AN ELECTRO-OPTICAL DEVICE AND METHOD

Abstract: A method and an electro-optical device are presented for affecting one or more conditions of an input light beam impinging on the device. The electro-optical device is composed of at least one domain-patterned ferroelectric crystal structure with inverted domains, and an electrodes' arrangement on the surface of the at least one structure connected to a voltage source. The electrodes' arrangement is composed of at least one electrode set defining at least one channel of light propagation through the structure. Controlling voltage supply to the electrodes allows for at least one of the following: affecting at least one of intensity and phase profiles of the input beam in a wavelength dependent manner, affecting a direction of propagation of at least one wavelength component of the input light beam; and providing attenuation for different polarization components of the input light beam.

Description: An Electro-Optical Device and Method FIELD OF THE INVENTION This invention relates to an electro-optical device based on a domain-patterned structure. The device is particularly useful in optical communications for filtering, switching, modulation, etc. BACKGROUND OF THE INVENTION Filters and other wavelength selective elements are widely used as passive devices relying, for example, on thin-film interference or on fixed diffraction gratings. One kind of active device, such as a tunable or electrically-controllable filter, relies on interference. These include two-beam interferometers (e.g., Michelson, Mach-Zehnder) and multiple-beam interferometers (e.g., Fabry-Perot), where the optical path length can be varied by various mechanisms, e.g., by using thermal, piezoelectric or electro-optic effects. Filters utilizing these interferometers are usually sensitive to environmental perturbations, since variations of a fraction of the wavelength in the optical path length may substantially alter the filter's performance. Other types of tunable or electrically-controllable filters rely on diffraction, e.g., Bragg diffraction. With these types of filter, extremely wide free-spectral range, as well as good spectral resolution, can be attained, and these filters are usually less sensitive to environmental perturbations than interference-based filters. The most widely used filters of this kind are acousto-optic tunable filters, disclosed, for example in the following publication: "Acousto optic tunable filter" , S. E. Harris and R. W. Wallace, Journal of the Optical Society of America 59, 744 (1968). However, acousto-optic tunable filters require continuous injection of an acoustic wave into the material, and therefore consume relatively high electrical power. In addition, they shift the frequency of light, and are inherently slow (typical switching speed exceeding 500 nsec), which makes them impractical for packet switching in high-speed optical communication systems. Some of the above problems can be solved by using an electro-optic tunable filter, where an electro-optic grating is formed by placing inter-digital electrodes on the surface of an electro-optic material. In this case, the electric field has a suitable shape for filtering in the material only in a small region close to the electrodes. This device is mainly used with optical waveguides, but not with freely propagating beams in bulk crystals. Electro-optic modulators in bulk can be used only with a relatively wide period of electrodes, e.g., 300μm, as disclosed in the following publication: "Digital electro-optic grating deflector and modulator", J. M. Hammer, Applied Physics Letters 18, 147-149 (1971). In this case, high spectral resolution cannot be achieved. In the last few years, techniques of patterning the domain structure of ferroelectric crystals such as LiNb0 3 , KTiOP0 and LiTa0 3 have been developed, and disclosed for example in the following publications: "Quasi-phase-matched optical parametric oscillator in bulk periodically poled LΪNbO^ ", L. E. Myers et al., J. Opt. Soc. Am B 2102-2116 (1995), and U.S. Patent Nos. 5,193,023 and 6,074,594. According to these techniques, permanent grating of non-linear susceptibility can be written into the material, for example, by applying once a very high field through patterned electrodes. The grating period can be in the range of several microns. The ferroelectric materials that can be domain-patterned are commercially available in large quantities, and the method of patterning the domains is well established. The reversal of the ferroelectric domains also reverses the sign of the electro-optic coefficient. This is disclosed, for example in the following publication: "Electric-field induced cylindrical lens, switching and deflection devices composed of the inverted domains in LϊNb0 3 crystals ", M. Yamada, M. Saitoh and H. Ooki, Applied Physics Letters 69, 3659-3661 (1996). Applying an external electric field will create a refractive index pattern inside the material, since the same electric field that increases the refractive index in one domain will reduce the refractive index in the inverted domain. Hence, the refractive index pattern depends also on the domain pattern of the ferroelectric crystal, and not only on the external electric field. Electro-optic devices based on domain-patterned ferroelectric crystals were used for deflection, modulation and beam focusing, as disclosed, for example, in US Patent No. 5,786,926. SUMMARY OF THE INVENTION There is a need in the art to facilitate the tuning and controlling of the propagation of an optical signal by providing a novel electro-optical device and method for propagating an input light beam through an optical system utilizing the electro-optical effect in domain-patterned ferroelectric crystals with inverted domains. The technique of the present invention provides for wavelength-dependent filtering, switching, modulation, temporal pulse shaping, controllable dispersion, equalizing, as well as for attenuating different polarization components of the input beam. The device of the present invention provides for a wide free spectral range, high spectral resolution, low power consumption and fast switching speed. Optical filters and other wavelength-selective optical elements according to the invention can be used with freely propagating beams. Electrically-controlled optical filters and other wavelength-selective optical elements are very important for optical communication systems. Dense wavelength division multiplexed (DWDM) optical communication systems require devices that can selectively manipulate different, closely spaced optical channels. One example of such an optical device that is often