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The fifth stable offset in integral Eilenberg–Mac Lane homology vanishes
Statement
Assume AC. For every integer and any CW model ,
Facts & Assumptions
Given: AC and marked CW models .
The Axiom of Choice is inherited from the cohomology, fibration and CW suppliers.
Circle and path-loop models for Eilenberg–Mac Lane induction identifies the actual strict fiber of with , contracts its total space, and identifies as a marked . Finite join models for the circle and the two-point group and Milnor's join model is a contractible free G-space give the contractible infinite-sphere total and the numerable principal bundle in the actual weak CW model. Numerable fiber bundles are hurewicz fibrations and Long exact sequence of homotopy groups of a fibration give its homotopy exact sequence. Existence and homotopy uniqueness of Eilenberg--Mac Lane spaces supplies marked model comparison. Cohomology ring of infinite complex projective space computes the integral cohomology of as , , and its degreewise finite homology.
Homological Serre spectral sequence, Cohomological Serre spectral sequence and Multiplicative cohomological Serre spectral sequence supply the actual constant-system sequences, strong convergence, and the total-degree Leibniz rule. Absolute Hurewicz theorem at the first nonzero degree makes -connected with its first integral homology in degree . The singular pair sequences of Long exact sequence of a pair and Long exact sequence of a pair in singular cohomology apply to the actual path total and strict fiber without a CW-pair hypothesis; their boundary and connector maps are natural.
Topological universal coefficient short exact sequence for cohomology, The universal coefficient theorem for homology over a PID and The fundamental theorem of finitely generated abelian groups from PID modules give coefficient comparisons and the cyclic decomposition. Rational cohomology of Eilenberg–Mac Lane spaces in one generator computes rational cohomology as a polynomial algebra on the degree- fundamental class for even , and an exterior algebra for odd .
A transgressive simple fiber system gives a polynomial base proves the mod-two polynomial-base comparison for a transgressive simple fiber system. Relative lifts produce cohomological transgressions proves the relative-lift transgression statement and its compatibility with each square, with the actual strict fiber.
The mod-two square algebra, admissible sequences, and excess, Adem relations for Steenrod squares and Steenrod normalization, instability, suspension, and top square fix admissibility, excess, Adem reduction, instability and top squares. Reduction of the integral Bockstein is the first Steenrod square gives .
Proof
First derive the integral degree-two model from the actual principal bundle in [F1]. Its total is contractible and its fiber is a marked . The fibration exact sequence gives for every , while its component segment gives because is connected. Thus is a CW , with its degree-two generator marked by this connecting isomorphism. Marked uniqueness in [F1] compares it with the chosen , so the integral ring and finite-homology base case apply to that actual model. All integral homology groups of every are finitely generated. Start with in [F1], and induct on using its path fibration. Within this induction induct on the base homology degree . In the homological sequence the bottom term has no incoming differential. Every outgoing target has bidegree with smaller base degree. Its group is finitely generated by the coefficient UCT, the induction on , and the finite generation of the fiber homology. Hence every outgoing image is finitely generated. Only finitely many such maps occur, and the surviving subgroup is zero because the total space is contractible. The successive kernels express the bottom group as a finite extension of finitely generated images. This proves the induction; all bases are simply connected, so there is no coefficient monodromy.
We construct the mod-two calculation for the integral models, rather than use a theorem about . For , the algebra is polynomial on with admissible, containing no , and . The initial case is the polynomial ring on from [F1]. For the induction, powers of each polynomial generator form a simple system: unique binary expansion of each exponent makes products of distinct such powers a basis. The following index calculation identifies these powers without a hidden counting step. If is admissible, then . When , its operation on is the square of by the top-square formula. Removing the first entry repeatedly therefore expresses it as a unique -power of an admissible sequence of excess less than . Conversely, prepend to an admissible of excess at most ; it remains admissible, has excess , and evaluates to the square. Thus the simple system is indexed precisely by admissible sequences with no and excess at most .
We now give the entire odd-prime calculation needed, rather than import an odd-primary operation algebra. Fix an odd prime and . In all following path sequences, denotes the fundamental base class of degree and the fundamental fiber class of degree . Their first differential is ; replacing a marked generator by its negative fixes the sign if necessary. Leibniz gives when is even. For an odd , one has since is a unit. Coefficient systems in nonzero free rows are literal copies of ; a torsion row uses , not an unjustified tensor-product formula. Such coefficients vanish for by connectivity.
The fundamental fiber class has a relative lift transgressing to the fundamental base class. Put , and , for . Represent the marked generator by . Contract the disk to a chosen boundary point and apply to the contraction, read from that point to ; this gives a continuous lift with and . By the connecting marking in [F1], its boundary represents the marked generator of . Absolute Hurewicz in [F2], transported along the marked equivalence , makes that boundary the generator of . Since is contractible, the singular pair boundary is an isomorphism and the lower positive relative homology vanishes. Thus represents its generator, which sends to the marked generator of . The UCT and naturality of evaluation now give in the actual relative cohomology group: both evaluate as one on this generator. No CW structure on is asserted. By [F4] every composite is relatively transgressive with representative . Apply the Borel comparison [F4] to the locally finite simple system from step 1.2; it gives the polynomial algebra on admissible sequences of excess at most , equivalently less than , containing no . This proves the induction, including linear independence.
For , the fiber is , , and , with since . Through total degree nine, only occurs in a first-column source. If , all are units; the displayed pairs cancel, leaving only in base degrees zero and three through degree nine. To justify that no unlisted bottom class is hidden, take the first such base column. Its possible incoming sources have smaller base column, hence column zero or three. The zero-column powers and column-three products have just been paired by , so no source survives to hit it. It would survive to the contractible total, a contradiction.
