Spontaneous Parametric Down Conversion final presentation.pdf · Results of SPDC Investigation 145...

33
Spontaneous Parametric Down Conversion Sean Gallivan & Kerry Olivier

Transcript of Spontaneous Parametric Down Conversion final presentation.pdf · Results of SPDC Investigation 145...

Page 1: Spontaneous Parametric Down Conversion final presentation.pdf · Results of SPDC Investigation 145 345 545 745 945 1145 1345 1.5 2 2.5 3 3.5 4 4.5 Coincidence Counts/Second B Angle

Spontaneous Parametric Down Conversion

Sean Gallivan & Kerry Olivier

Page 2: Spontaneous Parametric Down Conversion final presentation.pdf · Results of SPDC Investigation 145 345 545 745 945 1145 1345 1.5 2 2.5 3 3.5 4 4.5 Coincidence Counts/Second B Angle

General Overview

Conservation of Energy:

Conservation of Momentum:

Page 3: Spontaneous Parametric Down Conversion final presentation.pdf · Results of SPDC Investigation 145 345 545 745 945 1145 1345 1.5 2 2.5 3 3.5 4 4.5 Coincidence Counts/Second B Angle

Why is it called SPDC?

• Spontaneous: Generated by quantum vacuum fields

• Parametric: Phase relationship between input and output fields

• Down Conversion: Signal & Idler frequencies are lower than pump

Page 4: Spontaneous Parametric Down Conversion final presentation.pdf · Results of SPDC Investigation 145 345 545 745 945 1145 1345 1.5 2 2.5 3 3.5 4 4.5 Coincidence Counts/Second B Angle

Why Should I Care?

• Production of single photons

• Photon entanglement is ripe for quantum information experiments

• It’s cool!

Page 5: Spontaneous Parametric Down Conversion final presentation.pdf · Results of SPDC Investigation 145 345 545 745 945 1145 1345 1.5 2 2.5 3 3.5 4 4.5 Coincidence Counts/Second B Angle

Lab Setup to Investigate SPDC

Page 6: Spontaneous Parametric Down Conversion final presentation.pdf · Results of SPDC Investigation 145 345 545 745 945 1145 1345 1.5 2 2.5 3 3.5 4 4.5 Coincidence Counts/Second B Angle

Results of SPDC Investigation

145

345

545

745

945

1145

1345

1.5 2 2.5 3 3.5 4 4.5

Coin

cide

nce

Coun

ts/S

econ

d

B Angle (Degrees)

Coincidence Counts as Leg A is Held Constant and Leg B is Swept

Page 7: Spontaneous Parametric Down Conversion final presentation.pdf · Results of SPDC Investigation 145 345 545 745 945 1145 1345 1.5 2 2.5 3 3.5 4 4.5 Coincidence Counts/Second B Angle

Gaussian Fit of Data

2.0 2.5 3.0 3.5 4.0Angle °

200

400

600

800

1000

1200

Coincidences AB

Page 8: Spontaneous Parametric Down Conversion final presentation.pdf · Results of SPDC Investigation 145 345 545 745 945 1145 1345 1.5 2 2.5 3 3.5 4 4.5 Coincidence Counts/Second B Angle

Measurement of

Page 9: Spontaneous Parametric Down Conversion final presentation.pdf · Results of SPDC Investigation 145 345 545 745 945 1145 1345 1.5 2 2.5 3 3.5 4 4.5 Coincidence Counts/Second B Angle

Results

• Best measurement: = .713 Standard Deviation = .0123>23 Standard Dev.’s below 1(10 measurements, 10s per measurement)

• Worst measurement: = .702Standard Deviation = .052402>5 Standard Dev.’s Below 1(10 measurements, 1s per measurement)

Page 10: Spontaneous Parametric Down Conversion final presentation.pdf · Results of SPDC Investigation 145 345 545 745 945 1145 1345 1.5 2 2.5 3 3.5 4 4.5 Coincidence Counts/Second B Angle

Single Photon Interference

Page 11: Spontaneous Parametric Down Conversion final presentation.pdf · Results of SPDC Investigation 145 345 545 745 945 1145 1345 1.5 2 2.5 3 3.5 4 4.5 Coincidence Counts/Second B Angle
Page 12: Spontaneous Parametric Down Conversion final presentation.pdf · Results of SPDC Investigation 145 345 545 745 945 1145 1345 1.5 2 2.5 3 3.5 4 4.5 Coincidence Counts/Second B Angle

