IoP Masterclass The Physics of Flavour at the Large Hadron Collider Tim Gershon University of Warwick April 14 th 2010.

Slides:



Advertisements
Similar presentations
Mitglied der Helmholtz-Gemeinschaft The Fate of Antimatter January 17, 2013 | Hans Ströher JARA|FAME Inauguration.
Advertisements

Bruce Kennedy, RAL PPD Particle Physics 2 Bruce Kennedy RAL PPD.
The Big Bang, the LHC and the Higgs Boson Dr Cormac O’ Raifeartaigh (WIT)
The Large Hadron Collider. The coldest and emptiest place in the solar system The highest energies ever created Cameras the size of cathedrals A machine.
The coldest and emptiest place in the solar system. The highest energies ever created. Cameras the size of cathedrals. A machine 27km long. LHC Overview.
Discrete Space-Time Symmetries Xiao-Gang He USTC, Nanakai, and NTU 1. Discrete Space-Time Symmetries 2. The Down Fall of Parity P Symmetry 3. The Down.
ATLAS Experiment at CERN. Why Build ATLAS? Before the LHC there was LEP (large electron positron collider) the experiments at LEP had observed the W and.
Bruce Kennedy, RAL PPD Particle Physics 2 Bruce Kennedy RAL PPD.
The Asymmetry between Matter and Antimatter Besma M’charek FEW, Vrije Universiteit Amsterdam.
Advanced topics in Particle Physics: LHC physics, 2011 Jeroen van Tilburg 1/55 Overview of flavour physics.
The 2008 Nobel Prize in Physics. Symmetries Symmetries often give us a way to characterize how forces interact. Here, a mirror symmetry flips left and.
Quantum Electrodynamics Dirac Equation : spin 1/2.
October 2011 David Toback, Texas A&M University Research Topics Seminar 1 David Toback Texas A&M University Research Topics Seminar September 2012 Cosmology.
The Big Bang, the LHC and the Higgs Boson Dr Cormac O’ Raifeartaigh (WIT)
Recreating the Big Bang with the Large Hadron Collider at CERN 1 Public Lecture – Jammu September 2013 Professor David Evans The University of Birmingham,
1 Oct 8 th, 2003Gerhard Raven CP violation: The difference between matter and antimatter Gerhard Raven Vrije Universiteit Amsterdam, Subatomic Physics.
Particle Physics Professor Kay Kinoshita University of Cincinnati.
Measurement of CP violation with the LHCb experiment at CERN
Motivations Lectures outline Chris Parkes University of Manchester Visiting Professor AGH University of Science and Technology Matter anti-matter symmetry.
The Higgs Boson: without the maths and jargon David Hall Graduate Seminar Series St Catherine’s College MCR 11 th May 2011.
Joseph Haley Joseph Haley Overview Review of the Standard Model and the Higgs boson Creating Higgs bosons The discovery of a “Higgs-like” particle.
Symmetry and Its Violation -unifying concept of universe- Tatsuya Nakada Lausanne, 8 February 2000.
Vanya Belyaev (ITEP/Moscow) Физика на LHCb The material from the lectures by Profs. T.Nakada and S.Stone is used.
Name, Location/Meeting,Date LHC Big Questions. Name, Location/Meeting,Date String Theory! p+p+ p+p+
基本粒子. 2 The Periodic Table Mendeleev (1869) introduced the periodic table.
Particle Physics: Status and Perspectives Part 4: The Standard Model
Recreating the Big Bang with the World’s Largest Machine Prof Peter Watkins Head of Particle Physics Group The University of Birmingham Admissions Talk.
The Worlds Biggest Experiment. CERN…Conseil Européen pour la Recherche Nucléaire Large Hadron Collider Worlds most expensive science project!! Worlds.
The Professional Development Service for Teachers is funded by the Department of Education and Skills under the National Development Plan PARTICLE Physics.
PARTICLE PHYSICS Particles and Interactions. Classifying Particles Most particles fall broadly into two types which can then be broken down further The.
1 Antimatter 1Antimatter and the Universe 2Antimatter in the Laboratory 3Antimatter in Daily Life.
What is the Higgs??? Prof Nick Evans University of Southampton.
Living In the ANTI- Material World. (from Paul Dirac’s Nobel Lecture December 12, 1933) “If we accept the view of complete symmetry between positive and.
A singularity formed by a previous collapsed Universe? Multiple Universes? We just don’t know… YET What Caused It?
1 FK7003 Lecture 6 ● Isospin ● SU(2) and SU(3) ● Parity.
Experimental Particle Physics Do you want to discover… What is the origin of mass ? Discover the Higgs boson with ATLAS Why is there more matter than anti-matter.
LARGE HADRON COLLIDER at CERN RAS, Nov 2008 Alan Barr University of Oxford The.
Lecture 2: The First Second Baryogenisis: origin of neutrons and protons Hot Big Bang Expanding and cooling “Pair Soup” free particle + anti-particle pairs.
The CKM matrix & its parametrizations
Introduction to Particle Physics I Sinéad Farrington 18 th February 2015.
1 Particle Physics, The Mysteries of the Universe, and The LHC Nhan Tran Johns Hopkins University.
Angels, demons, CERN Rolf Landua Research Physicist (antimatter) Head of Education Group Rolf Landua Research Physicist (antimatter) Head of Education.
Introduction to Particle Physics II Sinéad Farrington 19 th February 2015.
Antimatter Mysteries 1 Rolf Landua Research physicist - Head of Education CERN.
IoP Masterclass The Physics of Flavour at the Large Hadron Collider Tim Gershon University of Warwick March 30 th 2011.
IoP Masterclass B PHYSICS Tim Gershon University of Warwick March 18 th 2009.
LECTURE 9 Chasing Relativistic Particles
The Standard Model of Particle Physics
European Organization for Nuclear Research
Cosmology and Particle Physics in a Single Experiment
CKM Matrix If Universe is the Answer, What is the Question?
The Physics of Neutrinos
Lecture 13 – the weak force
Hunting the Higgs Boson at the CERN Large Hadron Collider
Particle Physics.
Aim: How can we describe Fundamental Particles?
Matter vs. Antimatter The Question of Symmetry
Precision Probes for Physics Beyond the Standard Model
Elementary particles Spring 2005, Physics /24/2018 Lecture XXV.
Particle physics.
History of Particle Nuclear Physics!
3.3 The Atom and Electrons!.
What’s the matter with antimatter?
(and why it may one day save your life!)
Particle Physics Theory
Methods of Experimental Particle Physics
François PASSEBON & Jack WILLIS
Particle Physics: Status and Perspectives Part 4: The Standard Model
Early Universe.
Modern Studies of the Atom
Presentation transcript:

