Time and Quantum from Correlations

Slides:



Advertisements
Similar presentations
Gerard t Hooft Spinoza Institute, Utrecht University Utrecht University and.
Advertisements

Quantum Computing MAS 725 Hartmut Klauck NTU
Quantum Information Stephen M. Barnett University of Strathclyde The Wolfson Foundation.
Black Hole Evaporation, Unitarity, and Final State Projection Daniel Gottesman Perimeter Institute.
The General Linear Model Or, What the Hell’s Going on During Estimation?
Danny Terno Entropy and entanglement on the horizon joint work with Etera Livine gr-qc/ gr-qc/ Phys. Rev. A (2005)
Quantum One: Lecture 3. Implications of Schrödinger's Wave Mechanics for Conservative Systems.
Bell inequality & entanglement
6/9/2015Bell's Theorem1 Spooky Action at a Distance Bell’s Theorem and the Demise of Local Reality Natalia Parshina Peter Johnson Josh Robertson Denise.
An Algebraic Foundation for Quantum Programming Languages Andrew Petersen & Mark Oskin Department of Computer Science The University of Washington.
Introduction to Quantum Information Processing Lecture 4 Michele Mosca.
Quantum Mechanics from Classical Statistics. what is an atom ? quantum mechanics : isolated object quantum mechanics : isolated object quantum field theory.
Quantum Cryptography Prafulla Basavaraja CS 265 – Spring 2005.
MOHAMMAD IMRAN DEPARTMENT OF APPLIED SCIENCES JAHANGIRABAD EDUCATIONAL GROUP OF INSTITUTES.
EECS 598 Fall ’01 Quantum Cryptography Presentation By George Mathew.
Paraty, Quantum Information School, August 2007 Antonio Acín ICFO-Institut de Ciències Fotòniques (Barcelona) Quantum Cryptography.
Quantum correlations. Adam W. Majewski. Quantum entanglement. Ghhjhjj Quantum entanglement is a phenomenon that occurs when particles (subsystems) are.
Study and characterisation of polarisation entanglement JABIR M V Photonic sciences laboratory, PRL.
Ch 9 pages ; Lecture 21 – Schrodinger’s equation.
Romain Brette Ecole Normale Supérieure, Paris Philosophy of the spike.
Quantum Information, Communication and Computing Jan Kříž Department of physics, University of Hradec Králové Doppler Institute for mathematical physics.
Entropy localization and distribution in the Hawking radiation Horacio Casini CONICET-Intituto Balseiro – Centro Atómico Bariloche.
In 1887,when Photoelectric Effect was first introduced by Heinrich Hertz, the experiment was not able to be explained using classical principles.
Quantum, classical & coarse-grained measurements Johannes Kofler and Časlav Brukner Faculty of Physics University of Vienna, Austria Institute for Quantum.
Chang-Kui Duan, Institute of Modern Physics, CUPT 1 Harmonic oscillator and coherent states Reading materials: 1.Chapter 7 of Shankar’s PQM.
1 LES of Turbulent Flows: Lecture 1 Supplement (ME EN ) Prof. Rob Stoll Department of Mechanical Engineering University of Utah Fall 2014.
QUANTUM TELEPORTATION
QCCC07, Aschau, October 2007 Miguel Navascués Stefano Pironio Antonio Acín ICFO-Institut de Ciències Fotòniques (Barcelona) Cryptographic properties of.
ECE 8443 – Pattern Recognition ECE 8423 – Adaptive Signal Processing Objectives: Deterministic vs. Random Maximum A Posteriori Maximum Likelihood Minimum.
 Quantum State Tomography  Finite Dimensional  Infinite Dimensional (Homodyne)  Quantum Process Tomography (SQPT)  Application to a CNOT gate  Related.
6.852: Distributed Algorithms Spring, 2008 April 1, 2008 Class 14 – Part 2 Applications of Distributed Algorithms to Diverse Fields.
1 quantum mysteries again! quantum mysteries again! classical vs. quantum correlations ‘ quantum mechanics is weird” N. Bohr Bell’s inequality? QM VIOLATES.
MODULE 1 In classical mechanics we define a STATE as “The specification of the position and velocity of all the particles present, at some time, and the.
The Quantum Theory of Atoms and Molecules The Schrödinger equation and how to use wavefunctions Dr Grant Ritchie.
Quantum Two 1. 2 Evolution of Many Particle Systems 3.
H ij Entangle- ment flow multipartite systems [1] Numerically computed times assuming saturated rate equations, along with the lower bound (solid line)
PGM 2003/04 Tirgul 2 Hidden Markov Models. Introduction Hidden Markov Models (HMM) are one of the most common form of probabilistic graphical models,
Under the Influence of Spectral Entanglement: Polarization-Entanglement Swapping and Fusion Gates Travis Humble * and Warren Grice, Oak Ridge National.
Quantum computing, teleportation, cryptography Computing Teleportation Cryptography.
General Relativity Physics Honours 2008 A/Prof. Geraint F. Lewis Rm 560, A29 Lecture Notes 9.
Quantum Two 1. 2 Angular Momentum and Rotations 3.
Principal Component Analysis (PCA)
A1 “BASIC QUANTUM MECHANICS, AND SOME SURPRISING CONSEQUENCES” Anthony J. Leggett Department of Physics University of Illinois at Urbana-Champaign.
The awesome power of the notion of Computational Universality suggests a complementary thesis It from Bit: Physics is Informational Dynamics should be.
Cosmological Bell Inequalities Juan Maldacena AndyFest 2015 Warping the Universe: A celebration of the Science of Andrew Strominger.
Chapter 3 Postulates of Quantum Mechanics. Questions QM answers 1) How is the state of a system described mathematically? (In CM – via generalized coordinates.
Quantum Measurements: some technical background “Measurement postulate” “Projection postulate” The two aspects of measurement Density matrices, environments,
The Quantum Theory of Atoms and Molecules
Linear Algebra Review.
Origin of Hawking radiation and firewalls
Computability and Complexity
George E.A. Matsas Instituto de Física Teórica/Unesp
Solutions of black hole interior, information paradox and the shape of singularities Haolin Lu.
Quantum mechanics from classical statistics
The Postulates and General Principles
Complexity 6-1 The Class P Complexity Andrei Bulatov.
Quantum One.
Probabilistic Models with Latent Variables
Classical World because of Quantum Physics
Quantum computation with classical bits
Mathematical Foundations of BME
Product moment correlation
Quantum optics as a tool for visualizing fundamental phenomena
Linear Vector Space and Matrix Mechanics
Finite Heisenberg group and its application in quantum computing
Experimental Quantum Teleportation*
Chapter 9 Graph algorithms
MGS 3100 Business Analysis Regression Feb 18, 2016
Quantum One.
Quantum One.
Presentation transcript:

