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Ensuring Signal and Power Integrity

for High-Speed Digital Systems

An EMC Perspective

Christian Schuster

Institut für Theoretische Elektrotechnik

Technische Universität Hamburg-Harburg (TUHH)

Invited Presentation at the IEEE International Conference on Consumer

Electronics (ICCE), Berlin, September 6-9, 2015

C. Schuster, TUHH – 2

Abstract

With increasing data rates and reduced margin for communication

errors both consumer electronic products as well a large-scale

digital systems like data centers have to be designed very carefully

with respect to their “electrical integrity”. In this presentation two

aspects of this integrity, namely signal integrity (SI) and power

integrity (PI), will be explained in some detail. The focus will be put

mostly on packaging and electromagnetic compatibility (EMC)

aspects. Topics that will be addressed include discontinuities,

transmission line effects, crosstalk, bypassing and decoupling, via

and power plane effects, return current issues, and measurement

techniques. The presentation should be suitable for both a

technical and a non-technical audience. For more information on SI

and PI research at TUHH visit: http://www.tet.tuhh.de

C. Schuster, TUHH – 3

(1) Motivation

(2) SI, PI & EMI

(3) High-Speed Digital Systems

(4) Improving SI

(5) Improving PI

(6) Wrapping Up

Outline

C. Schuster, TUHH – 4

(1)

Motivation

C. Schuster, TUHH – 5

Digital Link Data Rates

Data Rate [Gb/s]

10

5

CPU to CPU Storage Network/ Peripherals

Infiniband

10.0

PCIe

5.0

Hyper

Transport

5.2

SA-SCSI

3.0

SATA III

6.0 Fibre

Channel

4.25

10G Ethernet

10.0

USB 2.0

0.5

FireWire

up 3.2

DVI

3.7

DDR3

8-12

C. Schuster, TUHH – 6

Digital Link Frequency Trends

C. Schuster, TUHH – 7

(2)

SI, PI & EMI

C. Schuster, TUHH – 8

Power Plane Ground Plane

Driver Via

Receiver

Digital Link Seen From ..

DC Power Supply

PCB

C. Schuster, TUHH – 9

.. a Signal Transmission Perspective

Signal Transmission Issues:

Attenuation, Reflection, Dispersion, Interference, Crosstalk

C. Schuster, TUHH – 10

.. a Signal Transmission Perspective

Signal Transmission Issues:

Attenuation, Reflection, Dispersion, Interference, Crosstalk

C. Schuster, TUHH – 11

.. a Power Delivery Perspective

Power Delivery Issues:

Voltage Drop, Switching Noise, Crosstalk

C. Schuster, TUHH – 12

.. a Power Delivery Perspective

Power Delivery Issues:

Voltage Drop, Switching Noise, Crosstalk

C. Schuster, TUHH – 13

.. an EMI Perspective

Electromagnetic Interference Issues:

Near Field Coupling, Radiated Emissions

C. Schuster, TUHH – 14

.. an EMI Perspective

Electromagnetic Interference Issues:

Near Field Coupling, Radiated Emissions

C. Schuster, TUHH – 15

SI + PI + EMI = Comprehensive EMC

Elements of a comprehensive EMC

C. Schuster, TUHH – 16

SI/PI Foundations and Resources

SI / PI

Transmission

Line Theory

Antenna

Theory

Network

Theory System Theory

Coupler &

Filter Design

EM Field

Theory

Communication

Theory

Circuit Design &

Simulation

Numerical

Techniques

Electromagnetic

Compatibility

HF Measurement

Techniques

CAD Tools

Material

Characterizationj

C. Schuster, TUHH – 17

SI/PI Foundations and Resources

© C. Schuster, TUHH

Figures © C. Schuster,

TET, TUHH

C. Schuster, TUHH – 18

SI/PI in the IEEE Community

Number of publications

found in IEEE Xplore

containing the index

terms:

“Signal Integrity“

“Power Integrity“

C. Schuster, TUHH – 19

SI/PI in the EMC Community

C. Schuster, TUHH – 20

SI/PI in the EMC Community

C. Schuster, TUHH – 21

(3)

