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Higher Structures Lisbon July 24-27, 2017 Instituto Superior T ecnico, Lisbon Homotopical Excision: (work to be done!) Ronnie Brown Ronnie Brown () Higher Structures Lisbon July 24-27, 2017 Instituto Superior T ecnico, Lisbon


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SLIDE 1

Higher Structures Lisbon July 24-27, 2017 Instituto Superior T´ ecnico, Lisbon Homotopical Excision: (work to be done!)

Ronnie Brown

Ronnie Brown () Higher Structures Lisbon July 24-27, 2017 Instituto Superior T´ ecnico, Lisbon Homotopical 1 / 19

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SLIDE 2

Contents

1a Background 1b Methodology

  • 2. Relative Homotopical Excision
  • 3. Origin of my work with Loday
  • 4. Squares of pointed spaces
  • 5. Crossed squares
  • 6. Squares of squares
  • 7. A nonabelian tensor product
  • 8. Categorical background
  • 9. Excision for unions of 3 spaces
  • 10. Conclusion: work to be done

Ronnie Brown () Higher Structures Lisbon July 24-27, 2017 Instituto Superior T´ ecnico, Lisbon Homotopical 2 / 19

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SLIDE 3
  • 1a. Background:

Ronnie Brown () Higher Structures Lisbon July 24-27, 2017 Instituto Superior T´ ecnico, Lisbon Homotopical 3 / 19

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SLIDE 4
  • 1a. Background:

In homotopy theory identifications in low dimensions affect high dimensional invariants. How to model this?

Ronnie Brown () Higher Structures Lisbon July 24-27, 2017 Instituto Superior T´ ecnico, Lisbon Homotopical 3 / 19

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SLIDE 5
  • 1a. Background:

In homotopy theory identifications in low dimensions affect high dimensional invariants. How to model this? Warning: sometimes you need information in dimension zero!

Ronnie Brown () Higher Structures Lisbon July 24-27, 2017 Instituto Superior T´ ecnico, Lisbon Homotopical 3 / 19

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SLIDE 6
  • 1a. Background:

In homotopy theory identifications in low dimensions affect high dimensional invariants. How to model this? Warning: sometimes you need information in dimension zero! Example: X = Sn ∨ [0, 2], πn(X, 0) ∼ = πn(Sn, 0). But πn(X, {0, 1, 2}) is clearly a free π1([0, 2], {0, 1, 2})-module.

Ronnie Brown () Higher Structures Lisbon July 24-27, 2017 Instituto Superior T´ ecnico, Lisbon Homotopical 3 / 19

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SLIDE 7
  • 1a. Background:

In homotopy theory identifications in low dimensions affect high dimensional invariants. How to model this? Warning: sometimes you need information in dimension zero! Example: X = Sn ∨ [0, 2], πn(X, 0) ∼ = πn(Sn, 0). But πn(X, {0, 1, 2}) is clearly a free π1([0, 2], {0, 1, 2})-module. Then identify 0, 1, 2 to a point:

Ronnie Brown () Higher Structures Lisbon July 24-27, 2017 Instituto Superior T´ ecnico, Lisbon Homotopical 3 / 19

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SLIDE 8
  • 1a. Background:

In homotopy theory identifications in low dimensions affect high dimensional invariants. How to model this? Warning: sometimes you need information in dimension zero! Example: X = Sn ∨ [0, 2], πn(X, 0) ∼ = πn(Sn, 0). But πn(X, {0, 1, 2}) is clearly a free π1([0, 2], {0, 1, 2})-module. Then identify 0, 1, 2 to a point: πn(Sn ∨ S1 ∨ S1, 0) is a free π1(S1 ∨ S1, 0)-module on 1 generator.

Ronnie Brown () Higher Structures Lisbon July 24-27, 2017 Instituto Superior T´ ecnico, Lisbon Homotopical 3 / 19

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SLIDE 9
  • 1a. Background:

In homotopy theory identifications in low dimensions affect high dimensional invariants. How to model this? Warning: sometimes you need information in dimension zero! Example: X = Sn ∨ [0, 2], πn(X, 0) ∼ = πn(Sn, 0). But πn(X, {0, 1, 2}) is clearly a free π1([0, 2], {0, 1, 2})-module. Then identify 0, 1, 2 to a point: πn(Sn ∨ S1 ∨ S1, 0) is a free π1(S1 ∨ S1, 0)-module on 1 generator. However in this talk all spaces will be pointed!

Ronnie Brown () Higher Structures Lisbon July 24-27, 2017 Instituto Superior T´ ecnico, Lisbon Homotopical 3 / 19

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SLIDE 10
  • 1a. Background:

In homotopy theory identifications in low dimensions affect high dimensional invariants. How to model this? Warning: sometimes you need information in dimension zero! Example: X = Sn ∨ [0, 2], πn(X, 0) ∼ = πn(Sn, 0). But πn(X, {0, 1, 2}) is clearly a free π1([0, 2], {0, 1, 2})-module. Then identify 0, 1, 2 to a point: πn(Sn ∨ S1 ∨ S1, 0) is a free π1(S1 ∨ S1, 0)-module on 1 generator. However in this talk all spaces will be pointed! Solution to general problem: try to find algebraic objects with structure in dimensions 0, 1, . . . , n,

Ronnie Brown () Higher Structures Lisbon July 24-27, 2017 Instituto Superior T´ ecnico, Lisbon Homotopical 3 / 19

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SLIDE 11
  • 1a. Background:

In homotopy theory identifications in low dimensions affect high dimensional invariants. How to model this? Warning: sometimes you need information in dimension zero! Example: X = Sn ∨ [0, 2], πn(X, 0) ∼ = πn(Sn, 0). But πn(X, {0, 1, 2}) is clearly a free π1([0, 2], {0, 1, 2})-module. Then identify 0, 1, 2 to a point: πn(Sn ∨ S1 ∨ S1, 0) is a free π1(S1 ∨ S1, 0)-module on 1 generator. However in this talk all spaces will be pointed! Solution to general problem: try to find algebraic objects with structure in dimensions 0, 1, . . . , n, modelling spaces with analogous structure.

Ronnie Brown () Higher Structures Lisbon July 24-27, 2017 Instituto Superior T´ ecnico, Lisbon Homotopical 3 / 19

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SLIDE 12
  • 1a. Background:

In homotopy theory identifications in low dimensions affect high dimensional invariants. How to model this? Warning: sometimes you need information in dimension zero! Example: X = Sn ∨ [0, 2], πn(X, 0) ∼ = πn(Sn, 0). But πn(X, {0, 1, 2}) is clearly a free π1([0, 2], {0, 1, 2})-module. Then identify 0, 1, 2 to a point: πn(Sn ∨ S1 ∨ S1, 0) is a free π1(S1 ∨ S1, 0)-module on 1 generator. However in this talk all spaces will be pointed! Solution to general problem: try to find algebraic objects with structure in dimensions 0, 1, . . . , n, modelling spaces with analogous structure. AIM: Colimit theorems for homotopically defined functors on Topological Data with values in strict higher groupoids,

Ronnie Brown () Higher Structures Lisbon July 24-27, 2017 Instituto Superior T´ ecnico, Lisbon Homotopical 3 / 19

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SLIDE 13
  • 1a. Background:

In homotopy theory identifications in low dimensions affect high dimensional invariants. How to model this? Warning: sometimes you need information in dimension zero! Example: X = Sn ∨ [0, 2], πn(X, 0) ∼ = πn(Sn, 0). But πn(X, {0, 1, 2}) is clearly a free π1([0, 2], {0, 1, 2})-module. Then identify 0, 1, 2 to a point: πn(Sn ∨ S1 ∨ S1, 0) is a free π1(S1 ∨ S1, 0)-module on 1 generator. However in this talk all spaces will be pointed! Solution to general problem: try to find algebraic objects with structure in dimensions 0, 1, . . . , n, modelling spaces with analogous structure. AIM: Colimit theorems for homotopically defined functors on Topological Data with values in strict higher groupoids, so enabling specific nonabelian calculations of some homotopy types and so of some classical invariants.

Ronnie Brown () Higher Structures Lisbon July 24-27, 2017 Instituto Superior T´ ecnico, Lisbon Homotopical 3 / 19

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SLIDE 14
  • 1b. Methodology

We consider functors

  • Topological

Data

  • H

Algebraic Data

  • B
  • such that

Ronnie Brown () Higher Structures Lisbon July 24-27, 2017 Instituto Superior T´ ecnico, Lisbon Homotopical 4 / 19

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SLIDE 15
  • 1b. Methodology

We consider functors

  • Topological

Data

  • H

Algebraic Data

  • B
  • such that

1) H is homotopically defined.

