Two-component spatial optical solitons in a four-state ladder system via electromagnetically induced transparency

2008 ◽  
Vol 372 (22) ◽  
pp. 4127-4134 ◽  
Author(s):  
Hui-jun Li ◽  
Guoxiang Huang
2015 ◽  
Vol 35 (2) ◽  
pp. 0227002 ◽  
Author(s):  
杜英杰 Du Yingjie ◽  
杨战营 Yang Zhanying ◽  
谢小涛 Xie Xiaotao ◽  
白晋涛 Bai Jintao

2020 ◽  
Vol 128 (10) ◽  
pp. 1433
Author(s):  
А. Саргсян ◽  
Ч.С. Адамс ◽  
Т.А. Вартанян ◽  
Д. Саркисян

The effect of electromagnetically-induced transparency in the ladder system of 5S1/2-5P3/2-5D5/2 levels of Rb atoms is studied. The effect of spectral narrowing of the dark resonance (DR) is shown depending on the density of atomic vapor and the thickness L of the spectroscopic cell, which contains Rb atomic vapor. The thickness L varies from 390 nm to 4 mm, the atomic density N increased to ~ 10^16 cm^-3, and intense coupling and weak probe radiation were used. The maximum effect, namely the 22-fold spectral narrowing of DR, was achieved in a cell with a thickness of L = 4 mm. With decreasing of the thickness L, the effect of spectral narrowing becomes weaker: for example, at L = 2 μm, a 2.4-fold spectral narrowing of DR occurs. The spectral narrowing of DR was practically absent at L = 0.8 μm, and with a further decrease to L = 0.4 μm with increasing of atomic vapor density, spectral broadening of DR began to occur. In almost all cases, at moderate atomic densities and high intensities of the coupling radiation, ~ 100% DR contrast was achieved. The effect of spectral narrowing and broadening of DR is explained.


2020 ◽  
Vol 10 (1) ◽  
Author(s):  
Dong Hoang Minh ◽  
Nga Luong Thi Yen ◽  
Khoa Dinh Xuan ◽  
Bang Nguyen Huy

Abstract We proposed a simple model for generation of controllable ultraslow optical solitons of a weak probe laser light in a degenerated two-level atomic medium under electromagnetically induced transparency assisted by a magnetic field. It is shown that bright and dark optical solitons can be formed from a probe light with controllable ultraslow group velocities at a few m/s by tuning the strength of a coupling light and/or the magnetic field. In addition to the ultraslow velocity, the advantage of this model is to use a sole laser for delivering both pump and probe lights. Furthermore, one can switch between bright and dark solitons by reversing the direction of the magnetic field. Such controllable ultraslow solitons are interested in finding applications in optical communications and optical data processing.


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