TY - JOUR
T1 - Bilinear forms and dark-soliton solutions for a fifth-order variable-coefficient nonlinear Schrödinger equation in an optical fiber
AU - Zhao, Chen
AU - Gao, Yi Tian
AU - Lan, Zhong Zhou
AU - Yang, Jin Wei
AU - Su, Chuan Qi
N1 - Publisher Copyright:
© 2016 World Scientific Publishing Company.
PY - 2016/9/10
Y1 - 2016/9/10
N2 - In this paper, a fifth-order variable-coefficient nonlinear Schrödinger equation is investigated, which describes the propagation of the attosecond pulses in an optical fiber. Via the Hirota's method and auxiliary functions, bilinear forms and dark one-, two-and three-soliton solutions are obtained. Propagation and interaction of the solitons are discussed graphically: We observe that the solitonic velocities are only related to β1(x), β2(x), β3(x) and β4(x), the coefficients of the second-, third-, fourth-and fifth-order terms, respectively, with x being the scaled distance, while the solitonic amplitudes are related to β1(x), β2(x), β3(x), β4(x) as well as the wave number. When β1(x), β2(x), β3(x) and β4(x) are the constants, or the linear, quadratic and trigonometric functions of x, we obtain the linear, parabolic, cubic and periodic dark solitons, respectively. Interactions between (among) the two (three) solitons are depicted, which can be regarded to be elastic because the solitonic amplitudes remain unchanged except for some phase shifts after each interaction in an optical fiber.
AB - In this paper, a fifth-order variable-coefficient nonlinear Schrödinger equation is investigated, which describes the propagation of the attosecond pulses in an optical fiber. Via the Hirota's method and auxiliary functions, bilinear forms and dark one-, two-and three-soliton solutions are obtained. Propagation and interaction of the solitons are discussed graphically: We observe that the solitonic velocities are only related to β1(x), β2(x), β3(x) and β4(x), the coefficients of the second-, third-, fourth-and fifth-order terms, respectively, with x being the scaled distance, while the solitonic amplitudes are related to β1(x), β2(x), β3(x), β4(x) as well as the wave number. When β1(x), β2(x), β3(x) and β4(x) are the constants, or the linear, quadratic and trigonometric functions of x, we obtain the linear, parabolic, cubic and periodic dark solitons, respectively. Interactions between (among) the two (three) solitons are depicted, which can be regarded to be elastic because the solitonic amplitudes remain unchanged except for some phase shifts after each interaction in an optical fiber.
KW - Hirota's method
KW - Optical fiber
KW - bilinear forms
KW - dark-soliton solutions
KW - fifth-order variable-coefficient nonlinear Schrödinger equation
UR - https://www.scopus.com/pages/publications/85084807643
U2 - 10.1142/S0217984916503127
DO - 10.1142/S0217984916503127
M3 - 文章
AN - SCOPUS:85084807643
SN - 0217-9849
VL - 30
JO - Modern Physics Letters B
JF - Modern Physics Letters B
IS - 24
M1 - 1650312
ER -