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38results about How to "Reduce dispersion effect" patented technology

Methods and apparatus for optical transmission of digital signals

A method of communicating digital information over a dispersive optical channel includes encoding the digital information into a plurality of data blocks, each of which includes a number of bits of the information. A time-varying electrical signal is generated which corresponds with each of said data blocks. The time-varying electrical signal is applied to an optical transmitter (122) to generate an optical signal which includes an asymmetrically amplitude limited transmitted signal modulated onto an optical carrier. The optical signal is then transmitted over the dispersive optical channel (106). At a receiving apparatus (104) the optical signal is detected to produce an electrical signal which corresponds with the asymmetrically amplitude limited transmitted signal. A frequency domain equalisation of the electrical signal mitigates the effect of dispersion of the optical channel (106) on the transmitted optical signal, and the equalised signal is decoded to recover the encoded data blocks and the corresponding transmitted digital information. The method enables bipolar signals to be transmitted over a dispersive unipolar optical channel, and reduces or eliminates the need to apply a high optical bias level at the transmitter, thereby improving optical power efficiency and enabling output power levels to be maintained below applicable safe levels, while simultaneously enabling the effects of channel dispersion to be substantially mitigated.
Owner:MONASH UNIV

Methods and apparatus for optical transmission of digital signals

A system (100) for transmitting digital information includes a transmitting apparatus (102) for generating an optical signal bearing digital information, a dispersive optical channel (104), and a receiving apparatus (110) for receiving the optical signal. The dispersive optical channel (104) is disposed to convey the optical signal from the transmitting apparatus (102) to the receiving apparatus (110). The transmitting apparatus includes an encoder (114) for encoding digital information into a series of blocks, each including a plurality of data symbols corresponding with one or more bits of digital information. A signal generator (118) generates a time-varying signal corresponding with each of said blocks. An optical transmitter (136) is arranged to apply the time-varying signal to an optical source (138) to produce an optical signal which includes an optical carrier and substantially only a single information bearing optical sideband in an optical frequency domain, the sideband corresponding with the time-varying signal. The receiving apparatus (110) includes an optical detector (146) for detecting the optical signal to produce a corresponding received time-varying electrical signal. The receiver further includes means (166) for generating a series of received data blocks from the time-varying electrical signal. An equaliser (168) performs an equalisation of received data symbols included in each data block to mitigate the effect of dispersion of the optical channel, thereby enabling the transmitted data symbols to be recovered.
Owner:MONASH UNIV

Methods and apparatus for optical transmission of digital signals

A system (100) for transmitting digital information includes a transmitting apparatus (102) for generating an optical signal bearing digital information, a dispersive optical channel (104), and a receiving apparatus (110) for receiving the optical signal. The dispersive optical channel (104) is disposed to convey the optical signal from the transmitting apparatus (102) to the receiving apparatus (110). The transmitting apparatus includes an encoder (114) for encoding digital information into a series of blocks, each including a plurality of data symbols corresponding with one or more bits of digital information. A signal generator (118) generates a time-varying signal corresponding with each of said blocks. An optical transmitter (136) is arranged to apply the time-varying signal to an optical source (138) to produce an optical signal which includes an optical carrier and substantially only a single information bearing optical sideband in an optical frequency domain, the sideband corresponding with the time-varying signal. The receiving apparatus (110) includes an optical detector (146) for detecting the optical signal to produce a corresponding received time-varying electrical signal. The receiver further includes means (166) for generating a series of received data blocks from the time-varying electrical signal. An equalizer (168) performs an equalization of received data symbols included in each data block to mitigate the effect of dispersion of the optical channel, thereby enabling the transmitted data symbols to be recovered.
Owner:MONASH UNIV

Hollow cube-corner prism optical delay line device with endogenous scale light source

The invention relates to a hollow cube-corner prism optical delay line device with an endogenous scale light source. The hollow cube-corner prism optical delay line device comprises a scale light source, a photoelectric sensor, an optical fiber coupler, a wavelength division multiplexer, collimators Z1 and Z2, plane reflecting mirrors F1 and F2, polarization controllers P1 and P2, a single-mode optical fiber, a rotary disk, hollow cube-corner prisms and a motor, wherein a scale light source signal is divided into two paths of light signals by the optical fiber coupler; the first path of light signals passes through the polarization controller P1 and the collimator Z1, is emitted to the plane reflecting mirror F1, returns along the same road and is received by the photoelectric sensor; and the second path of light signals passes through the polarization controller P2, the wavelength division multiplexer and the collimator Z2, is emitted to the hollow cube-corner prisms which are uniformly distributed on the rotary disk along the circumference, is guided for 180 DEG and then emitted to the plane reflecting mirror F2 and returns along the same road, and a returned signal is received by the photoelectric sensor and interferes with the first path of signals. The hollow cube-corner prism optical delay line device is simple in installation process and high in measuring speed, and signal to noise ratio and measuring accuracy are improved.
Owner:TIANJIN SUOWEI ELECTRONICS TECH

