Top Banner
Integer Matrices with Constrained Eigenvalues Cyclotomic matrices and charged signed graphs Graeme Taylor Edinburgh January 2009 Graeme Taylor, Edinburgh Integer Matrices with Constrained Eigenvalues, Cyclotomic matrices and charged signed graphs 1/24
47

Integer Matrices with Constrained Eigenvalues - Straylight

Feb 11, 2022

Download

Documents

dariahiddleston
Welcome message from author
This document is posted to help you gain knowledge. Please leave a comment to let me know what you think about it! Share it to your friends and learn new things together.
Transcript
Page 1: Integer Matrices with Constrained Eigenvalues - Straylight

Integer Matrices with Constrained EigenvaluesCyclotomic matrices and charged signed graphs

Graeme Taylor

Edinburgh

January 2009

Graeme Taylor, Edinburgh Integer Matrices with Constrained Eigenvalues, Cyclotomic matrices and charged signed graphs 1/24

Page 2: Integer Matrices with Constrained Eigenvalues - Straylight

A question

Which integer symmetric matrices have all eigenvalues in [−2, 2]?

Graeme Taylor, Edinburgh Integer Matrices with Constrained Eigenvalues, Cyclotomic matrices and charged signed graphs 2/24

Page 3: Integer Matrices with Constrained Eigenvalues - Straylight

Mahler Measure

Let P(z) = a0zd + · · ·+ ad = a0

∏di=1(z − αi ) be a non-constant

polynomial.

DefinitionThe Mahler Measure M(P) is given by

M(P) := |a0|d∏

i=1

max (1, |αi |)

I Clearly, M(P) ≥ 1 for all P.

I If M(P) = 1, then all roots of P lie in the unit circle.

Graeme Taylor, Edinburgh Integer Matrices with Constrained Eigenvalues, Cyclotomic matrices and charged signed graphs 3/24

Page 4: Integer Matrices with Constrained Eigenvalues - Straylight

Mahler Measure

Let P(z) = a0zd + · · ·+ ad = a0

∏di=1(z − αi ) be a non-constant

polynomial.

DefinitionThe Mahler Measure M(P) is given by

M(P) := |a0|d∏

i=1

max (1, |αi |)

I Clearly, M(P) ≥ 1 for all P.

I If M(P) = 1, then all roots of P lie in the unit circle.

Graeme Taylor, Edinburgh Integer Matrices with Constrained Eigenvalues, Cyclotomic matrices and charged signed graphs 3/24

Page 5: Integer Matrices with Constrained Eigenvalues - Straylight

Mahler Measure

Let P(z) = a0zd + · · ·+ ad = a0

∏di=1(z − αi ) be a non-constant

polynomial.

DefinitionThe Mahler Measure M(P) is given by

M(P) := |a0|d∏

i=1

max (1, |αi |)

I Clearly, M(P) ≥ 1 for all P.

I If M(P) = 1, then all roots of P lie in the unit circle.

Graeme Taylor, Edinburgh Integer Matrices with Constrained Eigenvalues, Cyclotomic matrices and charged signed graphs 3/24

Page 6: Integer Matrices with Constrained Eigenvalues - Straylight

Mahler Measure

Let P(z) = a0zd + · · ·+ ad = a0

∏di=1(z − αi ) be a non-constant

polynomial.

DefinitionThe Mahler Measure M(P) is given by

M(P) := |a0|d∏

i=1

max (1, |αi |)

I Clearly, M(P) ≥ 1 for all P.

I If M(P) = 1, then all roots of P lie in the unit circle.

Graeme Taylor, Edinburgh Integer Matrices with Constrained Eigenvalues, Cyclotomic matrices and charged signed graphs 3/24

Page 7: Integer Matrices with Constrained Eigenvalues - Straylight

Mahler Measure

I If A is an n × n integer symmetric matrix, then its associatedpolynomial is RA(z) := znχA(z + 1/z)

I If A has all eigenvalues in [−2, 2], then RA is a cyclotomicpolynomial- We describe A as a cyclotomic matrix.