used in wavelength-routed systems is an add/drop multiplexer (ADM), where data on one or more optical channels are dropped at a certain node, while new data is added onto the same wavelengths. Conventional ADMs are mainly passive devices. It is desired to create an ADM as an active (or re-configurable) device that enables to dynamically change the dropped and added channels, in order to adjust the number of channels to the varying traffic volume in different locations in the system. More advanced systems should be able to switch data packets at predetermined wavelengths, and require a switching time in the nanosecond range. The optical device according to the invention relies on a structure made of a ferroelectric crystal, such as LiNb0 3 , KTiOP0 4 , LiTa0 3 , MgOLiNb0 3 , KTi0AsO 4 , RbTiOAs0 4 , KNb0 3 , with patterned domains, and electrodes on the surface of the structure. In these domain-patterned crystals and in contrary to the standard mono-domain crystals, the refractive index pattern in the material is determined not only by the electrodes on the surface, but by the domain pattern as well. For a given domain pattern in the structure, by directing a light component of a predetermined wavelength onto the structure at a certain angle of incidence satisfying the Bragg condition for this predetermined wavelength, and applying voltage to the electrodes, this light component can be appropriately deflected to propagate with a certain direction. This can be used for selecting the light component of the predetermined wavelength from input light containing a plurality of wavelengths including this predetermined wavelength. There is thus provided according to one aspect of the present invention, a method of propagating an input light beam in an optical system to provide desired output of the system, the method comprising the steps of: (a)passing the input light beam, propagating in an input direction, through an electro-optical device composed of at least one domain-patterned ferroelectric crystal structure with inverted domains formed with an electrodes' arrangement on the structure's surface, said electrodes' arrangement comprising at least one electrode set defining at least one controllable channel of propagation of the input beam inside the structure; and (b) controlling voltage supply to the electrodes, thereby causing at least one of the following: (bι) affecting at least one of intensity and phase profiles of the input beam in a wavelength dependent manner, (b 2 ) affecting a direction of propagation of at least one wavelength component of the input light beam; and (b 3 ) providing attenuation for different polarization components of the input light beam. Preferably, the method also comprises affecting a shape of the input beam so as to provide a substantially elliptical shape of the beam impinging onto the electro-optical device. The method may also comprise the step of providing a predetermined orientation between the input beam and said electro-optical device, to thereby provide a predetermined angle of incidence of the input beam onto the electro-optical device. The angle of incidence preferably satisfies the Bragg condition. The affecting of the intensities of wavelength components results in equalizing the intensity profile of the input beam. The affecting of the phase of wavelength components of the input light beam enables for dispersion compensation to thereby reconstruct the profile of the input light beam. By changing the direction of propagation of a selected wavelength component of the input beam and allowing propagation of the other wavelength components of the input beam in the input direction, a drop filtering can be achieved. By appropriately changing the direction of propagation of the input beam from the input direction, the input beam can be added to another beam propagating through the structure. By using two such structures and appropriately controlling the voltage supply thereto, an add/drop filter can be achieved. By passing a light beam, resulting from the passage of the input beam through the channel inside the structure defined by the electrode set, through an additional channel inside the structure defined by an additional electrode set, multi-stage filtering or attenuating of the input light beam can be achieved. To provide attenuation for different polarization components, the input beam is split into two different linear polarization components. One of these components undergoes a 90-degree rotation, and the so-obtained two light components pass through the structure. Then, one of the light components emerging from the structure undergoes 90-degree polarization rotation, and the resulting two light components of different polarizations are combined into a combined output beam. The attenuation may be carried out in a polarization dependent manner, in which case the two split light components of the same polarization pass through the structure along two spaced-apart channels defined by two spaced-apart electrode sets. Alternatively, the attenuation may be carried out in a polarization independent manner. To this end, a common beam polarizing element is used for splitting the input beam and combining the output light components, and the split light components of the same polarization pass through the structure in opposite directions. According to another aspect of the present invention, there is provided an electro-optical device for carrying out the above method. By using the device according to the invention in an optical communication system, for example of the kind utilizing an optical amplifier with wavelength dependent gain, equalizing of the amplified power as a function of wavelength can be achieved. The device can be used for voltage controlled pulse shaping. In particular, this can be used to correct the dispersion accumulated in an optical or fiber-optic communication system, and can handle changing levels of dispersion by the appropriate selection of a patterned domain structure and applied voltage through the electrodes. The device can be used for wavelength dependent packet-switching in optical communication systems. By providing polarization beam splitters and retarders in the input port and at the output of the device, the wavelength-dependent transmission and dispersion can be separately controlled for different polarizations of light. For example, the device can be used to correct polarization dependent loss and polarization mode dispersion in optical systems. BRIEF DESCRIPTION OF THE DRAWINGS In order to understand the invention and to see how it may be carried out in practice, a preferred embodiment will now be described, by way of non-limiting