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US4515429A Expired / Lapsed US ⏱️ 0.0 years remaining

Nonlinear and bistable optical waveguide devices

Assignee: Nokia Bell Labs
•
Filing: 1980-05-27
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Granted: 1985-05-07
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Expires: 2000-05-27
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Abstract

Abstract Several types of nonlinear characteristics are provided in an optical device wherein at least two optical materials are constructed to provide a waveguide structure. At least one of the materials has a dominant nonlinear characteristic over the length of the waveguide that is commonly referred to as the Kerr effect. The index of refraction in this material is a function of the light intensity in the waveguide. By selecting materials that provide either positive or negative Kerr coefficients, and by constructing the device with the nonlinear material either as the core or as the cladding layer, power output versus input characteristics that exhibit both limiting and amplification can be provided. A bistable characteristic is provided in one of the embodiments by terminating the waveguide structure with a mirror. Specific embodiments using carbon disulfide and polydiacetylene as the nonlinear materials are disclosed.

Inventors

  • 👤 Peter W. Smith
  • 👤 Walter J. Tomlinson, III

Bibliographic Details

Application Number —
Jurisdiction US
Data Source google_patents
Last Synchronized 2026-10-23 04:12
CPC Classifications
G; G02; G02F; G02F1/00; G02F1/35; G02F1/3511; G02F1/3515; G02F3/00; G02F3/02; G02F3/024

Claims Analysis

Total Claims: 3
Claim 1
Independent Claim 168 words
A nonlinear optical device comprising at least two optical materials structurally arranged to provide an optical waveguide having a predetermined length, L, one of said two materials being bounded by the other of said two materials, at least one of said two materials having a dominant nonlinear effect over the length, L, of said waveguide characterized in that said at least one of said two materials has an index of refraction which changes by n 2 I with changes in light intensity, I, where n 2 is defined as a Kerr coefficient, and the length, L, of said waveguide is less than L R , the threshold length for stimulated Raman scattering, which is approximately 16/gI c , where I c is the light intensity at which the index of refraction of said at least one of said two materials equals the index of refraction of the other of said two materials, and g is the peak Raman gain for said at least one of said two materials.
Claim 2
Dependent Claim 168 words
A nonlinear optical device comprising at least two optical materials structurally arranged to provide an optical waveguide having a predetermined length, L, one of said two materials being bounded by the other of said two materials, at least one of said two materials having a dominant nonlinear effect over the length, L, of said waveguide characterized in that said at least one of said two materials has an index of refraction which changes by n 2 I with changes in light intensity, I, where n 2 is defined as a Kerr coefficient, and the length, L, of said waveguide is less than L R , the threshold length for stimulated Raman scattering, which is approximately 16/gI c , where I c is the light intensity at which the index of refraction of said at least one of said two materials equals the index of refraction of the other of said two materials, and g is the peak Raman gain for said at least one of said two materials.
Claim 3
Dependent Claim 26 words
A nonlinear optical device as defined in claim 1 where the optical device is further characterized in that one of said two materials is carbon disulfide.

References Cited (Backward Citations)

US4382660A Cited
US4196396A Cited
US4236785A Cited
US4431263A Cited

USPTO Annuity & Maintenance Windows

Annuity Stage Window Opens Payment Deadline Surcharge Period Until Estimated Fee Status
3.5 Years (Year 4) 1988-05-06 1988-11-05 1989-05-07 $2000.00 Window Closed / Lapsed
7.5 Years (Year 8) 1992-05-06 1992-11-05 1993-05-07 $3760.00 Window Closed / Lapsed
11.5 Years (Year 12) 1996-05-06 1996-11-05 1997-05-07 $7700.00 Window Closed / Lapsed

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