Supernilpotence and Higher Dimensional Congruences Andrew Moorhead - - PowerPoint PPT Presentation

supernilpotence and higher dimensional congruences
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Supernilpotence and Higher Dimensional Congruences Andrew Moorhead - - PowerPoint PPT Presentation

Supernilpotence and Higher Dimensional Congruences Andrew Moorhead Vanderbilt University August 5, 2018 Overview of Talk 1. Commutator Theory, Nilpotence, and Supernilpotence Overview of Talk 1. Commutator Theory, Nilpotence, and


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SLIDE 1

Supernilpotence and Higher Dimensional Congruences

Andrew Moorhead

Vanderbilt University

August 5, 2018

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SLIDE 2

Overview of Talk

  • 1. Commutator Theory, Nilpotence, and Supernilpotence
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SLIDE 3

Overview of Talk

  • 1. Commutator Theory, Nilpotence, and Supernilpotence
  • 2. Higher Dimensional Congruence Relations
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SLIDE 4

Overview of Talk

  • 1. Commutator Theory, Nilpotence, and Supernilpotence
  • 2. Higher Dimensional Congruence Relations
  • 3. A Stronger Term Condition and Commutator
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SLIDE 5

Overview of Talk

  • 1. Commutator Theory, Nilpotence, and Supernilpotence
  • 2. Higher Dimensional Congruence Relations
  • 3. A Stronger Term Condition and Commutator
  • 4. Supernilpotent Taylor Algebras
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SLIDE 6

Overview of Talk

  • 1. Commutator Theory, Nilpotence, and Supernilpotence
  • 2. Higher Dimensional Congruence Relations
  • 3. A Stronger Term Condition and Commutator
  • 4. Supernilpotent Taylor Algebras
  • 5. Supernilpotence Need Not Imply Nilpotence
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SLIDE 7

Commutator Theory

◮ The classical commutator for a universal algebra A is a binary

  • peration

[·, ·] : Con(A)2 → Con(A) that allows one to define abelianness and generalizations of abelianness such as solvability and nilpotence.

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SLIDE 8

Commutator Theory

◮ The classical commutator for a universal algebra A is a binary

  • peration

[·, ·] : Con(A)2 → Con(A) that allows one to define abelianness and generalizations of abelianness such as solvability and nilpotence.

◮ For example, an algebra A is said to be abelian if

[1, 1] = 0.

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SLIDE 9

Commutator Theory

◮ The classical commutator for a universal algebra A is a binary

  • peration

[·, ·] : Con(A)2 → Con(A) that allows one to define abelianness and generalizations of abelianness such as solvability and nilpotence.

◮ For example, an algebra A is said to be abelian if

[1, 1] = 0.

◮ The higher commutator is a higher arity operation that

generalizes the binary commutator, e.g. [·, . . . , ·

n

] : Con(A)n → Con(A)

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SLIDE 10

Nilpotence and Supernilpotence

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SLIDE 11

Nilpotence and Supernilpotence

Definition

Let A be an algebra and let θ ∈ Con(A). Set [θ]0 = (θ]0 := θ and [θ]i+1 := [[θ]i, [θ]i] and (θ]i+1 = [(θ]i, θ]TC. These produce two descending chains of congruences, called the derived and lower central series, respectively.

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SLIDE 12

Nilpotence and Supernilpotence

Definition

Let A be an algebra and let θ ∈ Con(A). Set [θ]0 = (θ]0 := θ and [θ]i+1 := [[θ]i, [θ]i] and (θ]i+1 = [(θ]i, θ]TC. These produce two descending chains of congruences, called the derived and lower central series, respectively.

  • 1. If [θ]n = 0 then θ is said to be n-step solvable.
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SLIDE 13

Nilpotence and Supernilpotence

Definition

Let A be an algebra and let θ ∈ Con(A). Set [θ]0 = (θ]0 := θ and [θ]i+1 := [[θ]i, [θ]i] and (θ]i+1 = [(θ]i, θ]TC. These produce two descending chains of congruences, called the derived and lower central series, respectively.

  • 1. If [θ]n = 0 then θ is said to be n-step solvable.
  • 2. If (θ]n = 0, then θ is said to be n-step nilpotent.
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SLIDE 14

Nilpotence and Supernilpotence

Definition

Let A be an algebra and let θ ∈ Con(A). Set [θ]0 = (θ]0 := θ and [θ]i+1 := [[θ]i, [θ]i] and (θ]i+1 = [(θ]i, θ]TC. These produce two descending chains of congruences, called the derived and lower central series, respectively.

  • 1. If [θ]n = 0 then θ is said to be n-step solvable.
  • 2. If (θ]n = 0, then θ is said to be n-step nilpotent.
  • 3. If θ is such that [θ, . . . , θ]
  • n+1

= 0, then θ is said to be n-step supernilpotent.

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SLIDE 15

Nilpotence and Supernilpotence

◮ Supernilpotence and nilpotence are the same for groups and

rings but in general they are different, even for expanded groups.

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SLIDE 16

Nilpotence and Supernilpotence

◮ Supernilpotence and nilpotence are the same for groups and

rings but in general they are different, even for expanded groups.

◮ Supernilpotence has received attention lately, partly because

  • f theorems of the type ‘nice property of finite nilpotent

groups holds for finite supernilpotent algebras of finite type,’ for example:

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SLIDE 17

Nilpotence and Supernilpotence

◮ Supernilpotence and nilpotence are the same for groups and

rings but in general they are different, even for expanded groups.

