Integral optical fiber coupler

• US 4,729,621 A
• Filed: 03/11/1985
• Issued: 03/08/1988
• Est. Priority Date: 03/11/1985
• Status: Expired due to Fees

• Current Assignee: Shiley Incorporated (Pfizer Inc.)
• Original Assignee: Shiley Incorporated (Pfizer Inc.)
• Inventors: Edelman, William
• Primary Examiner(s): LEE, JOHN D
• Application Number:
  US06/710,196
• Time in Patent Office: 1,093 Days
• Field of Search: 350/96.10, 350/96.15, 350/96.24, 350/96.25, 350/96.26, 350/96.18, 128/303.1, 128/6, 604/20, 604/21, 604/53, 219/121 L, 219/121 LM, 219/121 LZ
• US Class Current: 385/33
• CPC Class Codes: G02B 6/4203 Optical features

Abstract

A device for transferring high energy electromagnetic radiation from a laser to an optical fiber, which comprises a cone-shaped coupler having a wide proximal end and a narrow distal end, wherein the proximal end is in the form of a convex surface which acts as a focussing lens adapted to receive radiation from a laser and to transmit said radiation into and through said optical fiber and the distal end is attached to the input end of the optical fiber to form an integral assembly therewith, said cone-shaped coupler having a taper angle θ defined by the equation ##EQU1## wherein N.A. is the numerical aperture of the fiber material and μ is the refractive index of the material of the coupler at the wavelength of the incident radiation. A process for removing an obstruction by laser surgery using said device is also disclosed.

Claims

1. A device for transferring high energy electromagnetic radiation from an excimer laser to an optical fiber, which comprises a cone-shaped coupler having a wide proximal end and a narrow distal end, wherein the proximal end is in the form of a convex surface which acts as a focussing lens adapted to receive radiation from a laser and to transmit said radiation into and through said optical fiber and the distal end is attached to the input end of the optical fiber to form an integral assembly therewith, said cone-shaped coupler being made from a material having the same refractive index as that of the optical fiber and having a taper angle θ

defined by the equation ##EQU4## wherein N.A. is the numerical aperture of the fiber material and μ

is the refractive index of the material of the coupler at the wavelength of the incident radiation.

2. A device according to claim 1, in which the integral assembly of optical fiber and coupler is formed of fused silica having a refractive index of from 1.43 to 1.47.

3. A device according to claim 2, in which the taper angle is about 9.79°

.

4. A device according to claim 1 which is adapted to operate with an excimer laser producing radiation having a wavelength from 100 to 400 nm.

5. A method for producing a device according to claim 1, which comprises drawing out a solid rod of fused silica into a cone-shaped tapered body having a wide proximal end which is curved into a convex focussing lens and a narrow distal end which is of substantially the same diameter as an optical fiber to which it is to be attached and fusing said narrow distal end to the input end of said optical fiber to form an integral assembly therewith.

6. A method according to claim 5, in which the distal end of the tapered body is fused to the optical fiber by arc welding.

7. A method for producing a device according to claim 1, in which the cone-shaped coupler is formed as an integral extension of an optical fiber by forming the optical fiber in accordance with a conventional drawing process, slowing down the speed of draw to allow the diameter of the fiber to expand near the point at which the preform of fiber material is extruded and controlling the drawing speed and pressure applied to the preform so that the proximal end of the fiber becomes tapered into the desired cone-shaped configuration.

8. A method for producing a device according to claim 1, which comprises machining a solid rod of fused silica into a tapered body having a wide proximal end and a narrow distal end, the diameter of said distal end being larger than the diameter of an optical fiber to which the tapered body is to be attched, subjecting the input end of said optical fiber to conventional heating and pressing techniques to form a small bulge thereon which is of comparable diameter to that of the distal end of the tapered body and then mating the surface of said bulge to said distal end to form an integral assembly of the tapered body and said optical fiber.

9. A method according to claim 8, in which the tapered body and optical fiber are mated by thermal fusion.

10. A process for removing an obstruction by laser surgery which comprises subjecting the said obstruction to high energy electromagnetic radiation through an optical fiber which is coupled to an excimer laser by a cone-shaped coupler having a wide proximal end and a narrow distal end, wherein the proximal end is in the form of a convex surface which acts as a focussing lens adapted to receive said electromagnetic radiation and to transmit it into said optical fiber to form an integral assembly input end of the optical fiber to form an integral assembly therewith, said cone-shaped coupler being made from a material having the same refractive index as that of the optical fiber and having a taper angle θ

defined by the equation ##EQU5## wherein N.A. is the numerical aperture of the fiber material and μ

is the refractive index of the material of the coupler at the wavelength of the incident radiation.

11. A process according to claim 10, in which the cone-shaped coupler and optical fiber are both made of fused silica having a refractive index of from 1.43 to 1.47.

12. A process according to claim 11, in which the taper angle θ

is about 9.79°

.

13. A process according to claim 10, in which said excimer laser produces radiation having a wavelength of from 100 to 400 nm.

14. A process according to claim 13, in which said laser is a krypton fluoride excimer laser producing UV radiation having a wavelength of 248 nm.