a (brief) history of homotopy theoryweb.stanford.edu/~vogti/hismathseminar_homotopytheory.pdf ·...
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A (Brief) History of Homotopy Theory
Isabel Vogt
April 26, 2013
Motivation
Why I’m giving this talk:
“Dealing with ideas in the form they were firstdiscovered often shines a light on the primalmotivation for them (...) Why did anyone dream upthe notion of homotopy, and homotopy groups?”
–Mazur
Why you might be interested in listening:
Homotopy as a tool preceds homotopy as a concept
Homotopy groups were very elusive
Ushers in transition from analysis to topology
Isabel Vogt A (Brief) History of Homotopy Theory
What is Homotopy?
A continuousdeformation fromone path to theother
Red and Blue curves: the images of amaps
f, g : [0, 1] = Y → X
f and g are homotopic (as maps fromY into X) if there exists a family of ctsmaps ht for t ∈ [0, 1] such that
h0 = f, h1 = g
∀x ∈ [0, 1], t 7→ ht(x) continuous
Isabel Vogt A (Brief) History of Homotopy Theory
What is Homotopy?
f, g : X → Y , are homotopic ⇔
∃H : X × [0, 1]→ Y continuous
s.t. H(x, 0) = f(x), H(x, 1) = g(x)
Homotopy is an equivalence relation.
t = 0 t = 1
+
t = 0 t = 1
=
0 1/2 1
It is very important to remember this is dependent on thetopological spaces X → Y
Isabel Vogt A (Brief) History of Homotopy Theory
Homotopy Groups
Now consider based homotopy classes of maps of the sphere intothe space X:
π1(X,x0) = [S1, ∗;X,x0]
Why does this form a group:
e : S1 → x0 : the constant map is an identity
f−1 : indicates transversing f in the opposite direction
[f ][g] = [f · g] : indicates transversing first f and then g
can check associativity
all of these respect homotopy
Isabel Vogt A (Brief) History of Homotopy Theory
Origins of the concept of homotopy and the fundamental group
Analysis
Cauchy and mobility of path, 1825Riemann and connectivity, 1851Jordan and deformations of curves, 1866-1882
Analysis Situs
Poincare and a definition of π1 of a manifold, 1892
Isabel Vogt A (Brief) History of Homotopy Theory
Higher homotopy groups
Hopf, and a nontrivial map S3 → S2 , 1931
Cech, introduction of abstract homotopy groups, 1932
Hurewicz, higher homotopy groups and homotopyequivalence, 1935
Eilenberg and obstruction theory, 1940
Isabel Vogt A (Brief) History of Homotopy Theory
A summary
Cauchy, 1825
Riemann, 1851
Jordan, 1866-1882
Poincare, 1892
Hopf, 1931
Cech, 1932
Hurewicz, 1935
Eilenberg, 1940
Isabel Vogt A (Brief) History of Homotopy Theory
A summary
Cauchy, 1825
Riemann, 1851
Jordan, 1866-1882
Poincare, 1892
Hopf, 1931
Cech, 1932
Hurewicz, 1935
Eilenberg, 1940
What’s going on?
Hmmm....
Oh.
Isabel Vogt A (Brief) History of Homotopy Theory
The First Uses of Homotopy
Want to integrate some complex function f between theseendpoints, does the path matter?
Gauss and Poisson both note ∼ 1815 that it can!
Isabel Vogt A (Brief) History of Homotopy Theory
Cauchy’s Work on Integration
I =
∫ X+iY
x0+iy0
f(z)dz
Identify complex numbers with points in the plane
Introduce a “mobile curve” joining x0 + iy0 and X + iY
x = φ(t), y = χ(t), monotone functions of t, continuouslydifferentiable
I = A+ iB =
∫ T
t0
f(φ(t) + iχ(t))[φ′(t) + iχ′(t)
]dt
Theorem
The result is independent of the choice of φ and χ if f iscomplex differentiable for x0 ≤ x ≤ X, y0 ≤ y ≤ Y
Isabel Vogt A (Brief) History of Homotopy Theory
Cauchy’s Work on Integration
“If one wants to pass from one curve to another,which is not infinitely near the first, one can imagine athird mobile curve, which is variable in its shape, andhave it coincide successively and at different instanceswith both fixed curves.”
