We study the critical behavior, in a mean-field approximation, of a grand-canonical ensemble of nonplanar self-avoiding random surfaces (SAS's) which arises as an n{→}0 limit of a gauge-invariant theory. We show explicitly that our model is equivalent to the usual φ⁴ theory near the critical point, with the upper critical dimension equal to 4. The fractal dimension of SAS is 2.
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P. D. Gujrati (1989) studied this question.
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