2001
DOI: 10.1063/1.1338506
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Precise determination of the critical percolation threshold for the three-dimensional “Swiss cheese” model using a growth algorithm

Abstract: Precise values for the critical threshold for the three-dimensional ''Swiss cheese'' continuum percolation model have been calculated using extensive Monte Carlo simulations. These simulations used a growth algorithm and memory blocking scheme similar to what we used previously in three-dimensional lattice percolation. The simulations yield a value for the critical number density n c ϭ0.652 960Ϯ0.000 005, which confirms recent work but extends the precision by two significant figures.

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Cited by 197 publications
(165 citation statements)
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“…These include the pore-size functions (the distribution of the distance from a randomly chosen location in the void phase to the closest phase boundary), 46 the quantizer error (a moment of the poresize function, which is related to the principal relaxation time), 32,46 the order metric τ (a measure of the translational order of point configurations), 18 and the percolation threshold or the critical radius (the radius of the spheres at which a specific phase becomes connected) of each phase. [47][48][49][50] We compare the aforementioned physical and geometrical properties of our two-phase system derived from decorated stealthy ground states, as a function of the tuning parameter χ, with those of two other two-phase media: (1) equilibrium disordered (fluid) hard-sphere systems and (2) decorated Poisson point processes (idealgas configurations). The former has short-range order that is tunable by its volume fraction but no long-range order.…”
Section: -45mentioning
confidence: 99%
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“…These include the pore-size functions (the distribution of the distance from a randomly chosen location in the void phase to the closest phase boundary), 46 the quantizer error (a moment of the poresize function, which is related to the principal relaxation time), 32,46 the order metric τ (a measure of the translational order of point configurations), 18 and the percolation threshold or the critical radius (the radius of the spheres at which a specific phase becomes connected) of each phase. [47][48][49][50] We compare the aforementioned physical and geometrical properties of our two-phase system derived from decorated stealthy ground states, as a function of the tuning parameter χ, with those of two other two-phase media: (1) equilibrium disordered (fluid) hard-sphere systems and (2) decorated Poisson point processes (idealgas configurations). The former has short-range order that is tunable by its volume fraction but no long-range order.…”
Section: -45mentioning
confidence: 99%
“…For example, to accurately determine the percolation threshold of 3D fully penetrable spheres, Ref. 48 employed systems of up to N = 7 × 10 8 particles. The whole system is divided into smaller cubes and the content particles in each cube is generated only when such cube is being probed.…”
Section: E Calculating Percolation Thresholdsmentioning
confidence: 99%
“…H o w e v e r , w e n e e d t o t h e p e r c o l a t i o n threshold as it depends on the details of the system. Examples of applying percolation theory to uncorrelated (or even correlated) continuum systems that check the universality and determination of the percolation threshold of different models can be found elsewhere [Gawlinski and Stanley, 1981;Lee and Torquato., 1990;King, 1990;Berkowitz, 1995;Lorenz and Ziff, 2001;Baker et al, 2002].…”
Section: Percolation Theorymentioning
confidence: 99%
“…The value η c for which the transition occurs is known from numerical experiments to be η c = 0.34189(2) [40] and η c = 0.341888(3) [41] which is to date the most precise estimate of the critical filling.…”
Section: B Continuum Modelmentioning
confidence: 99%