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Richardson-Dushman thermionic emission

The analytic theory outlined above provides valuable insight into the factors that determine the efficiency of OI.EDs. However, there is no completely analytical solution that includes diffusive transport of carriers, field-dependent mobilities, and specific injection mechanisms. Therefore, numerical simulations have been undertaken in order to provide quantitative solutions to the general case of the bipolar current problem for typical parameters of OLED materials [144—1481. Emphasis was given to the influence of charge injection and transport on OLED performance. 1. Campbell et at. [I47 found that, for Richardson-Dushman thermionic emission from a barrier height lower than 0.4 eV, the contact is able to supply... [Pg.545]

From the Richardson-Dushman equation, the current density Je by thermionic emission can be obtained as... [Pg.119]

Thermionic emission. The number of electrons which escape from the metal surface increases rapidly with temperature (thermionic emission). In general, the higher the temperature and the lower the work function, the higher is the electron emissivity. The current density can be calculated by the Richardson-Dushman equation (in the absence of an external electrical field), according to i — AT exp(—rp/kT), where A is the Richardson constant (A cm K ), T is the temperature (K), and

work function (eV). For pure tungsten A — 60.2 (A cm K ) [1.91]. The thermionic current (A cm ) can then be calculated as i — 60.2r exp(—52230/T) [1.37]. [Pg.40]

In thermionic emission, the current density / obtained from the electrically heated filament in the presence of an electric field E obeys the modified Richardson-Dushman equation ... [Pg.1716]

The thermionic-emission current /th> in amperes, generated by a heated filament is described by the Richardson-Dushman equation... [Pg.355]

X 10 V m would be sufficient for this. The emission would follow the Richardson-Dushman law for thermionic emission, namely the current density would be... [Pg.443]

The thermionic electron emission current jT is described by the Dushman-Richardson relation [93,95] ... [Pg.28]


See other pages where Richardson-Dushman thermionic emission is mentioned: [Pg.544]    [Pg.437]    [Pg.544]    [Pg.437]    [Pg.293]    [Pg.293]    [Pg.815]    [Pg.28]   
See also in sourсe #XX -- [ Pg.439 ]




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