Abstract:
An interferometer which may be used in a Fourier transform infra red spectrometer comprises a beam splitter (10), first and second fixed mirrors (18,26), path length variation means (20), and a folding mirror (16). The optical components are mounted on a casting (8) such that the beam splitter (10) and folding mirror (16) are arranged parallel to each other and the fixed mirrors (18,26) are attached to a single face of the casting in the same plane. The path length variation means (20) comprises two parallel opposed mirrors (22,24) which are rotatable to vary the length of the optical path between the beam splitter (10) and the fixed mirror (26).
Abstract:
The wavelength (λ) of light to be measured is determined in accordance with the formula λ = Ds/N from the number (N) of interference fringes having predetermined repeating waveforms that occur when the optical path length is changed by the quantity Ds by moving continuously a movable portion (7) of an interference spectrometer portion (1) of a wavelength measuring apparatus at a constant speed. A wave number counter (13) counts the number of specific points in each period of the interference fringes entirely from a predetermined measuring start point to a predetermined measuring finish point to obtain wave number data (Na). A reference pulse generation portion (21) generates reference pulses having a higher frequency than the repeating waveforms of the interference fringes. Detection portions (22a, 23a) detect the first number of the reference pulses existing in one period of the interference fringes, the second number of the reference pulses existing inside the period from the measuring start point till the first specific point of the interference fringes in succession to the measuring start point and the third number of the reference pulses existing inside the period from the final specific point of the interference fringes to the measuring finish point. A calculation portion (26) corrects the wave number data (Na) to wave number data (N A ) inclusive of fraction values using the first, second and third numbers, and measures highly precisely the wavelength of light to be measured in accordance with the following equation: λ = Ds/N A .
Abstract:
There is disclosed an interference spectrophotometer which collects data while monitoring the position of a movable mirror by providing quadrature control to accurately perform coherent addition of data. The spectrophotometer includes a main interferometer (100), a control interferometer (12), a sliding controller (20) controlling movement of the movable mirror (6), an A/D converter (47) converting analog data obtained by the main interferometer into digital form, a register (106) for holding data obtained by one scan of the movable mirror, a memory (108) for accumulating data obtained by numerous scans of the movable mirror, an up/down counter (82) receiving the output signals from two detectors included in the control interferometer, and a decision part (110). When the counter's value varies, the counter causes the A/D converter to perform its A/D conversion. Then, the decision part checks the counter's value after the A/D conversion. If this value differs from the count value obtained prior to the A/D conversion, the data held in the register is discarded.
Abstract:
In a device which extracts an optical interference signal (SA) for analyzing the spectrum of light to be measured, the light (11) to be measured is incident to an optical interferometer (20) capable of sweeping an optical path difference and interference light output therefrom is converted into an electric signal to obtain an optical interference signal (SA). On the other hand, the optical power of the light (11) to be measured is extracted to create an optical power signal, which is provided to a divider, wherein the optical interference signal is divided by the optical power signal to obtain a noise-free optical interference signal.
Abstract:
There is disclosed an interference spectrophotometer which collects data while monitoring the position of a movable mirror by providing quadrature control to accurately perform coherent addition of data. The spectrophotometer includes a main interferometer (100), a control interferometer (12), a sliding controller (20) controlling movement of the movable mirror (6), an A/D converter (47) converting analog data obtained by the main interferometer into digital form, a register (106) for holding data obtained by one scan of the movable mirror, a memory (108) for accumulating data obtained by numerous scans of the movable mirror, an up/down counter (82) receiving the output signals from two detectors included in the control interferometer, and a decision part (110). When the counter's value varies, the counter causes the A/D converter to perform its A/D conversion. Then, the decision part checks the counter's value after the A/D conversion. If this value differs from the count value obtained prior to the A/D conversion, the data held in the register is discarded.
Abstract:
A particular area or areas are monitored for the presence of gaseous materials, particularly pollutants by analyzing background infrared radiation present in the selected area with a spectrometer and making the results of this analysis available in a form understandable to the person or device monitoring the area for the presence of specified gaseous materials. The results of the spectrometric analysis may, for example, be displayed on a video unit or they may be printed. Apparatus useful in the practice of this invention generally includes an interferometer of the Michaelson-Morely type having specific optical characteristics, a sensitive infrared detector, electronic data processor, and a device which records and/or displays the results of the determination(s). In a preferred embodiment, no radiation concentrating or focusing elements are used ahead of the beamsplitter of the Michelson-Morely interferometer, said interferometer having imaging optics which, combined with detector size, results in the optical field of view being essentially no larger than the area of the remote source employed.
Abstract:
In a two-beam interferometer for use in a Fourier transform spectrometer a swinging member (1) is provided with a pair of movable flat mirrors (2a, 2b) fixedly standing thereon oppositely in parallel at an interval, said swinging member (1) being adapted to be rotatably swung in planes meeting at right angles with directions in which said movable flat mirrors (2a, 2b) stand. Further, a beam splitter (4) making a reflected beam (5a) incident upon one of said pair of movable flat mirrors and making a transmitted beam (5b) incident upon the other of said a pair of movable flat mirrors and a pair of fixed mirrors (6a, 6b), upon which said reflected beam (5a) and said transmitted beam (5b) reflected by the respective movable flat mirrors are incident, and which make the respective beams incident upon said beam splitter (4) again through the respective movable flat mirrors, being arranged at positions other than the swinging member (1), such that the reflected beam (5a) and the transmitted beam (5b) incident upon the respective movable flat mirrors being incident upon the other opposite movable flat mirror and then upon said respective fixed mirrors (6a, 6b) and the beam splitter (4), respectively.
Abstract:
An improved interferometer is provided which is of simplified construction and gives enhanced, accurate interference analysis through provision of an alterable masking device (14) located at the interference plane which facilitates rapid computer analysis of an interference pattern. The interferometer of the invention preferably includes a source of electromagnetic radiation, a beam splitter (22), a lens (28) for convergence and interference of the beams, a masking device (14) located at the region of beam convergence, and detection apparatus (16) for receiving and analyzing radiation from the mask. The mask is preferably stationary and electrically alterable and advantageously includes a base along with separate, plural masking structures (36-48) mounted on one base face with electrical connections coupled to the separate masking structures. The masking structures are formed of a crystalline or polycrystalline thermo or electro diachromatic substance such as vanadium dioxide.
Abstract:
A remote sensor for detecting gas, vapour or aerosol comprising means to measure the change in temporal coherence of light of a selected narrow waveband when it interacts with the gas etc. The light can be provided by a laser source or spectrally filtered sunlight etc. Received radiation 41 is split in to two, beams by a Fresnel biprism 44 and then detected by a detector 46 sensitised by a modulating reticle 47 to interference fringes. A glass delay plate 45 of suitable thickness is placed in the path of one of the beams such that only received radiation having a temporal coherence greater than a minimum determined by the plate thickness produces an output signal from detector 46. The minimum temporal coherence is set higher than the temporal coherence of the illuminating radiation. In alternative arrangements a band-pass temporal coherence filter may be used and the sensor can be made to spectrally scan the field of view by using a tunable laser or a variable centre frequency band-pass optical filter.