35 results about "Acousto optic deflector" patented technology

The invention belongs to the technical field of laser, and discloses a laser beam splitting and combining device based on an acousto-optic deflector pair and application thereof, and the laser beam splitting and combining device comprises a transmitting optical fiber module, a first acousto-optic deflector, a diaphragm, a second acousto-optic deflector and a receiving optical fiber module which are sequentially arranged; the first acousto-optic deflector and the second acousto-optic deflector are arranged in parallel; the transmitting optical fiber module is used for transmitting laser to the first acousto-optic deflector; the first acousto-optic deflector and the second acousto-optic deflector are used for deflecting, splitting or combining laser beams; the diaphragm is used for blocking secondary diffracted light except the primary diffracted light; and the receiving optical fiber module is used for receiving the laser emitted from the second acousto-optic deflector. Therefore, the technical problems that in the prior art, the laser beam splitting function and the laser beam combining function are mutually independent, two kinds of operation cannot be considered in the same device, and real-time regulation and control over the light beam operation mode are lacked are solved.

The application relates to the field of laser micro-nano processing, in particular to a laser micro-nano processing device based on an acousto-optic deflector and a rotating mirror and a use method thereof, which comprises a pulse laser, a mirror group, an acousto-optic deflection module, a signal control unit, a beam splitting module, a rotating mirror and a flat-field focusing lens arranged in sequence; the acousto-optic deflection module comprises a first acousto-optic deflector and a second acousto-optic deflector, the first acousto-optic deflector and the second acousto-optic deflector are orthogonally arranged, the first acousto-optic deflector is arranged in parallel with the rotating shaft of the rotating mirror, the second acousto-optic deflector is arranged in perpendicular to the rotating shaft of the rotating mirror, through the arrangement of the two orthogonally arranged acousto-optic deflectors, the laser beam can be flexibly controlled to be deflected to any position in a rectangular scanning area, and in combination with the polygon rotating mirror, the polygon rotating mirror can be rotated only once along a processing track, the acousto-optic deflector can compensate and fill a processing pattern, and the technical effect that any shape can be realized is achieved.

The invention relates to a mobile laser scanning microscope (100) comprising: a chassis (10) with rollers (12), an optical table (30) connected to the chassis (10) via a vibration damper (20), an upper optical box (40) containing a scanning head (42) with acousto-optical deflectors, a pillar (60) connecting the upper optical box (40) to the optical table (30) and holding it at a distance above therefrom, a stage (31) arranged on the optical table (30), a microscope module (32) arranged above the stage (31) and comprising a microscope objective (33) optically coupled to the scanning head (42) and at least one detector (75a, 75b), at least one laser (35) arranged on the optical table (30), an optical beam path (36) guiding a beam of the at least one laser (35) from the at least one laser (35) through the upper optical box (40) to the objective (33), compartments (17) connected to the chassis (10) below the optical table (30) and housing power supplies (15) and control systems (16) of the microscope (100), and a light barrier system (50) having a cover (52) covering units arranged on the optical table (30).

The invention discloses an ultrashort pulse dynamic regulation and control device and method based on double acousto-optic deflectors, and belongs to the technical field related to laser. The device comprises an acousto-optic deflector group and a 4f optical system, the 4f optical system is formed by biconvex lenses with two times of focal length, and the optical axis is parallel to the horizontal plane; the 4f optical system changes the positive and negative of the symbols of acousto-optic effect group delay dispersion and improves the range of group delay dispersion; the acousto-optic deflector group is composed of two acousto-optic deflectors which are arranged in parallel and in opposite directions, and the two acousto-optic deflectors are located on the two sides of the 4f optical system respectively and are both perpendicular to the optical axis. First polarized light of an input light beam is converted into second polarized light through the first acousto-optic deflector, the second polarized light is converted into first polarized parallel light beams through the 4f optical system and the second acousto-optic deflector, and an output light beam is obtained. The acousto-optic deflector group provides continuously adjustable group delay dispersion and regulates and controls the pulse width of an output light beam. The device is low in cost, is simple to operate, and dynamically regulates and controls the pulse width of the output light beam.