High-Speed Digital Systems

C. Schuster, TUHH – 22

A High-Speed Digital System

Housing / Chassis

Connector

Package / Module

IC (Transmitter)

IC (Receiver)

Connector

Cable

Backplane / Motherboard

Socket

Da

ug

hte

rca

rd

C. Schuster, TUHH – 23

The SI Challenge

Connector

Interconnect

(Link)

C. Schuster, TUHH – 24

The ideal interconnect will simply delay the signal:

Any real interconnect will additionally change timing and amplitude:

t

Tx Rx

t

Tx Rx

Effect of Interconnects

C. Schuster, TUHH – 25

Jitter and Noise

The deviations in timing and amplitude are in general called:

t

Timing jitter or simply: JITTER

Amplitude noise or simply: NOISE

C. Schuster, TUHH – 26

NOISE

Receiver

Sampling

Point

In the eye diagram timing jitter and anplitude noise are defined as follows:

JITTER

Jitter and Noise

C. Schuster, TUHH – 27

The PI Challenge

Connector VRM

1 V

3.3 V

C. Schuster, TUHH – 28

Effect of Common Power Delivery

IC #1 IC #2

U0

ZPDN

PDN = Power Delivery Network

C. Schuster, TUHH – 29

Effect of Common Power Delivery

U0

R uIC L

iGate1, iGate2, …

Du

uIC = U0 - Du

...)()(...)()()( Gate1Gate1Gate1Gate1 D titidt

dLtitiRtu

"DC-drop or IR-drop" "DI-drop or DI-noise"

C. Schuster, TUHH – 30

(4)

Improving SI

C. Schuster, TUHH – 31

Improving Signal Integrity

1. Match terminations

2. Minimize discontinuities

3. Reduce Coupling

4. Limit attenuation

5. Balance deficiencies

C. Schuster, TUHH – 32

Tx

High performance digital links are mostly serial: HSS = HIGH SPEED SERIAL.

The technology is typically CMOS with the links being voltage mode,

unidirectional, serial, point-to-point, and source-synchronous. Both single-ended

and differential signaling can be found.

For improved bandwidth equalization is typically used in the Tx, Rx, or both.

CDR

.

.

.

Deserializer

Interconnect

Clock & Data Recovery

Data .

.

.

Serializer

Data

Clock

Equalizer

Equalizer

+ Slicer

Rx

Typical Digital Link Design

C. Schuster, TUHH – 33

Improving Signal Integrity

1. Match terminations

2. Minimize discontinuities

3. Reduce Coupling

4. Limit attenuation

5. Balance deficiencies

C. Schuster, TUHH – 34

Effect of Terminations

Let‘s use the following interconnect (link) model:

lZ ,,0

u0 u1 u2

LZSZ

Transmitter Receiver Interconnect

??

C. Schuster, TUHH – 35

Metal Dielectric

Microstrip

Line

Stripline

(symmetric)

(h = height of dielectric,

w = conductor width,

t = conductor thickness)

tw

hZ

8.0

98.5ln

41.1

87

r

0

tw

hZ

8.0

9.1ln

60

r

0

(h = height of dielectric,

w = conductor width,

t = conductor thickness)

Transmission Lines in Digital Systems

C. Schuster, TUHH – 36

Let‘s use the following interconnect (link) model:

lZ ,,0

u0 u1 u2

LZSZ

!max. and const.0

2 u

u

Effect of Terminations

??