◮ Supernilpotence has received attention lately, partly because

  • f theorems of the type ‘nice property of finite nilpotent

groups holds for finite supernilpotent algebras of finite type,’ for example:

  • 1. A finite Mal’cev algebra of finite type is supernilpotent if and
  • nly it is the product of prime power order nilpotent algebras.

(Freese & McKenzie, Kearnes, Aichinger & Mudrinski)

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SLIDE 18

Nilpotence and Supernilpotence

◮ Supernilpotence and nilpotence are the same for groups and

rings but in general they are different, even for expanded groups.

◮ Supernilpotence has received attention lately, partly because

  • f theorems of the type ‘nice property of finite nilpotent

groups holds for finite supernilpotent algebras of finite type,’ for example:

  • 1. A finite Mal’cev algebra of finite type is supernilpotent if and
  • nly it is the product of prime power order nilpotent algebras.

(Freese & McKenzie, Kearnes, Aichinger & Mudrinski)

  • 2. There is a polynomial time algorithm to solve the equation

satisfiability problem for a finite supernilpotent Mal’cev algebra

  • f finite type. (Kompatscher)
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SLIDE 19

Nilpotence and Supernilpotence

◮ The commutator is monotonic in each argument, so

nilpotence is stronger than solvability.

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SLIDE 20

Nilpotence and Supernilpotence

◮ The commutator is monotonic in each argument, so

nilpotence is stronger than solvability.

◮ The exact relationship between supernilpotence and

nilpotence has been unclear.

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SLIDE 21

Nilpotence and Supernilpotence

◮ The commutator is monotonic in each argument, so

nilpotence is stronger than solvability.

◮ The exact relationship between supernilpotence and

nilpotence has been unclear.

◮ Aichinger and Mudrinski have shown any supernilpotent

Mal’cev algebra is nilpotent.

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SLIDE 22

Nilpotence and Supernilpotence

◮ The commutator is monotonic in each argument, so

nilpotence is stronger than solvability.

◮ The exact relationship between supernilpotence and

nilpotence has been unclear.

◮ Aichinger and Mudrinski have shown any supernilpotent

Mal’cev algebra is nilpotent.

◮ Kearnes and Szendrei have announced that any finite

supernilpotent algebra is nilpotent.

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SLIDE 23

Nilpotence and Supernilpotence

◮ The commutator is monotonic in each argument, so

nilpotence is stronger than solvability.

◮ The exact relationship between supernilpotence and

nilpotence has been unclear.

◮ Aichinger and Mudrinski have shown any supernilpotent

Mal’cev algebra is nilpotent.

◮ Kearnes and Szendrei have announced that any finite

supernilpotent algebra is nilpotent.

◮ It follows from results of Wires that any supernilpotent

algebra generating a modular variety is nilpotent.

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SLIDE 24

Nilpotence and Supernilpotence

◮ The commutator is monotonic in each argument, so

nilpotence is stronger than solvability.

◮ The exact relationship between supernilpotence and

nilpotence has been unclear.

◮ Aichinger and Mudrinski have shown any supernilpotent

Mal’cev algebra is nilpotent.

◮ Kearnes and Szendrei have announced that any finite

supernilpotent algebra is nilpotent.

◮ It follows from results of Wires that any supernilpotent

algebra generating a modular variety is nilpotent.

◮ We can show any supernilpotent Taylor algebra is nilpotent.

(A Taylor algebra is an algebra that satisfies some nontrivial idempotent Mal’cev condition.)

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SLIDE 25

Nilpotence and Supernilpotence

◮ The commutator is monotonic in each argument, so

nilpotence is stronger than solvability.

◮ The exact relationship between supernilpotence and

nilpotence has been unclear.

◮ Aichinger and Mudrinski have shown any supernilpotent

Mal’cev algebra is nilpotent.

◮ Kearnes and Szendrei have announced that any finite

supernilpotent algebra is nilpotent.

◮ It follows from results of Wires that any supernilpotent

algebra generating a modular variety is nilpotent.

◮ We can show any supernilpotent Taylor algebra is nilpotent.

(A Taylor algebra is an algebra that satisfies some nontrivial idempotent Mal’cev condition.)

◮ Moore and M. have constructed a supernilpotent algebra that

is not solvable and hence not nilpotent. Note, this algebra is necessarily infinite and not Taylor.

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SLIDE 26

Commutator Definition

◮ The modular commutator can be equivalently defined with

either

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SLIDE 27

Commutator Definition

◮ The modular commutator can be equivalently defined with

either

  • 1. the term condition, or
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SLIDE 28

Commutator Definition

◮ The modular commutator can be equivalently defined with

either

  • 1. the term condition, or
  • 2. properties of a relation, usually called ∆.
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SLIDE 29

Commutator Definition

◮ The modular commutator can be equivalently defined with

either

  • 1. the term condition, or
  • 2. properties of a relation, usually called ∆.

Definition (Term Condition)

Let A be an algebra and take α, β, δ ∈ Con(A). We say that α centralizes β modulo δ when the following condition is met:

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SLIDE 30

Commutator Definition

◮ The modular commutator can be equivalently defined with

either

  • 1. the term condition, or
  • 2. properties of a relation, usually called ∆.

Definition (Term Condition)

Let A be an algebra and take α, β, δ ∈ Con(A). We say that α centralizes β modulo δ when the following condition is met:

◮ For all t ∈ Pol(A) and a0 ≡α b0 and a1 ≡β b1 with

|a0| + |a1| = σ(t),

  • t(a0, a1) ≡δ t(a0, b1) =

⇒ t(b0, a0) ≡δ t(b0, b1)

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SLIDE 31

Commutator Definition

◮ The modular commutator can be equivalently defined with

either

  • 1. the term condition, or
  • 2. properties of a relation, usually called ∆.

