OPTICAL ROUTER

Abstract

An optical routing element may include a planar dielectric photonic crystal which includes a lattice of holes having a first linear defect adjacent a second linear defect, with the two defects being separated by a central row of lattice holes. The first linear defect in the lattice of holes may form a first single mode line defect waveguide, and the second linear defect in the lattice of holes may form a second single mode line defect waveguide. Optical energy may be selectively coupled between the first and second waveguides across the central row of lattice holes. A free-carrier injector may be included to inject free-carriers into the dielectric photonic crystal, activation of which may alter selectivity of the optical coupling between the first and second waveguides. A plurality of optical routing elements with associated free-carrier injectors may be interconnected to form a bi-directional optical routing array.

Claims

1-28. (canceled)

29. An optical signal router comprising: a plurality of router input/output ports of the optical signal router each configured to connect to a corresponding external waveguide to optically communicate therewith; and an array of optical routing nodes interposed between the plurality of router input/output ports to selectively route optical signals between pairs of the router input/output ports, each optical routing node comprising: four bi-directional optical switches including a first bi-directional optical switch, a second bi-directional optical switch, a third bi-directional optical switch and a fourth bi-directional optical switch, each of the four bi-directional optical switches comprising a first switch input/output port, a second switch input/output port, a third switch input/output port and a fourth switch input/output port, each bi-direction optical switch configured to receive a first optical signal via either of the first and second switch input/output ports and output the first optical signal via a selected one of the third and fourth switch input/output ports, and configured to receive a second optical signal via either of the third and fourth switch input/output ports and to output the second optical signal via a selected one of the first and second switch input/output ports, at least a portion of each of eight input/output waveguides, each of the eight input/output waveguides shared with and directly connected to either a neighboring optical routing node of the array of optical routing nodes or a router input/output port of the plurality of router input/output ports to provide a corresponding bi-directional optical signal path therebetween, each of the eight input/output optical waveguides directly connected to a corresponding one of the first and third switch input/output ports of the four bi-directional optical switches, and four internal optical waveguides, each of the four internal optical waveguides directly connected to a second switch input/output port of one of the four bi-directional optical switches to a fourth switch input/output port of a neighboring one of the four bi-directional optical switches to provide a bi-directional optical signal path therebetween, the four internal optical waveguides and the four bi-directional optical switches thereby being connected to provide a bi-directional first closed loop optical signal path internal to the optical routing node, whereby the optical signal router is configurable to provide plural optical signal paths between selected pairs of the router input/output ports in response to a selected configuration of each bi-directional optical switches to simultaneously transmit optical signals between the selected pairs of the router input/output ports on the plural optical signal paths.

Description

BRIEF DESCRIPTION OF THE DRAWINGS

[0017] In the drawings, wherein like reference numerals refer to similar components:

[0018] FIG. 1 illustrates a bi-directional photonic crystal routing element;

[0019] FIGS. 2A & 2B show an image of a directional photonic crystal routing element and a dispersion diagram associated therewith;

[0020] FIGS. 3A-3C show the simulated output from a directional photonic crystal routing element;

[0021] FIG. 4 illustrates band diagrams corresponding to changes in the size of holes between two waveguides;

[0022] FIG. 5 illustrates a comparison between calculated and experimental results from a directional photonic crystal routing element;

[0023] FIGS. 6A-6F show the spectral response of a directional photonic crystal routing element in a series of infrared images at various input wavelengths;

[0024] FIG. 7 illustrates a band diagram showing the effect of changes in the refractive index in a directional photonic crystal routing element;

[0025] FIGS. 8A-8C show the simulated output from a switched directional photonic crystal routing element;

[0026] FIG. 9 illustrates changes in spectral output as compared to changes in the index of refraction;

[0027] FIG. 10 illustrates the relationship between cross and bar states for a photonic crystal routing element and moving between those two states based on changes in the phase mismatch;

[0028] FIG. 11 illustrates a directional photonic crystal routing element with a PIN diode;

[0029] FIGS. 12A-12D illustrate simulated results from a directional photonic crystal routing element with a PIN diode;

[0030] FIGS. 13A-13C illustrate the design of a directional photonic crystal routing element;

[0031] FIG. 14 illustrates the characteristics of a PIN diode when used with and without a directional photonic crystal routing element;

[0032] FIGS. 15A & 15B illustrate two different architectures for an optical router incorporating a plurality of bi-directional photonic crystal routing elements;