example only, with reference to the accompanying drawings, in which: Fig. 1A is a schematic illustration of an electro-optical device according to the invention; Figs. IB and 1C show typical transmission coefficient of the device of Fig. 1 A as a function of wavelength for, respectively, transmitted and Bragg-reflected output beams; Fig. 2 more specifically illustrates how the device of Fig. 1A can be used as an electrically-controlled wavelength selector; Fig. 3 schematically illustrates an add/drop switch utilizing the device of Fig. 1A; Figs. 4A to 4C illustrate the measurement results in the form of diffraction and transmission efficiency of the electro-optical device of the invention as a function of, respectively, wavelength, applied voltage and angle of incidence of the input beam; Fig. 4D illustrate experimental results in the form of three graphs, two of them showing the power as function of wavelength for the cases when, respectively, no voltage is applied to the crystal, and a 1000V voltage is supplied to the crystal; and the other graph presenting the ratio between the two functions; Fig. 5 schematically illustrates how the electro-optical device according to the present invention can be used in an optical communication system for producing voltage-controlled dispersion and pulse shaping; Figs. 6 and 7 illustrate the intensity and dispersion response of a filter using the electro-optical device of the present invention; Fig. 8 illustrates how the device according to the present invention can be used for separate control of the wavelength-dependent transmission and dispersion for different polarizations of light; Fig. 9 schematically illustrates a polarization insensitive scheme utilizing the electro-optical device of the present invention; Fig. 10 schematically illustrates how the device according to the invention can be used for correcting the wavelength-dependent distortions introduced by elements in an optical communication system; Figs. 11 and 12 illustrate how the electro-optical device of the present invention can be used as a dynamic gain equalizer; and. Figs. 13 and 14 illustrate two examples, respectively, of increasing the number of filtering processes in an optical communication system (e.g., equalizer) within a single domain-patterned device of the present invention. DETAILED DESCRIPTION OF THE INVENTION Referring to Fig. 1A, there is illustrated an electro-optical device 10 according to the invention. The device comprises a domain-patterned ferroelectric crystal structure 12 with an electrodes' arrangement 14 on the surface of the structure 12. It should be understood that the electrodes' arrangement is composed of at least one electrode set, comprising at least one pair of electrodes located at opposite sides of the structure (only one such electrode being shown in the figure). The electrodes' arrangement 14 is connectable to a voltage source 16, which is connectable to a control unit 19. An input light beam 18a is directed onto the structure 12 through an input port IP and passes through an optical beam-shaping unit.17, the purpose of which will be described further below. It should be noted that, although the beam-shaping unit 17 is exemplified here as a separate unit, it could be a constructional part of the input port D?. In the present example, the domains are shown as periodically inverted. It should, however, be noted that the periodicity of the inverted domains is not necessarily for the purposes of the present invention, and periodic gratings may be used as well. As shown by periodically/alternating inverted arrows, the reversal of the ferroelectric domains reverses the sign of the electro-optical coefficient. The input light beam 18a is directed onto the crystal structure 12 at an angle satisfying the Bragg condition (at first or higher order): . , n . mλ sm( ?κ ) = — - (1) 2nΛ wherein Θ B is the angle of incidence, λ is the wavelength of the light beam, n is the refractive index of the structure 12, m is the diffraction order number and Λ is the domain-patterned structure period. When no voltage is applied to the electrodes 14, all the power 18b propagates towards a transmission output port (not shown). Applying voltage through the electrodes 14 can switch a certain wavelength range from this direction to a reflection output direction 18c. Light at wavelengths that are far enough from the Bragg wavelength will not be switched, regardless of the applied voltage. A light component of a wavelength λ B contained in the input beam 18a and entering the device 10 at an angle of incidence (+θ B , m ) will be diffracted at an angle (-θ B,π ι) 5 provided the Bragg condition (1) is satisfied. Referring to Figs. IB and 1C, there are shown two graphs Pi and P 2 illustrating the typical transmission coefficient as a function of wavelength for, respectively, the transmitted and Bragg-reflected output beams 18b and 18c. The device 10 can operate as a wavelength selective optical switch or controllable filter. The process of controlling the filter transmission can be based on one or more of the following parameters: structure of the domains (geometry of the grating), the shape of the electrodes, the applied voltage, the beam shape and the beam angle of incidence. To use the device 10 as a wavelength selective switch, various angles of incidence of at least one input beam enable switching into output beams with different angles of propagation, where the switching depends on the wavelength range of the input beam(s). The application of a homogenous external electric field through the plane electrodes 14 to the periodically-poled crystal structure 12 (with a period Λ) creates a grating with the strength proportional to the strength of the electric field. The grating thickness is the entire thickness of the crystal, and therefore the beams do not have to be confined to a small region near the surface, thereby enabling the use of freely propagating beams. This is fundamentally different than applying voltage through periodic electrodes on a mono-domain crystal where the beams must be confined to a small region near the surface. This also allows using short gratings, and the state of the art for the period Λ, which is currently below lOμm. Short grating periods enable to obtain high spectral resolution. Light at sufficiently different wavelengths will not satisfy the Bragg condition, and therefore will not be affected by the external field. This feature is particularly attractive to DWDM optical communication systems, since it allows switching in or out a single channel, without altering all the other channels. The amount of light that is Bragg diffracted at every wavelength