Abstract:
A laser diode system permitting indirect measurement of optical power includes a laser diode which emits usable light from a front facet and spontaneously emits stray light substantially proportional to the usable light from another facet; and a light pipe disposed proximate to the laser diode which collects and waveguides only the stray light to thereby generate a stray light beam providing an indication of optical power.

Description:
This application claim benefit to provisional No. 60/110,052 filed Nov. 25, 1998. 
    
    
     BACKGROUND OF THE INVENTION 
     The present invention relates generally to a laser diode array. More specifically, the present invention relates to a laser diode array having integral structures that facilitate the measurement of optical power generated by the laser diode array. 
     Laser diodes degrade with time and use. Therefore, the current supplied to the laser diode to produce a predetermined optical power at the beginning of life of the laser diode will be different from the current needed to produce the same predetermined optical power at the end of the effective life, i.e., just prior to failure, of that laser diode. It will be appreciated that this fact gives rise to the need to recalibrate the Power vs. Current curve and subsequently control these parameters over the operating life of the laser diode array. This laser diode aging problem is exacerbated when the device being controlled is not a single laser diode but a laser diode array constructed from many laser diode bars, each laser diode bar including a plurality of distinct laser diodes. If one bar fails, then the array continues to operate but at a reduced output level, which could adversely affect the quality of the product being manufactured with the laser. 
     Moreover, it is often desirable to be able to directly monitor various performance parameters of a laser diode array or system. These performance parameters can include, but are not limited to: 
     (i) power output; 
     (ii) optical activity or output; 
     (iii) wavelength detection and tuning indications; 
     (iv) laser operation data of the pumped laser using light traveling back from the laser medium in the cavity to the diode pump source; 
     (v) pulse output characteristics of pulse-driven diode pump sources; and 
     (vi) feedback from damaged optical fiber links for detection and diagnostic purposes. 
     Coupling optics have been used for coupling output emissions of a laser diode pump source to an optical fiber. An example of such coupling optics is disclosed in U.S. Pat. No. 5,127,068 (hereinafter the &#39;068 patent), which is incorporated herein by reference. In the &#39;068 patent, radiation emitted from a laser diode bar, constructed from a plurality of emitters, is focused into a corresponding number of multi-mode optical fibers by means of coupling optics placed between the emitting facets of respective emitters and the ends of the multi-mode optical fibers. The coupling optics disclosed in the &#39;068 patent is simply a piece of the same multi-mode optical fiber, a strand of which extends along the length of a diode bar pump source. It will be appreciated that the coupling optics must be carefully positioned with respect to the emitter facets of the laser diode bar in order to properly collimate the emitter outputs. This is accomplished by aligning and securing the coupling optics in place with a suitable epoxy material. 
     Diagnosis of the performance characteristics for the system discussed immediately above are generally achieved by placing a beam sampling device, e.g., a beam splitter, in the path of the emitted light between any two of the diode pump source, the coupling optics, and the optical fiber. This diagnostic technique presents at least three problems: 
     (i) a beam sampler significantly increases the size of the package; 
     (ii) a beam sampler placed in the path of the emitted light attenuates a portion of the available light, which might otherwise be delivered; and 
     (iii) a beam sampler increases the cost of the system. 
     Moreover, even if the problem of limited space in the laser diode system were ignored, building a feedback subsystem for such a system would require extra mechanical components for stability. Such stabilizing elements add complexity to the feedback system as well as increase the weight and cost of the overall system. 
     In an attempt to overcome the problems mentioned above, U.S. Pat. No. 5,504,762 (hereinafter the &#39;762 patent), which is also incorporated herein by reference, proposed employing the optical fiber constituting the coupling optics to conduct stray radiation, which is not included in the beam that is generated in the emission path by small imperfections in the surface of the lens, to an alternate location. The optical fiber, having a first end and a second end, is oriented with respect to the coupling optics such that radiation from the emitter region is optically coupled into the optical fiber. The second end of the optical fiber is coupled to the laser cavity. A detector is positioned in a spaced, adjacent relationship to the coupling optics, i.e., in an emission path of the stray radiation. The detector detects at least a portion of the stray radiation, and produces a detected output in response to the stray radiation. 