Ronnie Brown () Higher Structures Lisbon July 24-27, 2017 Instituto Superior T´ ecnico, Lisbon Homotopical 4 / 19

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SLIDE 16
  • 1b. Methodology

We consider functors

  • Topological

Data

  • H

Algebraic Data

  • B
  • such that

1) H is homotopically defined. 2) HB is equivalent to 1.

Ronnie Brown () Higher Structures Lisbon July 24-27, 2017 Instituto Superior T´ ecnico, Lisbon Homotopical 4 / 19

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SLIDE 17
  • 1b. Methodology

We consider functors

  • Topological

Data

  • H

Algebraic Data

  • B
  • such that

1) H is homotopically defined. 2) HB is equivalent to 1. 3) The Topological Data has a notion of connected.

Ronnie Brown () Higher Structures Lisbon July 24-27, 2017 Instituto Superior T´ ecnico, Lisbon Homotopical 4 / 19

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SLIDE 18
  • 1b. Methodology

We consider functors

  • Topological

Data

  • H

Algebraic Data

  • B
  • such that

1) H is homotopically defined. 2) HB is equivalent to 1. 3) The Topological Data has a notion of connected. 4) For all Algebraic Data A, BA is connected.

Ronnie Brown () Higher Structures Lisbon July 24-27, 2017 Instituto Superior T´ ecnico, Lisbon Homotopical 4 / 19

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SLIDE 19
  • 1b. Methodology

We consider functors

  • Topological

Data

  • H

Algebraic Data

  • B
  • such that

1) H is homotopically defined. 2) HB is equivalent to 1. 3) The Topological Data has a notion of connected. 4) For all Algebraic Data A, BA is connected. 5) “Nice” colimits of connected Topological Data are :

Ronnie Brown () Higher Structures Lisbon July 24-27, 2017 Instituto Superior T´ ecnico, Lisbon Homotopical 4 / 19

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SLIDE 20
  • 1b. Methodology

We consider functors

  • Topological

Data

  • H

Algebraic Data

  • B
  • such that

1) H is homotopically defined. 2) HB is equivalent to 1. 3) The Topological Data has a notion of connected. 4) For all Algebraic Data A, BA is connected. 5) “Nice” colimits of connected Topological Data are : (a) connected, and

Ronnie Brown () Higher Structures Lisbon July 24-27, 2017 Instituto Superior T´ ecnico, Lisbon Homotopical 4 / 19

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SLIDE 21
  • 1b. Methodology

We consider functors

  • Topological

Data

  • H

Algebraic Data

  • B
  • such that

1) H is homotopically defined. 2) HB is equivalent to 1. 3) The Topological Data has a notion of connected. 4) For all Algebraic Data A, BA is connected. 5) “Nice” colimits of connected Topological Data are : (a) connected, and (b) preserved by H.

Ronnie Brown () Higher Structures Lisbon July 24-27, 2017 Instituto Superior T´ ecnico, Lisbon Homotopical 4 / 19

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SLIDE 22
  • 1b. Methodology

We consider functors

  • Topological

Data

  • H

Algebraic Data

  • B
  • such that

1) H is homotopically defined. 2) HB is equivalent to 1. 3) The Topological Data has a notion of connected. 4) For all Algebraic Data A, BA is connected. 5) “Nice” colimits of connected Topological Data are : (a) connected, and (b) preserved by H. The last is a generalised Seifert-van Kampen Theorem.

Ronnie Brown () Higher Structures Lisbon July 24-27, 2017 Instituto Superior T´ ecnico, Lisbon Homotopical 4 / 19

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SLIDE 23
  • 1b. Methodology

We consider functors

  • Topological

Data

  • H

Algebraic Data

  • B
  • such that

1) H is homotopically defined. 2) HB is equivalent to 1. 3) The Topological Data has a notion of connected. 4) For all Algebraic Data A, BA is connected. 5) “Nice” colimits of connected Topological Data are : (a) connected, and (b) preserved by H. The last is a generalised Seifert-van Kampen Theorem. We now recall an Excision Theorem of RB and Philip Higgins, JPAA, (1981)

Ronnie Brown () Higher Structures Lisbon July 24-27, 2017 Instituto Superior T´ ecnico, Lisbon Homotopical 4 / 19

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SLIDE 24
  • 2. Relative Homotopical Excision

Ronnie Brown () Higher Structures Lisbon July 24-27, 2017 Instituto Superior T´ ecnico, Lisbon Homotopical 5 / 19

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SLIDE 25
  • 2. Relative Homotopical Excision

Excision deals with Y = X ∪ B, A = X ∩ B, and, e.g., X, B are open in Y and considers the

Ronnie Brown () Higher Structures Lisbon July 24-27, 2017 Instituto Superior T´ ecnico, Lisbon Homotopical 5 / 19

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SLIDE 26
  • 2. Relative Homotopical Excision

Excision deals with Y = X ∪ B, A = X ∩ B, and, e.g., X, B are open in Y and considers the pushout of pairs (A, A)

  • i

(B, B)

  • (X, A)

j

(Y , B)

Ronnie Brown () Higher Structures Lisbon July 24-27, 2017 Instituto Superior T´ ecnico, Lisbon Homotopical 5 / 19

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SLIDE 27
  • 2. Relative Homotopical Excision

Excision deals with Y = X ∪ B, A = X ∩ B, and, e.g., X, B are open in Y and considers the pushout of pairs (A, A)

  • i

(B, B)

  • (X, A)

j

(Y , B)

Excision Theorem If (X, A) is (n − 1)-connected, then so also is (Y , B) and we get a pushout of modules (crossed if n = 2)

Ronnie Brown () Higher Structures Lisbon July 24-27, 2017 Instituto Superior T´ ecnico, Lisbon Homotopical 5 / 19

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SLIDE 28
  • 2. Relative Homotopical Excision

Excision deals with Y = X ∪ B, A = X ∩ B, and, e.g., X, B are open in Y and considers the pushout of pairs (A, A)

  • i

(B, B)

  • (X, A)

j

(Y , B)

Excision Theorem If (X, A) is (n − 1)-connected, then so also is (Y , B) and we get a pushout of modules (crossed if n = 2) (1, π1(A))

i∗

  • (1, π1(B))
  • (πn(X, A), π1(A))

j∗

(πn(Y , B), π1(B))

j∗ is “induced” by i∗

Ronnie Brown () Higher Structures Lisbon July 24-27, 2017 Instituto Superior T´ ecnico, Lisbon Homotopical 5 / 19

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SLIDE 29
  • 2. Relative Homotopical Excision

Excision deals with Y = X ∪ B, A = X ∩ B, and, e.g., X, B are open in Y and considers the pushout of pairs (A, A)

  • i

(B, B)

  • (X, A)

j

(Y , B)

Excision Theorem If (X, A) is (n − 1)-connected, then so also is (Y , B) and we get a pushout of modules (crossed if n = 2) (1, π1(A))

i∗

  • (1, π1(B))
  • (πn(X, A), π1(A))

j∗

(πn(Y , B), π1(B))

j∗ is “induced” by i∗ This implies the Relative Hurewicz Theorem by taking B = CA, a cone on A.

Ronnie Brown () Higher Structures Lisbon July 24-27, 2017 Instituto Superior T´ ecnico, Lisbon Homotopical 5 / 19

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SLIDE 30

Ronnie Brown () Higher Structures Lisbon July 24-27, 2017 Instituto Superior T´ ecnico, Lisbon Homotopical 6 / 19

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SLIDE 31

The case n = 2, X = CA, Y = B ∪ CA and A = ∨iS1

i

is a wedge of circles gives a 1949 Theorem of Whitehead on free crossed modules.

