| Class / Patent application number | Description | Number of patent applications / Date published |
|---|
| 359345000 | Particular pumping type (e.g., electrical, optical, nuclear, magnetic, etc.) | 19 |
| 20090161202 | APPARATUS FOR OPTICAL PARAMETRIC CHIRPED PULSE AMPLIFICATION (OPCPA) USING INVERSE CHIRPING AND IDLER - An OPCPA apparatus of the present invention includes an optical pulse stretcher ( | 06-25-2009 |
| 20090174932 | OPTICAL AMPLIFIER BANDWIDTH ALTERATION - The alteration of the bandwidth of an optical amplifier. Before alteration, optical signals having a first set of wavelengths are provided through a gain medium of the optical amplifier. In addition, a first pump having a set of pump wavelengths is propagated through the gain medium to thereby amplify the optical signals. After alteration, optical signals having at least a partially different set of wavelengths are able to be optically amplified by coupling a second pump into the optical medium. The second pump is at least partially distinct from the first pump in that the second pump includes at least one pump wavelength that was not included in the first pump. | 07-09-2009 |
| 20090174933 | EFFICIENT DISCRETE AMPLIFICATION - An optical amplification mechanism that introduces optical pump(s) into one port of an optical circulator. The optical circulator directs the optical pumps from that port into another port that is coupled to the output of a gain stage. The optical pump(s) then pass from the output to the input of the gain stage while amplifying an optical signal passing from the input to the output of the gain stage. A residual amount of optical pump(s) that exits the input of the gain stage is reflected back into the input of the gain stage. The reflected optical pump(s) then further assists in the amplification of the optical signal. Other embodiments are also disclosed. | 07-09-2009 |
| 20090303579 | Amplification of Energy Beams by Passage Through an Imploding Liner - Apparatus and methods are disclosed for amplifying an energy beam such as a beam of laser light or a charged particle beam. An exemplary method includes providing a liner having a first end, a second end, a liner axis, and a lumen extending along the liner axis and being bound by interior reflective walls of the liner. An energy beam is introduced into the first end of the liner. The beam propagates through the lumen from the first end to the second end as the beam reflects multiple times from the interior walls of the liner. Meanwhile, an implosive force is applied to the liner. The implosive force compresses the interior walls implosively toward the liner axis in a manner that amplifies the beam as the beam propagates through the lumen of the imploding liner. The amplified energy beam can be used for any of various purposes including ignition of a fusion target. | 12-10-2009 |
| 20100195196 | LASER BEAM AMPLIFIER AND LASER APPARATUS USING THE SAME - A laser beam amplifier with high optical axis stability is provided. The laser beam amplifier includes: a container for accommodating a laser medium; a pair of electrodes for performing discharge in the laser medium to form an amplification region for a laser beam in the laser medium; and an optical system for forming an optical path between a first point, upon which the laser beam is incident, and a second point, from which the laser beam is outputted, such that the amplification region is located in the optical path between the first point and the second point, wherein the first point and the second point are conjugate to each other, and the laser beam incident upon the first point is amplified while passing through the amplification region at least twice and then transferred to the second point. | 08-05-2010 |
| 20100290108 | LIGHT AMPLIFIER - A light amplifier includes first and second multi-pass amplifiers, an excitation light source, and a beam splitter. The second multi-pass amplifier includes a light attenuation portion provided in an optical path for a light pulse to travel to pass through a light amplification medium a plurality of times, for attenuating energy of the input light pulse. In addition, an excitation light pulse from the excitation light source is split by the beam splitter into two light pulses. These two pulses are input to the first and second multi-pass amplifiers, respectively. Thus, fluctuation in energy of the light pulse output from the light amplifier can be less than fluctuation in energy of the excitation light pulse. | 11-18-2010 |
