Embodiments of the present invention generally relate to optical devices and, more specifically to an optical device that is configured to discharge an output laser generated by a laser system.
High power laser systems have a broad range of applications throughout the scientific, industrial and medical fields. Laser systems generally include a pump module, a gain medium and a laser resonator. The pump module includes laser diodes or bars that generate pump energy. The gain medium absorbs the pump energy and emits laser light responsive to the absorbed energy. The laser resonator operates to generate a harmonic of the laser light. The laser light is discharged through an optical device onto the desired target.
Embodiments of the invention relate to an optical device configured to discharge laser light generated by a laser system. One embodiment of the optical device comprises a fiber cap, an optical fiber and a bond between the fiber cap and the optical fiber. The fiber cap comprises a cap body having a closed distal end and a bore having a tapered section. The optical fiber comprises cladding surrounding a core. A distal end of the cladding comprises a tapered section that engages the tapered section of the bore.
Another embodiment is directed to a fiber optic cap comprising a cap body having a closed distal end and a bore. The bore is configured to receive a distal end of an optical fiber and has a tapered section defined by a conically shaped interior wall aligned at a taper angle relative to a central axis of the bore. In one embodiment, the taper angle is less than 15 degrees.
Another embodiment of the invention is directed to a method of forming an optical device. In the method, a fiber cap comprising a cap body having a closed distal end is provided. A bore is formed in the cap body having a tapered section defined by a conically shaped interior surface aligned at a taper angle relative to a central axis of the bore. An optical fiber comprising cladding surrounding a core is provided and a tapered section is formed in a distal end of the cladding. The tapered section of the cladding is defined by a conically shaped exterior surface aligned at a taper angle relative to a central axis of the optical fiber. The distal end of the optical fiber is inserted into the bore of the cap body, wherein the tapered section of the bore overlaps the tapered section of the cladding. The fiber cap is then bonded to the optical fiber by bonding a portion of the interior surface to the exterior surface.
This Summary is provided to introduce a selection of concepts in a simplified form that are further described below in the Detailed Description. This Summary is not indented to identify key features or essential features of the claimed subject matter, nor is it intended to be used as an aid in determining the scope of the claimed subject matter. The claimed subject matter is not limited to implementations that solve any or all disadvantages noted in the Background.
The gain medium 102 is water cooled in exemplary embodiments, along the sides of the host. In one embodiment, the gain medium 102 includes an undoped end cap 114 bonded on a first end 116 of the gain medium 102, and an undoped end cap 118 bonded on a second end 120 of the gain medium 102. In one embodiment, the end 120 is coated so that it is reflective at the pump energy wavelength, while transmissive at a resonant mode of the system 100. In this manner, the pump energy that is unabsorbed at the second end 120 is redirected back through the gain medium 102 to be absorbed.
The pump module 104 produces the pump energy 108 within an operating wavelength range of the gain medium 102. The laser resonator 106 is configured to generate a harmonic of the laser light 112 output from the gain medium 102. In one embodiment, the laser resonator 106 includes a non-linear crystal (NLC) 150, such as a lithium borate (LBO) crystal or a potassium titanyl phosphate crystal (KTP), for generating a second harmonic of the laser beam 112 emitted by the gain medium 102.
In one embodiment, the gain medium 102 comprises a yttrium-aluminum-garnet crystal (YAG) rod with neodymium atoms dispersed in the YAG rod to form a Nd:YAG gain medium 102. The Nd:YAG gain medium 102 converts the pump light into the laser light 112 having a primary wavelength of 1064 nm. The laser resonator 106 generates the second harmonic of the 1064 nm laser light 164 having a wavelength of 532 nm. One advantage of the 532 nm wavelength is that it is strongly absorbed by hemoglobin in blood and, therefore, is useful in medical procedures to cut, vaporize and coagulate vascular tissue.
In one embodiment, the laser resonator 106 includes a Q-switch 152 that operates to change the laser beam 112 into a train of short pulses with high peak power to increase the conversion efficiency of the second harmonic laser beam.
The laser resonator 106 also includes reflecting mirrors 156, 158 and 162, folding mirror 110, and output coupler 160. The mirrors 110, 156, 158 and 162, and output coupler 160 are highly reflective at the primary wavelength (e.g., 1064 nm). The output coupler 160 is highly transmissive at the second harmonic output wavelength (e.g., 532 nm). The primary wavelength laser beam (e.g., 1064 nm) inside the resonator 106 bounces back and forth along the path between the minors 158 and 162, passing through the gain medium 102 and the non-linear crystal 150 to be frequency doubled to the second harmonic output wavelength (e.g., 532 nm) beam, which is discharged through output coupler 160 as the output laser 164. The Z-shaped resonant cavity can be configured as discussed in U.S. Pat. No. 5,025,446 by Kuizenga, imaging the resonant mode at one end of the gain medium 102 at the non-linear crystal 150. The configuration described is stable and highly efficient for frequency conversion. The configuration shown in
An optical coupler 166 is connected to a waveguide, such as an optical fiber 168. In one embodiment, the system 100 includes an optical device 170, which is formed in accordance with embodiments of the invention.
