Abstract:
A transmissive display system with a controllable display cell, such as a liquid crystal display cell, includes a pair of generally non-absorptive, high reflectance, low transmittance optical layers positioned opposite each other across the cell to provide improved image contrast. In one implementation, non-absorptive, high reflectance, low transmittance optical layers may be formed by dielectric coatings on inner surfaces of generally transmissive plates facing the display cell.
Abstract:
A device for optical parametric amplification utilizing four mirrors oriented in a nonplanar configuration where the optical plane formed by two of the mirrors is orthogonal to the optical plane formed by the other two mirrors and with the ratio of lengths of the laser beam paths approximately constant regardless of the scale of the device. With a cavity length of less than approximately 110 mm, a conversion efficiency of greater than 45% can be achieved.
Abstract:
A fiber optical attenuator utilizing the cut-off phenomenon for single mode propagation of an optical wave down a single mode fiber, comprising an element such as a pixelated liquid crystal element, capable of spatially changing the phase across the cross section of an input optical signal. Such a spatial phase change is equivalent to a change in the mode structure of the propagating wave. The signal propagating in the single mode output fiber is attenuated in accordance with the extent to which higher order modes are mixed into the low order mode originally present. When the mode is completely transformed to higher order modes, the wave is effectively completely blocked from entering the output single-mode fiber, and the attenuation is high. The level of attenuation is determined by the fraction of the wave which is converted to modes other than the lowest order mode, and is thus controllable by the voltage applied to the pixels of the liquid crystal element.
Abstract:
A reflection type Faraday rotator includes first to sixth reflection type sub-rotators. Light is made incident on the first to sixth sub-rotators while repeating reflecting thereat. A Faraday rotation occurs at a sub-rotator having a center wavelength equal to the wavelength of the light The sub-rotators are of reflection-type, have a larger bandwidth of outgoing light compared to a transmission type, and have center wavelengths (wavelength characteristics) different from one another. Thus, the effective wavelength range (the wavelength bandwidth) is increased. Expensive optical devices conventionally required for increasing the wavelength bandwidth are not needed. Accordingly, the cost can be reduced.
Abstract:
Single cell gap transflective liquid crystal display which provides that the backlight traverses the reflective pixel portion twice and thereby follows a path similar to that of the ambient light. A slant reflector is built on the path of the back light to reflect the transmitted light to the reflective portion so that the back light and ambient light follow similar paths.
Abstract:
This invention is related to method for assembling an optical attenuator to attenuate an optical beam. The method includes a step of a) collimating the optical beam from an input optical waveguide into a substantially collimated beam comprising an upper segmented-portion and a lower segmented-portion. The method further includes steps of b) transmitting the collimated onto a phase shifting means comprising at least an upper phase shifting means for generating a phase difference between the upper segmented-portion and the lower segmented-portion and c) generating a self-interference between the upper segmented-portion and the lower segmented-portion of the collimated beam and focusing the collimated beam into an output optical waveguide with an attenuation resulting from the self-interference.
Abstract:
An object of the invention is to provide a small and low-cost variable polarization plane rotator that can control a rotation angle of the polarization plane easily, and an optical device using the same. To this end, a variable polarization plane rotator according to the present invention is provided with a null/4 phase plate having an optical axis in the same direction as, or at a 90 degree angle relative to, a polarization direction of input light beam, to apply a 90 degree phase difference between polarization components parallel to and perpendicular to the optical axis thereof, a phase difference variable element having an optical axis at a null45 degree angle relative to the optical axis of the null/4 phase plate, to apply a variable phase difference between the polarization components parallel to and perpendicular to the optical axis thereof, and a phase difference adjustment section that adjusts the variable phase difference of the phase difference variable element, wherein the input light beam, after being transmitted through the phase difference variable element to be into elliptically polarized light or circularly polarized light, is transmitted through the null/4 phase plate to be into linearly polarized light, to thereby rotate the polarization plane of the input light beam by an angle corresponding to the phase difference applied by the phase difference variable element.
Abstract:
A variable optical attenuator including: a birefringent element positioned to separate an input optical signal into two spatially separated, orthogonally polarized beams; a LC modulator positioned to receive the orthogonally polarized beams and selectively alter their polarizations; a reflective element positioned to reflect the beams back through the LC modulator and the birefringent element, wherein the birefringent element recombines orthogonally polarized components of the reflected beams to produce an output optical signal; and a controller coupled to the LC modulator to selectively cause the LC modulator to alter the polarizations of the orthogonally polarized beams, wherein during operation the controller is responsive to a request to variably attenuate the intensity of the output optical signal relative to the intensity of the input optical signal to one of multiple non-zero attenuation settings.
Abstract:
The present invention relates to variable attenuation of an light beam by use of polarization rotators in which the degree of rotation of the polarization is determined by an externally-applied control signal leading to variable attenuation of the light beam under the control of the external signal. Randomly polarized light arrives at input port to the variable optical attenuator, encounters a birefringent crystal, is split into orthogonal polarization components and emerges from the crystal separated by a walk-off distance. The light beams then impinge on the surface of wave plates (polarization rotators) that are configured to cause a rotation of the plane of polarization by null45null and null45null rotation. Both light beams then impact a variable polarization rotator in which the plane of polarization is rotated through a angle that can be varied in response to an externally-applied control signal. The maximum operating range ( 0 to 100% attenuation) is achieved when the variable rotator is capable of rotations in the range null45null. A lesser range of attenuation is achievable with a smaller range of polarization rotation. The light beams then encounter a second birefringent crystal used as a beam displacer. The beams next encounter two wave plates configured to produce rotation angles of 0null and 90null respectively. The beams next strike a retroreflector that interchanges the vertical positions of the beams incident thereon. The returning light beams next encounter wave plates in the reverse direction followed by a reverse traverse that causes a rotation in the same sense and magnitude as on the forward traverse. The beams next encounter wave plates wave plates and birefringent crystal in the reverse direction, emerging at an output port attenuated in intensity.
Abstract:
An arrangement (10) for efficiently generating tunable pulsed laser output at 8-12 microns. The arrangement (10) includes a laser (12), a first optical parametric oscillator (14) of unique design, and a second optical parametric oscillator (22). The first oscillator (14) is constructed with an energy shifting crystal (20) and first and second reflective elements (16) and (18) disposed on either side thereof. Energy from the laser (12) at a first wavelength is shifted by the crystal and output at a second wavelength. The second wavelength results from a secondary process induced by a primary emission of energy at a third wavelength, the third wavelength resulting from a primary process generated from the first wavelength in the crystal. Mirror coatings are applied on the reflective elements (16 and/or 18) for containing the primary emission and enhancing the secondary process. The second optical parametric oscillator (22) then shifts the energy output by the first OPO (14) at the second wavelength to the desired fourth wavelength. In the illustrative embodiment, the first optical parametric oscillator (14) includes an x-cut rubidium titanyl arsenate crystal (20) and the second optical parametric oscillator (22) includes a silver gallium selenide crystal. The first wavelength is approximately 1.06 microns, the second wavelength is approximately 3.01 microns, the third wavelength is approximately 1.61 microns, and the fourth wavelength is in the range of 8-12 microns.