The laser processing system based on the acousto-optic deflector comprises an XYZ motion platform, a laser, an acousto-optic deflection assembly, a galvanometer and a focusing field lens are arranged above the XYZ motion platform, the acousto-optic deflection assembly, the galvanometer and the XYZ motion platform are sequentially arranged along an emergent light path of the laser, and the acousto-optic deflection assembly, the galvanometer and the XYZ motion platform are all electrically connected with a controller. The controller controls the acousto-optic deflection assembly to compensate the movement speed and precision of the galvanometer and the XYZ movement platform in real time. The position of a workpiece to be machined is controlled through the XYZ motion platform, meanwhile, the machining path of a laser beam is modulated through the acousto-optic deflection assembly and the galvanometer, and by means of linkage control among the acousto-optic deflection assembly, the galvanometer and the XYZ motion platform, the acousto-optic deflection assembly compensates the motion speed and motion precision of the XYZ motion platform and the galvanometer in real time; therefore, high-speed and high-precision laser processing without frequent start and stop of the XYZ motion platform and the galvanometer is realized, and the fault rate and the wear rate of frequent start and stop of the XYZ motion platform and the galvanometer are reduced.

The invention relates to the technical field of laser processing, in particular to a method and system for rapidly preparing a micropore array, and the method comprises the following steps: S1, placing a workpiece to be processed on a high-precision three-dimensional motion platform; s2, a laser light path is adjusted, and a laser beam emitted by a laser sequentially passes through a beam shaping system, an acousto-optic deflector and a galvanometer and then is focused on the surface of the workpiece to be machined; s3, the acousto-optic deflector scans according to a pre-edited machining pattern, machining of a single micropore is conducted on the current machining point, and after machining of the single micropore is completed, the galvanometer jumps the laser beam to the next machining point; and S4, the step S3 is repeated until machining of the whole micropore array is completed. The acousto-optic deflector and the galvanometer work cooperatively, the acousto-optic deflector is used for carrying out path scanning according to a pre-edited machining pattern, machining of a single micropore is carried out on a current machining point, and after machining of the single micropore is completed, the galvanometer is used for enabling the laser beam to jump to the next machining point, so that the machining efficiency and the machining effect can be greatly improved; therefore, rapid preparation of the micropore array is realized.

The invention belongs to the technical field of quantum physics and quantum, and particularly relates to an AOD optical tweezers array automatic correction method and system based on a neural network, and the method comprises the following steps: generating an initial AOD optical tweezers array through an acousto-optic deflector; acquiring an image of the initial AOD optical tweezers array, and preprocessing the image; inputting the preprocessed image into a first neural network and a second neural network; calculating a global frequency compensation amount according to the average position deviation and a pre-calibrated frequency-position relation factor; generating an intensity compensation table covering a full frequency domain through an interpolation method based on the intensity gain compensation factors of the optical tweezers; and updating the driving frequency of the AOD according to the global frequency compensation amount, updating the driving amplitude of each channel of the AOD according to the intensity compensation table, and outputting the corrected AOD optical tweezers array. By integrating the neural network model and the closed-loop control process, the full automation of the position and intensity correction of the optical tweezers array is realized.

The invention relates to a scanning device (1) for a light microscope (100) with an acousto-optic deflector (10) for deflecting a first illumination light beam (L1) of a first wavelength and a second illumination light beam (L2) of a second wavelength, which differs from the first wavelength, and a control unit (13) for generating sound waves of a first frequency range and a second frequency range separate from the first frequency range in the acousto-optic deflector (10), wherein the first frequency range and the second frequency range are selected such that the first illumination light beam (L1) is deflected by the sound waves of the first frequency range and the second illumination light beam (L2) is deflected independently of the first illumination light beam (L2) by the sound waves of the second frequency range.as well as a light microscope (100) with the scanning device (1) and a method for deflecting a first and a second illumination light beam (L1, L2).

