The Uncertainty Principle and the Quarks

Similar documents
Hunting for elusive particles at LHC: Start of Run II

Elementary Particle Physics Glossary. Course organiser: Dr Marcella Bona February 9, 2016

A first trip to the world of particle physics

Physics 4213/5213 Lecture 1

Particle Physics (concise summary) QuarkNet summer workshop June 24-28, 2013

The God particle at last? Science Week, Nov 15 th, 2012

INTRODUCTION TO THE STANDARD MODEL OF PARTICLE PHYSICS

The God particle at last? Astronomy Ireland, Oct 8 th, 2012

FACULTY OF SCIENCE. High Energy Physics. WINTHROP PROFESSOR IAN MCARTHUR and ADJUNCT/PROFESSOR JACKIE DAVIDSON

The ATLAS Experiment and the CERN Large Hadron Collider

The ATLAS Experiment and the CERN Large Hadron Collider

The Hunt for the Higgs (and other interesting stuff at the Tevatron) Robert Roser Fermi National Accelerator Laboratory

cgrahamphysics.com Particles that mediate force Book pg Exchange particles

High Energy Physics. QuarkNet summer workshop June 24-28, 2013

An Introduction to Particle Physics

Quantum Numbers. Elementary Particles Properties. F. Di Lodovico c 1 EPP, SPA6306. Queen Mary University of London. Quantum Numbers. F.

Name : Physics 490. Practice Final (closed book; calculator, one notecard OK)

The Standard Model. 1 st 2 nd 3 rd Describes 3 of the 4 known fundamental forces. Separates particle into categories

Lecture 02. The Standard Model of Particle Physics. Part I The Particles

Chapter 32 Lecture Notes

The Standard Model (part I)

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

Physics 214 Experimental Particle Physics. Lecture 1 What to expect.

Essential Physics II. Lecture 14:

Wesley Smith, U. Wisconsin, January 21, Physics 301: Introduction - 1

PHY-105: Introduction to Particle and Nuclear Physics

Results from the Tevatron: Standard Model Measurements and Searches for the Higgs. Ashutosh Kotwal Duke University

Lecture 18 - Beyond the Standard Model

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

Physics 214 Experimental Particle Physics. Lecture 1 What to expect.

Introduction to the Standard Model

9.2.E - Particle Physics. Year 12 Physics 9.8 Quanta to Quarks

Exam Results. Force between charges. Electric field lines. Other particles and fields

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

Properties of Elementary Particles

1. Introduction. Particle and Nuclear Physics. Dr. Tina Potter. Dr. Tina Potter 1. Introduction 1

Beyond Standard Model Effects in Flavour Physics: p.1

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

Nuclear and Particle Physics 3: Particle Physics. Lecture 1: Introduction to Particle Physics February 5th 2007

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

Neutrino Physics. Kam-Biu Luk. Tsinghua University and University of California, Berkeley and Lawrence Berkeley National Laboratory

Gian Gopal Particle Attributes Quantum Numbers 1

A Tour of the Standard Model of Elementary Particles and Fields

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

Dennis Silverman UC Irvine Physics and Astronomy Talk to UC Irvine OLLI May 9, 2011

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

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

Par$cles. Ma#er is made of atoms. Atoms are made of leptons and quarks. Leptons. Quarks. atom nucleus nucleon quark m m m m

Particle Physics. Tommy Ohlsson. Theoretical Particle Physics, Department of Physics, KTH Royal Institute of Technology, Stockholm, Sweden

Option 212: UNIT 2 Elementary Particles

Introduction. Read: Ch 1 of M&S

Physics 7730: Particle Physics

E = mc 2 Opening Windows on the World

PH5211: High Energy Physics. Prafulla Kumar Behera Room: HSB-304B

Particle + Physics at ATLAS and the Large Hadron Coillder

DEVIL PHYSICS THE BADDEST CLASS ON CAMPUS IB PHYSICS

Unravelling the Mysteries of Matter with the CERN Large Hadron Collider An Introduction/Overview of Particle Physics

Physics 661. Particle Physics Phenomenology. October 9, Physics 661, lecture 5 1

Modern physics 1 Chapter 13

Beyond the standard model? From last time. What does the SM say? Grand Unified Theories. Unifications: now and the future

The first one second of the early universe and physics beyond the Standard Model

The Discovery of the Higgs boson Matthew Herndon, University of Wisconsin Madison Physics 301: Physics Today. M. Herndon, Phys

32 IONIZING RADIATION, NUCLEAR ENERGY, AND ELEMENTARY PARTICLES

Quanta to Quarks. Science Teachers Workshop 2014 Workshop Session. Adrian Manning

Saturday 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 Dr. Rainer J. Fries

Search for a Z at an e + e - Collider Thomas Walker

Lecture PowerPoint. Chapter 32 Physics: Principles with Applications, 6 th edition Giancoli

Frontier Science: The mystery of Antimatter

e + e - (1) Silicon Vertex Detector

8.882 LHC Physics. High Energy Physics Overview. [Lecture 16, April 6, 2009] Experimental Methods and Measurements

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

The Standard Model of Particle Physics

I. Antoniadis CERN. IAS CERN Novice Workshop, NTU, 7 Feb 2014

The Standard Model, Supersymmetry and ZooFinder at CDF. Matthew C. Cervantes Department of Physics Texas A&M University Master defense: 7/21/2006

Elementary Particles, Flavour Physics and all that...

