High power laser assemblies are used in many applications, such as cutting lasers, welding lasers, and laser weaponry.
An important requirement of high power laser assemblies is to maximize output power, while minimizing beam size in the far field and simultaneously at the laser aperture. Laws of electromagnetic propagation dictate that for a given laser aperture size, far-field spot size cannot be smaller than a certain value. Laser assemblies that achieve this smallest value are referred to as diffraction limited.
Output of high power laser assembly can require a complex beam director. Unfortunately, existing beam director assemblies have a relatively large form factor due to the requirement to expand and direct laser beam without creating beam obstruction.
The present invention is directed to a laser that generates a combination beam, the laser including an optical amplifier array system that generates a plurality of laser beams; and a beam combiner that coherently combines the plurality of laser beams to form a combination beam having a hollow center in a near field. As an overview, the coherently combined laser beams allow for a high power assembly beam that is near diffraction limited. Further, the combination beam with the hollow center allows for the use of an on-axis, reflective beam expander (e.g. an on-axis reflective telescope) without (i) loss in power, (ii) degradation of beam quality or (iii) excessive heating of the beam expander. Generally, on-axis reflective telescopes have a smaller form factor than off-axis reflective telescopes. Further, reflective elements in the telescope are required in high power applications. As provided herein, the unique hollow geometry of the combination beam allows for a more efficient, smaller form factor device.
Stated in another fashion, the proposed laser produces a near diffraction-limited, high power beam having a hollow center. This allows for the use of a simpler, lighter, and smaller beam director that points the beam, and includes an on-axis, reflective beam expander.
In one embodiment, at least two or more of the laser beams are replicas of each other, and/or at least two or more of laser beams propagate along parallel axes and are positioned side-by-side. Stated in another fashion, in one embodiment, at least two or more of the laser beams have the same wavelength and approximately the same phase. For example, each of the laser beams can have the same wavelength and approximately the same phase.
In certain implementations, the combination beam has a power of at least six kilowatts.
In one implementation, the optical amplifier array system can include a seed laser that generates a seed output beam, a fiber splitter that splits the seed output beam into a plurality of seed split beams, and an amplifier assembly that amplifies each of the seed split beams to generate the plurality of laser beams. With this design, each laser beam has a high power, and each laser beam is a replica of the other laser beams.
In one embodiment, the beam combiner directs the plurality of laser beams to be substantially parallel to and spaced apart from a combination axis of the combination beam.
As provided herein, in one embodiment, the beam combiner can include a plurality of combiner fibers for transmitting and launching the plurality of laser beams. Further, each combiner fiber can have a fiber outlet, and the fiber outlets can be spaced apart and arranged in an outlet pattern having a hollow center.
The beam combiner can coherently combine the plurality of laser beams so that the combination beam has a substantially annular shaped cross-section with a substantially circular outer diameter and a substantially circular inner diameter.
The present invention is also directed to a system including the laser that generates the combination beam, and a beam director that points and expands the combination beam to provide an assembly beam having a hollow center in the near field and characteristics of a solid beam in a far field. In this design, the beam director includes a beam pointer downstream from the laser that points the combination beam that exits the laser, and a beam expander that expands the combination beam. The beam expander can be an on-axis beam expander that include a plurality of reflective elements that expand the combination beam. In one implementation, the beam expander includes a diverging element and a collimating element.
In another implementation, the present invention is directed to a method for generating a combination beam. The method can include generating a plurality of laser beams; and coherently combining the plurality of laser beams to form a combination beam having a hollow center in a near field region.
The novel features of this invention, as well as the invention itself, both as to its structure and its operation, will be best understood from the accompanying drawings, taken in conjunction with the accompanying description, in which similar reference characters refer to similar parts, and in which:
A number of Figures include an orientation system that illustrates an X axis, a Y axis that is orthogonal to the X axis, and a Z axis that is orthogonal to the X and Y axes. It should be noted that these axes can also be referred to as the first, second, and third axes.
As an overview, in certain embodiments, the optical amplifier array system 17 generates a plurality of amplified laser beams 24 (illustrated with arrows), and the beam combiner 18 coherently combines the laser beams 24 to form a hollow, combination beam 26. Next, the beam pointer 20 steers and directs the hollow combination beam 26 to the beam expander 21. Subsequently, the beam expander 21 expands the combination beam 26 to generate the assembly beam 12 that has a hollow center in a near field, and near diffraction limited beam in a far field.
