4.3 Article

Unprecedented plastic flow channel in gamma-B-28 through ultrasoft bonds: A challenge to superhardness

Journal

PHYSICAL REVIEW MATERIALS
Volume 2, Issue 12, Pages -

Publisher

AMER PHYSICAL SOC
DOI: 10.1103/PhysRevMaterials.2.123602

Keywords

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Funding

  1. National Natural Science Foundation of China [51672015, 51201148, U1530402, 11575288, 51402350]
  2. National Key Research and Development Program of China [2016YFC1102500]
  3. National Thousand Young Talents Program of China
  4. Fundamental Research Funds for the Central Universities
  5. project IT4Innovations: Path to Exascale [CZ.02.1.01/0.0/0.0/16_013/0001791]
  6. Czech Science Foundation [17-27790S]
  7. National Programme of Sustainability [LQ1602]
  8. National Key R&D Program of China [2016YFA0401503]

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A longstanding controversy remains whether gamma-B-28 is intrinsically superhard or not, i.e., H-upsilon >= 40 GPa. Here we perform comprehensive investigations on the mechanical properties of gamma-B-28 to reveal the plasticity and failure mode of gamma-B-28 through the unique combination of microindentation experiment, the ideal strength approach, and the ab initio informed Peierls-Nabarro model. A low load-invariant hardness of similar to 30 GPa is found for both polycrystalline and monocrystalline gamma-B-28. By carefully checking the strength anisotropy and strain facilitated phonon instability, a surprising ideal strength of 23.1 GPa is revealed along the (001)[010] slip system for gamma-B-28, together with an inferior Peierls stress of 3.2 GPa, both of which are close to those of B6O and ZrB12 yet much lower than those of diamond and c-BN. These results suggest that gamma-B-28 could not be intrinsically superhard. Atomistic simulation and electronic structure analysis uncover an unprecedented plastic flow channel through the specific ultrasoft bonding, which causes a dramatic softening of gamma-B-28. These findings highlight an approach to quantifying the realistic hardness by means of two plasticity descriptors beyond the elastic limit, i.e., the ideal strength approach and the Peierls-Nabarro model.

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