Status of Photonics Polymers for “Fiber to the Display”...Status of Photonics Polymers for...

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Status of Photonics Polymers for “Fiber to the Display” Faculty of Science and Technology, Keio University Faculty of Science and Technology, Keio University JST ERATO/SORST JST ERATO/SORST Yasuhiro Koike Yasuhiro Koike May 25, 2009 May 25, 2009 FINNISH FINNISH - - JAPANESE WORKSHOP JAPANESE WORKSHOP ON FUNCTIONAL MATERIALS ON FUNCTIONAL MATERIALS Espoo and Helsinki, Finland Espoo and Helsinki, Finland

Transcript of Status of Photonics Polymers for “Fiber to the Display”...Status of Photonics Polymers for...

  • Status of Photonics Polymers for “Fiber to the Display”

    Faculty of Science and Technology, Keio University Faculty of Science and Technology, Keio University JST ERATO/SORST JST ERATO/SORST

    Yasuhiro KoikeYasuhiro Koike

    May 25, 2009May 25, 2009FINNISHFINNISH--JAPANESE WORKSHOP JAPANESE WORKSHOP ON FUNCTIONAL MATERIALSON FUNCTIONAL MATERIALSEspoo and Helsinki, FinlandEspoo and Helsinki, Finland

  • LightwaveHeterogeneous

    Structure

    Polymer

  • Å(10-10)

    nm(10-9)

    µm(10-6)

    mm(10-3)

    Polarization

    PMMA

    PMMA/BzMA PMMA-DPP

    -

    Zero-Birefringence Polymer

    Scattering

    Highly Scattering Optical Transmission

    (HSOT) Polymer

    RefractionReflection

    High Speed Graded-Index Polymer Optical Fiber

    Correlation Length

    Rhodamine 6G-doped polymer

    High-Power Optical Fiber Amplifier and Laser

    AbsorptionEmission

    AbsorptionEmission

    Eu Chelate-dopedpolymer

    Zero absorption Loss Polymer

  • Ray Trajectory

    Comparison of Step-Index Plastic Optical Fiber (SI POF) and Graded-Index Plastic Optical Fiber (GI-POF).

    Ray Trajectory

  • High-Speed GI Plastic Optical Fiber

  • Total Attenuation Spectra of GI POFs.

    (μm)

    0

    500

    1000

    1500

    2000

    2500

    3000

    3500

    4000

    4500

    5000

    0.5 0.6 0.7 0.8 0.9 1.0 1.1 1.2 1.3Wavelength

    Perfluorinated polymer-base

    Perdeuterated PMMA-base

    PMMA -base

  • CYTOP(Perfluoro butenyl vinyl ether)-Asahi Glass Co.-

    CFO

    CFCF2CF2

    CF2

    CF2

    F2C CF O CF2 CF2 CF CF2 monomer

    polymer

    The material for commercial GI-POF (Lucina)Tg: ~108℃

  • Calculated bandwidth potential of PF polymer based GI-POF compared with that of silica based MMF.

    0.4 0.6 0.8 1.0 1.2 1.4 1.6波長 (μm)

    1G

    10G

    100G全フッ素化ポリマー系GI型 POF

    石英系マルチモードファイバー

    Wavelength (µm)

    PF polymer based GI-POF

    Silica based multimode fiber

    Bit

    Rat

    e

  • Development of data rate achieved by POF links

    0

    200

    400

    600

    800

    1000

    1200

    1400

    1990 1995 2000 2005 2010YearYear

    531Mbps•100m@650nmEssex Univ.

    1Gbps•30m@670nmIBM & Keio Univ.

    1Gbps•30m@670nmIBM & Keio Univ.

    2.5Gbps•200m@650nmKeio Univ., Mitsubishi Rayon,NEC & Eindhoven Univ. Tech.

    2.5Gbps•200m@1300nmKeio Univ. & Asahi glass & Fujitsu

    5Gbps•140m@1300nmKeio Univ., Asahi glass,& Eindhoven Univ. Tech.

