Colective elementary excitations of bose-einstein condensed two-dimensional magnetoexcitons strongly interacting with electrom-hole plasma
The collective elementary excitations of a system of Bose-Einstein condensed two- dimensional magnetoexcitons interacting with electron-hole(e-h) plasma in a strong perpendicular magnetic field are studied. The breaking of the gauge symmetry is introduced into the Hamiltonian following the Bogo...
Guardado en:
| Autores principales: | , , , , |
|---|---|
| Formato: | article |
| Lenguaje: | EN |
| Publicado: |
D.Ghitu Institute of Electronic Engineering and Nanotechnologies
2005
|
| Materias: | |
| Acceso en línea: | https://doaj.org/article/f75da7dc0ad741b58d228b54992e1b95 |
| Etiquetas: |
Agregar Etiqueta
Sin Etiquetas, Sea el primero en etiquetar este registro!
|
| Sumario: | The collective elementary excitations of a system of Bose-Einstein condensed two-
dimensional magnetoexcitons interacting with electron-hole(e-h) plasma in a strong
perpendicular magnetic field are studied. The breaking of the gauge symmetry is introduced
into the Hamiltonian following the Bogoliubov`s theory of quasiaverages.
The motion equations for the summary operators describing the creation and annihilation of magnetoexcitons as well as the density fluctuations of the electronhole(e-h) plasma were derived. They suggest the existence of magneto-exciton-plasmon complexes, the
energies of which differ by the energies of one or two plasmon quanta.
Starting with these motion equations one can study the Bose-Einstein Condensation
(BEC) of different magneto-exciton-plasmon complexes introducing different constants of the
broken symmetry correlated with their energies. The Green`s functions constructed from these
summary operators are two-particle Green`s functions. They obey the chains of equations expressing the two-particle Green`s functions through the four-particle and six-particle
Green`s functions. These chains were truncated in such a way that the six-particle Green`s
functions, were expressed through the two-particle ones. At the same time the elementary excitations with different wave vectors were decoupled. As a result of these simplifications
the Dyson-type equation in a matrix form for the two-particle Green`s functions was obtained.
The determinant constructed from the self-energy part 44 × ( , ) ij P ω ∑
G
gives rise to
dispersion equation. The dispersion relations were obtained in analytical form, when in the
self-energy parts ( , ) ij P ω ∑
G only the terms linear in Coulomb interaction were kept. Taking
into account also the terms quadratic in Coulomb interaction the dispersion equation becomes
cumbersome and it can be solved only numerically. |
|---|