A Basic Analysis of Interwire Capacitance in Ultra Micron Technologies

5
6/ 14/2016 A Basic Analy sis of Interwire Ca pacit ance in Ul tra Mi cr on T echnolo gie s ht tp: //www.desig n- reus e.com/ art icle s/33101/ in terwire- capaci t ance -a nalysis-i n- u lt ra -micr on-t echnolo gie s.html 1/ 5  design-reuse.cn  |  dr-embedded.com  |  Login  |  Subscr ibe to D&R SoC News Alert Trisha Ghosh, Rishabh Agarwal, Vishant Gotra (Freescale) ABSTRACT As the technology node decreases, meeting inter-wire or coupling capacitance becomes extremely critical and challenging in SOC design. Shrinking technology node leads to increase in di electric values, thus leading to higher capacitance and hence an incre ase in inaccuracies and power. In this paper, we propose effective ways to reduce interconnect capacitance in ultra micron technologies. INTRODUCTION As the technology node decreases, the challenges for the layout designer also increase. Shrinking technology node leads to an increase in dielectri c values, which leads to an increase in capacitance. Transistors can be scaled down in size such that the device delay decreases in direct proportion to the device dimensions. But the ca se is not the same with interconnects. For submicron-geometry chips, it is the interconnect delays, rather than the device delays that determine c hip pe rformance. If the interconnects are scaled down, it results in RC delays that begin to dominate the chip performance. In this article we disc uss the different types of capacitances encountered in ultra micron technology between interconnects. We also describe in detail the shielding of analog routes with the effect of capacitance and a few ways to reduce the capacitance. We also provide an idea concerning metal layer usage topology in accordance based on need and the application. BASIC FORMULA TO CALCULATE PARALLEL PLATE CAPACITANCE FIG1. Parallel Plate Capacitor In sub-micron technologies (greater than 90nm), only area capacitance is taken into calculation and we ignore coupling and fringe capacitance, but in deep sub-micron technologies (less than 65nm) 2D-3D fringe, coupling and area capacitance is also included. WHY CAPACITANCE INCREASES WITH DECREASING TECHNOLOGY NODE SiO2 has been the preferred gate insulator for silicon MOSFET since the 1960’s. Over the years, the oxide thickness has been reduced from 300nm for 10µm technology to 1.2nm for 65nm technology. There are two reasons for the relentless drive to reduce the oxide thickness. 1. A thinner oxide, i.e. a larger Cox raises I-on. A large I-on is desirable Enter Keywords....  SEARCH SILICON IP 16,000 IP Cores from 450 Vendors  RELA TED ARTICLES Method for Library Analysis Automation Analysis of RDC Paths for a million gate SoC SoC clock monitoring issues: Scenarios and root cause analysis An innovative methodology to reduce routing capacitance of ADC channels Efficient analysis of CDC violations in a mi llion gate SoC, part 2  See Freescale Semiconductor Latest Articles >> NEW ARTICLES Fronthaul Evolution Toward 5G: Standards and Proof of Concepts Thorough validation: the conundrum of Pulsed latch libraries turned practical as Spinner systems Lossless Medical Video Compression Using HEVC Neural Networks and the Rings of Power Methodology to lower supply voltage of standard cell libraries  See New Articles >> MOST POPULAR 1. Dynamic Memory Allocation and Fragmentation in C and C++ 2. Fronthaul Evolution Toward 5G: Standards and Proof of Concepts 3. How to calculate CPU utilization 4. Mixed-Signal IP Design Challenges in 28 nm and Beyond 5. Using SystemVerilog Assertions in RTL A Basic Analysis of Interwire Capac itance in Ultra Micron Technologies  Search Industry Articles  SEARCH IP NEWS INDUSTRY ARTICLES BLOGS VIDEOS SLIDES EVENTS

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Trisha Ghosh, Rishabh Agarwal, Vishant Gotra (Freescale)

ABSTRACT

As the technology node decreases, meeting inter-wire or coupling

capacitance becomes extremely critical and challenging in SOC design.

Shrinking technology node leads to increase in dielectric values, thus

leading to higher capacitance and hence an increase in inaccuracies  and

power. In this paper, we propose effective ways to reduce interconnect

capacitance in ultra micron technologies.

