Microlenses for coupling optical fibers to elliptical light beams

• US 5,256,851 A
• Filed: 02/28/1992
• Issued: 10/26/1993
• Est. Priority Date: 02/28/1992
• Status: Expired due to Term

• Current Assignee: American Telephone & Telegraph Company (AT&T, Inc.)
• Original Assignee: AT&T, Inc.
• Inventors: Presby, Herman M.
• Primary Examiner(s): Bovernick, Rodney B.
• Assistant Examiner(s): BARNS, STEPHEN
• Application Number:
  US07/843,481
• Time in Patent Office: 606 Days
• Field of Search: 219/121.66, 219/121.65, 219/121.68, 219/121.69, 219/121.75, 385/33
• US Class Current: 219/121.69
• CPC Class Codes: G02B 6/2552 reshaping or reforming of light guides for coupling using thermal heating, e.g. tapering, forming of a lens on light guide ends
• CPC Class Codes: G02B 6/4203 Optical features

Abstract

An asymmetric hyperbolic microlens on the end of a single-mode optical fiber enhances the fiber'"'"'s coupling to elliptical laser beams. The lenses, with controlled eccentricity ratios, are made by micromachining the end of the fiber with a pulsed CO₂ laser as the fiber is directed, preferably by computer control, about the focused laser beam. Coupling efficiencies of 90 percent (-0.75 dB) have been realized with single transverse mode lasers at a wavelength of 0.98 μm having an approximately 3 to 1 beam ellipicity. With multimode lasers at 1.48 μm having similar elliptical beams, the asymmetric lenses demonstrate an almost 2 dB increase in coupling efficiency over symmetric hyperbolic microlenses. Such lasers are useful to pump erbium-doped fiber amplifiers. About 120 mw was coupled from such a laser into single-mode fiber.

Claims

1. A process for fabricating an optical fiber microlens for coupling an optical power between an optical device having an asymmetric output light distribution and an optical fiber, the ellipticity ratio of the asymmetric modal area of the device being greater than 1.5:

1.0, which comprises;

laser micromachining an end portion of an optical fiber by ablating and heating the material of the end portion of the optical fiber by means of a laser beam, in which

said micromachining is conducted by removing a greater proportion of the material at opposite ends of one orthogonal axis of the optical fiber than at opposite ends of the other orthogonal axis, such as to produce a microlens having a given ellipticity ratio.

2. The process of claim 1, in which the ellipticity ratio of the modal area of the device ranges between 1.5:

1 and 10;

1.

3. The process of claim 1, in which first a symmetric microlens is produced at the end of the optical fiber, and then segments of the lens along the opposite ends of one orthogonal axis of the lens are ablated to introduce asymmetry to the lens.

4. The process of claim 3, in which first a desired segment of the cross-section of the microlens at one end of said one orthogonal axis is removed, followed by the removal of a matching segment at an opposite end of said one orthogonal axis.

5. The process of claim 1, in which said asymmetry is introduced by ablating the fiber sequentially at opposite ends of one orthogonal axis of the optical fiber during the rotation of the fiber about its longitudinal axis, until a desired segment of the cross-section of the fiber is removed at said opposite ends of said one orthogonal axis.

6. The process of claim 5, in which the laser beam is intermittently activated at intervals corresponding to 180°

positions of the fiber, so as to remove the segments along and adjacent to the opposite ends of said one orthogonal axis.

7. The process of claim 1 in which a symmetric microlens is partially formed on the end of the fiber, and then the laser beam is intermittently activated at intervals corresponding to 180°

positions of the fiber so as to remove segments of the fiber along and adjacent to opposite ends of one orthogonal axis of the fiber.

8. The process of claim 1 in which said laser micromachining is conducted by means of a pulsating laser beam.

9. The process of claim 1 in which the operating wavelength, λ

, of the optical power being coupled is within a range of from 0.2 to 2.5 μ

m.

10. The process of claim 1, in which the operating wavelength, λ

, of an optical power being coupled is within a range of from 0.2 to 1.6 μ

m.

11. The process of claim 10, in which said operating wavelength λ

is about 0.98 μ

m.

12. The process of claim 10, in which said operating wavelength is equal to about 1.48 μ

m.

13. The process of claim 1, in which said microlens results in a coupling efficiency exceeding 50 percent of the optical power being coupled.

14. The process of claim 1, in which said microlens results in coupling efficiency of the order of 90 percent.

15. The process of claim 1, in which said optical device is selected from the group consisting of lasers, semiconductor amplifiers, optical fiber amplifiers, pump sources for fiber amplifiers, modulators, photodetectors and integrated circuit waveguides.

16. The process of claim 1, in which said optical device is a laser.