Symmetric interferometers unbalanced by using light exposure to tailor the spectral behavior

• US 6,400,870 B1
• Filed: 01/10/2000
• Issued: 06/04/2002
• Est. Priority Date: 11/11/1999
• Status: Expired due to Fees

• Current Assignee: Alschatag Daff GmbH LLC (Intellectual Ventures LLC)
• Original Assignee: Her Majesty The Queen In Right of Canada As Represented By The Minister of Industry (The Republic of Canada)
• Inventors: Hill, Kenneth O., Islam, Mohammed Nazrul
• Primary Examiner(s): NGO, HUNG NHAT
• Application Number:
  US09/480,166
• Time in Patent Office: 876 Days
• Field of Search: 385/39, 385/48, 385/50, 385/42, 385/5, 385/14, 385/3
• US Class Current: 385/39
• CPC Class Codes: G02B 6/2821 using lateral coupling between contiguous fibres to split or combine optical signals
• CPC Class Codes: G02B 6/29355 Cascade arrangement of interferometers
• CPC Class Codes: G02B 6/29395 configurable, e.g. tunable or reconfigurable switching G02B6/35

Abstract

Unbalanced Mach-Zehnder interferometers (MZI) are useful for a number of applications including wavelength filters, gain flattening or gain equalization elements, and band splitters or combiners. A MZI is comprised of two couplers surrounding a phase shifting region, which consists of two arms with differential propagation constants. We disclose a means of using light exposure to unbalance a symmetric MZI consisting of substantially the same lengths of substantially the same fiber. In particular, the index of refraction of a fiber can be increased by exposure to ultraviolet light, and the magnitude of the change can be increased by using higher germanium doping or by hydrogen loading the fiber. The magnitude of the phase shift can be controlled accurately by varying the fiber length exposed, the light exposure intensity, the light exposure time, and the hydrogen loading or fiber composition. In addition, exposing the other arm,of the MZI to trim back the phase shift can compensate any over-exposure of the fiber. By starting with a symmetric MZI made from substantially the same fiber, low polarization sensitivity or polarization dependent loss can be achieved, and the device can operate over a wider overall wavelength range. Also, by using a MZI with substantially the same lengths of fibers and by placing those fibers parallel to one another, low environmental sensitivity can be achieved. Moreover, the use of light exposure to unbalance the MZI has the advantage of enabling precise tailoring of the spectral response with ease of manufacturing and high yields. The MZI devices can be cascaded to achieve more complicated filtering functions in lattice devices such as Lyot-Ohman filters or Solc filters.

Claims

1. A method of making an interferometric optical filter comprising the steps of:

a) providing a splitter and combiner;

b) providing two arms coupled to the splitter and combiner, the two arms each having a core and a cladding, the arms being substantially same optical path length and having substantially similar mode field diameters along the length thereof; and

,

c) irradiating a region of one of the two arms with light of a suitable intensity and duration so as to vary the refractive index n over a region of length L in a substantially uniform manner of said one of the two arms to provide a refractive index difference An and an optical path length difference between the two arms to effect a change Δ

f, where Δ

f is the spacing between a peak and null wavelength of the spectral response of the filter.

2. A method as defined in claim 1 wherein Δ

f is a sinusoidal spectral output response of the filter and wherein LΔ

n is substantially equal to c/2Δ

f.

3. A method of making an interferometric filter as defined in claim 2 wherein the splitter and combiner comprises a first and second optical coupler each providing a splitting and/or combining function, the two arms defined in step (b) being disposed between the first and second optical coupler, one of the two optical couplers for splitting light incident thereon into two branches corresponding to the two arms.

4. A method as defined in claim 2, wherein the step of irradiating a region is performed in a substantially uniform manner over the entire region of exposure to effect a substantially uniform refractive index change over said region.

5. A method as defined in claim 2 wherein the arms defined in step (a) have mode field diameters that are within 30% of each other along the length of the arms.

6. A method as defined in claim 5 wherein the refractive index along the core of each of the two arms is substantially uniform and wherein the refractive index difference between the two arms is no greater than 10% prior to said irradiating step (b).

7. A method of making an optical filter comprising the steps of:

a) providing an MZI having two substantially similar arms disposed between two optical couplers, the arms each having a core and a cladding and having a substantially same optical path length;

b) irradiating one of the two arms with light of a suitable intensity and duration so as to vary the refractive index of an irradiated region and to provide a relative difference in the optical path lengths between the two arms such that light divided by one of the couplers propagating along the two arms will be phase shifted when combined by the other of the couplers, wherein the refractive index remains varied for a substantial time after the step of irradiating is completed.

