Abstract:
A system and method for laser light amplification provides amplification of a laser light beam emitted from a laser light source as low-amplification seed laser light signal. The low-amplification seed laser light signal is transmitted to an amplification component. The amplification component amplifies the low-amplification seed laser light signal by stimulating emissions of the population inversion provided by a pumping diode to generate an amplified laser light signal. The system and method further directs the amplified laser light signal to an output destination. The result of the present invention is a system and method of operation providing higher pulse rates, improved pointing stability, and optionally variable pulse rates for a variety of uses, including for non-destructive laser ultrasonic testing of materials.

Description:
TECHNICAL FIELD OF THE INVENTION 
     The present invention relates generally to a system and method for laser light amplification and, more particularly, to a system and method for providing amplification of a laser beam emitted from a solid state laser that provides higher pulse rates, improved pointing stability, and optionally variable pulse rates for a variety of uses, including for non-destructive laser ultrasonic testing of materials. 
     BACKGROUND INFORMATION 
     Amplification of laser light is required for a variety of applications. Long haul telecommunication applications, such as those employing single mode optical fiber, often require optical repeater/amplifiers to boost sagging signal levels. Material processing applications may require very high power laser light to perform functions such as cutting of various materials and preparation of material surfaces. Applications requiring intense energy pulses of laser light employ some configuration for providing either time-varying optical amplification or intensity modulation of laser light. 
     One method for amplifying a laser beam is to employ a laser medium whose optical gain may be controlled by optical pumping. Optical pumping of a solid state laser medium is a common and conventional method used to create a population inversion of energy states for laser applications requiring high-gain. The laser medium providing high-gain, when optically pumped, may comprise a material such as neodymium yttrium-aluminum garnet (Nd 3+ :YAG), neodymium glass (Nd 3+ :glass), Erbium doped optical fiber (Er 3+ :silica), or Ruby rods (Cr 3+ :Al 2 O 3 ). These materials are merely exemplary candidates for high-gain laser media, and those skilled in the art will appreciate that any suitable material capable of maintaining an inverted population of energy states when optically-pumped may serve as an optical amplifier. Those laser media utilizing Nd 3+ :YAG are common, given the substantial optical gain near desired wavelengths near the 1.064 μm range. Additionally, Nd 3+ :YAG laser media provide linearity of pumping rate with respect to inverted population given its four-level transition system that is also well known to those skilled in the art. 
     To saturate an entire laser medium with an inverted population through optical pumping, a conventional method is to distribute a large array of laser diodes across the surface of the laser medium to form a pumping array. The light emitted from the individual laser diodes of the pumping array excites the laser medium and provide a very high optical gain for the energy transition level of the optically-pumped, inverted population within the high-gain laser medium, e.g., near the 1.064 μm range for Nd 3+ :YAG, near the 1.06 μm range for Nd 3+ :glass, near the 0.6943 μm range for Cr 3+ :Al 2 O 3 , near the 1.55 μm range for Er 3+ :silica, etc. 
     An integrated approach to performing laser light amplification and generating optical pulses utilizes gain switching of a laser medium. In this method of providing a high energy pulsed laser beam, the optical pumping of a high-gain laser medium itself is pulsed to generate a time varying gain of the high-gain laser medium through which a laser beam is propagating. This results in a pulsed output laser beam after an original laser light source has traveled through the high-gain laser medium that is being optically pumped in a time varying manner. 
     Each optical pumping cycle takes the high-gain laser medium through a transition which consists essentially of generating a sufficient energy state population through optical pumping to reach threshold for amplification. Before the optical pumping begins, the population of energy states is initially below threshold and optical amplification does not occur. After the high-gain laser medium has operated in an amplification mode for some time, then optical pumping is switched off, and the energy state population is subsequently depleted. By turning off the optical pumping, the population falls below threshold and the optical amplification is interrupted until the optical pumping again resumes and the population of energy states again reaches threshold. Such a method provides for a pulsing of the conditions in which laser light amplification may occur. Such a method is preferable to a method which merely blocks a highly amplified laser beam in that design considerations need not include the potentially loss energy due to the dumping of electromagnetic energy into a shutter assembly. Many other advantages are inherent to the fact that the solution is electronic, not incorporating any mechanical components for a mechanical shutter system. 