The invention discloses a laser tracking and pointing control method and device based on an acousto-optic deflector, and the device comprises a pulse laser source, an optical antenna module, an acousto-optic deflection module and a synchronous control module, and comprises the steps: generating narrow-linewidth pulse laser, and splitting the narrow-linewidth pulse laser into intrinsic light and detection light; the synchronous controller applies driving signals with horizontal and vertical deflection frequencies to the acousto-optic deflection module, and after direction driving is stable, the optical antenna module triggers and emits the probe light; after the reflected light reflected by the target object is received, coherent detection is carried out on the reflected light and the intrinsic light, a beat frequency electric signal is generated, the beat frequency electric signal is processed, and existence of the target object is determined; recording deflection frequency (fx1, fy1) when the target object is hit, taking the deflection frequency as reference frequency, and converting the deflection frequency into local scanning taking the reference frequency as the center of a scanning view field; and the reference frequency is tracked and corrected by repeated tracking and aiming.

The invention belongs to the technical field of light spot quality simulation optimization, and provides a light spot quality simulation optimization method based on an acousto-optic deflector and galvanometer cooperative system, and the method comprises the steps: simulating light field distribution in a high-speed motion state in simulation, obtaining a dynamic light spot form in real time, constructing a dynamic light spot intensity matrix, and combining a static light spot form to obtain a dynamic light spot intensity matrix; determining a light spot distortion rate corresponding to the time step length in the high-speed motion state; based on the light spot distortion rate corresponding to the time step length in the high-speed motion state, deviation analysis is carried out, and the distortion risk of the light spots in the high-speed motion state is evaluated; if the distortion risk is high, a control variable method is adopted, and simulation testing is conducted on the synchronous error value of the acousto-optic deflector and the galvanometer in the high-speed motion state; according to the method, accurate quantification and risk pre-judgment of light spot distortion are realized, a basis is provided for synchronization parameter optimization of a high-speed scanning system, and systematic control and reduction of the light spot distortion risk in a high-speed motion state are effectively supported.

The invention discloses a high-frequency three-dimensional laser-induced fluorescence imaging system and method based on an acousto-optic deflector, and relates to the field of laser diagnosis technology and combustion field three-dimensional imaging. By integrating a high-frequency laser technology, an AOD (Argon Oxygen Decarburization) rapid scanning technology and a multi-stage synchronous control algorithm, three-dimensional transient diagnosis and dynamic visualization of a high-temperature and high-pressure combustion field are realized, and a high-precision measurement means is provided for combustion efficiency optimization and pollutant generation mechanism research. According to the technical scheme, the imaging system comprises a high-frequency dye laser module, a light path shaping module, an AOD scanning module and a fluorescence imaging module; the high-frequency dye laser module outputs excitation laser with tunable wavelength; the AOD scanning module comprises an acousto-optic deflector scanning system; the fluorescence imaging module comprises a high-frequency camera arranged towards the combustion chamber and a flame collecting system. According to the invention, a dynamic light path shaping and temperature self-adaption algorithm is developed, and the three-dimensional reconstruction precision of a complex combustion field is improved to 0.1 mm level.

An optical scanner can include a sampler to receive a light beam and provide a sampled light beam including a portion of the light beam, a dispersive element to spectrally disperse the sampled light beam along a dispersion direction, one or more detectors to receive at least a portion of the sampled light beam dispersed along the dispersion direction, one or more acousto-optic deflectors (AODs) configured to deflect the light beam from the sampler, and a controller. The controller can determine a centroid of the sampled light beam dispersed along the dispersion direction based on a signal from at least one of the one or more detectors and generate a drive signal for at least one of the one or more AODs to deflect the light beam from the sampler along a selected deflection angle based on the centroid.

