Patent classifications
G01J2003/423
External cavity laser source
A tunable laser source that includes multiple gain elements and uses a spatial light modulator in an external cavity to produce spectrally tunable output is claimed. Several designs of the external cavity are described, targeting different performance characteristics and different manufacturing costs for the device. Compared to existing devices, the tunable laser source produces high output power, wide tuning range, fast tuning rate, and high spectral resolution.
Laser sensor for trace gas detection
Systems and methods are disclosed to determine the concentration of a species within a sample. An example method may include collecting optical loss data over a range of frequencies from the sample using a spectroscopy system; placing the optical loss data into a plurality of bins, each bin having a defined frequency width; determining an average optical loss data value for the optical loss values within each bin that have an optical loss value less than a threshold value; removing the optical loss data within each bin having a value outside a tolerance range bounding the average optical loss data value for the respective bin; fitting a spectral curve to the remaining optical loss data; and determining the concentration of the species within the sample based on the spectral curve.
Analytes monitoring by differential swept wavelength absorption spectroscopy methods
The present invention relates to a method, apparatus and system for measuring the content of either one or more gas analytes that may be part of a gas. The present invention applies a spectroscopic method that utilizes an extremely narrow linewidth laser beam that is absorbed when its wavelength is swept across the interval containing the absorption line of the analyte. The method, apparatus and system of the present invention is applicable to any analyte in gas phase that is part of a gas mixture, or to any analyte in a plasma phase, as well as analytes in other environments.
Self-referencing cavity enhanced spectroscopy (SRCES) systems and methods
Described self-referencing cavity enhanced spectroscopy (SRCES) systems and methods are tailored to acquiring spectra in a middle regime, in which signals are lower than optimal for conventional absorption spectroscopy, and absorption is higher than optimal for cavity ring-down spectroscopy (CRDS). Longitudinal mode resonance spectral peaks are analyzed individually to extract intensity ratios (e.g. maximum to minimum) and/or curve-fitting parameters, obviating the need to measure or precisely control the input light intensity.
APPARATUSES AND METHODS FOR ANOMALOUS GAS CONCENTRATION DETECTION
Embodiments of the disclosure are drawn to apparatuses and methods for anomalous gas concentration detection. A spectroscopic system, such as a wavelength modulated spectroscopy (WMS) system may measure gas concentrations in a target area. However, noise, such as speckle noise, may interfere with measuring relatively low concentrations of gas, and may lead to false positives. A noise model, which includes a contribution from a speckle noise model, may be used to process data from the spectroscopic system. An adaptive threshold may be applied based on an expected amount of noise. A speckle filter may remove measurements which are outliers based on a measurement of their noise. Plume detection may be used to determine a presence of gas plumes. Each of these processing steps may be associated with a confidence, which may be used to determine an overall confidence in the processed measurements/gas plumes.
Broadband or mid-infrared fiber light sources
A white light spectroscopy system includes a super continuum light source having an input light source including semiconductor diodes to generate an input beam having a wavelength shorter than 2.5 microns. The light source includes a cladding-pumped fiber optical amplifier to receive the input beam, and a photonic crystal fiber to receive the amplified optical beam to broaden the spectral width to 100 nm or more forming an output beam in the visible wavelength range. The output beam is pulsed with a repetition rate of 1 Megahertz or higher. The system also includes a lens and/or mirror to receive the output beam, to send the output beam to a scanning stage, and to deliver the received output beam to a sample. A detection system includes dispersive optics and narrow band filters followed by one or more detectors to permit approximately simultaneous measurement of at least two wavelengths from the sample.
Laser spiderweb sensor used with portable handheld devices
A portable spectrometer, including a smart phone case storing a portable spectrometer, wherein the portable spectrometer includes a cavity; a source for emitting electromagnetic radiation that is directed on a sample in the cavity, wherein the electromagnetic radiation is reflected within the cavity to form multiple passes of the electromagnetic radiation through the sample; a detector for detecting the electromagnetic radiation after the electromagnetic radiation has made the multiple passes through the sample in the cavity, the detector outputting a signal in response to the detecting; and a device for communicating the signal to a smart phone, wherein the smart phone executes an application that performs a spectral analysis of the signal.
Optical arrangement for the compensation of incorrect alignments of a reflector in relation to a light source
An optical arrangement has a light source, which emits a light beam along a first optical axis. A first reflector is provided, and a second reflector reflects light reflected by the first reflector. The first reflector has a transverse offset from the first optical axis to reflect light along a second optical axis which has a parallel offset of two times the transverse offset of the first optical axis. The second reflector reflects the light beam back to the first reflector along a third optical axis having a parallel offset with a fixed amount in a fixed transverse direction in relation to the second optical axis. The light beam is reflected by the first reflector along a fourth optical axis which has a parallel offset in relation to the first optical axis with a fixed amount counter to the fixed transverse direction.
CTIR SPECTROMETER FOR LARGE AREA ASSESSMENT OF GAS EMISSIONS
Systems for determining the presence and distribution of gas emissions in an area are provided. For example, a system may include one or more light detectors and one or more reflectors and/or one more retroreflectors disposed around the perimeter, a light source configured to emit light at a plurality of wavelengths towards the one or more light detectors and/or the one or more reflectors and/or one or more retroreflectors, and one or more processors configured to receive information representing light intensity detected by the one or more light detectors, respectively at each of the plurality of wavelengths and determine gases present in each path based on the light intensity detected by the respective detector at each of the plurality of wavelengths and distribution thereof. The path being either light source-respective detector, light source-respective reflector-respective detector or light source-respective retroreflector-respective detector. Other system may not use reflectors and/or retroreflectors.
GAS ABSORBANCE SPECTRUM MEASUREMENT DEVICE FREQUENCY LOCKING METHOD, AND GAS ABSORBANCE SPECTRUM MEASUREMENT METHOD
The gas absorption spectroscopic measurement device according to one embodiment of the present invention is provided with: a laser irradiation unit (1); and optical resonator (2), and a first detection unit (3) for detecting light taken out of the optical resonator (2). The gas absorption spectroscopic measurement device acquires the component concentration of a gas to be measured by CRDS (Cavity Ring-Down Spectroscopy) measurement. The laser irradiation unit (1) is provided with: a laser light source (10); a frequency conversion unit (12) configured to selectively output either laser light having the same frequency as the irradiation light source or laser light having a frequency of the laser light source multiplied by a prescribed number of times; a frequency modulation unit (13, 14) for modulating the frequency of the emitted laser light using a modulation signal, a second detection unit for detecting returning light derived from the irradiation light returning to the optical resonator (2); and a feedback control unit (191, 11) for generating an error signal affected by the difference between the frequency of the laser light emitted to the optical resonator (2) and the modulation signal based on the detection signal from the second detector (18), thereby controlling the oscillation frequency in the laser light source (10) in accordance with the error signal.