Optical communication means

Abstract: Disclosed are an optical interconnection network and process, having a phase-conjugate mirror and input and output side channels. In the network, time-reversed wave, of a light beam propagated through the output side channel, is generated in the phase-conjugate mirror to cause an interconnection between the input side channel and the output side channel. The energy of the time-reversed wave comes from a light beam propagated through the input side channel.

Description: BACKGROUND OF THE INVENTION Field of the Invention The present invention relates to an optical communication means usable for optical interconnection networks or optical crossbar switches and processes using a purely optical means for performing the switching of a signal between an input and output. The switching involves not only that of a one-to-one connection type between any selected input and output, but also those of a one-to-multiple connection or broadcasting type and a multiple-to-one connection type. Related Background Art Conventionally, an electric crossbar switch has been used as an interconnection means between the input and the output of a non-closed type information network. In the electric crossbar switch, however, the number of electric switches increases in proportion to the product of the number of input and output terminals. As a result, problems such as a shortage of transmission hands, the physical complexity of the system, the large size of the system, and similar problems are more likely to occur as the scale of the system becomes larger. Hence, it was difficult to make the scale of the system large. Furthermore, from Applied Optics. Vol. 27, no. 16, 15 August 1988, New York US, pages 3422-3428, S. Weiss et al. "Photorefractive dynamic optical interconnects" an optical communication means according to the preamble of the annexed claim 1 is known. SUMMARY OF THE INVENTION An object of the present invention is to provide an optical communication means in which a crossbar switch is achieved by pure optical means. This object is achieved by an optical communication means according to the annexed claims. The present invention will be more readily understood in connection with the following detailed description of the preferred embodiment in conjunction with the drawings. BRIEF DESCRIPTION OF THE DRAWINGS Figs. 1a-d are drawings for explaining a crossbar switching having a function of self-routing. Fig. 2 is a drawing for explaining the principle of a double phase-conjugate mirror (DPCM). Fig. 3 is a schematic view for explaining the propagation of a phase-conjugated wave in a multimode optical fiber. Fig. 4 is a schematic view of an embodiment of the present invention. DESCRIPTION OF THE PREFERRED EMBODIMENT Initially, the principle of the present invention will be described referring to an example of Fig. 1. In Fig. 1a, an input side 10 includes channel 1 through channel N, where the wavelength of an input signal in one channel is selected from one of wavelengths λ 1 ∼λ N . Thus, the self-routing function is achieved in such a manner that the input signals of the respective input side channels 1∼N designate their addresses or output side channels 1∼N by themselves, respectively. At an output side 20, there are arranged channels 1∼N corresponding to the wavelengths used at the input side 10. The wavelengths λ 1 ∼λ N at the input side respectively correspond to the channels 1∼N at the output side 20. Thereby, an interconnection or crossbar switch having an N × N self-routing function can be attained. An optical signal of one wavelength has, for example, a wavelength of λ 1 when the signal enters a switching system. The optical signal includes, as shown in Figs. 1a-1b, two cells, i.e., a control information or data field 3 containing an address data at the crossbar switch 6 and an information or data field 4. Fig. 1b shows the optical signal prior to pre-processing, Fig. 1c shows the signal after pre-processing and Fig. 1d shows the signal after crossbar switching. The control data field 3 of the signal is read in a pre-processing part 5, and the wavelength of the signal is converted into a wavelength (for example, a wavelength of λ N ) corresponding to the address data (output side channel) at the crossbar switch. At this time, the control data field 3 containing an address information at a next switching system and the original information field 4 are modulated in the wavelength λ N . In an embodiment described below, an explanation is begun with a stage after the pre-processing part 5. Therefore, after the signal passes the crossbar switch 6, the optical signal of the control information field 3 and the information field 4 are modulated, as shown in Fig. 1c, in the wavelength λ N and enter the next switching system. In connection with this, see