[0033] FIG. 16 illustrates an optical router and electrical and its optical routing performance;

[0034] FIG. 17 shows images of a bi-directional optical router;

[0035] FIGS. 18A and 18B illustrate experimental set-up and transmission results for a bi-directional optical router;

[0036] FIG. 19 shows an image of an eight port bi-directional optical router;

[0037] FIG. 20 illustrates a schematic diagram of the eight port bi-directional optical router shown in FIG. 19;

[0038] FIGS. 21A-21D illustrate four different routing options for an eight port bi-directional optical router;

[0039] FIG. 22 illustrates a reconfigurable optical cross-connect system utilizing bi-directional optical routers;

[0040] FIG. 23 illustrates a parity based reconfigurable optical cross-connect system utilizing bi-directional optical routers;

[0041] FIG. 24 shows an image of an optical switch node which may be incorporated into an optical FPGA; and

[0042] FIG. 25 shows an image of a fabricated switch node with PIN diodes and electrical contacts.

DETAILED DESCRIPTION OF VARIOUS EMBODIMENTS

[0043] The routing elements described herein may use photonic crystals (PhCs) along with the slow light effect in order to reduce and/or minimize the coupling length needed to switch the optical beam between two waveguides. By forming a defect in the PhC with a photonic band gap, photons can propagate only along the line defect, thus forming a waveguide. In the case of the coupler, two single mode waveguides may be brought into close proximity to each other, forming a two mode system. These two modes, called even and odd modes, may propagate with different group velocities, causing energy to flow from one waveguide into the other. The distance needed to achieve this coupling may generally be related to the inverse of the separation between the wave numbers of the two modes. Therefore, maximizing the separation of the two modes in k-space may serve to minimize the coupling distance. This may be achieved using the slow light effect, which causes a sharp change in the mode separation in k-space. Using this technique, coupling distances as short as 5 m may be obtained. The passive coupler, when combined with an active method for changing the refractive index, can be used as a highly sensitive switch.

[0044] Turning in detail to the drawings, FIG. 1 illustrates a bi-directional photonic crystal routing element 11. The routing element 11 is illustrated as including two waveguides 13, 15 and four input/output ports 17 coupled to the waveguides 13, 15. The waveguides 13, 15 may each be formed by linear defects in a lattice of holes 19 formed on a planar photonic crystal 21. The P and N electrodes 23, 25 of a PIN diode may be disposed on opposite sides of the lattice 19. The PIN diode may serve to change the refractive index of the PhC, thereby enabling use of the routing element 11 as an active optical switch.

[0045] The remainder of the disclosure below explores the properties of this bidirectional photonic routing element (four input/output ports), along with those of the simpler directional photonic routing element (one input port and two output ports), and applications for each as interconnected elements in routing fabric. Property and design highlights for these elements and routers may include: [0046] employing slow-light properties of planar photonic crystal structures; [0047] the slow-light properties (slow light factor=60) may enable compact device design; [0048] individual routing elements may be constructed with dimensions of 10 m5 m (20 photonic crystal lattice elements); [0049] a routing node may have overall dimensions of 50 m50 m; [0050] full bi-directional routing may be enabled; [0051] individual routing elements may be optimized to attain routing for low-refractive index changes (n=0.004); [0052] the power needed for routing may be optimized to less than 1 mW per routing element; [0053] the propagation loss may be about 0.0035 dB/m, or 410.sup.2 dB per routing element; [0054] coupling between waveguides in a routing element may exhibit an extinction ratio of about 17 dB; [0055] the ability to filter and route C-band channels with channel spacing of 4 nm and routing of C-band channels with channel spacing of 0.4 nm; [0056] pulse dispersion of 1.5 ps nm.sup.1 mm.sup.1 may be achieved; [0057] eight channel routing of interconnected routing elements, using various topologies, may be demonstrated; [0058] active tuning elements may be obtained, along with optimized device performance, for low routing power (1 mW) using optimal doping concentrations (510.sup.18 cm.sup.3); [0059] the switching time for a routing element with active tuning elements was experimentally demonstrated at 500 ns; and [0060] a dispersion-free regime of up to 160 Gb/s may be obtained.

