Abstract:
The disclosure relates to a portable and/or handheld bioagent detector and methodology described herein that is based in part on advanced Raman Chemical Imaging ('RCI') technology. According to one embodiment of the present disclosure, the detection system may include a fiber array spectral translator ('FAST') and may also include a probe which may include a complementary metal oxide semiconductor (CMOS) camera. The probe alleviates the need to place the main instrument close to an unconfined release of a potentially hazardous material and facilitates analysis of a sample that is situated in a hard-to-reach location while minimizing contamination of the detector and operator.
Abstract:
A hyper-spectral imaging filter has serial stages (33, 35) along an optical signal path, each stage having angularly arranged retarder elements (45, 47) and one or more polarizers (42, 44). The retarders can include tunable (such as abutted liquid crystals tuned in unison), fixed and/or combined tunable and fixed birefringences, and can be arranged in Sole, Lyot, Evans or similar configurations. Each stage has a periodic transmission characteristic with periodic bandpass peaks (52) spaced by free spectral range bandpass gaps. Distinctly different retardations are employed in cascaded stages, causing some stages to pass narrow bandpass peaks and other stages to have widely spaced bandpass peaks (large free spectral range). The transmission functions of the serial stages are superimposed, providing a high finesse ratio and good out-of- band rejection. Preferably at least some stages have tunable liquid crystals for at least part of their retardation, and are controlled to selectively align respective bandpass eaks.
Abstract:
An optical spectrum analyzer comprises a diffraction grating (DG), a polarization decomposing unit (PDM) for decomposing the input light beam into first and second light beams having mutually-perpendicular linear states of polarization, and two output ports (FP2/1, FP2/2) each for receiving from the grating, substantially exclusively, a respective one of the polarized light beams (LT, LR) after diffraction by the diffraction grating (DG). Each of the linearly-polarized light beams is directed onto the diffraction grating with its linear state of polarization at any prescribed angle to a corresponding plane of diffraction of the diffraction grating. The arrangement is such that the state of polarization of the light beams, at any particular wavelength within an operating band of the analyzer remains substantially unchanged with respect to time. The analyzer also may have a reflector (RAM) for reflecting the light beams leaving the diffraction grating after diffraction a first time so as to return them to the diffraction grating for diffraction a second time.
Abstract:
The illumination module (2) is for illuminating a plane measurement spot (3) of a reflection spectrometer (1). It comprises a plurality of light-emitting diodes (41.1-41.8). Light (21) is guided from the light-emitting diodes (41.1-41.8) to the measurement spot (3) by a circular conical mirror (6), such that the angle of incidence of the light (21) is essentially 45°. First (5.1-5.8) and second (7) apertures delimit the angular range of light. The reflection spectrometer (1) comprises the illumination module (2) described above, a dispersive optical element (8) for analyzing light emerging from the measurement spot (3), and a detector array (9).
Abstract:
A spectroscopic investigation system comprises: a source (LS) of a polychromatic beam of electromagnetic radiation (PPCLB); a polarizer (P); a stage (STG) for supporting a material system to be investigated; an analyser (A); at least one detector system (DET); and at least one compensator (C) (C') (C'') arranged to be continuously rotated during operation while said beam of electromagnetic radiation (PPCLB) passes therethrough. Said polychromatic beam of electromagnetic radiation is caused to interact with a material system (MS) on said stage (STG), pass through said analyser (A), and enter said at least one detector system (DET). The compensator comprises a combination of at least two zero-order wave plates (MOA, MOB), having their respective fast axes offset from zero or ninety degrees with respect to one another; or a combination of at least a first and a second effective zero-order wave plate (ZO1, ZO2), each effective zero-order wave plate comprising two multiple order wave plates (MOA1, MOA2, MOB1, MOB2) which are combined with the fast axes thereof oriented at substantially ninety degrees to one another; or a combination of at least one zero-order wave plate (MOA , MOB), and at least one effective zero-order wave plate (ZO2, ZO1).
