nLab Spin Chern-Simons theory (changes)

Showing changes from revision #8 to #9: Added | Removed | Changed

Context

Cohomology

cohomology

Special and general types

Special notions

Variants

Extra structure

Operations

Theorems

Quantum field theory

∞\infty-Chern-Weil theory

Contents

Idea

What is called Spin Chern-Simons theory is a (pre-)quantum field theory like Chern-Simons field theory but defined on/restricted to 3-manifolds equipped with spin structure and making use of that structure to divide the action functional (in the exponent) by 2.

(Beware that there is also ordinary GG-Chern-Simons theory for gauge group G=Spin(n)G = Spin(n) a spin group, which in traditional parlance one might also pronounce as “Spin Chern-Simons theory”, but which is different, in general, from Spin Chern-Simons theory in the sense discussed here.)

The division by 2 makes the holographically dual theory in 2d be the correct self-dual theory. The generalization of the Spin structure to higher dimensional Chern-Simons theory is that of integral Wu structure. In the next relevant case of 7d Chern-Simons theory this is related to the flux quantizaton condition on the supergravity C-field wholse holographically related self-dual higher gauge field is the 2-form-field in the 6d (2,0)-superconformal QFT on the M5-brane.

Properties

Relation to framed Chern-Simons theory

In general, Chern-Simons theory requires 3-manifolds equipped with 2-framings. But the combination of a 2-framing with a spin structure is essentially an actual framing, cf. Sawin 2002 p 2.

The following table lists classes of examples of square roots of line bundles

line bundlesquare rootchoice corresponds to
canonical bundleTheta characteristicover Riemann surface and Hermitian manifold (e.g.Kähler manifold): spin structure
density bundlehalf-density bundle
canonical bundle of Lagrangian submanifoldmetalinear structuremetaplectic correction
determinant line bundlePfaffian line bundle
quadratic secondary intersection pairingpartition function of self-dual higher gauge theoryintegral Wu structure

References

The idea of spin Chern-Simons theory originates with

Indication that the effective abelian Chern-Simons theory describing the fractional quantum Hall effect has to be understood, in general, as a spin Chern-Simons theory:

Further discussion:

For general (compact) gauge Lie groups:

  • Stephen F. Sawin: Invariants of Spin Three-Manifolds From Chern-Simons Theory and Finite-Dimensional Hopf Algebras, Advances in Mathematics 165 1 (2002) 35-70 [[arXiv:math/9910106](http://arxiv.org/abs/math/9910106), doi:10.1006/aima.2000.1935]

  • Jerome Jenquin, Classical Chern-Simons on manifolds with spin structure [[arXiv:0504524](http://arxiv.org/abs/math/0504524)]

  • Jerome Jenquin, Spin Chern-Simons and Spin TQFTs [[arXiv:0605239](http://arxiv.org/abs/math/0605239)]

Specifically for abelian gauge groups U(1) n\mathrm{U}(1)^n (abelian Chern-Simons theory):

  • Dmitriy Belov,Gregory Moore

    Dmitriy Belov, Gregory Moore: Classification of abelian spin Chern-Simons theories [[arXiv:hep-th/0505235](http://arxiv.org/abs/hep-th/0505235)]

    :Classification of abelian spin Chern-Simons theories [[arXiv:hep-th/0505235](http://arxiv.org/abs/hep-th/0505235)]
  • Dmitriy Belov, Gregory Moore, Holographic Action for the Self-Dual Field [[arXiv:hep-th/0605038](http://arxiv.org/abs/hep-th/0605038)]

    (in view ofself-dual higher gauge theory)

  • Takuya Okuda, Koichi Saito, Shuichi Yokoyama: U(1)U(1) spin Chern-Simons theory and Arf invariants in two dimensions, Nuclear Physics B 962 (2021) 115272 [doi:10.1016/j.nuclphysb.2020.115272, arXiv:2005.03203]

and with emphasis on the holographically dual self-dual higher gauge theory:

  • Dmitriy Belov, Gregory Moore, Holographic Action for the Self-Dual Field [[arXiv:hep-th/0605038](http://arxiv.org/abs/hep-th/0605038)]

    (based on work by Witten and Hopkins-Singer, see the references at self-dual higher gauge theory).

Last revised on March 30, 2025 at 10:29:02. See the history of this page for a list of all contributions to it.