Resonance Fluorescence of a Two-Level Atom Near a Metal Surface.

1983 ◽  
Author(s):  
Xi-yi Huang ◽  
Jui-teng Lin ◽  
Thomas F. George
1986 ◽  
Vol 85 (1) ◽  
pp. 567-572 ◽  
Author(s):  
Xi‐Yi Huang ◽  
Ki‐Tung Lee ◽  
Thomas F. George

1984 ◽  
Vol 80 (2) ◽  
pp. 893-899 ◽  
Author(s):  
Xi‐Yi Huang ◽  
Jui‐teng Lin ◽  
Thomas F. George

1984 ◽  
pp. 685-693 ◽  
Author(s):  
Xi-Yi Huang ◽  
Thomas F. George ◽  
Jui-teng Lin

2000 ◽  
Vol 62 (2) ◽  
Author(s):  
Hyunchul Nha ◽  
Young-Tak Chough ◽  
Kyungwon An

2016 ◽  
Vol 375 ◽  
pp. 38-42 ◽  
Author(s):  
V.A. Tomilin ◽  
L.V. Il'ichov

1998 ◽  
Vol 58 (1) ◽  
pp. 767-770 ◽  
Author(s):  
M. Jakob ◽  
G. Yu. Kryuchkyan

1980 ◽  
Vol 58 (7) ◽  
pp. 957-963 ◽  
Author(s):  
Constantine Mavroyannis

A theory on interference effects at high photon densities has been developed for two types of a single three-level atom for which transitions occur: (i) from two different upper levels to a common lower one and (ii) from a common upper level to two different lower levels. The excitation spectrum for the interference effects for the two types of atoms results from the symmetric and antisymmetric interference between the two electronic transitions of the system, respectively. The spectral function for the symmetric modes consists of three Lorentzian lines peaked at the frequencies ω = Δ and ω = Δ ± Ω and having spectral widths of the order of γ0 and 3γ0/4, respectively, where Δ is the beat frequency, Ω is the Rabi frequency, and γ0/2 is equal to the natural linewidth for a photon spontaneously emitted from an isolated atom. The antisy mmetric spectrum consists of the peak of ω = Δ, which has a delta-function distribution indicating the stability of the mode in question, and two Lorentzian lines peaked at ω = Δ ± Ω with radiative widths of the order of γ0/2. The excitation spectrum of each type of atom contains also a Lorentzian line describing the very low frequency mode of the system, respectively.


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