dorsal/arxiv
View SchemaSpectroscopic studies in open quantum systems
| Authors | I. Rotter, E. Persson, K. Pichugin, P. Seba |
|---|---|
| Categories | |
| ArXiv ID | quant-ph/0002038 |
| URL | https://arxiv.org/abs/quant-ph/0002038 |
| DOI | 10.1103/PhysRevE.62.450 |
| Journal | Phys.Rev.E62:450-461,2000 |
Abstract
The spectroscopic properties of an open quantum system are determined by the eigenvalues and eigenfunctions of an effective Hamiltonian H consisting of the Hamiltonian H_0 of the corresponding closed system and a non-Hermitian correction term W arising from the interaction via the continuum of decay channels. The eigenvalues E_R of H are complex. They are the poles of the S-matrix and provide both the energies and widths of the states. We illustrate the interplay between Re(H) and Im(H) by means of the different interference phenomena between two neighboured resonance states. Level repulsion along the real axis appears if the interaction is caused mainly by Re(H) while a bifurcation of the widths appears if the interaction occurs mainly due to Im(H). We then calculate the poles of the S-matrix and the corresponding wavefunctions for a rectangular microwave resonator with a scatter as a function of the area of the resonator as well as of the degree of opening to a guide. The calculations are performed by using the method of exterior complex scaling. Re(W) and Im(W) cause changes in the structure of the wavefunctions which are permanent, as a rule. At full opening to the lead, short-lived collective states are formed together with long-lived trapped states. The wavefunctions of the short-lived states at full opening to the lead are very different from those at small opening. The resonance picture obtained from the microwave resonator shows all the characteristic features known from the study of many-body systems in spite of the absence of two-body forces. The poles of the S-matrix determine the conductance of the resonator. Effects arising from the interplay between resonance trapping and level repulsion along the real axis are not involved in the statistical theory.
{
"annotation_id": "2aed8bc6-f11d-4205-9ab6-e373e2f88404",
"date_created": "2026-03-02T18:01:38.854000Z",
"date_modified": "2026-03-02T18:01:38.854000Z",
"file_hash": "25eebf1c3e0a3b0345f09ac2baa448b5ac704d31ab88362d364f0b838fccad9a",
"private": false,
"record": {
"abstract": "The spectroscopic properties of an open quantum system are determined by the\neigenvalues and eigenfunctions of an effective Hamiltonian H consisting of the\nHamiltonian H_0 of the corresponding closed system and a non-Hermitian\ncorrection term W arising from the interaction via the continuum of decay\nchannels. The eigenvalues E_R of H are complex. They are the poles of the\nS-matrix and provide both the energies and widths of the states. We illustrate\nthe interplay between Re(H) and Im(H) by means of the different interference\nphenomena between two neighboured resonance states. Level repulsion along the\nreal axis appears if the interaction is caused mainly by Re(H) while a\nbifurcation of the widths appears if the interaction occurs mainly due to\nIm(H). We then calculate the poles of the S-matrix and the corresponding\nwavefunctions for a rectangular microwave resonator with a scatter as a\nfunction of the area of the resonator as well as of the degree of opening to a\nguide. The calculations are performed by using the method of exterior complex\nscaling. Re(W) and Im(W) cause changes in the structure of the wavefunctions\nwhich are permanent, as a rule. At full opening to the lead, short-lived\ncollective states are formed together with long-lived trapped states. The\nwavefunctions of the short-lived states at full opening to the lead are very\ndifferent from those at small opening. The resonance picture obtained from the\nmicrowave resonator shows all the characteristic features known from the study\nof many-body systems in spite of the absence of two-body forces. The poles of\nthe S-matrix determine the conductance of the resonator. Effects arising from\nthe interplay between resonance trapping and level repulsion along the real\naxis are not involved in the statistical theory.",
"arxiv_id": "quant-ph/0002038",
"authors": [
"I. Rotter",
"E. Persson",
"K. Pichugin",
"P. Seba"
],
"categories": [
"quant-ph"
],
"doi": "10.1103/PhysRevE.62.450",
"journal_ref": "Phys.Rev.E62:450-461,2000",
"title": "Spectroscopic studies in open quantum systems",
"url": "https://arxiv.org/abs/quant-ph/0002038"
},
"schema_id": "dorsal/arxiv",
"source": {
"execution_id": "c42cc8ba-4678-4256-954d-dcf9e8614168",
"id": "arXiv Dataset IDs",
"type": "Model",
"variant": "snapshot-2026-03-01",
"version": "0.1.0"
},
"user_id": 1000002
}