# Physica A: Statistical Mechanics and its Applications

Physica A: Statistical Mechanics and its Applications > 1994 > 212 > 1-2 > 110-117

Physica A: Statistical Mechanics and its Applications > 1994 > 212 > 1-2 > 194-229

Physica A: Statistical Mechanics and its Applications > 1994 > 212 > 1-2 > 118-122

Physica A: Statistical Mechanics and its Applications > 1994 > 212 > 1-2 > 75-98

Physica A: Statistical Mechanics and its Applications > 1994 > 212 > 1-2 > 26-42

Physica A: Statistical Mechanics and its Applications > 1994 > 212 > 1-2 > 12-25

_{s}. A suitable transfer matrix approach allows to discuss adsorption isotherms, as well as geometrical and thermal fluctuations of the interface. For ζ

_{s}12 the same wetting exponent ψ = 13 as for flat substrate is obtained for the...

Physica A: Statistical Mechanics and its Applications > 1994 > 212 > 1-2 > 175-180

Physica A: Statistical Mechanics and its Applications > 1994 > 212 > 1-2 > 43-60

Physica A: Statistical Mechanics and its Applications > 1994 > 212 > 1-2 > 61-74

^{2}. The chaotic force f(t) is defined by f(t) = (y

_{n}

_{+}

_{1}- y )τ for nτ < t ≤ (n + 1)τ (n = 0, 1, 2, ), where y

_{n}

_{+}

_{1}is a chaotic sequence: y

_{n}

_{+}

_{1}= F (y ...

Physica A: Statistical Mechanics and its Applications > 1994 > 212 > 1-2 > 99-109

Physica A: Statistical Mechanics and its Applications > 1994 > 212 > 1-2 > 132-142

Physica A: Statistical Mechanics and its Applications > 1994 > 212 > 1-2 > 123-131

Physica A: Statistical Mechanics and its Applications > 1994 > 212 > 1-2 > 143-174

_{2}(N)-superconductors with N = 1,2, and 3 CuO

_{2}layers per molecular unit, and with chemical composition HgBa

_{2}Ca

_{N}

_{-}

_{1}Cu

_{N}O

_{2}

_{N}

_{+}

_{2}

_{+}

_{δ}and Tl

_{2}Ba

_{2}Ca

_{N}...

Physica A: Statistical Mechanics and its Applications > 1994 > 212 > 1-2 > 1-11

Physica A: Statistical Mechanics and its Applications > 1994 > 212 > 1-2 > 181-193

Physica A: Statistical Mechanics and its Applications > 1994 > 212 > 3-4 > 239-250

Physica A: Statistical Mechanics and its Applications > 1994 > 212 > 3-4 > 251-260

_{e}

_{f}

_{f}= 53 of the network backbone (without caustic singularities) and a turbulence intermittency exponent μ = 16. If there are singularities on these caustic networks then D...

Physica A: Statistical Mechanics and its Applications > 1994 > 212 > 3-4 > 308-313

Physica A: Statistical Mechanics and its Applications > 1994 > 212 > 3-4 > 277-298

Physica A: Statistical Mechanics and its Applications > 1994 > 212 > 3-4 > 369-381