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Simple Homotopy, Whitehead Groups, and Torsion
1 · Prerequisites
- Abelian Categories
- Binary Operations, Monoids, Groups and Subgroups
- Cardinal Arithmetic, Cofinality and the Alephs
- Categories, Functors and Natural Transformations
- Chain Complexes and Homology
- Chain Homotopy and the Homotopy Category
- Compactness
- Compactness in Metric Spaces
- Completeness, Completion, and Uniform Continuity
- Connectedness
- Construction of the Natural Numbers
- Construction of the Real Numbers via Cauchy Sequences
- Construction of the Real Numbers via Dedekind Cuts
- Continuity, IVT, EVT, and Uniform Continuity
- Cosets, Index and Lagrange's Theorem
- Countability and Uncountability
- Covering Spaces and Lifting
- Cw Complexes and Cellular Homology
- Determinants of Matrices over a Commutative Ring
- Divisibility, Euclidean Domains, Principal Ideal Domains and Unique Factorisation
- Dual Spaces, Bilinear and Quadratic Forms, and Sylvester's Law of Inertia
- Exactness and the Member Calculus
- Filters and Ultrafilters
- Finite Counting, Factorials and Binomial Coefficients
- Foundations of the Real Numbers for Analysis
- Free Groups and Presentations
- Free Modules, Exact Sequences, Projective and Injective Modules
- Function Space Topologies and the Exponential Law
- Gaussian Elimination, Elementary Matrices and Reduced Row Echelon Form
- Group Actions, Orbits, Stabilisers and Cayley's Theorem
- Group Homomorphisms and the Isomorphism Theorems
- Hausdorff via the Diagonal
- Higher Homotopy Groups and Cofiber Sequences
- Homology Axioms Degree and Classical Applications
- Homotopy and Homotopy Equivalence
- Hurewicz Whitehead Freudenthal and Cw Approximation
- Ideals, Quotient Rings and the Isomorphism Theorems for Rings
- Inner Product Spaces, Gram-Schmidt, Projections and Adjoints
- Limits and Colimits
- Limits of Real Functions
- Linear Independence, Bases and Dimension
- Linear Transformations, Rank-Nullity and Quotient Spaces
- Long Exact Sequences in Homology
- Mapping Cones Cylinders and Chain Triangles
- Metric Spaces
- Modules, Submodules, Quotient Modules and the Isomorphism Theorems
- Monotone Sequences, Bolzano-Weierstrass, and Cauchy Completeness
- Normal Subgroups and Quotient Groups
- Order, Zorn's Lemma, and the Axiom of Choice
- Ordinal Arithmetic and the First Uncountable Ordinal
- Ordinals, Cardinals, and Transfinite Recursion
- Partitions of Unity and Paracompactness
- Polynomial Rings, the Division Algorithm and Roots
- Preadditive and Additive Categories and Biproducts
- Reflective Subcategories and the Adjoint Functor Theorems
- Relations, Functions, and Quotients
- Relative Homology Excision and Mayer Vietoris
- Rings, Subrings, Integral Domains and Fields
- Rⁿ as a Normed Space; Vector-Valued Functions
- Roots, Rational Powers, and Classical Inequalities
- Separation Axioms: the Hierarchy
- Sequences and Limits
- Simple Field Extensions and the Construction of the Complex Numbers
- Simplicial Complexes and Simplicial Homology
- Simplicial Subdivision and Simplicial Approximation
- Singular Chains and Singular Homology
- Subspaces, Products, and Quotients
- Suprema and Infima
- Symmetric Groups, Cycle Decomposition and the Sign Homomorphism
- Tensor Products of Modules
- The Cantor Set, Baire Category, and Measure Zero in ℝ
- The Diagram Lemmas in an Abelian Category
- The Fundamental Group
- The Group Algebra and Representations of Finite Groups
- The Seifert–van Kampen Theorem
- The Topology of Euclidean Space
- The ZFC Axioms and the Basic Set Constructions
- Topological Spaces and Continuity
- Topology of ℝ
- Universal Properties, Representables and the Yoneda Lemma
- Vector Spaces, Linear Subspaces, Span and Direct Sums
2 · Summary
Simple homotopy refines homotopy equivalence of finite CW complexes by recording whether a map is built from finitely many elementary cell expansions and collapses. On the algebraic side, based universal-cover cellular chains are finite free right -modules; their contractible mapping cones define Whitehead torsion in . The module, matrix and sign conventions are fixed in the items before torsion is used.
The forward implication is immediate from the two-cell calculation and the composition formula. The converse is geometric. A finite relative homotopy equivalence is traded into two high consecutive cell degrees. Its relative homotopy boundary is an invertible group-ring matrix. Homotopies of attaching maps and finite collar expansions realize the stable elementary changes needed to turn a zero-torsion matrix into the identity; a final homotopy-level correction makes each matching lower cell a genuine free face. This proves the inclusion case before applying the cellular mapping cylinder to an arbitrary finite CW homotopy equivalence.
The page also constructs, for every Whitehead class, a finite CW inclusion realizing it. All construction and Whitehead-theorem uses here are finite; no Axiom of Choice is invoked. Smooth handles, Whitney tricks and the smooth -cobordism theorem lie outside this page.
3 · Logical flowchart
4 · Definitions, theorems and proofs
Elementary expansions and collapses of finite CW complexes
Definition
Let be a finite CW complex and let . Write for the closed unit ball, for its boundary sphere, and for a closed upper hemisphere of .
An elementary expansion of of dimension is an inclusion of CW complexes together with a homeomorphism of ball pairs and a continuous map such that
- is a characteristic map for a new -cell ,
- is a characteristic map for a new -cell ,
- the remaining boundary is old: , and
- as a CW complex, with a subcomplex.
The new -cell is called the free face of the new -cell. The restriction of to maps its interior homeomorphically onto and maps its boundary into ; it need not be a homeomorphism onto the closed cell, whose attaching map may identify boundary points. The complementary boundary of maps into . In particular, an attachment of only one -cell to a complex already containing the alleged free face is not an elementary expansion under this definition.
We say that collapses to by an elementary collapse and write when is an elementary expansion; the elementary collapse is the inverse formal operation removing the pair . A finite sequence of elementary expansions and elementary collapses, each performed relative to the cells retained by the previous steps, is a formal deformation; when every cell of a subcomplex is retained throughout, the deformation is written relative to , and the operations are then said to fix the retained subcomplex. The one-cell case attaches a new vertex and a new edge joining it to an old vertex, the new vertex being the free face.
Simple homotopy equivalence
Definition
Let and be finite CW complexes. A map is a simple homotopy equivalence if it is homotopic to a finite composite of maps between finite CW complexes in which each is either an elementary expansion inclusion, an elementary collapse map (Elementary expansions and collapses of finite CW complexes), or a cellular isomorphism. A cellular isomorphism here means a homeomorphism that carries the cell structure of its source isomorphically onto the cell structure of its target, so that it restricts to a homeomorphism between the interiors of corresponding cells; a general homeomorphism is not included by definition.
For a formal collapse , an elementary collapse map means any retraction of its expansion inclusion . Such maps exist: the characteristic ball strongly deformation retracts onto the complementary boundary disk, fixing that disk pointwise. This deformation descends through the attaching identifications to a strong deformation retraction of onto . If is its endpoint and is any retraction, composing this deformation with gives relative to . Thus and .
Every such composite is a homotopy equivalence (Homotopy equivalences, homotopy inverses and spaces of the same homotopy type): an expansion inclusion and its collapse map are homotopy inverses, and a cellular isomorphism is a homeomorphism. Consequently every simple homotopy equivalence is a homotopy equivalence.
For disconnected complexes the sequence respects the induced bijection on components: each operation is performed componentwise, and the composite maps the components of bijectively onto those of . The empty complex is allowed; the empty sequence exhibits the identity of a finite CW complex as a simple homotopy equivalence.
Homotopy of maps is transitive, so any map homotopic to a simple homotopy equivalence is again a simple homotopy equivalence. Concatenating two finite composites exhibits a composite of two simple homotopy equivalences as a simple homotopy equivalence as well.
Stable general linear and elementary groups for right modules
Definition
Throughout, is an associative unital ring, not assumed commutative (Ring: an abelian group under addition and a monoid under multiplication, with multiplication distributing over addition on both sides). For let be the set of column vectors with , made into a right -module by entrywise addition and the right action (Unital left and right modules over a ring; unqualified module means left module); for this is the zero module, whose unique element is the empty column. A map is right -linear when and .
Matrices. Every right-linear has a unique matrix , written , such that the sum being the finite sum in the additive group of ; uniqueness uses that the standard basis vectors of generate it and that columns of are the coordinate vectors of . If has matrix , then has matrix , with ; this is the displayed order and it uses only associativity and distributivity.
General linear group. Let be the group of matrices over possessing a two-sided inverse, with multiplication of matrices as the group operation and as the identity; by the previous paragraph is exactly the group of right-linear automorphisms of . The stabilization identifies with a subgroup of , and is the stable general linear group, in which every element is represented by some matrix. A matrix belongs to when there is a matrix satisfying both and ; either equation alone need not imply the other over an arbitrary unital ring. No determinant, commutativity, or rank function is used anywhere in this definition.
For a concrete one-sided inverse, take where has basis . Let and let , . Then , while , so the matrices and satisfy but not .
Elementary matrices. For , with and , let be the matrix with entry in position and elsewhere, and let be the corresponding elementary matrix. It is invertible with two-sided inverse , because and hence . Let be the subgroup of generated by all elementary matrices in for , and set . Let be the stable elementary subgroup, the subgroup of generated by the images of all elementary matrices. Elementary matrices are stable in the same way: in is the image of the elementary matrix with the same indices in .
Stable elementary matrices equal the commutator subgroup
Statement
For every associative unital ring , the stable elementary subgroup is a normal subgroup of and Consequently is abelian. Moreover, for every , an upper unitriangular matrix in specified ordered coordinates, with unless , lies in in those coordinates. The matrix of the same automorphism in any other ordered basis lies in the stable subgroup by normality, and hence lies in after some finite stabilization; this need not hold at the original matrix size.
Facts & Assumptions
Given: An associative unital ring and its stable groups and elementary matrices (Stable general linear and elementary groups for right modules).
is by definition the subgroup generated by all elementary matrices, , and matrix multiplication is the group operation, so denotes (Stable general linear and elementary groups for right modules).
A normal subgroup is a subgroup closed under conjugation, and the subgroup generated by a family is the smallest subgroup containing it (Normal subgroup: invariance under conjugation, The subgroup generated by a subset, the cyclic subgroup , and cyclic groups).
Proof
Let be pairwise distinct and . With and one has , , and , so expanding gives .
For the matrix lies in : with and one has , and each of is a product of elementary matrices with distinct indices, while and multiplying the first displayed block swap by the inverse of the second gives . The inverse of the second block swap is elementary because it is the inverse of a product of elementary matrices.
For the upper unitriangular claim, use the specified ordered basis as the coordinates in which the matrix is given; it has the standard form with unless , so it remains to prove directly that this coordinate matrix belongs to .
Every elementary matrix is a commutator: for and , stabilize if necessary so that some index distinct from and exists, and apply step 1.1 with and to get ; hence every generator of lies in , so .
For one has , which represents in ; each factor on the left lies in by step 1.2, so .
Argue by induction on : for the matrix is the empty product of elementary matrices, while for one writes with upper unitriangular of size and has , a product of elementary matrices because for ; the induction hypothesis gives , hence in the specified coordinates.
Steps 2.1 and 2.2 give , and a commutator subgroup is normal, so is normal in by [F2] and is abelian because every commutator lies in the kernel of the quotient map.
If another ordered basis is used, let be the matrix whose columns are that basis in the specified coordinates. The new matrix is . By step 2.3, , and by step 3.1 the stable subgroup is normal, so . By the definition of the stable elementary subgroup as the union under stabilization, this matrix belongs to for some finite after stabilization.
∎
K₁ of a ring and the Whitehead group of a discrete group
Definition
Let be an associative unital ring and let be its stable groups (Stable general linear and elementary groups for right modules). By Stable elementary matrices equal the commutator subgroup, is normal in and equals the commutator subgroup, so the quotient is an abelian group. This group is written additively: for the symbol denotes the class of the stabilized matrix in , and the group law is the one induced by matrix multiplication, so for compatible ; the class is unchanged by stabilization and equals the class of for every . The reduced group is the quotient of by the subgroup generated by the class of the matrix (The subgroup generated by a subset, the cyclic subgroup , and cyclic groups); in one has for every invertible .
Now let be a discrete group, with integral group ring , a unital ring with basis the classes of the group elements (The group ring of finitely supported formal -linear combinations of group elements, The group ring is a unital -algebra with basis , and each is a unit of ). The Whitehead group of is the quotient by the subgroup generated by the classes of the unit matrices . Reading the generators in the order , then , exhibits the same subgroup as , so there is a natural identification
Functoriality and well-definedness. A unital ring homomorphism carries invertible matrices to invertible matrices and elementary matrices to elementary matrices, hence induces and ; a group homomorphism induces the unital ring homomorphism , , which sends to and therefore descends to a homomorphism . These assignments are compatible with composition and preserve identities. If is an inner automorphism of , given by , then the induced ring automorphism of is conjugation by the unit , so on it acts as with the scalar matrix ; conjugation by a fixed invertible matrix is the identity on the quotient , because . Hence inner automorphisms of induce the identity on .
Integral group rings have invariant basis number
Statement
For every discrete group , the integral group ring has invariant basis number: an isomorphism of finite free right -modules forces . More generally, if is an associative unital ring admitting a unital ring homomorphism into a nonzero commutative unital ring , then an isomorphism of finite free right -modules forces .
Facts & Assumptions
Given: An associative unital ring with a unital ring homomorphism into a nonzero commutative unital ring .
For the module consists of column vectors with entrywise addition and the right action , every right-linear has a unique matrix with , and the matrix of a composite is the product in the displayed order (Stable general linear and elementary groups for right modules).
A unital ring homomorphism preserves sums, products and the identity, so entrywise application of commutes with matrix multiplication and with the identity matrices (Ring homomorphism: additive, multiplicative, and required to send to ).
Every nonzero commutative unital ring has invariant basis number for finite bases: as -modules implies (Every nonzero commutative ring has invariant basis number for finite bases).
For a group the integral group ring is a unital ring with basis the elements , and the augmentation is a ring homomorphism with (The group ring of finitely supported formal -linear combinations of group elements, The group ring is a unital -algebra with basis , and each is a unit of , The augmentation map and the augmentation ideal ).
