Phys Rev Lett 1993, 70:3615 10 1103/PhysRevLett 70 3615

Phys Rev Lett 1993, 70:3615. 10.1103/PhysRevLett.70.3615CrossRef 20. Wang YL, Gao HJ, Guo HM, Liu HW: Tip size effect on the appearance of a STM image for complex surfaces: theory versus experiment for Si(111)-7 × 7. Phys Rev B 2004, 70:073312.CrossRef 21. Razado IC, Zhang HM, Uhrberg RIG, Hansson GV: STM study of site selective hydrogen adsorption on Si(111)-7 × 7. Phys Rev B 2005, 71:235411.CrossRef

22. Byun JH, Ahn JR, Choi WH, Kang PG, Yeom HW: Photoemission and STM study of an In nanocluster GSK2879552 array on the Si(111)-7 × 7 surface. Phys Rev B 2008, 78:205314.CrossRef 23. Takayanagi K, Tanishiro Y, Takahashi M, Takahashi S: Structural analysis of Si(111)-7 × 7 by UHV transmission electron diffraction and microscopy. J Vac Sci Technol A 1985, 3:1502. 10.1116/1.573160CrossRef Competing interests The authors

declare that they have no competing interests. Authors’ contributions DJ conceived of the idea. KT designed the STM experiment and gave suggestions on the preparation of the sample. WD carried out the STM experiment, analyzed the data, and drafted the manuscript. YG carried out the XPS measurement. DJ, KT, and FK participated in the analysis of results. All authors read and approved the final manuscript.”
“Background Extensive research efforts have been recently dedicated to the synthesis of high-quality zinc oxide (ZnO) nanostructures, targeting high-performance electronic and optoelectronic applications [1–6]. selleck inhibitor Devices such as field-effect transistors [1], sensors [2], field emission [3] photovoltaic [4], room temperature UV lasers [5], and light-emitting diodes [6] have already been investigated in the literature. The interest in ZnO nanomaterials has been largely driven by the material’s excellent electrical and optoelectronic properties, including direct wide band-gap (3.37 eV), high exciton binding energy (60 meV), and moderate to high electron mobility (1 to 200 cm2/Vs) [1, 4]. Moreover, ZnO’s excellent piezoelectric and pyroelectric properties are finding widespread applications

targeting various energy harvesting systems [7–11]. Synthesis strategies, including GPX6 carbothermal reduction [12–22], pulse laser deposition [23], and hydrothermal [24] and electrochemical deposition [25], have been widely exploited for growing ZnO nanostructures such as nanowires (NWs), nanowalls (NWLs), and/or a hybrid of the two aforementioned nanostructures. Among them, carbothermal reduction of ZnO powder is offering high-quality ZnO nanostructures via the VLS process. In this process, a so-called seed thin layer of metal (such as Au) is first deposited onto the check details desired substrate. When increasing the temperature, the catalyst seed layer of metal is converted into nanoparticles. The nanoparticles can act as sink sites for vapors of the desired nanomaterial.

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