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Complex networks embedded in space: Dimension and scaling relations between mass, topological distance and Euclidean distance

Published 25 Jun 2012 in physics.soc-ph and cs.SI | (1206.5710v2)

Abstract: Many real networks are embedded in space, where in some of them the links length decay as a power law distribution with distance. Indications that such systems can be characterized by the concept of dimension were found recently. Here, we present further support for this claim, based on extensive numerical simulations for model networks embedded on lattices of dimensions de=1d_e=1 and de=2d_e=2. We evaluate the dimension dd from the power law scaling of (a) the mass of the network with the Euclidean radius rr and (b) the probability of return to the origin with the distance rr travelled by the random walker. Both approaches yield the same dimension. For networks with $\delta &lt; d_e$, dd is infinity, while for $\delta &gt; 2d_e$, dd obtains the value of the embedding dimension ded_e. In the intermediate regime of interest $d_e \leq \delta &lt; 2 d_e$, our numerical results suggest that dd decreases continously from d=∞d = \infty to ded_e, with d−de∼(δ−de)<sup>−1d - d_e \sim (\delta - d_e)<sup>{-1} for δ\delta close to ded_e. Finally, we discuss the scaling of the mass MM and the Euclidean distance rr with the topological distance ℓ\ell. Our results suggest that in the intermediate regime $d_e \leq \delta &lt; 2 d_e$, M(ℓ)M(\ell) and r(ℓ)r(\ell) do not increase with ℓ\ell as a power law but with a stretched exponential, $M(\ell) \sim \exp [A \ell<sup>{\delta&#39;</sup> (2 - \delta&#39;)}]$ and $r(\ell) \sim \exp [B \ell<sup>{\delta&#39;</sup> (2 - \delta&#39;)}]$, where $\delta&#39; = \delta/d_e$. The parameters AA and BB are related to dd by d=A/Bd = A/B, such that M(ℓ)∼r(ℓ)<sup>dM(\ell) \sim r(\ell)<sup>d. For $\delta &lt; d_e$, MM increases exponentially with ℓ\ell, as known for δ=0\delta=0, while rr is constant and independent of ℓ\ell. For δ≥2de\delta \geq 2d_e, we find power law scaling, M(ℓ)∼ℓ<sup>dℓM(\ell) \sim \ell<sup>{d_\ell} and r(ℓ)∼ℓ<sup>1/dminr(\ell) \sim \ell<sup>{1/d_{min}}, with dℓ⋅dmin=dd_\ell \cdot d_{min} = d.

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