English
Related papers

Related papers: Nuclear Matrix Elements for Neutrinoless Double-Be…

200 papers

The observation of neutrinoless double-beta decay (0${\nu}{\beta}{\beta}$) would show that lepton number is violated, reveal that neutrinos are Majorana particles, and provide information on neutrino mass. A discovery-capable experiment…

Instrumentation and Detectors · Physics 2018-06-15 LEGEND Collaboration , N. Abgrall , A. Abramov , N. Abrosimov , I. Abt , M. Agostini , M. Agartioglu , A. Ajjaq , S. I. Alvis , F. T. Avignone , X. Bai , M. Balata , I. Barabanov , A. S. Barabash , P. J. Barton , L. Baudis , L. Bezrukov , T. Bode , A. Bolozdynya , D. Borowicz , A. Boston , H. Boston , S. T. P. Boyd , R. Breier , V. Brudanin , R. Brugnera , M. Busch , M. Buuck , A. Caldwell , T. S. Caldwell , T. Camellato , M. Carpenter , C. Cattadori , J. Cederkäll , Y. -D. Chan , S. Chen , A. Chernogorov , C. D. Christofferson , P. -H. Chu , R. J. Cooper , C. Cuesta , E. V. Demidova , Z. Deng , M. Deniz , J. A. Detwiler , N. Di Marco , A. Domula , Q. Du , Yu. Efremenko , V. Egorov , S. R. Elliott , D. Fields , F. Fischer , A. Galindo-Uribarri , A. Gangapshev , A. Garfagnini , T. Gilliss , M. Giordano , G. K. Giovanetti , M. Gold , P. Golubev , C. Gooch , P. Grabmayr , M. P. Green , J. Gruszko , I. S. Guinn , V. E. Guiseppe , V. Gurentsov , Y. Gurov , K. Gusev , J. Hakenmüeller , L. Harkness-Brennan , Z. R. Harvey , C. R. Haufe , L. Hauertmann , D. Heglund , L. Hehn , A. Heinz , R. Hiller , J. Hinton , R. Hodak , W. Hofmann , S. Howard , M. A. Howe , M. Hult , L. V. Inzhechik , J. Janicskó Csáthy , R. Janssens , M. Ješkovský , J. Jochum , H. T. Johansson , D. Judson , M. Junker , J. Kaizer , K. Kang , V. Kazalov , Y. Kermaïdic , F. Kiessling , A. Kirsch , A. Kish , A. Klimenko , K. T. K. T. Knöpfle , O. Kochetov , S. I. Konovalov , I. Kontul , V. N. Kornoukhov , T. Kraetzschmar , K. Kröninger , A. Kumar , V. V. Kuzminov , K. Lang , M. Laubenstein , A. Lazzaro , Y. L. Li , Y. -Y. Li , H. B. Li , S. T. Lin , M. Lindner , I. Lippi , S. K. Liu , X. Liu , J. Liu , D. Loomba , A. Lubashevskiy , B. Lubsandorzhiev , G. Lutter , H. Ma , B. Majorovits , F. Mamedov , R. D. Martin , R. Massarczyk , J. A. J. Matthews , N. McFadden , D. -M. Mei , H. Mei , S. J. Meijer , D. Mengoni , S. Mertens , W. Miller , M. Miloradovic , R. Mingazheva , M. Misiaszek , P. Moseev , J. Myslik , I. Nemchenok , T. Nilsson , P. Nolan , C. O'Shaughnessy , G. Othman , K. Panas , L. Pandola , L. Papp , K. Pelczar , D. Peterson , W. Pettus , A. W. P. Poon , P. P. Povinec , A. Pullia , X. C. Quintana , D. C. Radford , J. Rager , C. Ransom , F. Recchia , A. L. Reine , S. Riboldi , K. Rielage , S. Rozov , N. W. Rouf , E. Rukhadze , N. Rumyantseva , R. Saakyan , E. Sala , F. Salamida , V. Sandukovsky , G. Savard , S. Schönert , A. -K. Schütz , O. Schulz , M. Schuster , B. Schwingenheuer , O. Selivanenko , B. Sevda , B. Shanks , E. Shevchik , M. Shirchenko , F. Simkovic , L. Singh , V. Singh , M. Skorokhvatov , K. Smolek , A. Smolnikov , A. Sonay , M. Spavorova , I. Stekl , D. Stukov , D. Tedeschi , J. Thompson , T. Van Wechel , R. L. Varner , A. A. Vasenko , S. Vasilyev , A. Veresnikova , K. Vetter , K. von Sturm , K. Vorren , M. Wagner , G. -J. Wang , D. Waters , W. -Z. Wei , T. Wester , B. R. White , C. Wiesinger , J. F. Wilkerson , M. Willers , C. Wiseman , M. Wojcik , H. T. Wong , J. Wyenberg , W. Xu , E. Yakushev , G. Yang , C. -H. Yu , Q. Yue , V. Yumatov , J. Zeman , Z. Zeng , I. Zhitnikov , B. Zhu , D. Zinatulina , A. Zschocke , A. J. Zsigmond , K. Zuber , G. Zuzel

The Bayesian discovery probability of future experiments searching for neutrinoless double-$\beta$ decay is evaluated under the popular assumption that neutrinos are their own antiparticles. A Bayesian global fit is performed to construct a…

High Energy Physics - Experiment · Physics 2017-09-13 Matteo Agostini , Giovanni Benato , Jason A. Detwiler

The discovery of neutrino masses through the observation of oscillations boosted the importance of neutrinoless double beta decay ($0\nu\beta\beta$). In this paper, we review the main features of this process, underlining its key role both…

High Energy Physics - Phenomenology · Physics 2016-04-20 S. Dell'Oro , S. Marcocci , M. Viel , F. Vissani

Neutrinoless double beta decay (NDBD) is the only experiment that could probe the Majorana nature of the neutrino. Here we study the theoretical implications of NDBD for models yielding tri-bimaximal lepton mixing like A4 and S4.