| 20110038037 | HOMOGENISER INCLUDING A PHASE PLATE - A system for homogenizing a laser pulse emitted by a laser source in order to illuminate a target homogeneously, the system having, between the laser source and the target: a phase plate constituted by a plurality of subpupils capable of generating a plurality of delayed laser beams towards the target, the path difference Δd between two adjacent delayed laser beams being greater than or equal to the length of the temporal coherence T | 02-17-2011 |
| 20120026579 | Resonant Optical Amplifier - Methods and systems for resonant optical amplification are disclosed, including generating electromagnetic radiation from a seed laser; coupling the seed laser electromagnetic radiation into an etalon, wherein the etalon comprises a gain medium comprising a gain, a length, and a roundtrip gain, wherein the gain medium is positioned between a first reflective surface comprising a first power reflectivity and a second reflective surface comprising a second power reflectivity; optically or electrically pumping the gain medium using a flash lamp, an arc lamp, a laser, an electric glow discharge, or an electric current to generate an amplified seed laser electromagnetic radiation; and coupling out the amplified seed laser electromagnetic radiation from the etalon. Other embodiments are described and claimed. | 02-02-2012 |
| 20120105948 | METHOD AND SYSTEM FOR COMPACT EFFICIENT LASER ARCHITECTURE - A laser amplifier module having an enclosure includes an input window, a mirror optically coupled to the input window and disposed in a first plane, and a first amplifier head disposed along an optical amplification path adjacent a first end of the enclosure. The laser amplifier module also includes a second amplifier head disposed along the optical amplification path adjacent a second end of the enclosure and a cavity mirror disposed along the optical amplification path. | 05-03-2012 |
| 20130215496 | ORGANIC/INORGANIC HYBRID OPTICAL AMPLIFIER WITH WAVELENGTH CONVERSION - A device and related fabrication method is provided for an organic/inorganic hybrid optical amplifier with a function of converting infrared light to visible light. The hybrid device integrates an inorganic heterojunction phototransistor (HPT), an embedded metal electrode mirror with a dual function as an optical mirror and charge injection electrode, and an organic light emitting diode (OLED). This integrated optical amplifier is capable of amplifying the incoming light and producing light emission with a power greater than that of the incoming signal. In the second aspect of the invention, the optical amplifier is capable of detecting an incoming infrared electromagnetic wave and converting the wave back to a visible light wave. The optical device has dual functions of optical power amplification and photon energy up-conversion. The optical amplifier device consists of an InGaAs/InP based HPT structure as photodetector, gold-coated metals as embedded mirror and a top-emission OLED. New optical up-conversion imaging devices are also provided that include focal-point array of the organic/inorganic hybrid optical amplifier devices in pixelated formats. The up-conversion imaging devices have a fast response time to enable gated operation for practical applications such as night vision, active surveillance, semiconductor wafer inspection and eye-safe infrared imaging. More importantly, the up-conversion imaging devices would be particularly useful for detecting ultra-low intensity infrared scenes. | 08-22-2013 |
| 20130308179 | NONLINEAR AND GAIN OPTICAL DEVICES FORMED IN METAL GRATINGS - In one aspect, an optical gain device is provided. The optical gain device comprises a metallic film and an optical gain medium. The metallic film has a plurality of slits therethrough. The plurality of slits are configured such that the film selectively and resonantly transmits light over a preselected frequency range. The optical gain medium is situated within or substantially near at least one slit of the plurality of slits. | 11-21-2013 |
| 20140218791 | SYSTEM AND METHOD FOR EMITTING OPTICAL PULSES IN VIEW OF A VARIABLE EXTERNAL TRIGGER SIGNAL - Method and system for emitting optical pulses in view of a desired output energy of the optical pulses and a variable external trigger signal, using a laser system having a seed laser oscillator optically coupled to one or more cascaded optical amplification stages. For each amplification stage, a plurality of sets of pump pulse parameters are provided, each associated with specific values of the output energy and the trigger period. Proper pumping parameters associated with the received desired value of the output energy and the trigger period of the received trigger signal are selected for each amplification stage, which is pumped accordingly before a seed optical pulse is launched through the system. | 08-07-2014 |
