Abstract
When there is a distribution of bond strengths, the transport exponent depends on this distribution.1–4 A distribution of bond strengths arises in the “Swiss cheese” models,2 where circular or spherical holes are randomly placed in a uniform transport medium. For example, in the 2D case a bond is present if two neighboring holes (radius α) do not overlap.
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References
P. N. Sen, J. N. Roberts B. I. Halperin (unpublished).
H. I. Halperin, S. Feng, P. N. Sen, Phys. Rev. Lett. 54, 2391 (1985).
P. M. Kogut, J. P. Straley, J. Phys. C 12, 2151 (1979).
A. Ben-Mizrahi, D. J. Bergman, J. Phys. C 14, 909 (1981).
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© 1986 Martinus Nijhoff Publishers,Dordrecht
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Sen, P.N., Roberts, J.N., Halperin, B.I. (1986). Non-Universal Critical Exponents for Transport in Percolating Systems. In: Stanley, H.E., Ostrowsky, N. (eds) On Growth and Form. NATO ASI Series, vol 100. Springer, Dordrecht. https://doi.org/10.1007/978-94-009-5165-5_28
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DOI: https://doi.org/10.1007/978-94-009-5165-5_28
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