Design of a Slow-Light Based Nanophotonic Routing Element

[0061] As a solution to the growing demand for optical intra-chip communication and routing, a dielectric 2D photonic crystal (PhC) directional coupler, which may be actively switched in plane, may be provided. This PhC device may be used to selectively couple light between two waveguides as a routing element, and it may be constructed having a device footprint less than 10 m10 m. The PhC device that meets these design specifications, as described below, may be referred to as a Coupled Photonic Crystal Waveguide (CPhCWG). When compared to traditional dielectric PhC couplers, the design of the CPhCWG may allow a larger coupling bandwidth with lower power consumption for active switching due to the ability to have small device dimensions.

[0062] An image of a directional CPhCWG 31 is shown in FIG. 2A. This directional CPhCWG 31 image is of a fabricated directional CPhCWG in a 260 nm Silicon-on-insulator (SOI) substrate. Similar devices could be fabricated in a SOI thicknesses ranging from about 210 nm to 270 nm. The directional CPhCWG 31 may include two coupled line defect photonic crystal waveguides 33 forming a single input port 35 and two output ports, referred to herein as the bar port 37 and the cross port 39. Each line defect waveguide may be formed by removing a row of holes in the PhC (i.e., not forming the row of holes during the manufacturing process, which is well-known to those of skill in the relevant arts), thereby restricting the propagation of light to only be in the direction of the removed row. The two proximal waveguides may then form a system of modes with overlapping profiles, as shown in the dispersion diagram of FIG. 2B. Here, the two modes are referred to as being even 41 and odd 43. The two modes may generally propagate in the waveguides with different group velocities, resulting in exchange of optical power between the two waveguides.

[0063] The directional CPhCWG 31 may include holes of two different sizes. The smaller holes 45 may form the bulk of the lattice, and the larger holes, referred to herein as central holes 47, may help control the characteristics of the modes that propagate in the waveguides. As is discussed in greater detail below, changing the diameter of the central holes 47 may aid in fine-tuning characteristics such as coupling efficiency and coupling length. At times, it may be convenient to measure the coupling length in terms of transverse lattice elements; one transverse lattice element 49 is shown outlined in FIG. 2A. With appropriate choices in hole diameters, certain spectra of optical energy may be coupled between the waveguides in as few as five transverse lattice elements.

[0064] The CPhCWG may utilize the slow light effect to reduce the physical device length while maintaining a longer effective interaction length between the waveguides. This effect may be realized by engineering the dilation of hole diameters in the PhC to flatten the band of the even mode. As a result of the light traveling slower in the PhC, the light may be subject to more of the material and device features, allowing for the coupling length to be less than 10 m. The increased interaction may also allow for a subtle index change of n=0.004 to switch the CPhCWG's output from one port to the next. The device characteristics may differ from traditional PhC couplers by offering a wider coupling bandwidth and reduced power requirements, but drawbacks may arise in the fabrication of the device. Because the optical properties of the device may be affected by the device design, perhaps more than with other devices, the tolerance of fabrication dimensions and effect of defects may be greatly amplified. For example, a dilation of 2 nm in a hole diameter of 330 nm may result in a 5 nm shift of the coupling wavelengths. The enhanced material interaction and low index change requirements may allow the CPhCWG to selectively couple between the two ports through free-carrier injection of an in-plane PIN diode. By using a PIN diode, free-carriers may be injected laterally across the PhC lattice, which may change the refractive index of the silicon and may directly shift the spectrum that is coupled between the waveguides. The routing element may naturally rest in the OFF state with no applied bias, coupling optical energy directed into the input port 35 to the cross port 39, and turning the routing element ON under forward bias, the optical spectrum may blue-shift, resulting in the optical energy being coupled to the bar port 37.

[0065] Such behavior can be observed through the finite-difference time-domain (FDTD) simulation results shown in FIGS. 3A-3C. FIG. 3A shows the simulated output of the directional CPhCWG for the bar and cross ports. FIG. 3B illustrates a simulated directional CPhCWG coupling input optical energy to the bar port, and FIG. 3C illustrates a simulated directional CPhCWG coupling input optical energy to the cross port. As depicted, FIG. 3B may represent the ON state for a directional CPhCWG, and FIG. 3C may represent the OFF state.

Design of Routing Element Using PhC Directional Coupler

[0066] The dispersion properties of the coupled waveguide modes can be extracted using the Plane Wave Expansion Method (PWEM) where the electromagnetic wave equation is solved as an eigenvalue problem with a periodic boundary condition and using a coupled waveguide structure as a unit cell for the analysis.

