Theory and Modern Applications
\(r = \frac{2-\beta }{\beta }\) | n = 32 | n = 64 | n = 128 | n = 256 | n = 512 | n = 1028 | |
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β = 0.2 | \(E_{\mathrm{max}_{I}}^{n}\) | 2.479E−2 | 7.233E−3 | 2.087E−3 | 6.000E−4 | 1.724E−4 | 4.951E−5 |
\(\text{rate}_{{E_{\mathrm{max}_{I}}^{n}}}\) | 1.777 | 1.793 | 1.798 | 1.799 | 1.800 | Â | |
\(E_{\mathrm{max}}^{n}\) | 5.647E−1 | 3.356E−1 | 1.823E−1 | 9.430E−2 | 4.748E−2 | 2.354E−2 | |
\(\text{rate}_{E_{\mathrm{max}}^{n}}\) | 0.751 | 0.880 | 0.951 | 0.990 | 1.012 | Â | |
\(\text{rate}_{E_{\mathrm{conv}}^{n}}\) | 0.700 | 0.746 | 0.767 | 0.777 | 0.783 | Â | |
β = 0.4 | \(E_{\mathrm{max}_{I}}^{n}\) | 6.318E−2 | 2.163E−2 | 7.225E−3 | 2.393E−3 | 7.906E−4 | 2.609E−4 |
\(\text{rate}_{E_{\mathrm{max}_{I}}^{n}}\) | 1.547 | 1.582 | 1.594 | 1.598 | 1.599 | Â | |
\(E_{\mathrm{max}}^{n}\) | 2.863E−1 | 1.468E−1 | 7.060E−2 | 3.209E−2 | 1.358E−2 | 5.086E−3 | |
\(\text{rate}_{{E_{\mathrm{max}}^{n}}}\) | 0.964 | 1.056 | 1.138 | 1.240 | 1.417 | Â | |
\(\text{rate}_{E_{\mathrm{conv}}^{n}}\) | 0.565 | 0.581 | 0.589 | 0.593 | 0.596 | Â | |
β = 0.6 | \(E_{\mathrm{max}_{I}}^{n}\) | 1.758E−1 | 7.328E−2 | 2.886E−2 | 1.110E−2 | 4.231E−3 | 1.607E−3 |
\(\text{rate}_{E_{\mathrm{max}_{I}}^{n}}\) | 1.263 | 1.344 | 1.378 | 1.392 | 1.397 | Â | |
\(E_{\mathrm{max}}^{n}\) | 1.758E−1 | 7.328E−2 | 2.886E−2 | 1.110E−2 | 1.225E−2 | 1.296E−2 | |
\(\text{rate}_{{E_{\mathrm{max}}^{n}}}\) | 1.263 | 1.344 | 1.378 | -0.142 | -0.082 | Â | |
\(\text{rate}_{E_{\mathrm{conv}}^{n}}\) | 0.398 | 0.405 | 0.407 | 0.407 | 0.406 | Â | |
β = 0.8 | \(E_{\mathrm{max}_{I}}^{n}\) | 5.185E−1 | 2.947E−1 | 1.479E−1 | 6.900E−2 | 3.100E−2 | 1.369E−2 |
\(\text{rate}_{E_{\mathrm{max}_{I}}^{n}}\) | 0.815 | 0.994 | 1.100 | 1.154 | 1.180 | Â | |
\(E_{\mathrm{max}}^{n}\) | 5.185E−1 | 2.947E−1 | 1.479E−1 | 7.440E−2 | 7.131E−2 | 6.516E−2 | |
\(\text{rate}_{{E_{\mathrm{max}}^{n}}}\) | 0.815 | 0.994 | 0.992 | 0.061 | 0.130 | Â | |
\(\text{rate}_{E_{\mathrm{conv}}^{n}}\) | 0.214 | 0.217 | 0.218 | 0.216 | 0.215 | Â |