Superlattice-structured ZnO nanohelix is a structure that is made of a coiling nanobelt, which is composed of ZnO nanostripes oriented alternatively in two different orientations (Science 2005, 309, 1700). The nanostripes run almost in parallel to the nanobelt direction but at an offset angle of approximately 5 degrees . We have measured the transport properties of a nanohelix and found its abnormal nonlinear characteristic. In comparison to the Ohmic transport property of a single crystal ZnO nanobelt measured under the same experimental conditions, the symmetric "Schottky-type" I-V property of the nanohelix is suggested due to nanostripe boundaries and surfaces, where built-in periodic back-to-back energy barriers might occur across the nanostripe interfaces as a result of polar charges and interface-strain-induced piezoelectric effect. The effective potential barrier across the nanostripe boundary is estimated to be approximately 24 meV. With the increasing of bias voltage, electrons can effectively tunnel through and thermionic emission across nanostripe boundaries, leading to a fast increase in transport current. It is suggested that the ZnO nanohelix could form a new type of band structure modulated superlattice for fabricating novel electronic devices.
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http://dx.doi.org/10.1021/nl802682c | DOI Listing |
Nanomaterials (Basel)
December 2017
Department of Mechanical Engineering, University of Minnesota, Minneapolis, MN 55455, USA.
Electric potential produced in deformed piezoelectric nanostructures is of significance for both fundamental study and practical applications. To reveal the piezoelectric property of ZnO nanohelices, the piezoelectric potential in single-crystal nanohelices was simulated by finite element method calculations. For a nanohelix with a length of 1200 nm, a mean coil radius of 150 nm, five active coils, and a hexagonal coiled wire with a side length 100 nm, a compressing force of 100 nN results in a potential of 1.
View Article and Find Full Text PDFNanoscale
April 2015
State Key Laboratory of Silicon Materials, School of Materials Science and Engineering, Zhejiang University, Hangzhou 310027, People's Republic of China.
A unique all-wurtzite ZnO/ZnSe hetero-nanohelix is formed via growing wurtzite ZnSe nanoteeth on ZnO nanobelts through a one step thermal evaporation method. The microstructure and growth mechanism of the hetero-nanohelix are investigated in detail. The formation of metastable wurtzite ZnSe is attributed to the wurtzite ZnO template.
View Article and Find Full Text PDFNano Lett
January 2009
Department of Chemical, Materials and Biomolecular Engineering & Institute of Materials Science, University of Connecticut, Storrs, Connecticut 06269-3136, USA.
Superlattice-structured ZnO nanohelix is a structure that is made of a coiling nanobelt, which is composed of ZnO nanostripes oriented alternatively in two different orientations (Science 2005, 309, 1700). The nanostripes run almost in parallel to the nanobelt direction but at an offset angle of approximately 5 degrees . We have measured the transport properties of a nanohelix and found its abnormal nonlinear characteristic.
View Article and Find Full Text PDFJ Nanosci Nanotechnol
January 2008
School of Materials Science and Engineering, Georgia Institute of Technology, Atlanta, GA 30332-0245, USA.
Nanowires (NWs) and nanobelts (NBs) are diverse classes of one-dimensional nanoscale materials with controllable size, composition, structure and corresponding physical and chemical properties. This article reviews the novel growth phenomena, unique properties and exciting applications of oxide NWs and NBs. First, the article gives a general introduction about the vapor-liquid-solid (VLS) growth method.
View Article and Find Full Text PDFNano Lett
November 2006
School of Materials Science and Engineering, Georgia Institute of Technology, Atlanta, Georgia 30332-0245, USA.
A superelasticity (shape memory) behavior has been discovered for the superlattice-structured ZnO nanohelices. By in situ manipulation using a nanoprobe, the nanohelix could elastically recover its shape after an extremely large axial stretching to a degree close to the theoretical limit, while suffering little residual plastic deformation. As a result, its spring constant can be increased continuously for up to 300-800%.
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