Abstract:
A spectroscopic rotating compensator material system investigation system including a photo array (DE's) for simultaneously detecting a multiplicity of wavelengths is disclosed. The spectroscopic rotating compensator material system investigation system is calibrated by a mathematical regression based technique involving, where desirable, parameterization of calibration parameters. Calibration is possible of calibration parameters. Calibration is possible utilizing a single two-dimensional data set obtained with the spectroscopic rotating compensator material system investigation system in a "material system present" or in a "straight-through" configuration.
Abstract:
Le dispositif comprend une torche à plasma (10-14) pour créer dans une enceinte (2) étanche un plasma HF (16) et injecter dans ce plasma un échantillon (6) contenant un élément à doser ; un laser (18) émettant des impulsions de longueur d'onde et de largeur spectrale appropriée à l'excitation de l'élément ; des prismes (22, 24) pour envoyer les impulsions laser dans le plasma afin que l'élément émette par fluorescence des impulsions lumineuses ; une lentille (46) pour conjuguer la zone excitée (36) du plasma par le laser sur un spectromètre (42) sélectionnant et transformant les impulsions émises par l'élément en un signal électrique ; une électronique (48, 50) pour traiter le signal électrique issu du spectromètre de manière synchrone avec les impulsions laser et des moyens (52) pour déterminer à partir du signal électrique traité, la quantité de l'élément contenu dans l'échantillon.
Abstract:
An acousto-optic frequency shifter having a long interaction region is used as an optical analyzer. A variable frequency signal generator (340) is used to drive an acoustic transducer (316) to launch an acoustic wave in contact with an optical fiber (300). The acoustic frequency is varied over a known range to generate acoustic waves having known wavelengths. An optical signal having an unknown optical wavelength is introduced into one end (302) of the optical fiber (300) in a first polarization mode. The effect of the acoustic wave on the optical signal is to cause coupling of the optical signal from the first polarization mode to a second orthogonal polarization mode. The amount of the coupling is dependent upon the phase matching between the acoustic wavelength and the optical beat length. The coupling between the polarization modes is maximum when the acoustic wavelength is equal to the optical beat length. The intensity of the optical signal coupled to the second polarization mode can be measured to determine the optical wavelength corresponding to the acoustic wavelength when the maximum intensity occurs.
Abstract:
A method and device for detecting dichroic and/or birefringent narrow spectral features in a sample is described. The method includes the steps of providing a beam of light having an optical frequency bandwidth which is narrow compared to the width of the narrow spectral feature and having a center frequency ωc which lies near the narrow spectral feature, polarization phase modulating a beam of light with a single RF frequency to provide a pure FM spectrum having upper and lower sidebands in which either the carrier and sidebands have been polarized differently with respect to one another, exposing the sample containing the narrow spectral feature to the polarized modulated light so that the FM sidebands probe the narrow spectral feature, polarization analyzing and then photodetecting the light emerging from the sample to detect a RF beat at the specific RF frequency used for the polarization phase modulation, and electronically monitoring the amp- l i tude of the RF beat signal to indicate the strength of the narrow spectral feature. The device includes a polarization phase modulator (17) and a polarization analyzer (18) positioned on opposite sides of the sample (16). In a preferred embodiment the polarization phase modulator produces a frequency modulated optical spectrum with the sidebands polarized precisely orthogonal to the carrier (Fig. 3).
Abstract:
The invention relates to a miniature spectrometer (10) for spectrometry and for image capture, comprising a detection unit (7) for detecting an optical parameter and an optical unit, comprising a polarizer (2), a Savart element (40), which comprises a first birefrigent element (4a) and a second birefrigent element (4b), and an analyzer (5), characterized in that a first liquid crystal element (3a) is arranged between the polarizer (2) and the Savart element (40), which is designed to adjust a fourth polarization axis (203) from a radiation (103) emitted from the first liquid crystal element such that, in an imaging mode of the miniature spectrometer (10), the radiation (103) emitted from the first liquid crystal element passes through the first birefrigent element (4a) without splitting and, in a spectrometer mode of the miniature spectrometer (10), the radiation (103) emitted from the first liquid crystal element is split in the first birefringent element (4a) into a first ordinary beam (500b) and a first extraordinary beam (500a) and wherein the analyzer (5) is arranged in the beam path behind the Savart element (40) and the detection unit (7) is arranged in the beam path behind the analyzer (5).