An introduction to methods of periodic poling for second-harmonic generation

Second-harmonic generation (SHG) can be produced by phase matching using the birefringence of nonlinear crystals via the modal dispersion in the case of optical waveguides. Such an approach limits the range of frequencies which can be doubled and also the choice of the nonlinear coefficients. One solution to both problems is to modify the crystal so as to have regions of periodic domain polarity. Whilst this approach does not allow a perfect phase match between the fundamental and harmonic, it nevertheless can be entirely constructive throughout the interaction length of the material and is termed quasi-phase matching (QPM). Periodic modulation of the nonlinear coefficient along the direction of propagation can achieve conversion efficiencies up to 20 times greater than with previous methods. Candidates of interest for quasi-phase-matching are wide band gap inorganic crystals such as LiNbO3, LiTaO3 and KTP, and also organic materials if they are transparent, stable against optical damage and have large nonlinear coefficients. To achieve QPM a variety of methods are being tried in order to invert domains periodically, either during the crystal growth phase, or subsequently by altering the lattice of the crystal. For inorganic ferroelectrics most effort has been concentrated on domain inversion in LiNbO3 and LiTaO3. Techniques have included application of pulsed electric fields, fields generated during electron bombardment, thermal pulsing or chemically driven movement of lithium. Many of the methods are semi-empirical in that the mechanisms by which the lattice re-structures are poorly understood. This review will therefore not only list the methods that are currently being used, but also comment on the underlying physical processes which allow, or prevent, the re-structuring of the lattice and the domain walls, whilst preserving the non-centrosymmetric characteristics of the lattice. An understanding of mechanisms is valuable for related poling applications in other crystals and it is further noted that many amorphous systems, including glasses used for optical fibre communication, may be stimulated to show periodic structural changes although the usage precedes the knowledge of the mechanisms. The commercial applications and research possibilities for efficient SHG guarantee that this topic area will continue to be central to photonics for a considerable time.

[1]  F. Altorfer,et al.  A neutron powder investigation of the high-temperature structure and phase transition in LiNbO3 , 1994 .

[2]  S. Thaniyavarn,et al.  Domain inversion effects in Ti‐LiNbO3 integrated optical devices , 1985 .

[3]  K. Kishima,et al.  Fabrication of periodically reversed domain structure for SHG in LiNbO3, by direct electron beam lithography at room temperature , 1991 .

[4]  C. J. E. Seppen,et al.  Efficient modal dispersion phase-matched frequency doubling in poled polymer waveguides , 1993 .

[5]  P. J. Chandler,et al.  Extended Short-wavelength Harmonic Production Using a Multilayer Waveguide Structure , 1994 .

[7]  P. J. Chandler,et al.  Second-harmonic generation in ion-implanted KTiOPO/sub 4/ planar waveguides , 1992 .

[8]  Tomoaki Yamada,et al.  Growth Ridges, Etched Hillocks, and Crystal Structure of Lithium Niobate , 1967 .

[9]  R. T. Lynch,et al.  An organic crystal with an exceptionally large optical second‐harmonic coefficient: 2‐methyl‐4‐nitroaniline , 1979 .

[10]  A. Savage,et al.  Pyroelectricity and Spontaneous Polarization in LiNbO3 , 1966 .

[11]  D. C. Hanna,et al.  Quasi-phase-matched blue light generation in bulk lithium niobate, electrically poled via periodic liquid electrodes , 1994 .

[12]  C. Bräuchle,et al.  Photoinduced generation of noncentrosymmetric structures in glassy liquid crystalline polysiloxanes for second harmonic generation , 1993 .

[13]  R. C. Miller SOME EXPERIMENTS ON THE MOTION OF 180 DOMAIN WALLS IN BaTiO$sub 3$ , 1958 .

[14]  H. Vanherzeele,et al.  Magnitude of the nonlinear-optical coefficients of KTiOPO(4). , 1992, Optics letters.

[15]  J. Zyss,et al.  Growth and characterization of a new material for nonlinear optics: Methyl-3-nitro-4-pyridine-1-oxide (POM) , 1984 .

[16]  V. Pruneri,et al.  Blue-light generation by quasi-phase-matched frequency doubling in thermally poled optical fibers. , 1995, Optics letters.

[17]  Kenneth D. Singer,et al.  Second harmonic generation in poled polymer films , 1986 .

[18]  G. Baldwin,et al.  An Introduction to Nonlinear Optics , 1969 .

[19]  D. A. Kleinman,et al.  Theory of Second Harmonic Generation of Light , 1962 .

[20]  Comment on ‘‘Domain inversion effects in Ti‐LiNbO3 integrated optical devices’’ [Appl. Phys. Lett. 46, 933 (1985)] , 1986 .

[21]  P. Hitchcock,et al.  A novel class of salts for second harmonic generation , 1989 .

[22]  Peter Günter,et al.  Phase-matched second harmonic blue light generation in ion implanted KNbO3 planar waveguides with 29% conversion efficiency , 1992 .

