This application is based upon and claims the benefit of priority of the prior Japanese Patent Application No. 2014-137875, filed on Jul. 3, 2014, the entire contents of which are incorporated herein by reference.
The embodiments discussed herein are directed to an optical element, a light transmitting device, and a light receiving device.
An optical element such as a wavelength multi/demultiplexing element is used for optical communication and optical interconnection. Silicon (Si) photonics has been recently drawing attention as a promising technology for large-capacity interconnection, and an improvement of transmission capacity per one photonic wire by wavelength division multiplexing (WDM) in a Si chip is expected. A wavelength multi/demultiplexer of Si photonic wire waveguide type, for example, is used as a multiplexer which multiplexes WDM optical signals, and a demultiplexer which demultiplexes a WDM optical signals for transmission/reception of WDM optical signals in the Si chip. As an example of such a multi/demultiplexer, there is a delayed interferometric element, and various studies regarding delayed interferometric elements have been conducted.
For example, it is reported that a flatness of multi/demultiplexed spectrum is improved by loading a ring waveguide coupled to a waveguide between a pair of optical couplers. However, even if the ring waveguide is used, it is difficult for a conventional delayed interferometric element to obtain a sufficient flatness without conducting a temperature control.
Patent Literature 1: Japanese Laid-Open Patent Publication No. 2013-186358
Patent Literature 2: Japanese Laid-Open Patent Publication No. 2013-205626
Non-Patent Literature 1: D. W. Kim, A. Barkai, R. Jones, N. Elek, H. Nguyen, and A. Liu, “Silicon-on-insulator eight-channel optical multiplexer based on a cascade of asymmetric Mach-Zehnder interferometers,” Optics Letters 33(5), 530-532 (2008)
Non-Patent Literature 2: F. Horst, “Silicon integrated waveguide devices for filtering and wavelength demultiplexing,” in Proceedings of 2010 Optical Fiber Communication Conference, OWJ3
Non-Patent Literature 3: J. Song, Q. Fang, S. H. Tao, M. B. Yu, G. Q. Lo, and D. L. Kwong, “Passive ring-assisted Mach-Zehnder interleaver on silicon-on-insulator,” Optics Express 16(12), 8359-8365 (2008)
Non-Patent Literature 4: S.-H. Jeong, S. Tanaka, T. Akiyama, S. Sekiguchi, Y. Tanaka, and K. Morito, “Flat-topped and low loss silicon-nanowire-type optical MUX/DeMUX employing multi-stage microring resonator assisted delayed Mach-Zehnder interferometers,” Optics Express 20(23), 26000-26011 (2012)
According to an aspect of the embodiments, an optical element includes: a first delayed interferometer; and a second delayed interferometer and a third delayed interferometer cascaded to the first delayed interferometer. The first delayed interferometer includes: a first optical coupler and a second optical coupler; a first waveguide between the first optical coupler and the second optical coupler; a second waveguide between the first optical coupler and the second optical coupler, the second waveguide being longer than the first waveguide; and a ring waveguide that is coupled to the first waveguide. A difference between a length of the first waveguide and a length of the second waveguide differs from a difference in lengths corresponding to a channel spacing by a length corresponding to a phase displacement caused by loading of the ring waveguide.
According to another aspect of the embodiments, a light transmitting device includes: a light source unit that emits a plurality of lights with different wavelengths; a modulator that modulates the plurality of lights; and the optical element, the optical element multiplexing the plurality of lights.
According to another aspect of the embodiments, a light receiving device includes: the optical element, the optical element demultiplexing an optical signal to a plurality of lights with different wavelengths; and a light receiver that receives the plurality of lights output from the optical element.
The object and advantages of the invention will be realized and attained by means of the elements and combinations particularly pointed out in the claims.
It is to be understood that both the foregoing general description and the following detailed description are exemplary and explanatory and are not restrictive of the invention.
The inventor of the present application conducted earnest studies regarding the reason why it is difficult for the conventional delayed interferometric element to obtain a multi/demultiplexed spectrum with high flatness without conducting the temperature control. As a result, it was clarified that a phase displacement accompanied by the loading of the ring waveguide occurs in the conventional delayed interferometric element.
