The meaning of weak value

Slides:



Advertisements
Similar presentations
Xkcd xkcd.com. Section 2 Recap ► ► Principle of Superposition: quantum states show interference and require both an amplitude and a phase for the parts.
Advertisements

Xkcd Xkcd.com.
Xkcd Xkcd.com. Section 3 Recap ► Angular momentum commutators:  [J x, J y ] = iħJ z etc ► Total ang. Mom. Operator: J 2 = J x 2 + J y 2 +J z 2 ► Ladder.
Quantum One: Lecture 1a Entitled So what is quantum mechanics, anyway?
PHY 042: Electricity and Magnetism Magnetic field in Matter Prof. Hugo Beauchemin 1.
Experimental Issues in Quantum Measurement Aephraim Steinberg Why does one thing happen and not another? When is a quantum measurement? Does a measurement.
The Quantum Mechanics of Simple Systems
The Postulates of Quantum Mechanics
Emergence of Quantum Mechanics from Classical Statistics.
Quantum statistics: a formal approach Reminder to axioms of quantum mechanics  state vector of the Hilbert space describes quantum mechanical system 
Quantum statistics of free particles Identical particles Two particles are said to be identical if all their intrinsic properties (e.g. mass, electrical.
Wavefunction Quantum mechanics acknowledges the wave-particle duality of matter by supposing that, rather than traveling along a definite path, a particle.
Reversible Weak Quantum Measurements 09 December 2008 Presented by: Adam Reiser Anuj Das Neil Kumar George O’Quinn.
If is an element of reality then If then is an element of reality For dichotomic variables:
Backward Evolving Quantum State Lev Vaidman 2 March 2006.
חוק המכפלה. It is always in ! The 3-boxes paradox.
Physics 452 Quantum mechanics II Winter 2011 Karine Chesnel.
Regionalized Variables take on values according to spatial location. Given: Where: A “structural” coarse scale forcing or trend A random” Local spatial.
The Everett Interpretation of Quantum Mechanics: 50 years on 19 – 21 July 2007 Time-symmetric quantum mechanics and the Many-Worlds Interpretation Lev.
Quantum Mechanics from Classical Statistics. what is an atom ? quantum mechanics : isolated object quantum mechanics : isolated object quantum field theory.
Chapter 3 Formalism. Hilbert Space Two kinds of mathematical constructs - wavefunctions (representing the system) - operators (representing observables)
Schrödinger We already know how to find the momentum eigenvalues of a system. How about the energy and the evolution of a system? Schrödinger Representation:
PHYS Quantum Mechanics PHYS Quantum Mechanics Dr Jon Billowes Nuclear Physics Group (Schuster Building, room 4.10)
Teleportation. 2 bits Teleportation BELL MEASUREMENT.
Quantum One: Lecture 2. Postulates of Schrödinger's Wave Mechanics.
Question A) B) C) D) E An electric field polarizes a metal block as shown.
MSEG 803 Equilibria in Material Systems 6: Phase space and microstates Prof. Juejun (JJ) Hu
Weak Values in Quantum Measurement Theory - Concepts and Applications - Yutaka Shikano 07M01099 Department of Physics, Tokyo Institute of Technology “Master.
Lecture 19: The deuteron 13/11/2003 Basic properties: mass: mc 2 = MeV binding energy: (measured via  -ray energy in n + p  d +  ) RMS.
Quantum Two 1. 2 Angular Momentum and Rotations 3.
Quantum Two 1. 2 Evolution of Many Particle Systems 3.
Question. Question A) B) C) D) E An electric field polarizes a metal.
1 Reading: Main 9.0, 9.1, 9.3 GEM 9.1.1, Knight Ch 20 BASIC WAVE CONCEPTS.
The Higgs Boson Observation (probably) Not just another fundamental particle… July 27, 2012Purdue QuarkNet Summer Workshop1 Matthew Jones Purdue University.
Wave Properties of Light. Characterization of Light Light has both a wavelike and particle like nature. Light has both a wavelike and particle like nature.
Effective Non-Hermitian Hamiltonian of a pre- and post-selected quantum system Lev Vaidman
Solvable Model for the Quantum Measurement Process Armen E. Allahverdyan Roger Balian Theo M. Nieuwenhuizen Academia Sinica Taipei, June 26, 2004.
Central Force Umiatin,M.Si. The aim : to evaluate characteristic of motion under central force field.
Chapter 4 Two-Level Systems, Spin. Two-level systems Let us start with the simplest non-trivial state space, with only two dimensions Despite its simplicity,
Basic Concepts Absolute Size The Superposition Principle Copyright – Michael D. Fayer, 2007 Size Classical MechanicsQuantum Mechanics RelativeAbsolute.
MODULE 5 HERMITICITY, ORTHOGONALITY, AND THE SPECIFICATION OF STATES we have stated that we need Hermitian operators because their eigenvalues are real.
1 Reading: QM Course packet – Ch 5 BASICS OF QUANTUM MECHANICS.
Measurement and Expectation Values
Q. M. Particle Superposition of Momentum Eigenstates Partially localized Wave Packet Photon – Electron Photon wave packet description of light same.
Electrostatics Forces and Fields
Quantum mechanics from classical statistics
Announcements Exam Details: Today: Problems 6.6, 6.7
Quantum One.
مناهج البحث العلمي Scientific Research Methods
4. The Postulates of Quantum Mechanics 4A. Revisiting Representations
A charge distribution lies along a segment of the positive x axis
The Postulates and General Principles
Waves and Fourier Expansion
Quantum One. Quantum One So what is quantum mechanics, anyway?
The basics By Mr. M.
Chapter 4 Two-Level Systems.
Quantum Two.
Chapter II Klein Gordan Field Lecture 5.
Lev Vaidman 23 August 2004, Cambridge Zion Mitrani Amir Kalev
Quantum One.
Quantum Mechanics Postulate 4 Describes expansion
PHY 184 Title: The Electric Field Week1 - Spring 2007 Lecture 4
Total Energy is Conserved.
Section 2.2: Statistical Ensemble
Physics 014 Electric fields 1.
QM2 Concept Test 11.1 In a 3D Hilbert space,
Bell Work: Electric Fields
Quantum One.
Quantum mechanics II Winter 2012
The two-state vector formalism of quantum mechanics
Presentation transcript:

