CA1258787A - Fiber optic coupler - Google Patents
Fiber optic couplerInfo
- Publication number
- CA1258787A CA1258787A CA000476580A CA476580A CA1258787A CA 1258787 A CA1258787 A CA 1258787A CA 000476580 A CA000476580 A CA 000476580A CA 476580 A CA476580 A CA 476580A CA 1258787 A CA1258787 A CA 1258787A
- Authority
- CA
- Canada
- Prior art keywords
- fiber
- rod
- coupler
- light
- transparent body
- Prior art date
- Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
- Expired
Links
Classifications
-
- G—PHYSICS
- G02—OPTICS
- G02B—OPTICAL ELEMENTS, SYSTEMS OR APPARATUS
- G02B6/00—Light guides; Structural details of arrangements comprising light guides and other optical elements, e.g. couplings
- G02B6/24—Coupling light guides
- G02B6/42—Coupling light guides with opto-electronic elements
- G02B6/4201—Packages, e.g. shape, construction, internal or external details
- G02B6/4256—Details of housings
- G02B6/4257—Details of housings having a supporting carrier or a mounting substrate or a mounting plate
- G02B6/4259—Details of housings having a supporting carrier or a mounting substrate or a mounting plate of the transparent type
-
- G—PHYSICS
- G02—OPTICS
- G02B—OPTICAL ELEMENTS, SYSTEMS OR APPARATUS
- G02B6/00—Light guides; Structural details of arrangements comprising light guides and other optical elements, e.g. couplings
- G02B6/24—Coupling light guides
- G02B6/42—Coupling light guides with opto-electronic elements
- G02B6/4201—Packages, e.g. shape, construction, internal or external details
- G02B6/4286—Optical modules with optical power monitoring
-
- G—PHYSICS
- G02—OPTICS
- G02B—OPTICAL ELEMENTS, SYSTEMS OR APPARATUS
- G02B6/00—Light guides; Structural details of arrangements comprising light guides and other optical elements, e.g. couplings
- G02B6/24—Coupling light guides
- G02B6/42—Coupling light guides with opto-electronic elements
- G02B6/4201—Packages, e.g. shape, construction, internal or external details
- G02B6/4287—Optical modules with tapping or launching means through the surface of the waveguide
- G02B6/4289—Optical modules with tapping or launching means through the surface of the waveguide by inducing bending, microbending or macrobending, to the light guide
Landscapes
- Physics & Mathematics (AREA)
- General Physics & Mathematics (AREA)
- Optics & Photonics (AREA)
- Optical Couplings Of Light Guides (AREA)
Abstract
FIBER OPTIC COUPLER
Abstract of the Disclosure A fiber optic coupler has a cylindrical rod protruding along the apex of an angled block. An optical waveguide is mounted to extend around part of the circumference of the rod. A transparent body is located on the side of the fiber remote from the rod, and the rod and the body are biased together to bend the fiber around the rod surface and to form an intimate contact between the transparent body and the curved part of the fiber. A light input or output device is positioned to direct light at or receive light from the curved fiber part through the transparent body.
_ j
Abstract of the Disclosure A fiber optic coupler has a cylindrical rod protruding along the apex of an angled block. An optical waveguide is mounted to extend around part of the circumference of the rod. A transparent body is located on the side of the fiber remote from the rod, and the rod and the body are biased together to bend the fiber around the rod surface and to form an intimate contact between the transparent body and the curved part of the fiber. A light input or output device is positioned to direct light at or receive light from the curved fiber part through the transparent body.
_ j
Description
- ~Z5~787 This invention relates to a fiber optic coupler particularly for minimizing light loss when splicing monomode fibers.
In the fabrication and installation of optical cable spans, lengths of optical waveguide are joined together end-to-end using for example a fusion splice. An example of splicing equipment and an operating procedure for using that equipment are described in United States Patent 4,274,707 (Pacey). Particularly for single mode waveguide in which light propagates substantially within a small core of the order of 10 microns in diameter, the cores of the waveguides which are to be spliced must be accurately aligned so that all the light from the core of one waveguide passes into the core of the other waveguide.