However, as a result of earnest studies conducted by the inventor, it was clarified that a difference Δφ1 of an optical signal propagating through the waveguide 1 between a phase in front of a coupling region 4 of the waveguide 1 and the ring waveguide 3 and a phase at a rear of the coupling region 4, does not coincide with a difference Δφ2 of the optical signal propagating through the waveguide 2 between a phase in front of a region 5, corresponding to the coupling region 4, and a phase at a rear of the region 5. Specifically, it was clarified that a phase displacement (Δφ1-Δφ2) caused by the loading of the ring waveguide 3 is included, other than the phase delay of φD and a phase delay caused by a manufacturing error, between the optical signal propagated through the coupling region 4 and the optical signal propagated through the region 5 corresponding to the coupling region 4. In a sample prepared by the inventor, for example, there was a relation presented in Table 1 among a distance between the waveguide 1 and the ring waveguide 3 in the coupling region 4, a length of the coupling region 4, a radius of curvature of a curved portion of the ring waveguide 3, and a relative phase difference (magnitude of phase displacement). The waveguide in the sample was a Si photonic wire waveguide, and a width of the waveguide was 440 nm.
As described above, it was clarified for the first time by the inventor that the phase displacement becomes larger as the distance in the coupling region 4 decreases. It was also clarified for the first time by the inventor that the phase displacement becomes larger as the length of the coupling region 4 increases. It was also clarified for the first time by the inventor that the magnitude of the phase displacement depends on the radius of curvature of the ring waveguide 3 and the widths of the waveguide 1 and the ring waveguide 3. The magnitude of the phase displacement indicates a finite value, and is not a fixed value. Specifically, it was clarified that the ring waveguide 3 exerts an influence on the phase of the optical signal which propagates through the waveguide 1, which has not been focused till now. In the conventional delayed interferometric element, the influence of the phase displacement as above is not taken into consideration, so that even when there is no manufacturing error, it is not possible to obtain a desired characteristic. The magnitude of the phase displacement may be considered based on a difference between an even mode and an odd mode, which are obtained by decomposing a mode distribution of the coupling region 4, and a mode of a delay waveguide.
The inventor further conducted earnest studies based on the above-described new findings, and as a result, it was found out that a flatness of multi/demultiplexed spectrum is improved by providing, to a delayed interferometer including a ring waveguide, a phase shifter that cancels a phase displacement caused by the loading of the ring waveguide.
Hereinafter, embodiments will be concretely described while referring to the attached drawings.
First, a first embodiment will be described. The first embodiment is an example of a wavelength demultiplexer.
An optical element 100 according to the first embodiment includes a delayed interferometer 110, as illustrated in
A delayed interferometer 120 and a delayed interferometer 130 are connected to the optical coupler 115. The delayed interferometer 120 includes an optical coupler 124, an optical coupler 125, and an optical coupler 126, a waveguide 121 and a waveguide 122 are connected between the optical coupler 124 and the optical coupler 125, and a waveguide 127 and a waveguide 128 are connected between the optical coupler 125 and the optical coupler 126. The delayed interferometer 130 includes an optical coupler 134, an optical coupler 135, and an optical coupler 136, a waveguide 131 and a waveguide 132 are connected between the optical coupler 134 and the optical coupler 135, and a waveguide 137 and a waveguide 138 are connected between the optical coupler 135 and the optical coupler 136. The waveguide 122 is longer than the waveguide 121 by a difference ΔL2, and the waveguide 128 is longer than the waveguide 127 by a difference ΔL1. The difference ΔL1 is twice the difference ΔL2. The waveguide 132 is longer than the waveguide 131 by a length obtained by subtracting a length equivalent of 0.5π radians from the difference ΔL2, and the waveguide 138 is longer than the waveguide 137 by a length obtained by subtracting a length equivalent of 1.0π radians from the difference ΔL1. The waveguide 112 is longer than the waveguide 111 by a length ΔLTotal obtained by subtracting a length ΔLPS of the phase shifter 116 from the difference ΔL1 (ΔLTotal=ΔL1−ΔLPS).
