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    Computing Teichm\"{u}ller Maps between Polygons

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    By the Riemann-mapping theorem, one can bijectively map the interior of an nn-gon PP to that of another nn-gon QQ conformally. However, (the boundary extension of) this mapping need not necessarily map the vertices of PP to those QQ. In this case, one wants to find the ``best" mapping between these polygons, i.e., one that minimizes the maximum angle distortion (the dilatation) over \textit{all} points in PP. From complex analysis such maps are known to exist and are unique. They are called extremal quasiconformal maps, or Teichm\"{u}ller maps. Although there are many efficient ways to compute or approximate conformal maps, there is currently no such algorithm for extremal quasiconformal maps. This paper studies the problem of computing extremal quasiconformal maps both in the continuous and discrete settings. We provide the first constructive method to obtain the extremal quasiconformal map in the continuous setting. Our construction is via an iterative procedure that is proven to converge quickly to the unique extremal map. To get to within ϵ\epsilon of the dilatation of the extremal map, our method uses O(1/ϵ4)O(1/\epsilon^{4}) iterations. Every step of the iteration involves convex optimization and solving differential equations, and guarantees a decrease in the dilatation. Our method uses a reduction of the polygon mapping problem to that of the punctured sphere problem, thus solving a more general problem. We also discretize our procedure. We provide evidence for the fact that the discrete procedure closely follows the continuous construction and is therefore expected to converge quickly to a good approximation of the extremal quasiconformal map.Comment: 28 pages, 6 figure

    Anomalous lattice contraction and emergent electronic phases in Bi-doped Eu2_2Ir2_2O7_7

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    We study the pyrochlore series (Eu1x_{1-x}Bix_x)2_2Ir2_2O7_7 for 0x1 0 \leq x \leq 1. We show that for small xx, the lattice undergoes an anomalous contraction but the all-in/all-out and metal-to-insulator transitions remain robust, and the resistivity approaches a 1/T1/T dependence at low-T, suggesting proximity to the Weyl semimetallic phase, as previously predicted theoretically. At the boundary between Eu2_2Ir2_2O7_7 and Bi2_2Ir2_2O7_7 a qualitatively different ground state emerges, which is characterized by its unusual metallic behavior and absence of magnetic ordering at least down to 0.020.02 K.Comment: 5 Pages, 4 figure

    BCS theory of nodal superconductors

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    This course has a dual purpose. First we review the successes of the weak-coupling BCS theory in describing new classes of superconductors discovered since 1979. They include the heavy-fermion superconductors, high-Tc cuprate superconductors, organic superconductors, Sr2RuO4, etc. Second, we present the quasiclassical approximation introduced by Volovik, which we extend to describe the thermodynamics and the thermal conductivity of the vortex state in nodal superconductors. This approach provides the most powerful tool to identify the symmetry of the energy gap function Delta(k) in these new superconductors.Comment: 31 pages, 33 figure

    Trajectory Aware Macro-cell Planning for Mobile Users

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    We design and evaluate algorithms for efficient user-mobility driven macro-cell planning in cellular networks. As cellular networks embrace heterogeneous technologies (including long range 3G/4G and short range WiFi, Femto-cells, etc.), most traffic generated by static users gets absorbed by the short-range technologies, thereby increasingly leaving mobile user traffic to macro-cells. To this end, we consider a novel approach that factors in the trajectories of mobile users as well as the impact of city geographies and their associated road networks for macro-cell planning. Given a budget k of base-stations that can be upgraded, our approach selects a deployment that impacts the most number of user trajectories. The generic formulation incorporates the notion of quality of service of a user trajectory as a parameter to allow different application-specific requirements, and operator choices.We show that the proposed trajectory utility maximization problem is NP-hard, and design multiple heuristics. We evaluate our algorithms with real and synthetic data sets emulating different city geographies to demonstrate their efficacy. For instance, with an upgrade budget k of 20%, our algorithms perform 3-8 times better in improving the user quality of service on trajectories in different city geographies when compared to greedy location-based base-station upgrades.Comment: Published in INFOCOM 201

    Dilute stuffing in the pyrochlore iridate Eu2Ir2O7Eu_2Ir_2O_7

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    The pyrochlore Eu2_2Ir2_2O7_7 has recently attracted significant attention as a candidate Weyl semimetal. The previous reports on this compound unanimously show a thermally induced metal to insulator (MI) transition, concomitant with antiferromagnetic (AFM) long-range ordering of the Ir-moments below TN_\textit{N} \sim 120 K. However, there are contradictory reports concerning the slope dρ/\rho/dT of the resistivity plots (ρ\rho) in the "metallic" state above the metal-insulator (MI) transition, and the value of ρ\rho in the insulating state, both of which show significant sample dependence. Here, we explore this issue by investigating six different Eu2_2Ir2_2O7_7 samples with slightly varying Eu:Ir ratio. High-resolution synchrotron powder diffraction are done to probe minor variations in the cell parameters of the various Eu2_2Ir2_2O7_7 samples investigated here. Specific heat (Cp _p ) and magnetic susceptibility of all the samples showed long-range antiferromagnetic ordering upon cooling below TN _\textit{N} \sim 120 K. The transitions are, however, found to be smeared out for the off-stoichiometric samples. We show that the sign of dρ/\rho/dT above the metal-insulator (MI) transition is highly sensitive to the unit cell length, which, in turn, depends on the level of Eu-stuffing at the Ir-site. Samples with composition close to the ideal stoichiometry (Eu : Ir = = 1) showed a change of sign of dρ/\rho/dT from negative to positive upon cooling below a certain temperature T ^* >> TMI_\textit{MI}. With increasing Eu-stuffing T ^* decreased until a negative dρ/\rho/dT persisted without any sign change down to TMI_\textit{MI}.Comment: 12 pages, 7 figure
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