Optical fiber amplifier and laser with flattened gain slope
First Claim
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1. 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.
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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.
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Citations
13 Claims
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1. A fiber optical amplifier having a flattened gain slope comprising:
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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. - View Dependent Claims (2, 3, 4)
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5. An optical fiber communication system comprising:
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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. - View Dependent Claims (6)
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7. An optical fiber laser having a flattened gain slope for outputting an optical carrier comprising:
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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. - View Dependent Claims (8, 9, 10)
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11. A method for flattening the gain slope of an optical fiber amplifier comprising the steps of:
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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. - View Dependent Claims (12, 13)
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Specification