Spin structure

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In geometry, a spin structure is an additional piece of data which can sometimes be specified on a vector bundle over a differentiable manifold. A spin structure on a vector bundle allows one to define associated spinor bundles, giving rise to the notion of a spinor in differential geometry.

Spin structures have wide applications to mathematical physics, in particular to quantum field theory where they are an essential ingredient in the definition of any theory with uncharged fermions. They are also of purely mathematical interest in differential geometry, algebraic topology, and K theory. They form the foundation for spin geometry.

Contents 1 Introduction 2 Spin structures 2.1 Obstruction 2.2 Classification 2.3 Application to particle physics 2.4 Examples 3 SpinC structures 3.1 Obstruction 3.2 Classification 3.2.1 Geometric picture 3.2.2 The details 3.2.3 Integral lifts of Stiefel-Whitney classes 3.3 Application to particle physics 3.4 Examples 4 Vector structures 4.1 Obstruction 4.2 Application to particle physics 5 See also 6 References 7 Further reading

[edit] Introduction

Let X be a paracompact topological manifold and E an oriented vector bundle on X of dimension n equipped with a fibre metric. This means that at each point of X, the fibre of E is an inner product space, and so determines spinor representations. A spinor bundle of E is a prescription for consistently associating a spinor representation to every point of X. There are topological obstructions to being able to do it, and consequently, a given bundle E may not admit any spinor bundle. In case it does, one says that the bundle E is spin.

This may be made rigorous through the language of principal bundles. The collection of oriented orthonormal frames of a vector bundle form a frame bundle P_SO(E), which is a principal bundle under the action of the special orthogonal group SO(n). A spin structure for P_SO(E) is a lift of P_SO(E) to a principal bundle P_Spin(E) under the action of the spin group Spin(n), by which we mean that there exists a bundle map φ : P_Spin(E) → P_SO(E) such that

φ(pg) = φ(p)ι(g), for all p ∈ P_Spin(E) and g ∈ Spin(n),

where ι : Spin(n) → SO(n) is the mapping of groups presenting the spin group as a double-cover of SO(n).

In the special case in which E is the tangent bundle, if a spin structure exists then one says that M is a spin manifold. Equivalently M is spin if the SO(n) principal bundle of orthonormal bases of the tangent fibers of M are a Z₂ quotient of a principal spin bundle.

[edit] Spin structures

[edit] Obstruction

A spin structure exists if and only if the second Stiefel-Whitney class w₂ of E vanishes. This is a result of Armand Borel and Friedrich Hirzebruch^[1]. Note, we have assumed is an orientable vector bundle.

[edit] Classification

When spin structures exist, the inequivalent spin structures on a manifold are in one-to-one correspondence with the elements of H¹(M,Z₂), which by the universal coefficient theorem is isomorphic to H₁(M,Z₂).

Intuitively, for each nontrivial cycle on M a spin structure corresponds to a binary choice of whether a section of the SO(N) bundle switches sheets when one encircles the loop. If w₂ vanishes then these choices may be extended over the two-skeleton, then (by obstruction theory) they may automatically be extended over all of M. In particle physics this corresponds to a choice of periodic or antiperiodic boundary conditions for fermions going around each loop.

[edit] Application to particle physics

In particle physics the spin statistics theorem implies that the wavefunction of an uncharged fermion is a section of the associated vector bundle to the spin lift of an SO(N) bundle E. Therefore the choice of spin structure is part of the data needed to define the wavefunction, and one often needs to sum over these choices in the partition function. In many physical theories E is the tangent bundle, but for the fermions on the worldvolumes of D-branes in string theory it is a normal bundle.

[edit] Examples

1. A genus g Riemann surface admits 2^2g inequivalent spin structures; see theta characteristic.
2. The complex projective space CP² is not spin.
3. All compact, orientable manifolds of dimension 3 or less are spin.

[edit] Spin^C structures

A spin^c structure is analogous, but uses the spin^c group, which is the U(1)-extension of SO(n) built on top of the extension by the cyclic group of order 2 in Spin(n). Specifically, it is the twisted-product . It is the quotient group obtained from with respect to the normal which is generated by the pair of covering transformations for the bundles and respectively. This makes the spin^c group both a bundle over the circle with fibre Spin(n), and a bundle over SO(n) with fibre a circle. ^[2]

[edit] Obstruction

A spin^c structure exists when the second Stiefel-Whitney class of the bundle E is in the image of the map (in other words, the third integral Stiefel-Whitney class vanishes). In this case one says that E is spin^c. Intuitively, the lift gives the Chern class of the square of the U(1) part of any obtained spin^c bundle.

[edit] Classification

When they exist, spin^c structures are classified by H²(M;Z).

[edit] Geometric picture

This has the following geometric interpretation, which is due to Edward Witten. When the spin^c structure is nonzero this square root bundle has a non-integral Chern class, which means that it fails the triple overlap condition. In particular, the product of transition functions on a three-way intersection is not always equal to one, as is required for a principal bundle. Instead it is sometimes −1.

This failure occurs at precisely the same intersections as an identical failure in the triple products of transition functions of the obstructed spin bundle. Therefore the triple products of transition functions of the full spin^c bundle, which are the products of the triple product of the spin and U(1) component bundles, are either 1²=1 or -1²=1 and so the spin^c bundle satisfies the triple overlap condition and is therefore a legitimate bundle.

