Growth of Single-Crystalline Cubic GaN Nanotubes with Rectangular Cross-Sections

2004 ◽  
Vol 16 (16) ◽  
pp. 1465-1468 ◽  
Author(s):  
J. Q. Hu ◽  
Y. Bando ◽  
J. H. Zhan ◽  
F. F. Xu ◽  
T. Sekiguchi ◽  
...  
Keyword(s):  
Cross Sections ◽  
Single Crystalline ◽  
Cubic Gan

Growth of Single-Crystalline Cubic GaN Nanotubes with Rectangular Cross-Sections.

ChemInform ◽  
2004 ◽  
Vol 35 (45) ◽  
Author(s):  
Junqing Hu ◽  
Yoshio Bando ◽  
Jinhua Zhan ◽  
Fangfang Xu ◽  
Takashi Sekiguchi ◽  
...  
Keyword(s):  
Cross Sections ◽  
Single Crystalline ◽  
Cubic Gan

scholarly journals Synthesis of Single Crystalline Tellurium Nanotubes with Triangular and Hexagonal Cross Sections

2006 ◽  
Vol 110 (2) ◽  
pp. 791-795 ◽  
Author(s):  
Paritosh Mohanty ◽  
Taejoon Kang ◽  
Bongsoo Kim ◽  
Jeunghee Park
Keyword(s):  
Cross Sections ◽  
Single Crystalline

Self-Assembled Highly Faceted Wurtzite-Type ZnS Single-Crystalline Nanotubes with Hexagonal Cross-Sections.

ChemInform ◽  
2005 ◽  
Vol 36 (44) ◽  
Author(s):  
Long-Wei Yin ◽  
Yoshio Bando ◽  
Jin-Hua Zhan ◽  
Mu-Sen Li ◽  
Dmitri Golberg
Keyword(s):  
Cross Sections ◽  
Single Crystalline ◽  
Self Assembled

Self-Assembled Highly Faceted Wurtzite-Type ZnS Single-Crystalline Nanotubes with Hexagonal Cross-Sections

2005 ◽  
Vol 17 (16) ◽  
pp. 1972-1977 ◽  
Author(s):  
L.-W. Yin ◽  
Y. Bando ◽  
J.-H. Zhan ◽  
M.-S. Li ◽  
D. Golberg
Keyword(s):  
Cross Sections ◽  
Single Crystalline ◽  
Self Assembled

A Simple Solution Route to Single-Crystalline Sb2O3Nanowires with Rectangular Cross Sections

2006 ◽  
Vol 110 (37) ◽  
pp. 18225-18230 ◽  
Author(s):  
Zhengtao Deng ◽  
Fangqiong Tang ◽  
Dong Chen ◽  
Xianwei Meng ◽  
Li Cao ◽  
...  
Keyword(s):  
Cross Sections ◽  
Simple Solution ◽  
Single Crystalline ◽  
Solution Route

Growth of Single-Crystalline Tris-(8-Hydroxyquinoline) Gallium Uniform Sub-Microrods and their Optical Properties

2017 ◽  
Vol 898 ◽  
pp. 1817-1823
Author(s):  
Cheng Hu Dai ◽  
Zhi Xian Wei ◽  
Zhi Yong Pang ◽  
Sheng Hao Han
Keyword(s):  
Optical Properties ◽  
Absorption Spectrum ◽  
Cross Sections ◽  
Organic Materials ◽  
Energy Gap ◽  
Blue Shift ◽  
Molecular Packing ◽  
Single Crystalline ◽  
One Dimensional ◽  
Α Phase

One dimensional (1-D) organic materials have a bright prospect in the field of optoelectronics. Intrigued by these, 1-D uniform sub-micrometer tris-(8-hydroxyquinoline) gallium (GaQ3) rods were prepared with surfactant by an extremely facial method. The GaQ3 rods with hexagonal cross sections had excellent crystallinity and optical properties. The measurement of the absorption spectrum showed that there was an obvious blue shift comparing with the GaQ3 film. This can be explained by that the molecular packing in the α-phase rods has a looser interligand spacing compared with the GaQ3 film, consequently resulting in reduced orbital overlap and larger energy gap.

Single-Crystalline Vanadium Dioxide Nanowires with Rectangular Cross Sections

2005 ◽  
Vol 127 (2) ◽  
pp. 498-499 ◽  
Author(s):  
Beth S. Guiton ◽  
Qian Gu ◽  
Amy L. Prieto ◽  
Mark S. Gudiksen ◽  
Hongkun Park
Keyword(s):  
Cross Sections ◽  
Vanadium Dioxide ◽  
Single Crystalline

Analysis of STEM micrographs of thick objects

1978 ◽  
Vol 36 (2) ◽  
pp. 106-107
Author(s):  
S. Golladay
Keyword(s):  
Inelastic Scattering ◽  
Multiple Scattering ◽  
Mass Distribution ◽  
Cross Sections ◽  
Phase Contrast ◽  
Image Point ◽  
Contrast Effects ◽  
Total Cross Sections ◽  
Elastic And Inelastic Scattering

The theory of multiple scattering has been worked out by Groves and comparisons have been made between predicted and observed signals for thick specimens observed in a STEM under conditions where phase contrast effects are unimportant. Independent measurements of the collection efficiencies of the two STEM detectors, calculations of the ratio σe/σi = R, where σe, σi are the total cross sections for elastic and inelastic scattering respectively, and a model of the unknown mass distribution are needed for these comparisons. In this paper an extension of this work will be described which allows the determination of the required efficiencies, R, and the unknown mass distribution from the data without additional measurements or models. Essential to the analysis is the fact that in a STEM two or more signal measurements can be made simultaneously at each image point.

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