Effects of atomic coherence on a rydberg atom undergoing a two-photon transition in a lossless cavity

1990 ◽  
Vol 75 (2) ◽  
pp. 189-196 ◽  
Author(s):  
Amitabh Joshi ◽  
R.R. Puri
2001 ◽  
Vol 15 (20) ◽  
pp. 857-865 ◽  
Author(s):  
AMITABH JOSHI

Propagation of pulses through a medium comprising of coherently prepared two-level atoms undergoing two-photon transition has been studied using Maxwell–Bloch equations. The solution of the electromagnetic field envelopes has been obtained under various conditions and the effect of initial atomic coherence is clearly brought out in these solutions.


2021 ◽  
Vol 19 (2) ◽  
pp. 025201
Author(s):  
Ning Liu ◽  
Sandan Wang ◽  
Jinpeng Yuan ◽  
Lirong Wang ◽  
Liantuan Xiao ◽  
...  

Abstract We experimentally investigate the 6S 1/2–8S 1/2 two-photon transition in cesium vapor by a single laser. A blue (455.5 and 459.3 nm) fluorescence signal is observed as a result of 822.5 nm laser beams illuminating the Cs vapor with a counter-propagating configuration. The dependences of the fluorescence intensity on the polarization combinations of the laser beams, laser power and vapor temperature are studied to obtain optimal experimental parameters. The frequency difference between the two hyperfine components of 4158 (7) MHz is measured with a Fabry–Perot interferometer as a frequency reference. Such a large spectral isolation and the insensitivity to the Earth’s magnetic field enable the 6S 1/2–8S 1/2 transition to be a stable frequency standard candidate for a frequency-doubled 1644 nm laser in the U-band window for quantum telecommunication.


1996 ◽  
Vol 21 (9) ◽  
pp. 659 ◽  
Author(s):  
P. T. Guerreiro ◽  
S. I. Najafi ◽  
J. Mackenzie ◽  
N. Peyghambarian ◽  
S. G. Lee ◽  
...  

2012 ◽  
Vol 10 (05) ◽  
pp. 1250053
Author(s):  
JAVAID ANWAR

A theory of two-photon phase-sensitive amplifier based on two-photon cascade is presented. The atomic coherence is produced by means of two dipole-allowed transitions driven by coherent fields; a practical alternative versus scheme employing coupling between dipole-forbidden levels. The regime of parameters under which a laser signal can be phase locked and amplified is discussed through the corresponding Fokker–Planck equation.


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