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 | \(E_{\mathrm{max}_{I}}^{n}\) | 2.204E−2 | 6.439E−3 | 1.858E−3 | 5.344E−4 | 1.535E−4 | 4.410E−5 |
\(\text{rate}_{E_{\mathrm{max}_{I}}^{n}}\) | 1.775 | 1.793 | 1.798 | 1.799 | 1.800 | Â | |
\(E_{\mathrm{max}}^{n}\) | 4.902E−2 | 2.435E−2 | 1.203E−2 | 5.917E−3 | 2.899E−3 | 1.413E−3 | |
\(\text{rate}_{{E_{\mathrm{max}}^{n}}}\) | 1.009 | 1.017 | 1.024 | 1.030 | 1.036 | Â | |
\(\text{rate}_{E_{\mathrm{conv}}^{n}}\) | 0.638 | 0.659 | 0.681 | 0.700 | 0.716 | Â | |
β = 0.4 | \(E_{\mathrm{max}_{I}}^{n}\) | 5.527E−2 | 1.897E−2 | 6.342E−3 | 2.101E−3 | 6.943E−4 | 2.291E−4 |
\(\text{rate}_{E_{\mathrm{max}_{I}}^{n}}\) | 1.543 | 1.581 | 1.594 | 1.598 | 1.599 | Â | |
\(E_{\mathrm{max}}^{n}\) | 5.527E−2 | 1.897E−2 | 8.380E−3 | 3.611E−3 | 1.421E−3 | 1.058E−3 | |
\(\text{rate}_{{E_{\mathrm{max}}^{n}}}\) | 1.543 | 1.179 | 1.214 | 1.346 | 0.426 | Â | |
\(\text{rate}_{E_{\mathrm{conv}}^{n}}\) | 0.523 | 0.539 | 0.553 | 0.564 | 0.573 | Â | |
β = 0.6 | \(E_{\mathrm{max}_{I}}^{n}\) | 1.515E−1 | 6.342E−2 | 2.502E−2 | 9.630E−3 | 3.671E−3 | 1.394E−3 |
\(\text{rate}_{E_{\mathrm{max}_{I}}^{n}}\) | 1.256 | 1.342 | 1.377 | 1.391 | 1.397 | Â | |
\(E_{\mathrm{max}}^{n}\) | 1.515E−1 | 6.342E−2 | 2.502E−2 | 9.630E−3 | 6.739E−3 | 5.411E−3 | |
\(\text{rate}_{{E_{\mathrm{max}}^{n}}}\) | 1.256 | 1.342 | 1.377 | 0.515 | 0.317 | Â | |
\(\text{rate}_{E_{\mathrm{conv}}^{n}}\) | 0.375 | 0.383 | 0.389 | 0.393 | 0.395 | Â | |
β = 0.8 | \(E_{\mathrm{max}_{I}}^{n}\) | 4.380E−1 | 2.510E−1 | 1.265E−1 | 5.908E−2 | 2.656E−2 | 1.173E−2 |
\(\text{rate}_{E_{\mathrm{max}_{I}}^{n}}\) | 0.803 | 0.989 | 1.098 | 1.153 | 1.179 | Â | |
\(E_{\mathrm{max}}^{n}\) | 4.380E−1 | 2.510E−1 | 1.265E−1 | 5.908E−2 | 2.697E−2 | 2.394E−2 | |
\(\text{rate}_{{E_{\mathrm{max}}^{n}}}\) | 0.803 | 0.989 | 1.098 | 1.131 | 0.172 | Â | |
\(\text{rate}_{E_{\mathrm{conv}}^{n}}\) | 0.199 | 0.202 | 0.203 | 0.204 | 0.204 | Â |