FABRICATION OF PATTERNED POLED DIELECTRIC STRUCTURES AND DEVICES

Abstract: A poled dielectric substrate is fabricated by creating a uniform potential, such as a ground by means of an electrode surface, adjacent a first surface of a polable dielectric material (6), such as a piezoelectric or lithium niobate, and then applying an electric field (20) adjacent a second surface of the polable dielectric material (8), where the electric field is spatially-modulated according to a three-dimensional modulation pattern with a field amplitude level at selected locations sufficient to cause atomic rearrangement within predefined regions in the polable material, and where the modulation pattern is controlled according to a modulation parameter. The control mechanism of modulation amplitude level may be protrusions of an electrically conductive material (15) extending toward the polable material or by modulated variation in the dielectric constant of a dielectric material separating the polable material from an electrode plate.

Description: FABRICATION OF PATTERNED POLED DIELECTRIC STRUCTURES AND DEVICES BACKGROUND OF THE INVENTION This invention relates to techniques for fabricating patterned poled structures and devices from polable materials, and in particular periodically poled dielectric structures, as well as devices incorporating periodically-poled structures. The invention has wide application in optical systems, and in particular to nonlinear optical systems, such as frequency doublers, optical parametric oscillators and amplifiers, optical waveguides and the like. The ferroelectric materials of choice for nonlinear optical interactions are LiNb0 3 , LiTa0 3 and KTP. Ferroelectric domain inversion is generally produced by in- diffusion and heat treatment, e.g., Ti in-diffusion, proton exchange and Ba in-diffusion respectively for the three materials. In LiNb0 3 and LiTa0 3 these poling techniques generate shallow domains in the polable materials, only suitable for shallow waveguide interactions. For maximum overlap with the optical waveguide modes and optimum device efficiency the domain inverted grating should have a rectangular shape with vertical domain walls. However, in LiNb0 3 the titanium in-diffusion process (U.S. Patent No. 5,036,220) creates a triangularly shaped domain inversion grating and in LiTa0 3 , proton exchange and heat treatment at around 600°C (U.S. Patent No. 5,249,191) produces semicircular shaped domains. These odd shaped, non-rectangular domains reduce the efficiency of the desired nonlinear interaction. In KTP the inverted domains generated by Ba diffusion (U.S. Patent N° 5,157,754, Van der Poel et al Appl. Phys. Lett. 57 (20) , p2074-6, 1990) are rectangular with vertical sidewalls due to the anisotropic nature of the diffusion process. But they are relatively shallow: they can be used for waveguide interactions but are not very efficient for bulk applications. An added complication to the KTP domain inversion process is that the domain inversion is performed in the same ion-exchange step as is used to form the optical waveguide. Although this means that only a single processing step is required to fabricate the device (rather than separate domain inversion and waveguide fabrication processes) , it also means that the waveguide and domain inversion dimensions cannot be independently optimized to achieve maximum performance. In order to obtain a periodically inverted domain pattern a segmented waveguide is formed consisting of alternating guiding ion-exchanged regions and non-guiding unexchanged crystal. The application of a different domain inversion procedure, such as electric field induced poling, would separate the two fabrication processes, allowing independent optimization. The domain inversion processes available in the prior art are limited to the fabrication of relatively shallow surface features that are only suitable for waveguide based interactions. [With the exception of periodically poled fibers of LiNb0 3 grown by the laser heated pedestal growth technique as described by Magel et al (Magel et al Appl. Phys. Lett. 56 (2), pl08-10, 1990). However, these periodically poled fibers suffer from the inability to control the domain dimensions and boundary positions to a sufficient degree to ensure phase matching over a long sample length greater than about 3 mm.] For higher power interactions, such as the frequency conversion of high power and pulsed laser systems, waveguide devices are unsuitable because the intensity generated on the front face of the crystal when launching into the waveguide far exceeds the material damage threshold. To avoid physical damage to the nonlinear crystal the high power beam focus must be relaxed. For periodic poled material to be useful in such cases, the poling must be quite uniform across the aperture of the bulk crystal. A domain inversion process is needed which will provide bulk periodic poling in ferroelectric materials. Electric field-induced poling, as demonstrated by Yamada et al in LiNb0 3 (U.S. Patent No. 5,193,023), offers the possibility of vertical walled domain structures for maximum performance and deep poling suitable for quasi-phase-matching of bulk interactions in all ferroelectrics. Yamada et al describe the use of patterned metal electrodes 22 deposited on the crystal ±z surfaces combined with the application of a pulsed high voltage 20, as illustrated in Figure 2a. The high voltage pulse exceeds the crystal coercive field and produces domain inversion 12 under the metal electrode. However, frequent destructive electrical breakdown events remain a problem and have so far prevented this poling technique from being adopted for device production. Reports of electric field poling work in the scientific literature [Yamada et al , Appl. Phys. Lett., 62 (5), p435-6, 1993, Yamada et al , ASSL and Blue Green Lasers 1993, paper CThAl-1, Optical Society of America.] are limited to crystal substrate thicknesses of lOOμm due to the destructive effects of electrical breakdown. Larger apertures are required for bulk crystal applications. Following the approach of Yamada et al , Burns et al [Burns et al , Paper CThC3-l, Compact Blue Green lasers 1994, Optical Society of America, Burns et al , Phot. Tech. Lett., Vol 6, p252-4, 1994] have very recently achieved domain inverted structures in about 250μm thick LiNb0 3 slabs. However, electrical breakdown events remain a problem, and the width of the inverted domains is not well defined by the photolithographically patterned metal electrode, significantly reducing the efficiency of the device. The use of electric fields to pole ferroelectric crystals in a patterned form for quasi-phase-matching was proposed in 1980 by Papuchon et al (U.S. Patent N° 4,236,785) based on x or y-cut crystal substrates. In that invention, crenulated electrode structures 24 were fabricated by photolithography on the x or y-cut surface 26 of the optical crystal as shown schematically in Figure 2b, with a period defined by the coherence length of the desired nonlinear interaction. A high voltage is applied across the two electrodes such that the electric field is antiparallel to the crystal z direction (the spontaneous polarization direction of the material) to periodically domain invert the crystal substrate. This periodic poling technique has since been realized using LiNb0 3 as the crystal substrate, and reported in the scientific literature, [Janzen et al , Integrated Photonics Research, paper TuD5-l, 1992, Optical society of America] , but the inverted domains are necessarily very shallow (<2μm) because the electric field between the coplanar electrodes does not penetrate deeply into the crystal. Also proposed by Papuchon et al was the deposition and patterning of a second electrode over that used for domain inversion, allowing the application of different voltages to the inverted and uninverted domain sections in the quasi- phase-matched grating, and the subsequent tuning of the quasi- phase-matched interaction wavelength peak using the electro- optic effect. Matsumoto et al (Electron. Lett., 27, p 2040-2, 1991) describes the second harmonic generation of blue light in electrically periodically poled LiTa0 3 waveguides. The z- cut LiTa0 3 crystal substrate was poled by applying a periodic electric field using interdigital electrodes while heating the sample to just below the Curie temperature about 610°C. The conversion efficiency of the waveguide device fabricated was significantly lower than those fabricated by proton exchange on the +z face and has not been pursued further. Siebert et al (Proc. Soc. Phot. Instr. Eng. , 1362, p370-6, 1991) report ferroelectric microdomain reversal on y- cut LiNb0 3 surfaces using the pyroelectric effect to generate an electric field. A pair of crenulated electrodes is patterned on the y-cut face separated by about 6μm along the z axis and with a period of 30μm. Heating the crystal to about 100°C generates sufficient voltage across the electrodes, due to the pyroelectric effect, to spatially periodically invert the ferroelectric domains between the electrodes. The electric fields do not however dip deep into the crystal, so the resulting domains are only about lμ deep, too shallow even for waveguide based interactions to be efficient. izuuchi et al (Appl. Phys. Lett., 62, pl860-2, 1993) disclose a technique for fabricating periodic domain inversion in x-cut LiTa0 3 using selective proton exchange and quick heat treatment, as performed more commonly on the z-cut face. The domain inverted regions are inclined at an angle to the z-axis in the y-z plane. However, quasi-phase-matched nonlinear interactions have yet to be demonstrated in such a domain inverted structure. Electric field poling is not limited to ferroelectric materials. Brueck et al (U.S. Patent N° 5,239,407) report the creation of a large second order nonlinearity in fused silica when exposed to a high electric field (about 5kV/mm) at elevated temperatures (250°-325° C) . The stable nonlinearity is thought to be due to the migration of ionic contaminant species within the fused silica under the influence of the applied electric field. Organic polymer materials can also be poled to produce second order optical nonlinearities by the application of electric fields (e.g. U.S. Patent 5,064,265). A pendant group which exhibits second order nonlinear susceptibility is added as a side chain to a thermoplastic polymer. Poling is achieved by heating the polymer near or above its glass transition temperature, applying a DC electric field to align the molecular dipoles of the side chain pendant groups in a uniaxial orientation, and cooling