is controlled by an electric field, and the rise time is in the nanosecond regime. The criterion for being far "enough" from the Bragg condition (known also as the "spectral resolution") is known from literature ("Coupled wave theory for thick hologram grating", H. Kogelnik, Bell System Technical Journal 48, 2909-2947 (1969)), and is given by: λ -A Aλ - (2) L • m • taa(0 B ) Assuming λ=1.55μm, Λ=6.5μm, L=25mm (crystal length) and m=3, the wavelength bandwidth becomes equal to 0.8nm, which is the channel spacing in DWDM systems. Narrower resolution of 0.4nm can also be achieved by using a longer (e.g., L=50mm) crystal. Turning back to Fig. 1 A, the beam-shaping unit 17 comprises suitable optics (e.g., cylindrical optics) to provide an elliptically-shaped beam propagating to the structure. By this, the spectral resolution of the optical device can be improved. This is associated with the following: The domain patterning process currently requires ferroelectric crystals with a thickness in the range of 0.5-lmm. There is also motivation to use a relatively thin crystal in order to lower the voltage requirements of the electrodes, since the electro-optic effect is proportional to the electric field, given by V/d, where Fis the voltage applied to the electrode and d is the crystal thickness. Usually, a beam with a circular cross section is used, but in this case, the spectral resolution of the device is reduced as well. For example, assuming d=0.5mm, a reasonable choice for a Gaussian beam radius size ω 0 that will have low clipping is as follows: d ω 0 = — ∞ l70μm (3) In this case, a diffraction angle is determined as: λ v diffraction = πcOr, Assuming for example that the wavelength λ is 1.55μm, the diffraction angle becomes equal to 2.9 milli Radian. Assuming a periodically patterned nonlinear crystal with a period Λ, the angular acceptance bandwidth is related to the spectral resolution through the ratio: θ Bragg Aλ (5) θ Bragg λ However, if the angular acceptance bandwidth becomes smaller than the diffraction angle, the spectral resolution of the device is limited by the angular spread of the beam. For example, using the values given above of Λ^δ.Sμm and m=3 in the periodically-poled LiNb0 3 , the spectral resolution near 1.55μm with a circular beam is 26.8nm instead of 0.8nm (33 times wider). This problem can be solved by using a beam of elliptical cross section, where the size of the beam in the orthogonal direction (X-direction) is no longer limited by the thickness of the device. To achieve the spectral resolution of 0.8nm, the radius of the beam should be larger than 5.7mm in the X-direction, but can remain 0.17mm in the Z-direction. It should be noted that even if thicker domain-patterned structures can be realized, it is still advantageous to use thin devices and elliptic beams in order to reduce the voltage requirements. Reference is made to Fig. 2 illustrating in more detail how the device 10 can be used as an electrically-controlled wavelength selector. As shown, an input light beam 21 propagating through an input fiber contains a plurality of light components of different wavelengths λ ls λ 2 , ..., λ n .ι, λ n , λ n+1 . When voltage is applied through the electrodes, either all input light or a part thereof is switched to a "drop" port 23 to enter a "drop" channel fiber, provided the wavelength of this light satisfies the Bragg condition (1), otherwise it comes out through a main output port 22 to enter an output fiber. When no voltage is applied, all the light comes out through the main output port. In a similar manner, although not specifically shown, an add-switch can be realized, where wavelength selective switching is performed on the input beam to change the direction of propagation of the input beam inside the device to propagate along a path of propagation of another light beam, to which the input beam is added. It should be understood that the time dependent voltage pattern can be used in the device 10. In this case, when modulating voltage is applied to the electrodes, only a wavelength or plurality of wavelengths satisfying a certain condition are modulated. The applied voltage does not affect light signals at other wavelengths. The device of Fig. 1A can also be used in an add/drop switching system. This is schematically illustrated in Fig. 3 showing a part of a communication system 60 utilizing two domain-patterned structures 10A and 10B, each constructed as the above-described device 10. An input beam 18a containing several light components of different wavelengths is supplied from an input fiber 61 so as to appropriately impinge onto the structure 10A, wherein a selected light component (wavelength) 18c is deflected towards an output fiber 62, while the other light components 18b propagate towards the structure 10B, which allows the propagation of the beam 18b to an output fiber 64. A light component 18d supplied from an input fiber 63 enters the structure 10B and is deflected thereinside so as to propagate along the optical path of the light component 18b. As shown, focusing optics (lenses) L are appropriately provided to ensure the desired light propagation in and out of the fibers. It should be understood that the geometry of gratings in the structures 10A and 10B, their orientation with respect to the input beams and applied voltages are appropriately selected to ensure add and drop functions of the system from and to the respective fibers. The specific filtered wavelength can be controlled by rotating the crystal 12 to change the angle of incidence or by changing the temperature of the device. Another option is to put several different gratings on the same chip with different electrodes and select the required channel by applying an electric field to the appropriate electrode. Switches, attenuators and modulators based on the concept of the present invention can be very fast. It is known that a pulse rise time of 1.2 nanoseconds can be achieved in an electro-optical Bragg deflector ("Nanosecond response of Bragg deflectors in periodically poled LiNb0 3 " H. Gnewuch et al., IEEE Photonics Technology Letters 10, 1730-1732 (1998)). It is important to note that in the device according to the present invention, since it is based on an electrostatic effect, the power consumption is minimal. For the experiment purposes, the inventors have constructed and tested a 12-mm long, 0.5-mm thick, periodically-poled LiNb0 3 -based device 10 with a poling period of 29.6μm. Wavelength and angle bandwidths have been measured up to the 5 th diffraction order, and a wavelength bandwidth of 15nm was obtained, in good agreement with theoretical modeling. Figs. 4A-4C illustrate the