     More specifically, FIG. 1 discloses an arrangement for coupling the radiation emitted from laser diode source  10 , which has a single emitter region, or a bar, having a plurality of emitters  20 ,  22  and  24 , into multi-mode optical fibers  26 ,  28  and  30 , which fibers are part of an optical fiber bundle  32 . The arrangement includes a coupling optics  18  disposed between the emitter facets of emitters  20 ,  22  and  24 , and the ends of multi-mode optical fibers  26 ,  28  and  30 . It will be noted that it is not necessary to couple a certain number of laser diode emitters to an equal number of fibers, fiber bundles, or other optical transfer elements. It is possible to overlay power from more than one emitter to a smaller number of fibers, fiber bundles, or optical transfer elements. It will also be noted that optical transfer devices can extend beyond fibers and can be substantially any optical device or media, either reflective, refractive or open media which is placed at the output of laser diode source  10  to allow the output to be effectively coupled to a desired application. Air is only one of many transfer elements. Other suitable transfer elements include fluids, liquids, and solids. 
     It should be mentioned that a spacing of approximately 60 microns from the near edge of coupling optics  18  to the diode facet is satisfactory for a 250-micron diameter fiber that has an index of refraction of 1.5. The optical spacing of the optical fiber end from coupling optics  18  should be as small as possible; a spacing of about 20 microns is acceptable. 
     It will be noted that the diameter of coupling optics  18  is chosen to be roughly equal to the diameter of the optical fiber to be coupled. The diameter of coupling optics  18  may be less than the diameter of the optical fiber to be coupled without loss in coupling efficiency. However, if such small coupling optics  18  diameters are used, the alignment of coupling optics  18  is more difficult. Coupling optics  18  is placed with respect to the output facets of laser diode source  10  in order to properly collimate them. This may be accomplished by carefully aligning coupling optics  18  and securing it in place with a suitable epoxy. 
     The NA of the optical fiber to be coupled is roughly equal to the low NA direction of diode source  10 , typically 0.1 to 0.15. This combination of coupling optics  18  and optical fiber results in a percentage greater than 80% coupling of the laser diode emitted energy into the multi-mode optical fiber. Coupling optics  18  and the butt-coupled end of the fiber have an anti-reflection coating to reduce reflections from these surfaces. 
     It will be noted that coupling optics  18  is cylindrical in cross-section. Those of ordinary skill in the art will recognize, however, that other cross-sectional shapes, including but not limited to, elliptical and hyperbolic, which can be useful for correction of particular spherical aberrations as known in the art, i.e., Kingslake,  Lens Design Fundamentals,  Academic Press, 1978. 
     As illustrated in FIG. 1, the optical fibers  26 ,  28  and  30  are rectangular in cross-section in order to reduce the total amount of glass in the fiber. The width of the rectangular fiber is chosen to be slightly larger than the diode emitting area The height is as small as possible, typically around 30 to 50 microns. It should be noted that although heights smaller than 30 to 50 microns may be used, such heights make alignment of the system more difficult. The diameter of coupling optics  18  is equal to the height of the rectangular fiber, e.g., 30 to 50 microns in the example given. The resulting fiber output is brighter since the total emission area is smaller. 
     Each emitter region  20 ,  22 , and  24  collectively produces an emitter region emission path of radiation  34  that is optically coupled to optical fibers  26 ,  28 , and  30 . Stray radiation is emitted from coupling optics along a stray radiation emission path  36 . In FIG. 1, stray radiation emission path  36  is generally perpendicular to emitter region emission path  34 . The light that is transmitted along stray radiation emission path  36  is not used to pump the laser medium. 
     Referring now to FIG. 2, a detector  38  is positioned in a spaced, adjacent relationship to the coupling optics  18 , along stray radiation emission path  36 . When coupling optics  18  is a fiber, detector  38  is positioned at one end, or both ends, of the fiber in an emission path of stray radiation, which is generated by coupling optics  18 . Detector  38  is a semiconductor photodiode, such as a semiconductor photodiode manufactured of materials including but not limited to silicon, germanium, alloys of gallium arsenide, and the like. Positioned between detector  38  and coupling optics  18  is an optical filter  40 , which filter eliminates visible light but passes infrared light. Detector  38  is attached to filter  40  to prevent variations due to alignment. Detector  38  detects at least a portion of the stray radiation from coupling optics  18 , and produces a detected output in response to the stray radiation. 