the polymer while still under the influence of the electric field to fix the alignment of the side chain molecules. The current art is unable to provide a number of features required for the manufacture of cheap visible light sources, based on quasi-phase-matched second-harmonic- generation, and bulk periodically poled material for nonlinear optical interactions. These problems are poor reproducibility from sample to sample, shallow inverted domains unsuitable for bulk optical interactions, and the destructive effects of electrical breakdown on the crystal substrate. The field of integrated optic waveguide frequency conversion devices has, in the prior art, been based almost exclusively on z-cut ferroelectric materials because the best developed of the known domain inversion processes are only applicable to z-cut surfaces and only produce shallow inverted domains. This is the case with titanium in-diffusion into LiNb0 3 and barium ion exchange in KTP. To access the largest nonlinear optical coefficient in these materials, d 33 , the pump and signal beams must be polarized along the z axis, requiring a transverse magnetic (TM) polarized waveguide mode (polarized perpendicular to the plane of the waveguide chip) . However, semiconductor diode lasers, which are the most attractive pump sources for many nonlinear optical frequency conversion interactions, are polarized in the transverse electric mode (TE) , i.e. polarized parallel to the plane of the diode, and therefore require a costly polarization rotation element to be inserted between the diode and nonlinear crystal. There is significant need therefore for a manufacturable technique of periodically poling x or y-cut ferroelectric crystals so that the waveguide mode can be TE polarized to match the diode laser input and still access the large d 33 nonlinear optical coefficient. Electric field poling is difficult since the electric field strength required for poling is close to the threshold for electric breakdown. In order to achieve poling, the applied field must be above that required for poling, but not too far above the breakdown field. In practice, this is very difficult to achieve, and the difficulty becomes more severe with larger samples where the breakdown field can vary across the sample. The prior art has an intrinsic difficulty with breakdown. Due to the electrode configuration, portions of the material experience an electric field which is significantly higher than the average applied field in the bulk of the sample. The electrode pattern which is used in the prior art concentrates the electric field, resulting in severe breakdown problems. It has been determined that the problem in the prior art is caused by the electrode geometry, which is typically formed photolithographically into a pattern as shown in Figure 2a (Prior Art) . A metal film 22 is patterned to form a continuous contact layer over the regions 12 where the poling is desired, and the film is removed over the areas 13 where the original poling is not to be disturbed. A field is applied between electrodes 21 and 22, typically during a short pulse, and poling is achieved above a certain applied voltage. Unfortunately, in many of the samples electric breakdown occurs at some time during the applied pulse, and the resulting arc discharge physically destroys the sample. Breakdown occurs with such a high probability that electric field poling has not been considered as a viable method for producing domain-inverted ferroelectric material. The problem with the prior art electrode arrangement can be seen from an analysis of the electric field pattern at the surface of the substrate material. In the geometry of Figure 2a, the normal component of the electric field on the surface in the gaps 23 between electrodes is almost exactly 0.5 times the value E Q of the electric field in the bulk far from the patterned electrode. This is shown for example by J.D. Jackson in his well known book Classical Electrodynamics (Second Edition) , in the section treating mixed boundary conditions. From Gauss 1 Law, it follows that the average normal field along the surface under the electrodes must be substantially higher than the bulk field E 0 . In LiNb0 3 , it has not been possible to consistently apply a field E 0 which exceeds the poling threshold without also exceeding the breakdown threshold somewhere in the sample. This problem is due to the enhancement of the field under the electrodes. If the spatial duty factor of the electrodes is 50% (i.e., the width of the electrodes is 50% of the period), the average normal field under the electrodes is l.5xE 0 . The peak field under the electrode is even larger. From Faraday's Law, we know that the normal component of the electric field varies continuously as a function of the position x from its value of 0.5xE o at one edge of the electrode up to its peak value and back down to 0.5xE o at the other edge of the electrode. We can estimate the magnitude of the peak field even without an explicit solution of the electrostatics problem if we assume a reasonable functional form for the x-variation of the normal field. Assuming a sinusoidal dependence, one can calculate a peak normal field of 2.5xE 0 . In reality, the peak field is somewhere in the neighborhood of twice the bulk field. The room temperature breakdown field of LiNb0 3 is reported by the Sony group (Yamada et al ) to be around 26 kV/mm. The required field for poling is between 22 and 24 kV/mm at room temperature, which leaves a margin of no more than 20%. The bulk field must exceed the poling field or domain reversal will not propagate through the sample. (While it is known that the poling field decreases at higher temperatures, the breakdown field also decreases, so that no large advantage is obtained at high temperature.) To achieve poling, the applied field must exceed the poling field, but the applied field must not exceed the breakdown field by too much for too long, or the sample will be destroyed by a catastrophic electron avalanche. The margin between the required and the maximum fields is clearly narrower than the factor-of-four variation in the applied field. The simple periodic electrode structure practiced in the prior art cannot maintain the largest (peak) applied field below the breakdown field in LiNb0 3 while still exceeding the poling field in the bulk of the polable material 8. A similar problem exists in other ferroelectric materials such as KTP and LiTa0 3 . A technique is needed to allow periodic poling while not exceeding the breakdown field. A periodic electrode structure is needed which modulates the applied field above and below the poling field along the surface of the sample (to control the spatial extent of the regions which are to invert their nonlinear optical polarity) , while controlling the peak field so that it does not exceed the breakdown field by too much or for too long during the applied voltage pulse. SUMMARY OF THE INVENTION According to the invention, a poled dielectric structure, such as is useful as a frequency doubler, is fabricated by creating a uniform potential, such as a ground by means of an electrode surface, adjacent a first surface of a polable dielectric material, such as a piezo-electric or lithium niobate, and then applying an electric field adjacent a second surface of the polable dielectric material, where the electric field is spatially-modulated according to a three- dimensional modulation pattern with a field amplitude level at selected locations sufficient to cause atomic rearrangement within predefined regions in the polable material, and where the modulation amplitude level of the modulation pattern is controlled according to a modulation parameter. The control mechanism of modulation amplitude level can be controlled by protrusions of an electrically-conductive material extending toward the polable material or by modulated variations in the dielectric constant of a dielectric separating the polable material from an electrode plate. The electrically-conductive material may be a plate, a deposited layer or a liquid. The pattern may be periodic and may be aligned to form patterned poled structures, including waveguides. A first electrode and a second electrode may be disposed opposed to one another across a wafer of polable material or they may be along edges of the polable material transverse to one another, with the electrode on the wafer surface having a crenulated edge directed toward the second electrode. According to a further embodiment of the invention, the modulation amplitude level may be selectively enhanced in piezo-electric materials by stressing the materials while applying a poling force. The shape of the control mechanism may include regions of field concentration formed for example by corners adjacent the surface of the polable material to promote nucleation (creation of initial growth centers) of controlled domain-orientation. The degree of domain- orientation can be controlled by limiting charge transfer between the control mechanism and the uniform potential electrode. Various products made according to the process are suggested. Desired poling results are achieved by modulated control of the electric field excursions produced by an electrode pattern. By reducing the peak value of the applied electric field, the invention allows the use of a higher average electric field without causing breakdown. Alternatively it reduces the probability of breakdown significantly at a fixed applied voltage, making possible poling of large, production-scale wafers. The invention will be better understood by reference to the following detailed description in connection with the accompanying drawings. BRIEF DESCRIPTION OF THE DRAWINGS Figure 1 is a cross-section of one example of a structure made according to the invention Figure 2a is a first structure according to the prior art. Figure 2b is a second structure according to the prior art. Figure 3 is a perspective view in partial cross section of an electric field controlling mask on a wafer of polable material. Figure 4 is a perspective view in partial cross section of an alternative electric field controlling mask on a wafer of polable material. Figure 5 is a perspective view in partial cross section of an alternative electric field conductive layer on a wafer of polable material. Figure 6 is a perspective view in partial cross section of an alternative electric field conductive structure adjacent a wafer of polable material. Figure 7 is a perspective view in partial cross section for illustration of stress-enhanced poling. Figure 8 is a plan view of a pattern of pole- controlling segments on