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Crystal electron injected into

Another relatively recent technique, in its own way as strange as Mossbauer spectrometry, is positron annihilation spectrometry. Positrons are positive electrons (antimatter), spectacularly predicted by the theoretical physicist Dirac in the 1920s and discovered in cloud chambers some years later. Some currently available radioisotopes emit positrons, so these particles arc now routine tools. High-energy positrons are injected into a crystal and very quickly become thermalised by... [Pg.238]

In nanocrystaUine semiconductor films (commonly obtained in CD), the crystal size may be too small to support an appreciable space charge layer. Charges in that case are separated by differing kinetics between electron and hole injection into the electrolyte. The upcoming discussion on nonannealed films treats this in somewhat more detail. (Chapter 9 discusses PECs and their principles of operation more fully.)... [Pg.85]

These materials are known as insertion or intercalation hosts. The overall electrochemical process of a lithium battery is illustrated schematically in Fig. 7.2. During discharge it involves the dissolution of lithium ions at the anode, their migration across the electrolyte and their insertion within the crystal structure of the host compound, while the compensating electrons travel in the external circuit to be injected into the electronic band structure of the same host. The charging process is the reverse and the cell reaction may be written as ... [Pg.199]

Fig. 20 Plots of H/kTc against 1 kTQ for electron and hole injection into anthracene crystals grown under different atmospheres open symbols refer to electrons and closed symbols to positive holes. (After Owen et al, 1974)... Fig. 20 Plots of H/kTc against 1 kTQ for electron and hole injection into anthracene crystals grown under different atmospheres open symbols refer to electrons and closed symbols to positive holes. (After Owen et al, 1974)...
Another method presented in this paper is the indirect eb method when the C -lace of a LiNbOs ferroelectric is preliminary coated by a highly defective layer of the amorphous photo-resist material pmma. The thickness of this dielectric layer is large enough to protect the LiNb03 from penetration of high energy electrons into the bulk. In the presented calculations and simulation a very limited number of electrons penetrated into the LiNbOs crystal, so most of the injected electron charge remains trapped in the pmma layer. [Pg.202]

SR makes possible diffraction studies of much smaller or poorly diffracting crystals. It has also the advantage of easily tunable wavelength. However, owing to an imperfect vacuum inside the chamber, the electron beam, and hence the SR intensity, tend to decay with time (until a new portion of electrons is injected into the ring) and the observed reflection intensities must be corrected correspondingly. [Pg.1110]

Bidirectional PCET also manifests itself in reductases. Crystal structures of hydrogenases [216-218] indicate that the mechanism for hydrogen production occurs by transporting protons into the active site along pathways distinct from those traversed by the electron equivalents. Electrons are putatively injected into the active site via a chain of [FeS] clusters, while proton channels and acid-base residues at the active site manage the substrate inventory. [Pg.553]


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