2007/08/31 by Pulak Ranjan Giri
Materials Science · Mathematics · Physics and Astronomy · #Bound state #Canonical quantization #Coupling constant #Creation and annihilation operators #Geometry #Hamiltonian (control theory) #Magnetism in coordination complexes #Mathematical analysis #Mathematical physics #Mathematics #Physics #Quantization (signal processing) #Quantum #Quantum Mechanics and Non-Hermitian Physics #Quantum chaos and dynamical systems #Quantum gravity #Quantum mechanics #Scaling #Second quantization #Upper and lower bounds #cond-mat.mtrl-sci #hep-th
paper · pdf · doi:10.1007/s10773-008-9692-3
published as Int.J.Theor.Phys.47:2583-2590,2008 · 5 pages, 6 figures, revtex4
arxiv created 2007/11/07 · openalex publication_date 2008/03/03 · arxiv updated 2009/12/01 · openalex created_date 2025/10/10 · openalex updated_date 2026/08/05
We argue that it is possible to bind neutral atom (NA) to the ferromagnetic wire (FW) by inequivalent quantization of the Hamiltonian. We follow the well known von Neumann's method of self-adjoint extensions (SAE) to get this inequivalent quantization, which is characterized by a parameter Σ∈ℝ(mod2π). There exists a single bound state for the coupling constant η2∈[0,1). Although this bound state should not occur due to the existence of classical scale symmetry in the problem. But since quantization procedure breaks this classical symmetry, bound state comes out as a scale in the problem leading to scaling anomaly. We also discuss the strong coupling region η2< 0, which supports bound state making the problem re-normalizable.