a surface. Figure 9 is a plan view of a pattern with waveguides. Figure 10 is a perspective view of a modulated- height mask. Figure 11-13 are perspective views of a process for making TE mode waveguide structures. Figure 14 illustrates a device with electrodes on transverse faces. Figure 15 is a perspecture view showing a crenulated electrode with a trough. Figure 16 is a perspective view in partial cross section of a modulated dielectric layer with electrodes adjacent a polable dielectric material. Figure 17 is a perspective view in partial cross section of a sliced poled wafer with a TE waveguide. DESCRIPTION OF SPECIFIC EMBODIMENTS The present invention comprises using a patterned dielectric spacer layer covered by a conducting layer. The conducting layer is brought to a predetermined voltage by drive circuitry, but the applied field at one surface of the sample is modulated by the (controllable) distance to the conducting layer. Figure 1 is a cross-section of one example of a structure made according to the invention. In Figure 1, an electrically-insulating layer 4 has been deposited and patterned to cover areas 13 where domain inversion is not desired. A continuous conducting layer 14, such as a conductive liquid, is then provided, making contact with the sample in the gaps 10 left by the patterned insulator, and covering the insulator. The equipotential surface defined by the conducting surface is therefore spatially corrugated in alignment with the field (the vertical direction) in a manner defined by the thickness and location of the remaining regions of insulating film. The advantage of this configuration over the prior art is most easily seen by examining the electric field distribution at the surface of the sample as a function of the differential thickness d of the patterned electrically- insulating layer. In the limit as d approaches zero, the electric field is totally uniform, and is equal to the bulk field E 0 , or the applied voltage divided by the thickness of the sample. In the limit where d is very large compared to the period P, the surface field is strongly modulated, with its maximum value under the regions where the conducting layer touches the surface, and its minimum value under the insulator regions. The x-dependence of the field takes on a characteristic functional form dictated by Maxwell's equations, and which depends only on the duty factor (for a periodic structure, far from edges and other pattern changes) . As the differential thickness d is varied between these two extremes, the modulation of the normal component of the applied electric field changes from its maximum value to zero. The importance of the present configuration and method of construction is this ability to control the modulation depth of the applied electric field, an ability virtually absent in the prior art. By adjusting the differential thickness d, the field modulation can be reduced enough to avoid breakdown while still achieving domain- reorientation or poling. The thickness d is a selected amplitude modulation parameter which can be adjusted to control the electric field strength in selecteed regions within the polable material 8, including in particular the peak-to-peak field variation at the surface 6. (By poling we mean the atomic orientation of the microscopic dipoles within the polable material. Poling can include domain reversal in a previously uniformly poled substrate, establishing a poling direction within a wafer which previously had domains of random orientation, or orienting a domain in a substrate which was partially poled.) The patterned layer may be a dielectric material which covers the areas which are not to be inverted. (In the prior art, the patterned layer is a metal and covers the areas whic- are to be inverted.) The invention is a method of applying the desired patterns, creating a uniform potential, and controlling the electric field according to a modulation pattern, the modulation pattern being for example produced by protrusions from a conductive material, which in the case of Figure 1 is a conductive liquid. Figure 1 illustrates schematically a cross section through a structure made according to the preferred embodiment method of a patterned poled dielectric material 2. The polable material 8, which is, in this preferred embodiment a ferroelectric crystal consisting of commercially-available single domain LiNb0 3 , is cleaned, e.g. by oxygen plasma ashing, to remove all hydrocarbon and other contaminants remaining from the polishing and handling processes. An electrically-insulating dielectric film 4 is deposited as a mask with a predetermined thickness in a preselected x-y pattern on a z-cut face 6 of the crystal. The electrically- insulating dielectric film is, for processing simplicity, composed of organic photoresist and may be up to several microns in thickness. (Other insulating materials such as Si0 2 or Ti0 2 may alternatively be used. Although electric insulation is desirable, it is not required of our dielectric materials, provided that the material withstands the high applied voltage without breakdown or deterioration.) The pattern of the electrically-insulating, electric-field- strength controlling mask with selected thickness, is obtained by exposing the photoresist through a suitable photomask using standard contact lithographic techniques. (An alternative patterning procedure would involve projection photolithography which requires no contact between the photomask and crystal substrate, and is more suited to high volume production applications) . The electric field controlling mask of Figure 1 is shown in perspective in Figure 3 and consists of a planar electrically-insulating film 4 deposited on the +z surface of the LiNb0 3 8, in which contact-windows 10 are patterned to allow direct electrical contact with the crystal by the electrode material (e.g., the conductive liquid). In the preferred embodiment with LiNb0 3 as the ferroelectric substrate crystal, the patterned electric field controlling mask is formed on the +Z crystal surface, as this is where domain nucleation occurs, followed by growth towards the -z face. As domain inversion is nucleated on the +z surface there is no need to provide a patterned mask on the -z face, consequently a planar electrically-conducting material provides suitable electrical contact to the -z face. In all embodiments for LiNb0 3 and other ferroelectric materials, such as LiTa0 3 , KTP, KNb0 3 , BaTi0 3 , SBN, Ag 3 AsS 3 , etc., and for other non-ferroelectric materials, such as certain polymers (having dipolar chromophores with large hyperpolarizability) and fused silica, the patterned electric field controlling mask should be applied to the material surface at which domain nucleation occurs. The polable material must be a dielectric for the electric field poling process to work because it must be capable of supporting an applied field without being destroyed. It need not be an insulating material as long as the induced currents cause no damage during the poling process. Electrical contact to a first surface 7 of the material, the -z surface, is made by a first electrically- conductive material 15 which may in any embodiment be, for instance, a liquid conductor, a thin metal film deposited on the -z surface, or a bulk electrical conductor adjacent to the -z surface. Note that adjacent in the context of the embodiments herein includes the use of coatings between materials (the surface and the conductor) . Electrical contact to a second surface 6 of the material, the +z surface, opposing the first surface, is achieved by the deposition of a second electrically-conductive material 14 (can be the same material as the first electrically conductive material) upon the electrically-insulating dielectric film. The opposing surface is somewhat distant from the first surface, and may be parallel to the first surface, or angled and/or curved and/or with corners, edges, and/or indentations, according to the application geometry. The planar local geometry shown in the figures therefore includes larger scale three dimensional structures in the polable dielectric material, and of course, the films have true three dimensional structure. The second electrically-conductive material in liquid form may be a saturated aqueous solution of a salt such as LiCl or KC1. The liquid conductor fills the contact-windows in the insulating dielectric film and contacts the crystal +z surface. Due to the small dimensions of the contact-windows, occasional air bubbles may be trapped between the liquid conductor and the second surface of the crystal, occasionally preventing good electrical contact from being made. Electrical contact to the liquid conductor is made using electrically-conducting plates 16, 17 or wires, allowing good current distribution as the area of the sample to be poled is increased. The liquid conductor is confined to the desired area(s) of the surface(s) of the polable material as illustrated schematically in Figure 1, e.g. using rubber o- rings 18, 19. Confinement is required to prevent the liquid conductor from creeping over the edges of the polable material and causing electrical flashover and a short circuit during the poling process. A pulsed high-voltage electrical potential is applied across the crystal substrate using a suitable power supply 20, to oppose the spontaneous polarization direction of the substrate crystal, i.e., a positive voltage is applied to the +z face of the crystal, and the -z face is grounded. Alternatively, a negative voltage may be applied to the electrically conducting material placed adjacent to the -z face while the means for controlling the electric field strength placed adjacent to the +z face is grounded. It is not necessary for the electrically conductive materials used for the electrodes to have the conductivity of a metal; it is sufficient that a uniform potential can be applied via the electrically conductive material during the poling process. The uniform potential may include small potential variations across the polable dielectric material provided that the resultant field variations at the nucleating surface for the domain inversion are small compared to the variations imposed by the means for controlling the electric field strength, and provided that the resultant field variations at the opposite surface of the polable dielectric material do not cause the bulk field strength to fall below the threshold field for propagation of the poling. It should also be noted that any ground is a sufficient electrode, no matter how far away it may be placed from the sample. If a ground plane is used as one of the