Spin bordism

1 Introduction

The spin bordism groups $\Omega_n^{Spin}$$== Introduction == <wikitex>; The spin bordism groups $\Omega_n^{Spin}$ of manifolds with spin structures are the homotopy groups of the Thom spectrum $MSpin$. </wikitex> == Calculation == <wikitex>; {{cite|Stong1968}} Preliminary results were by Novikov. The main calculation is due to Anderson, Brown, and Peterson {{cite|Anderson&Brown&Peterson1966}} who showed that all torsion is of order 2, being of two types: that arising by products with a framed $S^1$ and that which maps monomorphically into unoriented cobordism. $\Omega_*^{Spin}/Torsion$ is the subring of an integral polynomial ring on classes $x_{4i}$ (dimension 4i) consisting of all classes of dimension a multiple of 8 and twice the classes whose dimension is not a multiple of 8. Characteristic numbers: Cobordism is determined by $\Zz_2$ cohomology and $KO$-theory characteristic numbers. Relation to framed bordism: The image of framed cobordism is 0 except in dimensions k+1,8k+2$ where it is $\Zz_2$. Relation to oriented bordism: $MSpin\to MSO$ is an equivalence after inverting 2. The kernel of the map from spin to oriented bordism is in dimensions k + 1$ and k + 2$ only and is the part generated by framed manifolds. It is the ideal generated by the non-trivial class of degree 1. The image in unoriented cobordism is all classes for which the characteristic numbers divisible by $w_1$ and $w_2$ are zero. </wikitex> == KO-Characteristic numbers == <wikitex>; Since Spin-manifolds have a natural KO-orientation, we can evaluate polynomials in the [[KO-Characteristic classes|KO-Pontryagin classes]] $\pi^j$ to get characteristic numbers. For $J=(j_1,\dots, j_n)$ we set $\pi^J=\pi^{j_1}\dots \pi^{j_n}$ and $n(J)=\sum_i j_i$. Using the Thom isomorphism $KO(BSpin)\cong KO(MSpin)$ we get a map $\pi^J:MSpin\to KO$, for which Anderson,Brown and Peterson show that it factorizes through $ko\langle 4n(J)\rangle$ if $n(J)$ is even and $ko\langle 4n(J)-2\rangle$ if $n(J)$ is odd. {{beginthm|Theorem {{cite|Anderson&Brown&Peterson1966}}}} There are classes $x_i\in H^*(MSpin;\Zz_2)$ such that there is a 2-local homotopy equivalence $$(\pi^J,x_i): MSpin \to\bigvee_{n(J)even, \ 1\not \in J}ko \langle 4n(J)\rangle \vee \bigvee_{n(J)odd, \ 1\not \in J}ko \langle 4n(J)-2 \rangle \vee \bigvee_{i}\Sigma^{|x_i|}H\Zz_2$$ {{endthm}} </wikitex> == Low dimensions == <wikitex>; $\Omega_0^{Spin}=\Zz$, generated by a point. $\Omega_1^{Spin}=\Zz_2$, generated by the circle with the "antiperiodic" spin structure. $\Omega_2^{Spin}=\Zz_2$, generated by the square of the generator of the first bordism group. $\Omega_3^{Spin}=0$. $\Omega_4^{Spin}=\Zz$, generated by the Kummer surface. $\Omega_5^{Spin}=\Omega_6^{Spin}=\Omega_7^{Spin}=0$. $\Omega_8^{Spin}=\Zz\oplus \Zz$, generated by quaternionic projective space, and 1/4 of the square of the Kummer surface. </wikitex> == References == {{#RefList:}} <!-- Please modify these headings or choose other headings according to your needs. --> [[Category:Manifolds]] {{Stub}}\Omega_n^{Spin}$ of manifolds with spin structures are the homotopy groups of the Thom spectrum $MSpin$$MSpin$.

2 Calculation

[Stong1968] Preliminary results were by Novikov. The main calculation is due to Anderson, Brown, and Peterson [Anderson&Brown&Peterson1966] who showed that all torsion is of order 2, being of two types: that arising by products with a framed $S^1$$S^1$ and that which maps monomorphically into unoriented cobordism. $\Omega_*^{Spin}/Torsion$$\Omega_*^{Spin}/Torsion$ is the subring of an integral polynomial ring on classes $x_{4i}$$x_{4i}$ (dimension 4i) consisting of all classes of dimension a multiple of 8 and twice the classes whose dimension is not a multiple of 8.

