Abstract:
Methods and systems for generating near-infrared (NIR) images of biological targets are discussed. In one aspect, one or more radiation sources illuminate a target, with one or more detectors receiving the transmitted radiation. Such equipment can be used to generate a plurality of NIR images of a target. The images can be converted into frequency space, combined using chosen weighting factors, and deconvoluted into the spatial domain to provide a composite image. The composite image can have enhanced quality relative to the individual images, allowing for a richer set of information to be displayed. Other aspects such as scanning, background illumination correction, the use of filters, and additional techniques are also discussed.
Abstract:
Detecting the presence of a target material in a scene by using a multi-aperture interferometer system having a plurality of apertures at least one of which has an adjustable optical path length, by adjusting the aperture(s) to obtain a predetermined optical path length difference among the apertures, the predetermined optical path length difference being based on a source laser wavelength and a target material wavelength, illuminating the scene with the source laser, capturing a spectral data set corresponding to an interference pattern generated in the multi-aperture interferometer system for an illuminated point source in the scene, the spectral data set containing spatially distributed spectral data, and determining whether the target material is present at the illuminated point source based on a presence of spectral data in at least one side lobe of the spectral data set.
Abstract:
A photo-thermal interferometric spectroscopy system is disclosed that provides information about a chemical at a remote location. A first light source assembly is included that emits a first beam. The first beam has one or more wavelengths that interact with the chemical and change a refractive index of the chemical. A second laser produces a second beam. The second beam interacts with the chemical resulting in a third beam with a phase change that corresponds with the change of the refractive index of the chemical. A detector system is positioned remote from the chemical to receive at least a portion of the third beam. An adaptive optics system at least partially compensates the light beam degradation caused by atmospheric turbulence. A focusing system is used to bring together the light passed through the chemical; the focusing system includes a multimode fiber for the light collection, The detector system provides information on a phase change in the third beam relative to the second beam that is indicative of at least one of, absorption spectrum and concentration of the chemical.
Abstract:
A convenient and economical method and instrumentation to efficiently reduce offensive spectral noises due to water vapor and carbon dioxide gas often encountered in FTIR spectrophotometry is provided by spectrally monitoring and controlling the amount of water vapor and carbon dioxide gas inside the spectrophotometer such that both amounts in the sample and background measurements become congruent through remote open-close operation of water-vapor (or carbon dioxide gas) supplier and dehumidifier (or carbon dioxide gas adsorber). This new technique can be used: (1) Under the ambient humidity condition, saving time and money effectively. (2) Both in the closed spectrophotometer and in the open system. (3) And applicable to any FTIR accessory and measurement method, including transmission, external reflection, reflection-absorption, attenuated total reflection (ATR), and microscopy measurements.
Abstract:
A method and apparatus for an improved spectral imaging system is provided. The system is capable of measuring the fluorescence, luminescence, or absorption at selected locations on a sample plate. The emissions detection subassembly can tune to any wavelength within a continuum of wavelengths utilizing an interferometric spectral discriminator. The interferometric spectral discriminator creates an interferogram from which the wavelength spectra for each pixel of the array can be calculated, typically using Fourier transform analysis. In one aspect, the chromatic accuracy of the system is calibrated using a calibration slit placed in the input aperture of the input relay lens but outside of the sample image. The slit is illuminated using a source of known wavelength. The fringe count versus the wavelength of the slit illumination source is monitored and used to calibrate the spectral discriminator. In another aspect, a transparent optic is included in the interferometric spectral discriminator that can be inserted into the beam path whenever a monochrome image of the sample is required. The optic produces a large offset in the legs of the interferometer resulting in the fringe density becoming too large to resolve by the individual pixels of the detector array. In another aspect, the interferometric spectral discriminator includes a polarizing beam splitter. The polarizing beam splitter preferentially reflects one polarization while preferentially transmitting a second polarization, thus achieving improved efficiency while minimizing ghosting. In another aspect, a metaphase finder is used to locate areas of interest. The sample plate containing the material of interest is illuminated with light of a wavelength determined to preferentially scatter from objects the size of the metaphase spreads. The intensity of the scattered light versus the location on the sample plate is monitored and used to locate the areas of interest. Preferably the sample plate is also illuminated by light of a second wavelength which is not preferentially scattered by the objects of interest, thus representing the background scatter. By subtracting the background scatter from the primary scattered light, improved object discrimination is achieved.
Abstract:
A small packaged spectroscopic sensor unit is provided which measures or inspects an interior quality or ingredient of an inspection object by introducing light having passed through the interior of the inspection object to an optical fiber and analyzes the light spectroscopically. In this sensor unit, the fiber bundle receives only a light beam of incident angle less than a prescribed angle, the fiber bundle is twisted together to disperse and uniformize the irregularity of the introduced light at the light-emitting end, and the optical fiber bundle is held by an arranging holder to shape the light-emitting face of the fiber bundle to fit the light-receiving face of a light diffuser and the light-receiving face of a photoelectric conversion element. The sensor unit has a light diffuser for diffuse-transmitting the light emitted from the light-emitting face of the optical fiber bundle, a continuous variable interference filter placed on the light-emitting face of the light diffuser, and a photoelectric conversion element after the continuous variable interference filter. The optical paths of the optical fiber bundle, light diffuser, and the continuous variable interference filter are aligned to be connected. The above members are sealed airtightly in a package.
Abstract:
A spectral analysis system includes a signal processing system which provides a probe and a reference beam. The probe beam is applied to the target to be analyzed. The relative phase relationship of the two beams is varied. A scattered or transmitted portion of the probe beam is combined with the reference beam and a resulting interferometric signal is detected. An electronic processing and control system separates the spectral information in the electronic domain, processes the information and controls the system.
Abstract:
An interferometer (1) is arranged to form a first interference fringe pattern comprising at least ten interference fringes; recording an image of said first interference fringe pattern; perturbing an optical path in the interferometer (1) to form a second interference fringe pattern comprising at least ten interference fringes; and combining an image of said second interference fringe pattern with the recorded image of the first interference fringe pattern to produce a further image comprising a moiré fringe pattern arising from a difference or differences between the first and second interference fringe patterns. The combining step involves subtraction (4) of digital images. Different wavelengths and interferometers are used: Michelson, Mach-Zehnder, Fizeau, Twyman-Green. In this new approach, all the errors of a poor quality, misaligned system are accepted and then eliminated by the combination process, producing a moiré fringe pattern. The method enables very large aperture optical systems for traditional and engineering interferometers to be constructed from inexpensive and basic components.
Abstract:
A linear positioning apparatus includes an intermediate portion having an axis, and first and second end portions mounted with flexure legs thereto. The flexure legs accommodate motion of the intermediate portion relative to the end portions along the axis, but inhibit motion of the intermediate portion relative to the end portions in directions not parallel to the axis. The apparatus can accommodate forces having off-axis components, and produce motion that comprises substantially no off-axis component. The apparatus is useful in, for example, optical systems where precise linear motion is required.
Abstract:
A reference signal is used to track the actual behavior of the scanner in an interferometer to produce scanner-position data that can be used to correct errors introduced by scanner nonlinearities and other error sources. A narrow-band light source is advantageously utilized to cover the entire range of operation of the scanner. Because of the independent reference channel, the invention is suitable for implementation with all types of conventional interferometric techniques. The concept is preferably implemented by utilizing an additional light source and the same scanner used for the measurement, so that the OPD varies in synchronization of both the reference-signal and data-collection procedures. Alternatively, a high temporal-coherence filter may be used with the same light source and optical path used for the interferometric measurement.