As used herein, the term “near field” shall mean the region around the output aperture of the beam expander 21, and the term “far field” shall mean the region located many Rayleigh ranges away from the beam expander 21.
As provided herein, the coherently combined individual laser beams 24 allow for a high power beams 12, 26 that are near diffraction limited. As non-exclusive examples, the laser assembly 14 can be designed so that the power output of the beams 12, 26 is greater than ten, fifty, one hundred, three hundred, five hundred, or one thousand Kilowatts.
Further, the multiple laser beams 24 are arranged so that the combination beam 26 has the hollow center. Importantly, the hollow center allows for the beam expander 21 to be an on-axis reflective telescope while using the entire combination beam 26; and without (i) loss in power, (ii) degradation of quality of the assembly beam 12, and/or (iii) excessive heating of the beam expander 21. Generally, on-axis reflective telescopes 21 have a smaller form factor than off-axis reflective telescopes (not shown). Further, reflective elements in the telescope 21 are required in high power applications. Thus, the unique hollow geometry of the combination beam 26 allows for a more efficient, and smaller form factor, high-powered device 10.
The high powered device 10 disclosed herein can be used in a number of different applications. As non-exclusive examples, the device 10 can be used for industrial cutting, welding, or laser weaponry.
The beam pointer 20 directs and steers the combination beam 26 from the beam combiner 18 to the beam expander 21. For example, the beam pointer 20 can include one or more reflective elements (not shown in
The beam expander 21 adjusts and expands the combination beam 26 to provide the assembly beam 12 that has a hollow center in the near field and no hollow center in the far field. In the simplified embodiment illustrated in
It should be noted that in designs in which the beam pointer 20 does not direct the combination beam 26 through the collimating element 28, that the collimating element 28 can be designed without the element aperture 28A.
Additionally, the beam director 19 can include a beam mover assembly 29 (illustrated as a box) that is controlled to move one or more elements of the beam pointer 20 and the elements 27, 28 of the beam expander 21 to selectively direct (steer) the assembly beam 12. Stated in another fashion, the beam mover assembly 29 can be used to steer the assembly beam 12 and the output axis 12A. Moreover, the beam director 19 can include one or more structural frames (not shown in
With the present design, the device 10 generates and steers the assembly beam 12. As non-exclusive examples, the device 10 can be a cutting system, a welding system, or a laser weapon.
The system controller 22 controls the operation of the various components of the device 10. For example, the system controller 22 can be electrically connected to and control the components of optical amplifier array system 17, and the beam mover assembly 29. The system controller 22 can include one or more processors 22A and/or one or more electronic data storage devices 22B. The system controller 22 is illustrated in
The device 10 can be powered by a generator, a battery, or another power source.
Further, the assembly beam 12 is illustrated at five different locations, including a near field 13A, a transition range 13B, and a far field 13C along the output axis 12A. In this example, the assembly beam 12 has an annular shape in the near field 13A, and transitions to a near diffraction limited, solid beam 12 in the far field. Thus,
It should be noted that in the non-exclusive implementation of
The optical amplifier array system 217 outputs a plurality of fiber coupled, amplified optical outputs 224A-224F (Illustrated with dashed arrows) that are terminated into free space, amplified, laser beams that are coherently combined by the beam combiner 218. The design of the optical amplifier array system 217 can be varied to achieve the design parameters of the optical amplifier array system 217. In the non-exclusive embodiment illustrated in
The seed laser 230 is designed to emit a stable, single wavelength, seed output beam 230A (illustrated with a dashed arrow) at the desired wavelength of the assembly beam 212. As a non-exclusive example, the seed laser 230 can emit at a single wavelength in the 1060 to 1080 nanometer range (e.g. at 1064 nanometers).
In certain embodiments, the seed laser 230 can have a relatively low power. As non-exclusive examples, the seed output beam 230A can have a power of less than one, five, ten, or fifty milliwatts. However, other powers are possible. Moreover, as non-exclusive examples, the gain medium can be a semiconductor, a fiber laser, or a solid state laser. The seed laser 230 can include an optical, seed fiber 230B that transmits the emitting seed output beam 230A.
