Patent Document

CROSS REFERENCES TO CO-PENDING APPLICATIONS 
     None. 
     BACKGROUND OF THE INVENTION 
     1. Field of the Invention 
     This invention relates to beam shaping, and, more particularly, to beam stacking devices and methods for stacking beams which change the shape of a beam from a highly asymmetric non-diffraction-limited laser source, such as a high power laser diode bar, to a more symmetric, and thus more desirable and useful, profile. 
     2. Description of the Prior Art 
     While semiconductor lasers are widely used in both scientific and consumer devices, the relatively low power output of such devices has limited their use. The output power of semiconductor lasers has been increased by several different techniques, one being fabricating a multiple diode device in the form of an array of low power laser diodes on a single chip. While it is possible to fabricate such a multiple diode device having, for example, 10 laser diodes, the output of such a device is a beam having a highly elliptical shape or profile. That is, the output beam is much wider in the dimension corresponding to the necessary spacing between the laser diodes than in the dimension corresponding to the width of a single laser diode. In other words, the output beam has dramatically unequal M 2  dimensions in two orthogonal directions, thus resulting in a beam which is highly asymmetrical. 
     High power laser diode bars are attractive as optical sources for applications in pumping solid state lasers, in materials processing, and in the medical field. Unfortunately, the inconvenient shape, i.e., highly elliptical nature, of the output beam of laser diode bars makes them, by themselves, inappropriate for many of the uses which require a higher power output than is attainable from a single laser diode source. However, this has not been a fatal shortcoming because there exist techniques for reconfiguring the shape or profile of the output beam to make it less elliptical in nature; that is, to create an output beam whose dimensions in two orthogonal directions are more nearly equal, thus giving rise to an output beam which is substantially symmetrical. One such technique is the beam stacking device disclosed in European patent number EP0731932 and in corresponding International Application (PCT) number WO 95/15510, and it is that sort of technique which the present invention serves to improve. 
     The beam stacking device of European patent number EP0731932 and International Application number WO 95/15510 consists of two high reflectivity planar mirrors aligned approximately parallel and separated by a small distance. The two mirrors are offset transversely from each other in two directions so that small sections of each mirror are not obscured by the other. These unobscured sections form input and output apertures of the beam stacking device. The action of the beam stacking device is to chop the incident beam into a specific number of chopped parts and then to redirect and reposition these chopped parts so that they emerge from the beam stacking device one on top of another. Although this beam stacking device does reconfigure the output beam to a more favorable profile, it nevertheless has several disadvantages, the principal disadvantage being that, because the incident beam is chopped many times and many reflections are needed between the mirrors, losses due to reflection are great and, therefore, the transmission is low. 
     SUMMARY OF THE INVENTION 
     The general purpose of the present invention is to provide new beam stacking devices and methods of beam stacking which overcome the disadvantages of the prior art. This is achieved through the use of a prism assembly including entrance and exit apertures and total internal reflection surfaces. 
     More particularly, the beam stacking devices of this invention utilize a prism assembly into which an elliptical incident beam to be shaped, i.e., an incident beam effectively having greatly different M 2  parameters in two directions, is introduced through an entrance aperture and then sequentially reflected by four total internal reflection surfaces of the prism assembly such that on each round trip a chopped part of the beam emerges from an exit aperture and is stacked on top of the preceding chopped part. The lengths of the four total internal reflection surfaces provide for inward displacement of adjacent parts of the input beam incident on the entrance aperture, thereby compressing the input beam in one orthogonal direction. The width of the exit aperture provides the dimension of the emergent beam along the other orthogonal direction and is selected so that the input beam is expanded in the other orthogonal direction. Consequently, in comparison with the input beam at the entrance aperture, the output or emergent beam at the exit aperture has a reduced orthogonal dimension in one orthogonal direction and an increased orthogonal dimension in the other orthogonal direction. Stated in another manner, the effect of the beam stacking device is to decrease the size of the highly elliptical input beam along one orthogonal direction and to increase the size of the highly elliptical input beam along the other orthogonal direction, thereby reconfiguring the highly asymmetrical input beam into an output beam which is substantially symmetrical. Since the first round trip of the incident beam involves four total internal reflections, and each succeeding round trip involves another four additional reflections, the losses due to reflection are minimized. For example, in accordance with each of two embodiments of the invention, an elliptical incident beam comprising the output of a five laser diode bar can be combined to produce a single, more favorably shaped output beam with a total of only 55 internal reflections and, in another embodiment of the invention, with a total of only 60 internal reflections. 