Ronnie Brown () Higher Structures Lisbon July 24-27, 2017 Instituto Superior T´ ecnico, Lisbon Homotopical 6 / 19

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SLIDE 32

The case n = 2, X = CA, Y = B ∪ CA and A = ∨iS1

i

is a wedge of circles gives a 1949 Theorem of Whitehead on free crossed modules. This Excision Theorem is a special case, or application, of a Seifert-van Kampen Theorem for filtered spaces; see the book

Ronnie Brown () Higher Structures Lisbon July 24-27, 2017 Instituto Superior T´ ecnico, Lisbon Homotopical 6 / 19

slide-33
SLIDE 33

The case n = 2, X = CA, Y = B ∪ CA and A = ∨iS1

i

is a wedge of circles gives a 1949 Theorem of Whitehead on free crossed modules. This Excision Theorem is a special case, or application, of a Seifert-van Kampen Theorem for filtered spaces; see the book Nonabelian Algebraic Topology

Ronnie Brown () Higher Structures Lisbon July 24-27, 2017 Instituto Superior T´ ecnico, Lisbon Homotopical 6 / 19

slide-34
SLIDE 34

The case n = 2, X = CA, Y = B ∪ CA and A = ∨iS1

i

is a wedge of circles gives a 1949 Theorem of Whitehead on free crossed modules. This Excision Theorem is a special case, or application, of a Seifert-van Kampen Theorem for filtered spaces; see the book Nonabelian Algebraic Topology (EMS, 2011, 703 pp) which realises the methodology of the second slide to give an exposition of the border between homology and homotopy, using

Ronnie Brown () Higher Structures Lisbon July 24-27, 2017 Instituto Superior T´ ecnico, Lisbon Homotopical 6 / 19

slide-35
SLIDE 35

The case n = 2, X = CA, Y = B ∪ CA and A = ∨iS1

i

is a wedge of circles gives a 1949 Theorem of Whitehead on free crossed modules. This Excision Theorem is a special case, or application, of a Seifert-van Kampen Theorem for filtered spaces; see the book Nonabelian Algebraic Topology (EMS, 2011, 703 pp) which realises the methodology of the second slide to give an exposition of the border between homology and homotopy, using

Ronnie Brown () Higher Structures Lisbon July 24-27, 2017 Instituto Superior T´ ecnico, Lisbon Homotopical 6 / 19

slide-36
SLIDE 36

The case n = 2, X = CA, Y = B ∪ CA and A = ∨iS1

i

is a wedge of circles gives a 1949 Theorem of Whitehead on free crossed modules. This Excision Theorem is a special case, or application, of a Seifert-van Kampen Theorem for filtered spaces; see the book Nonabelian Algebraic Topology (EMS, 2011, 703 pp) which realises the methodology of the second slide to give an exposition of the border between homology and homotopy, using and not requiring the usual singular homology.

Ronnie Brown () Higher Structures Lisbon July 24-27, 2017 Instituto Superior T´ ecnico, Lisbon Homotopical 6 / 19

slide-37
SLIDE 37

The case n = 2, X = CA, Y = B ∪ CA and A = ∨iS1

i

is a wedge of circles gives a 1949 Theorem of Whitehead on free crossed modules. This Excision Theorem is a special case, or application, of a Seifert-van Kampen Theorem for filtered spaces; see the book Nonabelian Algebraic Topology (EMS, 2011, 703 pp) which realises the methodology of the second slide to give an exposition of the border between homology and homotopy, using and not requiring the usual singular homology.

Ronnie Brown () Higher Structures Lisbon July 24-27, 2017 Instituto Superior T´ ecnico, Lisbon Homotopical 6 / 19

slide-38
SLIDE 38

The case n = 2, X = CA, Y = B ∪ CA and A = ∨iS1

i

is a wedge of circles gives a 1949 Theorem of Whitehead on free crossed modules. This Excision Theorem is a special case, or application, of a Seifert-van Kampen Theorem for filtered spaces; see the book Nonabelian Algebraic Topology (EMS, 2011, 703 pp) which realises the methodology of the second slide to give an exposition of the border between homology and homotopy, using and not requiring the usual singular homology.

Ronnie Brown () Higher Structures Lisbon July 24-27, 2017 Instituto Superior T´ ecnico, Lisbon Homotopical 6 / 19

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SLIDE 39
  • 3. Origin of my work with Loday

In November 1981 as part of a visit to France, and at the suggestion of Michel Zisman, I visited Jean-Louis Loday in Strasbourg to give a seminar

  • n the work with Philip Higgins.

Ronnie Brown () Higher Structures Lisbon July 24-27, 2017 Instituto Superior T´ ecnico, Lisbon Homotopical 7 / 19

slide-40
SLIDE 40
  • 3. Origin of my work with Loday

In November 1981 as part of a visit to France, and at the suggestion of Michel Zisman, I visited Jean-Louis Loday in Strasbourg to give a seminar

  • n the work with Philip Higgins.

Jean-Louis got the point of the talk, and expected there could be a van Kampen Theorem for his catn-groups functor on n-cubes of pointed spaces.

Ronnie Brown () Higher Structures Lisbon July 24-27, 2017 Instituto Superior T´ ecnico, Lisbon Homotopical 7 / 19

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SLIDE 41
  • 3. Origin of my work with Loday

In November 1981 as part of a visit to France, and at the suggestion of Michel Zisman, I visited Jean-Louis Loday in Strasbourg to give a seminar

  • n the work with Philip Higgins.

Jean-Louis got the point of the talk, and expected there could be a van Kampen Theorem for his catn-groups functor on n-cubes of pointed spaces. He also told me of a conjecture he had. I interpreted this conjecture as a Triadic Hurewicz Theorem,

Ronnie Brown () Higher Structures Lisbon July 24-27, 2017 Instituto Superior T´ ecnico, Lisbon Homotopical 7 / 19

slide-42
SLIDE 42
  • 3. Origin of my work with Loday

In November 1981 as part of a visit to France, and at the suggestion of Michel Zisman, I visited Jean-Louis Loday in Strasbourg to give a seminar

  • n the work with Philip Higgins.

Jean-Louis got the point of the talk, and expected there could be a van Kampen Theorem for his catn-groups functor on n-cubes of pointed spaces. He also told me of a conjecture he had. I interpreted this conjecture as a Triadic Hurewicz Theorem, which from the RB/PJH point of view should be deduced from a Triadic Excision Theorem,

Ronnie Brown () Higher Structures Lisbon July 24-27, 2017 Instituto Superior T´ ecnico, Lisbon Homotopical 7 / 19

slide-43
SLIDE 43
  • 3. Origin of my work with Loday

In November 1981 as part of a visit to France, and at the suggestion of Michel Zisman, I visited Jean-Louis Loday in Strasbourg to give a seminar

  • n the work with Philip Higgins.

Jean-Louis got the point of the talk, and expected there could be a van Kampen Theorem for his catn-groups functor on n-cubes of pointed spaces. He also told me of a conjecture he had. I interpreted this conjecture as a Triadic Hurewicz Theorem, which from the RB/PJH point of view should be deduced from a Triadic Excision Theorem, which itself should be deduced from a Triadic van Kampen Theorem.

Ronnie Brown () Higher Structures Lisbon July 24-27, 2017 Instituto Superior T´ ecnico, Lisbon Homotopical 7 / 19

slide-44
SLIDE 44
  • 3. Origin of my work with Loday

In November 1981 as part of a visit to France, and at the suggestion of Michel Zisman, I visited Jean-Louis Loday in Strasbourg to give a seminar

  • n the work with Philip Higgins.

Jean-Louis got the point of the talk, and expected there could be a van Kampen Theorem for his catn-groups functor on n-cubes of pointed spaces. He also told me of a conjecture he had. I interpreted this conjecture as a Triadic Hurewicz Theorem, which from the RB/PJH point of view should be deduced from a Triadic Excision Theorem, which itself should be deduced from a Triadic van Kampen Theorem. Jean-Louis suggested a more general theorem could be easier to prove!

Ronnie Brown () Higher Structures Lisbon July 24-27, 2017 Instituto Superior T´ ecnico, Lisbon Homotopical 7 / 19

slide-45
SLIDE 45
  • 4. Squares of pointed spaces

J-L’s methods involves in the first dimension a square of pointed spaces Z := A

x

  • b

B

g

  • X

f

Y

Ronnie Brown () Higher Structures Lisbon July 24-27, 2017 Instituto Superior T´ ecnico, Lisbon Homotopical 8 / 19

slide-46
SLIDE 46
  • 4. Squares of pointed spaces

J-L’s methods involves in the first dimension a square of pointed spaces Z := A

x

  • b

B

g

  • X

f

Y

Now we expand this to a diagram of fibrations,

Ronnie Brown () Higher Structures Lisbon July 24-27, 2017 Instituto Superior T´ ecnico, Lisbon Homotopical 8 / 19

slide-47
SLIDE 47
  • 4. Squares of pointed spaces

J-L’s methods involves in the first dimension a square of pointed spaces Z := A

x

  • b

B

g

  • X

f

Y

Now we expand this to a diagram of fibrations, F(Z)

  • F(x)
  • F(g)
  • F(b)
  • A

x

  • b

B

g

  • F(f )

X

f

Y

Ronnie Brown () Higher Structures Lisbon July 24-27, 2017 Instituto Superior T´ ecnico, Lisbon Homotopical 8 / 19

slide-48
SLIDE 48
  • 4. Squares of pointed spaces

J-L’s methods involves in the first dimension a square of pointed spaces Z := A

x

  • b

B

g

  • X

f

Y

Now we expand this to a diagram of fibrations, F(Z)

  • F(x)
  • F(g)
  • F(b)
  • A

x

  • b

B

g

  • F(f )

X

f

Y

and say Z is connected if all these spaces are connected.

