The disclosure pertains to back-reflection protection in fiber and fiber-delivered laser systems.
High-power industrial laser systems generally produce beams having output powers in the range of several hundreds of Watts to several kW. It is often desirable to deliver the laser power to a processing head or work piece via an optical fiber. Laser systems that can be coupled into an optical fiber for delivery include fiber lasers, disk lasers, and diode- or lamp-pumped solid-state lasers (e.g., Nd:YAG). In these systems, the desired optical power is guided in the fiber core, but some power may also be present in the fiber cladding; this cladding light is undesirable because it can cause excessive heating of or damage to downstream components or optics, or it may otherwise interfere with work piece processing.
In typical fiber laser systems a signal beam is created in an active fiber that includes a rare-earth doped optical fiber core by delivering a pump beam to a cladding of the active fiber at a pump wavelength that is shorter than a signal beam wavelength. At the output of the fiber laser, cladding light may consist of unabsorbed pump light and signal light that has escaped from the core. For both fiber lasers and other lasers, cladding light may be introduced into a beam delivery fiber if launching of the laser beam couples some of the light into the cladding rather than the core. A processing beam directed to a target or work piece can experience reflection or scattering and can become back-coupled into the beam delivery fiber. This back-coupled light can be coupled into both the active or beam delivery fiber core and cladding, and can destabilize, damage, or otherwise interfere with the laser system.
Accordingly, systems that can remove and monitor both forward-propagating and backward-propagating cladding light and backward-propagating core light are needed, particularly to protect against high-power back-reflections.
According to one aspect a system includes an optical fiber situated to propagate a laser beam received from a laser source to an output of the optical fiber, a first cladding light stripper optically coupled to the optical fiber and situated to extract at least a portion of forward-propagating cladding light in the optical fiber, and a second cladding light stripper optically coupled to the optical fiber between the first cladding light stripper and the optical fiber output and situated to extract at least a portion of backward-propagating cladding light in the optical fiber.
According to another aspect, a method includes directing a material processing laser beam from a laser source from an output end of a beam delivery fiber to a target, receiving a returned portion of the material processing laser beam returned from the target, coupling the returned portion into the beam delivery fiber, extracting cladding light associated with the material processing laser beam in a first cladding light stripper optically coupled to the beam delivery fiber, and extracting cladding light associated with the returned portion of the material processing laser beam in a second cladding light stripper optically situated between the first cladding light stripper and the output end of the beam delivery fiber.
According to another aspect, a method includes detecting a characteristic associated with backward-propagating cladding light extracted with a cladding light stripper from a beam delivery fiber delivering a laser beam generated with a laser source, detecting a characteristic associated with backward-propagating core light in the beam delivery fiber, and adjusting one or more laser system characteristics in response to one or more of the detected backward-propagating cladding light and backward-propagating core light characteristics.
According to another aspect, a system includes a first cladding light stripper disposed between a laser source and a beam delivery fiber output situated in relation to a target, the first cladding light stripper situated to receive a material processing beam and to extract forward-propagating cladding light associated with the material processing beam from the beam delivery fiber, and a second cladding light stripper disposed between the first cladding light stripper and the beam delivery fiber output and situated to receive the material processing beam from the first cladding light stripper and to receive backward-propagating cladding light associated with the target, the second cladding light stripper situated to extract backward-propagating cladding light from the beam delivery fiber.
According to another aspect, a laser feedback monitoring system in a high-power laser system is provided, the high-power laser system configured to produce a laser beam from a laser source and to emit the laser beam from a delivery fiber output and to direct the emitted beam to a target, with the laser feedback monitoring system including a first cladding light stripper situated between the laser source and the delivery fiber output to receive the laser beam and to remove cladding light associated with the beam, a second cladding light stripper situated between the first cladding light stripper and the delivery fiber output to receive the beam from the first cladding light stripper and to remove residual cladding light associated with the beam and to receive light back-reflected from the target and coupled back into the delivery fiber output and to remove back-reflected cladding light, and at least one back-reflected cladding light detector coupled to the second cladding light stripper for detecting characteristics of the back-reflected cladding light.
The foregoing and other objects, features, and advantages will become more apparent from the following detailed description, which proceeds with reference to the accompanying figures.
As used in this application and in the claims, the singular forms “a,” “an,” and “the” include the plural forms unless the context clearly dictates otherwise. Additionally, the term “includes” means “comprises.” Further, the term “coupled” does not exclude the presence of intermediate elements between the coupled items.
The systems, apparatus, and methods described herein should not be construed as limiting in any way. Instead, the present disclosure is directed toward all novel and non-obvious features and aspects of the various disclosed embodiments, alone and in various combinations and sub-combinations with one another. The disclosed systems, methods, and apparatus are not limited to any specific aspect or feature or combinations thereof, nor do the disclosed systems, methods, and apparatus require that any one or more specific advantages be present or problems be solved. Any theories of operation are to facilitate explanation, but the disclosed systems, methods, and apparatus are not limited to such theories of operation.
Although the operations of some of the disclosed methods are described in a particular, sequential order for convenient presentation, it should be understood that this manner of description encompasses rearrangement, unless a particular ordering is required by specific language set forth below. For example, operations described sequentially may in some cases be rearranged or performed concurrently. Moreover, for the sake of simplicity, the attached figures may not show the various ways in which the disclosed systems, methods, and apparatus can be used in conjunction with other systems, methods, and apparatus. Additionally, the description sometimes uses terms like “produce” and “provide” to describe the disclosed methods. These terms are high-level abstractions of the actual operations that are performed. The actual operations that correspond to these terms will vary depending on the particular implementation and are readily discernible by one of ordinary skill in the art.
In some examples, values, procedures, or apparatus' are referred to as “lowest”, “best”, “minimum,” or the like. It will be appreciated that such descriptions are intended to indicate that a selection among many used functional alternatives can be made, and such selections need not be better, smaller, or otherwise preferable to other selections. Examples are described with reference to directions indicated as “above,” “below,” “upper,” “lower,” and the like. These terms are used for convenient description, but do not imply any particular spatial orientation.
As used herein, optical radiation refers to electromagnetic radiation at wavelengths of between about 100 nm and 10 μm, and typically between about 500 nm and 2 μm. Examples based on available laser diode sources and optical fibers generally are associated with wavelengths of between about 800 nm and 1700 nm. In some examples, propagating optical radiation is referred to as one or more beams having diameters, asymmetric fast and slow axes, beam cross-sectional areas, and beam divergences that can depend on beam wavelength and the optical systems used for beam shaping. For convenience, optical radiation is referred to as light or beams in some examples, and need not be at visible wavelengths. Forward-propagating light or optical beams or beam portions refer to light, beams, or beam portions that propagate in a common direction with a processing beam that is directed to a target. Backward-propagating light or optical beams or beam portions refer to light, beams, or beam portions that propagate in a common and opposite direction of a processing beam that is directed to a target.
Representative embodiments are described with reference to optical fibers, but other types of optical waveguides can be used having square, rectangular, polygonal, oval, elliptical or other cross-sections. Optical fibers are typically formed of silica (glass) that is doped (or undoped) so as to provide predetermined refractive indices or refractive index differences. In some, examples, fibers or other waveguides are made of other materials such as fluorozirconates, fluoroaluminates, fluoride or phosphate glasses, chalcogenide glasses, or crystalline materials such as sapphire, depending on wavelengths of interest. Refractive indices of silica and fluoride glasses are typically about 1.5, but refractive indices of other materials such as chalcogenides can be 3 or more. In still other examples, optical fibers can be formed in part of plastics. In typical examples, a doped waveguide core such as a fiber core provides optical gain in response to pumping, and core and claddings are approximately concentric. In other examples, one or more of the core and claddings are decentered, and in some examples, core and cladding orientation and/or displacement vary along a waveguide length.
As used herein, numerical aperture (NA) refers to a largest angle of incidence with respect to a propagation axis defined by an optical waveguide for which propagating optical radiation is substantially confined. In optical fibers, fiber cores and fiber claddings can have associated NAs, typically defined by refractive index differences between a core and cladding layer, or adjacent cladding layers, respectively. While optical radiation propagating at such NAs is generally well confined, associated electromagnetic fields such as evanescent fields typically extend into an adjacent cladding layer. In some examples, a core NA is associated with a core/inner cladding refractive index, and a cladding NA is associated with an inner cladding/outer cladding refractive index difference. For an optical fiber having a core refractive index ncore and a cladding index nclad, a fiber core NA is NA=√{square root over (n2core−n2clad)}. For an optical fiber with an inner core and an outer core adjacent the inner core, a cladding NA is NA=√{square root over (n2inner−n2outer)}, wherein ninner and nouter are refractive indices of the inner cladding and the outer cladding, respectively. Optical beams as discussed above can also be referred to as having a beam NA which is associated with a beam angular radius. While multi-core step index fibers are described below, gradient index designs can also be used.
In the examples disclosed herein, a waveguide core such as an optical fiber core is doped with a rare earth element such as Nd, Yb, Ho, Er, or other active dopants or combinations thereof. Such actively doped cores can provide optical gain in response to optical or other pumping. As disclosed below, waveguides having such active dopants can be used to form optical amplifiers, or, if provided with suitable optical feedback such as reflective layers, mirrors, Bragg gratings, or other feedback mechanisms, such waveguides can generate laser emissions. Optical pump radiation can be arranged to co-propagate and/or counter-propagate in the waveguide with respect to a propagation direction of an emitted laser beam or an amplified beam.