8. A method as defined in claim 7 wherein the step of irradiating is performed substantially uniformly and wherein the two substantially similar arms in step (a) have mode field diameters within 30% of one another.

9. A method of making an optical filter comprising the steps of:

a) providing an optical coupler for splitting and coupling light to or from two arms, the two arms being substantially similar in mode field diameter, the arms each having a core and a cladding and having a substantially same optical path length;

b) irradiating a region of at least one of the arms of the two arms with light of a suitable intensity and duration so as to vary the refractive index of the irradiated region substantially uniformly to vary the optical path length of at least one of the two arms and to provide a phase offset for light propagating within the two arms, wherein the refractive index remains varied for a substantial time after the step of irradiating is completed.

10. A method of making an optical filter as defined in claim 9 further comprising the step of hydrogen or deuterium loading of at least one of the waveguide arms prior to the irradiating step.

11. A method as defined in claim 9 further comprising the step of determining Δ

Leff that will provide a value of c/2Δ

f, where Δ

Leff=LΔ

n and where, c is the speed of light and Δ

f is the spacing between peak and null wavelengths from the filter, prior to the irradiating step.

12. A method as defined in claim 9, further comprising the step of determining by detecting light output from the filter when the irradiation step (b) should be terminated.

13. A method of making an optical filter comprising the steps of:

a) providing an optical coupler for splitting and coupling light to or from two arms, the two arms being substantially similar in mode field diameter, the arms each having a core and a cladding and having a substantially same optical path length;

b) irradiating a region of at least one of the arms of the two arms with light of a suitable intensity and duration so as to vary the refractive index of the irradiated region substantially uniformly to vary the optical path length of at least one of the two arms and to provide a phase offset for light propagating within the two arms; and

irradiating the other of the two arms with light of suitable intensity and duration to lessen the optical path length difference between the at least two arms.

14. A method of making an optical filter comprising the steps of:

providing a plurality of waveguide pairs between at least three optical couplers, each of the waveguides within a pair being substantially similar in mode field diameter along their length other than having an optical path length difference between waveguide pairs caused by one or more regions having had a light induced refractive index change.

15. An optical filter comprising:

an optical coupler for splitting and coupling light;

two unbalanced optical waveguide arms directly coupled with the optical coupler, the arms being substantially similar along their length other than having a dissimilarity caused by a refractive index change in at least one light irradiated region in at least one of the waveguides providing a difference in optical path length and refractive index between the arms that would otherwise not exist in the absence of light irradiation of at least one of the arms having been performed and which exists for a substantial period of time after the light irradiation is completed.

16. An optical filter comprising:

an optical coupler for splitting and coupling light; and

,

two unbalanced optical waveguide arms directly coupled with the optical coupler, the arms being substantially similar along their length other than having a dissimilarity caused by a refractive index change in at least one light irradiated region in at least one of the waveguides providing a difference in optical path length and refractive index between the arms that would otherwise not exist in the absence of light irradiation of at least one of the arms,

wherein the arms have mode field diameters along their length that are within 30% of each other in regions of the waveguide where the refractive index has not been modified by the use of light.

17. An optical filter as defined in claim 16 further comprising a second optical coupler directly coupled with the waveguide arms such that the arms are disposed between the two couplers.

18. An optical filter as defined in claim 16 wherein the arms of the same physical length, and mode field diameter and optical path length, other than a difference provided by irradiating at least one of the arms to provide an optical path length difference.

19. An optical filter as defined in claim 16 wherein a difference in Leff of an irradiated region is equal to c/2Δ

f.

20. An optical filter as defined in claim 16, wherein the filter further comprises two reflectors optically coupled with the arms for reflecting light received from the coupler back to the coupler.

21. An optical filter as defined in claim 17 wherein the filter is a Mach Zehnder interferometer.

22. An optical filter as defined in claim 17 comprising a third coupler disposed to receive light from the second coupler and having a pair of waveguide arms disposed between the second and third coupler, the arms being substantially similar along their length other than having a dissimilarity caused by a refractive index change in at least one light irradiated region in at least one of the waveguides providing a difference in optical path length and refractive index between the arms that would otherwise not exist in the absence of light irradiation of at least one of the arms to permanently change the refractive index.