scholarly journals Observation of the crystalline orientation dependence of the semiconductor–metal transition for thermal oxidation induced VO2 films over amorphous quartz glasses

AIP Advances ◽  
2021 ◽  
Vol 11 (12) ◽  
pp. 125232
Author(s):  
Mengtao Gong ◽  
Fei Huang ◽  
Shouqin Tian ◽  
Xiujian Zhao ◽  
Baoshun Liu
2011 ◽  
Vol 88 (5) ◽  
pp. 605-609 ◽  
Author(s):  
Tsuyoshi Nishimura ◽  
Osamu Nakatsuka ◽  
Shingo Akimoto ◽  
Wakana Takeuchi ◽  
Shigeaki Zaima

2008 ◽  
Vol 47 (3) ◽  
pp. 1461-1464 ◽  
Author(s):  
Youjun Fan ◽  
Ratno Nuryadi ◽  
Zainal A. Burhanudin ◽  
Michiharu Tabe

2005 ◽  
Vol 86 (16) ◽  
pp. 162903 ◽  
Author(s):  
Qing-Ming Wang ◽  
Yongping Ding ◽  
Qingming Chen ◽  
Minhua Zhao ◽  
Jinrong Cheng

2018 ◽  
Vol 57 (4S) ◽  
pp. 04FB06 ◽  
Author(s):  
Takuya Nagura ◽  
Shingo Kawachi ◽  
Kenta Chokawa ◽  
Hiroki Shirakawa ◽  
Masaaki Araidai ◽  
...  

Author(s):  
William J. Baxter

In this form of electron microscopy, photoelectrons emitted from a metal by ultraviolet radiation are accelerated and imaged onto a fluorescent screen by conventional electron optics. image contrast is determined by spatial variations in the intensity of the photoemission. The dominant source of contrast is due to changes in the photoelectric work function, between surfaces of different crystalline orientation, or different chemical composition. Topographical variations produce a relatively weak contrast due to shadowing and edge effects.Since the photoelectrons originate from the surface layers (e.g. ∼5-10 nm for metals), photoelectron microscopy is surface sensitive. Thus to see the microstructure of a metal the thin layer (∼3 nm) of surface oxide must be removed, either by ion bombardment or by thermal decomposition in the vacuum of the microscope.


Author(s):  
G. Thomas ◽  
K. M. Krishnan ◽  
Y. Yokota ◽  
H. Hashimoto

For crystalline materials, an incident plane wave of electrons under conditions of strong dynamical scattering sets up a standing wave within the crystal. The intensity modulations of this standing wave within the crystal unit cell are a function of the incident beam orientation and the acceleration voltage. As the scattering events (such as inner shell excitations) that lead to characteristic x-ray production are highly localized, the x-ray intensities in turn, are strongly determined by the orientation and the acceleration voltage. For a given acceleration voltage or wavelength of the incident wave, it has been shown that this orientation dependence of the characteristic x-ray emission, termed the “Borrmann effect”, can also be used as a probe for determining specific site occupations of elemental additions in single crystals.


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