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Quark matter formation in dense stellar objects
Quark matter formation in dense stellar objects

Multi-Majoron Modes for Neutrinoless Double
Multi-Majoron Modes for Neutrinoless Double

... of the more recent proposals, fall into only a few of the several possible categories — cases IB and IC of Table I. The other, unorthodox, categories remain essentially unexplored. The two exceptions to this statement are case IID, which was discovered and studied in ref. [5], and case IE, which con ...
Stability - HAL
Stability - HAL

arXiv:astro-ph/0612072v1 4 Dec 2006 Theory of core
arXiv:astro-ph/0612072v1 4 Dec 2006 Theory of core

Automatic scanning of emulsion films for the OPERA - INFN
Automatic scanning of emulsion films for the OPERA - INFN

Strangeness Production in Neutron Stars
Strangeness Production in Neutron Stars

The Weak Interaction - University of Warwick
The Weak Interaction - University of Warwick

Frontiers in Neutrino Astrophysics
Frontiers in Neutrino Astrophysics

... The Impossible Dream of Neutrino Astronomy “If [there are no new forces] -- one can conclude that there is no practically possible way of observing the neutrino.” Bethe and Peierls, Nature (1934) “Only neutrinos, with their extremely small interaction cross sections, can enable us to see into the i ...
Slides - Indico
Slides - Indico

Observation of New-Particle Production by High
Observation of New-Particle Production by High

The Non-Thermal Universe - Astroparticle physics in the Netherlands
The Non-Thermal Universe - Astroparticle physics in the Netherlands

HEPAP Subpanel - LIGO
HEPAP Subpanel - LIGO

... As the bearer of these lines, to whom I graciously ask you to listen, will explain to you in more detail, how because of the "wrong" statistics of the N and Li6 nuclei and the continuous beta spectrum, I have hit upon a deseperate remedy to save the "exchange theorem" of statistics and the law of co ...
Neutrino oscillations, energy-momentum conservation and
Neutrino oscillations, energy-momentum conservation and

Jan 27, 2000 Lessons learnt from the heavy tau lepton Fig. 1 Fig. 2
Jan 27, 2000 Lessons learnt from the heavy tau lepton Fig. 1 Fig. 2

Beta Decay
Beta Decay

... The neutrino is a very elusive particle. It can penetrate several light-years of lead before being absorbed. For this reason, the neutrino is extremely difficult to detect. The experimental detection of neutrinos occurred in 1956 in a Nobel prize winning experiment by Cowan and Reines. Enrico Fermi ...
The Family Problem: Extension of Standard Model with a
The Family Problem: Extension of Standard Model with a

... neutrinos and familons, very interesting and, albeit likely to be small, should eventually be investigated[6]. For example, in the elastic quark (or charged lepton) - neutrino scattering, the loop corrections would involve the Z^0 and in addition the familon loops and if the masses of the familons w ...
Family Gauge Theory
Family Gauge Theory

... A. Zee, Phys. Lett. B93 (1980) 389; Phys. Lett. B161 (1985) 141; Nucl. Phys. B264 (1986) 99; on the Zee model. W-Y. P. Hwang, Nucl. Phys. A844, 40c (2010); Intern. J. Mod. Phys. A24, 3366 (2009); Intern. J. Mod. Phys. Conf. Series 1, 5 (2011). W-Y. P. Hwang and Tung-Mow Yan, The Universe, 1-1, 5 (20 ...
Probing the Earth`s interior with a large
Probing the Earth`s interior with a large

Structural( biology( at( the( single( particle( level:( imaging( tobacco
Structural( biology( at( the( single( particle( level:( imaging( tobacco

Fermi and the Theory of Weak Interactions
Fermi and the Theory of Weak Interactions

Fermi and the Theory of Weak Interactions
Fermi and the Theory of Weak Interactions

... when we go from left to right-handed coordinate systems and hence the parity violation. This is the V{A form discovered by Sudarshan and Marshak, Feynman and Gell-Mann and Sakurai in 1957. Box 2. Violation of Left{Right Symmetry and CP Left{right symmetry is also called re°ection symmetry or parity ...
Probing the stability of superheavy dark matter particles with high
Probing the stability of superheavy dark matter particles with high

Electroweak Interactions : Neutral currents in neutrino`lepton elastic
Electroweak Interactions : Neutral currents in neutrino`lepton elastic

Cooling neutron stars: Theory and observations
Cooling neutron stars: Theory and observations

Dynamical Conformal and Electro
Dynamical Conformal and Electro

... Embedings into QFTs with classical conformal symmetry
 - SM: Coleman Weinberg effective potential – excluded
 - extended versions à work!
 à implications for Higgs couplings, dark matter, …
 à implications for neutrino masses
 è testable consequences @ LHC, DM search, neutrinos ...
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Neutrino



A neutrino (/nuːˈtriːnoʊ/ or /njuːˈtriːnoʊ/, in Italian [nɛuˈtrino]) is an electrically neutral elementary particle with half-integer spin. The neutrino (meaning ""little neutral one"" in Italian) is denoted by the Greek letter ν (nu). All evidence suggests that neutrinos have mass but that their masses are tiny, even compared to other subatomic particles. They are the only identified candidate for dark matter, specifically hot dark matter.Neutrinos are leptons, along with the charged electrons, muons, and taus, and come in three flavors: electron neutrinos (νe), muon neutrinos (νμ), and tau neutrinos (ντ). Each flavor is also associated with an antiparticle, called an ""antineutrino"", which also has no electric charge and half-integer spin. Neutrinos are produced in a way that conserves lepton number; i.e., for every electron neutrino produced, a positron (anti-electron) is produced, and for every electron antineutrino produced, an electron is produced as well.Neutrinos do not carry any electric charge, which means that they are not affected by the electromagnetic force that acts on charged particles, and are leptons, so they are not affected by the strong force that acts on particles inside atomic nuclei. Neutrinos are therefore affected only by the weak subatomic force and by gravity. The weak force is a very short-range interaction, and gravity is extremely weak on the subatomic scale. Thus, neutrinos typically pass through normal matter unimpeded and undetected.Neutrinos can be created in several ways, including in certain types of radioactive decay, in nuclear reactions such as those that take place in the Sun, in nuclear reactors, when cosmic rays hit atoms and in supernovas. The majority of neutrinos in the vicinity of the earth are from nuclear reactions in the Sun. In fact, about 65 billion (7010650000000000000♠6.5×1010) solar neutrinos per second pass through every square centimeter perpendicular to the direction of the Sun in the region of the Earth.Neutrinos are now understood to oscillate between different flavors in flight. That is, an electron neutrino produced in a beta decay reaction may arrive in a detector as a muon or tau neutrino. This oscillation requires that the different neutrino flavors have different masses, although these masses have been shown to be tiny. From cosmological measurements, we know that the sum of the three neutrino masses must be less than one millionth that of the electron.
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