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Lecture 9 Design

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Title: Lecture 9 Design


1
Lecture 9Design Leakages of Low-Voltage CMOS
Devices
  • Circuit design style
  • Leakage current in deep submicron transistors
  • Summary
  • Michael L. Bushnell
  • CAIP Center and WINLAB
  • ECE Dept., Rutgers U., Piscataway, NJ

2
Introduction
  • Lower MOS supply voltages save energy
  • Require low transistor threshold voltages
  • Causes sub-threshold leakage currents to be
    significant
  • Need to control leakage currents with device
    design
  • Need to run slower parts of circuit at lower
    voltage
  • Circuit design style (type of CMOS logic) is
    critical
  • High leakages require modified IDDQ testing
  • Modify to account for operating frequency

3
Power Versus Supply and Vt
4
Non-Clocked Logic
  • Static CMOS
  • nMOS
  • Pseudo-nMOS
  • Differential Cascode Voltage Switch (DCVS) Logic
  • Pass Transistor Logic

5
Static CMOS
  • Easy to design
  • Uses low power
  • Low sensitivity to noise and process variations
  • High noise margin
  • Scalable
  • Lower performance for large fanin gates,
    especially in pMOS tree
  • Power due to short-circuit, switching, and
    glitching currents
  • Standby mode power only due to leakages
    (neglect)

6
nMOS Logic
  • Ratioed logic R LOAD gt 4 X RPull-down

7
Pseudo-nMOS Logic
8
Pseudo-nMOS Logic
  • Less complex than static CMOS, so lower CL,
    faster
  • Unlike nMOS, load device unaffected by body
    effect
  • Ratioed design style good for large fanin
    NAND/NOR
  • Uses more power than static CMOS
  • Power always flows when pull-down network on

9
Differential Cascode Voltage Switched Logic (DCVS)
10
DCVS Logic
  • No static power dissipation
  • Faster (than static CMOS) because of ratioed
    logic
  • Two pull-down network functions are complementary
  • Larger area and switched capacitance
  • Inverters rarely needed
  • Sometimes can share hardware between two
    pull-down networks

11
Pass Transistor Logic
  • Switches in series implement AND function
  • Switches in parallel implement OR function
  • Fast, but transmits logic 1 as VDD Vtn
  • Needs logic level restorers

12
Complementary Pass Transistor Logic (CPL)
AND/NAND
B
B
A
AB
B
A B
A
B
13
Complementary Pass Transistor Logic (CPL)
XOR/XNOR

A B
A B

14
Complementary Pass-Transistor Logic (CPL)
  • Advantages
  • Differential output signals
  • Modular
  • Reduced internal CL low power
  • Can support reduced voltage swing
  • 32-bit Adder CPL has 10 lower power-delay
    product than static CMOS

15
Clocked Logic
  • Domino Logic
  • Differential Current Switch Logic (DCSL)
  • Uses less power than Domino logic
  • Higher performance at expense of higher power
    dissipation

16
Domino Logic
  • Keeper transistor very useful with leaky
    transistors

17
Domino Logic
  • Only implements non-inverting logic gates
  • Very good for large fanin gates NAND/NOR
  • Inputs connect only to 1 transistor reduced CL
  • Increased signal activity extra loads for clock
    line
  • High power usage compared with static CMOS
  • Many glitches due to clock
  • Spurious transitions not possible on output
  • Not as scalable as static CMOS
  • Lower noise immunity, so need higher Vt

18
Differential Current Switch Logic (DCSL) Gate
19
Differential Current Switch Logic
  • DCVS logic gate modified to reduce internal node
    voltage swings
  • T2, T3, T6, T7 cross-coupled inverter pair
  • T1 T4 Precharge outputs high
  • Note T12 sometimes needed to prevent internal
    node charge buildup
  • Advantage Once evaluation completed, high output
    is disconnected from n-tree, so further input
    changes ignored
  • No static paths from VCC to ground at end of
    evaluation
  • Can get completion signal by NANDing two outputs
  • Internal node swings for DCSL (DCSL2) are 1 V
    (0.3 V)

20
DCSL Gate Operation
  • When CLK low, Q and Q precharged high
  • When CLK high, nMOS tree inputs must be stable
  • T9, T10, T11 switched on by high CLK
  • Precharged outputs switch on T5, T6, T7, T8
  • Q and Q discharge asymmetrically towards ground
  • One of the paths to ground is stronger (say Q)
  • So, Q falls faster than Q
  • Cross-coupled inverter functions as sense
    amplifier
  • Boosts output voltage differential in the right
    direction, so Q swings high
  • Logic limits charge-up of internal nodes of nMOS
    tree to voltages much smaller than VCC
    Vtn (limit for DCVS Logic)

21
DCSL2 Gate (Precharged Low)
  • CLK high is precharge, CLK low is evaluation
  • Degraded gate propagation delay

22
DCSL3 (Best Version)
  • Removed T9 and T10, replaced with T9
  • Precharge Q and Q to Vtn or lower
  • Saves power, faster than DCSL2 (less O/P voltage
    swing)

23
Energy Consumption
24
CLK-to-Q Delay 90 / 10
25
CLK-to-Q Delay 50
26
Energy X Delay vs. n-Tree Height
27
Leakage Current in Deep Submicron Devices
  • Transistor off-state current when VGS 0
  • Long-channel devices dominated by
  • Drain-well leakage
  • Well-substrate leakage
  • Short-channel devices dominated by
  • Vt
  • Channel physical dimensions
  • Channel/surface doping profile
  • Drain/source junction depth
  • Gate oxide thickness
  • VDD, drain, and gate voltages