The integer operations make a commutative unital ring (The integers form a commutative ring). Its zero and unit are represented by and (The integers as equivalence classes of pairs of naturals, Arithmetic on the integers); these classes differ, since their equality would require in , whereas and (The natural numbers (von Neumann)). Thus is nonzero.
Proof
Suppose and are mutually inverse right-linear maps. By [F1] the images of the standard basis vectors have unique coordinate expressions, so and have matrices and with and for columns ; composing the coordinate formulas and using uniqueness of coordinates gives from and from .
Applying entrywise to the two matrix identities yields matrices and with and .
Since is commutative, the matrix defines an -linear map , , whose composite with is the identity in both orders by step 2.1; hence as -modules.
As is a nonzero commutative unital ring, [F3] applies to this isomorphism and gives .
For take : by [F4] the group ring is a unital ring and the augmentation is a unital ring homomorphism onto , which is a nonzero commutative unital ring by [F5]; step 4.1 therefore shows that an isomorphism of finite free right modules forces , and the general clause is step 4.1 itself.
A chain contraction makes the odd-to-even parity map invertible
Statement
Let be an associative unital ring and let be a bounded free right -chain complex, so that for all but finitely many and each is a free right -module. A chain contraction of is a family of right-linear maps with for every , that is, the identity of is null-homotopic and is contractible; equivalently as maps of graded modules. Write and , and let and be the odd-to-even and even-to-odd components of the degree-one perturbation of the differential.
Then:
For the matrix assertions in clause 2, choose a finite ordered basis of each and suppose that the concatenated bases and have equal size. Use these same bases for every parity map and every contraction below. A bracket on a parity map means the class of its square matrix in these source and target bases. The triangular assertions use decreasing degree order; the equality of classes holds in any fixed ordering of these bases.
- and are isomorphisms of right -modules, mutually inverse up to the unipotent correction : one has on and on , where raises degrees by two and is nilpotent. This holds over an arbitrary unital and uses no rank, freeness, commutativity or invariant-basis-number hypothesis.
- If is a second chain contraction, , and , then , and the composites are the identity plus maps that strictly raise degrees by even positive amounts. In particular, when the two displayed bases are finite and of the same size and ordered by decreasing degree, all four matrices are unipotent upper triangular and hence have class in , and
Facts & Assumptions
Given: A bounded free right -chain complex over a unital ring , a chain contraction , and a second chain contraction .
A complex is contractible exactly when its identity is null-homotopic, and a null-homotopy of the identity is a degree-one family with (A contractible complex, A chain homotopy).
Odd and even parts of a graded module are the direct sums of the modules of the corresponding degrees, and maps add by components (The direct sum of an indexed family of modules).
For a right -module and right-linear maps, the composite is computed by composing the components; and raises degree by one (Chain complex in an abelian category).
In the class is additive over products, , and every matrix that is unipotent and upper triangular in a finite ordered basis lies in , hence has class (K₁ of a ring and the Whitehead group of a discrete group, Stable elementary matrices equal the commutator subgroup).
A matrix is unipotent upper triangular in the degree-ordered basis when it is the identity plus a map raising degrees, and a product of matrices with a degree-raising factor has matrix computed by the block decomposition of [F2] (Stable general linear and elementary groups for right modules).
Proof
As a map of the graded module , by [F1] and ; restricting to and gives and .
The map raises degrees by two, and on the bounded complex it is nilpotent: for large. Hence is invertible on each of and with inverse , a finite sum. If the homogeneous bases are finite, its matrix in decreasing degree order is upper unitriangular and has class in by [F4]; no class is asserted for infinite bases.
For a homogeneous of even degree one computes and then ; applying and collecting the part of degree gives , and using , and this equals , while every remaining term lies in degree or . Hence with strictly raising degree by an even positive amount and .
From step 1.1, is invertible, so is injective; its composite in the other order is invertible, so it is surjective. Hence is an isomorphism, and by symmetry so is ; this used no finiteness or rank hypothesis beyond boundedness.
The same computation with and interchanged and replaced by gives with strictly raising degree by an even positive amount and . The maps and themselves raise degree by two, so their identity-plus maps are unipotent on the bounded complex; no square-zero assertion about is needed.
Assume now that the displayed bases are finite and of the same size, so that the matrices of , and the four corrections are defined; by steps 1.3 and 2.2 the four correction matrices are unipotent upper triangular in the degree-ordered bases, hence have class in by [F4], and additivity of the class gives .
Therefore in ; taking gives in addition , and the module-isomorphism assertions hold over an arbitrary associative unital ring without a rank or invariant-basis-number assumption. The equalities in this step retain the finite, equal-size basis hypothesis of step 3.1.
Finite based free complexes and contraction torsion
Definition
Let be an associative unital ring. A finite based free right -chain complex is a chain complex of right -modules (Chain complex in an abelian category, Unital left and right modules over a ring; unqualified module means left module) which is bounded, so that for all but finitely many , together with a preferred finite basis of the free right -module for every ; the union is the displayed basis and the elements of are the displayed basis vectors of degree . The degree-ordered bases are each written as a finite list by increasing degree and, within a degree, in the order fixed by . A chain contraction of is a right-linear family with (A chain contraction makes the odd-to-even parity map invertible).
Assume now that By the parity lemma (A chain contraction makes the odd-to-even parity map invertible) the odd-to-even component is an isomorphism of right -modules, so its matrix in the displayed bases , is an invertible square matrix over , and the contraction torsion of is the class of K₁ of a ring and the Whitehead group of a discrete group. The displayed bases fix the sign convention: the odd-to-even parity is used, not the even-to-odd one.
Automatic equality of basis sizes. If has invariant basis number, then always holds, because is an isomorphism of free right -modules ; in particular this applies to every group ring by Integral group rings have invariant basis number. Over a ring without invariant basis number the matrix formula is asserted only when the two displayed finite basis sizes agree, as above; the parity lemma itself needs no such hypothesis.
The two-term case. Let , let be a unit, and let be the complex with the displayed single basis vector in each of the degrees and and zero elsewhere. The contraction identity forces to be a unit and , , so the complex is contractible with that contraction. If is odd the map contains the component with matrix and no other nonzero component, so ; if is even the same component belongs to the even-to-odd map, on the remaining degree, and . Thus which is the parity sign used throughout this page.
Contraction torsion does not depend on the contraction
Statement
Let be a bounded finite based free right -chain complex over an associative unital ring , with displayed bases of equal finite size, and let and be two chain contractions of with . Then where are the contraction torsions of Finite based free complexes and contraction torsion. Their common value is written and called the torsion of the based complex . The equality uses no choice and no further hypothesis on the contraction.
Facts & Assumptions
Given: A bounded finite based free right -chain complex with two chain contractions and displayed bases of of equal size.
The contraction torsion is with the matrix of in the degree-ordered bases, viewed in (Finite based free complexes and contraction torsion).
For two contractions the parity lemma gives in , where is the even-to-odd component (A chain contraction makes the odd-to-even parity map invertible).
is the quotient of by the subgroup generated by , so classes equal in remain equal in (K₁ of a ring and the Whitehead group of a discrete group).
Proof
By the parity lemma both and are isomorphisms of right -modules, so in the displayed bases of equal size they have invertible square matrices and , and , the matrix of , is invertible as well.
Applying [F2] to the pair gives , and applying it to the pair gives ; hence in .
Reducing this equality along the quotient map of [F3] gives in , so the two contractions define the same torsion class; no contraction-dependent data remains, and the argument used only the displayed bases and the two contraction identities.
Basis-change, direct-sum and based exact-sequence formulas
Statement
Let be an associative unital ring and let be bounded finite based free right -chain complexes with displayed bases and defined torsion as in Finite based free complexes and contraction torsion, always in the reduced group . Then:
- (direct sums) If carries, in each degree, the concatenation of the displayed bases of and , then .
- (basis change) If the displayed degree- basis of is replaced by the basis whose vectors have coordinate columns the columns of the invertible matrix in the old basis, then .
- (based exact sequences) If is a degreewise based exact sequence of chain maps between contractible such complexes, with the basis of each the concatenation of the image of the basis of and a set mapping bijectively onto the basis of , then . In diagram form, let the two rows be degreewise based exact sequences of bounded finite based free right -complexes, with vertical chain maps forming a strictly commutative diagram. Suppose two of these maps are chain homotopy equivalences and each of the three mapping cones has equally many odd and even displayed basis vectors. Then all three maps are chain homotopy equivalences and . Here, for a vertical map , the notation is defined by , with the basis of followed by that of in cone degree ; the six row complexes themselves need not be contractible.
- (chain isomorphisms and cones) If is an isomorphism of bounded finite based free complexes with contractions and defined torsion (equal odd/even displayed basis sizes in each complex), and with equally many displayed basis vectors in and for every , and if is the algebraic mapping cone with carrying the basis of followed by that of (The mapping cone of a chain map), then and , where is written in the displayed bases. The degreewise equality makes each square; it is automatic over an invariant-basis-number ring, but not over an arbitrary unital ring.
Facts & Assumptions
Given: Bounded finite based free right -chain complexes with displayed bases and contractions, over an associative unital ring .
Torsion is for any chain contraction , is independent of the contraction, and lies in the reduced group, where classes are additive over products, , and (Finite based free complexes and contraction torsion, Contraction torsion does not depend on the contraction, K₁ of a ring and the Whitehead group of a discrete group).
For two contractions of one complex, in , and both maps are isomorphisms of right -modules (A chain contraction makes the odd-to-even parity map invertible).
A matrix that is unipotent upper triangular in a finite ordered basis lies in and has class , and the class of a block sum satisfies because , where and are stabilizations of and of a conjugate of (Stable general linear and elementary groups for right modules, Stable elementary matrices equal the commutator subgroup).
The mapping cone of a chain map has with differential , and a chain isomorphism is a chain map with an inverse (The mapping cone of a chain map, A chain homotopy equivalence).
A chain map is a chain homotopy equivalence exactly when its mapping cone is contractible (A chain map is a homotopy equivalence exactly when its cone is contractible).
Proof
For the given complexes the parity lemma provides isomorphisms and for every contraction ; all torsion classes below are computed from the odd-to-even components in the degree-ordered displayed bases, and equality in implies equality in .
For the direct sum use the contraction and the concatenated degree-ordered bases: the parity decomposition of is the direct sum of the parity decompositions, so the matrix of is, after permuting the source and target bases to group the two summands, the block matrix ; these permutations contribute only , which vanishes in the reduced group. The block matrix has class by [F3]; hence .
Let be a chain isomorphism of based complexes with defined torsion and equal displayed basis sizes in each degree, as in assertion 4, and a contraction of ; then is a contraction of , and where are the block matrices of the components in the displayed bases. Taking classes and using additivity gives , and since torsion does not depend on the contraction this holds for the displayed based complexes.
Let be the complex with and differential , carrying the displayed basis of in degree . Then is a contraction of , and , , so the matrix of is with the matrix of ; by [F2] and in also , so .
For a basis change as in assertion 2 let be the identity chain isomorphism from with the old basis to with the new basis; its component has matrix in the old and new bases, so step 1.3 gives .
For the based exact sequence choose a contraction of and, using the basis splitting, the explicit right-linear section that sends each displayed basis vector of to the displayed basis vector of complementary to the image of the basis of ; then defines a chain map with , and is a chain isomorphism whose matrix in each degree is in the displayed concatenated bases. By steps 1.2 and 2.1, because each of the finitely many unipotent matrices has class by [F3]; the diagram form follows after establishing the cone-sequence two-out-of-three argument below.
In a degreewise based exact sequence , if is contractible then the formula for the chain section in step 2.2 splits the sequence as chain complexes, so is a chain retract of ; if is contractible, choose a graded section and put , valued in . For a contraction of , the identity makes a chain section, so is a chain retract of . These two splittings show directly that if any two of are contractible then so is the third. In the diagram of assertion 3, strict commutativity and the cone differential give a degreewise exact sequence . Reordering the middle cone basis groups the two subcomplex summands before the two quotient summands, making this sequence based exact; these permutations contribute only in the reduced group. By [F5] two cones are contractible, hence all three are by the preceding splitting argument, and [F5] makes the third vertical map a chain homotopy equivalence. The assumed equality of parity basis counts licenses each cone torsion over arbitrary . Step 2.2 and the definition now give .
For an isomorphism the cone carries the degreewise based exact sequence with the concatenated bases, so by step 2.2 by step 1.3, which together with steps 1.2, 2.1 and 2.2 proves all the stated formulas.
Based cellular chains of a universal cover as finite free right group-ring modules
Definition
Let be a nonempty connected finite CW complex with supplied characteristic maps, let be a basepoint, put , and let be a chosen universal cover, which exists for the spaces considered here because a finite CW complex is locally path-connected and semilocally simply connected (Every nonempty path-connected locally path-connected semilocally simply connected space has a universal cover). Write for the integral group ring, a unital ring with basis the classes of the group elements (The group ring of finitely supported formal -linear combinations of group elements, The group ring is a unital -algebra with basis , and each is a unit of ).
Lifted CW structure. Every open cell is contractible, so splits into components each mapped homeomorphically onto ; such a component is an open cell of over . To obtain its lifted characteristic map, choose a point above the image of one interior point of the characteristic disk and lift the entire characteristic map through ; this is possible because is simply connected (Lifting criterion for maps from path-connected locally path-connected spaces), and its interior maps homeomorphically onto the chosen component over . The inverse alone cannot be composed with the characteristic map on its boundary, where that inverse is undefined. These lifted characteristic maps give the standard lifted CW structure (Cell attachment by a characteristic map, Skeleta, CW subcomplexes, and relative CW complexes). Its -skeleton is the union of the closed lifted cells over the cells of of dimension at most ; for a CW pair the preimage is a CW subcomplex of and is the -skeleton of the relative lifted structure.
Deck action. Identify with the deck group of by the no-reversal isomorphism of For a path-connected locally path-connected semilocally simply connected base, the deck group of a universal cover is isomorphic to the fundamental group, writing for the covering homeomorphism attached to ; thus , , and every carries lifted cells onto lifted cells of the same dimension. A deck transformation is determined by its value at one point and acts freely, so the lifts of a single cell are exactly the cells for one chosen lift .
Right group-ring action. The action of the deck group on the singular and cellular chains of is written on the left and the length-preserving insertion of inverses makes it a right action of by extended -bilinearly in and the group-ring coefficient (Relative singular homology, Oriented cellular chain group); in particular . Each is a homeomorphism of pairs and of pairs , so the action passes to the homology of those pairs.