electrodes, it should be kept close only to reduce the potential required to produce the needed electric fields within the polable dielectric material. Multiple high-voltage pulses may be applied to the sample, each with a duration ranging from μs to seconds. In all embodiments the applied effective potential must exceed the coercive field of the crystal at some point in the crystal in order to achieve poling. The domain-orienting potential threshold depends on the electrode configuration and the sample temperature. For the preferred embodiment with a photoresist insulating layer and a saturated LiCl electrode at room temperature, the domain-reversing potential threshold for a LiNb0 3 substrate crystal is around 23-24kV/mm. For fused silica, the effective domain-orienting potential is approximately 5 kV, independent of the thickness of the fused silica wafer. The electric field within the crystal is modulated by the differential thickness of the patterned insulating dielectric film. Thus domain inversion 12 is obtained under the contact-windows in the insulating electric field controlling mask, contrasting with the prior art (Figure 2a) where domain inversion is obtained directly beneath the patterned conductive mask 22. The inverted domains formed by the invention (Figure 1) have dimensions determined by, but not necessarily exactly the same size as, the dimensions of the configuration of photolithographically defined contact- windows on the insulating electric field controlling mask. It should be noted that direct electrical contact is not necessary for poling to occur. An insulating film may prohibit contact between any of the conducting electrodes and the polable material. Poling will still occur provided the applied electric field is above an effective field. If poling is performed at elevated temperatures, the domain reversal potential threshold is decreased. Experimentally it has been observed to drop from about 11.8kV at room temperature to about 8.9kV at 230°C, with electrical contact to the crystal made using electrically-conducting epoxy. Poling was performed in an oil bath heated on a hot plate. It has been reported (Janzen et al , ECOC'92 Companion workshop, 1992) that the crystal breakdown potential threshold also decreases with increasing sample temperature. However, our own experiments indicate that poling at an elevated temperature (<230°C) reduces the likelihood of breakdown occurring when combined with electrically-conducting epoxy contacts to the crystal. It is expected that the same reduction in breakdown likelihood will result from poling samples at elevated temperature using the methods of the invention. The sample temperature may be elevated during poling by, for instance, placing the entire poling electrode apparatus in an oven, or alternatively by illuminating the sample with a heat lamp. Electrical breakdown events which can occur during the electric field poling of LiNb0 3 are thought to be the result of an electron avalanche. Unlike the prior art, such as Yamada et al who reduced the effects of breakdown by thinning the substrate crystal (to about lOOμm) so that the electrons passed entirely through the crystal before obtaining sufficient energy to destroy the sample, in the present invention, breakdown is controlled by the modulation of the electric field due to a patterned insulating dielectric film, resulting in no electron avalanche effects. This enables thick substrates (>500μm) to be poled. In fact, the maximum sample thickness that can be poled appears limited simply by the available high voltage pulse. During poling, the voltage across the sample and the current flow are monitored. The charge transfer to the ferroelectric crystal is deliberately limited to the amount required to produce the desired domain inversion pattern, which is known to be about 1.4μC mm -2 for LiNb0 3 . The charge flow may be limited by 1) restricting the current flow in the circuit (for instance with a resistor connected in series with the crystal) , 2) restricting the applied voltage (the closer the applied voltage is to the poling threshold, the lower the current which flows) , 3) restricting the pulse length of the applied voltage, or by 4) any combination of these variables. By limiting the charge flow to that required to create the desired pattern, coalescence of the patterned (periodic) domains by lateral domain wall motion is prevented. (This would otherwise increase the domain inverted surface area and therefore require a larger charge transfer) . The dimensions and arrangement of the poled regions of the patterned poled material are set by the desired application of the patterned poled substrate. The dimensions of the patterned domain formation correspond to, but are not necessarily exactly the same as, the dimensions of the patterned contact-windows in the mask material. Using standard photolithographic techniques, feature dimensions as small as lμm can be realized in the insulating mask material, with any desired configuration. The depth of the domains is about equal to the thickness of the ferroelectric crystal, e.g. >500μm, and is limited only by the crystal substrate thickness. Liquid conductor contact has a particular advantage. It eliminates the poor current distribution ability of thin film metallic electrodes and wire bonded contacts, which otherwise would lead to localized heating and an increased likelihood of electrical breakdown, combined with poor edge quality of the inverted domains at the crystal +z surface. In a first alternative embodiment of the invention, the electrically-insulating dielectric film is composed of Si0 2 or other hard insulating dielectric material such as Ti0 2 or A1 2 0 3 , providing the twin advantages of greater electrical insulation and increased robustness when compared to simple photoresist layers. Thin film electrically-insulating oxide layers may be readily deposited by evaporation (or alternatively R-F sputtering) . Film thicknesses of >50nm are appropriate. The hard insulating layer is patterned to produce the desired electric field control configuration using standard photolithographic techniques and an etching process, e.g. wet etching in buffered oxide etch. (Alternative etching techniques which could be used include reactive ion beam etching or ion bombardment etching.) A hard oxide insulating layer such as Si0 2 is more suited to large volume production than the relatively soft photoresist layer as the hard patterned film is less likely to be damaged during processing and handling. In a second alternative embodiment of the invention, a different structure is used for the patterned electrically- insulating electric field control mask, which is shown in perspective and partial cross section in Figure 4. The mask is composed of one or more layers 28 of electrically- insulating dielectric material, which may have different chemical compositions, and which are deposited by suitable techniques on the +z face of the LiNb0 3 crystal. The mask is patterned using standard photolithographic techniques. Patterning may completely open contact-windows 10 on the LiNb0 3 by removing all the layers of the mask, or create a mask-thickness-modulation-region 30 by leaving one or more planar layers at least partly intact on the crystal surface, resulting in no direct electrical contact to the crystal. The electric field within the crystal is modulated by the varying thickness of the insulating mask such that domain inversion 12 only occurs in the high electric field regions beneath the mask-thickness-modulation-regions or open contact-windows. A single layer thickness modulated insulating mask structure which might for instance allow no direct electrical contact to the crystal surface can be created in a photoresist layer simply by underexposing the photoresist so that some material is left in all areas after development. A similar structure can be created in a hard insulator layer (e.g. Si0 2 or Ti0 2 ) by incompletely etching the planar layer, using for instance wet chemical etching, reactive ion etching or ion beam bombardment etching. An example of a multilayer insulating mask structure is a layer of Si0 2 deposited on the crystal +z face (e.g. by evaporation or sputtering) with a thickness of about 50-1000nm, covered by a layer of photoresist which may be up to a few microns in thickness. The photoresist layer is exposed and developed and the resulting pattern transferred to the Si0 2 layer by a suitable etching process (e.g.wet etching in buffered oxide etch), which may or may not penetrate completely through the Si0 2 layer to reach the crystal substrate. After patterning, the photoresist is left on the sample during poling, to increase the depth modulation of the insulating mask and therefore to increase the modulation of the electric field within the crystal. Note that the selective thickness of the dielectric film can be made to vary in many ways across the polable dielectric materials, including gradients of thickness, and periodic and aperiodic patterns of multiple heights. A third alternative embodiment of the invention eliminates the effects of air bubbles trapped within the contact-windows or mask-thickness-modulation-regions in the electric field controlling insulating mask. Such air bubbles locally reduce the electric field by increasing the stand-off of the liquid conductor and inhibit poling from occurring. An electrically-conductive layer 32 (e.g. Al or other metal) is deposited (e.g. by evaporation or sputtering) over the patterned insulating mask 4, as illustrated in Figure 5. The varied thickness of the mask is the amplitude modulation parameter which can be adjusted to produce the desired field modulation. Where the insulating mask material(s) has been completely removed 10 by the patterning process, the deposited electrically-conductive layer makes direct contact with the crystal surface. Overlaying the deposited conductive layer with a liquid electrical conductor results in electrical contact to all parts of a mask-thickness-modulation-region 10, 30, even if part of the region is covered by an air bubble, as long as the liquid conductor makes contact with the conductive layer at some point in the region. The continuous electrical contact over each mask-thickness-modulation-region translates into complete domain reversal and an improvement in the overall uniformity of the domain inversion pattern. Deposition of a thick electrically-conductive film over the patterned insulating mask allows electrical contact to be maintained over the entire deposited film, i.e. making electrical contact to any part of the thick deposited conducting film achieves