For , degree contains no product of two positive-degree generators from step 2.1. Its basis is exactly . Adem gives and . These are distinct basis classes in degree . Thus is injective on degree . Every reduction of an integral class is in its kernel, since . The coefficient exact sequence embeds into this kernel, so that quotient is zero. Finite generation from step 1.1 shows that has neither a free part nor any two-primary torsion.
For the same calculation has precisely one surviving group through that range: at bidegree , the cokernel on of . The source itself dies, since multiplication by three on is injective; dies with coefficient four. The first-unlisted-column argument of step 2.2 makes the other columns between three and eight zero. The surviving can only die by to , so contractibility makes that differential an isomorphism and . A differential into could only come from column zero, where has died, or column three with fiber degree five, which is zero; column eight would require . Therefore . This proves that through degree nine the nonzero positive groups are in degree three and, only for , in degree eight.
The next five calculations give a finite table, with if and if : for , through degree the nonzero positive groups are in degree , in degree , and also in degree when or . We verify every transition, including the extra degree. For , the free fiber generator is odd of degree three; its maps to , so the free base classes through degree ten are exactly . The torsion fiber class, if present, has degree eight; its only possible nonzero differential is its transgression to bottom degree nine. Earlier targets with nonzero base column four or eight have fiber degrees five or one, both zero; the potential target at has zero base group in degree six. All other targets have zero base column or zero fiber row. Contractibility makes an isomorphism onto . For bottom degree ten, the first-column source has fiber degree nine and is zero by step 3.2; columns four and eight require fiber degrees five and one, and column nine would require . Hence degree ten is zero.
For , the free fiber classes in the required range are in degrees four and eight. They die by and , with two a unit; the odd base class satisfies . The fiber in degree nine has no earlier nonzero target: the only candidate positive base column before its transgression is column five with fiber degree five, which is zero; other positive columns below ten vanish. Its therefore gives the sole torsion group in base degree ten. An incoming differential to degree eleven has first-column source degree ten, zero by step 4.1, or column-five source fiber degree five, also zero. Thus degree eleven is zero, and the stated table holds for .
For , the free fundamental fiber class has degree five. The possible is zero because its source is torsion and its target is free. Connectivity and the already computed lower groups leave this target equal to through page six; no earlier differential changes it. The torsion class consequently survives to its transgression , which is an isomorphism onto the bottom group in degree eleven. For degree twelve the first-column source is fiber degree eleven, zero by step 5.1. The sole other source is at with . Contractibility makes this surject onto the whole degree-twelve group. Its rational rank is one by [F3], so this surjection from is also injective. Hence degree twelve is , with no torsion. This explains why the torsion row at cannot be omitted even though the odd fundamental class has square zero.
For , the fiber in degree eleven transgresses isomorphically to the bottom group in degree twelve. All earlier possible positive-column targets have fiber degree at most five and vanish. The fiber class of degree twelve is killed earlier by , an isomorphism between the free copies of at and . Thus it cannot survive to hit degree thirteen. Every other positive-column source to degree thirteen again requires fiber degree at most five, below the fiber's first positive degree six. Hence . The free and torsion groups in all the stated ranges are now completely listed. The first-unlisted-column argument from step 2.2 rules out an additional bottom group at every intermediate zero degree in these finite calculations for : its surviving potential sources are exactly the free pair and the indicated single torsion transgression, already accounted for.
For , a mixed positive-column/positive-row term in total degree through would have degree at least . Thus only the axes occur in the whole relevant incoming-differential region. Every positive fiber class in degrees through transgresses to the next base degree, since the total space is contractible. The induction table of step 7.1 therefore shifts by one: base degree is , degree is , and degree is zero, with all intervening groups zero. In particular for every odd prime and . There is no additive extension ambiguity in these assertions about the bottom axis: its entire incoming list and its zero abutment have been specified.
Steps 3.1 and 8.1 eliminate every primary torsion subgroup of ; localization of cohomology agrees with cohomology with localized coefficients here by the finite-generation coefficient UCT, so these are the actual primary groups. By the cohomological UCT, its torsion subgroup is . The rational computation in [F3] gives , since . Finite generation from step 1.1 then kills both the torsion and free parts of . Thus , as claimed.
Depends on
- The Axiom of Choice
- Circle and path-loop models for Eilenberg–Mac Lane induction
- Cohomology ring of infinite complex projective space
- Homological Serre spectral sequence
- Cohomological Serre spectral sequence
- Multiplicative cohomological Serre spectral sequence
- Topological universal coefficient short exact sequence for cohomology
- The universal coefficient theorem for homology over a PID
- Rational cohomology of Eilenberg–Mac Lane spaces in one generator
- A transgressive simple fiber system gives a polynomial base
- Relative lifts produce cohomological transgressions
- The mod-two square algebra, admissible sequences, and excess
- Adem relations for Steenrod squares
- Steenrod normalization, instability, suspension, and top square
- Reduction of the integral Bockstein is the first Steenrod square
- Absolute Hurewicz theorem at the first nonzero degree
- Long exact sequence of a pair
- Long exact sequence of a pair in singular cohomology
- The fundamental theorem of finitely generated abelian groups from PID modules
- Finite join models for the circle and the two-point group
- Milnor's join model is a contractible free G-space
- Numerable fiber bundles are hurewicz fibrations
- Long exact sequence of homotopy groups of a fibration
- Existence and homotopy uniqueness of Eilenberg--Mac Lane spaces
Used by
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Sources
- Allen Hatcher, Spectral Sequences in Algebraic Topology, Chapter 1 (standard reference, not scraped)