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3/1/2015 1 Ma/CS 6b Class 23: Eigenvalues in Regular Graphs By Adam Sheffer Recall: The Spectrum of a Graph Consider a graph = , and let be the adjacency matrix of . The eigenvalues of are the eigenvalues of . The characteristic polynomial ; is the characteristic polynomial of . The spectrum of is = 1 ,…, 1 ,…, , where 1 ,…, are the eigenvalues of and is the multiplicity of .
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Page 1: Ma/CS 6b - California Institute of Technology2014-15/2term/ma006b/23 spectral 3.pdf · 3/1/2015 1 Ma/CS 6b Class 23: Eigenvalues in Regular Graphs By Adam Sheffer Recall: The Spectrum

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Ma/CS 6b Class 23: Eigenvalues in Regular Graphs

By Adam Sheffer

Recall: The Spectrum of a Graph

Consider a graph 𝐺 = 𝑉, 𝐸 and let 𝐴 be the adjacency matrix of 𝐺.

◦ The eigenvalues of 𝐺 are the eigenvalues of 𝐴.

◦ The characteristic polynomial 𝜙 𝐺; 𝜆 is the characteristic polynomial of 𝐴.

◦ The spectrum of 𝐺 is

𝑠𝑝𝑒𝑐 𝐺 =𝜆1, … , 𝜆𝑡𝑚1, … ,𝑚𝑡

,

where 𝜆1, … , 𝜆𝑡 are the eigenvalues of 𝐴 and 𝑚𝑖 is the multiplicity of 𝜆𝑖.

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Example: Spectrum

𝐴 =

0 1 0 11 0 1 001100 11 0

det 𝜆𝐼 − 𝐴 = det

𝜆 −1 0 −1−1 𝜆 −1 00−1−10𝜆 −1−1 𝜆

= 𝜆2 𝜆 − 2 𝜆 + 2 .

𝑠𝑝𝑒𝑐 𝐶4 =0 2 −22 1 1

𝑣1 𝑣2

𝑣3 𝑣4

Slight Change of Notation

Instead of multiplicities, let 𝜆1, … , 𝜆𝑛 be the not necessarily distinct eigenvalues of 𝑛.

For example, if the spectrum is 2 −12 2

,

we write 𝜆1 = 𝜆2 = 2 and 𝜆3 = 𝜆4 = −1 (instead of 𝜆1 = 2, 𝑚1 = 2, 𝜆2 = −1,𝑚2= 2).

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Recall: The Spectral Theorem

Theorem. Any real symmetric 𝑛 × 𝑛 matrix has real eigenvalues and 𝑛 orthonormal eigenvectors.

◦ By definition, any adjacency matrix 𝐴 is symmetric and real.

◦ The algebraic and geometric multiplicities are the same in this case.

◦ We have 𝜙 𝐴; 𝜆 = 𝜆 − 𝜆𝑖𝑛𝑖=1 .

◦ The multiplicity of an eigenvalue 𝜆 is 𝑛 − 𝑟𝑎𝑛𝑘 𝜆𝐼 − 𝐴 .

More Examples

We already derived the following:

◦ 𝑠𝑝𝑒𝑐 𝐾𝑛 =−1 𝑛 − 1𝑛 − 1 1

◦ 𝑠𝑝𝑒𝑐 𝐾𝑛,𝑚 =0 𝑚𝑛 − 𝑚𝑛

𝑚 + 𝑛 − 2 1 1

Our next goal is to study regular graphs.

◦ Can you come up with an eigenvector of any regular graph with 𝑛 vertices?

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Eigenvalues of Regular graphs

If 𝐴 is the adjacency matrix of a 𝑑-regular graph, then any row of 𝐴 contains exactly 𝑑 1’s.

◦ Thus, the vector 1𝑛 = 1,1,… , 1 is an eigenvector of 𝐴 with eigenvalue 𝑑.

Theorem. Let 𝐺 be a connected graph. The eigenvalue of 𝐺 of largest absolute value is the maximum degree if and only if 𝐺 is regular.

Proof

𝐴 – 𝑛 × 𝑛 adjacency matrix of a graph 𝐺.

Δ 𝐺 – the maximum degree of 𝐺.

𝑥 = 𝑥1, … , 𝑥𝑛 – eigenvector of eigenvalue 𝜆 of largest absolute value.

𝑥𝑗 = max𝑖|𝑥𝑖| .

