2016
DOI: 10.1021/acs.chemrev.6b00126
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Charge Generation Pathways in Organic Solar Cells: Assessing the Contribution from the Electron Acceptor

Abstract: Photocurrent generation in organic bulk heterojunction (BHJ) solar cells is most commonly understood as a process which predominantly involves photoexcitation of the lower ionization potential species (donor) followed by electron transfer to the higher electron affinity material (acceptor) [i.e., photoinduced electron transfer (PET), which we term Channel I]. A mirror process also occurs in which photocurrent is generated through photoexcitation of the acceptor followed by hole transfer to the nonexcited donor… Show more

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Cited by 207 publications
(180 citation statements)
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“…[4][5][6] Benefiting from the great efforts devoted to the design of new materials, [7][8][9][10][11][12][13] optimization of the blend morphology, [14][15][16][17][18] understanding the charge generation mechanism, [19][20][21][22][23][24][25][26] significant progress has been achieved in the last few years. [4][5][6] Benefiting from the great efforts devoted to the design of new materials, [7][8][9][10][11][12][13] optimization of the blend morphology, [14][15][16][17][18] understanding the charge generation mechanism, [19][20][21][22][23][24][25][26] significant progress has been achieved in the last few years.…”
mentioning
confidence: 99%
“…[4][5][6] Benefiting from the great efforts devoted to the design of new materials, [7][8][9][10][11][12][13] optimization of the blend morphology, [14][15][16][17][18] understanding the charge generation mechanism, [19][20][21][22][23][24][25][26] significant progress has been achieved in the last few years. [4][5][6] Benefiting from the great efforts devoted to the design of new materials, [7][8][9][10][11][12][13] optimization of the blend morphology, [14][15][16][17][18] understanding the charge generation mechanism, [19][20][21][22][23][24][25][26] significant progress has been achieved in the last few years.…”
mentioning
confidence: 99%
“…Thes patial distribution of the guest and host molecules in af ilm is important for understanding the behavior of phosphorescent emitters used in OLEDs,a s well as other materials such as thermally-activated delayed fluorescence emitters [3,4] and low donor content solar cells. [5] Films of phosphorescent light-emitting materials can undergo triplet-triplet annihilation (TTA), with the level dependent on the spatial distribution of the emitters. [6] Fçrster-type TTAt ends to be inefficient for low concentration blends of emissive iridium(III) complexes due to poor spectral overlap of their emission and absorption spectra.…”
mentioning
confidence: 99%
“…In OSCs, conversion of incident photons into the electric current involved four steps (Figure ): i) formation of intramolecular exciton upon absorption of photons; ii) exciton diffusion to ED and EA interfaces; where iii) it dissociates to form a germinate pair; and iv) charge separated and electron and holes are collected by the respective electrodes under an internal electric field . As excitons have very short lifetimes and exciton diffusion length is only 5–20 nm in BHJ, excitons must dissociate efficiently to maximize the PCE .…”
Section: Osc Parameters and Architecturementioning
confidence: 99%