[0067] FIG. 4 is a dispersion diagram for various mode profiles, each based on a different hole diameter in the PhC. From the dispersion diagram, it is evident that at certain frequencies, i.e., between 0.256 a/ and 0.268 a/, the wavevectors between even and odd modes are quite different. At the maximum point, the difference may be larger than 0.01. From the coupling length formulation (Eq. (3) below), a coupling length of around 5 lattices may be obtained. Such a short coupling length can be used for ultra compact optical routing applications.

[0068] The dispersion properties of the coupled waveguide structure can be tuned by changing the air hole sizes in the central row as well as the cladding surrounding both waveguides.

[0069] The dispersion diagrams with different air hole sizes are illustrated in FIG. 4. As the central hole diameter, d, increases from 0.6 a to 0.825 a, both even and odd modes shift to higher frequencies. As d increases to 0.825 a, there are two important features for the even mode as observed from the dispersion diagrams. First, the slopes of two modes are almost parallel within the frequency range from 0.255 to 0.267 a/. The large frequency range indicates large operational bandwidth. On the other hand, at frequency of 0.267 a/, the dispersion curvature becomes flat at k=0.4. As is known from the definition of group velocity, the group index will be very large in this case, and a significant slow light propagation in the photonic crystal waveguide can occur. As a result, the strong EM coupling between even and odd modes may lead to an efficient energy transition between waveguides, which may be used to reduce the coupling length. To this end, by means of the fine-tuning of air hole sizes, a large group index, which typically ranges from 40 to 400, may be achieved.

Fabrication and Characterization of Single Routing Elements

[0070] A prototype of a routing element, as shown in FIG. 2, may be fabricated using e-beam lithography and an Inductively Couple Plasma Reactive Ion Etch (ICP-RIE) with fluorine based chemistry for pattern transfer into the SOI wafer. Experimental characterization of a sample fabricated in this way was performed by fiber coupling an optical signal, supplied by a tunable laser source, into the photonic device. The routing element structure shown in FIG. 5 was simulated numerically with a coupling region of 12.8 m, and the routing element was experimentally fabricated and spectrally characterized with the tunable lasers.

[0071] In FIG. 5, the lighter regions within the image of the two wavelengths propagating through the device is scattered light from the waveguides being supported by the underlying oxide. It should be noticed that there is not a traceable amount of light detected that is scattering from the photonic crystal routing element. The characterization of the single photonic crystal routing element presented the routing of two wavelengths with a separation of 1.16 nm across two ports with an average extinction ratio of 17 dB, agreeing with a numerical analysis of the routing element.

[0072] Spectral responses of fabricated single routing elements with varying coupling lengths were performed, demonstrating the tunable nature of the channel spacing through the adjustment of the coupling length via inserting or removing the number of lattice sites that the photonic crystal couples over. The separation of 6 nm between routable wavelengths, as shown in FIGS. 6A-6F, where the input wavelength is tuned from 1550 nm to 1557 nm, illustrates the ability to passively route channels within the International Telecommunication Union (ITU) standards for optical routing.

Tuning Routing Elements

[0073] By taking advantage of the slow light effect in the coupled PhC waveguide, an active switching routing element can be designed using a nonlinear medium. As an example, thermal-optic and electro-optic free-carrier injection approaches may be applied to change the refractive index of the host material, thereby tuning the dispersion properties. In such way, this compact coupler can be used to achieve highly sensitive and tunable optical devices, such as tunable optical splitter. One approach that can be used is to change the refractive index through free-carrier injection, where two electrodes are lithographically defined to apply a current through the PIN junction, with the PhC disposed within the junction. Through free-carrier injection, the maximum change of index can be on the order of 0.01, which may provide enough dynamic range for the designed active routing element.

[0074] To investigate the sensitivity of the optical routing element, the refractive index of the silicon host material was tuned down by n=0.004 from the original index of 2.9. FIG. 7 illustrates the dispersion diagrams with refractive indices of 2.9 and 2.896. At a frequency of 0.2615 c/a, the wave vector difference of even and odd modes at n=0.004 are doubled compared with the case of n=0, which means that the coupling length is reduced by a factor of two. This may allow complete light switching to be achieved between the two waveguides with an index change of as little as 0.004. Depending upon the materials used, switching with yet smaller index changes may be achieved.

