Abstract

The local atomic structure in the amorphous ${\mathrm{Al}}_{\mathit{x}}$(${\mathrm{Cu}}_{0.4}$${\mathrm{Y}}_{0.6}$${)}_{100\mathrm{\ensuremath{-}}\mathit{x}}$ and ${\mathrm{Mg}}_{\mathit{x}}$(${\mathrm{Cu}}_{0.4}$${\mathrm{Y}}_{0.6}$${)}_{100\mathrm{\ensuremath{-}}\mathit{x}}$ (0\ensuremath{\le}x\ensuremath{\le}85) alloys was determined by neutron-diffraction experiments. The electronic structure near the Fermi level was determined using the same samples by means of x-ray photoemission spectroscopy and soft x-ray spectroscopy. Both sets of data are combined to determine self-consistently and uniquely the local atomic structure in both Al- and Mg-based amorphous alloys. The bonding nature and resulting atomic environment are found to depend significantly on whether the third element is Al or Mg. Based on the atomic and electronic structures thus derived, we could interpret the Al or Mg concentration dependence of the crystallization temperature, electronic specific-heat coefficient, and also that of the resistivity value of 300 K. The origin of the appearance of a positive Hall coefficient observed in the Al-based amorphous alloys but not in the Mg-based amorphous alloys is also briefly discussed. \textcopyright{} 1996 The American Physical Society.

Full Text
Paper version not known

Talk to us

Join us for a 30 min session where you can share your feedback and ask us any queries you have

Schedule a call

Disclaimer: All third-party content on this website/platform is and will remain the property of their respective owners and is provided on "as is" basis without any warranties, express or implied. Use of third-party content does not indicate any affiliation, sponsorship with or endorsement by them. Any references to third-party content is to identify the corresponding services and shall be considered fair use under The CopyrightLaw.