I So cyclotomic matrices yield integer polynomials RA with theminimal possible Mahler measure!

Graeme Taylor, Edinburgh Integer Matrices with Constrained Eigenvalues, Cyclotomic matrices and charged signed graphs 4/24

Page 8: Integer Matrices with Constrained Eigenvalues - Straylight

Mahler Measure

I If A is an n × n integer symmetric matrix, then its associatedpolynomial is RA(z) := znχA(z + 1/z)

I If A has all eigenvalues in [−2, 2], then RA is a cyclotomicpolynomial- We describe A as a cyclotomic matrix.

I So cyclotomic matrices yield integer polynomials RA with theminimal possible Mahler measure!

Graeme Taylor, Edinburgh Integer Matrices with Constrained Eigenvalues, Cyclotomic matrices and charged signed graphs 4/24

Page 9: Integer Matrices with Constrained Eigenvalues - Straylight

Mahler Measure

I If A is an n × n integer symmetric matrix, then its associatedpolynomial is RA(z) := znχA(z + 1/z)

I If A has all eigenvalues in [−2, 2], then RA is a cyclotomicpolynomial- We describe A as a cyclotomic matrix.

I So cyclotomic matrices yield integer polynomials RA with theminimal possible Mahler measure!

Graeme Taylor, Edinburgh Integer Matrices with Constrained Eigenvalues, Cyclotomic matrices and charged signed graphs 4/24

Page 10: Integer Matrices with Constrained Eigenvalues - Straylight

Mahler Measure

But any cyclotomic polynomial will have Mahler measure 1- whybother with the intermediate step of cyclotomic matrices?

Graeme Taylor, Edinburgh Integer Matrices with Constrained Eigenvalues, Cyclotomic matrices and charged signed graphs 5/24

Page 11: Integer Matrices with Constrained Eigenvalues - Straylight

Lehmer’s Conjecture

Now suppose P is a monic polynomial with integer coefficients.

I Lehmer’s Problem: For such polynomials with M(P) > 1, canM(P) be arbitrarily close to 1?

I If not, then there exists some λ > 1 such thatM(P) > 1⇒ M(P) > λ, forcing a ‘gap’ between cyclotomicand non-cyclotomic polynomials.

Graeme Taylor, Edinburgh Integer Matrices with Constrained Eigenvalues, Cyclotomic matrices and charged signed graphs 6/24

Page 12: Integer Matrices with Constrained Eigenvalues - Straylight

Lehmer’s Conjecture

Now suppose P is a monic polynomial with integer coefficients.

I Lehmer’s Problem: For such polynomials with M(P) > 1, canM(P) be arbitrarily close to 1?

I If not, then there exists some λ > 1 such thatM(P) > 1⇒ M(P) > λ, forcing a ‘gap’ between cyclotomicand non-cyclotomic polynomials.

Graeme Taylor, Edinburgh Integer Matrices with Constrained Eigenvalues, Cyclotomic matrices and charged signed graphs 6/24

Page 13: Integer Matrices with Constrained Eigenvalues - Straylight

Lehmer’s Conjecture

The smallest known Mahler measure greater than 1 for a monicpolynomial from Z[z ] is

λ0 = 1.176280818

which is the larger real root of the Lehmer polynomial

z10 + z9 − z7 − z6 − z5 − z4 − z3 + z + 1

Graeme Taylor, Edinburgh Integer Matrices with Constrained Eigenvalues, Cyclotomic matrices and charged signed graphs 7/24

Page 14: Integer Matrices with Constrained Eigenvalues - Straylight

From cyclotomic to non-cyclotomic?

I Likely candidates for small Mahler measure are polynomialsthat are ‘almost cyclotomic’- as few roots outside the unitcircle as possible.

