TY - JOUR
T1 - Two (2+1)-dimensional integrable nonlocal nonlinear Schrödinger equations
T2 - Breather, rational and semi-rational solutions
AU - Cao, Yulei
AU - Malomed, Boris A.
AU - He, Jingsong
N1 - Publisher Copyright:
© 2018 Elsevier Ltd
PY - 2018/9
Y1 - 2018/9
N2 - Recently, an integrable system of coupled (2+1)-dimensional nonlinear Schrödinger (NLS) equations was introduced by Fokas (Eq. (18) in Nonlinearity 29, 319324 (2016)). Following this pattern, two integrable equations [Eqs. (2) and (3)] with specific parity-time symmetry are introduced here, under different reduction conditions. For Eq. (2), two kinds of periodic solutions are obtained analytically by means of the Hirota's bilinear method. In the long-wave limit, the two periodic solutions go over into rogue waves (RWs) and semi-rational solutions, respectively. The RWs have a line shape, while the semi-rational states represent RWs built on top of the background of periodic line waves. Similarly, semi-rational solutions consisting of a line RW and line breather are derived. For Eq. (3), three kinds of analytical solutions,viz., breathers, lumps and semi-rational solutions, representing lumps, periodic line waves and breathers are obtained, using the Hirota method. Their dynamics are analyzed and demonstrated by means of three-dimensional plots. It is also worthy to note that Eq. (2) can reduce to a (1+1)-dimensional “reverse-space” nonlocal NLS equation by means of a certain transformation, Lastly, main differences between solutions of Eqs. (2) and (3) are summarized.
AB - Recently, an integrable system of coupled (2+1)-dimensional nonlinear Schrödinger (NLS) equations was introduced by Fokas (Eq. (18) in Nonlinearity 29, 319324 (2016)). Following this pattern, two integrable equations [Eqs. (2) and (3)] with specific parity-time symmetry are introduced here, under different reduction conditions. For Eq. (2), two kinds of periodic solutions are obtained analytically by means of the Hirota's bilinear method. In the long-wave limit, the two periodic solutions go over into rogue waves (RWs) and semi-rational solutions, respectively. The RWs have a line shape, while the semi-rational states represent RWs built on top of the background of periodic line waves. Similarly, semi-rational solutions consisting of a line RW and line breather are derived. For Eq. (3), three kinds of analytical solutions,viz., breathers, lumps and semi-rational solutions, representing lumps, periodic line waves and breathers are obtained, using the Hirota method. Their dynamics are analyzed and demonstrated by means of three-dimensional plots. It is also worthy to note that Eq. (2) can reduce to a (1+1)-dimensional “reverse-space” nonlocal NLS equation by means of a certain transformation, Lastly, main differences between solutions of Eqs. (2) and (3) are summarized.
KW - Bilinear method
KW - Breather solution
KW - PT-symmetry
KW - Rational solution
KW - Semi-rational solution
UR - http://www.scopus.com/inward/record.url?scp=85049728829&partnerID=8YFLogxK
U2 - 10.1016/j.chaos.2018.06.029
DO - 10.1016/j.chaos.2018.06.029
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AN - SCOPUS:85049728829
SN - 0960-0779
VL - 114
SP - 99
EP - 107
JO - Chaos, Solitons and Fractals
JF - Chaos, Solitons and Fractals
ER -