measurement results in the form of diffraction and transmission efficiency as a function of, respectively, wavelength, applied voltage and angle of incidence of the input beam. More specifically, in Fig. 4A, the diffraction and transmission efficiency as a function of wavelength is shown for the 3 rd order of diffraction. Here, graphs 31 and 32 correspond to the wavelength dependence of the transmitted and diffracted beams, respectively. In Fig.4B, graphs 41 and 42 correspond to the voltage dependency of the zero-order transmitted beam and 3 rd order diffracted beam, respectively. In Fig. 4C, three graphs 51, 52 and 53 are shown corresponding, respectively, to the angular dependence of the switch for three different angles of incidence of the input beam: θι=12.06 milli radian; θι=12.14 milli radian; and θι=12.29 milli radian. In these experiments, the device was also switched with an electric sine-wave at 7MHz (rise time of 50 nanoseconds). It should be noted that all the graphs in Figs. 4A-4C were normalized to 1, i.e., the results of the points of each graph were multiplied by a factor such that the peak of each graph was 1. To improve the spectral resolution of the device, the present invention enables to use high order diffraction grating. In the previous experiments utilizing the Bragg effect, as disclosed in the above-indicated publications, only the first diffraction order was employed. However, for high spectral resolution, it is better to use higher orders of diffraction. The spectral resolution of the device is proportional to 1/m 2 , where m is the diffraction order. This requires entering at an appropriate incidence angle θ B , m as described above. It was found by the inventors that diffraction efficiency of more than 90% can be reached for example at third order, and at the same time, the spectral resolution is improved by a factor of 9 with respect to the first order diffraction efficiency. Turning now to Fig. 4D, there are illustrated experimental results of using a 10 micron grating PPLN crystal having a 10 mm length and a 0.5 mm thick, operated at the third order of diffraction for wavelengths filtering. A broad-band light source was used to generate an input beam impinging onto the crystal at an angle which satisfies the 3 rd order Bragg diffraction condition for a wavelength of 1543 nm. Three graphs are shown, Ri, R 2 and R 3 , wherein graphs Ri and R 2 present the power as functions of wavelength for the cases when, respectively, no voltage is applied to the crystal, and a 1000V voltage supply to the crystal is provided. Graph R 3 presents the attenutation, i. e., the ratio between the two functions Ri and R 2 . As can be seen in the figure, the attenuation of the central wavelength of the filter is (-30) dB, i.e., 0.1% of the input light remains, so the efficiency in this case is 99.9%. The device 10 can be used for producing voltage-controlled dispersion and pulse shaping, for example aimed at correcting the dispersion accumulated in an optical or fiber-optic communication system, and can handle changing levels of dispersion by the appropriate selection of the patterned domain structure and applied voltage through electrodes. This is illustrated in Fig. 5, showing a part of an optical communication system 70 composed of a transmission unit 71 and the device 10 accommodated in the optical path of a transmitted signal TS. As shown, the transmitted signal TS, when reaching the device 10, is typically broadened owing to dispersion. By applying an appropriate voltage to the electrodes (via transmission of control signals 72 to the device 10), the shape of the transmitted signal is reconstructed to produce an output signal OS. As known, the filter transfer function of the electric field H(ω) is in general a complex function of the angular velocity ω of the signal, the phase response of the transfer function being given by the arctan of the ratio between the imaginary and real part of the function H(ω) : φ(ω) = arctan (Im (H(ω)) / (Re(H(ω))) (6) The group delay τ(ω) and the dispersion D(λ) are given by: dφ(ώ) τ(ω) = — dω (7) -£ Without the application of external voltage, the dispersion of the device 10 is that of the bulk material (crystal structure 12). Denoting the device length by L and the refraction index by n, the phase response is: ωnL/c. For example, for a 1cm long LiNb0 3 crystal structure, at a wavelength of 1550nm, the dispersion is -0.08ps/nm. This is calculated using the known Sellmeir equation ( "A temperature-dependent dispersion equation for congruently grown LϊNbOX, Optical & Quantum Electronics, Vol. 16, p. 373). Assuming that the crystal is periodically-poled so that the Bragg diffracted light is reflected with an angle of 180° with respect to the input light when an electric filed is applied to the device, the domain structure should have a period of λ/2nΛ « 0.362μm. In this case, the reflection coefficient and, in particular, its phase response can be calculated analytically (e.g., as disclosed in "Optical Waves in Layered Media ", P. Yeh, New York, Wiley, 1988). The delay and dispersion can then be calculated from the derivatives of the phase response, as shown above. Turning now to Figs. 6 and 7, there are illustrated the calculated intensity reflection profile of a domain-patterned LiNb0 3 (Fig. 6) and the calculated dispersion profile of this structure (Fig. 7) for Δn of 5xl0 "5 , both as a function of the wavelength λ. As shown, the dispersion can reach 880ps/nm, which is 4 orders of magnitude higher than the dispersion without the electric field. Hence, the group delay and the dispersion can be varied by applying an electric field to a domain-patterned crystal. This can be used to control the temporal shape of light pulses in general, and in particular, to dynamically compensate the dispersion accumulated in optical communication systems. It should be understood, although not specifically shown, that since the device according to the invention provides for a switching time in the nanosecond range, the device can be used for wavelength dependent packet-switching in optical communication systems. To this end, an electronic device of the kind capable of reading the header of a data packet is used to enable the selection of appropriate voltage to be applied to the electrodes so as to either switch the data packet or let it pass unaltered. Referring to Fig. 8, there is illustrated how the device according to the present invention can be used for separate control of the wavelength-dependent transmission and dispersion for different polarizations of light. A device 100 is of the kind providing two channels for light propagation 100a and 100b, each channel