TL;DR: In this article, the use of a phase filter to convert a gaussian laser beam into a beam with more uniform irradiance distribution is discussed, and the phase filter is calculated by employing an iterative procedure on a computer.
TL;DR: The optical transmission characteristics of electroformed metal grids with inductive and capacitive cross patterns have been investigated in the far-infrared spectral region and results are used to suggest construction guidelines for two-grid bandpass filters.
Abstract: The optical transmission characteristics of electroformed metal grids with inductive and capacitive cross patterns have been investigated in the far-infrared spectral region. The transmission characteristics of one-and two-grid devices are represented by transmission line theory parameters. Results are used to suggest construction guidelines for two-grid bandpass filters.
TL;DR: A simple method of constructing a holographic filter is described which transforms a Gaussian into a uniform beam and conserves 30% of the beam power.
Abstract: A simple method of constructing a holographic filter is described which transforms a Gaussian into a uniform beam and conserves 30% of the beam power.
TL;DR: In this paper, the design and performance of a 24-channel fluorescence detection system for use in x-ray absorption spectroscopy are discussed, and comparisons are drawn with other detection systems currently in use.
Abstract: The design and performance of a 24‐channel fluorescence detection system for use in x‐ray absorption spectroscopy are discussed, and comparisons are drawn with other detection systems currently in use. Each channel of the current system consists of a NaI scintillation detector with a filter and collimator arrangement designed to reduce the scatter and filter fluorescence background. Given a sufficiently intense and stable x‐ray source, this apparatus can record a useful EXAFS spectrum for an element (Z⩾23) at 100 ppm concentration in approximately 30 minutes. The new design permits the study of plate‐like samples (such as molybdenum enzyme solutions) unsuitable for previously described slit assemblies. Breaking the detection system up into discrete elements also allows (1) optimization of filter thickness for each direction, (2) use of a weighting scheme to optimize the total S/N, and (3) operation at high total count rates, while retaining the advantages of pulse counting electronics. The relative merits...
TL;DR: An optical filter member composed of a plurality of ND filters having different transmission factors and arranged circumferentially at regular intervals is disposed between a light source and a light guide of an endoscope as mentioned in this paper.
Abstract: An optical filter member composed of a plurality of ND filters having different transmission factors and arranged circumferentially at regular intervals is disposed between a light source and a light guide of an endoscope. When the optical filter member is rotated, a light beam with periodically varying luminance is transmitted through the light guide to illuminate an object inside a body cavity. Images of the object corresponding to different luminances are converted severally into video signals by a television camera. A signal component within a given level range is extracted from each of these video signals by a limiter. The signal components of the video signals are composed into video data to be supplied to a display. The display indicates the video data as an image with proper contrast.
TL;DR: An obstacle detector mounted on an automotive vehicle includes a light emitting element, which includes a semiconductor infrared laser, which transmits a light signal through an optical transmission system against any obstacle liable to present on the road on which the vehicle runs as mentioned in this paper.
Abstract: An obstacle detector mounted on an automotive vehicle includes a light emitting element, which includes a semiconductor infrared laser, which transmits a light signal through an optical transmission system against any obstacle liable to present on the road on which the vehicle runs The light signal has a wavelength which is 65 microns and which is of such a wavelength that solar light energy having the same wavelength as that of the light signal is not present, or is of very low intensity, at the surface of the earth and that the light energy from light sources such as the headlights of vehicles and/or streetlamps having substantially the same wavelength as that of the light signal, when the light energy has passed through the front glass of the headlights or streetlamps is not present or is of very low intensity An optical receiving system receives part of the light reflected by the obstacle and passes it to an optical filter which has a pass band width whose central wavelength is 65 microns The output of the filter is converted by a photodetector to a corresponding electrical signal for processing by a data processor in order to determine the distance from the vehicle to the obstacle, the azimuth of the obstacle, the velocity of the vehicle relative to the obstacle, etc
TL;DR: In-line fiber-optic spectral-bandpass filters with one, two, three, and four elements are designed in analogy to the Sole filters of bulk optics by bending the fiber into the form of small coils, which are rotated to suitable angles and arranged between polarizers.
