Abstract:
A system and method for sensing ambient light. The system has a first sensor for measuring a first ambient light level and a second sensor for measuring a second ambient light level. A processor in communication with the first sensor and the second sensor is configured to determine a relative intensity change in the ambient light levels for each of the first and second sensors. The processor also determines an ambient stability probability in response to the relative intensity changes in order to generate first and second filtered ambient light levels which are used as ambient light measurements.
Abstract:
A sensor head has a multiplicity of linear image sensors in correspondence with different radial directions of light emitted from a pixel in a pixel line of an LCD panel. The linear image sensors extends in the direction of the axis of an imaginary semi-cylinder. The linear image sensors have light receiving faces that are angularly spaced apart on an imaginary semi-cylinder, with their light receiving faces having normals passing through the axis of the imaginary semi-cylinder. Interposed in the space between the LCD pixel and the linear image sensors is an optical system having a multiplicity of light paths associated with respective angular components of the radiation emitted from the pixel line. Each of the light paths receives a predetermined angular component of light and transmits the light thus reveived to a corresponding one of the linear image sensors.
Abstract:
An apparatus for performing high speed scanning of an optical delay and its application for performing optical interferometry, ranging, and imaging, including cross sectional imaging using optical coherence tomography, is disclosed. The apparatus achieves optical delay scanning by using diffractive optical elements in conjunction with imaging optics. In one embodiment a diffraction grating disperses an optical beam into different spectral frequency or wavelength components which are collimated by a lens. A mirror is placed one focal length away from the lens and the alteration of the grating groove density, the grating input angle, the grating output angle, and/or the mirror tilt produce a change in optical group and phase delay. This apparatus permits the optical group and phase delay to be scanned by scanning the angle of the mirror. In other embodiments, this device permits optical delay scanning without the use of moving parts.
Abstract:
The earth horizon sensor apparatus uses first and second linear sensor arrays of sensor elements, the first and second linear sensor arrays being staggered with respect to each other. The sensor elements are preferably pyroelectric elements for detecting the presence or absence of infrared radiation from the Earth and Space. A microprocessor is used to determine which of the sensor elements subtends the diffuse horizon gradient and the constant zero radiance of Space. The attitude of the spacecraft is thereby calculated.
Abstract:
A method and apparatus for performing optical imaging on a sample wherein longitudinal scanning or positioning in the sample is provided by either varying relative optical path lengths for an optical path leading to the sample and to a reference reflector, or by varying an optical characteristic of the output from an optical source applied to the apparatus. Transverse scanning in one or two dimensions is provided on the sample by providing controlled relative movement between the sample and a probe module in such direction and/or by steering optical radiation in the probe module to a selected transverse position. The probe module may be an external module or may be an endoscope or angioscope utilized for scanning internal channels. Multiple optical paths may be provided for parallel scanning and focus may be enhanced by varying the focal point in the sample in synchronism with longitudinal scanning of the sample.
Abstract:
A two dimensional weak emitted light measuring device for determining and indicating the intensity and location of single photon light emitted from a specimen excited by radiation. The device includes an incident position detecting tube and a calculating unit for generating coordinates of the incident radiation and a data processing unit for producing specimen identification data in response to the coordinates and timing signals.
Abstract:
An atomic beam is excited by laser radiation to a state with large principal quantum number. The beam is irradiated with infrared or millimeter wave radiation which is to be detected. The atoms absorb the radiation by making transitions to higher-lying states. The transitions are sensed by applying an electric field which ionizes atoms in the final state, but not the initial state. The ions ae collected and detected by conventional pulse-counting or direct current methods.
Abstract:
A device for reconstruction of the absorption values in a layer of a body from measured values taken along strips in the body is disclosed. The absorption values are obtained from the measured values by an analog or a digital device, using a transversal filter in which the measured values are assigned weighting factors in accordance with predetermined criterion.
Abstract:
An improved integrating nephelometer having superior sensitivity and long-term stability to previous designs includes a container defining a measurement chamber. A continuously energized light source, such as a tungsten filament incandescent bulb, illuminates the measurement chamber through an opal glass diffuser. The intensity of the light source is regulated in one embodiment by a simple optical-electric feedback system, and in another embodiment by a voltage regulated supply. A cone of observation of the chamber is defined by a plurality of spaced, apertured plates located in the chamber, at right angles to the light source. A measuring photomultiplier tube views the cone of observation and provides an output signal including components resulting from detected photoelectrons, noise, and thermally emitted "dark current" electrons. A photon-detecting apparatus removes the noise component and provides an output pulse for each photoelectron and "dark current" electron. The output pulses are counted, and converted into an analog signal representing a desired extinction coefficient b.sub.scat by any one of a number of apparatus, including an averaging circuit, or a second counter and a D-to-A converter. Dark current compensation, if necessary, is effected by either subtracting a fixed value, or a value dependent on some environmental variable, from the measured value of b.sub.scat, or by utilizing a reversible counter apparatus and light source apparatus.Variations of this nephelometer are also described, including an instrument for automatically compensating for the component of b.sub.scat due to Rayleigh scatter by gases, an instrument which is sensitive to a plurality of wavelengths, and a self-calibrating instrument which is adapted for the measurement of total light scatter and back scatter at a plurality of wavelengths.
Abstract:
The light output of pyrotechnic luminants under dynamic conditions can be nitored to obtain data representative of ground surface illumination as a function of time and position of the illumination source. An array of photocells is disposed at substantially ground level throughout the range testing area, these photocells being sequentially scanned to provide a serial electrical data output during the firing of a pyrotechnic luminant-containing projectile over the range testing area. The serial data is transmitted to a remote control location whereat the data is received, sequentially demodulated, and converted into an optical display synchronously with the scanning in a pattern which simulates the illumination impinging on the photocell array. The position of the projectile over the range testing area is simultaneously tracked and a tracking information display is also provided. The illumination display pattern is recorded in correlation with the tracking information display so as to provide a frame-by-frame record of the ground surface illumination of the luminant as a function of time and the position of the illumination source.