311 results about "Spherical aberration" patented technology

The invention provides an all-solid-state high-power single-frequency laser based on an optical fiber-slab mixed structure, and relates to the technical field of solid lasers, and the all-solid-state high-power single-frequency laser comprises an all-solid-state continuous single-frequency seed module, an optical fiber pulse modulation module, an optical fiber pre-amplification module, a slab laser pre-amplification module, a slab laser main amplification module and a frequency multiplication module which are sequentially arranged; the lath laser pre-amplifier and the lath laser main amplifier are used for compensating thermally induced aberration generated by lath laser through multi-pass amplification designed according to the spherical aberration self-compensation principle, and then the quality of light beams is improved. In addition, a discrete mirror group is adopted to replace a complete amplifier cavity mirror, spontaneous radiation and parasitic oscillation in the working process of the amplifier are effectively restrained, nearly hundred mJ-magnitude single-frequency pulse laser with excellent light beam quality can be obtained, and application to laser radar detection or industry can be met.

The application discloses a multi-marked endoscopic imaging lens for digestive tract, and belongs to the field of biomedical microscopic endoscopic imaging. The endoscopic imaging lens comprises a first lens, a second lens, a third lens, a fourth lens, a fifth lens, a sixth lens and a seventh lens; the first lens focuses laser; the second lens is matched with the first lens to limit a light beam in an effective light aperture of the lens; the third lens corrects chromatic aberration; the fourth lens and the fifth lens are combined to correct aberration; the sixth lens adopts an aspheric lens to correct spherical aberration caused in a collimating and focusing system; and the seventh lens is matched with the sixth lens to correct chromatic aberration. The working spectral range of the microscopic objective lens group is 488-860 nm, the effective light aperture is less than 1.8 mm, the mechanical outer diameter is not greater than 2.6 mm, the numerical aperture at the object side or the tissue is 0.55, the imaging field of view is 450 microns, the magnification is 2.14 times, and the working distance is 84 microns. The effect of matching excitation and fluorescence spectrum of a clinically available fluorescence contrast agent is realized.

The invention discloses an aspheric keratoprosthesis lens column, a keratoprosthesis and an application method of the aspheric keratoprosthesis lens column, the whole lens column is cylindrical, the front surface of the lens column is a convex surface, the rear surface of the lens column is a concave surface, the rear surface of the lens column is a surface close to the retina, the front surface of the lens column is a surface far away from the retina, and the front surface and the rear surface of the lens column are both curved surfaces. And the spherical surfaces are rotationally symmetrical aspheric surfaces. The artificial cornea comprises a lens column and a support, and the lens column is installed on the support. The fixed position of the lens column is that the distance between the vertex of the rear surface of the lens column and the retina is 10-120mm, the focal plane is perpendicular to the optical axis, and the inclination angle of the focal plane is 0 degree. According to the lens column, spherical aberration and coma can be effectively corrected, and the imaging quality is improved; light scattering is reduced, the visual contrast at night and in a low-light environment is improved, and the visual experience of a patient is improved; the deviation tolerance of the implantation position is higher, and the operation difficulty and the risk of postoperative complications are reduced.

The invention relates to a large-view-field continuous zooming optical system from visible light to a near-infrared band. The system is sequentially provided with a front fixing group with positive focal power, a zooming group with negative focal power, a compensation group with positive focal power, a rear fixing group with negative focal power and an image plane I in the light propagation direction; wherein the zoom group is composed of a meniscus lens with negative focal power and a doublet lens; and the compensation group consists of a meniscus lens with positive focal power, a meniscus lens with negative focal power and a doublet lens with positive focal power. According to the invention, two groups of doublet lenses in different forms are adopted, a negative lens in one group of doublet lenses is crown glass with low refractive index and high Abbe number, and a positive lens in one group of doublet lenses is flint glass with high refractive index and low Abbe number; and in the other group of glued lenses, the negative lens is flint glass with high refractive index and low Abbe number, the positive lens is crown glass with low refractive index and high Abbe number, and the two types of glued lenses effectively control high-order spherical aberration caused by a large view field, correct field curvature and suppress chromatic aberration caused by a wide spectral range.

