Abstract
We obtain the nondegenerate one- and two-soliton solutions of the nonlocal nonlinear Schrödinger equation by using the nonstandard Hirota method. This unconventional method is used to bilinearize the nonlocal nonlinear Schrödinger equation and its related auxiliary equations, and some novel interaction properties of parity-time-symmetric two-soliton solutions are derived. The detailed asymptotic analysis is used to reveal the characteristics of energy conservation and energy redistribution before and after the collision between nondegenerate solitons. Experimental scheme to observe nondegenerate solitons is also proposed. This provides potential applications for the soliton interaction in the nonlocal wave model.
Similar content being viewed by others
Data availability
The datasets generated during and/or analyzed during the current study are available from the corresponding author on reasonable request.
References
Ren, P., Rao, J.G.: Bright-dark solitons in the space-shifted nonlocal coupled nonlinear Schrodinger equation. Nonlinear Dyn. 108, 2461–2470 (2022)
Chen, X., Mihalache, D., Rao, J.G.: Dynamics of degenerate and nondegenerate solitons in the two-component nonlinear Schrodinger equations coupled to Boussinesq equation. Nonlinear Dyn. 111, 697–711 (2023)
Yang, J., Song, H.F., Fang, M.S., Ma, L.Y.: Solitons and rogue wave solutions of focusing and defocusing space shifted nonlocal nonlinear Schrodinger equation. Nonlinear Dyn. 107, 3767–3777 (2022)
Wazwaz, A., Abu Hammad, M.M., El-Tantawy, S.A.: Bright and dark optical solitons for (3 + 1)-dimensional hyperbolic nonlinear Schrödinger equation using a variety of distinct schemes. Optik 270, 170043 (2022)
Zhang, S., Lan, P., Su, J.J.: Wave-packet behaviors of the defocusing nonlinear Schrodinger equation based on the modified physics-informed neural networks. Chaos 31, 113107 (2021)
Sugati, T.G., Seadawy, A.R., Alharbey, R.A., Albarakati, W.: Nonlinear physical complex hirota dynamical system: construction of chirp free optical dromions and numerical wave solutions. Chaos Solitons Fractals. 156, 111788 (2022)
Wang, H.T., Li, X., Zhou, Q., Liu, W.J.: Dynamics and spectral analysis of optical rogue waves for a coupled nonlinear Schrödinger equation applicable to pulse propagation in isotropic media. Chaos Solitons Fractals. 166, 112924 (2023)
Wazwaz, A.M., Albalawi, W., El-Tantawy, S.A.: Optical envelope soliton solutions for coupled nonlinear Schrödinger equations applicable to high birefringence fibers. Optik 255, 168673 (2022)
Ma, G.L., Zhao, J.B., Zhou, Q., Biswas, A., Liu, W.J.: Soliton interaction control through dispersion and nonlinear effects for the fifth-order nonlinear Schrödinger equation. Nonlinear Dyn. 106, 2479–2484 (2021)
Chakraborty, S., Nandy, S., Barthakur, A.: Bilinearization of the generalized coupled nonlinear Schrödinger equation with variable coefficients and gain and dark-bright pair soliton solutions. Phys. Rev. E. 91, 023210 (2015)
Triki, H., Porsezian, K., Senthilnathan, K., Nithyanandan, K.: Chirped self-similar solitary waves for the generalized nonlinear Schrödinger equation with distributed two-power-law nonlinearities. Phys. Rev. E. 100, 042208 (2019)