𝜆 𝑥𝑗 = 𝐴𝑥 𝑗 = 𝑥𝑖𝑣𝑖∈𝑁 𝑣𝑗

≤ deg 𝑣𝑗 𝑥𝑗 ≤ Δ 𝐺 𝑥𝑗 ,

So 𝜆 ≤ Δ 𝐺 .

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Δ 𝐺 – the maximum degree of 𝐺.

We proved that the absolute value of any eigenvalue of 𝐴 is at most Δ 𝐺 , using

𝜆 𝑥𝑗 = 𝐴𝑥 𝑗 = 𝑥𝑖𝑣𝑖∈𝑁 𝑣𝑗

≤ deg 𝑣𝑗 𝑥𝑗 ≤ Δ 𝐺 𝑥𝑗 .

For equality to hold, we need

◦ deg 𝑣𝑗 = Δ 𝐺 .

◦ 𝑥𝑖 = 𝑥𝑗 for each 𝑣𝑖 ∈ 𝑁 𝑣𝑗 .

That is, 𝑣𝑗 and all of its neighbors are of degree

Δ 𝐺 . Repeating the same argument for a neighbor 𝑣𝑖 implies that 𝑣𝑖’s neighbors are also of degree Δ 𝐺 . We continue to repeat the argument to obtain that the graph is regular.

Multiplicity

The previous proof also shows that any eigenvector 𝑥1, … , 𝑥𝑛 of the eigenvalue 𝑑 satisfies 𝑥1 = 𝑥2 = ⋯ = 𝑥𝑛.

Thus, the space of eigenvectors of the eigenvalue 𝑑 is of dimension 1 (that is, 𝑑 has multiplicity 1).

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The Spectrum of the Petersen Graph The Petersen graph 𝐺 = 𝑉, 𝐸 is a 3-

regular graph with 10 vertices.

◦ We know that it has eigenvalue 3 with eigenvector 110.

To find the other eigenvalues, we notice some useful properties:

◦ If 𝑢, 𝑣 ∈ 𝐸 then 𝑢 and 𝑣 have no common neighbors.

◦ If 𝑢, 𝑣 ∉ 𝐸 then 𝑢 and 𝑣 have exactly one common neighbor.

The Adjacency Matrix

The number of neighbors shared by 𝑣𝑖 and 𝑣𝑗 is 𝐴2 𝑖𝑗 . That is

𝐴2 𝑖𝑗 =

3, if 𝑖 = 𝑗,

0, if 𝑖 ≠ 𝑗 and 𝑣𝑖, 𝑣𝑗 ∈ 𝐸,

1, if 𝑖 ≠ 𝑗 and 𝑣𝑖, 𝑣𝑗 ∉ 𝐸.

That is, 𝐴2 + 𝐴 − 2𝐼 = 1𝑛×𝑛.

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The Additional Eigenvalues

We have 𝐴2 + 𝐴 − 2𝐼 = 1𝑛×𝑛.

Since 3 is an eigenvalue with eigenvector 1𝑛, the other eigenvectors are orthogonal to 1𝑛.

Thus, for an eigenvector 𝑣 of eigenvalue 𝜆 ≠ 3: 1𝑛×𝑛𝑣 = 0𝑛.

That is, 𝐴2 + 𝐴 − 2𝐼 𝑣 = 0𝑛.

If 𝑣 is an eigenvector of 𝜆 then we have 𝜆2𝑣 + 𝜆𝑣 − 2𝑣 = 0𝑛.

Thus, the additional eigenvalues of 𝐴 are 1,−2.

𝑠𝑝𝑒𝑐 𝐺 =3 1 −21 𝑚2 𝑚3

.

The Multiplicities

𝑠𝑝𝑒𝑐 𝐺 =3 1 −21 𝑚2 𝑚3

.

Recall that 𝜆𝑖10𝑖=1 = 𝑡𝑟𝑎𝑐𝑒 𝐴 = 0.

That is, 3 +𝑚2 − 2𝑚3 = 0.

Combining this with 𝑚2 +𝑚3 = 9 and 𝑚2, 𝑚3 ≥ 0, we obtain the unique solution 𝑚2 = 5,𝑚3 = 4.

𝑠𝑝𝑒𝑐 𝐺 =3 1 −21 5 4

.