The meaning of weak value Lev Vaidman

The meaning of weak value What is “a value of a variable”? Weak value controversy Weak value as an outcome of weak measurements Weak value as a property of a single system Experimental results

A value of a physical observable is classical Classical values always have definite values has a definite value eigenvalue is quantum The system is pre-selected is a statistical expectation value is quantum has no definite value The system is pre-selected post-selected is quantum The system is pre-selected and The system is described by the weak value Is the weak value statistical as the expectation value or definite as the eigenvalue?

Weak value as an outcome of a weak measurement

Quantum measurement of Collapse!

Weak measurement of with post-selection

Weak measurement of with post-selection

Weak measurement of with post-selection

Weak measurement of without post-selection

Weak value as an outcome of a weak measurement on condition of post-selection Weak value is a conditional expectation value

The two-state vector

The two-state vector

The weak value as a property of a single system The two-state vector is a complete description of a pre- and post-selected system in a particular time If the pre- and post-selected system is coupled to other systems through C, then its coupling at time t is described (completely) by the weak value

The meaning of “a value of ” is quantum The system is pre-selected and post-selected weak value is classical classical value The system is pre-selected is quantum eigenvalue The system is pre-selected is quantum expectation value is quantum The system is pre-selected and post-selected weak value = expectation value

The meaning of “a value of ” is quantum The system is pre-selected and post-selected weak value The system is pre-selected is quantum eigenvalue is quantum The system is pre-selected expectation value

Comparing states of external system after eigenvalue weak value expectation value Bures angle distance

System: charged particle, variable: electric field at the origin eigenvalue expectation value weak value

Pre- and post-selection superposition Example: spin 1 particle Eigenstate eigenvalue Superposition Pre- and post-selection superposition with weak value

Experiment visibility

Experiment comparing with BC reference visibility polarizer phase modulator BC visibility

B Experiment comparing with with BC reference visibility polarizer phase modulator B BC visibility

Summary Weak value is a property of a single pre- and post-selected system (It is not a property of a measuring procedure) An ensemble is needed only to test that it is true A pre and post-selected system interacts with external systems during infinitesimal time as if the weak value is an eigenvalue. It is significantly different from coupling of pre-selected only system with expectation value equal to the weak value.