[0075] To confirm the design, a bi-directional routing element was simulated by using the FDTD method. The design wavelength was chosen around 1500 nm. The background and central row air hole sizes were chosen as 240 nm and 340 nm, respectively. Different hole sizes may be selected depending upon the wavelength for which the routing element is designed. A total length of 14 lattice elements was used for the coupling. The routing element was fed with four dielectric waveguides. The dielectric waveguide had a width of 690 nm. Due to the strong mismatch between the group velocity of the dielectric waveguide and that of the coupled PhC waveguide, a spatial lattice tapering near the interface along the propagation direction was introduced to minimize the unwanted interface reflection. At both interfaces three PhC lattices were linearly tapered from 480 nm to 400 nm. Based on this design, an improved transmission was achieved in the simulations.

[0076] To characterize the spectrum response, a few detectors were placed at the two output ports, labeled port 3 and port 4 in FIGS. 8B & 8C, to record both transient and frequency spectra. FIG. 8A illustrates these spectra, which show that at a wavelength of 1513.6 nm, ports 3 and 4 achieve complete switching by an index change of 0.0004. FIGS. 8B & 8C illustrates this complete switching by simulation of the power flow through in a routing element having a refractive index of 2.9 in FIG. 8B and a refractive index of 2.896 in FIG. 8C. The steady state results of the electrical fields in the computational region demonstrate the high throughput coupling of the routing element.

[0077] In addition, the host material index may be continuously varied to study the modulation at the wavelength of 1513.6 nm. The transmission response of ports 3 and 4 versus the varying refractive index are illustrated in FIG. 9.

Actively Tuning Routing Elements

[0078] As has been indicated above, a routing element may be actively switched. For example, by applying an electric field, a change in the propagation constant and hence the index of refraction in the coupling region between the two waveguides, may be induced, and the system may change from a symmetric system of coupled PhC waveguides into a non-symmetric one. In this case the equation for the coupling length between the two waveguides may be modified to include the change in the refractive index caused by the external applied field as follows:

[00001]$\begin{array}{cc}{L}_E=\frac{}{2.Math.\sqrt{\left({}^2+{}^2.Math.n\right)}}& \left(1\right)\end{array}$

where L.sub.E is the length for full power transfer under external excitation.

[0079] Mathematically, the operation of the routing element can be formulated as being in either one of two states: the bar state (ON), when the energy launched at the near end of one of the waveguides exits from the far end of that same waveguide; and the cross state (OFF), when the energy launched at the near end of one of the waveguides exits at the far end of the other waveguide.

[0080] Using coupled mode theory, Equation (4) may be simplified to the following

(L).sup.2+(L).sup.2=(v).sup.2. (2)

where v is a positive integer, and where:

[00002]$\begin{array}{cc}.Math..Math.L=\left(2.Math.v-1\right).Math.\frac{}{2},& \left(3\right)\end{array}$

where v is again any positive integer. From Equation (3), the shortest length for complete coupling is determined to occur when L=/(2).

[0081] A plot of Equation (3) is shown in FIG. 10, which shows that the cross states lie at isolated points on the axis =0 corresponding to the synchronous case, whereas the bar states are represented by the arcs. Starting from a cross state, a bar state can be reached only by changing the phase mismatch shown by the dotted line. Or mathematically, starting from a cross state with L=/2, then the required phase mismatch can be found from Equation (2) as

[00003]$\begin{array}{cc}.Math..Math.=.Math..Math.n=\sqrt{3}.Math.\frac{}{L}.& \left(4\right)\end{array}$

The phase mismatch condition can be achieved by applying an external excitation which my thus result in switching between the cross and the bar states.

[0082] The loss tangent of the dielectric material in the coupling region can be modified by external commands to spoil the coupling, thereby re-routing the light. This may be characterized as an switch (not the classical switch), in which the change in optical absorption coefficient is employed (the change in conductance is proportional to ) as a modulating mechanism. The induced loss may not significantly attenuate the waves traveling in the straight-through channels. This behavior may be analogous to circumstances where electro-absorption has been assumed to reduce the Q of micro-ring resonators coupled to strip channel waveguides. To attain switching in the waveguides made from Si/air or Si/SiO.sub.2, the free-carrier absorption loss of Si can be controlled by (1) free-carrier injection from forward-biased PN junctions on the rods, (2) depletion of doped rods with MOS gates, or (3) generation of electrons and holes by above-gap light shining upon the coupling area, a contact less process. If the routing element is implemented in III-V semiconductor hetero-layers, then the electro-absorption effect may be used. As is illustrated in FIG. 11, a PIN diode is positioned with the routing element in the intrinsic region to introduce free-carriers into the PhC.