Based cellular chains. For each cell of choose an orientation of , that is, an orientation of the disk of its characteristic map, and choose one oriented lift carrying that orientation. Put The notation after the semicolon records the deck-induced -module structure; the homology coefficients are integral. By Relative homology of consecutive CW skeleta these integral homology groups are free abelian on the lifted cells. The right action above makes them finite free right -modules on one chosen oriented lift of each cell of (respectively each relative cell of ): the lifts of one cell form the -orbit , and bijects with that orbit. Using as a second homology coefficient group here would duplicate the lift-indexed generators and would not yield the claimed rank. Degrees without relative cells give the zero module, and for a disconnected finite the construction is applied componentwise with its component group ring.
Cellular basis ambiguities vanish in the Whitehead group
Statement
Let be an associative unital ring and let be the free right -module of column vectors.
- An elementary basis change of , that is, one whose change-of-basis matrix is a finite product of elementary matrices with and their inverses, changes the class in by .
- A reordering of a finite basis changes the class in by or by ; in particular it changes nothing in or in .
- For : replacing the chosen oriented lift of one cell of a finite CW complex by another, or reversing its orientation, is a change of basis in which exactly one basis vector is replaced by a unit with ; its class in is . In the same situation a change of basepoint path conjugates and acts trivially on , and two different basepoint paths act the same way.
- The quotients are genuinely distinct: there is a unit of a group ring that is not killed by the passage from to . Concretely, for and , the element is a unit of and its class is a nonzero element of .
The clauses about use no commutativity of ; clause 4 uses the determinant of the commutative ring .
Facts & Assumptions
Given: An associative unital ring , and for clauses 3 and 4 a discrete group with integral group ring .
For any unital ring , is the subgroup of generated by the stabilized elementary matrices with , and it is normal in with ; composition of right-linear maps of free right modules is ordinary matrix multiplication in the displayed order (Stable general linear and elementary groups for right modules, Stable elementary matrices equal the commutator subgroup).
is written additively with , and ; , and for a discrete group the Whitehead group is , where is the class of the unit matrix . A ring homomorphism induces maps on and , a group homomorphism induces a map on , and an inner automorphism of induces the identity on because on matrices it acts as conjugation by a scalar matrix (K₁ of a ring and the Whitehead group of a discrete group).
If the new degree- basis of a bounded contractible based free right -complex is the old basis right-multiplied by in column coordinates, then in (Basis-change, direct-sum and based exact-sequence formulas).
In the based cellular chains of a universal cover, choosing one oriented lift of every cell makes each a finite free right -module on those lifts, and the lifts of a single cell are exactly the cells for one chosen lift , with the deck transformation attached to ; in the right action the basis vector is therefore replaced by a group-ring unit (Based cellular chains of a universal cover as finite free right group-ring modules).
Over a commutative unital ring , , adding a multiple of one row to a distinct row leaves the determinant unchanged, and an invertible matrix has unit determinant (For same-sized finite square matrices over a commutative ring, , For every square matrix, including singular ones, a row swap negates the determinant, scaling a row by any scalar scales it, and row addition leaves it unchanged, An invertible square matrix over a commutative ring has unit determinant, The Leibniz determinant is column-multilinear, alternating and normalized over every commutative ring).
Determinant on over a commutative ring is the unique normalized alternating column-multilinear function, and it is also alternating and multilinear in the rows (The determinant is the unique normalized alternating multilinear function on the columns, The determinant is alternating and multilinear in the rows as well as in the columns).
For a group the group ring is a unital ring which as a -module is free with basis the elements , with and invertible with inverse (The group ring of finitely supported formal -linear combinations of group elements, The group ring is a unital -algebra with basis , and each is a unit of ).
Paths concatenate in traversal order and have reversals (Paths, path-connected spaces and path components). Based loops modulo homotopy rel endpoints form the fundamental group, with concatenation as product (Based loops and the fundamental group, Loop classes form the group under concatenation, Homotopies of continuous maps, homotopies relative to a subspace, and path homotopies relative to the endpoints). Continuous maps defined compatibly on a finite closed cover paste to a continuous map (Continuity may be checked on any open cover, and on any finite closed cover; composites of continuous maps are continuous).
Proof
Let and let be a product of elementary matrices and their inverses. By [F1] each factor lies in , so ; as , its class satisfies , and by additivity of the class in [F2] every finite product of elementary matrices and inverses has class as well.
In put and . Multiplying the three matrices gives , hence with ; since is the stabilization of the matrix , [F2] gives .
Let and let a based cellular complex over the universal cover be given as in [F4]. Replacing the chosen lift of a cell by the lift replaces one basis vector by , and reversing the orientation replaces one basis vector by its negative; the change-of-basis matrix is therefore diagonal with one entry or and all other entries . Its class in is or , both of which are in by the definition of in [F2].
For a path , define on loops at . Concatenating a homotopy rel endpoints with the fixed outer paths gives a homotopy rel endpoints, so the map is well defined and preserves products after inserting the cancellable middle path . Explicitly, for any path , the two formulas for and for agree at ; by pasting they contract rel endpoints. Reparametrising by likewise identifies bracketings and deletes constant paths. Thus is inverse to . For a second path , the composite carries to , conjugation by the loop at . By [F2] inner automorphisms act trivially on , so the two paths induce the same Whitehead-group map.
Let and . In distribute and use with : the last step because and . Hence is a unit of with inverse .
By [F7] the elements form a -basis of . Every element of the subgroup is a finite product of monomials , hence is itself for some , an element whose coefficient vector in that basis has exactly one nonzero entry; the coefficient vector of has the three nonzero entries . Therefore and .
Let be a commutative unital ring. Since is multiplicative with by [F5] and because is obtained from by adding times the -th row to the -th row, the determinant is unchanged under right multiplication by any product of elementary matrices; moreover for : the function is normalized, column-multilinear and alternating in the columns of , so it equals by the uniqueness in [F6]. Hence is compatible with stabilization and descends to a well-defined homomorphism with for every unit .
The matrix of a permutation of a finite basis that is a product of transpositions is a product of copies of padded by identity blocks, because permutation matrices for entries multiply by the composition rule of [F1] and the padded matrices are the stabilized transpositions. Hence by [F2] its class is , which is for even and for odd, so every reordering has class or in , and class in and in where .
For the homomorphism of step 1.7 sends the class of the matrix to , so it induces a homomorphism carrying the class of the unit of step 1.5 to the coset .
By the basis-change formula of [F3], a change of the displayed bases whose change-of-basis matrices all have class in leaves the torsion class in unchanged; combining with steps 2.1 and 1.3, neither a reordering of the cells, nor a reversal of an orientation, nor a change of the chosen lifts alters the torsion class in , and an elementary basis change does not alter the class in .
Since by step 1.6, that coset is not the identity coset, so the image of in is nonzero: the quotient map does not kill every unit.
Clauses 1 and 2 are steps 1.1 and 2.1, clause 3 is steps 1.3 and 1.4, and clause 4 is steps 1.5, 1.6, 1.7, 2.2 and 3.2; no step assumed commutativity of except in clauses about the commutative group ring , and no step used any choice principle.
Universal-cover boundaries, maps and homotopies respect the right group-ring action
Statement
Let be connected finite CW complexes, , , , , with chosen universal covers and and the based cellular chains of Based cellular chains of a universal cover as finite free right group-ring modules, so that is a finite free right -module and a finite free right -module.
- Boundaries are right-linear. Each cellular boundary satisfies for all and . Consequently every deck transformation is an automorphism of the underlying cellular chain complex of abelian groups. It is semilinear for conjugation: . It need not be right -linear or preserve the selected module basis.
- Lifted cellular maps are right-linear chain maps. Let be a based cellular map with an isomorphism. Choose points over the basepoints and the unique compatible lift with . Transport the right -module structure of along . Then induces a right -linear chain map. A different lift is linear for the correspondingly conjugated coefficient identification, rather than necessarily for this fixed one.
- Lifted cellular homotopies are right-linear chain homotopies with one coefficient transport. Let be based cellular maps, with an isomorphism, and let be a cellular homotopy from to which may move during the homotopy. Choose as in clause 2 and any lift of . Then the unique lift of beginning at ends at for a unique , and there are right -linear maps , with the source transported by , satisfying for every . The composite is right-linear for this transport, although alone is generally not right-linear when is nonabelian. If fixes and , then .
All three clauses are choice-free for finite CW complexes.
Facts & Assumptions
Given: Connected finite CW complexes with basepoints and chosen universal covers, , , and the based cellular chains of Based cellular chains of a universal cover as finite free right group-ring modules.
is free abelian on the lifted -cells, the right action is with the no-reversal deck isomorphism, and each is a homeomorphism carrying lifted cells to lifted cells (Based cellular chains of a universal cover as finite free right group-ring modules).
The cellular boundary is the connecting homomorphism of the pair followed by the quotient map to (Cellular boundary from three consecutive skeleta).
For a continuous map of pairs the induced map on singular chains commutes with the boundary, (The induced singular chain map of a continuous map, The singular boundary operator).
A relative -cycle is an ordinary chain with , and the connecting homomorphism of the pair sequence is on such cycles; relative homology is (Relative singular homology, Relative connecting homomorphism on cycles, Relative singular chain complex).
If is a homotopy from to , its prism operator satisfies (The prism operator of a homotopy, The singular chain homotopy formula).
Covering homotopies lift uniquely once the lift at time zero is prescribed, and two lifts of a map from a connected space which agree at one point agree everywhere (Existence and uniqueness of homotopy lifts through a covering map, Two lifts from a connected space that agree at one point agree everywhere).
For a based map , choose points over the basepoints. Its lift with satisfies under the no-reversal deck identifications. A different lift satisfies the same formula with conjugated by (For a path-connected locally path-connected semilocally simply connected base, the deck group of a universal cover is isomorphic to the fundamental group and uniqueness of lifts).
A continuous map of finite CW complexes is homotopic to a cellular map, and homotopic cellular maps of finite CW pairs admit a cellular homotopy (Cellular approximation for maps of CW pairs).
Proof
Let be represented by a relative cycle with , and let . By [F4] the connecting homomorphism satisfies and is natural for the map of pairs , so , using [F3]; the quotient map is likewise natural because it is induced by the inclusion of chain complexes. Hence with [F1] and [F2], .
Let be a cellular homotopy from to , and let be the lift of with , which exists and is unique by [F6] since is connected. Its end is a lift of , so it equals for a unique by [F6] and the free transitive deck action.
Applying step 1.1 with gives . Thus is an automorphism of the underlying integral cellular chain complex, with inverse . The right-action convention gives . This is semilinearity, not right-linearity for the fixed coefficients; the selected finite right-module basis can also change under .
Let be a lift of the cellular . Since is cellular, for every : because and ; an individual cell may map across several target cells or collapse. Hence carries into and into , so it induces maps on relative homology by naturality of the connecting homomorphisms and quotient maps as in step 1.1.
For with one has , because is cellular and ; hence the prism operator of [F5] maps into . In particular maps into and into , so it induces by .
The induced maps of step 2.2 commute with the differentials: for a relative cycle as in step 1.1, by [F3], and naturality of and of the quotient map gives .
For the map is a group isomorphism and by [F7], so on chains ; thus is right -linear for the transported source structure.
The class in step 2.3 is well defined: if is replaced by with , then by [F5] , where the first two terms lie in (step 2.2) and the last is a boundary in the relative complex ; adding a chain of changes by an element of .
Applying the identity of [F5] to and reducing modulo the subcomplexes defining the relative groups gives in , which is the displayed chain-homotopy identity; equivalently .
The operators of step 2.3 are right-linear: for by [F6] and [F7], since both sides are lifts agreeing at time zero, so exactly as in step 3.2. At time one this also proves that the composite is right-linear for ; it does not assert that is right-linear for the unmodified -module. If fixes and both endpoint lifts send to , uniqueness at gives .
Clause 1 is steps 1.1 and 2.1, clause 2 is steps 2.2, 3.1 and 3.2, and clause 3 is steps 1.2, 2.3, 3.3, 4.1 and 4.2; every step used only finite CW approximation [F8] where cellular maps were assumed, and no step used a choice principle.
A lifted finite CW equivalence has a contractible group-ring mapping cone
Statement
Let be a based homotopy equivalence of connected finite CW complexes, with a vertex and a vertex after choosing a cellular representative. Put and ; let and be universal covers with chosen points over the basepoints. Let be the compatible lift of a based cellular approximation of satisfying . Transport the right -module structure of the based cellular chains of to a right -module structure along . A different choice of basepoint or lift uses the corresponding transported coefficient identification.
Then is a chain homotopy equivalence of right -complexes. Consequently its algebraic mapping cone , with and differential , is a bounded contractible complex of finite free based right -modules, with target summands first. Contractibility comes from right-linear chain homotopies induced by based geometric deformation retracts, not from homology vanishing.
Facts & Assumptions
Given: The based finite CW equivalence and compatible cover lifts in the statement. Write for its finite cellular mapping cylinder, for the free-end inclusion, for the target inclusion, and for the standard collapse, so and .
The finite cellular mapping cylinder has and as CW subcomplexes. Its collapse is a strong deformation retraction onto , fixing pointwise throughout (Cellular mapping cylinders and relative cylinders are CW complexes).
Since and both and are homotopy equivalences, is a homotopy equivalence. A CW subcomplex inclusion which is a homotopy equivalence is a strong deformation retract, hence there is a retraction and a homotopy fixing throughout (Homotopy equivalences, homotopy inverses and spaces of the same homotopy type, Cw homotopy equivalence inclusions are strong deformation retracts).
Cellular approximation for finite CW pairs makes each retraction cellular relative to the fixed subcomplex and makes its deformation homotopy cellular relative to that subcomplex and its two cellular endpoint maps. The inclusions have the homotopy extension property (Cellular approximation for maps of CW pairs, Relative CW inclusions are cofibrations).
A based cellular map inducing a fundamental-group isomorphism has a compatible lift inducing a right-linear cellular chain map after coefficient transport. A lifted cellular homotopy that fixes its basepoint gives a right-linear chain homotopy between the compatible endpoint maps (Universal-cover boundaries, maps and homotopies respect the right group-ring action).
A chain map is a chain homotopy equivalence exactly when its algebraic mapping cone is contractible; the cone has the target summand followed by the shifted source and the displayed differential (A chain map is a homotopy equivalence exactly when its cone is contractible, The mapping cone of a chain map, A chain homotopy equivalence, A contractible complex).
