Analog Integrated Circuits Lecture 1 Introduction and MOS

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Analog Integrated Circuits Lecture 1: Introduction and MOS Physics ELC 601 – Fall 2013

Analog Integrated Circuits Lecture 1: Introduction and MOS Physics ELC 601 – Fall 2013 Dr. Ahmed Nader Dr. Mohamed M. Aboudina anader@ieee. org maboudina@gmail. com Department of Electronics and Communications Engineering Faculty of Engineering – Cairo University

2 Syllabus Week 1 2 3 4 5 6 7 Lecture/Studio Topic MOS Physics

2 Syllabus Week 1 2 3 4 5 6 7 Lecture/Studio Topic MOS Physics + Short Channel Effects Single Stage Amplifiers + Frequency Response Differential Amplifiers Current Sources/Mirrors Operational Amplifier Design Text book: Design of Analog CMOS Integrated Circuits by Behzad Razavi Website: http: //scholar. cu. edu. eg/anader/ Email: anader@ieee. org Office hours: Sunday 4: 00 – 5: 00 pm Monday 4: 00 – 5: 00 pm 2/25/2021 © Ahmed Nader, 2013 Chapter 2 + 16 3+6 4 5 9 10 10

3 Contents • • Analog Signal Processing Vs. Digital Signal Processing IC Fabrication Passives

3 Contents • • Analog Signal Processing Vs. Digital Signal Processing IC Fabrication Passives MOS: Device Physics – – – 2/25/2021 MOS Structure and Threshold Voltage MOS I-V Characteristics MOS Non-idealities (Channel length modulation, Body effect) Subthreshold Conduction MOS Intrinsic capacitance and small-signal model Velocity Saturation © Ahmed Nader, 2013

4 Digital Signal Processing 2/25/2021 © Ahmed Nader, 2013

4 Digital Signal Processing 2/25/2021 © Ahmed Nader, 2013

5 Analog Signal Processing 2/25/2021 © Ahmed Nader, 2013

5 Analog Signal Processing 2/25/2021 © Ahmed Nader, 2013

6 Analog Signal Processing 2/25/2021 © Ahmed Nader, 2013

6 Analog Signal Processing 2/25/2021 © Ahmed Nader, 2013

7 Data Converters 2/25/2021 © Ahmed Nader, 2013

7 Data Converters 2/25/2021 © Ahmed Nader, 2013

2/25/2021 © Ahmed Nader, 2013 8

2/25/2021 © Ahmed Nader, 2013 8

9 Integrated Circuits 2/25/2021 © Ahmed Nader, 2013

9 Integrated Circuits 2/25/2021 © Ahmed Nader, 2013

10 IC Fabrication § Semiconductor device fabrication is the process used to create integrated

10 IC Fabrication § Semiconductor device fabrication is the process used to create integrated circuits (silicon chips) § Done in a clean room (Fab facility) § Takes 6 -8 weeks 2/25/2021 © Ahmed Nader, 2013

11 Video 2/25/2021 © Ahmed Nader, 2013

11 Video 2/25/2021 © Ahmed Nader, 2013

12 Semiconductor Industry § § § 2/25/2021 Semiconductor IC industry had revenues that reached

12 Semiconductor Industry § § § 2/25/2021 Semiconductor IC industry had revenues that reached $295 billion last year (2012). Microcontrollers (MC), Digital Signal Processors (DSP) and Microprocessors (MP) have been the center of the IC revolution since the beginning. The Personal Computer (PC) boom of the last century has become the Smartphone, Entertainment Console, Notebook and Tablet explosion in the new millennium. Largest companies in that industry are: Intel with $50 billion revenue in 2012. Samsung Electronics ranked second. Qualcomm, Texas instruments, Toshiba rounding out the top 5. Largest manufacturers (Fab facilities): Intel, TSMC, STMicroelectronics, IBM © Ahmed Nader, 2013

13 CMOS Cross Section PDK=Process Development Kit Remember Z dimensions cannot be changed and

13 CMOS Cross Section PDK=Process Development Kit Remember Z dimensions cannot be changed and are fab dependent 2/25/2021 © Ahmed Nader, 2013

