Theory and Modern Applications
From: Non-polynomial spline method for the time-fractional nonlinear Schrödinger equation
α | h | \(e_{\infty}(h,\tau)\) (real part) | \(\mathit{rate2}_{\infty}\) | \(e_{\infty}(h,\tau)\) (Imag. part) | \(\mathit{rate2}_{\infty}\) |
---|---|---|---|---|---|
0.2 | 1/4 | 3.7584486e − 2 | ∗ | 7.0194896e − 2 | ∗ |
1/8 | 2.1460025e − 3 | 4.13041 | 3.9870246e − 3 | 4.13798 | |
1/16 | 1.3155654e − 4 | 4.02790 | 2.4435715e − 4 | 4.02825 | |
1/32 | 8.2162754e − 6 | 4.00105 | 1.5201566e − 5 | 4.00669 | |
0.4 | 1/4 | 3.9172112e − 2 | ∗ | 6.9118840e − 2 | ∗ |
1/8 | 2.2323011e − 3 | 4.13322 | 3.9321438e − 3 | 4.13569 | |
1/16 | 1.3682056e − 4 | 4.02817 | 2.4101573e − 4 | 4.02812 | |
1/32 | 8.5392992e − 6 | 4.00202 | 1.4999655e − 5 | 4.00613 | |
0.6 | 1/4 | 4.0855486e − 2 | ∗ | 6.7504824e − 2 | ∗ |
1/8 | 2.3249758e − 3 | 4.13524 | 3.8502877e − 3 | 4.13195 | |
1/16 | 1.4239539e − 4 | 4.02924 | 2.3604686e − 4 | 4.02782 | |
1/32 | 8.8294610e − 6 | 4.01143 | 1.4703310e − 5 | 4.00486 | |
0.8 | 1/4 | 4.2399284e − 2 | ∗ | 6.5355436e − 2 | ∗ |
1/8 | 2.4119363e − 3 | 4.13577 | 3.7401138e − 3 | 4.12715 | |
1/16 | 1.4702052e − 4 | 4.03610 | 2.2944121e − 4 | 4.02689 | |
1/32 | 8.3350082e − 6 | 4.14069 | 1.4399479e − 5 | 3.99404 |