     In one embodiment, a beam stacking device is formed of a prism assembly consisting of a right angle prism which provides the entrance aperture, and a rectangular parallelepiped prism with one edge cut away which provides the four total internal reflection surfaces and the exit aperture. 
     In a second embodiment, a beam stacking device is formed that includes two right angle prisms. One right angle prism provides the entrance aperture and two of the four total internal reflection surfaces. The other right angle prism, which has a portion cut away for the path of the entrance, provides the exit aperture and the other two of the four total internal reflection surfaces. 
     In a third embodiment, a beam stacking device consists of two prisms. One prism provides the entrance aperture and two of the four total internal reflection surfaces. The other prism provides the exit aperture, the other two of the four total internal reflection surfaces, and the path of the entrance. 
     In all of the embodiments the beam stacking devices permit focusing beams to small diameters, i.e., more nearly equal orthogonal dimensions, without significantly decreasing the brightness. The total internal reflection surfaces improve the quality of the transmission. The number of stacked beams is a function of the incident beam width and the size of the exit aperture. The shift of stacking beams in one direction is implemented by the size difference of the total internal reflection surfaces. 
     The entrance and exit apertures of the various embodiments can be switched, and can be implemented by cut away surfaces or by additional components such as right angle prisms. 
    
    
     BRIEF DESCRIPTION OF THE DRAWINGS 
     Other objects of the present invention and many of the attendant advantages of the present invention will be readily appreciated as the same becomes better understood by reference to the following detailed description when considered in connection with the accompanying drawings, in which like reference numerals designate like parts throughout the figures thereof and wherein: 
     FIGS. 1 a  and  1   b  show, respectively, plan and elevation schematic views of the first preferred embodiment; 
     FIGS. 2 a  and  2   b  show, respectively, plan and elevation schematic views of the second preferred embodiment; and, 
     FIGS. 3 a  and  3   b  show, respectively, plan and elevation schematic views of the third preferred embodiment. 
    
    
     DETAILED DESCRIPTION OF THE PREFERRED EMBODIMENTS 
     As shown in FIG. 1 a,  the beam stacking device  10  of this invention includes a prism assembly of two elements: a prism  12  in the form of a rectangular parallelepiped with one lateral edge cut away, thus forming a prism having pentagonal bases and five lateral faces or surfaces; and a right angle prism  14 . The lateral edges of prism  12  are identified by the letters A, B, C, D and E; and the lateral edges of prism  14  are identified by the letters D, E and F. For convenience herein, whenever referring to a particular lateral surface, such will be identified simply by specifying the two lateral edges which are the boundaries thereof. For example, the lateral surface bounded by lateral edges A and B is termed “surface AB”. Thus, relying on this convention and continuing with the description, the surface DF of prism  14  serves as an entrance aperture, and the surface AE of prism  12  serves as an exit aperture. The dihedral angles ∠ABC, ∠BCD and ∠CDE are 90 degrees. The dihedral angles ∠DEA and ∠EAB are 135 degrees. The dihedral angles ∠EDF and ∠FED are 45 degrees. The length AB is equal to the length BC. The length CD is equal to AB+(1/{square root over (2)})AE, and the length DE is equal to AB−(1/{square root over (2)})AE. The prisms  12  and  14  are made of, for example, the well known optical glass designated in the Schott optical glass catalog as BK 7 . In use, a beam  16  enters the entrance aperture at surface DF and proceeds to surface AB. The angle of incidence of the beam  16  at the surface AB is 45 degrees, which is larger than that of the total internal reflection at the interested wavelength. Total internal reflection of the beam  16  first occurs at the surface AB. Total internal reflection also occurs at the surfaces BC, CD and DE. When the beam  16  undergoes total internal reflection at the surface CD for the first time, a first chopped part  16   a  emerges from the exit aperture AE while the remaining portion directs to the surface DE and thence to the surface AB a second time. The width of the chopped part is equal to the width of the exit aperture AE. After the second round trip, the second chopped part  16   b  emerges from the exit aperture AE, but displaced beneath the first chopped part  16   a . For the purpose of illustration, the number of chopped parts is chosen to be five chopped parts  16   a ,  16   b ,  16   c ,  16   d  and  16   e.    