Isabel Vogt A (Brief) History of Homotopy Theory
Riemann and Connectivity
Definition
1 A surface is simply-connected if every cross-cut (interiorarc joining boundaries) on the surface divides the surface.
2 A surface has connectivity number n if n− 1 cross-cutsturn it into a simply-connected surface.
surface connectivity number
sphere 1torus 3
g-hole torus 2g + 1
Note: this is not in general equivalent to saying a space isn-connected using πn = 0!
Isabel Vogt A (Brief) History of Homotopy Theory
Riemann and Connectivity
Simply ConnectedIt does coincide with our standard definition of simplyconnected (π1(X) = 0)
By classification of surfaces, we only have the plane and thesphere that are simply connected ⇒ Jordan curve theorem
The quantifier is very necessary, there are even notnull-homotopic crosscuts that divide a surface which is notsimply connected
Isabel Vogt A (Brief) History of Homotopy Theory
Jordan and deformations of curves
In 1966, published a paper on closed curves on surfaces:
Definition
Any two closed contours, drawn on a given surface, are calledreducible into one another, if one can pass from one to the otherby a progressive deformation.
“Any two contours drawn inthe plane are reducible to one an-other; however this is not true onany surface: for instance, on atorus a meridian and a parallelare two irreducible contours.”
Isabel Vogt A (Brief) History of Homotopy Theory
Elementary Contours
S
A
C ′0
C ′′0
C ′1
C ′′1
P
b
Γ0 Γ1
•
•
•a0 •a1
Isabel Vogt A (Brief) History of Homotopy Theory
Elementary Contours
Figure: Punctured 2-hole torus
n : the maximal number of non-intersecting closed curves thatdo not divide the surface (what we call the genus)
Isabel Vogt A (Brief) History of Homotopy Theory
Elementary Contours
S
C ′0C ′′0
C ′1C ′′1
•a0 •
a1
Figure: Cut at these curves
C0, ..., Cn : the maximal curves that do not divide the surfaceC ′i and C ′′i : the two “sides” after the cuta0, ..., an : points on each curve
Isabel Vogt A (Brief) History of Homotopy Theory
Elementary Contours
S
C ′0C ′′0
C ′1C ′′1
Γ0 Γ1•a0 •
a1
Figure: Cut at the curves Γi as well
Γ0, ...,Γn : closed curves through the ai
Isabel Vogt A (Brief) History of Homotopy Theory
Elementary Contours
S
A
C ′0C ′′0
C ′1C ′′1b
Γ0 Γ1
••a0 •
a1
Figure: Choose a point on each boundary curve
b0, ..., bm : points on the boundary curves A0...Am
Isabel Vogt A (Brief) History of Homotopy Theory
Elementary Contours
S
A
C ′0C ′′0
C ′1C ′′1
P
b
Γ0 Γ1
•
••a0 •
a1
Figure: Choose a point P and connect it to the ai and bi
P : point on the surface
Isabel Vogt A (Brief) History of Homotopy Theory
Elementary Contours
Three types of “elementary contours”:
•
[PaiCiaiP ][Ci]
•
[PbiAibiP ][Ai]
•
[PaiΓiaiP ][Γi]
Isabel Vogt A (Brief) History of Homotopy Theory
Jordan’s Idea
Claim (Jordan)
Every closed contour on the surface S is reducible to a uniquesequence of elementary contours.
