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Theory and Modern Applications

Table 1 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

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

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

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

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

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

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

0

0

0

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

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

0

0

0

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

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

0

0

0

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

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

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

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

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

0