     Coupled to detector  38  is a signal processor  42 , e.g., a digital voltmeter, a sensitive amplifier with fixed or adjustable gain which can be constructed from inverting, noninverting amplifiers, comparators or difference amplifier components. Signal processor  42  receives the detected output from detector  38  and generates a processed output that is representative of a detected characteristic of the laser system associated with diode pump source  10 . A controller  44  couples the processed output from signal processor  42  to a diode power supply  46 . A computer  48  can be included and associated with controller  44 . Computer  48  includes a CPU coupled through a system bus. This system bus can include a keyboard, disk drive, or other non-volatile memory systems, display, and other peripherals, as known in the art. Also coupled to the bus are a program memory and a data memory. 
     From the discussion above, it will be appreciated that the feedback system for a laser diode bar cannot be readily adapted to a laser diode array constructed from a plurality of laser diode bars. For example, in order to sample the output of several laser diode bars  10 , each of the laser diode bars  10  would have associated therewith a separate coupling optics  18 . In addition, it will be noted that the each filament of the coupling optics  18  has an associated mechanical coupling device (not shown) to connect to the detector  38  and that additional structural elements must be included in the overall system to provide additional rigidity to the ends of the coupling optics  18  proximate to the detector  38  in the laser diode system depicted in FIG.  2 . 
     It would be highly desirable to provide a feedback system that is much simpler than those currently proposed. It would also be highly desirable to provide a sampling mechanism that is more robust than those currently proposed. There is a need for a feedback system that would not occupy the limited space between any two of the diode laser source, the coupling optics, a fiber bundle, a laser gain medium, and the focussing optics. There is also a need for a sampling mechanism which does not use light intended for use in pumping the laser medium as an input. In particular, there is an attendant need for a sampling mechanism which permits sampling of the output of the entire laser diode array without substantially impacting the footprint of the array, which would allow the arrays adjacent to one another in a multiple array system to be mounted with minimal separation. It would also be highly desirable to be able to selectively detect the optical power coming from the whole laser diode array or the optical power generated by any one of the individual laser diode bars in a laser diode array. 
     SUMMARY OF THE INVENTION 
     Based on the above and foregoing, it can be appreciated that there presently exists a need in the art for an improved laser diode array which overcomes the above-described deficiencies in the prior art. The present invention was motivated by a desire to overcome the drawbacks and shortcomings of the presently available technology, and thereby fulfill this need in the art. 
     It is often necessary to control the output power of a laser diode array and to monitor the power degradation over time. Preferably, the sampling mechanism can gauge optical power without resorting to inserting an optical element in front of the laser diode array, which would adversely affect output power. The laser diode array and/or system according to the present invention includes an integral power sampling subsystem, wherein at least one stability enhancing element of the laser diode array is employed as a light pipe to channel stray optical energy to a measurement element. According to one aspect of the present invention, side plates on this laser diode array are provided which simultaneously provide support for the array and a mechanism for collecting a sample of the light produced by the laser diode array. According to another aspect of the present invention, an electrical isolator advantageously maintains the electrode plates associated with one laser diode bar of the laser diode array parallel to one another while providing a mechanism for collecting a sample of the light produced by the laser diode bar. 
     The objects, features, and advantages according to the present invention are provided by a laser diode system permitting indirect measurement of optical power. Preferably, the laser diode system includes a laser diode which emits usable light from a front facet and spontaneously emits stray light substantially proportional to the usable light from another facet; and a light pipe disposed proximate to the laser diode which collects and waveguides the stray light to thereby generate a stray light beam providing an indication of optical power. 
     The objects, features and advantages according to the present invention are provided by a laser diode apparatus, which includes a laser diode which emits light in a first direction from a front facet, a heatsink electrode electrically coupled to a bottom facet of the laser diode, an electrode electrically coupled to a top facet of the laser diode, and an isolator disposed between the heatsink electrode and the electrode, the isolator including a light pipe collecting spontaneous emissions from at least one of a rear, a left side, and a right side facet and waveguiding the collected spontaneous emissions in a second direction opposite to the first direction. 
     The objects, features and advantages according to the present invention are provided by a laser diode system permitting indirect measurement of optical power. Advantageously, the laser diode system includes a laser diode which emits light in first direction from a front facet, a heatsink electrode electrically coupled to a bottom facet of the laser diode, an electrode electrically coupled to a top facet of the laser diode, an isolator disposed between the heatsink electrode and the electrode, and a structural element. Preferably, the structural element includes a light pipe which collects stray light different from but proportional to a usable component of the light and which waveguides the stray light in a second direction opposite to the first direction to thereby generate a stray light beam providing an indication of optical power. In an exemplary case, the structural element comprises a side plate of the laser diode system. 