In fact, he considers free deformations, so the sequence ofelementary contours must allow cyclic permutations
In hindsight, he has obtained a set of generators of π1S forS a genus n orientable surface with m boundary curves
With the relation:
[A0]...[Am−1][C0][Γ0][C0]−1[Γ0]
−1...[Cn−1][Γn−1][Cn−1]−1[Γn−1]
−1 ' 1
Isabel Vogt A (Brief) History of Homotopy Theory
Why didn’t he realize he wrote down generators for thefundamental group?
Isabel Vogt A (Brief) History of Homotopy Theory
Why didn’t he realize he wrote down generators for thefundamental group?
He lacked:
Continuous deformation of based loops (only requires theelementary contours to go through the point P )
Relation between “elementary contours”
The abstract group concept had not yet been formulated!
It is not obvious how to interpret the fundamental group asa permutation group
Isabel Vogt A (Brief) History of Homotopy Theory
Why didn’t he realize he wrote down generators for thefundamental group?
He lacked:
Continuous deformation of based loops (only requires theelementary contours to go through the point P )
Relation between “elementary contours”
The abstract group concept had not yet been formulated!
It is not obvious how to interpret the fundamental group asa permutation group
Isabel Vogt A (Brief) History of Homotopy Theory
A Classification Theorem
Theorem (Jordan, 1866)
Two orientable surfaces with boundaries are homeomorphic ifand only if they have the same genus and the same number ofboundary curves.
His terminology for homeomorphic: “applicable, one to theother without tearing or duplication”
Isabel Vogt A (Brief) History of Homotopy Theory
The Transition to Analysis Situs
The theory of integration provides an abelian structure∫α·β
f =
∫αf +
∫βf =
∫β·α
f
But if we integrated a multi-valued function this might notbe the case!
The permutations of values of a multi-valued functionalong α · β need not be the same as along β · αQuestions of underlying topology of a space began to bestudied in their own right!
Isabel Vogt A (Brief) History of Homotopy Theory
The Transition to Analysis Situs
The theory of integration provides an abelian structure∫α·β
f =
∫αf +
∫βf =
∫β·α
f
But if we integrated a multi-valued function this might notbe the case!
The permutations of values of a multi-valued functionalong α · β need not be the same as along β · αQuestions of underlying topology of a space began to bestudied in their own right!
Isabel Vogt A (Brief) History of Homotopy Theory
The Transition to Analysis Situs
The theory of integration provides an abelian structure∫α·β
f =
∫αf +
∫βf =
∫β·α
f
But if we integrated a multi-valued function this might notbe the case!
The permutations of values of a multi-valued functionalong α · β need not be the same as along β · α
Questions of underlying topology of a space began to bestudied in their own right!
Isabel Vogt A (Brief) History of Homotopy Theory
The Transition to Analysis Situs
The theory of integration provides an abelian structure∫α·β
f =
∫αf +
∫βf =
∫β·α
f
But if we integrated a multi-valued function this might notbe the case!
The permutations of values of a multi-valued functionalong α · β need not be the same as along β · αQuestions of underlying topology of a space began to bestudied in their own right!
Isabel Vogt A (Brief) History of Homotopy Theory
Poincare and the Fundamental Group
Buildup to the fundamental group :
Consider unbranched multi-valued functions Fi on amanifold
If the functions are continued around a loop, they undergoa permutation
He shows, permutations along closed paths on a manifoldform a group
Depends on the functions Fi !
Let G be group of all such functions
Isabel Vogt A (Brief) History of Homotopy Theory
Poincare and the Fundamental Group
Buildup to the fundamental group :
Consider unbranched multi-valued functions Fi on amanifold
If the functions are continued around a loop, they undergoa permutation
He shows, permutations along closed paths on a manifoldform a group
Depends on the functions Fi !
Let G be group of all such functions
Isabel Vogt A (Brief) History of Homotopy Theory
Poincare and the Fundamental Group
Introduces null-homotopic paths:
If the point M describes an infinitely smallcontour on the manifold, the functions F willreturn to their original values. This remains trueif M describes a loop on the manifold, that is tosay, if it varies from M0 to M1 following anarbitrary path M0BM1, then describes aninfinitely small contour and returns from M1 toM0 traversing the same path M1BM0.
