IMPROVED OPTICAL MODE MIXER USING FIBER OPTIC BUNDLE

Abstract: Improved optical mode mixers (52) for use in conjunction with optical fibers (64) and devices incorporating optical fibers are disclosed and claimed. The optical mode mixers (52) are formed from a coherent, orderly bundle of numerous small diameter optical fibers (64) in a longitudinally aligned, parallel array. The mode mixer (52) is optically linked to the fiber optic cable (36) and effectively reduces undesirable high order modes of light transmission while eliminating alignment sensitivity. The coherent fiber optic bundles may be as short as ten wavelengths of light in length and will have a diameter substantially equal to that of the fiber optic cable (36) to which they are coupled.

Description: IMPROVED OPTICAL MODE MIXER USING FIBER OPTIC BUNDLE FIELD OF THE INVENTION The present invention generally relates to fiber optic lig transmission. More particularly, the present invention relat to fiber optic light transmission in which it is desirable reduce or eliminate high order mode transmission forms. BACKGROUND OF THE INVENTION The utilization of light conducting optical fibers transmit light is well known in the art. The applicability an utilization of fiber optic cables and fibers is presentl reaching into virtually every facet of day to day life. Fibe optics are small, flexible, insensitive to electromagneti fields, and transmit vast quantities of information relati to conventional metallic conductors. As a result, considerabl development has been directed toward incorporating fiber optic into a wide variety of systems including telecommunications computers, and medical devices. Typically, optical cables are formed of glass or plasti clad cores which themselves are made of glass or plastic hav been drawn into relatively uniform, small diameter cables o fibers. The most commonly available in the market place ar the multimode fibers that will propagate light in a mixture o low and high order modes simultaneously (high and low orde modes refer to the angle of propagation of light within th fiber) . Single mode fibers are also available for thos applications where the modal interference associated wit multimode fibers is undesirable. In some applications fiber composition or geometry an external factors such as microbends or splices may responsible for increased attenuation of higher order modes o transmission. Additionally, the modal distribution may var along the length of the fiber due to these internal an external factors. Accordingly, early practitioners in the art performe accurate transmission measurements on both multimode and singl mode fibers in order to compensate for and reduce the influenc of external factors on transmission readings. Alternatively the multimode propagation effects associated with externa factors such as light launching conditions, bends or change in geometry may be accounted for by allowing the mod distribution to reach an equilibrium or steady-stat distribution. This distribution generally occurs automaticall after propagation has taken place over a certain fiber lengt depending upon the strength of the mode coupling within th particular fiber. At equilibrium the mode distributio propagates unchanged. As a result, the fiber attenuation an dispersion effects assume consistent or well-defined values. Unfortunately, in order to reach an equilibrium mod distribution in this manner it may require a fiber severa kilometers in length. While this may be suitable fo telecommunications requirements, packaging such a length fo utilization in space constrained environments is virtuall impossible. Accordingly, a number of alternative methods o obtaining an equilibrium modal distribution with shorter fibe lengths have been developed in the art. For example, modal equilibrium may be achieved using a optical source with a output modal distribution correspondin to the steady state mode distribution of the fiber of interest This technique may be achieved utilizing an optical arrangemen allowing the numerical aperture (a measure of the ligh gathering power of a fiber similar to the f/number of a len [NA=l/2f#] ) of the beam to be varied. Thus, by giving th input light beam an angular width equal to the equilibriu distribution numerical aperture of the fiber and adjusting th source spot size on the fiber input face to match the optica power distribution in a cross section of the fiber equilibriu mode equilibrium may be achieved. This is very difficult t achieve in practice. Alternative mode mixing or mode smoothing techniques quickl induce intermodal coupling within fiber lengths o approximately one meter or less. These generally involve t application of either mechanical perturbations to the fibe including deformations of the fiber cladding or core, or squa or other non-symmetric cross-sectional fiber configuration Each of these alternatives suffers from one or mo disadvantages. For example, it is often difficult to obta stable, reproducible optical characteristics from eith mechanical perturbations or deformations of the fibe Additionally, in