Six-Fold Degenerate Dark States in a Four-Level Atomic System
-
Abstract
With all driving fields on Raman resonance, a tripod-type atomic system quickly evolves into a dark state decoupled from the lossy excited level. The dark state depends strongly on field Rabi frequencies, spontaneous decay rates, and the initial atomic population in a complicated way. Analytical results reveal that it is a sixfold degenerate dark state with its three components superposed both coherently and incoherently due to population redistribution from spontaneous emission.
Article Text
-
-
-
About This Article
Cite this article:
WU Jin-Hui, CUI Cui-Li, BA Nuo, MA Qi-Rong, GUO Xiu-Zhen. Six-Fold Degenerate Dark States in a Four-Level Atomic System[J]. Chin. Phys. Lett., 2007, 24(2): 428-431.
WU Jin-Hui, CUI Cui-Li, BA Nuo, MA Qi-Rong, GUO Xiu-Zhen. Six-Fold Degenerate Dark States in a Four-Level Atomic System[J]. Chin. Phys. Lett., 2007, 24(2): 428-431.
|
WU Jin-Hui, CUI Cui-Li, BA Nuo, MA Qi-Rong, GUO Xiu-Zhen. Six-Fold Degenerate Dark States in a Four-Level Atomic System[J]. Chin. Phys. Lett., 2007, 24(2): 428-431.
WU Jin-Hui, CUI Cui-Li, BA Nuo, MA Qi-Rong, GUO Xiu-Zhen. Six-Fold Degenerate Dark States in a Four-Level Atomic System[J]. Chin. Phys. Lett., 2007, 24(2): 428-431.
|