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In the context of electron microscopists' changing attitudes to
charging effects, some basic aspects of these phenomenona are surveyed.
Methods of mapping internal charge distributions such as doping levels
in semiconductors, trap distributions, or internal electric fields in
insulators are discussed.
Quantitative Transmission Electron Microscopy at Jülich,
Germany
With the availability of resolution boosting and delocalization
minimizing techniques, for example, spherical aberration correction and
exit-plane wave function reconstruction, high-resolution transmission
electron microscopy is drawing to a breakthrough with respect to the
atomic-scale imaging of common semiconductor materials. In the present
study, we apply a combination of these two state-of-the-art techniques
to investigate lattice defects in GaAs-based heterostructures at atomic
resolution. Focusing on the direct imaging of stacking faults as well
as the core structure of edge and partial dislocations, the practical
capabilities of both techniques are illustrated. For the first time, we
apply the technique of bright-atom contrast imaging at negative
spherical aberration together with an appropriate overfocus setting for
the investigation of lattice defects in a semiconductor material. For
these purposes, the elastic displacements associated with lattice
defects in GaAs viewed along the [110] zone axis
are measured from experimental images using reciprocal space strain map
algorithms. Moreover, we demonstrate the benefits of the retrieval of the
exit-plane wave function not only for the elimination of residual
imaging artefacts but also for the proper on-line alignment of
specimens during operation of the electron microscope—a basic
prerequisite to obtain a fair agreement between simulated images and
experimental micrographs.
Trichomonads are flagellate protists, and among them Trichomonas
vaginalis and Tritrichomonas foetus are the most studied
because they are parasites of the urogenital tract of humans and
cattle, respectively. Microscopy provides new insights into the cell
biology and morphology of these parasites, and thus allows better
understanding of the main aspects of their physiology. Here, we review
the ultrastructure of T. foetus and T. vaginalis,
stressing the participation of the axostyle in the process of cell
division and showing that the pseudocyst may be a new form in the
trichomonad cell cycle and not simply a degenerative form. Other
organelles, such as the Golgi and hydrogenosomes, are also reviewed.
The virus present in trichomonads is discussed.
Ultrahigh-resolution imaging may be achieved using modifications of
the off-axis holography scheme in a scanning transmission electron
microscopy (STEM) instrument equipped with one or more electrostatic
biprisms in the illuminating system. The resolution is governed by the
diameter of a reference beam, reduced by channeling through a line of
atoms in an atomic-focuser crystal. Alternatively, the off-axis
holography may be combined with the Rodenburg method in which a
four-dimensional data set is obtained by recording a nanodiffraction
pattern from each point of the specimen as the incident beams are
scanned. An ultrahigh-resolution image is derived by computer
processing to give a particular two-dimensional section of this data
set. The large amount of data recording and data processing involved
with this method may be avoided if the two-dimensional section is
derived by recording the hologram while the four beams produced by two
perpendicular biprisms are scanned in opposing directions across the
specimen by varying the voltages on the biprisms. An equivalent scheme
for conventional TEM is also possible. In each case, the complex
transmission function of the specimen may be derived and resolutions of
about 0.05 nm may be expected.
Atom probe tomography is a technique for the nanoscale
characterization of microstructural features. Analytical techniques
have been developed to estimate the size, composition, and other
parameters of features as small as 1 nm from the atom probe tomography
data. These methods are outlined and illustrated with examples of
yttrium-, titanium-, and oxygen-enriched particles in a mechanically
alloyed, oxide-dispersion-strengthened steel.
Extended abstract of a paper presented at the Pre-Meeting Congress: Materials Research in an Aberration-Free Environment, at Microscopy and Microanalysis 2004 in Savannah, Georgia, USA, July 31 and August 1, 2004.
Crystal structure of nano-scale precipitates in age-hardening
aluminum alloys is a challenge to crystallography. The utility of
selected area electron diffraction intensities from embedded
precipitates is limited by double scattering via matrix reflections.
This effect can be signally reduced by the precession technique, which
we have used to collect extensive intensity data from the semicoherent,
metastable η′-precipitate in the Al-Zn-Mg alloy system. A
structure model in the space group P-62c is proposed from
high-resolution microscopy and electron diffraction intensities. The
advantages of using the precession technique for quantitative electron
diffraction is discussed.
This article summarizes findings from our previous investigations and
recent studies concerning precipitation in a maraging steel of type
13Cr-9Ni-2Mo-2Cu (at.%) with small additions of Ti (1 at.%) and Al (0.7
at.%). The material was investigated after aging at 475°C up to 400
h using both conventional and three-dimensional atom-probe analyses.
The process of phase decomposition in the steel proved to be
complicated. It consisted of precipitation of several phases with
different chemistry. A Cu-rich phase was first to precipitate and Mo
was last in the precipitation sequence. The influence of the complex
precipitation path on the material properties is discussed. The
investigation clearly demonstrated the usefulness of the applied
techniques for investigation of nanoscale precipitation. It is also
shown that, complementary methods (such as TEM and EFTEM) giving
structural and chemical information on a larger scale must be applied
to explain the good properties of the steel after prolonged aging.