being constructed as in the above-described device 10. This can be implemented by fabricating two domain-patterned ferroelectric crystal structures (12 in Fig. 1) arranged in a spaced-apart parallel relationship in a common crystal, and providing electrodes' arrangements 114a and 114b on the surfaces of the two structures. Input and output ports are provided with light directing means, generally at 34, composed of polarizing beam splitters 36a and 36b and retarders 38a and 38b accommodated upstream and downstream of the device 100. The device 100 operates in the following manner. An input arbitrary polarized beam IS passes through the polarizing beam splitter 36a, which reflects one light component of one polarization towards the channel 100a, and transmits the other light component of the other polarization towards a half-waveplate 38a. The light component emerging from the half-waveplate 38a is reflected by a mirror 40a towards the channel 100b. The output beam OSi ensuing from the channel 100a is reflected by a mirror 40b to pass through a half-waveplate 38b and a polarizing beam splitter 36b, and the output beam OS 2 ensuing from the channel 100b passes through the beam splitter 36b. The two polarization components propagate along the independent channels 114a and 114b of the device 100 and thus can be independently enhanced or weakened according to the user' needs. This can, for example, be used to provide the polarization independent operation of an optical system, correct polarization dependent loss and compensate polarization mode dispersion in optical systems. Turning now to Fig. 9, there is illustrated a polarization insensitive scheme 200 utilizing the device 10 (periodically poled lithium niobate (PPLN) in the present example) constructed as described above, and an optical circulator 202. An input light beam 204a supplied from an input channel IN enters the circulator 202 and emerges therefrom at an output channel O . Here, the light beam 204a impinges onto a polarizing beam splitter 206, which splits the beam into different linear polarization components 204b and 204c. One polarization component 204b passes through a half-wave plate 208 and is thereby rotated by 90 degrees, resulting in an output beam 204b' of the same polarization as that of the beam 204c. Two output beams 204b' and 204c counter-propagate through the crystal, and are recombined at the polarizing surface of the beam splitter 206 into an output beam 204d, which propagates along the channel OCi to enter the circulator and emerge therefrom at an output channel OUT. The following table presents experimental results of a measurement of the residual polarization dependent loss (PDL) in the above scheme 200. In this experiment, the PPLN crystal of a lOmμ period and a 10mm length was used. A single mode laser was tuned to the center of the filter absorption wavelength. The attenuation was achieved by applying different voltages to the electrode that activated the filter 10. The PDL was measured by altering the input state of polarization using a fiber polarization controller and measuring the difference between the highest and lower transmission levels. As can be seen from the data in the above table, the residual PDL is fairly small. Additionally, the device according to the invention can be used for correcting the wavelength-dependent distortions introduced by elements in optical communication systems. Many elements in the optical link, including Erbium doped fiber amplifiers (EDFAs), optical cross-connects, etc. have a non-uniform spectral response. While passive filters are currently used to correct the response, as optical systems become more complex, active equalization will be required, and it can be performed using the technique of the present invention. For example, by accommodating the device 10 upstream or downstream of an optical amplifier with wavelength dependent gain, or between two such amplifiers, the device can equalize the amplified power as a function of wavelength. This is illustrated in Fig. 10 showing a part of an optical communication system 300 composed of n transmitter units Ii, I 2 ,..., I n with different center wavelengths, a multiplexer 42, an optical amplifier with wavelength selective gain 44, the electro-optical device 10 constructed as described above, a demultiplexer 46, and n receiver units R ls R 2 ,..., R n . In the present example, the electro-optical device 10 operates as an electrically-controlled equalizing filter. As shown, the passage of a light signal through the optical amplifier 44 results in different intensities of light components of different wavelengths. By appropriately operating the device 10 (supplying control signals to its electrodes), the device equalizes the intensity of light components of different wavelengths, resulting in an output light signal of substantially equalized intensity profile propagating towards the demultiplexer 46. The distortions that the equalizer corrects may include distortions by an Erbium-doped fiber amplifier, by a Raman amplifier, by the wavelength-dependent loss of a transmission medium such as an optical fiber, by the wavelength dependent transmission of optical elements such as add/drop filters, etc. The equalizer may be operated before an amplifier, after an amplifier, in a mid-stage between two amplifiers or as a stand-alone device (having no amplifier). Dynamic equalization of the power between different channels is performed by applying voltages to several different gratings (thus having different spectral responses) Fig. 11 illustrates the use of the device 10 of the present invention in a dynamic gain equalizing application. As shown, an input signal IS containing light components of different wavelengths and different intensities has an intensity profile 50. The input signal IS passes through the device 10, which is operated by control signals 52 to apply an intensity compensating profile 54 to the signal IS. As a result, an output signal OS emerging from the device 10 has an equalized intensity profile 56. Fig. 12 shows the transmission as a function of wavelength (curve C) required for the gain equalization filter of an EDFA, as presented in the following article: IEEE Photonics Technology Papers 11, 536 (1999). A few points, generally at Ci, were taken from this graph to represent the required transmission. To create the appropriate transmission function, three gratings on a single periodically poled LiNb0 3 crystal were simulated, having the following parameters: Λi « 10 μm di » 5 mm Λ 2 « 10.1 μm d 2 « 6 mm Λ 3 « 10.15 μmd 3 « 6 mm The angle of light propagation in the material is chosen to be ~0.1047rad * 6°, the ratio