Abstract: In-line fiber-optic spectral-bandpass filters with one, two, three, and four elements are designed in analogy to the Solc filters of bulk optics by bending the fiber into the form of small coils, which are rotated to suitable angles and arranged between polarizers. One four-element filter has a bandwidth of 3.5% at a center wavelength of 704 nm and a free spectral range of 17%.
TL;DR: In this paper, the large optical anisotropy of liquid crystal molecules is employed to realize an efficient, voltage tunable Fabry-Perot filter for both visible and middle infrared.
Abstract: The large optical anisotropy of liquid crystal molecules is employed to realize an efficient, voltage tunable Fabry-Perot filter. Tuning has been demonstrated in both the visible and middle infrared. The small voltages required to tune over one free spectral range (FSR) result in a device having greater potential for designing filters having a larger range of FSRs, and therefore bandpass widths, than is possible for the solid electro-optic Fabry-Perot described in previous work.1 We show that for many commercially available liquid crystal materials, infrared operation is possible over wide regions where molecular absorptions do not occur.
TL;DR: In this article, two types of optical multi/demultiplexers using a single-mode fiber for a two-way transmission system were described, one consisting of four bandpass filters and a short wavelength pass filter or a long wavelength pass filtering.
Abstract: This paper describes two types of optical multi/demultiplexers using a single-mode fiber for a two-way transmission system. One type, the filter type, consists of four bandpass filters and a short wavelength pass filter or a long wavelength pass filter. The other, the filter-grating type, consists of two bandpass filters and a grating. The present multi/demultiplexers have four channels with 1.05, 1.15, 1.3, and 1.5 μm wavelengths. Total insertion losses are less than 2.3 and 3.2 dB for the filter type and the filter-grating type, respectively. Cross-talk between channels is less than -40 dB.
TL;DR: In this article, a brief review is given of how fundamental concepts of thin film optics (potential transmittance, the two-effective interfaces theorem, the principle of equivalent layers, matching conditions and absentee layers) are used to design optical coatings with controlled absorptance.
Abstract: A brief review is given of how fundamental concepts of thin film optics (potential transmittance, the two-effective-interfaces theorem, the principle of equivalent layers, matching conditions and absentee layers) are used to design optical coatings with controlled absorptance. The general principles are illustrated by a discussion of interference filters containing both dielectric and metallic layers, including the design and preparation of induced transmission filters. Reference is also made to coatings for optimizing the photon efficiencies of photodetectors. Further insight into how coatings with absorbing layers function is provided by consideration of the electric field distribution of radiation within the coatings.
TL;DR: An ultrahigh-Q, tunable optical filter with a FWHM bandwidth of 41 MHz is demonstrated and degenerate phase-conjugation experiments in sodium suggest that a quantum efficiency of greater than unity can be attained on a cw basis.
Abstract: An ultrahigh-Q tunable optical filter with a FWHM bandwidth of 41 MHz is demonstrated. The filtering is produced by nondegenerate phase conjugation through four-wave mixing in atomic-sodium vapor. The filter is observed to have a maximum quantum efficiency of 4 x 10^-3. However, degenerate phase-conjugation experiments in sodium suggest that a quantum efficiency of greater than unity can be attained on a cw basis.
TL;DR: In this paper, the first demonstration of a polarization independent, integrated-optic wavelength filter is reported. But the work is limited to a pair of mismatched Ti-diffused lithium niobate waveguides.
Abstract: We report the first demonstration of a polarization‐independent, integrated‐optic wavelength filter. Polarization‐independent filtering is achieved via wavelength selective TE↔TM conversion between a pair of mismatched Ti‐diffused lithium niobate waveguides. A peak coupling efficiency of ∼75% and 5‐A filter bandwidth have been achieved.
TL;DR: In this paper, an optical filter for selectively transmitting light in a passband at the wavelength λ, including an initial polarizer with a polarization direction perpendicular to a beam path and a final polarizer spaced from the first polarizer along the path and having the same polarization direction, is described.
