Abstract:
PROBLEM TO BE SOLVED: To generate peak intensity and pulse energy larger than those achieved with a single mode (SM) fiber, by increasing capacity for accumulating energy in an optical fiber amplifier before undesirable non-linearity and gain saturation start. SOLUTION: This optical amplifier includes: 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 to conform to a basic mode of the multiple mode fiber amplifier 12, and generates a mode-converted input beam to be input 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)2011,JPO&INPIT
Abstract:
PROBLEM TO BE SOLVED: To provide a fiber increased in polarization maintaining ability while reducing the amount of polarization mode coupling and polarization mode dispersion, and to provide a highly efficient fiber amplifier or laser with a large outer diameter for maintaining polarization so that pump light is guided in an inside clad while a large outside clad ensures the decrease of fiber core inner mode coupling. SOLUTION: The polarization maintaining fiber has a fiber core of multimode having an elliptic cross section; a first clad that surrounds the fiber core; a second clad that surrounds the first clad, and a coating that surrounds the second clad. The first clad has a circular cross section, and the second clad has a noncircular cross section. Single mode light is propagated to the fiber core. COPYRIGHT: (C)2009,JPO&INPIT
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 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 a modular, compact and widely wavelength tunable laser system of efficiently generating high-peak ultrashort pulses.SOLUTION: System compactness is ensured by employing efficient fiber amplifiers, directly or indirectly pumped by diode lasers. Peak power handling capability of the fiber amplifiers is expanded by using optimized pulse shapes, as well as dispersively broadened pulses. Dispersive broadening is introduced by dispersive pulse stretching in the presence of self-phase modulation and gain, resulting in formation of high-power parabolic pulses. After amplification, the dispersively stretched pulses are re-compressed nearly to their bandwidth limit by implementing another set of dispersive delay lines. To ensure a wide wavelength tunability of the whole system, Raman-shifting of the compact light sources of ultrashort pulses is implemented in conjunction with frequency conversion in nonlinear optical crystals. Further, positive dispersion optical amplifiers and Raman amplifier fibers are utilized.
Abstract:
PROBLEM TO BE SOLVED: To provide a fiber chirped pulse amplification system with high productivity, which has high pulse stretching ratio and compression ratio.SOLUTION: A polarization holding air clad fiber includes: a core region; a material clad region which surrounds a core; an air clad which substantially surrounds the material clad region; and a layer which surrounds the air clad. The polarization holding air clad fiber is provided in which the fiber polarization holding operation is attained by forming stress induced birefringence in an air clad fiber and assembling a stress formation region completely disposed inside the material clad region and completely surrounded by the material clad region.
Abstract:
PROBLEM TO BE SOLVED: To provide a fiber chirped pulse amplifier system allowing good productivity with large pulse stretching ratios and compressing ratios.SOLUTION: The chirped pulse amplification system comprises a seed pulse source to generate a short optical pulse, a stretcher to stretch a pulse, and a plurality of chain-wise coupled polarization maintaining fiber sections, where at least one of the polarization maintaining fibers is an amplifier.
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