Adhikari, S.K.: Bright solitons in coupled defocusing NLS equation supported by coupling: application to Bose-Einstein condensation. Phys. Lett. A. 346, 179–185 (2005)
Chen, J.B., Pelinovsky, D.E.: Rogue waves on the background of periodic standing waves in the derivative nonlinear Schrödinger equation. Phys. Rev. E. 103, 062206 (2021)
Ablowitz, M.J., Musslimani, Z.H.: Integrable nonlocal nonlinear schrödinger equation. Phys. Rev. Lett. 110, 064105 (2013)
Li, M., Xu, T.: Dark and antidark soliton interactions in the nonlocal nonlinear Schrödinger equation with the self-induced parity-time-symmetric potential. Phys. Rev. E. 91, 033202 (2015)
Yang, J.K.: Physically significant nonlocal nonlinear Schrödinger equation and its soliton solutions. Phys. Rev. E. 98, 042202 (2018)
Rao, J.G., He, J.S., Kanna, T., Mihalache, D.: Nonlocal M-component nonlinear Schrödinger equations: bright solitons, energy-sharing collisions, and positons. Phys. Rev. E. 102, 032201 (2020)
Su, J.J., Ruan, B.: N-fold binary Darboux transformation for the nth-order Ablowitz-Kaup-Newell-Segur system under a pseudo-symmetry hypothesis. Appl Math Lett. 125, 107719 (2022)
Shi, X.J., Li, J., Wu, C.F.: Dynamics of soliton solutions of the nonlocal Kundu-nonlinear Schrödinger equation. Chaos 29, 023120 (2019)
Su, J.J., Zhang, S., Ding, C.C.: Spatiotemporal distortion effects and interaction properties for certain nonlinear waves of the generalized AB system. Nonlinear Dyn. 106, 2415–2429 (2021)
Su, J.J., Zhang, S.: Nth-order rogue waves for the AB system via the determinants. Appl. Math. Lett. 112, 106714 (2021)
Stalin, S., Ramakrishnan, R., Senthilvelan, M., Lakshmanan, M.: Nondegenerate Solitons in Manakov System. Phys. Rev. Lett. 122, 043901 (2019)
Cai, Y.J., Wu, J.W., Lin, J.: Nondegenerate N-soliton solutions for Manakov system. Chaos Solitons Fractals. 164, 112657 (2022)
Stalin, S., Ramakrishnan, R., Lakshmanan, M.: Nondegenerate bright solitons in coupled nonlinear Schrödinger systems: recent developments on optical vector solitons. Photonics. 8, 258 (2021)
Geng, K.L., Mou, D.S., Dai, C.Q.: Nondegenerate solitons of 2-coupled mixed derivative nonlinear Schrödinger equations. Nonlinear Dyn. 111, 603–617 (2023)
Kheruntsyan, K.V., Drummond, P.D.: Multidimensional quantum solitons with nondegenerate parametric interactions: photonic and bose-einstein condensate environments. Phys. Rev. A. 61, 063816 (2000)
Ostrovskaya, E.A., Kivshar, Y.S., Skryabin, D.V., Firth, W.J.: Stability of multihump optical solitons. Phys. Rev. Lett. 83, 296 (1999)
Yan, Y.Y., Liu, W.J.: Soliton rectangular pulses and bound states in a dissipative system modeled by the variable-coefficients complex cubic-quintic ginzburg-landau equation. Chin. Phys. Lett. 38, 094201 (2021)
Zhang, R.F., Bilige, S.: Bilinear neural network method to obtain the exact analytical solutions of nonlinear partial differential equations and its application to p-gBKP equation. Nonlinear Dyn. 95, 3041–3048 (2019)
Sabirov, K.K., Yusupov, J.R., Aripov, M.M., Ehrhardt, M., Matrasulov, D.U.: Reflectionless propagation of Manakov solitons on a line: a model based on the concept of transparent boundary conditions. Phys. Rev. E. 103, 043305 (2021)