High Energy Physics - Phenomenology · Physics 2010-05-12 S. Morisi

The possibility to observe the neutrino-less double $ \beta $ decay and thus to prove the Majorana nature of neutrino as well as provide a sensitive measure of its mass is a major challenge of to-day's neutrino physics. As an attractive…

High Energy Physics - Phenomenology · Physics 2009-11-10 Z. Sujkowski , S. Wycech

Combined bounds on the Majorana neutrino mass for light and heavy neutrino exchange mechanisms are derived from current neutrinoless double beta decay (0{\nu}\b{eta}\b{eta}) search results for a variety of nuclear matrix element (NME)…

High Energy Physics - Experiment · Physics 2021-07-14 Steven D. Biller

Neutrinoless double-beta decay is a forbidden, lepton-number-violating nuclear transition whose observation would have fundamental implications for neutrino physics, theories beyond the Standard Model and cosmology. In this review, we…

Nuclear Experiment · Physics 2022-10-05 Michelle J. Dolinski , Alan W. P. Poon , Werner Rodejohann

Nuclear matrix elements (NME) are a crucial input for the interpretation of neutrinoless double beta decay data. We consider a representative set of recent NME calculations from different methods and investigate the impact on the present…

High Energy Physics - Phenomenology · Physics 2023-07-05 Federica Pompa , Thomas Schwetz , Jing-Yu Zhu

We consider the seesaw model with two right-handed neutrinos $N_1$ and $N_2$ which masses are hierarchical, and investigate their contribution to the neutrinoless double beta ($0 \nu \beta \beta$) decay. Although the lepton number is broken…

High Energy Physics - Phenomenology · Physics 2021-06-23 Takehiko Asaka , Hiroyuki Ishida , Kazuki Tanaka

When three Majorana neutrinos describe the solar and atmospheric neutrino data via oscillations, a nonzero measurement of neutrinoless double beta ($0\nu\beta\beta$) decay can determine the sum of neutrino masses $\sum m_\nu$ if the solar…

High Energy Physics - Phenomenology · Physics 2009-09-15 V. Barger , K. Whisnant

A natural explanation for the smallness of the neutrino mass requires them to be Majorana particles violating lepton number by two units. Since lepton number violation can have several interesting consequences in particle physics and…

High Energy Physics - Phenomenology · Physics 2007-12-18 Utpal Sarkar

The objective of the Majorana Experiment is to study neutrinoless double beta decay (0nbb) with an effective Majorana-neutrino mass sensitivity below 50 meV in order to characterize the Majorana nature of the neutrino, the Majorana mass…

Nuclear Experiment · Physics 2012-08-27 The Majorana collaboration

Neutrino masses can be generated radiatively. In such scenarios their masses are calculated by evaluating a self-energy diagram with vanishing external momentum, i.e. taking only the leading order term in a momentum expansion. The…

High Energy Physics - Phenomenology · Physics 2020-01-08 Werner Rodejohann , Xun-Jie Xu

The $\nu_M{\rm SM}$ is defined as the SM extended to include dimension-5 operators. In this model neutrino masses violate lepton number, and two parameters of the lepton mixing matrix, the Majorana phases, are yet to be constrained. One…

High Energy Physics - Phenomenology · Physics 2024-10-16 Avital Dery , Stefania Gori , Yuval Grossman , Zoltan Ligeti

If the electron neutrino has an effective nonzero Majorana mass, then neutrinoless double beta decay will occur. However, the latter is possible also with a negligible neutrino mass. We show how this may happen in a simple model of scalar…

High Energy Physics - Phenomenology · Physics 2009-11-07 Biswajoy Brahmachari , Ernest Ma

Neutrinoless double-beta decay (0$\nu\beta\beta$) decay is a hypothetical process that violates lepton number, and whose observation would unambiguously indicate that neutrinos are Majorana fermions. In the standard inverted-ordering…

Nuclear Experiment · Physics 2019-12-10 J. M. López-Castaño , I. Guinn

Nuclear matrix elements (NMEs) for neutrinoless double-beta ($0\nu\beta\beta$) decay in candidate nuclei play a crucial role in interpreting results from current experiments and in designing future ones. Accurate NME values serve as…

Nuclear Theory · Physics 2024-08-08 C. R. Ding , Gang Li , J. M. Yao

We analyze neutrinoless double beta decay ($0\nu\beta\beta$) within the framework of the Standard Model Effective Field Theory. Apart from the dimension-five Weinberg operator, the first contributions appear at dimension seven. We classify…

High Energy Physics - Phenomenology · Physics 2017-12-29 V. Cirigliano , W. Dekens , J. de Vries , M. L. Graesser , E. Mereghetti

The occurrence of the neutrinoless decay 0n-bb mode has fundamental consequences: first total lepton number is not conserved, and second, the neutrino is a Majorana particle. Further the effective mass measured allows to put an absolute…

High Energy Physics - Phenomenology · Physics 2007-05-23 Hans Volker Klapdor-Kleingrothaus

Accurate nuclear matrix elements (NMEs) for neutrinoless double beta decays of candidate nuclei are important for the design and interpretation of future experiments. Significant progress has been made in the modeling of these NMEs from…

Nuclear Theory · Physics 2021-01-12 J. M. Yao