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Theory and Modern Applications

Table 4 (Example 6.1) Comparing \(E^{\text{Re}}_{\infty }(h,\tau )\) and \(E^{\text{Im}}_{\infty }(h,\tau )\) with other methods

From: Quintic non-polynomial spline for time-fractional nonlinear Schrödinger equation

γ

\(E^{\text{Re}}_{\infty }(h,\tau )\)

\(E^{\text{Re}}_{\infty }(h,\tau )\)

\(E^{\text{Re}}_{\infty }(h,\tau )\)

\(E^{\text{Im}}_{\infty }(h,\tau )\)

\(E^{\text{Im}}_{\infty }(h,\tau )\)

\(E^{\text{Im}}_{\infty }(h,\tau )\)

Our method

QBG [16]

CNS [36]

Our method

QBG [16]

CNS [36]

0.10

3.1730e−07

4.6850e−04

3.1153e−06

1.5460e−07

7.7635e−04

6.2728e−06

0.30

2.1533e−06

4.9949e−04

3.3537e−06

1.1104e−06

3.2833e−04

6.5370e−06

0.70

3.9262e−05

6.6590e−04

3.9311e−05

3.2046e−05

1.0614e−03

3.2046e−05

0.90

1.9926e−04

8.4460e−04

1.9971e−04

1.4957e−04

1.3150e−03

1.4957e−04