     According to one aspect of the present invention, the laser diode system also includes a lens attached near the front facet of the laser diode so that only stray light, which is equal to the difference between the light and the usable component of the light, is optically coupled to the side plate. According to another aspect of the invention, the stray light corresponds to spontaneous emissions from one of a rear, a left side and a right side facet of the laser diode. When the stray light is produced by the rear facet of the laser diode, a secondary light pipe positioned between the laser diode and the isolator can be employed to route the stray light to the side plate. 
    
    
     BRIEF DESCRIPTION OF THE DRAWINGS 
     These and various other features and aspects of the present invention will be readily understood with reference to the following detailed description taken in conjunction with the accompanying drawings, in which like or similar numbers are used throughout, and in which: 
     FIG. 1 is a perspective view of a conventional arrangement for coupling the output from a laser diode bar into an optical fiber bundle; 
     FIG. 2 is a high-level block diagram of a conventional feedback system incorporating the coupling optics illustrated in FIG. 1; 
     FIG. 3 is an exploded view of a laser diode unit including a laser diode bar employed in the present invention; 
     FIG. 4 is a three-dimensional exploded view of selected portions of the laser diode unit illustrated in FIG. 3; 
     FIGS. 5 a-   5   c  collectively illustrate a laser diode array according to a first preferred embodiment of the laser diode array according to the present invention; 
     FIG. 6 illustrates an alternative configuration of the laser diode array of FIGS. 5 a-   5   c;    
     FIGS. 7 a-   7   b  collectively illustrate another alternative configuration of the laser diode array of FIGS. 5 a-   5   c;    
     FIG. 8 illustrates a second preferred embodiment of the present invention with respect to the laser diode unit depicted in FIGS. 3 and 4; 
     FIG. 9 illustrates a third preferred embodiment of the present invention with respect to the laser diode unit depicted in FIGS. 3 and 4; and 
     FIG. 10 illustrates a fourth preferred embodiment of the present invention with respect to the laser diode unit depicted in FIGS.  3  and  4 . 
    
    
     DETAILED DESCRIPTION OF THE PREFERRED EMBODIMENTS 
     As discussed above, it is desirable to control the output power of a laser diode array and to monitor the power degradation over time, preferably without inserting an optical element in front of the array, which would adversely affect output power. The improved laser diode array according to the present invention satisfies this desire by including an integral power monitor subsystem, wherein at least one stability enhancing element of the laser diode array is employed as a light pipe to channel stray optical energy to a measurement element. In the first through third preferred embodiments according to the present invention, the side plates on a laser diode array simultaneously provide support for the array and a mechanism for collecting a sample of the light produced by the array. According to a fourth preferred embodiment according to the present invention, an electrical isolator advantageously maintains the electrode plates of the laser diode array parallel to one another while providing a mechanism for collecting a sample of the light produced by the laser diode bar. Each of these preferred embodiments will be discussed below in turn. 
     With respect to the first several preferred embodiments, the improved laser diode array according to the present invention is constructed from an array of laser diode units. Preferably, these laser diode units are constructed from four major elements, as illustrated in FIGS. 3 and 4. In other words, each laser diode unit  100  is constructed from a heatsink electrode  102 , a laser diode bar  104 , an electrical isolator  106  and an electrode  108 . It should be noted that the small tabs  102   a, b  at the front of the heatsink electrode  102  serve as a place to mount the optics, which are discussed in detail below, for collimating the usable light generated by each laser diode unit  100 . It should also be noted from FIG. 4 that the top of the laser diode bar  104  advantageously contacts the underside of electrode  108 , i.e., the laser diode bar  104  protrudes above the surface of heatsink electrode  102  contacted by the electrode  108 , a portion of which advantageously is shaped to compensate for the thickness of the isolator  106 . 
     It will be appreciated that heat generated by the laser diode bar  104  is transferred to the heatsink electrode  102  for ultimate removal by coolant circulating in coolant channels  110  formed in the heatsink electrode  102 , the electrical isolator  106  and the electrode  108 . It will also be appreciated that the coolant is maintained in the coolant channels by a plurality of O-ring seals, which are generally denoted  112 . The coolant interconnections to the laser diode unit  100  are provided by a pair of O-ring seals  112  on the top and bottom of the laser diode unit. The O-rings on the top of the laser diode unit  100  advantageously can be retained by the combination of the electrical isolator  106  and the electrode  108 . 
