Abstract:
A system for measuring optical detector linearity according to the present invention employs a laser source that illuminates an integrating sphere. The sphere randomizes the laser signal phase and produces a uniform intensity over the sphere output. A collimator expands the sphere output for entry into an interferometer, where the incident optical energy is amplitude modulated in a sinusoidal fashion by a linear mechanical mirror movement. Optical band filters eliminate significant harmonic content being present on a pre-detected optical signal. Sampling of the detected signal energy is performed synchronous to the mechanical mirror position to assure sinusoidal response. The sampled signals are processed to separately determine signal harmonic components attributed to detector non-linearity and multiple laser reflections within the system. The system utilizes at least two measurements at two different laser intensities. An optional third measurement of background radiance may be applied to the first two measurements to enhance accuracy.
Abstract:
Real time high speed high resolution hyper-spectral imaging. (a) electromagnetic radiation collimating element (16), collimating electromagnetic radiation (44) emitted by objects (12) in a scene or a sample (14); (b) optical interferometer (18), receiving and dividing collimated object emission beam, generating interference images, and piezoelectrically determining and changing magnitude of optical path difference of divided collimated object emission beam; optical interferometer (18) includes: beam splitter (20′), fixed mirror (22), movable mirror (24), piezoelectric motor (26), displacing movable mirror (24) along axis (60), distance change feedback sensor (28), sensing and measuring change in distance of movable mirror (24) along axis (60), piezoelectric motor controller (30), actuating and controlling piezoelectric motor (26); and thermo-mechanically stable optical interferometer mount (32A); (c) camera optics (34), focusing interference images of each optical path difference; (d) detector (36), recording interference images; processing unit (38), and (f) display (40).
Abstract:
An optical part driving device for moving an optical part, comprises; a driving timing pulley, a pair of driven timing pulleys, a timing belt wound by the driving timing pulley and the driven timing pulleys and connected with the optical part between the pair of driven timing pulleys, and a pair of tension pulleys for tensing the timing belt on both sides of the driving timing pulley.
Abstract:
A moving mirror support device for use with photo-interferometers having first leaf springs arranged in parallel with one end thereof being fixed to a base; a coupling plate fixed to the other ends of the first leaf springs; and second leaf springs arranged in parallel with each of the first springs with one end thereof being fixed to the coupling plate and the other end being fixed to the moving mirror, whereby longitudinal and transverse displacements of the moving mirror can be more accurately controlled.
Abstract:
A method for imaging a quantity of gas present in the atmosphere of a selected area. The method comprises the steps of directing background infra-red radiation from the selected area into an interferometer; imaging the infra-red radiation emerging from the interferometer onto at least one infra-red detector: obtaining a plurality of Fouriertransform infra-red spectra in the 8-14 micrometer spectral region, each spectrum coitesponding to infra-red radiation collected from a different portion of the selected area; and displaying in a suitable form an infra-red image, the infra-red image comprising the plurality of infra-red spectra, or quantities derived therefrom. The temperature of the quantity of gas or ambient temperature is measured, the temperature of the background is measured, and the difference between the two measured temperatures is used to derive gas column densities from the infra-red spectra.
Abstract:
A Michelson interferometer includes a beamsplitter onto which an input light beam is directed. The beamsplitter divides the input light beam into a first beam portion incident upon a first fixed reflector and a second beam portion incident upon a movable retroreflector. The movable retroreflector reflects the second beam onto another fixed reflector and then back to the beamsplitter where the first and second beams are combined and directed to a detector. The movable retroreflector is attached to one end of a rotating arm moving at a constant angular velocity. The retroreflector reflects the second beam at a fixed location in its orbital path. The angular velocity of the retroreflector and rotating arm combination may be varied over a wide range to provide a large modulated frequency bandwidth. The operating duty cycle of the interferometer may be doubled by attaching a second retroreflector to the other end of the rotating arm, with the weights of the two retroreflectors counterbalancing each other. The interferometer's optical alignment is insensitive to angular tilt and lateral shear (horizontal and vertical translation) of the interferometer's scanning element.
Abstract:
In a Fourier spectrometer arrangement for Fourier transforming an interferogram for determining the optic spectrum of a radiation, the readout of the interferogram is decoupled from particular phase positions of the reference signal through elimination of otherwise required synchronization with an external fixed clock pulse to thereby enable a lowering of the reference frequency and simultaneously to maintain or increase the scan frequency of the interferogram. The Fourier spectrometer arrangement includes an extrapolation filter which receives the incoming reference signal and employs adaptive state estimation processes in order to generate extrapolation values by which the future course of the reference signal can be projected. These extrapolation values can be calculated at times which are closer together than, e.g., zero crossings of the reference signal and may have an arbitrary phase position thereto. In this manner, the interferogram can be scanned at times which are independent of the phase position of the reference signal and, if necessary, at shorter intervals.
Abstract:
A multiplicity of one-piece flexure plates are assembled in pairs to provide a support system on which a retroreflector may be mounted for reciprocal motion. Combined with balance bodies, the flexure plates provide a support system having portions that are dynamically and statically balanced with one another, irrespective of orientation, so as to thereby immunize the unit against extraneous forces. The motion transfer assembly is especially adapted for use to support a moving retroreflector in a two-arm interferometer that may further include a beamsplitter assembly constructed from a one-piece, integrally formed body, the body having convergent, optically flat planar surfaces of specular reflectance, and means for adjustably mounting a beamsplitter therein. The spectrometer is of modular construction, and employs an integrated clocking sub-assembly as well as a light-weight voice-coil motor.
Abstract:
A fast and effective way to step a relative position quantity by a reference interval. Each step in relative position includes open-loop and closed-loop control intervals. The invention contemplates an actuator capable of changing the relative position and a closed loop servo that acts on the actuator to keep the relative position centered on the nearest one of a series of reference values separated by the reference interval. The actuator is preferably capable of a fast response. Stepping the relative position is accomplished as follows, assuming an initial condition where the servo has locked the relative position to a particular initial reference value. First, the actuator is caused to change the relative position by an amount approximately equal to the reference interval in a manner that the servo cannot track the change, such as by disabling the servo. Servo control is then re-established, at which point the servo operates to keep the relative position centered on the nearest reference value. Servo control is maintained until a new step is required, at which time the process is repeated.
Abstract:
The velocity of a moving mirror in a Fourier-transform infrared spectrometer is controlled by a circuit which utilizes a preset counter to generate pulses with a preset duration which are initiated at the zero-crossings of the signal from a detector of a laser light beam passed through the interferometer. This pulse signal is averaged and summed with a bias voltage and integrated and amplified to produce a drive current which is supplied to a drive coil which drives the moving mirror. When the mirror is moving too slowly, such that the preset duration pulses become a smaller fraction of the total time between zero crossings, the integrator provides an increased driving current and hence an increase in the speed of the mirror. If the mirror is moving too rapdily, the preset duration of the counter pulses will become a larger fraction of the time between zero crossings with a resultant reduction in the driving current and hence the velocity of the moving mirror.