Wu–Yang dictionary

Mathematical physics relation

In topology and high energy physics, the Wu–Yang dictionary refers to the mathematical identification that allows back-and-forth translation between the concepts of gauge theory and those of differential geometry. The dictionary appeared in 1975 in an article by Tai Tsun Wu and C. N. Yang comparing electromagnetism and fiber bundle theory.[1] This dictionary has been credited as bringing mathematics and theoretical physics closer together.[2]

A crucial example of the success of the dictionary is that it allowed the understanding of monopole quantization in terms of Hopf fibrations.[3][4]

## History

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Equivalences between fiber bundle theory and gauge theory were hinted at the end of the 1960s. In 1967, mathematician Andrzej Trautman started a series of lectures aimed at physicists and mathematicians at King's College London regarding these connections.[4]

Theoretical physicists Tai Tsun Wu and C. N. Yang working in Stony Brook University, published a paper in 1975 on the mathematical framework of electromagnetism and the Aharonov–Bohm effect in terms of fiber bundles. A year later, mathematician Isadore Singer came to visit and brought a copy back to the University of Oxford.[2][5][6] Singer showed the paper to Michael Atiyah and other mathematicians, sparking a close collaboration between physicists and mathematicians.[2]

Yang also recounts a conversation that he had with one of the mathematicians that founded fiber bundle theory, Shiing-Shen Chern:[2]

> In 1975, impressed with the fact that gauge fields are connections on fiber bundles, I drove to the house of Shiing-Shen Chern in El Cerrito, near Berkeley. (I had taken courses with him in the early 1940s when he was a young professor and I an undergraduate student at the National Southwest Associated University in Kunming, China. That was before fiber bundles had become important in differential geometry and before Chern had made history with his contributions to the generalized Gauss–Bonnet theorem and the Chern classes.) We had much to talk about: friends, relatives, China. When our conversation turned to fiber bundles, I told him that I had finally learned from Jim Simons the beauty of fiber-bundle theory and the profound Chern-Weil theorem. I said I found it amazing that gauge fields are exactly connections on fiber bundles, which the mathematicians developed without reference to the physical world. I added ‘this is both thrilling and puzzling, since you mathematicians dreamed up these concepts out of nowhere.’ He immediately protested, ‘No, no. These concepts were not dreamed up. They were natural and real.'

In 1977, Trautman used these results to demonstrate an equivalence between a quantization condition for magnetic monopoles used by Paul Dirac back in 1931 and Hopf fibration, a fibration of a 3-sphere proposed io the same year by mathematician Heinz Hopf.[4] Mathematician Jim Simons discussing this equivalence with Yang expressed that “Dirac had discovered trivial and nontrivial bundles before mathematicians.”[4]

In the original paper, Wu and Yang added sources (like the electric current) to the dictionary next to a blank spot, indicating a lack of any equivalent concept on the mathematical side. During interviews, Yang recalls that Singer and Atiyah found great interest in this concept of sources, which was unknown for mathematicians but that physicists knew since the 19th century. Mathematicians started working on that, which lead to the development of Donaldson theory by Simon Donaldson, a student of Atiyah.[7][8]

## Description

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### Summarized version

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The Wu-Yang dictionary relates terms in particle physics with terms in mathematics, specifically fiber bundle theory. Many versions and generalization of the dictionary exist. Here is an example of a dictionary, which puts each physics term next to its mathematical analogue:[9]

Physics  | Mathematics

|

Potential  | Connection
Field tensor (interaction)  | Curvature
Field tensor-potential relation  | Structural equation
Gauge transformation  | Change of bundle coordinates
Gauge group | Structure group

### Original version for electromagnetism

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Aharonov-Bohm experiment: electrons pass around a cylinder where there is a non-zero magnetic field. Outside the cylinder the field strength is 0.

Wu and Yang considered the description of an electron traveling around a cylinder in the presence of a magnetic field inside the cylinder (outside the cylinder the field vanishes i.e.  f μ ν = 0 {\displaystyle f_{\mu \nu }=0} ). According to the Aharonov–Bohm effect, the interference patterns shift by a factor  exp ⁡ ( − i Ω / Ω 0 ) {\displaystyle \exp(-i\Omega /\Omega _{0})} , where  Ω {\displaystyle \Omega } is the magnetic flux and  Ω 0 {\displaystyle \Omega _{0}} is the magnetic flux quantum. For two different fluxes a and b, the results are identical if  Ω a − Ω b = N Ω 0 {\displaystyle \Omega _{a}-\Omega _{b}=N\Omega _{0}} , where  N {\displaystyle N} is an integer. We define the operator  S a b {\displaystyle S_{ab}} as the gauge transformation that brings the electron wave function from one configuration to the other  ψ b = S b a ψ a {\displaystyle \psi _{b}=S_{ba}\psi _{a}} . For an electron that takes a path from point P to point Q, we define the phase factor as

