In mathematics, a genus of a multiplicative sequence is a ring homomorphism from the ring of smooth compact manifolds up to the equivalence of bounding a smooth manifold with boundary (i.e., up to suitable cobordism) to another ring, usually the rational numbers, having the property that they are constructed from a sequence of polynomials in characteristic classes that arise as coefficients in formal power series with good multiplicative properties.
A genus
\varphi
\Phi(X)
\Phi(X\sqcupY)=\Phi(X)+\Phi(Y)
\sqcup
\Phi(X x Y)=\Phi(X)\Phi(Y)
\Phi(X)=0
The manifolds and manifolds with boundary may be required to have additional structure; for example, they might be oriented, spin, stably complex, and so on (see list of cobordism theories for many more examples). The value
\Phi(X)
\Z/2\Z
The conditions on
\Phi
\varphi
Example: If
\Phi(X)
\Phi
See main article: Multiplicative sequence. A sequence of polynomials
K1,K2,\ldots
p1,p2,\ldots
1+p1z+
2 | |
p | |
2z |
+ … =(1+q1z+
2 | |
q | |
2z |
+ … )(1+r1z+
2 | |
r | |
2z |
+ … )
implies that
\sumjKj(p1,p2,\ldots)zj=\sumjKj(q1,q2,\ldots)
j\sum | |
z | |
k |
Kk(r1,r2,\ldots)zk
If
Q(z)
K=1+K1+K2+ …
by
K(p1,p2,p3,\ldots)=Q(z1)Q(z2)Q(z3) …
where
pk
zi
pk
The genus
\Phi
\Phi(X)=K(p1,p2,p3,\ldots)
where the
pk
\Phi
The L genus is the genus of the formal power series
{\sqrt{z}\over\tanh(\sqrtz)}=\sumk\ge
22kB2kzk | |
(2k)! |
=1+{z\over3}-{z2\over45}+ …
where the numbers
B2k
\begin{align} L0&=1\\ L1&=\tfrac13p1\\ L2&=\tfrac1{45}\left(7p2-
2\right) | |
p | |
1 |
\\ L3&=\tfrac1{945}\left(62p3-13p1p2+2
3\right) | |
p | |
1 |
\\ L4&=\tfrac1{14175}\left(381p4-71p1p3-19
2 | |
p | |
2 |
+22
2 | |
p | |
1 |
p2-3
4\right) \end{align} | |
p | |
1 |
(for further L-polynomials see [1] or). Now let M be a closed smooth oriented manifold of dimension 4n with Pontrjagin classes
pi=pi(M)
M
[M]
\sigma(M)
\sigma(M)=\langleLn(p1(M),\ldots,pn(M)),[M]\rangle
This is now known as the Hirzebruch signature theorem (or sometimes the Hirzebruch index theorem).
The fact that
L2
p2
Since projective K3 surfaces are smooth complex manifolds of dimension two, their only non-trivial Pontryagin class is
p1
H4(X)
L1=-16
\operatorname{dim}\left(H2(X)\right)=22
The Todd genus is the genus of the formal power series
z | |
1-\exp(-z) |
=
| ||||
\sum | ||||
i=0 |
zi
with
Bi
\begin{align} Td0&=1\\ Td1&=
1{2} | |
c |
1\\ Td2&=
1{12} | |
\left |
(c2+
2 | |
c | |
1 |
\right)\\ Td3&=
1{24} | |
c |
1c2\\ Td4&=
1{720} | |
\left(-c |
4 | |
1 |
+4c2
2 | |
c | |
1 |
+
2 | |
3c | |
2 |
+c3c1-c4\right) \end{align}
The Todd genus has the particular property that it assigns the value 1 to all complex projective spaces (i.e.
n) | |
Td | |
n(CP |
=1
The  genus is the genus associated to the characteristic power series
Q(z)=
| |||||
(There is also an A genus which is less commonly used, associated to the characteristic series
Q(16z)
\begin{align} \hat{A}0&=1\\ \hat{A}1&=-\tfrac1{24}p1\\ \hat{A}2&=\tfrac1{5760}\left(-4p2+7
2\right) | |
p | |
1 |
\\ \hat{A}3&=\tfrac1{967680}\left(-16p3+44p2p1-31
3\right) | |
p | |
1 |
\\ \hat{A}4&=\tfrac1{464486400}\left(-192p4+512p3p1+
2 | |
208p | |
2 |
-904p2
2 | |
p | |
1 |
+
4\right) \end{align} | |
381p | |
1 |
The  genus of a spin manifold is an integer, and an even integer if the dimension is 4 mod 8 (which in dimension 4 implies Rochlin's theorem) – for general manifolds, the  genus is not always an integer. This was proven by Hirzebruch and Armand Borel; this result both motivated and was later explained by the Atiyah–Singer index theorem, which showed that the  genus of a spin manifold is equal to the index of its Dirac operator.
