Chern–Simons form

In mathematics, the Chern–Simons forms are certain secondary characteristic classes.^[1] The theory is named for Shiing-Shen Chern and James Harris Simons, co-authors of a 1974 paper entitled "Characteristic Forms and Geometric Invariants," from which the theory arose.^[2]

Definition

Given a manifold and a Lie algebra valued 1-form ${\displaystyle \mathbf {A} }$  over it, we can define a family of p-forms:^[3]

In one dimension, the Chern–Simons 1-form is given by

${\displaystyle \operatorname {Tr} [\mathbf {A} ].}$ 

In three dimensions, the Chern–Simons 3-form is given by

${\displaystyle \operatorname {Tr} \left[\mathbf {F} \wedge \mathbf {A} -{\frac {1}{3}}\mathbf {A} \wedge \mathbf {A} \wedge \mathbf {A} \right]=\operatorname {Tr} \left[d\mathbf {A} \wedge \mathbf {A} +{\frac {2}{3}}\mathbf {A} \wedge \mathbf {A} \wedge \mathbf {A} \right].}$ 

In five dimensions, the Chern–Simons 5-form is given by

${\displaystyle {\begin{aligned}&\operatorname {Tr} \left[\mathbf {F} \wedge \mathbf {F} \wedge \mathbf {A} -{\frac {1}{2}}\mathbf {F} \wedge \mathbf {A} \wedge \mathbf {A} \wedge \mathbf {A} +{\frac {1}{10}}\mathbf {A} \wedge \mathbf {A} \wedge \mathbf {A} \wedge \mathbf {A} \wedge \mathbf {A} \right]\\[6pt]={}&\operatorname {Tr} \left[d\mathbf {A} \wedge d\mathbf {A} \wedge \mathbf {A} +{\frac {3}{2}}d\mathbf {A} \wedge \mathbf {A} \wedge \mathbf {A} \wedge \mathbf {A} +{\frac {3}{5}}\mathbf {A} \wedge \mathbf {A} \wedge \mathbf {A} \wedge \mathbf {A} \wedge \mathbf {A} \right]\end{aligned}}}$ 

where the curvature F is defined as

${\displaystyle \mathbf {F} =d\mathbf {A} +\mathbf {A} \wedge \mathbf {A} .}$ 

The general Chern–Simons form ${\displaystyle \omega _{2k-1}}$  is defined in such a way that

${\displaystyle d\omega _{2k-1}=\operatorname {Tr} (F^{k}),}$ 

where the wedge product is used to define F^k. The right-hand side of this equation is proportional to the k-th Chern character of the connection ${\displaystyle \mathbf {A} }$ .

In general, the Chern–Simons p-form is defined for any odd p.^[4]

Application to physics

In 1978, Albert Schwarz formulated Chern–Simons theory, early topological quantum field theory, using Chern-Simons forms.^[5]

In the gauge theory, the integral of Chern-Simons form is a global geometric invariant, and is typically gauge invariant modulo addition of an integer.

See also

• Chern–Weil homomorphism
• Chiral anomaly
• Topological quantum field theory
• Jones polynomial

References

1. Freed, Daniel (January 15, 2009). "Remarks on Chern–Simons theory" (PDF). Retrieved April 1, 2020.
2. Chern, Shiing-Shen; Tian, G.; Li, Peter (1996). A Mathematician and His Mathematical Work: Selected Papers of S.S. Chern. World Scientific. ISBN 978-981-02-2385-4.
3. "Chern-Simons form in nLab". ncatlab.org. Retrieved May 1, 2020.
4. Moore, Greg (June 7, 2019). "Introduction To Chern-Simons Theories" (PDF). University of Texas. Retrieved June 7, 2019.
5. Kruglov, Sergey (2012). "Maxwell-Chern-Simons topologically massive gauge fields in the first-order formalism". International Journal of Theoretical Physics. 51 (1): 1–13. arXiv:1010.4728. Bibcode:2012IJTP...51....1K. doi:10.1007/s10773-011-0872-1. S2CID 254583801.

Further reading

• Chern, S.-S.; Simons, J. (1974). "Characteristic forms and geometric invariants". Annals of Mathematics. Second Series. 99 (1): 48–69. doi:10.2307/1971013. JSTOR 1971013.
• Bertlmann, Reinhold A. (2001). "Chern–Simons form, homotopy operator and anomaly". Anomalies in Quantum Field Theory (Revised ed.). Clarendon Press. pp. 321–341. ISBN 0-19-850762-3.