Definition (Term Condition)

Let A be an algebra and take α, β, δ ∈ Con(A). We say that α centralizes β modulo δ when the following condition is met:

◮ For all t ∈ Pol(A) and a0 ≡α b0 and a1 ≡β b1 with

|a0| + |a1| = σ(t),

  • t(a0, a1) ≡δ t(a0, b1) =

⇒ t(b0, a0) ≡δ t(b0, b1)

  • We write CTC(α, β; δ) whenever this is true.
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SLIDE 32

Commutator Definition

◮ The modular commutator can be equivalently defined with

either

  • 1. the term condition, or
  • 2. properties of a relation, usually called ∆.

Definition (Term Condition)

Let A be an algebra and take α, β, δ ∈ Con(A). We say that α centralizes β modulo δ when the following condition is met:

◮ For all t ∈ Pol(A) and a0 ≡α b0 and a1 ≡β b1 with

|a0| + |a1| = σ(t),

  • t(a0, a1) ≡δ t(a0, b1) =

⇒ t(b0, a0) ≡δ t(b0, b1)

  • We write CTC(α, β; δ) whenever this is true.

◮ The term condition may be described as a condition that is

quantified over a certain invariant relation of A which is called the algebra of (α, β)-matrices and is denoted M(α, β).

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Matrices

◮ A square is the graph 22; E, where two functions f , g ∈ 22

are connected by an edge if and only if their outputs differ in exactly one argument.

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Matrices

◮ A square is the graph 22; E, where two functions f , g ∈ 22

are connected by an edge if and only if their outputs differ in exactly one argument.

(0, 0) (1, 0) (0, 1) (1, 1)

◮ We say that a relation R on a set A is 2-dimensional if

R ⊆ A22 (R is a set of squares whos vertices are labeled by elements of A.)

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Matrices

◮ A square is the graph 22; E, where two functions f , g ∈ 22

are connected by an edge if and only if their outputs differ in exactly one argument.

(0, 0) (1, 0) (0, 1) (1, 1)

◮ We say that a relation R on a set A is 2-dimensional if

R ⊆ A22 (R is a set of squares whos vertices are labeled by elements of A.)

◮ M(α, β) is the subalgebra of A22 with generators

x y x y

  • : x ≡α y

y y x x

  • : x ≡β y
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SLIDE 36

Matrices

For δ ∈ Con(A) we have that α centralizes β modulo δ if the implication

α

β a b c d a b c d δ

holds for all (α, β)-matrices. This condition is abbreviated CTC(α, β; δ).

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SLIDE 37

Matrices

Similarly, we have that β centralizes α modulo δ if the implication

α

β a b c d a b c d δ

holds for all (α, β)-matrices. This condition is abbreviated CTC(β, α; δ).

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SLIDE 38

Matrices

◮ The binary commutator is defined to be

[α, β]TC =

  • {δ : C(α, β; δ)}
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SLIDE 39

Matrices

◮ The notions of matrices and centrality for three congruences

are defined similarly.

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SLIDE 40

Matrices

◮ The notions of matrices and centrality for three congruences

are defined similarly.

◮ A cube is the graph 23; E, where two functions f , g ∈ 23 are

connected by an edge if and only if their outputs differ in exactly one argument.

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SLIDE 41

Matrices

◮ The notions of matrices and centrality for three congruences

are defined similarly.

◮ A cube is the graph 23; E, where two functions f , g ∈ 23 are

connected by an edge if and only if their outputs differ in exactly one argument.

(0, 0, 0) (0, 1, 0) (1, 1, 0) (1, 0, 0) (0, 1, 1) (0, 0, 1) (1, 0, 1) (1, 1, 1)

◮ We say that a relation R on a set A is 3-dimensional if

R ⊆ A32 (R is a set of cubes whos vertices are labeled by elements of A.)

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SLIDE 42

Matrices

◮ The notions of matrices and centrality for three congruences

are defined similarly.

◮ A cube is the graph 23; E, where two functions f , g ∈ 23 are

connected by an edge if and only if their outputs differ in exactly one argument.

(0, 0, 0) (0, 1, 0) (1, 1, 0) (1, 0, 0) (0, 1, 1) (0, 0, 1) (1, 0, 1) (1, 1, 1)

◮ We say that a relation R on a set A is 3-dimensional if

R ⊆ A32 (R is a set of cubes whos vertices are labeled by elements of A.)

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SLIDE 43

Matrices

◮ For congruences θ0, θ1, θ2 ∈ Con(A), set M(θ0, θ1, θ2) ≤ A23

to be the subalgebra generated by the following labeled cubes:

x x x x y y y y y y y y x x x x x x x x y y y y θ0 θ1 θ2

M(θ0, θ1, θ2) is called the algebra of (θ0, θ1, θ2)-matrices.

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SLIDE 44

Centrality

◮ For δ ∈ Con(A), we say that θ0, θ1 centralize θ2 modulo δ

if the following implication holds for all (θ0, θ1, θ2)-matrices:

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SLIDE 45

Centrality

◮ For δ ∈ Con(A), we say that θ0, θ1 centralize θ2 modulo δ

if the following implication holds for all (θ0, θ1, θ2)-matrices:

θ0 θ1 θ2 a b c d e f g h

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SLIDE 46

Centrality

◮ For δ ∈ Con(A), we say that θ0, θ1 centralize θ2 modulo δ

if the following implication holds for all (θ0, θ1, θ2)-matrices:

θ0 θ1 θ2 a b c d e f g h δ

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SLIDE 47

Centrality

◮ For δ ∈ Con(A), we say that θ0, θ1 centralize θ2 modulo δ

if the following implication holds for all (θ0, θ1, θ2)-matrices:

θ0 θ1 θ2 a b c d e f g h δ

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SLIDE 48

Centrality

◮ For δ ∈ Con(A), we say that θ0, θ1 centralize θ2 modulo δ

if the following implication holds for all (θ0, θ1, θ2)-matrices:

θ0 θ1 θ2 a b c d e f g h δ

◮ This condition is abbreviated CTC(θ0, θ1, θ2; δ).