Characteristic numbers: Cobordism is determined by

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$\Zz_2$ cohomology and $KO$$KO$-theory characteristic numbers. Relation to framed bordism: The image of framed cobordism is 0 except in dimensions $8k+1,8k+2$$8k+1,8k+2$ where it is

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$\Zz_2$.

Relation to oriented bordism: $MSpin\to MSO$$MSpin\to MSO$ is an equivalence after inverting 2. The kernel of the map from spin to oriented bordism is in dimensions $8k + 1$$8k + 1$ and $8k + 2$$8k + 2$ only and is the part generated by framed manifolds. It is the ideal generated by the non-trivial class of degree 1.

The image in unoriented cobordism is all classes for which the characteristic numbers divisible by $w_1$$w_1$ and $w_2$$w_2$ are zero.

3 KO-Characteristic numbers

Since Spin-manifolds have a natural KO-orientation, we can evaluate polynomials in the KO-Pontryagin classes $\pi^j$$\pi^j$ to get characteristic numbers.

For $J=(j_1,\dots, j_n)$$J=(j_1,\dots, j_n)$ we set $\pi^J=\pi^{j_1}\dots \pi^{j_n}$$\pi^J=\pi^{j_1}\dots \pi^{j_n}$ and $n(J)=\sum_i j_i$$n(J)=\sum_i j_i$. Using the Thom isomorphism $KO(BSpin)\cong KO(MSpin)$$KO(BSpin)\cong KO(MSpin)$ we get a map $\pi^J:MSpin\to KO$$\pi^J:MSpin\to KO$, for which Anderson,Brown and Peterson show that it factorizes through $ko\langle 4n(J)\rangle$$ko\langle 4n(J)\rangle$ if $n(J)$$n(J)$ is even and $ko\langle 4n(J)-2\rangle$$ko\langle 4n(J)-2\rangle$ if $n(J)$$n(J)$ is odd.

Theorem [Anderson&Brown&Peterson1966] 3.1. There are classes $x_i\in H^*(MSpin;\Zz_2)$$x_i\in H^*(MSpin;\Zz_2)$ such that there is a 2-local homotopy equivalence

$\displaystyle (\pi^J,x_i): MSpin \to\bigvee_{n(J)even, \\ 1\not \in J}ko \langle 4n(J)\rangle \vee \bigvee_{n(J)odd, \\ 1\not \in J}ko \langle 4n(J)-2 \rangle \vee \bigvee_{i}\Sigma^{|x_i|}H\Zz_2$ $$\displaystyle (\pi^J,x_i): MSpin \to\bigvee_{n(J)even, \\ 1\not \in J}ko \langle 4n(J)\rangle \vee \bigvee_{n(J)odd, \\ 1\not \in J}ko \langle 4n(J)-2 \rangle \vee \bigvee_{i}\Sigma^{|x_i|}H\Zz_2$$

4 Low dimensions

$\Omega_0^{Spin}=\Zz$$\Omega_0^{Spin}=\Zz$, generated by a point.

$\Omega_1^{Spin}=\Zz_2$$\Omega_1^{Spin}=\Zz_2$, generated by the circle with the "antiperiodic" spin structure.

$\Omega_2^{Spin}=\Zz_2$$\Omega_2^{Spin}=\Zz_2$, generated by the square of the generator of the first bordism group.

$\Omega_3^{Spin}=0$$\Omega_3^{Spin}=0$.

$\Omega_4^{Spin}=\Zz$$\Omega_4^{Spin}=\Zz$, generated by the Kummer surface.

$\Omega_5^{Spin}=\Omega_6^{Spin}=\Omega_7^{Spin}=0$$\Omega_5^{Spin}=\Omega_6^{Spin}=\Omega_7^{Spin}=0$.

$\Omega_8^{Spin}=\Zz\oplus \Zz$$\Omega_8^{Spin}=\Zz\oplus \Zz$, generated by quaternionic projective space, and 1/4 of the square of the Kummer surface.

5 References

• [Anderson&Brown&Peterson1966] D. W. Anderson, E. H. Brown and F. P. Peterson, Spin cobordism, Bull. Amer. Math. Soc. 72 (1966), 256–260. MR0190939 (32 #8349) Zbl 0156.21605
• [Stong1968] R. E. Stong, Notes on cobordism theory, Princeton University Press, Princeton, N.J., 1968. MR0248858 (40 #2108) Zbl 0277.57010

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