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Abstract be a configuration of$$\textbf{p}$$ $p$n points in for some$$\mathbb R^d$$ ${R}^{d}$n and some . Each pair of points defines an edge, which has a Euclidean length in the configuration. A path is an ordered sequence of the points, and a loop is a path that begins and ends at the same point. A path or loop, as a sequence of edges, also has a Euclidean length, which is simply the sum of its Euclidean edge lengths. We are interested in reconstructing$$d \ge 2$$ $d\ge 2$ given a set of edge, path and loop lengths. In particular, we consider the unlabeled setting where the lengths are given simply as a set of real numbers, and are not labeled with the combinatorial data describing which paths or loops gave rise to these lengths. In this paper, we study the question of when$$\textbf{p}$$ $p$ will be uniquely determined (up to an unknowable Euclidean transform) from some given set of path or loop lengths through an exhaustive trilateration process. Such a process has already been used for the simpler problem of reconstruction using unlabeled edge lengths. This paper also provides a complete proof that this process must work in that edgesetting when given a sufficiently rich set of edge measurements and assuming that$$\textbf{p}$$ $p$ is generic.$$\textbf{p}$$ $p$ 
We consider the zeroenergy deformations of periodic origami sheets with generic crease patterns. Using a mapping from the linear folding motions of such sheets to forcebearing modes in conjunction with the Maxwell–Calladine index theorem we derive a relation between the number of linear folding motions and the number of rigid body modes that depends only on the average coordination number of the origami’s vertices. This supports the recent result by Tachi [T. Tachi,
Origami 6, 97–108 (2015)] which shows periodic origami sheets with triangular faces exhibit twodimensional spaces of rigidly foldable cylindrical configurations. We also find, through analytical calculation and numerical simulation, branching of this configuration space from the flat state due to geometric compatibility constraints that prohibit finite Gaussian curvature. The same counting argument leads to pairing of spatially varying modes at opposite wavenumber in triangulated origami, preventing topological polarization but permitting a family of zeroenergy deformations in the bulk that may be used to reconfigure the origami sheet.