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Related papers: Neutron beta-decay, Standard Model and cosmology

200 papers

For r-process nucleosynthesis the beta decay rates of very neutron-rich nuclei are important ingredients. We consider the region around the neutron number N=82 and calculate the half-lives and rates for a number of nuclei. Forms for beta…

Astrophysics · Physics 2008-12-01 Kamales Kar , Soumya Chakravarti

At present, the strongest upper limit on $\sum m_{\nu}$, the sum of neutrino masses, is from cosmological measurements. However, this bound assumes that the neutrinos are stable on cosmological timescales, and is not valid if the neutrino…

High Energy Physics - Phenomenology · Physics 2020-05-04 Zackaria Chacko , Abhish Dev , Peizhi Du , Vivian Poulin , Yuhsin Tsai

Precision measurements in neutron beta decay serve to determine the coupling constants of beta decay and allow for several stringent tests of the standard model. This paper discusses the design and the expected performance of the Nab…

We review the current status of precision measurements in allowed nuclear beta decay, including neutron decay, with emphasis on their potential to look for new physics beyond the standard electroweak model. The experimental results are…

Nuclear Experiment · Physics 2008-11-26 N. Severijns , M. Beck , O. Naviliat-Cuncic

A new tension is emerging between the tight cosmological upper bounds on the total neutrino mass ($\sum m_\nu \lesssim 0.06 \, \rm{eV}$) and the lower limits from oscillation experiments, with potentially far-reaching implications for…

Cosmology and Nongalactic Astrophysics · Physics 2026-01-09 Guillermo Franco Abellán

The standard cosmological model predicts the existence of a cosmic neutrino background with a present density of about 110 cm^{-3} per flavour, which affects big-bang nucleosynthesis, cosmic microwave background anisotropies, and the…

Astrophysics · Physics 2009-11-11 P. D. Serpico

A search for neutron-antineutron ($n-\bar{n}$) oscillation was undertaken in Super-Kamiokande using the 1489 live-day or $2.45 \times 10^{34}$ neutron-year exposure data. This process violates both baryon and baryon minus lepton numbers by…

High Energy Physics - Experiment · Physics 2015-04-16 Kamiokande collaboration , K. Abe , Y. Hayato , T. Iida , K. Ishihara , J. Kameda , Y. Koshio , A. Minamino , C. Mitsuda , M. Miura , S. Moriyama , M. Nakahata , Y. Obayashi , H. Ogawa , H. Sekiya , M. Shiozawa , Y. Suzuki , A. Takeda , Y. Takeuchi , K. Ueshima , H. Watanabe , I. Higuchi , C. Ishihara , M. Ishitsuka , T. Kajita , K. Kaneyuki , G. Mitsuka , S. Nakayama , H. Nishino , K. Okumura , C. Saji , Y. Takenaga , S. Clark , S. Desai , F. Dufour , A. Herfurth , E. Kearns , S. Likhoded , M. Litos , J. L. Raaf , J. L. Stone , L. R. Sulak , W. Wang , M. Goldhaber , D. Casper , J. P. Cravens , J. Dunmore , J. Griskevich , W. R. Kropp , D. W. Liu , S. Mine , C. Regis , M. B. Smy , H. W. Sobel , M. R. Vagins , K. S. Ganezer , B. Hartfiel , J. Hill , W. E. Keig , J. S. Jang , I. S. Jeoung , J. Y. Kim , I. T. Lim , K. Scholberg , N. Tanimoto , C. W. Walter , R. Wendell , R. W. Ellsworth , S. Tasaka , G. Guillian , J. G. Learned , S. Matsuno , M. D. Messier , A. K. Ichikawa , T. Ishida , T. Ishii , T. Iwashita , T. Kobayashi , T. Nakadaira , K. Nakamura , K. Nishikawa , K. Nitta , Y. Oyama , A. T. Suzuki , M. Hasegawa , H. Maesaka , T. Nakaya , T. Sasaki , H. Sato , H. Tanaka , S. Yamamoto , M. Yokoyama , T. J. Haines , S. Dazeley , S. Hatakeyama , R. Svoboda , G. W. Sullivan , R. Gran , A. Habig , Y. Fukuda , Y. Itow , T. Koike , C. K. Jung , T. Kato , K. Kobayashi , C. McGrew , A. Sarrat , R. Terri , C. Yanagisawa , N. Tamura , M. Ikeda , M. Sakuda , Y. Kuno , M. Yoshida , S. B. Kim , B. S. Yang , T. Ishizuka , H. Okazawa , Y. Choi , H. K. Seo , Y. Gando , T. Hasegawa , K. Inoue , H. Ishii , K. Nishijima , H. Ishino , Y. Watanabe , M. Koshiba , Y. Totsuka , S. Chen , Z. Deng , Y. Liu , D. Kielczewska , H. G. Berns , K. K. Shiraishi , E. Thrane , K. Washburn , R. J. Wilkes

We analyze the influence of decaying sterile neutrinos with the masses in the range 1-140 MeV on the primordial Helium-4 abundance, explicitly solving the Boltzmann equations for all particle species, taking into account neutrino flavour…

High Energy Physics - Phenomenology · Physics 2012-10-11 Oleg Ruchayskiy , Artem Ivashko

Neutrinoless double beta decay is a sensitive probe of the patterns of neutrino masses and mixings if the neutrinos are Majorana particles as well as other new physics scenarios beyond the standard model. In this talk, the present…

