And so to first order you know that model is that you know delay is the length.

Right? So, a shorter wire is a faster wire and a

longer wire is a slower wire. And you that's fine in terms of being

qualitatively okay. So, for example I can do something like

the bounding box is you know delta x plus delta y just like the placer.

you know we could use something like that we'd have some formula based on the

length of the bounding box. It's you know its its qualitiatvely okay

its not accurate it is in fact extremely crude.

The second source of delay is that we have to deal with the fact that delay is

effected by the electrical circuit drive limitation.

So, so that says look. What's really happening is not just the

length but the electrical loading on the wires.

So the, the delay is proportional to the length of the wire, the fan out of the

wire, the capacitance of the you know, the driven pins.

You know, a lot of, a lot of electrical stuff.

So for example, we would say look the delay is related to the fact that the

fanout is two, we have to account for the loading due to the two pins.

The delay is some kind of a function, it's a function of the bounding box.

The function of the size of the driver gate, the fan outs, and electrical

characteristics of the pins and so on. You know, this is qualitatively better,

and it's not that hard to curve fit some models for this data.

But it still just focuses on the pins really.

and it's not really focusing on the wire per say and it, it can still be really

off by, by a lot. Then ultimately you're forced to, to, to

admit that the delay comes from the electrical loading of the interconnect.

It depends critically on the exact geometry of the wired net.

I mean, I, I need to know the shape of the wire in order to figure this out.

And so, the real honest electrical model for one of these things is an electrical

circuit. You know, you have to model these things

as a circuit and you have to analyze them as a circuit.

And so the question is how do you analyze something like this as a circuit?

So, I mean, if we look at the simplest possible case where I'm, I'm routing

things in the first level of metal, you know there's a metal, a metal wire.

It's separated from the silicon surface itself by some stuff which we can just

treat as some sort of an insulating kind of layer.

you know, how am I actually going to model this thing as a circuit.

Now, you know, one of the first questions is, why do I have to model this as a

circuit? And the real answer is just that the

nanoscale will, you know, your transistors are measured in hundreds of

atoms across. The interconnect geometry is large

relative to the devices themselves and so it presents a significant amount of, sort

of, you know, electrical stuff that you just, you just can't ignore.

[NOISE] So, the most popular interconnect model that we're going to talk about are

things called RC Trees, R for resistor, C for capacitor.

So we're going to talk a little bit of circuits here.

but we're not going to do anything in any detail, an hopefully, you know, people

have seen this much circuit in some, in some basic high school.

Or maybe introductory college physics. Right, so here's my wire again.

And now I'm, I'm, I'm putting some dimension on it.

So you know the metal wire is L units long, it's H units high, it's a W units

wide. And it's sitting on top of an insulator

of height D. And that's sitting on top of the silicon

surface. So the first thing, in order to take this

hunk of metal. It just a great big purple metal bar, as

I've drawn it. Is to acknowledge that the metal has a

resistance to current flowing down its length.

So if you, you take some current, and you know you put it in one end, and it goes

through the wire. It comes out the other end, there's a

resistance, right? So that's what that zigzag line is.

Right, and in physics, we can write a formula for that resistance.

So that resistor value is rho, which is a material constant, times the length of

the wire divided by the width times the height.

And so the way you think about that is, how do you make a resistor bigger?

And the answer is, you make the wire longer, L is bigger.

How do you make a resistor smaller? And the answer is, you make the

cross-sectional area bigger, so there's sort of you know, more places for the

electrons to go through. Now, in an ASIC, I don't really get to

control all those parameters. Right?

I can control the length of the wire. And I can actually control the width of

the wire. But I can't control the height of the

wire. That's, that's the manufacturing process.

So we're not going to use a row. We're going to use just a little lower

case r, for our formula. So, the resistance R, is lower case r

times the length divided by W because I can control the length and I can control

the W. So I can model the resistance of this

wire to current flow. The other thing that this wire has, which

is maybe a little surprising, is that it has capacitance to the silicone

substrate. So you remember what a capacitor is?

A capacitor is just two conducting plates, separated by something that's not

conducting. And the thing that's interesting in this

case is that the thing that's conducting is the metal.

And the other thing that's conducting is the silicon surface and there's an

insulator between them which kind of prevents them from connecting to each

other. So you're going to remember what a

capacitor is just a metal plate or its a conducting plate separated by another

conducting plate from an insulator so in this case the metal is one of the plates

of the capacitor. The silicon is the other plate of the

capacitor, and the insulator is the, just the, the dielectric material that's in

between that's preventing them from connecting to each other.

So again, there's a physics formula. The capacitance is epsilon, which is some

material parameter stuff times the, basically the plate area of the

capacitor, which in this case is W times L.

Divided by the separation between the things where the conductors are, the

things where the charge goes, which in this case is d, the height of the

insulator. And again, I can't control all of this

stuff. So, for us, for the asic the formula that

we are interested in is that the capacitance is c, a smaller case

parameter c, multiplied by basically the footprint of the wire, the width times

the length. Because we can control the width and we

can control the length. Now I have to tell you this.

that model is incredibly simplistic. It's good enough for us to make some

progress. but it's incredibly simplistic.

So in a real capacitance. Or you know people just call this cap

very frequently. You get a capacitance between any pairs

of conducting surfaces. So in a multi layer metal process you get

caps between all the layers. So I've got a little diagram here.

It's three metal wires wide. It's kind of a cross section looking into

metal wires running out of the slide. Three blue metal wires on metal three.