     Now referring to FIGS. 5 a-   5   c,  it will be appreciated that a plurality of the laser diode units  100  advantageously can be stacked to any arbitrary height, to thereby form the laser diode assembly  202  of the laser diode array  200 . Typically, twenty laser diode units  100  are employed in the laser diode assembly  202 , although it will be noted that laser diode assembly&#39;s  202  containing more or fewer laser diode units  100  are possible. 
     Still referring to FIGS. 5 a  and  5   b,  it will be noted that the laser diode assembly  202  is disposed between manifolds  206   a,    206   b,  which, in an exemplary case, are attached to the laser diode assembly  202  by a plurality of bolts  204 . It should be mentioned that the manifolds  206   b,    206   a  serve as the electrical contacts to the laser diode assembly  202 , i.e., selected ones of the bolts  204  are electrically connected to the heatsink electrode  102  of the lowermost laser diode unit  100  in the laser diode assembly  202  while other selected ones of the bolts  204  are electrically connected to the electrode  108  of the uppermost laser diode unit  100  in the laser diode assembly  202 . It should also be noted that the manifolds  206   a,    206   b  include quick disconnect elements  208  provided with O-ring seals  208   a  for routing coolant to and removing coolant from the plurality of coolant channels  110  formed by the laser diode assembly  202 . Additional structural support for the laser diode array  200  advantageously is provided by a pair of side plates  210 ,  212 , as discussed in greater detail below. 
     As illustrated in FIGS. 5 b  and  5   c,  a series of cylindrical, aspheric, or prism lens  220  are aligned to the front of the laser diode assembly  202 . Preferably, each of the lenses  220  is attached to a corresponding heatsink electrode  102  at tabs  102   a,    102   b.  Preferably, the lenses  220  advantageously can be precisely aligned; this alignment being maintained because of the construction of the laser diode assembly  202 . Each of these optical elements, i.e., one of the lenses  220 , serves to collimate the output of one level of the laser diode assembly  202 , either in the transverse direction, the lateral direction, or both directions simultaneously. 
     In accordance with a first embodiment of the present invention, each lens  220  advantageously can be employed to sample the output of the laser diode unit  100  without degrading the amount of light applied to downstream optical elements. Stated another way, since the lenses  220  are normally as long as the corresponding laser diode bar  104  that they are being used to collimate, a significant amount of light is scattered along each lens  220 . Moreover, since each lens  220  has a higher index of refraction than the surrounding air, the light, which is scattered into high angles, is trapped in the lens  220 . This light propagates along the lens  220  and exits at the ends of the lenses  220 . Advantageously, the light exiting at the ends of the lenses  220  can be collected by one or both of the side plates  210 ,  212 . In the first preferred embodiment according to the present invention, the light is collected by a 45° angled facet on the side plates. The collected light is then waveguided via fiber optic cable  222  embedded in each side plate  210 ,  212  toward the back of the laser diode array  200  where it is combined into a single output. It will be appreciated that the combined output from all of the laser diode units  100  advantageously can be applied to a single detector  240  (depicted in FIG.  8 ). Alternatively, as shown in FIG. 6, each output of the respective laser diode units  100  advantageously can be separately waveguided to a detector array  230 . 
     It should be mentioned at this point that either or both of the side plates  210 ,  212  advantageously can include a “light pipe” for conveying stray light, i.e., light not contributing to the focused output of the lens  220 , to an optical detector, e.g., detector array  230  or detector  240 . Hereinafter, while only the side plate  210  will be addressed, it will be understood that either, or both of the side plates are encompassed by this terminology. 
     In an alternative to the first preferred embodiment according to the present invention illustrated in FIGS. 7 a  and  7   b,  the light is first collected by a 45° angled facet on the side plate  210  (see FIG.  8 ), and is then waveguided toward the back of the laser diode array  200  by the transparent side plate  210 . Since the index of the side plate  210  is 1.5, and the index of air is 1, the side plate  210  advantageously forms an excellent waveguide in the transverse direction. The concentration and mixing of the total power of the laser diode array  200  is accomplished by the taper cut into the side of the side plate  210 . This taper acts as a non-imaging concentrator, it directs the sampled light toward detector  240  (See FIG. 8.) mounted at the back of the laser diode assembly  202  in the laser diode array  200 . It should be mentioned that the tapered cut can be a cut directly in the side plate  210 , extending some fraction of the way through the side plate. Alternatively, the taper cut can be a separate waveguide section molded into an opaque side plate. It will be appreciated that this structure enables the laser diode system to monitor the output power of the laser diode assembly  202  at all times. Moreover, when combined with the system electronics, it is possible to monitor the continuous degradation of the performance of the laser diode array  200 . 
