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US5271024A Expired / Lapsed US ⏱️ 0.0 years remaining

Optical fiber amplifier and laser with flattened gain slope

Assignee: Ciena Corp
•
Filing: 1992-07-27
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Granted: 1993-12-14
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Expires: 2012-07-27
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Abstract

Abstract An in-fiber Bragg grating is used to flatten the gain slope of a fiber optical amplifier or optical fiber laser. The grating can be formed using photorefractive techniques, and is placed within a guided wave portion of a doped optical fiber. The grating is oriented at a nonperpendicular angle with respect to a longitudinal axis of the fiber, and has an interaction wavelength that is selected to flatten the gain slope of the device by diverting excess spontaneous emission therefrom. The interaction wavelength is preferably selected to correspond to a wavelength at or near that at which the spontaneous emission produced by the fiber peaks. <IMAGE>

Inventors

  • 👤 David R. Huber

Bibliographic Details

Application Number —
Jurisdiction US
Data Source google_patents
Last Synchronized 2026-10-26 16:37
CPC Classifications
H; H01; H01S; H01S3/00; H01S3/05; H01S3/06; H01S3/063; H01S3/067; H01S2301/00; H01S2301/04; H01S3/0675; H01S3/06754

Claims Analysis

Total Claims: 17
Claim 1
Independent Claim 110 words
A fiber optical amplifier having a flattened gain slope comprising: a length of doped optical fiber for amplifying an optical signal therein when pumped with a source of pump energy, said fiber producing spontaneous emission when pumped; and a Bragg grating within a guided wave portion of said doped optical fiber, said grating oriented at a nonperpendicular angle θ with respect to a longitudinal axis of said fiber and having an interaction wavelength selected to flatten the gain slope of the amplifier by diverting excess spontaneous emission from said fiber; where: ##EQU1## and Δ is the difference in index of refraction between a core and a cladding of said fiber.
Claim 2
Dependent Claim 110 words
A fiber optical amplifier having a flattened gain slope comprising: a length of doped optical fiber for amplifying an optical signal therein when pumped with a source of pump energy, said fiber producing spontaneous emission when pumped; and a Bragg grating within a guided wave portion of said doped optical fiber, said grating oriented at a nonperpendicular angle θ with respect to a longitudinal axis of said fiber and having an interaction wavelength selected to flatten the gain slope of the amplifier by diverting excess spontaneous emission from said fiber; where: ##EQU1## and Δ is the difference in index of refraction between a core and a cladding of said fiber.
Claim 3
Dependent Claim 33 words
An amplifier in accordance with claim 1 wherein said interaction wavelength is selected to correspond to a wavelength at or near the wavelength at which the spontaneous emission produced by said fiber peaks.
Claim 4
Dependent Claim 20 words
An amplifier in accordance with claim 2 wherein said grating is a photoinduced Bragg grating within said guided wave portion.
Claim 5
Dependent Claim 22 words
An amplifier in accordance with claim 1 wherein said fiber is an erbium-doped fiber and said interaction wavelength is about 1532 nm.
Claim 6
Dependent Claim 117 words
An optical fiber communication system comprising: an optical transmission path for carrying a plurality of optical signals to be distributed from a headend; and a plurality of optical amplifiers cascaded in series along said path for amplifying said optical signals, said optical amplifiers each comprising: a length of doped optical fiber for amplifying an optical signal therein when pumped with a source of pump energy; and a Bragg grating within a guided wave portion of said doped optical fiber, said grating oriented at a nonperpendicular angle with respect to a longitudinal axis of said fiber and having an interaction wavelength selected to flatten the gain slope of the amplifier by diverting excess spontaneous emission form said fiber.
Claim 7
Dependent Claim 117 words
An optical fiber communication system comprising: an optical transmission path for carrying a plurality of optical signals to be distributed from a headend; and a plurality of optical amplifiers cascaded in series along said path for amplifying said optical signals, said optical amplifiers each comprising: a length of doped optical fiber for amplifying an optical signal therein when pumped with a source of pump energy; and a Bragg grating within a guided wave portion of said doped optical fiber, said grating oriented at a nonperpendicular angle with respect to a longitudinal axis of said fiber and having an interaction wavelength selected to flatten the gain slope of the amplifier by diverting excess spontaneous emission form said fiber.
Claim 8
Dependent Claim 27 words