Methods and apparatus for optical transmission of digital signals

A method of communicating digital information over a dispersive optical channel includes encoding the digital information into a plurality of data blocks, each of which includes a number of bits of the information. A time-varying electrical signal is generated which corresponds with each of said data blocks. The time-varying electrical signal is applied to an optical transmitter (122) to generate an optical signal which includes an asymmetrically amplitude limited transmitted signal modulated onto an optical carrier. The optical signal is then transmitted over the dispersive optical channel (106). At a receiving apparatus (104) the optical signal is detected to produce an electrical signal which corresponds with the asymmetrically amplitude limited transmitted signal. A frequency domain equalization of the electrical signal mitigates the effect of dispersion of the optical channel (106) on the transmitted optical signal, and the equalized signal is decoded to recover the encoded data blocks and the corresponding transmitted digital information. The method enables bipolar signals to be transmitted over a dispersive unipolar optical channel, and reduces or eliminates the need to apply a high optical bias level at the transmitter, thereby improving optical power efficiency and enabling output power levels to be maintained below applicable safe levels, while simultaneously enabling the effects of channel dispersion to be substantially mitigated.
Owner:MONASH UNIV

Forecasting method for vehicle body structure-acoustic coupling based on smoothed finite element boundary element method

The invention provides a forecasting method for vehicle body structure-acoustic coupling based on a smoothed finite element boundary element method. The method comprises the following steps: generating a vehicle body structure-acoustic grid model; utilizing the smoothed finite element method to perform smooth processing on the stress field in a shell unit; adopting a mixed integral method to perform separate integral of shearing items subjected to shearing strain in the shell under a natural coordinate system; building a smooth Galerkin weak form of a vehicle body shell structure kinetic equation, and obtaining a dynamic equation after the weak form is subjected to discrete processing; creating an acoustic realistic model by using the boundary element method; according to the continuous displacement and pressure of the coupling interface, obtaining a structure-acoustic coupled smoothed finite element boundary element model; performing simulation forecasting by utilizing the coupled model. When the method is used for solving the vehicle body structure-acoustic coupling problem, relatively good calculation effect can be obtained, and the band frequency width can be analyzed more effectively. Moreover, the method has relatively low quality requirements on the model to reduce the pretreatment time, and has a wide engineering application prospect.
Owner:CHINA AUTOMOTIVE ENG RES INST

Double balanced mixer device

The invention discloses a double balanced mixer device which comprises a mixer chamber body, a mixer circuit, and a K type joint; the mixer circuit further comprises a mixer tube, a gold belt, gold wires, 50 omega coplanar waveguide, a coupling slot line, a 60 omega slot line, a dielectric substrate, and a lambada/8 short-circuit wire. According to the double balanced mixer device, the K type joint is adopted, the 50 omega coplanar waveguide is selected as the signal end and is transited to the coupling slot line, the coupling slot line is gradually changed to the 60 omega slot line and is added to the mixer tube, the 50 omega coplanar waveguide is coupled to the slot line by the adoption of a gold belt coupling mode, and capacitive quality of mixer diodes is counteracted; the broadband barron is achieved by the adoption of a magic T network which is composed of the coplanar waveguide, the coupling slot line and the slot line, crisscross of transmission lines is not needed and strong directivity is achieved, and isolation is improved; color dispersion effect of the coplanar waveguide is relieved; a golden wire bridge joint mode is adopted, so that the occurrence of a higher order mode is inhibited, and the higher order mode of the coupling slot line stimulated by radio frequency in the coplanar waveguide is prevented.
Owner:XIAN UNIV OF POSTS & TELECOMM

Spatial modulation Fourier transform infrared spectrometer based on grid beam splitter

The invention relates to the field of spectral analysis instruments, in particular to a spatial modulation Fourier transform infrared spectrometer based on a grid beam splitter. The spatial modulation Fourier transform infrared spectrometer based on the grid beam splitter resolves the problems that movable components exist inside the structure of an existing spectrometer, so that the spectrometer is large in size and weight. The spatial modulation Fourier transform infrared spectrometer based on the grid beam splitter comprises a collimation system, a sample pool, an interference system, a beam contracting system and a detector, wherein the interference system comprises a multi-stage small-ladder micro reflection mirror, the grid beam splitter and a multi-stage large-ladder micro reflection mirror; the light emitted by an infrared light source is collimated by the collimation system and becomes infrared parallel light, and the parallel light is absorbed by samples of the sample pool and then split by the grid beam splitter into two coherent light beams; the two light beams enter the multi-stage large-ladder micro reflection mirror and the multi-stage small-ladder micro reflection mirror respectively, and then are reflected to the grid beam splitter through the multi-stage small-ladder micro reflection mirror; after the light reflected by the grid beam splitter passes through the beam contracting system, interference fringes are obtained on the infrared area-array detector; Fourier transform is carried out on the interference fringes, and then the spectral information of an object to be detected can be obtained.
Owner:CHANGCHUN INST OF OPTICS FINE MECHANICS & PHYSICS CHINESE ACAD OF SCI