Composition of paths transversed in opposite directions:
M0AM1BM0 +M0BM1CM0 ≡M0AM1CM0
Emphasizes that M0AM1CM0 6≡M0CM1AM0
Isabel Vogt A (Brief) History of Homotopy Theory
Poincare and the Fundamental Group
Introduces null-homotopic paths:
If the point M describes an infinitely smallcontour on the manifold, the functions F willreturn to their original values. This remains trueif M describes a loop on the manifold, that is tosay, if it varies from M0 to M1 following anarbitrary path M0BM1, then describes aninfinitely small contour and returns from M1 toM0 traversing the same path M1BM0.
Composition of paths transversed in opposite directions:
M0AM1BM0 +M0BM1CM0 ≡M0AM1CM0
Emphasizes that M0AM1CM0 6≡M0CM1AM0
Isabel Vogt A (Brief) History of Homotopy Theory
Poincare and the Fundamental Group
Introduces null-homotopic paths:
If the point M describes an infinitely smallcontour on the manifold, the functions F willreturn to their original values. This remains trueif M describes a loop on the manifold, that is tosay, if it varies from M0 to M1 following anarbitrary path M0BM1, then describes aninfinitely small contour and returns from M1 toM0 traversing the same path M1BM0.
Composition of paths transversed in opposite directions:
M0AM1BM0 +M0BM1CM0 ≡M0AM1CM0
Emphasizes that M0AM1CM0 6≡M0CM1AM0
Isabel Vogt A (Brief) History of Homotopy Theory
But...
Even Poincare gets some stuff wrong
M0BM0 ≡ 0 if the closed contour M0BM0
constitutes the complete boundary of a 2-dimensionalmanifold contained in the the manifold.
But he latter corrects it:
K ≡ 0 mod V ⇔ there is a simply connected region in V ofwhich K is boundary
Isabel Vogt A (Brief) History of Homotopy Theory
But...
Even Poincare gets some stuff wrong
M0BM0 ≡ 0 if the closed contour M0BM0
constitutes the complete boundary of a 2-dimensionalmanifold contained in the the manifold.
But he latter corrects it:
K ≡ 0 mod V ⇔ there is a simply connected region in V ofwhich K is boundary
Isabel Vogt A (Brief) History of Homotopy Theory
But...
Even Poincare gets some stuff wrong
M0BM0 ≡ 0 if the closed contour M0BM0
constitutes the complete boundary of a 2-dimensionalmanifold contained in the the manifold.
But he latter corrects it:
K ≡ 0 mod V ⇔ there is a simply connected region in V ofwhich K is boundary
Isabel Vogt A (Brief) History of Homotopy Theory
The Fundamental Group
“In this way, on can imagine a group G satisfying the followingconditions:
1 For each closed contour M0BM0 there is a correspondingsubstitution S of the group
2 S reduces to the identical substitution if and onlyM0BM0 ≡ 0
3 If S and S′ correspond to the contours C and C ′ and ifC ′′ = C + C ′, the substitution corresponding to C ′′ will beSS′
This group G will be called the fundamental group of themanifold V . ”
Isabel Vogt A (Brief) History of Homotopy Theory
Why Higher Homotopy Groups?
Good question!
Vienna, 1931
Cech presents a description of higherhomotopy groups
πnX := [Sn, ∗;X,x0]
No applications for the homotopygroups
Only one theorem
They were abelian (for n ≥ 2)
Isabel Vogt A (Brief) History of Homotopy Theory
Why Higher Homotopy Groups?
Good question!
Vienna, 1931
Cech presents a description of higherhomotopy groups
πnX := [Sn, ∗;X,x0]
No applications for the homotopygroups
Only one theorem
They were abelian (for n ≥ 2)
Isabel Vogt A (Brief) History of Homotopy Theory
Why Higher Homotopy Groups?