     Another method for providing an electronic solution is to generate a high energy pulsed laser beam to maintain continuous optical pumping of the high-gain laser medium and to modulate the high-gain laser medium&#39;s loss coefficient. One method to perform such loss switching is to electronically modulate an optical absorber that is placed within the optical resonator cavity next to the high-gain laser medium. Such a configuration will permit the user to control the loss of the laser light traveling through the high-gain laser medium as opposed to controlling the rate at which optical pumping occurs. Those skilled in the art will recognize a variety of methods for performing loss switching of laser light contained within a the highgain laser medium including electrical modulation of an electro-optic crystal to perform intensity modulation of the laser beam. 
     Such a method is an extension of the gain switching method as an optical resonator&#39;s threshold energy state population difference is proportional to the resonator&#39;s loss coefficient. In this method, the loss coefficient is modulated to provide intermittent periods when the optical loss of the high-gain laser medium is prohibitively high to maintain oscillation. This results is creating an increased energy state threshold population to sustain oscillation, given the increased loss of the high-gain laser medium. Even though the energy state population would be sufficiently high for oscillation were the loss coefficient of the high-gain laser medium not increased, no optical amplification can occur during the period when the loss coefficient is elevated. 
     When the loss in suddenly decreased during the transition of a pulsing cycle the loss coefficient, the energy state population begins to deplete resulting from the decreased optical losses. The high-gain laser medium will amplify the laser light during the period when the energy state population exceeds the threshold condition for oscillation during the period that the loss coefficient is minimum. However, as the population continues to decrease, the population will eventually fall below the newly established energy state threshold for oscillation corresponding to the period of time when the loss coefficient is at its minimum during a modulation cycle. 
     These methods of performing electronic switching of either the gain or loss coefficients of the highgain laser medium often employ flashlamp optical pumping. The use of such a light source for performing the optical pumping presents some undesirable effects which significantly limit performance of the high-gain laser medium in providing pulses of laser light including the maximum pulse rate of the laser beam and the intensity with which the optical pumping must be performed. Such inherent problems may present significant problems for applications which require high pulse rates and suffer from limited power budgets. 
     Another problem that is introduced by the utilization of flashlamps to provide optical pumping is the broad spectral width of flashlamp produced light may prove very inefficient in that a large proportion of the light produced by the flashlamp does not serve to generate the inverted population of energy states. Flashlamp light outside of the spectral density range required for generating the inverted population is simply lost into the high-gain laser medium in the form of thermal heating. This heating of the high-gain laser medium may itself produce undesirable effects including beam pointing errors and self-focusing. The heating of the high-gain laser medium may increase to such levels that fracture of the solid-state crystals will limit the maximum peak or average power. 
     The pulse rate at which the laser amplifier may be switched is also limited by the physical properties of the flashlamps which provide the optical pumping. The electrical switching of the flashlamps is often associated with the thermal heating problems associated with the flashlamps themselves. This upper limit of pulse rate may also be determined in part by the intensity level at which the flashlamps must operate to generate an inverted energy state population above threshold. For example, if the energy transition of interest is near the periphery of the spectral density of the flashlamp, the flashlamp may necessitate operation at a very high power level to generate the inverted population. Such a situation may at the very least limit the duty cycle of the pulse rate to avoid overheating of the flashlamps themselves. 
     Additionally, the flashlamps intrinsically possess a start up time constant before they begin optical pumping. They do not respond instantaneously with the vertical transition of the electric signal which drives them. Consequently, the maximum pulse rate of the optical amplifier may be limited by the time constant corresponding to the start up of the flashlamps. Another consequence of the intrinsic response limitations of the flashlamps is a lower limit on the width of the pulse which may be generated using such a laser amplification system. Such a problem stems from the similar characteristic of the flashlamps in that they are limited in the speed with which they may switch on and off. The minimum pulse width which may be generated is often dictated by the minimum time in which the flashlamps may turn on and then turn off, including considering of the start up time constant of the flashlamps and evanescent decay of radiation from the flashlamps when turned off. 
