Abstract
The authors estimate the exponents characterising the self-avoiding surfaces using an approximation in the framework of a Flory-type theory. They find for planar self-avoiding surfaces embedded randomly in a fractal of dimensionality D': nu =3/(4+D'); for random surfaces of fractal dimension D embedded in a Euclidean space of dimensionality d: nu =3/(2D+d-2); and for fractal surfaces embedded in a structure of fractal dimensionality D': nu =3/(2D+D'-2).
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