14 Devices in a PDK 2/25/2021 © Ahmed Nader, 2013

14 Devices in a PDK 2/25/2021 © Ahmed Nader, 2013

15 Integrated Resistors 2/25/2021 © Ahmed Nader, 2013

15 Integrated Resistors 2/25/2021 © Ahmed Nader, 2013

16 Integrated Resistors 2/25/2021 © Ahmed Nader, 2013

16 Integrated Resistors 2/25/2021 © Ahmed Nader, 2013

17 Diffusion Resistors 2/25/2021 © Ahmed Nader, 2013

17 Diffusion Resistors 2/25/2021 © Ahmed Nader, 2013

18 Integrated Capacitors: Poly-Poly § In range of p. F § Accuracy +/-15% 2/25/2021

18 Integrated Capacitors: Poly-Poly § In range of p. F § Accuracy +/-15% 2/25/2021 © Ahmed Nader, 2013

19 Integrated Capacitors: MIM (Metal-Insulator-Metal) 2/25/2021 © Ahmed Nader, 2013

19 Integrated Capacitors: MIM (Metal-Insulator-Metal) 2/25/2021 © Ahmed Nader, 2013

20 Integrated Capacitors: MOM (Metal-Oxide-Metal) 2/25/2021 © Ahmed Nader, 2013

20 Integrated Capacitors: MOM (Metal-Oxide-Metal) 2/25/2021 © Ahmed Nader, 2013

21 Integrated Inductors § Widely Used in RF circuits (L in the range of

21 Integrated Inductors § Widely Used in RF circuits (L in the range of n. H) § Low quality factor 2/25/2021 © Ahmed Nader, 2013

22 Integrated Inductors: Multi-Layer Spiral Inductors 2/25/2021 © Ahmed Nader, 2013

22 Integrated Inductors: Multi-Layer Spiral Inductors 2/25/2021 © Ahmed Nader, 2013

23 An Example of a Commercial IBM Process 2/25/2021 © Ahmed Nader, 2013

23 An Example of a Commercial IBM Process 2/25/2021 © Ahmed Nader, 2013

24 An Example of a Commercial IBM Process 2/25/2021 © Ahmed Nader, 2013

24 An Example of a Commercial IBM Process 2/25/2021 © Ahmed Nader, 2013

25 Packaged Chip + Chip Micrograph Wi-Fi Receiver 17 mm 2 2/25/2021 © Ahmed

25 Packaged Chip + Chip Micrograph Wi-Fi Receiver 17 mm 2 2/25/2021 © Ahmed Nader, 2013

26 MOS Structure • A piece of polysilicon with a width of W and

26 MOS Structure • A piece of polysilicon with a width of W and length of L on top of a thin layer of oxide defines the gate area. • Source and drain areas are heavily doped. • Substrate usually tied to the most negative voltage. • Leff = L – 2 LD, where LD is the side diffusion of source and drain. 2/25/2021 © Ahmed Nader, 2013

27 MOS characteristics – Threshold Voltage 2/25/2021 © Ahmed Nader, 2013

27 MOS characteristics – Threshold Voltage 2/25/2021 © Ahmed Nader, 2013

28 MOS characteristics – Threshold Voltage • 2/25/2021 © Ahmed Nader, 2013

28 MOS characteristics – Threshold Voltage • 2/25/2021 © Ahmed Nader, 2013

29 MOS characteristics – Threshold Voltage • Remember PVT (Process, Voltage, Temperature Variations) 2/25/2021

29 MOS characteristics – Threshold Voltage • Remember PVT (Process, Voltage, Temperature Variations) 2/25/2021 © Ahmed Nader, 2013

30 MOS I-V characteristics • 2/25/2021 © Ahmed Nader, 2013

30 MOS I-V characteristics • 2/25/2021 © Ahmed Nader, 2013

31 MOS I-V characteristics 2/25/2021 © Ahmed Nader, 2013

31 MOS I-V characteristics 2/25/2021 © Ahmed Nader, 2013

32 MOS I-V characteristics • 2/25/2021 © Ahmed Nader, 2013

32 MOS I-V characteristics • 2/25/2021 © Ahmed Nader, 2013

33 MOS Device as a Resistor 2/25/2021 © Ahmed Nader, 2013

33 MOS Device as a Resistor 2/25/2021 © Ahmed Nader, 2013

34 MOS I-V characteristics • 2/25/2021 © Ahmed Nader, 2013

34 MOS I-V characteristics • 2/25/2021 © Ahmed Nader, 2013

35 MOS I-V characteristics • 2/25/2021 © Ahmed Nader, 2013

35 MOS I-V characteristics • 2/25/2021 © Ahmed Nader, 2013

36 MOS: In Saturation • 2/25/2021 © Ahmed Nader, 2013

36 MOS: In Saturation • 2/25/2021 © Ahmed Nader, 2013

37 MOS: Channel length modulation • Channel length modulation by VDS causes the saturation

37 MOS: Channel length modulation • Channel length modulation by VDS causes the saturation current to vary with VDS. λ is the channel length modulation parameter (V-1) 2/25/2021 © Ahmed Nader, 2013

