An Introduction to the Standard Model of Particle Physics

Size: px
Start display at page:

Download "An Introduction to the Standard Model of Particle Physics"

Transcription

1 An Introduction to the Standard Model of Particle Physics W. N. COTTINGHAM and D. A. GREENWOOD Ж CAMBRIDGE UNIVERSITY PRESS

2 Contents Preface. page xiii Notation xv 1 The particle physicist's view of Nature Introduction The construction of the Standard Model Leptons Quarks and systems of quarks Spectroscopy of systems of light quarks More quarks Quark colour Electron scattering from nucleons Particle accelerators Units 18 2 Lorentz transformations Rotations, boosts, and proper Lorentz transformations Scalars, contravariant and covariant four-vectors Fields The Levi-Civita tensor Time reversal and space inversion 24 3 The Lagrangian formulation of mechanics Hamilton's principle Conservation of energy Continuous systems A Lorentz covariant field theory The Klein-Gordon equation 31 VII

3 viii Contents 3.6 The energy-momentum tensor Complex scalar fields 34 Classical electromagnetism Maxwell's equations A Lagrangian density for electromagnetism Gauge transformations Solutions of Maxwell's equations Space inversion Charge conjugation Intrinsic angular momentum of the photon The energy density of the electromagnetic field Massive vector fields 44 The Dirac equation and the Dirac field The Dirac equation Lorentz transformations and Lorentz invariance The parity transformation Spinors The matrices y" Making the Lagrangian density real 54 Free space solutions of the Dirac equation A Dirac particle at rest The intrinsic spin of a Dirac particle Plane waves and helicity Negative energy solutions The energy and momentum of the Dirac field The m = 0 case: the neutrino 62 Electrodynamics Probability density and probability current The Dirac equation with an electromagnetic field Gauge transformations and symmetry Charge conjugation Neutrinos and charge conjugation The electrodynamics of a charged scalar field Particles at low energies and the Dirac magnetic moment 71 Quantising fields: QED Boson and fermion field quantisation Time dependence Perturbation theory 79

4 Contents 8.4 Renormalisation and renormalisable field theories The magnetic moment of the electron Quantisation in the Standard Model 86 9 The weak interaction: low energy phenomenology Nuclear beta decay Pion decay Conservation of lepton number Muon decay The interactions of muon neutrinos with electrons Symmetry breaking in model theories Global symmetry breaking and Goldstone bosons Local symmetry breaking and the Higgs boson Massive gauge fields SU(2) symmetry The gauge fields Breaking the SU{2) symmetry Identification of the fields The Weinberg-Salam electroweak theory for leptons Lepton doublets and the Weinberg-Salam theory Lepton coupling to the W ± Lepton coupling to the Z Conservation of lepton number and conservation of charge CP symmetry Mass terms in Z : an attempted generalisation Experimental tests of the Weinberg-Salam theory The search for the gauge bosons The W 1 bosons The Z boson The number of lepton families The measurement of partial widths Left-right production cross-section asymmetry and lepton decay asymmetry of the Z boson The electromagnetic and weak interactions of quarks Construction of the Lagrangian density Quark masses and the Kobayashi-Maskawa mixing matrix The parameterisation of the KM matrix CP symmetry and the KM matrix 137

5 X Contents 14.5 The weak interaction in the low energy limit The hadronic decays of the Z and W bosons Hadronic decays of the Z Asymmetry in quark production Hadronic decays of the W* The theory of strong interactions: quantum chromodynamics A local S 1/(3) gauge theory Colour gauge transformations on baryons and mesons Lattice QCD and asymptotic freedom The quark-antiquark interaction at short distances The conservation of quarks Isospin symmetry Chiral symmetry Quantum chromodynamics: calculations Lattice QCD and confinement Charmonium and bottomonium Perturbative QCD and deep inelastic scattering Perturbative QCD and e + e~ collider physics The Kobayashi-Maskawa matrix Semileptonic weak decays F cb and K ub V ad and nuclear ß decay CP symmetry violation in neutral kaon decays CP symmetry violation in В meson decays The CPrtheorem Anomalies The Adler Bell-Jackiw anomaly Cancellation of anomalies in electroweak currents Lepton and baryon anomalies Gauge transformations and the topological number The instability of matter, and matter genesis 183 Epilogue 184 Reductionism complete? 184 Appendix A An aide-memoire on matrices 185 A.l Definitions and notation 185 A.2 Properties of и х «matrices 186

6 Contents XI A.3 Hermitian and unitary matrices 187 Appendix В The groups of the Standard Model 190 B.l Definition of a group 190 B.2 Rotations of the coordinate axes, and the group SO(3) 191 B.3 The group SU(2) 192 B.4 The group SL (2,C) and the proper Lorentz group 195 B.5 Transformations of the Pauli matrices 196 B.6 Spinors 197 B.7 The group SU(3) 198 Appendix С Annihilation and creation operators 200 C.l The simple harmonic oscillator 200 C.2 An assembly of bosons 201 C.3 An assembly of fermions 202 Appendix D The parton model 204 D.l Elastic electron scattering from nucleons 204 D.2 Inelastic electron scattering from nucleons: the parton model 205 D.3 Hadronic states 210 References 213 Hints to selected problems 215 Index 233

Introduction to Elementary Particles

Introduction to Elementary Particles David Criffiths Introduction to Elementary Particles Second, Revised Edition WILEY- VCH WILEY-VCH Verlag GmbH & Co. KGaA Preface to the First Edition IX Preface to the Second Edition XI Formulas and Constants

More information

Quantum Field Theory 2 nd Edition

Quantum Field Theory 2 nd Edition Quantum Field Theory 2 nd Edition FRANZ MANDL and GRAHAM SHAW School of Physics & Astromony, The University of Manchester, Manchester, UK WILEY A John Wiley and Sons, Ltd., Publication Contents Preface

More information

PHYSICS PARTICLE. An Introductory Course of. Palash B. Pal. CRC Press. Saha Institute of Nuclear Physics. Kolkata, India. Taylor &.

