Optical fiber laser or amplifier including high reflectivity gratings

• US 5,323,404 A
• Filed: 11/02/1993
• Issued: 06/21/1994
• Est. Priority Date: 11/02/1993
• Status: Expired due to Term

• Current Assignee: Furukawa Electric North America Incorporated (Furukawa Electric Company Limited)
• Original Assignee: AT&T, Inc.
• Inventors: Grubb, Stephen G.
• Primary Examiner(s): Healy, Brian
• Application Number:
  US08/145,933
• Time in Patent Office: 231 Days
• Field of Search: 372/3, 372/6, 372/69, 372/70, 372/72, 372/92, 372/99, 372/102, 359/333, 359/334, 359/341, 359/345, 359/346, 385/31, 385/37
• US Class Current: 372/6
• 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 3/08086 Multiple-wavelength emission
• CPC Class Codes: H01S 3/302 in an optical fibre

Abstract

Novel optical fiber devices (amplifiers and lasers) are disclosed. The devices comprise one or more optical "cavities", depending on the type of device. The cavities typically are formed by means of in-line refractive index gratings in a length of silica-based optical fiber. The gratings typically have peak reflectivity of at least 98%. Use of such cavities enables CW pumping of the devices, making the devices suitable for use in optical fiber communication systems. In an exemplary embodiment the device is a Raman amplifier for 1.3 μm signal radiation, and in another exemplary embodiment the device is a Raman laser having an output suitable for pumping an Er-doped fiber amplifier. An exemplary pump radiation source is a laser diode-pumped CW Nd:YAG laser.

Claims

1. Apparatus comprising an optical device that comprises

a) a length of optical fiber;

b) means for introducing pump radiation of wavelength λ

_p into said length of optical fiber;

c) spaced-apart reflector means that define an optical cavity for radiation of a predetermined wavelength, with the cavity comprising at least a portion of the length of optical fiber;

wherein the device is adapted for emission of radiation of wavelength λ

_s ≠

λ

_p from said length of optical fiber;

characterized in that

d) the pump radiation is continuous wave radiation;

e) the reflector means comprise at least two pairs of reflectors, associated with each of said reflectors is a center wavelength of a reflection band, the two reflectors of a given pair have essentially the same center wavelength and are spaced apart, such that the reflectors of the given pair define an optical cavity for radiation of wavelength equal to said center wavelength of the reflectors of the given pair; and

f) associated with said given optical cavity is an added round trip loss for radiation of wavelength equal to said center wavelength, said added round trip loss being at most 1.5 dB.

2. Apparatus according to claim 1, wherein said optical fiber is silica-based optical fiber, and wherein the two reflectors of at least one of said pairs of reflectors are in-line optical fiber refractive index gratings in said optical fiber, with each of said two refractive index gratings having a peak reflectivity of at least 98%.

3. Apparatus according to claim 1, wherein the optical device is a Raman laser or a Brillouin laser, and wherein

i) λ

_s is greater than λ

_p ;

ii) said center wavelengths are λ

_i, where i=1, . . . n, with n being an integer equal to or greater than 2;

iii) said gratings are selected such that λ

_i =λ

_i-1 +Δ

λ

_i, where Δ

λ

_i is a length within a Stokes band associated with the optical fiber, and λ

_i-1 =λ

_p if i=1; and

iv) λ

_n ≦

λ

_s.

4. Apparatus according to claim 3, wherein the device is a Raman laser, the optical fiber is silica-based optical fiber, λ

_p is about 1.06 μ

m, λ

_s is about 1.5 μ

m, Δ

λ

_i corresponds to a Stokes shift of about 450 cm^-1, and n is greater than 2.

5. Apparatus according to claim 1, wherein the optical device is a Raman or Brillouin amplifier for radiation of wavelength λ

_s, and wherein

i) λ

_s is greater than λ

_p ;

ii) said center wavelengths are λ

_i, where i=1, . . . n, with n being an integer equal to or greater than 2;

iii) said gratings are selected such that λ

_i =λ

_i-1 +Δ

λ

_i, where Δ

λ

_i is a length within a Stokes band associated with the optical fiber; and

λ

_i-1 =λ

_p if i=1; and

iv) λ

_s is greater than λ

_n.

6. Apparatus according to claim 5, wherein the device is a Raman amplifier, the optical fiber is silica-based optical fiber, λ

_p is about 1.06 μ

m, Δ

λ

_i corresponds to a Stokes shift of about 450 cm ^-1 and λ

_s is approximately equal to 1.3 μ

m.

