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47results about How to "High gain factor" patented technology

Bragg reflection waveguide double-beam laser and application method thereof

ActiveCN102709810AImproved compactness and stabilityHigh gain factorLaser detailsSemiconductor lasersLaser scanningLight beam
The invention relates to a Bragg reflection waveguide double-beam laser which sequentially comprises an N-plane electrode, a substrate, a buffer layer, a lower waveguide layer, a defective layer, an upper waveguide layer, a cover layer and a P-plane electrode from bottom to top. An active region is arranged in the defective layer; the lower waveguide layer comprises a plurality of pairs of Bragg reflectors formed in a mode that N-type doped high and low refractive index material layers periodically and alternately grow; the upper waveguide layer comprises a plurality of pairs of Bragg reflectors formed in a mode that P-type doped high and low refractive index material layers periodically and alternately grow; and the effective refractive index of a guided mode is lower than those of the P-type doped low refractive index material layers and the N-type doped low refractive index material layers. The Bragg reflection waveguide double-beam laser disclosed by the invention can directly output two beams of stable laser with low transversal divergence, separated angles between the double beams and controllable power symmetry and has wide application prospect in the fields of high-speed laser scanning, high-precision laser detection, laser processing, an off-axis outer cavity, coherent coupling and the like.
Owner:CHANGCHUN INST OF OPTICS FINE MECHANICS & PHYSICS CHINESE ACAD OF SCI

Monolithically integrated electrical pumping bragg reflection waveguide terahertz laser device

The invention provides a monolithically integrated electrical pumping bragg reflection waveguide terahertz laser device, belongs to the field of photoelectric devices, and aims at solving the problems in existing terahertz laser output. According to the laser device, a bragg reflection waveguide structure is adopted in the vertical direction; the laser device comprises two adjacent distributed bragg reflection laser devices, a Y-waveguide beam coupler, a laser power amplifier and a passive bragg reflection waveguide nonlinear frequency conversion part, wherein the rear cavity surfaces of the two distributed bragg reflection laser devices are used for etching distributed bragg gratings which are slightly different in cycle and duty ratio respectively, so that a certain difference is formed between the output wavelengths of the two laser devices; two input ends of one side of the Y-waveguide beam coupler are respectively connected with the two laser devices; the other ends are coupled to output dual-wavelength laser; the laser power amplifier is connected with an output end of a Y waveguide and is used for carrying out power amplification on the injected dual-wavelength laser; and the passive bragg reflection waveguide nonlinear frequency conversion part is connected with the output end of the laser power amplifier, so that a difference frequency 1 / lambda1-1 / lambda2=1 / lambda3 is generated by the injected laser with two different wavelengths lambda1 and lambda2, thereby realizing output of the terahertz laser lambda3.
Owner:吉光半导体科技有限公司

Optical fiber of stimulated Brillouin scattering effect enhancement type

The invention discloses an optical fiber of a stimulated Brillouin scattering effect enhancement type, and the optical fiber comprises a fiber core and a wrapping layer surrounding the fiber core. The radius a of the fiber core is from 1 [mu]m to 7 [mu]m, and the fiber core is doped with one of GeO2, P2O, and Al2O3. The wrapping layer is doped with a material F. The relation between the refractive index difference delta n between the fiber core and the wrapping layer and the radius a of the fiber meets the conditions: a*a*delta n is greater than zero and not greater than 0120 [mu]m[2]. The relation between the sound speed difference delta V1 between the fiber core and the wrapping layer and the radius a of the fiber meets the conditions: a*a*delta V1 is greater than zero and not greater than 225 [mu]m[2]*m/s, so as to excite and generate single optical mode and single sound mode constraint stably in the optical fiber at the same time. The fiber core and the wrapping layer are respectively doped with different materials, thereby obtaining the common excitation of an acousto-optic field. A single brillouin gain peak is formed in the optical fiber through coupling. The position of the gain peak of a gain spectrum of the optical fiber is higher in gain coefficient, and the full width at half maximum of a brillouin gain spectrum is narrower and is about 10 MHz. Moreover, the optical fiber also can improve an absolute value of a chromatic dispersion parameter while enhancing the stimulated Brillouin scattering effect, and effectively inhibits an four-wave mixing effect nearby a normally-used working band window 1.55 [mu]m.
Owner:HUAZHONG UNIV OF SCI & TECH

