Glass large-core optical fibers

• US 9,632,243 B2
• Filed: 03/11/2015
• Issued: 04/25/2017
• Est. Priority Date: 09/26/2007
• Status: Active Grant

• Current Assignee: IMRA America Incorporated (Aisin Corp.)
• Original Assignee: IMRA America Incorporated (Aisin Corp.)
• Inventors: Dong, Liang, Li, Jun, McKay, Hugh, Fu, Libin, Marcinkevicius, Andrius
• Primary Examiner(s): Bolda, Eric
• Application Number:
  US14/644,779
• Publication Number:
  US 20150241628A1
• Time in Patent Office: 776 Days
• CPC Class Codes: G02B 6/02009 Large effective area or mode field radius, e.g. to reduce nonlinear effects in single mode fibres
• CPC Class Codes: G02B 6/02333 Core having higher refractive index than cladding, e.g. solid core, effective index guiding
• CPC Class Codes: G02B 6/02357 Property of longitudinal structures or background material varies radially and/or azimuthally in the cladding, e.g. size, spacing, periodicity, shape, refractive index, graded index, quasiperiodic, quasicrystals
• CPC Class Codes: G02B 6/02361 Longitudinal structures forming multiple layers around the core, e.g. arranged in multiple rings with each ring having longitudinal elements at substantially the same radial distance from the core, having rotational symmetry about the fibre axis
• CPC Class Codes: G02B 6/02366 Single ring of structures, e.g. "air clad"
• CPC Class Codes: G02B 6/02371 Cross section of longitudinal structures is non-circular
• CPC Class Codes: G02B 6/0283 Graded index region external to the central core segment, e.g. sloping layer or triangular or trapezoidal layer G02B6/0288, G02B6/0286 take precedence
• CPC Class Codes: G02B 6/0288 Multimode fibre, e.g. graded index core for compensating modal dispersion
• CPC Class Codes: G02B 6/14 Mode converters
• CPC Class Codes: H01S 3/06729 Peculiar transverse fibre profile
• CPC Class Codes: H01S 3/06754 Fibre amplifiers H01S3/06708 takes precedence
• CPC Class Codes: H01S 3/091 using optical pumping

Abstract

Embodiments of optical fiber may include cladding features that include a material (e.g., fluorine-doped silica glass) that may produce a very low relative refractive index difference with respect to cladding material in which the cladding features are disposed. This relative refractive index difference may be characterized by (n₁-n₂)/n₁, where n₁ is the index of refraction of the cladding material in which the cladding features are included, and n₂ is the index of refraction of the cladding features. In certain embodiments, the relative refractive index difference may be less than about 4.5×10⁻³. In various embodiments, the configuration of the cladding features including, for example, the size and spacing of the cladding features, can be selected to provide for confinement of the fundamental mode yet leakage for the second mode and higher modes, which may provide mode filtering, single mode propagation, and/or low bend loss.

Claims

1. A fiber optic amplifier system comprising:

an optical pulse source providing optical pulses having a nearly diffraction limited input spatial profile;

an optical pump source; and

a fiber comprising,

a first cladding region comprising a first cladding material having a first index of refraction, n1;

cladding features disposed in said first cladding region, said cladding features comprising a second cladding material having a second index of refraction, n2, wherein n2 is less than n1, and wherein the cladding features have a dimension d and a center-to-center spacing Λ

, and a ratio d/Λ

is in a range from 0.3 to 0.9;

a core region at least partially surrounded by said cladding features, said first cladding region and said cladding features configured such that said core region propagates at least one lower order mode having a wavelength, while limiting propagation of at least one higher order mode having the wavelength by providing said at least one higher order mode with a higher loss than the at least one lower order mode at the wavelength, wherein at least a portion of said core region is rare-earth doped, and

a pump cladding configured to receive pump energy from said optical pump source,

said fiber configured to receive said pulses and amplify said pulses such that the fiber optic amplifier system is configured to produce output pulses having nearly diffraction limited output spatial profiles and at least one output pulse having energy in a range from 10 μ

J to 10 mJ.

2. The fiber optic amplifier system of claim 1, wherein said fiber is configured as an all-glass, leakage channel fiber.

3. The fiber optic amplifier system of claim 1, wherein said first cladding material comprises a first glass that comprises fused silica, and wherein said second cladding material comprises a second glass that comprises fluorine-doped silica glass or boron-doped silica glass.

4. The fiber optic amplifier system of claim 1, wherein said core region has a diameter in a range from30 μ

m to 200 μ

m.

5. The fiber optic amplifier system of claim 1, wherein said first cladding region has a diameter in a range from 125 μ

m to 300 μ

m.

6. The fiber optic amplifier system of claim 1, wherein a relative refractive index difference characterized by (n1−

n

     2)/n1 is less than 4.5×

10<sup>−

3</sup>.

7. The fiber optic amplifier system of claim 1, wherein a repetition rate of said output pulses exceeds 1 kHz.

8. The fiber optic amplifier system of claim 7, wherein said repetition rate of said output pulses is below 1 MHz.

9. The fiber optic amplifier system of claim 1, wherein a pulse width of the at least one output pulse is below 1 ns.

10. The fiber optic amplifier system of claim 9, wherein said pulse width is above 1 ps.

11. The fiber optic amplifier system of claim 1, further comprising a pump guide to transmit a portion of said received pump energy to said core region.

12. The fiber optic amplifier system of claim 1, wherein said pump cladding is disposed beyond said first cladding region.

13. The fiber optic amplifier system of claim 1, wherein said pump cladding comprises a low index glass.

14. The fiber optic amplifier system of claim 13, wherein said low index glass comprises fluorine.

15. The fiber optic amplifier system of claim 1, wherein said pump cladding comprises a layer of air holes.

16. The fiber optic amplifier system of claim 1, wherein at least a portion of said pump cladding comprises a non-circular portion.

17. The fiber optic amplifier system of claim 16, wherein said non-circular portion is configured to increase mode mixing of a pump beam incident on said pump cladding.

18. A laser-based material processing system comprising:

the fiber optic amplifier system of claim 1; and

an optical system comprising a beam delivery optic to produce a spot on or within a material, said spot having a spot diameter in a range from 1 μ

m to 250 μ

m.

19. A laser-based radar system comprising the fiber optic amplifier system of claim 1.

20. The fiber optic amplifier system of claim 1, further comprising:

a single mode or few-mode input fiber coupled to said fiber to deliver pulses from said optical pulse source to said fiber, wherein a core of said input fiber is expanded and power coupled from the core of said input fiber to said fiber is substantially greater than obtainable with butt-coupling.

21. The fiber optic amplifier system of claim 1, wherein a ratio of the loss of said at least one higher order mode to the loss of said at least one lower order mode is greater than 10 and less than 1000.

22. The fiber optic amplifier system of claim 1, wherein said wavelength is in a range from 458 nm to 1550 nm.

23. The fiber optic amplifier system of claim 1, where said ratio d/Λ

is in a range from 0.5 to 0.8.

24. The fiber optic amplifier system of claim 1, where said ratio d/Λ

is in a range from 0.65 to 0.9.

25. The fiber optic amplifier system of claim 1, where said ratio d/Λ

is in a range from 0.75 to 0.85.