Photonic crystal waveguide arrays

• US 6,175,671 B1
• Filed: 10/01/1998
• Issued: 01/16/2001
• Est. Priority Date: 10/01/1998
• Status: Expired due to Term

• Current Assignee: RPX Clearinghouse LLC (RPX Corporation)
• Original Assignee: Nortel Networks Limited (Nortel Networks Corporation)
• Inventors: Roberts, Kim Byron
• Primary Examiner(s): Bovernick, Rodney
• Assistant Examiner(s): Stahl, Michael J.
• Application Number:
  US09/165,053
• Time in Patent Office: 838 Days
• Field of Search: 385/129-132, 385/14, 385/24, 385/27, 385/37, 385/39, 385/40, 385/45-47, 359/176, 359/177, 359/179, 359/194, 359/333, 359/337
• US Class Current: 385/14
• CPC Class Codes: B82Y 20/00 Nanooptics, e.g. quantum optics or photonic crystals
• CPC Class Codes: G02B 2006/1215 Splitter
• CPC Class Codes: G02B 2006/12159 Interferometer
• CPC Class Codes: G02B 6/12011 characterised by the arrayed waveguides, e.g. comprising a filled groove in the array section
• CPC Class Codes: G02B 6/12033 characterised by means for configuring the device, e.g. moveable element for wavelength tuning switching G02B6/35; thermo-optic devices G02F1/0147
• CPC Class Codes: G02B 6/1225 comprising photonic band-gap structures or photonic lattices
• CPC Class Codes: G02F 1/011 in optical waveguides, not otherwise provided for in this subclass
• CPC Class Codes: G02F 1/212 Mach-Zehnder type
• CPC Class Codes: G02F 1/3137 with intersecting or branching waveguides, e.g. X-switches and Y-junctions
• CPC Class Codes: G02F 2202/32 Photonic crystals
• CPC Class Codes: H01S 5/0268 Integrated waveguide grating router, e.g. emission of a multi-wavelength laser array is combined by a "dragon router"
• CPC Class Codes: H01S 5/11 Comprising a photonic bandgap structure

Abstract

A waveguide device for optical signals in an optical communication system relies upon photonic bandgap material to guide the optical signal via a plurality of pathways. A two-dimensional photonic bandgap material is formed in a planar slab of dielectric medium by a two-dimensional lattice in which discontinuities in the lattice region define waveguides. A waveguide array formed in the device allows multiple Mach-Zehnder interferometer devices to be constructed including small radius turns without significant losses. An optical signal equalizer formed of such a device relies upon the transfer function defined by a multiple arm Mach-Zehnder having arms of different length. By applying controlled modulation to propagation through the arms, an adaptive equalizer is formed. The adaptive equalizer has application in correcting gain tilt in line amplifiers of optical communications systems. The method of applying equalization may include measurement of the spectrum of the output optical signal and providing feedback to control the transfer function applied by the adaptive equalizer.

Claims

1. A waveguide device for an optical signal comprising;

a slab of dielectric medium;

a latticed region formed in the dielectric medium by a periodic array of lattice sites comprising localised structures having dielectric properties which are different from those of the surrounding medium, the periodic array being dimensioned such that a photonic bandgap exists in the latticed region inhibiting propagation of the optical signal therethrough; and

a waveguide region formed in the dielectric medium by discontinuities in the periodic array of lattice sites allowing propagation of the signal therethrough;

wherein the waveguide region defines an input region for the input of the optical signal, an output region for the output of the optical signal and a plurality of optical pathways for conducting respective components of the optical signal between the input and output regions;

wherein the waveguide region defines a cavity bounded by a boundary surface at the transition between the latticed region and the waveguide region, the cavity communicating with the input region and the output region; and

wherein the boundary surface constitutes a plurality of reflectors directing respective components of the optical signal via said respective optical pathways between the input region and the output region.

2. A device as claimed in claim 1 further comprising modulating means operable to modulate transmission of at least one of the components of the optical signal within the cavity.

3. A device as claimed in claim 2 wherein the modulating means comprises an array of modulating elements located in the cavity, each element being operable to modulate a respective component of the optical signal.

4. A device as claimed in claim 3 wherein the modulating elements comprise controlled latticed sites.

5. A waveguide device for an optical signal comprising;

a slab of dielectric medium;

a latticed region formed in the dielectric medium by a periodic array of lattice sites comprising localised structures having dielectric properties which are different from those of the surrounding medium, the periodic array being dimensioned such that a photonic bandgap exists in the latticed region inhibiting propagation of the optical signal therethrough; and

a waveguide region formed in the dielectric medium by discontinuities in the periodic array of lattice sites allowing propagation of the signal therethrough;

wherein the waveguide region defines an input region for the input of the optical signal, an output region for the output of the optical signal and a plurality of optical pathways for conducting respective components of the optical signal between the input and output regions; and

comprising modulating means operable to variably control transmission through a plurality of the optical pathways to adaptively define a transfer function of equalization applied to frequency components of the optical signal.

6. A device as claimed in claim 5 comprising control means for controlling the modulating means and operable to determine modulation parameters to be applied by the modulating means in response to input of data defining a desired transfer function for the applied equalization, wherein the modulation means is operable to modulate transmission of components of the optical signal via respective pathways in dependence upon values of respective modulation parameters.

7. A device as claimed in claim 6 further comprising measurement means operable to measure the spectrum of the optical signal output from the output region and wherein the control means is operable to determine the modulation parameters in accordance with the measured spectrum and the input data.