The term brightness is used herein to refer to optical beam power per unit area per solid angle. In some examples, optical beam power is provided with one or more laser diodes that produce beams whose solid angles are proportional to beam wavelength and beam area. Selection of beam area and beam solid angle can produce pump beams that couple selected pump beam powers into one or more core or cladding layers of double, triple, or other multi-clad optical fibers.
Referring now to
A returned beam portion 24 that is coupled into the output of the delivery fiber 16 is generally undesirable and can destabilize the laser system 10 or cause laser system degradation and failure. By arranging a pair of cladding light strippers, such as the first and second cladding light strippers 20, 22, laser systems such as the laser system 12 can be provided with robust protection from back-reflection. In particular, the second cladding light stripper 22, which is more proximal to the output of the delivery fiber 16 as shown in
The cladding light strippers 20, 22 can also be conveniently arranged in close proximity to each other and still retain optical or thermal isolation. For example, in some embodiments, the cladding light strippers 20, 22 can be separated and separately or jointly cooled or otherwise thermally managed. In other embodiments, the cladding light strippers 20, 22 are disposed on a common heat sink block 26 which is actively cooled with one or more cooling devices coupled to the heat sink block 26. Depending on the design of the cladding light strippers 20, 22, forward-propagating cladding light may also be partially removed by the second cladding light stripper 22, and backward-propagating cladding light may also be partially removed by the first cladding light stripper 20. Forward-propagating cladding light is generally undesirable because it can cause heating or damage to components downstream from the fiber laser, e.g., to the delivery cable or to optical systems employed to deliver the laser beam to the work piece.
Depending on the output power of the output beam 14 (which can be as little as 0.5 kW or less to as much as 10 kW or more) and other attributes of the high-power laser system 10, various forward-propagating cladding light and back-coupled light power contents can be expected during operation. For example, the laser system 10 configured to generate the output beam 14 with an output power of around 3 kW can include 300 W or more of forward-propagating cladding light that should be coupled out of the delivered beam 14 and dissipated to prevent system destabilization. Theoretically, up to the entirety of the output beam 14 could be back-reflected and coupled back into the output of the delivery fiber 16, though 100% back-coupling may be unlikely. With the 3 kW output beam 14, in typical examples approximately 300 W can be expected to become back-coupled, however the portion of the output beam 14 that is back-reflected, the variability of the portion, and the time dependence of the portion can be dependent on the application in which the high-power laser system output beam 14 is being used. Accordingly, back-coupled light and backward-propagating cladding light can range from being continuous to highly transient. In some system examples, 100 W or more of continuous forward-propagating cladding light is removed and 100 W or more of transient backward-propagating cladding light is removed. The cladding light strippers 20, 22 are thus operable to remove the cladding light and the removed light can be dumped in some manner, such as with a conductive sink like conductive block 26.
Referring now to
The laser system 40 also includes a stripped forward-propagating cladding light detector 58 coupled to the first cladding light stripper 50. The detector 58 is situated to detect one or more characteristics associated with the forward-propagating cladding light, such as power, wavelength, temporal characteristics (e.g., power variation, pulse duration, pulse repetition rate), temperature in proximity to the stripper 50, etc., and provides an associated detection signal to a system controller 60. The detector 58 can include one sensor for detecting a particular characteristic, one sensor for detecting a plurality of characteristics, or a plurality of sensors for detecting the same or different characteristics. In some examples, the first cladding light stripper 50 includes a volume formed in the conductive block 56, such as an integrating volume. The forward-propagating cladding light propagates along a fiber situated in the volume, such as a portion of the beam delivery fiber 46 or another fiber or fiber portion coupled to the beam delivery fiber 46. One or more sensors associated with the detector 58 can be situated in or near the volume so as to generate detection signals to detect forward-propagating cladding light characteristics. To moderate detected characteristics of cladding light, one or more optical filters may be used. Detected characteristics can also include specular or diffuse reflections of cladding light extracted from the optical fiber in which the forward-propagating cladding light is propagating.
The laser system 40 further includes a stripped backward-propagating cladding light detector 62 coupled to the second cladding light stripper 52 which detects one or more characteristics associated with the backward-propagating cladding light, such as power, wavelength, temporal characteristics, temperature, etc. In some examples, the detector 62 (and/or detector 58) can include one or more of a thermistor, thermal switch, and photodiode. The output of the detector 62 is also coupled to the controller 60. Because most or all of the forward-propagating cladding light associated with the beam 44 is removed by the forward-propagating cladding light stripper 50, the detector 62 is situated to detect back-reflected characteristics without the characteristics becoming tainted, skewed, or muddled by the forward-propagating cladding light energy. Similarly, since most or all of the backward-propagating cladding light energy is removed by the backward-propagating cladding light stripper 52, the process of detecting forward-propagating cladding light characteristics experiences improved accuracy in the presence of back-reflected light.
The system controller 60 is situated to receive one or more such detection signals that can be associated with corresponding beam characteristics and can initiate different system actions in response. For example, controller 60 is shown to be coupled with control output 64 to laser source 42. Based on the detected characteristics from detectors 58, 62, a laser interlock procedure can be executed that triggers a power disconnect or an adjustment of power level or some other characteristic associated with the laser system 40, including the laser source 42 and the output beam 44. For example, if the backward-propagating cladding light power or an associated temperature is excessive, the laser source 42 can be turned off, or a warning can be issued to the user. Abnormal increases or decreases of the forward-propagating cladding power may indicate a malfunction of the laser system, which can result in turning off the laser source 42 or issuing a warning to a user. In other examples, laser source 42 output power can be varied to compensate for a detected variation in forward-propagating cladding energy. Other laser system characteristics can be adjusted as well, including cooling system characteristics (e.g., fluid flow-rates, power level, etc.).
The cladding light strippers 50, 52 typically couple only cladding light, or poorly coupled cladding light, out of the optical delivery fiber 46. Both the forward- and backward-propagating core light associated with beam propagation in the delivery fiber 46 is generally unaffected. Backward-propagating core light can also lead to system degradation and failure, and the system controller 60 can be coupled to a backward-propagating core light detector 66, that is coupled to the laser source 42 and detects one or more characteristics associated with backward-propagating core light. The interlock control 64 of the controller 66 can also be configured to disconnect or adjust power or another laser system characteristic associated with the laser source 42. In some embodiments, detected cladding light and core light characteristics can include spectral characteristics, allowing deeper insights into system operation and particular application effects, and enabling a spectral-based interlock for the system 40 or spectral-based adjustment of laser system characteristics, including output beam power, pump source power, and temporal features.
In some examples, a detector 68 is coupled to the optical fiber 46 propagating the output beam 44 between the first and second cladding light strippers 50, 52. Because most or all of the forward and backward-propagating cladding light is removed by the strippers 50, 52, the length of optical fiber 46 extending between the strippers 50, 52 provides a location suitable to detect characteristics of core light associated with the propagating output beam 44 such that detection experiences less interference associated with forward or backward cladding light energy. In one example, a core light power characteristic is detected with detector 68 coupled to a core light detection chamber 70 without interfering with propagating beam 44 by receiving light scattered out of the core. The light detection chamber 70 can serve as an optical integrating volume such that detector 68 receives a multiply reflected, integrated characteristic of the scattered core light. In another example, the detector 68 is coupled so as to directly receive the scattered core light or one or more mirrors or lenses can be used to concentrate and direct the scattered core light to the detector 68. In a further example, an optical splice is disposed on the optical fiber 46 in the detection chamber 70. The detector 68 can then detect optical loss associated with the propagation of light through the optical splice, and such loss can vary in relation to the optical power and wavelength of the beam 44 propagating in the core of the fiber. It will be appreciated that various features of detectors 58, 62, 68 as well as the detected characteristics can be used together.
In various examples, values of particular detected optical characteristics can provide the actual or close to the actual characteristic sought, or the values can be empirically or observationally matched to different expected or actual characteristics. For example, the laser system can be operated at selected power levels and an output beam can be measured both in the presence and absence of cladding light strippers or other system components to determine the amount of cladding light that is removed and corresponding detected values. A table can be generated, and a function fitted to the table values, associating the different detected characteristics in relation to the actual characteristics.
Cladding light strippers can be made in a variety of ways. Some examples of cladding light strippers utilize an epoxy that surrounds an exposed cladding surface of an optical fiber in which an output beam and cladding light are propagating. Because the fiber cladding is coupled to an epoxy with selected refractive index and other characteristics, cladding light is successively stripped along the length of the epoxy-cladding interface. In other examples of cladding light strippers, the optical fiber includes one or more notches or other patterns (“microstructures”) penetrating the circumference of the exposed cladding. The notches are operable to disrupt the propagating cladding light by directing the cladding light away from and out of the optical fiber without substantially affecting the light propagating in the fiber core. The out-coupled cladding light then impacts an adjacent surface of a conductive block and is eventually converted to heat, which dissipates through the conductive block. In other examples of cladding light strippers, silica-based crystals are formed on the cladding surface to scatter the cladding light out of the fiber without substantially affecting the light propagating in the fiber core.