     As shown in the orthogonal view in FIG. 1 b,  chopped part  16   a  is sequentially reflected at surfaces AB, BC and CD and then emerges from exit aperture AE, but displaced beneath beam  16  due to the angle of incidence  18 . Chopped part  16   b  is sequentially reflected at surfaces AB, BC, CD and DE for two round trips and then emerges from exit aperture AE, but displaced beneath chopped part l 6   a  due to the angle of incidence. Chopped parts  16   c ,  16   d  and  16   e  undergo similar multiple round trip reflections at surfaces AB, BC, CD and DE until they finally emerge from exit aperture AE beneath chopped parts  16   b ,  16   c  and  16   d . Thus, the action of the beam stacking device  10  is effectively to chop the incident beam  16  into a specific number of chopped parts and then to redirect and reposition those chopped parts so that they emerge from the beam stacking device stacked one on top of another with a reduced orthogonal dimension corresponding to the direction of stacking and with an increased orthogonal dimension corresponding to the width of the exit aperture, thereby resulting in an output beam which is substantially symmetrical. 
     For many applications, it is desirable to minimize the gap between adjacent chopped parts by choosing the angle of incidence  18  in accordance with the equation, 
     
       
         sin 2θ/{square root over (n 2 +L −sin 2 +L θ)}≧dy/{square root over (2)}AB 
       
     
     where θ is the angle of incidence  18 , n is the index of BK 7  at the interested wavelength, and dy is the incident beam size in one direction. 
     Two alternate embodiments are illustrated in FIGS. 2 a , 2   b  and  3   a , 3   b . FIG. 2 a  shows a beam stacking device  20  of the invention which includes a prism assembly of two elements: a small prism  22  and a larger prism  24 . The lateral edges of prism  22  are identified by the letters G, H and I; and the lateral edges of the prism  24  are identified by the letters I, J and K. The surfaces GI and GK serve as entrance and exit apertures, respectively. A portion of the prism  24  is cut away to provide the path for the incident beam  26 . The dihedral angles ∠GHI, ∠HIJ and ∠IJK are 90 degrees. The dihedral angles ∠IGH, ∠HIG, ∠IKJ and ∠KIJ are 45 degrees. The dihedral angle ∠HGK is 135 degrees. The length GH is equal to the length HI. The length IJ is the same as the length JK, both being equal to GH+(1/{square root over (2)})GK. The prisms  22  and  24  are made of, for example, BK 7 . The angle of incidence of the beam  26  at the surface GH is 45 degrees, which is larger than that of the total internal reflection at the interested wavelength. Total internal reflection of the beam  26  first occurs at the surface GH. Total internal reflection of the beam  26  also occurs at the surfaces HI, IJ and JK. When the beam  26  undergoes total internal reflection at the surface JK for the first time, a first chopped part  26   a  emerges from the exit aperture GK while the remaining portion directs to the surface GH a second time. The width of the chopped part is equal to the width of the exit aperture GK. After the second round trip, the second chopped part  26   b  emerges from the exit aperture GK, but displaced beneath the first chopped part  26   a . This process continues until the entire incident beam is reconfigured. For the purpose of illustration, the number of chopped parts is chosen to be five chopped parts  26   a ,  26   b ,  26   c ,  26   d  and  26   e.    
