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Charge generation process, in OSC

In an all-polymer system, the excitons generate in the donor phase after the absorption of photons in active layer and then transform to the charge-transfer state, which will dissociate into free charge or recombine geminately. Those two processes compete with each other. A promoted efficiency of OSCs requires the inhibition of geminated recombination and the transformation of more excitons into free charges [134,135]. [Pg.312]


See other pages where Charge generation process, in OSC is mentioned: [Pg.307]    [Pg.309]    [Pg.312]    [Pg.293]    [Pg.295]    [Pg.298]    [Pg.307]    [Pg.309]    [Pg.312]    [Pg.293]    [Pg.295]    [Pg.298]    [Pg.311]    [Pg.318]    [Pg.297]    [Pg.304]    [Pg.564]    [Pg.309]    [Pg.310]    [Pg.312]    [Pg.314]    [Pg.295]    [Pg.296]    [Pg.298]    [Pg.300]    [Pg.142]    [Pg.2]    [Pg.6]    [Pg.76]   
See also in sourсe #XX -- [ Pg.293 , Pg.294 , Pg.295 , Pg.296 , Pg.297 , Pg.298 , Pg.299 ]

See also in sourсe #XX -- [ Pg.293 , Pg.294 , Pg.295 , Pg.296 , Pg.297 , Pg.298 , Pg.299 ]




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