The invention discloses a periscope head image difference compensation method and system, a computer and a storage medium, a periscope head comprises a reflecting prism, a lens group and a diffractive optical element, and the non-reflecting surface of the reflecting prism is provided with a polarization coating; the method comprises the following steps: constructing an optical path model according to design requirements of a periscope lens module, and carrying out aberration analysis on the optical path model; calculating a chromatic aberration compensation phase function of the diffractive optical element according to a chromatic aberration compensation formula; calculating a spherical aberration compensation phase function of the diffractive optical element according to a spherical aberration expansion formula; and calculating a total phase function of the diffractive optical element, and performing aberration compensation on the optical path model according to the total phase function. According to the long-focus periscope lens module, the total aberration of the periscope lens module can be compensated by utilizing the cooperation of the diffractive optical element and the reflecting prism with the polarization coating, so that the size of the long-focus periscope lens module is reduced, and the imaging quality of the long-focus periscope lens module is improved.

The invention relates to the technical field of microscopic optical imaging, and discloses a semiconductor conductive particle detection task-oriented differential interference optical system, which comprises an objective lens group and a differential interference module, the objective lens group comprises a front group, a middle group and a rear group which are arranged in sequence; the front group is used for ensuring a large aperture angle and less introduction of spherical aberration and chromatic aberration, the middle group is used for compensating various aberrations introduced by the front group, and the rear group is used for correcting field curvature; the differential interference module comprises a Nomarski prism, a polarizer and an analyzer which are arranged in sequence; the Nomarski prism is used for splitting and combining the linearly polarized light beams; the polarization analyzer is used for converting linearly polarized light which passes through the Nomarski prism and is orthogonal in polarization direction into linearly polarized light with the same polarization direction; the system further comprises a beam splitter and a barrel lens group. According to the invention, long working distance and large numerical aperture can be realized in the visible light wave band, the light path design is optimized so as to reduce aberration introduction, and the anti-interference capability to weak signals is enhanced.

The utility model provides a high-resolution spectral confocal measurement device, which includes a light source, a fiber coupler, a spectral confocal lens, a spectral analysis unit and a data processing unit. The spectral confocal lens is arranged between the fiber coupler and the sample to be measured. The spectral confocal lens includes a first lens, a second lens, a third lens, a fourth lens, a fifth lens and a sixth lens arranged in sequence. The first lens is a double concave lens, the second lens is a meniscus lens, the third lens is a plano-convex lens, the fourth lens is a double-cemented lens, the fifth lens is a meniscus lens, and the sixth lens is a meniscus lens. With such an arrangement, the spectral confocal lens is improved from multiple aspects such as expanding the incident light beam, correcting aberrations, reducing spherical aberrations, and correcting coma and chromatic aberration, thereby greatly improving the resolution of the lens. The light source is further connected to the spectral confocal lens through a fiber coupler, so that the entire device has a compact structure and is easy to integrate and install.

The invention relates to a 1.2-inch intelligent traffic monitoring system lens and a working method thereof. An optical imaging system of the lens is sequentially provided with a first lens to a fourteenth lens from an object space to an image space. Wherein the focal power of each lens adopts a positive and negative combined form, so that optical aberrations such as spherical aberration and the like are greatly reduced. Wherein the fourth lens and the fifth lens form an achromatic doublet lens group, the seventh lens and the eighth lens form an achromatic doublet lens group, the ninth lens and the tenth lens form an achromatic doublet lens group, and the eleventh lens, the twelfth lens and the thirteenth lens form an achromatic triplet lens group. Through reasonable lens matching, an optical system realizes large aperture, large target surface and no defocus in day and night, and through good correction of on-axis and off-axis aberrations, the lens has good imaging quality.

