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