28
Transistor Leakages
29
Transistor Leakages
  • I1 pn Reverse-Bias Current
  • I2 Weak Inversion
  • I3 Drain-Induced Barrier-Lowering (DIBL) Effect
  • I4 Gate-Induced Drain Leakage (GIDL)
  • I5 -- Punchthrough
  • I6 Narrow-Width Effect
  • I7 Gate Oxide Tunneling
  • I8 Hot-Carrier Injection

30
pn Reverse-Bias Current
  • Minority-carrier drift near edge of depletion
    region
  • Electron-hole pair generation in depletion region
    (reverse-biased junction)
  • If heavily doped, Zener tunneling may also happen
  • MOSFET added leakage
  • Between drain and well junction (due to overlap
    of gate to drain to well pn junctions)
  • Carrier generation in drain-to-well depletion
    regions
  • pn reverse-bias leakage f (junction area,
    doping)

31
Weak Inversion in 3.5 mm Technology Dominates
Leakage
  • Happens in nFET when gate is below Vt
  • Carriers diffuse through channel (no horizontal E)

32
CMOS Technologies
33
Subthreshold Swing (Slope) St
  • Has not increased with new technologies because
    tox got smaller and substrate doping profiles
    improved
  • Value of St 100 mV/decade is unacceptable

34
Drain-Induced Barrier-Lowering
  • Depletion region of drain interacts with source
    near channel surface
  • Lowers source potential barrier
  • Causes source to inject carriers into channel
    surface independently of gate voltage
  • More DIBL at higher VD and shorter Leff
  • Surface DIBL happens before deep bulk
    punchthrough
  • Fix DIBL
  • Higher surface channel doping
  • Shallow source/drain junction depths

35
DIBL Effects
  • Moves curve up, to right as VD increases
  • VD going from 0.1 to 2.7 V, ID changed 1.68
    decades
  • DIBL 1.55 mV/decade change of ID

36
Gate-Induced Drain Leakage
  • Generates carriers into substrate and drain from
    surface traps or band-to-band tunneling
  • Due to high electric field under gate/drain
    overlap region that causes deep depletion
  • Happens at low VG and high VD bias
  • Localized along channel width between gate and
    drain
  • Appears as hook in last figure
  • Increasing current for negative VG values
  • Major problem in Ioff current
  • Caused by thinner tox, higher VDD, and lightly
    doped drains

37
Punchthrough
  • Happens when drain and source depletion regions
    approach each other and touch
  • Lets channel current exist deep in sub-gate
    region
  • Gate loses control of sub-gate region
  • Varies quadratically with VD and with St
  • Viewed as subsurface version of DIBL

38
Narrow-Width Effect
  • Trench isolation
  • Dig trench in substrate and fill with SiO2 to
    isolate n and p MOSFETs
  • Non-trench isolated technologies
  • Vt increases for gate widths of 0.5 mm
  • Trench isolated technologies
  • Vt decreases for effective channel widths W
    0.5 mm

39
Gate Oxide Tunneling
  • High Eox electric field across oxide layer
    causes
  • Direct electron tunneling through gate
  • Fowler-Nordheim (FN) tunneling through oxide
    bands (usually only at higher Eox than chips use)
  • Currently a non-issue, expected to become
    dominant leakage condition as oxides get thinner

40
Tunneling
41
Hot-Carrier Injection
  • Short-channel transistors susceptible to hot hole
    and electron injection into oxide layer
  • Reliability risk
  • Increases as Leff is reduced unless VDD is scaled

42
Leakage Summary
  • GIDL dominates
  • DIBL dominates
  • Weak inversion dominates

43
Leakage Current Estimation
  • Ignore diode junction leakage
  • Subthreshold leakage increases exponentially with
    reduction of Vt
  • Necessary transistor model elements
  • Sub-zero VGS for nFET
  • Super-zero VGS for pFET
  • Body effect
  • DIBL

44
Subthreshold Current of MOSFET BSIM2 Model
  • Cox gate oxide C/unit area
  • m0 zero-bias mobility
  • n subthreshold swing coefficient
  • Vth0 zero-bias threshold voltage
  • VS source voltage (above bulk voltage)
  • g linearized body effect coefficient
  • h DIBL coefficient

45
Finding VDS for Transistor Stack
  • Parallel off transistors VDS and VS same for
    both
  • Series transistors leakages same through all
  • Consider all nFETs turned off
  • Equate top of stack transistor and 2nd transistor
    leakage currents
  • Solve for VDS2 in terms of VDD
  • Solve for VDSi in terms of VDSi-1

46
Computing Pleak
  • Get VDSi
  • Use Equation 5.2 to get Isub
  • Sum up
  • For large circuit
  • Determine pull-up and pull-down trees that are
    off
  • Turned-on transistors treated as short circuits
  • Ignore transistors parallel to turned-on
    transistors
  • Use above method to get leakage power
  • Calculate sensitivity to Vth

47
Input Selection for Standby Mode
  • Logic gate input vectors greatly affect leakage
    current
  • Can apply low leakage current vector in standby
    mode
  • Genetic algorithm (Chen et al.) to estimate
    standby leakage power

48
Summary
  • CMOS logic family greatly affects power
  • Pass transistor logic on SOI is most promising
  • Leakage current calculation in deep submicron
    transistors is important
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