The normalization of scattering states, far from being a rote step on the way to calculating expectation values (as is done in the bound state sector), contains important information regarding the density of the scattering spectrum (along with useful bound state information). For many applications, this information is more useful than the actual wavefunctions themselves. Even the simplest systems in 1D have nontrivial normalizations. In this paper we show that this normalization/density correspondence is a consequence of the completeness relation, and present formulas for calculating this spectrum for 1D, finite-range symmetric potentials. We then apply the formulas to the delta potential and the square well, and plot the corresponding spec...
We consider the 1d Schroedinger operator with random potential decaying of order \(\alpha\). The res...
The ground state energy ð¸ 0(ðœ†) of ð» 𜆠= − ð‘‘ 2 /ð‘‘ð‘¥ 2 − 𜆠𑒠−ð‘¥2 is computed fo...
For a quantum system, a density matrix ρ that is not pure can arise, via averaging, from a distribut...
The relation between phase shifts and bound states proved by Levinson for spherical symmetric potent...
Methods from scattering theory are introduced to analyze random Schroedinger operators in one dimens...
It is emphasized that one-dimensional, weak potentials have some special properties. They sustain a ...
(A. Wirzba, P. Cvitanovic ́ and N. Whelan) S the trace formulas have been derived assuming that t...
Methods from scattering theory are introduced to analyze random Schrödinger operators in one dimens...
We construct a family of hermitian potentials in 1D quantum mechanics that converges in the zero-ran...
We expand the quantum mechanical wavefunction in a complete set of orthonormal basis such that the m...
The problem of obtaining characteristics of bound nuclear states from continuum states data is discu...
Using formal scattering theory, the scattering wave functions are extrapolated to negative energies ...
In this contribution, we present a simple approach to the scattering problem usi...
We introduce a simplified effective-range function for charged nuclei, related to the modified K mat...
The method of the analytic continuation of the effective range function is applied to obtain the asy...
We consider the 1d Schroedinger operator with random potential decaying of order \(\alpha\). The res...
The ground state energy ð¸ 0(ðœ†) of ð» 𜆠= − ð‘‘ 2 /ð‘‘ð‘¥ 2 − 𜆠𑒠−ð‘¥2 is computed fo...
For a quantum system, a density matrix ρ that is not pure can arise, via averaging, from a distribut...
The relation between phase shifts and bound states proved by Levinson for spherical symmetric potent...
Methods from scattering theory are introduced to analyze random Schroedinger operators in one dimens...
It is emphasized that one-dimensional, weak potentials have some special properties. They sustain a ...
(A. Wirzba, P. Cvitanovic ́ and N. Whelan) S the trace formulas have been derived assuming that t...
Methods from scattering theory are introduced to analyze random Schrödinger operators in one dimens...
We construct a family of hermitian potentials in 1D quantum mechanics that converges in the zero-ran...
We expand the quantum mechanical wavefunction in a complete set of orthonormal basis such that the m...
The problem of obtaining characteristics of bound nuclear states from continuum states data is discu...
Using formal scattering theory, the scattering wave functions are extrapolated to negative energies ...
In this contribution, we present a simple approach to the scattering problem usi...
We introduce a simplified effective-range function for charged nuclei, related to the modified K mat...
The method of the analytic continuation of the effective range function is applied to obtain the asy...
We consider the 1d Schroedinger operator with random potential decaying of order \(\alpha\). The res...
The ground state energy ð¸ 0(ðœ†) of ð» 𜆠= − ð‘‘ 2 /ð‘‘ð‘¥ 2 − 𜆠𑒠−ð‘¥2 is computed fo...
For a quantum system, a density matrix ρ that is not pure can arise, via averaging, from a distribut...