The invention discloses a physical perception compiling method for parallel execution of a neutral atom array and a related device, and belongs to the field of quantum computation.The physical perception compiling method comprises the steps that a hardware plane is divided into two or more hardware subareas capable of being operated in parallel according to the physical independence of an acousto-optic deflector array; converting a to-be-compiled quantum circuit into a graph model, dividing all vertexes in the graph model into communities corresponding to the number of the sub-regions, and performing iterative optimization to generate a local sub-circuit and a global sub-circuit corresponding to the sub-regions; all the sub-lines are input into a solver to be compiled, mathematical constraints are applied in the compiling process, and executable compiling results are output; according to the method, a hardware calculation plane is divided into two or more hardware sub-regions capable of being operated in parallel according to the physical independence of the acousto-optic deflector array, and a global problem is decomposed into a local problem of parallel processing, so that the calculation complexity is greatly reduced, and the compiling speed is increased in order of magnitude.

The present application relates to the field of integrated photonics on chip, more particularly, to a high-efficiency on-chip acousto-optic deflector and a preparation method thereof. The acousto-optic deflector comprises a lithium niobate-silicon nitride heterostructure arranged on a silicon oxide substrate, and the lithium niobate-silicon nitride heterostructure comprises a lithium niobate thin film and a multimode coupler structure formed by silicon nitride. An interdigital transducer capable of exciting acoustic waves is arranged on the lithium niobate thin film. In the present application, the piezoelectric property of lithium niobate and the acousto-optic effect are utilized, the interdigital transducer and the multimode coupler principle in the photonic waveguide are integrated, and the Bragg diffraction is generated by the periodic structure formed by the photons and the acoustic waves, so as to finally realize deflection. The above-mentioned acousto-optic deflector reduces the size of the on-chip acousto-optic deflector, enhances the interaction between phonons and photons, and improves the efficiency. The lithium niobate and silicon nitride materials used are stable in properties, easy to process, and can be realized in large-scale integration on chip.

The present invention relates to a method for scanning an area using a multiphoton laser scanning microscope with an acousto-optic deflector. The method comprises scanning an area of ​​a disk located in an XY plane perpendicular to the optical axis of the microscope objective by applying a frequency drive signal to the deflector, the drive signal having a first term targeting the center of the disk and a second term for scanning the periphery of the disk. The invention also relates to a multiphoton laser scanning microscope with a drive system configured to perform this method.

This invention discloses an axial focusing system, a three-dimensional scanning device, and a scanning method based on an acousto-optic deflector, belonging to the field of laser-related technology. The axial focusing system based on an acousto-optic deflector introduces a defocusing amount that changes with the deflection angle of the acousto-optic deflector through a prism. When the deflection angle of the acousto-optic deflector changes, the propagation distance of the beam in the axial focusing system is altered, thereby changing the effective focal length of the equivalent lens. The axial displacement of the beam waist position of the emitted beam changes according to the defocusing amount. Therefore, by adjusting the driving frequency of the acousto-optic deflector, the deflection angle of the beam by the acousto-optic deflector can be adjusted, thus changing the defocusing amount of the axial focusing system and achieving dynamic and rapid axial focusing of the laser.

The application provides a transmitting module configured to emit a deflectable scanning light beam to a preset field of view range. The transmitting module comprises a light source module, at least one acousto-optic deflection device and a deflection driving module. The light source module is configured to emit a light beam. The at least one acousto-optic deflection device is configured to deflect the light beam. The deflection driving module is configured to output a square wave driving signal to drive the acousto-optic deflection device, and control the deflection angle of the acousto-optic deflection device to the light beam by adjusting the frequency of the square wave driving signal. The application also provides a driving control method of the transmitting module, and an optoelectronic detection device and an electronic device comprising the transmitting module.

