Stability of solitary waves in the nonlinear Dirac equation with arbitrary nonlinearity
arXiv:1405.5547 · doi:10.1103/PhysRevE.90.032915
Abstract
We consider the nonlinear Dirac equation in 1+1 dimension with scalar-scalar self interaction and with mass . Using the exact analytic form for rest frame solitary waves of the form for arbitrary , we discuss the validity of various approaches to understanding stability that were successful for the nonlinear Schrödinger equation. In particular we study the validity of a version of Derrick's theorem, the criterion of Bogolubsky as well as the Vakhitov-Kolokolov criterion, and find that these criteria yield inconsistent results. Therefore, we study the stability by numerical simulations using a recently developed 4th-order operator splitting integration method. For different ranges of we map out the stability regimes in . We find that all stable nonlinear Dirac solitary waves have a one-hump profile, but not all one-hump waves are stable, while all waves with two humps are unstable. We also find that the time , it takes for the instability to set in, is an exponentially increasing function of and decreases monotonically with increasing .
arXiv comment35 pages, 13 figures
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