PHYSICS PARTICLE. An Introductory Course of. Palash B. Pal. CRC Press. Saha Institute of Nuclear Physics. Kolkata, India. Taylor &. An Introductory Course of PARTICLE PHYSICS Palash B. Pal Saha Institute of Nuclear Physics Kolkata, India W CRC Press Taylor &. Francis Croup Boca Raton London New York CRC Press is an imprint of the &

More information

Contents. Preface to the First Edition Preface to the Second Edition

Contents. Preface to the First Edition Preface to the Second Edition Contents Preface to the First Edition Preface to the Second Edition Notes xiii xv xvii 1 Basic Concepts 1 1.1 History 1 1.1.1 The Origins of Nuclear Physics 1 1.1.2 The Emergence of Particle Physics: the

More information

Part III The Standard Model

Part III The Standard Model Part III The Standard Model Theorems Based on lectures by C. E. Thomas Notes taken by Dexter Chua Lent 2017 These notes are not endorsed by the lecturers, and I have modified them (often significantly)

More information

FYS 3510 Subatomic physics with applications in astrophysics. Nuclear and Particle Physics: An Introduction

FYS 3510 Subatomic physics with applications in astrophysics. Nuclear and Particle Physics: An Introduction FYS 3510 Subatomic physics with applications in astrophysics Nuclear and Particle Physics: An Introduction Nuclear and Particle Physics: An Introduction, 2nd Edition Professor Brian Martin ISBN: 978-0-470-74275-4

More information

Standard Model & Beyond

Standard Model & Beyond XI SERC School on Experimental High-Energy Physics National Institute of Science Education and Research 13 th November 2017 Standard Model & Beyond Lecture III Sreerup Raychaudhuri TIFR, Mumbai 2 Fermions

More information

Quantum Field Theory. and the Standard Model. !H Cambridge UNIVERSITY PRESS MATTHEW D. SCHWARTZ. Harvard University

Quantum Field Theory. and the Standard Model. !H Cambridge UNIVERSITY PRESS MATTHEW D. SCHWARTZ. Harvard University Quantum Field Theory and the Standard Model MATTHEW D. Harvard University SCHWARTZ!H Cambridge UNIVERSITY PRESS t Contents v Preface page xv Part I Field theory 1 1 Microscopic theory of radiation 3 1.1

More information

The Standard Model of Electroweak Physics. Christopher T. Hill Head of Theoretical Physics Fermilab

The Standard Model of Electroweak Physics. Christopher T. Hill Head of Theoretical Physics Fermilab The Standard Model of Electroweak Physics Christopher T. Hill Head of Theoretical Physics Fermilab Lecture I: Incarnations of Symmetry Noether s Theorem is as important to us now as the Pythagorean Theorem

More information

QUANTUM FIELD THEORY. A Modern Introduction MICHIO KAKU. Department of Physics City College of the City University of New York

QUANTUM FIELD THEORY. A Modern Introduction MICHIO KAKU. Department of Physics City College of the City University of New York QUANTUM FIELD THEORY A Modern Introduction MICHIO KAKU Department of Physics City College of the City University of New York New York Oxford OXFORD UNIVERSITY PRESS 1993 Contents Quantum Fields and Renormalization

More information

The Standard Model and Beyond

The Standard Model and Beyond Paul Langacker The Standard Model and Beyond CRC PRESS Boca Raton Ann Arbor London Tokyo Contents Preface xi 1 Notation and Conventions 1 1.1 Problems............................. 5 2 Review of Perturbative

More information

INTRODUCTION TO NUCLEAR AND PARTICLE PHYSICS

INTRODUCTION TO NUCLEAR AND PARTICLE PHYSICS INTRODUCTION TO NUCLEAR AND PARTICLE PHYSICS ASHOK DAS THOMAS FERBEL University of Rochester JOHN WILEY & SONS, INC. NEW YORK CHICHESTER BRISBANE TORONTO SINGAPORE CONTENTS Preface and Introduction Apologies

More information

An Introduction to. Michael E. Peskin. Stanford Linear Accelerator Center. Daniel V. Schroeder. Weber State University. Advanced Book Program

An Introduction to. Michael E. Peskin. Stanford Linear Accelerator Center. Daniel V. Schroeder. Weber State University. Advanced Book Program An Introduction to Quantum Field Theory Michael E. Peskin Stanford Linear Accelerator Center Daniel V. Schroeder Weber State University 4B Advanced Book Program TT Addison-Wesley Publishing Company Reading,

More information

This page intentionally left blank

This page intentionally left blank This page intentionally left blank AN INTRODUCTION TO THE STANDARD MODEL OF PARTICLE PHYSICS Second Edition The Standard Model of particle physics is the mathematical theory that describes the weak, electromagnetic

More information

Particle Physics I Lecture Exam Question Sheet

Particle Physics I Lecture Exam Question Sheet Particle Physics I Lecture Exam Question Sheet Five out of these 16 questions will be given to you at the beginning of the exam. (1) (a) Which are the different fundamental interactions that exist in Nature?

