TY - GEN
T1 - Localized modes in a nonlinear medium with a PT-symmetric dipole
AU - Mayteevarunyoo, Thawatchai
AU - Reoksabutr, Athikom
AU - Malomed, Boris A.
N1 - Publisher Copyright:
© 2014 IEEE.
PY - 2014/10/15
Y1 - 2014/10/15
N2 - We introduce the simplest one-dimensional model of a nonlinear system with the parity-time (PT ) symmetry, which makes it possible to find numerical solutions for localized modes ('solitons'). The PT -symmetric element is represented by a point-like (delta-functional) gain-loss dipole ∼ δ′(x), combined with the usual attractive potential ∼ δ(x). The nonlinearity is represented by self-focusing (SF) Kerr terms, both spatially uniform and localized ones. The system can be implemented in planar optical waveguides. For the sake of comparison, also introduced is the model with separated δ-functional gain and loss, embedded into the linear medium and combined with the δ-localized Kerr nonlinearity and attractive potential. Full analytical solutions for pinned modes are found in both models. The numerical solutions are obtained in the gain-loss-dipole model with the δ′- and δ- functions replaced by their Lorentzian regularization. With the increase of the dipole's strength, γ, the single-peak shape of the numerically found mode, supported by the uniform SF nonlinearity, transforms into a double-peak one. This transition coincides with the onset of the escape instability of the pinned soliton.
AB - We introduce the simplest one-dimensional model of a nonlinear system with the parity-time (PT ) symmetry, which makes it possible to find numerical solutions for localized modes ('solitons'). The PT -symmetric element is represented by a point-like (delta-functional) gain-loss dipole ∼ δ′(x), combined with the usual attractive potential ∼ δ(x). The nonlinearity is represented by self-focusing (SF) Kerr terms, both spatially uniform and localized ones. The system can be implemented in planar optical waveguides. For the sake of comparison, also introduced is the model with separated δ-functional gain and loss, embedded into the linear medium and combined with the δ-localized Kerr nonlinearity and attractive potential. Full analytical solutions for pinned modes are found in both models. The numerical solutions are obtained in the gain-loss-dipole model with the δ′- and δ- functions replaced by their Lorentzian regularization. With the increase of the dipole's strength, γ, the single-peak shape of the numerically found mode, supported by the uniform SF nonlinearity, transforms into a double-peak one. This transition coincides with the onset of the escape instability of the pinned soliton.
KW - PT -symmetry
KW - Solitons
UR - http://www.scopus.com/inward/record.url?scp=84911882431&partnerID=8YFLogxK
U2 - 10.1109/iEECON.2014.6925949
DO - 10.1109/iEECON.2014.6925949
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AN - SCOPUS:84911882431
T3 - 2014 International Electrical Engineering Congress, iEECON 2014
BT - 2014 International Electrical Engineering Congress, iEECON 2014
PB - Institute of Electrical and Electronics Engineers Inc.
T2 - 2014 International Electrical Engineering Congress, iEECON 2014
Y2 - 19 March 2014 through 21 March 2014
ER -