2017
DOI: 10.1016/j.physleta.2017.01.018
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Approximate analytic solutions to coupled nonlinear Dirac equations

Abstract: We consider the coupled nonlinear Dirac equations (NLDE's) in 1+1 dimensions with scalarscalar self interactions g 2 1 2 (ψψ) 2 + g 2 2 2 (φφ) 2 + g 2 3 (ψψ)(φφ) as well as vector-vector interactions of the form g 2 1 2 (ψγµψ)(ψγ µ ψ) + g 2 2 2 (φγµφ)(φγ µ φ) + g 2 3 (ψγµψ)(φγ µ φ). Writing the two components of the assumed solitary wave solution of these equation in the form ψ = e −iω 1 t {R1 cos θ, R1 sin θ}, φ = e −iω 2 t {R2 cos η, R2 sin η}, and assuming that θ(x), η(x) have the same functional form they … Show more

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Cited by 3 publications
(6 citation statements)
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“…10 we plot the growth rate of the "noise floor" versus L. The theoretical values are inferred from the spectral radius of Φ(L), which was found by the above analysis, via the relation (see (45a)): growth rate = ln ρ(Φ(L)) /L . (46) The agreement between our analysis and direct numerics is seen to be quite good. 44), (46).…”
Section: Unconditional Instability Of the "Noise Floor"supporting
confidence: 60%
See 4 more Smart Citations
“…10 we plot the growth rate of the "noise floor" versus L. The theoretical values are inferred from the spectral radius of Φ(L), which was found by the above analysis, via the relation (see (45a)): growth rate = ln ρ(Φ(L)) /L . (46) The agreement between our analysis and direct numerics is seen to be quite good. 44), (46).…”
Section: Unconditional Instability Of the "Noise Floor"supporting
confidence: 60%
“…(46) The agreement between our analysis and direct numerics is seen to be quite good. 44), (46). Circles are the result of SSM simulation, where we measured the amplitude of the Fourier harmonic at k = k max /2 and followed the procedure described at the end of Section 5.…”
Section: Unconditional Instability Of the "Noise Floor"supporting
confidence: 60%
See 3 more Smart Citations