nLab spin bordism

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Contents

Idea

A spin bordism is a B-bordism for the tangential structure ((B,f)-structure) being the spin structure. Its bordism homology theory and cobordism cohomology theory are described by the Thom spectrum MSpin.

Definition

Let MM and NN be nn-dimensional spin manifolds with respective spin structures τ M:MBSpin(n)\tau_M\colon M\rightarrow BSpin(n) and τ N:NBSpin(n)\tau_N\colon N\rightarrow BSpin(n). A n+1n+1-dimensional spin manifold WW with spin structure τ W:WBSpin(n+1)\tau_W\colon W\rightarrow BSpin(n+1) together with inclusions i:MWi\colon M\hookrightarrow\partial W and j:NWj\colon N\hookrightarrow\partial W so that:

W=i(M)+j(N); \partial W =i(M)+j(N);
kτ M=τ Wi; \mathcal{B}k\circ\tau_M =\tau_W\circ i;
kτ N=τ Wj \mathcal{B}k\circ\tau_N =\tau_W\circ j

with the canonical inclusion k:Spin(n)Spin(n+1)k\colon Spin(n)\rightarrow Spin(n+1) is a spin bordism between MM and NN. It is fully denoted by (W,M,N,i,j)(W,M,N,i,j), but usually WW is sufficient from context.

Spin bordism groups

Under the equivalence relation of spin bordism, all nn-dimensional closed spin manifolds form the spin bordism group Ω n Spin\Omega_n^Spin, which has the disjoint union as composition, the empty manifold as neutral element and the inversion of orientation as inversion. According to Thom's theorem, spin bordism groups are exactly the stable homotopy groups of the Thom spectrum MSpin:

Ω n Spinπ nMSpin=lim kπ n+kMSpin k. \Omega_n^Spin \cong\pi_n MSpin =\lim_{k\rightarrow\infty}\pi_{n+k}MSpin_k.

Since BSpin=BO4BSpin = BO\langle 4\rangle is 33-connected, the first three spin bordism groups (0n20\leq n\leq 2) coincide with the framed bordism groups?:

  • Ω 0 SpinΩ 0 fr\Omega_0^Spin \cong \Omega_0^fr\cong\mathbb{Z}, generated by the point space,

  • Ω 1 SpinΩ 1 fr 2\Omega_1^Spin \cong \Omega_1^fr\cong\mathbb{Z}_2,

  • Ω 2 SpinΩ 2 fr 2\Omega_2^Spin \cong \Omega_2^fr\cong\mathbb{Z}_2.

Further spin bordism groups include:

  • Ω 3 Spin1\Omega_3^Spin\cong 1,

  • Ω 4 Spin\Omega_4^Spin \cong \mathbb{Z}, generated by the Kummer surface,

  • Ω 5 SpinΩ 6 SpinΩ 7 Spin1\Omega_5^Spin \cong \Omega_6^Spin\cong\Omega_7^Spin\cong 1,

  • Ω 8 Spin 2\Omega_8^Spin \cong \mathbb{Z}^2, generated by the quaternionic projective plane P 2\mathbb{H}P^2 and an 8-manifold obtained from the Kummer surface,

  • Ω 11 Spin1\Omega_11^Spin \cong 1, which plays a role in the discussion of 11D supergravity (“M-theory”).


Here is a table of the first 100 spin (co)bordism groups:

(from Buchanan-McKean 2026)

Spin bordism ring

All spin bordism groups in a direct sum form the spin bordism ring:

Ω Spin nΩ n Spin, \Omega^Spin \coloneqq\bigoplus_{n\in\mathbb{N}}\Omega_n^Spin,

which has the cartesian product as additional composition and the singleton as an additional neutral element.

Properties

Proposition

Every nn-dimensional spin manifold is spin bordant to a min{3,n21}\min\left\{3,\left\lceil\frac{n}{2}-1\right\rceil\right\}-connected spin manifold, equivalently meaning that every spin bordism homology class in Ω n Spin\Omega_n^Spin can be represented by such a spin manifold. (For n7n\geq 7, the result stabilizes at a 3-connected spin manifold.)

(Botvinnik & Labbi 14, Lem. 3.2 (1))

Proposition

For nn-dimensional min{3,n21}\min\left\{3,\left\lceil\frac{n}{2}-1\right\rceil\right\}-connected spin manifolds MM and NN, a spin bordism W:MNW\colon M\rightsquigarrow N exists with MWM\hookrightarrow W also min{3,n21}\min\left\{3,\left\lceil\frac{n}{2}-1\right\rceil\right\}-connected.

(Botvinnik & Labbi 14, Lem. 3.2 (2))

Proposition

If a nn-dimensional kk-connected compact spin manifold MM with k2k\leq 2 and n2k+3n\geq 2k+3 is spin bordant to another compact spin manifold NN, then MM can be obtained from NN by surgery of codimension at least k+2k+2.

(Botvinnik & Labbi 14, Prop. 3.4)

flavors of bordism homology theories/cobordism cohomology theories, their representing Thom spectra and cobordism rings:

bordism theory\;M(B,f) (B-bordism):

References

About general BOBO\langle\ell\rangle bordisms:

See also:

Last revised on March 18, 2026 at 09:14:28. See the history of this page for a list of all contributions to it.