    4Gbps•300m@850nm12Gbps•100m@850nm

    Keio Univ., JST & Asahi glass,

    2.5Gbps•450m@1300nmKeio Univ. Mitsubishi Rayon,

    Eindhoven Univ. Tech. Asahi glass & Fujitsu

    11Gbps•100m@1300nmAsahi glass & Lucent Technologies

    1Gbps•1000m@850nmAsahi glass & Eindhoven Univ. Tech.

    10Gbps・100m@850nmFirst extrusion processAsahi glass, Chromis, Keio Univ.

    Preform Method

  • R&D Project of Polymer Devices for Constructing Next-Generation FTTH (METI, 2004-2006)

    Hopper for Core PolymerHopper for Clad

    Polymer

    Preform

    Extrusion ProcessPreform Method

  • A New Co-Extrusion Tower

    Hopper for Core and CladPolymer

    Diffusion Zone

    Control Panel

  • Å(10-10)

    nm(10-9)

    µm(10-6)

    mm(10-3)

    AbsorptionEmission Polarization Scattering

    RefractionReflection

    AbsorptionEmission

    PMMA

    PMMA/BzMA PMMA-DPP

    -

    High-Power Optical Fiber Amplifier and Laser Zero-Birefringence Polymer

    Highly Scattering Optical Transmission

    (HSOT) Polymer

    High Speed Graded-Index Polymer Optical Fiber

    Eu Chelate-dopedpolymer

    Rhodamine 6G-doped polymer

    Correlation Length

    Zero absorption Loss Polymer

  • Proposal of Highly Scattered Optical Transmission (HSOT) Polymer

  • Highly Scattering Optical TransmissionHighly Scattering Optical Transmission(HSOT)(HSOT) PolymerPolymer

    (A) PMMA(A) PMMA

    Laser Beam

    (B) HSOT polymer(B) HSOT polymer

    Laser Beam

    ScatterersScatterers

    1~10 1~10 μμmm

    (FIG.1.1, p.11)(FIG.1.1, p.11)

  • (B) HSOT backlighting system(B) HSOT backlighting system

    (A) Conventional backlighting system(A) Conventional backlighting system

    Prism sheetPrism sheet

    HSOT polymerHSOT polymer

    Reflection sheetLamp reflector

    Collection sheet(BEF)

    Diffusion sheet

    LampPrinted dot pattern Transparent

    light guide Transparent light guide

  • HSOT and conventional backlights

    HSOT and conventional HSOT and conventional backlightsbacklights

    LampLamp56mm56mm

    44mm44mm

    Conventional Conventional backlightbacklight

    HSOT HSOT backlightbacklight

    5674 cd/m2 3072 cd/m2

  • Bluish

    YellowishHSOT light pipe

    Color dispersion due to general light scattering phenomenon

    Is General Concept of Light Scattering Always True?

  • Photograph of Sunset

  • 0 deg.

    90 deg.

    α = 69.2

    α = 11.5α = 1.7

    Mie scattering theoryMie scattering theoryMie scattering theory

    λπα /2 r=

    ( )( )221

    2 122)( nn

    nbanK ++= ∑

    =αα

    ( ) 2212 8/),( πλθα iiI +=

    )(')()(')()(')()(')()(')()(')()(')()(')(

    αζαψαψαζαψαψαψαψαζαψαψαζαψαψαψαψ

    nnnn

    nnnnn

    nnnn

    nnnnn

    mmmmmmb

    mmmmmma

    −−

    =

    −−

    =

    2)1()1(

    12

    2)1()1(

    11

    )(cossin

    )(cos)1(

    12

    )(cossin

    )(cos)1(

    12

    ⎭⎬⎫

    ⎩⎨⎧

    +++

    =

    ⎭⎬⎫

    ⎩⎨⎧

    +++

    =

    =

    =

    θθ

    θθ

    θθ

    θθ

    ddPaPb

    nnni

    ddPbPa

    nnni

    nn

    nn

    n

    nn

    nn

    n

  • (A) (B)

    Observation result

    0

    1

    2

    3

    4

    0 3 6 9 12 15

    Particle diameter / μm

    Scat

    terin

    g ef

    ficie

    ncy

    435nm

    545nm

    615nm

    (A)

    (B)

    (435, 545, 615nm mean three peaks in spectrum of a cold fluorescent lamp.)

