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A Single Photon Source for Photon-atom Interaction

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A Single Photon Source for Photon-atom Interaction Xingxing Xing Centre for Quantum Info. & Quantum Control, Dept. of Physics, Univ. of Toronto – PowerPoint PPT presentation

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Title: A Single Photon Source for Photon-atom Interaction


1
A Single Photon Source for Photon-atom
Interaction
  • Xingxing Xing
  • Centre for Quantum
  • Info. Quantum Control,
  • Dept. of Physics, Univ. of Toronto

CQISC 2006, Calgary
2
Group member
  • Photonics lab _at_Toronto
  • Rob Adamson
  • Lynden (Krister) Shalm
  • Xingxing Xing
  • Dr. An-Ning Zhang
  • Prof. Aephraim Steinberg

3
Outline
  • Why single photon source?
  • Why photon-atom interaction?
  • How to build up a source?
  • What could we use the source for?

4
Motivation
  • Necessity of a single photon source?
  • Investigate non-classical behaviors
  • Use in quant logic, quant crypto., etc.

5
Motivation
  • Photons are ideal carrier for Quantum Info
    Processing and Q. Computation
  • easy to generate and manipulate
  • stable not interact much with environment
  • LOQC scheme could be essential as part of quantum
    computation networks
  • Problems
  • Photons dont interact much with envi. ? hard for
    storage
  • Experience losses during commu. ? reconstruct
    states
  • They dont interact with each other either! ?
    two-qubit gates?

6
Motivation
  • On the other hand, atoms are good for some
    aspects
  • They interact strongly with each other
  • ? good candidate for two-qubit gates
  • Long decoherence time is possible trapping
  • ? quantum memory and quantum repeater
  • Combination of the two Perfect!

7
Methods
Comparison of Different Schemes of Single photon
source
Different Sources Pros Cons
Attenuated laser easy Non-deterministic (Poisson)
Quantum dots Real single semiconductor tech Not feasible for photon-atom interaction
Single atom real single Hard (Kimbles heroic exp.)
Parametric down conversion Triggered deterministic Broadband1013 Hz Atomic 106 Hz
8
Methods
  • PDC is good, except for the bandwidth
  • Make use of cavity confine the spectrum, also
    known as Optical Parametric Oscillator (OPO)

9
Doppler-free Saturated Spectroscopy
  • Problem narrow linewidth of atoms 6MHz
  • Doppler shift
  • The frequency of a moving source/observer is
    shifted relative to the observer/source. NOTE
    the real freq. doesnt change!
  • For a moving observer
  • Vo speed of observer
  • positive if the observer is moving away
    from the source
  • negative if the observer is moving towards
    the source

10
Doppler
  • Stationary and moving source

11
Doppler effect in photon-atom interaction
  • Doppler broadening in absorption profile

12
OPO Setup
13
Testing of the laser linewidth
14
Next step
  • Optimize SHG
  • Setup OPO cavity and optimize it
  • Play with the source

15
Potential Applications
  • Electromagnetically Induced Transparency (EIT)
  • Quantum Memory
  • Quantum Repeater
  • As a tool to investigate the fundamentals of QM
    through interaction with cold atoms/BEC
  • Gap between Classical and quantum world?
  • Single photon - single atom?
  • For rent a single photon source for free space
    QKD

16
EIT
  • Group velocity coupling filed
  • The state of interaction system photon atom

17
Storage through EIT
Fleischhauer, PRL 84, 5094, 2000
18
Quantum repeater
L.-M., Duan et.al., 414, 413
19
Summary
  • A scheme for narrow bandwidth single-photon
    source (triggered deterministic)
  • Such photon-atom interaction could help fill the
    gap between LCQO and atomic physics
  • Questions? Comments? Suggestions?
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