ECE 546 Lecture 12 Integrated Circuits Spring 2016

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ECE 546 Lecture 12 Integrated Circuits Spring 2016 Jose E. Schutt-Aine Electrical & Computer

ECE 546 Lecture 12 Integrated Circuits Spring 2016 Jose E. Schutt-Aine Electrical & Computer Engineering University of Illinois jesa@illinois. edu ECE 546 – Jose Schutt-Aine 1

Integrated Circuits • IC Requirements – Biasing of ICs is based on the use

Integrated Circuits • IC Requirements – Biasing of ICs is based on the use of constant current sources – Use current mirrors – Source circuits are used as loads ECE 546 – Jose Schutt-Aine 2

Integrated Circuits • Analog Design Requirements – Analog ICs may need resistors and capacitors

Integrated Circuits • Analog Design Requirements – Analog ICs may need resistors and capacitors for the design of amplifiers – Resistors and capacitors occupy the space of tens or hundreds of MOS devices – It is important to minimize their use ECE 546 – Jose Schutt-Aine 3

Transistor Biasing ECE 546 – Jose Schutt-Aine 4

Transistor Biasing ECE 546 – Jose Schutt-Aine 4

Transistor Biasing ECE 546 – Jose Schutt-Aine 5

Transistor Biasing ECE 546 – Jose Schutt-Aine 5

Current Mirrors A current mirror will reproduce a reference current to the output while

Current Mirrors A current mirror will reproduce a reference current to the output while allowing the output voltage to assume any value within a specified range. Io=KIin where K is a factor that can be less than or equal or greater than 1 ECE 546 – Jose Schutt-Aine 6

MOS Current Mirror R is usually external to IC ECE 546 – Jose Schutt-Aine

MOS Current Mirror R is usually external to IC ECE 546 – Jose Schutt-Aine 7

MOS Current Mirror Assuming that the transistors are using the same process • Can

MOS Current Mirror Assuming that the transistors are using the same process • Can be limited by – Channel length modulation (l) – Threshold voltage mismatch – Imperfect geometrical matching ECE 546 – Jose Schutt-Aine 8

MOS Current Mirror • Some Properties 1. MOS current mirrors draw zero control current

MOS Current Mirror • Some Properties 1. MOS current mirrors draw zero control current better than BJT’s 2. Matching of threshold voltages harder than in BJT’s ECE 546 – Jose Schutt-Aine 9

Example A matched pair of MOSFETs are used in a current mirror witl l

Example A matched pair of MOSFETs are used in a current mirror witl l = 0. 032 V-1, m. Cox=70 m. A/V 2, W/2 L =10, and VT = 0. 9 V. Find the value of R to create an input current of 100 m. A. Calculate the output current when Vo = 3 V. Use drain current equation in active region to calculate We can now solve for the value of VGS ECE 546 – Jose Schutt-Aine 10

Example MOS Current Mirror ECE 546 – Jose Schutt-Aine 11

Example MOS Current Mirror ECE 546 – Jose Schutt-Aine 11

Example VGS = 1. 272 V The resistance needed is: The output current is

Example VGS = 1. 272 V The resistance needed is: The output current is calculated from: ECE 546 – Jose Schutt-Aine 12

Ideal MOS Common Source CKT ECE 546 – Jose Schutt-Aine 13

Ideal MOS Common Source CKT ECE 546 – Jose Schutt-Aine 13

PMOS Implementation of Active Load ECE 546 – Jose Schutt-Aine 14

PMOS Implementation of Active Load ECE 546 – Jose Schutt-Aine 14

PMOS Implementation of Active Load Can show that the 3 d. B point is

PMOS Implementation of Active Load Can show that the 3 d. B point is given: Large incremental load leads to high gain while maintaining acceptable DC current (resistor would not work) ECE 546 – Jose Schutt-Aine 15

Background • Differential Amplifiers – The input stage of every op amp is a

Background • Differential Amplifiers – The input stage of every op amp is a differential amplifier – Immunity to temperature effects – Ability to amplify dc signals – Well-suited for IC fabrication because – (a) they depend on matching of elements – (b) they use more components – Less sensitive to noise and interference – Enable to bias amplifier and connect to other stage without the use of coupling capacitors ECE 546 – Jose Schutt-Aine 16

Differential Amplifiers • Practical Considerations – Both inputs to a differential amplifier may have

Differential Amplifiers • Practical Considerations – Both inputs to a differential amplifier may have different voltages applied to them – In the ideal situation with perfectly symmetric stages, the common-mode input would lead to zero output – Temperature drifts in each stage are often common-mode signals – Power supply noise is a common-mode signal and has little effect on the output signal ECE 546 – Jose Schutt-Aine 17

MOS Differential Pair Ø Assume current source is ideal Ø Transistors should not enter

MOS Differential Pair Ø Assume current source is ideal Ø Transistors should not enter triode region

Common-Mode Operation Ø Input voltage vcm to both gates Ø Difference in voltage between

Common-Mode Operation Ø Input voltage vcm to both gates Ø Difference in voltage between the two drains is zero

Differential Input Voltage Ø Differential pair responds to differntial input signals by providing corresponding

Differential Input Voltage Ø Differential pair responds to differntial input signals by providing corresponding differential output signal between the two drains.