Vijayajayanthi, M., Kanna, T., Murali, K., Lakshmanan, M.: Harnessing energy-sharing collisions of Manakov solitons to implement universal NOR and OR logic gates. Phys. Rev. E. 97, 060201 (2018)
Rodrigues, J.D., Mendonça, J.T., Terças, H.: Turbulence excitation in counterstreaming paraxial superfluids of light. Phys. Rev. A. 101, 043810 (2020)
Watanabe, G., Zhang, Y.P.: Stabilization of nonlinear lattices: a route to superfluidity and hysteresis. Phys Rev A. 98, 013625 (2018)
Forest, M.G., McLaughlin, D.W., Muraki, D.J., Wright, O.C.: Nonfocusing instabilities in coupled, integrable nonlinear Schrödinger pdes. J. Nonlinear Sci. 10, 291–331 (2000)
Ling, L., Zhao, L.C., Guo, B.: Darboux transformation and multi-dark soliton for N-component nonlinear Schrödinger equations. Nonlinearity 28, 3243 (2015)
Lou, S.Y.: Multi-place physics and multi-place nonlocal systems. Commun. Theor. Phys. 72, 057001 (2020)
Ding, C.C., Gao, Y.T., Hu, L., Deng, G.F., Zhang, C.Y.: Vector bright soliton interactions of the two-component AB system in a baroclinic fluid. Chaos Solitons Fractals. 142, 110363 (2021)
Yu, F.J., Liu, C.P., Li, L.: Broken and unbroken solutions and dynamic behaviors for the mixed local–nonlocal Schrödinger equation. Appl. Math. Lett. 117, 107075 (2021)
Stalin, S., Senthilvelan, M., Lakshmanan, M.: Energy-sharing collisions and the dynamics of degenerate solitons in the nonlocal Manakov system. Nonlinear Dyn. 95, 1767–1780 (2019)
Stalin, S., Senthilvelan, M., Lakshmanan, M.: Degenerate soliton solutions and their dynamics in the nonlocal Manakov system: I symmetry preserving and symmetry breaking solutions. Nonlinear Dyn. 95, 343–360 (2019)
Ramakrishnan, R., Stalin, S., Lakshmanan, M.: Nondegenerate solitons and their collisions in Manakov systems. Phys. Rev. E. 102, 042212 (2020)
Anastassiou, C., Segev, M., Steiglitz, K., Giordmaine, J., Mitchell, M., Shih, M.F., Lan, S.: Energy-exchange interactions between colliding vector solitons. Phys. Rev. Lett. 83, 2332 (1999)
Mitchell, M., Segev, M., Christodoulides, D.N.: Observation of multihump multimode solitons. Phys. Rev. Lett. 80, 4657 (1998)
Stratmann, M., Pagel, T., Mitschke, F.: Experimental observation of temporal soliton molecules. Phys. Rev. Lett. 95, 143902 (2005)
Zhang, R.F., Li, M.C.: Bilinear residual network method for solving the exactly explicit solutions of nonlinear evolution equations. Nonlinear Dyn. 108, 521–531 (2022)
Funding
Zhejiang Provincial Natural Science Foundation of China (Grant No. LR20A050001); National Natural Science Foundation of China (Grant Nos. 12261131495, 12075210 and 12275240) and the Scientific Research and Developed Fund of Zhejiang A&F University (Grant No. 2021FR0009).
Author information
Authors and Affiliations
Corresponding authors
Ethics declarations
Conflict of interest
The authors have declared that no conflict of interest exists.
Ethical approval
This research does not involve human participants and/or animals.
Additional information
Publisher's Note
Springer Nature remains neutral with regard to jurisdictional claims in published maps and institutional affiliations.
