• Chinese Optics Letters
  • Vol. 13, Issue 4, 041901 (2015)
Guangyu Jiang1,* and Youwen Liu1,2
Author Affiliations
  • 1Department of Applied Physics, Nanjing University of Aeronautics and Astronautics, Nanjing 210016, China
  • 2Key Laboratory of Radar Imaging and Microwave Photonics, Ministry of Education, Nanjing University of Aeronautics and Astronautics, Nanjing 210016, China
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    DOI: 10.3788/COL201513.041901 Cite this Article Set citation alerts
    Guangyu Jiang, Youwen Liu, "Continuous generation of dissipative spatial solitons in two-dimensional Ginzburg–Landau models with elliptical shaped potentials," Chin. Opt. Lett. 13, 041901 (2015) Copy Citation Text show less
    (a) Stable soliton solution in Eq. (1). (b) Soliton dynamics for various sharpnesses (from top to bottom: n=0.1, 0.2, 0.3, 0.4, 0.5, 0.6, 0.7, 0.8, and 0.9) of the elliptical shaped potential when p=3 for M=2 and N=5. The transverse domain is (−50,50)×(−50,50).
    Fig. 1. (a) Stable soliton solution in Eq. (1). (b) Soliton dynamics for various sharpnesses (from top to bottom: n=0.1, 0.2, 0.3, 0.4, 0.5, 0.6, 0.7, 0.8, and 0.9) of the elliptical shaped potential when p=3 for M=2 and N=5. The transverse domain is (50,50)×(50,50).
    Regions of different soliton dynamics in the plane (n, p) when M=2 and N=5. In region A, for soliton localization; in region B, for soliton straight-line arrays; in regions C and D, for soliton evolution into one elliptical ring soliton array and a set of elliptical ring solitons, respectively; in region E, for soliton decay.
    Fig. 2. Regions of different soliton dynamics in the plane (n, p) when M=2 and N=5. In region A, for soliton localization; in region B, for soliton straight-line arrays; in regions C and D, for soliton evolution into one elliptical ring soliton array and a set of elliptical ring solitons, respectively; in region E, for soliton decay.
    Soliton dynamics for various sharpnesses (top: n=0.5, middle: n=0.6, bottom: n=0.7) of the elliptical shaped potential when p=3 for M=3 and (a) N=5; (b) N=6; (c) N=7; (d) N=8. The transverse domain is (−60,60)×(−60,60).
    Fig. 3. Soliton dynamics for various sharpnesses (top: n=0.5, middle: n=0.6, bottom: n=0.7) of the elliptical shaped potential when p=3 for M=3 and (a) N=5; (b) N=6; (c) N=7; (d) N=8. The transverse domain is (60,60)×(60,60).
    Regions of dynamic regimes in the plane (M, N) when p=3 and n=0.6.
    Fig. 4. Regions of dynamic regimes in the plane (M, N) when p=3 and n=0.6.
    Soliton dynamics for various sharpnesses n = (a) 0.5, (b) 0.6, and (c) 0.7 of the tapered-elliptical potential when p=1 for M=2 and N=5. The transverse domain is (−60,60)×(−60,60).
    Fig. 5. Soliton dynamics for various sharpnesses n = (a) 0.5, (b) 0.6, and (c) 0.7 of the tapered-elliptical potential when p=1 for M=2 and N=5. The transverse domain is (60,60)×(60,60).
    Guangyu Jiang, Youwen Liu, "Continuous generation of dissipative spatial solitons in two-dimensional Ginzburg–Landau models with elliptical shaped potentials," Chin. Opt. Lett. 13, 041901 (2015)
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