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czas-i-pomiary: Muon
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6 zapisanych źródełEvidence: 100 • authority: 72
A muon ( M(Y)OO-on; from the Greek letter mu (μ) used to represent it) is an elementary particle similar to the electron, with an electric charge of −1 e and a spin of 1/2 ħ, but with a much greater mass. It is classified as a lepton. As with other leptons, the muon is not thought to be composed of any constituent particles. The muon is an unstable subatomic particle with a mean lifetime of 2.2 μs. Muon decay is slower than many other unstable particles because the decay is mediated by the weak interaction and because the mass difference between the muon and the set of its decay products is small, providing few kinetic degrees of freedom for decay. Muon decay always produces an electron (…
Otwórz źródło ↗Evidence: 45 • authority: 72
In particle physics, a lepton is an elementary particle of half-integer spin (spin 1/2) that does not undergo strong interactions. Two main classes of leptons exist: charged leptons (also known as the electron-like leptons or muons), including the electron, muon, and tauon, and neutral leptons, better known as neutrinos. Charged leptons can combine with other particles to form various composite particles such as atoms and positronium, while neutrinos rarely interact with anything, and are consequently rarely observed. The best known of all leptons is the electron. There are six types of leptons, known as flavours, grouped in three generations. The first-generation leptons, also called ele…
Otwórz źródło ↗Evidence: 36 • authority: 72
A neutrino ( new-TREE-noh; denoted by the Greek letter ν) is an elementary particle that interacts via the weak interaction and gravity. The neutrino is so named because it is electrically neutral and because its rest mass is so small (-ino) that it was long thought to be zero. The rest mass of the neutrino is much smaller than that of the other known elementary particles (excluding massless particles). The weak force has a very short range, the gravitational interaction is extremely weak due to the very small mass of the neutrino, and neutrinos do not participate in the electromagnetic interaction or the strong interaction. Consequently, neutrinos typically pass through normal matter unimp…
Otwórz źródło ↗Evidence: 27 • authority: 72
Neutrino oscillation is a quantum mechanical phenomenon in which a neutrino created with a specific lepton family number ("lepton flavor": electron, muon, or tau) can later be measured to have a different lepton family number. The probability of measuring a particular flavor for a neutrino varies between three known states as it propagates through space. First predicted by Bruno Pontecorvo in 1957, neutrino oscillation has since been observed by a multitude of experiments in several different contexts. Most notably, the existence of neutrino oscillation resolved the long-standing solar neutrino problem. Neutrino oscillation is of great theoretical and experimental interest, as the precise p…
Otwórz źródło ↗Evidence: 27 • authority: 80
Probing \boldmath{$\tau$} lepton dipole moments at future Muon Colliders
Otwórz źródło ↗Evidence: 27 • authority: 88
Search for lepton-flavor-violating decays of the tau lepton at a future muon collider. Tau leptons can have lepton-flavor-violating (LFV) couplings to a muon or an electron and an Axion-Like Particle (ALP). ALPs are pseudo Nambu-Goldstone bosons associated with spontaneously broken global U(1) symmetries. LFV ALPs have been of a great interest in the last several decades as they can address some of the SM long-lasting problems. Assuming a future muon collider proposed by the Muon Accelerator Program (MAP), we search for LFV decays \tau→\ell a τ → ℓ a ( \ell=e,\mu ℓ = e , μ ) of one of the tau leptons produced in the muon-anti muon annihilation. The ALP mass is assumed to be in the range 100…
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