Single Photon Transistor

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    Introduction to Single Photon Transistor

    Surface plasmons

    Nanowires

    The concept of emitter atom SPT as a switch

    Nanotip for storing photon

    Limitations of nanowires

    Advantages

    Applications

    Conclusion

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    Single Photon transistor is an optical transistor .

    Propagation of the signal is controlled by the presence or

    absence of a Single Photon.

    The propagating signal is another Photon or a flow of

    Photons itself.

    Photons rarely interact with each other. Any possibleinteraction will be very weak at a single Photon level.

    Converting photons to charges in the form of surface

    plasmons will strengthen the interactions between Photons.

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    The word plasmon means charges.

    Surface plasmons form at a metal-dielectric interface.

    When stream of photons are applied to the interface , field

    associated with Photons polarizes the interface by inducing

    charges.

    The opposite charges align at the interface to form a waveof density that propagate along the metal-dielectric interface.

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    WHY NANOWIRES ??? Surface plasmons do not interact well with optical fibers.

    A possible solution is using conducting metal nanowires.

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    Typical nanowires has diameters less

    than 100nm.

    Metallic nanowires with diameters of

    40 - 60nms can be used for guidingsurface plasmons.

    Nanowire acts as the metal and the

    air surrounding the nanowire acts asdielectric.

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    EMITTER ATOM for inducing INTERACTION

    Surface plasmons cannot be made to hit each other.

    Use an emitter atom as anintermediary.

    Photons are shot at the atomusing nanowires.

    When they hit the atom an interaction occurs between thephotons.

    One Photon imparts information to the other Photon.

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    Emitter atom can achieve two

    energy levels;

    ground(|g>) and excited(|e>).

    State g

    The reflection coefficient isapproximately,

    r=-1(1-1/p)

    P= Purcell factor

    state eemitter will act like an open gate.

    TWO LEVEL EMITTER

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    THREE LEVEL EMITTER

    Emitter can have three energy levels |g>,|e> and ,surface

    plasmon state ,|s> .

    The |g> can go to |s> only by the application of a Photon

    which is our single photon.

    |s> is coupled to |e> by the application of an external field,(t), at Rabi Frequency.

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    The system is initialized in state g.Then a control pulse is sent(may or may not have a photon)

    If there was a photon present, the emitter will undergo a spin slip

    from g to s, and remain unchanged otherwise..

    Transistor is OFF when there is no external photon,and it is ON when single photon is present in theincoming field.

    continued

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    Nanotip is a nanowire tapered at the end.

    Single photon travels from one end of nanotip toemitter atom at the tapered end.

    Emitter is located along the z-axis of the nanotip.

    NANOTIP FOR STORING SINGLE PHOTON

    SPTNanotip

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    Long way efficient transportation is not possible

    Amplitude reduction

    Reduced clarity of surface plasmons

    Photons can effectively propagate through waveguides.

    Wave guide transfers photons to nanowires only atthe emitter .

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    DielectricNanowire Interfacing:

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    Work on broad range of frequencies of light

    Easy to fabricate

    Reduced size

    Very efficient

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    Optical computers

    Optical communications

    Photon detectors

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    The operation of the SPT is controlled by a single

    external photon stored in a nanotip.

    The flow of signal Photons through a nanowire can be

    controlled by changing the internal state of emitter atom

    assisted by a control field.

    A new world of optical circuits can be produced using SPT.

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    http://www.spectrum.ieee.org/aug07/5497Scheme for a Single-Photon Transistorbysaswato das // august 2007

    www.nature.com/naturephysics

    Nature Physics Vol 3 November 2007

    A single-photon transistor using nanoscale

    surface plasmons

    Darrick E. Chang, Anders S. Srensen, Eugene A.Demler and Mikhail D. Lukin

    www.springerlink.com/index/U5L25Q114741QP2V.pdf

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