The Weak Interaction
... Note: In this case flavor changes stay within a quark generation. Note: The strong interaction can be involved as well to create the quark-antiquark pair. ...
... Note: In this case flavor changes stay within a quark generation. Note: The strong interaction can be involved as well to create the quark-antiquark pair. ...
Ratio of Charge to Mass (e/m) for the Electron
... Now turn the magnetic field back on, and bring one end of a bar magnet as close as you can to the electrons' path and observe the spiral path which the electrons now follow. Can you explain why the presence of the extra field distorts the electron's path? How will the Earth's field affect the motion ...
... Now turn the magnetic field back on, and bring one end of a bar magnet as close as you can to the electrons' path and observe the spiral path which the electrons now follow. Can you explain why the presence of the extra field distorts the electron's path? How will the Earth's field affect the motion ...
-30- Section 9: f"
... Ex 12-3: Find the radius and density of an 56Fe nucleus. Binding energy = (c2)(difference between mass of nucleus and particles making it up) Ex: Binding energy of a deuteron - see section 5. Eb (in MeV) = (ZmH + Nmn - matom)(931.5) (masses in atomic mass units: 1 u = 1/12 mass of a 12C atom) mH = m ...
... Ex 12-3: Find the radius and density of an 56Fe nucleus. Binding energy = (c2)(difference between mass of nucleus and particles making it up) Ex: Binding energy of a deuteron - see section 5. Eb (in MeV) = (ZmH + Nmn - matom)(931.5) (masses in atomic mass units: 1 u = 1/12 mass of a 12C atom) mH = m ...
Overview of Neutrino Physics Issues and Opportunities Andr´ e de Gouvˆ
... Another νSM Why don’t we just enhance the fermion sector of the theory? One may argue that it is trivial and simpler to just add LYukawa = −yiα Li HN α + H.c., and neutrinos get a mass like all other fermions: miα = yiα v • Data requires y < 10−12 . Why so small? • Neutrinos are Dirac fermions. B − ...
... Another νSM Why don’t we just enhance the fermion sector of the theory? One may argue that it is trivial and simpler to just add LYukawa = −yiα Li HN α + H.c., and neutrinos get a mass like all other fermions: miα = yiα v • Data requires y < 10−12 . Why so small? • Neutrinos are Dirac fermions. B − ...
Ratio of Charge to Mass (e/m) for the Electron
... Now turn the magnetic field back on, and bring one end of a bar magnet as close as you can to the electrons' path and observe the spiral path which the electrons now follow. Can you explain why the presence of the extra field distorts the electron's path? How will the Earth's field affect the motion ...
... Now turn the magnetic field back on, and bring one end of a bar magnet as close as you can to the electrons' path and observe the spiral path which the electrons now follow. Can you explain why the presence of the extra field distorts the electron's path? How will the Earth's field affect the motion ...
Chapter 4
... - continuous spectrum: a spectrum in which all wavelengths within a given range are included - electromagnetic spectrum: consists of all electromagnetic radiation, arranged according to increasing wavelength ...
... - continuous spectrum: a spectrum in which all wavelengths within a given range are included - electromagnetic spectrum: consists of all electromagnetic radiation, arranged according to increasing wavelength ...
Charged particles and magnetic fields
... every probability that you will soon be able to tax it! ’ In fact it was more than 150 years later that this prediction of Faraday became true. In the last section we explored the electric field that surrounds a stationary electric charge. Questions to consider and discuss: What happens when a cha ...
... every probability that you will soon be able to tax it! ’ In fact it was more than 150 years later that this prediction of Faraday became true. In the last section we explored the electric field that surrounds a stationary electric charge. Questions to consider and discuss: What happens when a cha ...
Professor Liss
... But we haven’t found the stop quark yet. The more we don’t find it, the heavier it must be – if it exists at all… ...
... But we haven’t found the stop quark yet. The more we don’t find it, the heavier it must be – if it exists at all… ...
Lecture 31 April 06. 2016.
... •Atoms are made up with a central nucleus of protons and neutrons surrounded by a number of electrons equal to the number of protons. • The notation we use is 2He4 •2 is the atomic number = number of protons (and electrons) •4 is the mass number = number of protons + neutrons •Note atomic mass is th ...