More information

Lecture 11. Weak interactions

Lecture 11. Weak interactions Lecture 11 Weak interactions 1962-66: Formula/on of a Unified Electroweak Theory (Glashow, Salam, Weinberg) 4 intermediate spin 1 interaction carriers ( bosons ): the photon (γ) responsible for all electromagnetic

More information

FYS3510 Subatomic Physics. Exam 2016

FYS3510 Subatomic Physics. Exam 2016 FYS3510 Subatomic Physics VS 2015 Farid Ould-Saada Exam 2016 In addition to the items marked in blue, don t forget all examples and related material given in the slides, including the ones presented during

More information

Lecture 03. The Standard Model of Particle Physics. Part II The Higgs Boson Properties of the SM

Lecture 03. The Standard Model of Particle Physics. Part II The Higgs Boson Properties of the SM Lecture 03 The Standard Model of Particle Physics Part II The Higgs Boson Properties of the SM The Standard Model So far we talked about all the particles except the Higgs If we know what the particles

More information

Quarks, Leptons and Gauge Fields Downloaded from by on 03/13/18. For personal use only.

Quarks, Leptons and Gauge Fields Downloaded from  by on 03/13/18. For personal use only. QUARKS, LEPTONS & GAUGE FIELDS 2nd edition Kerson Huang Professor of Physics Mussuchusetts Institute qf Technology Y 8 World Scientific Singapore New Jersey London Hong Kong Publirhed by World Scientific

More information

Elementary Particle Physics

Elementary Particle Physics Yorikiyo Nagashima Elementary Particle Physics Volume 2: Foundations of the Standard Model WILEY- VCH WILEY-VCH Verlag GmbH & Co. KGaA Contents Preface XI Acknowledgments XV Color Plates XVII Part One

More information

OUTLINE. CHARGED LEPTONIC WEAK INTERACTION - Decay of the Muon - Decay of the Neutron - Decay of the Pion

OUTLINE. CHARGED LEPTONIC WEAK INTERACTION - Decay of the Muon - Decay of the Neutron - Decay of the Pion Weak Interactions OUTLINE CHARGED LEPTONIC WEAK INTERACTION - Decay of the Muon - Decay of the Neutron - Decay of the Pion CHARGED WEAK INTERACTIONS OF QUARKS - Cabibbo-GIM Mechanism - Cabibbo-Kobayashi-Maskawa

More information

Elementary Particles, Flavour Physics and all that...

Elementary Particles, Flavour Physics and all that... Elementary Particles, Flavour Physics and all that... 1 Flavour Physics The term Flavour physics was coined in 1971 by Murray Gell-Mann and his student at the time, Harald Fritzsch, at a Baskin-Robbins

More information

Outline. Charged Leptonic Weak Interaction. Charged Weak Interactions of Quarks. Neutral Weak Interaction. Electroweak Unification

Outline. Charged Leptonic Weak Interaction. Charged Weak Interactions of Quarks. Neutral Weak Interaction. Electroweak Unification Weak Interactions Outline Charged Leptonic Weak Interaction Decay of the Muon Decay of the Neutron Decay of the Pion Charged Weak Interactions of Quarks Cabibbo-GIM Mechanism Cabibbo-Kobayashi-Maskawa

More information

g abφ b = g ab However, this is not true for a local, or space-time dependant, transformations + g ab

g abφ b = g ab However, this is not true for a local, or space-time dependant, transformations + g ab Yang-Mills theory Modern particle theories, such as the Standard model, are quantum Yang- Mills theories. In a quantum field theory, space-time fields with relativistic field equations are quantized and,

More information

The Strong Interaction and LHC phenomenology

The Strong Interaction and LHC phenomenology The Strong Interaction and LHC phenomenology Juan Rojo STFC Rutherford Fellow University of Oxford Theoretical Physics Graduate School course Lecture 2: The QCD Lagrangian, Symmetries and Feynman Rules

More information

Introduction to the Standard Model New Horizons in Lattice Field Theory IIP Natal, March 2013

Introduction to the Standard Model New Horizons in Lattice Field Theory IIP Natal, March 2013 Introduction to the Standard Model New Horizons in Lattice Field Theory IIP Natal, March 2013 Rogerio Rosenfeld IFT-UNESP Lecture 1: Motivation/QFT/Gauge Symmetries/QED/QCD Lecture 2: QCD tests/electroweak

More information

Outline. Charged Leptonic Weak Interaction. Charged Weak Interactions of Quarks. Neutral Weak Interaction. Electroweak Unification

Outline. Charged Leptonic Weak Interaction. Charged Weak Interactions of Quarks. Neutral Weak Interaction. Electroweak Unification Weak Interactions Outline Charged Leptonic Weak Interaction Decay of the Muon Decay of the Neutron Decay of the Pion Charged Weak Interactions of Quarks Cabibbo-GIM Mechanism Cabibbo-Kobayashi-Maskawa

More information

Pions are Special Contents Chiral Symmetry and Its Breaking Symmetries and Conservation Laws Goldstone Theorem The Potential Linear Sigma Model Wigner

Pions are Special Contents Chiral Symmetry and Its Breaking Symmetries and Conservation Laws Goldstone Theorem The Potential Linear Sigma Model Wigner Lecture 3 Pions as Goldstone Bosons of Chiral Symmetry Breaking Adnan Bashir, IFM, UMSNH, Mexico August 2013 Hermosillo Sonora Pions are Special Contents Chiral Symmetry and Its Breaking Symmetries and

More information

SECOND PUBLIC EXAMINATION. Honour School of Physics Part C: 4 Year Course. Honour School of Physics and Philosophy Part C C4: PARTICLE PHYSICS