I Difficulty: There’s no obvious way to obtain such an ‘almostcyclotomic’ integer polynomial from a cyclotomic one.

I But given a cyclotomic matrix, we can tweak it slightly to givea non-cyclotomic matrix.

Graeme Taylor, Edinburgh Integer Matrices with Constrained Eigenvalues, Cyclotomic matrices and charged signed graphs 8/24

Page 15: Integer Matrices with Constrained Eigenvalues - Straylight

From cyclotomic to non-cyclotomic?

I Likely candidates for small Mahler measure are polynomialsthat are ‘almost cyclotomic’- as few roots outside the unitcircle as possible.

I Difficulty: There’s no obvious way to obtain such an ‘almostcyclotomic’ integer polynomial from a cyclotomic one.

I But given a cyclotomic matrix, we can tweak it slightly to givea non-cyclotomic matrix.

Graeme Taylor, Edinburgh Integer Matrices with Constrained Eigenvalues, Cyclotomic matrices and charged signed graphs 8/24

Page 16: Integer Matrices with Constrained Eigenvalues - Straylight

From cyclotomic to non-cyclotomic?

I Likely candidates for small Mahler measure are polynomialsthat are ‘almost cyclotomic’- as few roots outside the unitcircle as possible.

I Difficulty: There’s no obvious way to obtain such an ‘almostcyclotomic’ integer polynomial from a cyclotomic one.

I But given a cyclotomic matrix, we can tweak it slightly to givea non-cyclotomic matrix.

Graeme Taylor, Edinburgh Integer Matrices with Constrained Eigenvalues, Cyclotomic matrices and charged signed graphs 8/24

Page 17: Integer Matrices with Constrained Eigenvalues - Straylight

From cyclotomic to non-cyclotomic

Theorem (Cauchy Interlacing Theorem)

Let A be a real symmetric n × n matrix with eigenvaluesλ1 ≤ λ2 ≤ · · · ≤ λn.Let B be obtained from A by deleting row i and column i from A.Then the eigenvalues µ1 ≤ · · · ≤ µn−1 of B interlace with those ofA: that is,

λ1 ≤ µ1 ≤ λ2 ≤ µ2 ≤ · · · ≤ µn−1 ≤ λn

Graeme Taylor, Edinburgh Integer Matrices with Constrained Eigenvalues, Cyclotomic matrices and charged signed graphs 9/24

Page 18: Integer Matrices with Constrained Eigenvalues - Straylight

From cyclotomic to non-cyclotomic

We can run this process in reverse. Let B be a cyclotomic matrix,so its eigenvalues satisfy

−2 ≤ µ1 ≤ · · · ≤ µn−1 ≤ 2

Then if we ‘grow’ a matrix A from B by adding an extra row andcolumn, we have by interlacing

λ1 ≤ µ1 ≤ λ2 ≤ µ2 ≤ · · · ≤ µn−1 ≤ λn

Soλ2, . . . , λn−1 ∈ [µ1, µn−1] ⊆ [−2, 2]

At worst,λ1, λn 6∈ [−2, 2]

Graeme Taylor, Edinburgh Integer Matrices with Constrained Eigenvalues, Cyclotomic matrices and charged signed graphs 10/24

Page 19: Integer Matrices with Constrained Eigenvalues - Straylight

From cyclotomic to non-cyclotomic

We can run this process in reverse. Let B be a cyclotomic matrix,so its eigenvalues satisfy

−2 ≤ µ1 ≤ · · · ≤ µn−1 ≤ 2

Then if we ‘grow’ a matrix A from B by adding an extra row andcolumn, we have by interlacing

λ1 ≤ µ1 ≤ λ2 ≤ µ2 ≤ · · · ≤ µn−1 ≤ λn

Soλ2, . . . , λn−1 ∈ [µ1, µn−1] ⊆ [−2, 2]

At worst,λ1, λn 6∈ [−2, 2]

