t b e - d -1/3 4/18/2016 Particle Classification 3 Generations of Leptons and Quarks Standard Model
|
|
- Michael Nicholson
- 5 years ago
- Views:
Transcription
1 PHYS 342 Moern Physics Elementary Particles an Stanar Moel II Toay's Contents: a) Particle Collier b) Stanar Moel of Elementary Particles c) Fiel Bosons: qantization of for basic forces ) Higgs Boson: origin of mass e) Leptons an Qarks: fnamental material particles f) Mesons an Baryons: composite material particles g) Conservation Laws in particle physics h) Energy an Momentm in particle collision i) Particle Physics beyon Stanar Moel Particle Classification Harons are NOT elementary particles, an they are composite particles mae p by qarks. mesons are bosons an harons. baryons are fermions an harons. Stanar Moel 3 Generations of Leptons an Qarks the fnamental biling blocks of matter 1 st generation 2 n generation 3 r generation e e - +2/3 - +2/3 +2/3 c s -1-1/3-1/ Orinary matter Cosmic rays Accelerators t b -1/3 Leptons an Qarks have three generations: from low energy to high energy 1
2 Leptons an Qarks: spin-1/2 Fermions Qark Mass 3 generations are similar in everything bt the mass Mass 1 (GeV) E= mc 2 1 proton mass ~ 1GeV (1-27 Kg) Qarks Up Down Strange Charm Bottom Top GeV The mass grows larger in each sccessive family Top (iscovere 1995) Antiparticles for Leptons an Qarks Orinary Matter For every fnamental particle of matter, there is an anti-particle with same mass an properties bt opposite charge Matter e e /3-1/3 Anti-Matter e +1 e + positron -2/3 +1/3 Bar on top to inicate anti-particle Corresponent anti-particles exist for all three generations All anti-particles have been proce sing accelerators Leptons: netrino e = electron charge e e /3-1/3 Qarks: = p = own All stable(natral) matter aron s can be escribe sing first generation: electrons, netrinos, an qarks 2
3 Orinary Matter: Netrino Is the orinary niverse mae only of qarks an electrons? Electron, proton an netrons are rarities! For each of them in the Universe there is 1 billion netrinos Netrinos are the most abnant matter-particles in the Universe! Within each cm 3 of space: ~3 netrinos from Big Bang 1 cm 1 cm Netrinos are everywhere! in the oter space, on Earth, in or boies.. Orinary Matter: Netrino ner the Sn Every cm 2 of Earth srface is crosse every secon by more than 1 billion (1 1 ) netrinos proce in the Sn 14 netrinos per secon from Sn are zipping throgh yo No worries! Netrinos o not harm s. Or boies are transparent to netrinos Within yor boy at any instant: roghly 3 million netrinos from the Big Bang Orinary Matter: proton an netron Qarks have fractional electric charge! electric charge + 2/3 electric charge 1/3 proton (charge +1) netron (charge ) Qark Colors All qark flavors come in 3 versions, calle colors p own +2/3-1/3 Qarks combine together to form colorless particles -Baryons (three qarks: re+ green + ble = white) proton p Strong forces gle qarks together in bon states p n Mesons (qark-antiqark pair) sch as re + anti-re -bar state pion 3
4 Qarks have more qantm nmbers Qarks bil colorless Meson or Baryons Charge, Spin, Color Also: Baryon, Charm, Strangeness, Topness, Bottomness (like spin an charge, they are intrinsic properties!) c c J/ b b Y B mesons (bq) b b B - B + b b B B Many more mesons an baryons More Mesons More Baryons 4
5 "Yong man, if I col remember the names of these particles, I wol have been a botanist! E.Fermi to his stent L. Leerman (both Nobel lareates) The Particle Physicist s Bible: Particle Data Book Most particles are not stable an can ecay to lighter particles.. Conservation Laws in Particle Physics 1) Conservation of Energy 2) Conservation of Linear Momentm 3) Conservation of Anglar Momentm 4) Conservation of Electric Charge 5) Conservation of Ncleon Nmber 5) Conservation of Lepton Nmber 6) Conservation of Baryon Nmber 7) Conservation of Flavor Nmber (Flavoers incling Charm, Strangeness, Topness, Bottomness) 8) Conservation of some symmetries (charge-time-parity.) Nclear Reaction Energy an Momentm in particle collision 1) release energy is efine as the ifference of the rest mass between the initial particles an the particles proce after collision. ) 2) The release energy is share as kinetic energy of the particles proce after collision. Beyon the Stanar Moel 3) Relativistic Treatment is Manatory in particle physics 5