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Petersen Graph and 𝐾10

Problem. Can we partition the edges of 𝐾10 into three disjoint sets, such that each set forms a Petersen graph?

◦ 𝐾10 has 102= 45 edges, and the Petersen

graph has 15.

◦ In 𝐾10 every vertex is of degree 9, and in the Petersen graph 3.

Disproof

Assume, for contradiction, that the partition exists, and let 𝐴, 𝐵, 𝐶 be the adjacency matrices of the three copies of the Petersen graph.

The adjacency matrix of 𝐾10 is 110×10 − 𝐼.

That is, 𝐴 + 𝐵 + 𝐶 = 110×10 − 𝐼.

𝑉𝐴, 𝑉𝐵 – the vector subspaces of eigenvectors corresponding to the eigenvalue 1 in 𝐴 and 𝐵.

We know that dim𝑉𝐴 = dim𝑉𝐵 = 5.

Since both 𝑉𝐴 and 𝑉𝐵 are orthogonal to 110, they are not disjoint (otherwise we would have a set of 11 orthogonal vectors in ℝ10).

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Disproof (cont.) 𝐴, 𝐵, 𝐶 – the adjacency matrices of the three

copies of the Petersen graph in 𝐾10.

𝐴 + 𝐵 + 𝐶 = 1𝑛×𝑛 − 𝐼.

𝑉𝐴, 𝑉𝐵 – the vector subspaces of eigenvectors corresponding to the eigenvalue 1 in 𝐴 and 𝐵.

𝑉𝐴 and 𝑉𝐵 are not disjoint.

Let 𝑧 ∈ 𝑉𝐴 ∩ 𝑉𝐵. Since every vector in 𝑉𝐴 and 𝑉𝐵 is orthogonal to 1𝑛, so is 𝑧.

We have 𝐶𝑧 = 1𝑛×𝑛 − 𝐼 − 𝐴 − 𝐵 𝑧 = 0 − 𝑧 − 𝐴𝑧 − 𝐵𝑧= −3𝑧.

Contradiction since -3 is not an eigenvalue of 𝐶.

Four Things You Did Not Know About The Petersen Graph It has 15 edges and 2000 spanning trees.

It is the smallest 3-regular graph of girth 5 (this is called a 3,5 -cage graph).

It likes gardening, ballet, and building airplane models.

It has gotten divorced three times.

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Moore Graphs

A Moore graph is a graph that is 𝑑-regular, of diameter 𝑘, and whose number of vertices is

1 + 𝑑 𝑑 − 1 𝑖𝑘−1

𝑖=0

.

As can be easily checked, this is the minimum possible number of vertices of any graph of diameter 𝑘 and minimum degree 𝑑.

Examples of Moore Graphs

A Moore graph is a graph that is 𝑑-regular, of diameter 𝑘, and whose number of vertices is

1 + 𝑑 𝑑 − 1 𝑖𝑘−1

𝑖=0

.

What Moore graphs do we know?

◦ The Petersen graph is 3-regular, of diameter

2, and contains 1 + 3 3 − 1 𝑖1𝑖=0 = 10

vertices.

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Examples of Moore Graphs

A Moore graph is a graph that is 𝑑-regular, of diameter 𝑘, and whose number of vertices is

1 + 𝑑 𝑑 − 1 𝑖𝑘−1

𝑖=0

.

The Petersen graph is 3-regular, of diameter 2,

and contains 1 + 3 3 − 1 𝑖1𝑖=0 = 10 vertices.

Is there a Moore graph that is 2-regular and of diameter 2? 𝐶5

Moore Graphs of Diameter 2 and Girth 5 Recall that the girth of a graph is the

length of the shortest cycle in it.

Theorem. There exist 𝑑-regular Moore graphs with diameter 2 and girth 5 only for 𝑑 = 2,3,7, and possibly 57.

◦ The case of 𝑑 = 57 is an open problem.

◦ If it exists, it has 3250 vertices, and 92,625 edges.

The case of 𝑑 = 7

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𝐺 = 𝑉, 𝐸 – a 𝑑-regular graph of diameter 2, girth 5, and with

𝑉 = 1 + 𝑑 𝑑 − 1 𝑖1

𝑖=0

= 1 + 𝑑2.

Since the girth is five, if 𝑣𝑖 , 𝑣𝑗 ∈ 𝐸 then 𝑣𝑖 and

𝑣𝑗 have no common neighbors.