MOS Differential Pair Assume current source is ideal v. ID=vgs 1 -vgs 2 Output

MOS Differential Pair Assume current source is ideal v. ID=vgs 1 -vgs 2 Output is collected as v. D 2 -v. D 1 ECE 546 – Jose Schutt-Aine 21

MOS Differential Pair - If v. ID is positive, v. D 2 -v. D

MOS Differential Pair - If v. ID is positive, v. D 2 -v. D 1 is positive v. ID>0 vgs 1>vgs 2 ID 1 > ID 2 v. D 1 lower voltage point than v. D 2 For properation, MOSFETS should not enter triode region ECE 546 – Jose Schutt-Aine 22

DC Analysis ECE 546 – Jose Schutt-Aine 23

DC Analysis ECE 546 – Jose Schutt-Aine 23

Incremental Analysis Neglecting the body effect ECE 546 – Jose Schutt-Aine 24

Incremental Analysis Neglecting the body effect ECE 546 – Jose Schutt-Aine 24

Frequency Response When driven by a low-impedance signal source, the upper corner frequency is

Frequency Response When driven by a low-impedance signal source, the upper corner frequency is determined by the output circuit ECE 546 – Jose Schutt-Aine 25

Common-Mode Rejection Ratio Assume RSS >> 1/gm ECE 546 – Jose Schutt-Aine 26

Common-Mode Rejection Ratio Assume RSS >> 1/gm ECE 546 – Jose Schutt-Aine 26

Common-Mode Rejection Ratio (a) For single-ended output: ECE 546 – Jose Schutt-Aine 27

Common-Mode Rejection Ratio (a) For single-ended output: ECE 546 – Jose Schutt-Aine 27

Common-Mode Rejection Ratio (b) For differential output: ECE 546 – Jose Schutt-Aine 28

Common-Mode Rejection Ratio (b) For differential output: ECE 546 – Jose Schutt-Aine 28

Differential Amplifiers - Observations • Observations – The differential pair attenuates the input signal

Differential Amplifiers - Observations • Observations – The differential pair attenuates the input signal of each stage by a factor of one-half cutting the gain of each stage by one-half – The double-ended output causes the two singleended gains to be additive – Thus, the voltage gain of a perfectly matched differential stage is equal to that of a single stage ECE 546 – Jose Schutt-Aine 29

MOS Differential Amp with Active Load Replacing drain resistances with current sources, results in

MOS Differential Amp with Active Load Replacing drain resistances with current sources, results in much higher voltage gain and savings in chip area in diff amp ECE 546 – Jose Schutt-Aine 30

MOS Differential Amp - Equilibrium

MOS Differential Amp - Equilibrium

MOS Differential Amp with Active Load Current mirror action makes it possible to convert

MOS Differential Amp with Active Load Current mirror action makes it possible to convert the signal to single-ended form without loss of gain. The differential gain is: ECE 546 – Jose Schutt-Aine 32

MOS Differential Amp with Active Load The active-loaded MOS differential amplifier has a low

MOS Differential Amp with Active Load The active-loaded MOS differential amplifier has a low common-mode gain high CMRR The common-mode gain is: RSS is internal impedance of current source ECE 546 – Jose Schutt-Aine 33

MOS Differential Amp with Active Load Since RSS is large, Acm will be small

MOS Differential Amp with Active Load Since RSS is large, Acm will be small ECE 546 – Jose Schutt-Aine 34

CMOS OP Amp Example In the differential amplifier shown, Q 1 and Q 2

CMOS OP Amp Example In the differential amplifier shown, Q 1 and Q 2 form the differential pair while the current source transistors Q 4 and Q 5 form the active loads for Q 1 and Q 2 respectively. The dc bias circuit that establishes an appropriate dc voltage at the drains of Q 1 and Q 2 is not shown. The following specifications are desired: differential gain Ad = 80 V/V, IREF = 100 m. A, the dc voltage at the gates of Q 6 and Q 3 is +1. 5 V; the dc voltage at the gates of Q 7, Q 4 and Q 5 is – 1. 5 V. The technology available is specified as follows: mn. Cox=3 mp. Cox = 90 m. A/V 2; Vtn=|Vtp|=0. 7 V, VAn=|VAp| = 20 V. Specify the required value of R and the W/L ratios for all transistors. Also, specify ID and VGS at which each transistor is operating. For dc bias calculations, you may neglect channel-length modulation. Fill in the entries in the table provided to show your results. ECE 546 – Jose Schutt-Aine 35

CMOS OP Amp Example ECE 546 – Jose Schutt-Aine 36

CMOS OP Amp Example ECE 546 – Jose Schutt-Aine 36

CMOS OP Amp Example Drain currents are determined by symmetry and inspection VGS values

CMOS OP Amp Example Drain currents are determined by symmetry and inspection VGS values are also determined by inspection for all transistors except Q 1 and Q 2. To determine VGS for Q 1 and Q 2, we do the following: the equivalent load resistance will consist of ro 1 in parallel with ro 4 for Q 1 and ro 2 in parallel with ro 5 for Q 5. Since the ro’s are equal, this corresponds to ro/2. We have: ECE 546 – Jose Schutt-Aine 37

CMOS OP Amp Example Take polarity into account for PMOS To find W/L ratios,

CMOS OP Amp Example Take polarity into account for PMOS To find W/L ratios, use taking into account PMOS and NMOS devices separately ECE 546 – Jose Schutt-Aine 38

CMOS OP-AMP DESIGN TABLE Q 1 m. Cox 30 30 30 90 90 ID

CMOS OP-AMP DESIGN TABLE Q 1 m. Cox 30 30 30 90 90 ID 50 50 100 50 VGS -. 95 -1 W/L 57. 3 74 1. Q 2 Q 3 Q 7 Units 30 90 m. A/V 2 50 100 m. A +1 +1 -1 +1 V 12. 3 73. 1 24. 7 Q 4 Q 5 ECE 546 – Jose Schutt-Aine Q 6 39