One technique for optimizing waveguide end alignment at a splice site is to inject light locally upstream of the site and monitor the light output immediately downstream of the splice site.
The two fiber ends at the splice site are then manipulated until light transmission between the two fibers is maximized.
In our co-pending Canadian patent application serial number 453,707 there is disclosed a local launch and detect system.
The system has top and bottom transparent blocks, the top block having an angled surface with an angled protrusion dimensioned to fit in an angled recess in the lower bloch. The apex of the angle is sufficiently sharp that light propagating along a waveguide located between the two blochs is emitted as a beam at the angle. The device has a detector positioned to monitor the emitted light. A
corresponding unlt for launching light has a laser emitter in place of the detector.
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.
~2S~7~37 In the example specifica11y described in the co-pending specification, the curvature of the protruding angle was set to a desired angle of 146 with a radius of curvature of about 250 microns, this being the diameter also of the coated fiber being spliced.
In the operation of these units it has been found that frequently the fiber retained between the two blocks does not adopt the desired curvature at the apex of the angle. This is disadvantageous for a number of reasons. Firstly the light input device in the case of a local launch unit functions to focus light at a point which assumes a close contact between the fiber and the protruding angle. If the fiber does not in fact contact the block over the critical part of the protruding angle then light launched into the fiber core is not maximized. Similarly detection of maximum light by the local detection unit assumes close contact between the fiber and the protruding angle. Secondly, if the fiber is clamped in a position such that the angle through which the fiber is bent adjacent to the protruding angle is greater than 146 then the fiber is subjected to more stress than it need be.
To overcome this problem there is proposed according to the invention, a fiber optic coupler comprising a cylindrical rod, means for mounting the fiber to extend around a part of the circumference of the rod, a transparent body located on a side of the fiber remote from the rod, spring means for pressing the fiber between the rod and the transparent means to bias the fiber to adopt the radius of curvature of the rod and to form an intimate contact between the transparent body and the curved part of the fiber, and a light input or output device positioned to direct light at or receive light '' '' ' ~ ' ' : ' ' ., - :. . - .
.: ' ', .
~2S1~7~7 from the curved fiber part through the transparent body.
The rod, preferably made of metal, can adhere in a groove formed in a first block. Similarly the transparent body can form part of a second block, the two blocks having complementary surfaces and being mounted relative to one another inside a box fixed with a lid said spring means can be located between the lid and the first block, this arrangement permitting insertion of a fiber between the blocks with automatic applications of the spring bias to the fiber on closing the lid.
A groove can extend around at least said part of the rod circumference for location of the fiber therein. Aligned slots can be formed in one or both of the blocks whereby when the fiber is stretched taut between a pair of the slots, it is aligned with said groove in the rod. The transparent body can be reFractive index matched to the fiber outer coating, the outer coating being resilient to ensure the establishment of said intimate contact between the fiber and the transparent body. The transparent body can have a durable surface facing the fiber to prevent scratching, the durable surface provided by a glass upper layer overlying a mass of transparent epoxy, the light input or output device projecting into said transparent epoxy mass. The light input device can be a laser and t`or a light output unit, the device can be a PIN or avalanche photodiode.
Alternatively the input or output device can be combined with a fiber optic pigtail for guiding light to or from a detector or source respectively located outside the coupler blocks.
When the blocks are located in a position clamping the fiber therebetween, the complementary surfaces thereof should be ~258787 spaced from one another whereby the contact location is limited to the fiber contacts with the first and second blocks.
Preferably control means are provided to the pressure means whereby to insure that when splicing two fibers together the light output from the output unit is a maximum for a fixed input intensity and splice site loss.
An embodiment of the invention will now be described by way of example with reference to the accompanying drawings in which:-Figure 1 shows a perspective view of a coupler according to the invention;
Figure 2 is a cross-section through the device of Figure 1; and Figure 3 is a sectional view on the line III-III of Figure 2.
Referring to the drawings in detail, the unit of Figures 1 and 2 has an upper metal block part 10 and a lower metal block part 12, the block part 12 being fixed within a box 14 and the part 10 being fixed to a lid 16. A compression spring 50 extends between the block 10 and the lid 16. Extending into the sides of the box are slots 18 which are aligned with corresponding slots 20 within the lower block 12.
