Quantum Entanglement and Bells Inequalities Zachary Evans, Joel - - PowerPoint PPT Presentation

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Quantum Entanglement and Bells Inequalities Zachary Evans, Joel - - PowerPoint PPT Presentation

Quantum Entanglement and Bells Inequalities Zachary Evans, Joel Howard, Jahnavi Iyer, Ava Dong, and Maggie Han Institute of Optics, University of Rochester Opt 101 Meeting, December 4, 2012, Rochester NY Entanglement, What is it? A


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Quantum Entanglement and Bell’s Inequalities

Zachary Evans, Joel Howard, Jahnavi Iyer, Ava Dong, and Maggie Han

Opt 101 Meeting, December 4, 2012, Rochester NY

Institute of Optics, University of Rochester

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 A state of being of two or more particles with special strong correlations  Allows for reliable conclusions to be made about the state of one by the measurement of the state of the other  Non local  Multiple forms of entanglement (Energy, momentum, polarization, spin, etc…)

Distance

Entanglement, What is it?

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 A state of being of two or more particles with special strong correlations  Allows for reliable conclusions to be made about the state of one by the measurement of the state of the other  Non local  Multiple forms of entanglement (Energy, momentum, polarization, spin, etc…)

Entanglement, What is it?

Distance

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EPR and Bell

 EPR introduced entanglement, in 1935, but did not believe in it (“spooky action at a distance”)  Einstein disagreed with non-locality, and sought an alternate explanation involving hidden variables to complete quantum mechanical theory.  In 1964, John Bell developed a series of inequalities which allowed experimentalists to verify entanglement.  Clauser, Horne, Shimony, and Holt created the commonly-used version of Bell’s Inequality.  This experiment was made by Freedman and Clauser in 1972, and a more modern version was performed by Aspect in 1981 and 1982.

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Experiment: Set Up

1. Laser 2. Quartz plate 3. BBO Crystals 4. Polarizers 5. Interference Filters 6. Avalanche Photodiode Modules (APD)

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SLIDE 6

Experiment: Set Up

Argon Ion Laser ~363.8 nm Photo Detectors, Collecting System, Polarizers and Interference Filters BBO Crystals ~727.62 nm

BE VERY CAREFUL BE VERY CAREFUL BE VERY CAREFUL BE VERY CAREFUL BE VERY CAREFUL BE VERY CAREFUL

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Experiment: BBO Crystals

  • Creates Two Cones of Entangled Photons Via

SPDC

  • 10-10 Probability of photons SPDC
  • Two Vertically Polarized, Two Horizontally

Polarized from 45 degree incident polarization

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Experiment: Quartz Plate

  • Compensates for the phase difference

between the different polarizations that emerge from the BBO Crystal

  • Important to have overlapping cones
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Collecting the Correct Photons

Polarizer

  • Selects polarization

Interference Filter

  • Rejects Laser light

Microscope Objective

  • Focuses light into the
  • ptical fiber
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Counting the Photons

Avalanche Photo Detectors

  • Each detector detects single photons
  • Creates TTL pulses for the computer

to read Computer chip counts the number of electrical pulses from each detector (singles) and simultaneous pulses (coincidences)

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Basic Procedure

  • 1. Create SPDC photons in BBO crystals
  • 2. Change relative polarizer angle between

polarizer A and B (angle A – angle B)

  • 3. Measure number of simultaneous counts

(coincidence count) for that relative angle, and repeat

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SLIDE 12
  • A series of classical relationships determines

whether or not we have achieved entanglement.

  • If Bells inequality is violated for some value of

parameters then entanglement is shown to

  • ccur
  • 16 Coincidence Count measurements to

enter into the inequality and prove entanglement occurred

How to Prove Evidence of Entanglement

Bells Inequality's:

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SLIDE 13

How to Prove it

 Bells Inequality's!!

16 Measurements at definite angles alpha and beta If S is greater than 2, entanglement has be shown to

  • ccur
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Results:

Bell’s Inequality Violation

E(a,b) 0.830687 E(a‘,b‘) 0.437502 E(a‘,b) 0.342053 E(a,b‘)

  • 0.63068

2.240921 E Values N Values S Value

Coincidence counts 26.06104 4.683286 3.020993 21.81208 16.1685 23.45386 19.45366 6.812767 2.822459 37.80719 37.1211 8.819509 6.171918 12.08339 36.10151 24.83661 Polarizer A Polarizer B

  • 45
  • 22.5
  • 45

22.5

  • 45

67.5

  • 45

112.5

  • 22.5

22.5 67.5 112.5 45

  • 22.5

45 22.5 45 67.5 45 112.5 90

  • 22.5

90 22.5 90 67.5 90 112.5

Angles 1 second acquisition time

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SLIDE 15
  • 5

5 10 15 20 25 30 35 20 40 60 80 100 120 140 160 180 200 220 240 260 280 300 320 340 360 Coincidence Count Relative Polarizer Angle (Degrees)

Dependence of Coincidence Count of Relative Polarizer Angles

Polarizer A= 135 Degrees Polarizer A= 45 Degrees

Fringe Visibility: 1 > 0.71

Fringe Visibility

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500 1000 1500 2000 2500 3000 3500 4000 50 100 150 200 250 300 350 Singles Count Relative Polarization Degree

Singles Count Vs. Angle for 90 Degrees

Singles Count A Singles Count B

500 1000 1500 2000 2500 3000 3500 4000 4500 5000 50 100 150 200 250 300 350 Singles Count Relative Polarization Degree

Singles Count vs. Angle for 0 Degrees

Singles Count A Singles Count B

Singles Count

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SLIDE 17

Applications Of Entanglement

  • Quantum Computing
  • Quantum Encryption
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Quantum Computing

  • Advantages of Quantum Computing
  • Speed up computation, and more powerful

computation because the quantum computer might be able to do multiple calculations

  • simultaneously. And it also means parallel

calculation because of entanglement

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SLIDE 19
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Alice and Bob each receive one of a pair of entangled photons Measurements along parallel axes- key generation Oblique angles- test inequalities Evesdropping will destroy the entanglement and reduce the degree of violation in Bell's Inequalities.

Ekert Protocol

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Thank you Questions?

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http://arxiv.org/pdf/quant-ph/9912117.pdf http://plus.maths.org/content/os/issue35/features /ekert/index http://science.howstuffworks.com/science-vs- myth/everyday-myths/quantum-cryptology6.htm http://news.bbc.co.uk/2/hi/science/nature/766131 1.stm

Referenced Sources