Sn-filled single-crystalline Wurtzite-type ZnS nanotubes
Sn-filled single-crystalline Wurtzite-type ZnS nanotubes
复制标题
DOI:
10.1002/anie.200454205
复制
发表时间:
2004-01-01
影响因子:
16.6
通讯作者:
Golberg, D
中科院分区:
文献类型:
--
作者:
Hu, JQ;Bando, Y;Golberg, D
The ZnS nanotubes were synthesized in a horizontal hightemperature resistance furnace at a temperature of 11508C by using a mixture of ZnS and SnO powders as starting materials. After the furnace was cooled to room temperature under a stream of N2, a gray-colored product was collected from the inner wall of the tube downstream, where the temperature was between 180 and 2508C during heating. As shown in the scanning electron microscopy (SEM) image (Figure1a), numerous one-dimensional nanostructures with spherical particles at their tip ends were formed in the product. Most of them are straight and have lengths ranging from several to tens of micrometers. The X-ray diffraction (XRD) pattern (Figure 1b) of the product presents clear evidence that the nanostructures are composed of two crystalline phases, that is, hexagonal (wurtzite) ZnS (JCPDS: 36-1450; a= 3.8298 and c= 6.2573) and tetragonal Sn (β-Sn)(JCPDS: 04-0673; a= 5.831 and c= 3.182). No characteristic peaks from other impurities, such as ZnO, SnO, and SnO2 are detected in the XRD pattern.Transmission electron microscopy (TEM) and X-ray energy-dispersive spectrometry (EDS) reveal that the asgrown structures are in fact ZnS nanotubes filled with Sn. Normally, a Sn-filling occupies more than 70–80% of the entire cavity of a ZnS nanotube. Some of tubes have uniform diameters and wall thicknesses throughout their whole lengths (Figure 2a), and the diameters and wall thicknesses are 150–200 nm and 50–60 nm, respectively. Typically, a given tube is sealed with a Sn-filling at one end (note that each Snfilling terminates with a spherical Sn particle), whereas the other end and central part of the tube may be open and hollow, respectively. As shown in Figure 2b, the diameters and wall thicknesses of these tubes gradually decrease and become smaller and smaller along their lengths, from 180–250 nm and 60–80 nm at the thicker end to 80–120 nm and 25–