Abstract: A multiband photoconductive detector and method for simultaneously and separately detecting and distinguishing light or radiation from a large number of different wavelength bands is disclosed. The multiband photoconductive detector comprises a plurality of low energy gap semiconductor layers of preselected progressively decreasing thicknesses of a first material, a plurality of high energy gap semiconductor layers of a second material interleaved with the plurality of low energy gap semiconductor layers, and a plurality of pairs of electrical contacts respectively applied to the plurality of low energy gap semiconductor layers and adapted to respectively receive associated bias voltages to enable the plurality of low energy gap semiconductor layers to constitute a corresponding plurality of separate photoconductive detectors with a preselected plurality of different wavelength bands.

Abstract: An apparatus and method are disclosed for optimizing the modulation efficcy of a remotely-located, polarization-sensitive, integrated optic modulator which is addressed with a non-polarization preserving fiber link. In a preferred embodiment of the invention, the polarization state of an input light beam is changed as a function of first and second control signals that are applied to the polarization controller. The non-polarization preserving fiber link conveys the light beam with the changed polarization state to the integrated optic modulator. The integrated optic modulator modulates the light beam with the changed polarization state as a function of any information signal to develop an intensity modulated optical signal. If no information signal is present, the optical signal from the modulator is not modulated. An output fiber conveys the optical signal from the integrated optic modulator to a locally-positioned detector for detection.

Abstract: A room temperature solid state laser for producing a laser emission at a wavelength of substantially 2 microns is disclosed. In a preferred embodiment, the laser comprises: a laser crystal having a host crystal material doped with an effective percent concentration of CR.sup.3+ sensitizer ions and with an effective percent concentraton of Tm.sup.3+ activator ions; and a flashpump for exciting the laser crystal to produce a laser emission at substantially 2 microns at a slope efficiency of at least 2 percent.

Abstract: A room-temperature, solid state laser for producing a CW laser emission cinuously tunable over the approximate spectral range of 1.86 to 2.14 microns is disclosed. In a preferred embodiment, the laser comprises: a diode pump laser for producing a CW pump beam at a preselected wavelength; a laser cavity defined by first and second reflective elements opposing each other on a common axis to form a reflective path therebetween; a laser crystal disposed in the laser cavity, the laser crystal having a host material doped with a concentration of thulium activator ions sufficient to produce a CW laser emission in the range of a plurality of wavelengths determined by the Stark components in the .sup.3 F.sub.4 to .sup.3 H.sub.

Abstract: A room temperature laser system for producing a CW laser emission at substially 2.3 microns is disclosed. In a preferred embodiment, the laser system comprises a laser diode source for producing a CW pump beam at a preselected wavelength; and a fiber laser doped with thulium activator ions sufficient to produce an output CW laser emission at a wavelength in the range of 2.2-2.5 microns when the fiber laser is pumped by the CW pump beam.

Abstract: A room-temperature, laser-pumped, Q-switched, thulium-doped, solid state laser for producing pulses of laser emission at substantially 2 microns is disclosed. In a preferred embodiment, the laser comprises: a laser cavity defined by first and second reflective elements opposing each other on a common axis to form a reflective path therebetween; a laser crystal disposed in the laser cavity, the laser crystal having a host material doped with an amount of thulium activator ions sufficient to produce a laser emission at substantially 2 microns from the .sup.3 F.sub.4 to .sup.3 H.sub.

Abstract: A method of measuring the lattice parameter in an unknown single crystal by omparing its diffraction angle to a standard single crystal, on a double-crystal diffractometer is disclosed.

Abstract: In a preferred embodiment, the optometer apparatus includes: a pinhole apure plate having first and second horizontally positioned apertures disposed on opposite sides of a first optical axis; first and second orthogonally-oriented polarizing filters respectively covering the first and second horizontally positioned apertures; a positive lens having an optical axis on the first optical axis and being positioned at a distance of approximately one focal length from the pinhole aperture plate; a lens system having an optical axis on the first optical axis; a slit aperture plate having a vertical slit and being disposed on the first optical axis and between the positive lens and the lens system; third and fourth vertically positioned polarizing filters selectively disposed adjacent to the slit aperture plate to divide the slit vertically, the third and fourth polarizing filters being respectively oriented parallel to the first and second polarizing filters; a monochromatic light source for propagating light along

Abstract: An apparatus for measuring leaks associated with a sealed lamp assembly, ludes an RF source for establishing an ionizing discharge in association with the lamp assembly, a source of continuous-wave probe radiation for irradiating the established ionizing discharge, and a pickup coil and associated circuitry for monitoring current flow through the ionizing discharge in response to the probe irradiation of the ionizing discharge. A signal is provided representing changes in the ionizing discharge resulting from the probe irradiation. A partially reflecting mirror partially deflects a portion of the probe radiation before it reaches the ionizing discharge. A signal is provided representing the deflected probe radiation. A computer receives the signals representing the changes in the ionizing discharge and the signals representing the deflected probe radiation, whereby the computer provides data representing pressure changes in the sealed lamp assembly.

Abstract: A hydrophone mounted on the hull of a ship comprises an electromechanical ansducer made of void-containing ceramic material having a high piezoelectric sensitivity to water-borne acoustic sound signals, a transducer made of solid ceramic material having a low piezoelectric sensitivity to hydrostatic acoustic signals, both transducers having similar piezoelectric sensitivity to shipboard noise transmitted via the ship's hull and transducer mounting; and means for sensing and manipulating voltage signals generated in response to water-borne acoustic signals and mount-transmitted shipboard noise such that the mount transmitted noise signals are largely cancelled out and a relatively noise-free signal representing hydrostatically transmitted sound is obtained.

