Matches in SemOpenAlex for { <https://semopenalex.org/work/W4241554780> ?p ?o ?g. }
- W4241554780 endingPage "12" @default.
- W4241554780 startingPage "11" @default.
- W4241554780 abstract "The three dimensional (3D) structural characterization of nanoparticles is crucial in materials science since many properties heavily depend on size, surface to volume ratio and morphology. In addition, the ability to investigate the crystal structure is just as essential because the presence of defects and surface relaxation will directly affect plasmonic or catalytic properties. A well‐known example of strained nanoparticles are the so‐called “nanodecahedra” or “pentagonal bipyramids”. Such particles consist of five segments bound by {111} twin boundaries, yielding a crystallographic forbidden morphology. Therefore, measuring strain fields in nanodecahedra by transmission electron microscopy (TEM) has been the topic of several studies. However, it is important to note that such studies are based on 2D projections, hereby neglecting the 3D nature of the lattice strain. [1,2] Here, we will quantify the lattice strain in 3D based on high resolution electron tomography reconstructions. [3] Therefore, a continuous tilt series of 2D projection images was acquired using high angle annular dark field (HAADF) scanning transmission electron microscopy (STEM) and a dedicated alignment procedure was applied. These projection images are then used as an input for a model based tomography reconstruction algorithm. A major disadvantage of conventional reconstruction techniques is that a continuous volume is reconstructed hampering the extraction of atom coordinates without the use of dedicated post‐processing methods. [4] We could overcome this limitation by assuming that the 3D atomic potential can be modelled by 3D Gaussian functions. This hypothesis significantly simplifies the reconstruction problem to a sparse inverse problem, yielding the coordinates of the individual atoms as a direct outcome of the reconstruction. Visualizations of the final 3D reconstruction, obtained for a Au nanodecahedron containing more than 90,000 atoms, are presented in Figure 1.a–c along different viewing directions. Since the coordinates of the atoms are a direct outcome of the reconstruction, it becomes straightforward to calculate the 3D displacement map. We computed derivatives of the displacement map in such a manner that 3D volumes were obtained corresponding to ε xx and ε zz . Slices through the resulting ε xx and ε zz volumes are presented in Figure 1.d and Figure 1.f. Furthermore, the variation of the lattice parameters was investigated along x and z based on the same slices (Figure 1.e and Figure 1.g). Both along the x and z direction a systematic outward expansion of the lattice can be observed. The expansion along z is limited to a few of the outer atomic layers and shows an asymmetry (Figure 1.f–g) that is likely related to the fact that the decahedron is deposited on a carbon support." @default.
- W4241554780 created "2022-05-12" @default.
- W4241554780 creator A5003190223 @default.
- W4241554780 creator A5003329885 @default.
- W4241554780 creator A5008231285 @default.
- W4241554780 creator A5009706633 @default.
- W4241554780 creator A5013888065 @default.
- W4241554780 creator A5020421789 @default.
- W4241554780 creator A5054696921 @default.
- W4241554780 creator A5067251489 @default.
- W4241554780 creator A5067599369 @default.
- W4241554780 creator A5071000641 @default.
- W4241554780 creator A5085957218 @default.
- W4241554780 date "2016-12-20" @default.
- W4241554780 modified "2023-10-17" @default.
- W4241554780 title "Investigating lattice strain in Au nanodecahedrons" @default.
- W4241554780 cites W1446398432 @default.
- W4241554780 cites W2064394355 @default.
- W4241554780 cites W2312419339 @default.
- W4241554780 cites W332280818 @default.
- W4241554780 doi "https://doi.org/10.1002/9783527808465.emc2016.5519" @default.
- W4241554780 hasPublicationYear "2016" @default.
- W4241554780 type Work @default.
- W4241554780 citedByCount "0" @default.
- W4241554780 crossrefType "other" @default.
- W4241554780 hasAuthorship W4241554780A5003190223 @default.
- W4241554780 hasAuthorship W4241554780A5003329885 @default.
- W4241554780 hasAuthorship W4241554780A5008231285 @default.
- W4241554780 hasAuthorship W4241554780A5009706633 @default.
- W4241554780 hasAuthorship W4241554780A5013888065 @default.
