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Single Photon Interference Jeff, Jacob, Bryce, Edward, and Julie.

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Presentation on theme: "Single Photon Interference Jeff, Jacob, Bryce, Edward, and Julie."— Presentation transcript:

1 Single Photon Interference Jeff, Jacob, Bryce, Edward, and Julie

2 Young’s Double Slit Experiment YAY!

3 What is it?  First conducted in 1801 by Thomas Young  Light passed through a barrier with two slits (before it usually passed through a single slit to make the light coherent)  The light diffracted through each slit  Created interference pattern  In order to interfere the light that passes through the slit must be of the same frequency and polarization and it must be coherent

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5 Particles vs. Waves Particle  If light acts as a particle, only two slits will appear on the screen Wave  The light will diffract and interfere, making many fringes

6 Why is this important?  This proves light acts not only as a particle, but also as a wave!

7 Equations for the Fringes

8 Many Photon Interference Acquisition Time:.1 sec Attenuation: 3 optical depths Amplification: x1

9 Single Photon  When a single photon is used, wave interference is still present  It is impossible for a photon to act as a wave as it is can only go through one slit  If one slit is blocked, there is no interference

10 Energy of a Single Photon

11  Power of 1 photon per meter  P=9.421 ∗ 10 −11 W  The power of our laser is  P=9.1 ∗ 10 −7 W  So we use 3 optical depths to attenuate the beam to single photon energy levels.

12 Single Photon Interference Acquisition Time:.1 sec Attenuation: 3 optical depths Amplification: x100

13 Single Photon Interference Acquisition Time:.1 sec Attenuation: 3 optical depths Amplification: x200

14 Single Photon Interference Acquisition Time: 1 sec Attenuation: 3 optical depths Amplification: x100

15 Interferometry Mach-Zehnder Interferometer

16  Power of 1 photon per meter  P=9.421 ∗ 10 −11 W  The power of our laser is  P=6.17 ∗ 10 −5 W  So we use 5 optical depths to attenuate the beam to single photon energy levels.

17 Strong field Acquisition Time:.1sec Attenuation: 5 optical depths Amplification: x100

18 Single Photon Acquisition Time:.1 sec Attenuation: 5 optical depths Amplification: x100

19 Single Photon – Horizontal Polarization Blocked Acquisition Time:.1 sec Attenuation: 5 optical depths Amplification: x100

20 Single Photon – Vertical Polarization Blocked Acquisition Time:.1 sec Attenuation: 5 optical depths Amplification: x100

21 Important Observations  When path of photon is unknown, fringes are observed  When path of photon is known, fringes are not observed

22 Summary  Young’s Double Slit Experiment  Fringes were observed under high intensity, as well as with only a single photon.  Interferometer  Fringes were observed under high intensity as well as with only a single photon.  When either path of the interferometer was blocked, fringes were not observed.

23 What Problems Did We Encounter? Single Photon Interference Acquisition Time:.1 sec Attenuation: 5 optical depths Amplification: x100

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25 Conclusion  Single photons behaved the same way as the high intensity beam.  In the double slit experiment, the single photon appeared to interfere with itself – going through both slit simultaneously.  In the interferometer the single photon appeared to take both paths simultaneously – blocking a path removed interference fringes.

26 Sources  t/chp1719_light/lesson58.htm t/chp1719_light/lesson58.htm  slit/default.asp slit/default.asp  ubleslit.htm ubleslit.htm  pages/Demo/modern/demo/7a5520.htm pages/Demo/modern/demo/7a5520.htm  The book – Seeing the Light


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