Searching for beyond the Standard Model physics using the improved description of 100Mo 2νββ\\documentclass[12pt]{minimal} \\usepackage{amsmath} \\usepackage{wasysym} \\usepackage{amsfonts} \\usepackage{amssymb} \\usepackage{amsbsy} \\usepackage{mathrsfs} \\usepackage{upgreek} \\setlength{\\oddsidemargin}{-69pt} \\begin{document}$$2\ u \\beta \\beta $$\\end{document} decay spectral shape with CUPID-Mo

C Augier,A S Barabash,F Bellini,G Benato,M Beretta,L Bergé,J Billard,Yu A Borovlev,L Cardani,N Casali,A Cazes,E Celi,M Chapellier,D Chiesa,I Dafinei,F A Danevich,M De Jesus,T Dixon,L Dumoulin,K Eitel,F Ferri,B K Fujikawa,J Gascon,L Gironi,A Giuliani,V D Grigorieva,M Gros,D L Helis,H Z Huang,R Huang,L Imbert,A Juillard,H Khalife,M Kleifges,V V Kobychev,Yu G Kolomensky,S I Konovalov,J Kotila,P Loaiza,L Ma,E P Makarov,P De Marcillac,R Mariam,L Marini,S Marnieros,X F Navick,C Nones,E B Norman,E Olivieri,J L Ouellet,L Pagnanini,L Pattavina,B Paul,M Pavan,H Peng,G Pessina,S Pirro,D V Poda,O G Polischuk,S Pozzi,E Previtali,Th Redon,A Rojas,S Rozov,V Sanglard,J A Scarpaci,B Schmidt,Y Shen,V N Shlegel,F Šimkovic,V Singh,C Tomei,V I Tretyak,V I Umatov,L Vagneron,M Velázquez,B Ware,B Welliver,L Winslow,M Xue,E Yakushev,M Zarytskyy,A S Zolotarova

doi:10.1140/epjc/s10052-024-13286-4

Abstract

The current experiments searching for neutrinoless double-β\\documentclass[12pt]{minimal} \\usepackage{amsmath} \\usepackage{wasysym} \\usepackage{amsfonts} \\usepackage{amssymb} \\usepackage{amsbsy} \\usepackage{mathrsfs} \\usepackage{upgreek} \\setlength{\\oddsidemargin}{-69pt} \\begin{document}$$\\beta $$\\end{document} (0νββ\\documentclass[12pt]{minimal} \\usepackage{amsmath} \\usepackage{wasysym} \\usepackage{amsfonts} \\usepackage{amssymb} \\usepackage{amsbsy} \\usepackage{mathrsfs} \\usepackage{upgreek} \\setlength{\\oddsidemargin}{-69pt} \\begin{document}$$0\ u \\beta \\beta $$\\end{document}) decay also collect large statistics of Standard Model allowed two-neutrino double-β\\documentclass[12pt]{minimal} \\usepackage{amsmath} \\usepackage{wasysym} \\usepackage{amsfonts} \\usepackage{amssymb} \\usepackage{amsbsy} \\usepackage{mathrsfs} \\usepackage{upgreek} \\setlength{\\oddsidemargin}{-69pt} \\begin{document}$$\\beta $$\\end{document} (2νββ\\documentclass[12pt]{minimal} \\usepackage{amsmath} \\usepackage{wasysym} \\usepackage{amsfonts} \\usepackage{amssymb} \\usepackage{amsbsy} \\usepackage{mathrsfs} \\usepackage{upgreek} \\setlength{\\oddsidemargin}{-69pt} \\begin{document}$$2\ u \\beta \\beta $$\\end{document}) decay events. These can be used to search for Beyond Standard Model (BSM) physics via 2νββ\\documentclass[12pt]{minimal} \\usepackage{amsmath} \\usepackage{wasysym} \\usepackage{amsfonts} \\usepackage{amssymb} \\usepackage{amsbsy} \\usepackage{mathrsfs} \\usepackage{upgreek} \\setlength{\\oddsidemargin}{-69pt} \\begin{document}$$2\ u \\beta \\beta $$\\end{document} decay spectral distortions. 100Mo has a natural advantage due to its relatively short half-life, allowing higher 2νββ\\documentclass[12pt]{minimal} \\usepackage{amsmath} \\usepackage{wasysym} \\usepackage{amsfonts} \\usepackage{amssymb} \\usepackage{amsbsy} \\usepackage{mathrsfs} \\usepackage{upgreek} \\setlength{\\oddsidemargin}{-69pt} \\begin{document}$$2\ u \\beta \\beta $$\\end{document} decay statistics at equal exposures compared to the other isotopes. We demonstrate the potential of the dual read-out bolometric technique exploiting a 100Mo exposure of 1.47 kg ×\\documentclass[12pt]{minimal} \\usepackage{amsmath} \\usepackage{wasysym} \\usepackage{amsfonts} \\usepackage{amssymb} \\usepackage{amsbsy} \\usepackage{mathrsfs} \\usepackage{upgreek} \\setlength{\\oddsidemargin}{-69pt} \\begin{document}$$\ imes $$\\end{document} years, acquired in the CUPID-Mo experiment at the Modane underground laboratory (France). We set limits on 0νββ\\documentclass[12pt]{minimal} \\usepackage{amsmath} \\usepackage{wasysym} \\usepackage{amsfonts} \\usepackage{amssymb} \\usepackage{amsbsy} \\usepackage{mathrsfs} \\usepackage{upgreek} \\setlength{\\oddsidemargin}{-69pt} \\begin{document}$$0\ u \\beta \\beta $$\\end{document} decays with the emission of one or more Majorons, on 2νββ\\documentclass[12pt]{minimal} \\usepackage{amsmath} \\usepackage{wasysym} \\usepackage{amsfonts} \\usepackage{amssymb} \\usepackage{amsbsy} \\usepackage{mathrsfs} \\usepackage{upgreek} \\setlength{\\oddsidemargin}{-69pt} \\begin{document}$$2\ u \\beta \\beta $$\\end{document} decay with Lorentz violation, and 2νββ\\documentclass[12pt]{minimal} \\usepackage{amsmath} \\usepackage{wasysym} \\usepackage{amsfonts} \\usepackage{amssymb} \\usepackage{amsbsy} \\usepackage{mathrsfs} \\usepackage{upgreek} \\setlength{\\oddsidemargin}{-69pt} \\begin{document}$$2\ u \\beta \\beta $$\\end{document} decay with a sterile neutrino emission. In this analysis, we investigate the systematic uncertainty induced by modeling the 2νββ\\documentclass[12pt]{minimal} \\usepackage{amsmath} \\usepackage{wasysym} \\usepackage{amsfonts} \\usepackage{amssymb} \\usepackage{amsbsy} \\usepackage{mathrsfs} \\usepackage{upgreek} \\setlength{\\oddsidemargin}{-69pt} \\begin{document}$$2\ u \\beta \\beta $$\\end{document} decay spectral shape parameterized through an improved model, an effect never considered before. This work motivates searches for BSM processes in the upcoming CUPID experiment, which will collect the largest amount of 2νββ\\documentclass[12pt]{minimal} \\usepackage{amsmath} \\usepackage{wasysym} \\usepackage{amsfonts} \\usepackage{amssymb} \\usepackage{amsbsy} \\usepackage{mathrsfs} \\usepackage{upgreek} \\setlength{\\oddsidemargin}{-69pt} \\begin{document}$$2\ u \\beta \\beta $$\\end{document} decay events among the next-generation experiments.

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