General Ising S Spins (Blume Capel model)

Probabilities and Performances :

Figure: comparison of the autocorrelation time for various algorithms for the two dimensional ferromagnetic square lattices (2c). S=1, D=0, L=10 The critical temperatures are shown by the squares AW=Alias Walker AWHd=Restricted Alias Walker Hasting DHB=Direct Heat-Bath DHBd=Restricted Direct Heat-Bath Me  =Metropolis Med  = Restricted Metropolis
Figure: comparison of the time of simulation for various algorithms for the two dimensional ferromagnetic square lattices (2c), S=1, D=0, L=10 The critical temperatures are shown by the squares AW=Alias Walker AWHd=Restricted Alias Walker Hasting DHB=Direct Heat-Bath DHBd=Restricted Direct Heat-Bath Me  =Metropolis Med  = Restricted Metropolis
Figure: comparison of the rate of simulation for various algorithms for the ferromagnetic square lattices (2c). S=1, D=0, L=10 The critical temperatures are shown by the squares AW=Alias Walker AWHd=Restricted Alias Walker Hasting DHB=Direct Heat-Bath DHBd=Restricted Direct Heat-Bath Me  =Metropolis Med  = Restricted Metropolis
Figure: comparison of the time consumption at the critical temperature as function of D for various algorithms for the ferromagnetic square lattices (2c). S=1, L=10 AW=Alias Walker AWHd=Restricted Alias Walker Hasting DHB=Direct Heat-Bath DHBd=Restricted Direct Heat-Bath Me  =Metropolis Med  = Restricted Metropolis
Figure: comparison of the time consumption at the critical temperature as function of S for various algorithms for the ferromagnetic square lattices (2c). D=0, L=10 AW=Alias Walker AWHd=Restricted Alias Walker Hasting DHB=Direct Heat-Bath DHBd=Restricted Direct Heat-Bath Me  =Metropolis Med  = Restricted Metropolis

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