6 One Theory for the whole Universe GRAVITY UNIFIED FORCE? ELECTRO- MAGNETIC STRONG WEAK Looking for a simple elegant nifie theory ICP 42 the last one ICP 42: What is the maximm kinetic energy of the positron emitte in the ecay of a rest antimon? Step : Accoring to what yo have learne, what is the rest energy of netrino approximately? An what is the relation between netrino energy an its momentm. Step1: What is the release energy Q of the ecay? Step2: What oes this release energy convert to? Step3: To make the positron have the maximm kinetic energy, how o the netrinos move an how mch energy o the netrinos carry? (Can netrino takes zero energy? Why?) Step4: Accoring step 3, yo have two eqations. What are the two eqations? Step5: From the two eqations, get the maximm kinetic energy of the positron. Bt enless physics avances 36 people,13 teams, loss one! Monay: 1. Ulazimir Kasacheski, Jonathan Brown, an Vishal Patel, interview researchers at IUPUI 2. Lif Wang, Weiyan Deng, an Yfeng Zhang, Moern Experiments to Test Special Relativity 3. Stevie Bastin, Stjepan Kraljic, Zack Rowe, Gravitational wave/gravitons 4. Hongkn Zh, Giming Chen, an Jiawen Wang, First gravitational wave observation 5. Chanyi Chen, Zihao F, an Lingbin Meng, Introction to General Relativity 6. Chase Howar an Alex Canner, Gravitational lensing Wenesay: 7. Zongying X, Zheng Hang, an Jiani Xie, Blackboy Raiation 8. Dalton Eaton, Robert McKay, an Gy Wiss, Monte Carlo Simlation of Schroinger eqation 9. Aaron Boehm, Joseph Sorco, an Will Simms, Atomic physics explanation of helim laser 1. Josiah Alstott, Thomas Freestone, an Ross Wallgren, Atomic clock 11. Kailiang Chen, Zhong Jin, Peiming Zh, Qantm Information 12. Tianyang W, Haizhen Xie, an Bingcheng Zho, Netrino physics 13. Ryan, Particle Accelerator LHC 6
The projects that have been chosen so far include 36 people,13 teams. So far, So Good, expect 2/3 get >=B+
PHYS 342 Modern Physics Project Discussion III Today's Projects for Discussion: a) Study a particle accelerators Large Hadron Collider (LHC) b) Search for Dark Matter The projects that have been chosen
More informationParticles and fields. Today: Review Particle Physics. Question. Quantum Electrodynamics: QED. Electrons and photons
Exam 4: Fri. May 10, in-class 20 qestions, covers fission, fsion, particle physics No final exam. Essays retrne Friay Toay: Review Particle Physics Particles an fiels: a new pictre Qarks an leptons The
More informationOverview of particle physics
Overview of particle physics The big qestions of particle physics are 1. What is the niverse mae of? 2. How is it hel together? We can start at orinary istances an work or way own. Macroscopic stff is
More informationChapter 17. Weak Interactions
Chapter 17 Weak Interactions The weak interactions are meiate by W ± or (netral) Z exchange. In the case of W ±, this means that the flavors of the qarks interacting with the gage boson can change. W ±
More informationParticles as fields. Review Chap. 18: Particle Physics. Energy uncertainty. Quantum Electrodynamics: QED. Creating more particles
Final Exam: Thr. Dec. 21, 2:45-4:45 pm, 113 Psycholoy Bilin Exam is cmlative, coverin all material Review Chap. 18: Particle Physics an fiels: a new pictre Qarks an leptons The stron an weak interaction
More informationQUARK WORKBENCH TEACHER NOTES
QUARK WORKBENCH TEACHER NOTES DESCRIPTION Stents se cleverly constrcte pzzle pieces an look for patterns in how those pieces can fit together. The pzzles pieces obey, as mch as possible, the Stanar Moel
More informationSteve Smith Tuition: Physics Notes
Steve Smith Tition: Physics Notes E = mc 2 F = GMm r 2 sin θ m = mλ hν = φ + 1 2 mv2 Particle-opoly! Contents 1 Getting Reay to Play... 3 1.1 e Broglie s Formla..........................................
