2021
DOI: 10.1016/j.jpcs.2021.110190
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Blend ratio and applied voltage effects on the charge recombination in bulk heterojunction polymer solar cells based on anthracene-containing poly(arylene-ethynylene)-alt-poly(arylene-vinylene) studied using magnetoconductance

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Cited by 4 publications
(4 citation statements)
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“…As the magnetic field is increased, the amount of pair states mixed with the singlet state decreases, resulting in a decrease in singlet e–h pair recombination and, as a result, an increase in current. To calculate the recombination probability P r , we use the Stochastic Liouville equation (SLE) in the framework of the e–h pair model to calculate the density matrix from its equation of motion. The first term is the Liouville term, which describes how the density matrix evolves under the influence of the system’s Hamiltonian H . Hyperfine interactions ( ) and Zeeman splitting of the triplets ( ), where g ≈ 2 is the polaron g factor, μ B is the Bohr magneton, H⃗ app is the applied magnetic field, H⃗ hyp, i is the hyperfine field, S⃗ i is the spin operator of the individual polarons, and i denotes electron or hole, are included in this Hamiltonian.…”
Section: Results and Discussionmentioning
confidence: 99%
“…As the magnetic field is increased, the amount of pair states mixed with the singlet state decreases, resulting in a decrease in singlet e–h pair recombination and, as a result, an increase in current. To calculate the recombination probability P r , we use the Stochastic Liouville equation (SLE) in the framework of the e–h pair model to calculate the density matrix from its equation of motion. The first term is the Liouville term, which describes how the density matrix evolves under the influence of the system’s Hamiltonian H . Hyperfine interactions ( ) and Zeeman splitting of the triplets ( ), where g ≈ 2 is the polaron g factor, μ B is the Bohr magneton, H⃗ app is the applied magnetic field, H⃗ hyp, i is the hyperfine field, S⃗ i is the spin operator of the individual polarons, and i denotes electron or hole, are included in this Hamiltonian.…”
Section: Results and Discussionmentioning
confidence: 99%
“…could take place under spin thermal equilibrium conditions at room temperature [4,16], which is different from that of those inorganic giant magnetoresistances (MRs) generated by spin polarization. This implies that new mechanisms are responsible for OMR [17][18][19][20][21][22]. So far, three typical mechanisms have been mainly invoked to interpret the OMR phenomenon: the bipolaron model, the exciton-charge interaction model and the singlet-triplet conversion (STC) model.…”
Section: Introductionmentioning
confidence: 99%
“…In this model, the interaction between excitons and charges with spin of 1/2 is B dependent, causing a negative or positive OMR. The STC model was generally used to explain OMR in devices with bipolar carrier injection [20,21]. When a magnetic field suppresses the spin mixing between singlet and triplet excitons by hyperfine fields, OMR is generated since the singlets are easier to dissociate and recombine than triplets.…”
Section: Introductionmentioning
confidence: 99%
“…Moreover, the low carrier mobilities of the conducting polymers and the short lifetime of the exciton restrict the active layer thickness below 200 nm, so it is not possible to boost optical absorption by merely increasing the thickness [8][9][10][11][12][13][14]. Thus, in addition to the absorber layer composition and device architecture, the PCE in TFPSCs depends on the augmentation of the open-circuit voltage and the fill factor (FF) [15][16][17].…”
Section: Introductionmentioning
confidence: 99%