Finite CW cellular chains of universal covers are bounded finite free based right group-ring complexes; their finite direct sums are finite free on the concatenated bases (Based cellular chains of a universal cover as finite free right group-ring modules, The direct sum of an indexed family of modules).
Proof
If the original map is not cellular or the chosen basepoint is not a vertex, choose a vertex of , use its image under a based cellular approximation as the target vertex, and transport the previously selected fundamental groups along the basepoint paths. These finite choices do not affect the assertion after the specified coefficient transport. Hence work with the based cellular in the statement. Form , , and . By [F1], and are inverse up to a deformation fixing . Since is an equivalence, is an equivalence: if is a homotopy inverse of , then is a homotopy inverse of : , while and the equivalence detects .
Apply [F2] to to obtain a retraction and homotopy fixed on . The standard deformation gives and fixed on . By [F3] take and both homotopies cellular relative to the indicated fixed subcomplexes and their endpoint maps. In particular , , and the selected basepoints and stay fixed during the respective homotopies.
Let be the universal cover of . The prism edge from to identifies with by path transport. Since collapses this edge to the constant path at , the two inclusion isomorphisms identify with under . Fix a lift of in , lift that edge to select a lift of , and identify the connected preimages of and with the chosen and . They are connected universal covers because and are isomorphisms. Under these identifications the common deck ring becomes via , the source action is precisely the transport through , and the compatible lift of is .
For or , write and for its cellular retraction. Lift so that at the selected basepoint; lift starting at . Since fixes the basepoint in , uniqueness of covering homotopy lifts makes its end exactly . For every deck element , the two maps and are lifts of the same map and agree at time zero, so they agree for all . Thus the lifted deformation and its cellular prism are equivariant; under the right action they induce -linear chain homotopies and . No isolated deck transformation is claimed to be -linear.
Step 3.1 makes each and an -linear chain homotopy equivalence. For its retraction is , so is an -linear chain homotopy inverse to . Since by step 2.2, it is an -linear chain homotopy equivalence. An explicit inverse is : both composites reduce to identities using the two homotopies in step 3.1 and functoriality of the induced cellular chain maps.
Apply [F5] to the chain homotopy equivalence in step 4.1. Its cone is contractible with the stated differential. By [F6], both summands in degree are finite free based right -modules, so the ordered concatenation of their bases is a finite free basis, and the dimensions of bound the degrees in which the cone is nonzero. Thus the cone is bounded finite free based and contractible. The contraction follows from the two explicit equivariant lifted deformation homotopies in step 3.1 through the cone criterion; no homology-vanishing converse has been used.
Whitehead torsion of a finite CW homotopy equivalence
Definition
Let be a homotopy equivalence of finite CW complexes. Choose a vertex and, after taking a cellular representative still denoted , put , a vertex of ; set . Then the based induced map is an isomorphism (Homotopy equivalences, homotopy inverses and spaces of the same homotopy type). Other basepoints are compared by supplied paths in the independence theorem. Choose
- a cellular representative of , again written , and homotopies ensuring that the cellular representative is a homotopy equivalence (Cellular approximation for maps of CW pairs);
- universal covers and , chosen points above , and the compatible lift with of the cellular representative (Based cellular chains of a universal cover as finite free right group-ring modules);
- the based cellular chains of Based cellular chains of a universal cover as finite free right group-ring modules, with one oriented lift chosen for every cell of and of .
Coefficient transport. Transport the right -module structure on along the ring isomorphism , so that for . By Universal-cover boundaries, maps and homotopies respect the right group-ring action the transported boundary and the chain map are right -linear, and by A lifted finite CW equivalence has a contractible group-ring mapping cone is a chain homotopy equivalence of bounded complexes of finite based free right -modules.
The class. Form the algebraic mapping cone with the differential recorded in The mapping cone of a chain map, carrying in each degree the displayed basis of followed by that of , so that the target summands come first. This complex is bounded, finite based free and contractible, and has invariant basis number, so the contraction torsion of Finite based free complexes and contraction torsion is defined for it, is independent of the chosen contraction by Contraction torsion does not depend on the contraction, and lands in . Define using the quotient map of K₁ of a ring and the Whitehead group of a discrete group. Equivalently, is the image of the reduced class for any contraction of the cone.
Disconnected complexes. If has components , write for the fundamental group of a component at a chosen basepoint; every component of a finite CW complex has the homotopy type of a connected finite CW complex and contains a vertex, so this is defined. Since is a homotopy equivalence it maps components of bijectively onto components of , and the data above are chosen componentwise; the class has as its -component the torsion of the restriction to the component of corresponding to , computed with a basepoint in that component and its chosen lift. For connected this is the single class defined above.
Status. This is a definition by chosen data: the contraction, the cellular representative, the basepoint paths, the lifts, the orientations and the order of the cells are all auxiliary. The next theorem proves that the resulting class in does not depend on them; until then denotes the class attached to the displayed choices. No further quotient and no further choice principle is used, the cellular representative exists choice-free for finite complexes, and all choices made here are finite except the (finite) choice of cell lifts.
Whitehead torsion is independent of all auxiliary choices
Statement
Let be a homotopy equivalence of finite CW complexes and let be the class of Whitehead torsion of a finite CW homotopy equivalence attached to a choice of cellular representative, universal covers, lifts, basepoints, orientations, orders of the cells and chain contraction. Then the image of that class in depends on none of these choices.
Moreover:
- Changing the basepoint to transports under the canonical isomorphism of basepoint change, and two different paths from to induce the same isomorphism, so the transport is canonical; the same holds at the source.
- If is a second finite CW homotopy equivalence with the same target basepoint, then after the canonical identifications; in particular homotopic homotopy equivalences of finite CW complexes have equal torsion.
- For disconnected all statements hold componentwise in .
Facts & Assumptions
Given: A homotopy equivalence of finite CW complexes with the chosen data of Whitehead torsion of a finite CW homotopy equivalence, and a second choice of the same kind, written with primes.
is the image in of the contraction torsion of the based contractible complex with the target summands first, computed from the odd-to-even part of in the displayed bases (Whitehead torsion of a finite CW homotopy equivalence, Finite based free complexes and contraction torsion).
The contraction torsion of a bounded contractible based free complex does not depend on the contraction (Contraction torsion does not depend on the contraction).
If the degree- basis is replaced by the basis whose coordinate columns are the columns of the invertible matrix in the old basis, then in ; if is a chain isomorphism with equal degreewise displayed basis sizes then ; and unipotent upper triangular matrices have class (Basis-change, direct-sum and based exact-sequence formulas, Stable elementary matrices equal the commutator subgroup).
Reordering a basis changes the class in only by , reversing an orientation or replacing a chosen cell lift changes it by a unit of , and all of these classes vanish in ; a change of basepoint path conjugates the fundamental group, inner automorphisms induce the identity on , and two basepoint paths induce the same map there (Cellular basis ambiguities vanish in the Whitehead group).
Chain homotopic chain maps have chain-isomorphic mapping cones, by the unitriangular isomorphism on for a chain homotopy ; chain homotopy is compatible with composition, and a deck transformation is an additive chain isomorphism which is semilinear for the corresponding inner automorphism of the group ring (Homotopic maps have chain-isomorphic mapping cones, The mapping cone of a chain map, Chain homotopy is compatible with addition and composition, Universal-cover boundaries, maps and homotopies respect the right group-ring action).
A continuous map of finite CW complexes is homotopic to a cellular map, and homotopic cellular maps of finite CW pairs admit a cellular homotopy; both statements are choice-free for finite complexes (Cellular approximation for maps of CW pairs).
A lifted cellular homotopy induces a right-linear chain homotopy from the initial compatible lift to the deck-twisted endpoint composite, both interpreted with the initial map’s coefficient transport; the deck map alone need not be right-linear (Universal-cover boundaries, maps and homotopies respect the right group-ring action).
Proof
Replacing the contraction of the cone changes nothing, by [F2]; this proves independence of the contraction.
Consider a change of the displayed cellular bases only. In degree the cone basis is the concatenation of the basis of and of , so a change of the cell bases induces the block-diagonal basis change in degree ; by [F3] the torsion changes by . Reordering, reorienting or relifting cells changes only the individual factors , by permutation matrices, by diagonal matrices with a single entry , or by diagonal matrices with a single entry a group element, all of which have class in by [F4]; hence the class in is unchanged.
For a fixed based map and based cover identifications, a compatible lift is unique. Changing the chosen lift over the target basepoint by a deck map changes the compatible lift to and the coefficient identification from to , where . Indeed , so is -semilinear, generally not -linear. With this simultaneous coefficient change, is a semilinear chain isomorphism from the cone of to the cone of . In the transported target bases and unchanged source bases it preserves the displayed bases; using the original target lifts instead changes each target basis by a diagonal group unit. Inner automorphisms act trivially on and these diagonal units vanish there by [F4]. Thus the torsion class is unchanged under a change of compatible cover identification or lifted map.
A change of basepoint transports the coefficient group ring along the basepoint isomorphism of [F4], and every path gives the same map on because two such isomorphisms differ by an inner automorphism, which acts trivially; the same argument applies at the source, and the class of a componentwise definition on a disconnected target is transported componentwise.
Let be a second cellular representative of the given homotopy class, with compatible lift . By [F6] there is a cellular homotopy from to . Its lift beginning at ends at , and [F7] supplies a right-linear chain homotopy for the initial coefficient transport. Step 1.3 identifies the torsion of the latter map, after its corresponding inner coefficient transport, with the torsion of . Thus it remains to compare cones of the two chain-homotopic maps over the same ring.
For chain-homotopic the isomorphism of [F5] has matrix in the target-first cone bases, so by the isomorphism formula of [F3] the two cone torsions differ by a sum of classes of unipotent matrices, namely ; hence the two cones give the same class in and therefore the same class in . This proves independence of the cellular representative and of homotopic replacements.
Combining steps 1.1, 1.2, 1.3 and 1.4 gives independence of contraction, cell bases, cover identifications, lifts and basepoint paths; combining with step 3.1 gives independence of the cellular approximation and equality for homotopic homotopy equivalences; the disconnected statement is the componentwise reading of steps 1.1 through 1.4 and step 2.1.
Composition and based-pair sum formulas for Whitehead torsion
Statement
Let and be homotopy equivalences of finite CW complexes.
- (composition) in , where is induced by the group isomorphism of K₁ of a ring and the Whitehead group of a discrete group. If the complexes are disconnected this holds componentwise.
- (pairs) Let be a cellular map of finite CW pairs whose restrictions and are homotopy equivalences, with compatible basepoint paths on components. Then in for connected , where induces coefficient extension from each component of to the component of containing it, and is the induced map of relative based cellular chain complexes over . For disconnected , take this formula componentwise, summing the images of the -component torsions in each target component.
- (based exact sequences, algebraic form) For a degreewise based exact sequence of contractible bounded finite based free right -complexes whose displayed odd and even basis lists have equal size in each of , ; equivalently, in a strictly commutative based exact diagram of bounded finite based free right -complexes in which two of the three vertical maps are chain homotopy equivalences and the three mapping cones have equal odd and even displayed basis sizes, the torsion of the middle map is the sum of the torsions of the sub- and quotient maps.
Facts & Assumptions
Given: Finite CW complexes with basepoints, homotopy equivalences , , and for clause 2 a cellular map of finite CW pairs as stated.
is defined by chosen cellular representatives and compatible lifts as the image in of the contraction torsion of the based cone complex, and it is independent of all auxiliary choices, so it may be computed with any convenient representative and contraction; homotopic representatives give the same class (Whitehead torsion of a finite CW homotopy equivalence, Whitehead torsion is independent of all auxiliary choices).
Algebraic composition and sum formulas for maps whose cone torsions are defined: for chain homotopy equivalences , of finite based free -chain complexes one has ; for a commutative diagram of finite based free complexes with based exact rows in which two of the three vertical maps are chain homotopy equivalences and all three cones have equal odd and even displayed basis sizes, all three maps are chain homotopy equivalences and (Lück, Lemma 2.9(1) and 2.9(3), pp.29–30; the based exact sequence case follows from Basis-change, direct-sum and based exact-sequence formulas).
A lifted cellular map of a homotopy equivalence induces a right-linear chain homotopy equivalence of the based cellular chain complexes after transporting the source coefficients along the induced fundamental-group isomorphism, and deck twists and unipotent basis corrections do not change the class in (A lifted finite CW equivalence has a contractible group-ring mapping cone, Universal-cover boundaries, maps and homotopies respect the right group-ring action, Cellular basis ambiguities vanish in the Whitehead group).
For a finite CW pair , the integral cellular chains of the lifted inclusion form a degreewise based split sequence of finite free modules over the ambient group ring. Componentwise, is the module induced from the universal-cover cellular complex of each component of along its fundamental-group homomorphism into ; this remains true when that homomorphism is not injective. A homotopy equivalence of the components of induces a chain homotopy equivalence on these induced modules, because extension of scalars carries a chain inverse and its homotopies to a chain inverse and homotopies after induction (Based cellular chains of a universal cover as finite free right group-ring modules, A lifted finite CW equivalence has a contractible group-ring mapping cone, Relative singular homology).
Functoriality: a unital ring homomorphism, in particular the coefficient extension , carries invertible matrices to invertible matrices, elementary matrices to elementary matrices and the classes to , hence induces maps on and on compatible with composition (K₁ of a ring and the Whitehead group of a discrete group).
Proof
Choose cellular representatives of and compatible lifts of ; by [F3] the lifted chain maps are right-linear chain homotopy equivalences after transporting coefficients, and by [F3] again the composite differs from the lift of by a deck twist, which does not change classes in . Hence the algebraic composition formula of [F2] applies to the transported based complexes and gives the composition formula after applying the group isomorphism to the coefficient ring of the middle complex; this is the displayed formula, since the transport of from to is exactly by [F5].
For clause 2 write and , and transport all source coefficients through to . In each degree the lifted cells of split into those over and those outside , and similarly for . Hence [F4] gives two degreewise based exact rows and , joined by the three chain maps induced by . A lift of the cellular pair map preserves the subcomplexes, so the diagram commutes.
Taking algebraic mapping cones of the three vertical maps in step 1.2 gives the degreewise based exact sequence The first and middle cones are contractible: for the first, decompose componentwise and use the induced chain equivalences of [F4]; for the middle use [F3]. The last cone is contractible as well. Explicitly, a graded basis splitting of the exact sequence gives a graded section of the quotient and defect with values in the first cone; if contracts the first cone, is a chain section because and . The last cone is then a chain retract of the contractible middle cone, so it inherits a contraction. By the cone criterion of [F3], is a chain homotopy equivalence.