between the voltages applied to the three gratings is 1:0.515:0.546, and the voltage of the first device is set to provide an attenuation of 5.4dB at a wavelength of 1532nm. The simulation results have shown that the filters according to the present invention can be used to generate the transmission function of Fig. 12. The remaining differences between the desired transmission and the one obtained with the three gratings are of the order of about 0.5dB. Reference is now made to Figs. 13 and 14 illustrating two examples of increasing the number of filtering processes in an equalizer within a single domain-patterned device (wafer). This technique also provides for obtaining wavelength-dependent multiple add/drop filtering. In a system 400 shown in Fig. 13, an input light signal 402 sequentially passes through two sets of filters arranged in different areas of a crystal. As shown, the input signal is supplied from an input fiber 403a associated with a collimator 404a and a cylindrical lens 405a, and impinges onto a domain-patterned structure (crystal) 410 so as to pass thereinside along a first area 410a defined by an array of electrodes 406a (i.e., a first set of filters). The beam emerging from the crystal area 410a is reflected by a mirror 408a towards a mirror 408b through a cylindrical lens 409. The mirror 408b reflects the beam into the crystal 410 to provide the beam propagation along a second crystal area 410b defined by an array of electrodes 406b (i.e., a second set of filters). In other words, the mirror 408a provides a lateral translation of the beam emerging from the crystal area 410a, and the mirror 408b provides a further lateral translation of the beam. The beam emerging from the crystal area 410b is collected by a cylindrical lens 405b to thereby propagate into an output fiber 403b through a collimator 404b. It should be understood, and shown in Fig. 13 in dashed lines that at each filtering stage, a predetermined wavelength component can be dropped to a respective drop channel. As shown in Fig. 14, in a system 500 the number of filters in the optical path of an input beam 502 can be even more increased by directing the beam to sequentially propagate through three sets of filters defined by three arrays of electrodes 506a, 506b and 506c, respectively. This process may be repeated several times. There is a substantial benefit in cost (with respect to using two different crystals for this task), since the processing steps (writing the domains on the material, cutting, polishing and coating the crystal) are done only once. The present invention provides for efficient use of the round shape of a wafer to accommodate a desired number of filters within the wafer. This is easy to implement by writing the desired number of filters in a common photolithography process. Those skilled in the art will readily appreciate that various modifications and changes can be applied to the embodiments of the invention as hereinbefore exemplified without departing from its scope defined in and by the appended claims.

Claims: CLAIMS: 1. A method of propagating an input light beam through an optical system so as to provide desired output of the system, the method comprising the steps of: (a) passing the input light beam, propagating in an input direction, through an electro-optical device composed of at least one domain-patterned ferroelectric crystal structure with inverted domains formed with an electrodes' arrangement on the structure's surface, said electrodes' arrangement comprising at least one electrode set defining at least one controllable channel of propagation of the input beam inside the structure; and (b) controlling voltage supply to the electrodes, thereby causing at least one of the following: (bi) affecting at least one of intensity and phase profiles of the input beam in a wavelength dependent manner, (b 2 ) affecting a direction of propagation of at least one wavelength component of the input light beam; and (b ) providing attenuation for different polarization components of the input light beam. 2. The method according to Claim 1, and also comprising the step of affecting a shape of the input beam so as to provide a substantially elliptical cross-section beam impinging onto the electro-optical device. 3. The method according to Claim 1, and also comprising the step of providing a predetermined orientation between the input beam and said electro-optical device, to thereby provide a predetermined angle of incidence of the input beam onto the electro-optical device. 4. The method according to Claim 3, wherein said input light beam impinges onto said electro-optical device at an angle substantially satisfying the Bragg condition. 5. The method according to Claim l(bι), wherein said affecting comprises attenuating intensities of different wavelength components of the input beam, to thereby equalize (or modify) the spectral intensity profile of the input beam. 6. The method according to Claim l(bι), wherein said affecting comprises 5 changing the phase of different wavelength components of the input light beam, thereby enabling reconstruction of a desired profile of the input light beam. 7. The method according to Claim l(b 2 ), wherein said affecting of the direction of propagation comprises changing the direction of propagation of the input beam from said input direction, to thereby provide the propagation of the l o input beam along a predeteπnined path inside the structure. 8. The method according to Claim 7, providing for adding said input beam to a light beam propagating through the electro-optical device. 9. The method according to Claim l(b 2 ), wherein said affecting of the direction of propagation comprises changing the direction of propagation of a 15 predeteπnined wavelength component of the input beam from said input direction, while allowing the propagation of other wavelength components of the input beam in said input direction through the structure. 10. The method according to Claim 9, providing for dropping said predetermined wavelength component towards a drop channel of the system. 20 11. The method according to Claim l(b 2 ), comprising the steps of sequentially passing the input beam through said structure and an additional domain-patterned ferroelectric crystal structure with inverted domains formed with an electrodes' arrangement on the structure's surface, wherein the passage of the input beam through said structure results in changing the 25 direction of propagation of a predetermined wavelength component of said input beam from said input direction to an output direction towards a drop output channel of the system and allowing propagation of other wavelength components of the input beam in said input direction to enter said additional structure; an additional light beam of a certain wavelength impinges onto said additional structure and the direction of propagation of said additional light beam is affected to direct the additional light beam along the optical path of said other wavelength components of said input light beam, thereby providing propagation of said other light components of the input beam and said additional light beam towards an output add channel of the system. 