Graeme Taylor, Edinburgh Integer Matrices with Constrained Eigenvalues, Cyclotomic matrices and charged signed graphs 10/24

Page 20: Integer Matrices with Constrained Eigenvalues - Straylight

From cyclotomic to non-cyclotomic

We can run this process in reverse. Let B be a cyclotomic matrix,so its eigenvalues satisfy

−2 ≤ µ1 ≤ · · · ≤ µn−1 ≤ 2

Then if we ‘grow’ a matrix A from B by adding an extra row andcolumn, we have by interlacing

λ1 ≤ µ1 ≤ λ2 ≤ µ2 ≤ · · · ≤ µn−1 ≤ λn

Soλ2, . . . , λn−1 ∈ [µ1, µn−1] ⊆ [−2, 2]

At worst,λ1, λn 6∈ [−2, 2]

Graeme Taylor, Edinburgh Integer Matrices with Constrained Eigenvalues, Cyclotomic matrices and charged signed graphs 10/24

Page 21: Integer Matrices with Constrained Eigenvalues - Straylight

From cyclotomic to non-cyclotomic

We can run this process in reverse. Let B be a cyclotomic matrix,so its eigenvalues satisfy

−2 ≤ µ1 ≤ · · · ≤ µn−1 ≤ 2

Then if we ‘grow’ a matrix A from B by adding an extra row andcolumn, we have by interlacing

λ1 ≤ µ1 ≤ λ2 ≤ µ2 ≤ · · · ≤ µn−1 ≤ λn

Soλ2, . . . , λn−1 ∈ [µ1, µn−1] ⊆ [−2, 2]

At worst,λ1, λn 6∈ [−2, 2]

Graeme Taylor, Edinburgh Integer Matrices with Constrained Eigenvalues, Cyclotomic matrices and charged signed graphs 10/24

Page 22: Integer Matrices with Constrained Eigenvalues - Straylight

Cyclotomic Matrices: Indecomposability

If M decomposes as a block-diagonal matrix, then its eigenvaluesare those of the blocks. So we can build cyclotomic matrices fromblocks of smaller ones; to classify cyclotomic matrices it thereforesuffices to classify just the indecomposable ones.

Graeme Taylor, Edinburgh Integer Matrices with Constrained Eigenvalues, Cyclotomic matrices and charged signed graphs 11/24

Page 23: Integer Matrices with Constrained Eigenvalues - Straylight

Cyclotomic Matrices: Interlacing I

I If A is cyclotomic, so is any B obtained by deleting some setof rows and corresponding columns of A: B is described asbeing contained in A.

I If M is an indecomposable cyclotomic matrix that is notcontained in any strictly larger indecomposable cyclotomicmatrix, then M is described as being maximal.

I Theorem: Any non-maximal indecomposable cyclotomicmatrix is contained in a maximal one.

Graeme Taylor, Edinburgh Integer Matrices with Constrained Eigenvalues, Cyclotomic matrices and charged signed graphs 12/24

Page 24: Integer Matrices with Constrained Eigenvalues - Straylight

Cyclotomic Matrices: Interlacing I

I If A is cyclotomic, so is any B obtained by deleting some setof rows and corresponding columns of A: B is described asbeing contained in A.

I If M is an indecomposable cyclotomic matrix that is notcontained in any strictly larger indecomposable cyclotomicmatrix, then M is described as being maximal.

I Theorem: Any non-maximal indecomposable cyclotomicmatrix is contained in a maximal one.

Graeme Taylor, Edinburgh Integer Matrices with Constrained Eigenvalues, Cyclotomic matrices and charged signed graphs 12/24

Page 25: Integer Matrices with Constrained Eigenvalues - Straylight

Cyclotomic Matrices: Interlacing I

I If A is cyclotomic, so is any B obtained by deleting some setof rows and corresponding columns of A: B is described asbeing contained in A.

I If M is an indecomposable cyclotomic matrix that is notcontained in any strictly larger indecomposable cyclotomicmatrix, then M is described as being maximal.

