Abstract
A demultiplexer for use in a wavelength division multiplexed system. The demultiplexer comprises: an input waveguide, configured to receive a wavelength division multiplexed signal; a demultiplexing element, configured to demultiplex the multiplexed signal received from the input waveguide into a plurality of multi-mode demultiplexed signal components; a multi-mode output waveguide, the multi-mode output waveguide being coupled to the demultiplexing element and configured to receive one of the multi-mode demultiplexed signal components; and a splitter, coupled to the multi-mode output waveguide, and configured to split the received multi-mode demultiplexed signal component into two single-mode outputs.
Claims
1. A demultiplexer, for use in a wavelength division multiplexed system, the demultiplexer comprising: an input waveguide, configured to receive a wavelength division multiplexed signal; a demultiplexing element, configured to demultiplex the multiplexed signal received from the input waveguide into a plurality of multi-mode demultiplexed signal components; a multi-mode output waveguide, the multi-mode output waveguide being coupled to the demultiplexing element and configured to receive one of the multi-mode demultiplexed signal components; and a splitter, coupled to the multi-mode output waveguide, and configured to split the received multi-mode demultiplexed signal component into two single-mode outputs.
2. The demultiplexer of claim 1, wherein the splitter is configured to split the received multi-mode demultiplexed signal asymmetrically.
3. The demultiplexer of claim 1, wherein the splitter is configured to split the received multi-mode demultiplexed signal symmetrically.
4. The demultiplexer of claim 1, wherein the splitter is configured to provide each single-mode output to a respective transfer waveguide.
5. The demultiplexer of claim 4, wherein the demultiplexer is a receiver and includes a waveguide photodiode, connected at a first end to one of the transfer waveguides and connected at a second end to the other of the transfer waveguides.
6. The demultiplexer of claim 5, wherein the waveguide photodiode is configured to absorb at least 90% of the signal received from either end within a half of a length of the waveguide photodiode.
7. The demultiplexer of claim 4, wherein the demultiplexer includes an output Mach-Zehnder interferometer, connected to each of the respective transfer waveguides and operable as a wavelength filter.
8. The demultiplexer of claim 1, wherein the demultiplexer includes an input Mach-Zehnder interferometer, connected between the input waveguide and the demultiplexing element, the input Mach-Zehnder interferometer being operable as a wavelength filter.
9. The demultiplexer of any of claim 4, wherein the transfer waveguides have a similar or substantially identical optical path length.
10. The demultiplexer of claim 1, wherein the demultiplexing element is an arrayed waveguide grating, or an echelle grating.
11. The demultiplexer of claim 1, wherein the multi-mode output waveguide comprises a pair of waveguide ridges projecting from a shared waveguide slab.
12. The demultiplexer of claim 11, wherein each waveguide ridge is configured to support a single mode.
13. The demultiplexer of claim 1, wherein the splitter is a multi-mode interference coupler.
14. The demultiplexer of claim 1, comprising a plurality of multi-mode output waveguides, each being coupled to the demultiplexing element and configured to receive a respective one of the multi-mode demultiplexed signal components.
15. The demultiplexer of claim 14, wherein each multi-mode output waveguide is coupled to a respective splitter, each splitter being configured to split the received multi-mode demultiplexed signal component into two single-mode outputs.
Description
BRIEF DESCRIPTION OF THE DRAWINGS
[0029] Embodiments of the invention will now be described by way of example with reference to the accompanying drawings in which:
[0030] FIG. 1 shows a temperature synchronised demultiplexer;
[0031] FIG. 2 shows a wavelength synchronised demultiplexer;
[0032] FIG. 3 shows a detailed view of the output structure of the demultiplexers of FIGS. 1 and 2;
[0033] FIG. 4 shows a region of the output structure of FIG. 3;
[0034] FIGS. 5 and 6 show various optical modes launched into the free propagation region of the demultiplexer from the tSC region a function of phases shifts;
[0035] FIG. 7 is a plot of channel transmission against wavelength showing the passband of the output structure of FIG. 3;
[0036] FIG. 8 shows an output of a demultiplexer connected to a photodiode;
[0037] FIG. 9 shows a demultiplexer connected to a plurality of photodiodes;
[0038] FIG. 10 shows a plot of insertion loss against wavelength of the photodiodes shown in FIG. 9;
[0039] FIG. 11 shows a variant demultiplexer;
[0040] FIG. 12 is a plot of transmission against wavelength for the variant demultiplexer of FIG. 11;
[0041] FIG. 13 shows plots of transmission against wavelength for four different wavelengths for the variant demultiplexer of FIG. 11;
[0042] FIG. 14 shows a variant demultiplexer;
[0043] FIG. 15 is a plot of transmission against wavelength for the variant demultiplexer of FIG. 14; and
[0044] FIG. 16 shows plots of transmission against wavelength for four different wavelengths for the variant demultiplexer of FIG. 14.
DETAILED DESCRIPTION AND FURTHER OPTIONAL FEATURES
[0045] Aspects and embodiments of the present invention will now be discussed with reference to the accompanying figures. Further aspects and embodiments will be apparent to those skilled in the art.