The three-dimensional structure of the Plasmodium falciparum
ring stage has been explored by reconstruction from serial sections and
stereoscopic examination of tilted sections. The ring-like light
microscopic appearance is related to the shape and contents of the
biconcave discoidal parasite at this stage, its thick perimeter
containing most of the ribosomes and its thin center containing smooth
membrane organelles. The shapes of rings vary between flat and curved
cuplike forms. The rough endoplasmic reticulum is a branched network
continuous with the nuclear envelope. Evidence for a simple Golgi
complex is seen in the presence on the outer nuclear envelope of a
locus of coated vesicle budding associated with a single membranous
cisterna or cluster of smooth vesicles. In middle and late stage rings
this complex migrates along an extension of the nuclear envelope
continuous with the rough endoplasmic reticulum. Evidence is also
presented for a mechanism of exporting membrane from the parasite into
the parasitophorous vacuole membrane and beyond into the red blood
cell, by means of double-membraned vesicle-based exocytosis.
When a dielectric is irradiated by electrons with energy E
of several kiloelectron volts, a large number of processes take place:
backscattering of incident electrons, excitation and ionization of the
electrons in the dielectric with binding energies lower than
E, creation of excitons, radiative and nonradiative decays of
the excited and ionized states, slowing down of the primary and
secondary electrons, and thermalization in the conduction band. The
thermalized electrons can move freely in the unoccupied conduction
states of the material. If electric connection exists between the
dielectric and the apparatus, then the charges normally flow out.
Thermalized electrons can also be trapped in excited levels localized
in the band gap of the dielectric and nonradiative and radiative
recombinations from these levels can be observed. The number of the
trapped electrons varies with the structural characteristics of the
dielectric. In a monocrystal, this number is weak because the number of
the defect states in the band gap is small, making the localization of
the charges restricted. In contrast, in a polycrystal or amorphous
material, the number of the trapped electrons can be large and
increases with the disorder. Information on the charge effects suffered
by the sample during its irradiation can be deduced by studying the
trapping of electrons in localized states and, consequently, by
analyzing radiations emitted from these states in the visible and X-ray
ranges. In the case of oxides, F+ centers
(oxygen–ion vacancy having trapped one electron) and F
centers (F+ center having trapped a second
electron) are generally present. We will show that the
F+ [harr ] F conversion can be used to
study the dynamic of the trapping in the oxides. Application to various
samples of crystallized and amorphous alumina will be presented.
This article presents my reminiscences of the work in Chicago on the
correction or reduction of lens aberrations. Studies began in the early
1960s and extended over a period of almost 40 years, although it was
never the primary focus of the work of the laboratory. The account is
almost entirely based on my own memory, which is not a very reliable
instrument. It is not intended to be a review and is more accurately
describable as a personal recollection.
Quantitative Transmission Electron Microscopy at Jülich,
Germany
The pressure of crack-shaped cavities formed in silicon upon
implantation with helium and subsequent annealing is quantitatively
determined from the measurement of diffraction contrast features
visible in transmission electron micrographs taken under well-defined
dynamical two-beam conditions. For this purpose, simulated images,
based on the elastic displacements associated with a Griffith crack,
are matched to experimental micrographs, thus yielding unambiguous
quantitative data on the ratio p/μ of the cavity
pressure to the silicon matrix shear modulus. Experimental results
demonstrate cavity radii of some 10 nm and p/μ values
up to 0.22, which may be regarded as sufficiently high for the emission
of dislocation loops from the cracks.