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SLIDE 49

Centrality

◮ Here is a picture of CTC(θ1, θ2, θ0; δ):

1 2 a b c d e f g h δ

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SLIDE 50

Matrices

◮ For congruences θ0, θ1, θ2 we set

[θ0, θ1, θ2]TC =

  • {δ : CTC(θ0, θ1, θ2; δ)}
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SLIDE 51

Matrices

◮ For congruences θ0, θ1, θ2 we set

[θ0, θ1, θ2]TC =

  • {δ : CTC(θ0, θ1, θ2; δ)}

◮ Higher centrality and the commutator for arity ≥ 4 are

similarly defined.

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SLIDE 52

Matrices

◮ An n-dimensional hypercube is the graph Hn = 2n; E, where

two functions f , g ∈ 2n are connected by an edge if and only if their outputs differ in exactly one argument.

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SLIDE 53

Matrices

◮ An n-dimensional hypercube is the graph Hn = 2n; E, where

two functions f , g ∈ 2n are connected by an edge if and only if their outputs differ in exactly one argument.

◮ We say that a relation R on a set A is n-dimensional if

R ⊆ A2n

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SLIDE 54

Matrices

◮ An n-dimensional hypercube is the graph Hn = 2n; E, where

two functions f , g ∈ 2n are connected by an edge if and only if their outputs differ in exactly one argument.

◮ We say that a relation R on a set A is n-dimensional if

R ⊆ A2n

◮ Observation: The term condition definition of centrality

involving n-many congruences θ0, . . . , θn−1 is a condition that is quantified over (θ0, . . . , θn−1)-matrices, which are certain n-dimensional invariant relations M(θ0, . . . , θn−1) ≤ A2n that have generators of the form

x y

(n − 1)-dimensional cube θi f ∈ 2n such that f(i) = 0 f ∈ 2n such that f(i) = 1

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SLIDE 55

◮ Consider the n-dimensional hypercube Hn = 2n; E. For any

coordinate i ∈ n, there are two (n − 1)-dimensional hyperfaces that are ‘perpendicular’ to i:

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SLIDE 56

◮ Consider the n-dimensional hypercube Hn = 2n; E. For any

coordinate i ∈ n, there are two (n − 1)-dimensional hyperfaces that are ‘perpendicular’ to i:

  • 1. (Hn)0

i = {f ∈ 2n : f (i) = 0}; E and

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SLIDE 57

◮ Consider the n-dimensional hypercube Hn = 2n; E. For any

coordinate i ∈ n, there are two (n − 1)-dimensional hyperfaces that are ‘perpendicular’ to i:

  • 1. (Hn)0

i = {f ∈ 2n : f (i) = 0}; E and

  • 2. (Hn)1

i = {f ∈ 2n : f (i) = 1}; E.

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SLIDE 58

◮ Consider the n-dimensional hypercube Hn = 2n; E. For any

coordinate i ∈ n, there are two (n − 1)-dimensional hyperfaces that are ‘perpendicular’ to i:

  • 1. (Hn)0

i = {f ∈ 2n : f (i) = 0}; E and

  • 2. (Hn)1

i = {f ∈ 2n : f (i) = 1}; E.

(0, 0, 0, 1) (1, 0, 0, 1) (1, 1, 0, 1) (0, 0, 0, 0) (1, 0, 0, 0) (0, 1, 0, 0) (1, 1, 0, 0) (0, 0, 1, 0) (1, 0, 1, 0) (0, 1, 1, 0) (1, 1, 1, 0) (0, 1, 0, 1) (0, 0, 1, 1) (1, 0, 1, 1) (0, 1, 1, 1) (1, 1, 1, 1)

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SLIDE 59

◮ Consider the n-dimensional hypercube Hn = 2n; E. For any

coordinate i ∈ n, there are two (n − 1)-dimensional hyperfaces that are ‘perpendicular’ to i:

  • 1. (Hn)0

i = {f ∈ 2n : f (i) = 0}; E and

  • 2. (Hn)1

i = {f ∈ 2n : f (i) = 1}; E.

(0, 0, 0, 1) (1, 0, 0, 1) (1, 1, 0, 1) (0, 0, 0, 0) (1, 0, 0, 0) (0, 1, 0, 0) (1, 1, 0, 0) (0, 0, 1, 0) (1, 0, 1, 0) (0, 1, 1, 0) (1, 1, 1, 0) (0, 1, 0, 1) (0, 0, 1, 1) (1, 0, 1, 1) (0, 1, 1, 1) (1, 1, 1, 1)

(Hn)0

3 and (Hn)1 3

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SLIDE 60

◮ Consider the n-dimensional hypercube Hn = 2n; E. For any

coordinate i ∈ n, there are two (n − 1)-dimensional hyperfaces that are ‘perpendicular’ to i:

  • 1. (Hn)0

i = {f ∈ 2n : f (i) = 0}; E and

  • 2. (Hn)1

i = {f ∈ 2n : f (i) = 1}; E.

