Existence of solutions to Chern-Simons-Higgs equations on graphs

preprint2022arXivOpen access

Abstract

Let G=(V,E)G=(V,E) be a finite graph. We consider the existence of solutions to a generalized Chern-Simons-Higgs equation Δu=−λeg(u)(eg(u)−1)2+4π∑j=1Nδpj Δu=-λe^{g(u)}\left( e^{g(u)}-1\right)^2+4π\sum\limits_{j=1}^{N}δ_{p_j} on GG, where λλ is a positive constant; g(u)g(u) is the inverse function of u=f(υ)=1+υ−eυu=f(\upsilon)=1+\upsilon-e^{\upsilon} on (−∞,0](-\infty, 0]; NN is a positive integer; p1,p2,⋅⋅⋅,pNp_1, p_2, \cdot\cdot\cdot, p_N are distinct vertices of VV and δpjδ_{p_j} is the Dirac delta mass at pjp_j. We prove that there is critical value λcλ_c such that the generalized Chern-Simons-Higgs equation has a solution if and only if λ≥λcλ\geq λ_c . We also prove the existence of solutions to the Chern-Simons-Higgs equation Δu=λeu(eu−1)+4π∑j=1Nδpj Δu=λe^{u}(e^{u}-1)+4π\sum\limits_{j=1}^{N}δ_{p_j} on GG when λλ takes the critical value λcλ_c and this completes the results of An Huang, Yong Lin and Shing-Tung Yau (Commun. Math. Phys. 377, 613-621 (2020)).

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