The theory of homology ( dr. Greek ὁμός “equal, identical; common; mutual” and λόγος “doctrine, science ”) is a branch of mathematics that studies the constructions of some topological invariants called homology groups and cohomology groups . Also called homology theories are specific constructions of homology groups.
In the simplest case, a topological space the sequence of abelian homology groups is compared numbered by natural numbers . They are homotopy invariants and, in contrast to homotopy groups , they are easier to calculate and more geometrically clear, but for simply connected spaces they carry the same amount of information [1] .
However, the definition of homology is less explicit and uses some technical machinery [2] , and therefore there are several different theories of homology - both defined only for “good” topological spaces or requiring an additional structure , and more complex ones designed to work with pathological examples. Nevertheless, with the exception of such pathological cases, they usually coincide: for cell spaces this is ensured by the Steenrod – Eilenberg axioms .
Other common concepts of homology theory are homology with coefficients in an abelian group relative homology pairs of spaces and cohomology whose definitions are, in a sense, dual to the definition of homology. Cohomology is often considered because of the presence of multiplication on them. turning them into graded algebra .
Also called cohomology are invariants associated with other mathematical objects - groups , Lie algebras , sheaves . They are united by formal similarity - for example, the presence in their definition of the concept of homology of a chain complex - and in some cases, the presence of constructions that map topological spaces with suitable homologies to such objects.
General definition
Recall that Homotopy group
of space
Is a lot of mappings from
-dimensional sphere in
considered up to a continuous deformation . To determine homology
mappings of spheres are replaced by
-cycles that intuitively represent as closed (that is, without boundaries) oriented films of dimension
inside
, but in different definitions they formalize in different ways. The condition of continuous deformability is replaced by the condition that the difference of the cycles (their union, in which the second is taken with the opposite orientation) is the oriented boundary of the cycle of dimension one greater.
In standard notation, the group -cycles - (from German. Zyklus - "cycle"), group -boundaries - (from the English boundary - “border”), and the phrase “homology is a cycle up to a boundary” is written as
- .
To formalize this idea, it is necessary to strictly define the cycles and their boundaries, which for cycles of dimension leads to some difficulties [1] . The solution is to define an intermediate concept of a group -chains consisting of formal linear combinations of mappings in some standard elements depending on the chosen design. The border of standard elements is defined as a linear combination of standard elements of dimension one less with suitable orientations, which induces the display of the border . Then -cycles are defined as -chains with a zero border (in order for the equality of the border to zero to make sense, it is necessary to take not only positive, but also any linear combinations of standard elements, and set the border display with a sign). Thus, loops are the core , and borders are the image of the border:
- .
The condition that all boundaries are cycles takes the form of a chain complex condition: , and the homology of a topological space are the homology of this complex.
The choice of standard elements and the display of the border differs depending on the theory. In the theory of singular homology, such elements are simplexes , and a boundary mapping associates a simplex with the alternating sum of its faces. In the theory of simplicial homologies defined for simplicial complexes , there are also simplices, but not all, but included in the chosen simplicial decomposition. In the theory of cell homology defined for a cell complex , these are hyperspheres from a suitable skeleton, and the mapping of the boundary is more complicated.
Homological Theories
- Simplicial homology - homology is defined for very simple spaces ( simplicial complexes ).
They are defined quite simply, but the proof of their invariance and functoriality is rather complicated.
- Singular homology is another homology theory proposed by Lefschetz . Their definition requires working with infinite-dimensional spaces, but invariance and functoriality immediately become obvious.
- Cech homology is a homology theory that is best suited for working with pathological spaces.
Homology with coefficients in arbitrary groups
One can define homology, allowing the coefficients of simplexes in chains to be elements of any abelian group . That is, instead of groups view groups .
Homology groups (simplicial, singular, etc.) spaces with odds in the group are designated Usually apply a group of real numbers rational numbers , or a cyclic group of residues modulo - , and usually taken Is a prime, then is a field .
Another description. Applying to the complex
functor we get the complex
- ,
whose homology is homology with coefficients in .
Cohomology
In addition to chains, one can introduce the concept of cochains - mappings of the vector space of chains into a group . That is, the cochain space .
Boundary operator determined by the formula: (Where ) For such a boundary operator,
- , namely
- .
Therefore, similarly to what was said above, we can introduce the concept of cocycles , borders and cohomology .
The concept of cohomology is dual to the concept of homology.
If a Is a ring then in the cohomology group natural multiplication is defined (the work of Kolmogorov - Alexander or -nproduct), which turns this group into a graded ring , called the cohomology ring .
In the case when - differentiable manifold , cohomology ring can be calculated using differential forms on (see Theorem de Rama ).
The concept of cohomology was introduced by Alexander and Kolmogorov .
Relative homology and exact homology sequence
Take the case of two topological spaces . Chain group (chains can be either with integer coefficients or with coefficients in any group ) Relative chains will be called elements of the factor group . Since the boundary operator on the subspace homology group translates , then can be determined on the quotient group boundary operator (we denote it in the same way) .