I Theorem: Any non-maximal indecomposable cyclotomicmatrix is contained in a maximal one.

Graeme Taylor, Edinburgh Integer Matrices with Constrained Eigenvalues, Cyclotomic matrices and charged signed graphs 12/24

Page 26: Integer Matrices with Constrained Eigenvalues - Straylight

Cyclotomic Matrices: Equivalence

Let On(Z) be the orthogonal group of n × n signed permutationmatrices, generated by matrices of the formdiag(1, 1, . . . , 1,−1, 1, . . . , 1) and permutation matrices.

I If M is cyclotomic and P ∈ On(Z), then M ′ = PMP−1 iscyclotomic since it has the same eigenvalues. We describe Mand M ′ as strongly equivalent.

I A matrix M ′ is then described as equivalent to M if it isstrongly equivalent to either M or −M.

Graeme Taylor, Edinburgh Integer Matrices with Constrained Eigenvalues, Cyclotomic matrices and charged signed graphs 13/24

Page 27: Integer Matrices with Constrained Eigenvalues - Straylight

Cyclotomic Matrices: Equivalence

Let On(Z) be the orthogonal group of n × n signed permutationmatrices, generated by matrices of the formdiag(1, 1, . . . , 1,−1, 1, . . . , 1) and permutation matrices.

I If M is cyclotomic and P ∈ On(Z), then M ′ = PMP−1 iscyclotomic since it has the same eigenvalues. We describe Mand M ′ as strongly equivalent.

I A matrix M ′ is then described as equivalent to M if it isstrongly equivalent to either M or −M.

Graeme Taylor, Edinburgh Integer Matrices with Constrained Eigenvalues, Cyclotomic matrices and charged signed graphs 13/24

Page 28: Integer Matrices with Constrained Eigenvalues - Straylight

Cyclotomic Matrices: Equivalence

Let On(Z) be the orthogonal group of n × n signed permutationmatrices, generated by matrices of the formdiag(1, 1, . . . , 1,−1, 1, . . . , 1) and permutation matrices.

I If M is cyclotomic and P ∈ On(Z), then M ′ = PMP−1 iscyclotomic since it has the same eigenvalues. We describe Mand M ′ as strongly equivalent.

I A matrix M ′ is then described as equivalent to M if it isstrongly equivalent to either M or −M.

Graeme Taylor, Edinburgh Integer Matrices with Constrained Eigenvalues, Cyclotomic matrices and charged signed graphs 13/24

Page 29: Integer Matrices with Constrained Eigenvalues - Straylight

Cyclotomic Matrices: Interlacing II

LemmaThe only cyclotomic 1× 1 matrices are

(0), (1), (−1), (2), (−2)

Corollary

By interlacing, the entries of an integer cyclotomic matrix must beelements of {0, 1,−1, 2,−2}.

Lemma

Apart from matrices equivalent to (2) or

(0 22 0

), any

indecomposable cyclotomic matrix has all entries from the set{0, 1,−1}.

Graeme Taylor, Edinburgh Integer Matrices with Constrained Eigenvalues, Cyclotomic matrices and charged signed graphs 14/24

Page 30: Integer Matrices with Constrained Eigenvalues - Straylight

Cyclotomic Matrices: Interlacing II

LemmaThe only cyclotomic 1× 1 matrices are

(0), (1), (−1), (2), (−2)

Corollary

By interlacing, the entries of an integer cyclotomic matrix must beelements of {0, 1,−1, 2,−2}.

Lemma

Apart from matrices equivalent to (2) or

(0 22 0

), any

indecomposable cyclotomic matrix has all entries from the set{0, 1,−1}.

Graeme Taylor, Edinburgh Integer Matrices with Constrained Eigenvalues, Cyclotomic matrices and charged signed graphs 14/24

Page 31: Integer Matrices with Constrained Eigenvalues - Straylight

Cyclotomic Matrices: Interlacing II

LemmaThe only cyclotomic 1× 1 matrices are

(0), (1), (−1), (2), (−2)

Corollary

By interlacing, the entries of an integer cyclotomic matrix must beelements of {0, 1,−1, 2,−2}.