More informationHadron Structure Theory I. Alexei Prokudin
Haron Strctre Theory I Alexei Prokin The plan: l Lectre I: Strctre of the ncleon l Lectre II Transverse Momentm Depenent istribtions (TMDs) Semi Inclsive Deep Inelastic Scattering (SIDIS) l Ttorial Calclations
More informationmon netrino ν μ ß 0 0 ta fi ta netrino ν fi ß 0 0 Particles have corresponing antiparticles which have the opposite spin an charge. Each of the
LECTURE 13 Elementary Particle Physics (The chart on the classroom wall can be fon at http://www-pg.lbl.gov/cpep/cpep sm large.html.) For Fnamental Forces As far as we know, there are jst for fnamental
More informationParticles and fields. Review Particle Physics. Question. Quantum Electrodynamics: QED. Seeing antiparticles
Final Exam: Mon. May 8, 2:45-4:45 pm, 2241 Cham. Exam is cmlative, coverin all material 40 qestions, 2 note sheets allowe Review Particle Physics Particles an fiels: a new pictre Qarks an leptons The weak
More informationAn Introduction to Particle Physics
An Introduction to Particle Physics The Universe started with a Big Bang The Universe started with a Big Bang What is our Universe made of? Particle physics aims to understand Elementary (fundamental)
More information1 Drawing Feynman Diagrams
1 Drawing Feynman Diagrams 1. A ermion (qark, lepton, netrino) is rawn by a straight line with an arrow pointing to the let: 2. An antiermion is rawn by a straight line with an arrow pointing to the right:
More informationOption 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 informationMatter: it s what you have learned that makes up the world Protons, Neutrons and Electrons
Name The Standard Model of Particle Physics Matter: it s what you have learned that makes up the world Protons, Neutrons and Electrons Just like there is good and evil, matter must have something like
More informationV. Hadron quantum numbers
V. Hadron qantm nmbers Characteristics of a hadron: 1) Mass 2) Qantm nmbers arising from space-time symmetries : total spin J, parity P, charge conjgation C. Common notation: 1 -- + 2 J P (e.g. for proton:
More informationParticle 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 informationVI. The quark model: hadron quantum numbers, resonances
VI. The qark model: hadron qantm nmbers, resonances Characteristics of a hadron: 1) Mass 2) Qantm nmbers arising from space symmetries : J, P, C. Common notation: J P (e.g. for proton: 1 2 --+ ), or J
More informationParticle Physics. Dr M.A. Thomson. ν e. e + W + Z 0 e + e - W - Part II, Lent Term 2004 HANDOUT VI. Dr M.A. Thomson Lent 2004
Particle Physics Dr M.A. Thomson e + W + Z 0 e + q q Part II, Lent Term 2004 HANDOUT VI 2 The Weak Interaction The WEAK interaction acconts for many ecays in particle physics e.g. μ! e νeνμ, fi! e νeνfi,
More informationChapter 32 Lecture Notes
Chapter 32 Lecture Notes Physics 2424 - Strauss Formulas: mc 2 hc/2πd 1. INTRODUCTION What are the most fundamental particles and what are the most fundamental forces that make up the universe? For a brick
More informationElementary Particle Physics Glossary. Course organiser: Dr Marcella Bona February 9, 2016
Elementary Particle Physics Glossary Course organiser: Dr Marcella Bona February 9, 2016 1 Contents 1 Terms A-C 5 1.1 Accelerator.............................. 5 1.2 Annihilation..............................