Wide-range and high-precision rolling angle measuring device and measuring method

The invention belongs to the field of photoelectric measurement of a rolling angle, and particularly discloses a wide-range and high-precision rolling angle measuring device. The measuring device comprises a double-frequency laser device, a light splitting prism, a phase meter and a computer, wherein the light splitting prism is arranged at the front end of the optical axis of the double-frequencylaser device, a first polarizer and a first photoelectric detector are sequentially arranged on the reflection optical axis of the light splitting prism; a quarter-wave plate and a depolarization light splitting prism are sequentially arranged on the transmission optical axis of the light splitting prism; a backward prism reflector, a half-wave plate and a four-angle cone reflector are sequentially arranged in the direction of the transmission optical axis of the depolarization light splitting prism; a plane reflecting mirror is arranged on one side of the four-angle cone reflector; a secondpolarizer and a second photoelectric detector are arranged in the reflection direction of the depolarization light splitting prism; the first photoelectric detector and the second photoelectric detector are connected with the phase meter, and the phase meter is connected with the computer. The measuring device enables the phase difference and the rolling of the half-wave plate to be in a linear relation, the rolling angle measuring range is enlarged, the size is small, and the measuring precision is high.
Owner:XI AN JIAOTONG UNIV

Optical fiber vibration detection system and optical fiber vibration detection method

The invention discloses an optical fiber vibration detection system and an optical fiber vibration detection method. An optical fiber vibration sensor is connected with a host computer, the optical fiber vibration sensor comprises a first circulator, N pumping light sources, and a first wavelength division multiplexer, the first circulator is connected with the first wavelength division multiplexer, the N pumping light sources are connected with the first wavelength division multiplexer, the first wavelength division multiplexer is connected to a remote gain module via a first sensing optical fiber, and the remote gain module is also connected with a second sensing optical fiber. Signal light emitted by the first circulator and pumping light emitted by the N pumping light sources enter the remote gain module via the first wavelength division multiplexer, and the pumping light is downloaded via the remote gain module for the amplification of the signal light. Therefore, the technical problem that the actual production requirement cannot be satisfied due to limited detection distance of the optical fiber vibration signal detection system is solved, and the accuracy of remote optical fiber vibration detection is improved.
Owner:PIPECHINA SOUTH CHINA CO

Image sharpening method and device

The embodiment of the invention discloses an image sharpening method and device. The method comprises the steps of converting a to-be-sharpened image frame from an RGB color space to a YUV color space, performing Gaussian low-pass filtering on a Y brightness component to obtain a Y brightness low-pass component, and performing subtraction on the Y brightness component and the Y brightness low-passcomponent to obtain a Y brightness high-frequency component; filtering the Y brightness component according to a preset filtering operator to obtain a Y brightness image background; calculating an image gradient map of the Y brightness component according to a preset gradient operator, and obtaining an image texture map of the Y brightness component according to the image gradient map; calculating to obtain a Y brightness minimum visual difference image according to the Y brightness image background and the Y brightness image texture map; calculating a gain coefficient based on the Y brightness minimum perceptible difference image and the Y brightness high-frequency component; and calculating the sharpened image according to the gain coefficient. Image details can be enhanced and noise enhancement can be avoided; and the obtained gain coefficient is more consistent with the visual characteristics of human eyes.
Owner:INFORMATION SCI RES INST OF CETC

Bragg reflection waveguide double-beam laser and application method thereof

The invention relates to a Bragg reflection waveguide double-beam laser which sequentially comprises an N-plane electrode, a substrate, a buffer layer, a lower waveguide layer, a defective layer, an upper waveguide layer, a cover layer and a P-plane electrode from bottom to top. An active region is arranged in the defective layer; the lower waveguide layer comprises a plurality of pairs of Bragg reflectors formed in a mode that N-type doped high and low refractive index material layers periodically and alternately grow; the upper waveguide layer comprises a plurality of pairs of Bragg reflectors formed in a mode that P-type doped high and low refractive index material layers periodically and alternately grow; and the effective refractive index of a guided mode is lower than those of the P-type doped low refractive index material layers and the N-type doped low refractive index material layers. The Bragg reflection waveguide double-beam laser disclosed by the invention can directly output two beams of stable laser with low transversal divergence, separated angles between the double beams and controllable power symmetry and has wide application prospect in the fields of high-speed laser scanning, high-precision laser detection, laser processing, an off-axis outer cavity, coherent coupling and the like.
Owner:CHANGCHUN INST OF OPTICS FINE MECHANICS & PHYSICS CHINESE ACAD OF SCI

