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 | \(E_{\mathrm{max}_{I}}^{n}\) | 1.992E−2 | 5.794E−3 | 1.670E−3 | 4.801E−4 | 1.379E−4 | 3.961E−5 |
\(\text{rate}_{E_{\mathrm{max}_{I}}^{n}}\) | 1.782 | 1.795 | 1.798 | 1.800 | 1.800 | Â | |
\(E_{\mathrm{max}}^{n}\) | 5.719E−1 | 3.434E−1 | 1.894E−1 | 9.953E−2 | 5.104E−2 | 2.584E−2 | |
\(\text{rate}_{{E_{\mathrm{max}}^{n}}}\) | 0.736 | 0.859 | 0.928 | 0.964 | 0.982 | Â | |
\(\text{rate}_{E_{\mathrm{conv}}^{n}}\) | 0.921 | 0.981 | 0.994 | 1.004 | 1.005 | Â | |
β = 0.4 | \(E_{\mathrm{max}_{I}}^{n}\) | 3.875E−2 | 1.307E−2 | 4.346E−3 | 1.437E−3 | 4.745E−4 | 1.566E−4 |
\(\text{rate}_{E_{\mathrm{max}_{I}}^{n}}\) | 1.567 | 1.589 | 1.596 | 1.599 | 1.600 | Â | |
\(E_{\mathrm{max}}^{n}\) | 3.110E−1 | 1.691E−1 | 8.825E−2 | 4.511E−2 | 2.281E−2 | 1.147E−2 | |
\(\text{rate}_{{E_{\mathrm{max}}^{n}}}\) | 0.879 | 0.938 | 0.968 | 0.984 | 0.992 | Â | |
\(\text{rate}_{E_{\mathrm{conv}}^{n}}\) | 0.999 | 1.020 | 1.023 | 1.020 | 1.016 | Â | |
β = 0.6 | \(E_{\mathrm{max}_{I}}^{n}\) | 7.709E−2 | 3.042E−2 | 1.171E−2 | 4.465E−3 | 1.696E−3 | 6.432E−4 |
\(\text{rate}_{E_{\mathrm{max}_{I}}^{n}}\) | 1.341 | 1.377 | 1.391 | 1.397 | 1.399 | Â | |
\(E_{\mathrm{max}}^{n}\) | 1.927E−1 | 1.011E−1 | 5.184E−2 | 2.627E−2 | 1.323E−2 | 6.639E−3 | |
\(\text{rate}_{{E_{\mathrm{max}}^{n}}}\) | 0.930 | 0.963 | 0.981 | 0.990 | 0.995 | Â | |
\(\text{rate}_{E_{\mathrm{conv}}^{n}}\) | 1.024 | 1.037 | 1.038 | 1.034 | 1.030 | Â | |
β = 0.8 | \(E_{\mathrm{max}_{I}}^{n}\) | 1.551E−1 | 7.262E−2 | 3.268E−2 | 1.444E−2 | 6.326E−3 | 2.761E−3 |
\(\text{rate}_{E_{\mathrm{max}_{I}}^{n}}\) | 1.095 | 1.152 | 1.179 | 1.191 | 1.196 | Â | |
\(E_{\mathrm{max}}^{n}\) | 1.551E−1 | 7.262E−2 | 3.303E−2 | 1.668E−2 | 8.391E−3 | 4.210E−3 | |
\(\text{rate}_{{E_{\mathrm{max}}^{n}}}\) | 1.095 | 1.137 | 0.985 | 0.991 | 0.995 | Â | |
\(\text{rate}_{E_{\mathrm{conv}}^{n}}\) | 1.016 | 1.031 | 1.036 | 1.037 | 1.037 | Â |