     The present invention overcomes or eliminates the problems and limitations of known systems and methods for detecting high-speed laser-induced ultrasound to provide a system and method for laser beam amplification from a solid state laser that yields high pulse rates, improved pointing stability, and optionally variable pulse rates for non-destructive laser ultrasonic testing of materials, as well as a variety of other uses. 
     SUMMARY OF THE INVENTION 
     According to one aspect of the present invention, there is provided a method for generating an amplified laser beam at a high pulse rate that includes generating a low-amplification seed laser light signal. The method further includes transmitting the lowamplification seed laser light signal to an amplification component. The low-amplification seed laser light signal is amplified in the amplification component by stimulating emissions of the population inversion that a pumping diode provides. The result of this amplifying step is to yield an amplified laser light signal. The amplified laser light signal is then directed to an output destination. 
     The present invention provides a system and method for providing amplification of laser light from a solid state laser while maintaining the physical properties of the laser light by minimizing amplification induced distortion. A seed laser possessing desired physical properties including a single longitudinal mode with a desired linewidth is passed through a high-gain laser medium. The high-gain laser medium is optically pumped using a pumping array of laser diodes distributed across the high-gain laser medium. The electric current which drives the pumping array may be a timevarying signal which consequently provides time-varying optical gain and lasing conditions within the laser medium. The amplified laser beam may then be pulsed at a pulse rate corresponding to the frequency of the time-varying signal comprising the electric current which drives the pumping array of laser diodes. 
     The present invention may be employed in applications which require a particularly narrow or pure spectral density such as applications involving optical interferometry which often require a single longitudinal mode having a very stable center frequency and linewidth. For such applications in which the purity of the initial seed laser is amplified to generate a pulse stream of laser light having a desired intensity level, duty cycle and pulse rate, an optical isolation assembly may be used to minimize back reflection of the laser light into the seed laser light source. Undesirable parasitic feedback may corrupt the seed laser source resulting in deleterious performance of the seed laser including amplitude noise and multimode operation. Such effects may be disastrous for those applications requiring a spectrally pure laser source. One conventional method, well known to those skilled in the art, for providing optical isolation of a laser beam which minimizes back reflections into the original light source comprises a Faraday rotator and two polarizers which provide for light propagation in only one direction through the optical isolation assembly by using the non-reciprocal rotation of a polarized lightwave provided by a Faraday rotator. 
     Additional optical isolation assemblies may be included in the invention for providing beam splitting of the original laser beam for directing the amplified, pulsed output laser beam or directing of the original laser beam through the high-gain laser medium multiple times for even greater amplification than a single pass through the high-gain laser medium. 
     The present invention generates an amplified and pulsed laser beam which possesses similar physical properties of the original seed laser including a desired center frequency and linewidth for use within an optical interferometer to perform ultrasonic detection. Additionally, the output intensity of the pulsed, amplified laser beam may be modulated to extend the dynamic range of detection within an optical interferometric system. Electro-optic modulators comprising Pockels or Kerr effect crystals are well known to those skilled in the art for providing intensity modulation of a laser beam. 
     The present invention provides an important technical advantage by performing optical pumping of a high-gain laser medium using a pumping array of laser diodes. This method permits optical pumping within a very narrow wavelength regime selected by the use of appropriate laser diodes to minimize optically-induced thermal heating of the laser medium. This advantage is provided primarily by the fact that the appropriate choice of laser diodes which comprise the pumping array may be chosen to optically pump within a specific wavelength regime thereby not incurring significant thermal heating by radiation bombardment of the highgain laser medium with optical pumping outside of the energy transition level of interest. 
     The present invention provides another technical advantage by providing for maximizing the pulse rate and controlling the pulse width of the resulting amplified pulsed laser beam by performing the optical pumping using a pumping array comprising a multiplicity of laser diodes. The maximum pulse rate for the present invention will be determined largely by the speed at which the laser diodes may be turned on and turned off and the allowed duty cycle. 
     The present invention provides another technical advantage by minimizing amplification induced distortion of a seed laser beam. Many applications, including optical interferometry, require a highly amplified beam with a uniform wavefront and good pointing stability. 
     The present invention provides another technical advantage by providing for intensity modulation of the output laser beam thereby expanding the detection dynamic range within interferometric systems. 
