- Figure: The probability P(x) and the test function f(x) for various algorithms.
FLA=Fast Linear Algorithm
Cr =Creutz
Me =Metropolis
P2=P(x) with h=2
|
|
- Figure: comparison of the time of simulation for various algorithms
for the stacked triangular antiferromagnetic lattices.
The critical temperature is shown by the squares
- FLA=Fast Linear Algorithm
- Cr =Creutz
- Fa =Fabricius
- Ke =Kennedy
- MeG =Metropolis standard using 4 Gaussian random numbers.
- MeS =Metropolis, the first angle, sin2(theta)is chosen from
a sinus distribution and the rejection method
- Med =like MeS but the first angle is constrained
to be around the old spin (0 < first angle < d).
|
|
- Figure: comparison of the rate of simulation for various algorithms
for the stacked triangular antiferromagnetic lattices.
The critical temperature is shown by the squares
- FLA=Fast Linear Algorithm
- Cr =Creutz
- Fa =Fabricius
- Ke =Kennedy
- Me =Metropolis .
- Med = Metropolis but the first angle is constrained
to be around the old spin (0 < first angle < d).
|
|