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Sample-electron interaction

Electron ionization occurs when an electron beam crosses an ion source (box) and interacts with sample molecules that have been vaporized into the source. Where the electrons and sample molecules interact, ions are formed, representing intact sample molecular ions and also fragments produced from them. These molecular and fragment ions compose the mass spectrum, which is a correlation of ion mass and its abundance. El spectra of tens of thousands of substances have been recorded and form the basis of spectral libraries, available either in book form or stored in computer memory banks. [Pg.15]

To explore the possibility of electronic Interaction between the reduced titanium oxide and Pt, 1 ML of Pt was deposited on both fully oxidized and partially reduced T102. The reduced sample was prepared by Ar" " sputtering of the TIO2 substrate prior to metal deposition. Introducing reduced Tl centers at the Pt-Tl Interface. [Pg.84]

H2 TDS was used as the highest H2 desorption temperature (370 K) occurs below the temperature regime of encapsulation. For the reduced sample there was a 70% decrease In H2 chemisorption and a 33 K shift to lower temperatures when the unannealed sample (first H2 TDS) was compared to the sample annealed at 370 K (second H2 TDS). No change In the AES was observed after either the first or second TDS, showing that the Pt overlayer does not Island or encapsulate. We take these low Pt coverage experiments to Indicate an electronic Interaction (preferably bond formation, which does not require significant charge transfer) between Pt and reduced Tl species that Is activated at about 370 K. [Pg.84]

The electron interaction between nanosized gold particles and iron oxide support is only one factor which determines the properties of the gold/oxide system. For instance, in the Au/FeO,c/Si02/Si(l 0 0) model sample the depth profile (after successive Ar ion bombardment at a... [Pg.100]

The radiation that results from nuclear de-excitation has to be distinguished from the prompt radiation, i.e., from the photons that pass through the sample without interaction and from those that are scattered by the electrons. This is achieved if three characteristic times (Ati, At2, and t) are properly related ... [Pg.479]

Anomalous X-ray diffraction or resonant scattering refers to the modification of its intensity due to absorption processes involving interactions between the X-ray beam and the atoms in the sample. This interaction combines the chemical and short-range order sensitivity of absorption with the long-range order sensitivity of diffraction. This results in a chemical selectivity, i.e. it is possible to differentiate elements with close atomic numbers or even cations with the same number of electrons like Rb+ and Sr2+... [Pg.82]

In the NO-SCR by NH3, we note the highest reduction activity and selectivity on catalyst containing both vanadium and molybdenum than catalysts issued containing Mo or V, only. Furthermore, it should be underlined that a higher efficiency is obtained with ZSM-5 as host structure than samples issued from USY and MOR. Where a higher loss of porous volume were observed. On the basis of characterization data it has been suggested that the observed synergism in the SCR reaction is related to the existence of electronic interaction between the V and Mo species. In particular, it has been proposed that the presence of such electronic interactions modifies the catalysts redox properties, which have been claimed an essential property in the NO-SCR by NH3 reaction. [Pg.132]

We note, however, that measurements of protofilaments are not exact. Protofilament diameters are often measured from negative-stain electron micrographs, which may introduce errors and/or variability in size due to drying-induced deformation of the sample, sample-stain interactions, and variable staining (Chapman et al., 1990 Kiselev et al., 1990). Additionally,... [Pg.266]

Fig. 11.2. Diagram of the components of an El source. Gaseous samples (gases or vaporized liquids or solids) are introduced into the ionization chamber using a reservoir with molecular leak, direct insertion probe or as an eluent from a GC column. The collimated stream of 70 eV electrons interacts with the neutral analyte molecules to generate stable radical cations (M+ ) and unstable radical cations (M+ ) that undergo dissociation reactions to form the characteristic fragment ions observed in many El mass spectra. Fig. 11.2. Diagram of the components of an El source. Gaseous samples (gases or vaporized liquids or solids) are introduced into the ionization chamber using a reservoir with molecular leak, direct insertion probe or as an eluent from a GC column. The collimated stream of 70 eV electrons interacts with the neutral analyte molecules to generate stable radical cations (M+ ) and unstable radical cations (M+ ) that undergo dissociation reactions to form the characteristic fragment ions observed in many El mass spectra.
With this technique, under an especially equipped electron microscope, high-energy electrons are focused on a fine probe and directed at the point of interest in the specimen. The electrons interacting with the sample atoms cause the emission of the characteristic X-rays, which are detected and identified for qualitative analysis and used, generally through suitable standardization, to perform also a quantitative analysis. [Pg.66]

To understand the sample (material) magnetism, one needs to comprehend the nature of molecular magnetism. The two paramagnetic components of the salt can take part in electron exchanges (EE). One type of electron exchange is D+ <— A and the other is D+ — A . These types of electron interactions are depicted in EE graphs from 1 to 5 in Scheme 8.14. [Pg.420]

In Auger transitions, incident electrons interact with the inner shell electrons E of the sample. The vacancy created by an ejected inner shell electron is filled by an outer shell electron (Ei), and a second outer shell electron ( 2) is ejected leaving the atom in a doubly ionized state. The electrons ejected from the outer shells are called Auger electrons, named after the Frenchman Pierre Auger, who discovered the effect. Thus, AES measures the energies of the Auger electrons ( a) emitted from the first 10 A of a sample surface. The energy equation is expressed as... [Pg.431]

In transmission electron microscopy (TEM), a beam of highly focused and highly energetic electrons is directed toward a thin sample (< 200 nm) which might be prepared from solution as thin film (often cast on water) or by cryocutting of a solid sample. The incident electrons interact with the atoms in the sample, producing characteristic radiation. Information is obtained from both deflected and nondeflected transmitted electrons, backscattered and secondary electrons, and emitted photons. [Pg.133]

In solution, however, lattice-stabilisation effects no longer apply and the dissociation of homocyclic sulfur dications occurs readily. The formation of the cation radical 85" in solutions of sulfur in 65% oleum has been firmly established by EPR studies of samples that were 92% enriched with 8 (/= 3/2). The 16-line spectrum shown in Figure 12.13 is consistent with a cyclic structure in which the unpaired electron interacts with five equivalent 8 nuclei [(2x5x3/2)-Hl = 16]. [Pg.287]

For thick substrates, backscattered electrons from the substrate decrease contrast and the minimum dimension increases to about 20 nm. For thick resists, and samples thick compared to the primary electron penetration range, electron scattering in the resist (forward scattering) and backscattering of electrons from the substrate, become more important than the electron interaction range. In these cases, exposure dose is sometimes altered according to the local pattern density to compensate for variations in the backscattered... [Pg.25]

Polymers of poly(L-ornithine) possessing varying contents of azobenzene groups, from 20% up to almost 100% [Scheme 5, VIII (n= 3)], were found to be essentially a-helical in HFP when the samples were kept in the dark. The CD spectra also exhibited a couplet of bands centered at about 320 nm, attributed to electronic interactions between the azo side chains in the trans configuration. Irradiation at 360 nm and the consequent trans—xis photoisomerization, abolished the side chain CD... [Pg.414]


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Electronic interactions

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