    
    
     BRIEF DESCRIPTION OF THE DRAWINGS 
     For a more complete understanding of the present invention and the advantages thereof, reference is now made to the following description taken in conjunction with the accompanying drawings in which like reference numerals indicate like features and wherein: 
     FIG. 1A shows a polarization selective assembly comprising an optical isolator; 
     FIG. 1B shows a polarization selective assembly comprising a four port optical device providing polarization selective directing of a laser beam; 
     FIG. 2 shows a configuration of a laser light source capable of preventing optical feedback and varying the intensity variation of the laser light by rotating a half waveplate; 
     FIG. 3 shows another configuration of a laser light source capable of preventing optical feedback and varying the intensity variation of the laser light using an electro-optic modulator; 
     FIG. 4 shows one possible embodiment of the invention comprising a four pass, dual rod laser media pulsed laser light source; 
     FIG. 5 shows another possible embodiment of the invention comprising a dual pass, dual rod laser media pulsed laser light source; 
     FIG. 6 shows another possible embodiment of the invention comprising a four pass, single slab laser medium pulsed laser light source; 
     FIG. 7 shows another possible embodiment of the invention comprising a four pass, dual slab laser media pulsed laser light source; 
     FIG. 8 shows another possible embodiment of the invention comprising an eight pass, single slab laser medium pulsed laser light source; 
     FIG. 9A shows one alternative embodiment of the present invention; and 
     FIG. 9B shows still a further alternative embodiment of the present invention. 
    
    
     DETAILED DESCRIPTION OF THE INVENTION 
     Embodiments of the present invention are illustrated in the FIGUREs, like numerals being used to refer to like and corresponding parts of the various drawings. 
     The present invention provides a system and method for providing amplification of laser light from a solid state laser while maintaining the physical properties of the laser light while minimizing amplification induced distortion. A seed laser possessing desired physical properties including a single longitudinal mode with a desired linewidth is passed through a highgain laser medium. The center frequency of the seed laser source may be chosen appropriately as to perform within specific applications such as optical interferometry which require very coherent light. The high-gain laser medium is optically pumped using a pumping array of laser diodes distributed across the high-gain laser medium. The electric current which drives the pumping array may be a time-varying signal which consequently provides time-varying optical gain and lasing conditions within the laser medium. The amplified laser beam may then be pulsed at a pulse rate corresponding to the frequency of the time-varying signal comprising the electric current which drives the pumping array of laser diodes. 
     FIG. 1A shows a polarization selective assembly comprising an optical isolator  10 . A typical arrangement of an optical isolator passes a laser beam  18  through a first polarizer  12 . The polarized light then passes through a Faraday rotator  14 . A Faraday rotator provides optical rotation of a polarized light way in a non-reciprocal fashion. That is to say, polarized light passes through the Faraday rotator will rotate in one and only one direction regardless of the direction of propagation of the laser beam through the material. For example, a laser beam  18  traveling through Faraday rotator  14  rotates clockwise as it propagates in the direction of the arrows of laser beam  18 , then a laser beam  18  traveling in the opposite direction of the arrows of laser beam  18  will also rotate clockwise. Faraday rotators  14  are well known to those skilled in the art, and may comprise a number of materials including yttrium-iron-garnet (YIG) or terbium-gallium-garnet (TGG). 
     The first polarizer  12  transmits only P-state light from the input  18 . After traveling through Faraday rotator  14 , laser beam  18  is rotated 45°. Following the Faraday rotator is a half waveplate  16  which provides an additional 45° of polarization rotation in the opposite direction of Faraday rotator  14 . Light polarized in a P-state traveling in the direction of the arrows has a net rotation of zero. A half waveplate and its operation are well known to those skilled in the art. Light polarized in a p-state traveling in the direction of the arrows of laser beam  18  through the optical isolator  10  travels unencumbered, yet light (possibly unpolarized, such as from random scattering) traveling in the opposite direction of the arrows of laser beam  18  through the optical isolator  10  is blocked. This stems from the fact that the Faraday rotator exhibits non-reciprocal angular rotation of a polarized light beam. Light traveling in the opposite direction of the arrows of laser beam  18  is polarized by the a polarizer  12 , then pass through a half waveplate  16  and then through the Faraday rotator  14  for a net rotation of 90°. The Faraday rotator  14  will rotate the light one half of the angular difference between the two polarizers  12  so that when light traveling in the opposite direction of the arrows of laser beam  18  meets the originally first polarizer  12 , at an angle of incidence that is perpendicular to the polarizer&#39;s pass axis thereby completely blocking back reflections through the optical isolator  10 . In effect, an optical isolator  10  serves as an optical diode or check valve. 