Referring to
Laser source 102 is expanded to show an example of a laser source herein suitable for generating the high power fiber-coupled output beam 104. It will be appreciated that a variety of types and variations of laser sources are possible that can be configured to produce a fiber-delivered high power output beam, including laser sources configured to detect different operating system characteristics and to receive different control commands. Other examples of suitable laser sources include fiber lasers, fiber amplifiers, disk lasers, diode-pumped solid-state lasers, lamp-pumped lasers, and direct-diode lasers, each of which can be configured to operate at a wavelength that can be transmitted to the processing head or work piece using an optical fiber.
As shown, the exemplary laser source 102 includes a plurality of pump modules 118 that produce pump beams at a pump wavelength and couple the pump beams into a pump delivery fiber 120. The plurality of pump delivery fibers 120 is coupled to a pump or pump-signal combiner 122 which combines received pump light into a combined pump output 124. The output 124 is coupled to a fiber laser oscillator 126 that generates the output beam 104 in an active core of the fiber oscillator using the coupled pump light. The pump delivery fibers 120 are arranged in various configurations about an input of the combiner 122. An additional fiber 128 is coupled to a center position of the input of the combiner 122 and can be coupled to one or more components, including an aiming laser 130, a detector 132, or a beam dump 134. The aiming laser 130 emits an aiming beam which can assist with the use of the system 100 by showing the expected location for the beam 104 at the target 108. The center position occupied with the additional fiber 128 is also convenient for detection and removal of core light that is not contained by the oscillator 126. In particular, back-reflected light 116 that is coupled into the core of the delivery fiber 106 may not be removed by the cladding light strippers 110, 112 and can propagate through to the laser source 102.
The core detector 132 is thus situated to detect characteristics associated with core light propagating past the combiner 122 and to provide the detected characteristics to a system controller 136. Based in part or in whole on the received characteristics, the controller 136 can adjust other system characteristics, such as the power level supplied to the pump modules 118 using controller output 138, in order to protect or enhance system 100 performance. Moreover, the central position of the fiber 128 of the combiner 122 ensures most or all of the core light received by the combiner 122 from the direction of the oscillator 126 is directed into the fiber 128, which can then be detected with core light detector 132 and removed with beam dump 134. A detector 140 which detects forward-propagating cladding light is coupled to the first cladding light stripper 110 and provides information about forward-propagating cladding light characteristics to the controller 136. A detector 142 which detects backward-propagating cladding light is coupled to the second cladding light stripper 112 and provides information about backward-propagating cladding light characteristics to the controller 136. Independently or in concert, the detectors 132, 140, 142 can detect beam and system characteristics that can be utilized to optimize, protect, or otherwise enhance performance of laser system 100.
In
In view of the many possible embodiments to which the principles of the disclosed technology may be applied, it should be recognized that the illustrated embodiments are only representative examples and should not be taken as limiting the scope of the disclosure. Alternatives specifically addressed in these sections are merely exemplary and do not constitute all possible alternatives to the embodiments described herein. For instance, various components of systems described herein may be combined in function and use. We therefore claim all that comes within the scope and spirit of the appended claims.
This application is a continuation of U.S. application Ser. No. 14/816,211, filed Aug. 3, 2015, which claims the benefit of U.S. Provisional Application No. 62/032,043, filed on Aug. 1, 2014, both of which are hereby incorporated by reference in their entirety.
Number | Name | Date | Kind |
---|---|---|---|
3388461 | Lins | Jun 1968 | A |
4138190 | Bryngdahl | Feb 1979 | A |
4252403 | Salisbury | Feb 1981 | A |
4266851 | Salisbury | May 1981 | A |
4475027 | Pressley | Oct 1984 | A |
4475789 | Kahn | Oct 1984 | A |
4713518 | Yamazaki et al. | Dec 1987 | A |
4863538 | Deckard | Sep 1989 | A |
4998797 | van den Bergh et al. | Mar 1991 | A |
5008555 | Mundy | Apr 1991 | A |
5153773 | Muraki et al. | Oct 1992 | A |
5252991 | Storlie et al. | Oct 1993 | A |
5319195 | Jones | Jun 1994 | A |
5463497 | Muraki et al. | Oct 1995 | A |
5475415 | Noethen | Dec 1995 | A |
5509597 | Laferriere | Apr 1996 | A |
5523543 | Hunter, Jr. et al. | Jun 1996 | A |
5745284 | Goldberg et al. | Apr 1998 | A |
5748824 | Smith | May 1998 | A |
5818630 | Fermann et al. | Oct 1998 | A |
5864430 | Dickey et al. | Jan 1999 | A |
5903696 | Krivoshlykov | May 1999 | A |
5909306 | Goldberg et al. | Jun 1999 | A |
5932119 | Kaplan et al. | Aug 1999 | A |
5986807 | Fork | Nov 1999 | A |
5999548 | Mori et al. | Dec 1999 | A |
6072184 | Okino et al. | Jun 2000 | A |
6132104 | Bliss et al. | Oct 2000 | A |
6265710 | Walter | Jul 2001 | B1 |
6330382 | Harshbarger et al. | Dec 2001 | B1 |
RE37585 | Mourou et al. | Mar 2002 | E |
6353203 | Hokodate et al. | Mar 2002 | B1 |
6362004 | Noblett | Mar 2002 | B1 |
6426840 | Partanen et al. | Jul 2002 | B1 |
6433301 | Dunsky et al. | Aug 2002 | B1 |
6434177 | Jurgensen | Aug 2002 | B1 |
6483973 | Mazzarese et al. | Nov 2002 | B1 |
6490376 | Au et al. | Dec 2002 | B1 |
6496301 | Koplow et al. | Dec 2002 | B1 |
6542665 | Reed et al. | Apr 2003 | B2 |
6556340 | Wysocki et al. | Apr 2003 | B1 |
6577314 | Yoshida et al. | Jun 2003 | B1 |
6639177 | Ehrmann et al. | Oct 2003 | B2 |
6671293 | Kopp et al. | Dec 2003 | B2 |
6711918 | Kliner et al. | Mar 2004 | B1 |
6724528 | Koplow et al. | Apr 2004 | B2 |
6772611 | Kliner et al. | Aug 2004 | B2 |
6777645 | Ehrmann et al. | Aug 2004 | B2 |
6779364 | Tankala et al. | Aug 2004 | B2 |
6801550 | Snell et al. | Oct 2004 | B1 |
6825974 | Kliner et al. | Nov 2004 | B2 |
6839163 | Jakobson et al. | Jan 2005 | B1 |
6882786 | Kliner et al. | Apr 2005 | B1 |
6895154 | Johnson et al. | May 2005 | B2 |
6917742 | Po | Jul 2005 | B2 |
6941053 | Lauzon et al. | Sep 2005 | B2 |
6963062 | Cyr et al. | Nov 2005 | B2 |
6989508 | Ehrmann et al. | Jan 2006 | B2 |
7068900 | Croteau et al. | Jun 2006 | B2 |
7079566 | Kido et al. | Jul 2006 | B2 |
7099533 | Chenard | Aug 2006 | B1 |
7116887 | Farroni et al. | Oct 2006 | B2 |
7146073 | Wan | Dec 2006 | B2 |
7148447 | Ehrmann et al. | Dec 2006 | B2 |
7151787 | Kulp et al. | Dec 2006 | B2 |
7157661 | Amako | Jan 2007 | B2 |
7170913 | Araujo et al. | Jan 2007 | B2 |
7184630 | Kwon et al. | Feb 2007 | B2 |
7235150 | Bischel et al. | Jun 2007 | B2 |
7257293 | Fini et al. | Aug 2007 | B1 |
7317857 | Manyam et al. | Jan 2008 | B2 |
7349123 | Clarke et al. | Mar 2008 | B2 |
7359604 | Po | Apr 2008 | B2 |
7373070 | Wetter et al. | May 2008 | B2 |
7382389 | Cordingley et al. | Jun 2008 | B2 |