Since the diameter is two, if 𝑣𝑖, 𝑣𝑗 ∉ 𝐸 then 𝑣𝑖

and 𝑣𝑗 have exactly one common neighbor.

Thus, the adjacency matrix 𝐴 satisfies

𝐴2 𝑖𝑗 =

𝑑, if 𝑖 = 𝑗,

0, if 𝑖 ≠ 𝑗 and 𝑣𝑖, 𝑣𝑗 ∈ 𝐸,

1, if 𝑖 ≠ 𝑗 and 𝑣𝑖 , 𝑣𝑗 ∉ 𝐸.

That is, we have 𝐴2 + 𝐴 − 𝑑 − 1 𝐼 = 1𝑛×𝑛.

Proof (cont.)

𝐺 = 𝑉, 𝐸 – a 𝑑-regular graph of diameter 2, girth 5, and with 𝑉 = 1 + 𝑑2.

𝐴2 + 𝐴 − 𝑑 − 1 𝐼 = 1𝑛×𝑛.

𝜆 ≠ 𝑑 – an eigenvalue of 𝐴 with eigenvector 𝑣. Since 𝜆 ≠ 𝑑, 𝑣 is orthogonal to 1𝑛. Thus 𝐴2 + 𝐴 − 𝑑 − 1 𝐼 𝑣 = 0𝑛, or 𝜆2𝑣 + 𝜆𝑣 − 𝑑 − 1 𝑣 = 0.

This implies that 𝜆2 + 𝜆 − 𝑑 + 1 = 0, so

𝜆2,3 = −1 ± 1 + 4 𝑑 − 1

2= −1 ± 4𝑑 − 3

2.

We thus have 𝑠𝑝𝑒𝑐 𝐺 =𝑑 𝜆2 𝜆31 𝑚2 𝑚3

.

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Finding the Multiplicities

We have 𝜆2 = −1+ 4𝑑−3

2, 𝜆3 = −

1− 4𝑑−3

2,

𝑠𝑝𝑒𝑐 𝐺 =𝑑 𝜆2 𝜆31 𝑚2 𝑚3

.

0 = 𝑡𝑟𝑎𝑐𝑒 𝐴 = 𝑑 + 𝜆2𝑚2 + 𝜆3𝑚3

= 𝑑 −𝑚2 +𝑚32+𝑚3 −𝑚22

4𝑑 − 3.

Since 𝑚2 +𝑚3 = 𝑛 − 1 = 𝑑2, we have

𝑑2 − 2𝑑 = 𝑚3 −𝑚2 4𝑑 − 3.

This can happen if either 𝑚2 = 𝑚3 or 4𝑑 − 3 = 𝑠2 for some integer 𝑠.

If 𝑚2 = 𝑚3 than 𝑑2 − 2𝑑 = 0, implying 𝑑 = 2.

The Case of 4𝑑 − 3 = 𝑠2

𝑑2 − 2𝑑 = 𝑚3 −𝑚2 4𝑑 − 3.

Assume that 4𝑑 − 3 = 𝑠2 for some integer 𝑠. That is, 𝑑 = 𝑠2 + 3 /4.

Substituting into the above equation: 𝑠2 + 3 2

16−2𝑠2 + 6

4= 𝑚3 −𝑚2 𝑠.

Setting 𝑚3 −𝑚2 = 2𝑚3 − 𝑑2, we have

𝑠4 + 6𝑠2 + 9 − 8𝑠2 − 24 = 32𝑚3𝑠 − 𝑠5 − 6𝑠3 − 9𝑠.

𝑠5 + 𝑠4 + 6𝑠3 − 2𝑠2 + 9 − 32𝑚3 𝑠 = 15.

So 𝑠 must divide 15, and we get 𝑠 ∈ ± 1,3,5,15 , which implies 𝑑 ∈ 1,3,7,57 .

The case 𝑑 = 1 leads to 𝐾2. Not a Moore graph.

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Recall: Independent Sets

Consider a graph 𝐺 = 𝑉, 𝐸 . An independent set in 𝐺 is a subset 𝑉′ ⊂ 𝑉 such that there is no edge between any two vertices of 𝑉′.

Finding a maximum independent set in a graph is a major problem in theoretical computer science.

◦ No polynomial-time algorithm is known.

Past Bounds

Let 𝐺 = (𝑉, 𝐸) be a graph.