Democritus, a fifth century B.C. philosopher, is credited with being the first

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

Fundamental Particles

Units and dimensions

Particle physics today. Giulia Zanderighi (CERN & University of Oxford)

Lecture 39, 40 Supplement: Particle physics in the LHC era

Outline: Introduction Search for new Physics Model driven Signature based General searches. Search for new Physics at CDF

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

Cosmology and particle physics

A brief history of accelerators, detectors and experiments: (See Chapter 14 and Appendix H in Rolnick.)

Introduction to Particle Physics. HST July 2016 Luis Alvarez Gaume 1

Physics 424: Dr. Justin Albert (call me Justin!)

A Brief History of Modern Physics

Analyzing CMS events

Experimental verification of the Salaam-Weinberg model. Pásztor Attila, Eötvös University Experimental Particle Physics Student Seminar

ATLAS. Questions and Answers

The Quark Parton Model

FYS3510 Subatomic Physics. Exam 2016

The Strong Interaction and LHC phenomenology

The Goals of Particle Physics

The Scale-Symmetric Theory as the Origin of the Standard Model

Option 212: UNIT 2 Elementary Particles

Physics 662. Particle Physics Phenomenology. February 21, Physics 662, lecture 13 1

3 Dimensional String Theory

Transcription:

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 what we know and do not know in particle physics

Heisenberg uncertainty principle The Uncertainty Principle key concept of Quantum Mechanics tiny h = 10 34 J s Consequence x p h 2 physics at small scale (quantum h) is not deterministic! operate with probabilities instead cannot know exact position and momentum at the same time Counterintuitive, even Einstein was wrong: I cannot believe that God would choose to play dice with the universe.

The Uncertainty Principle Example: electron around a nucleus only probability function (wave function) no circular orbits quantized (discrete) energies Quantization of angular momentum: orbital L = r p = h n spin (internal) S = h 2 n Counterintuitive, but Einstein was right (photoelectric effect): light quanta from Planck s E = hω (photon)

The Quarks : from the Smallest to the Largest On the smallest and largest scale: what are we made of and why (Galaxy cluster 1E 0657-66: X-ray, Optical, Grav. Lensing)

.

From Molecules to Quarks XXth century: reaching deep into matter, Quarks Chemistry Atomic Physics Particle Physics

Fermions S = h 2 (matter) Elementary Particles (anti-matter) leptons quarks Bosons S = h (force carries): EM strong (weak force later)

Periodic Table of Baryons: Proton, Neutron,... Three quarks make up a Baryon: Petar s discovery: Σ b (ddb) and Σ + b (uub)

Like Periodic Table of Atoms

Periodic Table of Mesons Quark-antiquark make up a Meson: ground state (L=S=0) Vector meson S=1 h

How do We See Particles We see semi-stable particles by tracks in matter: Table-top illustrations Complex multi-ton detectors

Movie?

How do We See Particles Most particles live too short to be seen directly see decay products (c=3 10 8 m/s): life-time and energy (mass) uncertainty of a resonance : the Uncertainty Principle (part 2): t E h

Unstable Particles The Uncertainty Principle (part 2): Γ 0 τ 0 = h compare: E t h Probability (1 GeV 2 10 27 kg proton mass) Breit-Wigner resonance

Unstable particles decay Feynman diagram: Decay Dynamics Decay study elementary particles and interactions (this strong decay is mostly understood)

Decay Kinematics We often understand decay dynamics through kinematics

Decay Kinematics We often understand decay dynamics through kinematics Conservation of orbital momentum: L z = +1 L z = 0 Y 0 1 (cos θ) 2 Y +1 1 (cos θ) 2 cos θ cos θ

Weak Interactions Massive carries weak (short-range) mass 80-90 GeV Special interactions: change type of quark change families left-handed fermions violate Parity and C violate CP symmetry

.

Look Beyond the Standard Model Mysterious Higgs field gives mass to particles Need something beyond the SM large matter-dominance dark matter light Higgs

Possible Extension: Super-Symmetry New (super)symmetry: Q fermion = boson Q boson = fermion Solve: (1) natural light Higgs (2) dark matter lightest χ 0 1 (3) large matter/antimatter Just around the corner in mass...

.

Reaching Highest Energy mc 2 = E

Large Hadron Collider: 2008

Movie?

The Uncertainty Principle Heavy objects for a short instant t: E t h get mc 2 E 500GeV Possible: penguin loop 5GeV 80GeV 0.1GeV 175GeV

Types of Penguins 1993: EM penguin 1997: gluonic penguin rate 3.5 10 4 harder due to gluons

Loops penguin loop mixing box Best constraints on supersymmetry and New Physics

Study penguin B φk One Example

New Particles through Uncertainty Principle?

artist view http://today.slac.stanford.edu/a/2006/10-26.htm

.

Kinematics: Producing the B Mesons Dynamics:

Producing the B Mesons 2000-2007: nearly billion B mesons study few in a million processes

Producing the B Mesons

Kinematics of the Decay Find 4 tracks : find 1-2/week B 0 φk 0 (K + K )(K + π ) rare < 1 in 100,000

Reconstructing Kinematics in the Detector BABAR detector at SLAC: B 0 φk 0 (K + K )(K + π ) B 0 φk 0 (K + K )(π + π ) K K + K K + π + π π + π

The Heart of the BABAR Detector JHU teams on silicon detectors on BABAR, CDF, and CMS

The BABAR Detector

Movie?