contact with all of the mask- thickness-modulation-regions in the electric-field-controlling insulating mask. Electrical contact to the conducting film can be made by a liquid electrical conductor or alternatively by direct contact to a bulk electrically-conducting material adjacent to the +z surface. In a fourth alternative embodiment of the invention, a patterned second electrically-conductive material 36 having protrusions 38 in a configuration of modulated height 40 is used to control the electric field strength within the polable dielectric material, as illustrated in Figure 6. The protrusions have selected heights to determine the modulation of the applied electric field strength, and selected transverse dimensions to determine the pattern of the electric field modulation. They may be composed of the same material as the electrode 36, or they may be fabricated from another electrically conductive material deposited on the electrode. A first electrically-conducting material 34, e.g., a metal plate, thin film or liquid conductive material, is placed adjacent a first surface, the -z surface 7, of the LiNb0 3 crystal. The patterned second electrically-conductive material is placed over a second surface, the +z surface 6, of the LiNb0 3 crystal, the second surface opposing the first surface and such that the protrusions confront the second surface. The differential distance 42 between the first electrically-conductive material and the patterned second electrically-conductive material is the parameter which controls the electric field strength in selected regions within the polable dielectric material. Upon application of an effective electrical potential 20 between the first electrically-conductive material and second electrically- conductive materials, poling 12 occurs only where the electric field in the polable dielectric material exceeds the domain inversion potential threshold of the material. The poling process produces selective reversal of domains in the polable dielectric material, in a pattern according to, but not necessarily with exactly the same dimensions as, the configuration of protrusions on the patterned second electrically-conducting material, resulting in a patterned poled dielectric structure 2. Note that the protrusions may be filled in with a dielectric material as long as they create a modulated electric field. The planar configuration of the protrusions 39 of the second electrically-conductive material is defined by the desired application for the patterned poled material. The planar configuration may have significant curvature so that over a distance corresponding to many protrusions the surface defined by the protrusions takes on a strongly three dimensional character. Each protrusion may be designed to contain one or more regions of electric field concentration 54 which serve to nucleate domain formation. The region of electric field concentration may consist of a corner bounding one of the selected regions of electric field control. If the region of field control is a conductive material, the corner must be an outside corner; if it is a dielectric material, the corner must be an inside corner, producing field concentration in a conducting material which is formed around the dielectric material template. The configuration of protrusions on the patterned electrically-conducting material can be produced by photolithographically patterning a layer of photoresist on the surface of the material and transferring the pattern into the material by etching, e.g. wet chemical etching, reactive ion etching or ion beam bombardment etching. The modulated height of the protrusions is determined by the duration of the etching process. In another alternative embodiment of the invention (Figure 16) , a patterned dielectric film 212 having a modulated dielectric constant is used to control the electric field strength on the surface 220 and within the polable dielectric material 210 as illustrated in Figure 16. The dielectric film 212 contains regions of enhanced 218 and/or diminished 226 dielectric constant to accomplish the modulation. The regions of modulated dielectric constant are arranged in the two dimensions locally transverse to the surface 220 of the polable dielectric material. A first electrically conductive material (electrode) 216 is placed adjacent the surface 222, and a second electrically conductive material 214 is placed adjacent the dielectric film which confronts the surface 220. The voltage source 224 is used to apply a potential between the two electrodes, the potential being above the threshold for causing domain orientation to occur in the material 210. The thickness 228 of the dielectric material is one parameter for controlling the modulation of the applied electric field strength, and the magnitude of the modulation of the dielectric constant of the film 212 is another parameter for controlling the modulation. The process of the invention may be enhanced by the application of stress or strain at the LiNb0 3 crystal surface, which will generate electric fields within the crystal due to the piezoelectric effect. The generated electric fields may either add to or subtract from the applied poling potential to assist or inhibit the poling process. A periodic stress can be applied to the crystal surface via the patterned electric field controlling insulating mask as suggested by the fields 46 illustrated in Figure 7. By depositing, at elevated (or depressed) temperature, a planar layer 44 with a temperature coefficient of expansion different to that of LiNb0 3 , and then cooling to room temperature, a stress is generated in the planar layer and exerted on the crystal 46. The tensile or compressive nature of the stress in the layer can be chosen by depositing a film with a higher or lower coefficient of thermal expansion respectively. Patterning of the planar layer, using photolithographic techniques, to form the electric field control mask 4, 44 generates a periodic strain across the crystal surface. Alternatively the planar layer can be deposited at room temperature, patterned, and the crystal heated to an elevated temperature (or cooled) during the poling process to generate the periodic strain. Patterning of a compressively strained layer exerts a tensile strain on the crystal under the center of the electrical field control mask, and a compressive strain on the crystal at the edge of the mask where the layer is able to expand towards the center of the patterned window 10. An example of a suitable planar layer is Si0 2 which has a coefficient of thermal expansion of about 5.5xlO~ 7 /°C compared to about 15xlO "6 /°dC for LiNb0 3 along the x and y axes. Applying a strain along the x axis results in an electric field generated along the z axis due to the e 311 coefficient of the piezoelectric tensor. For LiNb0 3 with an Si0 2 overlayer, the generated electric field is about ±12 volts per mm/°C of temperature differential from the Si0 2 layer deposition temperature (V/mm/°C). Thus with a temperature differential of 100°C from the layer deposition temperature, an internal field of about 1200V/mm is generated, which assists or opposes the applied poling voltage depending on the type of strain applied to the crystal. When a poling force is applied to the polable dielectric material, the piezo-electric field pattern produced by the stress can be used to modulate the poling force above and below the effective force required for domain orientation. If the modulation is applied in the regions where nucleation of domain reversal occurs, it can be effective in creating a poling pattern within the polable material. In the case of electric field poling, uniform electrodes can be used with the poling pattern being controlled by the stressing pattern. The field assisted approach may also be applied with other poling techniques such as ion indiffusion, outdiffusion, and quick heat treatment. Other alternative embodiments of the invention include the use of other types of polable materials. Other ferroelectric crystals which are suitable include for instance, LiTa0 3 , KTP, KDP and its isomorphs, KNb0 3 , BaTi0 3 , SBN, Ag 3 AsS 3 , etc. The invention is also applicable to the patterned poling of non-ferroelectric materials such as fused silica and organic polymers. In each of these cases the patterned electric field controlling material used to define the patterned poling is formed on or placed adjacent to the crystal surface on which the inverted domains nucleate (e.g. +z for LiNb0 3 ) . It has been empirically determined, that when a configuration of electric field-controlling material is used to establish a poling pattern for fabricating a patterned poled dielectric structure, the poled domains are nucleated from regions of the field-controlling material which concentrate the electric field. Controlling the electric field using a photolithographically patterned electrically- conductive material, e.g. a metal film, deposited on the -i-z face of LiNb0 3 results in poled domain nucleation at outside corners of the metal film pattern, where the inside angle between adjacent sides of the conducting film pattern feature is less than 180°, when a high voltage pulse or pulses is/are applied between the patterned metal electrode on the +z face and a planar metal electrode on the -z face, with electrical contact to the metal electrodes made by bonding wires to the metal layers using an electrically-conducting epoxy. A corner, in the context of a planar pattern, means the junction of two boundaries which intersect at an angle at a geometric feature which is somewhat rounded on the scale of the pattern. An inside angle is an angle measured with the arc inside the structure. In the case of a three dimensional pattern, a corner means the intersection of an edge and a surface at a geometric feature which is somewhat rounded on the scale of the pattern. An outside corner contains less than a 180 degree inside angle between the axis of the corner and some axis in the plane. A point is a special case of an outside corner where edges meet. All of these regions enhance electric field strength, with an enhancement reduced by the degree of rounding relative to the scale of the pattern, and all types of outside corners can be used to nucleate domain inversion. To achieve uniform patterned poling over a large crystal, a field-controlling electrically-conductive material structure 48 consisting of a plurality of planar segments 50 of electrically conducting material is fabricated on the +z face of the crystal, as illustrated in Figure 8. This structure is distinguished by having a high and uniform density of corners for