Yayın:
Petviashvili Method for the Fractional Schrödinger Equation

Yükleniyor...
Küçük Resim

Kurum Yazarları

Item type:Araştırmacı/Yazar,
Bayındır, Cihan
Profesor

Danışman

Bölüm / Program

Dergi Başlığı

Dergi ISSN

Cilt Başlığı

Yayıncı

MDPI AG

Türü

Araştırma Projeleri

Akademik Birimler

Dergi Sayısı

Özet

In this paper, we extend the Petviashvili method (PM) to the fractional nonlinear Schrödinger equation (fNLSE) for the construction and analysis of its soliton solutions. We also investigate the temporal dynamics and stabilities of the soliton solutions of the fNLSE by implementing a spectral method, in which the fractional-order spectral derivatives are computed using FFT (Fast Fourier Transform) routines, and the time integration is performed by a 4th order Runge–Kutta time-stepping algorithm. We discuss the effects of the order of the fractional derivative, α, on the properties, shapes, and temporal dynamics of the soliton solutions of the fNLSE. We also examine the interaction of those soliton solutions with zero, photorefractive and q-deformed Rosen–Morse potentials. We show that for all of these potentials, the soliton solutions of the fNLSE exhibit a splitting and spreading behavior, yet their dynamics can be altered by the different forms of the potentials and noise considered.

Tanım

Dergi veya Seri

Fractal and Fractional

ISSN

ISBN

Haklar

OPEN

Anahtar Kelimeler

QA299.6-433, fractional nonlinear Schrödinger equation, Petviashvili method, potential function, solitons, q-deformation, potential function, Petviashvili method, FOS: Physical sciences, Pattern Formation and Solitons (nlin.PS), Nonlinear Sciences - Pattern Formation and Solitons, fractional nonlinear Schrödinger equation, q-deformation, solitons, QA1-939, Thermodynamics, QC310.15-319, Mathematics, Analysis

Alıntı

Koleksiyonlar

Onay

Gözden geçir

Tamamlayıcı Bilgiler

Referans Gösteren

Related Patent

Related Goal

0
Görüntülenme
0
İndirme
Altmetric
Dimensions
PlumX Metrikleri
BIP! Indicators
Google Scholar
Scholar'da Ara ↗