With the existing of coverage holes, the Quality of Service (such as event response, package delay, and the life time et al.) of a Wireless Sensor Network (WSN) may become weaker. In order to recover the holes, one can locate them by identifying the boundary nodes on their edges. Little effort has been made to distinguish the boundary nodes in a model where wireless sensors are randomly deployed on a three-dimensional surface. In this paper, we propose a distributed method which contains three steps in succession. It first projects the 1-hop neighborhood of a sensor to the plane. Then, it sorts the projected nodes according to their angles and finds out if there exists any ring formed by them. At last, the algorithm validates a circle to confirm that it is a ring surrounding the node. Our solution simulates the behavior of rotating a semicircle plate around a sensor under the guidance of its neighbors. Different from the existing results, our method transforms a three-dimensional problem into a two-dimensional one and maintaining its original topology, and it does not rely on any complex Hamiltonian Cycle finding to test the existence of a circle in the neighborhood of a sensor. Simulation results show our method outperforms others at the correctness and effectiveness in identifying the nodes on the edges of a three-dimensional WSN.

BaSnO3 is proposed as a new insulating material with good surface coverage of the lower superconductor electrode for superconductor/insulator/superconductor (SIS) tunnel junctions made of high-Tc superconductor YBa2Cu3Ox (YBCO). This paper reports on investigation of the epitaxial nature of BaSnO3 on YBCO thin films and YBCO/BaSnO3 /YBCO trilayer formation that are grown in situ by reactive co-evaporation in oxygen radicals. Investigation was done by reflection high-energy electron diffraction (RHEED), atomic force microscopy (AFM), and X-ray diffraction (XRD). these observations confirm that (001)-oriented YBCO and (100)-oriented BaSnO3 thin films with atomically smooth surfaces grow epitaxially on each other. In addition, cross-sectional transmission electron microscopy (TEM) observation reveals that an approximately 4-nm-thick layer of BaSnO3 perfectly covers the lower YBCO thin film surface steps to a height of 1 to 2 unit cells of YBCO. The zero-resistance critical temperature Tc zero of both the upper and the lower YBCO thin films is higher than about 86 K.