Then on top of them, three blue metal wires on metal four.

And then on top of that two but not three pink metal wires in metal five.

left to right three boxes on the bottom layer, three boxes on the middle layer; a

left box and middle box, but no right box.

And what I'm showing you is between every pair of surfaces of conducting surfaces,

there's a capacitor. So, up on the third row of conductors.

There is a capacitor between the side of one metal five wire, and the side of

another metal five wire. Those are fringe capacitors between two

adjacent wires on the same layer. There are and I'm showing this sort of

the right wires in row one and row two. there are overlap capacitances between

wires on Adjacent layers. What we're basically talking about in our

derivation are overlap capacitances between a wire and whatever's below it.

there are sidewall fringe capacitances in which between the side of one wire and

the top of another wire, if there's not another wire in the way.

this stuff is incredibly complicated, you need real live computational

electromagnetics to do this stuff. And depending on how accurately you want

it there are really good approximations for how you do this.

When you look a realistic process, you typically get numbers that just involve,

some, some parameters and, you know? How long is the wire and, you know, how

much do things overlap? And, you know?

You can calculate first order numbers that are, that are very helpful.

And if you need really really accurate numbers, you have to go off and do some

more sophisticated computational stuff. We're not going to touch any of this

stuff. I'm just going to use the lower case r

and the lower case c that I showed you on the previous slide.

Now, the Interconnect model that is the most famous and the most useful and the

most practical is something called a Pi model.

And it's called a Pi model, because the circuit we're about to build looks like a

Pi, the Greek letter Pi. And so, it accounts for the resistance of

this wire and the capacitance. Now, so, the first thing to think of is

that the current goes in one end of the metal.

And the current comes out the other end of the metal.

And I'm drawing those two big circles, because those are nodes.

Those are electrical nodes. And those are going to get, going to,

going to appear when I draw this as a circuit.

And so when I draw this as a circuit. What happens is, I get a resistance

between those two nodes, right? Because there's a resistance to the

current going in one of those circles, and coming out the other.

But I also get capacitance, right? And where the capacitance goes.

Right depending whether you are seeing this signal before.

The capacitance in the model I am showing you goes to ground.

Right and so we see people drawing that with, with a solid triangle, we see

people drawing that with a an open triangle.

And I'm not drawing it in my slides, but sometimes you see people drawing it with

three little lines that get narrower like a point.

And so this is a Pi model and one resistor and two capacitors.

So the resistor is lowercase R times L divided by W, length divided by width.

The capacitor value is C times W times L and I put half the capacitor on the left

and half the capicator on the right. Because one of the things its very

convenient is to make this model symmetric.

So I split the capacitor with half of it on the left and half of it on the right

this is a wonderful small model and I only need two numbers.

Right, I need the R number and I need the C number, and I can fully paramiterize

this little Circut model. But this is just one piece of metal.

And the big idea is i replace every straight wire segment in my wire with a

Pi model. All right, so, I've got a whole bunch of

pieces of wire. One, two, three, four, five in this

particular case. and I'm going to take every single one of

those wire segments every single one of those straight line segments and replace

it with one resistor and two capacitors. And if you're saying to yourself, wow if

I have a great big wire that has a lot of bends and kinks and stuff like that

there's a whole lot of resistors and a whole lot of capacitors.

And the answer is, yes it's just the way it works.

And one of the things I am not doing in the wires that I am showing you, is I'm

not showing you any VLs. VLs typically actually just get modeled

as a resistor. Okay.

So that's actually pretty easy to deal with.

and so every straight line segment becomes a Pi model but the other seems to

be a little bit of complexity here right. And one of the things to be aware of in

that this that, that, that thing is just that node right there.

Okay. And so I've got one, two, three, four,

five wire segments. I've got one, two, three, four, five Pi

models with a resistor and three capacitors.

There's three wire segments coming together at that point there.

And the thing to be really, you know, very clearly aware of, is that those

nodes are all electrically connected. So I'm going to draw a circle here.

I'm going to draw a circle here. I'm going to draw a circle here.

And I'm just saying look, all those capacitors are actually connected at the

same node. So, I'm even just going to draw little

dotted lines to sort of highlight that. and this is sort of awkward, and it would

be nice if there was a little bit of a circuit kind of a trick we could do,

because this is looking just a little bit complicated.

So I'll just remind you that there's a nice simplification rule from basic

circuits or physics, wherever you learned it.

Parallel capacitors can be replaced by one bigger[COUGH] capacitor.

And you just add the capacitor numbers together.

So in that place where those three capacitors were all connected, you add

the capacitor numbers together. So literally, any place multiple ends of

a wire segment come together in one of these connected Pi models.

You just add the capacitors together and the resistors just connect.

Right? So, in this particular case, when I was

at that, sort of, junction in the wire, and I had three capacitors, right?

What actually happened, was that they all got replaced by one value of capacitor.

An we get something, that actually looks kind of simple, you know, not so

tremendously complicated. This is something called an RC tree.

So why is it called an RC tree? It's called an RC tree because it's a

tree of resistors. You look at that object and you say, oh,

that's a tree. It's got a, it's got a root and it's got

leaves. And when I walk down the links on the

tree, what I'm walking over is the resistors and it's got capacitors hanging

off of it. So this is a really famous object.

And one of the reasons it's famous is because it's simple to analyze.

And turns out I don't even need to analyze it like like a, like a circuit to

be able to extract some value from it. So let's go do that next.

[SOUND]