Abstract: Disclosed is an optical filter for selectively transmitting light in a passband at the wavelength λ, including an initial polarizer with a polarization direction perpendicular to a beam path and a final polarizer spaced from the initial polarizer along the path and having the same polarization direction. A birefringent element is positioned between the polarizers with an optic axis perpendicular to the path and rotated with respect to the polarization direction, the element having a birefringence which is zero at the wavelength λ. Lyot-Ohman and Solc embodiments of the filter are also described.
TL;DR: In this article, an optical track is provided which rotates with the assembly of interference filters to generate pulses from index markings in the optical track, spaced so that one pulse is generated for each angstrom of variation of the center frequency transmitted through an interference filter.
Abstract: In an instrument adapted particularly for analyzing agricultural products, such as grain, interference filters are rotated successively through an infrared wide wavelength band beam of light, which irradiates a sample of the product. Each of the interference filters operates to transmit a narrow wavelength band of light, the center frequency of which is scanned through a range of values as the angle of incidence of the beam of light to the interference filter varies as the filter rotates through the beam of light. An optical track is provided which rotates with the assembly of interference filters to generate pulses from index markings in the optical track. The markings in the optical track are spaced so that one pulse is generated for each angstrom of variation of the center frequency transmitted through an interference filter. The pulses are counted in the counter and the counts in the counter are used to control the selection of intensities reflected from the sample to be used in the analysis of the sample.
TL;DR: In this article, an approach for determining the position of a surface in which radiation from an optical radiant source is applied to the surface and, by means of a lens system, an image of the radiation is produced on a photoelectric receiver.
Abstract: Apparatus is disclosed for determining the position of a surface in which radiation from an optical radiant source is applied to the surface and, by means of a lens system, an image of the radiation is produced on a photoelectric receiver. A laser serves as the radiant source, and is aimed at an angle of inclination relative to an optical axis of the lens system at a point of a surface which, by virtue of its temperature, emits visible radiation in the same wavelength range as the Laser. The surface extends approximately perpendicularly of the optical axis and is subject to positional variations along the said optical axis. The beam is directed from the irradiated point to the photoelectric receiver through a narrow-band optical filter of which the pass band includes the laser wavelength.
TL;DR: In this paper, a temperature pattern distribution measuring method and apparatus by which portions of light from parts of an area of an object whose temperature distribution pattern is to be measured, and whose parts are in a predetermined pattern, are passed through first and second optical filters which respectively pass different wavelengths of light.
Abstract: A temperature pattern distribution measuring method and apparatus by which portions of light from parts of an area of an object whose temperature distribution pattern is to be measured, and whose parts are in a predetermined pattern, are passed through first and second optical filters which respectively pass different wavelengths of light. The level of engery passed by the respective filters for the respective portions of light are determined by scanning the light from the filters with a pickup device or devices and, by using the determined energy levels, an arithmetic unit carries out a two-color temperature determining operation for the respective parts of the area for determining the temperature on each part of the area of the object. The temperature pattern of the area of the object can thereby be determined from the temperatures of the parts of the area.
TL;DR: In this paper, a brief review of the properties of linear electro-optic materials is presented followed by descriptions of tunable birefringence interference filters, Fabry-Perot devices, and other novel filter structures.
Abstract: Electro-optically tunable spectral filters have been developed over the years and now include a rather diverse collection of devices. These devices, which are of increased importance for remote sensing applications, employ linear electro-optic (Pockets) materials such that tuning is accomplished via externally controlled voltages. A brief review of the properties of linear electro-optic materials is presented followed by descriptions of tunable birefringence interference filters, Fabry-Perot devices, and other novel filter structures. Recent developments in electro-optic tunable filters are included. Issues relating to the further development of infrared tunable spectral filters are discussed.