Kitayama et al., "Third Optical Communication Systems Symposium Material, OCS 89-1S∼11S (1989)", Optical Communication System Special Study Committee (Electronics Information Communication Society). Next, the principle will be described, by which the crossbar switching between input and output is performed in a purely optical manner, and how a self-routing control for conducting the switch control by an input signal itself is achieved. Such a structure using a DPCM and a multimode optical fiber is utilized for explaining this principle. Fig. 2 shows the DPCM. In Fig. 2, an electro-optic crystal 21 has a photorefractive effect (PR effect). The PR effect is a phenomenon that a space-charged electric field distribution is generated in a crystal 21 by light irradiating thereinto, causing a change in the refractive index of the crystal 21, due to a linear electro-optic effect (Pockels effect). As an example of such a crystal, there are ferroelectric electro-optic crystals such as barium titanate (BaTiO 3 ) and semiconductor electro-optic crystals such as GaAs. Here, BaTiO 3 is used as an example. In Fig. 2, when a c-axis of the barium titanate crystal 21 is oriented in an appropriate direction as shown in Fig. 2, an incoming light 22 is scattered in the crystal 21 and the scattered light and the incoming light 22 interact with each other to form a multiplicity of refractive index gratings in the crystal 21. In this case, an exchange of energy is conducted between the scattered light and the incoming light 22 due to a nonlinear interaction causing an energy transfer from the incoming light 22 to the scattered light. This is called a two-wave mixing. On the other hand, when another incoming light 23 enters the crystal 21 from the left side of Fig. 2, additional refractive index gratings are formed in the crystal 21 due to the interaction between the incoming light 23 and its scattered light causing an energy transfer from the incoming light 23 to its scattered light. During such a process, a common refractive index grating of a group of the refractive index gratings formed by the incoming lights 22 and 23 and the respective scattered lights diffracts the respective incoming lights 22 and 23 to cause an induced scattering which strengthens the common refractive index grating. As a result, only the common refractive index grating survives in a steady state. It should be noted that the incoming lights 22 and 23 do not need to be coherent with each other since the refractive index gratings are formed by the incoming light 22 and its scattered light 25 and by the incoming light 23 and its scattered light 24. Therefore, when the incoming lights 22 and 23 exist in the crystal 21 at the same time, the scattered lights 24 and 25 become phase-conjugated waves of the incoming lights 22 and 23, respectively, even if the incoming lights 22 and 23 are incoherent with each other. Further, a remarkable feature exists in that energies of those phase-conjugated waves 24 and 25 come from the incoming lights 23 and 22, respectively (not 22 and 23). That is, the phase-conjugated waves 24 and 25 are diffraction lights of the incoming lights 23 and 22, respectively, that are diffracted by the above-discussed refractive index grating. In more detail, the phase-conjugated wave 24 receives its energy and bias phase component from the incoming light 23 while being a round-trip (time-reversed) wave of the incoming light 22, and the phase-conjugated wave 25 receives its energy and bias phase component from the incoming light 22 while being a round-trip (time-reversed) wave of the incoming light 23. With respect to theoretical and experimental details thereof, see B. Fischer et al., "IEEE J. Quantum Electron. QE-25, 550-569 (1989)". Fig. 3 shows the characteristics of a phase-conjugated wave is propagated through a multimode optical fiber. An arrangement in which a light beam propagated through a multimode optical fiber 31 enters a phase conjugate mirror (PCM) 32 through a lens 33 is now considered. Assuming that two incoming lights 34 and 35 enter the multimode optical fiber 31 at different angles, a light beam emerging from the multimode optical fiber 31 will be in a speckled stateand its polarization state will be disturbed because modal dispersal and intermodal scrambling or scattering occur in the multimode optical fiber 31. In this case, however, when the phase conjugate mirror 32 produces a complete phase-conjugate wave for the light emerging from the right side end of the fiber 31 (including its polarization state), a reflection light from the PCM 32 propagates from right to left through a path identical with a propagation path from left to right since the reflection light is a time-reversed wave for the incoming light. The reflection light then emerges from the left end of the fiber 31 at the same angle