Optical fiber vibration detection system and optical fiber vibration detection method

The invention discloses an optical fiber vibration detection system and an optical fiber vibration detection method. An optical fiber vibration sensor is connected with a host computer, the optical fiber vibration sensor comprises a first circulator, N pumping light sources, and a first wavelength division multiplexer, the first circulator is connected with the first wavelength division multiplexer, the N pumping light sources are connected with the first wavelength division multiplexer, the first wavelength division multiplexer is connected to a remote gain module via a first sensing optical fiber, and the remote gain module is also connected with a second sensing optical fiber. Signal light emitted by the first circulator and pumping light emitted by the N pumping light sources enter the remote gain module via the first wavelength division multiplexer, and the pumping light is downloaded via the remote gain module for the amplification of the signal light. Therefore, the technical problem that the actual production requirement cannot be satisfied due to limited detection distance of the optical fiber vibration signal detection system is solved, and the accuracy of remote optical fiber vibration detection is improved.
Owner:PIPECHINA SOUTH CHINA CO

Image sharpening method and device

An image sharpening method and device according to an embodiment of the present invention includes: converting an image frame to be sharpened from an RGB color space to a YUV color space, and performing Gaussian low-pass filtering on a Y luminance component to obtain a Y luminance low-pass component, Calculate the difference between the Y luminance component and the Y luminance low-pass component to obtain the Y luminance high-frequency component; filter the Y luminance component according to the preset filtering operator to obtain the Y luminance image background; calculate the Y luminance according to the preset gradient operator The image gradient map of the component, and the image texture map of the Y brightness component is obtained according to the image gradient map; according to the Y brightness image background and the Y brightness image texture map, the Y brightness minimum perceptible difference image is calculated; based on the Y brightness minimum perceptible difference image and Y luminance high-frequency components, calculate the gain coefficient; calculate the sharpened image according to the gain coefficient. The image sharpening method of the present invention can enhance image details and avoid noise enhancement; the obtained gain coefficient is more in line with the visual characteristics of human eyes.
Owner:INFORMATION SCI RES INST OF CETC

A Stimulated Brillouin Scattering Enhanced Optical Fiber

The invention discloses an optical fiber of a stimulated Brillouin scattering effect enhancement type, and the optical fiber comprises a fiber core and a wrapping layer surrounding the fiber core. The radius a of the fiber core is from 1 [mu]m to 7 [mu]m, and the fiber core is doped with one of GeO2, P2O, and Al2O3. The wrapping layer is doped with a material F. The relation between the refractive index difference delta n between the fiber core and the wrapping layer and the radius a of the fiber meets the conditions: a*a*delta n is greater than zero and not greater than 0120 [mu]m[2]. The relation between the sound speed difference delta V1 between the fiber core and the wrapping layer and the radius a of the fiber meets the conditions: a*a*delta V1 is greater than zero and not greater than 225 [mu]m[2]*m / s, so as to excite and generate single optical mode and single sound mode constraint stably in the optical fiber at the same time. The fiber core and the wrapping layer are respectively doped with different materials, thereby obtaining the common excitation of an acousto-optic field. A single brillouin gain peak is formed in the optical fiber through coupling. The position of the gain peak of a gain spectrum of the optical fiber is higher in gain coefficient, and the full width at half maximum of a brillouin gain spectrum is narrower and is about 10 MHz. Moreover, the optical fiber also can improve an absolute value of a chromatic dispersion parameter while enhancing the stimulated Brillouin scattering effect, and effectively inhibits an four-wave mixing effect nearby a normally-used working band window 1.55 [mu]m.
Owner:HUAZHONG UNIV OF SCI & TECH
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