7394476 | Cordingley et al. | Jul 2008 | B2 |
7421175 | Varnham | Sep 2008 | B2 |
7463805 | Li et al. | Dec 2008 | B2 |
7526166 | Bookbinder et al. | Apr 2009 | B2 |
7527977 | Fruetel et al. | May 2009 | B1 |
7537395 | Savage-Leuchs | May 2009 | B2 |
7592568 | Varnham et al. | Sep 2009 | B2 |
7593435 | Gapontsev et al. | Sep 2009 | B2 |
7748913 | Oba | Jul 2010 | B2 |
7764854 | Fini | Jul 2010 | B2 |
7781778 | Moon et al. | Aug 2010 | B2 |
7783149 | Fini | Aug 2010 | B2 |
7835608 | Minelly et al. | Nov 2010 | B2 |
7839901 | Meleshkevich et al. | Nov 2010 | B2 |
7876495 | Minelly | Jan 2011 | B1 |
7880961 | Feve et al. | Feb 2011 | B1 |
7920767 | Fini | Apr 2011 | B2 |
7924500 | Minelly | Apr 2011 | B1 |
7925125 | Cyr et al. | Apr 2011 | B2 |
7955905 | Cordingley et al. | Jun 2011 | B2 |
7955906 | Cordingley et al. | Jun 2011 | B2 |
8027555 | Kliner et al. | Sep 2011 | B1 |
8071912 | Costin, Sr. et al. | Dec 2011 | B2 |
8217304 | Cordingley et al. | Jul 2012 | B2 |
8237788 | Cooper et al. | Aug 2012 | B2 |
8243764 | Tucker et al. | Aug 2012 | B2 |
8251475 | Murray et al. | Aug 2012 | B2 |
8269108 | Kunishi et al. | Sep 2012 | B2 |
8270441 | Rogers et al. | Sep 2012 | B2 |
8270445 | Morasse et al. | Sep 2012 | B2 |
8278591 | Chouf et al. | Oct 2012 | B2 |
8288683 | Jennings et al. | Oct 2012 | B2 |
8310009 | Saran et al. | Nov 2012 | B2 |
8317413 | Fisher et al. | Nov 2012 | B2 |
8362391 | Partlo et al. | Jan 2013 | B2 |
8395084 | Tanaka | Mar 2013 | B2 |
8414264 | Bolms et al. | Apr 2013 | B2 |
8433161 | Langseth et al. | Apr 2013 | B2 |
8442303 | Cheng et al. | May 2013 | B2 |
8472099 | Fujino et al. | Jun 2013 | B2 |
8509577 | Liu | Aug 2013 | B2 |
8526110 | Honea et al. | Sep 2013 | B1 |
8537871 | Saracco | Sep 2013 | B2 |
8542145 | Galati | Sep 2013 | B2 |
8542971 | Chatigny | Sep 2013 | B2 |
8593725 | Kliner et al. | Nov 2013 | B2 |
8711471 | Liu et al. | Apr 2014 | B2 |
8728591 | Inada et al. | May 2014 | B2 |
8755649 | Yilmaz et al. | Jun 2014 | B2 |
8755660 | Minelly | Jun 2014 | B1 |
8774237 | Maryashin et al. | Jul 2014 | B2 |
8781269 | Huber et al. | Jul 2014 | B2 |
8809734 | Cordingley et al. | Aug 2014 | B2 |
8835804 | Farmer et al. | Sep 2014 | B2 |
8873134 | Price et al. | Oct 2014 | B2 |
8947768 | Kliner et al. | Feb 2015 | B2 |
8948218 | Gapontsev et al. | Feb 2015 | B2 |
8953914 | Genier | Feb 2015 | B2 |
9014220 | Minelly et al. | Apr 2015 | B2 |
9136663 | Taya | Sep 2015 | B2 |
9140873 | Minelly | Sep 2015 | B2 |
9158066 | Fini et al. | Oct 2015 | B2 |
9170359 | Van Bommel et al. | Oct 2015 | B2 |
9207395 | Fini et al. | Dec 2015 | B2 |
9217825 | Ye et al. | Dec 2015 | B2 |
9250390 | Muendel et al. | Feb 2016 | B2 |
9310560 | Chann et al. | Apr 2016 | B2 |
9322989 | Fini et al. | Apr 2016 | B2 |
9325151 | Fini et al. | Apr 2016 | B1 |
9339890 | Woods et al. | May 2016 | B2 |
9366887 | Tayebati et al. | Jun 2016 | B2 |
9397466 | McComb et al. | Jul 2016 | B2 |
9431786 | Savage-Leuchs | Aug 2016 | B2 |
9442252 | Genier | Sep 2016 | B2 |
9507084 | Fini et al. | Dec 2016 | B2 |
9537042 | Dittli et al. | Jan 2017 | B2 |
9547121 | Hou et al. | Jan 2017 | B2 |
9634462 | Kliner et al. | Apr 2017 | B2 |
9837783 | Kliner et al. | Dec 2017 | B2 |
10310201 | Kliner | Jun 2019 | B2 |
20010050364 | Tanaka et al. | Dec 2001 | A1 |
20020097963 | Ukechi et al. | Jul 2002 | A1 |
20020146202 | Reed et al. | Oct 2002 | A1 |
20020158052 | Ehrmann et al. | Oct 2002 | A1 |
20020176676 | Johnson et al. | Nov 2002 | A1 |
20030031407 | Weisberg et al. | Feb 2003 | A1 |
20030059184 | Tankala et al. | Mar 2003 | A1 |
20030095578 | Kopp et al. | May 2003 | A1 |
20030118305 | Reed et al. | Jun 2003 | A1 |
20030213998 | Hsu et al. | Nov 2003 | A1 |
20030219208 | Kwon et al. | Nov 2003 | A1 |
20040013379 | Johnson et al. | Jan 2004 | A1 |
20040086245 | Farroni et al. | May 2004 | A1 |
20040112634 | Tanaka et al. | Jun 2004 | A1 |
20040207936 | Yamamoto et al. | Oct 2004 | A1 |
20040208464 | Po | Oct 2004 | A1 |
20050002607 | Neuhaus et al. | Jan 2005 | A1 |
20050027288 | Oyagi et al. | Feb 2005 | A1 |
20050041697 | Seifert et al. | Feb 2005 | A1 |
20050168847 | Sasaki | Aug 2005 | A1 |
20050185892 | Kwon et al. | Aug 2005 | A1 |
20050233557 | Tanaka et al. | Oct 2005 | A1 |
20050259944 | Anderson et al. | Nov 2005 | A1 |
20050265678 | Manyam et al. | Dec 2005 | A1 |
20050271340 | Weisberg et al. | Dec 2005 | A1 |
20060013532 | Wan | Jan 2006 | A1 |
20060024001 | Kobayashi | Feb 2006 | A1 |
20060054606 | Amako | Mar 2006 | A1 |
20060067632 | Broeng et al. | Mar 2006 | A1 |
20060219673 | Varnham et al. | Oct 2006 | A1 |
20060275705 | Dorogy et al. | Dec 2006 | A1 |
20060291788 | Po | Dec 2006 | A1 |
20070075060 | Shedlov et al. | Apr 2007 | A1 |
20070104436 | Li et al. | May 2007 | A1 |
20070104438 | Varnham | May 2007 | A1 |
20070147751 | Fini | Jun 2007 | A1 |
20070178674 | Imai et al. | Aug 2007 | A1 |
20070195850 | Schluter et al. | Aug 2007 | A1 |
20070215820 | Cordingley et al. | Sep 2007 | A1 |
20080037604 | Savage-Leuchs | Feb 2008 | A1 |
20080141724 | Fuflyigin | Jun 2008 | A1 |
20080181567 | Bookbinder et al. | Jul 2008 | A1 |
20080246024 | Touwslager et al. | Oct 2008 | A1 |
20090034059 | Fini | Feb 2009 | A1 |
20090059353 | Fini | Mar 2009 | A1 |
20090080835 | Frith | Mar 2009 | A1 |
20090122377 | Wagner | May 2009 | A1 |
20090127477 | Tanaka et al. | May 2009 | A1 |
20090152247 | Jennings et al. | Jun 2009 | A1 |
20090154512 | Simons et al. | Jun 2009 | A1 |
20090175301 | Li et al. | Jul 2009 | A1 |
20090274833 | Li | Nov 2009 | A1 |
20090297108 | Ushiwata et al. | Dec 2009 | A1 |
20090314752 | Manens et al. | Dec 2009 | A1 |
20100025387 | Arai et al. | Feb 2010 | A1 |
20100067013 | Howieson et al. | Mar 2010 | A1 |
20100067860 | Ikeda et al. | Mar 2010 | A1 |
20100129029 | Westbrook | May 2010 | A1 |
20100150186 | Mizuuchi | Jun 2010 | A1 |
20100163537 | Furuta et al. | Jul 2010 | A1 |
20100225974 | Sandstrom | Sep 2010 | A1 |
20100230665 | Verschuren et al. | Sep 2010 | A1 |
20110058250 | Liu et al. | Mar 2011 | A1 |
20110080476 | Dinauer et al. | Apr 2011 | A1 |
20110091155 | Yilmaz et al. | Apr 2011 | A1 |
20110127697 | Milne | Jun 2011 | A1 |
20110133365 | Ushimaru et al. | Jun 2011 | A1 |
20110163077 | Partlo et al. | Jul 2011 | A1 |
20110187025 | Costin, Sr. | Aug 2011 | A1 |
20110248005 | Briand et al. | Oct 2011 | A1 |
20110278277 | Stork Genannt Wersborg | Nov 2011 | A1 |
20110279826 | Miura et al. | Nov 2011 | A1 |
20110297229 | Gu et al. | Dec 2011 | A1 |
20110305256 | Chann | Dec 2011 | A1 |
20120002919 | Liu | Jan 2012 | A1 |
20120051084 | Yalin et al. | Mar 2012 | A1 |
20120051692 | Seo | Mar 2012 | A1 |
20120082410 | Peng et al. | Apr 2012 | A1 |
20120127097 | Gaynor et al. | May 2012 | A1 |
20120145685 | Ream et al. | Jun 2012 | A1 |
20120148823 | Chu | Jun 2012 | A1 |
20120156458 | Chu | Jun 2012 | A1 |
20120168411 | Farmer et al. | Jul 2012 | A1 |
20120262781 | Price et al. | Oct 2012 | A1 |
20120295071 | Sato | Nov 2012 | A1 |
20120301733 | Eckert et al. | Nov 2012 | A1 |
20120301737 | Labelle et al. | Nov 2012 | A1 |
20120321262 | Goell et al. | Dec 2012 | A1 |
20120329974 | Inada et al. | Dec 2012 | A1 |
20130005139 | Krasnov et al. | Jan 2013 | A1 |
20130022754 | Bennett et al. | Jan 2013 | A1 |
20130023086 | Chikama et al. | Jan 2013 | A1 |
20130027648 | Moriwaki | Jan 2013 | A1 |
20130038923 | Jespersen et al. | Feb 2013 | A1 |
