Methods for signal transmission in optical fiber

• US 7,139,454 B2
• Filed: 02/09/2005
• Issued: 11/21/2006
• Est. Priority Date: 06/30/2003
• Status: Expired due to Fees

• Current Assignee: II-VI Delaware, Inc. (Coherent Corp.)
• Original Assignee: Finisar Corporation (II-VI Incorporated)
• Inventors: Cox, James A., Chen, Bo Su
• Primary Examiner(s): Kianni, Kaveh
• Assistant Examiner(s): LEPISTO, RYAN A
• Application Number:
  US11/054,682
• Publication Number:
  US 20050201680A1
• Time in Patent Office: 650 Days
• Field of Search: 385/33
• US Class Current: 385/33
• CPC Class Codes: G02B 6/32 having lens focusing means positioned between opposed fibre ends with lens being an integral part of the single fibre end G02B6/262
• CPC Class Codes: G02B 6/4206 Optical features G02B6/4207, G02B6/421 take precedence

Abstract

This disclosure concerns methods for transmitting a signal in an optical system. In one example, the method begins when an optical signal is generated. Then, the optical signal is manipulated such that the optical signal defines a substantially annular intensity profile, where power of the optical signal varies in the intensity profile. Finally, the optical signal is launched into an input face of an optical fiber such that a predetermined part of the intensity profile of the optical signal is located proximate an optical axis associated with the optical fiber.

Claims

1. A method for transmitting a signal in an optical system, the method comprising:

generating an optical signal along an optical axis for transmission through an optical element;

positioning the optical element so that a surface discontinuity is positioned along the optical axis such that the optical signal defines a substantially symmetric intensity profile; and

launching the optical signal into an input face of an optical fiber such that a relative minimum of an incident field amplitude of the intensity profile is located proximate an optical axis associated with the optical fiber.

2. The method as recited in claim 1, wherein an axicon function is provided with respect to the optical signal via the surface discontinuity.

3. The method as recited in claim 1, wherein a PSF of the optical signal at the input face of the fiber is TIA/EIA 492AAAB compliant.

4. The method as recited in claim 1, wherein the relative minimum of the incident field amplitude of the intensity profile is located proximate a center of the intensity profile.

5. The method as recited in claim 1, wherein the relative minimum of the incident field amplitude of the intensity profile comprises a dark spot of Arago.

6. The method as recited in claim 1, wherein the intensity profile is substantially symmetric about the relative minimum of the incident field amplitude.

7. The method as recited in claim 1, wherein the intensity profile is substantially annular.

8. A method for transmitting a signal in an optical system, the method comprising:

generating an optical signal;

manipulating the optical signal such that the optical signal defines a substantially annular intensity profile that is substantially symmetric about a relative minimum of an incident field amplitude wherein the step of manipulating includes the steps of;

implementing an axicon function with respect to the optical signal; and

defocusing the optical signal such that the portion of the optical signal having a desired substantially annular intensity profile occurs at a predetermined defocused place; and

launching the optical signal into a first end of an optical fiber such that the relative minimum of the incident field amplitude is located proximate a center of the first end of the optical fiber.

9. The method as recited in claim 8, wherein the optical signal is transmitted through a multimode optical fiber.

10. The method as recited in claim 8, wherein the optical signal comprises 850 nm laser light.

11. The method as recited in claim 8, wherein the optical signal is capable of supporting a data rate of about 10 Gb/s within the optical fiber.

12. The method as recited in claim 8, further comprising substantially maintaining the substantially annular form of the intensity profile at a second end of the optical fiber.