7. Apparatus according to claim 4, the apparatus being an optical fiber communication system that further comprises

i) transmitter means that comprise means for generating a signal radiation of wavelength λ

_signal ;

ii) receiver means, spaced apart from the transmitter means, that comprise means for detecting the signal radiation of wavelength λ

_signal ;

iii) optical fiber transmission means that signal-transmissively connect the transmitter and receiver means;

iv) means for coupling the output radiation of wavelength λ

_s of said Raman laser into said optical fiber transmission means.

8. An optical fiber communication system according to claim 7, wherein λ

_signal is about 1.5 μ

m, the system comprising an erbium-doped fiber amplifier located intermediate the transmitter and receiver means, and the means for coupling the output radiation of the Raman laser into the optical transmission means are spaced from said erbium-doped fiber amplifier, with λ

_s selected such that the radiation of wavelength λ

_s serves as pump radiation of the erbium-doped fiber amplifier.

9. An optical fiber communication system according to claim 8, wherein the means for coupling the output radiation of the Raman laser into the optical fiber transmission means are located close to or at the receiver means.

10. Apparatus according to claim 6, the apparatus being an optical fiber communication system that further comprises

i) transmitter means that comprise means for generating a signal radiation of wavelength λ

_s ;

ii) receiver means, spaced apart from the transmitter means, that comprise means for detecting the signal radiation of wavelength λ

_s ; and

iii) optical fiber transmission means that signal-transmissively connect the transmitter and receiver means, wherein said Raman amplifier is located intermediate said transmitter and receiver means, and said length of optical fiber forms at least part of said optical fiber transmission means.

11. Apparatus according to claim 1, further comprising a source of seed radiation of wavelength λ

_seed essentially equal to the center wavelength associated with one of said at least two pairs of reflectors, and means for coupling said seed radiation into the optical cavity defined by said one pair of reflectors.

12. Apparatus according to claim 5, further comprising means for introducing pump radiation of wavelength λ

_p'"'"' ≠

λ

_p into said length of optical fiber.

13. Apparatus according to claim 5, further comprising a pair of reflectors having a center wavelength λ

_n'"'"' ≠

λ

_n, with λ

_n'"'"' selected to provide the amplifier with a broadened gain bandwidth.

14. Apparatus according to claim 3, further comprising a reflector having center wavelength essentially equal to λ

_s and peak reflectivity of at least 98%.

15. Apparatus according to claim 3, further comprising an unpaired reflector having center wavelength essentially equal to λ

_p.

16. Apparatus comprising an optical device that comprises

a) a length of optical fiber;

b) means for introducing pump radiation of wavelength λ

_p into said length of optical fiber;

c) spaced-apart reflector means that define an optical cavity for radiation of a predetermined wavelength, with the cavity comprising at least a portion of the length of optical fiber;

wherein the device is adapted for emission of radiation of wavelength λ

_s ≠

λ

_p from said length of optical fiber;

characterized in that

d) the pump radiation is continuous wave radiation;

e) the reflector means comprise at least one pair of reflectors, associated with each of said reflectors being a center wavelength of a reflection band and a peak reflectivity, with the two reflectors of the at least one pair having essentially the same center wavelength and being spaced apart, such that the reflectors of the at least one pair define an optical cavity for radiation of wavelength equal to said center wavelength of the reflectors of the at least one pair, each of the two reflectors of the at least one pair having a peak reflectivity of at least 98%;

f) associated with said given optical cavity is an added round trip loss for radiation of wavelength equal to said center wavelength, said added round trip loss being at most 1.5 dB; and

g) said center wavelength is less than λ

_p.

17. Apparatus according to claim 16, wherein λ

_s is less than λ

_p and the optical device is an anti-stokes Raman amplifier or Raman laser.

18. Apparatus according to claim 16, wherein the length of optical fiber is silica-based optical fiber, λ

_p is about 1.32 μ

m, λ

_s is greater than λ

_p, and the device is a four-photon mixing amplifier for radiation of wavelength λ

_s.

19. Apparatus according to claim 16, wherein the length of optical fiber is silica-based optical fiber, λ

_p is about 1.32 μ

m, λ

_s is greater than λ

_p, the reflector means further comprise an unsymmetrical pair of reflectors having a center wavelength greater than λ

_p, with one of the reflectors of the unsymmetrical pair having peak reflectivity of at least 98% and the other of the reflectors having peak reflectivity less than 98%, and the device is a four-photon mixing laser.

20. Apparatus according to claim 19, further comprising means for generating the pump radiation of wavelength λ

_p, said means comprising a Raman laser comprising an optical cavity for radiation of wavelength equal to said center wavelength of the reflectors of the at least one pair.

21. Apparatus according to claim 20, wherein the center wavelength of the reflectors of the at least one pair is about 1.09 μ

m, and λ

_s is about 1.67 μ

m.