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Table 1 \(L_{2}\)-comparison for problem (1)

From: Legendre spectral collocation method for distributed and Riesz fractional convection–diffusion and Schrödinger-type equation

Our spectral results at \(\mathcal{M}=2\) and different values of \(\mathcal{N}\)

δ

4

6

8

1.2

3.38359 × 10−3

7.23926 × 10−4

1.7081 × 10−12

1.4

3.78916 × 10−3

9.39218 × 10−4

5.07319 × 10−13

1.8

4.77345 × 10−3

1.74284 × 10−3

1.17669 × 10−12

Local discontinuous Galerkin method [57]

 

K

5

10

15

20

N = 1

1.2

5.97 × e−02

8.6 × e−03

3.4 × e−03

1.8 × e−03

1.4

2.84 × e−02

5.8 × e−03

2.5 × e−03

1.3 × e−03

1.8

1.91 × e−02

4.5 × e−03

1.9 × e−03

9.9 × e−04

N = 2

1.2

3.52 × e−02

4.3 × e−03

1.2 × e−03

4.8 × e−04

1.4

1.57 × e−02

2.1 × e−03

5.9 × e−04

2.6 × e−04

1.8

1.45 × e−02

1.8 × e−03

5.5 × e−04

2.2 × e−04