Persuaded by others that they could not possibly containany additional information above the already knownabelian homology groups
Cech actually withdrew his paper
π1X encompasses more information than its abeliancounterpart H1(X)
H1(X;Z) ' π1X/[π1X,π1X]
Isabel Vogt A (Brief) History of Homotopy Theory
Why Higher Homotopy Groups? - In Hindsight
There’s interesting stuff going on: Hopf fibration
Compare to H∗(Sn) = 0 for ∗ > n
Action of the fundamental group on higher homotopygroups
Eilenberg’s obstruction theory
Isabel Vogt A (Brief) History of Homotopy Theory
Hurewicz and a redefinition, 1935
Let Ω(X,x0) be the loop space: set of based loops
S1 → X
with basepointx1 : S1 → x0
and the compact-open topology.
Definition/Proposition
1 Ωp(X,x0) = Ω(Ωp−1 (X,x0) , xp−1
)2 πp(X,x0) = π1
(Ωp−1 (X,x0) , xp−1
)
Isabel Vogt A (Brief) History of Homotopy Theory
An Action of π1 on πn
Given a path α : [0, 1]→ X with endpoints a, b ∈ X, induces anisomorphism
πn(X, a) ' πn(X, b)
Depends only on the homotopy class of the map.
π1(X) acts by automorphisms on every πn(X,x0)
Isabel Vogt A (Brief) History of Homotopy Theory
Homotopy Groups of Spheres
Brouwer: 1912: degrees of maps on a sphere
[f ]∼←→ degf
Hopf: 1925-1930: maps of spheres into spheres
“...may righty be called the starting point ofhomotopy theory”
–Dieudonne
The Hopf fibration: S3 p−→ S2
Hurewicz: 1935: πmS1 = 0 for m ≥ 2
Freudenthal: 1937: homotopy suspension
πi(Sn) ' πi+1(S
n+1) : i < 2n− 1
Isabel Vogt A (Brief) History of Homotopy Theory
Brouwer and Degree
Let f : Sn → Sn, then
f∗ : Hn(Sn)→ Hn(Sn)
given byα ∈ Z 7→ dα
then, deg f = d
Brower’s definition:Involves simplicial approximation andcounting
Theorem (Brouwer)
The degree of a map is invariant under homotopy.
Isabel Vogt A (Brief) History of Homotopy Theory
Brouwer and Degree
At ICM 1912, conjectured that the converse was also true:
Conjecture
For M a connected, compact, orientable n-dimensionalmanifold, and f and g two continuous maps
M → Sn
of the same degree, then f ' g.
Published a proof for M = S2
Incredibly long, dense, intricate, and imprecise!
