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An ordinary gauge field (such as the electromagnetic field or the fields that induce the nuclear force) is a field (in the sense of physics) which is locally represented by a differential 1-form (the “gauge potential”) and whose field strength is locally a differential 2-form. For instance, in the case of the electromagnetic field this differential 2-form is the Faraday tensor.
Roughly speaking, a higher gauge field is similarly a field which is locally represented by differential forms of higher degree.
An explanation as to why an ordinary gauge field has a gauge potential given locally by a differential 1-form $A$ is that the trajectory of a charged particle is a 1-dimensional curve in spacetime $X$, its worldline, hence a smooth function $\gamma \colon \Sigma_1 \to X$, and the canonical way to produce an action functional on the mapping space of such curves is the integration of 1-forms over curves:
This is the parallel transport map or the holonomy map, if $\Sigma_1$ is a closed manifold. The contribution to the Euler-Lagrange equation of the particle obtained from the variation of this action functional is the Lorentz force which is exerted by the background gauge field on the particle.
When one generalizes in this picture from 0-dimensional particles with 1-dimensional worldlines to $p$-dimensional particles (often called “p-branes”) with $(p+1)$-dimensional worldvolumes $\gamma_{p+1} \colon \Sigma_{p+1} \to X$, then one needs, locally, a differential (p+1)-form $A_{p+1}$ on spacetime $X$
The field strength or flux of such a higher gauge field is, accordingly, locally the $(p+2)$-form $F_{p+2}$.
The archetypical example of such a higher gauge field is the (hypothetical) Kalb-Ramond field or B-field (a precursor of the axion field under KK-compactification) to which the charged 1-brane, the “string”, couples. This is locally a differential 2-form $B_2$, and the gauge-coupling term in the action functional for the string is accordingly, locally, of the form
This continues: next one may consider “2-branes”, i.e. membranes, and these will couple to a 3-form gauge field. For instance, the membrane which gives the name to M-theory (the M2-brane) couples to a 3-form field called the supergravity C-field.
But there is an important further aspect to higher gauge fields which makes this simple picture of higher degree differential forms drastically more rich:
Where an ordinary gauge field has gauge transformations $A_1 \mapsto A'_1$ given locally by smooth functions (0-forms) $\lambda_0$ via the de Rham differential $d_{dR}$
so a higher gauge field has higher gauge transformations given locally by $p$-forms $\lambda_p$:
But for $p \geq 0$ then a crucial new effect appears: these gauge transformations, being higher differential forms themselves, have “gauge-of-gauge transformations” between them, given by lower degree forms.
This phenomenon implies that higher gauge fields have a rich global (“topological”) structure, witnessed by the higher analog of their instanton sectors. Namely, while a higher gauge field to which a p-brane may couple is locally given by a $(p+1)$-form $A_{p+1}$, as one moves across coordinate charts this form gauge transforms by a $p$-form, which then itself, as one passes along two charts, transforms by a $(p-1)$-form, and so on.
The global structure for higher gauge fields obtained by carrying out this globalization via higher gauge transformations is the higher analog of that of a fiber bundle with connection on a bundle in higher differential geometry. This is sometimes known as a gerbe or, more generally, a principal infinity-bundle.
In fact the situation that there is just one gauge potential of degree $(p+1)$ with field strength of degree $(p+2)$ is just the simplest case, the “ordinary” case. More abstractly one says that such higher gauge fields are cocycles in ordinary differential cohomology.
More generally it may happen in higher gauge theory that the gauge potential is a formal linear combination of differential forms in various degrees.
The canonical example of this phenomenon is the RR-field in string theory. This has, locally, a gauge potential which is a differential form in every even degree, or every odd degree. If one is careful about the higher gauge transformations in this situation to find the correct global structure (the “instanton sector”) of the higher gauge field, then one finds that this now is a cocycle in a differential generalized cohomology, namely, in what is called differential topological K-theory. This may be understood as a higher and generalized form of the famous Dirac charge quantization condition for the electromagnetic field, see Freed 00. A lot of the fine detail of the anomaly cancellation in type II string theory depends on being careful about the global nature of this K-theoretic higher gauge RR-field (Distler-Freed-Moore 09)
Introduction and exposition includes
John Baez, John Huerta, An invitation to higher gauge theory, General Relativity and Gravitation 43 (2011), 2335-2392 (arXiv:1003.4485)
PhysicsForums-Insights Why higher category theory in physics?
