Theory and Modern Applications
From: Symmetry reductions of the \((3+1)\)-dimensional modified Zakharov–Kuznetsov equation
\(\mathcal{V}_{1}\) | \(\mathcal{V}_{2}\) | \(\mathcal{V}_{3}\) | \(\mathcal{V}_{4}\) | \(\mathcal{V}_{5}\) | \(\mathcal{V}_{6}\) | |
---|---|---|---|---|---|---|
\(\mathcal{V}_{1}\) | 0 | \(\frac{2}{3}k\mathcal{V}_{3}-\mathcal{V}_{2}\) | \(-\frac{1}{3}\mathcal{V}_{3}\) | 0 | \(-\frac{1}{3}\mathcal{V}_{5}\) | \(-\frac{1}{3}\mathcal{V}_{6}\) |
\(\mathcal{V}_{2}\) | \(\mathcal{V}_{2}-\frac{2}{3}k\mathcal{V}_{3}\) | 0 | 0 | 0 | 0 | 0 |
\(\mathcal{V}_{3}\) | \(\frac{1}{3}\mathcal{V}_{3}\) | 0 | 0 | 0 | 0 | 0 |
\(\mathcal{V}_{4}\) | 0 | 0 | 0 | 0 | \(\mathcal{V}_{6}\) | \(-\mathcal{V}_{5}\) |
\(\mathcal{V}_{5}\) | \(\frac{1}{3}\mathcal{V}_{5}\) | 0 | 0 | \(-\mathcal{V}_{6}\) | 0 | 0 |
\(\mathcal{V}_{6}\) | \(\frac{1}{3}\mathcal{V}_{6}\) | 0 | 0 | \(\mathcal{V}_{5}\) | 0 | 0 |