Results of Single Photon Interference

0

200

400

600

800

1000

1200

1400

1600

1800

2000

0 0.00005 0.0001 0.00015 0.0002 0.00025 0.0003

Coin

cide

nce

Coun

ts

Angular Displacement of BDP

Single Photon Interference In a Quantum Eraser (θ1 = 38°, V = 81.9%)

AB

AB'

Page 13: Spontaneous Parametric Down Conversion final presentation.pdf · Results of SPDC Investigation 145 345 545 745 945 1145 1345 1.5 2 2.5 3 3.5 4 4.5 Coincidence Counts/Second B Angle

Visibility of Interference Patterns & Quantum Erasers

• θ1 = 38°, Visibility = 81.9%, Expected g2 = .24 (SD = .42)• θ1 = 10°, Visibility = 30.2%, Expected g2 = .24 (SD = .36)• θ1 = 0° , Visibility = 31.4%, Expected g2 = .24 (SD = .29)• θ3 = 0°, Visibility = 17.5%, Expected g2 = .24 (SD = .16)

Page 14: Spontaneous Parametric Down Conversion final presentation.pdf · Results of SPDC Investigation 145 345 545 745 945 1145 1345 1.5 2 2.5 3 3.5 4 4.5 Coincidence Counts/Second B Angle

Local Realism

• Locality: A measurement in one location cannot affect a measurement performed elsewhere

• Reality: ‘real’ objects have measurable quantities regardless of if we look at them or not

Page 15: Spontaneous Parametric Down Conversion final presentation.pdf · Results of SPDC Investigation 145 345 545 745 945 1145 1345 1.5 2 2.5 3 3.5 4 4.5 Coincidence Counts/Second B Angle

Bell’s Inequality & Testing Local Realism

• Joint probability of photons polarized in 2 directions:

• Bell-Clauser-Horne Inequality:

Page 16: Spontaneous Parametric Down Conversion final presentation.pdf · Results of SPDC Investigation 145 345 545 745 945 1145 1345 1.5 2 2.5 3 3.5 4 4.5 Coincidence Counts/Second B Angle

Attempted Local Realism Setup

Page 17: Spontaneous Parametric Down Conversion final presentation.pdf · Results of SPDC Investigation 145 345 545 745 945 1145 1345 1.5 2 2.5 3 3.5 4 4.5 Coincidence Counts/Second B Angle

New Equipment for Local Realism

• Paired BBO

• Berek Compensator

Orientation Dial:Rotates housing (orienting the slow axis of the compensator plate)

Retardance Indicator: How much retardance to apply

Page 18: Spontaneous Parametric Down Conversion final presentation.pdf · Results of SPDC Investigation 145 345 545 745 945 1145 1345 1.5 2 2.5 3 3.5 4 4.5 Coincidence Counts/Second B Angle

Minimizing Noise

Page 19: Spontaneous Parametric Down Conversion final presentation.pdf · Results of SPDC Investigation 145 345 545 745 945 1145 1345 1.5 2 2.5 3 3.5 4 4.5 Coincidence Counts/Second B Angle
Page 20: Spontaneous Parametric Down Conversion final presentation.pdf · Results of SPDC Investigation 145 345 545 745 945 1145 1345 1.5 2 2.5 3 3.5 4 4.5 Coincidence Counts/Second B Angle

Clothing makes a big difference

Page 21: Spontaneous Parametric Down Conversion final presentation.pdf · Results of SPDC Investigation 145 345 545 745 945 1145 1345 1.5 2 2.5 3 3.5 4 4.5 Coincidence Counts/Second B Angle

Future Project Plans

• Labview Programming for Local Realism/obtain motorized waveplates

• Find optimal density filter attenuation• Get 4 of the same density filters• Find some way of better regulating A’ and B’

leg angles (they swivel too easily)• Set up a curtain to pull back and forth across

the white board

Page 22: Spontaneous Parametric Down Conversion final presentation.pdf · Results of SPDC Investigation 145 345 545 745 945 1145 1345 1.5 2 2.5 3 3.5 4 4.5 Coincidence Counts/Second B Angle

Questions?