FCT-FDM forward simulation method based on dispersion viscosity wave equation

The invention discloses an FCT-FDM forward simulation method based on a dispersion viscosity wave equation. A propagation characteristic of a dispersion viscosity wave is researched from the perspective of the numerical simulation. Calculating steps of FCT-FDM is stated, a fluid saturation model is designed, the method is utilized to simulate propagation of the dispersion viscosity wave, and comparing and analyzing are carried out on a numerical result and a sound wave simulation result. The result indicates that relative to a sound wave, the dispersion viscosity wave is obviously attenuated on the amplitude, and the phase position is notably changed. The attenuation degree of the dispersion viscosity wave mainly depends on a dispersion attenuation coefficient and a value of the dispersion attenuation coefficient. According to the FCT-FDM forward modeling method based on the dispersion viscosity wave equation, an effective tool is provided for the numerical simulation of a seismic wave, in particular to a medium containing fluid. The FCT-FDM forward modeling method based on the dispersion viscosity wave equation can be used for describing the attenuation and the phase-shift characteristic of the seismic wave in the fluid medium. In addition, the method is easy to achieve, and the operability is high.
Owner:XI AN JIAOTONG UNIV

Hollow cube-corner prism optical delay line device with endogenous scale light source

The invention relates to a hollow cube-corner prism optical delay line device with an endogenous scale light source. The hollow cube-corner prism optical delay line device comprises a scale light source, a photoelectric sensor, an optical fiber coupler, a wavelength division multiplexer, collimators Z1 and Z2, plane reflecting mirrors F1 and F2, polarization controllers P1 and P2, a single-mode optical fiber, a rotary disk, hollow cube-corner prisms and a motor, wherein a scale light source signal is divided into two paths of light signals by the optical fiber coupler; the first path of light signals passes through the polarization controller P1 and the collimator Z1, is emitted to the plane reflecting mirror F1, returns along the same road and is received by the photoelectric sensor; and the second path of light signals passes through the polarization controller P2, the wavelength division multiplexer and the collimator Z2, is emitted to the hollow cube-corner prisms which are uniformly distributed on the rotary disk along the circumference, is guided for 180 DEG and then emitted to the plane reflecting mirror F2 and returns along the same road, and a returned signal is received by the photoelectric sensor and interferes with the first path of signals. The hollow cube-corner prism optical delay line device is simple in installation process and high in measuring speed, and signal to noise ratio and measuring accuracy are improved.
Owner:TIANJIN SUOWEI ELECTRONICS TECH

Passive optical network system and device thereof

The invention provides an optical network unit in a passive optical network system and an uplink wavelength generation method of the optical network unit. The optical network unit comprises a semiconductor laser and a semiconductor optical amplifier, and is characterized in that the semiconductor laser is used for selecting and locking a specific wavelength from a plurality of wavelengths of external injection light and transmitting a single-mode coherent light source of the specific wavelength; and the semiconductor optical amplifier is used for generating and amplifying a wide-spectrum light source and modulating uplink data to the single-mode coherent light source of the specific wavelength, wherein the semiconductor optical amplifier is a quantum dot semiconductor optical amplifier; and the semiconductor laser can adopt an FP laser to select and lock a specific wavelength from the plurality of wavelengths of the external injection light through bias tuning. The plurality of wavelengths of the external injection light form a plurality of reflection wavelengths via a remote node through reflection. The method provided by the invention is low in implementation cost, conducive to commercial implementation and high in output power, and meets high-speed uplink data modulation requirements and colorless performance of the PON (Passive Optical Network) system.
Owner:ALCATEL LUCENT SHANGHAI BELL CO LTD

Totally-reflective femtosecond stimulated Raman spectrometer

ActiveCN110596073AAvoid optical dispersionContinuously tunable wavelengthRaman scatteringBeam splitterFemtosecond pulsed laser
The invention discloses a totally-reflective femtosecond stimulated Raman spectrometer. The Raman spectrometer comprises a light source module, two beam splitters, two optical delay lines, a reflectorset, a concave mirror, a diaphragm, a spectral filtering module and a first spectrometer, wherein a femtosecond pulse laser generated by the light source module is split into two laser beams after passing through the first beam splitter, the reflected beam serves as actinic pump light and focuses on a sample after passing through a first reflector, a second reflector, a third reflector, the firstoptical delay line, a fourth reflector, a fifth reflector, a sixth reflector, a seventh reflector and the concave mirror sequentially; the transmitted beam is reflected after passing through the second beam splitter, serves as detection light and focuses on the sample after passing through an eighth reflector, a ninth reflector, a tenth reflector, an eleventh reflector, the seventh reflector andthe concave mirror sequentially, and the transmitted light is collected by the first spectrometer after passing through the diaphragm; and the second laser beam is transmitted after passing through the second beam splitter to serve as Raman pump light and focuses on the sample after passing through a twelfth reflector, a thirteenth reflector, a fourteenth reflector, the spectral filtering module,the second optical delay line, a fifteenth reflector, a sixteenth reflector, the seventh reflector and the concave mirror sequentially.
Owner:GUANGDONG UNIV OF TECH
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