2012
DOI: 10.1002/aenm.201200077
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Thermodynamic Efficiency Limit of Molecular Donor‐Acceptor Solar Cells and its Application to Diindenoperylene/C60‐Based Planar Heterojunction Devices

Abstract: In organic photovoltaic (PV) cells, the well‐established donor‐acceptor (D/A) concept enabling photo‐induced charge transfer between two partners with suitable energy level alignment has proven extremely successful. Nevertheless, the introduction of such a heterojunction is accompanied with additional energy losses as compared to an inorganic homojunction cell, owing to the presence of a charge‐transfer (CT) state at the D/A interface. Based on the principle of detailed balance, a modified Shockley‐Queisser th… Show more

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Cited by 89 publications
(148 citation statements)
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“…[5][6][7][8][9][10] In a practical solar cell both V oc and the LED quantum efficiency, Q LED , are reduced relative to their thermodynamic limits by non-radiative recombination pathways, the degree of which can be quantified via a reciprocity theorem. [11][12][13][14][15][16][17] Therefore, it is of high interest in the field of organic photovoltaics to reduce these non-radiative recombination losses, thereby bringing the V oc closer to the radiative limit. Recently, indacenodithiophene (IDT) copolymers have shown promising field-effect transistor mobilities and solar cell performance.…”
Section: Introductionmentioning
confidence: 99%
“…[5][6][7][8][9][10] In a practical solar cell both V oc and the LED quantum efficiency, Q LED , are reduced relative to their thermodynamic limits by non-radiative recombination pathways, the degree of which can be quantified via a reciprocity theorem. [11][12][13][14][15][16][17] Therefore, it is of high interest in the field of organic photovoltaics to reduce these non-radiative recombination losses, thereby bringing the V oc closer to the radiative limit. Recently, indacenodithiophene (IDT) copolymers have shown promising field-effect transistor mobilities and solar cell performance.…”
Section: Introductionmentioning
confidence: 99%
“…[7,10] However, because of both the low carrier mobility and the interpenetrated nature of typical BHJ blends, there is a non-negligible probability that dissociated free carriers recombine again at the large D-A interface (nongeminate recombination) before being collected at the electrodes. [7,11] These nonradiative recombinations can be a major loss mechanism p-1 that strongly reduces the power conversion efficiency in BHJ solar cells, [12][13][14][15][16] and are mainly influenced by the energy difference between the highest occupied molecular level ε D1 of D (called HOMO of D) and the lowest unoccupied level ε A2 of A (called LUMO of A). Since it was experimentally found for several donor-acceptor material combinations [5,[17][18][19] that the open circuit voltage U oc is proportional to this effective energy gap, the nonradiative recombination losses can be traced back to a drop of U oc .…”
mentioning
confidence: 99%
“…Reproduced with permission. [13] Copyright 2012, Wiley-VCH. be used to calculate an upper limit for the PCE of an excitonic solar cell.…”
Section: Introductionmentioning
confidence: 99%
“…be used to calculate an upper limit for the PCE of an excitonic solar cell. [12,13] Therein, the single step profile with an onset at the energy gap E g (which has to be identified with the optical gap of the organic semiconductor having the smaller gap) and unity absorbance α g 1 has to be extended by a second step corresponding to the CT state, which is characterized by two parameters E CT and α CT . E CT is lower than E g by the driving force ΔE CT and the absorption strength α CT typically is of the order of 10 −3 times the fundamental absorption across the optical gap.…”
Section: Introductionmentioning
confidence: 99%