Apply the based exact sequence formula of [F2] to step 2.1. The cone bases in each degree are concatenations of the bases of the lifted subcomplex and quotient cells, up to cell permutations whose classes vanish in by [F3]. Hence the middle cone torsion is the sum of the first and last cone torsions. The first is the image under componentwise coefficient extension: the induced complex over is obtained by extending the component coefficient rings and their chosen bases, so its contraction matrix is the scalar extension of the contraction matrix for . The last is by definition of algebraic cone torsion. Passing to proves .
Clause 3 is the algebraic statement of [F2] as proved from Basis-change, direct-sum and based exact-sequence formulas; clause 1 is step 1.1 and clause 2 is steps 1.2, 2.1 and 3.1. No step used a choice principle beyond finitely many cell and lift choices, and no step used a smooth, handle or cobordism statement.
An elementary CW expansion has zero Whitehead torsion
Statement
Let be an elementary expansion of finite CW complexes. Then its Whitehead torsion vanishes, componentwise. In suitable oriented lifts the only nonzero relative cellular boundary of the pair is in two consecutive degrees, where and ; this is a contractible two-term complex, and in .
Facts & Assumptions
Given: An elementary expansion of finite CW complexes of dimension , with new cells and , and, in the connected case, and .
In an elementary expansion the new -cell is a free face of the new -cell: the characteristic map restricts to a characteristic map , homeomorphic on the open cell, and all other boundary values of lie in the previously constructed complex ; moreover with a subcomplex, the pair deformation retracts onto , and the operation is taken componentwise and fixes the retained subcomplex (Elementary expansions and collapses of finite CW complexes).
For a finite CW pair the relative cellular chains over the universal cover are the finite free right -modules on the chosen oriented lifts of the relative cells, the lifts of one cell are the cells , the right action is , and the cellular boundary is right -linear; for a disconnected finite the constructions are applied componentwise and assembled by direct sums (Based cellular chains of a universal cover as finite free right group-ring modules, Universal-cover boundaries, maps and homotopies respect the right group-ring action).
For a homotopy equivalence of finite CW complexes, is the image in of the contraction torsion of the algebraic mapping cone of the lifted cellular chain map, with the target summands recorded first in each degree, and for disconnected the class is the tuple of the classes of the componentwise restrictions (Whitehead torsion of a finite CW homotopy equivalence).
The algebraic mapping cone of a chain map has and differential (The mapping cone of a chain map).
If is a homotopy equivalence of connected finite CW complexes and is a lift of a cellular approximation, then is a chain homotopy equivalence of right -complexes and is a bounded based free right -complex which is contractible (A lifted finite CW equivalence has a contractible group-ring mapping cone).
For a bounded finite based free right -complex with and a chain contraction , the contraction torsion is the class of the matrix of in the degree-ordered displayed bases, and it does not depend on the contraction (Finite based free complexes and contraction torsion, Contraction torsion does not depend on the contraction).
For bounded finite based free right -complexes, torsion is additive over direct sums with concatenated bases; replacing the displayed degree- basis by bases whose coordinate columns are the columns of an invertible matrix changes the torsion by , so a reordering of a displayed basis changes torsion in by a sum of classes that are or ; and for a degreewise based exact sequence of contractible such complexes, (Basis-change, direct-sum and based exact-sequence formulas).
is written additively, , and for a discrete group one has , where is the class of the matrix ; in particular maps to in (K₁ of a ring and the Whitehead group of a discrete group).
An upper unitriangular matrix in specified ordered coordinates of lies in in those coordinates. After an arbitrary change of basis its matrix lies in the stable subgroup by normality, possibly only after stabilization at the elementary-matrix level. In either case its class is in and in (Stable elementary matrices equal the commutator subgroup, Stable general linear and elementary groups for right modules).
An elementary expansion is a homotopy equivalence: deform the characteristic ball onto its complementary boundary disk, fixing that disk. The deformation descends through the attaching map and is the identity on , giving a strong deformation retraction of onto (Homotopy equivalences, homotopy inverses and spaces of the same homotopy type, [F1]).
Proof
Assume first that is connected and put , ; by [F1] the new cells are and with . Choose an oriented lift of and an oriented lift of in the universal cover . By [F2] the relative cellular chain complex is a bounded finite based free right -complex with exactly two basis vectors, in degree and in degree , and all other terms zero.
The boundary of in the relative complex is a unit multiple of the free face: by [F1] the characteristic map is a homeomorphism from the interior of onto , maps into , and maps the complementary boundary into . On the quotient by , this face is one characteristic disk, so its relative incidence degree is even when its boundary points are identified in the closed cell. Thus in the cellular chains of the coefficient of in is for the deck transformation relating the two chosen lifts, and in right-module coordinates . Writing , the differential of has the matrix on right-module coordinate columns (so the coordinate map is left multiplication by ).
Define and in all other degrees. Then and , while on the only other degree the complex is zero, so and is contractible with .
Compute . If is odd, then and with matrix ; if is even, then and with matrix . In both cases [F6] gives in , and since with , the definition of in [F8] kills the class: the image of in is .
Write and , embedded in by the inclusion . This inclusion is well defined because in degree the displayed basis of is the basis of together with the lift when and together with nothing otherwise, so is a direct summand of . It is a chain map because is a subcomplex of by [F1], so preserves , and because the differential of displayed in [F4] then sends to ; by [F4] restricted to these submodules it is exactly the differential of .
The quotient of by is : the quotient in degree has basis the images of the complementary basis vectors, namely the lift for and none otherwise, matching the basis of of step 1.1, and the induced differential sends the class of to the class of , whose -part dies in the quotient and whose remaining part is the relative boundary computed in step 1.2; equivalently for the relative quotient map is a chain map with kernel . Hence is degreewise based exact after reordering the displayed basis of in each degree as the basis of followed by the image of the basis of ; a reordering of a displayed basis changes torsion in by a sum of classes of permutation matrices, each of which is or there ([F7], clause 2).
All three complexes of step 2.1 are contractible, bounded and based free: by step 1.3, by the explicit contraction , since and give , and by [F5] applied to the homotopy equivalence of [F10]. Hence [F7] gives in .
Claim: for every bounded finite based free right -complex . The contraction of step 3.1 is available, so by [F6] the torsion is the class of the matrix of in the displayed degree-ordered bases of and . Each basis vector occupies exactly two slots of , namely and , and the formula of step 3.1 matches them: the source slot maps to its matched slot with coefficient plus one correction term, namely when is odd and when is even. Order both bases by increasing degree and, within a degree, with the second summand before the first; this makes the matching order-preserving, and the correction term of a source slot always lies in a strictly earlier target slot, because for odd it lies in degree and for even it lies in the second summand of the degree- target block whose matched slot is in the first summand of that block. Hence in these matched orders the matrix is upper unitriangular, since each correction is in an earlier row than its matched diagonal entry, and has class by [F9]. Returning to the prescribed degree-ordered bases permutes rows and columns; these permutations contribute only classes of , killed in by [F7]. Thus the torsion in the prescribed bases is in .
Combining steps 3.1 and 4.1 with step 1.4: in . Its image is in by step 1.4, and therefore in , because is by [F3] the image of under the quotient map . This proves the first assertion for connected ; it also proves that the identity map of a based cellular complex of any finite CW complex has zero torsion.
Componentwise: for arbitrary finite CW complexes , the two new cells of the elementary expansion lie in a single component of , and is a bijection since with the free face attached inside by [F1]. By the componentwise definition of in [F3] and additivity over direct sums in [F7], is the tuple whose -entry is the torsion of the restriction of the component with the new cells and whose other entries are the torsions of the identity inclusions of the remaining components, each of which vanishes by step 5.1; the restriction falls under steps 1.1 through 5.1, so in . The relative complex of is concentrated in degrees and with the single entry of step 1.2, , and in by [F8].
Simple homotopy equivalences have zero torsion
Statement
Every simple homotopy equivalence of finite CW complexes has in the correctly transported target Whitehead group; for disconnected the vanishing holds componentwise in .
Facts & Assumptions
Given: A simple homotopy equivalence of finite CW complexes.
is simple when is homotopic to a finite composite in which each is an elementary expansion, an elementary collapse, or a cellular isomorphism, a cellular isomorphism meaning a homeomorphism carrying the cell structure of its source isomorphically onto that of its target; every such composite is a homotopy equivalence, a composite of simple homotopy equivalences is again simple, any map homotopic to a simple homotopy equivalence is simple, for disconnected complexes each operation is performed componentwise and respects the induced bijection on components, and the empty sequence exhibits the identity as simple (Simple homotopy equivalence, Homotopy equivalences, homotopy inverses and spaces of the same homotopy type).
The class attached to a choice of cellular representative, universal covers, lifts, basepoints, orientations, orders of the cells and chain contraction is independent of all these choices; homotopic homotopy equivalences of finite CW complexes have equal torsion; basepoint changes transport the class canonically; and for disconnected the statements hold componentwise (Whitehead torsion is independent of all auxiliary choices).
For homotopy equivalences , of finite CW complexes, in , componentwise for disconnected complexes (Composition and based-pair sum formulas for Whitehead torsion).
If is an elementary expansion of finite CW complexes, then (An elementary CW expansion has zero Whitehead torsion).
is the image in of the contraction torsion of the algebraic mapping cone of the lifted cellular chain map, for chosen cellular representative, universal covers and lift; the definition is by chosen data and produces a class in the Whitehead group of the target (Whitehead torsion of a finite CW homotopy equivalence).
An elementary collapse is the inverse formal operation of an elementary expansion: if is an elementary expansion then the pair deformation retracts onto , so the collapse map satisfies for the inclusion (Elementary expansions and collapses of finite CW complexes, Simple homotopy equivalence).
The identity map of the cover induces the identity matrix in the displayed based cellular bases of Based cellular chains of a universal cover as finite free right group-ring modules: the basis is one chosen oriented lift per cell, and the identity carries each such lift to itself, with the right module structure transported along the induced isomorphism of fundamental groups.
The cone differential is for the identity chain map. Its contraction torsion is the class of in ; a finite unitriangular matrix has class zero, and permutation matrices contribute only in that reduced group (The mapping cone of a chain map, Finite based free complexes and contraction torsion, Stable elementary matrices equal the commutator subgroup, K₁ of a ring and the Whitehead group of a discrete group, Cellular basis ambiguities vanish in the Whitehead group).
Proof
For every finite CW complex , the composition formula [F3] applied to gives , since the identity induces the identity on its Whitehead group. Subtracting gives , componentwise.
An elementary expansion has by [F4].
Let be a cellular isomorphism. By [F5] the class is computed from a chosen cellular representative, universal covers, lifts, basepoints, orientations and orders, and by [F2] the class in does not depend on these choices. Choose a universal cover and take the cover of to be , which is again a universal cover, with lift , so that ; with this choice is the identity chain map of the based free right -complex , by [F7] and the transport of coefficients along . For any finite based complex , the cone of its identity has contraction : . Pair the two cone slots of each vector , namely in degree and in degree . Order these pairs by increasing , with the same within-degree order in both parity bases. The odd-to-even map sends the source slot to its paired target slot with coefficient , plus a term involving , hence in a strictly earlier pair. Its matrix is upper unitriangular in these matched orders. Returning to the prescribed bases only permutes rows and columns, which does not change reduced torsion by [F8]. Thus has torsion , and by [F5].
Assume first that is connected and write for the fundamental group of the connected complex . By [F1] there is a chain with every elementary or a cellular isomorphism and ; by [F2] homotopic homotopy equivalences have equal torsion, so , and by [F3] applied inductively a sum of transported torsions of the factors. Hence it suffices to prove that each elementary factor and each cellular isomorphism of the sequence has torsion zero in the Whitehead group of its target; for we have and by [F2] and step 1.1.
Let be an elementary collapse, the corresponding elementary expansion, so that by [F6]; both and are homotopy equivalences by [F1] and [F6]. Applying [F3] to the pair gives in , and by step 1.1 while by step 1.2; hence .
By steps 1.2, 1.3 and 2.2 every factor of the sequence of step 2.1 has zero torsion, so the transported sum of step 2.1 vanishes and in . This proves the assertion for connected ; the case of disconnected follows componentwise, since each restricts to an elementary operation or a cellular isomorphism on the components that it meets and to a homeomorphism of the remaining components, the induced summands are as in [F2] and [F3], and each summand vanishes by the connected argument applied to that component (with the empty sequence handled by step 2.1).
The target of a finite cellular mapping cylinder is a simple subcomplex
Statement
For any cellular map of finite CW complexes, the target inclusion is a finite composite of elementary expansions. If is a homotopy equivalence, the source inclusion is a homotopy equivalence, and for the canonical retraction ; is a homotopy inverse of , is homotopic relative to to a finite composite of elementary collapse maps, and has zero torsion.
Facts & Assumptions
Given: A cellular map of finite CW complexes, the mapping cylinder with its inclusions and canonical retraction .
An elementary expansion of dimension attaches a pair of cells such that the characteristic map of the upper cell restricts on one boundary disk to a characteristic map of the new -cell, homeomorphic on its interior, while all complementary boundary values lie in the previously constructed subcomplex . The pair deformation retracts onto . A finite composite of elementary expansions is a formal deformation, and the operation is componentwise (Elementary expansions and collapses of finite CW complexes).
For a cellular equal to the identity on a common subcomplex , the quotient is a CW complex whose cells are those of , those of the free end , and one -cell for every -cell of ; its embedded copies and are subcomplexes, and the map with , is a strong deformation retraction fixing (Cellular mapping cylinders and relative cylinders are CW complexes).
A map is a simple homotopy equivalence if it is homotopic to a finite composite of elementary expansions, elementary collapses and cellular isomorphisms; every such composite is a homotopy equivalence, composites of simple homotopy equivalences are simple, and any map homotopic to a simple homotopy equivalence is simple (Simple homotopy equivalence).
Every simple homotopy equivalence of finite CW complexes has zero Whitehead torsion in the target Whitehead group; in particular the identity map of a finite CW complex, exhibited as simple by the empty sequence, has zero torsion (Simple homotopy equivalences have zero torsion).
For homotopy equivalences , of finite CW complexes, (Composition and based-pair sum formulas for Whitehead torsion).
is defined for homotopy equivalences of finite CW complexes, taking values in the Whitehead group of the target, with the componentwise convention for disconnected targets (Whitehead torsion of a finite CW homotopy equivalence).
A map is a homotopy equivalence if there is with and ; such a is a homotopy inverse of (Homotopy equivalences, homotopy inverses and spaces of the same homotopy type).
