Abstract
The collective modes of the ν=1/2 state in double-quantum-well systems are analyzed within the framework of the single-mode approximation. The dependence of these modes on the interwell spacing is discussed. The derivation of the plasma sum rules for the two-component classical plasmas corresponding to the unpolarized [mmn] states is derived in the Appendixes.
- Received 14 December 1992
DOI:https://doi.org/10.1103/PhysRevB.48.10926
©1993 American Physical Society