Skip to main content

Theory and Modern Applications

Table 2 The commutation relations of infinitesimal generators \(\mathcal{X}_{1}\), \(\mathcal{X}_{2}\), \(\mathcal{X}_{3}\)

From: A new fourth-order integrable nonlinear equation: breather, rogue waves, other lump interaction phenomena, and conservation laws

\([\mathcal{X}_{i},\mathcal{X}_{j}]\)

\(\mathcal{X}_{1}\)

\(\mathcal{X}_{2}\)

\(\mathcal{X}_{3}\)

\(\mathcal{X}_{4}\)

\(\mathcal{X}_{1}\)

\(\mathcal{X}_{1}\)

\(\mathcal{X}_{2}\)

\(\mathcal{X}_{3}\)

\(\epsilon \mathcal{X}_{1}+\mathcal{X}_{4}\)

\(\mathcal{X}_{2}\)

\(\mathcal{X}_{1}\)

\(\mathcal{X}_{2}\)

\(\mathcal{X}_{3}\)

\(-\epsilon \mathcal{X}_{2}+\mathcal{X}_{4}\)

\(\mathcal{X}_{3}\)

\(\mathcal{X}_{1}\)

\(\mathcal{X}_{2}\)

\(\mathcal{X}_{3}\)

\(3\epsilon \mathcal{X}_{3}+\mathcal{X}_{4}\)

\(\mathcal{X}_{4}\)

\(e^{-\epsilon }\mathcal{X}_{1}\)

\(e^{\epsilon }\mathcal{X}_{2}\)

\(e^{-3\epsilon }\mathcal{X}_{3}\)

\(\mathcal{X}_{4}\)