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Emission of x-rays

Systems, based on a method of inspection of slice by slice, in a number of cases allow to solve put problems. But for obtaining of higher resolution it is necessary to have an opportunity to increase number of inspected slices. It results in significant increasing of collection data time that is inadmissible in some applications. Besides this, the maximum allowable number of researched slices is rigidly limited by hardware opportunities of tomographs, and also by level of emission of x-ray sources. [Pg.216]

Used effects Phonon excitation (20 meV-1 eV) Plasmon and interband excitations (1-50 eV) Inner-shell ionization (A = ionization energy loss) Emission of x-ray (continuous/characteristic, analytical EM)... [Pg.1626]

Edx is based on the emission of x-rays with energies characteristic of the atom from which they originate in Heu of secondary electron emission. Thus, this technique can be used to provide elemental information about the sample. In the sem, this process is stimulated by the incident primary beam of electrons. As will be discussed below, this process is also the basis of essentially the same technique but performed in an electron spectrometer. When carried out this way, the technique is known as electron microprobe analysis (ema). [Pg.271]

Figure 1 Schematic of an EDS system on an electron column. The incident electron interacts with the specimen with the emission of X rays. These X rays pass through the window protecting the Si (Li) and are absorbed by the detector crystal. The X-ray energy is transferred to the Si (Li) and processed into a dig-itai signal that is displayed as a histogram of number of photons versus energy. Figure 1 Schematic of an EDS system on an electron column. The incident electron interacts with the specimen with the emission of X rays. These X rays pass through the window protecting the Si (Li) and are absorbed by the detector crystal. The X-ray energy is transferred to the Si (Li) and processed into a dig-itai signal that is displayed as a histogram of number of photons versus energy.
Another application involves the measurement of copper via the radioisotope Cu (12.6-hour half-life). Since Cu decays by electron capture to Ni ( Cu Ni), a necessary consequence is the emission of X rays from Ni at 7.5 keV. By using X-ray spectrometry following irradiation, sensitive Cu analysis can be accomplished. Because of the short range of the low-energy X rays, near-surface analytical data are obtained without chemical etching. A combination of neutron activation with X-ray spectrometry also can be applied to other elements, such as Zn and Ge. [Pg.678]

The basis of XRE analysis is the photoelectric absorption and the subsequent emission of X-ray photons characteristic of the fingerprints of analyte atoms in the sample. Element composition can be quantified by the relative intensities of the indivi-... [Pg.181]

When the accelerating voltage reaches a specific value (dependent on the nature of the target material), the electrons from the beam are capable of knocking out core-level electrons from the target material, thus giving rise to core vacancies. These are quickly filled by electrons in upper levels and this results in the emission of X-ray photons of characteristic energies which depend on the... [Pg.267]

Not all excited atoms will relax by the re-emission of X-rays and the... [Pg.339]

This particular transition results in the emission of x-ray radiation known as the K,y line. For transfer from the M shell into the K shell, the energy of the Kp line is given by ... [Pg.220]

In interaction with atomic nuclei leading to the emission of x-ray photons. This is referred to as Bremsstrahlung (electromagnetic radiation emitted when a charged particle changes its velocity due to such interaction). [Pg.28]

Fig. 6.19.(a) Emission of X-rays from an aluminum or magnesium target, and (b) the scattering behavior of diffracted X-rays. (Reprinted with permission from G. A. Somorjai, Chemistry in Two Dimensions Surfaces, Cornell University Press, 1981, Fig. 2.8.)... [Pg.79]

Electron capture decay produces a vacancy in the atomic electron shells and secondary processes that lead to filling that vacancy by the emission of X-rays and Auger electrons occur. These X-rays permit the detection of EC decays. [Pg.213]

Doppler velocity may provide a Mossbauer spectrum with a large increase in the signal to noise ratio compared to that obtained in the transmission mode. The type of radiation used to generate the scattered Mossbauer spectrum depends on the internal conversion coefficient a a large value of a, which favors the emission of X rays by the Mdssbauer isotope, makes X-ray detection appropriate, while a small value of a favors y-ray detection. [Pg.163]

Neutron activation analysis (NAA) technique has also been used for determining low levels of barium in human blood (Olehy et al. 1966). This technique is based on the interaction of the nuclei of individual barium atoms with neutron irradiation, resulting in the emission of x-rays (photons). Detection limits of 7 pg barium/L of erythrocyte and 66 pg barium/L of plasma were obtained (Olehy et al. 1966). The advantages of the NAA technique are its nondestructive nature of sample and minimum sample manipulation. Disadvantages of this technique include its high costs and a nuclear reactor may not be readily available to many laboratories. [Pg.89]

We determined the absorption of the laser pulse by recording the scattered and specularly rehected laser light with 47r-arranged calorimeters. In front of the calorimeters, a 2-mm thick quartz plate was installed to block charged particles and X-rays. In some experiments, low-order harmonics of the laser beam were analyzed using a monochromatic meter. Crystal spectrometers were used to record the plasma self-emission of X-rays, from which the ionization states of the target materials were obtained. [Pg.322]

From a simple cascade calculation model It can be shown that about 60% of the muons stopped in the target will pass through the D levels of course, the natural emission of X-rays, during the cascade of the iT, represents our main physical background, from which we have to sort out the small increase due to the laser-stimulated emission. [Pg.993]

Scanning electron microsopy (SEM) and electron microprobe analysis (EMA) — A scanning focused electron beam causes the ionization of core levels similar to scanning AES. An alternative and thus a competing process to the ejection of Auger electrons is the emission of X-ray fluorescence radiation. These X-rays... [Pg.651]

Not all excited atoms will relax by the re-emission of X-rays and the proportion that do is known as the fluorescence yield factor radiation absorbed /, and the intensity of the fluorescent emission If are thus related by... [Pg.336]

A solid sample is bombarded with a beam of energetic protons, causing the emission of x-rays, characteristic of the elements present. May employ a microbeam (hence MICROPIXE)... [Pg.447]

Iodine Isotope. There are many radioactive isotopes of iodine. Four are commercially available. For most purposes, one of these, I, is the most useful because it has a reasonable half-life (60 days), it decays to a stable isotope, and it decays by an electron capture process that results in a cascade of low energy electrons and the emission of X-rays and y-rays. [Pg.248]

During bombardment of solids with electrons or X-rays secondary electrons from the target atoms are excited and partly ejected. The ejection ofX andL electrons is followed by a reordering process which leads to the emission of X-rays or Auger electrons from outer shells. [Pg.40]


See other pages where Emission of x-rays is mentioned: [Pg.448]    [Pg.194]    [Pg.272]    [Pg.628]    [Pg.99]    [Pg.349]    [Pg.150]    [Pg.463]    [Pg.1639]    [Pg.339]    [Pg.222]    [Pg.2]    [Pg.49]    [Pg.1685]    [Pg.13]    [Pg.59]    [Pg.108]    [Pg.339]    [Pg.177]    [Pg.231]    [Pg.125]    [Pg.991]    [Pg.333]    [Pg.341]    [Pg.431]    [Pg.36]    [Pg.343]   
See also in sourсe #XX -- [ Pg.74 ]




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Emission x-ray

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