ライフサイエンスコーパス: nanobelt

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

15 Micrometer-long nanobelt and nanowires from deposition of perylenediimid

16 Pearl chain formation involving short nanobelts and particles was also observed in the two DEP

17 to fewer unpassivated surface states in the nanobelts; and (iii) enhanced charge separation due to t

18 Nitrogen-doped anatase titania nanobelts are prepared via hydrothermal processing and s

19 The as-synthesized oxide nanobelts are pure, structurally uniform, and single cry

20 The nanobelts are single crystals elongated preferentially i

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

24 The nanobelts could be an ideal system for fully understandi

25 .03, and 1/z = 0.39 +/- 0.12; (2) D > 40 nm, nanobelt crystals are formed gradually on the caterpilla

26 pid roughening process, and the formation of nanobelt crystals.

27 ge of a lateral PNG built on a single PMN-PT nanobelt demonstrates the potential application of PMN-P

28 More interesting, ECL of a single nanobelt deposited on an ultramicroelectrode was observe

29 assembled via ultralong molybdenum trioxide nanobelts, displays an excellent average transmittance o

30 inated by transforming into a single-crystal nanobelt dominated by nonpolar (0110) surfaces.

31 Moreover, the nanobelts exhibit a lower electron-hole recombination ra

32 The nanobelts exhibit birefringence enhanced by 1 order of m

33 he CoSe2 nanobelts, the as-prepared Ag-CoSe2 nanobelts exhibited a higher current density and a lower

34 s microrods (for 1), nanoprisms (for 2), and nanobelts (for 3).

35 TiO2 was not cytotoxic except for the nanobelt form, which was cytotoxic and induced significa

36 NO3)3 played a crucial role in promoting the nanobelt formation in the initial stage.

37 al and uniradial loop-by-loop winding of the nanobelt formed a complete ring.

38 c and piezophototronic effects in a-axis GaN nanobelts from 77 to 300 K is investigated.

39 The large-scale synthesis of Si3N4 nanobelts from quartz and graphite on a graphite-felt su

40 enerator (PNG) is built on the single PMN-PT nanobelt, generating a maximum output voltage of ~1.2 V.

41 The ultra-long alpha-Si3N4 nanobelts grew via a combined VLS-base and nanobranches

42 The preferential elongation of the nanobelts in the [010] direction contributes to this enh

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

46 However, the nanobelt may have some initial bending, surface roughnes

47 nc oxide nanorings formed by self-coiling of nanobelts may be useful for investigating polar surface-

48 Orthorhombic Pb3O2Cl2 (mendipite) nanobelts micrometers in length and tens of nanometers w

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

51 The transport properties of GaN nanobelts (NBs) are tuned using a piezotronic effect whe

52 The nanobelts of DD-PTCDI fabricated in solution can feasibl

53 Bending of polar-surface-dominated (PSD) nanobelts of ZnO can be explained by one of two processe

54 A single alpha-Si3N4 nanobelt or nanobranch gave a strong UV-blue emission ba

55 ZnS wurtzite nanobelts provide a model that is useful not only for un

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

58 The prepared nanobelts show an enhanced fluorescence emission and rel

59 As a result, the coated nanobelts show improved rate, cycling, and thermal capab

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

62 Relative to the CoSe2 nanobelts, the as-prepared Ag-CoSe2 nanobelts exhibited

63 -P25), anatase spheres (TiO2-A), and anatase nanobelts (TiO2-NBs)] and three forms of multiwalled car

64 phologies in aggregate: one-dimensional (1D) nanobelt vs zero-dimensional (0D) nanoparticle.

65 xide consisting of a superlattice-structured nanobelt was formed spontaneously in a vapor-solid growt

66 Negative DEP (repulsion) of the nanobelts was observed in the low-frequency range (<100

67 1-10 MHz), positive DEP (attraction) of the nanobelts was observed.

68 Ethanol suspended SnO(2) nanobelts were introduced into the microchannel, and the

69 ion, morphology, and microstructure of Si3N4 nanobelts were investigated by X-ray diffraction, Fourie

70 The single crystalline nanobelts were successfully fabricated with an ionic com

71 The Si3N4 nanobelts were well crystallized and grow along the [101

72 The Si3N4 nanobelts were ~4-5 mm long and ~60 nm thick and exhibit

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 = ~

76 change method to fabricate lamellar Ag-CoSe2 nanobelts with controllable conductivity.

77 esostructure; further exfoliation results in nanobelts with minimum sizes around 4 nm.

78 t also for improving synthesis of metastable nanobelts with quantum effects for electronic and optica

79 Single-crystalline anatase TiO(2) nanobelts with two dominant surfaces of (101) facet exhi

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