Lemma

Apart from matrices equivalent to (2) or

(0 22 0

), any

indecomposable cyclotomic matrix has all entries from the set{0, 1,−1}.

Graeme Taylor, Edinburgh Integer Matrices with Constrained Eigenvalues, Cyclotomic matrices and charged signed graphs 14/24

Page 32: Integer Matrices with Constrained Eigenvalues - Straylight

The question, refined

Our original question thus reduces to classifying all maximal,indecomposable, cyclotomic, symmetric {−1, 0, 1}-matrices, up toequivalence.

Graeme Taylor, Edinburgh Integer Matrices with Constrained Eigenvalues, Cyclotomic matrices and charged signed graphs 15/24

Page 33: Integer Matrices with Constrained Eigenvalues - Straylight

Charged Signed Graphs

A convenient representation of such a matrix M is given by acharged, signed graph G .

I Mii = 0 gives a neutral vertex i , denoted •.I Mii = 1 gives a positively-charged vertex i , denoted ⊕.

I Mii = −1 gives a negatively-charged vertex i , denoted .

I Mij = 1, i 6= j gives a positive edge between vertices i and j ,denoted .

I Mij = −1, i 6= j gives a negative edge between vertices i andj , denoted · · · · · · .

Graeme Taylor, Edinburgh Integer Matrices with Constrained Eigenvalues, Cyclotomic matrices and charged signed graphs 16/24

Page 34: Integer Matrices with Constrained Eigenvalues - Straylight

Charged Signed Graphs

A convenient representation of such a matrix M is given by acharged, signed graph G .

I Mii = 0 gives a neutral vertex i , denoted •.I Mii = 1 gives a positively-charged vertex i , denoted ⊕.

I Mii = −1 gives a negatively-charged vertex i , denoted .

I Mij = 1, i 6= j gives a positive edge between vertices i and j ,denoted .

I Mij = −1, i 6= j gives a negative edge between vertices i andj , denoted · · · · · · .

Graeme Taylor, Edinburgh Integer Matrices with Constrained Eigenvalues, Cyclotomic matrices and charged signed graphs 16/24

Page 35: Integer Matrices with Constrained Eigenvalues - Straylight

Charged Signed Graphs

A convenient representation of such a matrix M is given by acharged, signed graph G .

I Mii = 0 gives a neutral vertex i , denoted •.I Mii = 1 gives a positively-charged vertex i , denoted ⊕.

I Mii = −1 gives a negatively-charged vertex i , denoted .

I Mij = 1, i 6= j gives a positive edge between vertices i and j ,denoted .

I Mij = −1, i 6= j gives a negative edge between vertices i andj , denoted · · · · · · .

Graeme Taylor, Edinburgh Integer Matrices with Constrained Eigenvalues, Cyclotomic matrices and charged signed graphs 16/24

Page 36: Integer Matrices with Constrained Eigenvalues - Straylight

Cyclotomic Graphs

I M indecomposable ⇔ G connected.

I Maximality: M not contained in a larger cyclotomic matrix ⇔G not an induced subgraph of a larger cyclotomic graph.

I M1 a permutation of M2 ⇔ G1 is a re-labelling of G2.

I Conjugation of M by kth diagonal matrix ⇔ Switching ofsigns of all edges incident at vertex k of G .

Graeme Taylor, Edinburgh Integer Matrices with Constrained Eigenvalues, Cyclotomic matrices and charged signed graphs 17/24

Page 37: Integer Matrices with Constrained Eigenvalues - Straylight

Cyclotomic Graphs

I M indecomposable ⇔ G connected.

I Maximality: M not contained in a larger cyclotomic matrix ⇔G not an induced subgraph of a larger cyclotomic graph.