Ronnie Brown () Higher Structures Lisbon July 24-27, 2017 Instituto Superior T´ ecnico, Lisbon Homotopical 8 / 19

slide-49
SLIDE 49
  • 4. Squares of pointed spaces

J-L’s methods involves in the first dimension a square of pointed spaces Z := A

x

  • b

B

g

  • X

f

Y

Now we expand this to a diagram of fibrations, F(Z)

  • F(x)
  • F(g)
  • F(b)
  • A

x

  • b

B

g

  • F(f )

X

f

Y

and say Z is connected if all these spaces are connected. Then we use π1 to form the square of groups

Ronnie Brown () Higher Structures Lisbon July 24-27, 2017 Instituto Superior T´ ecnico, Lisbon Homotopical 8 / 19

slide-50
SLIDE 50
  • 4. Squares of pointed spaces

J-L’s methods involves in the first dimension a square of pointed spaces Z := A

x

  • b

B

g

  • X

f

Y

Now we expand this to a diagram of fibrations, F(Z)

  • F(x)
  • F(g)
  • F(b)
  • A

x

  • b

B

g

  • F(f )

X

f

Y

and say Z is connected if all these spaces are connected. Then we use π1 to form the square of groups Π(Z) := π1(F(Z))

  • π1(F(x))
  • π1(F(b))

π1(A)

Ronnie Brown () Higher Structures Lisbon July 24-27, 2017 Instituto Superior T´ ecnico, Lisbon Homotopical 8 / 19

slide-51
SLIDE 51

In the case X, B ⊆ Y , A = X ∩ B this is equivalent to the classical diagram

Ronnie Brown () Higher Structures Lisbon July 24-27, 2017 Instituto Superior T´ ecnico, Lisbon Homotopical 9 / 19

slide-52
SLIDE 52

In the case X, B ⊆ Y , A = X ∩ B this is equivalent to the classical diagram π3(Y ; B, X)

  • π2(X, A)
  • π2(B, A)

π1(A)

Ronnie Brown () Higher Structures Lisbon July 24-27, 2017 Instituto Superior T´ ecnico, Lisbon Homotopical 9 / 19

slide-53
SLIDE 53

In the case X, B ⊆ Y , A = X ∩ B this is equivalent to the classical diagram π3(Y ; B, X)

  • π2(X, A)
  • π2(B, A)

π1(A)

With the operations of π1(A) on the other groups

Ronnie Brown () Higher Structures Lisbon July 24-27, 2017 Instituto Superior T´ ecnico, Lisbon Homotopical 9 / 19

slide-54
SLIDE 54

In the case X, B ⊆ Y , A = X ∩ B this is equivalent to the classical diagram π3(Y ; B, X)

  • π2(X, A)
  • π2(B, A)

π1(A)

With the operations of π1(A) on the other groups and the generalised Whitehead product h : π2(B, A) × π2(X, A) → π3(Y ; B, X)

Ronnie Brown () Higher Structures Lisbon July 24-27, 2017 Instituto Superior T´ ecnico, Lisbon Homotopical 9 / 19

slide-55
SLIDE 55

In the case X, B ⊆ Y , A = X ∩ B this is equivalent to the classical diagram π3(Y ; B, X)

  • π2(X, A)
  • π2(B, A)

π1(A)

With the operations of π1(A) on the other groups and the generalised Whitehead product h : π2(B, A) × π2(X, A) → π3(Y ; B, X) this gives a structure called a Crossed Square.

Ronnie Brown () Higher Structures Lisbon July 24-27, 2017 Instituto Superior T´ ecnico, Lisbon Homotopical 9 / 19

slide-56
SLIDE 56

In the case X, B ⊆ Y , A = X ∩ B this is equivalent to the classical diagram π3(Y ; B, X)

  • π2(X, A)
  • π2(B, A)

π1(A)

With the operations of π1(A) on the other groups and the generalised Whitehead product h : π2(B, A) × π2(X, A) → π3(Y ; B, X) this gives a structure called a Crossed Square. So we have a functor H : (Squares of pointed spaces) → (Crossed Squares). We also say (Y ; B, X) is connected if the square Z of spaces on the previous slide is connected.

Ronnie Brown () Higher Structures Lisbon July 24-27, 2017 Instituto Superior T´ ecnico, Lisbon Homotopical 9 / 19

slide-57
SLIDE 57
  • 5. Crossed Squares

L

λ′

  • λ
  • N

ν

  • M

µ

P

and h : M × N → L P acts on L, M, N so M, N act on L, M, N

Ronnie Brown () Higher Structures Lisbon July 24-27, 2017 Instituto Superior T´ ecnico, Lisbon Homotopical 10 / 19

slide-58
SLIDE 58
  • 5. Crossed Squares

L

λ′

  • λ
  • N

ν

  • M

µ

P

and h : M × N → L P acts on L, M, N so M, N act on L, M, N A crossed square should be thought of as a crossed module of crossed modules.

Ronnie Brown () Higher Structures Lisbon July 24-27, 2017 Instituto Superior T´ ecnico, Lisbon Homotopical 10 / 19

slide-59
SLIDE 59
  • 5. Crossed Squares

L

λ′

  • λ
  • N

ν

  • M

µ

P

and h : M × N → L P acts on L, M, N so M, N act on L, M, N A crossed square should be thought of as a crossed module of crossed modules. Two basic rules are: h(mm′, n) = h(mm′, mn)h(m, n),

Ronnie Brown () Higher Structures Lisbon July 24-27, 2017 Instituto Superior T´ ecnico, Lisbon Homotopical 10 / 19

slide-60
SLIDE 60
  • 5. Crossed Squares

L

λ′

  • λ
  • N

ν

  • M

µ

P

and h : M × N → L P acts on L, M, N so M, N act on L, M, N A crossed square should be thought of as a crossed module of crossed modules. Two basic rules are: h(mm′, n) = h(mm′, mn)h(m, n), h(m, nn′) = h(m, n)h(nm, nn′),

Ronnie Brown () Higher Structures Lisbon July 24-27, 2017 Instituto Superior T´ ecnico, Lisbon Homotopical 10 / 19

slide-61
SLIDE 61
  • 5. Crossed Squares

L

λ′

  • λ
  • N

ν

  • M

µ

P

and h : M × N → L P acts on L, M, N so M, N act on L, M, N A crossed square should be thought of as a crossed module of crossed modules. Two basic rules are: h(mm′, n) = h(mm′, mn)h(m, n), h(m, nn′) = h(m, n)h(nm, nn′),

Ronnie Brown () Higher Structures Lisbon July 24-27, 2017 Instituto Superior T´ ecnico, Lisbon Homotopical 10 / 19

slide-62
SLIDE 62
  • 5. Crossed Squares

L

λ′

  • λ
  • N

ν

  • M

µ

P

and h : M × N → L P acts on L, M, N so M, N act on L, M, N A crossed square should be thought of as a crossed module of crossed modules. Two basic rules are: h(mm′, n) = h(mm′, mn)h(m, n), h(m, nn′) = h(m, n)h(nm, nn′), h is a biderivation, cf a rule for commutators

Ronnie Brown () Higher Structures Lisbon July 24-27, 2017 Instituto Superior T´ ecnico, Lisbon Homotopical 10 / 19

slide-63
SLIDE 63
  • 6. Squares of squares

A standard trick is that a (pushout) square of pointed spaces Z := A

  • B
  • X

Y

Ronnie Brown () Higher Structures Lisbon July 24-27, 2017 Instituto Superior T´ ecnico, Lisbon Homotopical 11 / 19

slide-64
SLIDE 64
  • 6. Squares of squares

A standard trick is that a (pushout) square of pointed spaces Z := A

  • B
  • X

Y

can be turned into

Ronnie Brown () Higher Structures Lisbon July 24-27, 2017 Instituto Superior T´ ecnico, Lisbon Homotopical 11 / 19

slide-65
SLIDE 65
  • 6. Squares of squares

A standard trick is that a (pushout) square of pointed spaces Z := A

  • B
  • X

Y

can be turned into Z := A A A A

  • A B

A B

  • A A

X X

A B

X Y

Ronnie Brown () Higher Structures Lisbon July 24-27, 2017 Instituto Superior T´ ecnico, Lisbon Homotopical 11 / 19

slide-66
SLIDE 66
  • 6. Squares of squares

A standard trick is that a (pushout) square of pointed spaces Z := A

  • B
  • X

Y

can be turned into Z := A A A A

  • A B

A B

  • A A

X X

A B

X Y a (pushout) square of squares.