SECOND PUBLIC EXAMINATION. Honour School of Physics Part C: 4 Year Course. Honour School of Physics and Philosophy Part C C4: PARTICLE PHYSICS 754 SECOND PUBLIC EXAMINATION Honour School of Physics Part C: 4 Year Course Honour School of Physics and Philosophy Part C C4: PARTICLE PHYSICS TRINITY TERM 04 Thursday, 9 June,.30 pm 5.45 pm 5 minutes

More information

Weak interactions and vector bosons

Weak interactions and vector bosons Weak interactions and vector bosons What do we know now about weak interactions? Theory of weak interactions Fermi's theory of weak interactions V-A theory Current - current theory, current algebra W and

More information

Introduction to Quantum Chromodynamics (QCD)

Introduction to Quantum Chromodynamics (QCD) Introduction to Quantum Chromodynamics (QCD) Jianwei Qiu Theory Center, Jefferson Lab May 29 June 15, 2018 Lecture One The plan for my four lectures q The Goal: To understand the strong interaction dynamics

More information

Quantum Field Theory. Kerson Huang. Second, Revised, and Enlarged Edition WILEY- VCH. From Operators to Path Integrals

Quantum Field Theory. Kerson Huang. Second, Revised, and Enlarged Edition WILEY- VCH. From Operators to Path Integrals Kerson Huang Quantum Field Theory From Operators to Path Integrals Second, Revised, and Enlarged Edition WILEY- VCH WILEY-VCH Verlag GmbH & Co. KGaA I vh Contents Preface XIII 1 Introducing Quantum Fields

More information

PRINCIPLES OF PHYSICS. \Hp. Ni Jun TSINGHUA. Physics. From Quantum Field Theory. to Classical Mechanics. World Scientific. Vol.2. Report and Review in

PRINCIPLES OF PHYSICS. \Hp. Ni Jun TSINGHUA. Physics. From Quantum Field Theory. to Classical Mechanics. World Scientific. Vol.2. Report and Review in LONDON BEIJING HONG TSINGHUA Report and Review in Physics Vol2 PRINCIPLES OF PHYSICS From Quantum Field Theory to Classical Mechanics Ni Jun Tsinghua University, China NEW JERSEY \Hp SINGAPORE World Scientific

More information

Lecture 3: Quarks and Symmetry in Quarks

Lecture 3: Quarks and Symmetry in Quarks Lecture 3: Quarks and Symmetry in Quarks Quarks Cross Section, Fermions & Bosons, Wave Eqs. Symmetry: Rotation, Isospin (I), Parity (P), Charge Conjugate (C), SU(3), Gauge symmetry Conservation Laws: http://faculty.physics.tamu.edu/kamon/teaching/phys627/

More information

2.4 Parity transformation

2.4 Parity transformation 2.4 Parity transformation An extremely simple group is one that has only two elements: {e, P }. Obviously, P 1 = P, so P 2 = e, with e represented by the unit n n matrix in an n- dimensional representation.

More information

Electroweak Theory: 2

Electroweak Theory: 2 Electroweak Theory: 2 Introduction QED The Fermi theory The standard model Precision tests CP violation; K and B systems Higgs physics Prospectus STIAS (January, 2011) Paul Langacker (IAS) 31 References

More information

Electron-positron pairs can be produced from a photon of energy > twice the rest energy of the electron.

Electron-positron pairs can be produced from a photon of energy > twice the rest energy of the electron. Particle Physics Positron - discovered in 1932, same mass as electron, same charge but opposite sign, same spin but magnetic moment is parallel to angular momentum. Electron-positron pairs can be produced

More information

Index. Cambridge University Press Modern Particle Physics Mark Thomson. Index. More information.

Index. Cambridge University Press Modern Particle Physics Mark Thomson. Index. More information. accelerators list of, 26 action at a distance, 5 adjoint spinor, 91 ALEPH experiment, 434 α S, value of, 258 angular momentum algebra in quantum mechanics, 46 ladder operators, 47 anomalous magnetic moment,

More information

Lecture 8. September 21, General plan for construction of Standard Model theory. Choice of gauge symmetries for the Standard Model

Lecture 8. September 21, General plan for construction of Standard Model theory. Choice of gauge symmetries for the Standard Model Lecture 8 September 21, 2017 Today General plan for construction of Standard Model theory Properties of SU(n) transformations (review) Choice of gauge symmetries for the Standard Model Use of Lagrangian

More information

The Gauge Principle Contents Quantum Electrodynamics SU(N) Gauge Theory Global Gauge Transformations Local Gauge Transformations Dynamics of Field Ten

The Gauge Principle Contents Quantum Electrodynamics SU(N) Gauge Theory Global Gauge Transformations Local Gauge Transformations Dynamics of Field Ten Lecture 4 QCD as a Gauge Theory Adnan Bashir, IFM, UMSNH, Mexico August 2013 Hermosillo Sonora The Gauge Principle Contents Quantum Electrodynamics SU(N) Gauge Theory Global Gauge Transformations Local

More information

The Strong Interaction and LHC phenomenology

The Strong Interaction and LHC phenomenology The Strong Interaction and LHC phenomenology Juan Rojo STFC Rutherford Fellow University of Oxford Theoretical Physics Graduate School course Introduction and motivation: QCD and modern high-energy physics

More information

FYS3510 Subatomic Physics. Exam 2016

FYS3510 Subatomic Physics. Exam 2016 FYS3510 Subatomic Physics VS 2015 Farid Ould-Saada Exam 2016 In addition to the items marked in blue, don t forget all examples and related material given in the slides, including the ones presented during