[0046] FIG. 1 shows a temperature synchronised demultiplexer 100. The demultiplexer includes an input waveguide 102, which is configured to receive a wavelength division multiplexed signal (the dotted line). This signal is single-modal, and the input waveguide is a single-mode waveguide. This wavelength division multiplexed signal is provided into a demultiplexing element 104, in this example an Echelle grating or arrayed-waveguide grating (AWG) which demultiplexes the multiplexed signal into a plurality of multi-mode demultiplexed signal components. Each of the multi-mode (or multi-modal) signal components covers a different wavelength. The demultiplexer includes a plurality of output multi-mode waveguides 106a-106d, the output multi-mode waveguides are each connected to a respective splitter 108a-108d. The splitters are configured to split the respective received multi-mode demultiplexed signal into two single-mode outputs. These single mode outputs are then sent downstream for processing (the dashed lines). The Mach-Zehnder interferometers recombine the signal to a single waveguide efficiently. The MZI design is such that the input multimode structure receives light at its two modes from different wavelengths, and the MZI combines those wavelengths at the single output waveguide which then goes to the photodiodes.
[0047] In this example the temperature synchronized demultiplexer 100 includes an input Mach-Zehnder interferometer 110. The input Mach-Zehnder interferometer 110 is configured to operate as a wavelength filter, and is temperature synchronized in that the input changes its position to compensate for temperature drift. The temperature synchronized demultiplexer 100 also includes a plurality of output Mach-Zehnder interferometers 112a-112d. Each output Mach-Zehnder interferometer is connected to a respective splitter via a transfer waveguide and is operable as a wavelength filter. The output Mach-Zehnder interferometers also each multiplex two wavelengths which are an equal distance from the channel centre so as to get a “flat-top” response.
[0048] FIG. 2 shows a wavelength synchronised demultiplexer 200. Structurally the wavelength synchronized demultiplexer 200 is the same, or substantially the same, as the temperature synchronized demultiplexer 100, and so like features are indicated by like reference numerals. However in this demultiplexer, the input Mach-Zehnder interferometer 110 is operable to change its input position to composite for a change of wavelength. Similarly, the output Mach-Zehnder interferometers 112a-112d each multiplex from different positions as the position shifts with temperature.
[0049] FIG. 3 shows a detailed view of the input structure of the demultiplexers 100 and 200. The input structure comprises an input waveguide Wio, which is connected to a splitter Wmmi_1×2 (in this example a multi-mode interference splitter). The splitter has two outputs, which connect to respective arms of a Mach-Zehnder interferometer. In this example, the width of the upper arm is around 1.5 μm (Web), whereas the width of at least a portion of the lower arm is around 3 μm (W delay) and a path length difference of ΔL/2 is introduced in the lower arm relative to the upper arm. Each arm couples to a coupler, Wmmi_2×2, via waveguides Wio and the coupler recombines the signals. An additional region, tSC, is provided coupled to the combiner, and allows for control over the coupling between the output waveguides of the 2×2MMI which results in turn in better insertion losses and less passband ripples. tSC may have a length of at least 1 μm and no more than 20 μm. The resulting mode is launched into the input free propagation region of the demultiplexing element. The value of dimension L.sub.c shown in FIG. 3 may be at least 10 μm and no more than 1000 μm. The gap may be at least 0.2 μm and no more than 10 μm.
[0050] FIG. 4 shows the region tSC of the output structure of FIG. 3. This region includes two upstanding waveguide ridges with a shared slab. FIGS. 5 and 6 show various optical modes launched into the free propagation region from the tSC region a function of phase shifts. FIG. 7 is a plot of channel transmission against wavelength showing the passband of the Mach-Zehnder interferometer of FIG. 3. As can be seen, a relatively lower passband ripple and insertion loss can be achieved across a range of wavelengths.
[0051] The same structure shown in FIG. 3 can be used for each output from the demultiplexers 100 and 200, where the light would pass from the right-hand side to the left-hand side. That is, the light would enter the region tSC before being split into the Mach-Zehnder interferometer and subsequently recombined in Wmmi_1×2.
[0052] FIG. 8 shows an output of a demultiplexer, not including the output structure shown in FIG. 3, connected to a photodiode. The multimode output of the demultiplexer (either an AWG or echelle grating) is connected to a splitter which divides the power (P.sub.1n(λ)) into two single mode waveguides: P.sub.1 and P.sub.2, where P.sub.1+P.sub.2=|E.sub.tot|.sup.2, E.sub.1 and E.sub.2 are the respective single modes, E.sub.tot=α.sub.1 (λ)E.sub.1+α.sub.2(λ)E.sub.2, |E.sub.tot|.sup.2=T(λ)P.sub.in(λ), and T(λ) is the demultiplexers channel response. The splitter is provided by a waveguide which, in a first section, is wide and supports at least two modes and connects directly to two narrower single mode waveguides. The splitter can achieve a very low excess loss, which means that no matter how the power in the multimode waveguide is distributed between the two single modes, all of the power will always be coupled with some varying ratio between the two single mode waveguides. As the distribution of power between the two modes of the multimode waveguide is determined by the demultiplexer structure, it will depend on wavelength. Therefore, no matter the wavelength, the total guide power of the multimode waveguide will be equal to the sum of the two guided powers in the two single mode waveguides, though the relative ratio in each single mode waveguide will change with wavelength.