nucleation of domain orientation. Each segment of Figure 8 has four corners for nucleation; the domain orientation propagates outwards from the nucleation points, under the conducting electrodes, to merge together near the middle of the segments, forming almost completely oriented areas substantially under the segments. The straight sectors of pole control 52 formed by each line of segments are then almost completely domain oriented. By sectors of pole control, we mean geometric areas composed of multiple segments, wherein the poling induced in the material is substantially controlled to be a desired value, when averaged over the segment poled regions and the gaps in the sector. The desired value may be very close to 100% as for instance in phase matching gratings, or it may be a much " lower value, as for instance where several regions of pole control are to be distinguished in their function by their average poling fraction. The sector may be a multiply connected region containing other structures. Such a structure can readily be fabricated by depositing a suitable electrically-conducting material (e.g. a metal such as Aluminum) and using standard photolithographic techniques to create the desired pattern. Embodiments of the patterned electric field controlling structure should be fabricated on the +z face of LiNb0 3 as this is where domains nucleate, with growth towards the -z face. For other polable materials, such as LiTa0 3 , KTP, KNb0 3 , BaTi0 3 , SBN, Ag 3 AsS 3 , fused silica and polymers etc, the patterned electric field controlling mask should also be applied to the crystal surface at which domain nucleation occurs. The segments are aligned to comprise at least one sector 52 of pole control across the surface of the polable dielectric material. Each one of the segments includes at least one region 54 adapted to support the concentration of electric fields. The field concentration region may comprise a corner having an inside angle of less than 180° between adjacent sides, to promote nucleation of poling. During the applied high voltage pulse(s) domains spread laterally from the nucleation sites into the region of high electrical field defined by the segments of electric field controlling material, producing complete poling of each segment. Electrical continuity between the segments throughout the configuration is maintained via interconnecting conductive regions 56, ensuring good current distribution and uniformly patterned poling across the entire electric field control structure. Electrical connection of the electrical potential source to the patterned electrical conductor can be made by wire bonding or direct contact with the electrical conductor. Electrical connection to the -z face of the crystal is made by a further electrically-conducting material which may in ary embodiment be, for instance, a liquid electrical conductor, a thin metal film deposited on the -z surface, or a bulk electrical conductor adjacent to the -z surface. The sectors of aligned segments of electric field control material can be arrayed to define a periodic pattern along an axis. The relative arrangement of the segments within a sector and of one sector to another can be adjusted to achieve the poling pattern required for a desired application. For a bulk optic nonlinear optical frequency converter the field controlling material configuration of Figure 8 is appropriate. The sectors comprising the aligned segments and the electrical interconnections between the segments are offset from one another so that a colli ated (or focussed) laser beam travelling through the polable material perpendicular to the sectors sees a uniformly poled grating when integrated along the length of the device and the generated signal beam(s) can be maintained in the TEM 00 single transverse mode. The efficiency in this case is reduced from the ideal instance, which consists of uniform long bars stretching across the entire device aperture, because of the presence of both gaps between the segments and electrical interconnections among the segments. The reduction in the efficiency is determined by the duty cycle of the segments within a sector combined with the duty cycle of the electrical interconnections between the segments. The case of individual segments of length 20μm separated by gaps of 2μm, with lμm wide electrical interconnections reduces the efficiency to about 80% of the ideal case. For an integrated optic waveguide-based nonlinear optical frequency converter, an embodiment of the desired electric field controlling structure is illustrated in Figure 9. The sectors of the aligned segments 52 are arrayed such that an optical waveguide 58 can pass through a single row 60 of the segments 50. The electrical interconnections 56 between the segments are fabricated outside the path of the waveguide 58, so the efficiency of this embodiment is 100% of that of the ideal uniform long-bar configuration. Alignment of the waveguide with the poled segments can readily be achieved using suitable photolithographic alignment marks. An alternative embodiment of the inventions of Figures 1, 3, 6, 8 and 9 is illustrated in Figure 10. Here an electrically-insulating mask 62 forms the electric field controlling structure for thickness modulation used to establish a high domain nucleation density poling pattern for fabricating a patterned poled crystal. The segments 50 are formed by modulating the thickness 40 of the insulating mask 62, using photolithographic (and) etching processes. The insulating mask 62 may be formed of multiple planar layers of different chemical compositions. The mask thickness modulation may vary between completely removing sections of the insulating mask, and leaving part of one or more of the planar layers of the insulating mask intact. Each mask thickness modulation segment includes at least one electric field concentrating region 54. The electric field concentrating region may take the form of a corner of the segment where the included angle between adjacent sides of the mask thickness modulation region is less than 180°. The thickness modulated electric field control insulating mask is overlaid by an electrically-conducting material (not shown) , which may be for example, a liquid electrical conductor or alternatively a metal film deposited on the insulating mask, which is electrically-connected to the source of electrical potential. The general arrangements of the sectors and the segments required to fabricate bulk and waveguide frequency conversion devices are the same as those used for the electric field controlling electrically-conducting material as illustrated in Figures 8 and 9, except that there is no longer any need to provide the electrical interconnections between the segments, as this function is achieved by the electrically-conducting overlayer on the thickness modulated insulating mask. In all of the methods of fabricating patterned poled devices described above, the pattern is selected according to the application. A simple pattern is the periodic grating pattern in which the domain is inverted between two directions with 50% duty cycle. This pattern is used for example in nonlinear frequency conversion in quasi phase matched structures. The period of this pattern is selected to phase match the desired nonlinear interaction. An important variation of the above techniques is the use of a patterned electrode to imprint the poling pattern into the sample material as described above with Figure 6. This configuration has the advantage that no processing (other than polishing and cleaning) is required on the sample to be patterned by poling. If the structure is inherent in the electrodes, the samples can be mass produced as rapidly as they can be mounted, poled, and dismounted from the electrodes. While the discussions of the alternative poling configurations do not necessarily refer to this possibility, these configurations can also be adapted to the patterned electrode configuration. For example, in Figure 5, the conducting material 32 and the patterned dielectric material 4 can be bonded to the surface of an external electrode (not shown) which is used to physically place the layers 4 and 32 adjacent to the polable dielectric material 8 as shown. While the adjacent placing includes the case without any significant gap, there may be a small gap between the layers 4 and 32 and the material 8, provided that the gap is small compared to the typical dimensions of the pattern according to which the layers are corrugated. If the gap is small, the change in the magnitude of the electric field in the material 8 is not too severe. The patterns of electrically conductive material of Figures 5, 6, 8, and 9 can all be attached to or fabricated into an electrode used for mass production of electric field poled wafers. The pattern of dielectric material of spatially varying dielectric constant of Figure 16 can also be attached to an electrode for mass production. The dielectric layer structures of Figures 3, 4 and 10 can also be overlaid with a deposition of conducting material as in Figure 5, and attached to an electrode for mass production. The invention further provides a process for creating transverse electric (TE) polarized periodically poled waveguide devices which access the large d 33 nonlinear optical coefficient. The periodically poled substrate is a ferroelectric crystal which may be, for instance, LiNb0 3 , LiTa0 3 , KTP, KNb0 3 , BaTiθ 3 , SBN, Ag 3 AsS 3 , etc. The process is illustrated schematically in Figure 17. The polable dielectric material substrate 8 is poled as shown in regions 248 which penetrate substantially into the bulk substrate. The substrate wafer is preferably LiNb0 3 , in which case the z axis (the optical axis of the nonlinear material) is oriented as shown by the vector 246. An annealed proton exchanged (APE) waveguide diffused into the top z-cut surface of the wafer will form a TM waveguide as shown for waveguide 242. To form a TE waveguide using the favorable APE technique, an x- cut or y-cut region must be exposed (or an intermediate cut between the pure x- and y-cuts can be used) . The cut 240 reveals an edge with the poling axis 246 substantially in the plane of the edge. The waveguide 244 may be fabricated in the edge by annealed proton exchange, forming a TE polarized waveguide. This is useful for example in periodically poled frequency conversion devices if the poling extends into the bulk of the substrate. Figures 11, 12, 13 illustrate a low cost fabrication technique for a LiNb0 3 substrate as an example. Step 1 involves periodically poling a z-cut LiNb0 3 substrate 150 using the methods of