[23]  N. Bloembergen,et al.  Interactions between light waves in a nonlinear dielectric , 1962 .

[24]  M. Fejer,et al.  Quasi‐phase‐matched second‐harmonic generation of blue light in periodically poled LiNbO3 , 1990 .

[25]  M. Yamada,et al.  First‐order quasi‐phase matched LiNbO3 waveguide periodically poled by applying an external field for efficient blue second‐harmonic generation , 1993 .

[26]  D. Ostrowsky,et al.  Cerenkov configuration second harmonic generation in proton-exchanged lithium niobate guides , 1990 .

[27]  J. Cazaux,et al.  Some physical descriptions of the charging effects of insulators under incident particle bombardment , 1992 .

[28]  A. Yariv,et al.  Phase matching by periodic modulation of the nonlinear optical properties , 1972 .

[29]  M. Fejer,et al.  Infrared radiation generated by quasi‐phase‐matched difference‐frequency mixing in a periodically poled lithium niobate waveguide , 1991 .

[30]  J. Cazaux,et al.  Some considerations on the electric field induced in insulators by electron bombardment , 1986 .

[31]  D. Bolmont,et al.  Using decomposed disilane as a gas source for Si epitaxial growth on Ge (111): Photoemission studies , 1990 .

[32]  M. Fejer,et al.  Second-harmonic generation of green light in periodically poled planar lithium niobate waveguide , 1989 .

[33]  P. Townsend,et al.  Second‐harmonic generation in ion‐implanted quartz planar waveguides , 1991 .

[34]  Characteristics of periodically domain‐inverted LiTaO3 , 1992 .

[35]  S. Miyazawa Ferroelectric domain inversion in Ti‐diffused LiNbO3 optical waveguide , 1979 .

[36]  G. E. Peterson,et al.  Nonstoichiometry and Crystal Growth of Lithium Niobate , 1971 .

[37]  R. C. Miller,et al.  Direct Observation of Antiparallel Domains During Polarization Reversal in Single-Crystal Barium Titanate , 1959 .

[38]  W. J. Kozlovsky,et al.  Blue light generation by frequency doubling in periodically poled lithium niobate channel waveguide , 1989 .

[39]  I. Camlibel Spontaneous Polarization Measurements in Several Ferroelectric Oxides Using a Pulsed‐Field Method , 1969 .

[40]  Response to ``Comment on `Domain inversion effects in Ti-LiNbO3 integrated optical devices' '' [Appl , 1986 .

[41]  Hiroshi Shimizu,et al.  Ferroelectric domain inversion caused in LiNbO3 plates by heat treatment , 1987 .

[42]  J. Feinberg,et al.  High-resolution map of the dc electric field in second-harmonic-generating glass , 1994 .

[43]  Robert A Norwood,et al.  Quasi-phase-matched frequency doubling over 5 mm in periodically poled polymer waveguide , 1990 .

[44]  H. Stadler Ferroelectric polarization reversal in single crystals , 1992 .

[45]  Keiichi Mito,et al.  Phase‐matched second‐harmonic generation in novel corona poled glass waveguides , 1992 .

[46]  Tetsuo Taniuchi,et al.  Characteristics of periodically domain-inverted LiNbO3 and LiTaO3 waveguides for second harmonic generation , 1991 .

[47]  Herman Vanherzeele,et al.  Potassium titanyl phosphate: properties and new applications , 1989 .

[48]  Steven R. J. Brueck,et al.  Dynamics of second-harmonic generation in fused silica , 1994 .

[49]  F. Laurell,et al.  Blue light generated by frequency doubling of laser diode light in a lithium niobate channel waveguide , 1989, IEEE Photonics Technology Letters.

[50]  M. V. Hobden Phase‐Matched Second‐Harmonic Generation in Biaxial Crystals , 1967 .

[51]  M. Hayashi Kinetics of Domain Wall Motion in Ferroelectric Switching. I. General Formulation , 1972 .

[52]  Shinsuke Umegaki,et al.  Characteristics of optical second-harmonic generation due to Čerenkov-radiation-type phase matching , 1990 .

[53]  S. Umegaki,et al.  Theoretical analysis of Cerenkov-type optical second-harmonic generation in slab waveguides , 1992 .

[54]  A. G. Chynoweth,et al.  Dynamic Method for Measuring the Pyroelectric Effect with Special Reference to Barium Titanate , 1956 .

[55]  Kazuhisa Yamamoto,et al.  Highly efficient quasi‐phase‐matched second‐harmonic generation using a first‐order periodically domain‐inverted LiTaO3 waveguide , 1992 .

[56]  Werner Wirges,et al.  Selective poling of nonlinear optical polymer films by means of a monoenergetic electron beam , 1994 .

[57]  E. Conwell Theory of second-harmonic generation in optical waveguides , 1973 .

[58]  R. C. Miller,et al.  Motion of 180° Domain Walls in Metal Electroded Barium Titanate Crystals as a Function of Electric Field and Sample Thickness , 1960 .

