-Benitez M. C.,Carter M.,Chawla A.,Chen H.,Cherwinka J. J.,Chin Y. T.,Chott N. I.,Converse M. V.,Cottle A.,Cox G.,Curran D.,Dahl C. E.,David A.,Delgaudio J.,Dey S.,de Viveiros L.,Di Felice L.,Ding C.,Dobson J. E. Y.,Druszkiewicz E.,Eriksen S. R.ORCID,Fan A.,Fearon N. M.,Fieldhouse N.,Fiorucci S.,Flaecher H.,Fraser E. D.,Fruth T. M. A.,Gaitskell R. J.,Geffre A.,Genovesi J.,Ghag C.,Gibbons R.,Gokhale S.,Green J.,van der Grinten M. G. D.,Haiston J. J.,Hall C. R.,Han S.,Hartigan-O’Connor E.,Haselschwardt S. J.,Hernandez M. A.,Hertel S. A.,Heuermann G.,Homenides G. J.,Horn M.,Huang D. Q.,Hunt D.,Jacquet E.,James R. S.,Johnson J.,Kaboth A. C.,Kamaha A. C.,Kannichankandy M.,Khaitan D.,Khazov A.,Khurana I.,Kim Y. D.,Kim J.,Kingston J.,Kirk R.,Kodroff D.,Korley L.,Korolkova E. V.,Kraus H.,Kravitz S.,Kreczko L.,Kudryavtsev V. A.,Leonard D. S.,Lesko K. T.,Levy C.,Lin J.,Lindote A.,Linehan R.,Lippincott W. H.,Lopes M. I.,Lorenzon W.,Lu C.,Luitz S.,Majewski P. A.,Manalaysay A.,Mannino R. L.,Maupin C.,McCarthy M. E.,McDowell G.,McKinsey D. N.,McLaughlin J.,McLaughlin J. B.,McMonigle R.,Miller E. H.,Mizrachi E.,Monte A.,Monzani M. E.,Morales Mendoza J. D.,Morrison E.,Mount B. J.,Murdy M.,Murphy A. St. J.,Naylor A.,Nelson H. N.,Neves F.,Nguyen A.,Nikoleyczik J. A.,Olcina I.,Oliver-Mallory K. C.,Orpwood J.,Palladino K. J.,Palmer J.,Pannifer N. J.,Parveen N.,Patton S. J.,Penning B.,Pereira G.,Perry E.,Pershing T.,Piepke A.,Qie Y.ORCID,Reichenbacher J.,Rhyne C. A.,Riffard Q.,Rischbieter G. R. C.,Riyat H. S.,Rosero R.,Rushton T.,Rynders D.,Santone D.,Sazzad A. B. M. R.,Schnee R. W.,Shaw S.,Shutt T.,Silk J. J.,Silva C.,Sinev G.,Siniscalco J.,Smith R.,Solovov V. N.,Sorensen P.,Soria J.,Stancu I.,Stevens A.,Stifter K.,Suerfu B.,Sumner T. J.,Szydagis M.,Taylor W. C.,Tiedt D. R.,Timalsina M.,Tong Z.,Tovey D. R.,Tranter J.,Trask M.,Tripathi M.,Tronstad D. R.,Vacheret A.,Vaitkus A. C.,Valentino O.,Velan V.,Wang A.,Wang J. J.,Wang Y.,Watson J. R.,Webb R. C.,Weeldreyer L.,Whitis T. J.,Williams M.,Wisniewski W. J.,Wolfs F. L. H.,Woodford S.,Woodward D.,Wright C. J.,Xia Q.,Xiang X.,Xu J.,Yeh M.,Zweig E. A.

Abstract

AbstractWeakly interacting massive particles (WIMPs) may interact with a virtual pion that is exchanged between nucleons. This interaction channel is important to consider in models where the spin-independent isoscalar channel is suppressed. Using data from the first science run of the LUX-ZEPLIN dark matter experiment, containing 60 live days of data in a 5.5 tonne fiducial mass of liquid xenon, we report the results on a search for WIMP-pion interactions. We observe no significant excess and set an upper limit of 1.5 × 10−46 cm2 at a 90% confidence level for a WIMP mass of 33 GeV/c2 for this interaction.

Funder

All are in acknowledgements

Publisher

Springer Science and Business Media LLC

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