A multi-stage parallel spectroscopy system has a plurality of dispersion stages, with the output of one dispersion stage serving as input to the next dispersion stage. Each dispersion stage separates input radiation into respective spectral components along a respective dispersion axis. In embodiments, the dispersion axes for the dispersion stages are substantially parallel to each other. Thus, the disclosed systems may be considered single-axis parallel spectroscopy configurations, in contrast to cross-axis parallel spectroscopy configurations. An optical system disposed in an optical path between dispersion stages can spatially filter a set of wavelengths from the input to the next dispersion stage to increase spectral extinction without sacrificing throughput or parallel operation. In some embodiments, the same dispersive element provides the spectral separation for multiple dispersion stages, by way of a recirculating optical system that redirects the spectral output from the dispersive element back to its input.

An optical spectrometer module for analysing samples. The optical spectrometer module comprises two or more sample holders. Each sample holder is adapted to receive and reproducibly position a sample in fixed locations within the optical spectrometer module. Each sample holder is also adapted to receive a light beam to thereby enable a sample contained in the sample holder to be exposed to the received light beam. Each sample holder is further adapted to enable light transmitted through the sample holder to exit the sample holder. The optical spectrometer module also comprises two or more electro-thermal components. Each electro-thermal component is thermally coupled to a respective sample holder to control the temperature of the sample holder.

Immersion tip of a probe for Raman spectroscopy comprising a cylindrical body equipped with a collimating optic and/or a window and designed to be immersed in a liquid to be analysed, the cylindrical body consisting of two parts separated by a slit intended to allow the liquid to be analysed to pass through it, the first part being hollow and traversed from a first end by light emission and reception signals, the other end opposite the first being closed by the collimating optic and/or the window, the second part being configured to prevent any reception of stray light other than that passing through the slit and comprising a part made of a light-absorbent material arranged facing the window.

A spectroscopic system may include: a probe having a probe tip and an optical coupler, the optical coupler including an emitting fiber group and first and second receiving fiber groups, each fiber group having a first end and a second end, wherein the first ends of the fiber groups are formed into a bundle and optically exposed through the probe tip; a light source optically coupled to the second end of the emitting fiber group, the light source emitting light in at least a first waveband and a second waveband, the second waveband being different from the first waveband; a first spectrometer optically coupled to the second end of the first receiving fiber group and configured to process light in the first waveband; and a second spectrometer optically coupled to the second end of the second receiving fiber group and configured to process light in the second waveband.

Image acquisition apparatuses, spectral apparatuses, methods and storage mediums for use with same are provided herein. At least one apparatus includes: a diffraction element irradiated by a light; a fiber for receiving reflected scattered light from a subject; a diffraction grating dispersing the transmitted light into light fluxes of wavelength bands again; an optical system imaging the split light fluxes; and an imaging device near the focal point of the optical system. An image is changed by rotating the diffraction grating, from which a two-dimensional image is acquired. The transmitted light may be branched into two or more, and input to a collimator lens and imaged as multiple spectral sequences by the optical system. At least one apparatus may form light fluxes traveling at different angles; and may acquire spectral information of the reflected and scattered light. Preferably, for the luminous fluxes, no gap exists in an image.

A confocal optical system-based measurement apparatus includes: a light source; a light projecting optical fiber group; a light receiving optical fiber group; a spectroscope; and a confocal optical system configured to condense each of a plurality of beams from a plurality of light projecting optical fibers to irradiate a sample therewith, and cause a plurality of beams from a plurality of condensing points on the sample to form images on the plurality of light receiving optical fibers, respectively, wherein the light projecting optical fiber group includes the plurality of light projecting optical fibers configured to receive light from the light source, the light receiving optical fiber group includes the plurality of light receiving optical fibers configured to guide received light to the spectroscope, the shape of an end face of the light projecting optical fiber group and the shape of an end face of the light receiving optical fiber group are in a mirror image relationship, and in the light projecting optical fiber group and the light receiving optical fiber group, the shape of an end face of each light projecting optical fiber and the shape of an end face of a light receiving optical fiber corresponding thereto are in a mirror image relationship.

A system and method for imaging a sample using Raman spectrometry. Optical fibers having opposite first ends and second ends are arranged with the first ends and second ends in respective two-dimensional arrays. The two-dimensional arrays maintain relative positions of the optical fibers to one another from the first ends to the second ends in a way that the first end of each optical fibers of the bundle can simultaneously collect a corresponding Raman signal portion scattered from specific spatial coordinates of the area of the sample. The so-collected Raman signal portions are propagated towards the corresponding second end, from which are outputted and detected simultaneously using an array of detectors.

Embodiments include a spectral reflectance system comprising a light source. The system includes a platform configured to retain a sample. The system includes an optical director positioned in the optical path between the light source and the platform. The optical director couples light from the light source to the platform. The system includes a detector positioned to receive reflected light from the sample. The detector generates a signal representing the reflected light. The system includes a focusing system coupled to the optical director. In response to the signal the focusing system automatically focuses the light on the sample by controlling a position of the optical director to maximize a strength of the signal.

A hybrid image-pupil optical reformatter and method for optional use with a spectrometer is disclosed, which performs beam slicing in pupil space and stacks replicas of the input source generated from the pupil beam slices in image space. The optical reformatter comprises a collimator which receives an input light and produces a collimated beam; a first optical element which receives the collimated beam, redirects portions of the collimated beam back toward the collimator as reimaged beams and permits portions of the collimated beam to pass; a second optical element which receives the reimaging beams and redirects the reimaging beams back toward the collimator and the first optical element; to form an output beam comprising the portions of the collimated beams that are not redirected toward the collimator by the first optical element. Also disclosed is the use of the reformatter for reformatting the input light of a spectrometer system, and the use of the reformatter as part of a spectrometer device.

A multi-stage parallel spectroscopy system has a plurality of dispersion stages, with the output of one dispersion stage serving as input to the next dispersion stage. Each dispersion stage separates input radiation into respective spectral components along a respective dispersion axis. In embodiments, the dispersion axes for the dispersion stages are substantially parallel to each other. Thus, the disclosed systems may be considered single-axis parallel spectroscopy configurations, in contrast to cross-axis parallel spectroscopy configurations. An optical system disposed in an optical path between dispersion stages can spatially filter a set of wavelengths from the input to the next dispersion stage to increase spectral extinction without sacrificing throughput or parallel operation. In some embodiments, the same dispersive element provides the spectral separation for multiple dispersion stages, by way of a recirculating optical system that redirects the spectral output from the dispersive element back to its input.