Authors | I.V. Boyko1 , O.A. Bagrii-Zayats2, H.B. Tsupryk1, Y.M. Stoianov1 |
Affiliations |
1Ternopil National Technical University, 56, Ruska Str., 46001 Ternopil, Ukraine 2Ternopil State Medical University, 1, Voli Str., 46000 Ternopil, Ukraine |
Е-mail | boyko.i.v.theory@gmail.com |
Issue | Volume 10, Year 2018, Number 6 |
Dates | Received 15 July 2018; revised manuscript received 07 December 2018; published online 18 December 2018 |
Citation | I.V. Boyko, O.A. Bagrii-Zayats, H.B. Tsupryk, Y.M. Stoianov, J. Nano- Electron. Phys. 10 No 6, 06001 (2018) |
DOI | https://doi.org/10.21272/jnep.10(6).06001 |
PACS Number(s) | 73.21.Fg, 73.21.Cd, 74.55. + v |
Keywords | Quantum cascade laser (3) , Quantum cascade detector, Electron-electron interaction, Cubic Schrödinger equation. |
Annotation |
In the model of rectangular potential wells and barriers and the model of effective masses for an electron, using the exact solutions of the nonlinear cubic Schrödinger equation, a quantum-mechanical theory of the stationary electronic spectrum and oscillator forces of quantum transitions taking into account electron-electron interaction in the Hartree-Fock approximation was developed.The inclusion electron-electron interaction reduces the intensity of quantum transitions between the first electron states and reduces the value of detected energy, it is shown by an example of a two-well plane semiconductor nanostructure, that can function as an active zone of a quantum cascade detector. |
List of References |