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US4416013A Expired / Lapsed US ⏱️ 0.0 years remaining

Distributed feedback laser employing the stark effect

Assignee: United States Department of the Navy
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Filing: 1981-11-30
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Granted: 1983-11-15
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Expires: 2001-11-30
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Abstract

Abstract An apparatus and method for producing distributed feedback in a laser. Electrodes, formed on opposite sides of a waveguide cavity, form a spatially periodic electric field in an amplification medium which exhibits the Stark effect. The field induces a modulation in the laser gain function of the medium which produces laser feedback.

Inventors

  • 👤 Mary S. Tobin

Bibliographic Details

Application Number —
Jurisdiction US
Data Source google_patents
Last Synchronized 2026-10-26 12:46
CPC Classifications
H; H01; H01S; H01S3/00; H01S3/05; H01S3/06; H01S3/063; H01S3/0632; H01S3/0635

Claims Analysis

Total Claims: 11
Claim 1
Independent Claim 64 words
A distributed feedback (DFB) laser comprising: an amplification medium for amplifying light at the lasing frequency, said amplification medium being of the type which exhibits the Stark effect; means for pumping said medium to generate a population inversion therein, and means for producing a spatially varying electric field in said amplification medium of sufficient intensity that an induced Stark effect will produce laser feedback.
Claim 2
Dependent Claim 64 words
A distributed feedback (DFB) laser comprising: an amplification medium for amplifying light at the lasing frequency, said amplification medium being of the type which exhibits the Stark effect; means for pumping said medium to generate a population inversion therein, and means for producing a spatially varying electric field in said amplification medium of sufficient intensity that an induced Stark effect will produce laser feedback.
Claim 3
Dependent Claim 14 words
The DFB laser recited in claim 1, wherein: said amplification medium is a gas.
Claim 4
Dependent Claim 19 words
The DFB laser recited in claim 2, further comprising: a hollow waveguide within which said amplification medium is confined.
Claim 5
Dependent Claim 36 words
The DFB laser recited in claim 3, wherein said electric-field-producing means comprises: electrode means positioned inside of said waveguide means for producing said electric field within said amplification medium; and means for energizing said electrode means.
Claim 6
Dependent Claim 44 words
The DFB laser recited in claim 4, wherein said electrode means comprises: a plurality of metal strips located on opposing interior surfaces of said waveguide and spaced from each other in a direction substantially parallel to the direction of light propogation through said waveguide.
Claim 7
Dependent Claim 35 words
The DFB laser recited in claim 5, wherein: said metal strips are separated by a distance equal to 1/2 nλ, where n is a positive integer and λ is the wavelength of the lasing light.
Claim 8
Independent Claim 55 words
A method of lasing comprising: inducing a population inversion in an amplification medium for amplifying light at the lasing frequency, said amplification medium being of the type which exhibits the Stark effect; and producing a spatially varying electric field in said amplification medium of sufficient intensity that an induced Stark effect will produce laser feedback.
Claim 9
Independent Claim 55 words
A method of lasing comprising: inducing a population inversion in an amplification medium for amplifying light at the lasing frequency, said amplification medium being of the type which exhibits the Stark effect; and producing a spatially varying electric field in said amplification medium of sufficient intensity that an induced Stark effect will produce laser feedback.
Claim 10
Dependent Claim 13 words
The method recited in claim 7, wherein: said amplification medium is a gas.
Claim 11
Dependent Claim 56 words
The method recited in claim 7 or 8, wherein: said electric field is periodically varying in a direction substantially parallel to the propogation of laser light in said amplification medium and wherein the period of the spatial variation is 1/2 nλ, where n is a positive integer and λ is the wavelength of the lasing light.

References Cited (Backward Citations)

US3760292A Cited
US3884549A Cited
US3970959A Cited
US3939439A Cited
US4002998A Cited
US4087764A Cited

USPTO Annuity & Maintenance Windows

Annuity Stage Window Opens Payment Deadline Surcharge Period Until Estimated Fee Status
3.5 Years (Year 4) 1986-11-14 1987-05-16 1987-11-15 $2000.00 Window Closed / Lapsed
7.5 Years (Year 8) 1990-11-14 1991-05-16 1991-11-15 $3760.00 Window Closed / Lapsed
11.5 Years (Year 12) 1994-11-14 1995-05-16 1995-11-15 $7700.00 Window Closed / Lapsed

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