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Electron Source Preparation

Preparation of electron or beta sources is accomplished by observing these two [Pg.444]

The source backing material should be as thin as possible, to avoid backscat-tering from the source. [Pg.444]

A thin piece of Mylar or metallic foil (a few microns thick) is mounted on a metal ring (see Fig. 13.13). This is the source support. [Pg.444]

Using a pipette, a small amount of the radioisotope is placed on the source support. [Pg.444]


Microsomes are a membrane fraction prepared from subcellular structures containing cytochrome P450 and its reductase. Cyt P450 reductase uses NADPH as an electron source and can bring about the one-electron reduction of a range of xenobiotics. [Pg.46]

Another example concerns the initial electronic reduction of a-nitrostilbene (Todres, Dyusengaliev, Ustynyuck 1982 Todres, Dyusengaliev, Sevast yanov 1985 Todres Tsvetkova 1987 Charoenkwan and others, in preparation). The reduction develops as in process (a) in Scheme 2-7 if the mercury cathode as well as the cyclooctatetraene dianion are electron sources, and as in process (b) if the same stilbene enters the charge-transfer complexes with bis(pyridine)-tungsten tetra(carbonyl) or uranocene. For (b), the charge-transfer bands in the electronic spectra are fixed. So the mentioned data reveal a great difference in electrochemical and chemical reduction processes (a) and (b). [Pg.103]

Radical anions can be prepared from phenazines using zinc(II)/potassium hydroxide in dimethyl sulfoxide as the electron source. Phenazine has a relatively high reduction potential and reacts spontaneously with tetrabutylammonium borohydride in benzene or tetrahydrofuran to give the corresponding radical anion. ... [Pg.296]

There is a major drawback, however, to the preparation of carbon onions by electron bombardment the amounts obtained are extremely small and thus render the examination of bulk properties virtually impossible. Only high-energy electron sources outside an HRTEM would enable the production of macroscopic amounts. S till a further development of this method is of considerable interest as the carbon onions made from diamond are very uniform in quality. [Pg.305]

Allylations. Allylating agents prepared from allyl halides, CrCl, NiBrj, and MejSiCl react with carbonyl compounds, provided that tetrakis(dimethylamino)ethylene is used as electron source. [Pg.140]

An alternative source preparation which has not been widely adopted is the Sn(reaction using 10-MeV deuterons in a cyclotron [6]. The Sb decays by electron capture with a 38-hour half-life to the 23-88-keV level as shown in Fig. 14.1. 25-keV K-X-rays are also produced in the electron-capture process, so that in most respects the decay is similar to the ii9ffl5 transition. [Pg.373]

Under the common title of electron spectroscopy, this section discusses the most important problems of electron, positron, and beta-ray energy measurements back-scattering, energy resolution and detector response functions, energy calibration, and source preparation. [Pg.439]

Very little is known about the nature of rotational energy transfer in a collision between an electronically excited molecule and a ground-state atom or molecule. In the few reported studies the experimental method is fundamentally the same as that described at the beginning of Section III.A. An initial rotational distribution is established by narrow-band excitation. The fluorescence emission contour is recorded twice, under collision-free and thermal equilibrium conditions, and then again under conditions such that there is one collision during the lifetime of the excited state. The differences in the rotational contours of the three emission spectra are then used to infer the pathway of rotational energy transfer, and the rate of that transfer. Some examples of the emission spectra recorded under these conditions are shown in Fig. 22. Because of the small spacings between the rotational levels of polyatomic molecules most excitation sources prepare nonthermal superpositions of rotational states rather than pure rotational states, and this complicates interpretation of the observations. [Pg.258]

Use of the LS counter for alpha-particle spectral analysis is discussed in Section 8.3.2. Source preparation is simpler, but energy resolution is worse than with the solid-state detector. Special source preparation and electronic pulse-shape selection can improve resolution. [Pg.168]

One-dimensional conducting polymer nanomaterials have been utilized as the field emission electron sources for flat panel displays [365-367]. Conducting polymer nanotubes or nanowires were mostly prepared by the electrochemical polymerization within the cylindrical pores of alumina membranes, and the field emission characteristics were evaluated. As a typical example, a field emission cell was composed of PEDOT nanowire (conductivity, 3.4 x 10 S cm ) tips (cathode) and ITO (anode). The turn-on field of PEDOT nanowire was 3.5-4.0 jiAcm at 10V jim , and the current density increased up to 100 xAcm at 4.5 V jim . The field enhancement factor of the PEDOT nanowire tips was 1200 and this value was comparable to that of CNT. PPy nanowire and PANI nanotube was also prepared using nanoporous template, and their field emission characteristics were investigated [365]. PPy nanowire and PANI nanotubes showed the turn-on fields of 3.5-4.0 and 5.0 jjlA cm at 6 and 8 V im . These studies offered a great feasibility of conducting polymers as the building blocks for all-polymer field emission displays. [Pg.244]

Aberration corrected electron microscopes are now widely available and resolutions of 0.05 nm are possible in the latest instruments. For many bulk systems the accuracy of atomic scale structural characterisation is no longer determined by the microscope but by the difficulty of preparing a suitable thin representative specimen. In contrast, nanoparticle systems are inherently nano-sized and in combination with the use of novel 2D crystals as ultra thin supports,are ideally suited to exploit the full potential of the latest microscopes. Advances in TEM image resolution have stimulated complementary improvements of associated instrumentation including high brightness electron sources, stable power supplies and large... [Pg.98]


See other pages where Electron Source Preparation is mentioned: [Pg.444]    [Pg.444]    [Pg.1624]    [Pg.263]    [Pg.131]    [Pg.104]    [Pg.125]    [Pg.149]    [Pg.9]    [Pg.30]    [Pg.535]    [Pg.307]    [Pg.183]    [Pg.457]    [Pg.210]    [Pg.29]    [Pg.396]    [Pg.1093]    [Pg.82]    [Pg.1619]    [Pg.347]    [Pg.193]    [Pg.1624]    [Pg.486]    [Pg.502]    [Pg.445]    [Pg.135]    [Pg.412]    [Pg.397]    [Pg.95]    [Pg.301]    [Pg.2864]    [Pg.903]    [Pg.1456]    [Pg.731]    [Pg.50]    [Pg.22]    [Pg.61]    [Pg.473]   


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