Octobor 17 2002


Cooling of 201 and 603 atoms respectively

Both carved-out sphere systems went through constant temperature MD at 1000K. A million steps (4.3ns) for 201 atoms and half a million (2.15ns) for 603 atoms. After that, the systems went through Andersen Thermostat with the sampling rate of 0.01*dt. The systems were equilibrated at a certain temperature level for a certain time, then cooled down to a lower temperature level. The temperature levels of 1000K, 900K, 800K, 700K, 600K, 500K, 400K, 300K, 200K and 100K were performed. At each temperature level, the system of 201 atoms was equilibrated for ten million steps (43ns) and that of 603 atoms was five million steps (21.5ns).


 

Parallel tempering of 201 atoms

The same Andersen thermostat program was modified to run parallel with parallel tempering algorithm. The system configurations at different temperature levels were trying to swap the configurations according to the swapping rule of
acc(o->n) = min ( 1, exp[(1/kTi - 1/kTj) * (ui - uj)] )
Where T is the system temperature and u is the system total potential energy.

For the system of 201 atoms, ten million steps (43ns) were perfromed for the temperature levels of 200K, 233K, 267K, 300K, 350K, 400K, 450K, 500K, 550K, 600K, 650K, 700K, 750K, 800K, 900K and 1000K. The initial configurations were taken from the results of cooling. The acceptance probabilites of swapping were:

temperature levels
acceptance probabilities (%)
200K -- 233K
3.776
233K -- 267K
6.562
267K -- 300K
12.366
300K -- 350K
4.376
350K -- 400K
5.599
400K -- 450K
8.808
450K -- 500K
10.205
500K -- 550K
12.376
550K -- 600K
15.682
600K -- 650K
 19.319
650K -- 700K
22.879
700K -- 750K
27.279
750K -- 800K
32.425
800K -- 900K
9.648
900K -- 1000K
12.881

The positions of the initial configurations were also tracked. The tracks of the initial configurations of 200K and 500K are shown as examples:

The picture shows that the configurations were really brought up and down the temperature levels.