Vector solitons for the reduced Maxwell-Bloch equations with variable coefficients in nonlinear optics. (January 2018)

• Record Type: Journal Article
• Authors: Chai, Jun; Tian, Bo; Sun, Wen-Rong; Liu, De-Yin
• Is Part Of: Superlattices and microstructures. Volume 113(2018)
• Page Start: 194
• Page End: 203
• Publication Date: 2018-01
• Subjects: Reduced Maxwell-Bloch equations with variable coefficients -- Inhomogeneous two-level dielectric medium -- Symbolic computation -- Vector soliton; Superlattices as materials -- Periodicals; Microstructure -- Periodicals; Semiconductors -- Periodicals; Superréseaux -- Périodiques; Microstructure (Physique) -- Périodiques; Semiconducteurs -- Périodiques; 621.38152
• DOI: 10.1016/j.spmi.2017.10.040
• Languages: English
• ISSNs: 0749-6036

Abstract

Abstract: Under investigation in this paper is the reduced Maxwell-Bloch equations with variable coefficients, which describe the propagation of the intense ultra-short optical pulses through an inhomogeneous two-level dielectric medium. Hirota method and symbolic computation are applied to solve such equations. By introducing the dependent variable transformations, we give the bilinear forms, vector one-, two- and N -soliton solutions in analytic forms. The types of the vector solitons are analyzed: Only the bright-single-hump solitons can be observed in q and r 1, the soliton in r 2 is the bright-double-hump soliton, and there exist three types of solitons in r 3, including the dark-single-hump soliton, dark-double-hump soliton and dark-like-bright soliton, with q as the inhomogeneous electric field, r 1 and r 2 as the real and imaginary parts of the polarization of the two-level medium, and r 3 as the population difference between the ground and excited states. Figures are presented to show the vector soliton solutions. Different types of the interactions between the vector two solitons are presented. In each component, only the overtaking elastic interaction can be observed. Highlights: The reduced Maxwell-Bloch equations are studied. Only the bright-single-hump solitons can be observed in the components q and r 1 . The soliton in r 2 is the bright-double-hump soliton. There exist three types of solitons in r 3, including the dark-single-hump soliton, dark-double-hump soliton and dark-like-bright soliton. Different types of the interactions between the vector two solitons are discussed. In each component, only the overtaking elastic interaction can be observed.