I M1 a permutation of M2 ⇔ G1 is a re-labelling of G2.

I Conjugation of M by kth diagonal matrix ⇔ Switching ofsigns of all edges incident at vertex k of G .

Graeme Taylor, Edinburgh Integer Matrices with Constrained Eigenvalues, Cyclotomic matrices and charged signed graphs 17/24

Page 38: Integer Matrices with Constrained Eigenvalues - Straylight

Cyclotomic Graphs

I M indecomposable ⇔ G connected.

I Maximality: M not contained in a larger cyclotomic matrix ⇔G not an induced subgraph of a larger cyclotomic graph.

I M1 a permutation of M2 ⇔ G1 is a re-labelling of G2.

I Conjugation of M by kth diagonal matrix ⇔ Switching ofsigns of all edges incident at vertex k of G .

Graeme Taylor, Edinburgh Integer Matrices with Constrained Eigenvalues, Cyclotomic matrices and charged signed graphs 17/24

Page 39: Integer Matrices with Constrained Eigenvalues - Straylight

Cyclotomic Graphs

I M indecomposable ⇔ G connected.

I Maximality: M not contained in a larger cyclotomic matrix ⇔G not an induced subgraph of a larger cyclotomic graph.

I M1 a permutation of M2 ⇔ G1 is a re-labelling of G2.

I Conjugation of M by kth diagonal matrix ⇔ Switching ofsigns of all edges incident at vertex k of G .

Graeme Taylor, Edinburgh Integer Matrices with Constrained Eigenvalues, Cyclotomic matrices and charged signed graphs 17/24

Page 40: Integer Matrices with Constrained Eigenvalues - Straylight

A picture is worth a thousand matrices

So we can represent an equivalence class of cyclotomic matrices bya cyclotomic graph.

Graeme Taylor, Edinburgh Integer Matrices with Constrained Eigenvalues, Cyclotomic matrices and charged signed graphs 18/24

Page 41: Integer Matrices with Constrained Eigenvalues - Straylight

Classification

Charged Sporadics S7, S8,S′8:

Graeme Taylor, Edinburgh Integer Matrices with Constrained Eigenvalues, Cyclotomic matrices and charged signed graphs 19/24

Page 42: Integer Matrices with Constrained Eigenvalues - Straylight

Classification

Infinite family C+±2k , k ≥ 2:

Graeme Taylor, Edinburgh Integer Matrices with Constrained Eigenvalues, Cyclotomic matrices and charged signed graphs 20/24

Page 43: Integer Matrices with Constrained Eigenvalues - Straylight

ClassificationUncharged Sporadic S14:

Graeme Taylor, Edinburgh Integer Matrices with Constrained Eigenvalues, Cyclotomic matrices and charged signed graphs 21/24

Page 44: Integer Matrices with Constrained Eigenvalues - Straylight

ClassificationUncharged Sporadic S16:

Graeme Taylor, Edinburgh Integer Matrices with Constrained Eigenvalues, Cyclotomic matrices and charged signed graphs 22/24

Page 45: Integer Matrices with Constrained Eigenvalues - Straylight

Classification

Infinite family T2k , k ≥ 3:

Graeme Taylor, Edinburgh Integer Matrices with Constrained Eigenvalues, Cyclotomic matrices and charged signed graphs 23/24

Page 46: Integer Matrices with Constrained Eigenvalues - Straylight

Thanks for listening!

Slides and references online at http://maths.straylight.co.uk

Graeme Taylor, Edinburgh Integer Matrices with Constrained Eigenvalues, Cyclotomic matrices and charged signed graphs 24/24

Page 47: Integer Matrices with Constrained Eigenvalues - Straylight

Thanks for listening!

Slides and references online at http://maths.straylight.co.uk

Graeme Taylor, Edinburgh Integer Matrices with Constrained Eigenvalues, Cyclotomic matrices and charged signed graphs 24/24