More informationIllustrations of a Modified Standard Model: Part 1-The Solar Proton- Proton Cycle
Illstrations of a Modified : Part 1-The Solar Proton- Proton Cycle by Roger N. Weller, (proton3@gmail.com), Febrary 23, 2014 Abstract A proposed modification of the, when applied to the Solar Proton-Proton
More informationINTRODUCTION 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 informationOption 212: UNIT 2 Elementary Particles
Department of Physics and Astronomy Option 212: UNIT 2 Elementary Particles SCHEDULE 26-Jan-15 13.pm LRB Intro lecture 28-Jan-15 12.pm LRB Problem solving (2-Feb-15 1.am E Problem Workshop) 4-Feb-15 12.pm
More informationPhysics 4213/5213 Lecture 1
August 28, 2002 1 INTRODUCTION 1 Introduction Physics 4213/5213 Lecture 1 There are four known forces: gravity, electricity and magnetism (E&M), the weak force, and the strong force. Each is responsible
More informationLight flavor asymmetry of polarized quark distributions in thermodynamical bag model
Inian Jornal of Pre & Applie Physics Vol. 5, April 014, pp. 19-3 Light flavor asymmetry of polarize qark istribtions in thermoynamical bag moel K Ganesamrthy a & S Mrganantham b* a Department of Physics,
More informationCosmology and particle physics
Cosmology and particle physics Lecture notes Timm Wrase Lecture 5 The thermal universe - part I In the last lecture we have shown that our very early universe was in a very hot and dense state. During
More informationNuclear and Particle Physics 3: Particle Physics. Lecture 1: Introduction to Particle Physics February 5th 2007
Nuclear and Particle Physics 3: Particle Physics Lecture 1: Introduction to Particle Physics February 5th 2007 Particle Physics (PP) a.k.a. High-Energy Physics (HEP) 1 Dr Victoria Martin JCMB room 4405
More informationParticle 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 informationcgrahamphysics.com Particles that mediate force Book pg Exchange particles
Particles that mediate force Book pg 299-300 Exchange particles Review Baryon number B Total # of baryons must remain constant All baryons have the same number B = 1 (p, n, Λ, Σ, Ξ) All non baryons (leptons
More informationLecture PowerPoint. Chapter 32 Physics: Principles with Applications, 6 th edition Giancoli
Lecture PowerPoint Chapter 32 Physics: Principles with Applications, 6 th edition Giancoli 2005 Pearson Prentice Hall This work is protected by United States copyright laws and is provided solely for the
More informationEssential Physics II. Lecture 14:
Essential Physics II E II Lecture 14: 18-01-16 Last lecture of EP2! Congratulations! This was a hard course. Be proud! Next week s exam Next Monday! All lecture slides on course website: http://astro3.sci.hokudai.ac.jp/~tasker/teaching/ep2
More information1. What does this poster contain?
This poster presents the elementary constituents of matter (the particles) and their interactions, the latter having other particles as intermediaries. These elementary particles are point-like and have
More informationElectron-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 informationLecture 2: The First Second origin of neutrons and protons
Lecture 2: The First Second origin of neutrons and protons Hot Big Bang Expanding and cooling Soup of free particles + anti-particles Symmetry breaking Soup of free quarks Quarks confined into neutrons
More informationChapter 46. Particle Physics and Cosmology
Chapter 46 Particle Physics and Cosmology Atoms as Elementary Particles Atoms From the Greek for indivisible Were once thought to be the elementary particles Atom constituents Proton, neutron, and electron
More informationParticle Physics, Fall 2012 Solutions to Final Exam December 11, 2012
Particle Physics, Fall Solutions to Final Exam December, Part I: Short Answer [ points] For each of the following, give a short answer (- sentences, or a formula). [5 points each]. [This one might be har
More informationFundamental 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 informationNuclear and Particle Physics - Lecture 16 Neutral kaon decays and oscillations
1 Introction Nclear an Particle Phyic - Lectre 16 Netral kaon ecay an ocillation e have alreay een that the netral kaon will have em-leptonic an haronic ecay. However, they alo exhibit the phenomenon of
More informationWhat is matter and how is it formed?