20130087694 | Creeden et al. | Apr 2013 | A1 |
20130095260 | Bovatsek et al. | Apr 2013 | A1 |
20130146569 | Woods et al. | Jun 2013 | A1 |
20130148925 | Muendel et al. | Jun 2013 | A1 |
20130182725 | Karlsen et al. | Jul 2013 | A1 |
20130223792 | Huber et al. | Aug 2013 | A1 |
20130228442 | Mohaptatra et al. | Sep 2013 | A1 |
20130251324 | Fini et al. | Sep 2013 | A1 |
20130272657 | Salokatve | Oct 2013 | A1 |
20130299468 | Unrath et al. | Nov 2013 | A1 |
20130308661 | Nishimura | Nov 2013 | A1 |
20130343703 | Genier | Dec 2013 | A1 |
20140044143 | Clarkson et al. | Feb 2014 | A1 |
20140086526 | Starodubov et al. | Mar 2014 | A1 |
20140104618 | Potsaid et al. | Apr 2014 | A1 |
20140155873 | Bor | Jun 2014 | A1 |
20140177038 | Rrataj et al. | Jun 2014 | A1 |
20140178023 | Oh et al. | Jun 2014 | A1 |
20140205236 | Noguchi et al. | Jul 2014 | A1 |
20140233900 | Hugonnot et al. | Aug 2014 | A1 |
20140241385 | Fomin et al. | Aug 2014 | A1 |
20140268310 | Ye et al. | Sep 2014 | A1 |
20140313513 | Liao | Oct 2014 | A1 |
20140332254 | Pellerite et al. | Nov 2014 | A1 |
20140333931 | Lu et al. | Nov 2014 | A1 |
20140334788 | Fini et al. | Nov 2014 | A1 |
20150049987 | Grasso et al. | Feb 2015 | A1 |
20150104139 | Brunet et al. | Apr 2015 | A1 |
20150125114 | Genier | May 2015 | A1 |
20150125115 | Genier | May 2015 | A1 |
20150138630 | Honea et al. | May 2015 | A1 |
20150165556 | Jones et al. | Jun 2015 | A1 |
20150241632 | Chann et al. | Aug 2015 | A1 |
20150293300 | Fini et al. | Oct 2015 | A1 |
20150293306 | Huber et al. | Oct 2015 | A1 |
20150316716 | Fini et al. | Nov 2015 | A1 |
20150331205 | Tayebati et al. | Nov 2015 | A1 |
20150349481 | Kliner | Dec 2015 | A1 |
20150352664 | Errico et al. | Dec 2015 | A1 |
20150378184 | Tayebati et al. | Dec 2015 | A1 |
20160013607 | McComb et al. | Jan 2016 | A1 |
20160059354 | Sercel et al. | Mar 2016 | A1 |
20160097903 | Li et al. | Apr 2016 | A1 |
20160104995 | Savage-Leuchs | Apr 2016 | A1 |
20160111851 | Kliner et al. | Apr 2016 | A1 |
20160116679 | Muendel et al. | Apr 2016 | A1 |
20160158889 | Carter et al. | Jun 2016 | A1 |
20160187646 | Ehrmann | Jun 2016 | A1 |
20160218476 | Kliner et al. | Jul 2016 | A1 |
20160285227 | Farrow et al. | Sep 2016 | A1 |
20160320565 | Brown et al. | Nov 2016 | A1 |
20160320685 | Tayebati et al. | Nov 2016 | A1 |
20160369332 | Rothberg et al. | Dec 2016 | A1 |
20170090119 | Logan et al. | Mar 2017 | A1 |
20170110845 | Hou et al. | Apr 2017 | A1 |
20170162999 | Saracco et al. | Jun 2017 | A1 |
20170271837 | Hemenway et al. | Sep 2017 | A1 |
20170293084 | Zhou et al. | Oct 2017 | A1 |
20170336580 | Tayebati et al. | Nov 2017 | A1 |
20170363810 | Holland et al. | Dec 2017 | A1 |
20180059343 | Kliner | Mar 2018 | A1 |
20180203185 | Farrow et al. | Jul 2018 | A1 |
Number | Date | Country |
---|---|---|
102448623 | May 2012 | CN |
102844942 | Dec 2012 | CN |
103490273 | Jan 2014 | CN |
103606803 | Feb 2014 | CN |
4200587 | Apr 1993 | DE |
10321102 | Dec 2004 | DE |
1266259 | May 2011 | EP |
2587564 | May 2013 | EP |
2642246 | Sep 2013 | EP |
WO 1995011100 | Apr 1995 | WO |
WO 1995011101 | Apr 1995 | WO |
WO 2004027477 | Apr 2004 | WO |
WO 2012102655 | Aug 2012 | WO |
WO 2013090236 | Jun 2013 | WO |
WO 2017008022 | Jan 2017 | WO |
WO 2017136831 | Aug 2017 | WO |
Entry |
---|
Adelman et al., “Measurement of Relative State-to-State Rate Constants for the Reaction D+H2(v, j)→HD(v′, j′)+H,” J. Chem. Phys., 97:7323-7341 (Nov. 15, 1992). |
Advisory Action from U.S. Appl. No. 15/607,410, dated Sep. 24, 2018, 6 pages. |
Alcock et al., Element Table, Canadian Metallurgical Quarterly, 23:309-311 (1984). |
Affine Transformation—from Wolfram MathWorld, http://mathworld.wolfram.com/AffineTransformation.html, downloaded Feb. 21, 2014, 2 pages. |
Alfano et al., “Photodissociation and Recombination Dynamics of I2—in Solution,” Ultrafast Phenomena VIII, (Springer-Verlag, New York), pp. 653-655 (Jan. 1993). |
Applicant-Initiated Interview Summary from U.S. Appl. No. 15/607,399, dated May 25, 2018, 3 pages. |
Applicant-Initiated Interview Summary from U.S. Appl. No. 15/607,399, dated Jul. 27, 2018, 9 pages. |
Applicant-Initiated Interview Summary from U.S. Appl. No. 15/607,410, dated May 25, 2018, 3 pages. |
Applicant-Initiated Interview Summary from U.S. Appl. No. 15/607,410, dated Jul. 24, 2018, 9 pages. |
Applicant-Initiated Interview Summary from U.S. Appl. No. 15/607,411, dated Jan. 17, 2018, 2 pages. |
Applicant-Initiated Interview Summary from U.S. Appl. No. 15/607,411, dated Sep. 12, 2018, 17 pages. |
“ARM,” Coherent, available at: http://www.corelase.fi/products/arm/, 6 pages, retrieved May 26, 2017. |
Bernasconi et al., “Kinetics of Ionization of Nitromethane and Phenylnitromethane by Amines and Carboxylate Ions in Me2SO-Water Mixtures. Evidence of Ammonium Ion-Nitronate Ion Hydrogen Bonded Complex Formation in Me2SO-Rich Solvent Mixtures,” J. Org. Chem., 53:3342-3351 (Jul. 1988). |
Blake et al., “The H+D2 Reaction: HD(v=1, J) and HD(v=2, J) Distributions at a Collision Energy of 1.3 eV,” Chem. Phys. Lett., 153:365-370 (Dec. 23, 1988). |
Caprio, “Investigation of emission modes in the SLM of AISI 316L: modelling and process diagnosis,” Ph.D. Thesis, Polytechnic University of Milan, 3 pages (Apr. 28, 2017).—Abstract only. |
Daniel et al., “Novel technique for mode selection in a large-mode-area fiber laser,” Conference on Lasers and Electro-Optics 2010, OSA Technical Digest (CD) (Optical Society of America), paper CWCS, 2 pages (Jan. 2010). |
Daniel et al., “Novel technique for mode selection in a multimode fiber laser,” Optics Express, 19:12434-12439 (Jun. 20, 2011). |
Di Teodoro et al., “Diffraction-Limited, 300-kW Peak-Power Pulses from a Coiled Multimode Fiber Amplifier,” Optics Letters, 27:518-520 (May 2002). |
Di Teodoro et al., “Diffraction-limited, 300-kW-peak-power Pulses from a Yb-doped Fiber Amplifier,” Conference on Lasers and Electro-Optics, OSA Technical Digest (Optical Society of America, Washington, DC), p. 592-593 (May 22-24, 2002). |
Di Teodoro et al., “High-peak-power pulsed fiber sources,” Proc. of SPIE, 5448:561-571 (Sep. 20, 2004). |
“Efficient and Simple Precision, Laser Processing Head PDT-B,” HIGHYAG, 6 pages, (Jan. 2010). |
Eichenholz, “Photonic-crystal fibers have many uses,” Optoelectronics World, 4 pages (Aug. 2004). |
“ENSIS Series,” Amada America, Inc., available at: http://www.amada.com/america/ensis-3015-aj, 2 pages, retrieved May 26, 2017. |
“EX-F Series,” MC Machinery Systems, Inc., available at: https://www.mcmachinery.com/products-and-solutions/ex-f-series/, 2 pages, retrieved May 26, 2017. |
Farrow et al., “Bend-Loss Filtered, Large-Mode-Area Fiber Amplifiers: Experiments and Modeling,” Proceedings of the Solid State and Diode Laser Technology Review (Directed Energy Professional Society), P-9, 5 pages (2006). |
Farrow et al., “Compact Fiber Lasers for Efficient High-Power Generation,” Proc. of SPIE, 6287:62870C-1-62870C-6 (Sep. 1, 2006). |
Farrow et al., “Design of Refractive-Index and Rare-Earth-Dopant Distributions for Large-Mode-Area Fibers Used in Coiled High-Power Amplifiers,” Proc. of SPIE, 6453:64531C-1-64531C-11 (Feb. 22, 2007). |
Farrow et al., “High-Peak-Power (>1.2 MW) Pulsed Fiber Amplifier,” Proc. of the SPIE, 6102:61020L-1-61020L-11 (Mar. 2006). |
Farrow et al., “Numerical Modeling of Self-Focusing Beams in Fiber Amplifiers,” Proc. of the SPIE, 6453:645309-1-645309-9 (2007). |