The invention relates to a microlens array spherical aberration correction method based on a high-order linear ordinary differential equation. The problem that an existing microlens array spherical aberration correction method is poor in microlens array spherical aberration correction effect is solved. The method comprises the following steps: firstly, establishing a high-order linear ordinary differential equation used for describing a single-lens light propagation path in a micro-lens array, and introducing a non-constant coefficient function; based on a set initial condition and the obtained pixel initial coordinates of the element image array, solving a simultaneous equation of the light field space geometrical relationship and a high-order linear ordinary differential equation by utilizing a formulation reduced-order iterative numerical solution algorithm to obtain an aberration matrix of the element image array; and feeding back the aberration matrix to a spatial function of the element image array mapped to the light field, and changing the pixel horizontal coordinate and vertical coordinate positions of the corresponding element image according to the distance from the pixel point to the optical axis of the corresponding lens to complete the spherical aberration correction of the microlens array. According to the invention, the spherical aberration correction capability of the integrated imaging system can be improved, and the stereo imaging quality is improved.

The invention provides an optical system and electronic equipment. The optical system comprises a lens group, the lens group comprises a first lens group, a second lens group and a third lens group, and the first lens group comprises a first lens, a second lens, a third lens, a fourth lens and a fifth lens; the second lens group comprises a sixth lens, a seventh lens, an eighth lens, a ninth lens and a tenth lens; the third lens group comprises an eleventh lens, a twelfth lens, a thirteenth lens and a fourteenth lens; fG1 / f is more than-1.40 and less than-0.60; -4.50 < = F1112 / F1314 < =-1.40; fG2 / FG3 is more than 1.00 and less than 3.05; fG1 is the combined focal length of the first lens group, f is the effective focal length of the optical system, F1112 is the combined focal length of the eleventh lens and the twelfth lens, F1314 is the combined focal length of the thirteenth lens and the fourteenth lens, FG2 is the combined focal length of the second lens group, and FG3 is the combined focal length of the third lens group. The optical system effectively corrects spherical aberration, reduces the sensitivity of the optical system, and facilitates the realization of compactness and miniaturization.

The utility model discloses bionic compound eye type mine displacement monitoring special equipment, which relates to the technical field of mine safety monitoring, and comprises a shell, the shell is composed of a plurality of groups of sensing surfaces and a plurality of groups of supporting nodes, a three-ring optical system is integrated on each sensing surface, and the bottom of the shell is provided with a tenon-and-mortise quick-release interface matched with the sensing surfaces for use. The shell is in the shape of a truncated icosahedron hemisphere, the sensing face is in the shape of a regular hexagon, and the supporting nodes are in the shape of a regular pentagon. According to the utility model, the horizontal field of view is expanded to 270 degrees and the vertical field of view reaches 120 degrees through the eccentric prisms, the 4 * 4 microprism aberration correction array dynamically compensates wide-angle distortion, the microlenses employ gradient refraction design to correct spherical aberration and field curvature, light is focused into 1.2 [mu] m light spots which are matched with the photonic crystal waveguide mode field diameter, and the adjacent microlens fields of view overlap 40%. The FPGA is fused with multi-channel data, so that the signal-to-noise ratio is increased to 40dB +, accurate acquisition and processing of light are ensured, high-precision three-dimensional deformation monitoring is realized, and fine change conditions of mine rock strata can be captured.

The invention provides a multi-focus pulse light beam parallel processing method and system based on space beam splitting, and relates to the technical field of semiconductor material laser processing, and the method comprises the steps that a laser generator emits pulse laser to a SiC crystal ingot; the light path adjusting unit performs beam splitting and modulation on the pulse laser to obtain multiple beams of sub-pulse laser; the spatial light modulator performs spherical aberration compensation on the multiple beams of sub-pulse laser, performs phase modulation on the sub-pulse laser by adopting a hologram method to generate various target light fields, and modulates the target light fields in real time by switching holograms to obtain multi-focus pulse laser; the laser processing head unit is used for focusing multi-focus pulse laser in the SiC crystal ingot to set the depth; and the motion base station controls the SiC crystal ingot and the multi-focus pulse laser to perform relative motion and adjusts the relative position between the SiC crystal ingot and the laser processing head unit, scanning processing of the SiC crystal ingot is completed on a preset depth and a preset advancing route, and finally a processed wafer is obtained.