More information

Anomaly. Kenichi KONISHI University of Pisa. College de France, 14 February 2006

Anomaly. Kenichi KONISHI University of Pisa. College de France, 14 February 2006 Anomaly Kenichi KONISHI University of Pisa College de France, 14 February 2006 Abstract Symmetry and quantization U A (1) anomaly and π 0 decay Origin of anomalies Chiral and nonabelian anomaly Anomally

More information

Fundamental Particles and Forces

Fundamental Particles and Forces Fundamental Particles and Forces A Look at the Standard Model and Interesting Theories André Gras PHYS 3305 SMU 1 Overview Introduction to Fundamental Particles and Forces Brief History of Discovery The

More information

QCD in the light quark (up & down) sector (QCD-light) has two mass scales M(GeV)

QCD in the light quark (up & down) sector (QCD-light) has two mass scales M(GeV) QCD in the light quark (up & down) sector (QCD-light) has two mass scales M(GeV) 1 m N m ρ Λ QCD 0 m π m u,d In a generic physical system, there are often many scales involved. However, for a specific

More information

STANDARD MODEL and BEYOND: SUCCESSES and FAILURES of QFT. (Two lectures)

STANDARD MODEL and BEYOND: SUCCESSES and FAILURES of QFT. (Two lectures) STANDARD MODEL and BEYOND: SUCCESSES and FAILURES of QFT (Two lectures) Lecture 1: Mass scales in particle physics - naturalness in QFT Lecture 2: Renormalisable or non-renormalisable effective electroweak

More information

Weak interactions, parity, helicity

Weak interactions, parity, helicity Lecture 10 Weak interactions, parity, helicity SS2011: Introduction to Nuclear and Particle Physics, Part 2 2 1 Weak decay of particles The weak interaction is also responsible for the β + -decay of atomic

More information

INTRODUCTION TO THE STANDARD MODEL OF PARTICLE PHYSICS

INTRODUCTION TO THE STANDARD MODEL OF PARTICLE PHYSICS INTRODUCTION TO THE STANDARD MODEL OF PARTICLE PHYSICS Class Mechanics My office (for now): Dantziger B Room 121 My Phone: x85200 Office hours: Call ahead, or better yet, email... Even better than office

More information

Gauge Theories of the Standard Model

Gauge Theories of the Standard Model Gauge Theories of the Standard Model Professors: Domènec Espriu (50%, coordinador) Jorge Casalderrey (25%) Federico Mescia (25%) Time Schedule: Mon, Tue, Wed: 11:50 13:10 According to our current state

More information

Isospin. K.K. Gan L5: Isospin and Parity 1

Isospin. K.K. Gan L5: Isospin and Parity 1 Isospin Isospin is a continuous symmetry invented by Heisenberg: Explain the observation that the strong interaction does not distinguish between neutron and proton. Example: the mass difference between

More information

Parity violation. no left-handed ν$ are produced

Parity violation. no left-handed ν$ are produced Parity violation Wu experiment: b decay of polarized nuclei of Cobalt: Co (spin 5) decays to Ni (spin 4), electron and anti-neutrino (spin ½) Parity changes the helicity (H). Ø P-conservation assumes a

More information

Paul Langacker. The Standard Model and Beyond, Second Edition

Paul Langacker. The Standard Model and Beyond, Second Edition Paul Langacker The Standard Model and Beyond, Second Edition Contents Preface xi Chapter 1 Notation and Conventions 1 1.1 PROBLEMS 5 Chapter 2 Review of Perturbative Field Theory 7 2.1 CREATION AND ANNIHILATION

More information

4. The Standard Model

4. The Standard Model 4. The Standard Model Particle and Nuclear Physics Dr. Tina Potter Dr. Tina Potter 4. The Standard Model 1 In this section... Standard Model particle content Klein-Gordon equation Antimatter Interaction

More information

Introduction to particle physics Lecture 6

Introduction to particle physics Lecture 6 Introduction to particle physics Lecture 6 Frank Krauss IPPP Durham U Durham, Epiphany term 2009 Outline 1 Fermi s theory, once more 2 From effective to full theory: Weak gauge bosons 3 Massive gauge bosons:

More information

Hadron Physics & Quantum Chromodynamics Adnan Bashir, IFM, UMSNH, Mexico August 2013 Hermosillo Sonora

Hadron Physics & Quantum Chromodynamics Adnan Bashir, IFM, UMSNH, Mexico August 2013 Hermosillo Sonora Hadron Physics & Quantum Chromodynamics Adnan Bashir, IFM, UMSNH, Mexico August 2013 Hermosillo Sonora Hadron Physics & QCD Part 1: First Encounter With Hadrons: Introduction to Mesons & Baryons, The Quark

More information

Particle Physics Lecture 1 : Introduction Fall 2015 Seon-Hee Seo

Particle Physics Lecture 1 : Introduction Fall 2015 Seon-Hee Seo Particle Physics Lecture 1 : Introduction Fall 2015 Seon-Hee Seo Particle Physics Fall 2015 1 Course Overview Lecture 1: Introduction, Decay Rates and Cross Sections Lecture 2: The Dirac Equation and Spin

More information

Particle Physics. Dr Victoria Martin, Spring Semester 2012 Lecture 1: The Mysteries of Particle Physics, or Why should I take this course?