     FIG. 1B shows a polarization selective circulator assembly comprising a four port optical device  11  providing polarization selective directing of a laser beam. A laser beam  18  enters a polarizing beam splitter  17  in which polarized light aligned to one axis of the polarizing beam splitter  17  passes through, and polarized light not aligned to that one axis of the polarizing beam splitter  17  is rejected. For the portion of laser beam  18  which passes through polarizing beam splitter  17 , it then passes through a Faraday rotator  14  followed by a half waveplate  16  for directing the laser beam  18 . Another polarizing beam splitter  17  may be used to direct the remaining portion of laser beam  18  again into two sub-components comprising gain path laser beam  13  and aperture path laser beam  15 . Four port optical device  11  may be used to provide steering of components of laser beam  18  in various directions within an optical circuit while minimizing back reflections in the opposite direction of the arrows of laser beam  18 . 
     FIG. 2 shows a first configuration of a laser light source  20  capable of preventing optical feedback and varying the intensity variation of the laser light by rotating a half waveplate. Laser light source  22  may comprise a single longitudinal light source operated at continuous wave operation. The emitted laser beam  18  from the laser light source  22  inherently possesses a significant polarization and a half waveplate  16  permits the aligning of that polarization along a predetermined axis of polarizer  12  contained within optical isolator  10 . Such a configuration is used to minimize any parasitic, undesirable back reflection of laser light into the laser light source  22  which may result in deleterious effects such as wavelength drift and linewidth broadening of the laser light source  22 . The half waveplate  16  may be angularly aligned to various angles of incidence of the polarizer  12  to vary the intensity of the laser beam  18  which exits laser light source  22  and travels through the optical system. Those skilled in the art will recognize that a number of optical isolators  10  may be used to decrease even further the possibility of back reflected light into the laser light source  22  by cascading several optical isolators  10 . 
     FIG. 3 shows another configuration of a laser light source  30  capable of preventing optical feedback and varying the intensity variation of the laser light using an electro-optic modulator. An optical isolator  10  may also be used to prevent reflected light from entering into the laser light source  22  and causing undesired effects as described above. Additionally, an intensity modulator  32  may be placed either in front of the optical isolator  10  or after for modulating the intensity of the laser beam  18  as it then travels through the remainder of an optical circuit. Those skilled in the art will recognize a wide variety of electro-optic modulators which will serve the function of intensity modulator  32  including Pockels effect elements utilizing the linear electro-optic effect and Kerr effect elements utilizing the quadratic electro-optic effect. A very common material candidate for a Pockels cells is Lithium niobate (LiNbO 3 ) 
     FIG. 4 shows one possible embodiment of the invention comprising a four pass, dual [could be a single or “n” rods; two is just an example] rod laser media pulsed laser light source  40 . Note, however, that source  40  may be formed of one or many rods, as other considerations may dictate. This embodiment shows laser light source  20  which emits laser beam  18  which passes through an isolator  10  and is directed using a first mirror  42  through a beam expander  46  for broadening the beam waist of laser beam  18  to minimize the divergence of laser beam  18  as it propagates through free space given its inherently Gaussian nature. Laser beam  18  then passes through four port optical device  11  in which laser beam  18  is directed to the gain path laser beam  13 . The gain path laser beam  13  passes through two high-gain laser media  48  and then through a phase correction plate and a Faraday rotator  49  where the linear polarization of laser beam  18  is rotated 45°. 