The invention discloses an aspheric objective lens for a micro-jet laser processing head, and belongs to the field of micro-jet laser equipment, the processing head comprises a window, a water cavity and a spray head, the spray head comprises a spray hole, the aspheric objective lens, the window, the water cavity and the spray head are sequentially arranged along the optical axis direction of the aspheric objective lens, and the aspheric objective lens is used for focusing laser into the water cavity and the spray hole; the aspheric objective lens comprises a meniscus positive lens and a plano-convex aspheric positive lens which are coaxially arranged in sequence, laser is converged by the meniscus positive lens and then enters the plano-convex aspheric positive lens, and the laser is converged by the plano-convex aspheric positive lens and then penetrates through the water cavity to enter the spray hole; the surface, facing the meniscus positive lens, of the plano-convex aspheric positive lens is an even-order aspheric surface, and the surface, facing the window piece, of the plano-convex aspheric positive lens is a plane, so that the spherical aberration of the aspheric objective lens can be reduced, and the laser processing effect is improved.

An aberration-free laser spot scanning apparatus, comprising a resonant scanner (1), a first concave mirror (2), a second concave mirror (3), an X-axis galvanometer scanning mirror (4), a third concave mirror (5), a fourth concave mirror (6) and a Y-axis galvanometer scanning mirror (7) which are sequentially arranged in the direction of light beam propagation. Compared with existing laser spot scanning apparatuses that generally use a lens as an optical relay element between scanning mirrors, replacing the lens with a concave mirror to complete optical relay between scanning mirrors can avoid spherical aberration in a focusing transmission element, while also reducing the optical power loss generated by light transmission through a glass element, so that the aberration-free laser spot scanning apparatus can be applied to an optical microscopic imaging (e.g., laser confocal and two-photon imaging) system.

The invention discloses an off-axis paraboloid mirror image difference correction high-resolution C-T type spectrum detection method and device, and belongs to the technical field of spectrum imaging and detection. The collimating mirror and the convergent mirror are off-axis parabolic mirrors. The off-axis parabolic mirror is used for correcting the spherical aberration of the spectrometer; suppressing and correcting coma of the spectrometer by using the off-axis angles of the collimating mirror and the convergent mirror and focal length symmetric structure parameters; the field curvature of the spectrograph is corrected by calculating the optimal grating position; performing linear array integral detection on the convergent light by using a small-pixel deep refrigeration array detector; by combining high and low density gratings, the gratings are switched under the application requirements of different wave band ranges, resolving power and scanning speed, and rapid light splitting detection from ultraviolet to infrared broadband is realized; high-precision grating rotary scanning and angle monitoring are utilized, and large-range spectral broadband and high-resolution detection is realized through spectral line splicing. According to the invention, wide-spectrum, high-resolution and high-sensitivity rapid detection of Raman, infrared, emission, absorption and other spectral signals can be realized.

The invention provides an optical lens, which comprises six lenses in total, and sequentially comprises a first lens with negative focal power, a second lens with negative focal power, a third lens with negative focal power, a fourth lens with negative focal power, a fifth lens with negative focal power and a sixth lens with negative focal power from an object plane to an imaging plane along a light transmission direction, the object side surface of the second lens is a convex surface; the object side surface of the third lens is a convex surface, and the image side surface of the third lens is a convex surface; the object side surface of the fourth lens is a concave surface, and the image side surface of the fourth lens is a concave surface; the fifth lens has positive focal power, and the image side surface of the fifth lens is a convex surface; the sixth lens has focal power, the object side surface of the sixth lens is a concave surface, and the image side surface of the sixth lens is a concave surface near the optical axis; the object plane, the main plane of the optical lens and the imaging plane intersect at a line. According to the optical lens provided by the invention, through reasonable matching of the focal power and the surface type of each lens, spherical aberration and trapezoidal distortion can be effectively corrected, and the imaging quality is greatly improved.