(0, 0, 0, 1) (1, 0, 0, 1) (1, 1, 0, 1) (0, 0, 0, 0) (1, 0, 0, 0) (0, 1, 0, 0) (1, 1, 0, 0) (0, 0, 1, 0) (1, 0, 1, 0) (0, 1, 1, 0) (1, 1, 1, 0) (0, 1, 0, 1) (0, 0, 1, 1) (1, 0, 1, 1) (0, 1, 1, 1) (1, 1, 1, 1)

(Hn)0

0 and (Hn)1

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SLIDE 61

◮ Take h ∈ A2n. We consider h as a vertex labeled

n-dimensional hypercube. For any coordinate i ∈ n, there are two (n − 1)-dimensional vertex labeled hyperfaces that are perpendicular to i, which we denote

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SLIDE 62

◮ Take h ∈ A2n. We consider h as a vertex labeled

n-dimensional hypercube. For any coordinate i ∈ n, there are two (n − 1)-dimensional vertex labeled hyperfaces that are perpendicular to i, which we denote

  • 1. h0

i and

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SLIDE 63

◮ Take h ∈ A2n. We consider h as a vertex labeled

n-dimensional hypercube. For any coordinate i ∈ n, there are two (n − 1)-dimensional vertex labeled hyperfaces that are perpendicular to i, which we denote

  • 1. h0

i and

  • 2. h1

i .

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SLIDE 64

◮ Take h ∈ A2n. We consider h as a vertex labeled

n-dimensional hypercube. For any coordinate i ∈ n, there are two (n − 1)-dimensional vertex labeled hyperfaces that are perpendicular to i, which we denote

  • 1. h0

i and

  • 2. h1

i . a b c d e f g s i j k l m n

  • p

h ∈ A2n

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SLIDE 65

◮ Take h ∈ A2n. We consider h as a vertex labeled

n-dimensional hypercube. For any coordinate i ∈ n, there are two (n − 1)-dimensional vertex labeled hyperfaces that are perpendicular to i, which we denote

  • 1. h0

i and

  • 2. h1

i . a b c d e f g s i j k l m n

  • p

h ∈ A2n h0

3 and h1 3

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SLIDE 66

◮ Take h ∈ A2n. We consider h as a vertex labeled

n-dimensional hypercube. For any coordinate i ∈ n, there are two (n − 1)-dimensional vertex labeled hyperfaces that are perpendicular to i, which we denote

  • 1. h0

i and

  • 2. h1

i . a b c d e f g s i j k l m n

  • p

h ∈ A2n h0

1 and h1 1

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SLIDE 67

◮ For R ⊆ A2n, set

Ri = {h0

i , h1 i : h ∈ R}.

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SLIDE 68

◮ For R ⊆ A2n, set

Ri = {h0

i , h1 i : h ∈ R}. ◮ Fact: Suppose A is a member of a permutable variety, and

take (θ0, . . . , θn−1) ∈ Con(A)n. Then, M(θ0, . . . , θn−1)i is a congruence relation, for all i ∈ n.

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SLIDE 69

◮ For R ⊆ A2n, set

Ri = {h0

i , h1 i : h ∈ R}. ◮ Fact: Suppose A is a member of a permutable variety, and

take (θ0, . . . , θn−1) ∈ Con(A)n. Then, M(θ0, . . . , θn−1)i is a congruence relation, for all i ∈ n.

◮ This leads to a nice characterization of the commutator for

permutable varieties.

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SLIDE 70

Theorem (Binary Commutator)

Let V be a permutable variety and let A ∈ V. For α, β ∈ Con(A), the following are equivalent:

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SLIDE 71

Theorem (Binary Commutator)

Let V be a permutable variety and let A ∈ V. For α, β ∈ Con(A), the following are equivalent:

  • 1. x, y ∈ [α, β]TC
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SLIDE 72

Theorem (Binary Commutator)

Let V be a permutable variety and let A ∈ V. For α, β ∈ Con(A), the following are equivalent:

  • 1. x, y ∈ [α, β]TC

2. x y x x

  • ∈ M(α, β)
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SLIDE 73

Theorem (Binary Commutator)

Let V be a permutable variety and let A ∈ V. For α, β ∈ Con(A), the following are equivalent:

  • 1. x, y ∈ [α, β]TC

2. x y x x

  • ∈ M(α, β)

3. a y a x

  • ∈ M(α, β) for some a ∈ A
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SLIDE 74

Theorem (Binary Commutator)

Let V be a permutable variety and let A ∈ V. For α, β ∈ Con(A), the following are equivalent:

  • 1. x, y ∈ [α, β]TC

2. x y x x

  • ∈ M(α, β)

3. a y a x

  • ∈ M(α, β) for some a ∈ A

4. x y b b

  • ∈ M(α, β) for some b ∈ A.
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SLIDE 75

◮ Let V be a modular variety and let A ∈ V. For α, β ∈ Con(A),

define ∆α,β to be the transitive closure of M(α, β)0.

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SLIDE 76

◮ Let V be a modular variety and let A ∈ V. For α, β ∈ Con(A),

define ∆α,β to be the transitive closure of M(α, β)0.

a b c d e0 f0 e1 f1 e2 f2 en fn en−1 fn−1 1 a b c d ∈ ∆α,β

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SLIDE 77

◮ Let V be a modular variety and let A ∈ V. For α, β ∈ Con(A),

define ∆α,β to be the transitive closure of M(α, β)0.

a b c d e0 f0 e1 f1 e2 f2 en fn en−1 fn−1 1 a b c d ∈ ∆α,β

◮ Fact: Both (∆α,β)0 and (∆α,β)1 are congruence relations.

