Abstract:
PROBLEM TO BE SOLVED: To provide a laser optical source for producing a pulse laser beam comprising a plurality of ultrashort optical pulses whose repetition frequencies are variable. SOLUTION: The laser optical source comprises a fiber oscillator for outputting an optical pulse and a pulse stretcher arranged in order to receive the optical pulse. The optical pulse has an optical pulse width. The pulse stretcher has dispersion for expanding the optical pulse width to produce an extended optical pulse. The laser optical source further comprises a fiber amplifier arranged in order to receive the extended optical pulse. The fiber optical amplifier has a profit for amplifying the extended optical pulse. The laser optical source comprises a grating compressor which has dispersion for reducing the optical pulse width and which can be automatically adjusted. The grating compressor automatically adjusts the dispersion for different repetition frequencies. COPYRIGHT: (C)2008,JPO&INPIT
Abstract:
PROBLEM TO BE SOLVED: To provide a means which generates a high power optical pulse of femtosecond level. SOLUTION: A high power optical pulse-generating device has a fiber oscillator 10 which generates signal light; an amplifying fiber 11 which has nonlinear phase delay and receives, amplifies and compresses the signal light, the amplifying fiber acting as a Soliton Raman compressor (SRC); and a PPLN 20 (periodic polling LiNbO 3 ) which is a frequency converter which frequency-converts an amplified optical pulse into a high power optical pulse. A dispersion compensating fiber 18 compensates for the dispersion. The optical pulse is reflected by a Faraday rotation mirror (FRM) 19 to form a double-path form. The signal light receives energy from the pump light fed from a pump 16 and is amplified and compressed, and a high power pulse of femtosecond level is obtained, at a frequency at which frequency conversion is performed by the PPLN frequency convertor 20. COPYRIGHT: (C)2008,JPO&INPIT
Abstract:
PROBLEM TO BE SOLVED: To provide an optical fiber which propagates lower order modes while limiting high order modes. SOLUTION: There is provided an optical waveguide like a large core multi-mode optical fiber. This multi-mode optical fiber has a core and a clad area. This optical fiber includes a matrix material having two or more holes, and the two or more holes are in the clad area to form a border on the core area. The matrix includes silica glass, and the holes may be airholes. There is provided holey rods. The rods and optical fibers may be used in many optical systems such as an optical amplification systems, lasers, short pulse generators and Q-switch lasers. COPYRIGHT: (C)2008,JPO&INPIT
Abstract:
PROBLEM TO BE SOLVED: To provide an amplifier for a short optical pulse being small in size, having increased strength, enhanced reliability, and excellent performance for cost effectiveness. SOLUTION: The amplifier for a short optical pulse has miniaturized size, has increased strength and reliability, and has enhanced cost performance. The present invention is particularly effective for a chirped pulse amplification system in which a pulse is stretched, amplified, and re-compressed. A fiber and a bulk amplifier are used for the amplification of the pulse. A crystal for doubling the frequency can be inserted in the optical path of the pulse between the two amplifiers. Although a laser amplifier is pumped by a laser of the same material as that of the laser amplifier, the laser for the pumping and the laser for the amplification are operated under different conditions. COPYRIGHT: (C)2004,JPO
Abstract:
PROBLEM TO BE SOLVED: To suppress a Q-switch pulse by disposing a first and a second reflectors on the counterposed ends of a gain medium, disposing a third reflector apart from the first reflector in a resonator, and further disposing a saturable absorber between Fabry-Perot etalons. SOLUTION: A first reflector 42a and a second reflector 38a for forming an optical resonator 20a are disposed on the counterposed ends of a fiber gain medium 10a such as an Er-doped light amplifying fiber of an integrated saturable absorber/optical power limiter. Then, a beam splitter 64a as a third reflector apart from the first reflector 42a is disposed in the optical resonator 20a to form a Fabry-Perot etalon nearly resonant at laser frequency. A saturable absorber 34a for inducing a mode locked laser pulse is disposed between the Fabry-Perot etalons.
