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Low energy resolvent asymptotics of the multipole Aharonov--Bohm Hamiltonian

T. J. Christiansen, K. Datchev, M. Yang

TL;DR

This work derives low-energy resolvent expansions for the Aharonov–Bohm Hamiltonian with multiple poles, revealing that the total flux $\beta=\sum_k \alpha_k$ dictates distinct analytic structures. When $\beta$ is an integer, the operator is conjugate to a compact perturbation of the Laplacian, yielding a three-term resolvent expansion with logarithmic terms; for non-integer $\beta$, a model resolvent $P_{\beta}$ governs the near-zero behavior, and the resolvent exhibits a mixed expansion with powers determined by $|\beta|$ and $1-|\beta|$. The resolvent has meromorphic continuation to the logarithmic cover $\Lambda$ (and to $\Lambda_q$ for rational $\beta$), and these expansions underpin the long-time wave asymptotics, showing an interpolation between even- and odd-dimensional scattering depending on $\beta$. The results extend the low-energy scattering theory to multi-pole Aharonov–Bohm systems and provide explicit leading-order terms and structural insights into the zero-energy regime. This has implications for understanding wave propagation and decay in magnetic systems with multiple topological singularities.

Abstract

We compute low energy asymptotics for the resolvent of the Aharonov--Bohm Hamiltonian with multiple poles for both integer and non-integer total fluxes. For integral total flux we reduce to prior results in black-box scattering while for non-integral total flux we build on the corresponding techniques using an appropriately chosen model resolvent. The resolvent expansion can be used to obtain long-time wave asymptotics for the Aharonov--Bohm Hamiltonian with multiple poles. An interesting phenomenon is that if the total flux is an integer then the scattering resembles even-dimensional Euclidean scattering, while if it is half an odd integer then it resembles odd-dimensional Euclidean scattering. The behavior for other values of total flux thus provides an `interpolation' between these.

Low energy resolvent asymptotics of the multipole Aharonov--Bohm Hamiltonian

TL;DR

This work derives low-energy resolvent expansions for the Aharonov–Bohm Hamiltonian with multiple poles, revealing that the total flux dictates distinct analytic structures. When is an integer, the operator is conjugate to a compact perturbation of the Laplacian, yielding a three-term resolvent expansion with logarithmic terms; for non-integer , a model resolvent governs the near-zero behavior, and the resolvent exhibits a mixed expansion with powers determined by and . The resolvent has meromorphic continuation to the logarithmic cover (and to for rational ), and these expansions underpin the long-time wave asymptotics, showing an interpolation between even- and odd-dimensional scattering depending on . The results extend the low-energy scattering theory to multi-pole Aharonov–Bohm systems and provide explicit leading-order terms and structural insights into the zero-energy regime. This has implications for understanding wave propagation and decay in magnetic systems with multiple topological singularities.

Abstract

We compute low energy asymptotics for the resolvent of the Aharonov--Bohm Hamiltonian with multiple poles for both integer and non-integer total fluxes. For integral total flux we reduce to prior results in black-box scattering while for non-integral total flux we build on the corresponding techniques using an appropriately chosen model resolvent. The resolvent expansion can be used to obtain long-time wave asymptotics for the Aharonov--Bohm Hamiltonian with multiple poles. An interesting phenomenon is that if the total flux is an integer then the scattering resembles even-dimensional Euclidean scattering, while if it is half an odd integer then it resembles odd-dimensional Euclidean scattering. The behavior for other values of total flux thus provides an `interpolation' between these.
Paper Structure (21 sections, 14 theorems, 69 equations, 2 figures)

This paper contains 21 sections, 14 theorems, 69 equations, 2 figures.

Key Result

Theorem 1

Let $\chi \in C_c^\infty(\mathbb{R}^2)$, and $f_1,\;u$ be as in eq:waveIntro. Suppose no three elements of $S$ are colinear. Then, as $t\rightarrow \infty$,

Figures (2)

  • Figure 1: In this example, $\tilde{\alpha} = \alpha_j$ on $\Gamma_j$ for $j = 2$ and $j=5$, $\tilde{\alpha} = \alpha_3 + \alpha_4$ on $\Gamma_3$, and $\tilde{\alpha} = \alpha_4$ on $\Gamma_4 \setminus \Gamma_3$.
  • Figure 2: Examples for which we can compute $G$ and $C_{\vec{A}}$.

Theorems & Definitions (24)

  • Theorem 1
  • Theorem 2
  • Theorem 3
  • Theorem 4
  • Lemma 3.1
  • proof
  • Lemma 3.2
  • proof
  • Lemma 4.1
  • proof
  • ...and 14 more