scholarly journals Bounds on light sterile neutrino mass and mixing from cosmology and laboratory searches

2021 ◽  
Vol 104 (12) ◽  
Author(s):  
Steffen Hagstotz ◽  
Pablo F. de Salas ◽  
Stefano Gariazzo ◽  
Sergio Pastor ◽  
Martina Gerbino ◽  
...  
1987 ◽  
Vol 194 (4) ◽  
pp. 477-481 ◽  
Author(s):  
J. Arafune ◽  
M. Fukugita ◽  
T. Yanagida ◽  
M. Yoshimura

1988 ◽  
Vol 207 (1) ◽  
pp. 79-85 ◽  
Author(s):  
John G. Learned ◽  
Sandip Pakvasa ◽  
Thomas J. Weiler

1996 ◽  
Vol 53 (11) ◽  
pp. 6361-6373 ◽  
Author(s):  
A. Bottino ◽  
N. Fornengo ◽  
C. W. Kim ◽  
G. Mignola

1998 ◽  
Vol 13 (25) ◽  
pp. 4409-4423 ◽  
Author(s):  
DAVID O. CALDWELL

New experimental results, if correct, require at least one light sterile neutrino, in addition to the three active ones, to accommodate the mass differences required to explain the solar νe deficit, the anomalous μ/e ratio produced by atmospheric neutrinos, and either the candidate events for νμ→ νe (or [Formula: see text]) from the LSND experiment, or the possible need for a hot component of dark matter. This neutrino mass pattern can not only accommodate all these four requirements, but also provide a robust solution to a problem presently making heavy-element synthesis by supernovae impossible and resolve a possible discrepancy between big bang nucleosynthesis theory and observations.


1992 ◽  
Vol 283 (3-4) ◽  
pp. 446-453 ◽  
Author(s):  
E.W. Beier ◽  
E.D. Frank ◽  
W. Frati ◽  
S.B. Kim ◽  
A.K. Mann ◽  
...  

1989 ◽  
Vol 04 (06) ◽  
pp. 535-541
Author(s):  
JIANG LIU

A theoretical pattern for the MSW oscillation that takes νeL into a sterile particle is discussed. The required small neutrino mass is induced by a seesaw formula, in which the heavy neutrino mass term is of the order of the grand unification scale. Realizations of our scheme are illustrated by a simple SU (2)L × U (1)Y model.


2014 ◽  
Vol 23 (12) ◽  
pp. 1450080 ◽  
Author(s):  
Osvaldo Civitarese ◽  
Mercedes Elisa Mosquera ◽  
María Manuela Sáez

In the present work, we discuss the effects of the inclusion of sterile–active neutrino oscillations during the production of primordial light-nuclei. We assume that the sterile neutrino mass-eigenstate might oscillate with the two lightest active neutrino mass-eigenstates, with mixing angles ϕ1 and ϕ2. We also allow a constant renormalization (represented by a parameter (ζ)) of the sterile neutrino occupation factor. Taking ζ and the mixing angles as free parameters, we have computed distribution functions of active and sterile neutrinos and primordial abundances. Using observable data we set constrains in the free parameters of the model. It is found that the data on primordial abundances are consistent with small mixing angles and with a value of ζ smaller than 0.65 at 3σ level.


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