A map homotopic to a homotopy equivalence is a homotopy equivalence (A continuous map homotopic to a homotopy equivalence is itself a homotopy equivalence).
Proof
Take in [F2], so that is the ordinary mapping cylinder with , and , and , ; its cells are the cells of , the free-end cells for the cells of , and the prism cells of dimension for the -cells of , finitely many in all.
Order the cells of the finite complex by increasing dimension and, for each -cell of with characteristic map , let denote the subcomplex obtained from the previously built subcomplex by first attaching the free-end cell and then the prism cell . Its closure is the image of and its boundary consists of the pieces , and ; under the identification the first piece maps into , under the cellularity of the middle piece maps into , and the last piece is exactly the closed free-end cell attached in the previous step. The ball pair is homeomorphic to , so the characteristic prism map exhibits an -cell pair with free face corresponding to an upper hemisphere, so is an elementary expansion of dimension by [F1].
Performing the steps of step 1.2 for the finitely many cells of in increasing dimension gives a finite chain of elementary expansions whose composite is , so is a simple homotopy equivalence by [F3] and by [F4].
By step 1.1, , and by [F2] the strong deformation retraction gives , so is a homotopy inverse of the homotopy equivalence in the sense of [F7]. Applying [F5] to the composable homotopy equivalences and gives in ; the left side is by [F4] and by step 2.1, hence . Reverse the expansion sequence of step 2.1 and choose the elementary collapse retraction for each pair. Their composite fixes . If is the deformation from to supplied by [F2], then is a homotopy from to , relative to . Thus is homotopic relative to to that collapse composite and has zero torsion; no equality of these retractions is asserted.
Suppose now that is a homotopy equivalence. By [F7] and step 1.1, , so is homotopic to the composite ; here is a homotopy equivalence by hypothesis, is a homotopy equivalence by step 3.1, and a composite of homotopy equivalences is a homotopy equivalence, so is a homotopy equivalence by [F8].
In the situation of step 4.1 the maps and are homotopy equivalences with , so [F5] applies to the pair and gives in by [F6], since by step 3.1.
For disconnected and the construction is componentwise: maps each component of into a component of , over a target component the cylinder is together with the cylinders on all components of mapping into , while target components receiving none are unchanged. The expansion sequence of step 1.2 is performed component by component, and the identities of steps 2.1–5.1 hold in the corresponding summands of the Whitehead groups by [F6].
Cell trading puts a finite relative equivalence in two high degrees
Statement
Let be finite connected CW complexes with the inclusion a homotopy equivalence. Relative to , finitely many elementary expansions and collapses transform into a pair whose relative cells occur only in two adjacent degrees with . The deformation respects the homotopy class and transports the relative torsion. The low-dimensional - and -cell cases are included, using connectedness and the induced -isomorphism.
Facts & Assumptions
Given: Finite connected CW complexes whose inclusion is a homotopy equivalence.
An elementary expansion of dimension is an inclusion of CW complexes equipped with a homeomorphism of ball pairs and a continuous map that is a characteristic map for a new -cell and restricts on to a characteristic map for a new -cell, with all remaining boundary values in . The new -cell is the free face; the restriction is homeomorphic on its interior, while boundary identifications in its closure are allowed (Elementary expansions and collapses of finite CW complexes).
An elementary collapse is the inverse formal operation removing the two new cells of an elementary expansion. A finite sequence of elementary expansions and collapses, performed relative to the cells retained at each step, is a formal deformation (Elementary expansions and collapses of finite CW complexes).
For every based pair the sequence is exact at each term with an incoming and outgoing arrow (Long exact sequence of relative homotopy groups).
A map of CW pairs that is continuous and cellular on , with having finitely many cells, is homotopic rel through maps of pairs to a cellular map with for every , and two cellular maps homotopic rel admit a cellular homotopy rel with the prescribed endpoints. These finite-relative-source assertions hold without any choice principle (Cellular approximation for maps of CW pairs).
If is a CW subcomplex whose inclusion is a homotopy equivalence, then strongly deformation retracts onto (Cw homotopy equivalence inclusions are strong deformation retracts).
A map of finite CW complexes is a simple homotopy equivalence if it is homotopic to a finite composite of maps each of which is an elementary expansion, an elementary collapse, or a cellular isomorphism (Simple homotopy equivalence).
Every simple homotopy equivalence of finite CW complexes has in (Simple homotopy equivalences have zero torsion).
For homotopy equivalences and of finite CW complexes one has in (Composition and based-pair sum formulas for Whitehead torsion).
For a cellular map of finite CW complexes the target inclusion is a finite composite of elementary expansions; if is a homotopy equivalence then for the canonical retraction (The target of a finite cellular mapping cylinder is a simple subcomplex).
If is a relative CW complex then has the homotopy extension property, hence is a cofibration (Relative CW inclusions are cofibrations).
Proof
Since the inclusion is a homotopy equivalence, it induces isomorphisms for every and a bijection ; exactness of [F3] at for then forces , and connectivity of together with makes every vertex of the endpoint of a path in from a vertex of .
For let be a relative vertex; the path of step 1.1 starting at is a homotopy with the identity on the point and , the boundary condition being vacuous.
Suppose all relative cells of outside have dimension at least , and let be a relative -cell with attaching map . For , injectivity of makes null-homotopic in , so choose a filling with boundary . The sphere obtained by gluing to the reverse of represents a class of ; surjectivity of permits changing by a sphere map in until this glued sphere is null. The resulting null-homotopy is precisely a homotopy from into fixing its entire boundary. For , choose a path in connected between the endpoints of and use the isomorphism to homotope the two paths rel endpoints; the separate case is handled by the vertex path.
Put , with its actual CW structure inherited from . Extend the homotopy of step 2.2 (or the vertex path of step 2.1) by the identity on to a map ; it descends through the attaching identifications because the boundary track is fixed. Its endpoint is a retraction . Apply [F4] to relative to , obtaining a cellular and a homotopy rel from to . Concatenate with , and apply the cellular-homotopy clause of [F4] to the maps and , relative to . Both endpoint maps and the fixed track are cellular. Restriction along the characteristic map now gives a homotopy with , , and , since . Its boundary lies in . This applies approximation on , not on a sphere whose attaching map might be noncellular.
Write , an -ball. Attach an -cell to by , whose image lies in by the endpoint and boundary bounds of step 3.1. Then attach an -cell using a boundary sphere written as two -disks glued along their boundary: map one disk by and the other by the characteristic map of , with matching boundary parameterizations. This defines a CW complex and an elementary expansion , with as its free face. The subspace is a subcomplex. Denote by below.
In the subcomplex the cell is a free face of : the attaching map of restricts on the face to the characteristic map of , a homeomorphism from the open disk onto , and maps the complementary part into by step 3.1; no other cell of has the interior of in its closure, since and is the only other cell of outside . Hence is an elementary collapse and is an elementary expansion of of dimension .
By [F5] and [F10] the pair admits a strong deformation retraction with , and . First apply [F4] to the endpoint retraction to obtain a cellular map homotopic to relative to . The subspace is a CW subcomplex of , so its inclusion is a cofibration by [F10]. Extend the endpoint homotopy from to across by HEP while retaining the bottom identity and the fixed track. This produces a deformation from to , fixed on , whose restriction to all of is cellular. Now apply [F4] to this prism map relative to to make the entire homotopy cellular without changing its bottom, side or top. With the product CW structure, lies in the -skeleton of , so the resulting homotopy satisfies ; its endpoint satisfies for every . The later push uses both this endpoint bound and the prism bound: if an attaching sphere lands in , its side track lands in . No degree- bound on the full track is asserted.
Push claim. Let be any map, put with characteristic map of its new cell, and put with characteristic map ; then and are related by finitely many elementary expansions and collapses. Indeed is the complex with the cell attached along and is the complex with that cell attached, so is obtained from by adding back the elementary expansion pair; moreover matches at .
In the situation of step 7.1 build from by attaching a further -cell along and a -cell whose boundary disk is glued by the usual three pieces: the face by , the face by the characteristic map of , and the side by , which is legitimate as a CW attaching map because and the bound of step 6.1 puts its side track in ; the two end values agree with the corresponding face maps. Then is an elementary expansion of dimension with free face , and likewise is an elementary expansion of dimension with free face the -cell of ; both use [F1], the side values lying in .
In the closure of the new -cell meets exactly in , so it is disjoint from the interior of ; therefore the interior of lies in the closure of no cell of other than and , and the elementary collapse of step 5.1 is still available in : . Reading the move of step 8.1 followed by the collapse just constructed gives a formal deformation , so and are related by elementary expansions and collapses.
Transport along a deformation. If is a formal deformation of finite CW complexes in which each collapse step admits the cellular retraction data of step 6.1, and is an attaching map, then is related by elementary expansions and collapses to , where is obtained from by composing with the cellular inclusions of the expansion steps and the time-one maps of the collapse steps. This is proved by induction on : a collapse step is step 9.1 applied with and , an expansion step changes no attaching data because differs only by the expansion pair, and the induction hypothesis is then applied to the remaining steps with the transported attaching map, which is legitimate because the time-one maps are cellular on the complex they contract.
Trading one cell. Take as in step 5.1 and attach the relative cells of other than in their original CW order, followed by the new -cell of . This is a legitimate relative CW filtration over : every old cell's attaching image lies in the earlier old skeleta (now including ), and the last cell attaches by , which is present by then. It is not asserted that the other old relative cells of degrees and lie in , nor that the new last cell attaches to alone. Repeatedly applying step 10.1 to push each attaching map across the collapse produces a formal deformation from to a complex in which each has the same dimension as the corresponding old cell, and the final new cell has dimension . This is the finite push construction in Cohen’s cell-trading construction, printed pp.25–26.
Consequences for the trading step. By steps 4.1 and 11.1 the complexes and are related by finitely many elementary expansions and collapses, and every move is performed relative to the cells retained by the previous steps and fixes ; the relative cells of over are the relative cells of other than , each with the same dimension, together with one cell of dimension . Hence has one relative -cell fewer than , has no relative cells of dimension below , and agrees with in the number of relative cells in every degree other than and .
For the iteration, let be a finite CW complex containing and related to by a formal deformation fixing ; the composite of the moves restricts to the identity on and is a homotopy equivalence , so applying step 1.1 to the pairs and and using exactness of [F3] at for gives as well.
Iterating step 12.1 for using the data of steps 2.1, 2.2 and 13.1 removes all relative cells of dimension at most two and yields a finite CW complex , related to by finitely many elementary expansions and collapses relative to , all of whose relative cells have dimension at least three.
Choose once and for all an integer . For each in this finite list, apply step 12.1 to every relative -cell then present. Each trade deletes one -cell and creates only an -cell, so no later trade creates a cell in a degree already processed. By step 13.1 the required relative homotopy groups remain zero. At the end no relative cell has degree below , while every old cell had degree at most and every created cell has degree at most . Thus the only possible relative degrees are , exactly the fixed-target argument of Cohen’s two-layer reduction, printed pp.26–27.
Torsion transport. The composite of the moves of the deformation is a finite composite of elementary expansions, elementary collapses and identities between finite CW complexes, hence a simple homotopy equivalence by [F6] and satisfies in by [F7]; writing and for the inclusions, and [F8] give , so the relative torsion is transported by .
By steps 14.1, 15.1 and 16.1 the finitely many elementary expansions and collapses constructed above carry to a pair whose relative cells lie only in two adjacent degrees with , the deformation fixes and hence respects the homotopy class of the inclusion, and the relative torsion is transported along it; the cells of dimension and were removed in the first iteration using the connectedness data of step 2.1 and the -isomorphism of step 1.1. ∎
Two high relative cell layers have free homotopy bases and their cellular boundary matrix
Statement
Let be connected finite CW complexes, let be an isomorphism, and suppose that the relative cells of over occur only in dimensions with . Put together with the relative -cells and . Then and are finite free right -modules on the chosen oriented characteristic cells, up to . The triple boundary is represented in those bases by the relative cellular differential . If is a homotopy equivalence, is an isomorphism, hence its matrix is invertible.
The right -module structure meant here is induced on the universal-cover relative homotopy groups by deck transformations, with basepoints transported back along paths in the corresponding simply connected subspaces or , and then transported to the base-side groups by the covering isomorphisms of step 3.2 below. The change-of-basepoint map is independent of the path because those subspaces are simply connected. A chosen oriented characteristic cell means one chosen lift of the cell together with one orientation of it. Changing the lift multiplies the corresponding basis element by an element of and reversing the orientation multiplies it by , so the basis is determined only up to these factors ; every such change alters a representing matrix only by the corresponding change of basis, and the assertions below are unaffected by it.
Facts & Assumptions
Given: Connected finite CW complexes whose relative cells occur only in dimensions with , with an isomorphism; a basepoint that is a vertex, the universal cover , and for .
Relative to , finitely many elementary expansions and collapses transform into a pair whose relative cells occur only in two adjacent degrees with , and the deformation respects the homotopy class of the inclusion and transports the relative torsion (Cell trading puts a finite relative equivalence in two high degrees).
For a CW pair with universal cover , the preimage is a CW subcomplex of the lifted CW structure, the -skeleton of that structure is , and the preimage of a relative sum is its -skeleton; a deck transformation is determined by its value at one point and acts freely, so the lifts of a single cell are exactly the cells for one chosen lift (Based cellular chains of a universal cover as finite free right group-ring modules).
On the chains of the deck group acts on the left and the right -action is , and each is a homeomorphism of the pairs , so the action passes to the homology of those pairs; for chosen oriented lifts of the relative cells the group is a finite free right -module on those lifts, the lifts of one cell forming the -orbit of the chosen lift (Based cellular chains of a universal cover as finite free right group-ring modules).
Let be a nonempty simply connected CW complex, , and , and attach a set of oriented -cells directly to with supplied characteristic maps ; then and are free abelian on these cells, with basis elements and satisfying for the relative Hurewicz map , the class is represented by moving the marked boundary value of to through and extending, and the result is independent of these choices and choice-free (A relative single cell layer has compatible homotopy and homology bases).
If a CW pair has all cells outside of dimension at least , then is a bijection when and is an isomorphism for at every ; no choice principle is used (High relative cells do not change lower homotopy).
Let be path-connected and locally path-connected, based, and a covering; a based lift of exists if and only if , and it is then unique (Lifting criterion for maps from path-connected locally path-connected spaces).
For every the sphere is simply connected, in particular ( is simply connected for every ).
