1,392 research outputs found

    Approximate Zero Modes for the Pauli Operator on a Region

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    Let PΞ©,tA\mathcal{P}_{\Omega,tA} denoted the Pauli operator on a bounded open region Ξ©βŠ‚R2\Omega\subset\mathbb{R}^2 with Dirichlet boundary conditions and magnetic potential AA scaled by some t>0t>0. Assume that the corresponding magnetic field B=curl AB=\mathrm{curl}\,A satisfies B∈Llog⁑L(Ξ©)∩CΞ±(Ξ©0)B\in L\log L(\Omega)\cap C^\alpha(\Omega_0) where Ξ±>0\alpha>0 and Ξ©0\Omega_0 is an open subset of Ξ©\Omega of full measure (note that, the Orlicz space Llog⁑L(Ξ©)L\log L(\Omega) contains Lp(Ξ©)L^p(\Omega) for any p>1p>1). Let NΞ©,tA(Ξ»)\mathsf{N}_{\Omega,tA}(\lambda) denote the corresponding eigenvalue counting function. We establish the strong field asymptotic formula NΞ©,tA(Ξ»(t))=t2Ο€βˆ«Ξ©βˆ£B(x)βˆ£β€‰dxβ€…β€Š+o(t) \mathsf{N}_{\Omega,tA}(\lambda(t))=\frac{t}{2\pi}\int_{\Omega}\lvert B(x)\rvert\,dx\;+o(t) as tβ†’+∞t\to+\infty, whenever Ξ»(t)=Ceβˆ’ctΟƒ\lambda(t)=Ce^{-ct^\sigma} for some Οƒβˆˆ(0,1)\sigma\in(0,1) and c,C>0c,C>0. The corresponding eigenfunctions can be viewed as a localised version of the Aharonov-Casher zero modes for the Pauli operator on R2\mathbb{R}^2.Comment: 28 pages; for the sake of clarity the main results have been reformulated and some minor presentational changes have been mad

    Asymptotics for Erdos-Solovej Zero Modes in Strong Fields

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    We consider the strong field asymptotics for the occurrence of zero modes of certain Weyl-Dirac operators on R3\mathbb{R}^3. In particular we are interested in those operators DB\mathcal{D}_{B} for which the associated magnetic field BB is given by pulling back a 22-form Ξ²\beta from the sphere S2\mathbb{S}^2 to R3\mathbb{R}^3 using a combination of the Hopf fibration and inverse stereographic projection. If ∫S2Ξ²β‰ 0\int_{\mathbb{S}^2}\beta\neq0 we show that βˆ‘0≀t≀Tdim Ker DtB=T28Ο€2β€‰βˆ£βˆ«S2Ξ²βˆ£β€‰βˆ«S2∣β∣+o(T2) \sum_{0\le t\le T}\mathrm{dim}\,\mathrm{Ker}\,\mathcal{D}_{tB} =\frac{T^2}{8\pi^2}\,\biggl\lvert\int_{\mathbb{S}^2}\beta\biggr\rvert\,\int_{\mathbb{S}^2}\lvert{\beta}\rvert+o(T^2) as Tβ†’+∞T\to+\infty. The result relies on Erd\H{o}s and Solovej's characterisation of the spectrum of DtB\mathcal{D}_{tB} in terms of a family of Dirac operators on S2\mathbb{S}^2, together with information about the strong field localisation of the Aharonov-Casher zero modes of the latter.Comment: 24 pages, typos corrected, some minor rewordin
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