Quantification of High Resolution Electron Microscopy and Electron Diffraction by the Imaging Plate

Author(s):  
Daisuke Shindo ◽  
Kenji Hiraga ◽  
Makoto Hirabayashi ◽  
Tetsuo Oikawa ◽  
Nobufumi Mori

Taking advantages of “Imaging Plate” (IP), i.e., a wide dynamic range and good linearity for electron intensity, high resolution electron microscope (HREM) images and electron diffraction (ED) patterns were quantitatively investigated. Observations of HREM images and ED patterns were made by the TEM-IP System (PIXsys TEM) using electron microscopes JEM-4000EX and JEM-2000FX, respectively. The data on the IP with an effective size of 102×77 mm2 was converted into digital data of 2048 × 1536 pixels with 4096 gray levels and analyzed with the IP-processor of the PIXsys TEM and a large-computer ACOS-2020.Since the IP is highly sensitive to incident electrons, the beam convergence can be lowered for HREM observations, and so the effect of the dumping envelope due to the beam divergence can be reduced. In Fig. 1, an HREM image of an oxide W-Ta-O, taken at a direct magnification of 1,500,000x and an exposure time of 2 s, shows fine contrast of partially ordered cation distributions. Although the phase contrast of the HREM image is rather weak, the image was recorded with about 1100 effective gray levels which are much larger than the 256 gray levels normally used in a conventional image processing system. Intensity distributions in two parts of the image near the crystal edge (A) and at a relatively thicker region (B) are visualized with perspective drawings in Figs. 2(a) and 2(b), and compared quantitatively with contour maps in Figs. 3(a) and 3(b), respectively. It was noticed that projected atomic potentials of the block structure unit (see the inset of Fig. 1) were revealed faithfully in A, having intensity minima at heavy atomic columns (H), whereas the low potential regions (L) have sharp intensity maxima at the thicker region B. These observed images will be compared quantitatively with calculated ones, taking into account the dynamical diffraction effect.

Author(s):  
D. Shindo

Imaging plate has good properties, i.e., a wide dynamic range and good linearity for the electron intensity. Thus the digital data (2048x1536 pixels, 4096 gray levels in log scale) obtained with the imaging plate can be used for quantification in electron microscopy. By using the image processing system (PIXsysTEM) combined with a main frame (ACOS3900), quantitative analysis of electron diffraction patterns and high-resolution electron microscope (HREM) images has been successfully carried out.In the analysis of HREM images observed with the imaging plate, quantitative comparison between observed intensity and calculated intensity can be carried out by taking into account the experimental parameters such as crystal thickness and defocus value. An example of HREM images of quenched Tl2Ba2Cu1Oy (Tc = 70K) observed with the imaging plate is shown in Figs. 1(b) - (d) comparing with a structure model proposed by x-ray diffraction study of Fig. 1 (a). The image was observed with a JEM-4000EX electron microscope (Cs =1.0 mm).


Author(s):  
M. Pan

It has been known for many years that materials such as zeolites, polymers, and biological specimens have crystalline structures that are vulnerable to electron beam irradiation. This radiation damage severely restrains the use of high resolution electron microscopy (HREM). As a result, structural characterization of these materials using HREM techniques becomes difficult and challenging. The emergence of slow-scan CCD cameras in recent years has made it possible to record high resolution (∽2Å) structural images with low beam intensity before any apparent structural damage occurs. Among the many ideal properties of slow-scan CCD cameras, the low readout noise and digital recording allow for low-dose HREM to be carried out in an efficient and quantitative way. For example, the image quality (or resolution) can be readily evaluated on-line at the microscope and this information can then be used to optimize the operating conditions, thus ensuring that high quality images are recorded. Since slow-scan CCD cameras output (undistorted) digital data within the large dynamic range (103-104), they are ideal for quantitative electron diffraction and microscopy.


Author(s):  
K. Hiraga ◽  
D. Shindo ◽  
M. Hirabayashi ◽  
T. Oikawa ◽  
N. Mori ◽  
...  

The “Imaging Plate” (IP) has three superior characteristics, i.e., high sensitivity to the electron beam, and a wide dynamic range and good linearity for electron dose compared with conventional EM films. The use of the IP is expected to lead to quantitative analysis of electron microscopy. The purpose of the present work is to examine the possibility of application of the IP to the quantitative analysis of electron diffraction and high-resolution electron microscopy.By using the TEM-IP System developed by Oikawa et al., which is published in this conference, electron diffraction patterns and high-resolution electron micrographs taken on the IP with an effective size of 102 х 77 mm2 were convertedinto digital data of 2048 х 1536 pixels with 4096 gray levels. Observations of electron diffraction patterns and high-resolution electron micrographs were made with a 200 kV (JEM-2000FX) and a 400 kV (JEM-4000EX) electron microscope, respectively.


Author(s):  
D. Shindo ◽  
T. Ohishi ◽  
S. Iijima ◽  
K. Hiraga ◽  
T. Oikawa ◽  
...  

The excellent properties of the imaging plate (IP), i.e., a wide dynamic range and good linearity for the electron intensity, are promising for quantitative analysis of diffuse scattering since they allow a small dynamical diffraction effect to be evaluated with ‘dynamical factor’. In this paper, we first present accurate measurement of thermal diffuse scattering (TDS), which contributes dominantly to the background of electron diffraction patterns. Secondly, we present a method of extracting weak signal scattering intensities from the background, and apply it to the analysis of diffuse scattering caused from short-range ordered structures.Electron microscope images were obtained with a JEM-2000EXII electron microscope. Image processing was carried out by using a computer system (ACOS 2020) at Tohoku University. Electron diffraction patterns were recorded by using the TEM-IP system (PIXsysTEM). The details of the IP data handling were presented in the previous paper.Figure 1 shows an electron diffraction pattern obtained from an Au thin film ( t ∼ 40nm) at room temperature.


Author(s):  
M. José-Yacamán

Electron microscopy is a fundamental tool in materials characterization. In the case of nanostructured materials we are looking for features with a size in the nanometer range. Therefore often the conventional TEM techniques are not enough for characterization of nanophases. High Resolution Electron Microscopy (HREM), is a key technique in order to characterize those materials with a resolution of ~ 1.7A. High resolution studies of metallic nanostructured materials has been also reported in the literature. It is concluded that boundaries in nanophase materials are similar in structure to the regular grain boundaries. That work therefore did not confirm the early hipothesis on the field that grain boundaries in nanostructured materials have a special behavior. We will show in this paper that by a combination of HREM image processing, and image calculations, it is possible to prove that small particles and coalesced grains have a significant surface roughness, as well as large internal strain.


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