     A second preferred embodiment according to the present invention will now be described while referring to FIGS. 4 and 8, where the side plate  210  is adapted to receive stray light produced by random spontaneous emissions from the edge of the laser diode bar  104 . From FIG. 4 it will be appreciated that at least a portion of the laser diode bar  104  extends above the heatsink electrode  102 . Thus, emissions from the laser diode bar  104  advantageously can be collected at the side plate  210 . It will also be appreciated that the alternative configurations of the side plate  210  illustrated in FIGS. 5 a,    5   b,    6 ,  7   a,  and  7   b  are also applicable to the side plate  210 . In fact, all configurations of the side plate permitting stray spontaneous emissions from the laser diode bar  104  to be collected are considered to fall within the scope of the present invention. 
     For example, in a third alternative embodiment according to the present invention illustrated in FIG. 9, the spontaneous emissions from the rear of laser diode bar  104  advantageously can be collected by a secondary light pipe  106   a,  which is disposed between the laser diode bar  104  and the isolator  106 . The secondary light pipe  106   a  is preferably constructed from a transparent material such as glass, although other plastic or crystalline materials, to name a few, can also be employed. Advantageously, the surface  106   b  of the secondary light pipe  106   a  can be treated or otherwise prepared to promote further reflections whereby the spontaneous emissions are coupled out of the secondary light pipe  106   a  and into the side plate  210 , i.e., the primary light pipe. It will be appreciated that the alternative configurations of the side plate  210  illustrated in FIGS. 5 a,    5   b,    6 ,  7   a,  and  7   b  are also applicable to the side plate  210  illustrated in FIG.  9 . 
     Referring now to FIG. 10, in a fourth preferred embodiment according to the present invention, the light pipe which conducts spontaneous emissions from the rear surface of laser diode bar  104  advantageously can be a suitably configured isolator  106 , which includes a taper  107  cut into the side of the isolator  106 . It will be appreciated that the taper  107  transitions to a straight section in order to avoid the coolant channels  110 . This taper  107  acts as a non-imaging concentrator; it directs the sampled light toward a detector, e.g., one of the detectors Det. 1 -Det.  4  included in the detector array  230  of FIG. 6, which advantageously can be positioned along the axis of the laser diode unit  100 , i.e., mounted at the back of the laser diode assembly  202  in the laser diode array  200 . It should be mentioned that the tapered cut could be a cut directly in the isolator  106 , extending some fraction of the way thorough the isolator. Alternatively, the taper cut can be a separate waveguide section molded into an opaque isolator  106 . It will be appreciated that this structure enables the laser diode system to monitor the output power of the individual laser diode units  100  in the laser diode assembly  202  at all times. Moreover, when combined with the system electronics, it is possible to monitor the continuous degradation of the performance of discrete elements of the laser diode array  200 . 
     It will be appreciated that the laser diode system discussed above provides a feedback mechanism which is both much simpler and more robust than other feedback mechanisms. In addition, it will be noted that the feedback mechanism permits the optical power output of a laser diode array to be sampled either collectively or section-by-section, depending on the configuration, throughout the effective life of the laser diode array. When the feedback mechanism permits section-by-section sampling of laser diode bar optical power output, the feedback mechanism permits early identification of under performing laser diode bars. 
     It will also be appreciated that by incorporating the sampling and/or feedback mechanism into a structural member of the laser diode array, the footprint of the laser diode array remains virtually unchanged. Advantageously, the sampling mechanism for the laser diode array according to the present invention does not occupy the limited space, (i) between the diode source and the coupling optics or (ii) the coupling optics and fiber bundle or laser medium. In other words, the light intended for use downstream of the laser diode or laser diode bar is not used as an input to the feedback and/or sampling mechanism. 
     Although presently preferred embodiments of the present invention have been described in detail hereinabove, it should be clearly understood that many variations and/or modifications of the basic inventive concepts herein taught, which may appear to those skilled in the pertinent art, will still fall within the spirit and scope of the present invention, as defined in the appended claims.