The fiber splitter 232 splits the seed output beam 230A into a plurality of seed split beams 232A-232F (illustrated with dashed arrows) that each have a common wavelength. In simplified example illustrated in
Alternatively, the fiber splitter 232 can be design to split the seed output beam 230A into more than six, or fewer than six, separate seed split beams 232A-232F. As alternative, non-exclusive examples, the fiber splitter 232 can be designed to split the seed output beam 230A into at least four, ten, thirty, fifty, one hundred, or two hundred separate seed split beams 232A-232F. Generally speaking, the power output of the assembly beam 212 (illustrated in
In the embodiment illustrated in
The phase controller 236 includes the plurality of individual phase control modules 236A-236F for individually modulating the phase of each seed split beam 232A-232F so that phase of all the laser beams 224A-224F is coherent (phase of each laser beam 224A-224F is approximately the same). Thus, the number of individual phase control modules 236A-236F will correspond to the number of seed split beams 232A-234F. In the non-exclusive embodiment illustrated in
In
The amplifier assembly 240 individually amplifies each of the seed split beams 232A-232F to generate the plurality of laser beams 224. More specifically, the amplifier assembly 240 includes the plurality of individual fiber amplifiers 240A-240F for individually amplifying each seed split beam 232A-232F. Thus, the number of individual fiber amplifiers 240A-240F will correspond to the number of seed split beams 232A-234F. In
Each fiber amplifier 240A-240F can be an optical amplifier that amplifies the respective seed split beam 232A-232F directly. Each fiber amplifier 240A-240F can be designed and selected based on the desired wavelength and power of the assembly beam 212. In alternative, non-exclusive examples, each fiber amplifier 240A-240F can amplify the respective seed split beam 232A-232F at least 102, 103, 104, or 105 times. Further, as alternative, non-exclusive examples, each fiber amplifier 240A-240F can amplify the respective seed split beam 232A2-32F so that each laser beam 224A-224F has an output power of at least 0.5, 1.5, 3, or 5 kilowatts.
With the present design, the optical amplifier array system 217 generates the plurality of laser beams 224A-224F having the same wavelength and having relative phases actively controlled by the phase controller 236 for highest beam quality in the combination beam 226. Stated in another fashion, the each of the plurality of laser beams 224A-224F will have the same wavelength and approximately the same phase using the phase controller 236. In alternative, non-exclusive examples, as used herein, the term “approximately the same phase” shall mean that the difference in phase between the plurality of laser beams 224A-224F is less than 0.05, 0.1, 0.15, or 0.2 Radians RMS.
It should be noted that the system controller 222 can control the seed laser 230, the fiber splitter 232, the phase control modules 236A-236F, and the fiber amplifiers 240A-240F to achieve the desired laser beams 224A-224F.
The beam combiner 218 collimates and spatially combines the plurality of laser beams 224A-224F exiting the fiber array 242 to create the uniquely shaped combination beam 226. With this design, the use of coherently combined laser beams 224A-224F (i) allows for the scaling of laser power by adding or removing laser beams 224A-224F, and (ii) allows for the intentional shaping of the near-field intensity distribution of the combination beam 226 to suit the design of the beam expander 221.
The design of the beam combiner 218 can be varied pursuant to the teachings provided herein. In the non-exclusive embodiment illustrated in
The combiner fiber array 242 includes a plurality of combiner fibers 242A-242F for individually transmitting and launching the laser beams 224A-224F from the amplifier assembly 240. Thus, the number of individual combiner fibers 242A-242F will correspond to the number of laser beams 224A-224F. In
In the non-exclusive embodiment illustrated in
In one embodiment, each combiner fiber 242A-242F includes a fiber inlet 243A that is connected to the respective fiber amplifier 240A-240F, and a fiber outlet 243B that directs the respective laser beam 224A-224F along the desired axis 248A-248F. In one non-exclusive embodiment, each fiber outlet 243B can include a separate end cap 243C that protects the output facet.
The combiner frame assembly 244 retains the individual combiner fibers 242A-242F near the distal end 243B to hold the distal ends 243B so that the individual laser beams 224A-224F are launched and directed along the desired paths. For example, the combiner frame assembly 244 can be a rigid frame secured to the mounting base 216 that maintains the desired positions of the fiber outlets 243B. Thus, the design of the combiner frame assembly 224 can be varied to achieve the desired positions of the fiber outlets 243B to achieve the desired design of the combination beam 226.