What is matter and how is it formed? Lesson 6: Subatomic Particles Subatomic particles refers to particles that are more "fundamental" than... Are these fundamental particles or are they made up of smaller,
More informationW + W - Z 0. Question. From Last Time. Fundamental Matter Particles. The Standard Model. Carriers of the weak force. Ice Cube
From Last Time Dissse the weak interation All qarks an leptons have a weak harge They interat throgh the weak interation Weak interation often swampe y eletromagneti or strong interation. Interation with
More informationSaturday Morning Physics -- Texas A&M University. What is Matter and what holds it together? Dr. Rainer J. Fries. January 27, 2007
Saturday Morning Physics -- Texas A&M University Particles and Forces What is Matter and what holds it together? Dr. Rainer J. Fries January 27, 2007 Zooming in on the World around us Particles and Forces
More informationSaturday Morning Physics -- Texas A&M University Dr. Rainer J. Fries
Saturday Morning Physics -- Texas A&M University Particles and Forces What is Matter and what holds it together? Dr. Rainer J. Fries January 27, 2007 Zooming in on the World around us Particles and Forces
More informationThe God particle at last? Astronomy Ireland, Oct 8 th, 2012
The God particle at last? Astronomy Ireland, Oct 8 th, 2012 Cormac O Raifeartaigh Waterford Institute of Technology CERN July 4 th 2012 (ATLAS and CMS ) A new particle of mass 125 GeV I The Higgs boson
More informationThe God particle at last? Science Week, Nov 15 th, 2012
The God particle at last? Science Week, Nov 15 th, 2012 Cormac O Raifeartaigh Waterford Institute of Technology CERN July 4 th 2012 (ATLAS and CMS ) A new particle of mass 125 GeV Why is the Higgs particle
More informationWeak Interactions. The Theory of GLASHOW, SALAM and WEINBERG
Weak Interactions The Theory of GLASHOW, SALAM and WEINBERG ~ 1959-1968 (Nobel 1979) Theory of the unified weak and electromagnetic interaction, transmitted by exchange of intermediate vector bosons mass
More informationKatsushi Arisaka University of California, Los Angeles Department of Physics and Astronomy
11/14/12 Katsushi Arisaka 1 Katsushi Arisaka University of California, Los Angeles Department of Physics and Astronomy arisaka@physics.ucla.edu Seven Phases of Cosmic Evolution 11/14/12 Katsushi Arisaka
More informationQuantum Numbers. Elementary Particles Properties. F. Di Lodovico c 1 EPP, SPA6306. Queen Mary University of London. Quantum Numbers. F.
Elementary Properties 1 1 School of Physics and Astrophysics Queen Mary University of London EPP, SPA6306 Outline Most stable sub-atomic particles are the proton, neutron (nucleons) and electron. Study
More informationParticle physics: what is the world made of?
Particle physics: what is the world made of? From our experience from chemistry has told us about: Name Mass (kg) Mass (atomic mass units) Decreasing mass Neutron Proton Electron Previous lecture on stellar
More informationChapter 3. Building Hadrons from Quarks
P570 Chapter Bilding Hadrons from Qarks Mesons in SU() We are now ready to consider mesons and baryons constrcted from qarks. As we recall, mesons are made of qark-antiqark pair and baryons are made of
More informationMost 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 informationMost 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 informationFundamental Particles
Fundamental Particles Standard Model of Particle Physics There are three different kinds of particles. Leptons - there are charged leptons (e -, μ -, τ - ) and uncharged leptons (νe, νμ, ντ) and their
More informationSome fundamental questions
Some fundamental questions What is the standard model of elementary particles and their interactions? What is the origin of mass and electroweak symmetry breaking? What is the role of anti-matter in Nature?
