Experimental Issues in Quantum Measurement Aephraim Steinberg Why does one thing happen and not another? When is a quantum measurement? Does a measurement.

Slides:



Advertisements
Similar presentations
Department of Computer Science & Engineering University of Washington
Advertisements

Quantum One: Lecture 1a Entitled So what is quantum mechanics, anyway?
The idea of the correlation femtoscopy is based on an impossibility to distinguish between registered particles emitted from different points because.
We’ve spent quite a bit of time learning about how the individual fundamental particles that compose the universe behave. Can we start with that “microscopic”
1 quantum teleportation David Riethmiller 28 May 2007.
Observing the quantum nonlocality in the state of a massive particle Koji Maruyama RIKEN (Institute of Physical and Chemical Research) with Sahel Ashhab.
A microstate of a gas of N particles is specified by: 3N canonical coordinates q 1, q 2, …, q 3N 3N conjugate momenta p 1, p 2, …, p 3N Statistical Mechanics.
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.
The two-state vector. ? ? At time t: ? Erasing the past.
PHYS Quantum Mechanics PHYS Quantum Mechanics Dr Gavin Smith Nuclear Physics Group These slides at:
Spin Quantum Number and Spin Example: Electron, s = ½ (fermion) Implications? Spin angular momentum is INTRINSIC to a particle mass charge spin More 
Group work Show that the Sx, Sy and Sz matrices can be written as a linear combination of projection operators. (Projection operators are outer products.
Fermions and non-commuting observables from classical probabilities.
Quantum Mechanics from Classical Statistics. what is an atom ? quantum mechanics : isolated object quantum mechanics : isolated object quantum field theory.
P460 - many particles1 Many Particle Systems can write down the Schrodinger Equation for a many particle system with x i being the coordinate of particle.
Bose Einstein Condensation Condensed Matter II –Spring 2007 Davi Ortega In Diluted Gas.
Quantum One: Lecture 2. Postulates of Schrödinger's Wave Mechanics.
Modern Physics lecture 3. Louis de Broglie
Lecture 9 Particle in a rectangular well (c) So Hirata, Department of Chemistry, University of Illinois at Urbana-Champaign. This material has been developed.
6. Second Quantization and Quantum Field Theory
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.
Physics 451 Quantum mechanics I Fall 2012 Oct 17, 2012 Karine Chesnel.
Lecture 2. Postulates in Quantum Mechanics
Introduction to tunneling times and to weak measurements How does one actually measure time ? (recall: there is no operator for time) How long does it.
Weak Values with Decoherence (Typo in Program) Yutaka Shikano and Akio Hosoya Department of Physics, Tokyo Institute of Technology Based on arXiv:
Weak measurement of cotunneling time
Statistical mechanics How the overall behavior of a system of many particles is related to the Properties of the particles themselves. It deals with the.
5. Formulation of Quantum Statistics
Experimental Issues in Quantum Measurement Being a quantum physicist is like being an alcoholic....the first step is to admit you have a problem. Today,
Effective Non-Hermitian Hamiltonian of a pre- and post-selected quantum system Lev Vaidman
5.2 QUANTUM THEORY AND THE ATOM PART 2 The quantum mechanical model of the atom.
Solvable Model for the Quantum Measurement Process Armen E. Allahverdyan Roger Balian Theo M. Nieuwenhuizen Academia Sinica Taipei, June 26, 2004.
Dynamics of a BEC colliding with a time-dependent dipole barrier OSA Frontiers in Photonics 2006 starring Chris Ellenor as Mirco Siercke Aephraim Steinberg’s.
Modern Physics lecture X. Louis de Broglie
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?
Review of lecture 5 and 6 Quantum phase space distributions: Wigner distribution and Hussimi distribution. Eigenvalue statistics: Poisson and Wigner level.
Physics for Scientists and Engineers, 6e
Optical implementation of the Quantum Box Problem Kevin Resch Jeff Lundeen Aephraim Steinberg Department of Physics, University of Toronto AKA: Let's Make.
1 Reading: QM Course packet – Ch 5 BASICS OF QUANTUM MECHANICS.
Basic Concepts Absolute Size The Superposition Principle Copyright – Michael D. Fayer, 2007 Size Classical MechanicsQuantum Mechanics RelativeAbsolute.
Lecture 26 — Review for Exam II Chapters 5-7, Monday March 17th
Topic #1: Atomic Structure and Nuclear Chemistry
Quantum Measurements: some technical background “Measurement postulate” “Projection postulate” The two aspects of measurement Density matrices, environments,
Phy107 Fall From Last Time… Today Superposition of wave functions Indistinguishability Electron spin: a new quantum effect The Hydrogen atom and.
The meaning of weak value
Q. M. Particle Superposition of Momentum Eigenstates Partially localized Wave Packet Photon – Electron Photon wave packet description of light same.
Chapter V Interacting Fields Lecture 3 Books Recommended:
Chapter III Dirac Field Lecture 2 Books Recommended:
The Bohr Model, Wave Model, and Quantum Model
Experimental Inquiry Template.
Quantum Physics Comes of Age I incident II transmitted reflected.
Quantum One. Quantum One So what is quantum mechanics, anyway?
Consider the He atom. The Hamiltonian is
Welcome back from fall break Comments on mid-term exam
Quantum One.
Flame Test Recap WCHS Chemistry.
QM1 Concept test 1.1 Consider an ensemble of hydrogen atoms all in the ground state. Choose all of the following statements that are correct. If you make.
Choose all of the following observables for which it will be convenient to use the coupled representation to find the probabilities of different outcomes.
PHY 741 Quantum Mechanics 12-12:50 PM MWF Olin 103
Chapter II Klein Gordan Field Lecture 3 Books Recommended:
Reading: Chapters #5 in Shankar; quantum mechanical systems in 1-dim
“Addition” of angular momenta – Chap. 15
Linear Vector Space and Matrix Mechanics
Second quantization and Green’s functions
Quantum One.
Presentation transcript:

Experimental Issues in Quantum Measurement Aephraim Steinberg Why does one thing happen and not another? When is a quantum measurement? Does a measurement necessarily disturb the system, and how? What can we say about an observable before we measure it? Does a wave function describe a single particle, or only an ensemble? Is a wave function a complete description of a single particle? Can we predict the past? Lectures: Tuesday, 10-11, Kleiner Hörsaal (auf Englisch, es tut mir leid)

Atoms falling out of a lattice trap As the trap is lowered, each quantum state falls out at a different time – we can see “by eye” how many atoms were in each energy eigenstate.

momentum position Probability P(0,0) < 0 ?! The Wigner quasiprobability function...combining many such measurements, we can completely describe the quantum state of the atoms.

Some topics we’ll cover Must “collapse” really happen? alternate pictures of measurements and correlations How much can we say about the past? weak measurements and postselection... Can we measure the entire state of a particle? density-matrix and Wigner function reconstruction Can we distinguish between indistinguishable things? non-orthogonal state discrimination Are there different things we can never distinguish between? different preparations of identical density matrices Can we measure something without interacting with it? “Vaidman’s bomb” experiment Can we undo the disturbance introduced by a measurement? The “quantum eraser” Can we use the measurement process to accomplish tasks? Measurement-induced nonlinearity, LOQC LECTURES: TUESDAYS 10-11, Kleiner Hörsaal