We compare two implementations of a new algorithm called the pivot met
hod for the location of the global minimum of a multiple minima proble
m. The pivot method uses a series of randomly placed probes in phase s
pace, moving the worst probes to be near better probes iteratively unt
il the system converges. The original implementation, called the ''low
est energy pivot method,'' chooses the pivot probes with a probability
based on the energy of the probe. The second approach, called the ''n
earest neighbor pivot method,'' chooses the pivot probes to be the nea
rest neighbor points in the phase space. We examine the choice of dist
ribution by comparing the efficiency of the methods for Gaussian versu
s generalized q-distribution, based on the Tsallis entropy in the relo
cation of the probes. The two implementations of the method are tested
with a series of test functions and with several Lennard-Jones cluste
rs of various sizes. It appears that the nearest neighbor pivot method
using the generalized q-distribution is superior to previous methods.
(C) 1997 American Institute of Physics.