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SLIDE 78

Theorem (Binary Commutator)

Let V be a modular variety and let A ∈ V. For α, β ∈ Con(A), the following are equivalent:

  • 1. x, y ∈ [α, β]TC

2. x y x x

  • ∈ ∆α,β

3. a y a x

  • ∈ ∆α,β for some a ∈ A

4. x y b b

  • ∈ ∆α,β for some b ∈ A.
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SLIDE 79

θ0 θ1 θ2 Theorem: Let V be a permutable variety. Take θ0, θ1, θ2 ∈ Con(A) for A ∈ V. The following are equivalent: x, y ∈ [θ0, θ1, θ2] (2) (1) (3) (4) (5) ∈ M(θ0, θ1, θ2) ∈ M(θ0, θ1, θ2) ∈ M(θ0, θ1, θ2) ∈ M(θ0, θ1, θ2) x x x x x x x y x y x y x y a a b b c c d d e e f f h h i i j j There exist elements of A such that

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SLIDE 80

θ0 θ1 θ2 Theorem: Let V be a modular variety. Take θ0, θ1, θ2 ∈ Con(A) for A ∈ V. The following are equivalent: x, y ∈ [θ0, θ1, θ2] (2) (1) (3) (4) (5) ∈ ∆θ0,θ1,θ2 ∈ ∆θ0,θ1,θ2 ∈ ∆θ0,θ1,θ2 ∈ ∆θ0,θ1,θ2 x x x x x x x y x y x y x y a a b b c c d d e e f f h h i i j j There exist elements of A such that

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SLIDE 81

Higher Dimensional Congruence Relations

Definition

Let R ⊆ A2n be an n-dimensional relation on some set A. R is called an n-dimensional equivalence relation if for all i ∈ n, each Ri is an equivalence relation.

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SLIDE 82

Higher Dimensional Congruence Relations

Definition

Let R ⊆ A2n be an n-dimensional relation on some set A. R is called an n-dimensional equivalence relation if for all i ∈ n, each Ri is an equivalence relation.

Definition

Let A be an algebra with underlying set A. Let R ∈ A2n be an n-dimensional equivalence relation. R is called an n-dimensional congruence if R is preserved by the basic operations of A.

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SLIDE 83

Higher Dimensional Congruence Relations

Definition

Let R ⊆ A2n be an n-dimensional relation on some set A. R is called an n-dimensional equivalence relation if for all i ∈ n, each Ri is an equivalence relation.

Definition

Let A be an algebra with underlying set A. Let R ∈ A2n be an n-dimensional equivalence relation. R is called an n-dimensional congruence if R is preserved by the basic operations of A.

◮ Fix n ≥ 1. The collection of all n-dimensional congruences of

an algebra A is an algebraic lattice, which we denote by Conn(A).

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SLIDE 84

Higher Dimensional Congruence Relations

Definition

Let R ⊆ A2n be an n-dimensional relation on some set A. R is called an n-dimensional equivalence relation if for all i ∈ n, each Ri is an equivalence relation.

Definition

Let A be an algebra with underlying set A. Let R ∈ A2n be an n-dimensional equivalence relation. R is called an n-dimensional congruence if R is preserved by the basic operations of A.

◮ Fix n ≥ 1. The collection of all n-dimensional congruences of

an algebra A is an algebraic lattice, which we denote by Conn(A).

◮ There are n distinct embeddings from Con1(A) into Conn(A).

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SLIDE 85

Con1(A)

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SLIDE 86

Con1(A) Con2(A) φ0

2

α

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SLIDE 87

Con1(A) Con2(A) φ0

2

φ0

2(α) =

x y x y

  • : x, y ∈ α
  • α
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SLIDE 88

Con1(A) Con2(A) φ0

2

φ0

2(α) =

x y x y

  • : x, y ∈ α
  • φ1

2

φ1

2(β) =

x x y y

  • : x, y ∈ β
  • α

β

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SLIDE 89

Con1(A) Con2(A) φ0

2

φ0

2(α) =

x y x y

  • : x, y ∈ α
  • φ1

2

φ1

2(β) =

x x y y

  • : x, y ∈ β
  • α

β ∆α,β Define ∆α,β = φ0

2(α) ∨ φ1 2(β)

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SLIDE 90

Higher Dimensional Congruence Relations

◮ Fix a dimension n and take i ∈ n. For a pair x, y ∈ A2, let

Cubei(x, y) ∈ A2n be such that

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SLIDE 91

Higher Dimensional Congruence Relations

◮ Fix a dimension n and take i ∈ n. For a pair x, y ∈ A2, let

Cubei(x, y) ∈ A2n be such that

1.

  • Cubei(x, y)

i is the (n − 1)-dimensional cube with each

vertex labeled by x.

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SLIDE 92

Higher Dimensional Congruence Relations

◮ Fix a dimension n and take i ∈ n. For a pair x, y ∈ A2, let

Cubei(x, y) ∈ A2n be such that

1.

  • Cubei(x, y)

i is the (n − 1)-dimensional cube with each

vertex labeled by x.

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SLIDE 93

Higher Dimensional Congruence Relations

◮ Fix a dimension n and take i ∈ n. For a pair x, y ∈ A2, let

Cubei(x, y) ∈ A2n be such that

1.

  • Cubei(x, y)

i is the (n − 1)-dimensional cube with each

vertex labeled by x. 2.

  • Cubei(x, y)

1

i is the (n − 1)-dimensional cube with each

vertex labeled by y.

◮ Define φi n : Con1(A) → Conn(A) by

φi

n(α) = {Cubei(x, y) : x, y ∈ α}

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SLIDE 94

Con1(A) Conn(A) θ0 θn−1 φ0

n

φn−1

n

∆θ0,...,θn−1 Define ∆θ0,...,θn−1 =

i φi n(θi)

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SLIDE 95

Characterizing Joins

◮ Let A be an algebra and let θ be an equivalence relation on A.

