TY - JOUR
T1 - First exit time of termites and random super-normal conductor networks
AU - Adler, J.
AU - Aharony, A.
AU - Stauffer, D.
PY - 1985
Y1 - 1985
N2 - The resistance of a random super-normal conductor network is calculated through the diffusion of a 'termite', which performs a random walk on the normal bonds and has the same probability to exist from any point on a cluster of superconducting bonds. The first time, T, that the termite exits at a distance r from the origin (averaged over many configurations and runs) is found to behave as T approximately r2k/ for r<< xi ( xi is the percolation correlation length) and as T approximately r2(pc-p) s for r>> xi (( pc-p)-s describes the divergence of the conductivity as p to pc-, p being the concentration of the superconductor). Scaling arguments are used to show that k=1+s/(2+ theta ), where (2+ theta ) is the fractal dimension of random walks on single clusters at pc. Numerical simulations at two dimensions (d=2) yields s=1.34+or-0.10 and k=1.34+or-0.03, in agreement with scaling. The authors also show that the probability of return to the origin at time t behaves as t-dk2/. Preliminary results at d=1 and other calculations methods are also discussed.
AB - The resistance of a random super-normal conductor network is calculated through the diffusion of a 'termite', which performs a random walk on the normal bonds and has the same probability to exist from any point on a cluster of superconducting bonds. The first time, T, that the termite exits at a distance r from the origin (averaged over many configurations and runs) is found to behave as T approximately r2k/ for r<< xi ( xi is the percolation correlation length) and as T approximately r2(pc-p) s for r>> xi (( pc-p)-s describes the divergence of the conductivity as p to pc-, p being the concentration of the superconductor). Scaling arguments are used to show that k=1+s/(2+ theta ), where (2+ theta ) is the fractal dimension of random walks on single clusters at pc. Numerical simulations at two dimensions (d=2) yields s=1.34+or-0.10 and k=1.34+or-0.03, in agreement with scaling. The authors also show that the probability of return to the origin at time t behaves as t-dk2/. Preliminary results at d=1 and other calculations methods are also discussed.
UR - https://www.scopus.com/pages/publications/18144365065
U2 - 10.1088/0305-4470/18/3/006
DO - 10.1088/0305-4470/18/3/006
M3 - ???researchoutput.researchoutputtypes.contributiontojournal.article???
AN - SCOPUS:18144365065
SN - 0305-4470
VL - 18
SP - L129-L136
JO - Journal of Physics A: Mathematical and General
JF - Journal of Physics A: Mathematical and General
IS - 3
M1 - 006
ER -