     As shown in the orthogonal view in FIG. 2 b , chopped part  26   a  is sequentially reflected at surfaces GH, HI, IJ and JK and then emerges from exit aperture GK, but displaced beneath beam  26  due to the angle of incidence  28 . Chopped part  26   b  is sequentially reflected at surfaces GH, HI, IJ and JK for two round trips and then emerges from exit aperture GK, but displaced beneath chopped part  26   a  due to the angle of incidence. Chopped parts  26   c ,  26   d  and  26   e  undergo similar multiple round trip reflections at surfaces GH, HI, IJ and JK until they finally emerge from exit aperture GK beneath parts  26   b ,  26   c  and  26   d . Thus, as with the beam stacking device  10 , the action of the beam stacking device  20  is effectively to chop the incident beam  26  into a specific number of chopped parts and then to redirect and reposition those chopped parts so that they emerge from the beam stacking device stacked one on top of another, thereby attaining a beam with improved orthogonal dimensions which enable its use in applications incapable of the original unmodified beam. 
     FIGS. 3 a  and  3   b  show another alternate embodiment of a beam stacking device in accordance with the invention. Illustrated in these figures is a beam stacking device  30  which includes a prism assembly of two elements: a small prism  32  and a larger prism  34 . The lateral edges of prism  32  are identified by the letters G, H and I; and the lateral edges of the prism  34  are identified by the letters I, L, M and G. The surfaces GI and GM serve as entrance and exit apertures, respectively. A portion of the prism  34  is cut away to provide the path for the incident beam  36 . The dihedral angles ∠GHI, ∠HIL and ∠ILM are 90 degrees. The dihedral angles ∠IGH, ∠HIG and ∠GIL are 45 degrees. The dihedral angles ∠LMG and ∠MGH are 135 degrees. The length GH is equal to the length HI. The length IL is equal to GH+(1/{square root over (2)})GM, and the length LM is equal to GH−(1/{square root over (2)})GM. The prisms  32  and  34  are made of, for example, BK 7 . The angle of incidence of the beam  36  at the surface GH is 45 degrees, which is larger than that of the total internal reflection at the interested wavelength. Total internal reflection of the beam  36  first occurs at the surface GH. Total internal reflection of the beam  36  also occurs at the surfaces HI, IL and LM. When the beam  36  undergoes total internal reflection at the surface IL for the first time, a first chopped part  36   a  having a width equal to the width of the exit aperture GM emerges from the exit aperture GM while the remaining portion of the beam  36  directs to the surface LM and then undergoes a second round trip of sequential reflections at surfaces GH, HI and IL. Upon undergoing total internal reflection a second time at surface IL, a second chopped part  36   b  emerges from the exit aperture GM, but displaced beneath the first chopped part  36   a . As this process continues, the beam  36  is chopped into further parts which emerge from the exit aperture GM stacked on top of one another. For the purpose of illustration, the number of chopped parts is chosen to be five chopped parts  36   a ,  36   b ,  36   c ,  36   d  and  36   e.    
     MODE OF OPERATION 
     In all three embodiments of the invention, the incident beam to be reconfigured passes through an entrance aperture of a prism assembly, undergoes total internal reflection at four total internal reflection surfaces of the prism assembly step by step, and is chopped into a number of parts which emerge from an exit aperture of the prism assembly. The emerged chopped parts are stacked on top of one another due to the angle of incidence of the beam and the size difference of the four total internal reflection surfaces. The result is a reconfigured beam which has a more favorable profile in two orthogonal directions, thus rendering it suitable for use as an attractive and viable optical source in a variety of applications. 
     Various modifications can be made to the present invention without departing from the apparent scope hereof.

Technology Category: 3