Abstract:
The invention describes techniques for the control of the spatial as well as spectral beam quality of multi-mode fiber amplification of high peak power pulses as well as using such a configuration to replace the present diode-pumped, Neodynium based sources. Perfect spatial beam-quality can be ensured by exciting the fundamental mode in the multi-mode fibers with appropriate mode-matching optics and techniques. The loss of spatial beam-quality in the multi-mode fibers along the fiber length can be minimized by using multi-mode fibers with large cladding diameters. Near diffraction-limited coherent multi-mode amplifiers can be conveniently cladding pumped, allowing for the generation of high average power. Moreover, the polarization state in the multi-mode fiber amplifiers can be preserved by implementing multi-mode fibers with stress producing regions or elliptical fiber cores These lasers find application as a general replacement of Nd: based lasers, especially Nd:YAG lasers. Particularly utility is disclosed for applications in the marking, micro-machining and drilling areas.
Abstract:
By compensating polarization mode-dispersion as well chromatic dispersion in photonic crystal fiber pulse compressors, high pulse energies can be obtained from all-fiber chirped pulse amplification systems. By inducing third-order dispersion in fiber amplifiers via self-phase modulation, the third-order chromatic dispersion from bulk grating pulse compressors can be compensated and the pulse quality of hybrid fiber/bulk chirped pulse amplification systems can be improved. Finally, by amplifying positively chirped pulses in negative dispersion fiber amplifiers, low noise wavelength tunable seed source via anti-Stokes frequency shifting can be obtained.
Abstract:
One or more single mode few-moded or multimode fibers are incorporated into a bundle to carry input to a fiber amplifier or output from a fiber amplifier or a fiber laser. The input is at the signal wavelength, which is the wavelength where amplification or lasing occurs. Each of the fibers in the bundle is cleaved individually or as a group and fiber ends are aligned in the same plane. The fiber amplifier or fiber laser may include a double clad fiber and the other fibers of the bundle couple light for cladding pumping. The device may also include a mode filter for controlling the output mode.
Abstract:
A method for material processing using a pulsed laser includes generating a beam of laser pulses, focusing the beam in a plane above the surface of a workpiece, causing breakdown of matter at a lasing point, and removing or modifying material of the workpiece. Positioning the focal plane of the laser above the workpiece permits the use of higher intensity laser beam pulses and minimizes ill effects of workpiece surface conditions on laser energy absorption. In a second aspect, a method for material processing further includes using vacuum to remove the material removed by the beam, preferably by a push-pull type air vacuum system located slightly above the workpiece surface, thereby providing cleaner workpiece and feature surfaces.
Abstract:
A multiple-wavelength ultrashort-pulse laser system includes a laser generator producing ultrashort pulses at a fixed wavelength, and at least one and preferably a plurality of wavelength-conversion channels. Preferably, a fiber laser system is used for generating single-wavelength, ultrashort pulses. An optical split switch matrix directs the pulses from the laser generator into at least one of the wavelength conversion channels. An optical combining switch matrix is disposed downstream of the wavelength-conversion channels and combines outputs from separate wavelength-conversion channels into a single output channel. Preferably, waveguides formed in a ferroelectric substrate by titanium indiffusion (TI) and/or proton exchange (PE) form the wavelength-conversion channels and the splitting and combining matrices. Use of the waveguide allows efficient optical parametric generation to occur in the wavelength-conversion channels at pulse energies achievable with a mode-locked laser source. The multiple-wavelength laser system can replace a plurality of different, single-wavelength laser systems. One particular application for the system is a multi-photon microscope, where the ability to select the ultrashort-signal wavelength of the laser source accommodates any single fluorescent dye or several fluorescent dyes simultaneously. In its simplest form, the system can be used to convert the laser wavelength to a more favorable wavelength. For example, pulses generated at 1.55 .mu.m by a mode-locked erbium fiber laser can be converted to 1.3 .mu.m for use in optical coherence tomography or to 1.04-1.12 .mu.m for amplification by a Yterbium amplifier, allowing amplification of pulses which can be used in a display, printing or machining system.
