Photonics Research, 2018, 6 (9): 09000875, Published Online: Aug. 15, 2018
Solitons in the fractional Schrödinger equation with parity-time-symmetric lattice potential
Figures & Tables
Fig. 1. (a) Photonic band structure for FSE with PT-symmetric periodic potential, when V i = 0.4 (red line) and 0.55 (blue line). (b) Imaginary parts of the band structure for V i = 0.55 .
Fig. 2. (a) Soliton field profile (real part: blue line, imaginary part: red line) for β = 0.8 . (b) The spectral distribution | ϕ ˜ ( k ) | in the inverse space. (c) Transverse power flow (red line) of the soliton. (d) Spectrum of the linearization operator for the soliton solution in (a). (e) Stable propagation perturbed with weak noise. The light gray line in (a) and (d) represents the scaled real part of the potential. For all cases, V i = 0.4 and A = 1 .
Fig. 3. (a) Soliton field profile (real part: blue line, imaginary part: red line). The light gray line denotes the real part of the potential. (b) The perturbation growth rate profile for the soliton solution in (a). (c) Unstable PT soliton propagation perturbed with weak noise. In all cases, V i = 0.55 and β = 0.8 .
Fig. 4. (a) Domains of stability on the plane (β , V i ) for 1D solitons. Solitons are stable in the blue region. The red line denotes the lower edge of the semi-infinite forbidden gap. (b) The maximum real part of perturbation growth rate versus β for V i = 0.4 and A = 1 .
Fig. 5. (a) Band structure of a 2D-PT potential for Eq. (4 ) in linear form. The inset displays the band structure in the reduced Brillouin zone. (b) The profile of a 2D soliton when β = 5.55 . (c) The spectral profile | ϕ ˜ ( k x , k y ) | in the inverse space. (d) Transverse power flow (indicated by arrows) for the soliton in (b) within one cell. “L” and “G” indicate the loss and gain regions, respectively. For all cases, A = 4 and V i = 0.2 .
Xiankun Yao, Xueming Liu. Solitons in the fractional Schrödinger equation with parity-time-symmetric lattice potential[J]. Photonics Research, 2018, 6(9): 09000875.