Then, θ is an admissible relation if and only if θ is compatible with the unary polynomials of A.

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SLIDE 96

Characterizing Joins

◮ Let A be an algebra and let θ be an equivalence relation on A.

Then, θ is an admissible relation if and only if θ is compatible with the unary polynomials of A.

◮ This generalizes to:

Theorem

Let A be an algebra and let n ≥ 1. An n-dimensional equivalence relation θ is admissible if and only if θ is compatible with the n-ary polynomials of A.

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SLIDE 97

Proof Idea

a0 b0 c0 d0 , ∈ θ Take a1 b1 c1 d1 , a2 b2 c2 d2 , a3 b3 c3 d3

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SLIDE 98

Proof Idea

a0 b0 c0 d0 , ∈ θ Take a1 b1 c1 d1 , a2 b2 c2 d2 , a3 b3 c3 d3 Then, c0 d0 d0 d0 d0 a0 b0 b0 b0 b0 c0 d0 d0 d0 d0 c0 d0 d0 d0 d0 c0 d0 d0 d0 d0 a1 a1 a1 a1 b1 b1 b1 b1 b1 b1 c1 c1 c1 c1 c1 c1 d1 d1 d1 d1 d1 d1 d1 d1 d1 a2 a2 a2 a2 a2 a2 a2 a2 a2 b2 b2 b2 b2 b2 b2 c2 c2 c2 c2 c2 c2 d2 d2 d2 d2 a3 a3 a3 a3 a3 a3 a3 a3 a3 a3 a3 a3 a3 a3 a3 a3 b3 b3 b3 b3 c3 c3 c3 c3 d3 ∈ θ

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SLIDE 99

Proof Idea

a0 b0 c0 d0 , ∈ θ Take a1 b1 c1 d1 , a2 b2 c2 d2 , a3 b3 c3 d3 Then, c0 d0 d0 d0 d0 a0 b0 b0 b0 b0 c0 d0 d0 d0 d0 c0 d0 d0 d0 d0 c0 d0 d0 d0 d0 a1 a1 a1 a1 b1 b1 b1 b1 b1 b1 c1 c1 c1 c1 c1 c1 d1 d1 d1 d1 d1 d1 d1 d1 d1 a2 a2 a2 a2 a2 a2 a2 a2 a2 b2 b2 b2 b2 b2 b2 c2 c2 c2 c2 c2 c2 d2 d2 d2 d2 a3 a3 a3 a3 a3 a3 a3 a3 a3 a3 a3 a3 a3 a3 a3 a3 b3 b3 b3 b3 c3 c3 c3 c3 d3 ∈ θ Compatibility with binary polynomials is sufficient to show compatibility with a 4-ary

  • peration.
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SLIDE 100

Characterizing Joins

◮ ∆θ0,...,θn−1 = i φi n(θi) is therefore obtained by

  • 1. Closing φi

n(θi) under all n-ary polynomials and then

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SLIDE 101

Characterizing Joins

◮ ∆θ0,...,θn−1 = i φi n(θi) is therefore obtained by

  • 1. Closing φi

n(θi) under all n-ary polynomials and then

  • 2. taking a sequence of transitive closures, cycling through all

possible directions possibly ω-many times.

◮ Notice: M(θ0, . . . , θn−1) ≤ ∆θ0,...,θn−1. We use this larger

collection to define a stronger term condition.

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SLIDE 102

Hypercentrality

For δ ∈ Con(A) we have that α hypercentralizes β modulo δ if the implication

α

β a b c d a b c d δ

holds for all members of ∆α,β. This condition is abbreviated CH(α, β; δ).

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SLIDE 103

Hypercentrality

Similarly, we have that β hypercentralizes α modulo δ if the implication

α

β a b c d a b c d δ

holds for all members of ∆α,β. This condition is abbreviated CH(β, α; δ).

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SLIDE 104

Hypercentrality

◮ For congruences θ0, θ1 we set

[θ0, θ1]H =

  • {δ : CH(θ0, θ1; δ)}
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SLIDE 105

Hypercentrality

◮ For congruences θ0, θ1 we set

[θ0, θ1]H =

  • {δ : CH(θ0, θ1; δ)}

◮ Higher arity hypercentrality and the higher arity

hypercommutator similarly defined.

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SLIDE 106

Theorem (Binary Hyper Commutator)

Let A be an algebra. For α, β ∈ Con(A), the following are equivalent:

  • 1. x, y ∈ [α, β]H

2. x y x x

  • ∈ ∆α,β

3. a y a x

  • ∈ ∆α,β for some a ∈ A

4. x y b b

  • ∈ ∆α,β for some b ∈ A.
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SLIDE 107

Theorem (Binary Hyper Commutator)

Let A be an algebra. For α, β ∈ Con(A), the following are equivalent:

  • 1. x, y ∈ [α, β]H

2. x y x x

  • ∈ ∆α,β

3. a y a x

  • ∈ ∆α,β for some a ∈ A

4. x y b b

  • ∈ ∆α,β for some b ∈ A.

◮ A similar characterization of the higher arity hyper

commutator also holds.