The application belongs to the field of quantum physics and quantum technology, and particularly relates to an AOD optical tweezer array automatic correction method and system based on a neural network, comprising the following steps: generating an initial AOD optical tweezer array through an acousto-optic deflector; collecting an image of the initial AOD optical tweezer array and pre-processing the image; inputting the pre-processed image into a first neural network and a second neural network; calculating a global frequency compensation amount according to the average position deviation and a pre-calibrated frequency-position relationship factor; generating an intensity compensation table covering the whole frequency domain through an interpolation method based on the intensity gain compensation factor of each optical tweezer; updating the driving frequency of the AOD according to the global frequency compensation amount, and updating the driving amplitude of each channel of the AOD according to the intensity compensation table, and outputting the corrected AOD optical tweezer array. Through the integration of the neural network model and the closed-loop control process, the position and intensity correction of the optical tweezer array is fully automated.

A programmable multiple-point illuminator for an optical microscope includes a light source and a spatial light modulator (SLM). The modulated light beam can scan across a sample placed under the microscope objective, the sample being provided with fluorophores. The SLM includes a first acousto-optic deflector and a second acousto-optic deflector, the first acousto-optic deflector having a first modulation plane and the second acousto-optic deflector having a second modulation plane, said two acousto-optic deflectors being arranged in cascade. The SLM includes a telescope relay to conjugate the first modulation plane with the second modulation plane. The illuminator includes an arbitrary waveform generator that can synthesize holograms, and is arranged to simultaneously inject a first such hologram into the first acousto-optic deflector and a second such hologram into the second acousto-optic deflector, in order for the SLM to modulate the light beam in response to said holograms.

Provided herein are a method and device for laser ray tracing measurement of intraocular distances and structures. Generally, the device has a laser, pairs of acousto-optical deflectors, drivers, frequency generators, and beam splitters, a telescope and collimating lens, a basic optometric channel and a processing unit arranged and configured to probe an eye with modulated laser beams oriented to cross along optically determinable paths. Analysis of the detectable backscattered radiation is used to confirm the position of a beam cross-point and to calculate the distance thereof to an apex of the cornea. Data obtained from repeated probing is used to reconstruct the intraocular structure of the eye.

The invention is suitable for the technical field of laser processing, and provides a laser processing method, a controller, laser processing equipment and a circuit board. The laser processing method comprises the steps that an initial processing graph corresponding to a target processing structure on a workpiece to be processed is obtained, and the size of the initial processing graph in any linear direction exceeds the laser scanning range of an acousto-optic deflector; according to the laser scanning range of the acousto-optic deflector, the initial processing graph is partitioned and corrected, a plurality of sub-processing graphs are obtained, each sub-processing graph comprises a target laser scanning path, and the size of each sub-processing graph in each linear direction is within the laser scanning range of the acousto-optic deflector; and according to the target laser scanning path in each sub-processing graph, controlling an acousto-optic deflector to deflect the laser beam so as to sequentially process each sub-processing graph on the to-be-processed workpiece to obtain a target processing structure. According to the embodiment of the invention, the laser processing efficiency can be improved.

The invention discloses a method for repairing the tip end of an APU turbine blade through laser cladding. The method comprises the steps that cleaning pretreatment is conducted on a blade defect area; acquiring a thickness distribution model of the blade by utilizing scanning equipment and generating a processing path; the blade is installed to a posture adjusting assembly, cladding process parameters are adjusted in real time based on the thickness distribution model, the laser power is in direct proportion to the section thickness of the blade, and the scanning speed is in inverse proportion to the section thickness; alloy powder and protective gas are conveyed through the powder conveying system and the gas path system, and a local protective atmosphere is formed above the molten pool; a laser cladding head is driven by a translation mechanism to perform cladding layer by layer according to a path, and the geometric dimension and energy density distribution of light spots are adjusted in real time through a built-in acousto-optic deflector and a built-in electro-optic deflector; and finally, cooling, stress relief and quality detection are executed. According to the method, high-quality repairing of the tip of the blade is achieved by precisely and dynamically regulating and controlling laser parameters and light spot forms.

