Silver micro-and nanocrystals with sizes of -2-3.5 llm and -50-100 nm were uniaxially compressed under nonhydrostatic pressures (strong deviatoric stress) up to -30 GPa at room temperature in a symmetric diamond-anvil cell and studied in situ using angle-dispersive synchrotron X-ray diffraction. A cubic to trigonal structural distortion along a 3-fold rotational axis was discovered by careful and comprehensive analysis of the apparent lattice parameter and full width at half maximum, which are strongly dependent upon the Miller index and crystal size. 1 In the past fifteen years, much attention has been paid to the high pressure behavior of nanomaterials, especially the pressure-induced structural transformations in semiconductor 1O nanocrystals. I -In contrast, there are few reports on structural transformations and distortions in noble metals under high pressure due to their close-packed structures. It is generally accepted that sub millimeter crystals of silver (~149 !lm) and palladium (~250 Jlll1) are stable in the face-centered cubic (fcc) structure at room temperature up to at least 91. Two samples of conventional, irregularly-structured Ag crystals were purchased from Aldrich and used in our comparative study. They have reported average sizes and purities of2-3.5 Jlll1 and 99.9+%and <100 nm and 99.5%, respectively and are referred to as micro-and nano-Ag powders from hereon. Figure 1 shows representative scanning and transmission electron micrographs (SEM and TEM, respectively) of the Ag samples. These samples were uniaxially compressed under nonhydrostatic pressures up to -30 OPa in a symmetric diamond-anvil cell (DAC) and studied in situ using angle-dispersive synchrotron X-ray diffraction. Two ruby grains, located in the center and at the edge of the samples, respectively, were used for pressure calibration and radial pressure gradient estimation. 17 Detailed experimental procedures are similar to our previous report.
162 Figure 2 shows X-ray diffraction patterns, up to ~30 GPa, for the micro-and nano-Ag powders.From first analysis, it appeared that no phase transfonnations or distortions occurred because no splits, disappearances, or appearances of the diffraction peaks were observed. But when the d-spacing of the (200) peak was carefully compared with that of the (111) The apparent lattice parameters a200 and alll and their ratio a200/al II for the nano-Ag powder are shown in Figure 3a and Figure 3b, respectively. It is well-known that ahkl of Ag with the idealized fcc structure is not dependent upon the Miller index; however, according to Figure 3, it becomes apparent that ahktCP) in the nano-Ag is actually strongly dependent upon the Miller index when P > 1.9 OPa. In general, a200, was always larger than the corresponding alII and the higher the pressure, the larger the relative difference (within the pressure range of 0 to 11.2 GPa). Specifically, the relative difference at ambient pressure was less than 0.03% but increased to 0.37% at a pressure of 11.2 GPa. Beyond 11.2 GPa, this difference d...