Chapter 11 Frequency Response 11.1 11.2 11.3 11.4 11.5 11.6 11.7 11.8 11.9 Fundamental Concepts High-Frequency Models of Transistors Analysis Procedure Frequency Response of CE and CS Stages Frequency Response of CB and CG Stages Frequency Response of Followers Frequency Response of Cascode Stage Frequency Response of Differential Pairs Additional Examples 1 Chapter Outline CH 11 Frequency Response 2 High Frequency Roll-off of Amplifier As frequency of operation increases, the gain of amplifier decreases. This chapter analyzes this problem. CH 11 Frequency Response 3 Example: Human Voice I Natural Voice Telephone System Natural human voice spans a frequency range from 20Hz to 20KHz, however conventional telephone system passes frequencies from 400Hz to 3.5KHz. Therefore phone CH 11conversation Frequency Response differs from face-to-face conversation. 4 Example: Human Voice II Path traveled by the human voice to the voice recorder Mouth Air Recorder Path traveled by the human voice to the human ear Mouth Air Ear Skull Since the paths are different, the results will also be different. CH 11 Frequency Response 5 Example: Video Signal High Bandwidth Low Bandwidth Video signals without sufficient bandwidth become fuzzy as they fail to abruptly change the contrast of pictures from complete white into complete black. CH 11 Frequency Response 6 Gain Roll-off: Simple Low-pass Filter In this simple example, as frequency increases the impedance of C1 decreases and the voltage divider consists of C1 and R1 attenuates Vin to a greater extent at the output. CH 11 Frequency Response 7 Gain Roll-off: Common Source Vout 1 g mVin RD || C s L The capacitive load, CL, is the culprit for gain roll-off since at high frequency, it will “steal” away some signal current and shunt it to ground. CH 11 Frequency Response 8 Frequency Response of the CS Stage Vout Vin g m RD RD2 C L2 2 1 At low frequency, the capacitor is effectively open and the gain is flat. As frequency increases, the capacitor tends to a short and the gain starts to decrease. A special is ω=1/(RDCL), where the gain drops by 3dB. CH 11frequency Frequency Response 9 Example: Relationship between Frequency Response and Step Response H s j 1 R12C12 2 1 t Vout t V0 1 exp u t R1C1 The relationship is such that as R1C1 increases, the bandwidth drops and the step response becomes slower. CH 11 Frequency Response 10 Bode Plot s s 1 1 z1 z 2 H ( s ) A0 s s 1 1 p1 p2 When we hit a zero, ωzj, the Bode magnitude rises with a slope of +20dB/dec. When we hit a pole, ωpj, the Bode magnitude falls with a ofResponse -20dB/dec CH 11slope Frequency 11 Example: Bode Plot p1 1 RD C L The circuit only has one pole (no zero) at 1/(R DCL), so the slope drops from 0 to -20dB/dec as we pass ωp1. CH 11 Frequency Response 12 Pole Identification Example I p1 p2 1 RS Cin Vout Vin CH 11 Frequency Response 1 1 RD C L g m RD 2 p21 1 2 p2 2 13 Pole Identification Example II p1 1 1 RS || Cin gm CH 11 Frequency Response p2 1 RD C L 14 High-Pass Filter Response Vout Vin R1C1 R12C1212 1 The voltage division between a resistor and a capacitor can be configured such that the gain at low frequency is reduced. CH 11 Frequency Response 15 Example: Audio Amplifier Ci 79.6nF CL 39.8nF Ri 100 K g m 1 / 200 In order to successfully pass audio band frequencies (20 Hz-20 KHz), large input and output capacitances are needed. CH 11 Frequency Response 16 Capacitive Coupling vs. Direct Coupling Capacitive Coupling Direct Coupling Capacitive coupling, also known as AC coupling, passes AC signals from Y to X while blocking DC contents. This technique allows independent bias conditions between Direct coupling does not. CH 11stages. Frequency Response 17 Typical Frequency Response Lower Corner CH 11 Frequency Response Upper Corner 18 MOS Intrinsic Capacitances For a MOS, there exist oxide capacitance from gate to channel, junction capacitances from source/drain to substrate, and overlap capacitance from gate to CH 11source/drain. Frequency Response 19 Gate Oxide Capacitance Partition and Full Model The gate oxide capacitance is often partitioned between source and drain. In saturation, C2 ~ Cgate, and C1 ~ 0. They are in parallel with the overlap capacitance to form CGS and CGD. CH 11 Frequency Response 20 Transit Frequency gm 2f T CGS gm 2f T C Transit frequency, fT, is defined as the frequency where the current gain from input to output drops to 1. CH 11 Frequency Response 21 Example: Transit Frequency Calculation 3 n VGS VTH 2fT 2 2L L 65nm VGS VTH 100mV n 400cm 2 /(V .s ) fT 226GHz CH 11 Frequency Response 22