Using atomic resolution electron microscopy, scientists at LBNL’s
National Center for Electron Microscopy (NCEM) have discovered a new type
of crystalline “defect” that forms at boundaries between grains
in polycrystalline metals. The defect occurs at the line of intersection
between certain grain boundaries and surfaces and takes the form of a
chevron-like, V-shaped region less than 5 nm across. This discovery has
implications for grain growth in polycrystalline materials, the equilibrium
structure of grain boundaries, and the possibility of stabilizing new
phases in the nanoscale size regime.
Structures formed at grain boundaries are of fundamental
importance in determining the physical properties of polycrystalline materials.
Nearly all structural metals are used in their polycrystalline form and
the structure and composition of their grain boundaries affects their superplastic
deformation, embrittlement, corrosion, and electronic or superconducting
behavior.
The
local atomic structure of a material is altered at grain boundaries to accommodate
the deviation from the crystalline order of the bulk material. The structure
in these regions depends on a combination of a number of macroscopic crystallographic
parameters and on the atomic interactions characteristic for the material.
Great progress has been made in recent years in our understanding of grain
boundary behavior by correlating experimental |

observations
with atomistic simulations. A particularly notable advance was the discovery
of “grain boundary dissociation” in materials such as copper,
with low “stacking fault” energy, the increase in energy due
to a mistake in the stacking sequence of
densely packed crystal planes. In this phenomenon, rather than forming
immediately adjacent to one another, two grains are separated by a solid
wetting layer of the same composition as the adjoining grains, but differing
in structure or orientation.
In research reported here, NCEM’s new One-Ångstrom Microscope
was employed to examine regions in gold where the grain boundary reaches
a free surface. It was found that, in this area, a small chevron-shaped
“defect” region is formed that has a different crystalline
structure from either of the adjacent grains (see figure). This region
can be considered the one-dimensional equivalent of the solid wetting
layer described above as grain boundary dissociation. Detailed examination
clearly reveals that it is formed from a series of “stacking faults”
parallel to the two inclined sides. Atomistic simulations confirmed that
the observed structure corresponds to an energy minimum and predicted
that the structure should be stable only over a narrow size range of a
few nanometers, in agreement with observation.
Defects of this type had not been reported previously. Although the new
phenomenon has been, to date, observed only in gold, it is expected to
occur more generally in all materials with low stacking fault energy.
The defects may also be considered a dissociation of a line junction between
a grain boundary and a surface, or the wetting of such a line by a solid
“wire” of different structure. This solid “wire”
is naturally limited to nanometer dimensions in the direction normal to
the junction line. By exploiting the principles first demonstrated in
this work, it may eventually become possible to generate nanowires of
specific sizes and shapes and to control their position and orientation.
U.
Dahmen, (510) 486-4627, Materials Sciences Division (510 486-4755), Berkeley
Lab.
T. Radetic, F. Lançon, and U. Dahmen, “Chevron Defect at
the Intersection of Grain Boundaries
with Free Surfaces in Au,” Phys. Rev. Lett. 89, 085502 (2002).
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