It is understood that any suitable optical fiber may be used in the device 170. An exemplary optical fiber 172 of the prior art that can be used to form the optical device 170 is illustrated in the partial side cross-sectional view of
In one embodiment, the nylon jacket 176 and the hard cladding 178 are removed from the distal end 184 to expose the cladding 180, as illustrated in the side plan view of
The tapered section 190 of the cladding 180 can be formed using any suitable technique. In one embodiment, the cladding 180 is laser machined using, for example, a CO2 laser, to form the tapered section 190. In another embodiment, the tapered section 190 is formed in the cladding 180 using a suitable lathe or diamond lap.
One embodiment of the optical fiber 172 comprises a polished optical surface 200 formed at the terminating end 194 of the exposed cladding 180 and core 182. The polished optical surface 200 can be formed in accordance with conventional techniques. In one embodiment, the polished optical surface 200 is forwardly inclined at an angle 202 to reflect laser light 204 that is transmitted through the core 180 laterally relative to the central axis 196. In one embodiment, the angle 202 is approximately 37-38 degrees relative to the central axis 196, which causes the laser light 204 to be output at an angle 206 of approximately 74-76 degrees relative to the central axis 196.
When the fiber 172 includes the polished optical surface 200 (represented in phantom) at the terminating end 194, the length L of the tapered section 190 is selected such that the tapered section 190 at least overlaps the optical surface 200. Preferably, the length L of the tapered section 190 is selected to ensure that the tapered section 190 includes a section that completely surrounds the core 182 in a plane that is perpendicular to the central axis 196.
One common optical fiber 172 utilized in laser systems has a core outer diameter of 600 μm and a cladding outer diameter of 840 μm. Another on optical fiber 172 utilized in laser systems has a core outer diameter of 750 μm and a cladding outer diameter of 1050 μm. Other optical fibers may also be used for the fiber 172.
In one embodiment, the tapered section 220 extends from the proximal end 216 toward the distal end 210, as shown in
Embodiments of the optical device 170 include the combination of one or more of the embodiments of the optical fiber 172 and one or more of the embodiments of the cap body 174 described above.
The bore 212 of the cap body 174 is sized to receive the distal end 184 of the optical fiber 172. In one embodiment, the distal end 184 of the optical fiber 172 and the bore 212 are coaxial to a central axis 228 of the device 170. As a result, the conically shaped exterior surface 192 of the tapered section 190 of the optical fiber 172 is parallel to the conically shaped interior surface 222 of the tapered section 220 of the bore 212 due to the alignment of the surfaces 192 and 212 at the same taper angle 198 relative to the central axis 228.
In one embodiment, at least a portion of the tapered section 220 of the bore 212 overlaps a portion of the tapered section 190 of the optical fiber 172, and the corresponding portions of the conical surfaces 192 and 222 engage each other. In one embodiment, the tapered section 220 engages the tapered section 190 over a distance of at least 2.0 millimeters measured in the direction of the central axis 228. While the embodiments of the optical device 170 illustrated in
One embodiment of the optical device 170 comprises a bond 230 between the optical fiber 172 and the cap body 174, best shown in
One embodiment of the bond 230 comprises a fusion of the overlapping surfaces 192 and 222 of the tapered sections 190 and 220. In one embodiment, the cladding 180 and the body cap 174 are formed of silica. In one embodiment, the fusion bond 230 is formed by thermally fusing the overlapping surfaces 192 and 222 together. Conventional thermal fusion techniques may be used to form the thermal fusion bond 230.
In accordance with another embodiment, the fusion bond 230 is formed by chemically fusing the overlapping surfaces 192 and 222 together. Chemically fusing the surfaces 192 and 222 together eliminates significant thermal stresses that can develop from thermal fusion bonding, which can cause the optical device 170 to fail. Additionally, thermal fusion bonding can optically distort surfaces of the device 170, which can degrade performance.
In one embodiment, the chemical fusion bond 230 is formed through a hydroxide-catalyzed hydration and dehydration. In this method, hydroxide ions contained, for example, in an aqueous solution, are applied to at least one of the surfaces 192 and 212 and the surfaces 192 and 212 are then placed sufficiently close to each other to form at least one chemical bond between them. Suitable hydroxides for the aqueous solution include the ionic salts NaOH, KOH, NH.sub.4 OH, sodium ethoxide, and potassium ethoxide. A detailed explanation of this method of chemically fusing two silicate surfaces together is provided in U.S. Pat. No. 6,284,085, which is incorporated herein by reference in its entirety. Other chemical fusion techniques can also be used to fuse the surfaces 192 and 212 together and form the fusion bond 230.