some applications even one meter of fiber difficult to package and may require coiling into a fib spool. Additionally, mode mixers based upon sinusoidal point deformations in the optical fiber cladding and/or co may be unstable over time and are exquisitely sensitive changes in the amplitude and shape of the deformation. Thu thermal and mechanical variations may result in nonreproducab transmission characteristics. Mode mixers based up non-symmetric fiber cross sections are physically compact y suffer losses incurred in the conversion of the mode fie distributions from circularly symmetric to non-symmetr distributions. Moreover, non-symmetrical fibers are difficu and expensive to fabricate. These problems are particularly well illustrated consideration of the utilization of fiber optics in medic apparatus due to the physical size constraints inherent in su devices. Medical apparatus and instrumentation have in rece years incorporated the benefits of fiber optic cable whe fiber optics have been adapted to illuminate organs a structures internal to the human body without the need f excessive external cutting and tissue trauma. Additionall arthroscopic surgery and laser treatments using fiber opt cables to transport light have become accepted and comm practices. Recently devices utilizing fiber optics to monit internal body organs and functions before, during and aft surgical procedures have been developed. These types monitoring equipment include oximeters which measure the oxyg content of the blood as it travels throughout the body t monitor cardiac function. Generally speaking, most modern oximeters utilize a cathete or probe which is inserted into the blood stream through major artery or vein. The tip of the oximeter probe supplie light through a fiber optic cable. Light reflected from re blood cells is detected through an adjacent fiber optic cabl in the probe which is connected to a detector. A salin solution or other anticoagulant solution is emitted from th end of the oximeter in order to prevent coagulation of th blood or clot formation around the working end of the oximeter Additional requirements of an oximeter or other apparatu which measures the intensity of reflected light is that reference must be established so that the intensity of th detected light can be compared with the accurately know intensity of the transmitted light. In order to accomplis this, an optical coupler or splitter is used. This coupler ma be realized using several graded index rod lenses (such as "SELFOC" lens as manufactured by NSG America, Inc., or th like) . It has been observed that oximeters and other fiber opti apparatus that rely on the intensity of reflected light t generate data perform better when the light emitted is of particular mode or modal distribution. In many such oximeters the desired modal distribution of light in the emitting fibe is one which yields a far field optical intensity spatia distribution which is approximately Gaussian and distribute symmetrically about the optical axis of the emitting fiber. Such a radiation pattern of output light is measured wit a far-field scanning apparatus similar to those device commonly used in the art to measure the numerical aperture o optical fibers. In order to eliminate undesired modes, the conventiona approach in the art is to use a single mode fiber optic cable or to transmit the optical signal through a multimode fibe optic cable which may be quite long. In either approac precise alignment of the light source and all intermedia optics is required in order to achieve the proper mod distribution. Though relatively effective, a number of significa drawbacks are associated with these prior art apparatu Conveniently packaging a several kilometer long multimode fib optic cable into a workable device is virtually impossibl As a result, compromises have been made attempting to u shorter coiled fiber optic cables. In addition to the packaging problems, the precise alignment requirements a considerable expense and manufacturing complexity to the devices as highly trained operators are required to repeated test and align the delicate fiber optic components. Sing mode fiber optic cables may be unsuitable for many uses as is difficult to couple useful amounts of optical power in them from common optical sources such as LEDs. In additio tend to be very expensive, and do not tolerate sharp bends the fiber optic cable. As noted above, these problems may be common to virtual all apparatus utilizing fiber optic cables to transm information and are not limited to oximeters and relat apparatus. Accordingly, it would be a significant step forward in t fiber optic cable art if these drawbacks could be economical overcome. Such a development would improve the accuracy a cost effectiveness of fiber optic devices, greatly increasi their utility and applicability. The present invention is su a step forward. Thus, it is an object of the present invention to provi a mode mixer that effectively attenuates, or eliminat undesired modes of light transmission. It is a further objection of the present invention