In this embodiment, the first outlet pattern 250 is centered about a pattern axis 250A, and the outlet axes 252A-252F are parallel to and equally spaced apart from the pattern axis 250A. Further, the outlet axes 252A-252F are spaced apart from the pattern axis 250A and are distributed about the pattern axis 250A. With this design, the fiber outlets 243B are spaced apart and arranged in an annular pattern (with a hollow center) that is centered about the pattern axis 250A.
In the non-exclusive embodiment illustrated in
Referring back to
In one embodiment, each lens 242A, 246C, 242F can be a spherical lens having an optical axis that is aligned with the respective beam axis 248A-248F. In alternative, non-exclusive embodiments, each lens 242A, 246C, 242F can have a diameter of less than approximately one, two, three, four, five or ten millimeters. The type of material utilized for each lens 242A, 246C, 242F can be selected to work with the wavelength of the laser beams 224A-224F. Each lens 242A, 246C, 242F may be spherical or aspherical. In one embodiment, each lens 242A, 246C, 242F is secured to the mounting base 216.
In a non-exclusive embodiment, a Numerical Aperture of each lens 242A, 246C, 242F is chosen to approximately match a Numerical Aperture of its respective laser beam 224A-224F. Stated in another fashion, each lens 242A, 246C, 242F is designed to have an acceptance angle that approximately matches a cone of its respective laser beam 224A-224F. This results in the most compact system, and has the further advantage of maximizing the beam size relative to the lens diameter.
Further, the laser beams 224A-224F are arranged so that the combination beam 226 has a substantially annular shaped cross-section (illustrated with dashed lines) in the near field and has a hollow center 226B. In this embodiment, combination beam 226 has a substantially circular outer diameter 226C and a substantially circular inner diameter 226D.
As used herein, “substantially annular” shall mean that at least seventy-five percent of an annular shape is filled with light. Further, as used herein, “substantially circular outer diameter” shall mean that a circle (illustrated with dashes) can be made that tightly surrounds and encircles the combined light beams 224A-224F. Moreover, as used herein, “substantially circular inner diameter” shall mean that a circle (illustrated with dashes) can be made that is tightly surrounded and encircled by the combined light beams 224A-224F.
It should be noted that the combination beam 226 can be designed so that the diameters 226C, 226D of the combination beam 226 correspond to the design of the beam director 219 (illustrated in
In
The pointer elements 270, 272, 274, 276 are reflective elements that are spaced apart and arranged in a rectangular pattern. In this embodiment, (i) the first pointer element 270 redirects the combination beam 226 ninety degrees at the second pointer element 272; (ii) the second pointer element 272 redirects the combination beam 226 ninety degrees at the third pointer element 274; (iii) the third pointer element 274 redirects the combination beam 226 ninety degrees at the fourth pointer element 276; and (iv) the fourth pointer element 276 is positioned between the diverging element 227 and the collimating element 228 of the beam expander 221, and the fourth pointer element 276 redirects the combination beam 226 ninety degrees at the diverging element 227.
In this implementation, the expander elements 227, 228 of the beam expander 221 and the fourth pointer element 276 are coupled to and move with the second pointer frame 280. Further, the expander elements 227, 228, the fourth pointer element 276 and the second pointer frame 280 function as a second axis module that is rotated by the second frame mover 284 about the second axis 268. Moreover, the first pointer element 270, the second pointer element 272, the third pointer element 274, and the second axis module are coupled to and move with the first pointer frame 278. Additionally, the pointer elements 270, 272, 274, the second axis module, and the first pointer frame 278 function as a first axis module that is rotated by the first frame mover 282 about the first axis 266.
Stated in another fashion, in this design, (i) the first frame mover 282 is controlled to selectively rotate the first pointer frame 278 along with the pointer elements 270, 272, 274, 276, the second pointer frame 280, the second frame mover 284, and the beam expander 221 relative to the laser 214 (illustrated in
In this design, each of the pointer elements 270, 272, 274, 276 can be a reflective element that is appropriately coated to reflect light in the wavelengths of the combination beam 226.
In
Further, it should be noted that one or more of the pointer frames 278, 280 can include one or more rigid structural frames 286 (only one is shown as a box) that couple one or more elements 227, 228, 270, 272, 274, 276 together. For example, one or more structural frames 286 can (i) couple the elements 227, 228 of the beam expander 221 together and/or to the second pointer frame 280; and/or (ii) couple the pointer elements 270, 272, 274, 276 together or to the respective frames 278, 280. Unfortunately, these structural frames 286 can partly block/obstruct the combination beam 226 and/or the assembly beam 212.