As shown in sectional view in Figure 2, the two blocks 10, 12 have generally complementary angled surfaces 22, 24. Extending along the apex and protruding from the angled part of the top block 10 is a cylindrical metal rod 26 which adheres in a cylindrical groove 2 along the apex. A groove 30 (Figure 3) having a depth of 100 microns and an included angle of 60 extends around the rod 26 in alignment : ' , .
~ '' ~ ' ' ~:S~7~7 with the slots 20.
The lower block has angle surfaces meeting at 146 with a light input or output device 40 aligned to a line projecking from the apex of the surfaces at an angle 7.5 below the horizontal and 24.3 below the top surface of a glass plate 34. The rod 26 has a radius of curvature of 2.8 millimeters.
The metal lower block 12 has a column 32 of transparent epoxy and a top glass plate 34 flush with the angle face. Extending into the lower block is a bore 36 of 1/4 inch diameter which terminates in a further bore 38 of 1/16 inch diameter. A graded refractive index rod 40 which functions as a converging lens is lodged in the smaller bore 36 and a multimode pigtail fiber 42 with protective jacketing is secured by adhesive within a ferrule 44 which is itself mounted by an epoxy within the wider bore 36. The end of 15 the pigtail fiber projects from the ferrule 44 and is aligned with the axis of the lens 40. The end of the lens remote from the fiber projects into the epoxy mass 32. The other end of the fiber 42 is secured in a position in which it receives the output of a GaAs/GaAlAs semiconductor laser 46 (not shown) having an output wavelength of 0.84 microns.
In use an optical fiber 48 having a resilien-t jacket 49 is positioned so as to extend between the slots 20 whereby it is aligned to the groove 30. The lid 16 is then closed to bias the fiber 48 by means of the spring 50 between the top block 10 and the bottom block 12. The arrangement provides a light-tight enclosure for the portion of the fiber 48 within the box 14. The pressure set on the fiber is determined by the stiffness of spring 50 and the depth of two - ~ -.
~2Si~7~7 cylindrical holes 51, 52 in the lid and the upper block 10. The force should not exceed 1 kg otherwise damage to fiber coating 49 occurs. A
minimum force of 500 grams is required in order to ensure intimate contact of resilient fiber coating 49 with top glass plate 34.
At this pressure, the rod 26 presses the fiber 48 against the planar faces of the lower block immediately adjacent to the angle. This has two effects. Firstly the fiber is caused to adopt the curvature of the rod outer circumFerence where it contacts the rod at groove 30, and secondly, the resilient coating 49 on the fiber is deformed slightly so as to effect an intimate contact between the fiber and the glass plate 34 . -rhe epoxy 36, the glass of plate 34, and the fiber coating material 49 are index matched to one another so that there is minimal light los-t from reflection. The glass plate is 1 millimeter thick and the epoxy is available under the tradename EP0 + TEK 301-2, being an optically clear epoxy whose index is close to that of the glass and the UV curable acrylate fiber coating.
At the rod 26 a relatively sharply angled region is developed in the fiber, the radius of curvature of the fiber being that of the rod. The lens 40 is positioned so as to focus light from the pigtail fiber 42 directly at the fiber angle which is as sharp an angle as possible commensurate with limiting short term stress on the fiber 4~ below that which might result in fracture. If the bend in the fiber had a relatively large radius of curvature, then light injected at one point of the fiber would to some extent, be scattered out of the fiber in the curved portion downstream of where the light enters. By ensuring: (i) that the injected light is properly focussed at the fiber angle; (ii) the apex of the fiber angle is sharp, and .
~ ~ .
. . .
125~378~7 (iii) the axis angles of 40 and 42 are 7.5 below hor;zontal (ie.
24.5 below the angle of the glass plate surface) light loss downstream of the light entry point is minimized. A low wavelength laser is used since the number of modes which can be launched into a fiber is proportional to the inverse of laser wavelength~ In addition, the local launch device is intended for use with a photocell using particularly sensitive silicon photodetectors which have a peak response in the low wavelength regime.
