Using the CHARM II result for the charge radius of the muon-neutrino |2>|<6.0×10-33cm2, we place a bound on -7.9×10-33cm2≤2>LR≤7.9×10-33cm2. We discuss the relationship between the electron neutral couplings gVeV and gVeA and the LR model parameters. We also estimate a bound...
Measurement of the muon neutrino inclusive charged-current cross section in the energy range of 1-3 GeV with the T2K INGRID detector We report a measurement of the $u_{\\mu}$-nucleus inclusive charged current\ncross section (=$\\sigma^{cc}$) on iron using data from exposed to the J...
The addition of a charge to the neutral neutrino lattices of the muon or pion changes the simple cubic lattices of the neutral particles to face-centered cubic lattices of the charged particles, which is essential for the stability of the particles.doi:10.48550/arXiv.0909.3681Koschmieder E. L...
A muon (m_{\mu}c^2 = 105.7 MeV) at rest decays into a electron (m_ec^2 = 0.511 MeV) and a neutrino (whose mass is very nearly zero). What is the Kelectron and Kneutrino in MeV? Alpha particles (charge +2e, mass 6.68 x 10^-27 kg) are accelerat...
Large experimental programmes in the fields of nuclear and particle physics search for evidence of physics beyond that explained by current theories. The observation of the Higgs boson completed the set of particles predicted by the standard model, which
Secondly, the energy spectrum of the external muons is significantly harder than for the con- tained vertices. This is a consequence of the in- crease of the muon range with energy. A much higher range of neutrino energies contributes to ...
of nuclearK-capture is accompanied by the emergence of an electron neutrino (νe), e–+ p → n + νe, and the absorption of a negative muon (μ–) is accompanied by the emergence of a muon neutrino (vμ), μ–+ p→ n + νμ; in the process of beta decay of a neutron (n...
This two-neutrino double beta decay (2νββ) is in full agreement with lepton number conservation and all known physics laws. In fact, it was predicted theoretically a long time ago by Maria Goeppert–Mayer [24]. As discussed in detail in [18] and in a forthcoming section of the ...
Thus, the COHERENT results would be sensitive to the U(1)′ models with gauge couplings to electron or muon neutrinos [27, 42–46]. Moreover, due to the change of neutrino propaga- tion in matter in terms of neutral current NSIs, the long-baseline neutrino oscillation exper- iments ...
We propose a kinematical enhancement of the tt¯ charge asymmetry at the LHC by selecting events with the tt¯ centre of mass frame highly boosted along the beam axis. This kinematical selection increases the asymmetries and their significance up to a factor of two in a rather model-independ...