More informationPar$cles. Ma#er is made of atoms. Atoms are made of leptons and quarks. Leptons. Quarks. atom nucleus nucleon quark m m m m
Par$cles Ma#er is made of atoms atom nucleus nucleon quark 10-10 m 10-14 m 10-15 m 10-18 m Atoms are made of leptons and quarks Leptons ν e e Quarks u d What Have We Learned? Rela?vis?c Quantum Mechanics
More informationL23/24, part 1: let s end up with the story of relativity
L23/24, part 1: let s end up with the story of relativity Special relativity showed that space and time are not absolute Instead they are inextricably linked in a fourdimensional combination called spacetime
More informationI. Antoniadis CERN. IAS CERN Novice Workshop, NTU, 7 Feb 2014
I. Antoniadis CERN IAS CERN Novice Workshop, NTU, 7 Feb 2014 1 2 3 the Large Hadron Collider (LHC) Largest scientific instrument ever built, 27km of circumference >10 000 people involved in its design
More informationConstraints on fourth generation Majorana neutrinos
Jornal of Physics: Conference Series Constraints on forth generation Majorana netrinos To cite this article: Alexaner Lenz et al 2010 J. Phys.: Conf. Ser. 259 012096 Relate content - Lepton nmber, black
More informationElementary particles, forces and Feynman diagrams
Elementary particles, forces and Feynman diagrams Particles & Forces quarks Charged leptons (e,µ,τ) Neutral leptons (ν) Strong Y N N Electro Magnetic Y Y N Weak Y Y Y Quarks carry strong, weak & EM charge!!!!!
More informationDEVIL PHYSICS THE BADDEST CLASS ON CAMPUS IB PHYSICS
DEVIL PHYSICS THE BADDEST CLASS ON CAMPUS IB PHYSICS LSN 7-3: THE STRUCTURE OF MATTER Questions From Reading Activity? Essential Idea: It is believed that all the matter around us is made up of fundamental
More informationElectroweak Pion decay in the Bethe-Salpeter approach
Electroweak Pion ecay in the Bethe-Salpeter approach Wali Ahme Mian in collaboration with Axel Maas an Helios Sanchis-Alepz Bon states in QCD an beyon St. Goar Feb. 20th-23th, 2017 W. A. Mian Electroweak
More informationDemocritus, a fifth century B.C. philosopher, is credited with being the first
This paper will give a general overview of the current thoughts on the building blocks of atoms through the scope of the Standard Model. There will be an abridged explanation of the interactions that these
More informationIntro to Particle Physics and The Standard Model. Robert Clare UCR
Intro to Particle Physics and The Standard Model Robert Clare UCR Timeline of particle physics Ancient Greeks Rutherford 1911 Rutherford Chadwick Heisenberg 1930 s Hofstader Gell-Mann Ne eman 1960 s Timeline
More informationPHYSICS 489/1489 LECTURE 16: WEAK INTERACTION OF HADRONS
PHYSICS 489/1489 LECTURE 16: WEAK INTERACTION OF HADRONS ANNOUNCEMENTS Problem Set 3 e on Friay 1700 No cla next Teay No office hor Monay, Teay Sorry! Pleae feel free to en me email abot qetion, etc. or
More informationModern physics 1 Chapter 13
Modern physics 1 Chapter 13 13. Particle physics Particle studied within the ATLAS-project CERN In the beginning of 1930, it seemed that all the physics fundaments was placed within the new areas of elementary
More informationPost-Sphaleron Baryogenesis and n n Oscillations. K.S. Babu
Post-Sphaleron Baryogenesis an n n Oscillations K.S. Bab Oklahoma State University INT Workshop on Netron-Antinetron Oscillations University of Washington, Seattle October 23 27, 2017 Base on: K. S. Bab,
More informationThe ATLAS Experiment and the CERN Large Hadron Collider
The ATLAS Experiment and the CERN Large Hadron Collider HEP101-2 April 5, 2010 A. T. Goshaw Duke University 1 HEP 101 Plan March 29: Introduction and basic HEP terminology March 30: Special LHC event:
More informationToday. The nature of the Universe - Beyond the Standard Model
Today The nature of the Universe - Beyond the Standard Model Dark Matter and Dark Energy String Theory and the quest to unify gravity and quantum theory Begin watching PBS NOVA special The Elegant Universe
More informationToday. The goals of science. The nature of the Universe - Beyond the Standard Model
