a single photon source for photon-atom interaction
DESCRIPTION
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. Group member. Photonics lab @Toronto Rob Adamson Lynden (Krister) Shalm Xingxing Xing Dr. An-Ning Zhang - PowerPoint PPT PresentationTRANSCRIPT
A Single Photon Source for
Photon-atom InteractionXingxing XingCentre for Quantum Info. & Quantum Control, Dept. of Physics, Univ. of Toronto
CQISC 2006, Calgary
CQISC 2006, Calgary 2Xingxing Xing, U.of Toronto
Group member
Photonics lab @Toronto
Rob Adamson
Lynden (Krister) Shalm
Xingxing Xing
Dr. An-Ning Zhang
Prof. Aephraim Steinberg
CQISC 2006, Calgary 3Xingxing Xing, U.of Toronto
Outline
Why single photon source? Why photon-atom interaction? How to build up a source? What could we use the source for?
CQISC 2006, Calgary 4Xingxing Xing, U.of Toronto
Motivation
Necessity of a single photon source?
Investigate non-classical behaviors
Use in quant logic, quant crypto., etc.
CQISC 2006, Calgary 5Xingxing Xing, U.of Toronto
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 computatio
n networks
Problems Photons don’t interact much with envi. hard for storage Experience losses during commu. reconstruct s
tates They don’t interact with each other either! two-qubit gat
es?
CQISC 2006, Calgary 6Xingxing Xing, U.of Toronto
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!
CQISC 2006, Calgary 7Xingxing Xing, U.of Toronto
Methods
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 (Kimble’s heroic exp.)
Parametric down conversion
Triggered deterministic
Broadband:1013 Hz
Atomic: 106 Hz
Comparison of Different Schemes of Single photon source
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Methods
PDC is good, except for the bandwidth Make use of cavity: confine the spectrum, also known as
Optical Parametric Oscillator (OPO)
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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. doesn’t 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
v
vff 0
0 1
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Doppler
Stationary and moving source
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Doppler effect in photon-atom interaction Doppler broadening in absorption profile
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OPO Setup
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Testing of the laser linewidth
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Next step…
Optimize SHG
Setup OPO cavity and optimize it
Play with the source…
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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…
CQISC 2006, Calgary 16Xingxing Xing, U.of Toronto
EIT
Group velocity & coupling filed
The state of interaction system: photon + atom:
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Storage through EIT
Fleischhauer, PRL 84, 5094, 2000
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Quantum repeater
L.-M., Duan et.al., 414, 413
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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?