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 | 3.8355790e − 2 | 4.3293e − 1 | 6.9716586e − 2 | 6.1119e − 1 |
1/9 | 1.3134983e − 3 | 7.0520e − 2 | 2.3999262e − 3 | 3.5128e − 2 |
1/14 | 2.2989563e − 4 | 2.1979e − 2 | 4.1516336e − 4 | 1.4733e − 2 |
1/19 | 6.7510083e − 5 | 1.0068e − 2 | 1.2139583e − 4 | 7.1997e − 3 |
1/24 | 2.6166613e − 5 | 5.2146e − 3 | 4.7854800e − 5 | 3.8478e − 3 |
1/29 | 1.2194745e − 5 | 2.8610e − 3 | 2.2402366e − 5 | 2.1771e − 3 |