Dr Mark Hadley Parity Violation: The Biggest Scientific Blunder of the 20th Century?

Slides:



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

: The mirror did not seem to be operating properly: A guide to CP violation C hris P arkes 12/01/2006.
Radius of Observable Universe and Expansion Rate vs time, k = 0  = 0 Radiation dominated R = 3 x cm R = 10 cm R. =10 18 c c.
Quantum Theory The worst scientific theory of all time Dr Mark J Hadley Dept of Physics.
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.
Uniwersytet JagiellońskiInstytut Fizyki Jacek BierońZakład Optyki Atomowej Time-reversal symmetry violation in heavy atoms Kraków, 24 IV 2008.
Brian Meadows, U. Cincinnati Discrete Symmetries Noether’s theorem – (para-phrased) “A symmetry in an interaction Lagrangian corresponds to a conserved.
Symmetries and conservation laws:
Shu-Yu Ho Date : 2010/9/20 QFT study group
…new vocabulary from Hawking Chaps 9-11 Space-like, time-like variables…subject to Heisenberg time: an imaginery dimension; spacelike & timelike conjugate.
1 FK7003 Lecture 8 ● CP -violation ● T -violation ● CPT invariance.
Lattice Spinor Gravity Lattice Spinor Gravity. Quantum gravity Quantum field theory Quantum field theory Functional integral formulation Functional integral.
Applications of Mathematics to Science and Engineering* Dr. Barbara Hale Physics Department Missouri S&T * talk given to the Student Chapter of MAA Missouri.
Symmetries By Dong Xue Physics & Astronomy University of South Carolina.
Dr Mark Hadley A Gravitational Explanation for Quantum Theory & non-time-orientable manifolds.
The Ideas of Unified Theories of Physics Tareq Ahmed Mokhiemer PHYS441 Student.
Welcome to GT5 Wormholes Time machines and Energy conditions Chairperson Dr. Mark Hadley MG11 Berlin.
Parity Conservation in the weak (beta decay) interaction
+ } Relativistic quantum mechanics. Special relativity Space time pointnot invariant under translations Space-time vector Invariant under translations.
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.
Modern Physics LECTURE II.
Aug 29-31, 2005M. Jezabek1 Generation of Quark and Lepton Masses in the Standard Model International WE Heraeus Summer School on Flavour Physics and CP.
Symmetries and conservation laws
Quantum Electrodynamics Dirac Equation : spin 1/2.
The Development of Particle Physics
Particle Physics Particle Physics Chris Parkes Symmetries,Invariances and Conservation laws (Or how to decide whether to shake hands with an alien!) Conserved.
P Spring 2003 L6Richard Kass Parity Let us examine the parity operator (P) and its eigenvalues. The parity operator acting on a wavefunction is defined.
Lecture 5 – Symmetries and Isospin
10 lectures. classical physics: a physical system is given by the functions of the coordinates and of the associated momenta – 2.
Lecture 15: Beta Decay 23/10/2003 Neutron beta decay: light particles or “leptons”, produced in association. Neutrino presence is crucial to explain.
Symmetry and Its Violation -unifying concept of universe- Tatsuya Nakada Lausanne, 8 February 2000.
Symmetry and conservation Laws Submitted: Pro. Cho By Adil Khan.
1 FK7003 Elementary Particle Physics David Milstead A4:1021 tel: /
Prolog Text Books: –W.K.Tung, "Group Theory in Physics", World Scientific (85) –J.F.Cornwell, "Group Theory in Physics", Vol.I, AP (85) Website:
Vanya Belyaev (ITEP/Moscow) Физика на LHCb The material from the lectures by Profs. T.Nakada and S.Stone is used.
Monday, Nov. 20, 2006PHYS 3446, Fall 2006 Jae Yu 1 PHYS 3446 – Lecture #20 Monday, Nov. 20, 2006 Dr. Jae Yu 1. Parity Properties of Parity Determination.
Fundamental principles of particle physics Our description of the fundamental interactions and particles rests on two fundamental structures :
Particle Physics II Chris Parkes CP Violation
Wave-Particle Duality - the Principle of Complementarity The principle of complementarity states that both the wave and particle aspects of light are fundamental.
1 FK7003 Lecture 6 ● Isospin ● SU(2) and SU(3) ● Parity.
P Spring 2003 L5 Isospin Richard Kass
Dr. Bill Pezzaglia Particle Physics Updated: 2010May20 Modern Physics Series 1 ROUGH DRAFT.
Prepared By A.K.M. Moinul Haque Meaze Student ID: Center for High Energy Physics Kyungpook National University Daegu Daegu Republic.
CERN, 8 February, 2001 Egil Lillestøl, CERN & Univ. of Bergen Lectures recorded at :

