Optical amplifier, optical amplifying system, wavelength converter, optical amplification method, and optical communication system

Patent metadata

Field	Value
Publication number	US-9270076-B2
Application number	US-201314018225-A
Country	US
Kind code	B2
Filing date	Sep 4, 2013
Priority date	Mar 4, 2011
Publication date	Feb 23, 2016
Grant date	Feb 23, 2016

Abstract

An optical amplifier includes an optical gain fiber into which signal light and pump light are input and at least one relative phase shifter is inserted. Preferably, the relative phase shifter is inserted so that the relative phase in the lengthwise direction of the optical gain fiber falls within a predetermined range containing 0.5π. Preferably, the optical gain fiber is a highly non-linear optical fiber having a non-linearity constant of at least 10/W/km. Preferably, the dispersion of the optical gain fiber is within the range from −1 ps/nm/km to 1 ps/nm/km in an amplification band. Preferably, the absolute value of the dispersion slope of the optical gain fiber at a zero dispersion wavelength is no greater than 0.05 ps/nm 2 /km.

First claim

What is claimed is:

1. An optical parametric amplifier comprising:
two or more optical gain fibers; and
at least one relative phase shifter being inserted between the optical gain fibers and shifting a phase of a light at and near wavelength of a pump light without substantially shifting a phase of a signal light, both the pump light and the signal light being inputted to the optical parametric amplifier.

2. The optical parametric amplifier according to claim 1 , wherein the relative phase shifter is inserted so that relative phase falls within a predetermined range including 0.5π in a lengthwise direction of the optical gain fibers.

3. The optical parametric amplifier according to claim 1 , wherein each of the optical gain fibers is a highly nonlinear optical fiber of which nonlinear constant is equal to or greater than 10 [1/W/km].

4. The optical parametric amplifier according to claim 1 , wherein a dispersion of each of the optical gain fibers is within a range from −1 [ps/nm/km] to 1 [ps/nm/km] in an amplification band.

5. The optical parametric amplifier according to claim 1 , wherein an absolute value of dispersion slope of each of the optical gain fibers at a zero-dispersion wavelength is equal to or smaller than 0.05 [ps/nm 2 /km].

6. The optical parametric amplifier according to claim 1 , wherein the relative phase shifter is an optical fiber.

7. The optical parametric amplifier according to claim 6 , wherein a relative phase shift value is adjusted based on a length of the optical fiber.

8. The optical parametric amplifier according to claim 1 , wherein the relative phase shifter is a dielectric multilayer film filter.

9. The optical parametric amplifier according to claim 8 , wherein a relative phase shift value is adjusted based on tilt of the dielectric multilayer film filter.

10. The optical parametric amplifier according to claim 8 , wherein the dielectric multilayer film filter is an all-pass filter which transmits all wavelengths therethrough.

11. The optical parametric amplifier according to claim 1 , wherein the relative phase shifter is a device in which a dielectric multilayer film filter and two optical fibers with collimator lenses corresponding to input and output are assembled.

12. The optical parametric amplifier according to claim 11 , wherein the dielectric multilayer film filter is of a reflection type, light inputted into the optical fiber is collimated by the collimator lens at an end of the optical fiber, outputted to a space, and made incident to the dielectric multilayer film filter, the dielectric multilayer film filter reflects light so that light is incident into another optical fiber with the collimator lens, and light is outputted from the another optical fiber with the collimator lens.

13. The optical parametric amplifier according to claim 12 , wherein in a wavelength range of the signal light to be amplified and a wavelength range of idler light to be generated corresponding to wavelength of the pump light and the signal light, dispersion of the optical fiber with the collimator lens used in the device is within a range from −1 [ps/nm/km] to 1 [ps/nm/km].

14. The optical parametric amplifier according to claim 1 , wherein the relative phase shifter is a fiber Bragg grating.

15. The optical parametric amplifier according to claim 14 , wherein relative phase shift value is adjusted based on a magnitude of transmission loss or a magnitude of reflectance at Bragg wavelength of the fiber Bragg grating.

