The disclosure herein provides a device, a method and a computer-readable storage medium for quantitative phase imaging, and relates to the field of quantitative phase imaging. The specific implementation scheme is: Obtain a multiplexed interferogram of the sample, where the multiplexed interferogram is a sample beam composed of at least two beams with different wavelengths to illuminate the sample and penetrate into the cube beam splitter Combine at least two beams with different wavelengths as the reference beam, and the combined beam is the imaging image sampled by the camera; and perform phase retrieval on the multiplexed interference image to obtain each beam of the sample in the composite sample beam The phase map at the wavelength of Using the embodiments of the disclosure herein, one imaging acquisition and one phase retrieval are to acquire the phase maps of at least two wavelength channels.

An optochemical sensor unit including: an optical waveguide; a transmitting unit for emitting a first transmission signal for exciting a luminophore; a receiving unit for receiving a received signal comprising a signal component emitted by the excited luminophore; a measuring chamber for receiving a fluid, wherein the fluid includes magnetic microspheres; a membrane arranged between the measuring chamber and a measuring medium for exchanging an analyte between the measuring medium and the fluid in the measuring chamber, wherein the measuring diaphragm is impermeable to the magnetic microspheres; and an electromagnet for attracting magnetic microspheres to a sensor membrane with a fluid-contacting surface and/or to a fluid-contacting surface of the optical waveguide, or to a surface of a transparent substrate layer of the optical sensor unit that is connected to the optical waveguide.

A optical system and imaging device provide simultaneous or sequential optogenetic stimulation of different locations within a biological sample and fluorescence imaging of the locations. The systems include an illumination array with multiple electrically addressable elements that select a spatial pattern of illumination, an optical fiber bundle with fibers coupled between the array element and target locations at the sample, a fluorescence illumination source, and an imaging system for measuring fluorescence returning from the target locations. The optical imaging devices include a housing and a sample connector configured for receiving a first optical fiber bundle connection including multiple optical fibers. The sample connector has an indexing feature to maintain a fixed relationship between the fibers and internal optical paths of the device. The imaging devices also include an indexed input connector to receive another fiber bundle that carries the stimulus pattern, and a fluorescence excitation input connector.

There is described a fiber-optic sensor for measuring a light signal from a fluorescible sample comprising heavy metal ions, for example. The fiber-optic sensor comprises an optical fiber having a side surface by which the light signal from the fluorescible sample is inputted. The optical fiber is corrugated to form at least two gratings on the side surface of the optical fiber. Each grating comprises periodically longitudinally spaced-apart valleys on the surface of the optical fiber, and is longitudinally spaced apart from any other grating of the at least two gratings.

An assay device is disclosed comprising a housing and a test portion, electronic circuitry and an optical assembly each a least partially located in the housing. The test portion comprises one or more test zones adapted to receive an analyte and a fluorescent label associated with the analyte, the fluorescent label being excitable by excitation light and adapted to emit emission light upon excitation by excitation light. The electronic circuitry comprises one or more light sources and one or more light detectors. The optical assembly comprises one or more excitation light guides adapted to guide excitation light from the one or more light sources to the one or more test zones, and/or one or more emission light guides adapted to guide emission light from the one or more test zone to the one or more light detectors.

A light-emission detection apparatus is provided for individually condensing light emitted from each emission point of an emission-point array using each condensing lens of a condensing-lens array to forma light beam and detecting each light beam incident on a sensor in parallel. The light-emission detection apparatus can be downsized and high sensitivity and low crosstalk can be simultaneously accomplished when a certain relation between the diameter of each emission point, a focal length of each condensing lens, an interval of condensing lenses, and an optical path length between each condensing lens and a sensor is satisfied.

Disclosed is apparatus (1) for measuring fluorescence and absorbance of a substance in a sample, said apparatus (1) comprising: a flow cell (2) for containing a sample, a first light source (3), a first conductor (5) for transmitting light from the first light source (3) to the flow cell (2) for irradiating a sample contained therein, a second conductor (7) for transmitting light from the flow cell (2) to a sample detector (9) arranged to detect an electromagnetic radiation that has passed through said cell (2), and a processing unit (16) arranged to receive a first signal (31) from a reference detector (15) and a second signal (32) from the sample detector (9) and to determine an absorbance based on said first and second signals (31,32), said apparatus (1) further comprising a second light source (4), a third conductor (6) for transmitting light from the second light source (4) to the cell (2) and wherein the sample detector (9) is further arranged to also detect fluorescence signals in the light that has passed through the flow cell (2). The invention also relates to a method for measuring the absorbance and the fluorescence of a substance in a sample.

Disclosed herein are configurations for few-mode fiber optical endoscope systems employing distal optics and few-mode, double-clad or other optical fiber wherein the systems directing an optical beam to a sample via the optical fiber; collecting light backscattered from the sample; direct the backscattered light to a detector via the optical fiber; and detect the backscattered light; wherein the directed optical beam is single mode and the collected light is one or more higher order modes.

Presented herein are apparatuses for use in capillary separations. An apparatus includes a coupling that integrates a capillary with a voltage source, a sheath liquid system, a fluid exit port, and a manifold. The coupling may be an elbow connector or equivalent. The manifold receives incident light from an incident light input, and emitted light is collected by a collected light output. The capillary enters the manifold at an input for the capillary, traverses the coupling, and terminates at the fluid exit port, for example an electrospray emitter. The capillary may also enter the manifold at an input for the capillary and terminates inside the manifold.

The disclosure relates to methods and devices for monitoring the concentration of a substance, preferably oxygen, in a cell or tissue, e.g., in cells of the human skin. In particular, it provides a method for determining the concentration of a quencher, such as oxygen and/or the concentration of a probe, e.g., a heme precursor such as protoporphyrin IX (PpIX), wherein the probe is capable of exhibiting luminescence (delayed fluorescence (DF) or phosphorescence) and or transient triplet absorption, preferably, deDF, in a living cell. The method comprises steps of exciting the probe, measuring the lifetime of the luminescence exhibited by said probe, herein, in the presence of the quencher, the lifetime is shortened as compared to the lifetime in the absence of the quencher, and correlating said lifetime with said concentration. The disclosed method leads to more precise results than conventional methods, because of adaptations based on the understanding of the influence of the concentration of the probe and its excitation fluence rate (intensity) on the analysis. For example, the simultaneous time-resolved detection of the probe excimer and monomer DF allows estimation of the probe concentration and compensation of the probe self-quenching effect in the quencher concentration calculation, increasing the measurement precision. Taking into account second order triplet interactions also permits the interpretation of non-exponential decays and further improvement of the quencher and probe concentration estimation. Disclosed methods rely, e.g., on measurement at different emission wavelengths and application of an adaptive Stern-Volmer relationship, the decay central fitting method and/or a mixed orders approach. Said method can be applied, e.g., for bedside monitoring of patients. Also disclosed is the use of the PpIX precursor 5-aminolevulinic acid (5-ALA), or derivatives thereof, in this method, and a device suitable therefor.