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Microscopic techniques transmission electron

The morphology of SLN dispersions can be investigated by different electron microscopic techniques. Transmission electron microscopy (TEM) is the most commonly used technique although also e.g. scanning electron microscopy (SEM) was used to study SLN dispersions. ... [Pg.410]

Like most other electron microscope techniques. transmission electron microscopy allows... [Pg.1112]

The extent of phase separation can be measured directly by the scanning electron microscope (SEM), transmission electron microscope (TEM), optical microscope, and light or X-ray scattering technique. It is also investigated indirectly by measuring certain physical properties, such as glass transition temperature. [Pg.111]

Modem instmments use all of these signals to extract information about a sample. These include the scanning electron microscope, the transmission electron microscope, the electron microprobe, and the auger nanoprobe. For many of these techniques, a conductive... [Pg.521]

Microscopy is a key approach which is frequently used for the characterizatitm of composite latex particles. There are a wide range of microscopes which can be used to analyze latexes, such as the optical microscope (OM), scanning electron microscope (SEM), transmission electron microscope (TEM), scanning transmission electron microscope (STEM) and the atomic force microscope (AFM). The choice of the microscope technique depends on the resolution and size range needed (i.e. nanometres to microns). The most important factor in microscopy is contrast. If the contrast is low, it becomes very difficult to distinguish between... [Pg.171]

In order to supplement micro-mechanical investigations and advance knowledge of the fracture process, micro-mechanical measurements in the deformation zone are required to determine local stresses and strains. In RTFs craze zones can develop that are important microscopic features around a crack tip governing strength behavior. Plastics fracture is preceded by the formation of a craze zone that is a wedge shaped region spanned by oriented micro-fibrils. Methods of craze zone measurements include optical emission spectroscopy, diffraction techniques, scanning electron microscope, and transmission electron microscopy. [Pg.861]

For physical techniques, transmission electron microscopy (TEM) seems to be the optimal technique for measuring the size of nanoparticles, as it allows us to look at them directly. However, its use is problematic. For example, the analysis is carried out on a microscopic amount of catalyst, and is hardly representative of the whole sample. Many observations must be made on each of several independently loaded samples in order to get reliable data, with the considerable expen-ditme of time that entails. Moreover, small or flat nanoparticles may be lost due to the insufficient contrast. However, a careful use of TEM is very valuable in some cases. [Pg.589]

When attempting to see membrane structures below one micrometer the possible microscopic techniques are electron microscopy (EM), which can be supplied by an additional elemental scanning (EDS) device (see Chapter 3). In this case and also in transmission electron microscopy (TEM) [7] the samples need to be dry. It is often quite difficult to study polymer membranes with these microscopic techniques because the densities of most materials are the same. Therefore, marker systems should be used like radioactive tracers, fluorescent staining or dendrimeric staining. Today, in environmental scanning electron microscopy (ESEM) one can work also with wet samples. [Pg.4]

Before the advent of the SEM (Johari, 1971), several tools, such as the optic microscope, the transmission electron microscope, the electron microprobe analyzer, and X-ray fluorescence, were employed to accomplish partial characterization this information was then combined for a fuller description of materials. Each of these tools has proficiency in one particular aspect and complements the information obtained with other instruments. The information is partial because of the inherent limitations of each method, such as the invariably cumbersome specimen preparation, specialized observation techniques and interpretation of results. [Pg.154]

Transmission electron microscopy (TEM) can resolve features down to about 1 nm and allows the use of electron diffraction to characterize the structure. Since electrons must pass through the sample however, the technique is limited to thin films. One cryoelectron microscopic study of fatty-acid Langmuir films on vitrified water [13] showed faceted crystals. The application of TEM to Langmuir-Blodgett films is discussed in Chapter XV. [Pg.294]

Historically, EELS is one of the oldest spectroscopic techniques based ancillary to the transmission electron microscope. In the early 1940s the principle of atomic level excitation for light element detection capability was demonstrated by using EELS to measure C, N, and O. Unfortunately, at that time the instruments were limited by detection capabilities (film) and extremely poor vacuum levels, which caused severe contamination of the specimens. Twenty-five years later the experimental technique was revived with the advent of modern instrumentation. The basis for quantification and its development as an analytical tool followed in the mid 1970s. Recent reviews can be found in the works by Joy, Maher and Silcox " Colliex and the excellent books by Raether and Egerton. ... [Pg.137]

