Abstract: In one aspect, methods of determining the shape of a sessile drop are described herein. In some embodiments, a method described herein comprises measuring a first shape parameter of a sessile drop to obtain a first shape parameter value, measuring a second shape parameter of the drop to obtain a second shape parameter value, and using the first and second shape parameter values to calculate a third shape parameter value of a third shape parameter of the drop.

Abstract: In one aspect, methods of determining the shape of a sessile drop are described herein. In some embodiments, a method described herein comprises measuring a first shape parameter of a sessile drop to obtain a first shape parameter value, measuring a second shape parameter of the drop to obtain a second shape parameter value, and using the first and second shape parameter values to calculate a third shape parameter value of a third shape parameter of the drop.

Abstract: In various exemplary embodiments, the present invention provides a system for the light-induced directed self-assembly (LIDSA) of periodic sub-wavelength nanostructures, including: a light source for delivering a beam of photons; a reaction chamber disposed adjacent to the light source; a gas including one or more precursor materials disposed within the reaction chamber; and a substrate disposed within the reaction chamber, wherein the substrate is positioned and configured to receive the beam of photons; wherein the beam of photons causes a periodic sub-wavelength nanostructure of one or more constituents of the one or more precursor materials to form on a surface of the substrate. In various exemplary embodiments, the present invention also provides an associated method.

Abstract: In various exemplary embodiments, the present invention provides a system for the light-induced directed self-assembly (LIDSA) of periodic sub-wavelength nanostructures, including: a light source for delivering a beam of photons; a reaction chamber disposed adjacent to the light source; a gas including one or more precursor materials disposed within the reaction chamber; and a substrate disposed within the reaction chamber, wherein the substrate is positioned and configured to receive the beam of photons; wherein the beam of photons causes a periodic sub-wavelength nanostructure of one or more constituents of the one or more precursor materials to form on a surface of the substrate. In various exemplary embodiments, the present invention also provides an associated method.

Abstract: An optical performance monitor particularly well-suited for use in dense wavelength-division multiplexed (DWDM) systems includes both a nonlinear optical detector and a conventional linear detector. The nonlinear optical detector, which may comprise a quadratic detector, is used to provide information, on a channel-by-channel basis, regarding chromatic dispersion, polarization mode dispersion and accumulated amplified spontaneous emission (ASE) noise in each signal wavelength.

Abstract: Embodiments of the invention include system for monitoring the effectiveness of pulse shaping in a nonlinear optical fiber (40). The spectral content of the pulse, after passing through the nonlinear fiber (40), provides an indication of how effectively the pulse was regenerated. A portion of the pulse exiting the nonlinear fiber is tapped off and its pulse energy is measured in at least one selected spectral region. The selected spectral region is one in which the pulse tends to gain energy when effective regeneration is taking place. The information concerning the effectiveness of pulse shaping in a nonlinear optical fiber is fed back to dynamically change the residual dispersion at the regenerator input. The spectral measurement leads to a control signal (48) to indicate a level of performance of the system, or to improve the performance of the system by adjusting an operational parameter.

Abstract: Embodiments of the invention include system for monitoring the effectiveness of pulse shaping in a nonlinear optical fiber (40). The spectral content of the pulse, after passing through the nonlinear fiber (40), provides an indication of how effectively the pulse was regenerated. A portion of the pulse exiting the nonlinear fiber is tapped off and its pulse energy is measured in at least one selected spectral region. The selected spectral region is one in which the pulse tends to gain energy when effective regeneration is taking place. The information concerning the effectiveness of pulse shaping in a nonlinear optical fiber is fed back to dynamically change the residual dispersion at the regenerator input. The spectral measurement leads to a control signal (48) to indicate a level of performance of the system, or to improve the performance of the system by adjusting an operational parameter.

Abstract: An optical performance monitor particularly well-suited for use in dense wavelength-division multiplexed (DWDM) systems includes both a nonlinear optical detector and a conventional linear detector. The nonlinear optical detector, which may comprise a quadratic detector, is used to provide information, on a channel-by-channel basis, regarding chromatic dispersion, polarization mode dispersion and accumulated amplified spontaneous emission (ASE) noise in each signal wavelength.