Optimal spanners for axis-aligned rectangles

The dilation of a geometric graph is the maximum, over all pairs of points in the graph, of the ratio of the Euclidean length of the shortest path between them in the graph and their Euclidean distance. We consider a generalized version of this notion, where the nodes of the graph are not points but axis-parallel rectangles in the plane. The arcs in the graph are horizontal or vertical segments connecting a pair of rectangles, and the distance measure we use is the $L_1$-distance. The dilation of a pair of points is then defined as the length of the shortest rectilinear path between them that stays within the union of the rectangles and the connecting segments, divided by their $L_1$-distance. The dilation of the graph is the maximum dilation over all pairs of points in the union of the rectangles.We study the following problem: given n non-intersecting rectangles and a graph describing which pairs of rectangles are to be connected, we wish to place the connecting segments such that the dilation is minimized. We obtain four results on this problem: (i) for arbitrary graphs, the problem is NP-hard; (ii) for trees, we can solve the problem by linear programming on $\mathrm{O}(n^2)$ variables and constraints; (iii) for paths, we can solve the problem in time $\mathrm{O}(n^3\log n)$; (iv) for rectangles sorted vertically along a path, the problem can be solved in $\mathrm{O}(n^2)$ time, and a $(1+\varepsilon )$-approximation can be computed in linear time.     

Spectral stiff problems in domains surrounded by thin bands: Asymptotic and uniform estimates for eigenvalues

We consider an asymptotic spectral problem for a second order differential operator, with piecewise constants coefficients, in a two-dimensional domain ${\Omega }_{\varepsilon }$. Here ${\Omega }_{\varepsilon }$ is ${\Omega }_{\varepsilon }=\Omega \cup {\omega }_{\varepsilon }\cup \Gamma$, where Ω is a fixed open bounded domain with boundary Γ, ${\omega }_{\varepsilon }$ is a curvilinear strip of variable width $\mathrm{O}(\varepsilon )$, and $\Gamma =\overline{\Omega }\cap {\overline{\omega }}_{\varepsilon }$. The density and stiffness constants are of order $\mathrm{O}({\varepsilon }^{-m-t})$ and $\mathrm{O}({\varepsilon }^{-t})$ respectively in this strip, while they are of order $\mathrm{O}(1)$ in the fixed domain Ω; t and $t+m$ are positive parameters and $\varepsilon \in (0,1)$. Imposing the Neumann condition on the boundary of ${\Omega }_{\varepsilon }$, for $t⩾0$ and $m⩾-t$ we provide asymptotics for the eigenvalues and eigenfunctions as $\varepsilon \to 0$. We obtain sharp estimates of convergence rates for the eigenpairs in the case where $t=1$ and $m=0$, which can, in fact, be extended to other cases.