Microwave-assisted synthesis of single-crystalline tellurium nanorods and nanowires in ionic liquids.
Microwave-assisted synthesis of single-crystalline tellurium nanorods and nanowires in ionic liquids.
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DOI:
10.1002/anie.200353101
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发表时间:
2004-03
影响因子:
--
通讯作者:
Yingjie Zhu;Wei-wei Wang;Rui-Juan Qi;Xianluo Hu
中科院分区:
文献类型:
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作者:
Yingjie Zhu;Wei-wei Wang;Rui-Juan Qi;Xianluo Hu
Figure 2a and b show TEM micrographs for the same sample as in Figure 1 (sample 1), from which one can see Te nanorods with diameters mostly ranging from% 15 to% 40 nm (a minority of them have diameters of 40 to 100 nm) and with lengths up to% 700 nm. Each nanorod is straight and has a uniform diameter along its entire length. The aspect ratios of most nanorods are in the range from 10 to 20. The aspect ratio is defined as the length of the major axis divided by the width of the minor axis. Nanorods are defined as structures with widths of 1–100 nm and aspect ratios greater than 1 but less than 20; and nanowires are analogous structures with aspect ratios greater than 20.[31] Figure 2 c shows a single Te nanorod with a diameter of 32 nm and a length of 610 nm (aspect ratio% 19), its corresponding electron diffraction pattern is shown in Figure 2d which was obtained by focusing the electron beam along the [11 0] direction. Electron diffraction patterns on different nanorods or different positions of a given single nanorod were essentially the same as shown in Figure 2d, thus indicating that nanorods were single-crystalline. The electron diffraction pattern can be indexed to the hexagonal structure, which is consistent with the result obtained from XRD. Figure 2e shows the high-resolution transmission electron microscopy (HRTEM) micrograph of the same single nanorod as shown in Figure2c, which provides more detailed structural information on these nanorods. The HRTEM shows that the nanorod is structurally singlecrystalline with the periodic fringe spacing of 5.927 along the longitudinal axis of the nanorod, which corresponds to the interplanar spacing between the (001) planes of the hexagonal Te. This indicates that Te nanorods had the preferential growth direction along the [001] zone axis (c axis of the crystal lattice), which is consistent with the results obtained from Te nanorods prepared by other methods.[26, 29]By controlling the experimental parameters, exclusive nanowires or nanorods could be produced. Figure 2 f shows the TEM micrograph of sample 2 prepared under a different procedure (see Experimental Section) from sample 1 by the MAIL method. One can see that nanowires instead of nanorods were produced. Most of these nanowires have diameters ranging from 20 to 100 nm, and a minority has diameters in the range of 100–500 nm. The lengths of these nanowires are tens of micrometers. Figure 2 g shows several nanowires from sample 2. The corresponding electron diffraction pattern of the longest nanowire in Figure 2 g is shown in Figure 2 h. The electron diffraction pattern of the nanowire (Figure 2 h) is essentially the same as that of the nanorod (Figure2d), indicating that nanorods and nanowires have the same preferential growth direction along the [001] zone axis (c axis of the crystal lattice). The temperature has a significant influence on the morphology of Te. NaBH4 reacts with TeO2 to form Te even at room temperature. However, no nanorods or nanowires were observed at temperatures between room temperature and 1308C (Table 1, sample 3). Te nanorods as well as spherical nanoparticles were observed in the temperature range of 130 to 1508C (sample 4). When the temperature was increased to 1808C (sample 1) or higher, only nanorods were observed. However, diameters of nanorods increased significantly when the temperature was higher than 2008C. A similar situation exists for the preparation of Te nanowires. Therefore, the optimum temperature for the production of Te nanorods or nanowires is around 1808C.