Hrl Laboratories, LLC

Hughes Aircraft Company

Hughes Electronics Corporation

Other

Raytheon Company

Sdl Inc.

Mrl Laboratories, LLC

David M Pepper

Gilmore Joseph Dunning

Thomas R O'Meara

Keyvan R Sayyah

David S Sumida

Marvin B Klein

Hans W Bruesselbach

Monica Minden

Marvin E Klein

Bernard H Soffer

Hossein H Izadpanah

Anson Y Au

Richard C Lind

Phillip V Mitchell

Daniel Frederic Sievenpiper

Peter David Brewer

Tsung-Yuan Hsu

David D Nolte

Gerald David Bacher

Uzi Efron

Shin-Tson Wu

Bruno F Pouet

Bryan H Fong

Richard P Berg

David F Welch

Yuri Owechko

Daniel Yap

Robert J Lang

Emanuel Marom

Jesse N Matossian

Marko Sokolich

Ronald Regis Stephens

Jack L Feinberg

Robert W Schumacher

Stuart MacCormack

Metin S Mangir

Stephen W McCahon

Dennis C Jones

Cris Jones

Ruth A Mullen

Richard R Craig

Wilbur P Brown, Jr

G David Bacher

Davis A Rockwell

Deborah Vogel

Keyyan Sayyah

John Anthony Coy

Meng P Chiao

Kenneth Bacher

A spatially and spectrally distributed long-laser system. Spatially separated phase-conjugate mirrors (PCMs) define a long-laser resonator cavity. The PCMs define, respectively, a power transmitting unit (master), and a power receiving unit (slave), as well as providing a secure two-way communications link between the units. The long-laser is mode-locked, minimizing third-party interception and detection. A wavefront-reversal device, using a MEMS spatial phase modulator, integrated with a retroreflector array, provides a true phase-conjugate (time-reversed) replica of the beam at each end of the system, providing auto-alignment, diffraction-limited performance, compensation for static and dynamic phase and polarization distortions, minimizing the FOV and scattering. The retroreflecting array initiates the oscillation mode. The SPM adaptive optical system bootstraps the retro-array by forming a simultaneous closed-loop system. The PCM emulates a deformable mirror with an integrated cat's eye retro-array, on a pixel-by-pixel basis, equivalent to a true wave-front reversal device at each end of the system.

Spectrally and spatially distributed phase-conjugate, long-laser resonator

A diffraction-limited, programmable pulse shaping network using a virtually integrated phased array (VIPA)-grating pair, integrated with a 2-d transmissive phase-only spatial light modulator (SLM) and a retro-array phase-conjugate mirror (RA-PCM). A high-temporal resolution, broadband pulse shaping network is realized using a 2-D VIPA-grating dispersive element pair, with a programmable SLM at a common Fourier transform plane. True wavefront reversal ('time reversal') is realized using a self-starting RA-PCM, which compensates for system path distortions, misalignment, beam wander, vibrations and optical aberrations. Upon reverse transit through the system, the RA-PCM wavefront matches the set of virtual images emerging from the VIPA. The RA-PCM is a self-starting, low-power device, without frequency shifts, doesn't require pump beams and/or the need for high-intensity stimulated scattering threshold conditions to be met. Polarization decoupling enables the RA-PCM to compensate for optical distortions, while enabling the SLM to generate real time Fourier phase masks for programmable pulse shaping.

Programmable pulse shaper using a VIPA-grating pair integrated with a spatial light modulator and a retro-array phase-conjugate mirror

An IR laser source providing light in the IR spectrum, the laser source comprising a pump laser operating at a frequency equivalent to wavelength shorter than 2 &#x3bc;m and at a predetermined power, and an optic fiber coupled to the pump laser. The optic fiber has at least a section of a hollow core photonic crystal fiber, the at least a section of hollow core photonic crystal fiber being designed to have at least a passband in the IR spectrum and being filled with a molecular gas for triggering at least one Stoke's shift in the light entering the at least a section of hollow core photonic crystal fiber for the particular power of the pump laser, the at least one Stoke's shift be selected to cause the light entering the at least a section of hollow core photonic crystal fiber to shift in frequency into the passband in the IR spectrum of the hollow core photonic crystal fiber.

