Table 1 Data presentation for curve of normalized frequency with ion nonextensive parameter.
From: Initial analytical theory of plasma disruption and experimental evidence
q\(=\)2.5 | q\(_{F_\text{i}}\) | (–1)\(^{+}\) | 0 | (1/3)− | (1/3)\(^{+}\) | 0.5293 | 0.5324 | (3/5)− | (3/5)\(^{+}\) | 0.775 | 1 | 1.565 | 2 | \(+\infty\) |
\(\omega _\text{r}\)R\(_{0}\)/v\(_\text{ti}\) | 0.2478 | 0.4089 | 0.6279 | \(+\infty\) | 1.7251\(+\)0.0004i | 1.7248\(+\)0.2091i | \(+\infty +\infty\)i | \(+\infty\) | 1.7737 | 1.4079 | 1.0227 | 0.8766 | 0 | |
q\(=\)3.3 | q\(_{F_\text{i}}\) | (–1)\(^{+}\) | 0 | (1/3)− | (1/3)\(^{+}\) | 0.5543 | 0.5543 | (3/5)− | (3/5)\(^{+}\) | 0.775 | 1 | 1.565 | 2 | \(+\infty\) |
\(\omega _\text{r}\)R\(_{0}\)/v\(_\text{ti}\) | 0.1903 | 0.3128 | 0.4757 | \(+\infty\) | 1.6248\(+\)0.0021i | 1.6248\(+\)0.0021i | \(+\infty +\infty\)i | \(+\infty\) | 1.7176 | 1.3747 | 1.0030 | 0.8607 | 0 | |
q\(=\)4.0 | q\(_{F_\text{i}}\) | (–1)\(^{+}\) | 0 | (1/3)− | (1/3)\(^{+}\) | 0.5671 | 0.5671 | (3/5)− | (3/5)\(^{+}\) | 0.775 | 1 | 1.565 | 2 | \(+\infty\) |
\(\omega _\text{r}\)R\(_{0}\)/v\(_\text{ti}\) | 0.1580 | 0.2591 | 0.3925 | \(+\infty\) | 1.5797\(+\)0.0043i | 1.5797\(+\)0.0043i | \(+\infty +\infty\)i | \(+\infty\) | 1.6907 | 1.3591 | 0.9940 | 0.8533 | 0 |
