demonstration of two-plasmon quantum interference hyunseok lee 1
TRANSCRIPT
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■ Overview
• Background Recap• Surface Plasmon • Two Photon Quantum Interference
• Experiment Procedure• Schematic• Theoretical analysis• Waveguide Design
• Result & Conclusion• Measurement• Conclusion• Future research
Plasmonic TPQI
Recap
Surface Plasmon
TPQI
Procedure
Schematic
Theory
WaveguideDesign
Result
Conclusion
Future re-search
3
■ Surface Plasmon
• Electronic-optical excitations
• Strongly interact with environment• Decoherence question unsettled
• Test of indistinguishability!
Plasmonic TPQI
Recap
Surface Plasmon
TPQI
Procedure
Schematic
Theory
WaveguideDesign
Result
Conclusion
Future re-search
4
Plasmonic TPQI
■ Two Photon Quantum Interference
Recap
Surface Plasmon
TPQI
Procedure
Schematic
Theory
WaveguideDesign
Result
Conclusion
Future re-search
Represent the electric fields of the modes by annihilation operators:
Represent the action of the beam splitter by an operator with two assumptions:
Then the final state of the system given one photon in each input follows:
Detectors placed at the outputs will never click simultaneously!
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■ Schematic (1)
• Laser -> SPDC -> single photon pairs• Waveguide -> converted to plasmon -> TPQI • Back to photon -> detectors
Plasmonic TPQI
Recap
Surface Plasmon
TPQI
Procedure
Schematic
Theory
WaveguideDesign
Result
Conclusion
Future re-search
6
■ Schematic (2) Plasmonic
TPQI
Recap
Surface Plasmon
TPQI
Procedure
Schematic
Theory
WaveguideDesign
Result
Conclusion
Future re-search
* C. Hong, Z. Ou, L. Mandel, Phys. Rev. Lett. 59, 2044-2046 (1987).
• Dielectric case
• Challenge: Plasmonic waveguide• Theory• Simulation• Fabrication
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■ TPQI in a Lossy Coupler (1)Plasmonic
TPQI
Recap
Surface Plasmon
TPQI
Procedure
Schematic
Theory
WaveguideDesign
Result
Conclusion
Future re-search
• Supermodes
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■ TPQI in a Lossy Coupler (2)Plasmonic
TPQI
Recap
Surface Plasmon
TPQI
Procedure
Schematic
Theory
WaveguideDesign
Result
Conclusion
Future re-search
𝑃 (1a ,1b )=|𝑡|4+|𝑟|4+ [𝑡 2𝑟 ∗2+𝑟 2𝑡∗ 2 ¿ 𝐼 ,
𝐻𝑂𝑀𝑣𝑖𝑠𝑖𝑏𝑖𝑙𝑖𝑡𝑦=1−𝑃 (1a ,1b ; 𝐼=1 )𝑃 (1a ,1b ; 𝐼=0 )
=1−2cos2∆𝜃 .
*S. Barnett, J. Jeffers, A. Gatti, R. Loudon,Phys. Rev. A. 57, 2134(1998)
Coin
cide
nce
Rate
Delay
Ideal TPQI with loss
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■ SimulationPlasmonic
TPQI
Recap
Surface Plasmon
TPQI
Procedure
Schematic
Theory
WaveguideDesign
Result
Conclusion
Future re-search
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■ Waveguide Design (1)Plasmonic
TPQI
Recap
Surface Plasmon
TPQI
Procedure
Schematic
Theory
WaveguideDesign
Result
Conclusion
Future re-search
• DLSPPW design• Optimized dimension & material
* R. Briggs, J. Grandidier, S. Burgos, E. Feigenbaum, H. A. Atwa-ter, Nano Lett. 2010, 10(12)
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■ Waveguide Design (2)Plasmonic
TPQI
Recap
Surface Plasmon
TPQI
Procedure
Schematic
Theory
WaveguideDesign
Result
Conclusion
Future re-search
• Dielectric waveguide for comparison• S-bends prevent stray light background
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94.4+/-0.3%
0.12+/-0.01 ps
■ MeasurementPlasmonic
TPQI
Recap
Surface Plasmon
TPQI
Procedure
Schematic
Theory
WaveguideDesign
Result
Conclusion
Future re-search
• Plasmonic TPQI is clearly shown
93.2+/-1.0%
0.11+/-0.01 ps
Plasmonic TPQIPhotonic TPQI
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■ ConclusionPlasmonic
TPQI
Recap
Surface Plasmon
TPQI
Procedure
Schematic
Theory
WaveguideDesign
Result
Conclusion
Future re-search
• Successfully demonstrated unam-biguous quantum interference in plasmonic waveguides• Close correspondence between di-
electric and plasmonic• Identical photons remain indistinguish-
able
• High degree of coherence• Application in quantum computing if
loss can be mitigated.
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■ Future ResearchPlasmonic
TPQI
Recap
Surface Plasmon
TPQI
Procedure
Schematic
Theory
WaveguideDesign
Result
Conclusion
Future re-search
• Further study of plasmon• Dispersive regime
• Extending the technology• Integrated quantum photonics
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■ AcknowledgementsPlasmonic
TPQI
Recap
Surface Plasmon
TPQI
Procedure
Schematic
Theory
WaveguideDesign
Result
Conclusion
Future re-search
• Air Force Office of Scientific Research• Kavli Nanoscience Institute
• Further reading:J. S. Fakonas, H. Lee, Y. A. Kelaita, H. A. Atwater, Nat. Photonics 8, 317–320 (2014).
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