Particle Physics. Dr Victoria Martin, Spring Semester 2012 Lecture 1: The Mysteries of Particle Physics, or Why should I take this course? Particle Physics Dr Victoria Martin, Spring Semester 2012 Lecture 1: The Mysteries of Particle Physics, or Why should I take this course? Contents: Review of the Standard Model! What we know! What we don

More information

Fundamental Symmetries - l

Fundamental Symmetries - l National Nuclear Physics Summer School MIT, Cambridge, MA July 18-29 2016 Fundamental Symmetries - l Vincenzo Cirigliano Los Alamos National Laboratory Goal of these lectures Introduce the field of nuclear

More information

Part I. Many-Body Systems and Classical Field Theory

Part I. Many-Body Systems and Classical Field Theory Part I. Many-Body Systems and Classical Field Theory 1. Classical and Quantum Mechanics of Particle Systems 3 1.1 Introduction. 3 1.2 Classical Mechanics of Mass Points 4 1.3 Quantum Mechanics: The Harmonic

More information

Fundamentals of Neutrino Physics and Astrophysics

Fundamentals of Neutrino Physics and Astrophysics Fundamentals of Neutrino Physics and Astrophysics Carlo Giunti Istituto Nazionale di Fisica Nucleare, Sezione di Torino and Dipartimento di Fisica Teorica, Universita di Torino, Italy Chung W. Kim Korea

More information

Standard Model of Particle Physics SS 2012

Standard Model of Particle Physics SS 2012 Lecture: Standard Model of Particle Physics Heidelberg SS 22 Fermi Theory Standard Model of Particle Physics SS 22 2 Standard Model of Particle Physics SS 22 Fermi Theory Unified description of all kind

More information

Organisatorial Issues: Exam

Organisatorial Issues: Exam Organisatorial Issues: Exam Date: - current date: Tuesday 24.07.2012-14:00 16:00h, gr. HS - alternative option to be discussed: - Tuesday 24.07.2012-13:00 15:00h, gr. HS - Friday 27.07.2012-14:00 16:00h,

More information

Introduction to particle physics Lecture 12: Weak interactions

Introduction to particle physics Lecture 12: Weak interactions Introduction to particle physics Lecture 12: Weak interactions Frank Krauss IPPP Durham U Durham, Epiphany term 2010 1 / 22 Outline 1 Gauge theory of weak interactions 2 Spontaneous symmetry breaking 3

More information

Particle Physics Outline the concepts of particle production and annihilation and apply the conservation laws to these processes.

Particle Physics Outline the concepts of particle production and annihilation and apply the conservation laws to these processes. Particle Physics 12.3.1 Outline the concept of antiparticles and give examples 12.3.2 Outline the concepts of particle production and annihilation and apply the conservation laws to these processes. Every

More information

Particle Physics. All science is either physics or stamp collecting and this from a 1908 Nobel laureate in Chemistry

Particle Physics. All science is either physics or stamp collecting and this from a 1908 Nobel laureate in Chemistry Particle Physics JJ Thompson discovered electrons in 1897 Rutherford discovered the atomic nucleus in 1911 and the proton in 1919 (idea of gold foil expt) All science is either physics or stamp collecting

More information

Overview. The quest of Particle Physics research is to understand the fundamental particles of nature and their interactions.

Overview. The quest of Particle Physics research is to understand the fundamental particles of nature and their interactions. Overview The quest of Particle Physics research is to understand the fundamental particles of nature and their interactions. Our understanding is about to take a giant leap.. the Large Hadron Collider

More information

Standard Model of Particle Physics SS 2013

Standard Model of Particle Physics SS 2013 Lecture: Standard Model of Particle Physics Heidelberg SS 23 Fermi Theory Standard Model of Particle Physics SS 23 2 Standard Model of Particle Physics SS 23 Weak Force Decay of strange particles Nuclear

More information

Physics 129 LECTURE 6 January 23, Particle Physics Symmetries (Perkins Chapter 3)

Physics 129 LECTURE 6 January 23, Particle Physics Symmetries (Perkins Chapter 3) Physics 129 LECTURE 6 January 23, 2014 Particle Physics Symmetries (Perkins Chapter 3) n Lagrangian Deductions n Rotations n Parity n Charge Conjugation Gauge Invariance and Charge Conservation The Higgs

More information

Gian Gopal Particle Attributes Quantum Numbers 1

Gian Gopal Particle Attributes Quantum Numbers 1 Particle Attributes Quantum Numbers Intro Lecture Quantum numbers (Quantised Attributes subject to conservation laws and hence related to Symmetries) listed NOT explained. Now we cover Electric Charge

More information

Derivation of Electro Weak Unification and Final Form of Standard Model with QCD and Gluons 1 W W W 3

Derivation of Electro Weak Unification and Final Form of Standard Model with QCD and Gluons 1 W W W 3 Derivation of Electro Weak Unification and Final Form of Standard Model with QCD and Gluons 1 W 1 + 2 W 2 + 3 W 3 Substitute B = cos W A + sin W Z 0 Sum over first generation particles. up down Left handed

More information

SECOND PUBLIC EXAMINATION. Honour School of Physics Part C: 4 Year Course. Honour School of Physics and Philosophy Part C C4: PARTICLE PHYSICS

SECOND PUBLIC EXAMINATION. Honour School of Physics Part C: 4 Year Course. Honour School of Physics and Philosophy Part C C4: PARTICLE PHYSICS A047W SECOND PUBLIC EXAMINATION Honour School of Physics Part C: 4 Year Course Honour School of Physics and Philosophy Part C C4: PARTICLE PHYSICS TRINITY TERM 05 Thursday, 8 June,.30 pm 5.45 pm 5 minutes

More information

DEEP INELASTIC SCATTERING

DEEP INELASTIC SCATTERING DEEP INELASTIC SCATTERING Electron scattering off nucleons (Fig 7.1): 1) Elastic scattering: E = E (θ) 2) Inelastic scattering: No 1-to-1 relationship between E and θ Inelastic scattering: nucleon gets