Those relative chains that the boundary operator translates into will be called relative cycles , and the chains that are its values are relative boundaries . Because on absolute chains, then the same will be true for relative, hence . Factor group called a group of relative homologies .
Since every absolute cycle in is also relative, then we have a homomorphism By the functorial property, the embedding leads to homomorphism .
In turn, we can construct a homomorphism which we define as follows. Let be - a relative chain that defines a cycle from . Consider it as an absolute chain in (accurate to elements ) Since this is a relative cycle, then will be zero up to a certain chain . Put equal to the chain homology class .
If we take another absolute chain defining the same relative cycle, then we will have where . We have , but since is the border in then and define the same element in the homology group . If we take a different relative cycle giving the same element in the group of relative homologies where Is the relative boundary, due to the fact that boundary for relative homologies where from here but , but - border in .
Therefore, the homology class defined uniquely. Clearly linear operator that he is a homomorphism. So we have homomorphisms:
- ;
- and
- ;
- and
It can be proved that this sequence is exact , that is, the image of any homomorphism is equal to the kernel of the next homomorphism.
Axioms of Steenrod - Eilenberg
In addition to the simplicial and singular homology already known to us, there are other theories of homology and cohomology, for example, cellular homology , Aleksandrov-Cech cohomology, de Ram cohomology , etc. Stinrod and Eilenberg defined a system of axioms of the theory of (co) homology. First, they determine the so-called. valid pair class topological spaces satisfying the following properties:
- If a then and .
- If a then where - closed interval [0,1].
- where - single point space.
In the Steenrod - Eilenberg homology theory, each admissible pair and any integer k corresponds to an Abelian group and continuous display of pairs homomorphism corresponds (Space identified with a couple ) , and with ), and the following axioms are fulfilled:
- The identity mapping of the pair corresponds to an identical homomorphism .
- ( functoriality )
- A boundary homomorphism is defined , and if , then for the corresponding homomorphism right for any dimension .
- Let be and - attachments, and Are the corresponding homomorphisms, Is a boundary homomorphism. Then the sequence determined by them
exact ( axiom of accuracy ). - If display are homotopic , then the corresponding homomorphisms are equal for any dimension ( axiom of homotopy invariance ).
- Let be - open subset , and its closure is contained in the interior of the set then if the pairs and belong to an admissible class, then for any dimension investment corresponds to an isomorphism ( axiom of excision ).
- For single point space for all dimensions . Abelian group called a group of coefficients ( axiom of dimension ).
For singular homology, an admissible class of pairs consists of all pairs of topological spaces. Previously defined groups of singular homologies with coefficients in the group their mappings and boundary homomorphism satisfy all these axioms. If we take the class of polyhedra as an admissible class, then we can prove that the homology defined using this system of axioms coincides with simplicial.
Similarly, we can introduce a system of axioms for cohomology, which is completely analogous.
You only need to keep in mind that mapping corresponds to ( contravariance ) and that the boundary homomorphism increases dimension.
Extraordinary homologies
In the Steenrod – Eilenberg axiom system, the axiom of dimension is not as important as the others.
Theories of (co) homology that can have nonzero (co) homology groups of a one-point space for dimensions are called extraordinary or generalized. The most important extraordinary theories are the Atiyah K-theory (note the important contribution to this theory of Hirzebruch , Bott and Adams ) and R. Thom's bordism theory.
See also
- Homological Algebra
- Homotopy
- Fundamental class
- Homotopy groups
Notes
- ↑ 1 2 Fomenko, Fuchs, 1989 , p. 95.
- ↑ Hatcher, 2002 , p. 97.
Literature
- Vick J.W. Homology Theory. Introduction to algebraic topology. - M .: ICMMO , 2005
- Dold A. Lectures on Algebraic Topology. - M .: Mir, 1976
- Dubrovin B.A., Novikov S.P., Fomenko A.T. Modern geometry: Methods of homology theory. - M .: Science, 1984
- Seifert G., Trelfall V. Topology. - Izhevsk: RHD, 2001
- Lefschetz S. Algebraic topology. - M .: IL, 1949
- Novikov P.S. Topology. - 2 ed. corrected and add. - Izhevsk: Institute for Computer Research, 2002
- Prasolov V.V. Elements of the homology theory. - M .: ICMMO , 2006
- Svittser R. M. Algebraic topology. - homotopy and homology. - M .: Science, 1985
- Spienier E. Algebraic Topology. - M .: Mir, 1971
- Steenrod N., Eilenberg S. Foundations of algebraic topology. - M .: Fizmatgiz, 1958
- Fomenko A. T. , Fuchs D. B. The course of homotopy topology . - M .: Nauka, 1989 .-- 528 p. - ISBN 5020139297 .
- Algebraic Topology . - Cambridge University Press, 2002. - ISBN 0521795400 .