- W4241554780 hasAuthorship W4241554780A5020421789 @default.
- W4241554780 hasAuthorship W4241554780A5054696921 @default.
- W4241554780 hasAuthorship W4241554780A5067251489 @default.
- W4241554780 hasAuthorship W4241554780A5067599369 @default.
- W4241554780 hasAuthorship W4241554780A5071000641 @default.
- W4241554780 hasAuthorship W4241554780A5085957218 @default.
- W4241554780 hasBestOaLocation W42415547801 @default.
- W4241554780 hasConcept C11413529 @default.
- W4241554780 hasConcept C120665830 @default.
- W4241554780 hasConcept C121332964 @default.
- W4241554780 hasConcept C146088050 @default.
- W4241554780 hasConcept C147080431 @default.
- W4241554780 hasConcept C171250308 @default.
- W4241554780 hasConcept C185592680 @default.
- W4241554780 hasConcept C192562407 @default.
- W4241554780 hasConcept C193016168 @default.
- W4241554780 hasConcept C207114421 @default.
- W4241554780 hasConcept C207467116 @default.
- W4241554780 hasConcept C20885615 @default.
- W4241554780 hasConcept C24890656 @default.
- W4241554780 hasConcept C2524010 @default.
- W4241554780 hasConcept C2776799497 @default.
- W4241554780 hasConcept C2781204021 @default.
- W4241554780 hasConcept C33923547 @default.
- W4241554780 hasConcept C41008148 @default.
- W4241554780 hasConcept C53120450 @default.
- W4241554780 hasConcept C57493831 @default.
- W4241554780 hasConcept C75806775 @default.
- W4241554780 hasConcept C8010536 @default.
- W4241554780 hasConcept C89957378 @default.
- W4241554780 hasConceptScore W4241554780C11413529 @default.
- W4241554780 hasConceptScore W4241554780C120665830 @default.
- W4241554780 hasConceptScore W4241554780C121332964 @default.
- W4241554780 hasConceptScore W4241554780C146088050 @default.
- W4241554780 hasConceptScore W4241554780C147080431 @default.
- W4241554780 hasConceptScore W4241554780C171250308 @default.
- W4241554780 hasConceptScore W4241554780C185592680 @default.
- W4241554780 hasConceptScore W4241554780C192562407 @default.
- W4241554780 hasConceptScore W4241554780C193016168 @default.
- W4241554780 hasConceptScore W4241554780C207114421 @default.
- W4241554780 hasConceptScore W4241554780C207467116 @default.
- W4241554780 hasConceptScore W4241554780C20885615 @default.
- W4241554780 hasConceptScore W4241554780C24890656 @default.
- W4241554780 hasConceptScore W4241554780C2524010 @default.
- W4241554780 hasConceptScore W4241554780C2776799497 @default.
- W4241554780 hasConceptScore W4241554780C2781204021 @default.
- W4241554780 hasConceptScore W4241554780C33923547 @default.
- W4241554780 hasConceptScore W4241554780C41008148 @default.
- W4241554780 hasConceptScore W4241554780C53120450 @default.
- W4241554780 hasConceptScore W4241554780C57493831 @default.
- W4241554780 hasConceptScore W4241554780C75806775 @default.
- W4241554780 hasConceptScore W4241554780C8010536 @default.
- W4241554780 hasConceptScore W4241554780C89957378 @default.
- W4241554780 hasLocation W42415547801 @default.
- W4241554780 hasOpenAccess W4241554780 @default.
- W4241554780 hasPrimaryLocation W42415547801 @default.
- W4241554780 hasRelatedWork W2001556419 @default.
- W4241554780 hasRelatedWork W2034518976 @default.
- W4241554780 hasRelatedWork W2071750104 @default.
- W4241554780 hasRelatedWork W2090919632 @default.
- W4241554780 hasRelatedWork W2093191132 @default.
- W4241554780 hasRelatedWork W2112037220 @default.
- W4241554780 hasRelatedWork W2209351154 @default.
- W4241554780 hasRelatedWork W2568206242 @default.
- W4241554780 hasRelatedWork W3137199871 @default.
- W4241554780 hasRelatedWork W4241554780 @default.
- W4241554780 isParatext "false" @default.
- W4241554780 isRetracted "false" @default.