As described above, each of the delayed interferometer 120 and the delayed interferometer 130 has a structure of delayed Mach-Zehnder interferometer (DMZI), and the delayed interferometer 110 has a structure of delayed Mach-Zehnder interferometer loaded with micro-ring waveguide (M-DMZI).
Each of the optical coupler 114, the optical coupler 115, the optical coupler 124, the optical coupler 125, the optical coupler 126, the optical coupler 134, the optical coupler 135, and the optical coupler 136 is, for example, a directional coupler or a MMI (multimode interference) coupler. A Si photonic wire waveguide having a cross-sectional structure illustrated in
A buried oxide layer 12 of Si oxide, a Si layer 13, and a Si oxide layer 14 are provided on a Si substrate 11 in a channel structure illustrated in
Next, the difference ΔL1 and the length of the phase shifter 116 will be described. The difference ΔL1 is represented by an expression (1).
ΔL1=(λDMZI×m)/NEq (1)
λDMZI, n, and NEq indicate a center wavelength, a diffraction order, and an effective refractive index of the waveguide 111 and the waveguide 112, respectively, in the delayed interferometric part of the delayed interferometer 110. The delayed interferometric part includes the waveguide 112, and the waveguide 111 excluding a part of the phase shifter 116. A center wavelength λMRR of a micro-ring resonator (MRR) including the ring waveguide 113 and the waveguide 111 is represented by an expression (2). Specifically, in the present embodiment, an antiresonance condition is satisfied. Further, in the present embodiment, an optical coupling ratio KMRR of the micro-ring resonator is about 85%, for example.
λMRR=λDMZI−0.5×Δν (2)
Δν indicates a channel spacing. Therefore, the center wavelength λDMZI can be determined by the channel spacing Δν and the center wavelength λMRR, and the difference ΔL1 can be determined by the center wavelength λDMZI, the diffraction order m, and the effective refractive index NEq. A value obtained by subtracting the difference ΔL1 from the length ΔLTotal corresponds to the length ΔLPS.
The channel spacing Δν is represented by an expression (3).
Δν=λDMZI2/(2×NGr×ΔL1) (3)
In the present embodiment, for example, the channel spacing Δν is 800 GHz, and each of the waveguide 111 and the waveguide 112 has the structure illustrated in
If each of the waveguide 111 and the waveguide 112 has the structure illustrated in
With the use of the optical element 100 as described above, since the delayed interferometer 110 includes the appropriate phase shifter 116, the phase displacement caused by the loading of the ring waveguide 113 is cancelled. Thus, the phase displacement, which has not been conventionally focused, is eliminated, resulting in that an optical multiplexed spectrum with excellent flatness can be obtained and that an excellent roll-off characteristic of a side band can be achieved while securing a desired channel spacing without performing a complicated control such as a temperature control. A low crosstalk can be obtained while realizing a small size due to the function of the ring waveguide 113.
Next, a second embodiment will be described. The second embodiment is an example of a wavelength demultiplexer.
In the second embodiment, the phase shifter 116 is not provided, and a phase shifter 216 is included in the waveguide 112, while the phase shifter 116 is included in the waveguide 111 in the first embodiment as described above. A length of the phase shifter 216 is −0.26 μm. The other structure is similar to that of the first embodiment.
In the second embodiment, since the phase shifter 216 is provided, a length of the waveguide 112 is shorter than that of the first embodiment by 0.26 μm, and since the phase shifter 116 is not provided, a length of the waveguide 111 is shorter than that of the first embodiment by 0.26 μm.
Therefore, similar to the first embodiment, the waveguide 112 is longer than the waveguide 111 by the length ΔLTotal. Thus, an effect similar to that of the first embodiment can be obtained.
Next, a third embodiment will be described. The third embodiment is an example of a wavelength demultiplexer.