If is a covering, a homotopy and a lift of , then there is a unique lift of extending (Existence and uniqueness of homotopy lifts through a covering map).
For every based pair the relative homotopy sequence is exact at each term with an incoming and outgoing arrow, the arrows being homomorphisms where both group structures exist (Long exact sequence of relative homotopy groups).
Restriction to the face defines the boundary , a homomorphism for , and maps and homotopies of based pairs act functorially on these boundaries (Relative homotopy operations are well defined in their valid degrees); relative nullity is equivalent to compression of a disk model into fixing the whole disk boundary, so classes and boundary values may be computed on disk models (Relative cubical disk model and compression).
If a morphism of long exact sequences in an abelian category is an isomorphism at four consecutive terms around a term, then it is an isomorphism at that term as well (Five lemma for a morphism of long exact sequences).
For and the triple sequence is natural in based maps of triples and exact at its three middle terms, where is the boundary for followed by the relative map for ; these statements need no choice and no CW hypotheses (Relative homotopy exact sequence of a triple in group degrees).
The absolute Hurewicz homomorphism is and the relative one is , where is the class whose homology boundary is the positive boundary-sphere generator; both are well-defined, natural in based maps and based maps of pairs, and reversing both orientations multiplies them by (Absolute and relative Hurewicz homomorphisms).
For a CW pair , an ordinary homology theory and , , the groups are direct sums of copies of the coefficient group indexed by the relative -cells, and the differential is the triple boundary to followed by its map to , with (Any ordinary homology theory has a cellular chain complex on a cw pair).
For a path-connected, locally path-connected and semilocally simply connected base, the deck group of a universal cover is isomorphic to the fundamental group by the assignment carrying a loop class to the deck transformation that moves the chosen fibre point to the corresponding lifted endpoint of that loop (For a path-connected locally path-connected semilocally simply connected base, the deck group of a universal cover is isomorphic to the fundamental group).
For a covering and a path in with a point of , there is a unique lift of starting at (Existence and uniqueness of path lifts through a covering map).
Monodromy acts on each covering fibre by bijections, and its orbit through a point is exactly the intersection of the path component of with that fibre (Monodromy acts by fibre bijections, and its orbits are the intersections of path components with the fibre).
A covering is a continuous surjection in which every point of the base has an evenly covered neighbourhood , that is, is a disjoint union of open sets each mapped homeomorphically onto ; these are the sheets over (Covering maps, evenly covered neighbourhoods, fibres, sheets, and trivial coverings).
If is a CW subcomplex whose inclusion is a homotopy equivalence, then strongly deformation retracts onto (Cw homotopy equivalence inclusions are strong deformation retracts).
A based map induces maps on homotopy groups, identities and composition are preserved, based homotopic maps induce equal maps, and based homotopy equivalences induce isomorphisms (Higher homotopy groups are functorial and based homotopy invariant).
If is a path in from to , it induces a change-of-basepoint isomorphism ; these maps have the identity, inverse-path and path-composition properties of the absolute change-of-basepoint maps, and loops in act on the relative homotopy groups. Thus if is simply connected, the isomorphism is independent of the path between its endpoints (Hatcher, Algebraic Topology, §4.1, printed pp.341–342 and 345).
For every discrete group , an isomorphism of finite free right -modules forces (Integral group rings have invariant basis number).
Proof
The situation of the statement is the one produced by [F1]: for a finite relative homotopy equivalence the cell-trading lemma yields, relative to , a formal deformation to a pair whose relative cells lie in two adjacent degrees, with the deformation respecting the homotopy class of the inclusion and transporting the relative torsion, and this statement therefore applies to each pair so produced; conversely it applies verbatim to any pair satisfying its two-layer hypothesis. All claims below concern a pair with relative cells only in the two degrees , a vertex basepoint , and .
Let be a universal cover and put and , where . Then and are CW subcomplexes of the lifted CW structure, is carried by and the lifts of the relative -cells, and is carried by and the lifts of the relative -cells. This distinction matters when has cells above dimension . The deck group is identified with and acts freely on , the lifts of a single cell forming one orbit , and the right action on chains is , which passes to the homology of the pairs .
The restrictions and are coverings: if is an evenly covered neighbourhood of a point with sheets over , then is the disjoint union of the sets , each mapped homeomorphically onto because .
Every relative -cell of has attaching map with image in , and is simply connected because , so the attaching map lifts to by the lifting criterion; hence the relative cells of are exactly the lifts of the relative -cells, attached directly to , and the relative cells of are the lifts of the relative -cells, attached directly to because is simply connected for .
The space is path-connected and simply connected. The monodromy action of on the fibre is transitive, because the monodromy of a loop class is the deck transformation of the universal cover [F15], the deck group is transitive on the lifts of the vertex [F2], and is onto since it is an isomorphism; hence the whole fibre over lies in one path component of [F17], and every point of is joined to that fibre by a lifted path [F16], so is path-connected. Also is trivial: for a loop at with one has , so and then because is injective, and a null-homotopy of in lifts through the covering to a null-homotopy of because is trivial [F6].
Applying the high-relative-cells lemma to the pair , whose relative cells all have dimension , gives a bijection and an isomorphism ; by step 1.5 the space is therefore nonempty, path-connected and simply connected.
By the single-cell-layer lemma applied to , and the lifted -cells with their lifted characteristic maps, and are free abelian on the lifts of the relative -cells, with basis classes and satisfying ; the construction is choice-free and the class is independent of the choices made in representing it.
For the covering induces an isomorphism : it is injective because a null-homotopy of the composite of a based map with lifts to a null-homotopy of that map by homotopy lifting [F8], and it is surjective because is simply connected for , so every based map lifts through the covering by the lifting criterion [F6, F7]. The same argument applies to the coverings and .
Suppose now that the inclusion is a homotopy equivalence. By [F19] strongly deformation retracts onto , and the time-one map of that retraction satisfies and , so by [F20] the map is an isomorphism for every . Exactness of the pair sequences [F9] then gives for every : for both and are isomorphisms, so the kernel of and the image of vanish, while for the isomorphism makes the pointed set trivial since and are connected. In particular and .
By the same lemma applied to , and the lifted -cells, and are free abelian on the lifts of the relative -cells, with .
The covering projection is a based map of pairs, so by functoriality of boundaries [F10] it induces a morphism between the long exact sequences of and and between those of and ; these sequences are exact [F9], and the comparison maps in the degrees are isomorphisms by step 2.3, all of those degrees being at least because . The five lemma [F11] applied to the window and to the window therefore gives isomorphisms of abelian groups and .
If the inclusion is a homotopy equivalence, the triple boundary is an isomorphism. In the triple sequence of [F12] with , and , exactness at makes it surjective, because is trivial by step 2.4 and the kernel of is therefore all of . It is also injective: write for it and for the pair boundary , so that with ; if then by exactness of the pair at , say , and composing with , which kills by exactness of the pair at , gives , so that because is an isomorphism and thus ; then exactness of the pair at writes for the map , which by naturality of the pair sequences in the map of pairs factors as the composite of with and is therefore zero because by step 2.4; hence and is injective.
For either lifted pair, write and let be its simply connected subspace ( for and for ). Define the right action by where is any path in from to and changes the basepoint back to . Such paths exist, and [F21] makes the result independent of the path. This is a right action: applying and then applies and concatenates the path from to with the image under of the path from to , a path from to ; path-composition for gives . The class construction in [F4] moves the marked boundary value through ; applying transports that move, and any path used to define the translated cell class differs from the transported path by a loop in simply connected , so [F21] identifies the based classes. Thus is the basis class of the lift . The corresponding change-of-basepoint shell lies in , so relative Hurewicz sends this class to . As the lifts form a free -orbit [F2], each homotopy and homology basis set is a free -orbit.
The relative Hurewicz homomorphisms of steps 2.2 and 3.1 are isomorphisms because they carry a free basis to a free basis, and for the triple the square with upper row and lower row , joined vertically by , commutes: the triple boundary is the boundary of the pair followed by the relative map of [F12], on disk models these are restriction to the boundary sphere followed by the induced map of pairs [F10], and is natural in based maps of pairs with [F13], so for a disk model one has , the middle equality because has homology boundary the positive sphere generator.
Choose one oriented lift for each relative cell and write . By step 4.1, is the basis class of ; as varies these are exactly the lifts of , once each. Therefore and are finite free right -modules on the chosen oriented characteristic cells, and the same holds for and with the classes .
With one has , and . Apply [F14] to integral homology of the universal-cover pair. Its differential is precisely the composite in the square of step 4.2: the triple boundary to followed by the map to . Deck transformations commute with the integral connecting maps, so this differential is right -linear on the free abelian groups indexed by lifted cells. Thus its matrix in one chosen lift per cell is exactly the matrix of ; no second change of coefficients to is made.
Define the right action of on and on by ; this is a well-defined right action because is an isomorphism by step 3.2 and the cover-side action is the right action established in step 4.1. Thus is an isomorphism of right -modules carrying the basis of step 5.1 to a basis of the base-side module. Hence and are finite free right -modules on the chosen oriented characteristic cells: replacing the chosen lift by replaces by , and reversing the orientation replaces by , so the basis is determined only up to these factors , and such a change alters a representing matrix only by the corresponding change of basis.
The isomorphism of step 3.2 carries the chosen basis of the cover to the chosen basis of the base, and by step 6.1 the boundary of the statement is the image under of the triple boundary of step 4.2; hence the matrix of in the chosen bases is exactly the matrix of the relative cellular differential computed in step 5.2.
By steps 7.1 and 3.3 the triple boundary is represented in the chosen bases by and is an isomorphism whenever the inclusion is a homotopy equivalence. Since , [F22] forces its finite free source and target ranks to be equal, so the representing matrix is square; the matrices of the isomorphism and its inverse are mutually inverse by the coordinate description of right-linear maps. In the degenerate case in which the pair has no relative cells both modules are the zero module and the empty matrix is invertible. ∎
Cell slides and stabilizations realize elementary group-ring matrices
Statement
Let be a homotopy-equivalence inclusion of connected finite CW complexes, with only relative cells in degrees , . Put , choose oriented lifts, and let be the invertible relative boundary matrix in the right-module column convention. A finite formal deformation fixing realizes for elementary matrices over and . Reordering, reversing orientations, and changing lifts implement permutations and diagonal factors . Every resulting pair has the same relative simple type over .
Facts & Assumptions
Given: The finite connected homotopy-equivalence pair and chosen bases in the statement.
In two high relative cell degrees, the relative homotopy groups have free right -bases on the lifted cells, their triple boundary is the cellular boundary, and for a homotopy equivalence this boundary is an isomorphism (Two high relative cell layers have free homotopy bases and their cellular boundary matrix).
An elementary expansion adds a free-face cell pair and its collapse removes it; both operations may fix a retained subcomplex (Elementary expansions and collapses of finite CW complexes).
The inclusion of a CW subcomplex is a cofibration, so homotopies of its attaching maps extend over finite cell attachments (Relative CW inclusions are cofibrations).
Reordering, orientation reversal and a new deck lift change a group-ring cellular basis by a permutation or a diagonal factor ; elementary changes and these trivial units do not change its Whitehead class (Cellular basis ambiguities vanish in the Whitehead group).
The stable elementary subgroup is normal in (Stable elementary matrices equal the commutator subgroup).
For the pair the kernel of is the image of . For , the standard sphere classes map to the relative cell basis, so any class in is a sum of those sphere classes with group-ring coefficients and a class from (Long exact sequence of relative homotopy groups, [F1]).
Proof
Each attaching sphere of a relative -cell maps into . Its class in maps to zero in because the cell fills it. The inclusion is a homotopy equivalence, so that homomorphism is injective; each attaching sphere is therefore null-homotopic in . This also holds for , where the relevant group is .
A chosen null-homotopy changes that attaching map to a constant map through the standard collar: attach a copy of the -cell and an -cell whose two cap faces are the old and new characteristic disks and whose side is the homotopy, then collapse the old cap. This is precisely the two-expansion/collapse comparison of homotopic attaching maps in Cohen’s attaching-map comparison (printed p.23), carried out relative to using [F2] and [F3]. Repeat finitely for the lower cells and push the attaching maps of the upper cells across each collapse by the same collar construction. Thus the pair is formally deformed relative to to simplified form, where every lower -cell is trivially attached at the chosen base vertex of . The deformation does not change its relative simple type.
In simplified form put , and write for the attaching map of the th upper -cell and for its relative class. Given distinct upper indices and , represent the based sphere class by a finite pinch-and-whisker map : one sphere summand gives , and the finitely many other signed summands give the -translates of . Since , is abelian; the right group-ring action and triple boundary are those of [F1], so the relative image of is . This constructs an attaching map for a new upper cell, not a replacement characteristic disk for an existing lower cell.
Attach at the basepoint of a trivially attached -cell and an -cell whose attaching sphere wraps once around that new -sphere and misses the old relative cells. The new lower cell is a free face after choosing the evident characteristic maps, so this is an elementary expansion relative to ; its relative boundary adds a diagonal block and zero off-diagonal blocks. Repeating gives .
Let be the CW subcomplex containing and all upper cells except ; since , it contains . The attaching sphere extends over the characteristic disk of in , so every whiskered multiple is null-homotopic in . Thus and the map of step 3.1 are homotopic as maps into . Apply the finite collar expansion/collapse comparison of homotopic attaching maps, as in step 2.1, to replace the th upper cell attached by with a new upper cell attached by ; all other cells and stay fixed. In the unchanged lower basis and the upper basis in which only is replaced by its new characteristic class, the th boundary column changes from to by step 3.1, while every other column stays fixed. Hence the new matrix is in the right-module column convention. The reverse collar realizes its inverse . This is Cohen’s cell-slide construction, printed pp.31–32, translated from his upper-indexed row notation.
For an elementary left factor and an matrix , normality [F5] gives in the stable group. Thus for some finite , the matrix is a product of elementary matrices of size . First perform the stabilizations of step 3.2. The upper-cell slides of step 4.1 for that product then change to . This establishes the desired operation with extra identity pairs; the next step removes those pairs geometrically. No unstabilized normality is assumed.
The lower skeleton is still : the slides changed only upper attaching maps. For an added lower index , the corresponding upper attaching map has relative class , and every other upper map has zero th coordinate. By [F6], the first is homotopic in to , where traverses the th lower sphere once and lies in ; represent this sum with the traversal on one disk and the -map on its complementary disk. Every other upper map is homotopic to a finite sum of sphere terms using only the other lower indices and a term in , so it can avoid the interior of this lower cell. Make these replacements using the collar construction of step 2.1. Now the th lower cell is a genuine free face of its matched upper cell, and no other upper cell meets its interior. Collapse this pair. The other relative coordinates are unchanged because the homotopies took place in and the remaining maps avoid that pair. Repeating for the added indices leaves exactly the matrix . Thus stabilization has not weakened the claimed original-size operation.