provide a mode mixer that reduces system sensitivity to optic alignment and external factors. It is an additional object of the present invention t provide a mode mixer which may be rapidly, efficiently, an economically integrated into an optical system and whic couples minimal volume. SUMMARY OF THE INVENTION These and other objects are achieved by the elegantly simpl mode mixer of the present invention which comprises a pluralit of small diameter optic fibers longitudinally aligned i parallel, each being smaller in diameter than the diameter o the fiber optic cable used to transport the light beam. Th mode mixer of the present invention can be readily incorporate into existing devices and effectively eliminates the need fo an extremely long, cumbersome section of fiber optic cable typ mode mixer, single mode fiber optic cables nonsymmetri cross-section optical conduits, or sensitive mechanica deformation type mode mixers to remove undesired high orde modes of light transmission. As a result, the presen invention greatly reduces the sensitivity to alignment of th optical components within the system. This reduction in sensitivity also reduces the sensitivit of the optical system to mechanical shock, vibration, connecto alignment, and thermal changes that could not be tolerated b the devices of prior art. Thus, apparatus incorporating th mode mixer of the present invention are considerably easier an significantly less expensive to manufacture and calibrate, an more robust in operation. Other features and advantages of the present invention wil become apparent from the following detailed description o exemplary embodiments thereof, taken in conjunction with th accompanying drawings, which illustrate, by way of example, th principles of the present invention. BRIEF DESCRIPTION OF THE DRAWINGS Fig. 1 is a plan view of an exemplary prior art fiber opt cardiac catheter with an integral oximeter. Fig. 2 is a plan view of a fiber optic cardiac catheter wi 5 an integral oximeter utilizing the mode mixer of the prese invention. Fig. 3 is a cross-sectional view of a section of the mo mixer of the present invention taken along plane 3-3 of Fi 2. 0 Fig. 4 is a cross-sectional view of an exemplary individu EMA structure. Fig. 5 is a plan view of a prior art graded index rod le optical coupler showing the light transfer characteristi thereof. 5 Fig. 6 is a plan view of a graded index rod lens optic coupler incorporating the mode mixer of the present inventio Fig. 7 is a plot of the far field radiation scan of t light emission intensity of prior art devices showing intensi as a function of light exit angle with respect to a fiber opt 0 cable propagating two different wavelengths of light. Fig. 8 is a plot of the far field radiation scan of t light emission intensity of the present invention showi intensity as a function of light exit angle with respect to fiber optic cable propagating two different wavelengths , 5 light. Fig. 9 is a cross-sectional view of a fiber optic cab incorporating a mode mixer of the present invention. DETAILED DESCRIPTION 0 Though the present invention is widely applicable virtually all apparatus utilizing fiber optic cable, t features and advantages of the present invention are readi illustrated in the context of an exemplary cardiac cathet oximeter. Accordingly, without limiting the scope of t present invention, the exemplary embodiment of the presen invention will be discussed in this context. Referring more particularly to the drawings, Fig. l show an example of a prior art fiber optic cardiac catheter with a integral oximeter generally indicated by reference 12. Th device consists of a housing 14 containing a light source 2 which, in the exemplary embodiment, supplies both red an infrared light. Those skilled in the art will appreciate tha other characteristic wavelengths of light may be utilized wit the present invention as well as single wavelengths. Th output light from source 20 is transmitted through optica fiber cable 22 to mode mixer 24. Though optical fiber "cable typically includes a protective jacketing, for purposes of th present invention cable 22 may or may not be jacketed. Mod mixer 24 is illustrated as a coil of multimode fiber opti cable as discussed above. As those skilled in the art wil appreciate, this prior art coil is considerably shorter tha the multi-kilometer length necessary to effectively eliminat high order mode light transmissions from the device and is mor a compromise to package as much fiber optic cable as possibl in the device to decrease high order mode transmission withou making the apparatus unwieldy. Nonetheless, mode mixer 24 doe attenuate or eliminate high order modes of light transmission to a limited extent. High order modes of light are those which reflect at a angle nearly perpendicular to the wall of the fiber opti cable. It is desirable to eliminate these high order mod light transmissions from the device because the presence o uncontrolled high order mode distributions tend to distort th accuracy of the measuring system. Additionally, high orde mode distributions