... •Atoms are made up with a central nucleus of protons and neutrons surrounded by a number of electrons equal to the number of protons. • The notation we use is 2He4 •2 is the atomic number = number of protons (and electrons) •4 is the mass number = number of protons + neutrons •Note atomic mass is th ...
constitution of matter, the standard model
... whim: It was discovered in 1974 almost simultaneously at both the Stanford Linear Accelerator Center (SLAC) and at Brookhaven National Laboratory (BNL). The fifth and sixth quarks were sometimes called truth and beauty in the past. The bottom quark was discovered at Fermi National Lab (Fermilab) in ...
... whim: It was discovered in 1974 almost simultaneously at both the Stanford Linear Accelerator Center (SLAC) and at Brookhaven National Laboratory (BNL). The fifth and sixth quarks were sometimes called truth and beauty in the past. The bottom quark was discovered at Fermi National Lab (Fermilab) in ...
Chapter 5 Review Answer Key
... Thompson put gas into a glass tube at a near-vacuum and put a charge through it, causing a beam of light. When an electromagnet was placed near the tube, the beam was deflected away from the negative and towards the positive. The results were the same for all gases he used, thus he proved that since ...
... Thompson put gas into a glass tube at a near-vacuum and put a charge through it, causing a beam of light. When an electromagnet was placed near the tube, the beam was deflected away from the negative and towards the positive. The results were the same for all gases he used, thus he proved that since ...
Subatomic particles worksheet answers
... unauthorized appearance of attorney administration had satis. particles GCU 1 1 received by the sheriff. Have the triangular lot negative integer including zero benefit of the domi. Muons, neutrinos, supersymmetric partners, the infamous Higgs boson - with so many different subatomic particles flyin ...
... unauthorized appearance of attorney administration had satis. particles GCU 1 1 received by the sheriff. Have the triangular lot negative integer including zero benefit of the domi. Muons, neutrinos, supersymmetric partners, the infamous Higgs boson - with so many different subatomic particles flyin ...
Lepton
A lepton is an elementary, half-integer spin (spin 1⁄2) particle that does not undergo strong interactions, but is subject to the Pauli exclusion principle. The best known of all leptons is the electron, which is directly tied to all chemical properties. Two main classes of leptons exist: charged leptons (also known as the electron-like leptons), 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.There are six types of leptons, known as flavours, forming three generations. The first generation is the electronic leptons, comprising the electron (e−) and electron neutrino (νe); the second is the muonic leptons, comprising the muon (μ−) and muon neutrino (νμ); and the third is the tauonic leptons, comprising the tau (τ−) and the tau neutrino (ντ). Electrons have the least mass of all the charged leptons. The heavier muons and taus will rapidly change into electrons through a process of particle decay: the transformation from a higher mass state to a lower mass state. Thus electrons are stable and the most common charged lepton in the universe, whereas muons and taus can only be produced in high energy collisions (such as those involving cosmic rays and those carried out in particle accelerators).Leptons have various intrinsic properties, including electric charge, spin, and mass. Unlike quarks however, leptons are not subject to the strong interaction, but they are subject to the other three fundamental interactions: gravitation, electromagnetism (excluding neutrinos, which are electrically neutral), and the weak interaction. For every lepton flavor there is a corresponding type of antiparticle, known as antilepton, that differs from the lepton only in that some of its properties have equal magnitude but opposite sign. However, according to certain theories, neutrinos may be their own antiparticle, but it is not currently known whether this is the case or not.The first charged lepton, the electron, was theorized in the mid-19th century by several scientists and was discovered in 1897 by J. J. Thomson. The next lepton to be observed was the muon, discovered by Carl D. Anderson in 1936, which was classified as a meson at the time. After investigation, it was realized that the muon did not have the expected properties of a meson, but rather behaved like an electron, only with higher mass. It took until 1947 for the concept of ""leptons"" as a family of particle to be proposed. The first neutrino, the electron neutrino, was proposed by Wolfgang Pauli in 1930 to explain certain characteristics of beta decay. It was first observed in the Cowan–Reines neutrino experiment conducted by Clyde Cowan and Frederick Reines in 1956. The muon neutrino was discovered in 1962 by Leon M. Lederman, Melvin Schwartz and Jack Steinberger, and the tau discovered between 1974 and 1977 by Martin Lewis Perl and his colleagues from the Stanford Linear Accelerator Center and Lawrence Berkeley National Laboratory. The tau neutrino remained elusive until July 2000, when the DONUT collaboration from Fermilab announced its discovery.Leptons are an important part of the Standard Model. Electrons are one of the components of atoms, alongside protons and neutrons. Exotic atoms with muons and taus instead of electrons can also be synthesized, as well as lepton–antilepton particles such as positronium.