Today The nature of the Universe - Beyond the Standard Model Dark Matter and Dark Energy String Theory and the quest to unify gravity and quantum theory Begin watching PBS NOVA special The Elegant Universe
More informationThe Uncertainty Principle and the Quarks
The Uncertainty Principle and the Quarks Andrei Gritsan Johns Hopkins University August, 2007 JHU Quarknet Meeting Outline The Uncertainty Principle quantum mechanics with elementary particles The Quarks
More informationPhys 102 Lecture 28 Life, the universe, and everything
Phys 102 Lecture 28 Life, the universe, and everything 1 Today we will... Learn about the building blocks of matter & fundamental forces Quarks and leptons Exchange particle ( gauge bosons ) Learn about
More information2007 Section A of examination problems on Nuclei and Particles
2007 Section A of examination problems on Nuclei and Particles 1 Section A 2 PHYS3002W1 A1. A fossil containing 1 gramme of carbon has a radioactivity of 0.03 disintegrations per second. A living organism
More informationNew Concept of Magnetic Monopoles
New Concept of Magnetic Monopoles Ilgaitis Prūsis 1, Peteris Prūsis 2 Abstract All attempts to find Dirac magnetic monopoles have remained unsuccessful until now. Only quasi particles with characteristics
More informationPossible holographic universe, graviton rest mass, mass gap and dark energy
JJJPL report 0423-2 (2015); vixra:1508.0292 (2015). Possible holographic niverse, graviton rest mass, mass gap and dark energy Jae-Kwang Hwang JJJ Physics Laboratory, 1077 Beech Tree Lane, Brentwood, TN
More informationQuantum 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 informationChapter 22: Cosmology - Back to the Beginning of Time
Chapter 22: Cosmology - Back to the Beginning of Time Expansion of Universe implies dense, hot start: Big Bang Future of universe depends on the total amount of dark and normal matter Amount of matter
More informationA Brief History of Modern Physics
A Brief History of Modern Physics Modern Physics rests on two pillars: 1. Theory of Relativity (Einstein) Special Relativity 1905 General Relativity 1915 nature of space and time (phenomena at high speed)
More informationComplementing the Lagrangian Density of the E. M. Field and the Surface Integral of the p-v Vector Product
Applie Mathematics,,, 5-9 oi:.436/am..4 Pblishe Online Febrary (http://www.scirp.org/jornal/am) Complementing the Lagrangian Density of the E. M. Fiel an the Srface Integral of the p- Vector Proct Abstract
More informationIntroduction to Particle Physics and the Standard Model. Robert Clare UCR
Introduction to Particle Physics and the Standard Model Robert Clare UCR Timeline of particle physics Ancient Greeks Rutherford 1911 Rutherford Chadwick Heisenberg 1930 s Hofstader Gell-Mann Ne eman 1960
More informationCosmic rays. l Some come from the sun (relatively low energy) and some from catastrophic events elsewhere in the galaxy/universe
Special relativity The laws of physics are the same in all coordinate systems either at rest or moving at constant speed with respect to one another The speed of light in a vacm has the same vale regardless
More informationWeak 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 informationPHYS 3446 Lecture #17
PHY 3446 Lecture #7 Monday, Nov. 6, 26 Dr.. Elementary Particle Properties Quantum Numbers trangeness Isospin Gell-Mann-Nishijima Relations Production and Decay of Resonances Monday, Nov. 6, 26 PHY 3446,
More informationCHAPTER 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 informationParticle Physics (concise summary) QuarkNet summer workshop June 24-28, 2013
Particle Physics (concise summary) QuarkNet summer workshop June 24-28, 2013 1 Matter Particles Quarks: Leptons: Anti-matter Particles Anti-quarks: Anti-leptons: Hadrons Stable bound states of quarks Baryons:
More informationEinige interessante Aspekte der in der Zielsetzung genannten Fragestellungen. Appetithappen -> Antworten spaeter in der Vorlesung.