Abstract:
A two-photon fluorescence microscope employs two laser beams having pulses of respective wavelengths .lambda..sub.2 and .lambda..sub.3, which cause two-photon emission of a fluorophore when the pulses are spatially and temporally overlapping. The pulses of the two beams of wavelengths .lambda..sub.2 and .lambda..sub.3 are combined at some crossing angle .theta. within the specimen, causing two-photon absorption within a line-shaped region during each instant of overlap. As the pulses pass through each other, the overlapping line-shaped region moves such that a slice of the fluorophore-containing specimen is excited by two-photon absorption during the overlap period. Lateral scanning is effected without moving parts by adjusting the relative delay of the pulses in the two beams. When the crossing angle .theta. is set to 0, i.e., when the two beams are directed along the same axis, the pulses of the two beams form a pancake-shaped volume in which two-photon excitation occurs as the pulses spatially and temporally overlap while traveling in opposite directions. A two-dimensional detector, such as a two-dimensional charge coupled device (CCD) array, can be used to detect a two-dimensional portion of the specimen at one time without lateral scanning. A three-dimensional image can be produced by adjusting the time delay between the two pulses, thereby changing the location of the "pancake" volume created by the intersection of the two pulses.
Abstract:
The present invention is directed to providing an environmentally stable, ultra-short pulse source. Exemplary embodiments relate to passively modelocked ultra-short fiber lasers which are insensitive to temperature variations and which possess only negligible sensitivity to pressure variations. Further, exemplary embodiments can be implemented in a cost-effective manner which render them commercially practical in unlimited applications. Arbitrary fiber lengths (e.g., on the order of 1 millimeter to 1 kilometer, or greater) can be used to provide an ultra-short pulse with a cost-effective architecture which is commercially practical.
Abstract:
A method of forming a porous composite separator layer for an electrochemical cell comprising the steps of printing a thin layer of a separator precursor solution on the surface of one of the electrochemical cell electrodes, curing the thin layer of separator precursor solution so that it transforms into a microporous composite separator structure. In the preferred embodiment, the separator precursor solution is formulated as an ink comprising a silica aerogel filler material dispersed in a solution of polymer binder which is dissolved in a suitable solvent. The process allows the manufacture of thin and flexible composite separators which are conformally bonded to the underlying electrodes.
Abstract:
The present invention is directed to methods and apparatuses for performing temporal scanning using ultra-short pulsewidth lasers in which only minimal (micro-scale) mechanical movement is required. The invention also relates to methods for obtaining high-accuracy timing calibration, on the order of femtoseconds. A dual laser system is disclosed in which the cavity of one or more of the lasers is dithered, by using a piezoelectric element. A Fabry-Perot etalon is used to generate a sequence of timing pulses used in conjunction with a laser beam produced by the laser having the dithered laser cavity. A correlator correlates a laser pulse from one of the lasers with the sequence of timing pulses to produce a calibrated time scale. The methods and apparatuses of the present invention are applicable to many applications requiring rapid scanning and time calibration, including, but not limited to metrology, characterization of charge dynamics in semiconductors, electro-optic testing of ultrafast electronic and optoelectronic devices, optical time domain reflectometry, and electro-optic sampling oscilloscopes.
Abstract:
The present invention relates to an apparatus and a method for detecting pulses of light energy from at least two fields of view. A first detector having a first bias detects a pulse received at a first point in time. A second detector having a second bias, different from the first bias, detects a pulse received at a second point in time. A processor compares an output of the first detector with a first threshold to produce a signal representing receipt of a pulse from a first field of view. The processor also compares an output of the second detector with a second threshold, different from the first threshold, to produce a signal representing receipt of a pulse from a second field of view. Because the detectors are biased with different biases, the detected pulses are easily distinguished. Thus, multiple fields of view can be detected without complex hardware. The detectors can be biased with opposite polarities so that background noise is cancelled out. In a system and method for detecting pulses of light energy from at least two fields of view, a transmitter transmits pulses of light energy into a first field of view and into a second field of view. A single transmitter can be used to emit signals towards multiple fields of view. Thus, the transmitter only has to emit signals once for multiple samples, increasing the number of samples that can be taken per sample period.