the invention of Figure 1 and its alternative embodiments. The resultant inverted domains 12 extend completely through the crystal substrate, the thickness of which is while maintaining the dimension and periodicity of patterned poling which is imposed by the photolithographically patterned electric field-controlling mask on the +z surface. After periodic poling and removal of the patterned insulating mask, the z-cut substrate is sliced using saw cuts 152 as shown in Figure 11, creating thin strips 156 perpendicular to the inverted domain bars 12 using a wafer saw. The individual strips are rotated by 90° about the y axis shown in Figure 11, exposing the x (or y) cut faces. The z-cut faces are cemented together 158, e.g. with shellac or an epoxy cement, to form a composite wafer 160 (Figure 12) . (Note that if the poled regions are oriented along the y axis of the material instead of the x axis as shown in Figure 11, the cut and the rotation will be along the x axis.) Unpoled x-cut material may be cemented around the edges of the patterned poled pieces to increase the surface area of the composite wafer. The + and -x faces (or + and -y) faces of the composite wafer are optically polished, for instance using a Logitech Precision Polishing Machine, to yield an optically flat and scratch free composite substrate composed of multiple sections of bulk periodically poled material. A thin film 162, e.g. 200nm of Si0 2 or Al, is deposited on one of the polished x-cut (or y-cut) surfaces to act as a waveguide mask. Photoresist is spun on top of the deposited film and exposed through a suitable photomask. After developing and hardbaking the photoresist, the waveguide mask pattern 164 is transferred to the deposited thin film by wet etching in, for instance buffered oxide etch (alternatively a lift-off technique can be used to deposit and pattern the waveguide mask after the development of the photoresist layer) resulting in the structure illustrated in Figure 13. The waveguide mask pattern defines waveguides with propagation direction along the thin strips of crystal, that is along the axis of the periodic poling pattern. The composite wafer is now diced perpendicular to the waveguide propagation direction, into device length sections 166, and the crystal endfaces 168 optically polished to enable coupling into the waveguide (Figure 13) . Waveguides are ideally formed using the annealed proton exchange (APE) process. Alternatively, ions other than protons may also be indiffused or ion exchanged into the polable material. In the case of APE, the composite wafer strips are immersed in molten benzoic acid to exchange protons from the acid for lithium ions in the crystal. The resulting step index waveguide is then annealed for several hours at around 300°C to diffuse the protons deeper into the crystal and create a low-loss waveguide with high optical nonlinearity. Finally, the individual device slices are separated and cleaned, each device chip having a multiplicity of waveguides running perpendicular to the periodically poled domain inversion grating structure. The APE waveguide increases the crystal extraordinary refractive index, forming a waveguide for light polarized along the z-axis, which in x or y cut material is TE polarized. Thus this invention yields a TE polarized quasi-phase-matched domain inverted waveguide which removes the need for a polarization rotation element between a TE polarized semiconductor diode laser and the waveguide chip. An alternative fabrication process would perform the waveguide exchange and annealing steps before the composite wafer is diced and the end faces polished, so as to avoid damage to the fragile end faces during handling. Poling of x (or y) cut ferroelectric crystals an be achieved using an electric field and an electrode configuration of a first electrode 190 and a second electrode 180 as shown in Figure 16. The second electrode 180 is formed by patterning (using standard photolithographic techniques) an electrically conductive material deposited on the x (or y) cut surface 182 of a ferroelectric crystal substrate , which could consist of LiNb0 3 , LiTa0 3 , KTP, KNb0 3 , BaTi0 3 , SBN, Ag 3 AsS 3 , etc, some hundreds of microns from the edge 184 of the crystal. For a substrate of LiNb0 3 , the crenulated edge 186 of the electrode must extend towards the -z face 188 of the crystal so that domains 12 nucleate on the patterned electrode and grow towards the -z face. A large number of electrodes may be fabricated on a wafer in an essentially parallel array which can then be sliced to create individual strips. The first electrode 190 is formed from electrically conductive material, which may consist of a metal plate, placed adjacent to the z-cut side face of the strip. Alternatively a film of conductive material, such as a metal, may be deposited directly on the z-cut surface of the strip. A number of strips may be stacked together before poling to provide a mass manufacturable process. A continuous or pulsed electric field greater than the coercive field of the crystal (about 20kV/mm) is applied across the two electrodes to produce poling of the crystal. The applied voltage opposes the spontaneous polarization direction of the substrate crystal, i.e. a negative pulse should be applied to an electrode formed on the -z face of the crystal. As the first electrode is adjacent a side face of the crystal, the applied electric field extends deep into the crystal, resulting in deep poled domain formation between the first electrode placed adjacent to the z-cut face of the crystal and the patterned second electrode. The first electrode is substantially planar, parallel to the . second electrode. The electrodes may include angles and curves such that they separate from each other, provided that the applied field is sufficient to produce poling in the desired regions. The patterned second electrode spatially modulates the applied electric field to achieve periodic domain inversion by producing poling only in the high electric field regions. After domain inversion the second conductive electrode may be stripped from the crystal and a waveguide 192 fabricated, using standard photolithographic techniques, in the poled region of the crystal, and propagating along the y (or x) axis. For a substrate of LiNb0 3 the waveguide would preferably be fabricated by the annealed proton exchange technique because of its insensitivity to photorefractive damage. Other waveguides may also be used. An alternative electrode arrangement for poling x or y cut ferroelectric crystals is shown in Figure 15. A standard wafer scale photolithographic process is used to pattern a large number of thin film first conductive electrodes 180 (e.g. Al) on the x (or y) cut face of the ferroelectric crystal. In the case of the substrate crystal 200 being LiNb0 3 , the crenulated edge 186 of each the first conductive electrode should face towards the -z surface 188 of the crystal so that domains 12 can nucleate on the patterned first electrode and grow along the -z direction. After patterning the first electrodes, a photoresist layer is spun onto the wafer surface and hard baked to provide a liftoff mask for the second electrode 202 deposition step. A dicing saw is used to cut shallow (about 50μm deep) trenches 204 between the first conductive electrodes. An electrically conductive film 202 (e.g. Al) is deposited into the trenches, using for example sputtering, to create a second electrode on the -z cut face of the trench. The photoresist film is UBSTITUTESHEET(RULE26) removed with commercial resist stripper (or acetone) . Electrical connection to the first conductive electrodes on the x (or y) face may be made by wire bonding. Contact to the second electrodes on the z-cut faces of the trenches can be made using physical contact (or a solder bond) . Application of a continuous or pulsed electric field greater than the coercive field of the crystal (about 20kV/mm) and opposing the crystal spontaneous polarization (the negative pulse is applied to the -z face of the region being poled) across the first conductive electrode and the second conductive electrode causes poling of the crystal. As the second electrode on the -z face of the trench extends below the level of the x (or y) cut face, the electric field dips deep into the crystal and forms deep domains. The patterned first electrode on the x (or y) cut face spatially modulates the applied electric field to create periodic domain inversion. A substantially parallel array of electrodes may be fabricated on a substrate. Poling can achieved in a single step if the trench electrodes are all interconnected, for example along one end of the trench electrodes to the side of the desired pattern, and if all of the crenulated electrodes are interconnected, for example along the other end, forming an interdigitated pattern. The desired effective potential can then be applied to all electrode pairs at the same time if electrical contact is made for example to the end connections. After removal of the primary electrode on the x (or y) cut face, a waveguide 192 is fabricated in the domain inverted region of the crystal using standard photolithographic techniques. Ideally the annealed proton exchange process would be used for a LiNb0 3 substrate. The waveguide should be fabricated in a region between the two electrode locations where the poling has penetrated substantially into the polable material. After waveguide fabrication the wafer is diced and end polished to produce individual device chips, each with a multiplicity of periodically poled TE polarized waveguides. In the case of polable materials other than LiNb0 3 being used as the substrate material, e.g. LiTa0 3 , KTP, KNb0 3 , BaTi0 3 , SBN, Ag 3 AsS 3 , fused silica or organic polymers, the orientation of the patterned first electrode and the second electrode is determined by the material surface at which domain nucleation occurs. The patterned first electrode must be positioned at the nucleation surface of the volume to be poled. This invention enables fabrication of patterned poled LiNb0 3 at low cost, in bulk form, and in novel configurations. The applications which the invention makes possible include high density optical storage, information display, fluorescence detection, and printing. Several unique laser systems use this material. The invention has now been explained with reference to specific embodiments. Other embodiments will be apparent to those of ordinary skill in the art. Therefore, it is not intended that the invention be limited, except as indicated by the appended claims, which form a part of this invention description.

