QPM and PPLN

download QPM and PPLN

of 18

Transcript of QPM and PPLN

  • 8/12/2019 QPM and PPLN

    1/18

    Quasi Phase Matching

  • 8/12/2019 QPM and PPLN

    2/18

    Quasi Phase Matching

    Periodicmodification ofproperties of NLmedium

    Correct relative phaseat regular intervalwithout matchingphase velocity

    QPM does not rely on BPM, only polarization

    can be used, including cases where all waves

    parallelly polarized with respect to one another

    Largest deff found in ferroelectrics LiNbO3,

    LiTaO3, and isotropic media GaAs where BPM is

    not possible

  • 8/12/2019 QPM and PPLN

    3/18

    Domain Reversal

    Electric Field poling in bulk crystals of ferroelectric families, KTP families Patterning a periodic electrode on one surface of the crystal

    Applying voltage to produce a field exceeding coercive field to reversedomains in electrode region

    LiNbO3/LiTaO3:Transparent near UV

    LiNbO3-28pm/V, absorption edge:220nm, shortest shg:386 nm LiTaO3-16pm/V, absorption edge:277nm, shortest shg:325 nm

    Mid-infrared: Multi-photon Absorption-4-5 m-> limit high poweroperation

    CW interaction:6.6m

    Short pulse operation:7.25 m Photorefractive effect->MgO doping

    GRIIRA

    Mg-LN: Grating period-1.4m, thickness-1mm

    Challenge in increasing thickness due to pulsed poling, diffusion bonding

  • 8/12/2019 QPM and PPLN

    4/18

    Other CrystalsKTP families: d33-17,15,16 pm/V

    QPM SHG wavelength: PPKTP: minimum-359 nm, maximum 2.74 m

    Length- 8mm

    Resistant to photo-refraction

    Gray tracking-long lived color centers under intense visible radiation

    Depends on ->intensity, spot diameter , pulse repetition rate, method of crystal growth.

    Draw back:

    Multi-photon absorption

    Difficulty in average power operation

    Semiconductor families: III-V, II-VI mid-IR applicationGaAs: 95 pm/V, transparent upto 3 phonon peak-12m

    Thermal Conductivity-52W/m-k

    Coherence length-10-100 m

    Challenge- in fabrication, corresponds to high loss

    Grating period achieved-40m in.5mm thick crystal, 20m in 200 m thick crystal

  • 8/12/2019 QPM and PPLN

    5/18

    Grating Transversely varying grating Multi grating,->array of grating

    fan grating->continuous tuning of QPMbased on wavelength

    angled grating->Tilt domain pattern atsmall angle to o/p facet of crystal

    Radially varying grating

    Uniformely patterned grating->conversionwill vary radially, leaving a radially varyinglength of medium unpoled

    deff vary radially, with radially varyingduty cycle of QPM grating

    Longitudinally varying grating Multigrating->two or more grating in sequencein same crystal->phase matching SHG in 1stgrating ->combine with fundamental andproduce 3rdharmonic in 2ndgrating->reducedno of interface, simpler anti-reflection coatingrequirement

  • 8/12/2019 QPM and PPLN

    6/18

    Analytical expression for grating

  • 8/12/2019 QPM and PPLN

    7/18

    Analytical expression for grating

  • 8/12/2019 QPM and PPLN

    8/18

    Different gratingsLinear-chirped gratings

    Apodized gratings

    Fibbonacci gratings

  • 8/12/2019 QPM and PPLN

    9/18

    Different gratingsPhase reversed gratings

  • 8/12/2019 QPM and PPLN

    10/18

    Periodically chirped gratings

    Summed component aperiodic gratings

  • 8/12/2019 QPM and PPLN

    11/18

    Numerical modeling of errors in 1D QPM

    gratings and its effect on parametric process

    Numerical modeling of stochastic domain errors

  • 8/12/2019 QPM and PPLN

    12/18

    effect of periodicity

    Duty cycle fluctuations

    Numerical modeling of errors in 1D QPM

    gratings and its effect on parametric process

  • 8/12/2019 QPM and PPLN

    13/18

    External factors

    Numerical modeling of errors in 1D QPM

    gratings and its effect on parametric process

  • 8/12/2019 QPM and PPLN

    14/18

    LiNbO3-properties

    Photorefractive Effect

    Pyro-electric Effect

    Piezo electric Effect

  • 8/12/2019 QPM and PPLN

    15/18

    Photorefractive Effect

    Extrinsic defect- presence of Fe+. Cu+,Rh+ in

    LN->intermediate energy level between

    conduction and valence band ->electrons in

    that level get optically excited for longexposure to laser beam->electrons migrate to

    Conduction band leaving holes and diffuse

    through crystal to low-intensity region->generation of local electric field changing

    refractive index

  • 8/12/2019 QPM and PPLN

    16/18

    Reduction of Photorefractive effect

    Application of external Electric field tocancel photo-induced internal Electricfield at 170C->Limit operation in visiblerange

    Dope with Mg,Zn, Hf which are photo-resistant, beyond Optical DamageThreshold which enhance optical damage

    Below ODT- dopant occupying Nb5+Li+

    Above ODT-dopant replaces Nb/Li Non-dopant LN-tolerate 10KW/sq.cm

    Near stoichiometry-1000KW/sq.cm dueto fewer intrinsic defects, no impurities

    ODT @ MG-LN- 4.6 mol% MgO->100 foldincrease in Optical damage resistance

    ODT@Zn-LN--6 mol% Zn->Zn replacesNb5+Li below ODT, Zn replaces Li+ aboveODT

  • 8/12/2019 QPM and PPLN

    17/18

    Pyro-electric effect

  • 8/12/2019 QPM and PPLN

    18/18

    FDTD in 2D Lithium Niobate