Abstract: The Application relates to optically transparent electrostatic transducers. In some embodiments, the transducers comprise graphene. Such transducers are capable of functioning as acoustic sensors and/or transmitters as a singulated device or in an array configuration. Also provided are methods of manufacturing and using such transducers.

Abstract: The Application relates to optically transparent electrostatic transducers. In some embodiments, the transducers comprise graphene. Such transducers are capable of functioning as acoustic sensors and/or transmitters as a singulated device or in an array configuration. Also provided are methods of manufacturing and using such transducers.

Abstract: Described are micro electrostatic transducers and methods of making such devices. The micro electrostatic transducer is an integrated component transducing device fabricated from materials allowing for low cost, high volume manufacturing. The device includes a sheet of graphene forming the diaphragm with two electrode layers above and below the diaphragm to introduce the audio signal.

Abstract: Described are micro electrostatic transducers and methods of making such devices. The micro electrostatic transducer is an integrated component transducing device fabricated from materials allowing for low cost, high volume manufacturing. The device includes a sheet of graphene forming the diaphragm with two electrode layers above and below the diaphragm to introduce the audio signal.

Abstract: The Application relates to optically transparent electrostatic transducers. In some embodiments, the transducers comprise graphene. Such transducers are capable of functioning as acoustic sensors and/or transmitters as a singulated device or in an array configuration. Also provided are methods of manufacturing and using such transducers.

Abstract: Described are micro electrostatic transducers and methods of making such devices. The micro electrostatic transducer is an integrated component transducing device fabricated from materials allowing for low cost, high volume manufacturing. The device includes a sheet of graphene forming the diaphragm with two electrode layers above and below the diaphragm to introduce the audio signal.

Abstract: An optical transmission system enables launching at least 17 dBm of optical power at 1550 nm wavelength into an e.g. 50 km long span of standard telecommunications single-mode optical fiber, without incurring unacceptable penalties from stimulated Brillouin scattering, damage to optical phase modulators from excessive drive power or thermal effects, or signal degradations caused by the SBS suppression. High frequency modulation of the laser drive current is combined with lower frequency modulation of the phase of the laser output light that is itself varied over a range of approximately 25 MHz. This two tone modulation raises the SBS threshold to greater than 17 dBm in the 1550 nm wavelength region when the laser has a line width less than 10 MHz, under cw operation. By thereby dividing the task of spectral partitioning between the laser and the phase modulator, the RF input power level to the phase modulator is manageable and the laser operates in a regime that does not cause clipping.

Abstract: An optical coherence-domain reflectometry system provides an interferometer driven by a broadband incoherent light source with the device under test connected to one arm of the interferometer and a movable scanning mirror in the other arm providing a reference signal. The mirror moves at a controlled velocity to produce a Doppler shift in the reference signal frequency. The interference signal is detected and measured by a receiver. In the case where the receiver is a polarization diversity receiver, an intensity modulator and a polarization controller are incorporated into the reflectometer for use in calibrating the receiver. Calibration is also provided for a single photodetector receiver.

Abstract: A lightwave component analyzer and method for determining chromatic dispersion in single mode optical fiber. The lightwave component analyzer initially performs various measurements that are used in the determination of chromatic dispersion in single mode optical fiber. The lightwave component analyzer then computes a chromatic dispersion factor using the measured parameters, as well as additional parameters which are stored in the analyzer or entered by a user. Various expressions are described for computation of chromatic dispersion in single mode optical fiber.