- Figure: comparison of the autocorrelation time for various algorithms
for the two dimensional ferromagnetic square lattices (2c). q=3, L=20
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
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- Figure: comparison of the time of simulation for various algorithms
for the two dimensional ferromagnetic square lattices (2c) and the three
dimensional antiferromagnetic cubic lattice (3c), q=3, L=20
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
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- Figure: comparison of the rate of simulation for various algorithms
for the ferromagnetic square lattices (2c) and the three
dimensional antiferromagnetic cubic lattice (3c). q=3, L=20
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
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- Figure: comparison of the time consumption at the critical temperature
as function of the lattice size for various algorithms
for the ferromagnetic square lattices (2c). q=3
- 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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- Figure: comparison of the time consumption at the critical temperature
as function of the number of state q for various algorithms
for the ferromagnetic square lattices (2c). L=20
- 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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