Abstract: An optical telephone and communication system with interferometers at the transmitter and receiver can use optical time-delay difference and differential frequency shift modulation and multiplexing techniques. The power to the system is provided from either a remote optical source through the optical network or a local optical source. The optical network provides one or two optical connections to the sets. Part of the optical signal from the network is converted to electrical energy stored in a rechargeable battery. The optical sources used have a known coherence function, wavelength and coherence length Lc. The transmitter converts the information to phase variation in one arm of the transmitter interferometer and the receiver recovers this signal by using a matched interferometer. The path imbalance between the two arms of either interferometer is greater than Lc. Each set is assigned a particular time delay difference and/or differential frequency shift for addressing.

Abstract: A secure optical interferometric communication system and network with multiple access capability where one or more transmitters have an interferometer with phase/Doppler shift difference modulation of spread spectrum type which is used for secure communication with one or more receivers on the optical network where the spread spectrum modulation is known to one or more receivers. The optical source can be of narrow optical spectrum or broad optical spectrum. In the case of the broad optical spectrum source, the path length difference of the transmitting interferometer can be also used to increase the security communication where the path length imbalance is known to one or more receiver, and number of users on the multiple access network. The interferometric communication system, especially with broad spectrum optical sources, can interwork with conventional wavelength division multiplexing (WDM) system and time division multiplexing (TDM) system.

Abstract: In a tunable optical source, a diffraction device 115 is used to provide wavelength selective feedback to a laser diode 100. The diffraction device 115 is at least partially fabricated in a material whose refractive index is controllable so as to control the diffraction performance of the device. This allows the diffraction device 115 to be used in tuning the optical source, potentially without using moving parts. For instance, the refractive index can be controlled using a temperature change across material of the device 115. The diffraction device 115 can be mounted in free space in an external cavity with respect to the laser diode 100. Novel forms of diffraction device 115 are described. Tunable optical sources of this type can be used for instance in communications, particularly wavelength division multiplexing.

Abstract: An optical telephone and communication system with interferometers at the transmitter and receiver can use optical time-delay difference and differential frequency shift modulation and multiplexing techniques. The power to the system is provided from either a remote optical source through the optical network or a local optical source. The optical network provides one or two optical connections to the sets. Part of the optical signal from the network is converted to electrical energy stored in a rechargeable battery. The optical sources used have a known coherence function, wavelength and coherence length Lc. The transmitter converts the information to phase variation in one arm of the transmitter interferometer and the receiver recovers this signal by using a matched interferometer. The path imbalance between the two arms of either interferometer is greater than Lc. Each set is assigned a particular time delay difference and/or differential frequency shift for addressing.

Abstract: In a tunable optical source, a diffraction device 115 is used to provide wavelength selective feedback to a laser diode 100. The diffraction device 115 is at least partially fabricated in a material whose refractive index is controllable so as to control the diffraction performance of the device. This allows the diffraction device 115 to be used in tuning the optical source, potentially without using moving parts. For instance, the refractive index can be controlled using a temperature change across material of the device 115. The diffraction device 115 can be mounted in free space in an external cavity with respect to the laser diode 100. Novel forms of diffraction device 115 are described. Tunable optical sources of this type can be used for instance in communications, particularly wavelength division multiplexing.

Abstract: An external cavity laser assembly in which the laser chip is within a hermetically sealed package and the external cavity is outside the hermetic package. A collimating lens in a screw threaded mounting is disposed outside the hermetic package, the screw thread permitting focussing. The cavity is turned by rotation and translation of a grating, the position of which is electrically controlled via piezoelectric stacks. Thermal expansion of the stacks is compensated by mounting the grating on a rod of suitable material (e.g., ceramic) which also serves to reduce the cavity length while allowing maximum piezoextension. In a second embodiment the assembly is a tunable laser amplifier, with a grating being driven in a similar manner to provide the tuning.