Examples of prequantum field theories II: Higher gauge fields
For technical introduction to the RR-field as a higher gauge field (for more see at Dirac charge quantization):
Daniel Freed, Dirac charge quantization and generalized differential cohomology, Surveys in Differential Geometry, Int. Press, Somerville, MA, 2000, pp. 129–194 (arxiv:hep-th/0011220)
Jacques Distler, Dan Freed, Greg Moore, Orientifold Précis in: Hisham Sati, Urs Schreiber (eds.) Mathematical Foundations of Quantum Field and Perturbative String Theory Proceedings of Symposia in Pure Mathematics, AMS (2011) (arXiv:0906.0795, slides)
Deriving higher gauge symmetries through the variational bicomplex:
For foundations of higher prequantum field theory see
For foundations of higher gauge theory formalized in homotopy type theory see
For higher gauge theory in condensed matter physics see
Chenchang Zhu, Tian Lan, Xiao-Gang Wen, Topological non-linear σ-model, higher gauge theory, and a realization of all 3+1D topological orders for boson systems, (arXiv:1808.09394)
J.P. Ang, Abhishodh Prakash, Higher categorical groups and the classification of topological defects and textures, (arXiv:1810.12965)
Discussion of higher gauge theory modeling the Green-Schwarz mechanisms for anomaly cancellation in heterotic string theory, on M5-branes, and in related systems (ordered by arXiv time-stamp):
Hisham Sati, Urs Schreiber, Jim Stasheff, Twisted Differential String and Fivebrane Structures, Comm. Math. Phys. 315 (2012) 169-213 (arXiv:0910.4001, doi:10.1007/s00220-012-1510-3)
(via adjusted Weil algebras, see there for more)
Domenico Fiorenza, Hisham Sati, Urs Schreiber, The $E_8$ moduli 3-stack of the C-field in M-theory, Comm. Math. Phys. 333 1 (2015) 117-151 (arXiv:1202.2455)
Clay Cordova, Thomas Dumitrescu, Kenneth Intriligator, Exploring 2-Group Global Symmetries, J. High Energ. Phys. 2019 184 (2019) (arXiv:1802.04790, doi:10.1007/JHEP02(2019)184)
Francesco Benini, Clay Cordova, Po-Shen Hsin, On 2-Group Global Symmetries and Their Anomalies, J. High Energ. Phys. 2019 118 (2019) (arXiv:1803.09336, doi:10.1007/JHEP03(2019)118)
Domenico Fiorenza, Hisham Sati, Urs Schreiber, Twistorial Cohomotopy implies Green-Schwarz anomaly cancellation (arXiv:2008.08544)
Clay Cordova, Thomas T. Dumitrescu, Kenneth Intriligator, 2-Group Global Symmetries and Anomalies in Six-Dimensional Quantum Field Theories, J. High Energ. Phys. 2021, 252 (2021) (arXiv:2009.00138, doi:10.1007/JHEP04(2021)252)
Michele Del Zotto, Kantaro Ohmori, 2-Group Symmetries of 6D Little String Theories and T-Duality, Annales Henri Poincaré 22 (2021) 2451–2474 (arXiv:2009.03489, doi:10.1007/s00023-021-01018-3))
Hisham Sati, Urs Schreiber, The character map in equivariant twistorial Cohomotopy implies the Green-Schwarz mechanism with heterotic M5-branes (arXiv:2011.06533)
Yasunori Lee, Kantaro Ohmori, Yuji Tachikawa, Matching higher symmetries across Intriligator-Seiberg duality (arXiv:2108.05369)
Last revised on March 8, 2023 at 18:36:48. See the history of this page for a list of all contributions to it.