The invention discloses a multi-label endoscopic imaging lens for a digestive tract, and belongs to the field of biomedical microscopic endoscopic images. The endoscopic imaging lens comprises a first lens, a second lens, a third lens, a fourth lens, a fifth lens, a sixth lens and a seventh lens. The first lens focuses laser, and the second lens is matched with the first lens to limit a light beam in an effective clear aperture of the lens; the third lens corrects chromatic aberration; a fourth lens and a fifth lens are combined to correct aberration; the sixth lens is an aspheric lens and corrects spherical aberration brought in collimation and focusing systems, and the seventh lens is matched with the sixth lens to correct chromatic aberration. The working spectral range of the microscope objective set is 488-860 nm, the effective clear aperture is smaller than 1.8 mm, the mechanical outer diameter is not larger than 2.6 mm, the numerical aperture at the object space or the tissue is 0.55, the imaging view field is 450 microns, the magnification factor is 2.14 times, and the working distance is 84 microns. And the effect of matching excitation and fluorescence spectrum of a clinically available fluorescence contrast agent is realized.

The invention discloses a miniaturized large-target-surface low-distortion aerial photographing lens and module. The aerial photographing lens comprises a first lens, a second lens, a third lens, a fourth lens, a fifth lens, a sixth lens, a diaphragm, a seventh lens, an eighth lens, a ninth lens, a tenth lens, an eleventh lens, a twelfth lens, a thirteenth lens, a fourteenth lens and a fifteenth lens which are sequentially arranged from the object side to the image side along the optical axis. Through reasonable lens structure design and curvature radius control, excellent low distortion performance is realized, and the geometric accuracy of an image is ensured. The design of fifteen lenses is adopted, sufficient design freedom is provided, various aberrations such as spherical aberration are effectively corrected, high resolution is achieved, and a large-target-surface photosensitive element is matched; through focal power distribution and aberration correction, the imaging effect of an edge field of view is remarkably improved, and the definition consistency of the center and the edge of a picture is ensured.

The invention relates to the technical field of optical imaging, and discloses an automatic aberration correction system and method for remote sensing light field imaging, and the method comprises the steps: constructing an aberration sensitive feature set through dynamic projection coding and multispectral synchronous collection, and improving the aberration perception capability of a complex scene in combination with polarized light information; establishing a three-dimensional aberration field model based on a light field gradient decomposition and multi-focal length coupling model; calculating an optimal focusing parameter and a digital phase compensation mask in combination with physical driving optimization and data driving compensation; and dynamic adaptive correction is realized based on real-time aberration monitoring and light field entropy minimization optimization. According to the method, aberration such as spherical aberration, coma aberration and curvature of field can be effectively inhibited, and the resolution and depth estimation precision of remote sensing light field imaging are improved.

A first lens group comprises at least two balsaming lenses, and a first lens is used for correcting partial spherical aberration and partial field curvature of the dual-waveband confocal microscope objective; the second lens group comprises at least one balsaming lens and is used for receiving the light beams from the first lens group and correcting partial spherical aberration and partial chromatic aberration of the dual-band confocal microscope objective; the third lens group comprises at least three independent lenses, and is used for converging the light beams from the first lens group and the second lens group and correcting the residual spherical aberration of the dual-band confocal microscope objective; and the lenses in the first lens group, the second lens group and the third lens group are coaxially arranged in sequence along an optical axis. Compared with an existing product, the dual-waveband confocal microscope objective has the advantages of being dual-waveband confocal, high in resolution, long in working distance, large in view field range and the like.

The application discloses a large-view-field object-side telecentric projection imaging method and a lens for a vehicle lamp. Incident light rays are converged through two large-aperture meniscus lens; the converged light rays are reduced in size and aberration through a double cemented lens group composed of a first negative double-concave lens and a first positive double-convex lens; the light rays are further converged through a second negative meniscus lens, so that the light rays all enter a diaphragm; chromatic aberration is corrected through three cemented lenses, and aberration is further reduced, and a spherical aberration can be corrected since the aperture diaphragm is located on the object side of the three cemented lenses; the light path is further converged through two double-convex lens groups, and distortion is reduced, the light rays enter a TIR total reflection prism, pass through a protective glass, and are clearly imaged on a DMD image plane. The imaging method provided by the application can realize object-side telecentric projection imaging under a large view field through the cooperation of conditional expressions and positive and negative focal lengths between the lenses, and the imaging is high in definition.

