The present invention relates to an optical waveguide device.
Priority is claimed on Japanese Patent Application No. 2009-225725, filed on Sep. 30, 2009, the content of which is incorporated herein by reference.
An existing optical waveguide device will be described by exemplifying a Modulator with Polarization Beam Combiner shown in
However, in the configuration of
Further, in the configuration of
The invention is made in view of the above-described circumstances, and it is an object of the invention to provide a small optical waveguide device with little reflected light.
The invention is made to solve the above-described problems. According to the invention, there is provided an optical waveguide device including: an optical waveguide element of which a first output waveguide is inclined with respect to an output end face and a second output waveguide is inclined with respect to both the first output waveguide and the output end face; and a lens that allows the beams respectively output from the first and second output waveguides to be parallel to each other.
Further, according to the optical waveguide device of the invention, the first and second output waveguides preferably are symmetrical to each other with respect to the normal line of the output end face.
Further, according to the optical waveguide device of the invention, the lens preferably allow the beams respectively output from the first and second output waveguides to be collimated beams parallel to each other.
Further, according to the optical waveguide device of the invention, the optical waveguide device preferably includes: a polarization beam rotating unit that rotates the polarization of the beam output from the optical waveguide element or the lens; and a polarization beam combining unit that polarizes and combines the beams output from the polarization beam rotating unit.
Further, according to the optical waveguide device of the invention, the optical waveguide element preferably include first and second optical modulating units, and is an optical modulator that outputs modulated beams using the first and second optical modulating units from the first and second output waveguides.
According to the invention, it is possible to provide a small optical waveguide device with little reflected light.
Hereinafter, an embodiment of the invention will be described in detail by referring to the drawings.
The modulator body 10 is an optical waveguide element (LN optical modulator) in which optical waveguides and a modulation electrodes are mounted on a substrate formed of lithium niobate (LiNbO3: referred to as LN).
The optical waveguides of the modulator body 10 has a nest structure in which both arms of a Mach-Zehnder waveguide MA are equipped with Mach-Zehnder waveguides MB and MC, both arms of the Mach-Zehnder waveguide MB are equipped with Mach-Zehnder waveguides 101 and 102, and both arms of the Mach-Zehnder waveguide MC are equipped with Mach-Zehnder waveguides 103 and 104. That is, the input beam toward the modulator body 10 is introduced into an input waveguide 106 of the Mach-Zehnder waveguide MA, and is branched into the Mach-Zehnder waveguides MB and MC on the arms. Further, the beam which is input to the Mach-Zehnder waveguide MB is branched into the Mach-Zehnder waveguides 101 and 102, and the beam which is input to the Mach-Zehnder waveguide MC is branched into the Mach-Zehnder waveguides 103 and 104. Then, the output beams from the Mach-Zehnder waveguides 101 and 102 are multiplexed by the Mach-Zehnder waveguide MB and are introduced into the arm 108 of the Mach-Zehnder waveguide MA. The output beams from the Mach-Zehnder waveguides 103 and 104 are multiplexed by the Mach-Zehnder waveguide MC and are introduced into the arm 109 of the Mach-Zehnder waveguide MA.
The Mach-Zehnder waveguides 101 to 104 (the optical modulating units) form an LN optical modulator together with the modulation electrodes (not shown) respectively installed therein. For example, a driving signal of 10 Gb/s is applied from a driving circuit (not shown) to the modulation electrode of each of the LN optical modulators 101 to 104, and each of the LN optical modulators 101 to 104 outputs a modulated beam which is modulated into 10 Gb/s. As the modulation type of the LN optical modulators 101 and 102 of the Mach-Zehnder waveguide MB, DQPSK (differential quadric-phase shift keying) is used herein. The same applies to the modulation types of the LN optical modulators 103 and 104 of the Mach-Zehnder waveguide MC. The beams which are introduced into the arms 108 and 109 of the Mach-Zehnder waveguide MA by DQPSK becomes a modulated beams of 20 Gb/s.
The arm 108 of the Mach-Zehnder waveguide MA is formed so that the vicinity (an output waveguide 1081) of one end face M of the LN substrate (the modulator body 10) forms an angle θ1 with respect to the normal line of the end face M. Further, in the same way, the arm 109 of the Mach-Zehnder waveguide MA is formed so that the vicinity (an output waveguide 1091) of the end face M forms an angle θ2 with respect to the normal line of the end face M. In this way, since the output waveguides 1081 and 1091 are inclined with respect to the end face M, the reflected light from the end face M toward the output waveguides 1081 and 1091 may be reduced.