In the detector unit, as described in our co-pending Canadian patent application serial number 453,707 filed May 7, 1984 the laser and the lens 40 are replaced by a photocell which can be sited either within the coupler or at the remote end of a pigtail fiber such as fiber 42. Also, as described in the co-pending application, a single unit can be constructed with a pair of detectors, a pair of light emitters or a combination of a detector and a light emitter. As further described in that patent application, a skeletal unit can be made so as to accept plug-in emitting or detecting devices.
The choice of fiber angle is important since it is a compromise between minimizing light beam size and minimizing fiber stress. The fiber included angle of 146, an angle between the fiber and the axis of the launch or detection device of 24.5 and a rod diameter of 2.8 millimeters recited in this specific example, are values which depend on the relative refractive indexes of the fiber, the jacket material and the coupler block. They depend also on the ability of the fiber to withstand bending stresses. For other types ~` ~
lZ5~7~7 of fiber, the fiber included angle, the angle between the f;ber and the electro-optic device, and the apex radius will be d;fferent.
When using the launch and detection couplers in conjunction with a splicing equipment, the couplers are fixed on either side of the splicing equipment. An upstream fiber is led through the a light input or injection coupler into a splicing zone where the end of the fiber is clamped. The downstream fiber is led through a light output or monitoring coupler and its end portion is clamped at the splicing zone. In the splicing zone one of the fiber ends can be moved incrementally in x, y and z directions using a micromanipulator unit. In use light is launched from the laser into the pigtail fiber 42 housed within a shield 53 as shown in Figure 1 and at the lens 40 is focussed at the fiber core on the upstream side of the splice site. In turn, light is monitored by a silicon photodetector within the downstream detector unit and directed to a level detection circuit. Although manipulation can be achieved mannually, the detector output can be used directly to manipulate the position of one or other of the fiber ends at the splice zone. A
suitable control circuit is described in our copending Canadian patent application Serial Number 485,873, filed June 28, 1985. Subsidiary control loops can be used at each coupler to ensure that pressure on the fibers at each coupler is maintained at a value which maximizes the detector output. To ensure accuracy of monitoring, the output level of the laser is stabilized and detector sensitivity is made dependent on the laser output level to compensate for changes in lasing efficiency.
:. :
.
: '' ' ' : ', ,:' ~ ' '- '' ' .
In the fabrication and installation of optical cable spans, lengths of optical waveguide are joined together end-to-end using for example a fusion splice. An example of splicing equipment and an operating procedure for using that equipment are described in United States Patent 4,274,707 (Pacey). Particularly for single mode waveguide in which light propagates substantially within a small core of the order of 10 microns in diameter, the cores of the waveguides which are to be spliced must be accurately aligned so that all the light from the core of one waveguide passes into the core of the other waveguide.
One technique for optimizing waveguide end alignment at a splice site is to inject light locally upstream of the site and monitor the light output immediately downstream of the splice site.
The two fiber ends at the splice site are then manipulated until light transmission between the two fibers is maximized.
In our co-pending Canadian patent application serial number 453,707 there is disclosed a local launch and detect system.
The system has top and bottom transparent blocks, the top block having an angled surface with an angled protrusion dimensioned to fit in an angled recess in the lower bloch. The apex of the angle is sufficiently sharp that light propagating along a waveguide located between the two blochs is emitted as a beam at the angle. The device has a detector positioned to monitor the emitted light. A
corresponding unlt for launching light has a laser emitter in place of the detector.
~$
A ~
&~ , .
.
~2S~7~37 In the example specifica11y described in the co-pending specification, the curvature of the protruding angle was set to a desired angle of 146 with a radius of curvature of about 250 microns, this being the diameter also of the coated fiber being spliced.
In the operation of these units it has been found that frequently the fiber retained between the two blocks does not adopt the desired curvature at the apex of the angle. This is disadvantageous for a number of reasons. Firstly the light input device in the case of a local launch unit functions to focus light at a point which assumes a close contact between the fiber and the protruding angle. If the fiber does not in fact contact the block over the critical part of the protruding angle then light launched into the fiber core is not maximized. Similarly detection of maximum light by the local detection unit assumes close contact between the fiber and the protruding angle. Secondly, if the fiber is clamped in a position such that the angle through which the fiber is bent adjacent to the protruding angle is greater than 146 then the fiber is subjected to more stress than it need be.
