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DETErmine_bath n :

This flag starts n identical copies of a procedure aiming to determine a suitable temperature (or temperature range) for all four annealing modes. This we do as follows : the temperature is set to a sufficiently remote (very high) value20of T0 = 0.6250. The system is equilibrated at this temperature for $ \Delta$t=10000 time steps and the mean value of the resulting R-factors (say, $ \bar{R}_{0}^{}$) is saved. Then the temperature is set to T1 = T0/2 = 0.31250 and the procedure repeated up to and including T13 = 0.0000763 which will give us $ \bar{R}_{{13}}^{}$. For every pair of average R-factors $ \bar{R}_{n}^{}$, $ \bar{R}_{{n+1}}^{}$, we calculate $ \Delta$$ \bar{R}_{n}^{}$ = $ \bar{R}_{n}^{}$ - $ \bar{R}_{{n+1}}^{}$ and then we do a cubic spline interpolation on the resulting $ \Delta$$ \bar{R}_{n}^{}$'s and from that we determine the temperature T0 for which $ \Delta$$ \bar{R}$ is maximum21. A graphical representation of the results from this calculation are written in the file temp.ps (a postscript file, only produced when the keyword POSTSCRIPT is on).



Footnotes

... value20
The probability of accepting a move against the gradient is exp(- |$ \Delta$R|/T). Now, |$ \Delta$R| is the absolute value of the difference between two values of the conventional R factor and, so, takes values of the order of 10-1. For, say, T = 10, the probability of accepting a move against the gradient is 0.990, ie practically all moves are accepted and so the system is thermally disordered.
... maximum21
The quantity $ \Delta$$ \bar{R}$/$ \Delta$T is analogous to the specific heat from statistical mechanics. A large value of $ \Delta$$ \bar{R}$/$ \Delta$T signifies that a ``phase'' transition is occurring at the corresponding temperature, and so the cooling rate should be as low as possible at this temperature range.

next up previous contents
Next: CONStant : Up: GROUP 3 : Annealing Previous: FINAl_temp T :   Contents
NMG, January 2005