Time and Quantum from Correlations Vlatko Vedral vlatko.vedral@gmail.com

Marginals Given some random variables and some marginal distributions, can we construct a global probability that reproduces the marginals? Sometimes the marginals are simply incompatible; e.g p(A,B) = ½,0,0, ½ while p(B,C)=1/3,0,0,2/3. (because p(B) is different in two cases)

Quantum This is known as quantum “contextualty”. Sometimes there is no overall probability distribution (even though there are no inconsistencies at the lower level), but there is an global quantum state that can account for the marginals. This is known as quantum “contextualty”.

Example - KCBS We have a pentagram. Each vertex can be coloured either red or blue. An edge is said to match if both of its vertices have the same colour. Otherwise, it's a mismatch. In a classical probabilistic model, the total number of mismatches has to be an even number, i.e. 0, 2 or 4. So, with a probability mixture over hidden variable assignments, the expectation value of the sum of mismatches over all of the 5 edges has to lie between 0 and 4. Can have a larger average with quantum states and quantum measurements.

Examples – Bell’s inequalities Given P(A1,B1), P(A1,B2), P(A2,B1), P(A2,B2), find P(A1,A2,B1,B2) such that the average of Bell operator is greater than 2. Cannot be done, but there is a quantum state and measurements that achieve 2root2. N.b. of course here we have an extra constraint of “locality”.

Quantum Principle The fact that there are marginals that are not incompatible, yet do not arise from an overall probability, forces us to use the quantum description. Could it be that there are marginals that cannot be explained quantumly, yet still exist in nature?

Pseudo-density matrix Pretend that different instances of time are like different Hilbert spaces and write a physical state that extends over multiple times. For instance, think of a qubit measured at two different times (with no evolution in-between).

Negative eigenvalue There is no physical state for two qubits of this type. Hence, this object is a pseudo-density (i.e. it has a negative eigen value.

Note… i.e. PDM is a partial transpose T of |00> + |11> maximally entangled Bell state.

Time from correlations We observe marginals that cannot be described by an overall density matrix. Forces us to acknowledge the existence of a time dimension.

Aside: an analogy with special relativity Start with time as fundamental and events as taking place in time. Then postulate: there are pairs of events for which neither one is before the other, nor are they simultaneous. This forces us to acknowledge that space has to have more than one dimension.

Space and time from PDMs? Given R, can we “distill” (reconstruct) space and time from it? Negativity of eigenvalues signals the presence of temporal correlations. However, temporal correlations can look like spatially separable as well as spatially entangled states.

3 time measurements Interesting possible states from 3 temporal pseudo densities: For All reduced states are physical, but the overall is not.

Dynamics out of R? Dynamics can be seen as a teleportation through time via the “entangled” pseudo-density matrix. Measure 12, and subsequently apply To get

Violation of monogamy In a pseudo density matrix we can have maximal entanglement between 1 and 2 and 1 and 3 at the same time. Monogamy: Pseudo-density:

Genovese experiments (INRiM)

Open Timelike curves problem       A’ A B

But… Could the state AA’B actually be a pseudo-state; This could save linearity at the price of introducing time-like correlations

Black-hole information loss? If black hole evaporates by emitting entangled pairs of particles, then after half of it has evaporated, it seems that the remaining black hole is now fully entangled to outside. Yet, if it continues to evaporate via the same (Hawking) mechanism, this seems to lead to a violation of the monogamy of entailment.

Final speculation Just after crossing the event horizon, time and space change their signature in the Schwarzschild metric. This looks like a transposition