0. Einführung Einige interessante Aspekte der in der Zielsetzung genannten Fragestellungen. Appetithappen -> Antworten spaeter in der Vorlesung. Folien auf Englisch (aus anderer Vorlesung ausgeliehen)
More information.! " # e " + $ e. have the same spin as electron neutrinos, and is ½ integer (fermions).
Conservation Laws For every conservation of some quantity, this is equivalent to an invariance under some transformation. Invariance under space displacement leads to (and from) conservation of linear
More informationEpisode 535: Particle reactions
Episode 535: Particle reactions This episode considers both hadrons and leptons in particle reactions. Students must take account of both conservation of lepton number and conservation of baryon number.
More informationA Theory of Dark Matter
DOI c Inian Acaemy of Sciences A Theory of Dark Matter JAIDEV B. PARMAR Abstract. A moel of the Universe is constrcte an a nmber of problems in Contemporary physics like Baryon Asymmetry, Dark Matter,
More informationLecture 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 informationThe Dark Side of the Higgs Field and General Relativity
The Dark Side of the Higgs Field and General Relativity The gravitational force attracting the matter, causing concentration of the matter in a small space and leaving much space with low matter concentration:
More informationFUNDAMENTAL PARTICLES CLASSIFICATION! BOSONS! QUARKS! FERMIONS! Gauge Bosons! Fermions! Strange and Charm! Top and Bottom! Up and Down!
FUNDAMENTAL PARTICLES CLASSIFICATION! BOSONS! --Bosons are generally associated with radiation and are sometimes! characterized as force carrier particles.! Quarks! Fermions! Leptons! (protons, neutrons)!
More informationChemical Engineering 412
Chemical Engineering 412 Introductory Nuclear Engineering Introduction 1 Spiritual Thought 2 The sweetest experience I know in life is to feel a prompting and act upon it and later find out that it was
More informationOverview. 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 informationTwo questions from the exam
Two qestions from the exam 3. When the sn is located near one of the horizons, an observer looking at the sky directly overhead will view partially polarized light. This effect is de to which of the following
More informationFYS3510 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 informationBeyond the standard model? From last time. What does the SM say? Grand Unified Theories. Unifications: now and the future
From last time Quantum field theory is a relativistic quantum theory of fields and interactions. Fermions make up matter, and bosons mediate the forces by particle exchange. Lots of particles, lots of
More informationIoP Masterclass B PHYSICS. Tim Gershon University of Warwick March 18 th 2009
IoP Masterclass B PHYSICS Tim Gershon University of Warwick March 18 th 2009 The Standard Model 2 Some Questions What is antimatter? Why are there three colours of quarks? Why are there so many bosons?
More informationLecture 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 informationEvidence for a fourth quark from weak interaction-the GIM mechanism
Evience for a fourth quark from weak interaction-the GIM mechanism Haris Ðapo November 01 2007 Outline 1 Motivation 2 Before charm 3 Charm 4 After charm 5 Conclusions hat o we want to achieve? Electroweak
More informationThe 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 informationA Tour of the Standard Model of Elementary Particles and Fields
A Tour of the Standard Model of Elementary Particles and Fields What Do We Know About the Fundamental Structure of Nature and How Do We Know It? Dr. Michael G. Strauss The University of Oklahoma Elementary
More information