In this embodiment, the beam expander 221 is somewhat similar to a beam expanding, on-axis telescope. In this non-exclusive embodiment, the beam expander 221 includes a disk shaped, convex collimating diverging element 227, and an annular disk shaped, concave collimating element 228. In one embodiment, the elements 227, 228 and the fourth pointer element 276 are spaced apart from each other, and centered on an element axis 288 that is coaxial with the output axis 212A. Further, in this embodiment, the fourth pointer element 276 directs and steers the combination beam 226 at the diverging element 227.
The diverging element 227 expands and/or diverges the laser beams of the combination beam 226. Subsequently, the collimating element 228 re-collimates each of the laser beams of the combination beam 226 to generate the assembly beam 212. Stated in another manner, the collimating element 228 collimates the laser beams of the combination beam 226 that have exited from the diverging element 227.
Together, the expander elements 227, 228 are a beam expander, expanding the combination beam 226 to the larger collimated assembly beam 212. In certain non-exclusive alternative embodiments, the beam expander 221 can be designed to increase the diameter (combination beam 226 compared to the assembly beam 212) by a factor of at least one and a half, two, three, four, five or six, and reduce divergence accordingly. With this design, by using a single beam expander 221, i.e. a single telescope, beam divergence is minimized, and power output can be efficiently scaled by combining laser beams 224A-224F (illustrated in
In
The diverging element 227 can be convex disk shaped and have an outer diameter 227A. Further, the diverging element 27 can be divided into a disk shaped center region 27B located on the element axis 54, and an annular disk shaped outer region 27C that encircles the center region 288. Moreover, the collimating element 228 can be concave, annular disk shaped to define an element aperture 228A, and can have an inner diameter 28B and an outer diameter 228C. Alternatively, the collimating element 228 can be designed without the element aperture 228A.
In
As provided above, the combination beam 226 is uniquely designed to be annular shaped and have a hollow center. With this design, the rays from the combination beam 226 are only incident on the outer region 227C and not the inner region 227B of the diverging element 227. As a result thereof, the entire combination beam 226 is reflected back to the collimating element 228, and the overall power of the laser beams 24A-24F forms the assembly beam 212. In summary, the present invention takes advantage of flexibility in the coherently combined laser beams 24A-24F to use it with on-axis telescope 221 without: (i) loss in power, (ii) degradation of quality of the assembly beam 212, or (iii) excessive heating of the device 10. Stated in another fashion, the hollow combination beam 226 can be used with no performance loss with an on-axis telescope 221, with less size, weight, power consumption and cost than an off-axis telescope.
For example, with reference to
At this time, the assembly beam 212 has a substantially annular shaped cross-section in the near field and has a hollow center 212B. In this embodiment, assembly beam 212 has a substantially circular outer diameter 212D and a substantially circular inner diameter 212E. It should be noted that the beam combiner 218 (illustrated in
As used herein, “substantially annular” shall mean that at least seventy-five percent of an annular shaped is filled with light. Further, as used herein, “substantially circular outer diameter” shall mean that a circle can be made that tightly surrounds and encircles the light that exits the beam expander 221. Moreover, as used herein, “substantially circular inner diameter” shall mean that a circle can be made that is tightly surrounded and encircled by the light that exits the beam expander 221.
It should be noted that size of the assembly beam 212 will depend upon the design of the combination beam 226 and the design of the beam expander 221. In alternative, non-exclusive examples, the device 210 can be designed so that the assembly beam 212 has (i) an outer diameter 212B of between six and twenty-four inches, and (ii) an inner diameter 212C of between one and six inches.
It should be noted that
While the particular devices 10, 210 as shown and disclosed herein are fully capable of obtaining the objects and providing the advantages herein before stated, it is to be understood that it is merely illustrative of the presently preferred embodiments of the invention and that no limitations are intended to the details of construction or design herein shown other than as described in the appended claims.
This application claims priority on U.S. Provisional Application No. 62/945,692 filed on Dec. 9, 2019, and entitled “DEVICE WITH A HOLLOW OUTPUT BEAM”. As far as permitted, the contents of U.S. Provisional Application No. 62/945,692 are incorporated herein by reference.
Filing Document | Filing Date | Country | Kind |
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PCT/US2020/063810 | 12/8/2020 | WO |
Number | Date | Country | |
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62945692 | Dec 2019 | US |