Patent classifications
G01N2201/0635
System and method for synchronized fluorescence capture
A system and method for high resolution multi-fluorescence imaging with synchronized image acquisition amongst sensors can be used to simultaneously capture fluorescence signals from multiple fluorophores over extremely large fields of view. The system can include an array of micro-cameras, along with a particular arrangement of fluorescent filters that can be fixed in one location or moved to new locations.
SPECTRAL CONFOCAL MEASUREMENT DEVICE AND MEASUREMENT METHOD THEREOF
A spectral confocal measurement device includes a light source portion, configured to emit a broad-spectrum light beam with a certain wavelength range in a first predetermined path; an optical sampling portion, configured to converge the broad-spectrum light beam emitted from the light source portion on different measurement surfaces of an object to be measured, and output a reflected light in a second predetermined path that is different from a reverse direction of the first predetermined path; and a measurement portion, configured to receive and process the reflected light from the optical sampling portion to obtain a measurement result. The device can improve measurement accuracy and reduce production costs. In addition, a spectral confocal measurement method is also provided.
SYSTEMS AND METHODS FOR STRUCTURED ILLUMINATION MICROSCOPY
The technology disclosed relates to structured illumination microscopy (SIM). In particular, the technology disclosed relates to capturing and processing, in real time, numerous image tiles across a large image plane, dividing them into subtiles, efficiently processing the subtiles, and producing enhanced resolution images from the subtiles. The enhanced resolution images can be combined into enhanced images and can be used in subsequent analysis steps.
High-throughput hyperspectral imaging systems
High-throughput hyperspectral imaging systems are provided. According to an aspect of the invention, a system includes an excitation light source; an objective that is configured to image excitation light onto the sample, such that the excitation light causes the sample to emit fluorescence light; a channel separator that is configured to separate the fluorescence light into a plurality of spatially dispersed spectral channels; and a sensor. The excitation light source includes a light source and a plurality of lenslet arrays. Each of the lenslet arrays is configured to receive light from the light source and to generate a pattern of light, and the patterns of light generated by the lenslet arrays are combined to form the excitation light. The objective is configured to simultaneously image each of the patterns of light to form a plurality of parallel lines or an array of circular spots at different depths of the sample.
OPTICAL DISCRIMINATION APPARATUS AND METHODS ADAPTED TO MONITOR REACTIONS
An optical discrimination apparatus adapted for use in PCR testing and the like. The apparatus includes a multi-color light emitter to emit excitation light, a sample holder configured to hold dye-marked nucleic acid fragments in a PCR solution at a position configured to receive the excitation light along a first direction, light emission collection optics configured to collect scattered excitation light and light emission (fluorescent emission) from the sample holder along a second direction that is approximately orthogonal to the first direction, a spectrally-dispersive element configured to spectrally disperse scattered light and emission light, and a spectral detector configured to receive the separated emission light and excitation light on different photosites of the spectral detector. Systems and methods are provided, as are other aspects.
ETALON MID-INFRARED PROBE FOR SPECTROSCOPIC TISSUE DISCRIMINATION
An etalon-based mid-infrared probe can be configured for spectroscopic tissue discrimination, such as between non-normal (e.g., cancerous) and normal (e.g., healthy) tissue. A broadband light source can be applied to the etalon to generate fringes at spectroscopic wavelengths of interest, which can be delivered to a tissue specimen via a fiber loop probe. A response signal can be spectral dispersed across a parallel array of detector pixels, such as using a diffraction grating, and signal processed for performing the tissue classification. A learning model can be trained, using full IR spectral data, for applying a reduced set of wavelengths for performing the spectroscopic tissue analysis and classification.
Metrology methods and optical schemes for measurement of misregistration by using hatched target designs
A metrology system configured to measure overlay errors on a sample is disclosed. The metrology system measures overlay error on the sample in a first direction and/or a second direction simultaneously or sequentially. The metrology system comprises an illumination sub-system configured to illuminate a hatched overlay target on the sample with one or more illumination lobes. The metrology system further comprises an objective lens and a detector at an image plane configured to image the hatched overlay target. A controller is configured to direct illumination source to generate the illumination lobes, receive images of the hatched overlay target, and calculate the overlay errors between a first layer of the sample and a second layer of the sample.
MULTI-TRACK RAMAN WELL PLATE READER
A microplate reader simultaneously obtains Raman measurements from samples contained in non-adjacent wells. At least two Raman probes are positioned perpendicularly above or below the microplate to simultaneously acquire Raman spectra data of the non-adjacent liquid samples. Each probe is coupled to a laser and a spectrometer and includes a lens focusing laser light within the sample and collecting light from the sample for the spectrometer. The spectrometer may include a 2D imaging sensor (sCMOS or CCD) to image light from multiple probes simultaneously, spaced from one another to reduce crosstalk. A positioner moves the microplate plate or probes to acquire data from a different subset of non-adjacent samples, and may also vary laser focus within wells during data acquisition. Multiple fluorescence probes may simultaneously acquire fluorescence data from the same samples, or non-adjacent samples. Probes may be fiber-coupled and positioned within a reaction chamber of a liquid handling system.
3D REFRACTIVE INDEX TOMOGRAPHY AND STRUCTURED ILLUMINATION MICROSCOPY SYSTEM USING WAVEFRONT SHAPER AND METHOD THEREOF
An ultra-high-speed 3D refractive index tomography and structured illumination microscopy system using a wavefront shaper and a method using the same are provided. A method of using an ultra-high-speed 3D refractive index tomography and structured illumination microscopy system that utilizes a wavefront shaper includes adjusting an irradiation angle of a plane wave incident on a sample by using the wavefront shaper, measuring a 2D optical field, which passes through the sample, based on the irradiation angle of the plane wave, and obtaining a 3D refractive index image from information of the measured 2D optical field by using an optical diffraction tomography or a filtered back projection algorithm.
Scanning luminescence light microscope with gratings of luminescence inhibition light and further light
A scanning luminescence light microscope for spatial high resolution imaging a structure marked with a luminescent marker comprises a light source for luminescence inhibition light and for further light; a light shaping and aligning device; and a detector registering luminescence light emitted by the luminescent marker. The device, by means of two optical gratings and an objective lens, forms two crossing line gratings of the luminescence inhibition light, and two crossing line gratings of the further light so that local intensity minima of an overall intensity distribution of the luminescence inhibition light are delimited in at least two directions, and that local intensity maxima or local intensity minima of an overall intensity distribution of the further light coincide with the local intensity minima of the luminescence inhibition light. Further, the device moves the overall intensity distributions of the further light and the luminescence inhibition light to scan the structure.