Φ Q P = exp ⁡ ( − i Ω 0 ∫ P Q A μ d x μ ) {\displaystyle \Phi _{QP}=\exp \left(-{\frac {i}{\Omega _{0}}}\int _{P}^{Q}A_{\mu }\mathrm {d} x^{\mu }\right)} ,

where  A μ {\displaystyle A_{\mu }} is the electromagnetic four-potential. For the case of a SU2 gauge field, we can make the substitution

A μ = i b μ k X k {\displaystyle A_{\mu }=ib_{\mu }^{k}X_{k}} ,

where  X k = − i σ k / 2 {\displaystyle X_{k}=-i\sigma _{k}/2} are the generators of SU2,  σ k {\displaystyle \sigma _{k}} are the Pauli matrices. Under these concepts, Wu and Yang showed the relation between the language of gauge theory and fiber bundles, was codified in following dictionary:[2][10][11]

Wu–Yang dictionary (1975)[1] Gauge field terminology  | Bundle terminology

|

gauge (or global gauge)  | principal coordinate bundle
gauge type  | principal fiber bundle
gauge potential  b μ k {\displaystyle b_{\mu }^{k}} | connection on principal fiber bundle
S b a {\displaystyle S_{ba}} (see above in this section)  | transition function
phase factor  Φ Q P {\displaystyle \Phi _{QP}} | parallel displacement
field strength f μ ν k {\displaystyle f_{\mu \nu }^{k}} | curvature
source[a] J μ k {\displaystyle J_{\mu }^{k}} | ?
electromagnetism  | connection on a U1(1) bundle
isotopic spin gauge field  | connection on a SU2 bundle
Dirac's monopole quantization | classification of U1(1) bundle according to first Chern class
electromagnetism without monopole  | connection on a trivial U1(1) bundle
electromagnetism with monopole  | connection on a nontrivial U1(1) bundle

1. ^ The original table also included the note: "i.e. electrical source. This is the generalization (See Ref.[12]) of the concept of electric charges and currents."

## See also

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* 't Hooft–Polyakov monopole
* Wu–Yang monopole

## References

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1. ^ a b Wu, Tai Tsun; Yang, Chen Ning (1975-12-15). "Concept of nonintegrable phase factors and global formulation of gauge fields". Physical Review D. 12 (12): 3845–3857. doi:10.1103/PhysRevD.12.3845. ISSN 0556-2821.
2. ^ a b c d e Poo, Mu-ming; Chao, Alexander Wu (2020-01-01). "Conversation with Chen-Ning Yang: reminiscence and reflection". National Science Review. 7 (1): 233–236. doi:10.1093/nsr/nwz113. ISSN 2095-5138. PMC 8288855. PMID 34692035.
3. ^ Woit, Peter (5 April 2008). "Stony Brook Dialogues in Mathematics and Physics". Not even wrong blog. Retrieved 2023-03-14.
4. ^ a b c d Friedman, John L. (2015). "Historical note on fiber bundles". Physics Today. 68 (6): 11. doi:10.1063/PT.3.2799.
5. ^ Wells, Raymond O'Neil; Weyl, Hermann (1988). The Mathematical Heritage of Hermann Weyl. American Mathematical Soc. ISBN 978-0-8218-1482-6.
6. ^ Freed, Daniel S. (2021). "Isadore Singer Transcended Mathematical Boundaries". Quanta Magazine.
7. ^ Yang, C. N. (2009). "C. N. Yang: Stony Brook Masters Series" (Interview). Interviewed by Bill Zimmerman.
8. ^ Wilson, Robin; Gray, Jeremy (2012-12-06). Mathematical Conversations: Selections from The Mathematical Intelligencer. Springer Science & Business Media. ISBN 978-1-4613-0195-0.
9. ^ Zeidler, Eberhard (2008-09-03). Quantum Field Theory II: Quantum Electrodynamics: A Bridge between Mathematicians and Physicists. Springer Science & Business Media. ISBN 978-3-540-85377-0.
10. ^ Boi, Luciano (2004). "Geometrical and topological foundations of theoretical physics: from gauge theories to string program". International Journal of Mathematics and Mathematical Sciences. 2004 (34): 1777–1836. doi:10.1155/S0161171204304400. ISSN 0161-1712.
11. ^ Wells, Raymond O'Neil; Weyl, Hermann (1988). The Mathematical Heritage of Hermann Weyl. American Mathematical Soc. ISBN 978-0-8218-1482-6.
12. ^ Yang, C. N. (1974-08-12). "Integral Formalism for Gauge Fields". Physical Review Letters. 33 (7): 445–447. doi:10.1103/PhysRevLett.33.445. ISSN 0031-9007.