- 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).
			
  
		  
	 | 
	
		 
	 |