Abstract:
A polarization measuring device is operated by passing light having a predetermined input polarization state to a sample for a potentially polarization changing interaction and from the sample through a polarization selective analyzer and to an intensity detector. The method proceeds by varying an angle between the output polarization state of the light emanating from the sample and the analyzer. The wavelength of the light reaching the intensity detector is varied, and a plurality of intensity measurements are performed successively at different constellations of polarization. Spectral modulation states and corresponding intensity values are stored together with polarization and spectral values representing the corresponding constellation. The polarization modulation and the spectral modulation are performed simultaneously and continuously, and during a single, monotonic variation of the polarization modulation state, the spectral modulation state is varied plural times and during each spectral modulation period (τλ) plural successive intensity measurements are performed.
Abstract:
A spectrum adjuster produces a pure analyte spectrum and includes: a dynamic opacity optic that receives input light, receives an adjustment signal, produces primary adjusted light, and produces secondary adjusted light from the input light based on the adjustment signal; a light source in optical communication with the dynamic opacity optic; a detector in optical communication with the dynamic opacity optic and that receives transmitted light from the sample and produces a transmitted light signal based on an amount of transmitted light received; and an adjustment controller that receives the transmitted light signal, produces the adjustment signal, and communicates the adjustment signal to the dynamic opacity optic.
Abstract:
A photoacoustic gas analyzer may include: a gas chamber configured to receive a gas to be analyzed therein, a radiation source configured to emit into the gas chamber electromagnetic radiation with a time-varying intensity adapted to selectively excite gas molecules of N mutually different gas types the concentrations of which are to be determined in the gas received in the gas chamber, thereby generating acoustic waves, an acoustic-wave sensor configured to detect acoustic waves generated by the electromagnetic radiation emitted by the radiation source into the gas to be analyzed, and a control unit operatively connected to the radiation source and the acoustic-wave sensor. The control unit may be configured: to control the radiation source to emit electromagnetic radiation with a time-varying intensity and to modulate the frequency at which the intensity is varied with a modulation signal taking on at least N mutually different values, to receive from the acoustic-wave sensor signals indicative of detected acoustic waves generated by the electromagnetic radiation emitted by the radiation source into the gas to be analyzed, to determine at least N mutually different signal amplitudes associated with respective N mutually different frequencies at which the intensity of the emitted electromagnetic radiation is varied, and to determine from the determined signal amplitudes the concentrations of the N mutually different gas types.
Abstract:
Systems for measuring optical properties of a specimen are disclosed. The systems are configured to sample signals related to the measurement of the properties of a specimen, and perform software-based coherent detection of the signals to generate resulting measurements are based on the signals acquired at substantially the same time instance. This facilitates the displaying or generating of the desired measurements in real time. In one configuration, the system is configured to direct a modulated light signal at a selected wavelength incident upon a specimen. In another configuration, the system is configured to direct a combined light signal, derived from a plurality of light signals at different wavelengths and modulated with different frequencies, incident upon a specimen. In yet another configuration, the system is configured to direct a plurality of light signals modulated with different frequencies incident upon different regions of a specimen.
Abstract:
Method and gas analyzer for measuring the concentration of a gas component in a sample gas, wherein to measure the concentration of a gas component in a sample gas, a laser diode is actuated by a current and light generated by the laser diode is guided through the sample gas to a detector, the current is simultaneously varied within periodically successive sampling intervals for the wavelength-dependent sampling of an absorption line of interest of the gas component, and the current can be additionally modulated sinusoidally based on wavelength modulation spectroscopy with a low frequency and small amplitude, such that a measuring signal generated by the detector is evaluated to form a measurement result, where to improve the measuring signal-noise ratio and achieve a much lower detection limit with the same measuring distance, the current is modulated with a high (RF) frequency in the GHz range so that no wavelength modulation occurs, and an RF modulation amplitude is selected at the maximum level using the linear control range of the laser diode where, before evaluation, the measuring signal is demodulated at the radio frequency.
Abstract:
Methods and apparatuses (500) of generating and processing a real-time time-domain cavity ringdown spectroscopy (CRDS) signal from absorbing species m an optical detection system having an optical ringdown cavity (200) using off-axis paths (230) are provided. At least one modulated light signal (570) is generated using one or more light sources (520), each modulated at specified modulation frequency. Each modulated signal has harmonic frequency components and is input off-axis (230) relative to the cavity's optical axis (220). The cavity contains mirrors (210, 212, 214; 310; 410; 510, 512, 514) arranged in a predetermined configuration. The optical axis (220) is defined by a path passing through centers of mirrors (210, 212, 214; 310; 410; 510, 512, 514). The modulated light signal (570) is resonated off axis (230) without astigmatic optical. elements to produce CRDS signal and passes at least twice through cavity and across the mirrors (210, 212, 214; 310; 410; 510, 512, 814) without interfering, with itself. An overall path length through cavity is greater than path length of optical axis. A photodetector detects (550) the CROS signal, which is demodulated (560) dependent upon selected harmonics.
Abstract:
A laser spectrometer and method for measuring gas component concentration in a measurement gas, wherein light intensity from a wavelength-tunable laser diode is detected after irradiation of the measurement gas and a reference gas, and the concentration of the gas component is determined based on reduction of the light intensity by the absorption of light at the position of a selected absorption line of the gas component, and the position of the absorption line of the gas component is referenced based on a selected absorption line of the reference gas, and wherein there is a mixed operation consisting of actual measurements of fast concentration changes of the gas component to be measured and a short reference/standardization phase for wavelength referencing, line locking and standardization, where the duration of the actual measurement is measured such that measuring conditions remain constant and do not deviate from those during the reference/standardization phase.
Abstract:
The present invention relates generally to monitoring of biochemical amplification reactions using electromagnetic radiation, and more particularly to an apparatus for optical monitoring of isothermal and thermally-cycled amplification reactions using radiation ranging from the ultraviolet region through the infrared regions of the electromagnetic spectrum. Moreover, the method discussed herein could be similarly applied to any process that results in biochemical amplification, regardless of the specific technique employed.
Abstract:
An intracavity laser absorption infrared spectroscopy system for detecting trace analytes in vapor samples. The system uses a spectrometer in communications with control electronics, wherein the control electronics contain an analyte database that contains absorption profiles for each analyte the system is used to detect. The system can not only detect the presence of specific analytes, but identify them as well. The spectrometer uses a hollow cavity waveguide that creates a continuous loop inside of the device, thus creating a large path length and eliminating the need to mechanically adjust the path length to achieve a high Q-factor. In a preferred embodiment, the laser source may serve as the detector, thus eliminating the need for a separate detector.
Abstract:
A method and analyser for identifying, verifying or otherwise characterising a sample involves emitting electromagnetic radiation in at least one beam at a sample. The electromagnetic radiation includes at least two different wavelengths. A sample detector detects affected electromagnetic radiation resulting from the emitted electromagnetic radiation affected by the sample and provides output representing the detected affected radiation. A processor determines sample coefficients from the output and identifies, verifies or otherwise characterises the sample using the sample coefficients and training coefficients determined from training samples. The coefficients reduce sensitivity to a sample retainer variation and/or are independent of concentration.