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The electric polarizability and the spread of the total position tensors are used to characterize the metallic vs insulator nature of large (finite) systems. Finite clusters are usually treated within the open boundary condition formalism. This introduces border effects, which prevents a fast convergence to the thermodynamic limit and which can be eliminated within the formalism of periodic boundary conditions. Recently, we have introduced an original approach to periodic boundary conditions, named Clifford Boundary Conditions. It considers a finite fragment extracted from a periodic system and the modification of its topology into that of a Clifford Torus. The quantity representing the position is modified in order to fulfill the system periodicity. In this work, we apply the formalism of Clifford Boundary Conditions to the case of Carbon Nanotubes, whose treatment results to be particularly simple for the Zigzag geometry. Indeed, we demonstrate that at the H\"uckel level these nanotubes, either finite or periodic, are formally equivalent to a collection of {\em non-interacting dimerized linear chains}, thus simplifying their treatment. This equivalence is used to describe some nanotube properties as the sum of the contributions of the independent chains and to identify the origin of peculiar behaviors (such as the conductivity). Indeed, if the number of hexagons along the circumference is a multiple of three a metallic behavior is found, namely a divergence of both the (per electron) polarizability and total position spread of at least one linear chain. These results are in agreement with those in the literature from Tight-Binding calculations.

approaches. We demonstrate that the Wigner regime can be reached using small values of the confinement parameter. To obtain physical insight in our results we analyze them with a semi-analytical model for two electrons. Thanks to electronic-structure properties such as the one-body density and the particle-hole entropy, we are able to define a path that connects the Wigner regime to the Fermi-gas regime by varying the confinement parameter. In particular, we show that the particle-hole entropy as a function of the confinement parameter smoothly connects the two regimes. Moreover, it exhibits a maximum that could be interpreted as the transition point between the localized and delocalized regimes.