Here, it is desirable to set the angles θ1 and θ2 formed between the output waveguides 1081 and 1091 and the normal line of the end face M to be in the range of, for example, 2° to 4°. In the case of θ1=θ2=2°, the reflection loss (return loss) in the end faces M of the output waveguides 1081 and 1091 becomes 30 dB. In the case of θ1=θ2=3.5°, the reflection loss becomes 55 dB. On the contrary, the reflection loss is 13 dB when the output waveguides 1081 and 1091 are perpendicular to the end face M, that is, θ1=θ2=0°. Accordingly, compared to this case, in this embodiment, the reflected light from the end face M toward the output waveguides 1081 and 1091 is drastically reduced.
The ½-wave plate 30a rotates the polarization plane of the beam output from the output waveguide 1081 by 45°. Further, the ½-wave plate 30b rotates the polarization plane of the beam output from the output waveguide 1091 by 45° in a direction opposite to that of the beam output from the output waveguide 1081. Accordingly, the polarization planes of the beam output from the ½-wave plate 30a and the beam output from the ½-wave plate 30b are inclined with respect to each other by 90°.
With regard to the cylindrical lens 20, the refractive index of the lens, the curvature of the lens curved face, and the thickness of the lens are set so that the beams output from the ½-wave plates 30a and 30b are collimated and the optical axes of the beams passing through the cylindrical lens 20 are parallel to each other. Since the beams which are incident to the cylindrical lens 20 are disposed so as to be inclined with respect to the optical axis of the cylindrical lens 20, the beams output from the cylindrical lens 20 may be parallelized when the refractive index of the cylindrical lens 20, the curvature thereof, and the thickness thereof are adjusted in this way. Accordingly, there is no need to install a prism 60 which changes the optical path as in the existing configuration of
In the element to combine polarization beam 40, two beams, which are incident to the different incident positions with polarization planes different by 90°, from the cylindrical lens 20, are output to the same optical path. Accordingly, a modulated beam of 40 Gb/s is obtained by combining modulated beams of 20 Gb/s of which the polarization planes are inclined with respect to each other by 90°. As the element to combine polarization beam 40, for example, an element formed from rutile or calcite may be used. However, particularly, it is desirable to use a Savart plate which is formed by bonding two plates (the polarizing and separating plates 40a and 40b) having the same thickness and formed from rutile or the like so that the optical axes are perpendicular to each other. When the Savart plate is used, since the optical lengths of the beam from the arm 108 and the optical lengths of the beam from the arm 109 are equal, two beams may be polarized and combined with no difference in the optical path.
While the embodiment of the invention has been described by referring to the drawings, the detailed configuration is not limited to the above-described configuration, and the design and the like may be modified into various forms within the scope of the concept of the invention.
For example, the rotation angle of the polarization plane using the ½-wave plate 30a may be 90°, and the rotation angle of the polarization plane using the ½-wave plate 30b may be 0°. Further, as shown in
Further, instead of the cylindrical lens 20, a Selfoc lens may be used. When the refractive index distribution and the thickness (the length in the optical axis direction) of the Selfoc lens are appropriately set, the beams output from the ½-wave plates 30a and 30b may be collimated and the optical axes of the beams passing through the Selfoc lens may be parallel to each other.
Further, as described above, the output waveguides 1081 and 1091 need to form the angles θ1 and θ2 with respect to the normal line of the end face M, but may not necessarily intersect each other inside the LN substrate (the modulator body 10) as shown in
Further, in the above-described embodiment, the Modulator with Polarization Beam Combiner has been exemplified, but the invention is not limited thereto. That is, the invention may be applied to the optical waveguide element other than the LN optical modulator.
According to the invention, it is possible to provide a small optical waveguide device with little reflected light.
Number | Date | Country | Kind |
---|---|---|---|
2009-225725 | Sep 2009 | JP | national |
Filing Document | Filing Date | Country | Kind | 371c Date |
---|---|---|---|---|
PCT/JP2010/066580 | 9/24/2010 | WO | 00 | 3/28/2012 |