Farrow et al., “Peak-Power Limits on Fiber Amplifiers Imposed by Self-Focusing,” Optics Lett., 31:3423-3425 (Dec. 1, 2006). |
Fève et al., “Four-wave mixing in nanosecond pulsed fiber amplifiers,” Optics Express, 15:4647-4662 (Apr. 16, 2007). |
Fève et al., “Limiting Effects of Four-Wave Mixing in High-Power Pulsed Fiber Amplifiers,” Proc. of the SPIE, 6453:64531P-1-64531P-11 (Feb. 22, 2007). |
Final Office action from U.S. Appl. No. 15/607,411, dated Feb. 1, 2018, 27 pages. |
Final Office action from U.S. Appl. No. 15/607,399, dated May 3, 2018, 31 pages. |
Final Office action from U.S. Appl. No. 15/607,410, dated May 11, 2018, 29 pages. |
Fini, “Bend-compensated design of large-mode-area fibers,” Optics Letters, 31:1963-1965 (Jul. 1, 2006). |
Fini, “Large mode area fibers with asymmetric bend compensation,” Optics Express, 19:21866-21873 (Oct. 24, 2011). |
Fini et al., “Bend-compensated large-mode-area fibers: achieving robust single-modedness with transformation optics,” Optics Express, 21:19173-19179 (Aug. 12, 2013). |
First Office Action from Chinese Application No. 201410455972.X, dated Jan. 26, 2016, 21 pages (with English translation). |
First Office Action from Chinese Application No. 201480019324.8, dated Apr. 5, 2017, 20 pages (with English translation). |
First Office Action for related Chinese Application No. 201610051671.X, dated Jun. 4, 2018, 25 pages (with English translation). |
First Office Action for related Chinese Application No. 201510468218.4, dated Dec. 4, 2018, 14 pages (with English translation). |
Fox et al., “Effect of low-earth orbit space on radiation-induced absorption in rare-earth-doped optical fibers,” J. Non-Cryst. Solids, 378:79-88 (Oct. 15, 2013). |
Fox et al., “Gamma Radiation Effects in Yb-Doped Optical Fiber,” Proc. of the SPIE, 6453:645328-1-645328-9 (Feb. 23, 2007). |
Fox et al., “Gamma-Radiation-Induced Photodarkening in Unpumped Optical Fibers Doped with Rare-Earth Constituents,” IEEE Trans. on Nuclear Science, 57:1618-1625 (Jun. 2010). |
Fox et al., “Investigation of radiation-induced photodarkening in passive erbium-, ytterbium-, and Yb/Er co-doped optical fibers,” Proc. of the SPIE, 6713:67130R-1-67130R-9 (Sep. 26, 2007). |
Fox et al., “Radiation damage effects in doped fiber materials,” Proc. of the SPIE, 6873:68731F-1-68731F-9 (Feb. 22, 2008). |
Fox et al., “Spectrally Resolved Transmission Loss in Gamma Irradiated Yb-Doped Optical Fibers,” IEEE J. Quant. Electron., 44:581-586 (Jun. 2008). |
Fox et al., “Temperature and Dose-Rate Effects in Gamma Irradiated Rare-Earth Doped Fibers,” Proc. of SPIE, 7095:70950B-1-70950B-8 (Aug. 26, 2008). |
Ghasemi et al., “Beam shaping design for coupling high power diode laser stack to fiber,” Applied Optics, 50:2927-2930 (Jun. 20, 2011). |
Ghatak et al., “Design of Waveguide Refractive Index Profile to Obtain Flat Model Field,” SPIE, 3666:40-44 (Apr. 1999). |
Goers et al., “Development of a Compact Gas Imaging Sensor Employing cw Fiber-Amp-Pumped PPLN OPO,” Conference on Lasers and Electro-Optics, OSA Technical Digest (Optical Society of America, Washington, DC), p. 521 (May 11, 2001). |
Goldberg et al., “Deep UV Generation by Frequency Tripling and Quadrupling of a High-Power Modelocked Semiconductor Laser,” Proceedings of the Quantum Electronics and Laser Science Conference, QPD18-2 (Baltimore) 2 pages (May 1995). |
Goldberg et al., “Deep UV Generation by Frequency Quadrupling of a High-Power GaAlAs Semiconductor Laser,” Optics Lett., 20:1145-1147 (May 15, 1995). |
Goldberg et al., “High Efficiency 3 W Side-Pumped Yb Fiber Amplifier and Laser,” Conference on Lasers and Electro-Optics, OSA Technical Digest (Optical Society of America, Washington, DC), p. 11-12 (May 24, 1999). |
Goldberg et al., “Highly Efficient 4-W Yb-Doped Fiber Amplifier Pumped by a Broad-Stripe Laser Diode,” Optics Lett., 24:673-675 (May 15, 1999). |
Goldberg et al., “High-Power Superfluorescent Source with a Side-Pumped Yb-Doped Double-Cladding Fiber,” Optics Letters, 23:1037-1039 (Jul. 1, 1998). |
Goldberg et al., “Tunable UV Generation at 286 nm by Frequency Tripling of a High-Power Modelocked Semiconductor Laser,” Optics Lett., 20:1640-1642 (Aug. 1, 1995). |
Golub, “Laser Beam Splitting by Diffractive Optics,” Optics and Photonics News, 6 pages (Feb. 2004). |
Han et al., “Reshaping collimated laser beams with Gaussian profile to uniform profiles,” Applied Optics, 22:3644-3647 (Nov. 15, 1983). |
Headrick et al., “Application of laser photofragmentation-resonance enhanced multiphoton ionization to ion mobility spectrometry,” Applied Optics, 49:2204-2214 (Apr. 10, 2010). |
Hemenway et al., “Advances in high-brightness fiber-coupled laser modules for pumping multi-kW CW fiber lasers,” Proceedings of SPIE, 10086:1008605-1-1008605-7 (Feb. 22, 2017). |
Hemenway et al., “High-brightness, fiber-coupled pump modules in fiber laser applications,” Proc. of SPIE, 8961:89611V-1-89611V-12 (Mar. 7, 2014). |
Hoops et al., “Detection of mercuric chloride by photofragment emission using a frequency-converted fiber amplifier,” Applied Optics, 46:4008-4014 (Jul. 1, 2007). |
Hotoleanu et al., “High Order Modes Suppression in Large Mode Area Active Fibers by Controlling the Radial Distribution of the Rare Earth Dopant,” Proc. of the SPIE, 6102:61021T-1-61021T-8 (Feb. 23, 2006). |
“How to Select a Beamsplitter,” IDEX—Optics & Photonics Marketplace, available at: https://www.cvilaseroptics.com/file/general/beamSplitters.pdf, 5 pages (Jan. 8, 2014). |
Huang et al., “Double-cutting beam shaping technique for high-power diode laser area light source,” Optical Engineering, 52:106108-1-106108-6 (Oct. 2013). |
Injeyan et al., “Introduction to Optical Fiber Lasers,” High-Power Laser Handbook, pp. 436-439 (2011). |
International Search Report and Written Opinion for International Application No. PCT/US2013/060470, 7 pages, dated Jan. 16, 2014. |
International Search Report and Written Opinion for International Application No. PCT/US2014/017841, 5 pages, dated Jun. 5, 2014. |
International Search Report and Written Opinion for International Application No. PCT/US2014/017836, 6 pages, dated Jun. 10, 2014. |
International Search Report and Written Opinion for related International Application No. PCT/US2016/041526, 6 pages, dated Oct. 20, 2016. |
International Search Report and Written Opinion for related International Application No. PCT/US2016/053807, 6 pages, dated Jan. 19, 2017. |
International Search Report and Written Opinion for International Application No. PCT/US2016/063086, 6 pages, dated Mar. 23, 2017. |
International Search Report and Written Opinion for International Application No. PCT/US2017/014182, 9 pages, dated Mar. 31, 2017. |
International Search Report and Written Opinion from International Application No. PCT/US2017/034848, dated Nov. 28, 2017, 15 pages. |
International Search Report and Written Opinion from International Application No. PCT/US2018/024908, dated Jul. 19, 2018, 8 pages. |
International Search Report and Written Opinion for International Application No. PCT/US2018/026110, 12 pages, dated Aug. 8, 2018. |
International Search Report and Written Opinion from International Application No. PCT/US2018/024904, dated Aug. 30, 2018, 5 pages. |
Ishiguro et al., “High Efficiency 4-kW Fiber Laser Cutting Machine,” Rev. Laser Eng., 39:680-684 (May 21, 2011). |