Biological Sciences: Advances in Imaging of Cytoskeletal Dynamics, Structure, Regulation, and Functions
Biological Sciences: 3D Electron Microscopy of Macromolecules: Unveiling Structural/Functional Relationships through Imaging Conformational Changes
Biological Sciences: Biomaterials
Biological Sciences: Imaging Technology in the Study of Cardiovascular Development and Disease
Biological Sciences: Microscopy of Plant Pathogenic Microbes and Their Interactions with Host Plants
Biological Sciences: Microscopic Analysis of Nervous System Development and Function
Biological Sciences: Microscopy in Microbiology
Physical Sciences: Characterization of Novel Nanostructures for Applications in Sensing, Nanoelectronics and Biotechnology
Physical Sciences: The Characterization and Performance of Advanced Coatings and Thin Films
Physical Sciences: Interfaces: A Symposium in Honor of Manfred Rühle
Physical Sciences: Metallography of High-Temperature Materials and Life Assessment
Physical Sciences: Microscopy and Microanalysis in Catalysis
Physical Sciences: Microscopy and Microanalysis of Nanotechnology
Physical Sciences: Nanostructure and Dynamics of Molecular Assemblies: Biomembranes, Proteins, Surfactants, Polymers and Liquid-crystals
Physical Sciences: Unraveling Magnetic Structure at the Nanoscale to Understand Magnetic Properties
Advances in Instrumentation and Techniques: Accessorizing the SEM
Advances in Instrumentation and Techniques: Advances in Confocal Optical Microscopy Technology
Advances in Instrumentation and Techniques: Advances in Visualizing Tissue Chemistry at the Cellular Level Using Infrared and Raman Microspectroscopy and Imaging
Advances in Instrumentation and Techniques: Analysis of Protein Dynamics in Living Cells by Quantitative Light Microscopy
Advances in Instrumentation and Techniques: Biological Specimen Preparation and Labeling
Advances in Instrumentation and Techniques: Digital Imaging
Advances in Instrumentation and Techniques: Electron Energy-Loss and X-ray Absorption Spectroscopies: Focus on Anisotropic Properties
Advances in Instrumentation and Techniques: FIB/Dual Platform Applications and Techniques in Biological and Physical Sciences
Advances in Instrumentation and Techniques: In Situ Characterization of Dynamic Processes by Variable Pressure Electron Microscopy
Advances in Instrumentation and Techniques: Metallography: Preparation, Application and Evaluation for the 21st Century
Advances in Instrumentation and Techniques: Metallurgical Failure Analysis: Present and Future
Advances in Instrumentation and Techniques: Microscopy and Microanalysis in the Real World: Textiles, Pharmaceuticals, Photonics, and Biomedical/Forensics
Advances in Instrumentation and Techniques: Micro X-ray Techniques: New Compositional and Structural Characterization Tools
Advances in Instrumentation and Techniques: Order in Disorder: Probing the Structure of Amorphous Materials
Advances in Instrumentation and Techniques: Quantitative Techniques in Biological Imaging
Advances in Instrumentation and Techniques: Quantitative X-ray Microanalysis: Focus on Extraterrestrial and Terrestrial Specimens
Advances in Instrumentation and Techniques: Scanned Probe Microscopy: Probing Surfaces at the Nanoscale
Advances in Instrumentation and Techniques: Stereology and 3D Digital Imaging
Advances in Instrumentation and Techniques: Tomographic Techniques in Biological and Physical Sciences
The resolution achieved in low-dose electron microscopy of biological
macromolecules is significantly worse than what can be obtained on the
same microscopes with more robust specimens. When two-dimensional
crystals are used, it is also apparent that the high-resolution image
contrast is much less than what it could be if the images were perfect.
Because specimen charging is one factor that might limit the contrast
and resolution achieved with biological specimens, we have investigated
the use of holey support films that have been coated with a metallic
film before depositing specimens onto a thin carbon film that is
suspended over the holes. Monolayer crystals of paraffin
(C44H90) are used as a test specimen for this
work because of the relative ease in imaging Bragg spacings at ∼0.4
nm resolution, the relative ease of measuring the contrast in these
images, and the similar degree of radiation sensitivity of these
crystals when compared to biological macromolecules. A metallic coating
on the surrounding support film does, indeed, produce a significant
improvement in the high-resolution contrast for a small fraction of the
images. The majority of images show little obvious improvement,
however, and even the coated area of the support film continues to show
a significant amount of beam-induced movement under low-dose
conditions. The fact that the contrast in the best images can be as
much as 25%–35% of what it would be in a perfect image is
nevertheless encouraging, demonstrating that it should be possible, in
principle, to achieve the same performance for every image. Routine
data collection of this quality would make it possible to determine the
structure of large, macromolecular complexes without the need to grow
crystals of these difficult specimen materials.
The goal of this article is first to review the charging effects
occurring when an insulating material is subjected to electron
irradiation in a scanning electron microscope (SEM) and next their
consequences from both scanning electron microscopy and electron probe
microanalysis (EPMA) points of view. When bare insulators are observed,
the so-called pseudo mirror effect leads to an anomalous contrast and
also to an erroneous surface potential,
VS, measurement when a Duane–Hunt
limit (DHL) method is used. An alternative possibility is to use an
electron toroidal spectrometer (ETS), specially adapted to a SEM, which
directly gives the VS value. In the case
of a bulk specimen coated with a grounded layer, although the layer
prevents external effects of the trapped charge, the electric field
beneath the coating is reinforced and leads to loss of ionizations that
reduces the number of generated X-ray photons. To take into account
both effects mentioned above, whether the studied insulator is coated
or not, a method is proposed to deduce the trapped charge inside the
insulator and the corresponding internal or external electric field.
Improvements in STEM and TEM Instrumentation for Materials Science Applications
Extended abstract of a paper presented at the Pre-Meeting Congress: Materials Research in an Aberration-Free Environment, at Microscopy and Microanalysis 2004 in Savannah, Georgia, USA, July 31 and August 1, 2004.