     Typically, high-gain laser media  48  comprising glass materials such as Nd 3+ :glass are inherently amorphous and non-birefringent whereas semiconductor materials such as Nd 3+ :YAG might degrade the polarization state of laser beam  18  as it passes through them. In the case of optically birefringent high-gain laser media, the use of an adjustable waveplate for phase compensation can improve the performance of the system. The phase correction plate compensates for any rod birefringence, which may be thermally induced The high-gain laser media  48  may comprise any material that will sustain an inverted population of energy states when optically pumped. It then reflects off of an end mirror  44  which then passes through the Faraday rotator  49  again where it is rotated an additional 45°, orthogonal to the polarization of the original laser beam  18 . 
     The reflected laser beam then passes a second time through high-gain laser media  48  and into four port optical device  11  where it is directed into the direction of aperture path laser beam  15  and then reflects off a mirror  42  where it passes through an aperture  43  which helps to minimize self-oscillations caused by amplified spontaneous emissions from the gain medium. Beam  15  reflects at end mirror  44  retracing its path back into four port optical device  11  where it is again directed to pass through high-gain laser media  48  for a third pass. It then travels through to Faraday rotator  49  and to end mirror  44  where it is again reflected and retraces its path in passing through Faraday rotator  49 , being converted into the same linear polarization as the original gain path laser beam  13  in its first pass through high-gain laser media  48 . The gain path laser beam  13  then passes a fourth time through high-gain laser media  48  and into the four port optical device  11  where it is directed to pass out in the direction of output laser beam  19 . 
     Each high-gain optical medium  48  is optically pumped to generate an inverted population of energy states using a pumping array  51  of laser diodes driven by a diode driver  52  which delivers electric current to operate the laser diodes of the pumping array  51 . To generate pulses of amplified laser light, a trigger signal  54  is used to drive the diode driver  52  which operates the pumping array  51  of laser diodes. The pulse rate at which the output laser beam  19  may be pulsed is governed most directly by the frequency of the trigger signal  54  which is used to pulse the diode driver  52 . The switching of the optical pumping results in gain switching of the high-gain laser medium  48  which serves to provide for a pulsing of the conditions in which laser light amplification may occur. The result is an amplified, pulsed output laser beam  19 . 
     FIG. 5 shows another possible embodiment of the invention comprising, for example, a dual pass, dual rod laser media pulsed laser light source  50 . This embodiment is strikingly similar to four pass, dual rod laser media pulsed laser light source  40 . The main difference is that there exists no four port optical device  11  is replaced by a single polarizing beam splitter  17 . 
     FIG. 6 shows another possible embodiment of the invention comprising, for example, a four pass, single slab laser medium pulsed laser light source  60 . This embodiment shows laser light source  20  which emits laser beam  18  which is isolated from feedback with isolator  10  and is directed through beam expander  46  for broadening the beam waist of laser beam  18  to minimize the divergence of laser beam  18  as it propagates through free space given its inherently Gaussian nature. Laser beam  18  then passes through polarizing beam splitter  17  in which polarized light aligned to one axis of the polarizing beam splitter  17  passes through, and polarized light not aligned to that one axis of the polarizing beam splitter  17  is redirected in the direction of an output. laser beam  19 . For the portion of laser beam  18  which passes through polarizing beam splitter  17 , it then passes through a Faraday rotator  14  followed by a half waveplate  16  and a second polarizer  17  for directing the laser beam  18  through high-gain laser media  48 . Slab designs pass P-state with high efficiency because the face is almost at Brewsters Angle. The high-gain laser media  48  may comprise any material that will sustain an inverted population of energy states when optically pumped. It then reflects off of turning mirror  42 . The reflected laser beam then reflects off of a second turning mirror  42 , passes a second time through high-gain laser media  48  and is directed into the direction of laser beam  15  and then reflects off end mirror  44  before retracing its path back into the high-gain laser media  48  for a third pass. It then reflects off mirror  44  to mirror  44  where it is again reflected and retraces its path in passing through high-gain laser media  48  for a fourth time and into the polarizer  17  and half waveplate for aligning the laser beam along a predetermined incidence angle. The laser beam  18  then passes a second time through Farady rotator  14 . After traveling through Faraday rotator  14 , the laser beam  18  has been rotated to be orthogonal to the original laser beam. Laser beam  18  enters polarizing beam splitter  17  where it is directed to pass out in the direction of output laser beam  19 . 
