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  7. (Spectral; Fall 23) 29 - A quick comment about interlacing and chromatic numbers

(Spectral; Fall 23) 29 - A quick comment about interlacing and chromatic numbers

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Course site: https://www.stevebutler.org/spectral2023 Presenter: https://www.stevebutler.org/ In our last lecture we mention some interlacing results as well as talk about chromatic numbers.
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0:01
I do want to mention one thing that we haven't talked about, which is interlacing, because
0:07
if I don't say it, I feel like I will have done a disservice to the field.
0:16
We're not going to go through and do proofs.
0:20
Most of them rely on Rayleigh-Ritz type arguments and mins of maxes and all these weird things.
0:31
So we'll skip that and just sort of state some results and we'll try to do an application.
0:37
And I hope we'll succeed in the application.
0:40
But what's the idea of interlacing?
0:42
Well, the idea is we have a graph G of some sort.
0:48
Here's our graph G. And then we do something to it.
0:52
So maybe we just take a little piece of it out.
0:57
There's this vertex that used to be here,
1:00
and we've deleted it as an example of something
1:03
that we could do.
1:04
So we might have G minus a vertex.
1:08
x. Or maybe we could talk about g minus just a single edge. Now, once you do something
1:16
like this, you've changed your graph. And if you change your graph, you may, and usually
1:24
do, change your eigenvalues. And so there's the question, how are these related? Because
1:32
So, intuition says small changes should lead to small changes.
1:41
You know, it's kind of like calculus, right?
1:46
Make a small change, you're not going to go wildly different
1:48
unless you have some sort of discontinuity.
1:51
And so the question is, well, does that apply here?
1:55
And the answer is yes, and that's what interlacing is about.
1:59
And there's different matrices and different matrices have different properties.
2:04
And so let's talk about some of our favorites.
2:08
And so we'll start with the adjacency matrix.
2:15
And for the adjacency matrix, we'll compare our graph G, which will have eigenvalues lambda
2:26
1 up to lambda n.
2:28
and I should actually put these in order. So lambda 1 less than or equal to all the way up to lambda n.
2:34
And then we'll compare it with g minus a vertex v.
2:39
So this is muon all the way up to mu and minus 1.
2:46
And what happens? Well, if you think about the actual matrices of these,
2:52
How does the adjacency matrix for our graph G
2:57
relate to the adjacency matrix for G minus V?
3:08
So size-wise it's smaller.
3:09
What else happens though?
3:12
So you have your adjacency matrix for G, and you have
3:16
the vertex V is indexing a row and a column.
3:20
What do you do? Yeah, you delete this row
3:26
So, delete that column, and then life is good.
3:31
And so in particular, what happens is we end up with a principal sub matrix.
3:38
Now, this is because the adjacency matrix doesn't have to worry about degrees.
3:44
Most of our other matrices do.
3:47
And so, because you have this very nice principal sub matrix,
3:51
you get the following very nice result which says,
3:56
hey, your eigenvalues are going to interlace.
4:00
So lambda 1 less than or equal to mu 1 less than or equal to lambda 2 less than or equal
4:06
to mu 2 and so forth all the way down till you get to the end and mu n minus 1 is less
4:15
than or equal to lambda n.
4:18
All right.
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