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EP1081881A2 Expired / Lapsed EP ⏱️ 0.0 years remaining

Chromatic dispersion compensation

Assignee: Nortel Networks Ltd
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Filing: 2000-06-13
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Granted: —
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Expires: 2020-06-13
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Abstract

Abstract An optical waveguide (11, 71) provided with a linearly chirped Bragg reflective grating (13, 73) can be employed as a device that provides linear dispersion compensation. The amount of the linear dispersion thereby provided can be rendered adjustable by adjustment of the magnitude of axial strain imposed upon the grating. If the chirp is purely linear, and if also, the strain is at all times uniform along the length of the grating, adjustment of the strain magnitude will have no such effect. This requires the presence of a quadratic chirp term, but such a term introduces its own transmission penalty. This penalty is compensated at least in part by causing the light to make a reflection in a further Bragg reflection grating (14, 74) whose quadratic component of chirp has the opposite sign to that of the other Bragg reflection grating, but a substantially matched modulus. The effect of the strain is to scale the effective pitch of the Bragg reflection grating by scaling its physical pitch. An alternative way of achieving a similar effect is to change the effective refractive index of the waveguide in which the grating is formed, for instance by changing its temperature.

Inventors

  • 👤 Julian A. Felis
  • 👤 Andrew J. Collar
  • 👤 Howard N Rourke

Bibliographic Details

Application Number —
Jurisdiction EP
Data Source google_patents
Last Synchronized 2026-11-08 15:11
CPC Classifications
H; H04; H04B; H04B10/00; H04B10/25; H04B10/2507; H04B10/2513; H04B10/2519

Claims Analysis

Total Claims: 12
Claim 1
Independent Claim 189 words
A method of providing adjustable magnitude linear dispersion of light, in which method light is caused to make a first reflection in a first optical waveguide (11, 71) provided with an associated first chirped Bragg grating reflector (13, 73) that exhibits chirp by virtue of having grating elements at an effective pitch which is a function of position along the grating, which effective pitch is the product of the physical pitch of the grating elements at any position along the length of the grating with the refractive index of the waveguide at that position; which method is characterised in that the light which makes said first reflection in said first waveguide additionally makes a second reflection in a second waveguide (12, 72) provided with an associated second chirped Bragg grating reflector (14, 74) whose chirp is such that said first and second Bragg grating reflectors have quadratic components of chirp of opposite sign and substantially matched modulus; and wherein the aggregate magnitude of linear dispersion afforded to light making said two reflections is adjustable by effecting a differential scaling of the effective pitches of the two Bragg grating reflectors.
Claim 2
Dependent Claim 24 words
A method as claimed in claim 1, wherein said differential scaling is effected by a differential axial straining of the two Bragg grating reflectors.
Claim 3
Dependent Claim 23 words
A method as claimed in claim 1, wherein said differential scaling is effected by a differential heating of the two Bragg grating reflectors.
Claim 4
Dependent Claim 20 words
A method as claimed in claim 1, 2 or 3, wherein the Bragg grating reflectors are sampled Bragg grating reflectors.
Claim 5
Independent Claim 188 words
A device exhibiting linear dispersion of adjustable magnitude, which device includes a first optical waveguide (11, 71) provided with an associated first chirped Bragg grating reflector (13, 73) that exhibits chirp by virtue of having grating elements at an effective pitch which is a function of position along the grating, which effective pitch is the product of the physical pitch of the grating elements at any position along the length of the grating with the refractive index of the waveguide at that position; which device is characterised in that it additionally includes a second optical waveguide (12, 72) provided with an associated second chirped Bragg grating reflector (14, 74) whose chirp is such that said first and second Bragg grating reflectors have quadratic components of chirp of opposite sign and substantially matched modulus, which first and second waveguides are arranged to define an optical transmission path in the device that includes a reflection in one grating and then in the other, and wherein the device includes means (15, 55, 65, 75, 76) to effect a differential scaling of the effective pitches of the two chirped Bragg grating reflectors.
Claim 6
Dependent Claim 17 words
A device as claimed in claim 5, wherein the Bragg grating reflectors are sampled Bragg grating reflectors.
Claim 7
Dependent Claim 19 words
A device as claimed in claim 5 or 6, wherein the first and second waveguides are optical fibre waveguides.
Claim 8
Dependent Claim 48 words
A device as claimed in claim 5, 6 or 7, wherein said means is a strain applicator (55, 65) mechanically coupled with the first waveguide and adapted to impart to the first waveguide, over the length of its Bragg grating, a substantially uniform axial strain of adjustable magnitude.
Claim 9
Dependent Claim 28 words
A device as claimed in claim 8, wherein the strain applicator (55) imparts adjustable magnitude tensile strain to the first waveguide over the length of its Bragg grating.
Claim 10
Dependent Claim 28 words
A device as claimed in claim 8, wherein the strain applicator (65) imparts adjustable magnitude compressive strain to the first waveguide over the length of its Bragg grating.
Claim 11
Dependent Claim 38 words
A device as claimed in claim 5, 6 or 7, wherein said means is a thermal regulator (75, 76) adapted to maintain a uniform temperature difference of adjustable magnitude between said first and second chirped Bragg reflection gratings.
Claim 12
Dependent Claim 17 words
A device as claimed in claim 11, wherein said first and second optical waveguides are polymer waveguides.

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