    HSOT polymer

    Camera

    Scattering

    transmitting

    Transmitting

    Fluorescent lamp

    Scattering Efficiency

  • 5000

    6000

    7000

    8000

    9000

    0 10 20 30 40 50 60 70Distance from lamp (mm)

    Optimized HSOTOptimized HSOTNot optimized HSOTNot optimized HSOT

    White

    Blue

    Yellow

    Col

    or te

    mpe

    ratu

    re (K

    )

    Color Dispersion on HSOT Backlights

  • SONY Vaio Note seriesPanasonic Let’s Note seriesTOSHIBA Dynabook seriesSamsung, Dell etc.

    Notebook PCsNotebook PCs Various Mobile DevicesVarious Mobile Devices

    Mobile phonesPDAPocket TV

    HSOT Polymer Products

  • Å(10-10)

    nm(10-9)

    µm(10-6)

    mm(10-3)

    AbsorptionEmission Polarization Scattering

    RefractionReflection

    AbsorptionEmission

    PMMA

    PMMA/BzMA PMMA-DPP

    -

    High-Power Optical Fiber Amplifier and Laser Zero-Birefringence Polymer

    Highly Scattering Optical Transmission

    (HSOT) Polymer

    High Speed Graded-Index Polymer Optical Fiber

    Eu Chelate-dopedpolymer

    Rhodamine 6G-doped polymer

    Correlation Length

    Zero absorption Loss Polymer

  • ・ Extrusion processing・・・High speed, Low costand zero-birefringence.

    Zero-birefringence polymers

    ・・ Solvent CastingSolvent Casting・・・・・・Low birefringence, Low birefringence, High cost.High cost.

    Advantage of zeroAdvantage of zero--birefringence optical polymersbirefringence optical polymers

    BirefringenceFlexibility

    Light weightLow cost

  • Figure Polarization property in a birefringent medium.

    Changing in pChanging in polarization stateolarization statethrough a birefringent mediumthrough a birefringent medium

    Input Polarization

    x

    ϕ

    y

    x

    z

    yy

    x

    x

    Output Polarization

    y

    Retardation

  • Anisotropic molecule dopant methodRandom copolymerization method

    Random copolymerization

    Zero-birefringence copolymer

    Positive (+) birefringence monomer

    Negative(-) birefringence monomer

    MMA / BzMA = 82 / 18 (wt./wt.)

    Our proposal of compensating orientationalbirefringence of polymers

    Our proposal of compensating Our proposal of compensating orientationalorientationalbirefringence of polymersbirefringence of polymers

    C H CHTypical Typical dopantdopant

    Drawing

    Polarizability ellipsoid of anisotropic molecule

    Polarizability ellipsoid of monomer unit

    MMA / trans-stilbene = 100 / 3 (wt./wt.)

  • polarizer analyzer

    (a) PMMA

    (c) PMMA-trans-stilbene (3 wt.%)

    (b) MMA/BzMA=82/18 (wt./wt.)

    Injection molded samplesInjection molded samplesInjection molded samples

  • Photoelastic BirefringencePhotoelastic Birefringence

    PolarizersStress is added

    Stress is released

    n⊥

    n//

    c : Photoelastic Coefficient

    Δσ: Stress

    Δn = n// - n⊥= c・Δσ

  • CH2 C

    CH3

    C O

    O CH3

    CH2 C

    CH3

    C O

    O CH2 CF3

    CH2 C

    CH3

    C O

    O CH2

    Methyl methacrylate(MMA)

    2,2,2-Trifluoroethyl methacrylate (3FMA)

    Benzyl methacrylate(BzMA)

    trans-stilbene

    Anisotropic Dopant

    Monomers

    OB:Negative

    Binary Copolymers Containing an Anisotropic Dopant

    Components of Zero-Zero PolymersComponents of ZeroComponents of Zero--Zero PolymersZero Polymers

    # OB: Orientational Birefringence

    PB: Photoelastic Birefringence

    OB:PositivePB:NegativePB:Negative

    OB:PositivePB:Positive

    OB:PositivePB:Positive

    Ternary Copolymers

  • -4

    -3

    -2

    -1

    0

    1

    0 0.2 0.4 0.6 0.8

    Orie

    ntat

    iona

    lbire

    fring

    ence

    (x10

    -4)

