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Election tunneling

Fig. 8-38. Redox electron transfer at film-covered metal electrodes (a) transfer of redox electionB across a thin semiconductor film (direct tunneling transfer of electrons), (b) transfer of redox elections throu a thidc semiconductor film (indirect transfer of elections through electron levels in a thick film). Fig. 8-38. Redox electron transfer at film-covered metal electrodes (a) transfer of redox electionB across a thin semiconductor film (direct tunneling transfer of electrons), (b) transfer of redox elections throu a thidc semiconductor film (indirect transfer of elections through electron levels in a thick film).
Fig. 1. Self energy of the election Green function averaged over impurity potential inside the grains and over tunneling elements between the grains. Averaging over the impurity potential is represented by the dotted line (a) while tunneling elements are represented by crossed circles (b). Fig. 1. Self energy of the election Green function averaged over impurity potential inside the grains and over tunneling elements between the grains. Averaging over the impurity potential is represented by the dotted line (a) while tunneling elements are represented by crossed circles (b).
Sustainable development and the multidisciplinary use of the underground are also debated within the electives related to tunnelling and geo-risk management. The speeifieity of these courses is to help to raise awareness among students of any possible ethical, social, environmental, aesthetic, economic and legal implications of their work, to which they will act appropriately. The importance of the human factor and a clear communication line between all parties involved in a construction project is stressed. Site visits also provide the opportunity to introduce non technical issues, to students not willing to follow a full course on the topic. [Pg.79]

Love, J. D. and Winkler, C. (1978) A universal tunnelling coefficient for step- and graded-index multimode fibers. Opt. Quant. Elect., 10, 341-51. [Pg.152]

As a light microscopic particle, electron easily tunnels through a potential barrier, therefore, the process is governed by general tunneling law formulated by Gamov. The principle theoretical comstone for condenced-phase ET was laid by Franck and Libby (1949-1952) who asserted that the Frank-Condon principle is applicable not only to the vertical radiative processes but also to nonradiative horizontal election transfer. [Pg.281]


See other pages where Election tunneling is mentioned: [Pg.174]    [Pg.1038]    [Pg.415]    [Pg.13]    [Pg.174]    [Pg.1038]    [Pg.415]    [Pg.13]    [Pg.38]    [Pg.754]    [Pg.82]    [Pg.354]    [Pg.2792]    [Pg.120]    [Pg.854]    [Pg.865]    [Pg.80]    [Pg.288]    [Pg.51]   
See also in sourсe #XX -- [ Pg.107 , Pg.151 ]




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Electivity

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