To overcome this problem there is proposed according to the invention, a fiber optic coupler comprising a cylindrical rod, means for mounting the fiber to extend around a part of the circumference of the rod, a transparent body located on a side of the fiber remote from the rod, spring means for pressing the fiber between the rod and the transparent means to bias the fiber to adopt the radius of curvature of the rod and to form an intimate contact between the transparent body and the curved part of the fiber, and a light input or output device positioned to direct light at or receive light '' '' ' ~ ' ' : ' ' ., - :. . - .
.: ' ', .
~2S1~7~7 from the curved fiber part through the transparent body.
The rod, preferably made of metal, can adhere in a groove formed in a first block. Similarly the transparent body can form part of a second block, the two blocks having complementary surfaces and being mounted relative to one another inside a box fixed with a lid said spring means can be located between the lid and the first block, this arrangement permitting insertion of a fiber between the blocks with automatic applications of the spring bias to the fiber on closing the lid.
A groove can extend around at least said part of the rod circumference for location of the fiber therein. Aligned slots can be formed in one or both of the blocks whereby when the fiber is stretched taut between a pair of the slots, it is aligned with said groove in the rod. The transparent body can be reFractive index matched to the fiber outer coating, the outer coating being resilient to ensure the establishment of said intimate contact between the fiber and the transparent body. The transparent body can have a durable surface facing the fiber to prevent scratching, the durable surface provided by a glass upper layer overlying a mass of transparent epoxy, the light input or output device projecting into said transparent epoxy mass. The light input device can be a laser and t`or a light output unit, the device can be a PIN or avalanche photodiode.
Alternatively the input or output device can be combined with a fiber optic pigtail for guiding light to or from a detector or source respectively located outside the coupler blocks.
When the blocks are located in a position clamping the fiber therebetween, the complementary surfaces thereof should be ~258787 spaced from one another whereby the contact location is limited to the fiber contacts with the first and second blocks.
Preferably control means are provided to the pressure means whereby to insure that when splicing two fibers together the light output from the output unit is a maximum for a fixed input intensity and splice site loss.
An embodiment of the invention will now be described by way of example with reference to the accompanying drawings in which:-Figure 1 shows a perspective view of a coupler according to the invention;
Figure 2 is a cross-section through the device of Figure 1; and Figure 3 is a sectional view on the line III-III of Figure 2.
Referring to the drawings in detail, the unit of Figures 1 and 2 has an upper metal block part 10 and a lower metal block part 12, the block part 12 being fixed within a box 14 and the part 10 being fixed to a lid 16. A compression spring 50 extends between the block 10 and the lid 16. Extending into the sides of the box are slots 18 which are aligned with corresponding slots 20 within the lower block 12.
As shown in sectional view in Figure 2, the two blocks 10, 12 have generally complementary angled surfaces 22, 24. Extending along the apex and protruding from the angled part of the top block 10 is a cylindrical metal rod 26 which adheres in a cylindrical groove 2 along the apex. A groove 30 (Figure 3) having a depth of 100 microns and an included angle of 60 extends around the rod 26 in alignment : ' , .
~ '' ~ ' ' ~:S~7~7 with the slots 20.
The lower block has angle surfaces meeting at 146 with a light input or output device 40 aligned to a line projecking from the apex of the surfaces at an angle 7.5 below the horizontal and 24.3 below the top surface of a glass plate 34. The rod 26 has a radius of curvature of 2.8 millimeters.
The metal lower block 12 has a column 32 of transparent epoxy and a top glass plate 34 flush with the angle face. Extending into the lower block is a bore 36 of 1/4 inch diameter which terminates in a further bore 38 of 1/16 inch diameter. A graded refractive index rod 40 which functions as a converging lens is lodged in the smaller bore 36 and a multimode pigtail fiber 42 with protective jacketing is secured by adhesive within a ferrule 44 which is itself mounted by an epoxy within the wider bore 36. The end of 15 the pigtail fiber projects from the ferrule 44 and is aligned with the axis of the lens 40. The end of the lens remote from the fiber projects into the epoxy mass 32. The other end of the fiber 42 is secured in a position in which it receives the output of a GaAs/GaAlAs semiconductor laser 46 (not shown) having an output wavelength of 0.84 microns.