INTRODUCTION

As the technology node decreases, the challenges for the layout designer

also increase. Shrinking technology node leads to an increase in dielectric

values, which leads to an increase in capacitance. Transistors can be

scaled down in size such that the device delay decreases in direct

proportion to the device dimensions. But the case is not the same with

interconnects. For submicron-geometry chips, it is the interconnect delays,

rather than the device delays that determine c hip  performance. If the

interconnects are scaled down, it results in RC delays that begin to

dominate the chip performance.

In this article we discuss the different types of capacitances encountered in

ultra micron technology between interconnects. We also describe in detail

the shielding of analog routes with the effect of capacitance and a few

ways to reduce the capacitance. We also provide an idea concerning metal

layer usage topology in accordance based on need and the application.

BASIC FORMULA TO CALCULATE PARALLEL PLATE CAPACITANCE

FIG1. Parallel Plate Capacitor 

In sub-micron technologies (greater than 90nm), only area capacitance is

taken into calculation and we ignore coupling and fringe capacitance, but in

deep sub-micron technologies (less than 65nm) 2D-3D fringe, coupling and

area capacitance is also included.

WHY CAPACITANCE INCREASES WITH DECREASING TECHNOLOGY

NODE

SiO2 has been the preferred gate insulator for silicon MOSFET since the

1960’s. Over the years, the oxide thickness has been reduced from 300nm

for 10µm technology to 1.2nm for 65nm technology.

There are two reasons for the relentless drive to reduce the oxide

thickness.

1. A thinner oxide, i.e. a larger Cox raises I-on. A large I-on is desirable

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Analysis of RDC Paths for a million gateSoC

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See Freescale Semiconductor Latest Articles >>

NEW ARTICLES

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MOST POPULAR

1. Dynamic Memory Allocation andFragmentation in C and C++

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A Basic Analysis of Interwire Capacitance in Ultra Micron Technologies

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for maximizing the circuit speed.

2. To control Vt roll-off (and therefore the sub-threshold leakage)

FIG2. Decreasing Trend in Oxide Thickness with Decreasing Technology 

EFFECTS OF INCREASING CAPACITANCE

1. INCREASE IN POWER – Increase in capacitance leads to increase in

RC, and hence increase in chip power.

2. INCREASED CROSSTALK BETWEEN ANALOG SIGNALS – As the

capacitance of a given signal shoots its required specifications, itsaccuracy also increases.

3. DIE AREA IMPACT – In order to meet capacitance specifications, the

signals need to be spaced as far as possible. This requirement can

lead to an increase in die area.

TYPES OF CAPACITANCE FORMED BETWEEN INTERCONNECTS

1. SELF CAPACITANCE (Metal to Substrate capacitance)

The simplest structure examined here is an isolated metal line over the

silicon substrate. The capacitance formed between the substrate and any

metal layer above is called self or area capacitance. Thus this capacitance

is always formed. The value of this capacitance is dependent on two

factors, length and metal layer used. Metal-oxide-silicon capacitance has

slightly different characteristics than metal-oxide-metal. Small changes in

capacitance can result due to inversion in the field regions or other

substrate effects. This is an inherent advantage of measurement in the

case of metal-to-substrate capacitances.

2. Mutual Coupling Capacitance  (INTERWIRE CAPACITANCES)

Capacitance between metal lines of the same layer is referred to as inter-

wire or coupling capacitance. This is a major problem in deep submicron

technologies due to tighter pitch and higher metal aspect ratios. An

undesired voltage spike resulting from this capacitive coupling is

commonly referred to as crosstalk. The presence of another nearby line

will increase the total capacitance of the isolated line. This added

capacitance must be taken into account when routing global signals such as

clocks, determining driver sizes and line widths/spacing etc.

3. Fringe Capacitance

Fringe capacitance is formed between non-overlapping sidewall of one

conductor and surface/sidewall of a second conductor on the same ordifferent layer from the first one. This type of capacitance becomes

significant as we route in higher layers because higher layers are thicker.

For higher metal layers, inter-wire effects are more pronounced due to

increased metal heights and lessened substrate effects. Since most signals

are routed on lower levels, crosstalk is less critical in higher layers

normally carrying power and ground. But sometimes while routing analog

nets, signals having special requirements (like less resistance, crosstalk)

need to be routed in higher metal layers. The method used to shield the

special signal routes is to cover the upper and lower area of the signal

route by other grounded metal planes. Although, this affects coupling

capacitance, it helps in reducing any crosstalk with any other signal route.

The grounded metal plane attracts all the disturbances in the form of 

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electric fields which could have hampered the original signal originally.

This is a trade-off between total capacitance and noise imputation.