38 MOS: Channel length modulation λ undesired second order effect 2/25/2021 © Ahmed Nader,

38 MOS: Channel length modulation λ undesired second order effect 2/25/2021 © Ahmed Nader, 2013

39 MOS: Substrate or Body Effect • 2/25/2021 © Ahmed Nader, 2013

39 MOS: Substrate or Body Effect • 2/25/2021 © Ahmed Nader, 2013

40 MOS: Bulk Driven Can be used in low-voltage applications 2/25/2021 © Ahmed Nader,

40 MOS: Bulk Driven Can be used in low-voltage applications 2/25/2021 © Ahmed Nader, 2013

41 Body Effect: Non-linearity 2/25/2021 © Ahmed Nader, 2013

41 Body Effect: Non-linearity 2/25/2021 © Ahmed Nader, 2013

42 Substrate: Where to connect it? For NMOS • To the most negative available

42 Substrate: Where to connect it? For NMOS • To the most negative available potential • To a carefully designed potential (for example source such that VSB=0) in the case of twin well process or triple well (deep NWELL) process 2/25/2021 © Ahmed Nader, 2013

43 Triple Well Option 2/25/2021 © Ahmed Nader, 2013

43 Triple Well Option 2/25/2021 © Ahmed Nader, 2013

44 Region of Operation: Conceptual Visualization • VDS < VGS-VTH MOS transistor in linear

44 Region of Operation: Conceptual Visualization • VDS < VGS-VTH MOS transistor in linear region. • In linear region, MOS transistor acts as a resistor or a switch. NMOS 2/25/2021 PMOS © Ahmed Nader, 2013

45 MOS: Subthreshold (Weak Inversion) • Subthreshold Conduction: For VGS near VTH, ID has

45 MOS: Subthreshold (Weak Inversion) • Subthreshold Conduction: For VGS near VTH, ID has an exponential dependence on VGS: Max transconductance efficiency Used for low currents & low frequency applications 2/25/2021 © Ahmed Nader, 2013

46 MOS: Intrinsic Capacitance C 1 is the gate-channel capacitance C 2 is the

46 MOS: Intrinsic Capacitance C 1 is the gate-channel capacitance C 2 is the channel-bulk depletion capacitance C 3 & C 4 is the overlap gate-source(drain) capacitance C 5 & C 6 is the source/drain –bulk junction capacitance (bottomplate and sidewall) Note that junction capacitors are voltage-dependent (non-linear) • • 2/25/2021 © Ahmed Nader, 2013

47 MOS: Intrinsic Capacitance • 2/25/2021 © Ahmed Nader, 2013

47 MOS: Intrinsic Capacitance • 2/25/2021 © Ahmed Nader, 2013

48 MOS Device as a Capacitor: Varactor Assignment 1 a: There is a special

48 MOS Device as a Capacitor: Varactor Assignment 1 a: There is a special device with n-doping in an NWELL. Plot the characteristics of such a device. Comment on its properties. 2/25/2021 © Ahmed Nader, 2013

49 Small Signal Model • The slope of the diode characteristic at the Q-point

49 Small Signal Model • The slope of the diode characteristic at the Q-point is called the diode conductance and is given by: • gd is small but non-zero for ID = 0 because slope of diode equation is nonzero at the origin. • Diode resistance is given by: 2/25/2021 © Ahmed Nader, 2013

50 Small Signal Operation of a Diode Subtracting ID from both sides of the

50 Small Signal Operation of a Diode Subtracting ID from both sides of the equation, For id to be a linear function of signal voltage vd , This represents the requirement for small-signal operation of the diode. 2/25/2021 © Ahmed Nader, 2013

51 Current Controlled Attenuator Magnitude of ac voltage vo developed across diode can be

51 Current Controlled Attenuator Magnitude of ac voltage vo developed across diode can be controlled by value of dc bias current applied to diode. From dc equivalent circuit ID = I, From ac equivalent circuit, For RI = 1 k. W, IS = 10 -15 A, If I = 0, vo = vi, magnitude of vi is limited to only 5 m. V. If I = 100 m. A, input signal is attenuated by a factor of 5, and vi can have a magnitude of 25 m. V. 2/25/2021 © Ahmed Nader, 2013

