2023
DOI: 10.1016/j.ijleo.2023.171254
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Adaptation of Caputo residual power series scheme in solving nonlinear time fractional Schrödinger equations

Bahadır Kopçasız,
Emrullah Yaşar
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Cited by 7 publications
(1 citation statement)
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“…Besides the time-fractional diffusion equation, lots of scholars have developed many schemes to cope with the time fractional Burgers' equation, like the operator splitting approach and artificial boundary method [19], the nonuniform Alikhanov formula of the Caputo time fractional derivative and Fourier spectral approximation in space [20], the L1 scheme and the local discontinuous Galerkin method [21], the Lucas polynomials coupled with finite difference method [22], the fourth-order compact difference scheme [23], the L1 implicit difference scheme based on non-uniform meshes [24], a secondorder energy stable and nonuniform time-stepping scheme [25], a collocation approach with trigonometric tension B-splines [26], the cubic B-spline functions and θ-weighted scheme [27], the local projection stabilization virtual element method [28], a compact difference scheme [29], the Caputo-Katugampola fractional derivative by extending the Laplace transform [30], and the tailored finite point method based on exponential basis [31]. For the time-fractional Schrödinger equations, lots of researchers have proposed many algorithms, like the conformable natural transform and the homotopy perturbation method [32], the conformable fractional derivatives modified Khater technique and the Adomian decomposition method [33], the Laplace Adomian decomposition method and the modified generalized Mittag-Leffler function method [34], a Caputo residual power series scheme [35], and the extended Kudryashov method [36].…”
Section: Introductionmentioning
confidence: 99%
“…Besides the time-fractional diffusion equation, lots of scholars have developed many schemes to cope with the time fractional Burgers' equation, like the operator splitting approach and artificial boundary method [19], the nonuniform Alikhanov formula of the Caputo time fractional derivative and Fourier spectral approximation in space [20], the L1 scheme and the local discontinuous Galerkin method [21], the Lucas polynomials coupled with finite difference method [22], the fourth-order compact difference scheme [23], the L1 implicit difference scheme based on non-uniform meshes [24], a secondorder energy stable and nonuniform time-stepping scheme [25], a collocation approach with trigonometric tension B-splines [26], the cubic B-spline functions and θ-weighted scheme [27], the local projection stabilization virtual element method [28], a compact difference scheme [29], the Caputo-Katugampola fractional derivative by extending the Laplace transform [30], and the tailored finite point method based on exponential basis [31]. For the time-fractional Schrödinger equations, lots of researchers have proposed many algorithms, like the conformable natural transform and the homotopy perturbation method [32], the conformable fractional derivatives modified Khater technique and the Adomian decomposition method [33], the Laplace Adomian decomposition method and the modified generalized Mittag-Leffler function method [34], a Caputo residual power series scheme [35], and the extended Kudryashov method [36].…”
Section: Introductionmentioning
confidence: 99%