[edit] The details

The above intuitive geometric picture may be made concrete as follows. Consider the short exact sequence Z →Z →Z₂ where the first arrow is multiplication by 2 and the second is reduction modulo 2. This induces a long exact sequence on cohomology, which contains

where the second arrow multiplication by 2, the third is induced by restriction modulo 2 and the fourth is the associated Bockstein homomorphism β.

The obstruction to the existence of a spin bundle is an element w₂ of H²(M,Z₂). It reflects the fact that one may always locally lift an SO(N) bundle to a spin bundle, but one needs to choose a Z₂ lift of each transition function, which is a choice of sign. The lift does not exist when the product of these three signs on a triple overlap is -1, which yields the Cech cohomology picture of w₂.

To cancel this obstruction, one tensors this spin bundle with a U(1) bundle with the same obstruction w₂. Notice that this is an abuse of the word bundle, as neither the spin bundle nor the U(1) bundle satisfies the triple overlap condition and so neither is actually a bundle.

A legitimate U(1) bundle is classified by its Chern class, which is an element of H²(M,Z). Identify this class with the first element in the above exact sequence. The next arrow doubles this Chern class, and so legitimate bundles will correspond to even elements in the second H²(M,Z), while odd elements will correspond to bundles that fail the triple overlap condition. The obstruction then is classified by the failure of an element in the second H²(M,Z) to be in the image of the arrow, which, by exactness, is classified by its image in H²(M,Z₂) under the next arrow.

To cancel the corresponding obstruction in the spin bundle, this image needs to be w₂. In particular, if w₂ is not in the image of the arrow, then there does not exist any U(1) bundle with obstruction equal to w₂ and so the obstruction cannot be cancelled. By exactness, w₂ is in the image of the preceding arrow only if it is in the kernel of the next arrow, which we recall is the Bockstein homomorphism β. That is, the condition for the cancellation of the obstruction is

W₃ = βw₂ = 0

where we have used the fact that the third integral Stiefel-Whitney class W₃ is the Bockstein of the second Stiefel-Whitney class w₂ (this can be taken as a definition of W₃).

[edit] Integral lifts of Stiefel-Whitney classes

This argument also demonstrates that second Stiefel-Whitney class defines elements not only of Z₂ cohomology but also of integral cohomology in one higher degree. In fact this is the case for all even Stiefel-Whitney classes. It is traditional to use an uppercase W for the resulting classes in odd degree, which are called the integral Stiefel-Whitney classes, and are labeled by their degree (which is always odd).

[edit] Application to particle physics

In quantum field theory charged spinors are sections of associated spin^c bundles, and in particular no charged spinors can exist on a space that is not spin^c. An exception arises in some supergravity theories where additional interactions imply that other fields may cancel the third Stiefel-Whitney class.

[edit] Examples

1. All compact, oriented, smooth manifolds of dimension 4 or less are spin^c.
2. All almost complex manifolds are spin^c.
3. All spin manifolds are spin^c.

[edit] Vector structures

While spin structures are lifts of vector bundles to associated spin bundles, vector structures are lifts of other bundles to associated vector bundles.

[edit] Obstruction

For example, consider an SO(8) bundle. The group SO(8) has three 8-dimensional representations, two of which are spinorial and one of which is the vector representation. These three representations are exchanged by an isomorphism known as triality. Given an SO(8) vector bundle E, the obstruction to the construction of an associated spin bundle is the second Stiefel-Whitney class w₂(E), which is an element of the second cohomology group with Z₂ coefficients. By triality, given an SO(8) spin bundle F, the obstruction to the existence of an associated vector bundle is another element of the same cohomology group, which is often denoted .

[edit] Application to particle physics

Vector structures were first considered in physics, in the paper Anomalies, Dualities and Topology of D=6, N=1 Superstring Vacua by Micha Berkooz, Robert Leigh, Joseph Polchinski, John Schwarz, Nathan Seiberg and Edward Witten. They were considering type I string theory, whose configurations consist of a 10-manifold with a Spin(32)/Z₂ principle bundle over it. Such a bundle has a vector structure, and so lifts to an SO(32) bundle, when the triple product of the transition functions on all triple intersection is the trivial element of the Z₂ quotient. This happens precisely when , the characteristic 2-cocycle with Z₂ coefficients, vanishes.

The following year, in The Mirror Transform of Type I Vacua in Six Dimensions, Ashoke Sen and Savdeep Sethi demonstrated that type I superstring theory is only consistent, in the absence of fluxes, when this characteristic class is trivial. More generally, in type I string theory the B-field is also a class in the second cohomology with Z₂ coefficients and they demonstrated that it must be equal to .

[edit] See also

• Spinor
• Spinor bundle

[edit] References

1. ^ Borel, A. and Hirzebruch, F. Characteristic classes and homogeneous spaces I, Amer. J. Math 80 (1958), 97-136)
2. ^ R.Gompf, Spin^c-structures and homotopy equivalences. Geometry and Topology, Vol 1, (1997) 41--50.

[edit] Further reading

• Something on Spin Structures by Sven-S. Porst is a short introduction to orientation and spin structures for mathematics students.