IoP Masterclass The Physics of Flavour at the Large Hadron Collider Tim Gershon University of Warwick April 14 th 2010

The Standard Model Tim Gershon, IoP Masterclass, April 14 th

Some Questions ● What is antimatter? ● Why are there three “colours” of quarks? ● Why are there so many bosons? These questions have well-understood answers 3 Tim Gershon, IoP Masterclass, April 14 th 2010

Some More Questions ● Why are there so many fermions? ● Why are there three “generations” of both quarks and leptons? ● Why are matter and antimatter different? We do not know the answers to these questions! 4 (“flavour”) (“CP violation”) Tim Gershon, IoP Masterclass, April 14 th 2010

Matter vs. antimatter ● In the Big Bang, matter and antimatter should have been produced in equal quantities ● In the Universe today, we observe only matter ⇒ need CP violation 5 Tim Gershon, IoP Masterclass, April 14 th 2010

Asymmetry of the Universe ● Paul Dirac, one of the greatest British physicists of all time, won the 1933 Nobel Prize for his prediction of the existence of antimatter ● In his Nobel lecture, Dirac concludes: “... we must regard it rather as an accident that [the solar system] contains a preponderance of negative electrons and positive protons. It is quite possible that for some of the stars it is the other way about, these stars being built up mainly of positrons and negative protons. In fact, there may be half the stars of each kind. ” ● It turns out there are not any antimatter stars ● Dirac did not know about CP violation! 6 Tim Gershon, IoP Masterclass, April 14 th 2010

What is CP Violation? ● Symmetries are powerful tools to understand nature ● Two important discrete symmetries are — C : charge conjugation (exchange particle and antiparticle) — P : parity (mirror transform all spatial coordinates) Need violation of combined CP symmetry to distinguish absolutely between matter & antimatter 7 Tim Gershon, IoP Masterclass, April 14 th 2010

CP Symmetry 8 P C Tim Gershon, IoP Masterclass, April 14 th 2010 Illustrated using the images of MC Escher CP Combined CP transformation ⇒ pictures look the same

CP Violation 9 P C Tim Gershon, IoP Masterclass, April 14 th 2010 Illustrated using the images of MC Escher CP Combined CP transformation ⇒ pictures look different!

The CKM Matrix ● Quark mixing described by Cabibbo-Kobayashi-Maskawa matrix ● Matrix elements are complex numbers — interactions of quarks and antiquarks can be different ⇒ CP violation! 10 down-type quarks as seen by the weak interaction physical down-type quarks (with well-defined masses) Tim Gershon, IoP Masterclass, April 14 th 2010 Makoto Kobaya shi Toshihid e Maskaw a Nobel Prize in Physics 2008

B Physics at the LHC ● CP violation appears to be central to understanding the questions discussed above ➢ eg. as shown by Kobayashi & Maskawa (1973), need at least three generations for CP violation to occur ● Kobayashi-Maskawa mechanism predicts large CP violation effects in particles containing b quarks ➢ need dedicated experiments to test KM predictions ● Exploit copious production of b quarks at the CERN Large Hadron Collider ➢ LHCb experiment 11 Tim Gershon, IoP Masterclass, April 14 th 2010

The LHC at CERN ● The world's largest machine ● Located at CERN laboratory near Geneva ● m circumference ● Emptier (10 –13 atm) and colder (1.9 K = –271.3° C) than outer space ● 1232 superconducting dipole magnets (8.33 T) ● Cost ~ £5 billion 12 Tim Gershon, IoP Masterclass, April 14 th 2010 Geneva Geneva airport LHCb experiment Main CERN site

LHC dipole magnets 13 Tim Gershon, IoP Masterclass, April 14 th 2010

Will the LHC destroy the earth? 14 Tim Gershon, IoP Masterclass, April 14 th 2010 No!

The LHCb Experiment 15 Tim Gershon, IoP Masterclass, April 14 th 2010 ● Searching for new sources of CP violation ➢ compare matter and antimatter ➢ look for disagreement with Standard Model predictions ➢ search for unexpected effects ● Requires an ultra-high precision detector ➢ operated by a collaboration of 700 physicists

Can the LHC be used to make antimatter bombs? 16 Tim Gershon, IoP Masterclass, April 14 th 2010 No!

Summary 17 Tim Gershon, IoP Masterclass, April 14 th 2010 ● Studies of B physics provide excellent opportunities to address one of the biggest questions about our Universe ➢ What causes the excess of matter over antimatter? ● By learning more about B physics and CP violation we hope to find clues about the theoretical structure of the Standard Model (and any theories beyond it) ➢ Why are there three generations of quarks and leptons? ● The Warwick group is actively involved in experiments at the forefront of this exciting area of research ➢ We hope the LHCb experiment will provide some answers!