The embodiment of the utility model provides a wide-angle lens, a shooting device and a movable platform. The wide-angle lens comprises a first lens group with negative focal power, a reflection optical element and a second lens group with positive focal power which are sequentially arranged from an object side to an image side along an optical axis, the first lens group comprises at least two negative lenses, the second lens group comprises at least five lenses, and the wide-angle lens satisfies the following conditions: 14lt; tTL / flt; 17; 90 degree lt; omega; wherein TTL is the distance on the optical axis from the object side surface of the lens closest to the object side to the imaging surface when an infinite object is focused, f is the overall focal length of the wide-angle lens, and omega is the maximum angle of the incident light of the lens closest to the object side. According to the embodiment of the utility model, the occurrence risk of ghosting and glare can be reduced, the spherical aberration can be well corrected, the lens size miniaturization can be realized while a larger field angle is ensured, and the imaging quality can be improved.

Embodiments of the present application provide an optical system for laser cutting, a laser processing device and a method. The optical system comprises, in sequence along an optical path direction, a laser, a beam processing element, a spherical aberration compensation assembly and an objective lens, wherein the laser is configured to emit a laser beam; the beam processing element is configured to process the laser beam to obtain a predetermined number of sub-beams; the spherical aberration compensation assembly comprises a predetermined number of sub-spherical aberration compensation elements, the predetermined number of sub-spherical aberration compensation elements correspond to the predetermined number of sub-beams one by one, and each sub-spherical aberration compensation element is configured to compensate the spherical aberration of the sub-beam passing through the corresponding sub-spherical aberration compensation element; and the sub-beams compensated by the sub-spherical aberration compensation elements are focused by the objective lens to form a burst point at a predetermined position of the processed object. The technical solution can obtain a better cutting effect with fewer cutting times or cutting layers, thereby effectively improving the efficiency of laser cutting.

The invention discloses an aspheric objective lens for a micro-jet laser processing head, belonging to the field of micro-jet laser equipment. The processing head comprises a window, a water cavity and a nozzle, and the nozzle comprises a nozzle. The aspheric objective lens, the window, the water cavity and the nozzle are arranged in sequence along the optical axis direction of the aspheric objective lens. The aspheric objective lens is used to focus laser light into the water cavity and the nozzle. The aspheric objective lens comprises a meniscus positive lens and a plano-convex aspheric positive lens which are arranged coaxially in sequence. After being converged by the meniscus positive lens, the laser light enters the plano-convex aspheric positive lens, and after being converged by the plano-convex aspheric positive lens, the laser light passes through the water cavity and enters the nozzle. The surface of the plano-convex aspheric positive lens facing the meniscus positive lens is an even aspheric surface, and the surface of the plano-convex aspheric positive lens facing the window is a plane, thereby reducing the spherical aberration of the aspheric objective lens and improving the processing effect of laser processing.

The embodiment of the present application provides an optical telescopic device and a multi-pupil eyepiece structure, the multi-pupil eyepiece structure comprises a first lens group with positive focal length, a second lens group with negative focal length and a third lens group with positive focal length arranged in sequence from an eye observation position to an imaging surface; the first lens group comprises a first lens for converging light; the second lens group comprises a second lens for compensating spherical aberration caused by the first lens group; the third lens group comprises a third lens with positive focal length and a fourth lens with negative focal length, the third lens is used for converging light, and the fourth lens is used for balancing residual aberration; the first lens, the second lens, the third lens and the fourth lens can meet imaging under different exit pupil conditions in multiple configurations.