C. Schuster, TUHH – 37

lZ ,,0

LZSZ

input acceptance TL transfer function

source transmission load transmission

source reflection load reflection

Effect of Terminations

C. Schuster, TUHH – 38

lZ ,,0

LZSZ

Effect of Terminations

!!1

)1(

1 SL

2

L

SL

2

L

0

trans

0

2

rrH

rHa

rrH

tHa

u

u

u

u

C. Schuster, TUHH – 39

Hu

u

2

1

0

2 0LS ZZZ

lZ ,,0

LZSZ

0L ZZ Hau

u

0

2

Effect of Terminations

C. Schuster, TUHH – 40

Matched interconnect:

Mismatched Interconnect:

Time

low source impedance

high source impedance

D2 T

Time

Vo

lta

ge

lossless transmisson line

Vo

lta

ge

DT

lossy transmisson line

Effect of Terminations

C. Schuster, TUHH – 41

3

4

2

5 6

1

1 kΩ1,Ω50,Ω10 L0S ZZZ

zero losses

2 Ω100,Ω50,Ω50 L0S ZZZ

zero losses

3 Ω50,Ω50,Ω50 L0S ZZZ

zero losses

4 Ω100,Ω50,Ω100 L0S ZZZ

zero losses

kΩ1,Ω50,Ω10 L0S ZZZ

non-zero losses

5

6 Ω50,Ω50,Ω50 L0S ZZZ

non-zero losses

(all lines have a delay of 0.1 ns)

Effect of Terminations

C. Schuster, TUHH – 42

Improving Signal Integrity

1. Match terminations

2. Minimize discontinuities

3. Reduce coupling

4. Limit attenuation

5. Balance deficiencies

C. Schuster, TUHH – 43

Packaging of Digital Systems

Connector

Interconnect

(Link)

C. Schuster, TUHH – 44

Effect of Lumped Discontinuities

Signal

Out

Signal

In

u1 u2 50

50 2.5

nH

Tx-Output Bond Wire Rx-Input

Source

Voltage

Received

Voltage

© C. Schuster, TUHH

C. Schuster, TUHH – 45

Effect of Lumped Discontinuities

Attenuation of high frequency signal components

„Slowing down" of the edges of a digital signal

Frequency [GHz] Time [ps]

Magnitude o

f u

2 /

u1

u2(t

) /

u1(t

)

Frequency Response Step Response

f0 ≈ 6.37 GHz t 1/w0 = 25 ps

C. Schuster, TUHH – 46

Effect of Lumped Discontinuities

u1 u2

Signal

In Signal

Out

50 50 1 pF

Tx-Output Via Rx-Input

Source

Voltage

Received

Voltage

© Y. Kwark, IBM

C. Schuster, TUHH – 47

Effect of Lumped Discontinuities

Attenuation of high frequency signal components !!

„Slowing down" of the edges of a digital signal !!

Frequency [GHz] Time [ps]

Magnitude o

f u

2 /

u1

u2(t

) /

u1(t

)

Frequency Response Step Response

f0 ≈ 6.37 GHz t 1/w0 = 25 ps

C. Schuster, TUHH – 48

Effect of Distributed Discontinuities

lZ ,, 0Z0Z

GHzl

cf 952.2

4

1 inch, 45 Ohm mismatched transmission line at c0 /2

Frequency Response

(Scattering Parameters)

C. Schuster, TUHH – 49

Overall Effect of Discontinuities

0 0 0 0

Port1 Port2

Z=49

P=1cm

300fF

2nHZ=48

P=15cm

300fF

2nH

300fF

Z=52

P=5cm

300fF

Z=48

P=1cm

2nH

C. Schuster, TUHH – 50

Improving Signal Integrity

1. Match terminations

2. Minimize discontinuities

3. Reduce coupling

4. Limit attenuation

5. Balance deficiencies

C. Schuster, TUHH – 51

Packaging of Digital Systems

Connector

Interconnect

(Link)

C. Schuster, TUHH – 52

(3) Near End (4) Far End

Aggressor Line (Active Line)

Victim Line (Quiet Line)

(1) Input (2) Output

Effect of Coupling

Consider two transmission lines in close proximity:

C. Schuster, TUHH – 53

IC

IC-NE IC-FE

Effect of Coupling

Consider two transmission lines in close proximity:

Capacitive Crosstalk

C. Schuster, TUHH – 54

UL

UL-NE UL-FE

Effect of Coupling

Consider two transmission lines in close proximity:

Inductive Crosstalk

C. Schuster, TUHH – 55

UL

IC

(3) Near End (4) Far End

(1) Input (2) Output

NEXT =

Near End Crosstalk (sum of ind. and cap. crosstalk)

FEXT =

Far End Crosstalk (difference of ind. and cap. crosstalk)

Consider two transmission lines in close proximity:

Effect of Coupling

C. Schuster, TUHH – 56

Improving Signal Integrity

1. Match terminations

2. Minimize discontinuities

3. Reduce Coupling

4. Limit attenuation

5. Balance deficiencies

C. Schuster, TUHH – 57

Attenuation usually increases with frequency. The exact calculation can be

difficult but for weakly lossy lines:

a convenient approximations exists:

with ac = attenuation due to conductor losses and ad = attenuation due to

dielectric losses. The following dependencies are often found:

with k = electrical conductivity and tan d = loss tangent.

CGLR ww and

dc22

aaa

C

LG

L

CR

dw tan~ CGkw /~R

Contributors to Line Losses

C. Schuster, TUHH – 58

Time Domain Effect of Losses

When taking into account DC losses the effect in the time domain is twofold:

edge degradation

DC drop

Time

Voltage

step response

without losses

step response

with losses

C. Schuster, TUHH – 59

For the frequency dependence follows with these assumptions:

In other words, a typical semi-

logarithmic plot of the magnitude

of the transfer function will be

dominated by a square root

behavior at lower and a linear

behavior at higher frequencies.

fflllleeeeeeH

dcdc constconst

~aaa

ffH dc constconst~ln

linear

square root

total

Frequency Dependence of Losses

C. Schuster, TUHH – 60

Dielectric Packaging Materials

Dielectric materials are typically classified with respect to their

relatice dielectric constant r and their loss tangent tan d:

tan d

r

Quartz (SiO2) Alumina (Al2O3)

"FR-4"

Silicon Teflon (PTFE)

C. Schuster, TUHH – 61

Improving Signal Integrity

1. Match terminations

2. Minimize discontinuities

3. Reduce coupling

4. Limit attenuation

5. Balance deficiencies

C. Schuster, TUHH – 62

Overview of Equalization Techniques

Tx

CDR

.

.

.

Deserializer

Interconnect

Clock & Data Recovery

Data .

.

.

Serializer

Data

Clock

Equalizer

Equalizer

+ Slicer

Rx

Most high speed serial links nowadays use some EQUALIZATION, i.e. some

kind of signal processing technique to correct for the degradations in the

interconnect, and thereby improve the quality of signals. When the corrections

are applied at the transmitter equalization is sometimes also called DE-

EMPHASIS or PRE-EMPHASIS. Apart from continuous time equalization (CTE)

signal processing takes place in the discrete time domain / digital filters.

C. Schuster, TUHH – 63

Overview of Equalization Techniques

In frequency domain the effect of equalization can be to some extent be

visualized as the flattening of the transfer function of the interconnect.

An interconncet with a completely flat transfer function would transmit a signal

undisturbed apart from a potential amplitude scaling.

f

TF

Interconnect

f

Equalization

f

Equalized Response

=

C. Schuster, TUHH – 64

Two big classes of (digital, discrete) equalization exist:

Equalization

Linear Feedforward

Equalization (LFE/FFE) Distributed Feedback

Equalization (DFE)

- Uses only information from the

current and previously received

bits

- Can be interpreted as a non-

recursive digital filter (finite

impulse response filter)

- Uses a feedback loop after the

signal has been decoded by an

LFE/FFE

- The output of the LFE/FFE is

added to the feedback loop

resulting in the equalized signal

Overview of Equalization Techniques

C. Schuster, TUHH – 65

(5)

Improving PI

C. Schuster, TUHH – 66

Improving Power Integrity

1. Decrease PDN impedance

2. Add decoupling

3. Add more decoupling

4. Use several power supplies

5. Use on-chip VRMs

C. Schuster, TUHH – 67

Discrete

Decoupling

Capacitors

(various sizes)

IC incl.

Power/Ground Grid

& Integrated Decaps

Printed Circuit Board incl.

