Quantum Systems at the Brink: Existence of Bound States, Critical Potentials and Dimensionality (original) (raw)

Finite Size Scaling for Criticality of the Schrödinger Equation

2010

By solving the Schrödinger equation one obtains the whole energy spectrum, both the bound and the continuum states. If the Hamiltonian depends on a set of parameters, these could be tuned to a transition from bound to continuum states. The behavior of systems near the threshold, which separates bound-states from continuum states, is important in the study of such phenomenon as: ionization of atoms and molecules, molecule dissociation, scattering collisions and stability of matter. In general, the energy is non-analytic as a function of the Hamiltonian parameters or a bound-state does not exist at the threshold energy. The overall goal of this chapter is to show how one can predict, generate and identify new class of stable quantum systems using large-dimensional models and the finite size scaling approach. Within this approach, the finite size corresponds not to the spatial dimension but to the number of elements in a complete basis set used to expand the exact eigenfunction of a gi...

Some bound state problems in quantum mechanics

Spectral Theory and Mathematical Physics: A Festschrift in Honor of Barry Simon’s 60th Birthday, 2007

We give a review of semi-classical estimates for bound states and their eigenvalues for Schrödinger operators. Motivated by the classical results, we discuss their recent improvements for single particle Schrödinger operators as well as some applications of these semi-classical bounds to multi-particle systems, in particular, large atoms and the stability of matter.

Necessary and sufficient conditions for existence of bound states in a central potential

Journal of Physics A-mathematical and General, 2003

We obtain, using the Birman-Schwinger method, a series of necessary conditions for the existence of at least one bound state applicable to arbitrary central potentials in the context of nonrelativistic quantum mechanics. These conditions yield a monotonic series of lower limits on the "critical" value of the strength of the potential (for which a first bound state appears) which converges to the exact critical strength. We also obtain a sufficient condition for the existence of bound states in a central monotonic potential which yield an upper limit on the critical strength of the potential.

A PRIORI ESTIMATES AND POSITIVITY FOR SEMICLASSICAL GROUND STATES FOR SYSTEMS OF CRITICAL SCHR¨ODINGER EQUATIONS IN DIMENSION TWO

We consider in the whole plane the following Hamiltonian coupling of Schrödinger equations −∆u + V 0 u = g(v) −∆v + V 0 v = f (u) where V 0 > 0, f, g have critical growth in the sense of Moser. We prove that the (nonempty) set S of ground state solutions is compact in H 1 (R 2) × H 1 (R 2) up to translations. Moreover, for each (u, v) ∈ S, one has that u, v are uniformly bounded in L ∞ (R 2) and uniformly decaying at infinity. Then we prove that actually the ground state is positive and radially symmetric. We apply those results to prove the existence of semiclassical ground states solutions to the singularly perturbed system −ε 2 ∆ϕ + V (x)ϕ = g(ψ) −ε 2 ∆ψ + V (x)ψ = f (ϕ) where V ∈ C(R 2) is a Schrödinger potential bounded away from zero. Namely, as the adimensionalized Planck constant ε → 0, we prove the existence of minimal energy solutions which concentrate around the closest local minima of the potential with some precise asymptotic rate.

Rigorous conditions for the existence of bound states at the threshold in the two-particle case

Journal of Physics A: Mathematical and Theoretical, 2007

In the framework of non-relativistic quantum mechanics and with the help of the Greens functions formalism we study the behavior of weakly bound states as they approach the continuum threshold. Through estimating the Green's function for positive potentials we derive rigorously the upper bound on the wave function, which helps to control its falloff. In particular, we prove that for potentials whose repulsive part decays slower than 1/r 2 the bound states approaching the threshold do not spread and eventually become bound states at the threshold. This means that such systems never reach supersizes, which would extend far beyond the effective range of attraction. The method presented here is applicable in the many-body case.

Quantum Systems at The Brink. Existence and Decay Rates of Bound States at Thresholds; Atoms

2019

It is well known that N -electron atoms undergoes unbinding for a critical charge of the nucleus Zc, i.e. the atom has eigenstates for the case Z > Zc and it has no bound states for Z < Zc. In the present paper we derive upper bound for the bound state for the case Z = Zc under the assumption Zc < N − K where K is the number of electrons to be removed for atom to be stable for Z = Zc without any change in the ground state energy. We show that the eigenvector decays faster as exp (

Quantum Systems at The Brink. Existence and Decay Rates of Bound States at Thresholds; Helium

arXiv (Cornell University), 2019

It is well known that N-electron atoms undergoes unbinding for a critical charge of the nucleus Z c , i.e. the atom has eigenstates for the case Z > Z c and it has no bound states for Z < Z c. In the present paper we derive upper bound for the bound state for the case Z = Z c under the assumption Z c < N − K where K is the number of electrons to be removed for atom to be stable for Z = Z c without any change in the ground state energy. We show that the eigenvector decays faster as exp −C |x| k where we sum K largest values of |x j |, j ∈ {1,. .. , N }. Our method do not require Born-Oppenheimer approximation.

Spectral singularities and zero energy bound states

The European Physical Journal D, 2011

Single particle scattering around zero energy is re-analysed in view of recent experiments with ultra-cold atoms, nano-structures and nuclei far from the stability valley. For non-zero orbital angular momentum the low energy scattering cross section exhibits dramatic changes depending on the occurrence of either a near resonance or a bound state or the situation in between, that is a bound state at zero energy. Such state is singular in that it has an infinite scattering length, behaves for the eigenvalues but not for the eigenfunctions as an exceptional point and has no pole in the scattering function. These results should be observable whenever the interaction or scattering length can be controlled.