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Samenvatting """The Standard Model is the theory of elementary building blocks of matter and of their forces. It is the most comprehensive physical theory ever developed, and has been experimentally tested with high accuracy. While most texts on this subject emphasise theoretical aspects, this textbook contains examples of basic experiments, before going into the theory.

This allows readers to see howmeasurements and theory interplay in the development of physics. The author examines leptons, hadrons and quarks, before presenting the dynamics and the surprising properties of the charges of the different forces. The textbook concludes with a brief discussion on the recent discoveries of physics beyond the Standard Model, and its connections with cosmology.

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Each chapter ends in the exercises, and solutions to some problems are included in the book. Complete solutions are available to instructors at www. This textbook is suitable for advanced undergraduate students and graduate students. Toon meer Toon minder. Recensie s 'I liked the first edition very much, and used it for my classes. I like the second edition even better Best of all, for the current version, there are some timely additions, most notably the discovery of the Higgs boson and an expanded chapter on neutrino oscillations Let us hope that Run 2 at the LHC will necessitate the writing of a third edition of this wonderful book.

This novel feature of the second edition makes [the book] even more attractive Cifarelli, Il Nuovo Saggiatore 'What is special about this book is that it requires very little effort for the [reader] to like it. It is very well presented and Ishak, Contemporary Physics Review of the first edition: 'Bettini's expertise shines brightly throughout the text The choice of topics and the level of detail are excellent The book is extremely well-written, topically informative and easy to read - but best of all it is full of physics Define the main terms in use to classify and name the elementary particles.

Make correct charge and flavour assignments to all the quark and lepton flavours; 2. Discuss qualitatively the relationship between symmetries and conservation laws.

Physics of Elementary Particles, - Prospectus - Universiteit Leiden

Know the conserved quantities of the four fundamental interactions and be able to make simple applications of conservation laws; 3. Be able to write-down the classical equation of motion for a charged particle in uniform magnetic and electric fields non-radiative approximation , and solve for its motion in each case.

Be able to discuss the main principles behind cathode ray tubes, mass spectrometers and particle accelerators; 4. Be able to discuss qualitatively, several natural sources of radiation.

Module content and teaching

In particle physics , an elementary particle or fundamental particle is a subatomic particle with no sub structure, thus not composed of other particles. Everyday matter is composed of atoms , once presumed to be matter's elementary particles— atom meaning "unable to cut" in Greek—although the atom's existence remained controversial until about , as some leading physicists regarded molecules as mathematical illusions, and matter as ultimately composed of energy.

As the s opened, the electron and the proton had been discovered, along with the photon , the particle of electromagnetic radiation. Via quantum theory, protons and neutrons were found to contain quarks — up quarks and down quarks —now considered elementary particles. Around , an elementary particle's status as indeed elementary—an ultimate constituent of substance—was mostly discarded for a more practical outlook, [1] embodied in particle physics' Standard Model , what's known as science's most experimentally successful theory.

All elementary particles are either bosons or fermions. These classes are distinguished by their quantum statistics : fermions obey Fermi—Dirac statistics and bosons obey Bose—Einstein statistics. Notes: 1.

Introduction to Nuclear and Particle Physics

In the Standard Model , elementary particles are represented for predictive utility as point particles. Though extremely successful, the Standard Model is limited to the microcosm by its omission of gravitation and has some parameters arbitrarily added but unexplained. Neutrons are made up of one up and two down quarks, while protons are made of two up and one down quark. Since the other common elementary particles such as electrons, neutrinos, or weak bosons are so light or so rare when compared to atomic nuclei, we can neglect their mass contribution to the observable universe's total mass.

FY3403: Particle Physics

Therefore, one can conclude that most of the visible mass of the universe consists of protons and neutrons, which, like all baryons , in turn consist of up quarks and down quarks. Some estimates imply that there are roughly 10 80 baryons almost entirely protons and neutrons in the observable universe. The number of protons in the observable universe is called the Eddington number.

