Optical Photonic Gates

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    Circuitos Fotnicos Integrados

    Portas Lgicas

    Vitaly F. Rodrguez-Esquerre

    [email protected]

    Departmento de Engenharia Eltrica

    Programa de Ps-Graduao em Engenharia Eltrica

    Universidade Federal de Bahia, Salvador, Brasil

    mailto:[email protected]:[email protected]
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    Motivao

    Fig. 1. IP Traffic Bandwitdh (2006-2015)

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    Alternativas

    Aumentar a capacidade das fibras instaladas

    -Tcnicas de modulao-Deteo coerente-Novos equipamentos

    Instalao de novas fibras

    -Fibras com mltiplos ncleos

    Processamento Totalmente ptico (limitao doscircuitos baseados em semicondutores)-Novos conceitos de guiamento-Portas lgicas pticas-Propriedades no-lineares-Assimetrias nas geometrias

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    Circuito Fotnico Integrado

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    Vantagens da Fotnica

    -Increase in the speed of computation.-Immune to electromagnetic interference.-Free from electrical short circuits.-Have low-loss transmission and large bandwidth.-Speed of light in photonic circuits will be close to speed of light in vacuum-Capable of communicating several channels in parallel without

    interference.-Possesses superior storage density and accessibility-No power loss due to excess of heating.-Life of the hardware of optical computer is more

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    Periodic Electromagnetic Media

    1887 1987

    with photonic band gaps: optical insulators

    2-D

    periodic intwo directions

    3-D

    periodic inthree directions

    1-D

    periodic inone direction

    Cristais Fotnicos

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    Planewave

    k

    for most l, beam(s) propagate through crystal withoutscattering (scattering cancels coherently)

    ...but for some l(~ 2a), no light can propagate: a photonic band gap

    a

    Cristais Fotnicos

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    Periodic Electromagnetic Media

    with photonic band gaps: optical insulators

    3D Pho to nic C rysta l with De fe c tscan trap light in cavities and waveguides(wires)

    Cristais Fotnicos

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    1D

    2D

    3D

    Cristais Fotnicos

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    Deep-etchedMacroporous silicon

    2D with vertical

    confinement:

    High vertical refractive

    index contrast,

    e.g. membranes

    or low vertical refractiveindex contrast

    e.g. GaAs or InP.

    Purely 2D:

    a = 1.5 m

    h = 100 m

    Cristais Fotnicos

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    Cristais Fotnicos

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    Question :How can we understand Photonic Crystals?

    Answer :Every Macroscopic Electromagnetic Phenomenoncan be understand by the Maxwell's Equations.

    kxe kytransversal propagation constant

    Cristais Fotnicos

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    Periodical Structures

    Square

    lattice

    Triangular

    Lattice

    Brillouin irreductible

    zone

    Bloch-Floquet theorem

    Cristais Fotnicos

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    Periodical Structures

    Square

    lattice

    Brillouin

    irreductible

    zone

    Cristais Fotnicos

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    Periodical Structures

    Triangular

    Lattice

    Brillouin

    irreductible

    zone

    Cristais Fotnicos

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    Porta Lgica AND

    Y.-P. Yangetal./OpticsCommunications297(2013)165168

    Fig. 1. Proposed photonic crystal logic AND gate

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    Porta Lgica AND

    Y.-P. Yangetal./OpticsCommunications297(2013)165168

    Fig. 5. Field evolutions of thedevice for (a) input(0,1), (b) input(1,0), and (c) input(1,1).

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    Porta Lgica AND

    Y.-P. Yangetal./OpticsCommunications297(2013)165168

    Fig. 5. Field evolutions of the device for (a) input(0,1), (b) input(1,0), and (c) input(1,1).

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    Porta Lgica AND

    P. Rani et al. / Optics Communications 298299 (2013) 227

    231

    Fig. 1. Schematic of all-optical AND logic gate.

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    Porta Lgica AND

    P. Rani et al. / Optics Communications 298299 (2013) 227

    231

    Fig. 7. Field distributions at steady state of the ANDlogicgate for(a) A=1, B=0; (b) A=0, B=1 and (c) A=1, B=1.

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    Porta Lgica AND

    P. Rani et al. / Optics Communications 298299 (2013) 227

    231

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    Puertas Lgicas XOR, XNOR, AND, OR

    Fig. 7. Structure of logic model with XOR, XNOR, NAND and OR functions

    W. Liu et al./Optics&LaserTechnology50(2013)5564

    6.9 m6.7 m

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    Puertas Lgicas XOR, XNOR, AND, OR

    W. Liu et al./Optics&LaserTechnology50(2013)5564

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    Portas Lgicas XOR, XNOR, AND, OR

    Fig. 13. (a), (b),(c)and(d)areschemasoflogicgatewithXOR,XNOR,NANDand ORlogicalfunctionsfordifferentBPSKsignals,respectively.