Abstract:
PROBLEM TO BE SOLVED: To provide a small-sized laser device which has both a laser oscillator to output optical pulses and a laser amplifier. SOLUTION: A small-sized fiber laser device has a laser oscillator connected to a laser beam source 88 for generating optical pulses and a laser amplifier connected to the laser oscillator for amplifying the generated optical pulses. The laser oscillator has a first optical fiber 42 which connects bulk parts to the laser beam source 88, and the laser amplifier 14 has a second optical fiber 62 which connects the bulk parts to a laser light source 92. The first and the second fibers 42 and 62 are wound around a common holder. A fiber tray is connected to a fiber bench, and the bulk parts of the laser oscillator and the laser amplifier are attached to the fiber bench.
Abstract:
PROBLEM TO BE SOLVED: To quickly, accurately and quantitatively distribute an electrolyte in pores with noncontact with the sealing surface or connecting surface of a battery by printing the electrolyte on the surface of an electrode, a separator, or two layers of electrode/separator by an ink jet printing method. SOLUTION: An ink jet head 300 has a plurality of nozzles 306, a plurality of printed porous two layers are fed under the ink jet head 300 in the arrow direction 1. A print head is preferably positioned 1-5 mm over the passing through two layers 204. Two layer 204 has a polymer gasket 212 whose periphery is printed, heated, and sealed. The ink jet head 300 supplies electrolyte drops 215A on the two layers 204 without polluting the surface 214 of the gasket 212, and pulse oscillation is conducted to form mother drops 215. The electrolyte drops 215A act like image forming pixel, and an image drawn with dots is formed on the surface of the two layer body 204.
Abstract:
PROBLEM TO BE SOLVED: To actualize the size reduction of the devices, the simplification of designing, low loss, high efficiency, wide bandwidth, controllability of dispersion characteristics, etc., as compared with a convertional dispersion delay line used for an extremely-short pulse system. SOLUTION: This extremely-short pulse amplifying device uses a chirp quasi- phase synchronous (QPM) grating 12 as a dispersion delay line for expanding extremely-short pulses. The QPM grating 12 which varies in cycle in the propagation direction of a beam generates a secondary higher harmonic at the same time. In general, the output of this secondary higher harmonic is modulated together with the amplitude and phase. The QPM grating 12 also expands the secondary higher harmonic of an input pulse of basic wavelength. In general, the periodic QPM grating 12 can efficiently generate secondary higher harmonic pulses which are optionally shaped.
Abstract:
PROBLEM TO BE SOLVED: To detect the distances to a plurality of targets with high resolution in real time by monitoring the number of reflected pulses produced in response to an emitted pulse and stopping the operation of a counting means when a prescribed number of reflected pulses is received. SOLUTION: When a pulse 128 is emitted from a vehicle 140, pulses 132, 134, 136, and 138 are reflected from vehicles 142, 144, 146, and 148 and the reflected pulses are used for determining the distances to the target vehicles 142, 144, 146, and 148 from the vehicle 140. Namely, a means which determines the time lag between the emitted pulse 128 and one of the reflected pulses 132, 134, 136, and 138 is provided. The determining means is composed of a clock generator which generates a clock pulse and a counter (counting means) which counts the clock pulse. A control means monitors the number of the reflected pulses produced in response to the emitted pulse and stops the operation of the counter when a prescribed number of reflected pulses is received.
Abstract:
PROBLEM TO BE SOLVED: To provide a means transmitting a very short light pulse with a high peak power to a required point in an optical device. SOLUTION: This very short light pulse transmitting device is provided with a pulse expander 20 receiving the super-short light pulse with a high peak power and expanding its pulse width and an optical fiber 30 transmitting the light pulse over a required distance and having the dispersion compensating other dispersion so that the light pulse is re-compressed sufficiently in the required point in the optical device 50. The pulse width of the light pulse is expanded by the expander 20, and a chirp light pulse with a low peak power is formed. Thus pulse whose dispersion is compensated while it is transmitted through the optical fiber 30, and is re-compressed by the optical fiber 30 or a compressor 40 to be transmitted to the optical device 50. Since the peak power in the optical fiber 30 is small, the super-short light pulse hardly by affected by a nonlinear effect.