“Classical entanglement” and cat states

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School of something FACULTY OF OTHER School of Physics and Astronomy FACULTY OF MATHEMATICAL AND PHYSICAL SCIENCES “Classical entanglement” and cat states Jacob Dunningham Paraty, August 2007

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School of Physics and Astronomy FACULTY OF MATHEMATICAL AND PHYSICAL SCIENCES. “Classical entanglement” and cat states. Jacob Dunningham. Paraty, August 2007. Overview. The consequences of entanglement: The emergence of classicality from the quantum world Number and phase of BEC - PowerPoint PPT Presentation

Transcript of “Classical entanglement” and cat states

Page 1: “Classical entanglement” and cat states

School of somethingFACULTY OF OTHER

School of Physics and AstronomyFACULTY OF MATHEMATICAL AND PHYSICAL SCIENCES

“Classical entanglement” and cat states

Jacob Dunningham

Paraty, August 2007

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Overview

The consequences of entanglement:

• The emergence of classicality from the quantum world

Number and phase of BEC

Position and momentum of micro-mirrors

Energy and time?

• Schrodinger cat states

How can we make them

How can we see them

What can we do with them

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Multi-particle

EntanglementsWILD PEDIGREE

Bunnies Cats Bats

Quantum Information

Everyday World

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Annihilation and creation operators (bosons)

annihilation

creation

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Annihilation and creation operators (bosons)

annihilation

creation

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Annihilation and creation operators (bosons)

Eigenvalue equation

is the number operator

annihilation

creation

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Annihilation and creation operators (bosons)

annihilation

creation

In the Fock (number state) basis, these can be written as the matrices:

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Annihilation and creation operators (bosons)

annihilation

creation

In the Fock (number state) basis, these can be written as the matrices:

An exercise in matrix multiplication confirms the bosonic commutation relation:

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Emergence of classicality

One of the most perplexing aspects of quantum theory is that microscopic objects can be in superpositions but macroscopic objects cannot

Schrödinger’s cat

To ‘see’ a coherent superposition, we need interference

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How do we see them?

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Detect interference of probe state corresponding to phase

Macroscopic variables

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Detect interference of probe state corresponding to phase

No interference if the macroscopic states are orthogonal

Macroscopic variables

Need coupling between them - “Lazarus operator”

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The key is to wash out the which-way informationNOON state

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The key is to wash out the which-way information

There is the problem of the environment

Tracing over the environment gives:

Described in detail by A. Ekert

yesterday

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Classical entanglement

Can also understand the emergence of classicality in terms of entanglement

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Classical entanglement

Can also understand the emergence of classicality in terms of entanglement

First it is helpful to consider BECs

• Macroscopic quantum entity

• Can probe quantum / classical divide

• Cold enough to enable quantum phase transitions

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What is a BEC?

Predicted 1924... ...Created 1995

S. Bose A. Einstein

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What is a BEC?

Bose-Einstein distribution:

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What is a BEC?

Bose-Einstein distribution:

Take

For consistency:

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What is a BEC?

Bose-Einstein distribution:

Take

For consistency:

Onset of BEC:

Cold and dilute

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How do we make them?

Trap them with magnetic and/or optical fields

Cool them using two main techniques:

1. Laser Cooling (link)

2. Evaporative Cooling (link)

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What is a BEC?

For our purposes, a BEC is a ‘macroscopic’ quantum entity - thickness of a human hair

All the atoms (~103 - 109) are in the same quantum state

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Phase of a BEC

Coherent state:

“Most classical” quantum state

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BEC Localisation

N NConservation of atom number:

?

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BEC Localisation

N NConservation of atom number:

?

Experiment

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BEC Localisation

First detection:

N Na b

We don’t know which BEC the atom came from

x

Position-dependent phase

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BEC Localisation

First detection:

N Na b

We don’t know which BEC the atom came from

x

Position-dependent phase

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BEC Localisation

N Na b

x

Probability density of second detection::

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BEC Localisation

N Na b

x

Probability density of second detection::

Feedback gives fringes with visibility ~ 0.5

After ~ N measurements:

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Robust relative phase state - classical

The phase of each condensate is still undefined:

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Fluffy bunny state

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Phase standard

N Na c

Nb

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Phase standard

N Na c

Nb

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Phase standard

N Na c

Nb

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Phase standard

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Properties

Absolute versus relative variables

a b c

• Robustness: subsequent measurements do not change the result – classical-like

• Transitivity: ingrained in our classical perception of the world

Entanglement is all around us – not just a “quantum phenomenon”!

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Position Localisation

Can do the same for position and momentum

Initial state of the mirrors:

Relative positionFlat

distribution

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Position Localisation

Can do the same for position and momentum

Initial state of the mirrors:

Relative positionFlat

distribution

Photon with momentum k, state before N:

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Position Localisation

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Position Localisation

Detection at D1:

Detection at D2:

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Position Localisation

1. Rau, Dunningham, Burnett, SCIENCE 301, 1081 (2003)

2. Dunningham, Rau, Burnett, SCIENCE 307, 872 (2005)

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Time

‘time’ ‘time’

No need to go through ‘middle-man’ of time

Angle of hour hand

Position of sun

Barbour view:

Position of sun

Angle of hour hand

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Entanglement of three particles

H|

|cn,m |n, m, E-n-m>

x23

x12

?

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Don’t need measurements

For every sequence of scattering events, a well-defined relative position (or phase) builds up

If we don’t measure the scattered particles the relative position is uncertain (classically)

Tracing over the scattered particles gives:

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Don’t need measurements

Just by shining light on particles they acquire a classical relative position - yet each particle remains highly quantum!

For every sequence of scattering events, a well-defined relative position (or phase) builds up

If we don’t measure the scattered particles the relative position is uncertain (classically)

Tracing over the scattered particles gives:

Well-localised state

Classical mixture

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Multi-particle

EntanglementsWILD PEDIGREE

Bunnies Cats Bats

Quantum Information

Everyday World

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Experimental progress

4 Be+ ions (2000)C60 molecules

(1999)

~ 109 Cooper pairs (2000)

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Experimental progress

4 Be+ ions (2000)C60 molecules

(1999)

~ 109 Cooper pairs (2000)

Future

Micro-mirrors

Biological systems?

(E. Coli)

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a

bc

Coupling between wells Interactions between atoms

Ref: Boyer et al, PRA 73, 031402 (2006)

Superfluid cats

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a

bc

Coupling between wells Interactions between atoms

Ref: Boyer et al, PRA 73, 031402 (2006)

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No rotation

Clockwise

Anticlockwise

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No rotation

Clockwise

Anticlockwise

Flow is quantized in units of 2 around the loop -- vortices

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How do we make them?

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How do we make them?

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How do we make them?

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How do we make them?

Cat

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Entanglement witness

Separable states

How do we see them?

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Metastable states

Spectroscopically scan the energy gap -- see it directly

How do we see them?

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What can we do with them?

+

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What can we do with them?

+For superfluid flows:

• Bell state experiments with macroscopic objects

• Precision measurements - quantum-limited gyroscopes

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Precision measurements of angular momentum

Gyroscopes

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Precision measurements of angular momentum

Can measure to within 1/N

Gyroscopes

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Summary

Next lecture: An even better way of using entanglement to make measurements

• The emergence of classicality from the quantum world

Number and phase of BEC

Position and momentum of micro-mirrors

• Schrodinger cat states

How can we make them

How can we see them

What can we do with them