Power/Ground Planes

High Power

DC Supply

Voltage

Regulator

Module

Package incl.

Power/Ground

Planes

PDN Elements

C. Schuster, TUHH – 68

Improving Power Integrity

1. Decrease PDN impedance

2. Add decoupling

3. Add more decoupling

4. Use several power supplies

5. Use on-chip VRMs

C. Schuster, TUHH – 69

A typical maximum ripple for ditigal systems is:

With a 10% value the following numbers can be obtained for

applications … of the early 1990'ies: … of 2000 and on:

PDN Impedance

Ω5.0

W5

Ω0.5/

A1

V0.5

Target

avg

avg0

avg

0

Z

P

iu

i

u

%10to%5ripple maximum0

max D

u

u

Ω001.0

W144

Ω01.0/

A120

V2.1

Target

avg

avg0

avg

0

Z

P

iu

i

u

= 1 m !

C. Schuster, TUHH – 70

Improving Power Integrity

1. Decrease PDN impedance

2. Add decoupling

3. Add more decoupling

4. Use several power supplies

5. Use on-chip VRMs

C. Schuster, TUHH – 71

Low Frequency Equivalent PDN Circuit

R L

U0 ~ ZIC ( f )

C. Schuster, TUHH – 72

… including a "decoupling" or "bypass" capacitor:

Low Frequency Equivalent PDN Circuit

R L

U0 ~ ZIC ( f ) C

… some nF to some mF

© C. Schuster, TUHH

C. Schuster, TUHH – 73

Heuristic explanation:

Frequency domain: Beyond the resonance frequency the capacitor

decouples the part of the PDN that lies "left" of him, i.e. the IC sees

only the impedance of the capacitor.

Time domain: The capacitor stores charges close to the IC that can

become currents needed for fast switching. It is like a "small battery".

Decoupling Effect

R L

U0 ~ ZIC ( f ) C

C. Schuster, TUHH – 74

Unfortunately, there is no ideal capacitor available in the real world!

Ideal world: … and real world:

R is also is called the EQUIVALENT SERIES RESISTANCE

(ESR) and L the EQUIVALENT SERIES INDUCTANCE (ESL).

As a consequence any real world capacitor behaves approximately

like an inductor beyond its resonance frequency:

Real Word Decoupling Capacitors

C R L C

LC/10 w

C. Schuster, TUHH – 75

Improving Power Integrity

1. Decrease PDN impedance

2. Add decoupling

3. Add more decoupling

4. Use several power supplies

5. Use on-chip VRMs

C. Schuster, TUHH – 76

More Decoupling

Speed of charge

delivery,

effective

frequency

~

board-level package-level chip-level

Amount of

charge, size

of decoupling

capacitance

C. Schuster, TUHH – 77

More Decoupling P

DN

Im

pedance

Target

Impedance

Inductance

of

VRM

Capacitance

of Bulk

Decaps

ESL of

Decaps, Pads

and Vias

Capacitance of

P/G Planes &

Small Decaps

ESL of Planes

and Inductance

of Package

Remaining

On.Chip

Inductance

500 MHz 10 GHz 1 GHz 1 MHz

Capacitance of

Decaps on

Package and IC

~

board-level package-level chip-level

C. Schuster, TUHH – 78

...),2,1,0,(22

22

rr

0

nm

b

n

a

mcfmn

Resonance frequencies of power/ground plane pairs:

Examples of standing wave patterns on a rectangular power/ground plane pair.

Power/Ground Plane Resoances

C. Schuster, TUHH – 79

(6)

Wrapping Up

C. Schuster, TUHH – 80

Comprehenisve EMC of Digital Systems

The basic goals of SI, PI, and EMI control for a digital system are

complementary to each other.

SIGNAL INTEGRITY: insure

acceptable quality of signals within

POWER INTEGRITY: insure

acceptable quality of power

delivery within

EMI: insure acceptable level of

interference with the outside

EMI

Frequency

Target

System

Frequency

PDN

Impedance

Target

System

SNR

Frequency

Target System