The interface properties can usually be independently measured by a number of spectroscopic and surface analysis techniques such as secondary ion mass spectroscopy (SIMS), X-ray photoelectron spectroscopy (XPS), specular neutron reflection (SNR), forward recoil spectroscopy (FRES), scanning electron microscopy (SEM) and transmission electron microscopy (TEM), infrared (IR) and several other methods. Theoretical and computer simulation methods can also be used to evaluate H t). Thus, we assume for each interface that we have the ability to measure H t) at different times and that the function is well defined in terms of microscopic properties. [Pg.354]

The majority of PH As biosynthesis is performed by various microorganisms, especially bacteria. They can produce PHAs from a number of substrates and accumulate in their cells as carbon source and energy reserve under imbalanced growth conditions such as nutrient limitation. Fig.7 shows PHA accumulated in their cells that are characterized by transmission electron microscopic (TEM) technique. [Pg.50]

The Fe-B nanocomposite was synthesized by the so-called pillaring technique using layered bentonite clay as the starting material. The detailed procedures were described in our previous study [4]. X-ray diffraction (XRD) analysis revealed that the Fe-B nanocomposite mainly consists of Fc203 (hematite) and Si02 (quartz). The bulk Fe concentration of the Fe-B nanocomposite measured by a JOEL X-ray Reflective Fluorescence spectrometer (Model JSX 3201Z) is 31.8%. The Fe surface atomic concentration of Fe-B nanocomposite determined by an X-ray photoelectron spectrometer (Model PHI5600) is 12.25 (at%). The BET specific surface area is 280 m /g. The particle size determined by a transmission electron microscope (JOEL 2010) is from 20 to 200 nm. [Pg.389]

Electron energy loss spectroscopy An analytical technique used to characterize the chemistry, bonding, and electronic structure of thin samples of materials. It is normally performed in a transmission electron microscope. The inelastically scattered electron beams are spectroscopically analyzed to give the energy spectrum of electrons after the interaction. [Pg.10]

Figure 9.3. Characterization of mesoporous Ti02 films templated by Pluronics block copolymers using diverse characterization techniques XRD pattern (a), transmission electron microscope (TEM) image (b), dark-field TEM image (c), and isotherms of Kr adsorption (d).The Pluronic-templated Ti02 films were calcined at 400°C (solid points) and 600°C (open points). The films were prepared according to Alberius et al. (Ref. 14). Figure 9.3. Characterization of mesoporous Ti02 films templated by Pluronics block copolymers using diverse characterization techniques XRD pattern (a), transmission electron microscope (TEM) image (b), dark-field TEM image (c), and isotherms of Kr adsorption (d).The Pluronic-templated Ti02 films were calcined at 400°C (solid points) and 600°C (open points). The films were prepared according to Alberius et al. (Ref. 14).
Transmission electron microscopy (TEM) is a powerful and mature microstructural characterization technique. The principles and applications of TEM have been described in many books [16 20]. The image formation in TEM is similar to that in optical microscopy, but the resolution of TEM is far superior to that of an optical microscope due to the enormous differences in the wavelengths of the sources used in these two microscopes. Today, most TEMs can be routinely operated at a resolution better than 0.2 nm, which provides the desired microstructural information about ultrathin layers and their interfaces in OLEDs. Electron beams can be focused to nanometer size, so nanochemical analysis of materials can be performed [21]. These unique abilities to provide structural and chemical information down to atomic-nanometer dimensions make it an indispensable technique in OLED development. However, TEM specimens need to be very thin to make them transparent to electrons. This is one of the most formidable obstacles in using TEM in this field. Current versions of OLEDs are composed of hard glass substrates, soft organic materials, and metal layers. Conventional TEM sample preparation techniques are no longer suitable for these samples [22-24], Recently, these difficulties have been overcome by using the advanced dual beam (DB) microscopy technique, which will be discussed later. [Pg.618]

Microscopic techniques, 70 428 Microscopists, role of, 76 467 Microscopy, 76 464-509, See also Atomic force microscopy (AFM) Electron microscopy Light microscopy Microscopes Scanning electron microscopy (SEM) Transmission electron microscopy (TEM) acronyms related to, 76 506-507 atomic force, 76 499-501 atom probe, 76 503 cathodoluminescence, 76 484 confocal, 76 483-484 electron, 76 487-495 in examining trace evidence, 72 99 field emission, 76 503 field ion, 76 503 fluorescence, 76 483 near-held scanning optical,... [Pg.586]

Even under magnifications of the order of 105, micro PS looks rather homogeneous under the transmission electron microscope, as shown in Fig. 7.2a. This is in contrast to the microstructure of meso PS, which can be revealed at this magnification, as shown in Fig. 7.2 b. It requires HREM techniques to reveal the struc-... [Pg.129]


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