Java—Transform a triangle to another triangle—Stack Overflow, http://stackoverflow.com/questions/1114257/transform-a-triangle-to-another-triangle?lq=1, downloaded Feb. 21, 2014, 3 pages. |
Johnson et al., “Experimental and Theoretical Study of Inhomogeneous Electron Transfer in Betaine: Comparisons of Measured and Predicted Spectral Dynamics,” Chem. Phys., 176:555-574 (Oct. 15, 1993). |
Johnson et al., “Ultrafast Experiments on the Role of Vibrational Modes in Electron Transfer,” Pure and Applied Chem., 64:1219-1224 (May 1992). |
Kliner, “Novel, High-Brightness, Fibre Laser Platform for kW Materials Processing Applications,” 2015 European Conference on Lasers and Electro-Optics—European Quantum Electronics Conference (Optical Society of America, 2015), paper CJ_11_2, 1 page. (Jun. 21-25, 2015). |
Kliner et al., “4-kW fiber laser for metal cutting and welding,” Proc. of SPIE, 7914:791418-791418-8 (Feb. 22, 2011). |
Kliner et al., “Comparison of Experimental and Theoretical Absolute Rates for Intervalence Electron Transfer,” J. Am. Chem. Soc., 114:8323-8325 (Oct. 7, 1992). |
Kliner et al., “Comparison of Experimental and Theoretical Integral Cross Sections for D+H2(v=1, j=1)→HD(v′=1, j′)+H,” J. Chem. Phys., 95:1648-1662 (Aug. 1, 1991). |
Kliner et al., “D+H2(v=1, J=1): Rovibronic State to Rovibronic State Reaction Dynamics,” J. Chem. Phys., 92:2107-2109 (Feb. 1, 1990). |
Kliner et al., “Effect of Indistinguishable Nuclei on Product Rotational Distributions: H+HI→H2+I reactionsa),” J. Chem. Phys., 90:4625-4327 (Apr. 15, 1989). |
Kliner et al., “Efficient second, third, fourth, and fifth harmonic generation of a Yb-doped fiber amplifier,” Optics Communications, 210:393-398 (Sep. 15, 2002). |
Kliner et al., “Efficient UV and Visible Generation Using a Pulsed Yb-Doped Fiber Amplifier,” Conference on Lasers and Electro-Optics, OSA Technical Digest (Optical Society of America, Washington, DC), p. CPDC10-1-CPDC10-3 (May 19-22, 2002). |
Kliner et al., “Efficient visible and UV generation by frequency conversion of a mode-filtered fiber amplifier,” Proc. of SPIE, 4974:230-235 (Jul. 3, 2003). |
Kliner et al., “Fiber laser allows processing of highly reflective materials,” Industrial Laser Solutions, 31:1-9 (Mar. 16, 2016). |
Kliner et al., “High-Power Fiber Lasers,” Photonics & Imaging Technology, pp. 2-5 (Mar. 2017). |
Kliner et al., “Laboratory Investigation of the Catalytic Reduction Technique for Detection of Atmospheric NOy,” J. Geophys. Res., 102:10759-10776 (May 20, 1997). |
Kliner et al., “Laser Reflections: How fiber laser users are successfully processing highly reflective metals,” Shop Floor Lasers, available at: http://www.shopfloorlasers.com/laser-cutting/fiber/354-laser-reflections, 9 pages (Jan./Feb. 2017). |
Kliner et al., “Measurements of Ground-State OH Rotational Energy-Transfer Rates,” J. Chem. Phys., 110:412-422 (Jan. 1, 1999). |
Kliner et al., “Mode-Filtered Fiber Amplifier,” Sandia National Laboratories—Brochure, 44 pages (Sep. 13, 2007). |
Kliner et al., “Narrow-Band, Tunable, Semiconductor-Laser-Based Source for Deep-UV Absorption Spectroscopy,” Optics Lett., 22:1418-1420 (Sep. 15, 1997). |
Kliner et al., “Overview of Sandia's fiber laser program,” Proceedings of SPIE—The International Society for Optical Engineering, 6952:695202-1-695202-12 (Apr. 14, 2008). |
Kliner et al., “Photodissociation and Vibrational Relaxation of I2- in Ethanol,” J. Chem. Phys., 98:5375-5389 (Apr. 1, 1993). |
Kliner et al., “Photodissociation Dynamics of I2- in Solution,” Ultrafast Reaction Dynamics and Solvent Effects, (American Institute of Physics, New York), pp. 16-35 (Feb. 1994). |
Kliner et al., “Polarization-Maintaining Amplifier Employing Double-Clad, Bow-Tie Fiber,” Optics Lett., 26:184-186 (Feb. 15, 2001). |
Kliner et al., “Power Scaling of Diffraction-Limited Fiber Sources,” Proc. of SPIE, 5647:550-556 (Feb. 21, 2005). |
Kliner et al., “Power Scaling of Rare-Earth-Doped Fiber Sources,” Proc. of SPIE, 5653:257-261 (Jan. 12, 2005). |
Kliner et al., “Product Internal-State Distribution for the Reaction H+HI→H2+I,” J. Chem. Phys., 95:1663-1670 (Aug. 1, 1991). |
Kliner et al., “The D+H2 Reaction: Comparison of Experiment with Quantum-Mechanical and Quasiclassical Calculations,” Chem. Phys. Lett., 166:107-111 (Feb. 16, 1990). |
Kliner et al., “The H+para-H2 reaction: Influence of dynamical resonances on H2(v′=1, j′=1 and 3) Integral Cross Sections,” J. Chem. Phys., 94:1069-1080 (Jan. 15, 1991). |
Koplow et al., A New Method for Side Pumping of Double-Clad Fiber Sources, J. Quantum Electronics, 39:529-540 (Apr. 4, 2003). |
Koplow et al., “Compact 1-W Yb-Doped Double-Cladding Fiber Amplifier Using V-Groove Side-Pumping,” IEEE Photonics Technol. Lett., 10:793-795 (Jun. 1998). |
Koplow et al., “Development of a Narrowband, Tunable, Frequency-Quadrupled Diode Laser for UV Absorption Spectroscopy,” Appl. Optics, 37:3954-3960 (Jun. 20, 1998). |
Koplow et al., “Diode-Bar Side-Pumping of Double-Clad Fibers,” Proc. of SPIE, 5709:284-300 (Apr. 22, 2005). |
Koplow et al., “High Power PM Fiber Amplifier and Broadband Source,” Optical Fiber Communication Conference, OSA Technical Digest (Optical Society of America, Washington, DC), p. 12-13 (Mar. 7-10, 2000). |
Koplow et al., “Polarization-Maintaining, Double-Clad Fiber Amplifier Employing Externally Applied Stress-Induced Birefringence,” Optics Lett., 25:387-389 (Mar. 15, 2000). |
Koplow et al., “Single-mode operation of a coiled multimode fiber amplifier,” Optics Letters, 25:442-444 (Apr. 1, 2000). |
Koplow et al., Use of Bend Loss to Obtain Single-Transverse-Mode Operation of a Multimode Fiber Amplifier, Conference on Lasers and Electro-Optics, OSA Technical Digest (Optical Society of America, Washington, DC), p. 286-287 (May 7-12, 2000). |
Koplow et al., “UV Generation by Frequency Quadrupling of a Yb-Doped Fiber Amplifier,” IEEE Photonics Technol. Lett., 10:75-77 (Jan. 1998). |
Koponen et al., “Photodarkening Measurements in Large-Mode-Area Fibers,” Proc. of SPIE, 6453:64531E-1-64531E-12 (Feb. 2007). |
Kotlyar et al., “Asymmetric Bessel-Gauss beams,” J. Opt. Soc. Am. A, 31:1977-1983 (Sep. 2014). |
Kulp et al., “The application of quasi-phase-matched parametric light sources to practical infrared chemical sensing systems,” Appl. Phys. B, 75:317-327 (Jun. 6, 2002). |
“Laser cutting machines,” TRUMPF, available at: http://www.us.trumpf.com/en/products/machine-tools/products/2d-laser-cutting/innovative-technology/brightline.html, 9 pages, retrieved May 26, 2017. |
“Lasers & Fibers,” NKT Photonics, available at: https://www.nktphotonics.com/lasers-fibers/technology/photonic-crystal-fibers/, 4 pages, retrieved Feb. 13, 2018. |
Longhi et al., “Self-focusing and nonlinear periodic beams in parabolic index optical fibres,” J. Opt. B: Quantum Semiclass. Opt., 6:S303-S308 (May 2004). |
Maechling et al., “Sum Frequency Spectra in the C—H Stretch Region of Adsorbates on Iron,” Appl. Spectrosc., 47:167-172 (Feb. 1, 1993). |
McComb et al., “Pulsed Yb:fiber system capable of >250 kW peak power with tunable pulses in the 50 ps to 1.5 ns. range,” Proc. of SPIE, 8601:86012T-1-86012T-11 (Mar. 22, 2013). |
Moore et al., “Diode-bar side pumping of double-clad fibers,” Proc. of SPIE, 6453:64530K-1-64530K-9 (Feb. 20, 2007). |
Neuhauser et al., “State-to-State Rates for the D+H2(v=1, j=1)→HD(v′, j′)+H Reaction: Predictions and Measurements,” Science, 257:519-522 (Jul. 24, 1992). |
