Figures & data
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Figure 1. The change of ZnO particles morphology and microstructure caused by HPT processing. SEM images of as-synthesized (a) and compacted (b) ZnO particles with average particle sizes of 311 ± 150 nm and 304 ± 149 nm, respectively; (c) a BF-TEM image of as-synthesized ZnO particles; insert and arrows highlight the thickness fringes at the edge of the particles; (d) a SEM image of HPT-processed ZnO particles having average dimensions of 603 ± 243 nm and 78 ± 42 nm along the shearing direction (SD) and normal direction (ND), respectively; (e) a BF-TEM image of an HPT-processed ZnO particle; insert shows a SADP taken from the particle.
![Figure 1. The change of ZnO particles morphology and microstructure caused by HPT processing. SEM images of as-synthesized (a) and compacted (b) ZnO particles with average particle sizes of 311 ± 150 nm and 304 ± 149 nm, respectively; (c) a BF-TEM image of as-synthesized ZnO particles; insert and arrows highlight the thickness fringes at the edge of the particles; (d) a SEM image of HPT-processed ZnO particles having average dimensions of 603 ± 243 nm and 78 ± 42 nm along the shearing direction (SD) and normal direction (ND), respectively; (e) a BF-TEM image of an HPT-processed ZnO particle; insert shows a SADP taken from the particle.](/cms/asset/3f4ac82f-5c39-443a-98db-5a5fd92c27c0/tmrl_a_1821111_f0001_oc.jpg)
Figure 2. The wedge-like shape of the edge region on HPT-processed ZnO particles. (a) a schematic illustration of the frictional sliding, shear deformation and consolidation of the HPT-processed ZnO particles; (b) an ADF-STEM image of two HPT-processed ZnO particles with an overlap region, indicating that frictional sliding may occur between them; (c) a map of the relative thickness, t/λ, taken from a particle edge region highlighted in (b). The absolute thickness changes gradually from 0.32λ (29 nm) to 1.14λ (104 nm) from the edge to the interior of the particle, within a distance of 225 nm along the particle surface.
![Figure 2. The wedge-like shape of the edge region on HPT-processed ZnO particles. (a) a schematic illustration of the frictional sliding, shear deformation and consolidation of the HPT-processed ZnO particles; (b) an ADF-STEM image of two HPT-processed ZnO particles with an overlap region, indicating that frictional sliding may occur between them; (c) a map of the relative thickness, t/λ, taken from a particle edge region highlighted in (b). The absolute thickness changes gradually from 0.32λ (29 nm) to 1.14λ (104 nm) from the edge to the interior of the particle, within a distance of 225 nm along the particle surface.](/cms/asset/53a0f956-d312-4962-9810-4d086e39b813/tmrl_a_1821111_f0002_oc.jpg)
Figure 3. Gradient bandgap narrowing at the edge of an HPT-processed ZnO particle. (a) the ADF image of a deformed ZnO particle on which seven EELS acquisition locations are labeled; (b) a relative thickness map showing the t/λ changes from 0.22 at the outermost edge to 0.78 within 120 nm towards the interior of the particle; (c) seven VEEL spectra after ZLP and background subtraction. Note the increase of slopes of the low-loss spectra from point #1 to #7 with increasing thickness. Furthermore, the intensity of the humps before the bandgap onsets increased along with increasing thickness due to greater Cerenkov and surface effects.
![Figure 3. Gradient bandgap narrowing at the edge of an HPT-processed ZnO particle. (a) the ADF image of a deformed ZnO particle on which seven EELS acquisition locations are labeled; (b) a relative thickness map showing the t/λ changes from 0.22 at the outermost edge to 0.78 within 120 nm towards the interior of the particle; (c) seven VEEL spectra after ZLP and background subtraction. Note the increase of slopes of the low-loss spectra from point #1 to #7 with increasing thickness. Furthermore, the intensity of the humps before the bandgap onsets increased along with increasing thickness due to greater Cerenkov and surface effects.](/cms/asset/b4e23c6f-84b7-445f-9689-9acfe8f1a5c6/tmrl_a_1821111_f0003_oc.jpg)
Figure 4. The evolution of valence band maximum and conduction band minimum at the edge region studied by core-loss EELS of (a) O K-edge and (b) Zn L2,3-edge. The spectra are averaged from the strips shown in the insert in (b), and the background signals were subtracted. Note the arrow in (a) pointing at the characteristic peak a1.
![Figure 4. The evolution of valence band maximum and conduction band minimum at the edge region studied by core-loss EELS of (a) O K-edge and (b) Zn L2,3-edge. The spectra are averaged from the strips shown in the insert in (b), and the background signals were subtracted. Note the arrow in (a) pointing at the characteristic peak a1.](/cms/asset/aabaaebb-f431-4c9c-9e58-448244578efc/tmrl_a_1821111_f0004_oc.jpg)