scholarly journals Atomic-Scale Structure Investigation of CeO2/YSZ/Si Hetero-Interface by High Resolution Analytical Electron Microscope

2006 ◽  
Vol 55 (6) ◽  
pp. 419-426
Author(s):  
Takanori KIGUCHI ◽  
Naoki WAKIYA ◽  
Nobuyasu MIZUTANI ◽  
Kazuo SHINOZAKI
Author(s):  
Yoshio Bando ◽  
Yoshizo Kitami ◽  
Mamoru Mitcmo

One of the limitations in the use of the conventional analytical electron microscope (AEM) with lower voltages of 100 to 200 kV is based on its poor image resolution compared to normal transmission electron microscope. Because of this, it is difficult to carry out structure determination by directly observing individual atom arrangements in crystals. However, a new AEM with an intermediate voltage of 400 kV (JEM-4000EX, TEMSCAN) is fully capable of high resolution observation under equipment of an energy dispersive x-ray spectrometer (EDS) and an electron energy loss spectrometer (EELS). The present paper shows crystal structure images of sialon polytypes and corresponding EDS and EELS spectra, and describes the usefullness of combined techniques of structure imaging and microanalysis in structure-composition determination.


2000 ◽  
Vol 64 (21) ◽  
pp. 3663-3673 ◽  
Author(s):  
P Fenter ◽  
H Teng ◽  
P Geissbühler ◽  
J.M Hanchar ◽  
K.L Nagy ◽  
...  

1998 ◽  
Vol 4 (S2) ◽  
pp. 212-213
Author(s):  
R.D. Leapman ◽  
C.R. Swyt-Thomas ◽  
D. v. Agoston ◽  
N. Pivovarova ◽  
S.B. Andrews

In high-resolution biological energy-dispersive x-ray (EDX) microanalysis it is often necessary to measure very low elemental concentrations. As an example, calcium, a physiologically important element, typically occurs in subcellular compartments at concentrations of 10-100 atomic parts per million (corresponding to 1-10 millimole/kg dry weight of sample) and it is ultimately desirable to measure the concentration of this element with a standard error of ±1 atomic ppm (or ± 0.1 millimole/kg). Detection of calcium in biological specimens is further complicated by the presence of relatively high levels of potassium (around 0.5 atomic % or 500 millimole/kg), which gives rise to overlap of the K Kβ and Ca Kα peaks in the EDX spectrum. Counting statistics are frequently the limiting factor for detectability, but this is not necessarily the case because in the analytical electron microscope it is possible to collect spectra for long periods using a high probe current.


2009 ◽  
Vol 17 (3) ◽  
pp. 8-11 ◽  
Author(s):  
T. Isabell ◽  
J. Brink ◽  
M. Kawasaki ◽  
B. Armbruster ◽  
I. Ishikawa ◽  
...  

Few electron optical inventions have revolutionized the TEM/ STEM as profoundly as the spherical aberration (Cs) corrector has. Characterization of technologically important materials increasingly needs to be done at the atomic or even sub-atomic level. This characterization includes determination of atomic structure as well as structural chemistry. With Cs correctors, the sub-Angstrom imaging barrier has been passed, and fast atomic scale spectroscopy is possible. In addition to improvements in resolution, Cs correctors offer a number of other significant improvements and benefits.


Author(s):  
T. Yanaka ◽  
A. Yonezawa ◽  
K. Oosawa ◽  
T. Iwaki ◽  
S. Suzuki ◽  
...  

Total design concept of EM-002A is to realize the following essential performance, that is, 1) attainment to ultimate high resolution as the conventional electron microscope, 2) complete compatibility of the high resolution mode and the analytical mode, 3) identification of the analyzed region and the observed image with atomic-level resolution, 4) observation of ultra fine structure of the biological specimen with maximum high contrast and so on.[Electron source] Accelerating voltage ranges from 20kV to 120kV in 6 steps Double Cockroft-Walton circuit is used as the high voltage generator and the high frequency ripple voltage is reduced to 0.1V. Electron gun assembly is composed of high voltage alumina insulator, whose shape is so well designed as to suppress micro-discharge to the negligible order.[Objective lens and specimen chamber] The objective lens is a strong symmetrical lens where the specimen chamber is located between the symmetrical upper and lower objective lens magnetic circuits. The objective lens has two powerful pole pieces, one being used for the ultra high resolution mode and the other for the standard mode.


Author(s):  
T. Honda ◽  
H. Watanabe ◽  
K. Ohi ◽  
E. Watanabe ◽  
Y. Kokubo

An analytical electron microscope equipped with a side-entry goniometer (SEG) has recently become more widespread than a conventional electron microscope by the following reasons: (1) a variety of specimen holders, (2) large tilting angle with eucentricity. However, the resolution of SEG-system is about 0.4 nm, whereas the resolution of 0.25 nm or less can be obtained by an electron microscope equipped with a top-entry goniometer (TEG)1). Factors determining the resolution of an electron microscope are (1) the aberration coefficients of the objective lens, (2) stability of exciting currents, (3) illumination angle of the electron beam on the specimen, (4) energy spread of the electron beam, and ( 5) vibration and specimen drift. It has been usually difficult to observe high resolution images during use of the SEG system, because of the aberration coefficients of the objective lens, vibration and specimen drift. In order to obtain a resolution of less than 0.3 nm with SEG system at 200 kV, both of spherical and chromatic aberration coefficients should be reduced less than 2 mm. Moreover, relative amplitude of vibration between the specimen and pole pieces should be less than a half value of resolution limit. The image drift should be less than 0.02 nm/sec, because the exposure time usually required for photographing a high resolution image is about 5 second.


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