Theory and Modern Applications
n | \(\vphantom{\sum_{A_{A}}}q =\frac{1}{8}\) | \(q =\frac {1}{2}\) | \(q =\frac{8}{9}\) | ||||||
---|---|---|---|---|---|---|---|---|---|
\(\eta_{2}\) | \(\varGamma_{q}(\alpha_{2} - 1)\) | \(\vphantom{\sum_{A_{A}}}\frac{\eta_{2}}{\varGamma_{q}(\alpha _{2} - 1)}\) | \(\eta_{2}\) | \(\varGamma_{q}(\alpha_{2} - 1)\) | \(\frac{\eta_{2}}{\varGamma_{q}(\alpha_{2} - 1)}\) | \(\eta_{2}\) | \(\varGamma_{q}(\alpha_{2} - 1)\) | \(\frac{\eta_{2}}{\varGamma_{q}(\alpha_{2} - 1)}\) | |
1 | 0.5097 | 1.0329 | 0.4934 | 0.5010 | 1.0233 | 0.4896 | 0.3771 | 0.7200 | 0.5238 |
2 | 0.5101 | 1.0339 | 0.4933 | 0.5136 | 1.0534 | 0.4876 | 0.4010 | 0.7854 | 0.5106 |
3 | 0.5101 | 1.0341 | 0.4933 | 0.5198 | 1.0679 | 0.4867 | 0.4201 | 0.8356 | 0.5028 |
4 | 0.5101 | 1.0341 | 0.4933 | 0.5228 | 1.075 | 0.4863 | 0.4358 | 0.8757 | 0.4977 |
5 | 0.5101 | 1.0341 | 0.4933 | 0.5243 | 1.0786 | 0.4861 | 0.4490 | 0.9085 | 0.4942 |
6 | 0.5101 | 1.0341 | 0.4933 | 0.5250 | 1.0803 | 0.4860 | 0.4601 | 0.9359 | 0.4916 |
7 | 0.5101 | 1.0341 | 0.4933 | 0.5254 | 1.0812 | 0.486 | 0.4696 | 0.9589 | 0.4897 |
8 | 0.5101 | 1.0341 | 0.4933 | 0.5256 | 1.0816 | 0.4859 | 0.4778 | 0.9784 | 0.4883 |
9 | 0.5101 | 1.0341 | 0.4933 | 0.5257 | 1.0818 | 0.4859 | 0.4848 | 0.9952 | 0.4872 |
10 | 0.5101 | 1.0341 | 0.4933 | 0.5257 | 1.0819 | 0.4859 | 0.4910 | 1.0096 | 0.4863 |
11 | 0.5101 | 1.0341 | 0.4933 | 0.5258 | 1.0820 | 0.4859 | 0.4963 | 1.0221 | 0.4856 |
⋮ | ⋮ | ⋮ | ⋮ | ⋮ | ⋮ | ⋮ | ⋮ | ⋮ | ⋮ |
34 | 0.5101 | 1.0341 | 0.4933 | 0.5258 | 1.0821 | 0.4859 | 0.5336 | 1.1071 | 0.4820 |
35 | 0.5101 | 1.0341 | 0.4933 | 0.5258 | 1.0821 | 0.4859 | 0.5339 | 1.1077 | 0.4819 |
36 | 0.5101 | 1.0341 | 0.4933 | 0.5258 | 1.0821 | 0.4859 | 0.5341 | 1.1083 | 0.4819 |
37 | 0.5101 | 1.0341 | 0.4933 | 0.5258 | 1.0821 | 0.4859 | 0.5343 | 1.1088 | 0.4819 |
38 | 0.5101 | 1.0341 | 0.4933 | 0.5258 | 1.0821 | 0.4859 | 0.5345 | 1.1092 | 0.4819 |
39 | 0.5101 | 1.0341 | 0.4933 | 0.5258 | 1.0821 | 0.4859 | 0.5347 | 1.1096 | 0.4819 |
40 | 0.5101 | 1.0341 | 0.4933 | 0.5258 | 1.0821 | 0.4859 | 0.5348 | 1.1099 | 0.4819 |