More information

Flavour physics Lecture 1

Flavour physics Lecture 1 Flavour physics Lecture 1 Jim Libby (IITM) XI th SERC school on EHEP NISER Bhubaneswar November 2017 Lecture 1 1 Outline What is flavour physics? Some theory and history CKM matrix Lecture 1 2 What is

More information

Maxwell s equations. based on S-54. electric field charge density. current density

Maxwell s equations. based on S-54. electric field charge density. current density Maxwell s equations based on S-54 Our next task is to find a quantum field theory description of spin-1 particles, e.g. photons. Classical electrodynamics is governed by Maxwell s equations: electric field

More information

Maxwell s equations. electric field charge density. current density

Maxwell s equations. electric field charge density. current density Maxwell s equations based on S-54 Our next task is to find a quantum field theory description of spin-1 particles, e.g. photons. Classical electrodynamics is governed by Maxwell s equations: electric field

More information

Kern- und Teilchenphysik II Lecture 1: QCD

Kern- und Teilchenphysik II Lecture 1: QCD Kern- und Teilchenphysik II Lecture 1: QCD (adapted from the Handout of Prof. Mark Thomson) Prof. Nico Serra Dr. Marcin Chrzaszcz Dr. Annapaola De Cosa (guest lecturer) www.physik.uzh.ch/de/lehre/phy213/fs2017.html

More information

IoP Masterclass FLAVOUR PHYSICS. Tim Gershon, University of Warwick April 20 th 2007

IoP Masterclass FLAVOUR PHYSICS. Tim Gershon, University of Warwick April 20 th 2007 IoP Masterclass FLAVOUR PHYSICS Tim Gershon, University of Warwick April 20 th 2007 The Standard Model Tim Gershon, IoP Masterclass, April 20 th 2007 2 Some Questions What is antimatter? Why are there

More information

3.3 Lagrangian and symmetries for a spin- 1 2 field

3.3 Lagrangian and symmetries for a spin- 1 2 field 3.3 Lagrangian and symmetries for a spin- 1 2 field The Lagrangian for the free spin- 1 2 field is The corresponding Hamiltonian density is L = ψ(i/ µ m)ψ. (3.31) H = ψ( γ p + m)ψ. (3.32) The Lagrangian

More information

Nuclear and Particle Physics

Nuclear and Particle Physics Nuclear and Particle Physics W. S. С Williams Department of Physics, University of Oxford and St Edmund Hall, Oxford CLARENDON PRESS OXFORD 1991 Contents 1 Introduction 1.1 Historical perspective 1 1.2

More information

CHAPTER 14 Particle Physics

CHAPTER 14 Particle Physics CHAPTER 14 Particle Physics 14.1 Early Discoveries 14.2 The Fundamental Interactions 14.3 Classification of Particles 14.4 Conservation Laws and Symmetries 14.5 Quarks 14.6 The Families of Matter 14.7

More information

Fundamental Symmetries - 2

Fundamental Symmetries - 2 HUGS 2018 Jefferson Lab, Newport News, VA May 29- June 15 2018 Fundamental Symmetries - 2 Vincenzo Cirigliano Los Alamos National Laboratory Plan of the lectures Review symmetry and symmetry breaking Introduce

More information

Kern- und Teilchenphysik I Lecture 13:Quarks and QCD

Kern- und Teilchenphysik I Lecture 13:Quarks and QCD Kern- und Teilchenphysik I Lecture 13:Quarks and QCD (adapted from the Handout of Prof. Mark Thomson) Prof. Nico Serra Dr. Patrick Owen, Dr. Silva Coutinho http://www.physik.uzh.ch/de/lehre/phy211/hs2016.html

More information

Oddelek za fiziko. Top quark physics. Seminar. Author: Tina Šfiligoj. Mentor: prof. dr. Svjetlana Fajfer. Ljubljana, february 2012

Oddelek za fiziko. Top quark physics. Seminar. Author: Tina Šfiligoj. Mentor: prof. dr. Svjetlana Fajfer. Ljubljana, february 2012 Oddelek za fiziko Top quark physics Seminar Author: Tina Šfiligoj Mentor: prof. dr. Svjetlana Fajfer Ljubljana, february 2012 Abstract Top quark physics is a very active area in particle physics as it

More information

Discrete Transformations: Parity

Discrete Transformations: Parity Phy489 Lecture 8 0 Discrete Transformations: Parity Parity operation inverts the sign of all spatial coordinates: Position vector (x, y, z) goes to (-x, -y, -z) (eg P(r) = -r ) Clearly P 2 = I (so eigenvalues

More information

DISCRETE SYMMETRIES IN NUCLEAR AND PARTICLE PHYSICS. Parity PHYS NUCLEAR AND PARTICLE PHYSICS

DISCRETE SYMMETRIES IN NUCLEAR AND PARTICLE PHYSICS. Parity PHYS NUCLEAR AND PARTICLE PHYSICS PHYS 30121 NUCLEAR AND PARTICLE PHYSICS DISCRETE SYMMETRIES IN NUCLEAR AND PARTICLE PHYSICS Discrete symmetries are ones that do not depend on any continuous parameter. The classic example is reflection

More information

Most of Modern Physics today is concerned with the extremes of matter:

Most of Modern Physics today is concerned with the extremes of matter: Most of Modern Physics today is concerned with the extremes of matter: Very low temperatures, very large numbers of particles, complex systems Æ Condensed Matter Physics Very high temperatures, very large

More information

Option 212: UNIT 2 Elementary Particles

Option 212: UNIT 2 Elementary Particles Department of Physics and Astronomy Option 212: UNIT 2 Elementary Particles SCHEDULE 26-Jan-15 13.00pm LRB Intro lecture 28-Jan-15 12.00pm LRB Problem solving (2-Feb-15 10.00am E Problem Workshop) 4-Feb-15

More information

Quantum Numbers. F. Di Lodovico 1 EPP, SPA6306. Queen Mary University of London. Quantum Numbers. F. Di Lodovico. Quantum Numbers.