TL;DR: In this paper, a new circular dichroism (CD) and magnetic circular dichroidism (MCD) system with narrow bandwidth and high scanning rate has been developed, which is composed of an acoustic optical filter of TeO2 as a monochromator, a stress modulator, and a photomultiplier together with their operating devices and a computer system.
Abstract: A new circular dichroism (CD) and magnetic circular dichroism (MCD) system with narrow bandwidth and high scanning rate has been developed. The versatility of the system for the measurements of transient changes in CD and MCD has been also described. This new CD and MCD system is composed of an acoustic optical (AO) filter of TeO2 as a monochromator, a stress modulator, and a photomultiplier together with their operating devices and a computer system. The linearly polarized light from the AO filter is modulated to left‐ and right‐circularly polarized light by a stress modulator operated at 50 kHz. The absorbance difference of the left‐ and right‐circularly polarized light is detected by a photomultiplier, after passing through the sample. The whole optical system and detector system are matched in time by the same computer system. A rapid scanning was performed successfully at the rate of 50 nm range/10 ms, with better spectral resolution and higher signal‐to‐noise ratio than other commercially available ...
TL;DR: In this paper, the authors investigated the properties of polarization interference filters in the spectral regime between 5200 A and 5400 A, with a rate of dispersion that could provide a passband of only 1 A with a filter structure of several millimeters thick.
TL;DR: In this paper, a set of fine, uniform, translucent fibers mounted on a suitable holder is used to detect and register all validly sampled, single particle events, which can be used to accurately check the instrument calibration or response to particle size.
Abstract: A device comprising a set of fine, uniform, translucent fibers mounted on a suitable holder. When used in conjunction with appropriate neutral density optical filters, if necessary, on suitable particle sizing instruments, the device can easily and quickly be used to perform three important functions--namely, to accurately check the instrument calibration or response to particle size, to locate the limits of the optical depth of field in the particle illuminating beam, and to test the ability of the instrument to detect and register all validly sampled, single particle events.
TL;DR: In this paper, an optical polarization filter was constructed from a CdGa2S4 single crystal, which was temperature-tunable in the range 487-580 nm and the transmission at the maximum of the spectral characteristic was 48%.
Abstract: An optical polarization filter was constructed from a CdGa2S4 single crystal. This filter was temperature-tunable in the range 487–580 nm. Its pass band was 2 nm and the transmission at the maximum of the spectral characteristic was 48%. The filter was also capable of withstanding high-power laser radiation (damage threshold 32 MW/cm2).
TL;DR: In this paper, the formation of the intensity profile of laser radiation by the application of the spatial filtering and apodization method to a high-power neodymium system was investigated.
Abstract: A report is given of an investigation of the formation of the intensity profile of laser radiation by the application of the spatial filtering and apodization method to a high-power neodymium system. Optimal conditions are found for the filtering of spatial frequencies and the newly developed simplest vacuum spatial filter is described. The method for making soft apertures by the evaporation of metal films on glass substrates is reported together with a study of the apodizing properties of these apertures. A study of spatial coherence of apodized laser radiation is described. The results are given of the formation of a beam of high optical quality in a high-power system with an exit aperture 45 mm in diameter.
TL;DR: Novel passive recursive CCD bandpass filters have been realized using standard two-level-polysilicon gate NMOS technology to achieve low power consumption and an extremely stable center frequency and a bandwidth independently controlled by a capacitance ratio.
Abstract: Novel passive recursive CCD bandpass filters have been realized using standard two-level-polysilicon gate NMOS technology. A Chebyshev bandpass (w/SUB rel,/ /SUB 3/ /SUB dB/=3.1 percent) and a fully integrated CCD signal filter with an extremely narrow 3 dB bandwidth of 97 Hz (Q=1350) at 131.85 kHz center frequency were implemented by means of cascaded CCD resonators. The latter chip contains the necessary clock generation and biasing circuitry realized with dynamic circuit techniques to achieve low power consumption (40 mW per filter). Performing all filtering operations exclusively in the charge domain ensures filter passivity. An extremely stable center frequency and a bandwidth independently controlled by a capacitance ratio are the special advantages of such filters.