The application discloses a kind of aberration correction method and device under high numerical aperture objective lens two-photon lithography, and it is related to micro-nano manufacturing and laser processing technical field.The method comprises the following steps: establishing the two-photon lithography system parameter model for aberration correction;According to the preset target focal point distribution, the focal point phase to be loaded into spatial light modulator is calculated using GS algorithm;Calculate depth-dependent aberration and generate compensation phase;Superimpose total loading phase and generate SLM hologram;Adjust objective lens to make it align with the sample on translation stage, make immersion oil and sample surface closely contact, complete the immersion alignment of objective lens and sample;Make sample and focal point produce relative displacement, complete two-photon lithography processing under the condition of spherical aberration compensation;After processing after exposure sample, obtain three-dimensional microstructure with different depth voxel.The method can improve the consistency and forming quality of deep three-dimensional micro-nano processing.

The present application relates to the technical field of optical instruments, and discloses a microscope objective, which is suitable for at least a temperature environment of 50K to 150K and comprises: a front group unit, which comprises at least a first lens and a second lens arranged in sequence along an optical path, and is suitable for converging light rays and correcting spherical aberration; a middle group unit, which is arranged on the rear side of the optical path of the front group unit, comprises at least a first middle group and a second middle group, and is arranged in sequence along the optical path, each middle group is provided with at least two lenses arranged at intervals, and is suitable for correcting chromatic aberration; and a rear group unit, which is arranged on the rear side of the optical path of the middle group unit and comprises at least two lenses arranged at intervals; each lens contained in the front group unit, the middle group unit and the rear group unit is a single lens. By arranging each lens as a single lens, the combination connection of each unit and the whole microscope objective is avoided, the problems of damage, falling or air leakage in an extreme environment such as low temperature are avoided, and the application in a low-temperature environment is met.

This invention relates to the field of AR device technology, providing an AR optical lens and an AR device. The lens includes a first lens, a second lens, a third lens, a fourth lens, and a fifth lens arranged sequentially along the optical axis from the object side to the image side. The first lens has positive optical power, with a convex surface on the object side and a concave surface on the image side; the second lens has positive optical power, with a convex surface on the object side and a concave surface on the image side; the third lens has negative optical power, with both the object side and the image side being concave; the fourth lens has positive optical power, with a concave surface on the object side and a convex surface on the image side; and the fifth lens has negative optical power, with a concave surface on the object side and a convex surface on the image side. All lenses are aspherical lenses. This invention, through a positive-positive-negative-positive-negative optical power arrangement of lenses, can simultaneously correct various aberrations such as spherical aberration, field curvature, and distortion, effectively achieving a large field of view, low distortion, and high resolution imaging effect, enhancing the immersiveness and clarity of AR displays.

The application discloses a machining head for microjet laser processing, and relates to the technical field of microjet laser processing. The machining head comprises an objective lens, a window sheet, a water cavity and a nozzle, and the objective lens, the window sheet, the water cavity and the nozzle are coaxially arranged in sequence along a first direction. The objective lens comprises a lens barrel and first double cemented lenses, second double cemented lenses and a positive meniscus lens which are coaxially arranged in sequence in the lens barrel. The lens barrel comprises a first port and a second port, and the first direction is the direction from the first port to the second port. The spherical aberration generated by the combination of the first double cemented lenses, the second double cemented lenses, the positive meniscus lens and the window sheet satisfies a first preset range, and the chromatic aberration generated satisfies a second preset range. Thus, the chromatic aberration of blue light and green light can be corrected, and the applicability of the objective lens is improved.

The present invention relates to a method for correcting a spherochromatic aberration that occurs when examining a sample with a microscope. The microscope comprises an objective lens and a corrective device arranged in a beam path of the microscope for correcting a spherical aberration. According to the method, data for describing the spherical aberration as a function of a wavelength of light imaged by the microscope are provided. A sample is examined with the microscope, and at least one spectral range of the light imaged by the microscope is determined.A control parameter of the correction device is determined based on the provided data describing the spherical aberration as a function of wavelength for the at least one determined spectral range, in order to minimize the spherical aberration for the at least one determined spectral range. The correction device is then set to the determined control parameter. The invention further relates to a microscope, which is in particular a light microscope.