Claims: WHAT IS CLAIMED IS: 1. A method for fabricating a patterned poled dielectric structure comprising: placing a first electrically-conductive material adjacent a first surface of a polable dielectric material; placing adjacent a second surface of said polable dielectric material a means for controlling, according to a selected amplitude modulation parameter, electric field strength in selected regions within said polable dielectric material; and applying an effective potential between said first electrically-conductive material and said controlling means above a domain-orienting potential threshold to produce selective orientation of domains in a pattern in said polable dielectric material to produce said patterned poled dielectric structure. 2. The method according to claim 1 wherein said electric-field strength controlling means comprises second electrically-conductive material having protrusions in a configuration of modulated height confronting said second surface, said second surface opposing said first surface. 3. The method according to claim 1 wherein said electric-field strength controlling means comprises a second electrically conductive material and a dielectric material, said dielectric material having a modulated dielectric constant in two dimensions confronting said second surface and between said second surface and said second electrically- conductive material, said second surface opposing said first surface. 4. The method according to claim 2 further including applying a dielectric film of selective thickness according to a configuration between said second surface and said controlling means. 5. The method according to claim 1 wherein said placing of said controlling means comprises deposition of a second electrically-conductive material upon said dielectric film. 6. The method according to claim 4 wherein said controlling means is an electrically-conductive liquid. 7. The method according to claim 2 wherein said protrusions of said second electrically-conductive material have corners bounding said selected regions. 8. A method for fabricating a poled dielectric structure comprising: creating a uniform potential adjacent a first surface of a polable dielectric material; and applying an electric field adjacent a second surface of said polable dielectric material, said electric field being spatially-modulated according to a three-dimensional modulation pattern with a field amplitude level at selected locations sufficient to cause atomic rearrangement within predefined regions, modulation amplitude level of said modulation patterned being controlled according to a modulation parameter. 9. The method according to claim 8 wherein said modulation pattern comprises an electrically-conductive material having protrusions in a configuration of modulated height confronting said second surface, said second surface opposing said first surface. 10. The method according to claim 9 further including applying a dielectric film of selective thickness according to said configuration between said second surface and said electrically-conductive material. 11. The method according to claim 10 wherein said electrically-conductive material comprises a deposition upon said dielectric film. 12. The method according to claim 9 wherein said electrically-conductive material is an electrically-conductive liquid. 13. A patterned poled dielectric structure comprising: a polable dielectric material having a first surface and a second surface; a first electrically-conductive material adjacent said first surface; a means for controlling, according to a selected amplitude modulation parameter, electric field strength in selected regions within said polable dielectric material. 14. The structure according to claim 13 wherein said electric-field strength controlling means comprises second electrically-conductive material having protrusions in a configuration of modulated height confronting said second surface, said second surface opposing said first surface. 15. The structure according to claim 13 wherein said electric-field strength controlling means comprises a second electrically conductive material and a dielectric material, said dielectric material having a modulated dielectric constant in two dimensions confronting said second surface and between said second surface and said second electrically-conductive material, said second surface opposing said first surface. 16. The structure according to claim 14 further including a dielectric film of selective thickness according to a configuration between said second surface and said controlling means. 17. The structure according to claim 14 wherein said protrusions of said second electrically-conductive material have corners bounding said selected regions. 18. A configuration of field-controlling electrically-conductive structure for use in establishing a poling pattern for fabricating a patterned poled dielectric device, said structure comprising: a plurality of segments of said field-controlling electrically-conductive material aligned to comprise at least one sector of pole control across a surface of a polable dielectric material, each one of said segments including at least one region adapted to support concentration of electric fields to promote nucleation of poling. 19. The configuration according to claim 18 wherein said at least one concentration region of said field- controlling electrically-conductive material comprises a corner having an inside angle of less than 180°. 20. The configuration according to claim 18 wherein said sectors define a periodic pattern along an axis. 21. The configuration according to claim 18 further including conductive means for interconnecting electrically- conductive segments to a source of electric potential. 22. A method for fabricating a patterned poled structure comprising: stressing a polable piezo-electric material in a first pattern to induce an electric field pattern in said polable piezo-electric material while applying an effective poling force in a second pattern, aligned relative to said electric field pattern, to said polable piezo-electric material above a domain-orienting threshold to produce a patterned poled dielectric structure. 23. A method for fabricating a TE-mode-polarized optical waveguide in a bulk poled dielectric structure comprising: slicing a bulk-poled wafer material with a cut to expose an edge, such that a poling axis of said bulk poled dielectric structure lies approximately in the plane of said cut; and in-diffusing ions into said edge along a track to increase optical index of refraction along said track for TE- mode components of an optical signal along said edge. 24. A TE-mode-polarized optical waveguide in a bulk poled dielectric structure comprising: a sliced bulk-poled wafer material having an edge with a poling axis of said bulk poled dielectric structure lying approximately in the plane of said cut; and a track of in-diffused ions in said edge to increase optical index of refraction along said track for TE-mode components of an optical signal along said edge. 25. The waveguide according to claim 24 wherein said bulk poling is in a pattern which is traversed by said track. 26. A patterned poled dielectric structure formed by applying a potential between a first electrode and a second electrode comprising: a polable wafer material; a first electrode; and a second electrode, said second electrode being along a first substantially planar surface of said wafer material, said second electrode having a crenulated edge opposing said first electrode; wherein said first electrode is disposed on a second substantially planar surface of said wafer material transverse to said first surface such that an effective electric potential applied between said first electrode and said second electrode produces an electric field distribution which substantially penetrates said polable wafer material to induce domain orientation in selected regions of said polable material. 27. The structure according to claim 26 wherein said second planar surface is an edge of said wafer material. 28. The method substantially as shown and described. 29. The structure substantially as shown and described.

Inventors: DEACON DAVID A G, FIELD SIMON J, DEACON, DAVID, A., G., FIELD, SIMON, J.
Applicants: DEACON RESEARCH
Application year: 1995
Main classification: G02F1
IPC codes: G02B6, G02F1