The Aharonov–Bohm Hamiltonian is the energy operator which governs quantum particles moving in a solenoidal field in two dimensions. We analyze asymptotic properties of its Green function with spectral parameters in the unphysical sheet. As an application, we discuss the lower bound on resonance widths for scattering by two magnetic fields with compact supports at large separation. The bound is evaluated in terms of backward scattering amplitudes by a single magnetic field. A special emphasis is placed on analyzing how a trajectory oscillating between two magnetic fields gives rise to resonances near the real axis, as the distance between two supports goes to infinity. We also refer to the relation to the semiclassical resonance theory for ...
The diamagnetic inequality is established for the Schrödinger operator H (d) 0 in L 2 (Rd), d=2,3, d...
This paper is devoted to the symmetry and symmetry breaking properties of a two-dimensional magnetic...
Abstract. We consider the 3D Schrödinger operator H = H0 + V where H0 = (−i ∇ − A) 2 − b, A is a ma...
The Aharonov–Bohm Hamiltonian is the energy operator which governs quantum particles moving in a sol...
That vector potentials have a direct significance to quantum particles moving in magnetic fields is ...
AbstractWe consider the problem of quantum resonances in magnetic scattering by two solenoidal field...
We study the asymptotic properties in forward directions of resolvent kernels with spectral paramete...
We study the Aharonov–Bohm effect (AB effect) in quantum resonances for magnetic scattering in two d...
For a fixed magnetic quantum number m results on spectral properties and scattering theory are given...
For fixed magnetic quantum number $m$ results on spectral properties and scattering theory are given...
Abstract. Consider the scattering amplitude s(ω, ω′;λ), ω, ω ′ ∈ Sd−1, λ> 0, corresponding to an...
We study the Aharonov–Bohm effect (AB effect) in quantum resonances for magnetic scattering in two d...
A quantum particle interacting with a thin solenoid and a magnetic flux is described by a five-param...
We briefly review the scattering theory for the Schrödinger operator related to the Aharonov-Bohm ef...
The Levinson theorem is generalized for Aharonov-Bohm systems in two-dimensions. By this theorem, th...
The diamagnetic inequality is established for the Schrödinger operator H (d) 0 in L 2 (Rd), d=2,3, d...
This paper is devoted to the symmetry and symmetry breaking properties of a two-dimensional magnetic...
Abstract. We consider the 3D Schrödinger operator H = H0 + V where H0 = (−i ∇ − A) 2 − b, A is a ma...
The Aharonov–Bohm Hamiltonian is the energy operator which governs quantum particles moving in a sol...
That vector potentials have a direct significance to quantum particles moving in magnetic fields is ...
AbstractWe consider the problem of quantum resonances in magnetic scattering by two solenoidal field...
We study the asymptotic properties in forward directions of resolvent kernels with spectral paramete...
We study the Aharonov–Bohm effect (AB effect) in quantum resonances for magnetic scattering in two d...
For a fixed magnetic quantum number m results on spectral properties and scattering theory are given...
For fixed magnetic quantum number $m$ results on spectral properties and scattering theory are given...
Abstract. Consider the scattering amplitude s(ω, ω′;λ), ω, ω ′ ∈ Sd−1, λ> 0, corresponding to an...
We study the Aharonov–Bohm effect (AB effect) in quantum resonances for magnetic scattering in two d...
A quantum particle interacting with a thin solenoid and a magnetic flux is described by a five-param...
We briefly review the scattering theory for the Schrödinger operator related to the Aharonov-Bohm ef...
The Levinson theorem is generalized for Aharonov-Bohm systems in two-dimensions. By this theorem, th...
The diamagnetic inequality is established for the Schrödinger operator H (d) 0 in L 2 (Rd), d=2,3, d...
This paper is devoted to the symmetry and symmetry breaking properties of a two-dimensional magnetic...
Abstract. We consider the 3D Schrödinger operator H = H0 + V where H0 = (−i ∇ − A) 2 − b, A is a ma...