Abstract:
A heterodyne laser instantaneous frequency measurement system is disclosed. The system utilizes heterodyning of a pulsed laser beam with a continuous wave laser beam to form a beat signal. The beat signal is processed by a controller or computer which determines both the average frequency of the laser pulse and any changes or chirp of th frequency during the pulse.
Abstract:
In an interferometry wherein a light beam from a light source is divided in two, one of which is used as a reference beam and the other beam is used as an inspecting beam, and the two beams are projected again on an identical plane so as to form an interference pattern; a wavelength scanning type laser diode interferometry characterized in that a laser diode is employed as the light source, and that an injection current of the laser diode is modulated thereby to scan a wavelength of the laser diode and to change an intensity distribution of the interference pattern.
Abstract:
Method and device for realtime measurement of the state of polarization at a quasi-monochromatic light beam. Two quasi-monochromatic radiations with slightly different optical frequencies are generated. A radiation is converted into a 45.degree. linearly polarized radiation, while the other presents the polarization state imposed by a body under test. In each radiation, horizontal and vertical polarization components are separated, and then recombined into two different beams comprising radiations at both frequencies, respectively polarized in the same plane. Beatings between the two components of each beam are originated and from the two electrical signals in the radiofrequency range thus obtained the information is extracted on the relative phase and the amplitude of the two components of the radiation with polarization imposed by the body under test.
Abstract:
A scanning optical microscope causes a collimated light beam to impinge on a Bragg cell. A high frequency signal applied to another surface of the Bragg cell modulates the impinging light beam. The output of the Bragg cell comprises two waves: a portion of the impinging light beam which passes directly through the cell or diffraction grating, and a second deflected output beam whose frequency is shifted by the frequency of the applied signal. By modifying the frequency of the applied frequency signal, the deflected beam may be scanned across the surface, while the reference beam remains in place and serves as a phase reference. By detecting the two beams reflected from the surface on a single photodetector, shifts in phase and amplitude of the deflected beam can be determined. To provide further isolation of the system from external vibration, a second input light beam is applied to the diffraction grating, the input of this second beam being in a plane which is essentially perpendicular to the direction of the scanned output beam. This input beam, after passing through the diffraction grating, will provide two further beams which impinge on the surface. These two beams, which are to serve as reference beams, should be focused on a known flat surface; alternatively, the size of these beams may be expanded so their size is very large relative to any surface feature to be detected; or as a further alternative, they may be reflected from a known stable reference surface. In either event, the surface reflection of these beams is detected at a separate photodetector; upon mixing with the scan beam, the reference can be used to detect any changes in phase and amplitude, while cancelling out variations due to changes in frequency of the modulating optical wave.
Abstract:
A heterodyne phase-determining interferometer comprising a Smartt point diffraction interferometer (PDI) 10 in which the pinhole plate 22 is replaced by a half-wave, partially transmitting plate 22' with a pinhole 20 therein. The output beams 26 and 24 from the pinhole 20 are propagated through a frequency shifter 12 which includes a quarter-wave plate 28 whose axis is at 45.degree. to the polarization axes of the two beams 26 and 24 coming from the PDI 10, a half-wave plate 30 rotating at an angular frequency of .omega., and a linear polarizer which orients the polarization vectors of the two beams in the same direction along the propagation axis. The output of the frequency shifter 12 is a moving interference pattern consisting of alternate light and dark lines. This pattern is projected upon a phase-measuring means 14 comprising an array of photodetectors 34, 36 connected to a plurality of phase-to-voltage converters 38. There is one reference photodetector 34, the rest being test photodetectors. The reference photodetector 34 is connected to all phase-to-voltage converters 38, but each test photodetector 36 is connected to a different phase-to-voltage converter 38. The output of each converter 38 is the phase difference between the light at the point viewed by its associated test photodetector 36 and the light at the point viewed by the reference photodetector 34.
Abstract:
A device for the heterodyne detection of the image of targets illuminated by a laser, wherein the target reflects a wave .SIGMA..sub.1, which is amplified in an included refractive index variation medium also illuminated by a reference wave .SIGMA..sub.R derived from the laser to produce an amplified wave .SIGMA..sub.2. A portion of the wave .SIGMA..sub.1 prior to amplification is directed incident on a frequency shifter to produce frequency shifted wavefront .SIGMA..sub.10. Wavefront .SIGMA..sub.2 and the frequency-shifted wavefront .SIGMA..sub.10 are directed incident on the same partially reflection mirror to interfere with one another and the resultant beat interference wave is focused on a matrix of photodetectors and then filtered. This device has application to infrared image detection.
Abstract:
The invention provides optical measuring apparatus including a laser which is arranged to have an output of electromagnetic radiation including at least two different simultaneously-generated frequencies. This output is fed to a detector, such as an optical diode, which produces a corresponding electric signal at the difference (beat) frequency. The beat frequency, any change in the beat frequency, or any rate of change of the beat frequency can now be examined electrically to the degree of accuracy generally available in that art, usually to a much higher degree than is available in the optical or mechanical arts. The parameter to be examined may be that of an element causing the production of the beat frequency such as a birefringent material, or may be that of an element which changes the frequency in some way, such as an angular orientation of two quarter-wave plates.
Abstract:
The optical path lengths of a plurality of comparison laser beams directed to impinge upon a common target from different directions are compared to that of a master laser beam by using an optical heterodyne interferometric detection technique. The technique consists of frequency shifting the master laser beam and combining the master beam with a first one of the comparison laser beams to produce a time-varying heterodyne interference pattern which is detected by a photo-detector to produce an AC electrical signal indicative of the difference in the optical path lengths of the two beams which were combined. The optical path length of this first comparison laser beam is adjusted to compensate for the detected difference in the optical path lengths of the two beams. The optical path lengths of all of the comparison laser beams are made equal to the optical path length of the master laser beam by repeating the optical path length adjustment process for each of the comparison laser beams. In this manner, the comparison laser beams are synchronized or timed to arrive at the target within .+-.1.times.10.sup.-12 second of each other.
Abstract:
A portion of a first laser light beam of one optical frequency and a portion of a second laser light beam of a different optical frequency are mixed by a photoelectric device to produce an electrical reference signal having a countable intermediate frequency. Another portion of the first laser light beam traverses a fixed length optical path of an interferometer, and another portion of the second laser light beam traverses a variable length optical path of the interferometer. These other portions of the first and second laser light beams are mixed by another photoelectric device to produce an electrical information signal having the same countable intermediate frequency as the reference signal only while the optical length of the variable length optical path is not being changed. A reversible counter integrates the difference in frequency between the reference and information signals while the optical length of the variable length optical path is being changed to indicate the change in length of the variable length optical path.