A simultaneous left and right elementary operation is a finite composite of steps 5.1–6.1 and 4.1; stabilization may be inserted first. Basis permutations, orientations and lifts have exactly the effects asserted in [F4]. All constructions used finitely many cells and finitely many summands of a group-ring coefficient, and each map fixes , proving the statement. ∎
An identity relative homotopy matrix permits cell cancellation
Statement
Let be a connected finite CW pair with only relative cells in degrees , where . If the triple boundary in the chosen free homotopy bases is an identity matrix, then a finite sequence of elementary expansions and collapses relative to carries to . Equality of cellular incidence numbers is used through the relative homotopy boundary, never directly as a free-face condition.
Facts & Assumptions
Given: The two-layer pair and identity matrix in the statement.
The two relative homotopy groups have free group-ring bases on the cells and the triple boundary is represented by the relative cellular matrix (Two high relative cell layers have free homotopy bases and their cellular boundary matrix).
Relative CW inclusions are cofibrations, so attaching-map homotopies extend over subsequently attached cells (Relative CW inclusions are cofibrations).
An elementary expansion adds, and a collapse removes, a cell pair with a genuine specified free face (Elementary expansions and collapses of finite CW complexes).
The long exact homotopy sequence of a pair identifies the kernel of as the image of and sends each relative characteristic disk to its attaching-sphere class in (Long exact sequence of relative homotopy groups).
Proof
Write . For each lower characteristic class , the identity matrix supplies an upper class with triple boundary . The composite is zero by exactness of the triple/pair boundary construction. Thus : the attaching sphere of each lower cell is null-homotopic in .
Apply the finite homotopy-of-attaching-map collar of Cohen’s attaching-map comparison, printed p.23, to trivialize each lower attaching map, pushing upper maps along the induced deformation. This uses [F2] and [F3], and is the simplification established in Cell slides and stabilizations realize elementary group-ring matrices. The resulting lower skeleton has the form , and the relative homotopy matrix is still the identity after transporting its characteristic bases.
The relative inclusion of the wedge has, in degree , a split exact sequence : retraction splits the first map, and the constant lower attaching maps make the last boundary zero. A relative basis vector therefore has a spherical representative that maps a chosen -disk homeomorphically through the characteristic disk of and sends its complement to the basepoint in . More generally, a class with zero th relative coordinate has a representative avoiding the interior of , since its -linear sphere terms use only the other wedge summands and its residual term lies in .
Let be the attaching map of the th upper cell. Its relative image is by the identity-matrix hypothesis, while has the same image. Exactness in step 3.1 gives ; represent this difference by a based sphere in and pinch it into the complementary disk of . The resulting map is homotopic to through maps to and still maps one prescribed disk homeomorphically onto the lower th cell with every other point outside that cell. This is the homotopy-level correction in Cohen’s identity-matrix cancellation, printed p.30.
For , the identity matrix gives zero th relative coordinate to . By the last clause of step 3.1, homotope to an attaching map missing the interior of . Replace the upper attaching maps by these homotopic representatives, one at a time, via finite collar expansions and collapses relative to ; [F2] transports subsequent attachments. Afterward occurs in the boundary of exactly the corrected upper cell , and the corrected meets it on one disk by a homeomorphism. It is now a genuine free face and [F3] removes the pair.
The remaining pair still has only - and -cells, and its triple boundary in the remaining transported bases is the identity with row and column deleted: the other corrected upper maps have no term and the first upper map is gone. Induct on the finite common number ; for the pair already equals , while step 5.1 reduces by one. The finite concatenation of relative elementary moves proves the claim. ∎
Zero relative torsion gives a finite relative elementary deformation
Statement
Let be a homotopy-equivalence inclusion of connected finite CW complexes. If in , then is carried to by finitely many elementary expansions and collapses fixing , with only reorderings, orientation reversals and deck-lift changes of the cellular bases. This is the geometric converse for inclusions.
Facts & Assumptions
Given: The finite homotopy-equivalence inclusion with zero Whitehead torsion.
Finite relative cell trading fixes , transports torsion and leaves cells only in two degrees with (Cell trading puts a finite relative equivalence in two high degrees).
In that two-layer pair the relative cellular differential is an invertible matrix in the group-ring homotopy bases (Two high relative cell layers have free homotopy bases and their cellular boundary matrix).
Finite relative elementary moves realize left and right stable elementary matrix operations, identity-block stabilization, and the listed trivial basis changes (Cell slides and stabilizations realize elementary group-ring matrices).
An identity relative homotopy matrix permits cancellation of all relative cells by finite elementary moves (An identity relative homotopy matrix permits cell cancellation).
For , , in additive notation (K₁ of a ring and the Whitehead group of a discrete group).
The torsion of a homotopy-equivalence inclusion is the based relative universal-cover chain torsion, and for a two-term complex in degrees its class is in (Whitehead torsion of a finite CW homotopy equivalence).
A simple deformation has zero torsion and the composition formula transports inclusion torsion along it (Simple homotopy equivalences have zero torsion, Composition and based-pair sum formulas for Whitehead torsion).
Proof
Apply [F1] to obtain a two-high-layer pair and a simple homotopy equivalence fixing . By [F7], ; the group isomorphism induced by transports this equality without selecting a new generator.
Choose the finite lower and upper lifted-cell bases of [F2]. The cellular differential is , including the empty matrix when . By [F6] its torsion is , so zero torsion implies in . The parity sign has no effect on vanishing.
By the definition of the quotient [F5], there is a finite diagonal block with and , and a stabilization size , such that lies in the stable elementary subgroup. Equivalently, after a common finite stabilization, differs from a product of elementary matrices by finitely many trivial units. This uses equality in the direct limit , so the stabilization is finite; it does not assert that an arbitrary unit of is trivial.
Apply [F3] for the identity-block stabilization and for the finite elementary factors in the inverse order. Absorb each diagonal by changing the orientation or chosen deck lift of its corresponding cell. The resulting relative boundary matrix is the identity in the transported characteristic bases. Every move is a finite expansion or collapse relative to , and each basis change is merely a change of description of the same cells.
Apply [F4] to the resulting identity-matrix pair. It cancels all relative cells by finite elementary moves fixing . Concatenating this deformation with those of steps 1.1 and 4.1 gives the required finite formal deformation of to . If , [F4] is the empty deformation and the same conclusion holds. ∎
Every Whitehead class is realized by a finite CW homotopy equivalence
Statement
For a connected finite CW complex , and , there is a finite CW complex such that is a homotopy equivalence and . Only relative cells in two consecutive degrees , with even , are needed. For a disconnected finite , a prescribed class on each of its finitely many components is realized componentwise.
Facts & Assumptions
Given: A connected finite and a Whitehead class .
Each Whitehead class has a representative , with finite ; a zero class may be represented by an identity matrix (K₁ of a ring and the Whitehead group of a discrete group).
The relative boundary of a two-high-layer pair is the matrix of the triple homotopy boundary in oriented lifted-cell bases (Two high relative cell layers have free homotopy bases and their cellular boundary matrix).
For a simply connected -connected CW pair with nonempty simply connected base, the relative Hurewicz map is an isomorphism without any choice principle (Relative Hurewicz comparison through a choice-free weak model).
The cellular complex of a CW pair computes its relative singular homology (Cellular homology computes singular homology).
A weak homotopy equivalence between finite CW complexes is a homotopy equivalence without any choice principle (Whitehead theorem).
Attaching cells of dimension at least three preserves components and fundamental groups (High relative cells do not change lower homotopy); based maps from simply connected spheres lift to universal covers (Lifting criterion for maps from path-connected locally path-connected spaces).
Inclusion torsion is the torsion of its based relative universal-cover complex, with two-term sign when the upper cells have degree (Whitehead torsion of a finite CW homotopy equivalence, Composition and based-pair sum formulas for Whitehead torsion).
Proof
Choose with representing , allowing and for . Choose an even integer . Attach -cells by constant maps at the chosen base vertex to form . By [F6], and no lower relative homotopy is introduced.
Each is a finite integral sum of elements of . The th wedge sphere, preceded by a based whisker representing a group element and repeated by signed pinch maps, realizes its coefficient in . Since , this is an abelian group and finite sums of these maps are represented by based maps . For each column choose one such map whose relative coordinates are ; only finitely many explicit choices are needed. Attach -cells along the to form finite . The right-module column convention and [F2] make the relative cellular differential exactly .
By [F6] the map induces a component bijection and an isomorphism on . The inverse image of in the universal cover is the connected universal cover of : the -isomorphism makes the restricted cover connected, and a loop in it maps to a null loop in and hence is null in . Both and are simply connected. Their relative cellular chain complex is in degrees , so it has zero homology in every degree because is invertible. By [F4], for every .
Suppose some were nonzero and take the least such . Since the pair has no relative cells below , it is at least -connected and ; its base is simply connected. The choice-free comparison [F3] gives , a contradiction. Hence all relative homotopy groups vanish. Coverings induce isomorphisms on higher homotopy groups by lifting spheres and homotopies; together with the -isomorphism of step 3.1, is a weak homotopy equivalence.
Both and are finite, so the finite choice-free clause [F5] makes a homotopy equivalence. Its relative complex has upper degree , and is even, so . Therefore [F7] gives . For finitely many connected components, repeat the construction separately on each component and take their finite disjoint union; no component transport or infinite choice is involved. ∎
Whitehead torsion is the complete obstruction to finite CW simple homotopy
Statement
A homotopy equivalence of finite CW complexes is simple if and only if in , with basepoint changes transported canonically. This is a statement about finite CW complexes, with no smooth handle or cobordism assertion.
Facts & Assumptions
Given: A homotopy equivalence of finite CW complexes.
Every simple homotopy equivalence has zero Whitehead torsion (Simple homotopy equivalences have zero torsion).
For a cellular , the target inclusion is simple, the mapping cylinder is finite, and its retraction satisfies (The target of a finite cellular mapping cylinder is a simple subcomplex).
A finite connected homotopy-equivalence inclusion with zero torsion admits a finite elementary deformation relative to its source (Zero relative torsion gives a finite relative elementary deformation).
Whitehead torsion is invariant under cellular approximation and under the stated basepoint and cellular-basis choices (Whitehead torsion is independent of all auxiliary choices).
for composable finite CW homotopy equivalences (Composition and based-pair sum formulas for Whitehead torsion).
A map homotopic to a finite composite of elementary expansions, collapses and cellular isomorphisms is simple (Simple homotopy equivalence).
A map with finite CW source is homotopic to a cellular map without any choice principle (Cellular approximation for maps of CW pairs).
Proof
If is simple, [F1] gives on each target component.
Conversely suppose . By [F7] and [F4] replace by a cellular map in its homotopy class; this changes neither its torsion nor whether it is simple. The construction is finite because is finite. Work first on one connected component; a homotopy equivalence bijects the finite component sets.
Form the finite cellular mapping cylinder . Its target inclusion is simple by [F2], so [F1] gives . Since , [F5] yields . Also , whence . The retraction is a homotopy equivalence and induces an isomorphism on Whitehead groups, so .
The source inclusion is a homotopy equivalence of finite connected CW complexes. Apply [F3] to obtain a finite relative elementary deformation from to . Reversing that sequence shows is simple. The target inclusion is also simple, so its inverse retraction is homotopic to the reverse composite of its elementary moves and is simple by [F6]. Thus is simple. Repeat on each of the finitely many components and concatenate their finite move sequences. This proves the reverse implication and the asserted direct-sum statement. ∎
5 · Examples, counterexamples and false statements
None yet.
Sources
- Lück, §2.3, pp.34–35
- Cohen, §7, pp.24–26
- Casson, Simple Homotopy Theory, §4, p.30
- Lück, Definition 2.17, pp.34–35
- Lück, §2.1, pp.24–26
- Cohen, §8.3–8.4, pp.31–32
- Lück, Lemma 2.2, pp.25–26
- Lurie, Remark 12, p.4
- Cohen, §19, pp.62–65
- Lück, §2.2, contraction-torsion setup pp.27–28
- Lück, §2.2, equation (2.7), pp.27–28
- Lück, Lemma 2.9 and equation (2.11), pp.29–30
- Cohen, §§19–20, pp.62–69
- Lück, §2.2, pp.30–31
- Davis–Kirk, §11.4, p.343
- Davis–Kirk, Theorem 11.31(1), pp.343–344
- Cohen, §§19, 22, pp.62–65, 72–75
- Lück, §3.1, pp.27–31
- Lück, Definition 2.13, pp.30–31
- Cohen, §22, pp.72–75
- Lück, Definition 2.13 and Lemma 2.9, pp.29–31
- Cohen, §§19,22, pp.62–65,72–75
- Lück, Lemma 2.9, pp.29–30; Theorem 2.1, pp.23–24
- Cohen, §§20–23, pp.66–77
- Lurie, Lemma 2 and Proposition 4, pp.1–2
- Lück, Lemma 2.18(1), p.35
- Davis–Kirk, Theorem 11.31(2), p.344
- Cohen, §22, p.72
- Lück, Lemmas 2.19–2.20, p.36
- Cohen, §22.3, pp.72–73
- Cohen, §§7.3–7.4, pp.25–27
- Davis–Kirk, Theorem 11.31(3) sketch, pp.344–345
- Casson, Theorem 4.7, Chapter 4
- Cohen, §8.1 and beginning of §8.2, pp.28–30
- Lück, Theorem 2.21 proof sketch, pp.37–38
- Hatcher, Algebraic Topology, Proposition 4.21, and the relative Hurewicz and covering-space arguments of §4.2
- Hatcher, Algebraic Topology, §4.1 change-of-basepoint arguments
- Cohen, §§7.1, 7.4, 8.3–8.4, printed pp.23, 26–27, 31–32
- Casson, proof of Theorem 4.7, printed pp.32–34
- Cohen, §8.2, printed p.30
- Casson, proof of Theorem 4.7, printed pp.33–34
- Cohen, §§7.3–8.5, printed pp.25–33
- Casson, Theorem 4.7, printed pp.32–34
- Lück, Theorem 2.21, printed pp.37–38
- Lück, Lemma 2.18(2), printed pp.35–36
- Lurie, Remark 6, printed p.2
- Cohen, §§8.5 and 22, printed pp.32–33, 72–75