16. The optical parametric amplifier according to claim 14 , wherein a pumping wavelength is set outside a 3 dB wavelength band of transmission loss having a central wavelength at Bragg wavelength of the fiber Bragg grating, and phase of the pump light is shifted.

17. The optical parametric amplifier according to claim 16 , wherein a wavelength of the pump light is set at a longer wavelength side relative to Bragg wavelength of the fiber Bragg grating, and phase of the pump light is shifted.

18. The optical parametric amplifier according to claim 14 , wherein in a wavelength range of a signal light to be amplified and a wavelength range of idler light to be generated corresponding to a wavelength of the pump light and the signal light, dispersion of the fiber Bragg grating is within a range from −1 [ps/nm/km] to 1 [ps/nm/km].

19. The optical parametric amplifier according to claim 1 , wherein the relative phase shifter is a device which relaxes change, by temperature, in Bragg wavelength of a fiber Bragg grating.

20. The optical parametric amplifier according to claim 19 , wherein the relative phase shifter changes Bragg wavelength by stretching or shortening a fiber Bragg grating and adjusts phase-shift value at pumping wavelength.

21. The optical parametric amplifier according to claim 14 , wherein an optical isolator is disposed at a stage prior to the fiber Bragg grating.

22. The optical parametric amplifier according to claim 14 , wherein an optical isolator is disposed at a stage subsequent to the fiber Bragg grating.

23. The optical parametric amplifier according to claim 21 , wherein in a wavelength range of a signal light to be amplified and a wavelength range of idler light to be generated corresponding to a wavelength of the pump light and the signal light, a dispersion of an optical fiber which constitutes the disposed optical isolator module is within a range from −1 [ps/nm/km] to 1 [ps/nm/km].

24. The optical parametric amplifier according to claim 22 , wherein in a wavelength range of a signal light to be amplified and a wavelength range of idler light to be generated corresponding to a wavelength of the pump light and the signal light, a dispersion of an optical fiber which constitutes the disposed optical isolator module is within a range from −1 [ps/nm/km] to 1 [ps/nm/km].

25. The optical parametric amplifier according to claim 1 , wherein the relative phase shifter is a PLC.

26. The optical parametric amplifier according to claim 25 , wherein an optical circuit in the PLC is constituted by a circuit separating light of wavelength of pump light from light of wavelength other than the wavelength of the pump light, a circuit shifting phase of pump light, and a circuit coupling wavelength of pump light and light of wavelength other than the wavelength of the pump light.

27. The optical parametric amplifier according to claim 25 , wherein relative phase shift value is adjusted by using thermooptical effect of the PLC.

28. The optical parametric amplifier according to claim 25 , wherein temperature of the PLC is maintained constant by a temperature control element using Peltier element.

29. The optical parametric amplifier according to claim 25 , wherein the PLC is athermalized so that there is not change in operation wavelength by temperature change.

30. The optical parametric amplifier according to claim 1 , wherein the relative phase shifter is a device using a grating of a spatial optical system and an LCOS.

31. The optical parametric amplifier according to claim 1 , wherein the relative phase shifter shifts phase of the pump light by making use of a phase-adjusting function of an LCOS so that gain characteristics of the optical amplifier become flat.

32. The optical parametric amplifier according to claim 1 , wherein each of the optical g

Assignees

• Furukawa Electric Co Ltd

Inventors

• Takasaka Shigehiro
• Mimura Yu

Classifications

• H01S3/302

  in an optical fibre · CPC title

• H04B10/294 Primary

  in a multiwavelength system, e.g. gain equalisation · CPC title

• H01S2301/04

  Gain spectral shaping, flattening · CPC title

• H01S3/06725

  Fibre characterized by a specific dispersion, e.g. for pulse shaping in soliton lasers or for dispersion compensating [DCF] · CPC title

• H01S3/06754

  Fibre amplifiers (H01S3/06708 takes precedence) · CPC title