Theory and Modern Applications
From: A mass conserved splitting method for the nonlinear Schrödinger equation
λ, β | ϕ g (0) |
|
|
|
| E g | μ g |
|
---|---|---|---|---|---|---|---|---|
λ = − 0.2, β = 0.5 | 0.747990 | 0.247231 | 0.252333 | 0.099135 | − 0.171511 | 0.427188 | 0.354812 | 0.710398 |
λ = − 0.1, β = 0.25 | 0.749946 | 0.248765 | 0.250757 | 0.049763 | − 0.085918 | 0.463367 | 0.427212 | 0.708176 |
λ = − 0.02, β = 0.05 | 0.751125 | 0.249513 | 0.250000 | 0.009974 | − 0.017201 | 0.492285 | 0.485058 | 0.707106 |
λ = 0.02, β = − 0.05 | 0.751581 | 0.249878 | 0.249634 | − 0.009983 | 0.017208 | 0.506737 | 0.513963 | 0.706589 |
λ = 0.1, β = − 0.25 | 0.753250 | 0.251210 | 0.248312 | − 0.050082 | 0.086181 | 0.535622 | 0.571721 | 0.704716 |
λ = 0.2, β = − 0.5 | 0.755449 | 0.253038 | 0.246533 | − 0.100613 | 0.172734 | 0.571693 | 0.643814 | 0.702187 |