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Charged excitons

However, not all excitons have sufficiently long lifetimes to reach the interface before recombining. To circumvent this problem and increase device efficiency, heterostmcture devices have been fabricated. In these devices, donors and acceptors are mixed together to create a network that provides many internal interfaces where charge separation can occur. Heterostmcture devices made from the donor polymer... [Pg.245]

In low-dimensional systems, such as quantum-confined. semiconductors and conjugated polymers, the first step of optical absorption is the creation of bound electron-hole pairs, known as excitons [34). Charge photogcncration (CPG) occurs when excitons break into positive and negative carriers. This process is of essential importance both for the understanding of the fundamental physics of these materials and for applications in photovoltaic devices and photodctcctors. Since exciton dissociation can be affected by an external electric field, field-induced spectroscopy is a powerful tool for studying CPG. [Pg.138]


See other pages where Charged excitons is mentioned: [Pg.431]    [Pg.35]    [Pg.235]    [Pg.749]    [Pg.146]    [Pg.687]    [Pg.119]    [Pg.409]    [Pg.465]    [Pg.467]    [Pg.868]    [Pg.431]    [Pg.35]    [Pg.235]    [Pg.749]    [Pg.146]    [Pg.687]    [Pg.119]    [Pg.409]    [Pg.465]    [Pg.467]    [Pg.868]    [Pg.2500]    [Pg.348]    [Pg.240]    [Pg.242]    [Pg.243]    [Pg.245]    [Pg.726]    [Pg.22]    [Pg.60]    [Pg.63]    [Pg.68]    [Pg.88]    [Pg.105]    [Pg.106]    [Pg.126]    [Pg.126]    [Pg.129]    [Pg.131]    [Pg.137]    [Pg.138]    [Pg.139]    [Pg.141]    [Pg.170]    [Pg.182]    [Pg.196]    [Pg.196]    [Pg.219]    [Pg.226]    [Pg.328]    [Pg.377]    [Pg.381]    [Pg.382]    [Pg.383]    [Pg.402]    [Pg.405]    [Pg.431]    [Pg.433]    [Pg.442]   
See also in sourсe #XX -- [ Pg.35 ]




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