L-band amplification with detuned 980nm pump

• US 6,307,669 B1
• Filed: 10/12/1999
• Issued: 10/23/2001
• Est. Priority Date: 11/20/1998
• Status: Expired due to Term

• Current Assignee: II-VI Delaware, Inc. (Coherent Corp.)
• Original Assignee: Corning Incorporated
• Inventors: Flood, Felton A., Hall, Douglas W.
• Primary Examiner(s): Hellner, Mark
• Application Number:
  US09/417,262
• Time in Patent Office: 742 Days
• Field of Search: 359/341, 359/345, 359/341.3
• US Class Current: 359/341.3
• CPC Class Codes: H01S 2302/00 Amplification / lasing wavelength
• CPC Class Codes: H01S 2303/00 Pumping wavelength
• CPC Class Codes: H01S 3/067 Fibre lasers
• CPC Class Codes: H01S 3/094003 the pumped medium being a fibre
• CPC Class Codes: H01S 3/1603 rare earth
• CPC Class Codes: H01S 3/1608 erbium

Abstract

A method of operating an optical amplifier for improved gain and pump-to-signal conversion efficiency in a long wavelength spectral region (L-band) of the emission spectrum of a rare earth doped gain medium having a known pump absorption band involves the steps of providing an optical signal to the amplifier having a large-signal input power; and providing pumping light to the amplifier having a wavelength that is different from a center wavelength of the known pump absorption band for amplifying the optical signal. Signal gain and improved pump-to-signal conversion efficiency was demonstrated for an erbium L-band signal by detuning the pump between about ±0-30 nm on either side of the pump band center wavelength of 979-980 nm. An optical amplifier employing the described method is also disclosed.

Claims

1. A method of operating an L-Band optical amplifier for improved gain and pump-to-signal conversion efficiency in a long wavelength spectral region of the emission spectrum of a rare earth doped gain medium having a known pump absorption band, comprising the steps of:

a) providing an optical signal to the L-Band amplifier having a large-signal input power; and

b) providing pumping light to the L-Band amplifier having a wavelength that is different from a center wavelength of the pump absorption band for amplifying the optical signal, such that the L-Band amplifier'"'"'s gain is greater than gain at the center wavelength.

2. The method of claim 1, wherein the pumping light wavelength is in a range of ±

30 nm from the center wavelength of the known pump absorption band.

3. The method of claim 2, wherein the pumping light wavelength is in a range of ±

5 to 30 nm from the center wavelength of the known pump absorption band.

4. The method of claim 1, wherein the amplifier comprises a rare earth doped fiber gain medium.

5. The method of claim 4, wherein the rare earth doped fiber includes erbium as the punp light absorbing dopant.

6. The method of claim 4, wherein the amplifier'"'"'s rare earth doped fiber has a length greater than or equal to about 75 m.

7. The method of claim 2, wherein the center wavelength of the known pump absorption band is about 980 nm.

8. The method of claim 3, wherein the center wavelength of the known pump absorption band is about 980 nm.

9. The method of claim 1, wherein the L-band is from about 1565-1615 nm.

10. A method of operating an optical amplifier for improved gain and pump-to-signal conversion efficiency in a long wavelength spectral region (L-band) of the emission spectrum of a rare earth doped gain medium having a known pump absorption band, comprising the steps of:

a) providing an optical signal to the amplifier having a large-signal input power; and

b) providing pumping light to the amplifier having a wavelength that is detuned from a center wavelength of the known pump absorption band for amplifying the optical signal such that a value of the amplified signal power at any detuned pump wavelength is greater than the amplified signal power at the pump band center wavelength.

11. The method of claim 10, wherein the step of providing pumping light to the amplifier comprises detuning the pump light wavelength from the center wavelength in the range from about ±

5 to 30 nm.

12. The method of claim 10, wherein the center wavelength is about 980 nm.

13. The method of claim 10, wherein the L-band is from about 1565-1615 nm.

14. A method of operating an optical amplifier for improved gain and pump-to-signal conversion efficiency in a long wavelength spectral region (L-band) of the emission spectrum of a rare earth doped gain medium having a known pump absorption band, comprising the steps of:

a) providing an optical signal to the amplifier having a large-signal input power; and

b) providing pumping light to the amplifier having a wavelength that is detuined from a center wavelength of the known pump absorption band for amplifying the optical signal such that a measured value of ASE traveling counterdirectionally to the pump light is less at any detuned pump wavelength than the measured ASE at the pump band center wavelength.

15. The method of claim 14, wherein the step of providing pumping light to the amplifier comprises detuning the pump light wavelength from the center wavelength in the range from about ±

5 to 30 mn.

16. The method of claim 14, wherein the center wavelength is about 980 nm.

17. The method of claim 14, wherein the L-band is from about 1565-1615 nm.

18. An optical amplifier, comprising:

a rare earth doped gain stage having an emission spectrum and a known pump wavelength absorption band for amplifying an input signal having a wavelength in a long wavelength region of the emission spectrumn and a large input signal power;

a pump light source emitting an operating wavelength at a value different from a center wavelength of the pump absorption band, coupled to the gain stage;

wherein an amplified output signal has a signal power at said operating wavelength greater than an output signal when the operating wavelength is substantially the same as the center wavelength.

19. The amplifier of claim 18, wherein the long wavelength region of the emission spectrum is from about 1565-1615 nm, the center wavelength is about 980 nm, and the operating wavelength is in the range from about ±

5-30 nm from the center wavelength.