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相关论文: Invisible neutrino decay in precision cosmology

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The anisotropies of the Cosmic Neutrino Background (C$\nu$B) offer an ideal tool to test non-standard neutrino interactions, since they directly trace the perturbations in the neutrino distribution function. Here, we study how invisible…

宇宙学与河外天体物理 · 物理学 2025-10-20 Nicola Terzaghi , Guillermo Franco Abellán , Fabian Zimmer , Shin'ichiro Ando

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…

高能物理 - 唯象学 · 物理学 2020-05-04 Zackaria Chacko , Abhish Dev , Peizhi Du , Vivian Poulin , Yuhsin Tsai

We consider invisible neutrino decay $\nu_H \to \nu_l + \phi$ in the ultra-relativistic limit and compute the neutrino anisotropy loss rate relevant for the cosmic microwave background (CMB) anisotropies. Improving on our previous work…

高能物理 - 唯象学 · 物理学 2022-06-17 Joe Zhiyu Chen , Isabel M. Oldengott , Giovanni Pierobon , Yvonne Y. Y. Wong

Discovering neutrino decay would be strong evidence of physics beyond the Standard Model. Presently, there are only lax lower limits on the lifetime $\tau$ of neutrinos, of $\tau/m \sim 10^{-3}$ s eV$^{-1}$ or worse, where $m$ is the…

高能天体物理现象 · 物理学 2020-04-16 Mauricio Bustamante

Future direct observations of the Cosmic Neutrino Background (C$\nu$B) have the potential to explore a neutrino lifetime, especially in the region of the age of the universe, $t_0=4.35\times 10^{17}\ {\rm s}$. We forecast constraints on…

高能物理 - 唯象学 · 物理学 2022-03-09 Kensuke Akita , Gaetano Lambiase , Masahide Yamaguchi

Invisible neutrino decay modes are difficult to target at laboratory experiments, and current bounds on such decays from solar neutrino and neutrino oscillation experiments are somewhat weak. It has been known for some time that Cosmology…

高能物理 - 唯象学 · 物理学 2020-01-20 Miguel Escudero , Malcolm Fairbairn

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…

宇宙学与河外天体物理 · 物理学 2026-01-09 Guillermo Franco Abellán

We investigate a scenario in which neutrinos are coupled to a pseudoscalar degree of freedom $\ph$ and where decays $\nu_1 \to \nu_2+\ph$ and inverse decays are the responsible mechanism for obtaining equilibrium. In this context we discuss…

宇宙学与河外天体物理 · 物理学 2010-08-30 Anders Basboll , Ole Eggers Bjaelde

We investigate in detail the possibility of constraining neutrino decays with data from the cosmic microwave background radiation (CMBR). Two generic decays are considered \nu_H -> \nu_L \phi and \nu_H -> \nu_L \nu_L_bar \nu_L. We have…

天体物理学 · 物理学 2009-10-31 Steen Hannestad

We investigate the radiative decay of the cosmic neutrino background, and its impact on the spectrum of the cosmic microwave background (CMB) that is known to be a nearly perfect black body. We derive exact formulae for the decay of a…

At present, cosmological observations set the most stringent bound on the neutrino mass scale. Within the standard cosmological model ($\Lambda$CDM), the Planck collaboration reports $\sum m_\nu < 0.12\,\text{eV}$ at 95% CL. This bound,…

高能物理 - 唯象学 · 物理学 2021-09-06 Miguel Escudero , Jacobo Lopez-Pavon , Nuria Rius , Stefan Sandner

We discuss decays of ultra-relativistic neutrinos over cosmological distances by solving the decay equation in terms of its redshift dependence. We demonstrate that there are significant conceptual differences compared to more simplified…

宇宙学与河外天体物理 · 物理学 2012-10-16 Philipp Baerwald , Mauricio Bustamante , Walter Winter

Neutrino oscillation experiments and direct bounds on absolute masses constrain neutrino mass differences to fall into the microwave energy range, for most of the allowed parameter space. As a consequence of these recent phenomenological…

高能物理 - 唯象学 · 物理学 2008-11-26 A. Mirizzi , D. Montanino , P. D. Serpico

Four zero neutrino Yukawa textures in a specified weak basis, combined with $\mu\tau$ symmetry and type-I seesaw, yield a highly constrained and predictive scheme. Two alternately viable $3\times3$ light neutrino Majorana mass matrices…

高能物理 - 唯象学 · 物理学 2015-05-27 Biswajit Adhikary , Ambar Ghosal , Probir Roy

Precision measurements of the acoustic peaks of the cosmic microwave background indicate that neutrinos must be freely streaming at the photon decoupling epoch when T ~ 0.3 eV. This requirement implies restrictive limits on ``secret…

高能物理 - 唯象学 · 物理学 2013-05-29 Steen Hannestad , Georg Raffelt

Neutrinos are perhaps the most elusive known particles in the universe. We know they have some nonzero mass, but unlike all other particles, the absolute scale remains unknown. In addition, their fundamental nature is uncertain; they can…

核理论 · 物理学 2023-07-31 A. Belley , T. Miyagi , S. R. Stroberg , J. D. Holt

We reanalyze the cosmological constraints on the existence of a net universal lepton asymmetry and neutrino degeneracy. We show that neutrinos can begin to decouple at higher temperatures than previous estimates due to several corrections…

天体物理学 · 物理学 2007-05-23 M. Orito , T. Kajino , G. J. Mathews , R. N. Boyd

The light neutrino masses are at present most stringently constraint via cosmological probes. In particular the Planck collaboration reports $ \sum m_\nu \leq 0.12\,\mathrm{eV}$ at $95\%$ CL within the standard cosmological model. This is…

高能物理 - 唯象学 · 物理学 2022-05-17 Stefan Sandner

Cosmological parameter estimation exercises usually make the approximation that the three standard neutrinos have degenerate mass, which is at odds with recent terrestrial measurements of the difference in the square of neutrino masses. In…

天体物理学 · 物理学 2009-11-11 Anze Slosar

We investigate the non-radiative decay during nucleosynthesis of a massive tau neutrino with mass 0.1 - 1 MeV into an electron neutrino and a scalar or pseudoscalar particle, $\phi$. The full Boltzmann equation is used and shown to give…

高能物理 - 唯象学 · 物理学 2009-10-30 S. Hannestad
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