The invention provides a laser three-dimensional engraving machine suitable for superhard material processing. The laser three-dimensional engraving machine comprises a laser head, a focusing lens group, an acousto-optic deflection device, a polyhedral wedge prism group, a galvanometer, a galvanometer deflection motor and a focusing lens, the laser head generates pulse laser; the focusing lens group is used for adjusting a focal plane where a focal point is located after the laser passes through a focusing lens, and etching different height layers of the material; the acousto-optic deflection device linearly deflects the laser and controls the laser to be emitted to different side reflecting surfaces of the wedge-shaped prism at different moments; the polyhedral wedge-shaped prism group is formed by sequentially arranging a plurality of wedge-shaped prisms according to spatial positions, and laser is reflected by the side surfaces of the wedge-shaped prisms to form line scanning; the galvanometer deflection motor drives the galvanometer to deflect the line laser formed after passing through the wedge-shaped prism group, and line scanning line feed is implemented; and the focusing lens focuses the laser deflected by the galvanometer into a focal plane. High-speed ablation of laser on the surface of the hard and brittle material is achieved, heat accumulation is reduced, and the machining precision and efficiency are improved.

The application discloses a mini LED panel windowing system and method based on an acousto-optic deflector. The system comprises a laser, a front beam expander, an acousto-optic deflector, a diffraction plate, a rear beam expander and a galvanometer arranged in sequence along a light path of the laser. The laser is configured to emit a laser beam. The front beam expander is configured to expand the diameter of the laser beam to a required spot size for entering the acousto-optic deflector. The acousto-optic deflector is configured to control the deflection angle of the laser beam. The diffraction plate is configured to block Bragg diffraction light generated by the acousto-optic deflector and allow 0th-order and 1st-order diffraction beams to pass through. The rear beam expander is configured to expand the diameter of the light beam to a required focused spot size. The galvanometer is configured to jump to a next processing position after the acousto-optic deflector deflects by a preset angle.

A laser scanning microscopy system includes a laser whose beam is modified by an acousto-optic deflector that includes an optical element having a surface with one or more steps formed thereon; a conductive layer formed on the surface with the steps; one or more crystals secured to each step; and electrodes positioned on each surface of each crystal.

A device, a computer program, a computer readable medium and a method for controlling focus of a laser beam during a micro sweep are disclosed. The laser beam is received to an acousto-optic deflector, and acoustic waves are provided to the acousto-optic deflector. The acoustic waves are varied in frequency over time to vary a deflection angle of the laser beam over time thereby achieving the micro sweep of the laser beam. Furthermore, a rate of variation in frequency of the acoustic waves is adapted over a time of the micro sweep in such a way that differences in frequencies over the time of the micro sweep of the acoustic waves are caused in the acousto-optic deflector over a width of the laser beam in a direction parallel to the micro sweep when passing through the acousto-optic deflector, where the differences in frequencies over the time of the micro sweep are such that they cause a desired focus of the laser beam in a direction parallel with the micro sweep over the micro sweep.

This utility model relates to the field of atomic manipulation technology in quantum information processing devices, and more particularly to an optical addressing system for a two-dimensional single-atom array, comprising a laser arranged sequentially according to the optical path direction, a pair of orthogonally arranged acousto-optic deflectors, a first lens, a second lens, and a third lens, wherein the acousto-optic deflectors include an acousto-optic deflector (AOD). y Acoustic-optical deflector (AOD) x The acousto-optic deflector (AOD) y Acoustic-optical deflector (AOD) x The input terminals are respectively connected to the output terminals of an arbitrary waveform generator. This invention, through the combination of an acousto-optic deflector and a lens group, enables precise and rapid addressing of two-dimensional single-atom arrays. This invention possesses high stability and scalability, and can be extended to address larger-sized two-dimensional single-atom arrays, making it suitable for future large-scale quantum computing and quantum simulation systems.