Lecture 26 Differential Amplifiers (I) DIFFERENTIAL AMPLIFIERS Outline 1. 2. 3. Introduction Incremental analysis of differential amplifier Common-source differential amplifier Reading Assignment: Howe and Sodini, Chapter 11, Sections 11-1-11.3, 11.6 6.012 Electronic Devices and Circuits-Fall 2000 Lecture 26 1 Summary of Key Concepts • • In differential amplifiers, signals are represented by difference between two voltages Differential amplifier amplifies the difference between two voltages but rejects “common mode” signals – ⇒ Improved noise immunity • Using “half-circuit” technique, small-signal operation of differential amplifiers is analyzed by breaking the problem into two simpler ones – Differential mode problem – Common mode problem • • Common-mode rejection ratio (CMRR) is an important figure of merit for differential amplifiers Differential amplifiers require good device matching 6.012 Electronic Devices and Circuits-Fall 2000 Lecture 26 2 1. Introduction Two problems found in single-transistor amplifier stages are: • Bias and gain sensitivity to device parameters (µCox, V T) – Sensitivity can be mitigated but often at a price in terms of performance or cost (gain, power, device area, etc.) • Vulnerability to ground and power supply noise – In dense IC’s there is cross-talk, 60 Hz coupling, substrate noise, etc. 6.012 Electronic Devices and Circuits-Fall 2000 Lecture 26 3 Introduction (contd.) Solution : represent relevant signal by the difference between two voltages Differential Amplifier: • Amplifies difference between two voltages • Rejects components common to both voltages 6.012 Electronic Devices and Circuits-Fall 2000 Lecture 26 4 MOSFET Differential Amplifier Basic Configuration • vO responds to difference between vI’s – If vI1 = vI2 ⇒ symmetry ⇒ vO1 = vO2 ⇒ vO = 0 – If vI1 > vI2 ⇒ M1 conducts more than M2 ⇒ i1 > i2 ⇒ vO1 < vO2 ⇒ vO < 0 • vO insensitive to common mode signals: – If both vO1 and vO2 move in sync, symmetry is preserved ⇒ vO unchanged – If ground VDD or VSS have noise, symmetry preserved ⇒ vO unchanged – If VT or µCox change, symmetry preserved ⇒ vO unchanged. • Need precise device matching 6.012 Electronic Devices and Circuits-Fall 2000 Lecture 26 5 Differential-mode and Common-mode signals Distinguish between common-mode and differential-mode: v I1 = v IC + v ID , 2 v I 2 = v IC − Then: v ID = v I1 − v I 2 , v IC = v ID 2 v I1 + v I 2 2 Similarly at the output: v O1 = v OC + v OD , 2 v O 2 = v OC − v OD 2 Then: v OD = v O1 − v O 2 , 6.012 Electronic Devices and Circuits-Fall 2000 v OC = v O1 + v O 2 2 Lecture 26 6 2. Incremental analysis of differential amplifier Consider generic differential amplifier: Figures of Merit: Differential-mode voltage gain (want it high): adm = v od v id Common-mode voltage gain (want it small): acm = v oc v ic Common-mode rejection ratio (want it very high): CMRR = 6.012 Electronic Devices and Circuits-Fall 2000 a dm a cm Lecture 26 7 Incremental analysis of differential amplifier (contd.) Two steps to simplify the problem: 1. Use superposition and break the problem into two: 2. Exploit symmetry: Circuit broken into two “half circuits”. 6.012 Electronic Devices and Circuits-Fall 2000 Lecture 26 8 Incremental analysis of differential amplifier Differential-mode Analysis No voltage relative to ground along axis of symmetry ⇒ circuit identical to: 6.012 Electronic Devices and Circuits-Fall 2000 Lecture 26 9 Incremental analysis of differential amplifier Differential-mode Analysis (contd.) Need to solve: Differential-mode voltage gain: a dm v od v o 2 − v o1 = = v id v i 2 − v i1 In differential –mode: v i1 = − v i 2 = v id 2 and v o1 = − v o 2 Then: a dm 2 v o1 v o1 = = v id v id 2 6.012 Electronic Devices and Circuits-Fall 2000 Lecture 26 10 Incremental analysis of differential amplifier Common-mode Analysis No current across wires connecting the two half-circuits ⇒ circuit is identical to: 6.012 Electronic Devices and Circuits-Fall 2000 Lecture 26 11 Incremental analysis of differential amplifier Common-mode Analysis (contd.) Common-mode voltage gain: a cm v o 2 + v o1 v oc 2 = = v ic v ic In common–mode, vo1 = vo2, then: a cm 6.012 Electronic Devices and Circuits-Fall 2000 v o1 = v ic Lecture 26 12 3. Common-source differential amplifier (source-coupled pair) Biasing Issues: must keep MOSFET’s in saturation • Upper limit to VI1 and VI2: MI and M2 driven into linear regime: VIC, max = VO1 + VT = VT + VDD − R D I BIAS 2 • Lower limit to VI1 and VI2: set by circuit that implements IBIAS. 