4 reductions to finally apply a result of Klein on compactRiemann surfaces of genus 0
Questionable arguments
Isabel Vogt A (Brief) History of Homotopy Theory
Hopf and maps of spheres
Proved Hopf’s conjecture
⇒ [f ]∼←→ degf
⇒ πn(Sn)∼−→ Z
Introduced the Hopf invariant H(f)
Used that to prove that
π3(S2) ' Z
Isabel Vogt A (Brief) History of Homotopy Theory
The Hopf Fibration, 1931
S1 −→ S3 p−→ S2
Direct construction:Identify R4 with C2 and R3 with C× R
S3 := (z0, z1) : |z0|2 + |z1|2 = 1S2 := (z, x) : |z|2 + x2 = 1p(z0, z1) = (2z0z1, |z0|2 − |z1|2)
Clearly maps to S2, can check that
p(z0, z1) = p(w0, w1)⇔ (w0, w1) = λ(z0, z1), |λ| = 1
Isabel Vogt A (Brief) History of Homotopy Theory
The Hopf Fibration, 1931
S1 −→ S3 p−→ S2
Direct construction:Identify R4 with C2 and R3 with C× R
S3 := (z0, z1) : |z0|2 + |z1|2 = 1S2 := (z, x) : |z|2 + x2 = 1p(z0, z1) = (2z0z1, |z0|2 − |z1|2)
Clearly maps to S2, can check that
p(z0, z1) = p(w0, w1)⇔ (w0, w1) = λ(z0, z1), |λ| = 1
Isabel Vogt A (Brief) History of Homotopy Theory
Freudenthal and stable homotopy groups
The based (reduced) suspension of X, ΣX is defined as
ΣX = X × [0, 1]/(X × 0 ∪X × 1 ∪ x0 × [0, 1])
There is a natural bijection:
[X,x0; ΩY, y1]∼−→ [ΣX,x0;Y, y0]
(Σ and Ω are adjoint functors)
Isabel Vogt A (Brief) History of Homotopy Theory
Freudenthal and stable homotopy groups
[X,x0; ΩY, y1]∼−→ [ΣX,x0;Y, y0]
We also have a natural map (Y, y0)→ (ΩΣY, y1)
[X,x0;Y, y0] −→ [X,x0; ΩΣY, y1]
Putting the two together:
E : [X,x0;Y, y0] −→ [ΣX,x0; ΣY, y0]
In particular:
E : πr(Sn)→ πr+1(S
n+1)
Freudenthal showed that this is an isomorphism for r < 2n− 1and surjective for r = 2n− 1
Isabel Vogt A (Brief) History of Homotopy Theory
Freudenthal and stable homotopy groups
Which means:
πr(Sn)
E−→ πr+1(Sn+1)...
E−→ πr+k(Sn+k)...
Are isomorphisms for k > r − 2n+ 1
The homotopy groups of spheres stabilize!
Isabel Vogt A (Brief) History of Homotopy Theory
Freudenthal and stable homotopy groups
Which means:
πr(Sn)
E−→ πr+1(Sn+1)...
E−→ πr+k(Sn+k)...
Are isomorphisms for k > r − 2n+ 1
The homotopy groups of spheres stabilize!
Isabel Vogt A (Brief) History of Homotopy Theory
Samuel Eilenberg
Figure: Eilenberg
Isabel Vogt A (Brief) History of Homotopy Theory
Samuel Eilenberg
Figure: Hmmm...?
Isabel Vogt A (Brief) History of Homotopy Theory
Samuel Eilenberg
Figure: Eilenberg
Isabel Vogt A (Brief) History of Homotopy Theory
Eilenberg ⊆ Bourbaki
On homotopy groups and fibre spaces
Eilenberg +MacLane
Met in 1940 in Ann Arbor, wrote 15 papers together until1954
Introduced category theory, the concepts of Hom, Ext,functor, natural transformation
Cohomology of groups
The relation between homotopy and homology
Eilenberg + Steenrod
Axiomatized homology and cohomology
Eilenberg + Cartan
Homological Algebra
Isabel Vogt A (Brief) History of Homotopy Theory
Eilenberg Obstruction Theory
Given a mapX1 −→ Y
If Y is simply connected this extends to a map on X2.
Null-homotopy in Y gives a way to fill in 2-skeleton.
This generalizes:
Have a map defined on Xn, and (n+ 1)-cell σ
Attaching map gσ : Sn → Xn
f extends to σ if and only if f gσ is null-homotopic
Ie if the cochain c(f) : σ → [f gσ] ∈ Cn+1(X;πn(Y )) iszero
c(f): the obstruction cocycle
The immediate result: this is always possible if πn(Y ) = 0
Isabel Vogt A (Brief) History of Homotopy Theory
References
“History of Topology” edited by I.M. James
“A Brief, Subjective History of Homology and HomotopyTheory in This Century” by Peter Hilton
“A History of Algebraic and Differential Topology” byDieudonne
Isabel Vogt A (Brief) History of Homotopy Theory