Materials Map

Discover the materials research landscape. Find experts, partners, networks.

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The Materials Map is an open tool for improving networking and interdisciplinary exchange within materials research. It enables cross-database search for cooperation and network partners and discovering of the research landscape.

The dashboard provides detailed information about the selected scientist, e.g. publications. The dashboard can be filtered and shows the relationship to co-authors in different diagrams. In addition, a link is provided to find contact information.

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Materials Map under construction

The Materials Map is still under development. In its current state, it is only based on one single data source and, thus, incomplete and contains duplicates. We are working on incorporating new open data sources like ORCID to improve the quality and the timeliness of our data. We will update Materials Map as soon as possible and kindly ask for your patience.

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Reich, Shimon

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in Cooperation with on an Cooperation-Score of 37%

Topics

Publications (3/3 displayed)

  • 2002Interplay of Cs concentration, dimensionality and superconductivity in CsxWO318citations
  • 2002Synthesis and properties of alkali metal intercalated fullerene-like MS2 (M=W,MO) nanoparticlescitations
  • 2002Alkali metal intercalated fullerene-like MS2 (M = W, Mo) nanoparticles and their properties181citations

Places of action

Chart of shared publication
Popovitz-Biro, Ronit
2 / 15 shared
Tenne, Reshef
2 / 29 shared
Feldman, Yishai
2 / 15 shared
Wachtel, Ellen
2 / 7 shared
Lyakhovitskaya, V.
2 / 2 shared
Zak, A.
2 / 6 shared
Chart of publication period
2002

Co-Authors (by relevance)

  • Popovitz-Biro, Ronit
  • Tenne, Reshef
  • Feldman, Yishai
  • Wachtel, Ellen
  • Lyakhovitskaya, V.
  • Zak, A.
OrganizationsLocationPeople

article

Interplay of Cs concentration, dimensionality and superconductivity in CsxWO3

  • Reich, Shimon
Abstract

<p>It is known that Cs<sub>x</sub>WO<sub>3</sub>, 0.3 ≥ x ≥ 0.19, is a 3D superconductor. Below x = 0.19 a transition from a metal to an insulator occurs and for x = 0.10, for example, no superconductivity is observed. We find, however, that for x ≤ 0.05 superconductivity reappears. For x = 0.005 nominal concentration we observe a critical transition T<sub>c</sub> to the superconducting state at 5.9 K. This is observed in magnetic measurements, where a pronounced Meissner effect is present. X-ray photoelectron spectroscopy and transport measurements indicate that the SC state is confined to mesoscopic islands, some 10 nm thick on the surface of the Cs<sub>x</sub>WO<sub>3</sub> doped crystals. The bulk of the crystal is practically pure WO<sub>3</sub>. Thus during the high temperature crystal growth process, there is a redistribution of the Cs dopant as it migrates to the surface of the WO<sub>3</sub> crystals. From these observations, we conclude that upon reduction of the Cs nominal concentration below x = 0.05, a 2D superconductor is formed, while for x ≥ 0.19, the Cs<sub>x</sub>WO<sub>3</sub> bronze is a 3D superconductor.</p>

Topics
  • impedance spectroscopy
  • surface
  • x-ray photoelectron spectroscopy
  • bronze
  • superconductivity
  • superconductivity