- Betti number
In
algebraic topology , the Betti number of atopological space is, in intuitive terms, a way of counting the maximum number of cuts that can be made without dividing the space into two pieces. This defines, in fact, what is called the "first" Betti number. There is a sequence of Betti numbers defined.Each Betti number is a
natural number , orinfinity . For the most reasonable spaces (such ascompact manifold s, finitesimplicial complex es orCW complex es), the sequence of Betti numbers is 0 from some points onwards, and consists of natural numbers.The term "Betti numbers" was coined by
Henri Poincaré , the name being forEnrico Betti .Definition
For a non-negative
integer , the -th Betti number of the space is defined as the rank of theabelian group , the -thhomology group of . Equivalently, one can define it as thevector space dimension of , since the homology group in this case is a vector space over . Theuniversal coefficient theorem , in a very simple case, shows that these definitions are the same.More generally, given a field one can define , the -th Betti number with coefficients in , as the vector space dimension of .
Example: the first Betti number in graph theory
In
topological graph theory the first Betti number of a graph "G" with "n" vertices, "m" edges and "k" connected components equals:"m" − "n" + "k".
This may be proved straightforwardly by
mathematical induction on the number of edges. A new edge either increments the number of 1-cycles or decrements the number of connected components.See
cyclomatic complexity for an application of the first Betti number insoftware engineering .Properties
The (rational) Betti numbers do not take into account any torsion in the homology groups, but they are very useful basic topological invariants. In the most intuitive terms, they allow one to count the number of "holes" of different dimensions. For a
circle , the first Betti number is 1. For a general pretzel, the first Betti number is twice the number of holes.In the case of a finite simplicial complex the homology groups are finitely-generated, and so has a finite rank. Also the group is 0 when exceeds the top dimension of a simplex of .
For a finite CW-complex "K" we have:where denotes
Euler characteristic of "K" and any field "F".For any two spaces "X" and "Y" we have:where denotes the Poincaré polynomial of "X", i.e. the
generating function of the Betti numbers of "X"::seeKünneth theorem .If "X" is "n"-dimensional manifold, there is symmetry interchanging "k" and "n" − "k", for any "k"::under conditions (a "closed" and "oriented" manifold); see
Poincaré duality .The dependence on the field "F" is only through its characteristic. If the homology groups are torsion-free, the Betti numbers are independent of "F". The connection of "p"-torsion and the Betti number for
characteristic p , for "p" a prime number, is given in detail by theuniversal coefficient theorem (based onTor functors , but in a simple case).Examples
#The Betti number sequence for a circle is 1, 1, 0, 0, 0, ...;
#The Betti number sequence for a two-torus is 1, 2, 1, 0, 0, 0, ...;
#The Betti number sequence for a three-torus is 1, 3, 3, 1, 0, 0, 0, ... .In fact, for an "n"-
torus one should indeed see thebinomial coefficient s. This is a case of theKünneth theorem .It is possible for spaces that are infinite-dimensional in an essential way to have an infinite sequence of non-zero Betti numbers. An example is the infinite-dimensional
complex projective space , with sequence 1, 0, 1, 0, 1, ... that is periodic, withperiod length 2.Relationship with dimensions of spaces of
differential form sIn geometric situations when is a
closed manifold , the importance of the Betti numbers may arise from a different direction, namely that they predict the dimensions of vector spaces ofclosed differential form s "modulo "exact differential form s. The connection with the definition given above is via three basic results,de Rham's theorem andPoincaré duality (when those apply), and theuniversal coefficient theorem ofhomology theory .There is an alternate reading, namely that the Betti numbers give the dimensions of spaces of
harmonic form s. This requires also the use of some of the results ofHodge theory , about theHodge Laplacian .In this setting,
Morse theory gives a set of inequalities for alternating sums of Betti numbers in terms of a corresponding alternating sum of the number of critical points of aMorse function of a given index::
Witten gave an explanation of these inequalities by using the Morse function to modify the
exterior derivative in thede Rham complex .References
* F.W. Warner, Foundations of differentiable manifolds and Lie groups, Springer (1983).
* J.Roe, Elliptic Operators, Topology, and Asymptotic Methods, Second Edition (Research Notes in Mathematics Series 395), Chapman and Hall (1998).
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