Page 23: Spontaneous Parametric Down Conversion final presentation.pdf · Results of SPDC Investigation 145 345 545 745 945 1145 1345 1.5 2 2.5 3 3.5 4 4.5 Coincidence Counts/Second B Angle

More on SPCD & BBOs• Angle of down converted photon emission is defined by orientation

of optical axis of BBO with respect to the orthogonal face

• BBO emits down conversion photons in a cone (for type I down conversion)

Page 24: Spontaneous Parametric Down Conversion final presentation.pdf · Results of SPDC Investigation 145 345 545 745 945 1145 1345 1.5 2 2.5 3 3.5 4 4.5 Coincidence Counts/Second B Angle

Piezo Actuators

Page 25: Spontaneous Parametric Down Conversion final presentation.pdf · Results of SPDC Investigation 145 345 545 745 945 1145 1345 1.5 2 2.5 3 3.5 4 4.5 Coincidence Counts/Second B Angle

Calculating Angular Displacement

Beam separation as a function of optical axis angle theta and block length D

Page 26: Spontaneous Parametric Down Conversion final presentation.pdf · Results of SPDC Investigation 145 345 545 745 945 1145 1345 1.5 2 2.5 3 3.5 4 4.5 Coincidence Counts/Second B Angle

Beam Displacement Polarizers

Page 27: Spontaneous Parametric Down Conversion final presentation.pdf · Results of SPDC Investigation 145 345 545 745 945 1145 1345 1.5 2 2.5 3 3.5 4 4.5 Coincidence Counts/Second B Angle

‘Interference’ Without Quantum Erasure

400

600

800

1000

1200

1400

0 0.00005 0.0001 0.00015 0.0002 0.00025 0.0003

Coin

cide

nce

Coun

ts

Angular Displacement of BDP

Interference Pattern With No Quantum Erasure (θ1 = 10°, V = 30.2%)

AB

AB'

400

600

800

1000

1200

1400

0 0.0001 0.0002 0.0003 0.0004 0.0005

Coin

cide

nce

Coun

ts

Angular Displacement of BDP

Single Photon Interference With Little Quantum Erasure (θ1 = 0°, V = 31.4%)

AB

AB'

3000

3500

4000

4500

5000

5500

6000

6500

0 0.0001 0.0002 0.0003 0.0004 0.0005 0.0006

Coin

cide

nce

Coun

ts

Angular Displacement of BDP

Interference Pattern With No Quantum Erasure (θ3 = 0°, V = 17.5%)

AB

AB'

Page 28: Spontaneous Parametric Down Conversion final presentation.pdf · Results of SPDC Investigation 145 345 545 745 945 1145 1345 1.5 2 2.5 3 3.5 4 4.5 Coincidence Counts/Second B Angle

Avalanche Photodiodes

• Utilizes photoelectric effect• Impact ionization allows for small signal

detection (i.e. single photons) due to ‘self-sustaining avalanche’ with current in mAs

• This current is then subsided by lowering bias voltage down to breakdown voltage

Page 29: Spontaneous Parametric Down Conversion final presentation.pdf · Results of SPDC Investigation 145 345 545 745 945 1145 1345 1.5 2 2.5 3 3.5 4 4.5 Coincidence Counts/Second B Angle

Entangled States

• Assuming pump is at 45 degrees & BBO pairs are sufficiently close together: 2 photon pairs are indistinguishable

• Thus we must consider them to be superpositions of both possible polarizations:

Page 30: Spontaneous Parametric Down Conversion final presentation.pdf · Results of SPDC Investigation 145 345 545 745 945 1145 1345 1.5 2 2.5 3 3.5 4 4.5 Coincidence Counts/Second B Angle

Individual & Joint Probabilities

• If 2 photons are in entangled state, then measurements made on 1 photon are random

• Measurements made on pairs of photons will be perfectly correlated

Page 31: Spontaneous Parametric Down Conversion final presentation.pdf · Results of SPDC Investigation 145 345 545 745 945 1145 1345 1.5 2 2.5 3 3.5 4 4.5 Coincidence Counts/Second B Angle

Labview Woes

Page 32: Spontaneous Parametric Down Conversion final presentation.pdf · Results of SPDC Investigation 145 345 545 745 945 1145 1345 1.5 2 2.5 3 3.5 4 4.5 Coincidence Counts/Second B Angle

Labview Woes Cont’d

Page 33: Spontaneous Parametric Down Conversion final presentation.pdf · Results of SPDC Investigation 145 345 545 745 945 1145 1345 1.5 2 2.5 3 3.5 4 4.5 Coincidence Counts/Second B Angle

Overview of Troubleshooting Processes

Testing to see if you're even getting down conversion:• Try blocking the path down converted photons would take

right after the crystal: if the number decreases you are seeing down conversion, if it remains the same you are not

• for experiments other than 1, try rotating the waveplate: down converted light will oscillate back and forth, noise will remain constant

• try turning the pump off and on and simply look at how much of a difference you get

If you're getting 0 for any detection or coincidence, something is wrong.

• Check to see if all the detectors are on (on the front panel)• Check the fpga switches