13 research outputs found

    Two Multi-Objective Genetic Algorithms for Finding Optimum Design of an I-beam

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    A Phase Tunable Rotary Traveling Wave Oscillator: Analysis and Calibration

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    What Is the Maximum Achievable Oscillation Frequency in a Specified CMOS Process?

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    A fast charge pump PLL using a bang-bang frequency comparator with dead zone

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    The frequency synthesizer is one of the most challenging blocks in wireless transceivers; it works as a local oscillator in both the receiver and transmitter. It is generally based on a charge pump phase-locked loop (CPPLL) structure. If we can change the structure of the CPPLL or synthesizer to achieve fast locking, it can be used in applications to improve the locking time. Several methods have been introduced to increase the speed of the locking process. One way to achieve fast locking is to use a bang-bang frequency comparator (BBFC) in the feedthrough path to increase the locking speed. However, using the BBFC leads to unwanted ripple in the control voltage applied to the VCO; this ripple, in turn, leads to worse phase noise. In addition, an offset in the BBFC can produce cycle slipping. Applying a proper deadzone in the BBFC can help the system to overcome the unwanted ripple and cycle slipping. Simulations in MATLAB confirm that applying a deadzone equal to or larger than the frequency offset can suppress the unwanted ripple. © 2012 IEEE

    The role of charge pump mismatch in the generation of integer boundary spurs in fractional-N frequency synthesizers: Why worse can be better

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    Fractional-N frequency synthesizers exhibit spurious tones (spurs). Spurs outside the loop bandwidth can be attenuated by the loop filter. By contrast, in-band spurs cannot be removed by filtering and are therefore a major cause for concern. The frequency-to-phase conversion of the output of a digital sigma-delta modulator followed by charge-pump mismatch is known to cause in-band spurs; larger mismatch is thought to make the problem worse. By considering a simplified nonlinear model of the mechanism, we show how larger mismatch can paradoxically make the spur problem disappear. We illustrate our predictions using a simplified MATLAB model and confirm them by simulation using the CppSim behavioral simulator. © 2004-2012 IEEE
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