Already proved:

◦ 𝐺 has an independent set of size at least

1

1+ deg 𝑣𝑣∈𝑉

.

◦ If 𝐸 = 𝑉 ⋅𝑑

2, then 𝐺 has an independent

set of size at least 𝑉 /2𝑑.

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An Upper Bound

Theorem. For a 𝑑-regular graph 𝐺 = 𝑉, 𝐸 with smallest (most negative) eigenvalue 𝜆𝑛, the size of the largest

independent set of 𝐺 is at most 𝑛

1−𝑑/𝜆𝑛.

Example.

◦ 𝑠𝑝𝑒𝑐 𝐶4 =0 2 −22 1 1

.

◦ So at most 4

1−2

−2

= 2.

𝑣1 𝑣2

𝑣3 𝑣4

Recall: The Rayleigh Quotient The Rayleigh quotient is 𝑅 𝐴, 𝑥 = 𝑅(𝑥)

=𝑥𝑇𝐴𝑥

𝑥𝑇𝑥 for 𝑛 × 𝑛 matrix 𝐴 and 𝑥 ∈ ℝ𝑛.

Lemma. Let 𝐴 be a real symmetric 𝑛 × 𝑛 matrix. Then 𝑅 𝑥 attains its maximum and minimum at eigenvectors of 𝐴. (We do

not prove the lemma.)

Question. What is 𝑅 𝑥 when 𝑥 is an eigenvector of eigenvalue 𝜆?

◦𝑥𝑇 𝐴𝑥

𝑥𝑇𝑥=𝑥𝑇𝜆𝑥

𝑥𝑇𝑥= 𝜆.

◦ Thus, the min and max values of 𝑅 𝑥 are the min and max eigenvalues of 𝐴.

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𝜆𝑛 – the most negative eigenvalue of 𝐺.

𝑆 – a largest independent set of 𝐺.

1𝑆 = 𝑥1, … , 𝑥𝑛 – a vector with 𝑥𝑖 = 1 if 𝑣𝑖 ∈ 𝑆 (otherwise 𝑥𝑖 = 0).

𝑦 = 𝑛1𝑆 − 1𝑛 ⋅ 𝑆 .

𝑦𝑇𝐴𝑦 = 𝑛2 ⋅ 1𝑆𝑇𝐴1𝑆 − 2 𝑆 𝑛 ⋅ 1𝑆

𝑇𝐴1𝑛 + 𝑆2 ⋅ 1𝑛𝑇𝐴1𝑛.

Since 𝑆 is an independent set, we have

1𝑆𝑇𝐴1𝑆 = 𝐴𝑖𝑗𝑖,𝑗∈S = 0.

Since 𝐺 is 𝑑-regular, 1𝑆𝑇𝐴1𝑛 = 1𝑆

𝑇 ⋅ 𝑑1𝑛 = 𝑑 𝑆 , and also 1𝑛

𝑇𝐴1𝑛 = 1𝑛𝑇 ⋅ 𝑑1𝑛 = 𝑑𝑛.

Combining the above, we have 𝑦𝑇𝐴𝑦 = 0 − 2 𝑆 𝑛 ⋅ 𝑑 𝑆 + 𝑆 2 ⋅ 𝑑𝑛 = − 𝑆 2𝑑𝑛. 𝑦𝑇𝑦 = 𝑛21𝑆

𝑇1𝑆 − 2 𝑆 𝑛1𝑆𝑇1𝑛 + 𝑆

21𝑛𝑇1𝑛

= 𝑛2 𝑆 − 2 𝑆 2𝑛 + 𝑆 2𝑛 = 𝑆 𝑛 𝑛 − 𝑆 .

Completing the Proof

By the lemma, we have 𝑦𝑇𝐴𝑦

𝑦𝑇𝑦≥ 𝜆𝑛.

We have 𝑦𝑇𝐴𝑦 = − 𝑆 2𝑑𝑛. 𝑦𝑇𝑦 = 𝑆 𝑛 𝑛 − 𝑆 .

Thus

𝜆𝑛 ≤− 𝑆 2𝑑𝑛

𝑆 𝑛 𝑛 − 𝑆=−𝑑 𝑆

𝑛 − 𝑆.

𝜆𝑛 𝑛 − 𝑆 ≤ −𝑑 𝑆 → 𝑆 ≤𝑛

1 − 𝑑/𝜆𝑛

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The End


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