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Related papers: A Lower Bound on Neutrino Mass

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We explore the limits on neutrino mass which follow from a study of the long-range forces that arise from the exchange of massless or ultra-light neutrinos. Although the 2-body neutrino-exchange force is unobservably small, the many-body…

High Energy Physics - Phenomenology · Physics 2009-10-28 Ephraim Fischbach

It has been shown recently that the exchange of virtual neutrino pairs leads to an unphysically large energy-density in neutron stars and white dwarfs, unless neutrinos have a minimum mass, m > 0.4 eV. Here we consider the possibility that…

High Energy Physics - Phenomenology · Physics 2007-05-23 Brian Woodahl , Michelle Parry , Shu-Ju Tu , Ephraim Fischbach

Stellar objects (including our Sun, other stars of main sequence, white dwarfs, neutron stars etc.) contain strongly degenerate low energy sea of neutrinos (in neutron stars) or antineutrinos. The presence of this sea leads due to Pauli…

High Energy Physics - Phenomenology · Physics 2008-02-03 Alexei Yu. Smirnov , Francesco Vissani

It is supposed that the electron neutrino mass is related to the structures and masses of the $W^\pm$ and $Z^0$ bosons. Using a composite model of fermions (described elsewhere), it is shown that the massless neutrino is not consistent with…

General Physics · Physics 2007-05-23 V. N. Yershov

A lower bound on the light neutrino mass $m_\nu$ is derived in the framework of a geometrical interpretation of quantum mechanics. Using this model and the time of flight delay data for neutrinos coming from SN1987A, we find that the…

General Relativity and Quantum Cosmology · Physics 2009-11-11 G. Lambiase , G. Papini , R. Punzi , G. Scarpetta

Recently announced results from the KATRIN collaboration imply an upper bound on the effective electron anti-neutrino mass $m_{\nu_{e}}$, $m_{\nu_{e}}< 0.8~{\rm eV}/c^{2}$. Here we explore the implications of combining the KATRIN upper…

High Energy Physics - Phenomenology · Physics 2022-08-09 Ephraim Fischbach , Dennis E. Krause , Quan Le Thien , Carol Scarlett

The case for small neutrino mass differences from atmospheric and solar neutrino oscillation experiments has become compelling, but leaves the overall neutrino mass scale m_nu undetermined. The most restrictive limit of m_nu < 0.8 eV arises…

Astrophysics · Physics 2009-11-07 G. G. Raffelt

Massless neutrino exchange leads to a new long-range force between matter. Recently, it was claimed both that the potential energy due to this interaction i) dominates the total energy of neutron stars and ii) that it is zero. We…

High Energy Physics - Phenomenology · Physics 2009-10-30 M. Kachelriess

Neutrinos are the second most abundant particle in the universe. Since the last 50 years, Neutrino physics has been a source of limelight in modern physics because of the incredible characteristics of this elusive particle. According to the…

High Energy Physics - Phenomenology · Physics 2021-04-13 Athar Ahmad , Naila Islam

The interaction energy of the neutrons due to massless neutrino exchange in a neutron star has recently been proved, using an effective theory, to be extremely small and infrared-safe. Our comment here is of conceptual order: two approaches…

High Energy Physics - Phenomenology · Physics 2016-08-25 A. Abada , O. Pene , J. Rodriguez-Quintero

We determine the upper limit on the mass of the lightest neutrino from the most robust recent cosmological and terrestrial data. Marginalizing over possible effective relativistic degrees of freedom at early times ($N_\mathrm{eff}$) and…

The best upper bounds on the masses of stable and unstable light neutrinos derive from the upper bound on the total mass density, as inferred from the lower limit $t_0> 13$ Gyr on the dynamical age of the Universe: If the Universe is…

High Energy Physics - Phenomenology · Physics 2007-05-23 Sidney A. Bludman

If the neutrino is Majorana type and the electroweak phase transition is second or weak first order, neutrino-induced interactions together with sphaleron transitions have the potential to erase a previously generated baryon asymmetry of…

High Energy Physics - Phenomenology · Physics 2009-10-31 H. V. Klapdor-Kleingrothaus , St. Kolb , U. Sarkar

The exchange of two massless neutrinos gives rise to a long range force which couples to weakly charged matter. As has been noted previously in the literature, the potential for this force is $\VN \propto G_{F}^2 / r^5$ with…

High Energy Physics - Phenomenology · Physics 2009-10-22 S. D. H. Hsu , Pierre Sikivie

We have performed a thorough analysis of the constraints which can be put on neutrino parameters from cosmological observations, most notably those from the WMAP satellite and the 2dF galaxy survey. For this data we find an upper limit on…

Astrophysics · Physics 2009-11-07 Steen Hannestad

Assuming that neutrinos of non-zero rest mass dominate the mass density in the universe, and also the mass density on the scale of clusters of galaxies, one obtains the upper limit m < 20 eV/c^2 on their mass, independent of the values of…

Cosmology and Nongalactic Astrophysics · Physics 2009-03-14 D. G. Banhatti

Cosmological limits on neutrino masses are softened, by more than a factor 2, if Cold Dark Matter (CDM) and Dark Energy (DE) are coupled. In turn, a neutrino mass yielding $\Omega_\nu$ up to $\sim0.20$ allows coupling levels $\beta \simeq…

Astrophysics · Physics 2010-04-15 G. La Vacca , S. A. Bonometto , L. P. L. Colombo

A brief up-to-date review of the long range forces generated by two neutrino exchange is presented. The potential due to exchange of a massive neutrino-antineutrino pair between particles carrying weak charge might be larger than expected…

High Energy Physics - Phenomenology · Physics 2011-03-07 Maurizio Lusignoli , Silvano Petrarca

Cosmology at present provides the nominally strongest constraint on the masses of standard model neutrinos. However, this constraint extremely dependent on the nature of the dark energy component of the Universe. When the dark energy…

Astrophysics · Physics 2008-11-26 Steen Hannestad

New data from neutrino oscillation experiments motivate us to extend a successful mass relation for the charged leptons to the other fundamental fermions. This new universal relation requires a Dirac mass around 3 10^-2 eV for the lightest…

High Energy Physics - Phenomenology · Physics 2009-11-11 J. -M. Gerard , F. Goffinet , M. Herquet
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