8. A waveguide device for an optical signal comprising;

a slab of dielectric medium;

a latticed region formed in the dielectric medium by a periodic array of lattice sites comprising localised structures having dielectric properties which are different from those of the surrounding medium, the periodic array being dimensioned such that a photonic bandgap exists in the latticed region inhibiting propagation of the optical signal therethrough; and

a waveguide region formed in the dielectric medium by discontinuities in the periodic array of lattice sites allowing propagation of the signal therethrough;

wherein the waveguide region defines an input region for the input of the optical signal, an output region for the output of the optical signal and a plurality of optical pathways for conducting respective components of the optical signal between the input and output regions;

wherein the waveguide region defines a cavity bounded by a boundary surface at the transition between the latticed region and the waveguide region and a plurality of waveguides communicating with the cavity at different locations on the boundary surface, the cavity being formed with a linearly extending portion of the boundary surface; and

wherein the waveguide region further defines an input waveguide communicating with the cavity and positioned to direct the optical signal into grazing incidence with the linearly extending portion for creating surface wave propagation of the optical signal propagating in proximity with the linearly extending portion.

9. A device as claimed in claim 8 comprising modulating means operable to modulate properties of localised structures constituting the linearly extending portion of the boundary surface to variably control proportions of the optical signal deflected from surface wave propagation into the respective waveguides communicating with the cavity.

10. A method of applying equalization to an optical signal comprising the steps of;

inputting the optical signal to an input region of a waveguide device;

conducting components of the optical signal to an output region of the waveguide device via a plurality of respective optical pathways defined by the waveguide device; and

outputting the optical signal from the output region;

wherein the step of conducting the components of the optical signal comprises inhibiting propagation of the optical signal through a latticed region formed by a periodic array of lattice sties defining a photonic bandgap and propagating the components of the optical signal via a waveguide region formed by discontinuities in the periodic array of lattice sites;

wherein the waveguide region defines a cavity bounded by a boundary surface at the transition between the latticed region and the waveguide region, the cavity communicating with the input region and the output region; and

wherein the boundary surface constitutes a plurality of reflectors directing respective components of the optical signal via respective pathways between the input region and the output region.

11. A method as claimed in claim 10 further comprising the step of modulating transmission of at least one of the components of the optical signal within the cavity.

12. A method as claimed in claim 11 wherein the modulating step comprises operating an array of modulating elements located in the cavity, each element modulating a respective component of the optical signal.

13. A method as claimed in claim 12 wherein the modulating elements comprise controlled latticed sites.

14. A method of applying equalization to an optical signal comprising the steps of;

inputting the optical signal to an input region of a waveguide device;

conducting components of the optical signal to an output region of the waveguide device via a plurality of respective optical pathways defined by the waveguide device;

modulating transmission through at least one of the optical pathways to thereby modulate a respective component of the optical signal; and

outputting the optical signal from the output region;

wherein the step of conducting the components of the optical signal comprises inhibiting propagation of the optical signal through a latticed region formed by a periodic array of lattice sties defining a photonic bandgap and propagating the components of the optical signal via a waveguide region formed by discontinuities in the periodic array of lattice sites; and

wherein the modulating step comprises variably controlling transmission through a plurality of the optical pathways to adaptively define a transfer function of equalization applied to frequency components of the optical signal.

15. A method as claimed in claim 14 comprising a controlling step of determining modulation parameters to be applied in the modulating step in response to input of data defining a desired transfer function for the applied equalization, wherein the modulation step modulates transmission of components of the optical signal via respective pathways in dependence upon values of respective modulation parameters.

16. A method as claimed in claim 15 further comprising the step of measuring the spectrum of the optical signal output from the output region and wherein the controlling step determines the modulation parameters in accordance with the measured spectrum and the input data.

17. A method of dividing an optical signal into a plurality of components for conduction via respective waveguides comprising the steps of:

inputting the optical signal into a waveguide region defined by discontinuities in a latticed region in which propagation is inhibited by a photonic band gap;

directing the optical signal into grazing incidence with a linearly extending surface defined by a transition between the latticed region and the waveguide region so that surface wave propagation of the optical signal occurs in proximity with the linearly extending surface;

deflecting portions of the surface wave by scattering from the linearly extending surface; and

conducting the deflected portions into said waveguides.

18. A method as claimed in claim 17 including the step of modulating properties of localised structures defining lattice sites in the latticed region at the transition defining the linearly extending surface, and controlling said modulation so as to variably control the proportions of said optical signal deflected into the respective waveguides.

19. An optical communications system comprising at least one waveguide device for an optical signal, said at least one waveguide device comprising:

a slab of dielectric medium;

a latticed region formed in the dielectric medium by a periodic array of lattice sites comprising localised structures having dielectric properties which are different from those of the surrounding medium, the periodic array being dimensioned such that a photonic bandgap exists in the latticed region inhibiting propagation of the optical signal therethrough;

a waveguide region formed in the dielectric medium by discontinuities in the periodic array of lattice sites allowing propagation of the signal therethrough; and

a line amplifier operable to amplify said optical signal;

wherein the waveguide region defines an input region for the input of the optical signal, and output region for the output of the optical signal and a plurality of optical pathways for conducting respective components of the optical signal between the input and output regions; and

wherein said waveguide device constitutes a component of said line amplifier.

20. An optical communication system as claimed in claim 19 wherein said waveguide device is operable to correct gain tilt in said line amplifier.