In use an optical fiber 48 having a resilien-t jacket 49 is positioned so as to extend between the slots 20 whereby it is aligned to the groove 30. The lid 16 is then closed to bias the fiber 48 by means of the spring 50 between the top block 10 and the bottom block 12. The arrangement provides a light-tight enclosure for the portion of the fiber 48 within the box 14. The pressure set on the fiber is determined by the stiffness of spring 50 and the depth of two - ~ -.
~2Si~7~7 cylindrical holes 51, 52 in the lid and the upper block 10. The force should not exceed 1 kg otherwise damage to fiber coating 49 occurs. A
minimum force of 500 grams is required in order to ensure intimate contact of resilient fiber coating 49 with top glass plate 34.
At this pressure, the rod 26 presses the fiber 48 against the planar faces of the lower block immediately adjacent to the angle. This has two effects. Firstly the fiber is caused to adopt the curvature of the rod outer circumFerence where it contacts the rod at groove 30, and secondly, the resilient coating 49 on the fiber is deformed slightly so as to effect an intimate contact between the fiber and the glass plate 34 . -rhe epoxy 36, the glass of plate 34, and the fiber coating material 49 are index matched to one another so that there is minimal light los-t from reflection. The glass plate is 1 millimeter thick and the epoxy is available under the tradename EP0 + TEK 301-2, being an optically clear epoxy whose index is close to that of the glass and the UV curable acrylate fiber coating.
At the rod 26 a relatively sharply angled region is developed in the fiber, the radius of curvature of the fiber being that of the rod. The lens 40 is positioned so as to focus light from the pigtail fiber 42 directly at the fiber angle which is as sharp an angle as possible commensurate with limiting short term stress on the fiber 4~ below that which might result in fracture. If the bend in the fiber had a relatively large radius of curvature, then light injected at one point of the fiber would to some extent, be scattered out of the fiber in the curved portion downstream of where the light enters. By ensuring: (i) that the injected light is properly focussed at the fiber angle; (ii) the apex of the fiber angle is sharp, and .
~ ~ .
. . .
125~378~7 (iii) the axis angles of 40 and 42 are 7.5 below hor;zontal (ie.
24.5 below the angle of the glass plate surface) light loss downstream of the light entry point is minimized. A low wavelength laser is used since the number of modes which can be launched into a fiber is proportional to the inverse of laser wavelength~ In addition, the local launch device is intended for use with a photocell using particularly sensitive silicon photodetectors which have a peak response in the low wavelength regime.
In the detector unit, as described in our co-pending Canadian patent application serial number 453,707 filed May 7, 1984 the laser and the lens 40 are replaced by a photocell which can be sited either within the coupler or at the remote end of a pigtail fiber such as fiber 42. Also, as described in the co-pending application, a single unit can be constructed with a pair of detectors, a pair of light emitters or a combination of a detector and a light emitter. As further described in that patent application, a skeletal unit can be made so as to accept plug-in emitting or detecting devices.
The choice of fiber angle is important since it is a compromise between minimizing light beam size and minimizing fiber stress. The fiber included angle of 146, an angle between the fiber and the axis of the launch or detection device of 24.5 and a rod diameter of 2.8 millimeters recited in this specific example, are values which depend on the relative refractive indexes of the fiber, the jacket material and the coupler block. They depend also on the ability of the fiber to withstand bending stresses. For other types ~` ~
lZ5~7~7 of fiber, the fiber included angle, the angle between the f;ber and the electro-optic device, and the apex radius will be d;fferent.
