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Foundations of Data Science

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y<br />

7<br />

3<br />

1<br />

1 3 7<br />

x<br />

Figure 5.10: Paths in a 2-dimensional lattice obtained from the 3-dimensional construction<br />

applied in 2-dimensions.<br />

dimensional example is<br />

1<br />

2 + 1 4 2 + 1 8 4 + · · · = 1 2 + 1 2 + 1 2 + · · · = ∞.<br />

In the analogous three dimensional construction, paths go up, to the right, and out <strong>of</strong><br />

the plane <strong>of</strong> the paper. The paths split three ways at planes given by x + y + z = 2 n − 1.<br />

Each time the paths split the number <strong>of</strong> parallel segments triple. Segments <strong>of</strong> the paths<br />

between splits are <strong>of</strong> length 1, 2, 4, etc. and the resistance <strong>of</strong> the segments are equal to<br />

the lengths. The resistance out to infinity for the tree is<br />

1<br />

3 + 1 9 2 + 1<br />

27 4 + · · · = 1 3<br />

(<br />

1 +<br />

2<br />

+ 4 + · · ·) = 1 3 9 3<br />

1<br />

1− 2 3<br />

= 1<br />

The resistance <strong>of</strong> the three dimensional lattice is less. It is important to check that the<br />

paths are edge-disjoint and so the tree is a subgraph <strong>of</strong> the lattice. Going to a subgraph is<br />

equivalent to deleting edges which only increases the resistance. That is why the resistance<br />

174

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