Comparaison des résultats selon la méthode
avec les transformées de Fourier rapides (extension .col) et selon
la méthode normale (extension .dat). L'algorithme de Métropolis
est utilisé pour les spin-flip.
N | M | U | beta | mu | mu prop | remdes | Mes | Nwarm | Bl | CPU time | fichiers |
16 | 16 | 4.00 | 2.00 | 0.00 | 0.00 | 1.00 | 10 | 0 | 1 | 0.12E+03 | 391.sae410016162re.col
391.sae410016162gi.col |
16 | 16 | 4.00 | 2.00 | 0.00 | 0.00 | 1.00 | 10 | 0 | 1 | 0.29E+03 | 391.sae410016162re.dat
391.sae410016162gi.dat |
16 | 16 | 4.00 | 4.00 | 0.00 | 0.00 | 1.00 | 10 | 0 | 1 | 0.33E+03 | 415.sae410016164re.col
415.sae410016164gi.col |
16 | 16 | 4.00 | 4.00 | 0.00 | 0.00 | 1.00 | 10 | 0 | 1 | 0.54E+03 | 415.sae410016164re.dat
415.sae410016164gi.dat |
16 | 16 | 4.00 | 3.00 | 0.00 | 0.00 | 1.00 | 10 | 0 | 1 | 0.23E+03 | 416.sae410016163re.col
416.sae410016163gi.col |
16 | 16 | 4.00 | 3.00 | 0.00 | 0.00 | 1.00 | 10 | 0 | 1 | 0.38E+03 | 416.sae410016163re.dat
416.sae410016163gi.dat |
16 | 16 | 4.00 | 2.00 | 0.00 | 0.00 | 1.00 | 40 | 10 | 1 | 0.65E+03 | 417.sae410016162re.col
417.sae410016162gi.col |
16 | 16 | 4.00 | 2.00 | 0.00 | 0.00 | 1.00 | 40 | 10 | 1 | 0.25E+04 | 417.sae410016162re.dat
417.sae410016162gi.dat |
16 | 16 | 4.00 | 2.00 | 0.00 | 0.00 | 1.00 | 90 | 10 | 1 | 0.28E+04 | 418.sae410016162re.col
418.sae410016162gi.col |
16 | 16 | 4.00 | 2.00 | 0.00 | 0.00 | 1.00 | 40 | 10 | 1 | 0.36E+04 | 418.sae410016162re.dat
418.sae410016162gi.dat |
8 | 8 | 4.00 | 2.00 | 0.00 | 0.00 | 1.00 | 100 | 10 | 1 | 0.20E+02 | 420.sae4100882re.col
420.sae4100882gi.col |
8 | 8 | 4.00 | 2.00 | 0.00 | 0.00 | 1.00 | 100 | 10 | 1 | 0.19E+02 | 420.sae4100882re.dat
420.sae4100882gi.dat |
8 | 8 | 4.00 | 2.00 | 0.00 | 0.00 | 1.00 | 900 | 100 | 9 | 0.18E+03 | 421.sae4100882re.col
421.sae4100882gi.col |
8 | 8 | 4.00 | 2.00 | 0.00 | 0.00 | 1.00 | 900 | 100 | 9 | 0.17E+03 | 421.sae4100882re.dat
421.sae4100882gi.dat |
8 | 8 | 4.00 | 2.00 | 0.00 | 0.00 | 1.00 | 5000 | 1000 | 50 | 0.25E+04 | 419.sae4100882re.col
419.sae4100882gi.col |
8 | 8 | 4.00 | 2.00 | 0.00 | 0.00 | 1.00 | 5000 | 1000 | 50 | 0.24E+04 | 419.sae4100882re.dat
419.sae4100882gi.dat |
8 | 8 | 4.00 | 3.00 | 0.00 | 0.00 | 1.00 | 900 | 100 | 9 | 0.33E+03 | 422.sae4100883re.col
422.sae4100883gi.col |
8 | 8 | 4.00 | 3.00 | 0.00 | 0.00 | 1.00 | 900 | 100 | 9 | 0.30E+03 | 422.sae4100883re.dat
422.sae4100883gi.dat |
8 | 8 | 4.00 | 4.00 | 0.00 | 0.00 | 1.00 | 900 | 100 | 9 | 0.19E+04 | 423.sae4100884re.col
423.sae4100884gi.col |
8 | 8 | 4.00 | 4.00 | 0.00 | 0.00 | 1.00 | 900 | 100 | 9 | 0.19E+04 | 423.sae4100884re.dat
423.sae4100884gi.dat |