Ronnie Brown () Higher Structures Lisbon July 24-27, 2017 Instituto Superior T´ ecnico, Lisbon Homotopical 11 / 19

slide-67
SLIDE 67
  • 6. Squares of squares

A standard trick is that a (pushout) square of pointed spaces Z := A

  • B
  • X

Y

can be turned into Z := A A A A

  • A B

A B

  • A A

X X

A B

X Y a (pushout) square of squares. If Z is a connected square so also are all the other vertices

  • f this square of squares.

Ronnie Brown () Higher Structures Lisbon July 24-27, 2017 Instituto Superior T´ ecnico, Lisbon Homotopical 11 / 19

slide-68
SLIDE 68
  • 6. Squares of squares

A standard trick is that a (pushout) square of pointed spaces Z := A

  • B
  • X

Y

can be turned into Z := A A A A

  • A B

A B

  • A A

X X

A B

X Y a (pushout) square of squares. If Z is a connected square so also are all the other vertices

  • f this square of squares.

Part of the van Kampen Theorem for squares gives the converse, concluding that the square Z is connected.

Ronnie Brown () Higher Structures Lisbon July 24-27, 2017 Instituto Superior T´ ecnico, Lisbon Homotopical 11 / 19

slide-69
SLIDE 69
  • 6. Squares of squares

A standard trick is that a (pushout) square of pointed spaces Z := A

  • B
  • X

Y

can be turned into Z := A A A A

  • A B

A B

  • A A

X X

A B

X Y a (pushout) square of squares. If Z is a connected square so also are all the other vertices

  • f this square of squares.

Part of the van Kampen Theorem for squares gives the converse, concluding that the square Z is connected. Considering “squares of squares”,

Ronnie Brown () Higher Structures Lisbon July 24-27, 2017 Instituto Superior T´ ecnico, Lisbon Homotopical 11 / 19

slide-70
SLIDE 70
  • 6. Squares of squares

A standard trick is that a (pushout) square of pointed spaces Z := A

  • B
  • X

Y

can be turned into Z := A A A A

  • A B

A B

  • A A

X X

A B

X Y a (pushout) square of squares. If Z is a connected square so also are all the other vertices

  • f this square of squares.

Part of the van Kampen Theorem for squares gives the converse, concluding that the square Z is connected. Considering “squares of squares”, or “cubes of cubes”, is analogous to using skeleta of CW-complexes, but allows also n-cubes of r-cubes!

Ronnie Brown () Higher Structures Lisbon July 24-27, 2017 Instituto Superior T´ ecnico, Lisbon Homotopical 11 / 19

slide-71
SLIDE 71
  • 7. A nonabelian tensor product

Ronnie Brown () Higher Structures Lisbon July 24-27, 2017 Instituto Superior T´ ecnico, Lisbon Homotopical 12 / 19

slide-72
SLIDE 72
  • 7. A nonabelian tensor product

By the algebraic part of the van Kampen Theorem for squares, applying Π to the square of squares Z gives a pushout of crossed squares of the form

Ronnie Brown () Higher Structures Lisbon July 24-27, 2017 Instituto Superior T´ ecnico, Lisbon Homotopical 12 / 19

slide-73
SLIDE 73
  • 7. A nonabelian tensor product

By the algebraic part of the van Kampen Theorem for squares, applying Π to the square of squares Z gives a pushout of crossed squares of the form

  • 1 1

1 P

  • 1 N

1 P

  • 1 1

M P

  • L N

M P

  • Ronnie Brown ()

Higher Structures Lisbon July 24-27, 2017 Instituto Superior T´ ecnico, Lisbon Homotopical 12 / 19

slide-74
SLIDE 74
  • 7. A nonabelian tensor product

By the algebraic part of the van Kampen Theorem for squares, applying Π to the square of squares Z gives a pushout of crossed squares of the form

  • 1 1

1 P

  • 1 N

1 P

  • 1 1

M P

  • L N

M P

  • What should be L?

Ronnie Brown () Higher Structures Lisbon July 24-27, 2017 Instituto Superior T´ ecnico, Lisbon Homotopical 12 / 19

slide-75
SLIDE 75
  • 7. A nonabelian tensor product

By the algebraic part of the van Kampen Theorem for squares, applying Π to the square of squares Z gives a pushout of crossed squares of the form

  • 1 1

1 P

  • 1 N

1 P

  • 1 1

M P

  • L N

M P

  • What should be L?

It has to be home for a new h : M × N → L.

Ronnie Brown () Higher Structures Lisbon July 24-27, 2017 Instituto Superior T´ ecnico, Lisbon Homotopical 12 / 19

slide-76
SLIDE 76
  • 7. A nonabelian tensor product

By the algebraic part of the van Kampen Theorem for squares, applying Π to the square of squares Z gives a pushout of crossed squares of the form

  • 1 1

1 P

  • 1 N

1 P

  • 1 1

M P

  • L N

M P

  • What should be L?

It has to be home for a new h : M × N → L. This turns out to be the universal biderivation, so we write it h : M × N → M ⊗ N, a nonabelian tensor product.

Ronnie Brown () Higher Structures Lisbon July 24-27, 2017 Instituto Superior T´ ecnico, Lisbon Homotopical 12 / 19

slide-77
SLIDE 77
  • 7. A nonabelian tensor product

By the algebraic part of the van Kampen Theorem for squares, applying Π to the square of squares Z gives a pushout of crossed squares of the form

  • 1 1

1 P

  • 1 N

1 P

  • 1 1

M P

  • L N

M P

  • What should be L?

It has to be home for a new h : M × N → L. This turns out to be the universal biderivation, so we write it h : M × N → M ⊗ N, a nonabelian tensor product. This is an algebraic example

Ronnie Brown () Higher Structures Lisbon July 24-27, 2017 Instituto Superior T´ ecnico, Lisbon Homotopical 12 / 19

slide-78
SLIDE 78
  • 7. A nonabelian tensor product

By the algebraic part of the van Kampen Theorem for squares, applying Π to the square of squares Z gives a pushout of crossed squares of the form

  • 1 1

1 P

  • 1 N

1 P

  • 1 1

M P

  • L N

M P

  • What should be L?

It has to be home for a new h : M × N → L. This turns out to be the universal biderivation, so we write it h : M × N → M ⊗ N, a nonabelian tensor product. This is an algebraic example

  • f identifications in dimensions < 3 producing structure in dimension 3.

Ronnie Brown () Higher Structures Lisbon July 24-27, 2017 Instituto Superior T´ ecnico, Lisbon Homotopical 12 / 19

slide-79
SLIDE 79

Ronnie Brown () Higher Structures Lisbon July 24-27, 2017 Instituto Superior T´ ecnico, Lisbon Homotopical 13 / 19

slide-80
SLIDE 80

Standard example: M, N ✂ P are normal subgroups of P and κ : M ⊗ N → P, m ⊗ n → [m, n]. is well defined.

Ronnie Brown () Higher Structures Lisbon July 24-27, 2017 Instituto Superior T´ ecnico, Lisbon Homotopical 13 / 19

slide-81
SLIDE 81

Standard example: M, N ✂ P are normal subgroups of P and κ : M ⊗ N → P, m ⊗ n → [m, n]. is well defined. Special case: M = N = P: the crossed square

Ronnie Brown () Higher Structures Lisbon July 24-27, 2017 Instituto Superior T´ ecnico, Lisbon Homotopical 13 / 19

slide-82
SLIDE 82

Standard example: M, N ✂ P are normal subgroups of P and κ : M ⊗ N → P, m ⊗ n → [m, n]. is well defined. Special case: M = N = P: the crossed square P ⊗ P

  • P

1

  • P

1

P

Ronnie Brown () Higher Structures Lisbon July 24-27, 2017 Instituto Superior T´ ecnico, Lisbon Homotopical 13 / 19

slide-83
SLIDE 83

Standard example: M, N ✂ P are normal subgroups of P and κ : M ⊗ N → P, m ⊗ n → [m, n]. is well defined. Special case: M = N = P: the crossed square P ⊗ P

  • P

1

  • P

1

P

gives the homotopy 3-type of SK(P, 1),

Ronnie Brown () Higher Structures Lisbon July 24-27, 2017 Instituto Superior T´ ecnico, Lisbon Homotopical 13 / 19

slide-84
SLIDE 84

Standard example: M, N ✂ P are normal subgroups of P and κ : M ⊗ N → P, m ⊗ n → [m, n]. is well defined. Special case: M = N = P: the crossed square P ⊗ P

  • P

1

  • P

1

P

gives the homotopy 3-type of SK(P, 1), allowing descriptions of π2, π3, and Whitehead product π2 × π2 → π3 as ([x], [y]) → (x ⊗ y)(y ⊗ x).