52 Small-Signal Model of a MOS (Two-Port Model) Using 2 -port y-parameter network, The

52 Small-Signal Model of a MOS (Two-Port Model) Using 2 -port y-parameter network, The port variables can represent either time-varying part of total voltages and currents or small changes in them away from Q-point values. 2/25/2021

53 Small-Signal Model of a MOS Transconductance: Output resistance: • Since gate is insulated

53 Small-Signal Model of a MOS Transconductance: Output resistance: • Since gate is insulated from channel by gate-oxide input resistance of transistor is infinite. • Small-signal parameters are controlled by the Q-point. • For same operating point, MOSFET has lower transconductance and lower output resistance that BJT. 2/25/2021

54 MOS Transistor 2/25/2021 © Ahmed Nader, 2013

54 MOS Transistor 2/25/2021 © Ahmed Nader, 2013

55 MOS Transistor Small Signal Model: Body Effect Drain current depends on threshold voltage

55 MOS Transistor Small Signal Model: Body Effect Drain current depends on threshold voltage which in turn depends on v. SB. Back-gate transconductance is: 0 < < 1 is called back-gate tranconductance parameter. 2/25/2021 © Ahmed Nader, 2013

56 Small-Signal Model of a MOS: High Frequency Model • Voltage dependent current source

56 Small-Signal Model of a MOS: High Frequency Model • Voltage dependent current source (gm. Vgs) models dependence of drain current on gate-source voltage • Output resistance models dependence of drain current on drainsource voltage (channel length modulation) • Voltage dependent current source (gmb. Vbs) models dependence of drain current on bulk-source voltage (body effect) 2/25/2021 © Ahmed Nader, 2013

57 MOS Transistor Useful Model • Small Signal: + - 2/25/2021 © Ahmed Nader,

57 MOS Transistor Useful Model • Small Signal: + - 2/25/2021 © Ahmed Nader, 2013

58 MOS Transistor Special Cases Bias point 2/25/2021 © Ahmed Nader, 2013

58 MOS Transistor Special Cases Bias point 2/25/2021 © Ahmed Nader, 2013

59 Deep Sub-Micron Technologies • 2/25/2021 © Ahmed Nader, 2013

59 Deep Sub-Micron Technologies • 2/25/2021 © Ahmed Nader, 2013

60 • Fixed for the technology and fixed L Low-voltage – High. Speed trade-off

60 • Fixed for the technology and fixed L Low-voltage – High. Speed trade-off 2/25/2021 © Ahmed Nader, 2013

61 Deep Sub-Micron Technologies Some small geometry effects: 1 - Gate leakage 2 -

61 Deep Sub-Micron Technologies Some small geometry effects: 1 - Gate leakage 2 - Threshold voltage variation 3 - Output impedance variation with VDS (non-linearity) 4 - Mobility degradation with vertical field 5 - Velocity saturation 6 - Reliability Effects (GO, Hot Carrier, NBTI, . . ) 7 - Stress Effects (STI, Well Proximity, . . ) Assignment 1 b: Choose one of those effects and describe it in details (physical meaning, effect on performance, etc. ) 2/25/2021 © Ahmed Nader, 2013

62 Deep Sub-Micron Technologies What about scaling of Vth? 2/25/2021 © Ahmed Nader, 2013

62 Deep Sub-Micron Technologies What about scaling of Vth? 2/25/2021 © Ahmed Nader, 2013

63 Deep Sub-Micron Technologies – Mobility degradation with Vertical Field • Carriers are confined

63 Deep Sub-Micron Technologies – Mobility degradation with Vertical Field • Carriers are confined to a narrower region below oxidesilicon interface leading to more carrier scattering and hence lower mobility 2/25/2021 © Ahmed Nader, 2013

64 Deep Sub-Micron Technologies – Velocity Saturation • 2/25/2021 © Ahmed Nader, 2013

64 Deep Sub-Micron Technologies – Velocity Saturation • 2/25/2021 © Ahmed Nader, 2013

65 Deep Sub-Micron Technologies – Velocity Saturation • 2/25/2021 © Ahmed Nader, 2013

65 Deep Sub-Micron Technologies – Velocity Saturation • 2/25/2021 © Ahmed Nader, 2013

66 MOS Device Models Level 3 Model BSIM (Berkeley Short-Channel IGFET Model) 2/25/2021 ©

66 MOS Device Models Level 3 Model BSIM (Berkeley Short-Channel IGFET Model) 2/25/2021 © Ahmed Nader, 2013