In one embodiment, the terminating end 194 of the optical fiber 172 includes the forward inclined polished optical surface 200, which is configured to reflect laser light 204 transmitted through the core 182 laterally relative to the central axis 196 (
In one embodiment, the bond comprises an adhesive. In one embodiment, the adhesive comprises at least one fluorocarbon polymer. The term “fluorocarbon polymer,” as used herein, is a perfluoro or fluorocarbon polymer (fluoropolymer) or oligomer. Exemplary fluorocarbon polymers suitable for use in forming the adhesive are marketed under the trade names Cytop™, Krytox®, Fomblin® Z DOL, and others.
Although the present invention has been described with reference to preferred embodiments, workers skilled in the art will recognize that changes may be made in form and detail without departing from the spirit and scope of the invention.
The present application is based on and claims the benefit of U.S. provisional patent application Ser. No. 61/118,857, filed Dec. 1, 2008, the content of which is hereby incorporated by reference in its entirety.
| Number | Name | Date | Kind |
|---|---|---|---|
| 3933455 | Chown | Jan 1976 | A |
| 4381882 | Sabine | May 1983 | A |
| 4669467 | Willett et al. | Jun 1987 | A |
| 4672961 | Davies | Jun 1987 | A |
| 4732448 | Goldenberg | Mar 1988 | A |
| 4740047 | Abe et al. | Apr 1988 | A |
| 5061265 | Abela et al. | Oct 1991 | A |
| 5074632 | Potter | Dec 1991 | A |
| 5242438 | Saadatmanesh et al. | Sep 1993 | A |
| 5269777 | Doiron et al. | Dec 1993 | A |
| 5292320 | Brown et al. | Mar 1994 | A |
| 5343543 | Novak, Jr. et al. | Aug 1994 | A |
| 5354294 | Chou | Oct 1994 | A |
| 5428699 | Pon | Jun 1995 | A |
| 5486171 | Chou | Jan 1996 | A |
| 5495541 | Murray et al. | Feb 1996 | A |
| 5496307 | Daikuzono | Mar 1996 | A |
| 5496308 | Brown et al. | Mar 1996 | A |
| 5498260 | Rink et al. | Mar 1996 | A |
| 5509917 | Cecchetti et al. | Apr 1996 | A |
| 5512078 | Griffin | Apr 1996 | A |
| 5530780 | Ohsawa | Jun 1996 | A |
| 5537499 | Brekke | Jul 1996 | A |
| 5562657 | Griffin | Oct 1996 | A |
| 5571099 | Purcell, Jr. et al. | Nov 1996 | A |
| 5638483 | Konwitz | Jun 1997 | A |
| 5695583 | van den Bergh et al. | Dec 1997 | A |
| 5807390 | Fuller et al. | Sep 1998 | A |
| 5824005 | Motamedi et al. | Oct 1998 | A |
| 6246817 | Griffin | Jun 2001 | B1 |
| 6270492 | Sinofsky | Aug 2001 | B1 |
| 6284085 | Gwo | Sep 2001 | B1 |
| 6398778 | Gu et al. | Jun 2002 | B1 |
| 6522806 | James, IV et al. | Feb 2003 | B1 |
| 6626582 | Farrar et al. | Sep 2003 | B2 |
| 6687436 | Griffin | Feb 2004 | B2 |
| 6712526 | Fleenor | Mar 2004 | B1 |
| 6829411 | Easley | Dec 2004 | B2 |
| 6986764 | Davenport et al. | Jan 2006 | B2 |
| 7909817 | Griffin et al. | Mar 2011 | B2 |
| 20050165279 | Adler et al. | Jul 2005 | A1 |
| 20060291061 | Iyama et al. | Dec 2006 | A1 |
| 20070106286 | Harschack et al. | May 2007 | A1 |
| 20070189683 | Griffin | Aug 2007 | A1 |
| 20080287936 | Stinson et al. | Nov 2008 | A1 |
| 20110002584 | Griffin | Jan 2011 | A1 |
| 20110038580 | Griffin | Feb 2011 | A1 |
| Number | Date | Country |
|---|---|---|
| 0689797 | Jan 1996 | EP |
| 60250322 | Dec 1985 | JP |
| 62011820 | Jan 1987 | JP |
| 03111040 | May 1991 | JP |
| 10155805 | Jun 1998 | JP |
| 2001346891 | Dec 2001 | JP |
| 2008073263 | Jun 2008 | WO |
| 2008073264 | Jun 2008 | WO |
| Entry |
|---|
| U.S. Appl. No. 12/517,883, filed Jun. 5, 2009. |
| International Search Report and Written Opinion of PCT/US2007/024964, filed Dec. 6, 2007. |
| U.S. Appl. No. 61/118,857, filed Dec. 1, 2008. |
| International Search Report and Written Opinion of PCT/US2007/024963, filed Dec. 6, 2007. |
| U.S. Appl. No. 12/517,879, filed Jun. 5, 2009. |
| Number | Date | Country | |
|---|---|---|---|
| 20100135617 A1 | Jun 2010 | US |
| Number | Date | Country | |
|---|---|---|---|
| 61118857 | Dec 2008 | US |