12. The method according to Claim l(b l5 b 2 ), and also comprising the step of passing a light beam, resulting from the passage of said input beam through the channel inside the structure defined by the electrode set, through an additional channel inside the structure defined by an additional electrode set, thereby enabling multi-stage filtering or attenuating of the input light beam. 13. The method according to Claim l(b 3 ), wherein the attenuation for different polarization components of the input beam comprises the steps of: - splitting the input beam into two different linear polarization components; - applying a 90° polarization rotation to one of the polarization components, thereby providing two spatially separated components of the input beam of the same polarization; - passing said two spatially separated components through the structure, thereby providing two output light components of the input beam emerging from the structure; - applying a 90° polarization rotation to one of the output light components; - combining the two output light components of the different polarizations into a combined output light beam. 14. The method according to Claim 13, providing polarization independent attenuation of the different polarization component of the input beam, said two light components propagating through said structure in opposite directions. 15. The method according to Claim 13, providing polarization dependent attenuation of the different polarization component of the input beam, said two light components propagating through said structure along two spaced-apart channels defined by the two spaced-apart electrode sets, respectively. 16. An electro-optical device for carrying out the method of Claim 1, the device comprising: (i) at least one domain-patterned ferroelectric crystal structure with inverted domains; (ii) an electrodes' arrangement on the surface of said at least one structure connectable to a controllable voltage source to provide selective voltage supply to the electrodes, said electrodes' arrangement comprising at least one electrode set defining at least one channel of light propagation through the structure; (iii) an input unit defining at least one input channel for directing the input light beam onto said at least one structure; and (iv) a control unit for selectively operating at least one of the voltage source and the input unit . 17. The device according to Claim 16, wherein said at least one crystal structure is fabricated from one of the following materials: LiNb0 3 , KTiOP0 4 , and LiTaO s , MgOLiNb0 3 , KTiOAs0 4 , RbTiOAs0 4 , KNb0 3 . 18. The device according to Claim 16, wherein the input unit comprises a light directing assembly to provide a predetermined angle of incidence of the input beam onto the structure. 19. The device according to Claim 16, wherein the input unit comprises a beam shaping assembly to provide a substantially elliptical cross-section of the beam impinging onto the structure. 20. The device according to Claim 16, wherein the input unit comprises a beam polarizing means and a polarization rotating means to thereby split the input beam into two different linear polarization components and apply 90° rotation to one of the split components, thereby enabling attenuation ofdifferent polarization components of the input beam. 21. The device according to Claim 20, wherein - said electrodes' arrangement comprises an additional electrode set, the two electrode sets being arranged in a spaced-apart relationship on the structure's surface, thereby defining two spaced-apart channels inside the structure; - said beam polarizing means comprises an input beam polarizing element accommodated in the optical path of the input beam propagating towards the structure to split the input beam into two different polarization components, and an output polarizing element accommodated in optical paths of two light components emerging from the structure to thereby produce a combined output beam; and - said polarization rotating means comprises an input polarization rotating element accommodated in the optical path of one of the split light components, and an output polarization rotating element accommodated in the optical path of one of the light components emerging from the structure and propagating towards the output beam polarizing element. 22. The device according to Claim 20, wherein - said beam polarizing means comprises a polarizing element accommodated in the optical path of the input beam propagating towards the structure to thereby split the input beam into two different polarization components, and in the optical path of light emerging from the structure to thereby produce a combined output beam; - said polarization rotating means comprises a polarization rotating element, which is accommodated so as to be in the optical path of one of the spilt light components of the input beam and in the optical path of one light component emerging from the structure and propagating towards said beam polarizing element; - a light circulator is provided being accommodated in the optical path of the input beam to thereby direct the input beam towards said structure through the beam polarizing element, and in the optical path of said combined output beam to thereby direct it towards an output channel. 23. The device according to Claim 16, operable as a controllable wavelength-dependent device for performing at least one of the following functions: filtering, switching, modulating, equalizing, dispersion compensating and attenuating. 24. The device according to Claim 16, operable as an attenuator for different polarization components of the input beam. 25. The device according to Claim 16, and also comprising an additional domain-patterned feπoelectric crystal structure with inverted domains formed with electrodes' arrangement on the surface of the additional structure, the device being operable as an add/drop filter.

Inventors: ARIE ADY, BURSTEIN AMIR, ARIE, ADY, BURSTEIN, AMIR
Applicants: ARIE ADY, BURSTEIN AMIR, ZETTALIGHT INC, ARIE, ADY, BURSTEIN, AMIR, ZETTALIGHT INC.
Application year: 2001
Main classification: G02F1
IPC codes: G01N35, G02F1, H01S3