Molecular dynamics modeling of mechanical loss in amorphous tantala and titania-doped tantala

Jonathan P. Trinastic, Rashid Hamdan, Chris Billman, and Hai-Ping Cheng
Phys. Rev. B 93, 014105 – Published 25 January 2016

Abstract

The mechanical loss (Q1) intrinsic to amorphous oxides is the limiting factor for sensitive, high-precision gravitational wave detectors and optical devices. Recent experimental work suggests that doping amorphous tantala with titania reduces Q1, however, the physical processes underlying this reduction are unknown. Here, we calculate Q1 for pure and titania-doped tantala using numerical methods combined with molecular dynamics simulations that have atomic levels of resolution. Our results match experimental trends that titania doping decreases the magnitude of the low-temperature loss peak characteristic of these materials, with 62% titanium cation doping minimizing Q1 at low temperature. We provide a microscopic explanation for this reduced loss by examining how doping affects the potential energy landscape, strain coupling constant, relaxation time, and other properties of the amorphous materials within the framework of the double-well potential model. Analyzing configurational changes provides an atomic description of the transitions driving mechanical loss at various temperatures in these oxides. These results identify the important parameters contributing to Q1 that are most affected by doping and provide guidance for how to screen for optimal doping combinations to minimize loss in other materials.

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  • Received 29 October 2015
  • Revised 11 January 2016

DOI:https://doi.org/10.1103/PhysRevB.93.014105

©2016 American Physical Society

Physics Subject Headings (PhySH)

Condensed Matter, Materials & Applied Physics

Authors & Affiliations

Jonathan P. Trinastic, Rashid Hamdan, Chris Billman, and Hai-Ping Cheng*

  • Department of Physics and Quantum Theory Project, University of Florida, Gainesville, Florida 32611, USA

  • *cheng@qtp.ufl.edu

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Issue

Vol. 93, Iss. 1 — 1 January 2016

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