Ronnie Brown () Higher Structures Lisbon July 24-27, 2017 Instituto Superior T´ ecnico, Lisbon Homotopical 13 / 19

slide-85
SLIDE 85

Standard example: M, N ✂ P are normal subgroups of P and κ : M ⊗ N → P, m ⊗ n → [m, n]. is well defined. Special case: M = N = P: the crossed square P ⊗ P

  • P

1

  • P

1

P

gives the homotopy 3-type of SK(P, 1), allowing descriptions of π2, π3, and Whitehead product π2 × π2 → π3 as ([x], [y]) → (x ⊗ y)(y ⊗ x).

Ronnie Brown () Higher Structures Lisbon July 24-27, 2017 Instituto Superior T´ ecnico, Lisbon Homotopical 13 / 19

slide-86
SLIDE 86

Standard example: M, N ✂ P are normal subgroups of P and κ : M ⊗ N → P, m ⊗ n → [m, n]. is well defined. Special case: M = N = P: the crossed square P ⊗ P

  • P

1

  • P

1

P

gives the homotopy 3-type of SK(P, 1), allowing descriptions of π2, π3, and Whitehead product π2 × π2 → π3 as ([x], [y]) → (x ⊗ y)(y ⊗ x). So this brings the nonabelian tensor product into homotopy theory.

Ronnie Brown () Higher Structures Lisbon July 24-27, 2017 Instituto Superior T´ ecnico, Lisbon Homotopical 13 / 19

slide-87
SLIDE 87

Standard example: M, N ✂ P are normal subgroups of P and κ : M ⊗ N → P, m ⊗ n → [m, n]. is well defined. Special case: M = N = P: the crossed square P ⊗ P

  • P

1

  • P

1

P

gives the homotopy 3-type of SK(P, 1), allowing descriptions of π2, π3, and Whitehead product π2 × π2 → π3 as ([x], [y]) → (x ⊗ y)(y ⊗ x). So this brings the nonabelian tensor product into homotopy theory. My web bibliography on the nonabelian tensor product www.groupoids.org.uk/nonabtens.html now has 160 entries, dating from 1952, with most interest from group theorists, because of the commutator connection, and the fun of calculating examples.

Ronnie Brown () Higher Structures Lisbon July 24-27, 2017 Instituto Superior T´ ecnico, Lisbon Homotopical 13 / 19

slide-88
SLIDE 88
  • 8. Categorical background

The forgetful functor Φ : L N M P

  • → (M → P, N → P)

has a left adjoint

Ronnie Brown () Higher Structures Lisbon July 24-27, 2017 Instituto Superior T´ ecnico, Lisbon Homotopical 14 / 19

slide-89
SLIDE 89
  • 8. Categorical background

The forgetful functor Φ : L N M P

  • → (M → P, N → P)

has a left adjoint D : (M → P, N → P) → M ⊗ N N M P

  • Ronnie Brown ()

Higher Structures Lisbon July 24-27, 2017 Instituto Superior T´ ecnico, Lisbon Homotopical 14 / 19

slide-90
SLIDE 90
  • 8. Categorical background

The forgetful functor Φ : L N M P

  • → (M → P, N → P)

has a left adjoint D : (M → P, N → P) → M ⊗ N N M P

  • and Φ is a fibration and cofibration of categories. These aspects are

relevant to homotopical excision

Ronnie Brown () Higher Structures Lisbon July 24-27, 2017 Instituto Superior T´ ecnico, Lisbon Homotopical 14 / 19

slide-91
SLIDE 91
  • 8. Categorical background

The forgetful functor Φ : L N M P

  • → (M → P, N → P)

has a left adjoint D : (M → P, N → P) → M ⊗ N N M P

  • and Φ is a fibration and cofibration of categories. These aspects are

relevant to homotopical excision and to calculate colimits of crossed squares.

Ronnie Brown () Higher Structures Lisbon July 24-27, 2017 Instituto Superior T´ ecnico, Lisbon Homotopical 14 / 19

slide-92
SLIDE 92
  • 8. Categorical background

The forgetful functor Φ : L N M P

  • → (M → P, N → P)

has a left adjoint D : (M → P, N → P) → M ⊗ N N M P

  • and Φ is a fibration and cofibration of categories. These aspects are

relevant to homotopical excision and to calculate colimits of crossed squares. Φ also has a right adjoint of the form

Ronnie Brown () Higher Structures Lisbon July 24-27, 2017 Instituto Superior T´ ecnico, Lisbon Homotopical 14 / 19

slide-93
SLIDE 93
  • 8. Categorical background

The forgetful functor Φ : L N M P

  • → (M → P, N → P)

has a left adjoint D : (M → P, N → P) → M ⊗ N N M P

  • and Φ is a fibration and cofibration of categories. These aspects are

relevant to homotopical excision and to calculate colimits of crossed squares. Φ also has a right adjoint of the form R : (M → P, N → P) → M ×P N N M P

  • Ronnie Brown ()

Higher Structures Lisbon July 24-27, 2017 Instituto Superior T´ ecnico, Lisbon Homotopical 14 / 19

slide-94
SLIDE 94
  • 8. Categorical background

The forgetful functor Φ : L N M P

  • → (M → P, N → P)

has a left adjoint D : (M → P, N → P) → M ⊗ N N M P

  • and Φ is a fibration and cofibration of categories. These aspects are

relevant to homotopical excision and to calculate colimits of crossed squares. Φ also has a right adjoint of the form R : (M → P, N → P) → M ×P N N M P

  • Ronnie Brown ()

Higher Structures Lisbon July 24-27, 2017 Instituto Superior T´ ecnico, Lisbon Homotopical 14 / 19

slide-95
SLIDE 95
  • 9. Excision for unions of 3 sets

Ronnie Brown () Higher Structures Lisbon July 24-27, 2017 Instituto Superior T´ ecnico, Lisbon Homotopical 15 / 19

slide-96
SLIDE 96
  • 9. Excision for unions of 3 sets

Now extend Homotopical Excision from Y = X ∪ B

Ronnie Brown () Higher Structures Lisbon July 24-27, 2017 Instituto Superior T´ ecnico, Lisbon Homotopical 15 / 19

slide-97
SLIDE 97
  • 9. Excision for unions of 3 sets

Now extend Homotopical Excision from Y = X ∪ B to the case Y = X ∪ B1 ∪ B2, all open in Y .

Ronnie Brown () Higher Structures Lisbon July 24-27, 2017 Instituto Superior T´ ecnico, Lisbon Homotopical 15 / 19

slide-98
SLIDE 98
  • 9. Excision for unions of 3 sets

Now extend Homotopical Excision from Y = X ∪ B to the case Y = X ∪ B1 ∪ B2, all open in Y . We set B0 = B1 ∩ B2, Ai = X ∩ Bi, i = 0, 1, 2,

Ronnie Brown () Higher Structures Lisbon July 24-27, 2017 Instituto Superior T´ ecnico, Lisbon Homotopical 15 / 19

slide-99
SLIDE 99
  • 9. Excision for unions of 3 sets

Now extend Homotopical Excision from Y = X ∪ B to the case Y = X ∪ B1 ∪ B2, all open in Y . We set B0 = B1 ∩ B2, Ai = X ∩ Bi, i = 0, 1, 2, giving a 3-cube:

Ronnie Brown () Higher Structures Lisbon July 24-27, 2017 Instituto Superior T´ ecnico, Lisbon Homotopical 15 / 19

slide-100
SLIDE 100
  • 9. Excision for unions of 3 sets

Now extend Homotopical Excision from Y = X ∪ B to the case Y = X ∪ B1 ∪ B2, all open in Y . We set B0 = B1 ∩ B2, Ai = X ∩ Bi, i = 0, 1, 2, giving a 3-cube: Z := A0

  • A2
  • A1
  • X
  • B0
  • B2
  • B1

Y

1 2 3

  • Ronnie Brown ()