6.012 Electronic Devices and Circuits-Fall 2000 Lecture 26 13 Common-source differential amplifier (small-signal equivalent circuit model) 6.012 Electronic Devices and Circuits-Fall 2000 Lecture 26 14 Common-source differential amplifier Differential-mode half circuit v id v o1 = −g m1R D 2 Then the differential mode gain is a dm = v o1 = −g m1R D v id 2 6.012 Electronic Devices and Circuits-Fall 2000 Lecture 26 15 Common-source differential amplifier Common-mode half circuit g m1R D v o1 = − • v ic 1 + 2g m1rob Then the common-mode gain is a cm v o1 g m1R D = =− v ic 1+ 2g m1rob Common-mode Rejection Ratio (CMRR): CMMR = adm − g m1R D = 1 + 2g m1rob = a cm − g m1R D 1 + 2g m1rob To get good CMRR, need good current source. 6.012 Electronic Devices and Circuits-Fall 2000 Lecture 26 16 Large-signal response of differential amplifier Examine large-signal transfer function: • • • If vI1 = vI2 ⇒ vO1 = vO2 ⇒ vO = 0 If vI1 > vI2 ⇒ M1 conducts more than M2 ⇒ i1 > i2 ⇒ vO1 < vO2 ⇒ vO < 0 If vI1 >> vI2 ⇒ M1 conducts strongly, M2 turns off ⇒ i1 ≈ IBIAS, i2 ≈ 0 ⇒ v O1 = v O1,min = VDD − I BAIS R D , v O 2 = v O1,max = VDD v OD,min = −I BAIS R D • Symmetric behavior for vI1 < vI2 and vI1 << vI2 6.012 Electronic Devices and Circuits-Fall 2000 Lecture 26 17 Large-signal response of differential amplifier (contd.) Saturating behavior for large differential input signals: vID that leads to amplifier saturation (vI1 >> vI2 ): v ID,sat = v GS1 − v GS 2 With: v GS1 = VT + I BAIS W µCox 2L v GS 2 = VT Then: v ID,sat = 6.012 Electronic Devices and Circuits-Fall 2000 I BAIS W µCox 2L Lecture 26 18 Large-signal response of differential amplifier (contd.) For small vID, vO is linear in vI ⇒ differential amplifier For large vID, vO saturates: once vID is large enough, vO independent of vID ⇒ logic inverter • • Can do logic with this: • • Logic 0 = -VID,sat, logic 1 = VID,sat Regenerative if VO (swing) >VID,sat • • • Used in some MOSFET logic styles Used with Si BJTs: Emitter-Coupled Logic (ECL) And GaAs FETs: Source-Coupled FET Logic (SCFL) 6.012 Electronic Devices and Circuits-Fall 2000 Lecture 26 19 What did we learn today? Summary of Key Concepts • • In differential amplifiers, signals are represented by difference between two voltages Differential amplifier amplifies the difference between two voltages but rejects “common mode” signals – ⇒ Improved noise immunity • Using “half-circuit” technique, small-signal operation of differential amplifiers is analyzed by breaking the problem into two simpler ones – Differential mode problem – Common mode problem • • Common-mode rejection ratio (CMRR) is an important figure of merit for differential amplifiers Differential amplifiers require good device matching 6.012 Electronic Devices and Circuits-Fall 2000 Lecture 26 20 Wrap-up of 6.012 6.012: Introductory subject to microelectronic devices and circuits • MICROELECTRONIC DEVICES – Semiconductor physics: electrons / holes and drift / diffusion – Metal-oxide-semiconductor field-effect transistors (MOSFETs): drift of carriers in inversion layer – Bipolar junction transistors (BJTs): minority carrier diffusion • MICROELECTRONIC CIRCUITS – Digital circuits (mainly CMOS): no static power dissipation; power ↓, delay ↓ & density ↑ as W & L ↓ – Analog circuits (BJT and CMOS): fτ ↑ and gm ↑ as L ↓: however, Avomax ↓ as L ↓ Follow-on Courses • • • • • • 6.152J — Microelectronics Processing Technology 6.720J — Integrated Microelectronic Devices 6.301 — Solid State Circuits 6.371 — Introduction to VLSI Systems 6.374 — Analysis and Design of Digital ICs 6.775 — Design of Analog MOS LSI 6.012 Electronic Devices and Circuits-Fall 2000 Lecture 26 21