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Todd class

Characteristic class in algebraic topology

In mathematics, the Todd class is a certain construction now considered a part of the theory in algebraic topology of characteristic classes. The Todd class of a vector bundle can be defined by means of the theory of Chern classes, and is encountered where Chern classes exist , most notably in differential topology, the theory of complex manifolds and algebraic geometry. In rough terms, a Todd class acts like a reciprocal of a Chern class, or stands in relation to it as a conormal bundle does to a normal bundle.

The Todd class plays a fundamental role in generalising the classical Riemann-Roch theorem to higher dimensions, in the Hirzebruch-Riemann-Roch theorem and the Grothendieck-Hirzebruch-Riemann-Roch theorem.

01History

It is named for J. A. Todd, who introduced a special case of the concept in algebraic geometry in 1937, before the Chern classes were defined. The geometric idea involved is sometimes called the Todd-Eger class. The general definition in higher dimensions is due to Friedrich Hirzebruch.

02Definition

To define the Todd class \operatorname {td} (E) where E is a complex vector bundle on a topological space X, it is usually possible to limit the definition to the case of a Whitney sum of line bundles, by means of a general device of characteristic class theory, the use of Chern roots (aka, the splitting principle). For the definition, let

Q(x)={\frac {x}{1-e^{-x}}}=\sum _{i=0}^{\infty }{\frac {B_{i}}{i!}}x^{i}=1+{\dfrac {x}{2}}+{\dfrac {x^{2}}{12}}-{\dfrac {x^{4}}{720}}+\cdots

be the formal power series with the property that the coefficient of x^{n} in Q(x)^{n+1} is 1, where B_{i} denotes the i-th Bernoulli number (with B_{1}=+{\frac {1}{2}}). Consider the coefficient of x^{j} in the product

\prod _{i=1}^{m}Q(\beta _{i}x)\

for any m>j. This is symmetric in the \beta _{i}s and homogeneous of weight j: so can be expressed as a polynomial \operatorname {td} _{j}(p_{1},\ldots ,p_{j}) in the elementary symmetric functions p of the \beta _{i}s. Then \operatorname {td} _{j} defines the Todd polynomials: they form a multiplicative sequence with Q as characteristic power series.

If E has the \alpha _{i} as its Chern roots, then the Todd class

\operatorname {td} (E)=\prod Q(\alpha _{i})

which is to be computed in the cohomology ring of X (or in its completion if one wants to consider infinite-dimensional manifolds).

The Todd class can be given explicitly as a formal power series in the Chern classes as follows:

\operatorname {td} (E)=1+{\frac {c_{1}}{2}}+{\frac {c_{1}^{2}+c_{2}}{12}}+{\frac {c_{1}c_{2}}{24}}+{\frac {-c_{1}^{4}+4c_{1}^{2}c_{2}+c_{1}c_{3}+3c_{2}^{2}-c_{4}}{720}}+\cdots

where the cohomology classes c_{i} are the Chern classes of E, and lie in the cohomology group H^{2i}(X). If X is finite-dimensional then most terms vanish and \operatorname {td} (E) is a polynomial in the Chern classes.

03Properties of the Todd class

The Todd class is multiplicative:

\operatorname {td} (E\oplus F)=\operatorname {td} (E)\cdot \operatorname {td} (F).

Let \xi \in H^{2}({\mathbb {C} }P^{n}) be the fundamental class of the hyperplane section. From multiplicativity and the Euler exact sequence for the tangent bundle of {\mathbb {C} }P^{n}

0\to {\mathcal {O}}\to {\mathcal {O}}(1)^{n+1}\to T{\mathbb {C} }P^{n}\to 0,

one obtains

\operatorname {td} (T{\mathbb {C} }P^{n})=\left({\dfrac {\xi }{1-e^{-\xi }}}\right)^{n+1}.

04Computations of the Todd class

For any algebraic curve C the Todd class is just \operatorname {td} (C)=1+{\frac {1}{2}}c_{1}(T_{C}). Since C is projective, it can be embedded into some \mathbb {P} ^{n} and we can find c_{1}(T_{C}) using the normal sequence

0\to T_{C}\to T_{\mathbb {P^{n}} }|_{C}\to N_{C/\mathbb {P} ^{n}}\to 0

and properties of chern classes. For example, if we have a degree d plane curve in \mathbb {P} ^{2}, we find the total chern class is

{\begin{aligned}c(T_{C})&={\frac {c(T_{\mathbb {P} ^{2}}|_{C})}{c(N_{C/\mathbb {P} ^{2}})}}\\&={\frac {1+3[H]}{1+d[H]}}\\&=(1+3[H])(1-d[H])\\&=1+(3-d)[H]\end{aligned}}

where [H] is the hyperplane class in \mathbb {P} ^{2} restricted to C.

05Hirzebruch-Riemann-Roch formula

For any coherent sheaf F on a smooth compact complex manifold M, one has

\chi (F)=\int _{M}\operatorname {ch} (F)\wedge \operatorname {td} (TM),

where \chi (F) is its holomorphic Euler characteristic,

\chi (F):=\sum _{i=0}^{{\text{dim}}_{\mathbb {C} }M}(-1)^{i}{\text{dim}}_{\mathbb {C} }H^{i}(M,F),

and \operatorname {ch} (F) its Chern character.

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Sources and credits

This article is adapted from the Wikipedia article Todd class, written by its contributors and licensed under CC BY-SA 4.0. Fathomly has changed the layout, removed citation markers, navigation and maintenance notices, and adjusted punctuation. This adapted version is shared under the same license. For references, see the original article.

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