Notice of Preliminary Rejection from the Korean Intellectual Property Office for related Application No. 10-2015-7025813, dated Jun. 26, 2018, 18 pages. |
Office Action for related Chinese Application No. 201480022179.9, 5 pages, dated Mar. 30, 2017 (no English translation). |
Office Action for related Korea Application No. 10-2014-0120247, dated Apr. 14, 2017, 11 pages (with English translation). |
Office action from U.S. Appl. No. 15/074,838, dated May 19, 2017, 12 pages. |
Office Action for related Chinese Application No. 201380075745.8, 21 pages, dated Jun. 2, 2017 (with English translation). |
Office action from U.S. Appl. No. 15/607,399, dated Sep. 20, 2017, 25 pages. |
Office action from U.S. Appl. No. 15/607,411, dated Sep. 26, 2017, 15 pages. |
Office action from U.S. Appl. No. 15/607,410, dated Oct. 3, 2017, 32 pages. |
Office Action for related Korea Application No. 10-2014-0120247, dated Oct. 18, 2017, 6 pages (with English translation). |
Office action from U.S. Appl. No. 15/607,411, dated Jun. 12, 2018, 19 pages. |
Office action from U.S. Appl. No. 15/607,399, dated Sep. 14, 2018, 19 pages. |
Office action from U.S. Appl. No. 15/938,959, dated Jul. 18, 2018, 6 pages. |
Office action from U.S. Appl. No. 15/939,064, dated Jul. 27, 2018, 7 pages. |
Office action from U.S. Appl. No. 15/939,064, dated Oct. 5, 2018, 22 pages. |
Office action from U.S. Appl. No. 15/938,959, dated Oct. 5, 2018, 22 pages. |
Official Action for related Taiwan application No. 103130968 dated Jun. 7, 2017, 5 pages (with English translation). |
Official Letter and Search Report from the Taiwan Intellectual Property Office for related Application No. 103106020, 21 pages, dated Apr. 20, 2016 (with English translation). |
Official Letter and Search Report from the Taiwan Intellectual Property Office for related Application No. 102139285, 21 pages, dated Jun. 13, 2016 (with English translation.). |
Official Letter and Search Report from the Taiwan Intellectual Property Office for related Application No. 102139285, 8 pages, dated Nov. 21, 2016 (with English translation). |
Official Letter and Search Report from Taiwan Application No. 103130968, dated Dec. 20, 2016, 16 pages (with English translation). |
Official Letter and Search Report from Taiwan Application No. 103106020, dated Jun. 6, 2017, 7 pages (with English translation). |
PCI-6110, Multifunction I/O Device, http.//www.ni.com/en-us-support/model.pci-6110.html, downloaded Dec. 15, 2017, 1 page. |
Price et al., “High-brightness fiber-coupled pump laser development,” Proc. of SPIE, 7583:758308-1-758308-7 (Feb. 2010). |
Rinnen et al., “Construction of a Shuttered Time-of-Flight Mass Spectrometer for Selective Ion Detection,” Rev. Sci. Instrum., 60:717-719 (Apr. 1989). |
Rinnen et al., “Effect of Indistinguishable Nuclei on Product Rotational Distributions: D+DI→D2+I,” Chem. Phys. Lett., 169:365-371 (Jun. 15, 1990). |
Rinnen et al. “Quantitative Determination of HD Internal State Distributions via (2+1) REMPI,” Isr. J. Chem., 29:369-382 (Mar. 7, 1989). |
Rinnen et al., “Quantitative determination of H2, HD, and D2 internal state distributions via (2+1) resonance-enhanced multiphoton ionization,” J. Chem. Phys., 95:214-225 (Jul. 1, 1991). |
Rinnen et al., “The H+D2 Reaction: “Prompt” HD Distributions at High Collision Energies,” Chem. Phys. Lett., 153:371-375 (Dec. 23, 1988). |
Rinnen et al., “The H+D2 Reaction: Quantum State Distributions at Collision Energies of 1.3 and 0.55 eV,” J. Chem. Phys., 91:7514-7529 (Dec. 15, 1989). |
Romero et al., “Lossless laser beam shaping,” J. Opt. Soc. Am. A, 13:751-760 (Apr. 1996). |
Russell, “Photonic-Crystal Fibers,” IEEE JLT, 24:4729-4749 (Dec. 2006). |
Saleh et al., “Chapter 9.4 Holey and Photonic-Crystal Fibers,” Fundamentals of Photonics, Second Edition, pp. 359-362 (2007). |
Sanchez-Rubio et al., “Wavelength Beam Combining for Power and Brightness Scaling of Laser Systems,” Lincoln Laboratory Journal, 20:52-66 (2014). |
Saracco et al., “Compact, 17 W average power, 100 kW peak power, nanosecond fiber laser system,” Proc. of SPIE, 8601:86012U-1-86012U-13 (Mar. 22, 2013). |
Schrader et al., “Fiber-Based Laser with Tunable Repetition Rate, Fixed Pulse Duration, and Multiple Wavelength Output,” Proc. of the SPIE, 6453:64530D-1-64530D-9 (Feb. 20, 2007). |
Schrader et al., “High-Power Fiber Amplifier with Widely Tunable Repetition Rate, Fixed Pulse Duration, and Multiple Output Wavelengths,” Optics Express, 14:11528-11538 (Nov. 27, 2006). |
Schrader et al., “Power scaling of fiber-based amplifiers seeded with microchip lasers,” Proc. of the SPIE, 6871:68710T-1-68710T-11 (Feb. 2008). |
Search Report from the Taiwan Intellectual Property Office for related Application No. 102139285, 21 pages, dated Sep. 1, 2015 (with English translation). |
Search Report from the Taiwan Intellectual Property Office for related Application No. 102139285, 9 pages, dated Sep. 4, 2017 (with English translation). |
Second Office Action from Chinese Application No. 201410455972.X, dated Nov. 22, 2016, 22 pages (with English translation). |
Second Office Action from Chinese Application No. 201480019324.8, dated Nov. 16, 2017, 21 pages (with English translation). |
Second Office Action from Chinese Application No. 201380075745.8, dated Feb. 26, 2018, 6 pages (with English translation). |
Sheehan et al., “Faserlaser zur Bearbeitung hochreflektierender Materialien (Fiber laser processing of highly reflective materials),” Laser, 3:92-94 (Jun. 2017). |
Sheehan et al. “High-brightness fiber laser advances remote laser processing,” Industrial Laser Solutions, 31:1-9 (Nov. 2, 2016). |
Sun et al., “Optical Surface Transformation: Changing the optical surface by homogeneous optic-null medium at will,” Scientific Reports, 5:16032-1-16032-20 (Oct. 30, 2015). |
Third Office Action from Chinese Application No. 201480019324.8, dated Apr. 13, 2018, 8 pages (with English translation). |
Tominaga et al., “Femtosecond Experiments and Absolute Rate Calculations on Intervalence Electron Transfer in Mixed-Valence Compounds,” J. Chem. Phys., 98:1228-1243 (Jan. 15, 1993). |
Tominaga et al., “Ultrafast Studies of Intervalence Charge Transfer,” Ultrafast Phenomena VIII, (Springer-Verlag, New York), pp. 582-584 (1993). |
“Triple Clad Ytterbium-Doped Polarization Maintaining Fibers,” nuFERN Driven to Light Specifications, 1 page (Jan. 2006). |
Varshney et al., “Design of a flat field fiber with very small dispersion slope,” Optical Fiber Technology, 9(3):189-198 (Oct. 2003). |
Wetter et al., “High power cladding light strippers,” Proc. of SPIE, 6873:687327-1-687327-8 (Jan. 21, 2008). |
Xiao et al., “Effects of laser modes on Nb segregation and Laves phase formation during laser additive manufacturing of nickel-based superalloy,” Materials Letters, 188:260-262 (Nov. 1, 2016). |
Xiao et al., “Fiber coupler for mode selection and high-efficiency pump coupling,” Optics Letters, 38:1170-1172 (Apr. 1, 2013). |
Yaney et al., “Distributed-Feedback Dye Laser for Picosecond UV and Visible Spectroscopy,” Rev. Sci. Instrum, 71:1296-1305 (Mar. 2000). |
Yu et al., “1.2-kW single-mode fiber laser based on 100-W high-brightness pump diodes,” Proc. of SPIE, 8237:82370G-1-82370G-7 (Feb. 16, 2012). |
Number | Date | Country | |
---|---|---|---|
20200064573 A1 | Feb 2020 | US |
Number | Date | Country | |
---|---|---|---|
62032043 | Aug 2014 | US |
Number | Date | Country | |
---|---|---|---|
Parent | 14816211 | Aug 2015 | US |
Child | 16417337 | US |