[0083] The design shown in FIG. 11 may need an extensive level of semiconductor device modeling to determine the optimal doping concentrations and doping profiles of the P and N regions, in order to minimize the electrical power needed to route the optical signal between the various output ports. Preferably, Phosphorous and Boron are used for the n-type and p-type dopants, respectively, with concentrations for each preferably in the range of 10.sup.18 to 10.sup.19 per cm.sup.3, and more preferably having a concentration of about 510.sup.18 per cm.sup.3. A commercially available package (Silvaco) was used for detailed analysis of the device used in an implementation. FIGS. 12A-12D illustrate snapshots of the Silvaco analysis as well as the current and charge distribution through the device. FIG. 12A illustrates a cross-sectional view of a routing element showing the P and N doping regions and approximate lateral doping profile that is to be fabricated. The vertical doping profile is preferably approximately uniform throughout. FIG. 12B illustrates a lateral cross sectional view of a routing element showing the intrinsic region. FIG. 12C illustrates the current density distribution in a routing element. FIG. 12D is a graph illustrating extracted I-V characteristics of simulated devices.

[0084] A directional routing element along with the PIN diode structure is shown in the design schematic of FIG. 13A. The gap between the P and N doping regions may be, e.g., 5 m. The voltage across the PIN diode may be controlled by the voltage source, which may enable the output of the routing element to be selected between the bar port and the cross port. FIG. 13B shows images of an exemplary routing element that was constructed with a PIN diode. In this image, the P-doped region is at the top of the image, the N-doped region is at the bottom of the image, and the PhC is disposed between the two doped regions. FIG. 13C shows an image of silicon waveguides coupling in and out of an exemplary routing element on a SOI platform, with gold contacts forming circuit connections for the PIN diode. In FIG. 14, the performance of a PIN diode is compared with and without a PhC in the depletion region.

Design and Fabrication of Bi-Directional Optical Routers

[0085] Given the bi-directional routing element, e.g., as shown in FIG. 1 several of these routing elements may be used as the basis for the design architecture of a bi-directional router. The architecture of two basic bi-directional routers, both of which may be used as a routing node for more complex routing fabrics, are shown in FIGS. 15A & 15B. Other types of routing nodes are possible, and the invention is not to be limited to these embodiments. FIG. 15A is based upon the well-known Manhattan architecture, and FIG. 15B is based upon the well-known honeycomb architecture. In either architecture, the optical signal between any adjacent or orthogonal ports can be redirected to any other port externally by modulating the coupling between the two waveguides of individual bi-directional routing elements. As such the optical signal can travel in either the forward, backward, upward or downward directions. This may provide an exceptional degree of reconfigurability.

[0086] The routing performance, switching table, and propagation loss for an example of a 22 routing fabric is shown in FIG. 16. In basic operation, an optical signal input at port A1 may pass through 4 elements to exit at port A2 and through 6 elements to exit at port B2. For the output at port A2, no routing elements may need to be ON, i.e., outputting optical energy at the bar port. For the output at port B2, only two routing elements, minimally, may need to be ON, which in an exemplary embodiment, may consume approximately 1 mW of total electrical power to attain this path and may incur a cost of approximately 0.24 dB of total optical loss.

[0087] A prototype of a 13 bi-directional routing node was fabricated, as is shown photographically in FIG. 17. The node shown in photo (a) may allow an optical signal to be incident upon the routing fabric at any one of the four ports, and may route the signal to any other of the three remaining ports. Photo (b) shows a single fundamental routing fabric element of the routing fabric, which can be structured to an mn array. Each fundamental routing fabric element may consist of four photonic crystal elements joined by bending silicon nanowire waveguides. Photo (c) shows that the PhC routing element may utilize the input and output of each line defect waveguide, which may allow each element to be bi-directional from every waveguide incident on the routing element. The density of the routing elements within the fabric may be easily adjusted by changing the bending radius of the nanowire waveguides, either to space out or condense the device footprint on a chip. In the fabricated prototype, the approximate lateral and vertical dimension of the routing fabric element is 50 m. Property and design highlights that may be achieved from such a routing fabric are listed in Table 1.