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SLIDE 108

Supernilpotent Taylor Algebras Are Nilpotent

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SLIDE 109

Supernilpotent Taylor Algebras Are Nilpotent

◮ Strategy:

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SLIDE 110

Supernilpotent Taylor Algebras Are Nilpotent

◮ Strategy:

  • 1. From the definitions, it follows that

[θ0, . . . , θn−1]TC ≤ [θ0, . . . , θn−1]H

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SLIDE 111

Supernilpotent Taylor Algebras Are Nilpotent

◮ Strategy:

  • 1. From the definitions, it follows that

[θ0, . . . , θn−1]TC ≤ [θ0, . . . , θn−1]H

  • 2. Demonstrate the commutator nesting property for the hyper

commutator: [[θ0, . . . , θi−1]H, θi, . . . , θn−1]H ≤ [θ0, . . . , θn−1]H

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SLIDE 112

Supernilpotent Taylor Algebras Are Nilpotent

◮ Strategy:

  • 1. From the definitions, it follows that

[θ0, . . . , θn−1]TC ≤ [θ0, . . . , θn−1]H

  • 2. Demonstrate the commutator nesting property for the hyper

commutator: [[θ0, . . . , θi−1]H, θi, . . . , θn−1]H ≤ [θ0, . . . , θn−1]H

  • 3. Show that [θ, . . . , θ]S = [θ, . . . , θ]H in a Taylor variety.
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SLIDE 113

Supernilpotent Taylor Algebras Are Nilpotent

◮ Strategy:

  • 1. From the definitions, it follows that

[θ0, . . . , θn−1]TC ≤ [θ0, . . . , θn−1]H

  • 2. Demonstrate the commutator nesting property for the hyper

commutator: [[θ0, . . . , θi−1]H, θi, . . . , θn−1]H ≤ [θ0, . . . , θn−1]H

  • 3. Show that [θ, . . . , θ]S = [θ, . . . , θ]H in a Taylor variety.
  • 4. (2) and (3) imply that

[[θ, . . . , θ]TC, θ, . . . , θ]TC = [[θ, . . . , θ]H, θ, . . . , θ]H ≤ [θ, . . . , θ]H = [θ, . . . , θ]TC

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SLIDE 114

Supernilpotent

  • =

⇒ Nilpotent (work with Moore)

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SLIDE 115

Supernilpotent

  • =

⇒ Nilpotent (work with Moore)

Define A = O ∪ R ∪ G with G infinite, O = {oj

i : i, j ∈ ω}, and

R = {rj

i : i, j ∈ ω}.

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SLIDE 116

Supernilpotent

  • =

⇒ Nilpotent (work with Moore)

Define A = O ∪ R ∪ G with G infinite, O = {oj

i : i, j ∈ ω}, and

R = {rj

i : i, j ∈ ω}. Let A = A; t be the algebra with underlying

set A and a binary operation t with the table

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SLIDE 117

Supernilpotent

  • =

⇒ Nilpotent (work with Moore)

Define A = O ∪ R ∪ G with G infinite, O = {oj

i : i, j ∈ ω}, and

R = {rj

i : i, j ∈ ω}. Let A = A; t be the algebra with underlying

set A and a binary operation t with the table

x r j

4i

r j

4i+2

y r j

4i

r j

4i+2

t(x, y)

  • j

i

r j+1

i

  • j

i

r j+1

i+1

where t an injection into G otherwise.

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SLIDE 118

Supernilpotent

  • =

⇒ Nilpotent

◮ A is not solvable and hence not nilpotent.

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SLIDE 119

Supernilpotent

  • =

⇒ Nilpotent

◮ A is not solvable and hence not nilpotent. ◮ A is 2-step supernilpotent. To prove this it suffices to show

that h =

a b b a c e d c

∈ M(1, 1, 1) implies e = d.

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SLIDE 120

Supernilpotent

  • =

⇒ Nilpotent

◮ A is not solvable and hence not nilpotent. ◮ A is 2-step supernilpotent. To prove this it suffices to show

that h =

a b b a c e d c

∈ M(1, 1, 1) implies e = d.

◮ This example generalizes to ‘higher dimensions.’ There exist

algebras An that

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SLIDE 121

Supernilpotent

  • =

⇒ Nilpotent

◮ A is not solvable and hence not nilpotent. ◮ A is 2-step supernilpotent. To prove this it suffices to show

that h =

a b b a c e d c

∈ M(1, 1, 1) implies e = d.

◮ This example generalizes to ‘higher dimensions.’ There exist

algebras An that

  • 1. are not solvable in dimension n (no term in commutators up

to arity n evaluated at 1 produces 0)

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SLIDE 122

Supernilpotent

  • =

⇒ Nilpotent

◮ A is not solvable and hence not nilpotent. ◮ A is 2-step supernilpotent. To prove this it suffices to show

that h =

a b b a c e d c

∈ M(1, 1, 1) implies e = d.

◮ This example generalizes to ‘higher dimensions.’ There exist

algebras An that

  • 1. are not solvable in dimension n (no term in commutators up

to arity n evaluated at 1 produces 0)

  • 2. but are n-step supernilpotent.
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SLIDE 123

Supernilpotent

  • =

⇒ Nilpotent

◮ A is not solvable and hence not nilpotent. ◮ A is 2-step supernilpotent. To prove this it suffices to show

that h =

a b b a c e d c

∈ M(1, 1, 1) implies e = d.

◮ This example generalizes to ‘higher dimensions.’ There exist

algebras An that

  • 1. are not solvable in dimension n (no term in commutators up

to arity n evaluated at 1 produces 0)

  • 2. but are n-step supernilpotent.

◮ Question: Let [V] be a chapter in the lattice of interpretability

  • f types that does not lie above Olˇ

s´ ak’s variety. Is there a variety W ∈ [V] with a supernilpotent algebra that is not nilpotent?

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SLIDE 124

Thank you for attending this presentation.

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SLIDE 125

Thank you for attending this presentation. Thank you organizers!