PDF-electron, muon, neutrino have L = +1 anti-electron, anti-muon, anti-ne

electron and electronneutrino have 1 their antiparticles have 1 muon and muonneutrino have 1 their antiparticles have THUS there should be two types of neutrinos electronkind and muo. Space-Time Revisited. Antimatter. Feynman Diagrams. Quantum Electrodynamics. (Special) Relativity + Quantum = ?. Relativity. Deterministic. E = mc². Space-Time/Gravity. Quantum Mechanics . . Probabilistic. Hyperons. Classification of the Elementary Particles. Elementary particles are classified into groups according to their mass and spin properties. These are, referring to their masses: . (1) the photon with zero rest mass and spin 1. It is a massless boson. . Atoms in magnetic field. orbiting electron behaves like current loop . .  magnetic moment . μ. = current x area . interaction energy = . μ. ·B. (both vectors!) = . μ. ·B. . loop current = -. Context: Muon Collider and Neutrino Factory. 1997. : Colin . Johnson argued . that the next step after the ACOL antiproton production target should be a mercury jet target. . [U. Miss. Workshop, Jan 1997; my introduction to Muon Collider . MINERvA is studying neutrino interactions in unprecedented detail on a variety of different nuclei. Low . Energy (LE) . Beam Goals: . S. tudy . both signal and background reactions relevant . to oscillation experiments (current and future). and Earth Structures. By . Miriam Aczel. What are neutrinos?. They are almost . massless. —hardly feel the force of gravity. They have no electric charge—don’t feel the electromagnetic force. Have no . Quick review of Friday’s material. Collect homework. Next quiz: Friday (covers relativistic kinematics, flux and luminosity). Start on symmetries, conservation laws.. Friday’s plan. Dirac Equation. Context: Muon Collider and Neutrino Factory. 1997. : Colin . Johnson argued . that the next step after the ACOL antiproton production target should be a mercury jet target. . [U. Miss. Workshop, Jan 1997; my introduction to Muon Collider . Cioli Barazandeh, Angel . Gutarra-leon. and Walerian Majewski. Mentor: . Walerian. . Majewski. , Department of Physics . Northern Virginia Community College, Annandale, VA . Experiments. Hello, and welcome to my Presentation!. Abbreviations:AASLD,AmericanAssociationfortheStudyofLiverDiseases;anti-HBc,antibodytohepatitisBcoreantigen;anti-HBs,antibodytohepatitisBsurfaceantigen;anti-HBe,antibodytohepatiti ofliverdisease(drug-i 1. The basis of the potential of . muon. beams. Muon. mass:. 200. . m. e. ~ . m. m. ~ 0.1. . m. p. Muon. decay:. n. e. , . n. m. Precisely known energy spectrum. Energy frontier:. No . brem. -/beam-. Past and Present. Art McDonald. Queen’s University. And. SNOLAB. 1940’s to 1960’s:. Neutrino oscillations were proposed by . Pontecorvo. in 1957 motivated by initial reports of measurements by Davis with a Chlorine detector at a reactor. At that point, the transitions being considered were electron neutrino to electron anti-neutrino.. LHC, MAP, and LEMC. David . Neuffer. July 2018. 2. Outline. Next Heavy Lepton Collider . up to ~14 . TeV. in LHC tunnel. Needs muon source. PS or new MW proton . Linac. /storage ring. cooling …. or LEMC??. : . universal term for all weak-interaction transitions. . between two neighboring isobars. three different forms. β. -. , . β. +. & . EC. (. capture of an atomic electron.