Higher Structures Lisbon July 24-27, 2017 Instituto Superior T´ ecnico, Lisbon Homotopical 15 / 19

slide-101
SLIDE 101
  • 9. Excision for unions of 3 sets

Now extend Homotopical Excision from Y = X ∪ B to the case Y = X ∪ B1 ∪ B2, all open in Y . We set B0 = B1 ∩ B2, Ai = X ∩ Bi, i = 0, 1, 2, giving a 3-cube: Z := A0

  • A2
  • A1
  • X
  • B0
  • B2
  • B1

Y

1 2 3

  • This we regard as a map of squares ∂−

3 Z → ∂+ 3 Z.

Ronnie Brown () Higher Structures Lisbon July 24-27, 2017 Instituto Superior T´ ecnico, Lisbon Homotopical 15 / 19

slide-102
SLIDE 102
  • 9. Excision for unions of 3 sets

Now extend Homotopical Excision from Y = X ∪ B to the case Y = X ∪ B1 ∪ B2, all open in Y . We set B0 = B1 ∩ B2, Ai = X ∩ Bi, i = 0, 1, 2, giving a 3-cube: Z := A0

  • A2
  • A1
  • X
  • B0
  • B2
  • B1

Y

1 2 3

  • This we regard as a map of squares ∂−

3 Z → ∂+ 3 Z.

We assume that the square ∂−

3 Z is connected.

Ronnie Brown () Higher Structures Lisbon July 24-27, 2017 Instituto Superior T´ ecnico, Lisbon Homotopical 15 / 19

slide-103
SLIDE 103
  • 9. Excision for unions of 3 sets

Now extend Homotopical Excision from Y = X ∪ B to the case Y = X ∪ B1 ∪ B2, all open in Y . We set B0 = B1 ∩ B2, Ai = X ∩ Bi, i = 0, 1, 2, giving a 3-cube: Z := A0

  • A2
  • A1
  • X
  • B0
  • B2
  • B1

Y

1 2 3

  • This we regard as a map of squares ∂−

3 Z → ∂+ 3 Z.

We assume that the square ∂−

3 Z is connected.

Now we turn Z into a map in direction 3 of squares of squares!

Ronnie Brown () Higher Structures Lisbon July 24-27, 2017 Instituto Superior T´ ecnico, Lisbon Homotopical 15 / 19

slide-104
SLIDE 104

Ronnie Brown () Higher Structures Lisbon July 24-27, 2017 Instituto Superior T´ ecnico, Lisbon Homotopical 16 / 19

slide-105
SLIDE 105

Z := A0 A0 A0 A0

  • A0 A2

A0 A2

  • A0 A0

A1 A1

  • A0 A2

A1 X

  • B0 B0

B0 B0

  • B0 B2

B0 B2

  • B0 B0

B1 B1

B0 B2

B1 Y

1 2 3

  • Ronnie Brown ()

Higher Structures Lisbon July 24-27, 2017 Instituto Superior T´ ecnico, Lisbon Homotopical 16 / 19

slide-106
SLIDE 106

Z := A0 A0 A0 A0

  • A0 A2

A0 A2

  • A0 A0

A1 A1

  • A0 A2

A1 X

  • B0 B0

B0 B0

  • B0 B2

B0 B2

  • B0 B0

B1 B1

B0 B2

B1 Y

1 2 3

  • This is now a pushout 3-cube of squares of squares.

Ronnie Brown () Higher Structures Lisbon July 24-27, 2017 Instituto Superior T´ ecnico, Lisbon Homotopical 16 / 19

slide-107
SLIDE 107

Z := A0 A0 A0 A0

  • A0 A2

A0 A2

  • A0 A0

A1 A1

  • A0 A2

A1 X

  • B0 B0

B0 B0

  • B0 B2

B0 B2

  • B0 B0

B1 B1

B0 B2

B1 Y

1 2 3

  • This is now a pushout 3-cube of squares of squares.

Ronnie Brown () Higher Structures Lisbon July 24-27, 2017 Instituto Superior T´ ecnico, Lisbon Homotopical 16 / 19

slide-108
SLIDE 108

Z := A0 A0 A0 A0

  • A0 A2

A0 A2

  • A0 A0

A1 A1

  • A0 A2

A1 X

  • B0 B0

B0 B0

  • B0 B2

B0 B2

  • B0 B0

B1 B1

B0 B2

B1 Y

1 2 3

  • This is now a pushout 3-cube of squares of squares.

By the connectivity assumption, all squares of ∂−

3 Z are connected;

Ronnie Brown () Higher Structures Lisbon July 24-27, 2017 Instituto Superior T´ ecnico, Lisbon Homotopical 16 / 19

slide-109
SLIDE 109

Z := A0 A0 A0 A0

  • A0 A2

A0 A2

  • A0 A0

A1 A1

  • A0 A2

A1 X

  • B0 B0

B0 B0

  • B0 B2

B0 B2

  • B0 B0

B1 B1

B0 B2

B1 Y

1 2 3

  • This is now a pushout 3-cube of squares of squares.

By the connectivity assumption, all squares of ∂−

3 Z are connected; then by

the 2-d excision applied to the squares ∂−

i Z for i = 1, 2 we get that

Ronnie Brown () Higher Structures Lisbon July 24-27, 2017 Instituto Superior T´ ecnico, Lisbon Homotopical 16 / 19

slide-110
SLIDE 110

Z := A0 A0 A0 A0

  • A0 A2

A0 A2

  • A0 A0

A1 A1

  • A0 A2

A1 X

  • B0 B0

B0 B0

  • B0 B2

B0 B2

  • B0 B0

B1 B1

B0 B2

B1 Y

1 2 3

  • This is now a pushout 3-cube of squares of squares.

By the connectivity assumption, all squares of ∂−

3 Z are connected; then by

the 2-d excision applied to the squares ∂−

i Z for i = 1, 2 we get that the

squares of ∂+

3 Z except for the corner are connected.

Ronnie Brown () Higher Structures Lisbon July 24-27, 2017 Instituto Superior T´ ecnico, Lisbon Homotopical 16 / 19

slide-111
SLIDE 111

Z := A0 A0 A0 A0

  • A0 A2

A0 A2

  • A0 A0

A1 A1

  • A0 A2

A1 X

  • B0 B0

B0 B0

  • B0 B2

B0 B2

  • B0 B0

B1 B1

B0 B2

B1 Y

1 2 3

  • This is now a pushout 3-cube of squares of squares.

By the connectivity assumption, all squares of ∂−

3 Z are connected; then by

the 2-d excision applied to the squares ∂−

i Z for i = 1, 2 we get that the

squares of ∂+

3 Z except for the corner are connected.

It now follows from the van Kampen Theorem for 3-cubes of squares of spaces

Ronnie Brown () Higher Structures Lisbon July 24-27, 2017 Instituto Superior T´ ecnico, Lisbon Homotopical 16 / 19

slide-112
SLIDE 112

Z := A0 A0 A0 A0

  • A0 A2

A0 A2

  • A0 A0

A1 A1

  • A0 A2

A1 X

  • B0 B0

B0 B0

  • B0 B2

B0 B2

  • B0 B0

B1 B1

B0 B2

B1 Y

1 2 3

  • This is now a pushout 3-cube of squares of squares.

By the connectivity assumption, all squares of ∂−

3 Z are connected; then by

the 2-d excision applied to the squares ∂−

i Z for i = 1, 2 we get that the

squares of ∂+

3 Z except for the corner are connected.

It now follows from the van Kampen Theorem for 3-cubes of squares of spaces that the remaining corner square is connected and that

Ronnie Brown () Higher Structures Lisbon July 24-27, 2017 Instituto Superior T´ ecnico, Lisbon Homotopical 16 / 19

slide-113
SLIDE 113

Z := A0 A0 A0 A0

  • A0 A2

A0 A2

  • A0 A0

A1 A1

  • A0 A2

A1 X

  • B0 B0

B0 B0

  • B0 B2

B0 B2

  • B0 B0

B1 B1

B0 B2

B1 Y

1 2 3

  • This is now a pushout 3-cube of squares of squares.

By the connectivity assumption, all squares of ∂−

3 Z are connected; then by

the 2-d excision applied to the squares ∂−

i Z for i = 1, 2 we get that the

squares of ∂+

3 Z except for the corner are connected.

It now follows from the van Kampen Theorem for 3-cubes of squares of spaces that the remaining corner square is connected and that Π applied to this diagram gives a 3-pushout of crossed squares.