FIG3.Types Of Interconnect Capacitances

WAYS OF SHIELDING INTERCONNECTS

The methodology used presently for shielding is that shield wires are tied

statically to Vdd or ground. In this article, we explain the concept of 

coupling capacitance in terms of aggressor and victim. Many cases are

explained here which will help in deeply analyzing the change in

capacitance as the setup is changed. Each type of setup described below

has its own benefits in term of reduction of crosstalk and coupling

capacitance, but at the same time it can seriously affect metal availability

for routing.

SETUP 1: When there is only one net drawn in layer n

As can be seen from the figure, the signal route is in the design in layer n.

The capacitance value obtained for this route is because of the self area

capacitance (metal-to-substrate capacitance). There is no other route in

any other metal layer so there is no coupling and no fringe capacitance

present. As stated earlier, eliminating this type of capacitance is difficult.

This setup is most prone to noise and crosstalk, so sensitive signals are

always shielded.

Ctotal = Cself 

SETUP 2: When lateral shielding is performed in the design

As seen from the figure, there is a sensitive route in layer n which is

shielded from both sides in the same metal layer n. In this type of setup,

self area capacitance, fringe and coupling capacitance come into action.

The self area capacitance is due to the formation of capacitance between

the route and substrate. The coupling capacitance is due to the shields

placed in the same metal layer n. Distance is indirectly proportional to the

capacitance, so as the distance between signal and shield wires increases,

coupling capacitance decreases. However, this phenomenon vanishes after

a fixed distance between the sensitive routes and shields, thus there is no

further decrease in the coupling capacitance even after increasing the

spacing between shield line and signal wire. In this setup the susceptiblenet is shielded in the same metal on both the sides eliminating any noise

from the adjacent signal toggling in the same metal layer. This is shown in

the graph below.

Ctotal=Cself+Ccoupling (side metal) +Cfringe (side metal)

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FIG4.Axial/Lateral Shielding

SETUP 3: When tub shielding is performed in the design

In this setup, the sensitive route is shielded from the sides as well as from

the bottom, which eliminates any noise from the sides and bottom layer. In

the figure, the sensitive route in layer n is shielded from both the sides in

the same metal in layer n as well as from the adjacent lower layer n-1.

All types of capacitance exist in this setup. The capacitance value is more

than that for setup 2 because the coupling and fringe capacitance from the

layer below is also added to the calculation. In this setup, we determined

by experiment that the effect of coupling is significant up to two layersbelow or above the sensitive metal layer.

CCtotal=Cself + Coupling (side-metal) + Cfringe (side-metal) +

Coupling (lower-metal) + Cfringe (lower metal)

FIG5.Tub Shielding

SETUP 4: When coaxial shielding is performed in the design

In this, sensitive signal is routed like tub shielding setup in addition to an

adjacent layer above it layer n+1. This setup helps in completely isolating

the sensitive route from any noise or crosstalk.

But as more layers are used for shielding, there can be a problem of 

routing resource availability.

Figure below shows this setup.

SETUP 5: When tub shielding is performed only on the shields

There is another case where besides axial shielding being performed in

layer n, the shield wires are covered only with layer n-1 at the bottom. In

this case the signal route is not tub shielded. Thus, the area capacitance

nullified between signal in layer n and shield below in layer n -1. But a

serious disadvantage of this method is that the signal remains exposed at

the bottom to any noisy signal in layer n-1.

The table below shows the value of total capacitance in all the setups

explained above.

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Setup Shield in layer n-1 Shield in layer n Shield in Layer n+1 Total

Capacitance (fF)

Setup  Shield in layer

n-1

Shield in

layer n

Shield in Layer

n+1

Total Capacitance

(fF)

1 No No No 251.5

2 No Yes No 427.3

3 Yes Yes No 620.2

4 Yes Yes Yes 887.6

5 Yes Yes No 514.7

CONCLUSION

There is always some tradeoff involved in choosing between shielding and

meeting capacitance specifications for analog routes. If we try to shield the

signal well, we end up increasing capacitance and also eat up routing

resources. If we start increasing spacing between signals in order to

improve capacitance, we might blow up the die size. The designer thus has

to weigh all situations and combinations before making a decision.

REFERENCES

1. http://www-inst.eecs.berkeley.edu/

2.

http://www.eecs.berkeley.edu/~hu/PUBLICATIONS/Hu_papers/Hu_Melvyl/Hu_Melvyl_97_03.pdf 

 

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