The Stranger the Better

Slides:



Advertisements
Similar presentations
1.1b Particles & Radiation Quarks & Leptons
Advertisements

Quarks come in six different types, with six antipartners. On the A-level syllabus, you need to know about three: up, and down (which make up everyday.
PARTICLE PHYSICS. INTRODUCTION The recorded tracks of sub atomic particles resulting from the collision of two protons in the ATLAS experiment at the.
Garfield Graphics included with kind permission from PAWS Inc. All Rights Reserved. Strange Particles AS level Notes.
 Seeing Interactions Drawing Feynman Diagrams. Feynman Diagrams Richard Feynman created a pictorial representation of particle interactions which now.
Charge conservation: is the principle that electric charge can neither be created nor destroyed. The quantity of electric charge, the amount of positive.
Option 212: UNIT 2 Elementary Particles Department of Physics and Astronomy SCHEDULE 3-Feb pm Physics LRA Dr Matt Burleigh Intro lecture 7-Feb-05.
Elementary particles atom Hadrons Leptons Baryons Mesons Nucleons
The Particle Zoo. Too Many Particles Far from just finding Protons Neutrons Electrons Neutrinos and their antiparticles, during the 20 th century many.
Particle Physics Revision The Whole Lot. Announcements Physics revision tonight. Room C56 tomorrow morning. Mock Exams next Wednesday. Potential Divider.
Elementary Particles: Physical Principles Benjamin Schumacher Physics April 2002.
1 Conservation Kihyeon Cho April 5, 2011 HEP. What is the world made of? What holds the world together? Where did we come from? the smallest things in.
Option 212: UNIT 2 Elementary Particles Department of Physics and Astronomy SCHEDULE 26-Jan pm LRB Intro lecture 28-Jan pm LRBProblem solving.
PARTICLE PHYSICS Particles and Interactions. Classifying Particles Most particles fall broadly into two types which can then be broken down further The.
Aim: How can we explain the four fundamental forces and the standard model? Do Now: List all the subatomic particles that you can think of.
Particles and how they interact
Introduction to QED Quantum Electrodynamics Part IV.
© John Parkinson 1 e+e+ e-e- ANNIHILATION © John Parkinson 2 Atom 1x m n n n n Nucleus 1x m U Quarks 1x m U D ? ? ?
Subatomic Particles Lesson 10. Objectives describe the modern model of the proton and neutron as being composed of quarks. compare and contrast the up.
Classification of the Elementary Particles
[Secs 16.1 Dunlap] Conservation Laws - II [Secs 2.2, 2.3, 16.4, 16.5 Dunlap]
Feynman Diagrams Richard Feynman invented the concept of virtual photons as part of his theory of quantum electrodynamics. The maths is complicated – but,
The Particle Zoo Particle Physics Lesson 6. What are the charges? γ (photon) γ (photon) p (proton) p (proton) n (neutron) n (neutron) ν (neutrino) ν (neutrino)
Goal: To enjoy particle physics Objectives: Quarks, neutrinos, and Leptons – Oh my!
What makes up the nucleus? Nucleus is positively charged Different atoms have same electrical properties but different masses Isotopes – same atomic number,
The Theory of (Almost) Everything Standard Model.
Particle Physics "three quarks for Muster Mark" -James Joyce (Finnegan’s Wake) Contents: Particle Accelerators Quantum Electrodynamics and Feynman diagrams.
M. Cobal, PIF 2006/7 Quarks. Quarks are s = ½ fermions, subject to all kind of interactions. They have fractional electric charges Quarks and their bound.
10/29/2007Julia VelkovskaPHY 340a Lecture 4: Last time we talked about deep- inelastic scattering and the evidence of quarks Next time we will talk about.
7.3 The Structure of Matter
Units of E are typically eV and units of λ are typically nm Units of E are typically eV and units of λ are typically nm. Using the hc = 1240.
Particle Interactions
Standard Model for Sub-atomic Particles
Lecture 7 Parity Charge conjugation G-parity CP FK7003.
The Standard Model of Particle Physics
Particle Physics Lesson 6
Today’s plan Collect homework QCD leftovers Weak Interaction.
The Standard Model.
Developments of the quark model
Unit 7.3 Review.
The Standard Model strong nuclear force electromagnetic force
Particle Placemat.
Particle Physics.
PHL424: Feynman diagrams 1. In this case a neutron decays to a proton, an electron and an anti-neutrino via the weak interaction.
Advanced Topics Nuclear Physics ElementaryParticles General Relativity
The Mysterious Nucleus
Search for Order Ancient Greeks: Aristotle Earth Air Fire Water
The Quarks Inside Baryons
Particle Physics what do we know?
The Mysterious Nucleus
Particle Physics Part 1 -James Joyce Contents: Particle Accelerators
PHYS 663 Advanced Particles Physics
Particle physics.
Elementary Particles.
The Top Quark Discovery
A –Level Physics: Nuclear Physics Quarks
ELEMENTARY PARTICLES.
Do Now An electron in a hydrogen atoms drops from n=5 to n=4 energy level. What is the energy of the photon in eV? What is the frequency of the emitted.
More leptons.
Quarks Remember the family of ordinary matter consists of only 4 particles, (not counting their antiparticles) quark u d lepton (electron) e Lepton (electron.
Particle Physics Part 2 -James Joyce Contents: Conservation Laws
Particle Physics Lesson 6
Fundamental Particles
Atomic Structure Basic and Beyond.
Atomic Structure Basic and Beyond.
Physics 4 – April 23, 2019 P3 Challenge – Consider the reaction
Quarks Types Up Down Charmed Strange Top Bottom Formations Hadrons
Physics 4 – April 18, 2019 Agenda:
Particle Physics and The Standard Model
The Top Quark Search Joey Foley.
Presentation transcript:

The Stranger the Better December 20, 1947 A charged Kaon decaying into a muon and neutrino in this case the neutrino leaves no track A neutral Kaon (leaving no track as it is uncharged) decaying into two pions 1947 The discovery of a strange meson called the Kaon

K-mesons (Kaons): p + p- K0 + L0 K- mesons are produce in certain collisions. They eventually decay but live far too long 10-10s rather than 10-23 s p + p- K0 + L0 B no: 1 1 Check that this reaction conserves baryon number. The K meson is always produced with a (relatively) long lived baryon in this case a Λ0 We have a pair of strange particles. The Kaon was allocated a strangeness number of +1 and the lambda zero was given a strangeness number of -1

K-mesons (Kaons): p + p- K0 + L0 Strangeness number +1 -1 +1 -1 Many other particles were found with this ridiculously long lifetime. (1013 times longer than it should be!) It was found that strangeness number is conserved in any strong interaction

What is strangeness due to? Strange particles have a new type of quark called a strange quark which is very like a down quark with a charge of -1/3 but heavier s d u d ŝ The lambda particle has a strange quark and strangeness -1 The kaon has an antistrange quark and strangeness +1

How Does It Get There? p + π- K0 + Λ0 d u s d u d ŝ û d Notice that the strange and antistrange particle are always produced together. Notice that Strangeness is conserved here

s d u d d ŝ ŝ u ŝ ŝ ŝ s u s d u ŝ ŝ s ŝ s s ŝ s What is the strangeness of each of these mesons? What is the strangeness of each of these baryons?

Strangeness is conserved Particle S K +1 K- -1 S- S+ Strangeness is conserved in all strong interactions Which of these is forbidden? p+π-→ K-+ Σ+ π-+p → K++ Σ- K++ p → π++ Σ+

Some strange particles charge Baryon no S K +1,-1,0 +1 1 -1 X +1,-1 -2

Strange particles can decay but only do so by the weak interaction p + p- S -1 0 0 Not strange particles strange particle This is very much like a negative beta decay. It involves a change of quark flavour! Note that strangeness is not conserved in the weak interaction

L0 p + p- s u d W- π- Λo p π- W- A Feynman Diagram for the weak decay of a strange particle

Strangeness Rules We have a new quark called a strange quark Strangeness is conserved in strong interactions Strangeness is not conserved in weak interactions Strange quarks have a strangeness of -1 Antistrange particles have a strangeness of -1