[0053] After the splitter, the two single mode waveguides are coupled to the two counter propagating inputs of the photodiode, with equal group delay between the two paths, such that the signal (bits) arrive synchronously at the photodiode. The photodiode current will be the sum of the powers in the counter propagating inputs, and therefore will maintain the increased bandwidth of the demultiplexer.
[0054] FIG. 9 shows a demultiplexer connected to a plurality of photodiodes, implementing a 4 channel demultiplexer. The demultiplexer has 8 channels in pairs of two channels, each as a single mode waveguide. Each pair of channels has a centre separated by the desired channel spacing with the centre of the next pair of channels, but the channel pairs have optimized centre spacing and bandwidths to meet the desired system specification. Each of the single mode waveguides of a pair of channels is coupled to opposite ends of a photodiode, as described with reference to FIG. 8. Therefore pairs of single mode channels have a the following power transmission characteristics: {T.sub.1(λ), T.sub.2(λ)}, {T.sub.3(λ), T.sub.4(λ)}. The corresponding photodiodes have a photocurrent which depends on the wavelength λ as T.sub.PD1(λ)=T.sub.1(λ)+T.sub.2(λ), T.sub.PD2(λ)=T.sub.3(λ)+T.sub.4(λ). By careful consideration of T.sub.i(λ)+T.sub.i+1(λ) a flatter transmission spectrum with good crosstalk can be realised, as the crosstalk will only depend on the width of the narrower channels T.sub.i(λ). FIG. 10, showing a plot of insertion loss against wavelength of the photodiodes shown in FIG. 9, illustrates this point.
[0055] FIG. 11 shows a variant demultiplexer, which is wavelength-synchronized. The demultiplexer of FIG. 11 differs from that shown in FIGS. 1 and 2 in that the output waveguides of the demultiplexer do not have the same output structure shown in FIG. 3. Rather the demultiplexing element of FIG. 11 connects directly to a splitter, which provides dual waveguide outputs to photodiodes connected downstream. FIG. 12 is a plot of transmission against wavelength for the variant demultiplexer of FIG. 11. FIG. 13 shows passband plots for four different wavelengths for the variant demultiplexer of FIG. 11. The echelle has a baseline insertion loss of between 0.8 and 0.9 dB, with a grating period of 9 μm. The plots illustrate superior pass through properties across a range of wavelengths.
[0056] FIG. 14 shows a variant demultiplexer, which is wavelength-synchronized. The demultiplexer of FIG. 14 differs from that shown previously in that the output waveguides of the demultiplexer are multimodal waveguides. FIG. 15 is a plot of transmission against wavelength for the variant demultiplexer of FIG. 14. FIG. 16 shows passband plots for four different wavelengths for the variant demultiplexer of FIG. 14. The demultiplexer element is an echelle grating, with a baseline insertion loss of between 0.8 and 0.9 dB, and a grating period of 9 μm. The plots only consider the first 8 modes. The wavelength-synchronized Mach-Zehnder interferometer input broadens the flat-top response to 18 nm, and the outputs would be connected to multimode photodiodes.
[0057] The features disclosed in the description, or in the following claims, or in the accompanying drawings, expressed in their specific forms or in terms of a means for performing the disclosed function, or a method or process for obtaining the disclosed results, as appropriate, may, separately, or in any combination of such features, be utilised for realising the invention in diverse forms thereof.
[0058] While the invention has been described in conjunction with the exemplary embodiments described above, many equivalent modifications and variations will be apparent to those skilled in the art when given this disclosure. Accordingly, the exemplary embodiments of the invention set forth above are considered to be illustrative and not limiting. Various changes to the described embodiments may be made without departing from the spirit and scope of the invention.
[0059] For the avoidance of any doubt, any theoretical explanations provided herein are provided for the purposes of improving the understanding of a reader. The inventors do not wish to be bound by any of these theoretical explanations.
[0060] Any section headings used herein are for organizational purposes only and are not to be construed as limiting the subject matter described.
[0061] Throughout this specification, including the claims which follow, unless the context requires otherwise, the word “comprise” and “include”, and variations such as “comprises”, “comprising”, and “including” will be understood to imply the inclusion of a stated integer or step or group of integers or steps but not the exclusion of any other integer or step or group of integers or steps.
[0062] It must be noted that, as used in the specification and the appended claims, the singular forms “a,” “an,” and “the” include plural referents unless the context clearly dictates otherwise. Ranges may be expressed herein as from “about” one particular value, and/or to “about” another particular value. When such a range is expressed, another embodiment includes from the one particular value and/or to the other particular value. Similarly, when values are expressed as approximations, by the use of the antecedent “about,” it will be understood that the particular value forms another embodiment. The term “about” in relation to a numerical value is optional and means for example+/−10%.