    Pho

    toel

    astic

    bire

    frine

    nce

    (x10

    -6)

    Orientation function of polymer chains Principal stress differnce (MPa)

    -4

    -3

    -2

    -1

    0

    1

    0 0.05 0.1

    PMMA

    Composition of the zero-zero polymer

    P(MMA/3FMA=85/15) + trans-stilbene 2.8 wt%

    PMMA

    Birefringence of Binary Copolymers Containing an Anisotropic DopantBirefringence of Binary Copolymers Containing an Anisotropic Birefringence of Binary Copolymers Containing an Anisotropic DopantDopant

    Simultaneous elimination of the orientational birefringence and photoelasticbirefringence was achieved. Zero-zero polymers that exhibit no birefringence with any orientation of the polymer main chains and in elastic deformation was realized.

  • Injection MoldingInjection Molding

    35mm

    35mm

    2mmInjection

  • (a) 230 ˚C (b) 220 ˚C (c) 210 ˚CReave = 2.4 (nm) Reave = 4.7 (nm) Reave = 9.1 (nm)

    OrientationalOrientational birefringence increased with a decrease in molding birefringence increased with a decrease in molding temperature. The directions of fast axes were parallel to injectemperature. The directions of fast axes were parallel to injection tion direction.direction.

    P(MMA/BzMA = 92/8)

    <<

    Re = Δn x d (= 2mm)Re (nm)150 7.5 /,\,―,|:Fast axes

    InjectionInjectiondirectiondirection

    d=2mm35mm

    35mm

    Injection Molded Samples of Binary CopolymerInjection Molded Samples of Binary Copolymer

  • (a) 230 ˚C (b) 210 ˚C (c) 190 ˚CReave = 0.4 (nm) Reave = 0.5 (nm) Reave = 0.5 (nm)

    Ternary copolymer exhibited close to zero birefringence at any Ternary copolymer exhibited close to zero birefringence at any points regardless of molding temperature.points regardless of molding temperature.

    Re (nm)50 2.5

    /,\,―,|:Fast axes

    P(MMA/3FMA/BzMA = 52/42/6)

    Injection Molded Samples of the Ternary CopolymerInjection Molded Samples of the Ternary Copolymer

  • Å(10-10)

    nm(10-9)

    µm(10-6)

    mm(10-3)

    AbsorptionEmission Polarization Scattering

    RefractionReflection

    AbsorptionEmission

    PMMA

    PMMA/BzMA PMMA-DPP

    -

    High-Power Optical Fiber Amplifier and Laser Zero-Birefringence Polymer

    Highly Scattering Optical Transmission

    (HSOT) Polymer

    High Speed Graded-Index Polymer Optical Fiber

    Eu Chelate-dopedpolymer

    Rhodamine 6G-doped polymer

    Correlation Length

    Zero absorption Loss Polymer

  • Silica Fiber Core Network

    Graded Index Polymer Optical Fiber (GI POF)

    High-Speed Internet

    High-Speed Internet Core Network

    Keio University Network

    Telemedicine & Distance LearningRealized with Real-

    Time Communication

    Concept of “Fiber-to-the-Display” by Photonics Polymer Project at Keio University

    Collaborated withGigaHouseTownTM Project

    of Keio Engineering FoundationAsahi Glass Co., Ltd.Cisco Systems Inc.Fuji Photo Film Co., Ltd.IBM JapanKodak Japan Ltd.NTT EastMatsushita Electric Works, Ltd.Mitsubishi CorporationOmron CorporationSekisui Chemical Co., Ltd.Taisei Corporation, etc.

    High-Quality Large Screenproposed by Photonics Polymer Project

    Photonics Polymer Project

  • Telemedicine by internistTelemedicine by internist

    Internist

    Patients at Hiyoshi Campus projected on a screen

    Mita campus

  • EntertainmentSecurityEducation

    Education

    Vision of the Fiber-to-the-Display Project

    Security Entertainment

    Medical

    Medical

  • The Status of “Photonics Polymer” was reviewed , and the concept of “Fiber to the Display” was proposed.

    SummarySummary

    “Face-to-Face Communication”.

    We believe that the innovation of giga-bit technologies based on these photonics polymers will bring us back to