The Euclidean resonance and quantum tunneling
| dc.creator | Ivlev, B. I. | |
| dc.date | 2002-02-25 | |
| dc.date.accessioned | 2026-07-07T12:37:46Z | |
| dc.date.available | 2026-07-07T12:37:46Z | |
| dc.description | The extremely small probability of tunneling through an almost classical potential barrier may become not small under the action of the specially adapted non-stationary signal which selects the certain particle energy E_R. For particle energies close to this value, the tunneling rate is not small during a finite interval of time and has a very sharp peak at the energy E_R. After entering inside the barrier, the particle emits electromagnetic quanta and exits the barrier with a lower energy. The signal amplitude can be much less compared to the field of the static barrier. This phenomenon can be called the Euclidean resonance since the under-barrier motion occurs in imaginary time. The resonance may stimulate chemical and biochemical reactions in a selective way by adapting the signal to a certain particular chemical bond. The resonance may be used in search of the soft alpha-decay for which a conventional observation is impossible due to an extremely small decay rate. | |
| dc.description | 21 pages and 10 figures | |
| dc.identifier | https://arxiv.org/abs/quant-ph/0202145 | |
| dc.identifier | http://arxiv.org/abs/quant-ph/0202145 | |
| dc.identifier | Phys.Rev.A66:012102,2002 | |
| dc.identifier | doi:10.1103/PhysRevA.66.012102 | |
| dc.identifier.uri | http://salesiana.dossiersoluciones.com/handle/123456789/218556 | |
| dc.subject | Quantum Physics | |
| dc.title | The Euclidean resonance and quantum tunneling | |
| dc.type | text |