Ronnie Brown () Higher Structures Lisbon July 24-27, 2017 Instituto Superior T´ ecnico, Lisbon Homotopical 16 / 19

slide-114
SLIDE 114

This implies the Triadic Hurewicz Theorem

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slide-115
SLIDE 115

This implies the Triadic Hurewicz Theorem If the square diagram of (X; A1, A2) is connected then H3(X; A1, A2) ( = π3(X ∪ CA1 ∪ CA2; CA1, CA2)) is

  • btained from

Ronnie Brown () Higher Structures Lisbon July 24-27, 2017 Instituto Superior T´ ecnico, Lisbon Homotopical 17 / 19

slide-116
SLIDE 116

This implies the Triadic Hurewicz Theorem If the square diagram of (X; A1, A2) is connected then H3(X; A1, A2) ( = π3(X ∪ CA1 ∪ CA2; CA1, CA2)) is

  • btained from π3(X; A1, A2) by factoring out the operations of π1(A0) and

the generalised Whitehead product.

Ronnie Brown () Higher Structures Lisbon July 24-27, 2017 Instituto Superior T´ ecnico, Lisbon Homotopical 17 / 19

slide-117
SLIDE 117

This implies the Triadic Hurewicz Theorem If the square diagram of (X; A1, A2) is connected then H3(X; A1, A2) ( = π3(X ∪ CA1 ∪ CA2; CA1, CA2)) is

  • btained from π3(X; A1, A2) by factoring out the operations of π1(A0) and

the generalised Whitehead product. Abelianisation!

Ronnie Brown () Higher Structures Lisbon July 24-27, 2017 Instituto Superior T´ ecnico, Lisbon Homotopical 17 / 19

slide-118
SLIDE 118

This implies the Triadic Hurewicz Theorem If the square diagram of (X; A1, A2) is connected then H3(X; A1, A2) ( = π3(X ∪ CA1 ∪ CA2; CA1, CA2)) is

  • btained from π3(X; A1, A2) by factoring out the operations of π1(A0) and

the generalised Whitehead product. Abelianisation! More generally, we need to know how to compute 2- and 3-pushouts of crossed squares!

Ronnie Brown () Higher Structures Lisbon July 24-27, 2017 Instituto Superior T´ ecnico, Lisbon Homotopical 17 / 19

slide-119
SLIDE 119

This implies the Triadic Hurewicz Theorem If the square diagram of (X; A1, A2) is connected then H3(X; A1, A2) ( = π3(X ∪ CA1 ∪ CA2; CA1, CA2)) is

  • btained from π3(X; A1, A2) by factoring out the operations of π1(A0) and

the generalised Whitehead product. Abelianisation! More generally, we need to know how to compute 2- and 3-pushouts of crossed squares! There are some general principles, see Appendix B of Nonabelian Algebraic Topology, but currently a

Ronnie Brown () Higher Structures Lisbon July 24-27, 2017 Instituto Superior T´ ecnico, Lisbon Homotopical 17 / 19

slide-120
SLIDE 120

This implies the Triadic Hurewicz Theorem If the square diagram of (X; A1, A2) is connected then H3(X; A1, A2) ( = π3(X ∪ CA1 ∪ CA2; CA1, CA2)) is

  • btained from π3(X; A1, A2) by factoring out the operations of π1(A0) and

the generalised Whitehead product. Abelianisation! More generally, we need to know how to compute 2- and 3-pushouts of crossed squares! There are some general principles, see Appendix B of Nonabelian Algebraic Topology, but currently a lack of lots of simple computational examples for crossed squares!

Ronnie Brown () Higher Structures Lisbon July 24-27, 2017 Instituto Superior T´ ecnico, Lisbon Homotopical 17 / 19

slide-121
SLIDE 121

This implies the Triadic Hurewicz Theorem If the square diagram of (X; A1, A2) is connected then H3(X; A1, A2) ( = π3(X ∪ CA1 ∪ CA2; CA1, CA2)) is

  • btained from π3(X; A1, A2) by factoring out the operations of π1(A0) and

the generalised Whitehead product. Abelianisation! More generally, we need to know how to compute 2- and 3-pushouts of crossed squares! There are some general principles, see Appendix B of Nonabelian Algebraic Topology, but currently a lack of lots of simple computational examples for crossed squares! We also expect further applications in homotopy theory, and surely also in geometric topology!

Ronnie Brown () Higher Structures Lisbon July 24-27, 2017 Instituto Superior T´ ecnico, Lisbon Homotopical 17 / 19

slide-122
SLIDE 122
  • 10. Conclusion

Ronnie Brown () Higher Structures Lisbon July 24-27, 2017 Instituto Superior T´ ecnico, Lisbon Homotopical 18 / 19

slide-123
SLIDE 123
  • 10. Conclusion

The above argument extends to the case Y = X ∪ B1 ∪ · · · ∪ Bn.

Ronnie Brown () Higher Structures Lisbon July 24-27, 2017 Instituto Superior T´ ecnico, Lisbon Homotopical 18 / 19

slide-124
SLIDE 124
  • 10. Conclusion

The above argument extends to the case Y = X ∪ B1 ∪ · · · ∪ Bn. In this talk I have tried to indicate the flexibility and potential of the stated methodology for obtaining new precise results on homotopy types and so on homotopy invariants. It opens up lots of possibilities!

Ronnie Brown () Higher Structures Lisbon July 24-27, 2017 Instituto Superior T´ ecnico, Lisbon Homotopical 18 / 19

slide-125
SLIDE 125
  • 10. Conclusion

The above argument extends to the case Y = X ∪ B1 ∪ · · · ∪ Bn. In this talk I have tried to indicate the flexibility and potential of the stated methodology for obtaining new precise results on homotopy types and so on homotopy invariants. It opens up lots of possibilities! It was not till 1993 that I realised that I could not do some simple calculations with induced crossed modules, and asked for help from Chris

  • Wensley. This resulted in three joint papers, and a Chapter in the NAT

book.

Ronnie Brown () Higher Structures Lisbon July 24-27, 2017 Instituto Superior T´ ecnico, Lisbon Homotopical 18 / 19

slide-126
SLIDE 126
  • 10. Conclusion

The above argument extends to the case Y = X ∪ B1 ∪ · · · ∪ Bn. In this talk I have tried to indicate the flexibility and potential of the stated methodology for obtaining new precise results on homotopy types and so on homotopy invariants. It opens up lots of possibilities! It was not till 1993 that I realised that I could not do some simple calculations with induced crossed modules, and asked for help from Chris

  • Wensley. This resulted in three joint papers, and a Chapter in the NAT

book. Now I need some help, or independent work, on simple basic examples on pushouts and induced crossed squares, and work on higher dimensions!

Ronnie Brown () Higher Structures Lisbon July 24-27, 2017 Instituto Superior T´ ecnico, Lisbon Homotopical 18 / 19

slide-127
SLIDE 127
  • 10. Conclusion

The above argument extends to the case Y = X ∪ B1 ∪ · · · ∪ Bn. In this talk I have tried to indicate the flexibility and potential of the stated methodology for obtaining new precise results on homotopy types and so on homotopy invariants. It opens up lots of possibilities! It was not till 1993 that I realised that I could not do some simple calculations with induced crossed modules, and asked for help from Chris

  • Wensley. This resulted in three joint papers, and a Chapter in the NAT

book. Now I need some help, or independent work, on simple basic examples on pushouts and induced crossed squares, and work on higher dimensions! I think this should be related to work on higher rewriting, on which there are a couple of conferences this coming September, in Oxford and in Marseilles-Luminy.

Ronnie Brown () Higher Structures Lisbon July 24-27, 2017 Instituto Superior T´ ecnico, Lisbon Homotopical 18 / 19

slide-128
SLIDE 128

Some starter references

Ronnie Brown () Higher Structures Lisbon July 24-27, 2017 Instituto Superior T´ ecnico, Lisbon Homotopical 19 / 19

slide-129
SLIDE 129

Some starter references

Brown, R. and Loday, J.-L. “Van Kampen theorems for diagrams of spaces”. Topology 26 (3) (1986) 311–335. With an appendix by M. Zisman. Brown, R. and Loday, J.-L. “Homotopical excision, and Hurewicz theorems, for n-cubes of spaces”. Proc. London Math. Soc. (3) 54 (1) (1987) 176–192. Brown, R. “Computing homotopy types using crossed n-cubes of groups”. In ‘Adams Memorial Symposium on Algebraic Topology, 1’ (Manchester, 1990), London Math. Soc. Lecture Note Ser., Volume 175. Cambridge

  • Univ. Press, Cambridge (1992), 187–210.

Ronnie Brown () Higher Structures Lisbon July 24-27, 2017 Instituto Superior T´ ecnico, Lisbon Homotopical 19 / 19