TL;DR: In this paper, the photoacoustic effect was used to detect the vibrating membrane of an acousto-optically modulated laser or a directly intensity modulated diode.
Abstract: Mechanical or electromechanical resonators, such as metallic bars or piezoelectric plates, play a major role in telecommunication and instrumentation, particularly in filtering devices. Their success arises from the fact that they are easi ly excited with an electrical signal (directly or with a transducer). Will their role remain essential with the advent of optical communication techniques ? It seems to us that the answer to this question depends partly on the optical methods to be used in exciting these resonators. One solution could be the photoacoustic effect. We have carried out p reliminary experiments with membranes excited by a modulated optical beam. Silicon membranes of thickness about 10 urn, of diameter a few millimeters, were excited by an acoustooptically modulated laser or a directly intensity modulated diode. Their impulse or continuous responses (f 10 kHz) were detected by the deviation of a narrow light beam reflected by the vibrating membrane.
TL;DR: In this paper, the formulation of phase conjugation via nondegenerate four-wave mixing in a Doppler-broadened resonant medium is generalized to include non-enerate pump frequencies.
TL;DR: It has been found that phase mismatch provides a window factor to the reflectivity that masks the frequency spectrum of the medium and that the line profile depends on the geometrical configuration of the three interacting beams.
Abstract: Backward nearly degenerate four-wave mixing close to the atomic resonance line has been investigated experimentally. It has been found that phase mismatch provides a window factor to the reflectivity that masks the frequency spectrum of the medium and that the line profile depends on the geometrical configuration of the three interacting beams. The capability of obtaining an optical bandpass filter with nearly degenerate four-wave mixing has also been demonstrated experimentally.
TL;DR: In this paper, a fiber optical measuring device for measuring physical and/or chemical parameters is described, which comprises a transducer unit and an evaluating unit, connected via at least one light conductor.
Abstract: The invention relates to a fiber optical measuring device for measuring physical and/or chemical parameters. The device comprises a transducer unit and an evaluating unit, connected via at least one light conductor. One or more light sources in the evaluating unit, via said at least one light conductor, illuminate one or more optical filters located in the transducer unit which filter(s) is (are) sensitive to the parameter being measured. An optical detector arrangement in the evaluating unit analyzes the light emanating from the transducer unit. The detector arrangement consists of one or more photo-detectors, arranged to sense the light emitted from the transducer unit after this light has been affected by at least one filter belonging to the detector arrangement. The spectral properties of the detector filter(s) are controlled so that the detector arrangement is able to measure the correlation between the spectra of the transducer and detector filters. The correlation values are used as a measure of the condition of the transducer filter and thus of the parameter(s) being measured.
TL;DR: In this paper, an optical system focuses the light emitted by a region of the original on a plurality of photo-sensors, the output signals of which are then amplified, selectively inverted, and added.
Abstract: A scanning device movable with respect to an original is provided for scanning the latter. An optical system focuses the light emitted by a region of the original on a plurality of photo-sensors, the output signals of which are then amplified, selectively inverted, and added. The summed up signal thus obtained is input into a processor which generates a driving signal for controlling a stylus which moves in synchronism with the original relatively to a printing cylinder, and engraves on it an image of said region. The response of the photosensors to light which issues from different parts of the region can be regulated by means of optical filters having locally varying densities.
TL;DR: In this article, a color picture projection system with an optical filter for removing the effect of chromatic aberration was presented. But the optical filter was not used to remove the effects of color aberration.
Abstract: A color picture projection system having a color picture light source and a lens system for magnifying the picture to project the same on a screen is provided with an optical filter for removing the effect of chromatic aberration The lens system has a simple structure, for instance, two parallel lenses, each designed to pass a given wavelength In a first embodiment, an annular optical filter partially blocks red and blue light rays incident on one side thereof In a second embodiment, two coaxial annular optical filters are combined in a single filter to partially block the red light rays incident on a first portion thereof and to partially block red and blue rays incident on a second portion which is outside the first portion