as the incident angle of the incoming light. That is, reflection lights 36 and 37 are respectively phase-conjugate waves of the incoming lights 34 and 35, not only spatially, but also in the polarization state. When a PR crystal is used as the PCM 32, the PCM 32 in Fig. 3 produces a phase-conjugate wave solely for a given polarization component of the emerging light from the right end of the fiber 31 since the PR effect is caused only for the given polarization component of the incoming light. However, when a numerical aperture (N.A.) of each incoming light 34, 35 into the fiber 31 is sufficiently smaller than the N.A. of the fiber 31, and the intermode scrambling or scattering is thoroughly generated in the fiber 31, the emerging lights 36 and 37 emerge from the fiber 31 as phase-conjugate waves, respectively, preserving the polarization states of the incoming lights 34 and 35. This fact is confirmed theoretically and experimentally. In this connection, see Y. Tomita et al., "IEEE J. Quantum Electron. QE-25, 315-338 (1989)". Therefore, under the above conditions, the reflection lights 36 and 37 become phase-conjugate waves of the incoming lights 34 and 35, respectively, both spatially and in the polarization state. Based on the above-discussed principle, the optical interconnection or crossbar switching between input and output is performed in a purely optical manner, using the function of the PCM. Further, the self-routing control in which the switching control is performed by the input light signal itself is achieved by controlling its wavelength. According to the principle explained referring to Fig. 3, a connected response signal from the output side can reach the input side at the same time as that at which the connection between input and output sides is completed. As a result, it is possible to confirm whether the connection between the input side and the output side is proper or not, in real time at the input side. Fig. 4 shows an embodiment of the present invention. The DPCM shown in Fig. 2 is used as a phase-conjugate mirror 41. The above-mentioned PR crystal may preferably be used as a nonlinear optical crystal, but other materials may be used only if they can function as the DPCM. At both sides of the PCM 41, multimode optical fibers 46 and 47 are respectively connected through wavelength dispersal elements 42 and 43. A diffraction grating or the like is used as the wavelength dispersal element. It is assumed here that a light beam 52 corresponding to a channel 1 enters the left end of the multimode optical fiber 47 as an amplitude-modulated or phase-modulated light signal. The light beam is emitted from a single tunable laser or one of a plurality of tunable lasers. When the wavelength of the light beam 52 is set to, for example, λ N (in this connection, see the explanation of Fig. 1), the light beam 52 enters the wavelength dispersal element 43 after passing through the multimode optical fiber 47 and a lens 45. Here, the wavelength dispersal element 43 is adjusted such that light beams respectively enter the PCM 41 at spatially different angles depending upon wavelengths of the light beams. In the assumed case, the light beam 52 of the channel 1 enters the PCM 41 at an angle corresponding to the wavelength λ N . On the other hand, light beams 48 through 50 enter the right end of the multimode optical fiber 46 at different incident angles corresponding to wavelengths λ 1 ∼λ N . The light beams 48 through 50 having the wavelengths λ 1 ∼λ N correspond to output channels 1∼N, respectively. The incident light beams 48 through 50 at the output channel side always enter the right end of the multimode optical fiber 46 whether light beams 52 through 54 of the input channels 1∼N enter the fiber 47 or not. In this structure, if the incoming beam 52 of the wavelength λ N enters the PCM 41, two light beams of the wavelength λ N (one is the light beam 52 and the other is the light beam 50) form a common refractive index grating due to the induced scattering based on the above-discussed principle. As a result, phase-conjugated waves of the light beams 50 and 52 are generated in the PCM 41. Consequently, the amplitude-modulated or phase-modulated light signal from the incident light beam 52 is automatically coupled to the multimode optical fiber 46 at an efficiency of 100 % (excluding a Fresnel reflection) as a phase-conjugated wave of the incident light beam 50, after passing through the wavelength dispersal element 42 and a lens 44. The phase-conjugated wave then propagates through the multimode optical fiber 46 as a time-reversed wave of the incident light beam 50 and emerges from the channel N as alight beam 51. Similarly, the amplitude-modulated or phase-modulated light signal from the incident light beam 50 at the output side, which is generated in the PCM 41 as a