Fiber optic amplifier

• US 4,859,016 A
• Filed: 12/22/1987
• Issued: 08/22/1989
• Est. Priority Date: 11/25/1983
• Status: Expired due to Term

• Current Assignee: Board of Trustees of the Leland Stanford Junior University (Stanford Management Co.)
• Original Assignee: Board of Trustees of the Leland Stanford Junior University (Stanford Management Co.)
• Inventors: Digonnet, Michel J. F., Shaw, Herbert J.
• Primary Examiner(s): Lee, John D.
• Application Number:
  US07/137,870
• Time in Patent Office: 609 Days
• Field of Search: 350/96.15, 350/96.16, 372/6, 372/69, 372/94, 330/4, 330/4.3, 330/5, 330/84, 330/85
• US Class Current: 385/5
• CPC Class Codes: H01S 3/06787 Bidirectional amplifier
• CPC Class Codes: H01S 3/0933 of a semiconductor, e.g. light emitting diode
• CPC Class Codes: H01S 3/094003 the pumped medium being a fibre
• CPC Class Codes: H01S 3/094011 with bidirectional pumping, i.e. with injection of the pump light from both two ends of the fibre
• CPC Class Codes: H04B 10/291 in which processing or amplification is carried out without conversion of the main signal from optical form
• CPC Class Codes: H04B 10/2912 characterised by the medium used for amplification or processing
• CPC Class Codes: H04J 14/02 Wavelength-division multiplex systems

Abstract

An amplifier for use with fiber optic systems comprises a neodymium YAG crystal placed in series with a signal-carrying optical fiber. The ND:YAG crystal is supplied by the optical fiber with both the signal to be amplified, and pumping illumination. The pumping illumination is coupled onto the optical fiber by a multiplexing coupler which is used to combine the signal to be amplified and illumination from a pumping illumination source onto a single optical fiber. The pumping illumination inverts the neodymium ions within the ND:YAG crystal. The signal to be amplified propagates through this crystal to stimulate emission of coherent light from the neodymium ions, resulting in amplification of the signal. Because this arrangement permits the ND:YAG crystal to be end-pumped with pumping illumination, and because the length of the ND:YAG crystal may be substantially greater that the absorption length for the crystal at the wavelength of the pumping illumination, virtually all of the pumping illumination may be absorbed within the ND:YAG crystal and used for amplification of the signal carried by the optical fiber.

Claims

1. A fiber optic amplifier, comprising:

an optical fiber comprised of a material which will emit light in response to pumping;

a source of signals comprising light at a frequency of said emitted light;

a source of light for pumping said material; and

means for coupling both said signals and said light for pumping into an end of said optical fiber.

2. A fiber optic amplifier as defined in claim 1 in which said means for coupling comprises an optical coupler.

3. A fiber optic amplifier as defined in claim 2, wherein said optical coupler comprises a single-mode optical coupler.

4. A fiber optic amplifier as defined in claim 2 in which said optical coupler utilizes evanescent field coupling.

5. A fiber optic amplifier as defined in claim 3 in which said optical coupler provides different coupling coefficients for said signals and said light for pumping.

6. A fiber optic amplifier as defined in claim 5 in which said optical coupler has a coupling efficiency which is wavelength dependent and in which said signals and said light for pumping are at different wavelengths, yielding different coupling efficiencies for said signals and said light for pumping.

7. A fiber optic amplifier, comprising:

a fiber optic coupler including a pair of optical fibers juxtaposed to provide coupling of light at a first frequency between said fibers and to prohibit coupling of light at a second frequency between said fibers;

a source of pumping illumination coupled to a first end of one of said pair of fibers, said pumping illumination comprising light having said first frequency;

a source of a signal to be amplified, coupled to a first end of the other of said pair of fibers, said signal to be amplified comprising light having said second frequency; and

a laser fiber formed of material which will possess a laser transition at said second frequency of said signal to be amplified if said material is pumped with said pumping illumination, said laser fiber coupled at one end to a second end of said other of said pair of fibers.

8. A fiber optic amplifier as defined in claim 7 in which said fiber optical coupler has an effective interaction length at the juxtaposition of said optical fibers which is an even multiple of the coupling length of said fibers at said juxtaposition at a first wavelength corresponding to one of said first and second frequencies and an odd multiple of the coupling length of said fibers at said juxtaposition at a second wavelength corresponding to the other of said first and second frequencies.

9. A fiber optical amplifier as defined in claim 8, wherein said pair of optical fibers are laterally offset from one another to tune said coupler to provide said odd and even multiples.

10. A fiber optic amplifier as defined in claim 9, wherein said pair of optical fibers are arcuate and wherein the radius of said arcuate optical fibers is selected in accordance with the difference between said first and second wavelengths.

11. A fiber optic apparatus, comprising:

a source of pump light comprising light having a first wavelength;

an optical fiber comprising a laser material, said optical fiber emitting light at a second wavelength in response to pumping at said first wavelength; and

an optical coupler having an input port and an output port, said input port coupled to said pump source to receive light from said pump source, said output port coupled to said optical fiber for pumping said laser material, said coupler being highly wavelength discriminating so as to selectively couple one of said first and second wavelengths without substantial coupling of the other of said first and second wavelengths.

12. A method for amplifying a light signal carried by an optical fiber, comprising the steps of:

combining said light signal and pumping illumination on a single optical fiber; and

coupling said combined light signal and pumping illumination from said single optical fiber to one end of a fiber comprised of a material which will emit stimulated radiation at a wavelength of said light signal if pumped with said pumping illumination.

13. A method of amplifying a light signal as defined in claim 12, wherein said combining step comprises multiplexing said wavelength of said light signal and a wavelength of said pumping illumination in an optical coupler which is optically connected to said single optical fiber and which has a coupling efficiency which is wavelength dependent.

14. A method of amplifying a light signal as defined in claim 13, wherein said multiplexing step comprises:

juxtaposing a pair of optical fibers to provide an interaction length; and

applying said light signal to one of said fibers and said pumping illumination to the other of said fibers.

15. A method of amplifying a light signal as defined in claim 12, wherein the step of coupling comprises coupling said combined light signal and pumping illumination to a laser fiber having a diameter which is less than the absorption length of said laser fiber at said wavelength of said pumping illumination.