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The Majorana experiment: an ultra-low background search for neutrinoless double-beta decay

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arxiv 1111.5578 v1 pith:UM4PRYN4 submitted 2011-11-23 nucl-ex physics.ins-det

D. G. Phillips II , E. Aguayo , F. T. Avignone III , H. O. Back , A. S. Barabash , M. Bergevin , F. E. Bertrand , M. Boswell
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V. Brudanin M. Busch Y.-D.Chan C. D. Christofferson J. I. Collar D. C. Combs R. J. Cooper J. A. Detwiler P. J. Doe Y. Efremenko V. Egorov H. Ejiri S. R. Elliott J. Esterline J. E. Fast N. Fields P. Finnerty F. M. Fraenkle V. M. Gehman G. K. Giovanetti M. P. Green V. E. Guiseppe K. Gusey A. L. Hallin R. Hazama R. Henning A. Hime E. W. Hoppe M. Horton S. Howard M. A. Howe R. A. Johnson K. J. Keeter C. Keller M. F. Kidd A. Knecht O. Kochetov S. I. Konovalov R. T. Kouzes B. LaFerriere B. H. LaRoque J. Leon L. E. Leviner J. C. Loach S. MacMullin M. G. Marino R. D. Martin D.-M. Mei J. Merriman M. L. Miller L. Mizouni M. Nomachi J. L. Orrell N. R. Overman A. W. P. Poon G. Perumpilly G. Prior D. C. Radford K. Rielage R. G. H. Robertson M. C. Ronquest A. G. Schubert T. Shima M. Shirchenko K. J. Snavely D. Steele J. Strain K. Thomas V. Timkin W. Tornow I. Vanyushin R. L. Varner K. Vetter K. Vorren J. F. Wilkerson B. A. Wolfe E. Yakushev A. R. Young C.-H. Yu V. Yumatov C. Zhang
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classification nucl-exphysics.ins-det
keywords backgrounddecaydouble-betaexperimentmajorananeutrinolessdemonstratorneutrino
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The observation of neutrinoless double-beta decay would resolve the Majorana nature of the neutrino and could provide information on the absolute scale of the neutrino mass. The initial phase of the Majorana experiment, known as the Demonstrator, will house 40 kg of Ge in an ultra-low background shielded environment at the 4850' level of the Sanford Underground Laboratory in Lead, SD. The objective of the Demonstrator is to determine whether a future 1-tonne experiment can achieve a background goal of one count per tonne-year in a narrow region of interest around the 76Ge neutrinoless double-beta decay peak.

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    In asymptotically safe gravity, the Weinberg operator is shown to be irrelevant, so Standard Model neutrinos cannot get masses without new fields; type-I seesaw scales are bounded from above.

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