Appendix parameters in solutions (9) and (11)
Appendix parameters in solutions (9) and (11)
1.1 I. Parameters in solution (9)
1.2 II. Parameters in solution (11)
\(\begin{gathered} K_{m} = \sum\limits_{\begin{subarray}{l} m,n, \\ p,q = 1 \end{subarray} }^{2} {} F_{11}^{2n(1m)} \{ - 2d_{m}^{p(q)} \alpha_{21} (k_{2q} + \overline{k}_{2p} )(k_{11} + \overline{k}_{11} + k_{2n} + \overline{k}_{2m} )\sigma - D_{q}^{2(p)} [2(K_{2} - \overline{k}_{11} - \overline{k}_{2m} + \overline{k}_{2p} )\overline{k}_{2p} + 2(K_{2} - \overline{k}_{11} - \overline{k}_{2m} )k_{12} + \hfill \\ 2( - k_{11} - k_{2n} - \overline{k}_{11} - \overline{k}_{2m} )k_{2q} + k_{11}^{2} + k_{2n}^{2} - \overline{k}_{11}^{2} - \overline{k}_{2m}^{2} ]\} + \sum\limits_{\begin{subarray}{l} m,n, \\ p,q = 1 \end{subarray} }^{2} {} F_{12}^{2n(1m)} \{ - 2d_{m}^{p(q)} \alpha_{11} (k_{2q} + \overline{k}_{2p} )(k_{12} + \overline{k}_{11} + k_{2n} + \overline{k}_{2m} )\sigma - D_{q}^{1(p)} [(K_{2} \hfill \\ + \overline{k}_{11} + \overline{k}_{2m} - \overline{k}_{2p} )\overline{k}_{2p} + (k_{12} + k_{21} - k_{22} + \overline{k}_{11} + \overline{k}_{2m} )k_{11} + (k_{12} + k_{2n} + \overline{k}_{11} + \overline{k}_{2m} )k_{2q} + \frac{1}{2}( - k_{12}^{2} - k_{2n}^{2} + \overline{k}_{11}^{2} + \overline{k}_{2m}^{2} )]\} + \sum\limits_{\begin{subarray}{l} m,n, \\ p,q = 1 \end{subarray} }^{2} {} - 2XJ_{11}^{2q(qp)} \hfill \\ \sigma [(K_{2} + \overline{k}_{11} + \overline{k}_{21} - \overline{k}_{22} )\overline{k}_{2p} + ( - k_{11} - k_{12} - k_{2p} - \overline{k}_{11} )\overline{k}_{2n} + K_{1} \overline{k}_{11} + (k_{11} + k_{12} - k_{22} )k_{21} - (k_{11} + k_{12} )k_{22} + k_{11} k_{12} + \frac{1}{2}(k_{2m}^{2} - \overline{k}_{22}^{2} + 2\overline{k}_{11}^{2} )] \hfill \\ /2[(K_{1} + \overline{k}_{11} + \overline{k}_{21} + \overline{k}_{q1}^{2} + \overline{k}_{22} )\overline{k}_{q1} + (K_{1} + \overline{k}_{nm} + \overline{k}_{q2} )\overline{k}_{q2} + (K_{1} + \overline{k}_{nm} )\overline{k}_{nm} + (k_{1n} + k_{12} + k_{22} )k_{q1} + (k_{n1} + k_{n2} )k_{q2} + k_{n1} k_{n2} ], \hfill \\ \end{gathered}\) \(\begin{gathered} M = \sum\limits_{\begin{subarray}{l} m,n, \\ p,q = 1 \end{subarray} }^{2} {} - [(k_{11} + k_{12} - k_{21} + k_{22} + \overline{k}_{11} + \overline{k}_{12} + \overline{k}_{21} - \overline{k}_{22} )^{2} d_{q}^{n(m)} + 2\alpha_{np} \overline{\alpha }_{qp} ]\sigma H_{q}^{n(m)} - (k_{11} + k_{12} - k_{21} - k_{22} + \overline{k}_{11} + \overline{k}_{12} - \overline{k}_{21} - \overline{k}_{22} )^{2} F_{1} F_{2} \hfill \\ - 2\sum\limits_{\begin{subarray}{l} m,n,p \\ q,M,N = 1 \end{subarray} }^{2} {} [( - \alpha_{11} d_{n}^{q(M)} \overline{\alpha }_{m1} - \alpha_{M2} d_{n}^{n(n)} \overline{\alpha }_{n2} ) + M_{1} + \overline{M}_{1} ]\sigma F_{12}^{2N(pq)} - 2\sigma [\sum\limits_{\begin{subarray}{l} m,n,p \\ q,M,N = 1 \end{subarray} }^{2} {} (M_{2} + \overline{M}_{2} )] - (k_{11} - k_{12} + k_{21} - k_{22} + \overline{k}_{11} - \overline{k}_{12} + \overline{k}_{21} - \overline{k}_{22} )^{2} F_{12}^{2N(pq)} \hfill \\ - 2\sigma [( - \alpha_{NM} d_{n}^{q(2)} \overline{\alpha }_{pM} - \alpha_{2P} d_{m}^{m(p)} \overline{\alpha }_{qp} )\sigma + M_{3} + \overline{M}_{3} ]F_{11}^{2M(mn)} ,M_{1} = D_{M}^{1(n)} \overline{\alpha }_{m1} + d_{1}^{M(m)} \overline{\alpha }_{n2} ,M_{2} = D_{m}^{n(M)} \overline{J}_{1q}^{2p(pN)} + d_{m}^{n(M)} \overline{j}_{1q}^{2p(pN)} + \overline{E}_{m}^{n} \overline{J}_{21}^{22(p)} . \hfill \\ M_{3} = D_{N}^{2(q)} \overline{\alpha }_{p1} + d_{N}^{N(p)} \overline{\alpha }_{q2} . \hfill \\ \end{gathered}\) \(\begin{gathered} L_{m} = \sum\limits_{\begin{subarray}{l} m,n, \\ p,q = 1 \end{subarray} }^{2} {} F_{11}^{2n(1m)} \{ - 2d_{m}^{p(q)} \alpha_{21} (k_{2q} + \overline{k}_{2p} )(k_{11} + \overline{k}_{11} + k_{2n} + \overline{k}_{2m} )\sigma - d_{q}^{2(p)} [2(K_{2} - \overline{k}_{11} - \overline{k}_{2m} + \overline{k}_{2p} )\overline{k}_{2p} + 2( - k_{11} - k_{21} + k_{22} - \overline{k}_{11} - \overline{k}_{2m} )k_{12} \hfill \\ + 2( - k_{11} - k_{2n} - \overline{k}_{11} - \overline{k}_{2m} )k_{2q} + k_{11}^{2} + k_{2n}^{2} - \overline{k}_{11}^{2} - \overline{k}_{2m}^{2} ]\} + \sum\limits_{\begin{subarray}{l} m,n, \\ p,q = 1 \end{subarray} }^{2} {} F_{12}^{2n(1m)} \{ - 2d_{m}^{p(q)} \alpha_{11} (k_{2q} + \overline{k}_{2p} )(k_{12} + \overline{k}_{11} + k_{2n} + \overline{k}_{2m} )\sigma - d_{q}^{1(p)} [(K_{1} + \overline{k}_{11} + \hfill \\ \overline{k}_{2m} - \overline{k}_{2p} )\overline{k}_{2p} + (k_{12} + k_{21} - k_{22} + \overline{k}_{11} + \overline{k}_{2m} )k_{11} + (k_{12} + k_{2n} + \overline{k}_{11} + \overline{k}_{2m} )k_{2q} + \frac{1}{2}( - k_{12}^{2} - k_{2n}^{2} + \overline{k}_{11}^{2} + \overline{k}_{2m}^{2} )]\} + \sum\limits_{\begin{subarray}{l} m,n, \\ p,q = 1 \end{subarray} }^{2} {} - 2Xj_{11}^{2q(qp)} \sigma [(K_{1} + \overline{k}_{11} + \hfill \\ \overline{k}_{21} - \overline{k}_{22} )\overline{k}_{2p} + ( - k_{11} - k_{12} - k_{2p} - \overline{k}_{11} )\overline{k}_{2n} + L_{1} \overline{k}_{11} + (k_{11} + k_{12} - k_{22} )k_{21} - (k_{11} + k_{12} )k_{22} + k_{11} k_{12} + \frac{1}{2}(k_{2m}^{2} - \overline{k}_{22}^{2} + 2\overline{k}_{11}^{2} )]/2[(K_{1} + \overline{k}_{11} + \overline{k}_{21} + \hfill \\ \overline{k}_{q1}^{2} + \overline{k}_{22} )\overline{k}_{q1} + (K_{1} + \overline{k}_{nm} + \overline{k}_{q2} )\overline{k}_{q2} + (K_{1} + \overline{k}_{nm} )\overline{k}_{nm} + (k_{1n} + k_{12} + k_{22} )k_{q1} + (k_{n1} + k_{n2} )k_{q2} + k_{n1} k_{n2} ],m \ne n,p \ne q,K_{1} = k_{11} + k_{12} + k_{21} + k_{22} , \hfill \\ K_{2} = - k_{11} + k_{12} + k_{21} - k_{22} . \hfill \\ \end{gathered}\)
Rights and permissions
Springer Nature or its licensor (e.g. a society or other partner) holds exclusive rights to this article under a publishing agreement with the author(s) or other rightsholder(s); author self-archiving of the accepted manuscript version of this article is solely governed by the terms of such publishing agreement and applicable law.
About this article
Cite this article
Geng, KL., Zhu, BW., Cao, QH. et al. Nondegenerate soliton dynamics of nonlocal nonlinear Schrödinger equation. Nonlinear Dyn 111, 16483–16496 (2023). https://doi.org/10.1007/s11071-023-08719-w
Received:
Accepted:
Published:
Issue Date:
DOI: https://doi.org/10.1007/s11071-023-08719-w