Quantum Numbers. F. Di Lodovico 1 EPP, SPA6306. Queen Mary University of London. Quantum Numbers. F. Di Lodovico. Quantum Numbers. 1 1 School of Physics and Astrophysics Queen Mary University of London EPP, SPA6306 Outline : Number Conservation Rules Based on the experimental observation of particle interactions a number of particle

More information

Particle Physics. Lecture 12: Hadron Decays.!Resonances!Heavy Meson and Baryons!Decays and Quantum numbers!ckm matrix

Particle Physics. Lecture 12: Hadron Decays.!Resonances!Heavy Meson and Baryons!Decays and Quantum numbers!ckm matrix Particle Physics Lecture 12: Hadron Decays!Resonances!Heavy Meson and Baryons!Decays and Quantum numbers!ckm matrix 1 From Friday: Mesons and Baryons Summary Quarks are confined to colourless bound states,

More information

The Electro-Strong Interaction

The Electro-Strong Interaction The Electro-Strong Interaction Taking into account the Planck Distribution Law of the electromagnetic oscillators, we can explain the electron/proton mass rate and the Weak and Strong Interactions. Lattice

More information

Most of Modern Physics today is concerned with the extremes of matter:

Most of Modern Physics today is concerned with the extremes of matter: Most of Modern Physics today is concerned with the extremes of matter: Very low temperatures, very large numbers of particles, complex systems Æ Condensed Matter Physics Very high temperatures, very large

More information

Invariance Principles and Conservation Laws

Invariance Principles and Conservation Laws Invariance Principles and Conservation Laws Outline Translation and rotation Parity Charge Conjugation Charge Conservation and Gauge Invariance Baryon and lepton conservation CPT Theorem CP violation and

More information

6. QED. Particle and Nuclear Physics. Dr. Tina Potter. Dr. Tina Potter 6. QED 1

6. QED. Particle and Nuclear Physics. Dr. Tina Potter. Dr. Tina Potter 6. QED 1 6. QED Particle and Nuclear Physics Dr. Tina Potter Dr. Tina Potter 6. QED 1 In this section... Gauge invariance Allowed vertices + examples Scattering Experimental tests Running of alpha Dr. Tina Potter

More information

Week 3: Renormalizable lagrangians and the Standard model lagrangian 1 Reading material from the books

Week 3: Renormalizable lagrangians and the Standard model lagrangian 1 Reading material from the books Week 3: Renormalizable lagrangians and the Standard model lagrangian 1 Reading material from the books Burgess-Moore, Chapter Weiberg, Chapter 5 Donoghue, Golowich, Holstein Chapter 1, 1 Free field Lagrangians

More information

Aula/Lecture 18 Non-Abelian Gauge theories The Higgs Mechanism The Standard Model: Part I

Aula/Lecture 18 Non-Abelian Gauge theories The Higgs Mechanism The Standard Model: Part I Física de Partículas Aula/Lecture 18 Non-Abelian Gauge theories The The : Part I Jorge C. Romão Instituto Superior Técnico, Departamento de Física & CFTP A. Rovisco Pais 1, 1049-001 Lisboa, Portugal 2016

More information

The mass of the Higgs boson

The mass of the Higgs boson The mass of the Higgs boson LHC : Higgs particle observation CMS 2011/12 ATLAS 2011/12 a prediction Higgs boson found standard model Higgs boson T.Plehn, M.Rauch Spontaneous symmetry breaking confirmed

More information

Remainder of Course. 4/22 Standard Model; Strong Interaction 4/24 Standard Model; Weak Interaction 4/27 Course review 5/01 Final Exam, 3:30 5:30 PM

Remainder of Course. 4/22 Standard Model; Strong Interaction 4/24 Standard Model; Weak Interaction 4/27 Course review 5/01 Final Exam, 3:30 5:30 PM Remainder of Course 4/22 Standard Model; Strong Interaction 4/24 Standard Model; Weak Interaction 4/27 Course review 5/01 Final Exam, 3:30 5:30 PM Practice Final on Course Web Page See HW #12 (not to be

More information

May 7, Physics Beyond the Standard Model. Francesco Fucito. Introduction. Standard. Model- Boson Sector. Standard. Model- Fermion Sector

May 7, Physics Beyond the Standard Model. Francesco Fucito. Introduction. Standard. Model- Boson Sector. Standard. Model- Fermion Sector - Boson - May 7, 2017 - Boson - The standard model of particle physics is the state of the art in quantum field theory All the knowledge we have developed so far in this field enters in its definition:

More information

STUDY OF HIGGS EFFECTIVE COUPLINGS AT ep COLLIDERS

STUDY OF HIGGS EFFECTIVE COUPLINGS AT ep COLLIDERS STUDY OF HIGGS EFFECTIVE COUPLINGS AT ep COLLIDERS HODA HESARI SCHOOL OF PARTICLES AND ACCELERATORS, INSTITUTE FOR RESEARCH IN FUNDAMENTAL SCIENCES (IPM) The LHeC is a proposed deep inelastic electron-nucleon

More information

The Proton Radius Puzzle and the Electro-Strong Interaction

The Proton Radius Puzzle and the Electro-Strong Interaction The Proton Radius Puzzle and the Electro-Strong Interaction The resolution of the Proton Radius Puzzle is the diffraction pattern, giving another wavelength in case of muonic hydrogen oscillation for the

More information