Since the discovery of nanobelts of semiconducting oxides in 2001, [1] planar structures of nanobelts have been intensively researched because they present a good system for examining dimensionally confined and structurally well-defined physical and chemical phenomena. [1,2] Nanobelts, with a rectangular cross section and well-defined faceted surfaces, enable the observation of unique optical-confinement, microcavity, catalysis, and piezoelectricity effects. [3][4][5][6][7][8][9] According to classical waveguide theory, waveguides of different cross sections will exhibit different transverse optical modes.[10] Nanobelts with rectangular cross sections have been used as effective FabryPerot microcavities for lasing. [11] In the past few years, fieldeffect transistors, [12] nanometer-sized ultrasensitive gas sensors, [13] resonators, [14] and cantilevers [15] have been fabricated based on individual nanobelts. Thermal transport along the nanobelt has also been measured. [16] Recent studies on the preparation of rare-earth hydroxide and oxide nanostructures have shown that 1D nanostructures can be prepared by a hydrothermal method, which leads us to believe that 1D nanostructured hydroxides might be prepared via hydrothermal treatment of their counterpart oxides in an autoclave. [17][18][19] In turn, 1D nanostructured oxides might be obtained from dehydration of their counterpart nanostructured hydroxides. [17,18] However, the high pressure in an autoclave suggests high vessel costs, which, on a large scale, would result in expensive, high-tech production. Here, we develop an approach for the synthesis of ultralong nanobelt-like hydroxides by using a composite-hydroxide-mediated (CHM) synthesis method, [20,21] Lanthanum hydroxide (La(OH) 3 ) nanobelts were prepared by adding La(CH 3 COO) 3 to a mixture of hydroxides (NaOH/KOH = 51.5:48.5) in a covered Teflon vessel and heating the mixture in a furnace at 200°C for 48 h. An X-ray diffraction (XRD) pattern of the obtained La(OH) 3 product is shown in Figure 1b. All peaks can be perfectly indexed as the pure hexagonal phase (P6 3 /m (176), Joint Comittee on Powder Diffraction Standards (JCPDS) file number 36-1481) of La(OH) 3 , with lattice constants a = 6.529 Å and c = 3.859 Å.The morphology of the obtained La(OH) 3 product was characterized by scanning electron microscopy (SEM). Figure 1a gives the low-magnification image of La(OH) 3 , in which the nanobelts are seen to be up to a few millimeters in length. The beltlike structure is seen in the high-magnification images in Figure 1c . By examining the nanobelts in detail, we found that the ends have an arrowlike shape (Fig. 1e) and that the cross sections are rectangular (Fig. 1f).
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