TABLE-US-00001 TABLE 1 Properties exhibited by an example routing fabric Routing unit cell (node) 50 m 50 m dimensions Number of routing elements per 4 unit cell Propagation loss per routing 4 10.sup.2 dB/element element Switching (routing) power per 1 mW routing element Pulse dispersion 1.5 ps nm.sup.1 mm.sup.1 Free dispersion rate Up to 160 Gb/s Routing speed 500 ns per element Extinction ratio 17 dB Routing channel spacing 4 nm for routing element of 16a coupling length 2 nm for routing element of 36a coupling length 0.8 nm for routing element of 108a coupling length 0.4 nm for routing element of 162a coupling length

[0088] To passively characterize a routing node, the exemplary routing node pictured in FIG. 18A was constructed to allow monitoring of all possible output channels represented by waveguides (WG) 1-6. Spectral scans were performed by launching an optical signal into the input nanowire waveguide, and monitoring each output waveguide individually. The spectral characterization showed the optical signal was appropriately routed to waveguides WG3 and WG6 for their corresponding channels, maintaining a comparable performance of the single routing element with a channel separation of 1.16 nm and an average extinction ratio of about 12 dB. The measured outputs of WG3 and WG6 are shown in FIG. 18B. The remaining 4 probed waveguides remained a minimum of 17 dB below the channels optical signal strength. With this demonstration of acceptable single-node performance, the 8 port routing fabric shown in the photo of FIG. 19 was fabricated using 4 routing nodes. As is explained below, the 8 port routing fabric also performed as expected, and it is anticipated that routing fabrics with greater numbers of nodes, whether of similar architecture or having significantly different architecture, but using the same basic routing element as the primary building block, could be constructed using these same principles.

[0089] The network configurations and topologies presented below can be implemented for the cases of a single incoming fiber carrying N different wavelength channels, or an N fiber ribbon carrying a number of N different wavelength channels.

[0090] For an N port router, there are

[00004]$\underset{i=0}{\overset{\left(\frac{N}{2}-1\right)}{.Math.}}.Math..Math.\left(N-1-2.Math.i\right)$

ways to interconnect N-ports.

[0091] Therefore for N=8 there are 753=105 ways to connect an 8 port routing fabric. A conceptual design of an 8 port routing fabric, with port and element labeling, is shown in FIG. 20. FIGS. 21A-21D illustrate 4 possibilities out of the 112 ways to interconnect the 8 port routing fabric shown in FIG. 20. Each of these four different configurations may simultaneously interconnect 4 pairs of the available 8 ports. In each configuration, the routing elements in the ON state are listed in the column adjacent the listed pair of ports. With these select routing elements in the ON state, a pathway between the two indicated ports may be created for each configuration.

[0092] An optical crossconnect system in a reconfigurable optical network is illustrated in FIG. 22, which is an example of an optical crossconnect system utilizing a number of 16 port routing fabrics. Each routing fabric may interconnect an input from one of four channels within the optical network to any one of another four channels within the optical network.

[0093] An example of a parity-based optical crossconnect system in a reconfigurable optical network is illustrated in FIG. 23. This alternative to the system shown in FIG. 22 divides the incoming channels into odd and even channels and routes each channel based on its parity.

[0094] The routing element can further be implemented into a larger design as a switch in an optical routing fabric. For example, the switch node, shown in the photo of FIG. 24 alongside a switching table, has the functionality to route an optical signal as a 13 directional switch. The switch node may be symmetric, allowing it to be replicated in a nm array to form a large switch fabric that can function as an optical FPGA and perform operations such as routing, logic, integration and buffering. Although, with the freedom to choose the size of the array, it does not necessarily mean that if more ports in the array are needed, a 2D chip layout can accommodate the extra real estate required. As device densities continue to increase on chips, the ability to be released from the restrictions of photonic devices structured in a 2D substrate can allow for a new 3D photonic chip architecture by layering devices and building vertically on the chip. An alternative fabricated switch node is shown in the photos of FIG. 25, which also illustrates the PIN diode electrical contacts.

[0095] Thus, an optical signal router, both as a single optical signal routing element and as a plurality of interconnected optical signal routing elements, may be provided. While embodiments of this invention have been shown and described, it will be apparent to those skilled in the art that many more modifications are possible without departing from the inventive concepts herein. The invention, therefore, is not to be restricted except in the spirit of the following claims.