In the third embodiment, the phase shifter 116 is not provided, a phase shifter 316 is included in the waveguide 111, and a phase shifter 317 is included in the waveguide 112, while the phase shifter 116 is included in the waveguide 111 in the first embodiment as described above. A length of the phase shifter 316 is 0.13 μm, and a length of the phase shifter 317 is −0.13 μm. The other structure is similar to that of the first embodiment.
In the third embodiment, since the phase shifter 317 is provided, the length of the waveguide 112 is shorter than that of the first embodiment by 0.13 μm, and the length of the waveguide 111 to which the phase shifter 316 is provided instead of the phase shifter 116 is shorter than that of the first embodiment by 0.13 μm. Therefore, similar to the first embodiment, the waveguide 112 is longer than the waveguide 111 by the length ΔLTotal. Thus, an effect similar to that of the first embodiment can be obtained.
As is apparent from the second embodiment and the third embodiment, the phase shifter that suppresses the phase displacement caused by the loading of the ring waveguide may be provided to the waveguide to which the ring waveguide is coupled, to the other waveguide, or to both of the waveguides. The difference in the optical path lengths between the two waveguides generated due to the presence of the phase shifter, not the position at which the phase shifter is provided, is important.
Next, a fourth embodiment will be described. The fourth embodiment is an example of a light transmitting device.
As illustrated in
In the light transmitting device 400, optical signals are individually modulated by the optical modulator 420. The optical element 100 functions as the wavelength multiplexer, in which the modulated optical signals input into the optical coupler 126 and the modulated optical signals input into the optical coupler 136 are multiplexed by the optical element 100, and the multiplexed optical signal is output from the optical coupler 114. Since the optical element 100 exhibits the excellent spectrum flatness, even if the wavelength displacement is generated in the optical signals input into the optical element 100, and even if an operating wavelength shift occurs in the optical element 100 due to a temperature fluctuation, a low-loss is maintained, and a light transmission of wavelength division multiplexed (WDM) signals can be performed.
Next, a fifth embodiment will be described. The fifth embodiment is an example of a light transmitting device.
As illustrated in
In the light transmitting device 500, the optical signals before modulation input into the optical coupler 126 and the optical signals before modulation input into the optical coupler 136 are multiplexed by the optical element 100, and the multiplexed optical signal is output from the optical coupler 114. The multiplexed optical signal is modulated by the optical modulator 520 in a collective manner. An effect similar to that of the light transmitting device 400 can be obtained by the light transmitting device 500.
Next, a sixth embodiment will be described. The sixth embodiment is an example of a light receiving device.
As illustrated in
In the light receiving device 600, a wavelength division multiplexed optical signal (WDM signal) is input into the optical coupler 114, and demultiplexed, for each wavelength, into four types of optical signals by the optical element 100 to be output from the optical couplers 126 and 136. The optical signals of four wavelengths output from the optical couplers 126 and 136 are detected by the light receiver 610. Since the optical element 100 exhibits excellent spectrum flatness and low crosstalk performance, even if the wavelength displacement is generated in the optical signals input into the optical element 100, and even if the operating wavelength shift occurs in the optical element 100 due to the temperature fluctuation, the low-loss and the low crosstalk are maintained. Therefore, power penalty in an optical link can be suppressed when the light receiver 610 performs the detection.
The optical element 200 or 300 may be used instead of the optical element 100, in the fourth to sixth embodiments.
According to the above-described optical element and the like, since the lengths of the waveguides are appropriate, the spectrum with good flatness can be obtained through the simple control.
All examples and conditional language provided herein are intended for the pedagogical purposes of aiding the reader in understanding the invention and the concepts contributed by the inventor to further the art, and are not to be construed as limitations to such specifically recited examples and conditions, nor does the organization of such examples in the specification relate to a showing of the superiority and inferiority of the invention. Although one or more embodiments of the present invention have been described in detail, it should be understood that the various changes, substitutions, and alterations could be made hereto without departing from the spirit and scope of the invention.
Number | Date | Country | Kind |
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2014-137875 | Jul 2014 | JP | national |