| 20140268313 | HIGH POWER PULSED LIGHT GENERATION DEVICE - A high power pulsed light generation device includes: a master clock generator that generates a master signal; an optical oscillator that generates a pulsed light synchronized with the master clock signal; an optical amplifier that amplifies the pulsed light emitted from the optical oscillator to output a high power pulsed light; a pump semiconductor laser that generates a pulsed light for pumping the optical amplifier; a driving unit that drives the pump semiconductor laser by a pulsed driving current synchronized with the master clock signal; and a control unit which controls the driving unit and controls a gain of the optical amplifier for each pulse by changing a pulse width of the pulsed drive current from driving unit so as to change the pulse width of the pumping pulsed light. | 09-18-2014 |
| 20140293405 | METHOD AND DEVICE FOR OPTICAL PARAMETRIC CHIRPED PULSE AMPLIFICATION - An optical parametric amplification device and method. The method includes providing a pump pulse having a pump pulse duration, providing a chirped seed pulse having a seed pulse duration, sequentially passing the pump and seed pulses through amplification stages, wherein the pump and seed pulses are coupled into the amplification stages with varying mutual temporal overlap and the seed pulse is amplified at each amplification stage, an amplified signal pulse is provided by the seed pulse after amplification in a last ampli-fication stage, the seed pulse duration is longer than the pump pulse duration, the mutual temporal overlap of the pump and seed pulses is varied with different temporal ranges of the seed pulse amplified at each amplification stage. Compared with the seed pulse, the signal pulse has an increased energy in the spectral regions determined by the temporal overlap of the seed pulse with the pump. | 10-02-2014 |
| 20150295380 | OPTICALLY END-PUMPED SLAB AMPLIFIER COMPRISING PUMP MODULES ARRANGED IN A DISTRIBUTED MANNER - An optically end-pumped amplifier with a plate-shaped optical gain medium has a plurality of pump laser units for optically pumping the gain medium through at least one of the narrow side surfaces thereof. The pump laser units are designed such that the pump laser radiation, upon passing through the gain medium, has an elongated beam cross section having a short axis and a long axis running parallel to the main surfaces of the gain medium and propagates freely through the gain medium with respect to the short axis. They are arranged such that in each case the principal axes of the beam bundles of the pump laser units impinge on one of the pumped side surfaces in a plane perpendicular to the short axis at an angle to one another, wherein the beam cross sections of the beam bundles are superimposed on one another. | 10-15-2015 |
| 20150340833 | ENHANCEMENT RESONATOR INCLUDING NON-SPHERICAL MIRRORS - An enhancement resonator ( | 11-26-2015 |
| 20160013612 | METHOD OF DETERMINING DECREASE OF OPTICAL OUTPUT POWER IN OPTICAL AMPLIFIER APPARATUS AND OPTICAL AMPLIFIER SYSTEM | 01-14-2016 |
| 20160036194 | Laser Processing Device - Provided is a laser processing device capable of performing high-power laser processing while preventing reduction of life duration of a light source for excitation light. By collecting the light emitted from single emitters of a plurality of single emitter LDs onto one end face of an optical fiber cable, high-power excitation light is transmitted to a marking head through the optical fiber cable. Excitation light emitted from the other end face of the optical fiber cable is separated into first excitation light and second excitation light. The first excitation light excites a first laser medium to generate laser light. The generated laser light enters a second laser medium. The second excitation light enters the second laser medium. With this, the second laser medium is excited, and the laser light that has entered the second laser medium from the first laser medium is amplified. | 02-04-2016 |
| 20160079735 | LASER COMB GENERATOR - An optical comb generator for generating multiple optical wavelengths from a single source simultaneously for many optical channels on a semiconductor substrate. The comb generator provides narrow channel spacing using chirped Bragg grating with uniformly spaced grating pitches but with tapered waveguide to facilitate the fabrication process and generate laser comb channels with uniform line widths across all channels. The laser comb generator facilitates monolithic integration of many photonic integrated circuit elements. | 03-17-2016 |
