Abstract:
Method for the operation of a laser scanning microscope. The microscope includes an illumination beam path in which at least one illumination light source is arranged, a detection beam path in which at least one photomultiplier (PMT) is incorporated as detector, and a control unit for controlling fluorescence experiments. A sample is alternately illuminated at high intensity via the control unit, and the fluorescence decay behavior of sample points and/or sample regions is subsequently detected. The PMT is switched on and off depending on the illumination mode by the control unit via a switch directly in the high-voltage supply of the PMT.
Abstract:
An excitation light source emits excitation light to a target sample. An image sensor includes pixels arranged one-dimensionally or two-dimensionally, and receives measurement light from the sample according to the excitation light. A polarization selector arranged between the sample and image sensor includes pixels arranged one-dimensionally or two-dimensionally. Each pixel receives a corresponding portion of the measurement light, selects light having a polarization direction that corresponds to a driving signal applied to the pixels, and supplies this light to the image sensor. A measurement control unit supplies the cyclic driving signal having a first period T1 and acquires data I1, I2, I3, and I4 from each pixel of the image sensor for each exposure time segment T2=T1/4 obtained by dividing the first period T1 by 4.
Abstract:
Provided is a polarization analysis apparatus that can quickly measure the polarization properties of a sample. The polarization analysis apparatus includes a light source configured to emit light in a predetermined wavelength region, a polarizer configured to transmit the light emitted from the light source, a spatial phase modulator configured to transmit the light from the sample, an analyzer configured to transmit the light that has passed through the spatial phase modulator, and an imaging spectrometer configured to receive the light that has passed through the analyzer. The spatial phase modulator is formed of a birefringent material, and is configured to have different phase differences at respective positions in a first direction in a plane orthogonal to an optical axis. The imaging spectrometer disperses the received light in a second direction that is different from the first direction in the plane orthogonal to the optical axis.
Abstract:
A method for measuring a sample to identify a chemical includes receiving respective spectra for each of a plurality of chemicals. Using a processor, a plurality of binary mathematical filters are computed using the received spectra. A spatial light modulator is adjusted according to a selected mathematical filter. Light that has interacted with the sample is dispersed over the surface of the spatial light modulator, so that the spatial light modulator provides light at wavelengths corresponding to the selected mathematical filter. The light provided by the spatial light modulator is measured to provide a score corresponding to the selected mathematical filter. Filter scores are combined to determine a chemical amount. The processor can operate detection apparatus having a light source, an objective for focusing source light onto the sample, a spatial light modulator, and a detector for detecting the modulator output.
Abstract:
An imaging system includes a light source configured to illuminate a target and a camera configured to image light responsively emitted from the target and reflected from a spatial light modulator (SLM). The imaging system is configured to generate high-resolution, hyperspectral images of the target. The SLM includes a refractive layer that is chromatically dispersive and that has a refractive index that is controllable. The refractive index of the refractive layer can be controlled to vary according to a gradient such that light reflected from the SLM is chromatically dispersed and spectrographic information about the target can be captured using the camera. Such a system could be operated confocally, e.g., by incorporating a micromirror device configured to control a spatial pattern of illumination of the target and to modulate the transmission of light from the target to the camera via the SLM according to a corresponding spatial pattern.
Abstract:
Interferometric focusing (IF), rather than conventional geometric focusing, of excitation light onto a guide-star that is embedded deeply in tissue, increases its fluorescence intensity. The method can extend the depth of wavefront measurement and improve correction inside of tissues because of its ability to suppress both scattering of diffuse light and aberration of ballistic light. The results showed more than two times improvement in SNR and RMS error of the wavefront measurement. Although only ballistic light in the excitation path is corrected, the intensity after wavefront correction increased by 1.5 times. When applying IF to a two-photon microscope with a near infra-red laser, this method would further extend the measurement depth and achieve high SNR for the wavefront sensor.
Abstract:
A method of imaging a fluorescent sample includes the steps of: scanning fluorescent points of the sample using a scanner apparatus, thereby obtaining scanned fluorescent points; and imaging the scanned fluorescent points on a display, the scanning including the steps of predefining a scan field for the sample, which includes a set of scannable fluorescent points; and sequentially irradiating, at least one first subset of points of the set of points and at least one second subset of the set of points, which complements the first subset with respect to the set of points. The first and second subsets can be irradiated at different focal irradiation distances.
Abstract:
In an illumination system (12, 13) for a scatterometer, first and second spatial light modulators lie in a common plane and are formed by different portions of a single liquid crystal cell (260). Pre-polarizers (250) apply polarization to first and second radiation prior to the spatial light modulators. A first spatial light modulator (236-S) varies a polarization state of the first radiation in accordance with a first programmable pattern. Second spatial light modulator (236-P) varies a polarization state of the second radiation accordance with a second programmable pattern. A polarizing beam splitter (234) selectively transmits each of the spatially modulated first and second radiation to a common output path, depending on the polarization state of the radiation. In an embodiment, functions of pre-polarizers are performed by the polarizing beam splitter.
Abstract:
Interferometric focusing (IF), rather than conventional geometric focusing, of excitation light onto a guide-star that is embedded deeply in tissue, increases its fluorescence intensity. The method can extend the depth of wavefront measurement and improve correction inside of tissues because of its ability to suppress both scattering of diffuse light and aberration of ballistic light. The results showed more than two times improvement in SNR and RMS error of the wavefront measurement. Although only ballistic light in the excitation path is corrected, the intensity after wavefront correction increased by 1.5 times. When applying IF to a two-photon microscope with a near infra-red laser, this method would further extend the measurement depth and achieve high SNR for the wavefront sensor.
Abstract:
Method of fluorescence imaging including: illuminating a sample to excite its fluorescence and acquiring an image thereof; based on fluorescence spectral and spatial information from the sample's fluorescence image, segmenting the image into regions of similar spectral properties; for each image segment, exciting the fluorescence of the corresponding sample region, and detecting the corresponding fluorescence; based on modelling, determining expected fluorescence parameters from the fluorescence signals detected for each region; scanning the sample and determining final fluorescence parameters based on said expected fluorescence parameters.