are more sensitive to misalignments o optical system components than low-order modes transmissions Light exits from mode mixer 24 and is introduced to a grade index rod lens (GRIN Lens) optical coupler 26. Exemplary GRI Lenses include "SELFOC" lenses such as those manufactured b NSG America, Inc. , a subsidiary of Nippon Sheet Glass Compan Ltd. The GRIN Lens optically couples the output light fr mode mixer 24 to relay lens 28, and provides reflection of portion of the light supplied through fiber optic cable 30 reference detector 32. In this manner, a reference continuously available. The amplitude of this reference proportional to the amplitude of the light co ing out of mo mixer 24. Light is coupled through Jens 28 into detachable fiber opt cable 36. The light is then conducted through fiber opt cable 40 contained within catheter or cable bundle 16. T light is conveyed to distal catheter end 18 where it is emitt into the blood stream through the end of fiber optic cable 4 Reflected light is then conveyed back through a separate fib optic cable 42 within cable bundle 16, to light detector which is located in housing 14. The underlying principle of the fiber optic oximeter is th light of selected wavelengths is transmitted through one of t multimode optical fibers within the catheter bundle (fib optic cable 40 in Fig. 1) to the blood flowing past t catheter tip 18. The light is absorbed by the hemoglob constituents of the blood and is also scattered by blood cell The reflected light is then transmitted back to the seco optical fiber, fiber optic cable 42, to the photodetector 3 Because oxyhemoglobin and hemoglobin absorb light different at the selected wavelengths, the reflected light can analyzed to determine oxygen saturation. In the exemplary embodiment of the present invention lig source 20 contains both red LED (660 nanometer) and IR LED (8 nanometer) light launched into the core of a 500 micromet diameter PMMA type plastic optical fiber through a dichro beam splitter and microball lens (not shown) as known in t art. The plastic fiber optic cable has an exemplary numeric aperture of 0.47 and thus will collect all of the IR beam a will strip the high numerical aperture light of the red LE The coiled fiber on mode mixer 24 is approximately 20 cm long and produces an output beam with an overlap of red light and IR light close to 65%. In order to achieve the necessary overlap of 95% or better the IR light needs to be expanded and the high numerical aperture (high order mode) portion of the red light needs to be stripped out. This is accomplished with prior art by looping the fiber of mode mixer 24 into a small bend radius (0.5 inch diameter) in several turns. The final device used to limit the numerical aperture of both the red and IR light is the GRIN Lens 26 which acts as a one-to-one imager. The resultant output will have numerical aperture overlaps ranging from 92% to 100% and, when the output beam is coupled into catheter fiber 40, the far-field scan of red and IR light from catheter tip 18 shows and acceptable overlap as illustrated by the far-field radiation scan of Fig. 7. Those skilled in the art will appreciate that the overlap between the two wavelengths of light is not perfect and the pattern shows a dip at its peak. Thus, the accuracy of the prior art oximeter may be less than desirable and, more importantly, is extremely sensitive to component alignment within the oximeter. As known in the art, an optical modul with a low overlap will have a different coupling efficienc for different light. This difference will vary depending upon the medium surrounding the catheter tip. Therefore, goo overlap in the optical module is essential to the accuracy of the oximeter. The critical parameters for achieving acceptable overlap i such prior art devices include not only the material propertie but the position and alignment of the various optica components. This results in significant manufacturing cost and decreased reproducability or operational stability ove time as highly skilled operators are needed to calibrate an adjust each instrument. Nonetheless, in spite of thes drawbacks the prior art apparatus have proven general successful, though expensive. In this illustrative embodiment the amount of oxygen in t blood is determined by the ratio of the red and infrared sign supplied by light source 20 and measured by reference detect 32 and reflected light detector 34. The measured informati is then electronically transmitted to a processor (not show whose output is expressed in terms of percent oxyg saturation. Opening 44 in catheter end 18 provides a means for injecti of saline or an anti-clotting agent to prevent clotting on t end of catheter tip 18 interfering with the operation of t catheter. The fluid which exits through opening 44 introduced through opening 46. Various drugs also may introduced in this manner. As noted above, the components of the prior art device shown is Fig. 1 must be carefully aligned to avoid produci an undesirable, low overlap light modal distribution as sho in Fig. 7. Fine tuning adjustments