Abstract:
Certain disclosed embodiments concern an integrated imaging system that combined light-sheet microscopy, which enables considerable speed and phototoxicity gains, with quantitative-phase imaging. A method for using such imaging systems also is disclosed. In an exemplary embodiment, an integrated imaging system was used for multivariate investigation of live-cells in microfluidics.
Abstract:
Methods, systems and kits are described herein for detecting the results of an assay. In particular, the methods, systems and devices of the present disclosure rely on a difference between the diffusion rates of a reporter molecule and an analyte of interest in order to quantify an amount of analyte in a microfluidic device. The analyte may be a secreted product of a biological micro-object.
Abstract:
A system, including a structured illumination stage to provide a spatially modulated imaging field is provided. The system further includes a spatial frequency modulation stage to adjust the frequency of the spatially modulated imaging field, a sample interface stage to direct the spatially modulated imaging field to a sample, and a sensor configured to receive a plurality of fluorescence emission signals from the sample. The system also includes a processor configured to reduce a sample scattering signal and to provide a fluorescence emission signal from a portion of the sample including the spatially modulated imaging field. A method for using the above system to form an image of the sample is also provided.
Abstract:
Systems and methods are disclosed to enhance three-dimensional photoacoustic imaging behind, through, or inside a scattering material. Some embodiments can increase the optical fluence in an ultrasound transducer focus and/or enhance the optical intensity using wavefront shaping before the scatterer. The photoacoustic signal induced by an object placed behind the scattering medium can serve as feedback to optimize the wavefront, enabling one order of magnitude enhancement of the photoacoustic amplitude. Using the enhanced optical intensity, the object can be scanned in two dimensions and/or a spot can be scanned by re-optimizing the wavefront before post-processing of the data to reconstruct the image. The temporal photoacoustic signal provides information to reconstruct the third-dimensional information.
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.