Abstract: An integrated-optic, polarization-selective phase modulator is disclosed. a preferred embodiment of the invention a channel waveguide provides a path therethrough for polarized light having horizontal and vertical polarization components, and an electrode structure is disposed above the channel waveguide and is responsive to the application of a control voltage to the electrode structure for substantially phase modulating only the vertical component of the polarized light.

Abstract: A semiconductor laser structure for generating high frequency modulation of light intensity is disclosed. The apparatus comprises a seminconductor substrate, a semiconductor master laser and first and second semiconductor slave lasers fabricated adjacent to each other on the semiconductor substrate. Bias current applied to the master oscillator is modulated at a preselected frequency to cause the master laser to generate a plurality of optical frequency modulation sidebands. The first and second slave lasers, which are tuned to be close to the preselected first and second sidebands of the master laser, are injection-locked to the first and second preselected sidebands of the master laser.

Abstract: An apparatus for generating coherent radiation at a desired frequency is disclosed. In a preferred embodiment the apparatus comprises: an injection-locked semiconductor diode structure having a large active area for emitting a diffraction-limited beam at a preselected frequency; optics for focusing the diffraction-limited beam into a focused beam; a nonlinear crystal responsive to the focused beam for producing a beam of laser power which includes an output beam at a desired harmonic of the preselected frequency; and a device for passing the output beam in a given direction. In a modification of the preferred embodiment, the output of the injection-locked semiconductor diode structure is mixed with an emission from a laser source in the nonlinear crystal to produce a desired sum or difference frequency.

Abstract: An apparatus and method for minimizing polarization-induced signal fading in an interferometric fiber-optic sensor is disclosed. In a preferred embodiment of the invention, the polarization state of an input light beam is changed by a polarization controller as a function of first and second control signals applied to the controller. The input light beam with the changed polarization state is applied to the input of an interferometric fiber-optic sensor, causing the interferometric fiber-optic sensor to form an interference pattern at its output. This interference pattern is photodetected to develop an electrical signal that has a peak-to-peak amplitude proportional to the visibility of the interference pattern.

Abstract: A new serial interferometric fiber-optic sensor array configuration is diosed. In a preferred embodiment of the invention pulsed light from a laser source is transmitted into a long input fiber which forms a series of N sensor elements, each of optical path length L. Each sensor element is responsive to any change in an associated predetermined physical parameter for changing its optical path length. A small portion of the optical power in the input fiber is tapped-off to a long output fiber at tap points between adjacent sensor elements and at tap points before the first and after the last sensor elements in order to produce at the output of the last sensor element a series of N+1 pulses separated in the time domain. This series of N+1 pulses from the output of the last sensor element is applied to each of two paths in a compensating interferometer of optical path imbalance L.

Abstract: Three sampling circuits, a subtraction circuit, and a divider circuit cooate to sample an output signal from a nonlinear interferometric sensor at proper times, to subtract output signal samples to obtain a difference signal, and to divide an output signal sample into the difference signal to remove noise-induced modulation from the output signal.

Abstract: An improved gas sensor which optically senses a signal indication proportional to the concentration of a paramagnetic/diamagnetic gas in a gaseous mixture. In a preferred embodiment of the invention a chamber is adapted to contain a gaseous mixture to be measured for the concentration of a paramagnetic/diamagnetic gas in the mixture. An optical source provides light to a movable element coupled to the chamber. In response to the application of a magnetic field across the chamber, any paramagnetic/diamagnetic gas in the chamber causes the movable element to be displaced by a distance proportional to the concentration of the paramagnetic/diamagnetic gas in the gaseous mixture. A photodetector circuit receives light from the movable element having a characteristic indicative of the distance that the movable element was displaced. In response to such received light, the photodetector provides a signal output proportional to the concentration of the paramagnetic/diamagnetic gas in the gaseous mixture.

Abstract: A narrow-bandwidth, unstable laser resonator comprising: an output section ncluding a laser gain medium for generating and amplifying light, a first reflective element for reflecting and collimating light from the gain medium back through the gain medium, and a second reflective element having a hole therein, the second reflective element being responsive to the collimated light passed through the gain medium for reflecting most of the collimated light out of the unstable laser resonator as an output beam and for passing the remaining portion of the collimated light through the hole therein as a residual beam; and a feedback ring including an optical path, a beam splitter for passing a first portion of the residual beam into the optical path in a first direction, a frequency-narrowing element disposed at a position in the optical path where the first portion of the residual beam is collimated, the frequency-narrowing element being operative to narrow the frequency bandwidth of the first portion of the residua

Abstract: A method for growing a patterned superconductive oxide film of the general formula XZ.sub.2 Cu.sub.3 O.sub.6+x is disclosed, wherein X is yttrium, a lanthanide or a mixture thereof, Z is one or more alkaline earth elements and x is a number between 0 and 1. This patterned superconductive oxide film of XZ.sub.2 Cu.sub.3 O.sub.6+x is formed by preparing an aqueous solutuion of the nitrates of X, Z and Cu in the X:Z:Cu stoichiometric ratio of 1:2:3; spraying the aqueous nitrate solution onto a heated substrate to form on the substrate a thin film of XZ.sub.2 Cu.sub.3 O.sub.y material, wherein y is an undefined number; spot-heating preselected portions of the thin film in an oxygen-rich atmosphere to convert the preselected portions into the patterned superconductive oxide film of XZ.sub.2 Cu.sub.3 O.sub.6+x ; and removing the unheated thin film of XZ.sub.2 Cu.sub.3 O.sub.y material with a solvent.

Abstract: The invention presents means for protecting a remote sensing device such as missile seeker unit from damaging radiation outside of the sensing band of the detector and interrogating radiation attempting to determine the operating band of the sensor, its modulation rate, timing signal, or similar data which might be used to deteriorate the performance of the sensor.