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In terms of number of particles, some estimates imply that nearly all the matter, excluding dark matter , occurs in neutrinos, which constitute the majority of the roughly 10 86 elementary particles of matter that exist in the visible universe. The Standard Model of particle physics contains 12 flavors of elementary fermions , plus their corresponding antiparticles , as well as elementary bosons that mediate the forces and the Higgs boson , which was reported on July 4, , as having been likely detected by the two main experiments at the Large Hadron Collider ATLAS and CMS.

However, the Standard Model is widely considered to be a provisional theory rather than a truly fundamental one, since it is not known if it is compatible with Einstein 's general relativity. There may be hypothetical elementary particles not described by the Standard Model, such as the graviton , the particle that would carry the gravitational force , and sparticles , supersymmetric partners of the ordinary particles. The remaining six particles are quarks discussed below. For example, the most accurately known quark mass is of the top quark t at Estimates of the values of quark masses depend on the version of quantum chromodynamics used to describe quark interactions.

Quarks are always confined in an envelope of gluons which confer vastly greater mass to the mesons and baryons where quarks occur, so values for quark masses cannot be measured directly. Since their masses are so small compared to the effective mass of the surrounding gluons, slight differences in the calculation make large differences in the masses. Isolated quarks and antiquarks have never been detected, a fact explained by confinement. Every quark carries one of three color charges of the strong interaction ; antiquarks similarly carry anticolor.

Color-charged particles interact via gluon exchange in the same way that charged particles interact via photon exchange. However, gluons are themselves color-charged, resulting in an amplification of the strong force as color-charged particles are separated. Unlike the electromagnetic force , which diminishes as charged particles separate, color-charged particles feel increasing force.

However, color-charged particles may combine to form color neutral composite particles called hadrons. A quark may pair up with an antiquark: the quark has a color and the antiquark has the corresponding anticolor. The color and anticolor cancel out, forming a color neutral meson. Alternatively, three quarks can exist together, one quark being "red", another "blue", another "green". These three colored quarks together form a color-neutral baryon.

Symmetrically, three antiquarks with the colors "antired", "antiblue" and "antigreen" can form a color-neutral antibaryon. Quarks also carry fractional electric charges , but, since they are confined within hadrons whose charges are all integral, fractional charges have never been isolated. Evidence for the existence of quarks comes from deep inelastic scattering : firing electrons at nuclei to determine the distribution of charge within nucleons which are baryons. If the charge is uniform, the electric field around the proton should be uniform and the electron should scatter elastically.

Low-energy electrons do scatter in this way, but, above a particular energy, the protons deflect some electrons through large angles. The recoiling electron has much less energy and a jet of particles is emitted. This inelastic scattering suggests that the charge in the proton is not uniform but split among smaller charged particles: quarks. In the Standard Model, vector spin -1 bosons gluons , photons , and the W and Z bosons mediate forces, whereas the Higgs boson spin-0 is responsible for the intrinsic mass of particles.

Bosons differ from fermions in the fact that multiple bosons can occupy the same quantum state Pauli exclusion principle. Also, bosons can be either elementary, like photons, or a combination, like mesons. The spin of bosons are integers instead of half integers. Gluons mediate the strong interaction , which join quarks and thereby form hadrons , which are either baryons three quarks or mesons one quark and one antiquark.

Protons and neutrons are baryons, joined by gluons to form the atomic nucleus. Like quarks, gluons exhibit color and anticolor—unrelated to the concept of visual color—sometimes in combinations, altogether eight variations of gluons. The W bosons are known for their mediation in nuclear decay. The Z 0 does not convert charge but rather changes momentum and is the only mechanism for elastically scattering neutrinos.

The weak gauge bosons were discovered due to momentum change in electrons from neutrino-Z exchange. The massless photon mediates the electromagnetic interaction.