US4096446A
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Distributed feedback devices with perturbations deviating from uniformity for removing mode degeneracy
Assignee: AT&T Inc
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Filing: 1976-02-02
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Granted: 1978-06-20
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Expires: 1996-02-02
Abstract
Abstract Distributed feedback devices such as distributed feedback lasers are modified by introduction of a central coupling strength discontinuity or other deviation from uniform nature of the distributed perturbations, in order to promote the transmission of oscillation of a single mode in preference over the nearest redundant modes. The class of deviations from uniform coupling strength may be mathematically termed antisymmetric deviations, because they are deviations about the midpoint of the perturbation pattern which result in a distinction of effect of the two halves of the pattern, taking either half as a reference pattern by itself.
Inventors
- 👤 Herman Anton Haus
- 👤 Charles Vernon Shank
Bibliographic Details
Application Number
—
Jurisdiction
US
Data Source
google_patents
Last Synchronized
2026-10-23 12:15
CPC Classifications
H; H01; H01S; H01S3/00; H01S3/05; H01S3/06; H01S3/063; H01S3/0632; H01S3/0635; H01S5/00; H01S5/10; H01S5/12; H01S5/124
Claims Analysis
Total Claims: 6
Claim 1
Independent Claim
149 words
An optical frequency device for the stimulated emission of radiation comprising an active medium and a feedback mechanism, means for creating a population inversion in said active medium, said feedback mechanism comprising perturbations in the transmission characteristics of the medium substantially continuously along the length thereof, said perturbations having a feedback parameter, κ, and a spatial periodicity of λ o /2 where λ o is the wavelength in the medium of an optical wave at the Bragg frequency, said perturbations departing from uniformity in a step-wise change about the midpoint of the length of the medium sufficiently to produce an antisymmetric variation in the feedback parameter, κ, said step-wise change in perturbations including an extra quarter-wavelength space between two central perturbations, where the wavelength is the wavelength of the optical wave, thereby promoting the amplification of a single mode at λ o over the amplification of the adjacent modes.
Claim 2
Dependent Claim
149 words
An optical frequency device for the stimulated emission of radiation comprising an active medium and a feedback mechanism, means for creating a population inversion in said active medium, said feedback mechanism comprising perturbations in the transmission characteristics of the medium substantially continuously along the length thereof, said perturbations having a feedback parameter, κ, and a spatial periodicity of λ o /2 where λ o is the wavelength in the medium of an optical wave at the Bragg frequency, said perturbations departing from uniformity in a step-wise change about the midpoint of the length of the medium sufficiently to produce an antisymmetric variation in the feedback parameter, κ, said step-wise change in perturbations including an extra quarter-wavelength space between two central perturbations, where the wavelength is the wavelength of the optical wave, thereby promoting the amplification of a single mode at λ o over the amplification of the adjacent modes.
Claim 3
Dependent Claim
156 words
An optical frequency device for the stimulated emission of radiation comprising an active medium and a feedback mechanism, means for creating a population inversion in said active medium, said feedback mechanism comprising perturbations in the transmission characteristics of the medium substantially continuously along the length thereof, said perturbations having a feedback parameter, κ, and a spatial periodicity of λ o /2 where λ o is the wavelength in the medium of an optical wave at the Bragg frequency, said perturbations departing from uniformity via an antisymmetrical taper of coupling strength about the midpoint of the length of the medium sufficiently to produce an antisymmetric variation in the feedback parameter, κ, said antisymmetrical taper of coupling strength conforming to a variation equal to a sine wave variation multiplied by a straight line variation passing through zero at the midpoint, thereby promoting the amplification of a single mode at λ o over the amplification of the adjacent modes.
Claim 4
Dependent Claim
156 words
An optical frequency device for the stimulated emission of radiation comprising an active medium and a feedback mechanism, means for creating a population inversion in said active medium, said feedback mechanism comprising perturbations in the transmission characteristics of the medium substantially continuously along the length thereof, said perturbations having a feedback parameter, κ, and a spatial periodicity of λ o /2 where λ o is the wavelength in the medium of an optical wave at the Bragg frequency, said perturbations departing from uniformity via an antisymmetrical taper of coupling strength about the midpoint of the length of the medium sufficiently to produce an antisymmetric variation in the feedback parameter, κ, said antisymmetrical taper of coupling strength conforming to a variation equal to a sine wave variation multiplied by a straight line variation passing through zero at the midpoint, thereby promoting the amplification of a single mode at λ o over the amplification of the adjacent modes.
Claim 5
Dependent Claim
152 words
An optical frequency device for the stimulated emission of radiation comprising an active medium and a feedback mechanism, means for creating a population inversion in said active medium, said feedback mechanism comprising perturbations in the transmission characteristics of the medium substantially continuously along the length thereof, said perturbations having a feedback parameter, κ, and a spatial periodicity of λ o /2 where λ o is the wavelength in the medium of an optical wave at the Bragg frequency, said perturbations comprising metallic means for periodically loading the active medium, the perturbations departing from uniformity via a central step change about the midpoint of the length of the medium sufficiently to produce an antisymmetric variation in the feedback parameter, κ, said central step change being an increase in metallic loading width of about 50 percent, thereby promoting the amplification of a single mode at λ o over the amplification of the adjacent modes.
Claim 6
Dependent Claim
152 words
An optical frequency device for the stimulated emission of radiation comprising an active medium and a feedback mechanism, means for creating a population inversion in said active medium, said feedback mechanism comprising perturbations in the transmission characteristics of the medium substantially continuously along the length thereof, said perturbations having a feedback parameter, κ, and a spatial periodicity of λ o /2 where λ o is the wavelength in the medium of an optical wave at the Bragg frequency, said perturbations comprising metallic means for periodically loading the active medium, the perturbations departing from uniformity via a central step change about the midpoint of the length of the medium sufficiently to produce an antisymmetric variation in the feedback parameter, κ, said central step change being an increase in metallic loading width of about 50 percent, thereby promoting the amplification of a single mode at λ o over the amplification of the adjacent modes.
References Cited (Backward Citations)
USPTO Annuity & Maintenance Windows
| Annuity Stage | Window Opens | Payment Deadline | Surcharge Period Until | Estimated Fee | Status |
|---|---|---|---|---|---|
| 3.5 Years (Year 4) | 1981-06-19 | 1981-12-19 | 1982-06-20 | $2000.00 | Window Closed / Lapsed |
| 7.5 Years (Year 8) | 1985-06-19 | 1985-12-19 | 1986-06-20 | $3760.00 | Window Closed / Lapsed |
| 11.5 Years (Year 12) | 1989-06-19 | 1989-12-19 | 1990-06-20 | $7700.00 | Window Closed / Lapsed |