When using the launch and detection couplers in conjunction with a splicing equipment, the couplers are fixed on either side of the splicing equipment. An upstream fiber is led through the a light input or injection coupler into a splicing zone where the end of the fiber is clamped. The downstream fiber is led through a light output or monitoring coupler and its end portion is clamped at the splicing zone. In the splicing zone one of the fiber ends can be moved incrementally in x, y and z directions using a micromanipulator unit. In use light is launched from the laser into the pigtail fiber 42 housed within a shield 53 as shown in Figure 1 and at the lens 40 is focussed at the fiber core on the upstream side of the splice site. In turn, light is monitored by a silicon photodetector within the downstream detector unit and directed to a level detection circuit. Although manipulation can be achieved mannually, the detector output can be used directly to manipulate the position of one or other of the fiber ends at the splice zone. A
suitable control circuit is described in our copending Canadian patent application Serial Number 485,873, filed June 28, 1985. Subsidiary control loops can be used at each coupler to ensure that pressure on the fibers at each coupler is maintained at a value which maximizes the detector output. To ensure accuracy of monitoring, the output level of the laser is stabilized and detector sensitivity is made dependent on the laser output level to compensate for changes in lasing efficiency.
:. :
.
: '' ' ' : ', ,:' ~ ' '- '' ' .
Claims (12)
PROPERTY OR PRIVILEGE IS CLAIMED ARE DEFINED AS FOLLOWS:-
1. A fiber optic coupler comprising a cylindrical rod, means for mounting a fiber having a core, a cladding and a resilient coating to extend around a part of the circumference of the rod, a transparent body located on a side of the fiber remote from the rod, means for pressing the fiber between the rod and the transparent body whereby the fiber adopts the radius of curvature of the rod and the coating intimately contacts the transparent body, and a light input or output device positioned to direct light at or receive light from the fiber core at the curved fiber part, said light passing through the transparent body.
2. A coupler as claimed in claim 1 in which the rod is a metal rod.
3. A fiber optic coupler as claimed in claim 1 in which the rod adheres in a groove within a plastic block.
4. A coupler as claimed in claim 1 in which a fiber locating groove extends around at least a part of the circumference of the rod in a plane perpendicular to the axis of the rod.
5. A coupler as claimed in claim 1 further comprising means for setting the pressure on the fiber in a region of said rod whereby to deform the resilient coating of the fiber into intimate contact with the transparent body.
6. A coupler as claimed in claim 1 in which the transparent body has a durable glass surface to contact the fiber.
7. A coupler as claimed in claim 6 in which the glass surface forms one surface of a glass plate, the plate overlying a mass of transparent epoxy refractive index matched to said glass plate and wherein the light input or output device projects into the epoxy
8. A coupler as claimed in claim 1 in which the light input device is a laser having a focussing lens to focus emitted light at the core of the fiber at said curved fiber part.
9. A coupler as claimed in claim 1 in which the rod is fixed within a first angled block and the transparent body is fixed within a second angled block, the protruding angle in the first block projecting into and substantially complementary to a recessed angle in the second block, the blocks so mounted that contact between the blocks is limited to a zone immediately adjacent the rod.
10. A coupler as claimed in claim 9 in which the blocks are housed within a light tight housing.
11. A coupler as claimed in claim 1 further comprising means for setting the contact pressure between the rod, the fiber and the transparent body.
12. A coupler as claimed in claim 1 in which the rod has a diameter of about 3 millimeters.
Priority Applications (3)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| CA000476580A CA1258787A (en) | 1985-03-14 | 1985-03-14 | Fiber optic coupler |
| DE19853515195 DE3515195A1 (en) | 1984-05-07 | 1985-04-26 | FIBER OPTIC COUPLERS |
| GB08511358A GB2158607A (en) | 1984-05-07 | 1985-05-03 | Fiber optic coupler |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| CA000476580A CA1258787A (en) | 1985-03-14 | 1985-03-14 | Fiber optic coupler |
Publications (1)
| Publication Number | Publication Date |
|---|---|
| CA1258787A true CA1258787A (en) | 1989-08-29 |
Family
ID=4130028
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| CA000476580A Expired CA1258787A (en) | 1984-05-07 | 1985-03-14 | Fiber optic coupler |
Country Status (1)
| Country | Link |
|---|---|
| CA (1) | CA1258787A (en) |
-
1985
- 1985-03-14 CA CA000476580A patent/CA1258787A/en not_active Expired
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