A communication system in accordance with claim 5 wherein said optical amplifiers are erbium fiber amplifiers and the interaction wavelength of said gratings is about 1532 nm.
Claim 9
Dependent Claim 130 words
An optical fiber laser having a flattened gain slope for outputting an optical carrier comprising: a length of rare earth doped optical fiber for providing gain when pumped with a source of pump energy, said fiber producing spontaneous emission when pumped; a laser cavity incorporating said doped optical fiber and having an output for said optical carrier; and a Bragg grating within a guided wave portion of said doped optical fiber, said grating oriented at a nonperpendicular angle θ with respect to a longitudinal axis of said fiber and having an interaction wavelength selected to flatten the gain slope of the laser by diverting excess spontaneous emission from said fiber; where ##EQU2## and Δ is the difference in index of refraction between a core and a cladding of said fiber.
Claim 10
Dependent Claim 130 words
An optical fiber laser having a flattened gain slope for outputting an optical carrier comprising: a length of rare earth doped optical fiber for providing gain when pumped with a source of pump energy, said fiber producing spontaneous emission when pumped; a laser cavity incorporating said doped optical fiber and having an output for said optical carrier; and a Bragg grating within a guided wave portion of said doped optical fiber, said grating oriented at a nonperpendicular angle θ with respect to a longitudinal axis of said fiber and having an interaction wavelength selected to flatten the gain slope of the laser by diverting excess spontaneous emission from said fiber; where ##EQU2## and Δ is the difference in index of refraction between a core and a cladding of said fiber.
Claim 11
Dependent Claim 33 words
A laser in accordance with claim 7 wherein said interaction wavelength is selected to correspond to a wavelength at or near the wavelength at which the spontaneous emission produced by said fiber peaks.
Claim 12
Dependent Claim 20 words
A laser in accordance with claim 8 wherein said grating is a photoinduced Bragg grating within said guided wave portion.
Claim 13
Dependent Claim 22 words
A laser in accordance with claim 7 wherein said fiber is an erbium-doped fiber and said interaction wavelength is about 1532 nm.
Claim 14
Independent Claim 126 words
A method for flattening the gain slope of an optical fiber amplifier comprising the steps of: providing a length of doped optical fiber for amplifying an optical signal therein when pumped with a source of pump energy, said fiber producing spontaneous emission when pumped; and diverting excess spontaneous emission from said fiber using a Bragg grating situated within a guided wave portion of the fiber; wherein said grating has an interaction wavelength that is selected to correspond to a wavelength at or near the wavelength at which the spontaneous emission produced by said fiber peaks; and said grating is oriented at a nonperpendicular angle with respect to a longitudinal axis of said fiber to provide an exit path from the fiber for said excess spontaneous emission.
Claim 15
Independent Claim 126 words
A method for flattening the gain slope of an optical fiber amplifier comprising the steps of: providing a length of doped optical fiber for amplifying an optical signal therein when pumped with a source of pump energy, said fiber producing spontaneous emission when pumped; and diverting excess spontaneous emission from said fiber using a Bragg grating situated within a guided wave portion of the fiber; wherein said grating has an interaction wavelength that is selected to correspond to a wavelength at or near the wavelength at which the spontaneous emission produced by said fiber peaks; and said grating is oriented at a nonperpendicular angle with respect to a longitudinal axis of said fiber to provide an exit path from the fiber for said excess spontaneous emission.
Claim 16
Dependent Claim 35 words
A method in accordance with claim 11 wherein said nonperpendicular angle is an angle θ where: ##EQU3## and Δ is the difference in index of refraction between a core and a cladding of said fiber.
Claim 17
Dependent Claim 22 words
A method in accordance with claim 11 wherein said fiber is an erbium-doped fiber and said interaction wavelength is about 1532 nm.

References Cited (Backward Citations)

US4786132A Cited
US4911516A Cited
US5115338A Cited
US5134620A Cited
US5151908A Cited
US5166940A Cited
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USPTO Annuity & Maintenance Windows

Annuity Stage Window Opens Payment Deadline Surcharge Period Until Estimated Fee Status
3.5 Years (Year 4) 1996-12-13 1997-06-14 1997-12-14 $2000.00 Window Closed / Lapsed
7.5 Years (Year 8) 2000-12-13 2001-06-14 2001-12-14 $3760.00 Window Closed / Lapsed
11.5 Years (Year 12) 2004-12-13 2005-06-14 2005-12-14 $7700.00 Window Closed / Lapsed

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