2021
DOI: 10.1088/0256-307x/38/9/094201
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Soliton Rectangular Pulses and Bound States in a Dissipative System Modeled by the Variable-Coefficients Complex Cubic-Quintic Ginzburg–Landau Equation

Abstract: The complex cubic-quintic Ginzburg-Landau equation (CQGLE) is a universal model for describing a dissipative system, especially fiber laser. The analytic one-soliton solution of the variable-coefficients CQGLE is calculated by a modified Hirota method. Then, phenomena of soliton pulses splitting and stable bound states of two solitons are investigated. Moreover, rectangular dissipative soliton pulses of the variable-coefficients CQGLE are realized and controlled effectively in the theoretical research for the … Show more

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Cited by 116 publications
(30 citation statements)
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“…孤子这一概念在如非线性光学、原子物 理、凝聚态物理等诸多领域得到关注和应 用 [1][2][3][4] 。由于通常在介质中传播的光波或 脉冲其电磁包络非单色性,各部分会因为 传播速度不同而导致包络展宽。如在空间维 度,光波因为衍射效应使光束半径增大,在 时间维度则由于群速度色散致使脉冲展宽。 因而,在特殊条件下利用传播介质的非线性 效应或直接使用光纤放大器实现衰减补偿, 使非线性效应与衍射效应和色散效应达到平 衡,可以弥补线性传输过程中光波或脉冲的 发散 [5][6][7][8] 。这样的孤子具有稳定的、局域的、 类粒子的特性,被叫做光孤子。 根据光孤子所在的色散区域不同,光孤 子可分为明孤子和暗孤子。光孤子具有一系 列重要的应用价值 [9][10][11][12][13][14][15][16][17][18][19] ,例如将光孤子当作 比特信息应用于超快光学数字逻辑系统;还 可以研究超快光与物质之间的非线性相互作 用;应用于远程通信系统时,其中孤子的传 播可以用三次-五次复金兹堡-朗道(CGL)方 程来建模 [20][21][22] 。 三次-五次 CGL 方程是对被动锁模激光 器中区域动力学的一个持续估计 [23] CGL 方程 [24] :…”
Section: 介绍unclassified
“…孤子这一概念在如非线性光学、原子物 理、凝聚态物理等诸多领域得到关注和应 用 [1][2][3][4] 。由于通常在介质中传播的光波或 脉冲其电磁包络非单色性,各部分会因为 传播速度不同而导致包络展宽。如在空间维 度,光波因为衍射效应使光束半径增大,在 时间维度则由于群速度色散致使脉冲展宽。 因而,在特殊条件下利用传播介质的非线性 效应或直接使用光纤放大器实现衰减补偿, 使非线性效应与衍射效应和色散效应达到平 衡,可以弥补线性传输过程中光波或脉冲的 发散 [5][6][7][8] 。这样的孤子具有稳定的、局域的、 类粒子的特性,被叫做光孤子。 根据光孤子所在的色散区域不同,光孤 子可分为明孤子和暗孤子。光孤子具有一系 列重要的应用价值 [9][10][11][12][13][14][15][16][17][18][19] ,例如将光孤子当作 比特信息应用于超快光学数字逻辑系统;还 可以研究超快光与物质之间的非线性相互作 用;应用于远程通信系统时,其中孤子的传 播可以用三次-五次复金兹堡-朗道(CGL)方 程来建模 [20][21][22] 。 三次-五次 CGL 方程是对被动锁模激光 器中区域动力学的一个持续估计 [23] CGL 方程 [24] :…”
Section: 介绍unclassified
“…Jacobi elliptic function scheme [7,8], extended simplest equation technique [9][10][11], Fexpansion method [12,13], trial equation scheme [14,15], various rational (𝐺 ′ /𝐺)-expansion tools [16][17][18], exp-function approach [19,20], improved tanh approach [21], Darboux transformation approach [22], different Hirota schemes [23][24][25][26][27], Kudryashov technique [28] etc. This present study is conducted by implementing two competent techniques such as improved tanh and improved auxiliary equation.…”
Section: Introductionmentioning
confidence: 99%
“…The propagation characteristics of the optical soliton in an ideal optical fiber are generally represented by the nonlinear schrödinger equation (NLSE) [19][20][21][22][23][24]. But the optical fiber in an actual optical communication system is accompanied by gain or loss, and at this time, the system needs to be modeled by the complex Ginzburg-Landau equation (CGLE) [25][26][27][28][29]. At the same time, in the modern optical communication system, to optimize information transmission efficiency and reduce cost, the Wavelength Division Multiplexing (WDM) technology has been proposed [30][31][32].…”
Section: Introductionmentioning
confidence: 99%