High Energy Physics - Phenomenology · Physics 2009-10-31 R. N. Mohapatra

We explore the cosmological signals of theories in which the neutrinos decay into invisible dark radiation after becoming non-relativistic. We show that in this scenario, near-future large scale structure measurements from the Euclid…

Cosmology and Nongalactic Astrophysics · Physics 2021-02-17 Zackaria Chacko , Abhish Dev , Peizhi Du , Vivian Poulin , Yuhsin Tsai

It is possible that the proton is stable while atomic hydrogen is not. This is the case in models with new particles carrying baryon number which are light enough to be stable themselves but heavy enough so that proton decay is…

High Energy Physics - Phenomenology · Physics 2020-03-06 David McKeen , Maxim Pospelov

Using the time-of-flight technique, we measured the beta-delayed neutron emission of $^{132}$Cd. From our large-scale shell model (LSSM) calculation using the N$^3$LO interaction [Z.Y. Xu et al., Phys. Rev. Lett. 131, 022501 (2023)], we…

The existing calculations of the nuclear matrix elements of the neutrinoless double $\beta$-decay differ by about a factor three. This uncertainty prevents quantitative interpretation of the results of experiments searching for this…

High Energy Physics - Phenomenology · Physics 2008-11-26 S. M. Bilenky , J. A. Grifols

Yes, the photon. While a nonzero photon mass has been under experimental and theoretical study for years, the possible implication of a finite photon lifetime lacks discussion. The tight experimental upper bound of the photon mass restricts…

High Energy Physics - Phenomenology · Physics 2013-07-12 Julian Heeck

Tests on $B-L$ symmetry breaking models are important probes to search for new physics. One proposed model with $\Delta(B-L)=2$ involves the oscillations of a neutron to an antineutron. In this paper a new limit on this process is derived…

High Energy Physics - Experiment · Physics 2017-11-29 SNO Collaboration , B. Aharmim , S. N. Ahmed , A. E. Anthony , N. Barros , E. W. Beier , A. Bellerive , B. Beltran , M. Bergevin , S. D. Biller , K. Boudjemline , M. G. Boulay , B. Cai , Y. D. Chan , D. Chauhan , M. Chen , B. T. Cleveland , G. A. Cox , X. Dai , H. Deng , J. A. Detwiler , P. J. Doe , G. Doucas , P. -L. Drouin , F. A. Duncan , M. Dunford , E. D. Earle , S. R. Elliott , H. C. Evans , G. T. Ewan , J. Farine , H. Fergani , F. Fleurot , R. J. Ford , J. A. Formaggio , N. Gagnon , J. TM. Goon , K. Graham , E. Guillian , S. Habib , R. L. Hahn , A. L. Hallin , E. D. Hallman , P. J. Harvey , R. Hazama , W. J. Heintzelman , J. Heise , R. L. Helmer , A. Hime , C. Howard , M. Huang , P. Jagam , B. Jamieson , N. A. Jelley , M. Jerkins , K. J. Keeter , J. R. Klein , L. L. Kormos , M. Kos , A. Kruger , C. Kraus , C. B. Krauss , T. Kutter , C. C. M. Kyba , R. Lange , J. Law , I. T. Lawson , K. T. Lesko , J. R. Leslie , I. Levine , J. C. Loach , R. MacLellan , S. Majerus , H. B. Mak , J. Maneira , R. D. Martin , N. McCauley , A. B. McDonald , S. R. McGee , M. L. Miller , B. Monreal , J. Monroe , B. G. Nickel , A. J. Noble , H. M. O'Keeffe , N. S. Oblath , C. E. Okada , R. W. Ollerhead , G. D. OrebiGann , S. M. Oser , R. A. Ott , S. J. M. Peeters , A. W. P. Poon , G. Prior , S. D. Reitzner , K. Rielage , B. C. Robertson , R. G. H. Robertson , M. H. Schwendener , J. A. Secrest , S. R. Seibert , O. Simard , J. J. Simpson , D. Sinclair , P. Skensved , T. J. Sonley , L. C. Stonehill , G. Tesic , N. Tolich , T. Tsui , R. Van Berg , B. A. VanDevender , C. J. Virtue , B. L. Wall , D. Waller , H. Wan Chan Tseung , D. L. Wark , J. Wendland , N. West , J. F. Wilkerson , J. R. Wilson , A. Wright , M. Yeh , F. Zhang , K. Zuber

Beam and trap methods find incompatible results for the lifetime of the neutron: the former delivers a value which is about $8.7\pm2.1$ s longer than the latter. Very recently (1906.10024) it has been proposed that the inverse Zeno effect…

High Energy Physics - Phenomenology · Physics 2020-02-19 Francesco Giacosa

The modes of decay for the even-even isotopes of superheavy nuclei of Z = 118 and 120 with neutron number $160 \leq N \leq 204$ are investigated in the framework of the axially deformed relativistic mean field model. The asymmetry parameter…

Nuclear Theory · Physics 2018-03-20 M. Bhuyan

The Big-Bang nucleosynthesis (BBN) initial neutron abundance and the neutron lifetime depend on the magnitude of the Fermi coupling constant $G_F$. When allowing for radiative corrections, $G_F$ depends on the symmetry breaking Weinberg…

High Energy Physics - Phenomenology · Physics 2026-03-04 Cheng Tao Yang , Johann Rafelski

All existing "positive" results on two neutrino double beta decay in different nuclei were analyzed. Using procedure recommended by Particle Data Group weighted average values for half-lives of $^{48}$Ca, $^{76}$Ge, $^{82}$Se, $^{96}$Zr,…

Nuclear Experiment · Physics 2016-09-08 A. S. Barabash
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