are made to precisely ali each of the optical elements, including the positioning of ea element, as well as the tension applied to fiber optic cabl 22 and 30 and how tightly wrapped the fiber optic cable is mode mixer 24 as the intensity is sensitive to all of tho factors. In contrast, as illustrated in Fig. 2, the present inventi uses a fiber optic cable 50 to convey output light from lig source 20 to the GRIN Lens assembly in housing 26 and t output of the GRIN Lens assembly is then transferred throu mode mixer 52 which attenuates or eliminates undesirable hi order modes of light transmittal. Thus, the bulky coil prior art mode mixer 24 and the associated packaging a alignment problems can be eliminated from the device, desired. Light exits mode mixer 52 and is conveyed throu fiber optic cable 36 in detachable cable bundle or catheter to catheter end 18 in a conventional manner as with the prio art device. Mode mixer 52 is formed of a plurality of relatively smal diameter optical fibers oriented in parallel to one another An exemplary cross section 60 of the plurality of optica fibers 52 is shown in Fig. 3. The exemplary cross section 6 includes a number of optional extra mural absorption (EMA structures 62. EMA structures 62 function to eliminate stra light or crosstalk between fibers. In the present invention these EMA structures assist in attenuating or eliminating hig order modes of light transmissions but are not essential to th practice of the invention. These EMA structures can be in th form of a painting or coating on each fiber such as the laye of black glass 66 as shown in Fig. 4. Alternative EM structures may be produced by placing small amounts of blac glass or plastic in the interstices around each fiber in th bundle or in the form of the statistical EMA structures a represented by reference numerals 62 in which severa transmitting fibers have been replaced with black fibers. The diameter of the individual fibers 64 and 62 within th exemplary mode mixer bundle 52 may very widely as long as th diameter of each individual small diameter optical fiber i less than that of the fiber optic cable optically coupled t the mode mixer. Though it is contemplated as being within th scope of the present invention to utilize fibers each havin identical diameters ranging from approximately 3 microns to 6 microns or more, it is preferred that the coherent fiber opti bundle mode mixer of the present invention be formed from plurality of readily available, low cost standard fiber size ranging from approximately 6 to 8 microns. The diameter of th exemplary fiber optic cable 36 which * transports light t catheter 18 is approximately 250 microns in diameter. Thus there are approximately 10,000 6-8 micron diameter fibers i the exemplary mode mixer 52 which feed light from the GRIN Len to the fiber optic cable 36. The length of the mode mixer 52 is approximately inch this exemplary embodiment. It is recognized that a longer shorter mode mixer can be used within the scope of the prese invention. It is believed that a mode mixer which is long than approximately 10 wavelengths of the light bei transmitted should successfully attenuate or elimina undesired high order mode transmissions. The exact number wavelengths which will sufficiently attenuate high order mo transmissions is uncertain; however, favorable results shou be obtained in most cases with a length of less than inc In the commercial environment in which the present inventi operates it is desirable to use components of sufficient large size so that they can be assembled by hand, if necessar and their orientation adequately observed and secured by operator or technician. Thus, mode mixers smaller then in in length may be difficult to handle and assemble. The mo mixer itself can be fabricated utilizing conventional fib optic materials and techniques including those developed f the production of fiber optic faceplates such as tho available from Incom, Inc. of Southbridge, Massachusetts. The effectiveness of the mode mixer of the present inventi is best illustrated in the comparative far-field radiation sc light emission intensity plots of Figs. 7 and 8. Referri first to Fig. 7, which illustrates the far-field intensi profile of light from two optical sources, red light general represented by a solid line, and IR light represented by dashed line. It is apparent in Fig. 7 that the prior art mo mixer produces a spatial separation of light from the t optical sources as well as a significant drop off in intensi at a 45° angle. In contrast, the mode mixer of the prese invention produces a smooth almost Gaussian distribution light intensity with minimal differences between the t transmitted light signals and no peak drop off as shown in Fi 8. This greatly increases both the accuracy and t reproducability of the oximeter utilizing the prese invention. As a result, the present invention produces a oximeter that is simple and economical to manufacture, calibrate, and use. Attachment of the mode mixer to the GRIN lenses is shown i Fig. 6. In the prior art embodiment of Fig. 5, GRIN Lens 