Optical fiber amplifier and laser with flattened gain slope

• US 5,271,024 A
• Filed: 07/27/1992
• Issued: 12/14/1993
• Est. Priority Date: 07/27/1992
• Status: Expired due to Term

• Current Assignee: Level 3 Communications LLC (Lumen Technologies, Inc.)
• Original Assignee: General Instrument Corporation (CommScope Holding Company, Inc.)
• Inventors: Huber, David R.
• Primary Examiner(s): FONT, FRANK G
• Application Number:
  US07/919,921
• Time in Patent Office: 505 Days
• Field of Search: 372/6, 372/18, 372/19, 372/98, 372/102, 385/31, 385/37, 359/341, 359/342, 359/124, 359/127, 359/130
• US Class Current: 372/6
• CPC Class Codes: H01S 2301/04 Gain spectral shaping, flattening
• CPC Class Codes: H01S 3/067 Fibre lasers
• CPC Class Codes: H01S 3/0675 Resonators including a grating structure, e.g. distributed Bragg reflectors [DBR] or distributed feedback [DFB] fibre lasers
• CPC Class Codes: H01S 3/06754 Fibre amplifiers H01S3/06708 takes precedence

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.

Claims

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.

2. 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.

3. An amplifier in accordance with claim 2 wherein said grating is a photoinduced Bragg grating within said guided wave portion.

4. An amplifier in accordance with claim 1 wherein said fiber is an erbium-doped fiber and said interaction wavelength is about 1532 nm.

5. 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.

6. 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.

7. 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.

8. 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.

9. A laser in accordance with claim 8 wherein said grating is a photoinduced Bragg grating within said guided wave portion.

10. A laser in accordance with claim 7 wherein said fiber is an erbium-doped fiber and said interaction wavelength is about 1532 nm.

11. 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.

12. 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.

13. A method in accordance with claim 11 wherein said fiber is an erbium-doped fiber and said interaction wavelength is about 1532 nm.