Monday, Apr. 4, 2005PHYS 3446, Spring 2005 Jae Yu 1 PHYS 3446 – Lecture #16 Monday, Apr. 4, 2005 Dr. Jae Yu Symmetries Why do we care about the symmetry?
Lecture 7: Symmetries II Charge Conjugation Time Reversal CPT Theorem Baryon & Lepton Number Strangeness Applying Conservation Laws Section 4.6, Section.
P Spring 2002 L4Richard Kass Conservation Laws When something doesn’t happen there is usually a reason! Read: M&S Chapters 2, 4, and 5.1, That something.
Symmetries You may not think about it, but you make assumptions every day about symmetries. If I do an experiment, then pick up my apparatus and move it.
Quantum asymmetry between time and space &
Monday, Apr. 11, 2005PHYS 3446, Spring 2005 Jae Yu 1 PHYS 3446 – Lecture #18 Monday, Apr. 11, 2005 Dr. Jae Yu Symmetries Local gauge symmetry Gauge fields.
Phy107 Fall From Last Time… Today Superposition of wave functions Indistinguishability Electron spin: a new quantum effect The Hydrogen atom and.
Fundamental principles of particle physics Our description of the fundamental interactions and particles rests on two fundamental structures :
IoP Masterclass The Physics of Flavour at the Large Hadron Collider Tim Gershon University of Warwick April 14 th 2010.
IoP Masterclass B PHYSICS Tim Gershon University of Warwick March 18 th 2009.
Symmetries of the nuclear Hamiltonian (exact or almost exact)
Elementary Particle Physics
Lecture 7 Parity Charge conjugation G-parity CP FK7003.
CP Violation in the Standard Model
The Standard Model of Particle Physics
J.J. Gómez-Cadenas IFIC-Valencia Summer Student School CERN, July,2006
Symmetries of the nuclear Hamiltonian (exact or almost exact)
5. Wave-Particle Duality - the Principle of Complementarity
Fundamental principles of particle physics
Countries that signed the nuclear arms treaty with Iran
The Physics of Neutrinos
Handout 9 : The Weak Interaction and V-A
Matter vs. Antimatter The Question of Symmetry
5. Wave-Particle Duality - the Principle of Complementarity
Gauge theory and gravity
Presentation transcript:

Dr Mark Hadley Parity Violation: The Biggest Scientific Blunder of the 20th Century?

Mark Hadley Is Nature Symmetrical? We thought so until 1956 !! A Major change in our view of space and time 1.Round Earth 2.Heliocentric view of Universe 3.Special Relativity (time is not absolute) 4.General relativity (spacetime is curved) 5.Big bang – Universe finite in space and time 6.Expanding Universe (time asymmetry)

Mark Hadley Plan Parity violation – the conventional view My interest Review of Parity conservation –Mechanics –Electromagnetism –Weak Interactions An alternative view –Parity is Conserved !!

Mark Hadley Space Inversion Inversion = reflection + 180° rotation Axial or Pseudo vector

Mark Hadley Effect of Parity - momentum BeforeAfter The Parity Operator gives the transformation due an inversion of the spatial coordinates

Mark Hadley Effect of Parity - spin BeforeAfter

Mark Hadley Physical Review October 1956 p Tsung Dao Lee Chen Ning Yang Parity violation in the weak interactions

Start with a symmetrical state 60 Co Look for an asymmetric outcome e-e- 60 Ni + e - +υ e I(θ)dθ = k (1 + αcosθ )sinθdθ θ