7 consists of two elements 72 and 74 of approximately equa length. Input element 72 has light coupled into the optica cavity of element 72 through fiber optic cable 22 whic corresponds to the output of mode mixer 24 shown in Fig. 1. Once the light has entered the optical cavity of element 72, part of the light is reflected back to fiber optic cable 3 which conveys the reflected light to reference detector 32 a shown in Figs. 1 and 2. There is a gap between optical elemen 72 and optical element 74 of approximately 0.003 inch which ma be occupied by a material having a different refractive inde from that of optical elements 72 and 74. Light is directl coupled from optical element 72 to optical element 74 throug this gap. This light is conveyed to optical element 28 which, in the prior art, is a simple lens which focuses th transmitted light into fiber optic cable 36. This creates series of three lens elements 72, 74 and 28 referred to as trilens arrangement. In contrast, as shown in Fig. 6, a GRIN Lens illustratin the features of the present invention incorporates a fibe optic bundle mode mixer 52 in place of the simple output len 28 of the prior art. As with the prior art embodiment, mod mixer 52 is preferably bonded to optical element 74 wit optical cement such as Epotek 301 and the output of the fibe optic bundle is conveyed to fiber optic cable 36 through an ai gap which is approximately 0.003 inches wide. Accordingly, it is readily apparent that the mode mixer o the present invention is a simple substitution for existin prior art optical elements yet eliminates the need for singl mode fibers or lengthy and awkward multimode fiber opti attenuators. Moreover, in the prior art GRIN Lens th placement of lens 28 against optical element 74 could affe the performance of the device. More specifically, lens 28 h to be substantially centered about the output focal point optical element 74. As a result, this lead to difficulties manufacture and a large number of rejected device. contrast, the fiber optic bundle mode mixer of the prese invention is less sensitive to placement against optic element 74. Moreover, incorporating the fiber optic mode mix of the present invention significantly reduces the sensitivi of the device to light launching conditions or optic component alignment imperfections. Thus, manufacture of t device is considerably easier and less expensive. Further, eliminating the need for the prior art mode mixer 24 and i associated alignment problems the manufacture and adjustme of the device is simplified even more. As ari added benefi the elimination of additional elements and critical adjustme problems enhances the utility and operability of these devic by eliminating their sensitivity to shocks, thermal expansio and abuse. This improves the reliability and service life the devices. It should also be noted that the mode mixers of the prese invention can be utilized without eliminating prior a components such as mode mixer 24 in Fig. 1. Though the pri art mode mixer may be a redundant feature, the utilization the present invention does not require a complete redesign the device as it can be retrofitted to existing designs wi minimal modification. As noted above, the mode mixer of the present invention also readily applicable to a wide variety of fiber opt devices. For example, as shown in Fig. 9, the prese invention can be applied to fiber optic transmission lines inserting a fiber optic bundle mode mixer 94 between fib optic cables 90 and 92 (which may or may not be jacketed) . T diameter of fiber optic cable 90 need not be identical to t diameter of fiber optic cable 92; however, fiber optic mo mixer 94 is formed of one or more optical fibers 96, 98 an 100, each with a diameter that is smaller than either th diameter of fiber optic cable 90 or of fiber optic cable 92. Fiber optic mode mixer 94 also may contain EMA structure (not shown) to further attenuate or eliminate high order mode of light transmission. The diameter of each of the smalle diameter fibers of fiber optic mode mixer 94 is sufficientl less than the diameters of cables 90 and 92 to enable fibe optic mode mixer 94 to attenuate or eliminate high order mode of light transmission. For example, in one embodiment, fibe optic cable 90 has a diameter of 250 microns, as does fibe optic cable 92. Fiber optic mode mixer 94 has a simila diameter and is provided with a plurality of small diamete optical fibers each having a diameter of 6 to 8 microns. Th plurality of fibers within fiber optic mode mixer 94 may b arranged as shown in Fig. 3 resulting in approximately 10,00 fibers comprising fiber optic mode mixer 94. In closing, it is to be understood that the embodiments o the invention disclosed herein are illustrative of th principles of the invention. Other modifications may b employed which are within the scope of the invention and thus, the present invention is not limited to utilization i conjunction with cardiac catheters or oximeters. Accordingly, the present invention is not limited to that precisely as show and described in the present specification.

