Abstract
We study solutions to the Yang–Mills–Higgs equations on the maximal Cauchy development of the data given on a ball of radius R in \(\mathbb {R}^3\). The energy of the data could be infinite and the solution grows at most inverse polynomially in \(R-t\) as \(t\rightarrow R\). As applications, we derive pointwise decay estimates for Yang–Mills–Higgs fields in the future of a hyperboloid or in the Minkowski space \(\mathbb {R}^{1+3}\) for data bounded in the weighted energy space with weights \(|x|^{1+\epsilon }\). Moreover, for the abelian case of Maxwell–Klein–Gordon system, we extend the small data result of Lindblad and Sterbenz (IMRP Int Math Res Pap 109:1687-3017, 2006) to general large data (under same assumptions but without any smallness). The proof is gauge independent and it is based on the framework of Eardley and Moncrief (Commun Math Phys 83(2):171–191, 1982a, 1982b) together with the geometric Kirchhoff–Sobolev parametrix constructed by Klainerman and Rodnianski (J Hyperbolic Differ Equ 4(3):401–433, 2007). The new ingredient is a class of weighted energy estimates through backward light cones adapted to the initial data.
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Notes
We have \(A_{\mu } \cdot \phi =\beta _*(A_{\mu })(\phi )\), where \(\beta _*:\mathfrak {g}\rightarrow \mathfrak {u}(V)\) is the tangent map of \(\beta \).
If we formally expand the Yang–Mills field F near the spatial infinity
$$\begin{aligned} F=F_2+F_3+\cdots +F_k+\cdots ,\quad F_k=O(|x|^{-k}), \end{aligned}$$then \(F_2\), \(F_3\) and \(F_4\) vanish at any fixed time.
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Acknowledgements
S. Yang is supported by the National Science Foundation of China 12171011, 12141102 and the National Key R &D Program of China 2021YFA1001700. P. Yu is supported by the National Science Foundation of China 11825103, 12141102, MOST-2020YFA0713003 and Xiaomi Fellowship.
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Wei, D., Yang, S. & Yu, P. On the Global Dynamics of Yang–Mills–Higgs Equations. Commun. Math. Phys. 405, 4 (2024). https://doi.org/10.1007/s00220-023-04881-9
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DOI: https://doi.org/10.1007/s00220-023-04881-9