     In the present example, each high-gain optical medium  48  is optically pumped to generate an inverted population of energy states using pumping arrays  51  of laser diodes driven by a diode driver  52  which delivers electric current to operate the laser diodes of the two pumping arrays  51 . To generate pulses of amplified laser light, a trigger signal  54  is used to drive the diode driver  52  which operates the pumping arrays  51  of laser diodes. The pulse rate at which the output laser beam  19  may be pulsed is governed most directly by the frequency of the trigger signal  54  which is used to pulse the diode driver  52 . The switching of the optical pumping results in gain switching of the high-gain laser medium  48  which serves to provide for a pulsing of the conditions in which laser light amplification may occur. The result is an amplified, pulsed output laser beam  19 . 
     FIG. 7 shows another possible embodiment of the invention comprising a four pass, dual slab laser medium pulsed laser light source  70 . This embodiment is strikingly similar to four pass, single slab laser medium pulsed laser light source  60 , in that it uses the same number of diodes as in the FIG. 6 example. The main difference is that there exists a second slab laser medium  48  and mirror assemblies  72  (either mirrors or coatings) are placed on both of the high-gain laser media  48 . This may result in a system that is more efficient (per diode) than the system of FIG. 6, but with only a small added cost of the second slab. 
     FIG. 8 shows another possible embodiment of the invention comprising an eight pass, single slab laser medium pulsed laser light source  80 . This embodiment is strikingly similar to four pass, single slab laser medium pulsed laser light source  60 . The main difference is that there exists a plurality of turning mirrors  42  to direct the laser beam through the high-gain laser media  48  eight times and mirror assembly  72  (either mirrors or coatings) is placed on the high-gain laser media  48 . 
     FIG. 9A shows another possible embodiment of the present invention. FIG. 9A includes remote seeding of amplifier  54  with a fiber optic link. Laser light source  20  emits laser beam  18  which is isolated from feedback with optical isolator  10  and directed into input coupling optics and polarization preserving single-mode fiber optics. Polarization preserving single-mode fiber optic is coupled to amplifier  54 , which includes output coupling optics. Amplifier  54  (not including output coupling optics) is equivalent to the amplifier section shown in FIG.  6 . Amplifier methods illustrated in FIGS. 4,  5 ,  7  or  8  can be used, as well. Long-term stability of amplifier  54  is improved by de-coupling of laser beam  18 . If laser beam  18  laser “walks” but part of the light still couples into the polarization preserving single-mode fiber optic, then output of amplifier  54  may only drop a small amount. 
     FIG. 9B shows another possible embodiment of the present invention. FIG. 9B represents remote seeding of amplifier with internal modulators. Laser light source  20  emits laser beam  18  which is isolated from feedback with optical isolator  10 . Laser beam  18  is input in amplitude modulator, phase modulator and other beam/laser conditioning components. Prior to being input to polarization preserving single-mode fiber optics, laser beam  18  is input to input coupling optics. Laser beam  18  is output from polarization preserving single-mode fiber optics to output coupling optics. Laser beam  18  is amplified in a manner similar to that shown in FIG.  6 . Amplifying methods illustrated in FIGS. 4,  5 ,  7  or  8  can be used, as well. 
     The present invention provides several benefits including minimizing thermal heating of the high-gain laser medium by using laser diodes to perform the optical pumping. Using laser diodes which operate within a very narrow wavelength regime minimize optically-induced thermal heating of the laser medium in that little electromagnetic radiation outside of the desired spectrum bombards the high-gain laser medium as with conventional methods. 
     Using laser diodes for optically pumping the high-gain laser medium provides additional benefits including permitting a faster pulse rate, variable pulse rate. By performing optical amplification and pulsing in the manner described above, the present invention also minimizes amplification induced distortion of a seed laser beam. Consequently, the physical properties of the original seed laser beam are maintained in the resultant amplified, output beam. Many applications including optical interferometry require a highly amplified, spectrally pure output laser beam which the present invention will provide. To broaden the dynamic detection range of an optical interferometer employing the present invention, the intensity of the output laser beam may also be modulated. 
     Although the present invention has been described in detail, it should be understood that various changes, substitutions and alterations can be made hereto without departing from the spirit and scope of the invention as described by the appended claims.