Claims: CLAIMS: * What is Claimed Is: 1. An improved optical mode mixer for use in conjuncti with a fiber optic cable transmitting light of at least o characteristic wavelength, said mode mixer comprising; a coherent fiber optic bundle optically linked in lig conducting communication to said fiber optic cable and form of a plurality of longitudinally disposed, generally parallel small diameter optical fibers. 2. The improved optical mode mixer of claim 1 wherein sai plurality of longitudinally disposed, generally parallel, smal diameter optical fibers are arranged in an orderly pattern. 3. The improved optical mode mixer of claim 2 wherein sai orderly pattern is a close-packed grid. 4. The improved optical mode mixer of claim 1 furth comprising a plurality of extramural absorption structures. 5. The improved optical mode mixer of claim 1 wherein ea of said plurality of longitudinally disposed, general parallel, small diameter optical fibers has a diameter fr about 3 microns to 60 microns. 6. The improved optical mode mixer of claim 1 wherein ea of said plurality of longitudinally disposed, general parallel, small diameter optical fibers has a diameter fr about 3 microns to 10 microns. 7. The improved optical mode mixer of claim 1 wherein sa coherent fiber optic bundle comprises at least thr longitudinally disposed, generally parallel, small diamet optical fibers. 8. The improved optical mode mixer of claim 1 wherein said coherent fiber optic bundle comprises at least 1000 longitudinally disposed, generally parallel, small diameter optical fibers. 9. The improved optical mode mixer of claim 1 wherein said coherent fiber optic bundle has a length equal to a whole number multiple of said characteristic wavelength. 10. The improved optical mode mixer of claim 9 wherein said whole number multiple is at least 10. 11. The improved optical mode mixer of claim 1 wherein said coherent fiber optic bundle is optically linked in light conducting communication to said fiber optic cable by an adhesive bond. 12. A method for altering the mode distribution of light transmitted through a fiber optic cable, said method comprising the steps of: providing an optical mode mixer formed of a coherent bundle of a plurality of longitudinally disposed, generally parallel, small diameter optical fibers; and optically linking said optical mode mixer in light conducting communication with said fiber optic cable. 13. The method of claim 12 wherein said coherent bundle is formed of at least 3 longitudinally disposed, generally parallel, small diameter optical fibers. 14. The method of claim 12 wherein each of said small diameter optical fibers has a diameter from about 3 microns to 60 microns. 15. The method of claim 12 wherein said optically linki step further comprises forming a light conducting adhesive bo between said optical mode mixer and said fiber optic cable. 16. An improved, low cost, high efficiency catheter bas fiber optic oximeter comprising: at least one light source for generating a light outp having a characteristic wavelength; said light source optically connected to a means f splitting said light output into a transmitted output and reference output; means for detecting said reference output optical connected to said means for splitting said light output; a coherent fiber optic bundle optical mode mixer f altering the mode distribution and removing higher order mod of light from said light output, said optical mode mixer form of a plurality of longitudinally disposed, generally paralle small diameter optical fibers and optically connected to sa means for splitting said light output; and means for transmitting said light output from said optic mode mixer to a fiber optic cardiac catheter. 17. The improved fiber optic oximeter of claim 16 where said plurality of longitudinally disposed, generally paralle small diameter optical fibers forming said optical mode mix are arranged in an orderly pattern. 18. The improved fiber optic oximeter of claim 17 where said orderly pattern is a close-packed grid. 19. The improved fiber optic oximeter of claim 16 where said fiber optic bundle optical mode mixer further compris a plurality of extramural absorption structures. 20. The improved fiber optic oximeter of claim 16 wherei each of said plurality of longitudinally disposed, generall parallel, small diameter optical fibers has a diameter fro about 3 microns to 60 microns. 21. The improved fiber optic oximeter of claim 16 wherei said coherent fiber optic bundle optical mode mixer comprises at least 3 longitudinally disposed, generally parallel, small diameter optical fibers. 22. The improved fiber optic oximeter of claim 16 wherei said coherent fiber optic bundle optical mode mixer has length equal to at least 10 of said characteristic wavelengths of said light output. 23. An improved optical coupler comprising: a first graded index rod lens; a second graded index rod lens optically coupled to sai first graded index rod lens; and a coherent fiber optic bundle optically coupled in ligh conducting communication to said second graded index rod lens.

Inventors: KIM JAMES, MINOT MARK M, KIM, JAMES, MINOT, MARK, M.
Applicants: BAXTER INT, BAXTER INTERNATIONAL INC.
Application year: 1993
Main classification: G01N21
IPC codes: A61B5, G01N21, G02B6