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1 electrocatalytic performance of the Ag-CoSe2 nanobelts.
2 of the piezophototronic effect in a-axis GaN nanobelts.
3 f nitrogen-doped titanate-anatase core-shell nanobelts.
4 unctions are successfully fabricated in ZnSe nanobelts.
5 id body motion as well as deformation of the nanobelts.
6 using an example of Zn(x)Cd(1-x)S(y)Se(1-y) nanobelts.
7 ysis mechanism of the nitrogen-doped titania nanobelts.
8 mation together with in situ fracture of the nanobelts.
9 ws formed by bending single-crystal, PSD ZnO nanobelts.
10 l characteristics of the grown nanowires and nanobelts.
11 n and the side surfaces of the nanowires and nanobelts.
12 f-coiling process during the growth of polar nanobelts.
13 building functional devices along individual nanobelts.
14 thod for synthesizing ultra-long alpha-Si3N4 nanobelts along with a few nanowires and nanobranches on
17 to fewer unpassivated surface states in the nanobelts; and (iii) enhanced charge separation due to t
21 red to be initiated by circular folding of a nanobelt, caused by long-range electrostatic interaction
22 perature photoluminescence spectrum of Si3N4 nanobelts consists of three emission peaks centered at 4
23 on of the tin particle with the ZnO nanowire/nanobelt could be ordered (or partially crystalline) dur
25 .03, and 1/z = 0.39 +/- 0.12; (2) D > 40 nm, nanobelt crystals are formed gradually on the caterpilla
27 ge of a lateral PNG built on a single PMN-PT nanobelt demonstrates the potential application of PMN-P
29 assembled via ultralong molybdenum trioxide nanobelts, displays an excellent average transmittance o
33 he CoSe2 nanobelts, the as-prepared Ag-CoSe2 nanobelts exhibited a higher current density and a lower
40 enerator (PNG) is built on the single PMN-PT nanobelt, generating a maximum output voltage of ~1.2 V.
43 gy, with each nanowire being composed of two nanobelts joined along the growth direction to give a V-
44 calculations show that the morphology of ZnS nanobelts leads to a very high mechanical stability to a
45 nsformation into the superlattice-structured nanobelt led to the formation of a uniform nanohelix due
47 nc oxide nanorings formed by self-coiling of nanobelts may be useful for investigating polar surface-
49 e observations of the wide variety of SnO(2) nanobelt motions induced by ac dielectrophoresis (DEP) i
50 d on the continuous bridged-deformation of a nanobelt/nanowire using an atomic force microscope tip u
53 Bending of polar-surface-dominated (PSD) nanobelts of ZnO can be explained by one of two processe
56 he high d33 of the single-crystalline PMN-PT nanobelt results from the precise orientation control du
57 monstrate that morphology-tuned wurtzite ZnS nanobelts show a particular low-energy surface structure
60 ere we report a mechanistic study on a novel nanobelt structure that overcomes the drawback of sphere
61 emble in highly ordered few-micrometer-long 'nanobelts' that can be visualized by conventional micros
63 -P25), anatase spheres (TiO2-A), and anatase nanobelts (TiO2-NBs)] and three forms of multiwalled car
65 xide consisting of a superlattice-structured nanobelt was formed spontaneously in a vapor-solid growt
69 ion, morphology, and microstructure of Si3N4 nanobelts were investigated by X-ray diffraction, Fourie
73 ke (or ribbonlike) nanostructures (so-called nanobelts) were successfully synthesized for semiconduct
74 reasons: (i) greater charge mobility in the nanobelts, which is enabled along the longitudinal dimen
75 l (1 - x)Pb(Mg1/3Nb2/3)O3 - xPbTiO3 (PMN-PT) nanobelt with a superior piezoelectric constant (d33 = ~
78 t also for improving synthesis of metastable nanobelts with quantum effects for electronic and optica
80 ries of nanoscale Li(2)TiO(3)-coated LiMO(2) nanobelts with varied Ni, Co, and Mn contents was prepar
81 ons show that the exposed (101) facet of the nanobelts yields an enhanced reactivity with molecular O
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