By combining this index result with a Weitzenbock formula for the Dirac Laplacian, André Lichnerowicz deduced that if a compact spin manifold admits a metric with positive scalar curvature, its  genus must vanish. This only gives an obstruction to positive scalar curvature when the dimension is a multiple of 4, but Nigel Hitchin later discovered an analogous
\Z2
\Z2
A genus is called an elliptic genus if the power series
Q(z)=z/f(z)
{f'}2=1-2\deltaf2+\epsilonf4
for constants
\delta
\epsilon
One explicit expression for f(z) is
f(z)=
1 | |
a |
\operatorname{sn}\left(az,
\sqrt{\epsilon | |
where
a=\sqrt{\delta+\sqrt{\delta2-\epsilon}}
and sn is the Jacobi elliptic function.
Examples:
\delta=\epsilon=1,f(z)=\tanh(z)
\delta=-
1 | |
8 |
,\epsilon=0,f(z)=2\sinh\left(
1 | |
2 |
z\right)
\epsilon=\delta2,f(z)=
\tanh(\sqrt{\delta | |
z)}{\sqrt{\delta}} |
The first few values of such genera are:
1 | |
3 |
\deltap1
1 | |
90 |
\left[\left(-4\delta2+18\epsilon\right)p2+\left(7\delta2-9\epsilon\right
2\right | |
)p | |
1 |
]
1 | |
1890 |
\left[\left(16\delta3+108\delta\epsilon\right)p3+\left(-44\delta3+18\delta\epsilon\right)p2p1+\left(31\delta3-27\delta\epsilon\right
3\right | |
)p | |
1 |
]
Example (elliptic genus for quaternionic projective plane) :
\begin{align} \Phiell(HP2)&=
\int | |
HP2 |
\tfrac1{90}[(-4\delta2+18\epsilon
2-9\epsilon | |
)p | |
2+(7\delta |
2] | |
)p | |
1 |
\\ &=
\int | |
HP2 |
\tfrac1{90}[(-4\delta2+18\epsilon)(7u2)+(7\delta2-9\epsilon)(2u)2]\\ &=
\int | |
HP2 |
[u2\epsilon]\\ &=\epsilon
\int | |
HP2 |
[u2]\\ &=\epsilon*1=\epsilon \end{align}
Example (elliptic genus for octonionic projective plane, or Cayley plane):
\begin{align} \Phiell(OP2)&=
\int | |
OP2 |
\tfrac1{113400}\left[(-192\delta4+1728\delta2\epsilon+
2)p | |
1512\epsilon | |
4 |
+(208\delta4-1872\delta2\epsilon+
2\right] | |
1512\epsilon | |
2 |
\\ &=
\int | |
OP2 |
\tfrac1{113400}[(-192\delta4+1728\delta2\epsilon+1512\epsilon2)(39u2)+(208\delta4-1872\delta2\epsilon+1512\epsilon2)(6u)2]\\ &=
\int | |
OP2 |
[\epsilon2u2]\\ &=
2\int | |
\epsilon | |
OP2 |
[u2]\\ &=\epsilon2*1=\epsilon2\\ &=\Phiell(HP2)2 \end{align}
The Witten genus is the genus associated to the characteristic power series
Q(z)=
z | |
\sigmaL(z) |
=\exp\left(\sumk\ge{2G2k(\tau)z2k\over(2k)!}\right)
where σL is the Weierstrass sigma function for the lattice L, and G is a multiple of an Eisenstein series.
The Witten genus of a 4k dimensional compact oriented smooth spin manifold with vanishing first Pontryagin class is a modular form of weight 2k, with integral Fourier coefficients.