Mark Hadley Experimentalists Wu Ambler Hayward Hoppes Hudson National Bureau of Standards USA 1956

actual result I(θ)dθ = k (1 –v/c cosθ )sinθdθ

Mark Hadley Nobel prize winners 1957 Tsung Dao Lee Chen Ning Yang Parity violation in the weak interactions

Mark Hadley But not quite so simple……. Is the initial state symmetrical? “We see from this analysis that the logical path from the observed asymmetry to the inferred nonconservation of parity in β decay is considerably more complex than the popular presentations would indicate.” L. E. Ballentine:

Mark Hadley A gravitational explanation for quantum theory Aims to explain –QM –Particle spectrum –Fundamental interactions Predictions –No graviton (Gravity waves are just classical waves) –Spin-half –Parity is conserved

Mark Hadley Parity is violated - FACT All the books say so. The Nobel Prize Committee say so.

Doh !

Mark Hadley Explanations using GR Boundary Conditions Common source  

Doh !!

Mark Hadley Where have they gone wrong? Exactly what has been observed? Exactly what has been violated? What, exactly, is the definition of Parity?

Mark Hadley Parity in Newtonian Mechanics F = ma E = ½m v 2 F = m(-a) -F = m (-a) -F = (-m)(-a) F = (-m)(-a) (± )E = ½(± m) v 2 Before After Parity conserved  

Mark Hadley P operator is chosen: 1)For simplicity 2)To conserve parity 3)Supported by: Special Relativity: (t-component of the energy momentum 4-vector) General Relativity: Parity in Newtonian Mechanics

Magnetic field pointing out e-e- e-e- e-e- e-e- e-e- e-e- Parity in electromagnetism Start with a symmetrical state……

Mark Hadley Parity in Electromagnetism F = q(E + v x B) Note: -F = q(-E + -v x (-B)) -F = q(-E + -v x B) -F = -q(E + -v x B) -F = -q(E + -v x (-B)) Before After Parity conserved  

Parity on magnetic poles

Magnetic field pointing out e-e- e-e- e-e- e-e- e-e- Parity in electromagnetism

Magnetic field pointing in e-e- e-e- e-e- e-e- e-e-

Mark Hadley Duality Transforamtion The roles of E and B can be reversed by a duality transformation:

Parity in Electromagnetism In this order P operator is chosen: 1)To conserve parity 2)For simplicity 3)Supported by the covariant formulation:

Mark Hadley Effect of Parity The Parity Operator gives the transformation due an inversion of the spatial coordinates. We do not have a free choice of P operator. What are the transformations in beta decay?

Mark Hadley “We see from this analysis that the logical path from the observed asymmetry to the inferred nonconservation of parity in β decay is considerably more complex than the popular presentations would indicate.” L. E. Ballentine: The assumption that the Cobalt nucleous is symmetrical is not only non-trivial - it may well be wrong !

What is the mirror image of a Cobalt atom? 60 Co e-e- (not to scale) e-e- 60 Co e+e+ Anti 60 Co

Mark Hadley Parity Reverses –Momentum –Lepton number etc. –Charge Unchanged –Spin Is conserved

Mark Hadley Conclusions Space Inversion is a symmetry of Nature Parity is conserved The conventional P operator is not conserved.

Mark Hadley Just a change of convention? The conventional P operator may be combined with another transformation of degenerate multiplets. (eg particle anti- particle, neutrino flavours) Impacts on unifying theories. “Not merely a matter of convention: on other particles P could have the usual effect.” Weinberg

Mark Hadley Parity violation How could they get it so wrong?

Mark Hadley How could they get it so wrong? The Parity operation was defined before the experiments were done. –Particles were defined as eigenstates of Parity. –Simplicity of the operator took precendence over conservation - even though QFT required particles and antiparticles to be combined in the same equations. There was no higher theory to appeal to. Watch this space!

Mark Hadley Parity is Conserved

Mark Hadley Parity Lorentz Boost Eigenvectors of P, H,J 3 with eigenvalues 0,M,σ

Mark Hadley CP violation Boundary conditions –Matter dominated Universe T asymmetry (CPT theorem) –Expanding Universe Parity = CP for some particles only! More complicated effects of P on other degeneracies.