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.
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.
To define the Todd class
\operatorname{td}(E)
E
X
Q(x)=
x | |
1-e-x |
infty | |
=1+\dfrac{x}{2}+\sum | |
i=1 |
B2i | |
(2i)! |
x2i=1+\dfrac{x}{2}+\dfrac{x2}{12}-\dfrac{x4}{720}+ …
xn
Q(x)n+1
Bi
i
xj
m | |
\prod | |
i=1 |
Q(\betaix)
for any
m>j
\betai
j
\operatorname{td}j(p1,\ldots,pj)
p
\betai
\operatorname{td}j
Q
E
\alphai
\operatorname{td}(E)=\prodQ(\alphai)
which is to be computed in the cohomology ring of
X
The Todd class can be given explicitly as a formal power series in the Chern classes as follows:
\operatorname{td}(E)=1+
c1 | |
2 |
+
| ||||||||||
12 |
+
c1c2 | |
24 |
+
| ||||||||||||||||||||||
720 |
+ …
where the cohomology classes
ci
E
H2i(X)
X
\operatorname{td}(E)
The Todd class is multiplicative:
\operatorname{td}(E ⊕ F)=\operatorname{td}(E) ⋅ \operatorname{td}(F).
Let
\xi\inH2({C}Pn)
{C}Pn
0\to{lO}\to{lO}(1)n+1\toT{C}Pn\to0,
\operatorname{td}(T{C}Pn)=\left(\dfrac{\xi}{1-e-\xi
For any algebraic curve
C
\operatorname{td}(C)=1+c1(TC)
C
Pn
c1(TC)
and properties of chern classes. For example, if we have a degree0\toTC\to
n| T C \to
N C/Pn \to0
d
P2
where\begin{align} c(TC)&=
c(T |C) P2
c(N ) C/P2 \\ &=
1+3[H] 1+d[H] \\ &=(1+3[H])(1-d[H])\\ &=1+(3-d)[H] \end{align}
[H]
P2
C
See main article: Hirzebruch–Riemann–Roch theorem. For any coherent sheaf F on a smooth compact complex manifold M, one has
\chi(F)=\intM\operatorname{ch}(F)\wedge\operatorname{td}(TM),
\chi(F)
\chi(F):=
dimCM | |
\sum | |
i=0 |
(-1)idimCHi(M,F),
\operatorname{ch}(F)