phase-conjugated wave of the incident light beam 52, is automatically coupled to the multimode optical fiber 47 at an efficiency of 100 % (excluding a Fresnel reflection) after passing through the wavelength dispersal element 43 and the lens 45. The phase-conjugated wave then propagates through the multimode optical fiber 47 as a time-reversed wave of the incident light beam 52 and emerges from the channel 1 as a light beam 53. In such a process, a light signal from the incident light beam 52 (channel 1) as an input can be connected to the emerging light beam 51 (channel N) as an output through the multimode optical fibers 47 and 46. Moreover, the connected channel can be confirmed at the same time as that at which such connection is completed (i.e., simultaneously with this connection) because the emerging light beam 53 of the wavelength λ N can be detected at the input side. Thus, a set wavelength of each incident light beam at the input side can be selected from a group of λ 1 ∼λ N , and therefore, the optical interconnection network having the self-routing function of N × N can be realized. As explained in the foregoing, according to the present invention, a DPCM, for example, is used as a phase-conjugate mirror, and light beams are caused to be incident on the phase-conjugate mirror from both the input and output sides through, for example, a wavelength dispersal element and a multimode optical fiber. Thus, the crossbar switching between the input and the output is realized in a purely optical manner. Further, the self-routing is achieved by designating the output channel using the wavelength of the light beam from the input side. Moreover, the confirmation of the connection of the input channel to the output side is possible at the input side in real time, at the same time as that at which the connection between the input and the output is completed. Except as otherwise disclosed herein, the various components shown in outline or in block form in Figs. 1a-1d, 2, 3 and 4, are individually well-known and their internal construction and operation is not critical either to the making or using of this invention or to a description of the best mode of the invention. While the present invention has been described with respect to what is presently considered to be the preferred embodiment, it is understood that the invention is not limited to the disclosed embodiment.

Claims: An optical communication means comprising: a first multimode optical fiber ( 47 ), a second multimode optical fiber ( 46 ), and a double phase conjugate mirror ( 41 ) coupled between said multimode optical fibers ( 46, 47 ), for generating phase conjugated waves upon receipt of a first light beam ( 52 ) input in said first multimode optical fiber ( 47 ) and a second light beam ( 50 ) input in said second multimode optical fiber ( 47 ), said first light beam ( 52 ) being automatically coupled to said second multimode optical fiber ( 46 ) as a phase conjugated wave of said second light beam ( 50 ), said phase conjugated wave propagating through said second multimode optical fiber ( 46 ) as a time-reversed wave of said first light beam ( 52 ) and emerging therefrom as a third light beam ( 51 ), and said second light beam ( 50 ) being automatically coupled to said first multimode optical fiber ( 47 ) as a phase conjugated wave of said first light beam ( 52 ), said phase conjugated wave propagating through said first multimode optical fiber ( 47 ) as a time-reversed wave of said second light beam ( 50 ) and emerging therefrom as a fourth light beam ( 53 ), characterized in that between said first multimode fiber ( 47 ) and said double phase conjugate mirror ( 41 ) and said second multimode fiber ( 46 ) and said double phase conjugate mirror ( 41 ) wavelength dispersal elements ( 43, 44 ) are coupled for directing said light beams ( 50, 52 ) to enter said double phase conjugate mirror ( 41 ) at angles corresponding to the wavelengths of said light beams ( 50, 52 ). An optical communication means according to Claim 1, characterized in that said double phase conjugate mirror ( 41 ) comprises an electro-optic crystal having a photorefractive effect. An optical communication means according to Claim 1 or 2, characterized in that said first light beam ( 52 ) input into said first multimode optical fiber ( 47 ) is generated by means of a single tunable laser or one of a plurality of tunable lasers. An optical communication means according any one of the preceding Claims, characterized in that said first light beam ( 52 ) enters the multimode optical fiber ( 47 ) as an amplitude-modulated or phase-modulated light signal.

Inventors: TOMITA YASUO, TOMITA, YASUO, Tomita, Yasuo, c/o Canon Kabushiki Kaisha
Applicants: CANON KK, CANON KABUSHIKI KAISHA
Application year: 1992
Main classification: G02F1
IPC codes: G02F1, H04Q11