Abstract: Various embodiments provide for determining a capacitance (or capacitor value) of a circuit, determining a resistance-capacitance time constant (or RC time constant) of a circuit, or both. The circuit can comprise an integrated circuit (IC), such as a circuit implemented on die. An IC of some embodiments generates a frequency of a dock wave signal (e.g., an output signal) such that the clock wave signal encodes an effective capacitance of the IC, a RC time constant of the IC, or both. A component external to the IC, such as a controller, can receive the clock wave signal and determine the effective capacitance of the IC, the RC time constant of the IC, or both based on the received clock wave signal.

Abstract: Various embodiments provide for a circuit for measuring a frequency difference, a phase difference, or both of at least two clock signals (e.g., a reference clock signal and a feedback clock signal). In particular, various embodiments described herein may be used in a circuit design to convert an input phase of two clock signals to a frequency difference, which may be outputted in the form of a digital word. Additionally, various embodiments described herein may be used in a circuit design to convert an input phase of two clock signals as phase difference output, which may be outputted in the form of a digital word. Various embodiments can provide the frequency difference, the phase difference, or both in near real-time and with only a small amount of latency.

Abstract: A system for protecting walls/roofs from water uses a detachable flashing channel and a step flashing unit. The detachable flashing unit is a J shape structure which facilitates the protection of walls from rain water and the step flashing unit is a L shape structure also facilitating the protection of roofs from rain water.

Abstract: A laser pulse is injected into an unstable ring resonator-amplifier structure. Inside this resonator the laser pulse is amplified, spatially filtered and magnified. The laser pulse is recirculated in the resonator, being amplified, filtered and magnified on each pass. The magnification is chosen so that the beam passes through the amplifier in concentric non-overlapping regions similar to a single pass MOPA. After a number of passes around the ring resonator the laser pulse is spatially large enough to exit the ring resonator system by passing around an output mirror.

Abstract: A method is disclosed for apodizing a laser beam to smooth out the production of diffraction peaks due to optical discontinuities in the path of the laser beam, such method comprising introduction of a pattern of scattering elements for reducing the peak intensity in the region of such optical discontinuities, such pattern having smoothly tapering boundaries in which the distribution density of the scattering elements is tapered gradually to produce small gradients in the distribution density, such pattern of scattering elements being effective to reduce and smooth out the diffraction effects which would otherwise be produced. The apodizer pattern may be produced by selectively blasting a surface of a transparent member with fine abrasive particles to produce a multitude of minute pits. In one embodiment, a scattering apodizer pattern is employed to overcome diffraction patterns in a multiple element crystal array for harmonic conversion of a laser beam.

Abstract: A pair of uniaxial birefringent crystal elements are fixed together to form a serially arranged, integral assembly which, alternatively, provides either a linearly or elliptically polarized second-harmonic output wave or a linearly polarized third-harmonic output wave. The "extraordinary" or "e" directions of the crystal elements are oriented in the integral assembly to be in quadrature (90.degree.). For a second-harmonic generation in the Type-II-Type-II angle tuned case, the input fundamental wave has equal amplitude "o" and "e" components. For a third-harmonic generation, the input fundamental wave has "o" and "e" components whose amplitudes are in a ratio of 2:1 ("o":"e" reference first crystal). In the typical case of a linearly polarized input fundamental wave this can be accomplished by simply rotating the crystal assembly about the input beam direction by 10.degree..