Abstract:Conductive atomic
force microscopy (C-AFM) was employed to perform
conductivity measurements on a facet-specific Cu2O cube,
octahedron, and rhombic dodecahedron and intrinsic Si {100}, {111},
and {110} wafers. Similar I–V curves to those
recorded previously using a nanomanipulator were obtained with the
exception of high conductivity for the Si {110} wafer. Next, I–V curves of different Cu2O–Si
heterostructures were evaluated. Among the nine possible arrangements,
Cu2O octahedron/Si {100} wafer and Cu2O octahe… Show more
“…Figure 4 shows that electrical connection through a {111}‐bound Cu 2 O octahedron placed on a Si {100} wafer gives perfect current‐rectifying I–V curves, and white light illumination generates photocurrent. [ 45 ] Thus, the fabrication of semiconductor heterojunctions is a plausible design for field‐effect transistors. For the Cu 2 O {110}/Si{111} combination, there is a large photocurrent response, so such structure may have photodetector application.…”
Section: Development In Facet‐dependent Electrical Conductivity Prope...mentioning
confidence: 99%
“…(left) Measured I–V curves for a Cu 2 O octahedron on a Si {100} wafer with and without light illumination. (right) Measured I–V curves for a Cu 2 O rhombic dodecahedron on a Si {111} wafer with and without light illumination [ 45 ] …”
Section: Development In Facet‐dependent Electrical Conductivity Prope...mentioning
confidence: 99%
“…However, there is no [53] guarantee when two semiconductors are joined together, their photoconductivity should always increase, as the combination of a somewhat conductive Cu 2 O cube and a highly conductive Si {111} wafer is barely conductive even under light illumination. [45] In reality, when Cu 2 O cubes are decorated with ZnO, CdS, ZnS, and Ag 3 PO 4 nanoparticles, the composites remain photocatalytically inactive, attributed to the large band bending of the Cu 2 O {100} faces. [51][52][53][54] The interfacial band bending can be considered to be unmatched to prevent charges from crossing the interface (see Figure 5b,c).…”
Semiconductor crystals generally exhibit notable facet-dependent electrical conductivity and photocatalytic activity properties. If semiconductor nanocrystals of different shapes are available, their light absorption and emission bands can also display facet dependence, although bulk plus surface absorption combines to give the recorded spectra. All these physical phenomena can be understood, assuming a thin surface layer exists with slight structural deviations as predicted by density functional theory (DFT) calculations to give dissimilar band structures and hence different degrees of band bending and barriers to charge transport across a particular crystal face. This layer thereby tunes light absorption. Recent X-ray diffraction (XRD) and high-resolution transmission electron microscopy (HR-TEM) analyses begin to suggest the presence of the proposed surface layer.
“…Figure 4 shows that electrical connection through a {111}‐bound Cu 2 O octahedron placed on a Si {100} wafer gives perfect current‐rectifying I–V curves, and white light illumination generates photocurrent. [ 45 ] Thus, the fabrication of semiconductor heterojunctions is a plausible design for field‐effect transistors. For the Cu 2 O {110}/Si{111} combination, there is a large photocurrent response, so such structure may have photodetector application.…”
Section: Development In Facet‐dependent Electrical Conductivity Prope...mentioning
confidence: 99%
“…(left) Measured I–V curves for a Cu 2 O octahedron on a Si {100} wafer with and without light illumination. (right) Measured I–V curves for a Cu 2 O rhombic dodecahedron on a Si {111} wafer with and without light illumination [ 45 ] …”
Section: Development In Facet‐dependent Electrical Conductivity Prope...mentioning
confidence: 99%
“…However, there is no [53] guarantee when two semiconductors are joined together, their photoconductivity should always increase, as the combination of a somewhat conductive Cu 2 O cube and a highly conductive Si {111} wafer is barely conductive even under light illumination. [45] In reality, when Cu 2 O cubes are decorated with ZnO, CdS, ZnS, and Ag 3 PO 4 nanoparticles, the composites remain photocatalytically inactive, attributed to the large band bending of the Cu 2 O {100} faces. [51][52][53][54] The interfacial band bending can be considered to be unmatched to prevent charges from crossing the interface (see Figure 5b,c).…”
Semiconductor crystals generally exhibit notable facet-dependent electrical conductivity and photocatalytic activity properties. If semiconductor nanocrystals of different shapes are available, their light absorption and emission bands can also display facet dependence, although bulk plus surface absorption combines to give the recorded spectra. All these physical phenomena can be understood, assuming a thin surface layer exists with slight structural deviations as predicted by density functional theory (DFT) calculations to give dissimilar band structures and hence different degrees of band bending and barriers to charge transport across a particular crystal face. This layer thereby tunes light absorption. Recent X-ray diffraction (XRD) and high-resolution transmission electron microscopy (HR-TEM) analyses begin to suggest the presence of the proposed surface layer.
“…2,19,[26][27][28][29] In addition to the optical facet effect, the absorption band, and hence band gap, can shift continuously from quantum nanostructures to very large particles. [30][31][32] Because these semiconductor facet-dependent properties are interesting and potentially useful, as demonstrated in Cu 2 O-Si wafer heterostructures for current rectification, 33 it is desirable to explore the growth of other polyhedral inorganic crystals such as cadmium oxide to broaden the scope of investigation. CdO is an attractive candidate for shape-controlled particle synthesis with its rocksalt crystal structure and a known band gap of 2.18 eV giving a redbrown appearance.…”
CdO stellated octahedra, octahedra, {100}-truncated octahedra, and Cd(OH)2 hexagonal plates with respective average sizes of 147 nm, 700 nm, 2 m, and 105 nm have been synthesized by progressively increasing...
“…5 Utilizing the electrical facet effects, current rectification can be achieved through different surface plane or heterojunction combinations of Cu 2 O crystal-Si wafer. 27 This represents a novel design of field-effect transistors. With this potential, it is therefore interesting to extend conductivity measurements to silicon carbide (SiC) wafers for possible facet effects, as it is another third generation semiconductor with a wide band gap, high breakdown electric field and high thermal conductivity characteristics.…”
Intrinsic {0001} 4H-SiC wafer cut to expose {101 ̅0} and {12 ̅10} side faces allows for conductivity measurements on different crystal surfaces. The wafer has a band gap of 3.20...
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