The case of quantum-mechanical system (including electronic molecules) is considered where Hamiltonian allows a separation, in particular by the Faddeev method, of a weakly coupled channel. Width (i.~e.~ the imaginary part) of the resonance generated by a discrete spectrum eigenvalue of the separated channel is studied in the case where main part of the Hamiltonian gives itself another resonance. It is shown that if real parts of these resonances coincide and, at the same time, a coupling between the separated and main channels is sufficiently small then the width of the resonance generated by the separated (molecular) channel is inversely proportional to the width of the main (nuclear) channel resonance. This phenomenon being a kind of uni...
For two discrete-level quantum systems in interaction, we follow the displacement in the complex pla...
A fundamental aspect of scattering is the appearance of resonances, which appear in many systems. Al...
In dimension d = 1, 2, 3 we define a family of two-channel Hamiltonians obtained as point perturbati...
The case of quantum-mechanical system (including electronic molecules) is considered where Hamiltoni...
Results are obtained on perturbation of eigenvalues and half-bound states (zero-resonances) embedded...
The Hamilton operator of an open quantum system is non-Hermitian. Its eigenvalues are generally comp...
The trapping effect is investigated close to the elastic threshold. The nucleus is described as an O...
It has been recognized for some time that, when the discrete vibration rotation absorption bands con...
We address the question of whether there might exist a resonance in the nnΛ system, using a rank one...
Several studies of the vibrational resonances of diatomic molecular anions have shown evidence of ve...
We address the question of whether there might exist a resonance in the nnΛ system, using a rank one...
In memory of Pierre Duclos We examine perturbations of eigenvalues and resonances for a class of mul...
We study the width of a two-body resonance in a coupled-channel system. We demonstrate how the width...
We provide here a quantum mechanical investigation of the resonance states found in a study of conic...
We present some results on the perturbation of eigenvalues embedded at thresholds in a two channel m...
For two discrete-level quantum systems in interaction, we follow the displacement in the complex pla...
A fundamental aspect of scattering is the appearance of resonances, which appear in many systems. Al...
In dimension d = 1, 2, 3 we define a family of two-channel Hamiltonians obtained as point perturbati...
The case of quantum-mechanical system (including electronic molecules) is considered where Hamiltoni...
Results are obtained on perturbation of eigenvalues and half-bound states (zero-resonances) embedded...
The Hamilton operator of an open quantum system is non-Hermitian. Its eigenvalues are generally comp...
The trapping effect is investigated close to the elastic threshold. The nucleus is described as an O...
It has been recognized for some time that, when the discrete vibration rotation absorption bands con...
We address the question of whether there might exist a resonance in the nnΛ system, using a rank one...
Several studies of the vibrational resonances of diatomic molecular anions have shown evidence of ve...
We address the question of whether there might exist a resonance in the nnΛ system, using a rank one...
In memory of Pierre Duclos We examine perturbations of eigenvalues and resonances for a class of mul...
We study the width of a two-body resonance in a coupled-channel system. We demonstrate how the width...
We provide here a quantum mechanical investigation of the resonance states found in a study of conic...
We present some results on the perturbation of eigenvalues embedded at thresholds in a two channel m...
For two discrete-level quantum systems in interaction, we follow the displacement in the complex pla...
A fundamental aspect of scattering is the appearance of resonances, which appear in many systems. Al...
In dimension d = 1, 2, 3 we define a family of two-channel Hamiltonians obtained as point perturbati...