2017
DOI: 10.1038/nature21042
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Deciphering chemical order/disorder and material properties at the single-atom level

Abstract: Perfect crystals are rare in nature. Real materials often contain crystal defects and chemical order/disorder such as grain boundaries, dislocations, interfaces, surface reconstructions and point defects. Such disruption in periodicity strongly affects material properties and functionality. Despite rapid development of quantitative material characterization methods, correlating three-dimensional (3D) atomic arrangements of chemical order/disorder and crystal defects with material properties remains a challenge… Show more

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Cited by 276 publications
(345 citation statements)
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“…The as-prepared FePt NPs have a chemically disordered face centered cubic (fcc) structure (A1 phase), in which Fe and Pt atoms occupy randomly in fcc lattice. When annealing at temperature higher than 500°C, FePt undergoes a disorder-order transition, resulting in the formation of chemically ordered intermetallics with distinct crystal structures compared to the A1 phase [10,11]. According to FePt alloy equilibrium phase diagram, chemically ordered FePt intermetallics can form AuCu-type tetragonal (L1 0 -FePt) and AuCu 3 -type cubic (L1 2 -FePt 3 or L1 2 -Fe 3 Pt) structures depending on the chemical composition of the alloy [12].…”
Section: Introductionmentioning
confidence: 99%
“…The as-prepared FePt NPs have a chemically disordered face centered cubic (fcc) structure (A1 phase), in which Fe and Pt atoms occupy randomly in fcc lattice. When annealing at temperature higher than 500°C, FePt undergoes a disorder-order transition, resulting in the formation of chemically ordered intermetallics with distinct crystal structures compared to the A1 phase [10,11]. According to FePt alloy equilibrium phase diagram, chemically ordered FePt intermetallics can form AuCu-type tetragonal (L1 0 -FePt) and AuCu 3 -type cubic (L1 2 -FePt 3 or L1 2 -Fe 3 Pt) structures depending on the chemical composition of the alloy [12].…”
Section: Introductionmentioning
confidence: 99%
“…There are several approaches towards achieving high-resolution 3D imaging and spectroscopy, including electron tomography, hollow-cone illumination STEM and confocal STEM. Though electron tomography has achieved excellent 3D atom-by-atom imaging in some cases [3], it is not well-suited to typical plate-shape thin specimens. Since the successful development of higher-order aberration correctors [2], it has become possible to increase the illumination angle (α) up to 70 mrad.…”
mentioning
confidence: 99%
“…Since the successful development of higher-order aberration correctors [2], it has become possible to increase the illumination angle (α) up to 70 mrad. Therefore, optical depth sectioning with large-angle illumination (LAI) STEM [3] may allow us to solve three-dimensional materials problems. However, two technical difficulties must be overcome to perform atomic-scale optical depth sectioning via LAI-STEM [4].…”
mentioning
confidence: 99%
“…Using atomic electron tomography (AET) [1,[9][10][11][12][13][14], we determine the 3D coordinates of 6,569 iron and 16,627 platinum atoms in an FePt nanoparticle to correlate the 3D atomic structure with material properties at the single-atom level [15]. We identify rich structural variety and chemical order/disorder including 3D atomic composition, grain boundaries, anti-phase boundaries, anti-site point defects and swap defects.…”
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confidence: 99%