Molecular gas-filled hollow core photonic crystal fiber laser at infra-red wavelengths

An optical MEMS retro-reflective apparatus with modulation capability having a retro-reflecting structure including a pair of reflective surfaces; and a MEMS device for moving at least one of the reflective surfaces of said pair of reflective surfaces relative to another one of the reflective surfaces of said pair of reflective surfaces a distance which causes the pair of reflective surfaces to switch between a reflective mode of operation and a transmissive mode of operation. A substrate and a moveable grating structure may be substituted for the reflective surfaces.

Optical retro-reflective apparatus with modulation capability

A coherent laser receiver for receiving encoded light which may have propagated over an aberrated path, situated between a source of the encoded light and the coherent receiver. The coherent laser receiver comprises a bundle of optical fibers arranged in an array to receive light, as encoded from a distant optical transmitter or reflective surface, the encoded light from the distant optical transmitter or reflective surface is received by at least a majority of the fibers in the array. A plurality of light amplifiers is provided for amplifying the received encoded light. A control apparatus coherently combines a composite output of the bundle of optical fibers, the control apparatus includes at least one detector for detecting the a portion of the received encoded light, an output of the at least one detector being utilized to control the plurality of light amplifiers so that differential phases among individual fibers associated with said at least one detector in the bundle are minimized by said light amplifiers. A coherent detector is responsive to the composite output of the bundle for providing an output signal representative of the encoded information from the source.

Phase control of a fiber optic bundle

A method and apparatus for a photoinduced electromotive force sensor. The sensor has an active substrate formed of a semi-insulating photoconductor with sufficient carrier trap density to form an effective charge grating and pairs of electrodes disposed on the active substrate, where the sensor is configured to reduce the photovoltaic effect caused by the incident light in the vicinity of the electrodes. The shape or composition of the electrodes may be selected to reduce the photovoltaic effect or the electrodes may be disposed on the substrate to average out the photovoltaic effect arising from each one of the electrodes.

Method and apparatus for reduction of non-adaptive signals in photo-EMF sensors

Compact, tunable, efficient IR laser and IR guiding silica fibers

An optical time delay module has a plurality of time delay elements connected in a series and a plurality an optical output couplers wherein each of said optical output couplers is operationally connected between one or more time delay elements in said series, the optical output couplers providing a plurality of optical outputs from said module with different optical delays controlled by an analog voltage.

Optical tapped time delay modules and arrays

An optical time delay module has a plurality of time delay elements connected in a series and a plurality an optical output couplers wherein each of said optical output couplers is operationally connected between one or more time delay elements in said series, the optical output couplers providing a plurality of optical outputs from said module with different optical delays controlled by a digital control word.

Digitally controlled optical tapped time delay modules and arrays

The disclosed technology provides a dynamic interconnection system which allows to couple a pair of optical beams carrying modulation information. In accordance with the disclosed technology, two optical beams emanate from transceivers at two different locations. Each beam may not see the other beam point of origin (non-line-of-sight link), but both beams can see a third platform that contains the system of the disclosed technology. Each beam incident on the interconnection system is directed into the reverse direction of the other, so that each transceiver will detect the beam which emanated from the other transceiver. The system dynamically compensates for propagation distortions preferably using closed-loop optical devices, while preserving the information encoded on each beam.

Dynamic optical interconnect system reference signal formation

In some embodiments, a dynamic optical tag communication system is provided which includes high and low index CCR, both having a modulator, such as TCFP-MQWs on a first side of the CCR configured to modulate in a first temperature range, and a modulator on a second side of the CCR to modulate in a second temperature range. In some embodiments another high index CCR having corresponding first and second temperature range modulators is provided. In some embodiments, a CCR may have three modulators, such as MQWs, one configured to modulate in a first temperature range, another to modulate in a second temperature range, and yet another to modulate in a third temperature range. In some embodiments, a dynamic optical tag communication system has CCRs which include a high index CCR having a DDG modulator and a low index CCR having a DDG modulator.

Dynamic optical tag communicator and system using corner cube modulating retroreflector

A vibrometer system for determining the vibration spectrum of an object under examination. The vibrometer includes a bundle of optical fibers arranged in an array, wherein a majority of the fibers in the array are arranged to receive light reflected from the object under examination and a minority of the fibers in the array are arranged to transmit light to illuminate the object under examination, wherein the light reflected from the object under test by received by the majority of fibers was transmitted by the minority of fibers; a plurality of light amplifiers and detectors for amplifying and detecting the received light; and a coherent detector responsive to the detected light and to the transmitted light for providing an output signal representative of the vibration spectrum of the object under examination.

Optical vibrometer

Growing community of inventors

Malibu, CA, United States of America

David M Pepper