    W. Liu et al./Optics&LaserTechnology50(2013)5564

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    Portas Lgicas XOR, XNOR, AND, OR

    W. Liu et al./Optics&LaserTechnology50(2013)5564

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    Portas Lgicas XOR, XNOR, AND, OR

    Fig. 14. Field distributions to show the performance of the proposed all-optical logic gate with XOR, XNOR, NAND and ORfunctions for different BPSK signals, respectively.

    W. Liu et al./Optics&LaserTechnology50(2013)5564

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    Portas Lgicas XOR, XNOR, AND, OR

    Fig. 17. Field distributions of the logic model with XOR function (a)(e) at =1550 nm

    W. Liu et al./Optics&LaserTechnology50(2013)5564

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    Portas Lgicas em Silcio

    Fig. 1. Schematic structure of a two-dimensional silicon photonic crystal.

    Y. Fu et al. / Physics Letters A 377 (2013) 329333

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    Portas Lgicas em Silcio

    Fig. 2. Calculated steady state electric field distributions of all-optical OR gate. (a) Single signal light beam injected into

    input port A. (b) Single signal light beam injected

    into input port B. (c) Two single beams injected into input ports A and B, separately but simultaneously

    Y. Fu et al. / Physics Letters A 377 (2013) 329333

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    Portas Lgicas em Silcio

    Fig. 4. Calculated steady state electric field distributions of the NOT gate. (a) No signal light injected into input port A. (b)

    Single signal light beam injected into input port A.

    Y. Fu et al. / Physics Letters A 377 (2013) 329333

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    Portas Lgicas em Guias Convencionais

    Yuhei Ishizaka et al, JOURNAL OF LIGHTWAVE TECHNOLOGY,

    VOL. 29, NO. 18, SEPTEMBER 15, 2011

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    Infraestrutura

    02 salas climatizadas (Lab 17 e 18, 4 andar DEE)

    Algoritmos de simulao de propagao de ondas em 2D em ELEMENTOS FINITOS nodomnio da frequncia e do tempo.

    03 PCs I78 Gb RAM

    03 PCs I748 Gb RAM

    01 PC I764 Gb RAM

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    Alunos de Ps-Graduao

    Ana Jlia (Doutorado)Docente UnivasfPROPAGAO EM GUIAS EDISPOSITIVOS FOTNICOS NOCONVENCIONAIS

    Anderson (Doutorado)

    Bolsista FAPESBOTIMIZAO DE DISPOSITIVOS FOTNICOSE DE MICROONDAS UTILIZANDOCOMPUTAO BIO-INSPIRADA

    Juarez (Doutorado)

    Docente IFBAMODELAGEM DE GUIASPLASMNICOS

    Joaquim (Doutorado)Bolsista FAPESB

    NANOREFLETORES ENANOABSORVEDORES

    Francismari (Mestrado)

    Docente IFBAOTIMIZAO DE DISPOSITIVOSFOTONICOS USANDO COMPUTAOEVOLUTIVA

    Bernardo (Mestrado)ATERMALIZAO DE DISPOSITIVOS

    FOTNICOS

    Davi (Mestrado)Docente IFBA eBolsista CAPESDIODOS E PORTAS LGICAS

    Igor (Mestrado)Bolsista FAPESBGRADES DIELTRICASSUBMICROMTRICAS

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    Alunos de Graduao

    Luana da Frana Vieira

    Computao Bio-inspirada na Otimizao de Dispositivos Fotnicos

    Rafael Rodrigues dos Santos Andrade

    Tcnicas Hibridas na Otimizao de Dispositivos Fotnicos

    Igor Maia Teles Ruffini

    Modelagem e Projeto de Dispositivos Fotnicos Usando Redes Neurais

    Gabriel Santa Barbara da Silva E SilvaEstudo de absorvedores baseados em Dispositivos Metamateriais

    Scarlatt Vicente Freitas

    Reflexo em Grades Peridicas de Subcomprimento de Onda

    Joo Paulo de Azeredo Amaro

    Efeitos Trmicos em Dispositivos Fotnicos

    Patricia Martinez Kalil Nunez Teixeira

    Aperfeioamento de Recursos Didticos Hipermdicos com Mathematica - EletromagnetismoAplicado

    Priscila Oliveira de JesusDesenvolvimento de Recursos Didticos Hipermdicos com Mathematica - Fundamentos de Fotnica

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    Agradecimentos