Frequency response ISlide 2Frequency response of amplifersSlide 4The MOS TransistorThe Gate CapacitanceGate CapacitanceDiffusion CapacitanceSlide 9Exact frequency response of amplifiersThe Miller EffectApplication of Miller EffectSlide 13Slide 14Slide 15Slide 16Slide 17Slide 18Slide 19Slide 20Slide 211Frequency response I•As the frequency of the processed signals increases, the effects of parasitic capacitance in (BJT/MOS) transistors start to manifest•The gain of the amplifier circuits is frequency dependent, usually decrease with the frequency increase of the input signals•Computing by hand the exact frequency response of an amplifier circuits is a difficult and time-consuming task, therefore approximate techniques for obtaining the values of critical frequencies is desirable•The exact frequency response can be obtained from computer simulations (e.g SPICE). However, to optimize your circuit for maximum bandwidth and to keep it stable one needs analytical expressions of the circuit parameters or at least know which parameter affects the required specification and how2•The transfer function gives us the information about the behavior of a linear-time-invariant (LTI) circuit/system for a sinusoidal excitation with angular frequency •This transfer function is nothing but the ratio between the Fourier transforms of the output and input signals and it is also called the frequency response of the LTI circuit.• represents the gain magnitude of the frequency response of the circuit, whereas is the phase of frequency response. Often, it is more convenient to express gain magnitude in decibels. •To amplify a signal without distortion, the amplifier gain magnitude must be the same for all of the frequency components Frequency response II))(exp(|)(|))(exp(|)(|)(jTTjTT |)(|T)(3Frequency response of amplifers•A bode plot shows the the gain magnitude and phase in decibles versus frequency on logarithmic scale•A few prerequisites for bode plot:Laplace transform and network transfer functionPoles and zeros of transfer functionBreak frequencies•Some useful rules for drawing high-order bode plots:Decompose transfer function into first order terms. Mark the break frequencies and represent them on the frequency axis the critical values for changesMake bode plot for each of the first order termFor each first order term, keep the DC to the break frequency constant equal to the gain at DCAfter the break frequency, the gain magnitude starts to increase or decrease with a slope of 20db/decade if the term is in the numerator or denominatorFor phase plot, each first order term induces a 45 degrees of increase or decrease at the break frequency if the term is in the numerator or denominatorConsider frequencies like one-tenth and ten times the break frequency and approximate the phase by 0 and 90 degrees if the frequency is with the numerator (or 0 and -90 degrees if in the denominator)Add all the first order terms for magnitude and phase response4Frequency response of RLC circuitsE.g. 1E.g. 3)/arctan()/arctan()()/(1log20)/(1log20|)(|)(21,21,)(2121)(21222121221212bbbbdbvbbvffffffffffACRRfCRfCRRfjCfRjfA)/arctan()(2)/(1log20)|(|21,211)(bfffbffdbfvARCbfRCfjfvAE.g. 2)/arctan(90)()/(1log20)/log(2012|)(|)(21,)/(1)/()(212)(221212212bbbdbvbbbvffffffffACRRfffjffjRRRCRRfjCfRjfA5The MOS TransistorPolysiliconAluminum6The Gate Capacitancetoxn+n+Cross section viewLGate oxidexdxdLdPolysilicon gateTop viewGate-bulkoverlapSourcen+Drainn+W7Gate CapacitanceSDGCGCSDGCGCSDGCGCCut-ofResistive SaturationMost important regions in digital design: saturation and cut-off8Diffusion CapacitanceBottomSide wallSide wallChannelSourceNDChannel-stop implant NA1SubstrateNAWxjLS9Frequency response of common source MOS ampliferHigh-frequency MOS Small-signal equivalent circuitMOSFET common Source amplifierSmall-signal equivalent circuit for the MOS common source amplifierFrequency response analysis shows that there are three break frequencies, and mainly the lowest one determines the upper half-power frequency, thus the -3db bandwidth10•Exact frequency analysis of amplifier circuits is possible following the steps:Draw small-signal equivalent circuit (replace each component in the amplifier with its small-signal circuit)Write equations using voltage and current lawsFind the voltage gain as a ratio of polynomial of laplace variable sFactor numerator and denominator of the polynomial to determine break frequenciesDraw bode plot to approximate the frequency responseExact frequency response of amplifiers11The Miller Effect•Consider the situation that an impedance is connected between input and output of an amplifierThe same current flows from (out) the top input terminal if an impedance is connected across the input terminalsThe same current flows to (in) the top output terminal if an impedance is connected across the output terminalThis is know as Miller EffectTwo important notes to apply Miller Effect:There should be a common terminal for input and outputThe gain in the Miller Effect is the gain after connecting feedback impedance MillerinZ,MilleroutZ,fZGraphs from Prentice Hall12Application of Miller Effect•If the voltage gain magnitude is large (say larger than 10) compared to unity, thenwe can perform an approximate analysis by assuming is equal tofind the gain including loading effects ofuse the gain to find out Thus, using Miller Effect, gain calculation and frequency response characterization would be much simpler MilleroutZ,fvvfMilleroutZAAZZ 1,)(, fMilleroutzZMillerinZ,fZ13•If the feedback impedance is a capacitor ,then the Miller capacitance reflected across the input terminal is .•Therefore, connecting a capacitance from the input to output is equivalent to connecting a capacitance •Due to Miller effect, a small feedback capacitance appears across the input terminals as a much larger equivalent capacitance with a large gain (e.g. ). At high