Theory and Modern Applications
From: Non-polynomial spline method for the time-fractional nonlinear Schrödinger equation
h | \(e_{\infty}(h,\tau)\) (real part) | \(e_{\infty}(h,\tau)\) (Imag. part) | ||
---|---|---|---|---|
Our method | [11] | Our method | [11] | |
1/4 | 3.6866388e − 2 | 4.2824e − 1 | 7.0575277e − 2 | 6.1335e − 1 |
1/9 | 1.2682659e − 3 | 7.0404e − 2 | 2.4249059e − 3 | 7.6325e − 2 |
1/14 | 2.2076538e − 4 | 2.1873e − 2 | 4.1971919e − 4 | 2.6096e − 2 |
1/19 | 6.5146969e − 5 | 1.0022e − 2 | 1.2268149e − 4 | 1.2230e − 2 |
1/24 | 2.5400339e − 5 | 5.1958e − 3 | 4.8342660e − 5 | 6.4207e − 3 |
1/29 | 1.1938367e − 5 | 2.8536e − 3 | 2.2621457e − 5 | 3.5662e − 3 |