[59]  P. Townsend,et al.  A method of poling LiNbO3 and LiTaO3 below Tc , 1986 .

[60]  P. J. Chandler,et al.  Second Harmonic Generation in Ion Implanted Lithium Niobate Planar Waveguides , 1994 .

[61]  Theoretical Treatment of the Movement of 180° Domain in BaTiO3 Single Crystal , 1959 .

[62]  Fredrik Laurell,et al.  Fabrication of periodically domain-inverted channel waveguides in lithium niobate for second harmonic generation , 1989 .

[63]  H. Levinstein,et al.  Ferroelectric lithium niobate. 5. Polycrystal X-ray diffraction study between 24° and 1200°C , 1966 .

[65]  Barkhausen Pulses in Barium Titanate , 1958 .

[66]  Yaochun Shen Principles of nonlinear optics , 1984 .

[67]  W. J. Merz Switching Time in Ferroelectric BaTiO3 and Its Dependence on Crystal Thickness , 1956 .

[68]  Induced second-harmonic generation in planar waveguides by an externally applied periodic DC electric field: efficiency as a function of field structure , 1994 .

[69]  C. Peters,et al.  Generation of optical harmonics , 1961 .

[70]  Mool C. Gupta,et al.  Domain inversion in LiTaO3 by electron beam , 1992 .

[71]  W. Risk,et al.  Domain inversion in KTiOPO4 using electron beam scanning , 1993 .

[72]  C. Y. Chen,et al.  Reduction and Radiation Effects in Lithium Tantalate , 1984 .

[73]  R. Newton,et al.  Observation of the Ferro-Electric Barkhausen Effect in Barium Titanate , 1949 .

[74]  R. C. Miller,et al.  Velocity of Sidewise 180° Domain-Wall Motion in BaTiO 3 as a Function of the Applied Electric Field , 1958 .

[75]  Tetsuo Taniuchi,et al.  Second‐harmonic generation of blue light in a LiTaO3 waveguide , 1991 .

[76]  A. Ballman,et al.  Ferroelectric domain reversal in lithium metatantalate , 1972 .

[77]  Sisa Pityana,et al.  Frequency doubling in ion-implanted KTiOPO4 planar waveguides with 25 % conversion efficiency , 1993 .

[78]  Hans M. Hertz,et al.  QUASIPHASE-MATCHED SECOND HARMONIC GENERATION OF BLUE LIGHT IN ELECTRICALLY PERIODICALLY-POLED LITHIUM TANTALATE WAVEGUIDES , 1991 .

[79]  Blue-light generation by frequency doubling of a laser diode in a periodically domain-inverted LiTaO/sub 3/ waveguide , 1992, IEEE Photonics Technology Letters.

[80]  J. C. Cassidy,et al.  Nonlinear optical properties of urea , 1979 .

[81]  A. Chynoweth Effect of Space Charge Fields on Polarization Reversal and the Generation of Barkhausen Pulses in Barium Titanate , 1959 .

[82]  LiNbO/sub 3/ waveguide SHG device with ferroelectric-domain-inverted grating formed by electron-beam scanning , 1992 .

[83]  M. Sigelle,et al.  Determination of the electrooptic coefficients of 3‐methyl 4‐nitropyridine 1‐oxide by an interferometric phase‐modulation technique , 1981 .

[84]  S. Kurtz,et al.  ALPHA‐IODIC ACID: A SOLUTION‐GROWN CRYSTAL FOR NONLINEAR OPTICAL STUDIES AND APPLICATIONS , 1968 .

[85]  R. C. Miller,et al.  Optical Harmonic Generation in Single Crystal BaTiO 3 , 1964 .

[86]  B. U. Felderhof,et al.  Second harmonic generation in planar optical waveguides , 1990 .

[87]  G. Weinreich,et al.  Mechanism for the Sidewise Motion of 180° Domain Walls in Barium Titanate , 1960 .

[88]  Simultaneous blue and green second harmonic generation in quasiphase matched LiNbO3 waveguide , 1992 .

[89]  R. A. Myers,et al.  Large second-order nonlinearity in poled fused silica. , 1991, Optics letters.

[90]  Blue light generation in LiNbO3 waveguide SHG device with first order domain-inverted grating formed by EB scanning , 1992 .

[91]  P. Townsend,et al.  Thermal polarization reversal of lithium niobate , 1995 .

[92]  Ferroelectric-domain inversion induced by SiO2 cladding for LiNbO3 waveguide SHG , 1991 .

[93]  R. Kashyap Phase-matched periodic electric-field-induced second-harmonic generation in optical fibers , 1989 .

[94]  Hiromasa Ito,et al.  Fabrication of periodic domain grating in LiNbO3 by electron beam writing for application of nonlinear optical processes , 1991 .

[95]  M. M. Fejer,et al.  Quasi-Phase-Matched Interactions In Lithium Niobate , 1990, Optics & Photonics.