Abstract:
PROBLEM TO BE SOLVED: To provide a passively mode-locked fiber laser capable of generating linearly chirped high power parabolic pulses. SOLUTION: The passively mode-locked fiber laser for generating short light pulses, comprises a laser resonator having intra-cavity dispersion and a rare-earth-doped gain medium that is provided in the laser resonator, has positive dispersion of intracavity dispersion and operates so as to generate a value of intra-cavity self-phase modulation larger than π. The band width of an intra-cavity light pulse changes during propagation in the laser resonator. COPYRIGHT: (C)2009,JPO&INPIT
Abstract:
PROBLEM TO BE SOLVED: To provide a method of stabilizing a short pulse fiber laser which reduces a timing jitter caused by a variation in environmental condition such as vibration, air disturbance, a change in temperature to a minimum. SOLUTION: The method of stabilizing a short pulse fiber laser has a segregating step which segregates the fiber lasers 210 and 220 from an outside environment, a winding step which winds the fiber lasers 210 and 220 around a fiber spool 280, and an operating step which operates the fiber lasers 210 and 220 while the fiber lasers 210 and 220 are wound around the fiber spool 280. The fiber lasers 210 and 220 are wound around the fiber spool 280 and segregated from the outside environment, and therefore become free of influences of the variation in environmental condition and are stabilized. COPYRIGHT: (C)2008,JPO&INPIT
Abstract:
PROBLEM TO BE SOLVED: To provide a method for scribing or welding transparent materials. SOLUTION: A method for scribing transparent materials uses ultrashort laser pulses to create multiple scribe features with a single pass of the laser beam across the material, with at least one of the scribe features being formed below the surface of the material. This enables clean breaking of transparent materials. A method for welding transparent materials uses ultrashort laser pulses to create a bond through localized heating. The ultrashort pulse duration causes nonlinear absorption of the laser radiation, and the high repetition rate of the laser causes pulse-to-pulse accumulation of heat within the materials. The laser is focused near the interface of the materials, generating a high energy fluence at the region to be welded. This minimizes damage to the rest of the material and enables fine weld lines. COPYRIGHT: (C)2008,JPO&INPIT
Abstract:
PROBLEM TO BE SOLVED: To provide a p-type semiconductor zinc oxide (ZnO) film and a manufacturing method of this film. SOLUTION: A p-type ZnO material is deposited by using a pulsed laser deposition method (PLD). In this method, a pulsed laser beam is focused on a solid target comprising a mixture of a compound containing both Li and P with ZnO. By the high power density of the focused laser pulse, the material on the target surface is ablated. Then, plasma is formed, and this is deposited on the surface of the substrate. Moreover, there is described a pulsed laser deposition process using a transparent substrate including a pulsed laser source, a substrate that is transparent to the wavelength of the pulsed laser, and a multi-target system. The optical path of the pulsed laser is arranged in such a manner that the pulsed laser is incident from the back of the substrate to pass through the substrate and is focused on the target. By translating the substrate toward the target, the attachment of a micro pattern using the root of an ablation plume is permitted. COPYRIGHT: (C)2008,JPO&INPIT
Abstract:
PROBLEM TO BE SOLVED: To generate a pulse energy having a peak intensity larger than those achieved with a single mode (SM) fiber, by increasing a capacity for accumulating energy in an optical fiber amplifier before starting undesirable non-linearity and gain saturation. SOLUTION: The optical amplifier has a fiber oscillator 10 serving as a laser source, which generates an input beam having a mode close to diffraction limit; a multiple mode fiber amplifier 12; a mode converter 14; and a pump source 20. The mode converter 14 receives an input beam, converts a mode of the input beam so as to conform to a basic mode of the multiple mode fiber amplifier 12, and generates a mode-converted input beam to be inputted to the multiple mode fiber amplifier 12. The pump source 20 optically pumps the multiple mode fiber amplifier 12, and generates a strong output beam which is intrinsically amplified by the basic mode. COPYRIGHT: (C)2007,JPO&INPIT
Abstract:
PROBLEM TO BE SOLVED: To reduce to the minimum timing jitter caused by variations in environmental condition such as vibrations, disturbance of air, change in temperature. SOLUTION: Two lasers are configured by using the an identical component in an identical container so as to be pumped by the same pump laser while maintaining a state in which the two lasers can be controlled independently. In particular, in the case of a fiber laser, two fibers are wound together around the same shaft (spool). COPYRIGHT: (C)2004,JPO
Abstract:
PROBLEM TO BE SOLVED: To provide the chirped pulse amplifying device which is simple, inexpensive, and small-sized. SOLUTION: The limits of maximum pulse energy can be evaded by arranging quasi-phase synchronous(QPM) crystal 40 with chirped cycles. The crystal 40 generates a secondary higher harmonic in a single element and pulses expanded by a chirped Bragg grating 20 can be compressed. This constitution makes the device simple and small-sized and the energy of obtained extremely-short pulses substantially increases. Further, the use of this QPM crystal 40 makes possible the variable compensation of a linear and a nonlinear frequency chirp of the secondary higher harmonic. This property is used to make it possible to design the chirp pulse amplifying device which is inexpensive, small-sized, robust, and simple and outputs extremely short pulses.
Abstract:
PROBLEM TO BE SOLVED: To enable a mode-locked double clad fiber laser excited by a wide band diode laser array to generate pulses of the order of picoseconds or femtoseconds. SOLUTION: 560fsec pulses of maximum power 40pJ and wavelength 1560nm are generated by an Er/Yb fiber oscillator 101. 170fsec pulses of 50pJ can be generated in a cavity which is compensated for dispersion. A negative chirp fiber Bragg grating 105 is added so as to improve a cavity in dispersion controllability, whereby pulses of maximum power 1nJ and width 3psec can be generated. A saturated absorber 118 is used to make an oscillator start generating pulses, and a nonlinear polarization development is used for shaping pulses in a normal state.
Abstract:
PROBLEM TO BE SOLVED: To provide an optical sensor, which outputs a sufficiently large output power so that measurement can be readily performed even with an integral type optical sensor, and can output further accurate result without the requirements for through calibration and the highly controlled environment. SOLUTION: A waveguide 18 comprising a base material 16, which is doped with a rare earth element, is included in a device 12 of an integral type optical sensor. The ray, which is propagating along the waveguide 18, excites the element, and the element emits light. Thus, the total amount of the light propagating in the wavelength 18 is increased. Since the waveguide 18 itself acts as the laser, the change in optical characteristics of a material under analysis forming a part of a laser cavity affects on the operation of the laser. Therefore, the wavelength or the power of the light generated from the laser is changed directly in correspondence with the change in concentration of the material to be sensed. The change is emphasized by the intrinsic gain characteristic of the laser medium.
Abstract:
PURPOSE: To improve reliability and to reduce cost by amplifying a pulse energy by a plurality of stages of amplifiers to generate an amplified pulse energy. CONSTITUTION: A compact system 100 includes a means for amplifying the peak output of a pulse energy. A peak output amplification means includes a means for amplifying a pulse energy that is indicated as a two-stage erbium doping treatment fiber amplifier 1 10 and a means for compressing a pulse energy that is amplified by overlapping wavelength bands indicated as a lattice body compressor 112. The two-stage erbium doping treatment fiber amplifier 110 includes a first-stage energy amplifier 114 and a second-stage energy amplifier 116. Then, a variable diode laser 102 is generated a nano-order chirp pulse existing in the erbium doping treatment fiber is amplified, thus obtaining an ultra-short pulse with a high energy without causing the saturation energy breakdown of an amplifier.