Abstract:
A system and method for measuring a concentration of a gas in a container having at least one flexible or variable side or wall. The system and method comprising creating a determinable optical path length through the container having a shape. Positioning a light source head and a detector head against at least one of the least one flexible or variable side or wall. Transmitting a light signal between the light source head and the detector head through the determinable optical path length. Determining the concentration of the gas in the container based on detected light and the determinable optical path length.
Abstract:
An optical sensor and a method of operating the optical sensor are provided. The optical sensor includes a light source configured to emit a light, and a path adjuster configured to adjust a traveling path of the light to reflect the light at a first time, and allow the light to pass through the path adjuster at a second time. The optical sensor further includes a light receiver configured to receive a reference light among the reflected light, and receive, among the light passing through the path adjuster, a measurement light related to a target material.
Abstract:
A detection device having: a terahertz wave generation element; a terahertz wave detection element; a first transmission path arranged upon the terahertz wave generation element; a second transmission path arranged upon the terahertz wave detection element; and a sealed section arranged between the terahertz wave generation element and the terahertz wave detection element and separated from the first transmission path and the second transmission path, so as to surround the first transmission path and the second transmission path. A space between an emission surface in the first transmission path and an incident surface in the second transmission path is connected to a space between the first transmission path and the sealed section and to a space between the second transmission path and the sealed section.
Abstract:
A phase refractive index of a test object is measured with high accuracy. A phase difference between a reference light beam and a test light beam is measured by dividing light from a light source into the reference light beam and the test light beam, and causing interference between the test light beam transmitted through the test object and the reference light beam. A phase refractive index of the test object is calculated by calculating a value corresponding to an integral multiple of 2π included in the phase difference, based on a slope of a phase refractive index of a reference object with respect to wavelength.
Abstract:
The present invention is thus directed to an automated system and method of varying the optical path length in a sample that a light from a spectrophotometer must travel through. Such arrangements allow a user to easily vary the optical path length while also providing the user with an easy way to clean and prepare a transmission cell for optical interrogation. Such path length control can be automatically controlled by a programmable control system to quickly collect and stores data from different path lengths as needed for different spectrographic analysis. Such a methodology and system, as presented herein, is able to return best-match spectra with far fewer computational steps and greater speed than if all possible combinations of reference spectra are considered.
Abstract:
The invention relates to systems and methods for improving optical detection and sensitivity in situations in which emission of luminescent light is monitored. It is provided a sample carrier which achieves increased sensitivity of luminescent light detection. The sample carrier comprises a sample carrying part and a light reflecting part; wherein the light reflecting part is positioned to allow an optical collection and detection system to collect not only luminescent light emitted from the sample positioned on the sample carrying part in a direction of the optical collection and detection system, but also luminescent light emitted from the sample in a direction away from the optical collection and detection system and reflected in the direction of the optical collection and detection system via the light reflecting part. When an excitation light source is needed, the light reflecting part also allows the excitation light rays passing through the sample to hit the light reflecting part, and reflect back in the opposite direction thus the reflected excitation light also passes through the sample. Also provided are methods of using such a sample carrier.
Abstract:
A spectrophotometer (2) comprising a source of radiation (6), preferably optical radiation, disposed to emit radiation at a plurality of wavelengths towards a sample in a sample holder (4) and a detection arrangement 8 for detecting the radiation after its interaction with the sample. The sample holder (4) is adapted to present a plurality of different path lengths for the emitted radiation through the sample. An arithmetic unit (10;10b) is operably connected to receive an intensity dependent output from the detection arrangement (8) and is adapted to store an intensity value of the detected emitted radiation indexed to its wavelength at two or more path lengths of the plurality of different path lengths and to calculate a value dependent on the ratio of the indexed intensity values at each of two path lengths by which an indication of the presence of a substance of interest withiA spectrophotometer (2) comprise a source of radiation (6), preferably optical radiation, disposed to emit radiation at a plurality of wavelengths towards a sample in a sample holder (4) and a detection arrangement 8 for detecting the radiation after its interaction with the sample. The sample holder (4) is adapted to present a plurality of different path lengths for the emitted radiation through the sample. An arithmetic unit (10;10b) is operably connected to receive an intensity dependent output from the detection arrangement (8) and is adapted to store an intensity value of the detected emitted radiation indexed to its wavelength at two or more path lengths of the plurality of different path lengths and to calculate a value dependent on the ratio of the indexed intensity values at each of two path lengths by which an indication of the presence of a substance of interest within the retained sample can be obtained.
Abstract:
The device for measuring an optical absorption characteristic of a sample according to the present invention comprising a light source, a optical wave-guide having light input surface(s) and light output surface(s) that are opposite to each other, and a light reflecting surface on which a sample to be measured is disposed, through which the light passes and is reflected by a total reflection on the sample, one or more light transmitting means arranged between the light output surface of the optical wave-guide and the light input surface of the optical wave-guide so that the light is again entered into the optical wave-guide, and a processing device which receives the light re-exited from the optical wave-guide through the output surface and detects the optical absorption characteristics of the sample on the basis of the light received, whereby the light which passes through the optical wave-guide is conducted to the optical wave-guide again, the light is again entered the optical wave-guide, and the light is again reflected on the sample (FIG. 1).
Abstract:
A flow cell for absorbance detection with at least two different optical path lengths. It increases the range of analyte concentrations which can be measured compared with a conventional single path flow cell. Light from the two paths is combined onto the same photodetector. Calibration with known samples allows analyte concentrations to be measured. The dual or multi-path length flow cell may be used in equipment designed for single path flow cells.
Abstract:
Methods and apparatus for detecting biological activity within a sample are disclosed. The present invention provides a combination of a first and a second infrared light source arranged on the side of a sample vial, and a first and a second narrow-band infrared detector similarly arranged on the side of the vial approximately opposite the sources. The disclosed arrangement cancels the sources of error while measuring the carbon dioxide content of the headspace gas above the sample. In operation, the present invention sequentially measures the photocurrents generated at each detector with no source turned on, with the first source turned on, and with the second source turned on and the first source turned off. The CO.sub.2 absorption coefficient of the vial headspace gas is then calculated based on the photocurrents measured. This present invention allows compensation for source aging, detector aging, and vial wall thickness changes. Moreover, the present invention permits a determination of the absolute absorption coefficient at a selected wavelength, most preferably about 4.26 .mu.m, which is the CO.sub.2 absorption characteristic wavelength. The determination of the absolute CO.sub.2 concentration within the headspace permits the detection of bacterial growth processes. Additionally, the disclosed source/detector combination can be produced at low cost. Thus, in preferred embodiments, the apparatus of the present invention comprises a plurality of vials that are simultaneously monitored by providing each of the plurality of vials with its own source/detector combination and activating and deactivating the sources and detectors using a multiplexer/demultiplexer arrangement.