2007
DOI: 10.1016/j.jlumin.2006.08.030
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Wannier–Frenkel hybrid exciton in organic–semiconductor quantum dot heterostructures

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Cited by 13 publications
(4 citation statements)
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“…e proposed model is consistent with the experimentally verified carrier dynamics model shown in reference [28]. Due to this irregular arrangement, the exciton in this work can only be treated as a hybrid type of the Frenkel and Wannier exciton [29]. Figure 2(c) shows the coupling distance distribution among electrons and holes.…”
Section: Theoretical Simulation Schemessupporting
confidence: 83%
See 1 more Smart Citation
“…e proposed model is consistent with the experimentally verified carrier dynamics model shown in reference [28]. Due to this irregular arrangement, the exciton in this work can only be treated as a hybrid type of the Frenkel and Wannier exciton [29]. Figure 2(c) shows the coupling distance distribution among electrons and holes.…”
Section: Theoretical Simulation Schemessupporting
confidence: 83%
“…In this work, instead of calculating the eigenvalue directly, the excitonic distribution is represented as the distribution of exciton radius, i.e., the distance between the electron and hole based on the following consideration: e ultrahigh density of QD array studied in this Advances in Condensed Matter Physics work could be treated as a pseudo-two-dimensional quantum well structure due to the strong coupling between neighboring QDs. Moreover, meanwhile, the exciton binding energy of quantum well can be approximated as Eexciton ≈ − (ε r r eh ) − 1 based on formulas (28), (29), and (31) in reference [25], where ε r is the dielectric constant and r eh is the mean electron-hole distance. Experimentally, the exciton binding energy can be estimated from the PL peak energy using the following relation: E exciton � E G (orE HOMO− LUMO ) − E PL .…”
Section: Theoretical Simulation Schemesmentioning
confidence: 99%
“…acceptor materials. [16][17][18] The vibrational energy released due to the formation of CT excitons acts as the external energy to completely dissociate the CT excitons into free charge carries if it exceeds the binding energy of excitons. 18 These free charge carries are then transported to and collected on the respective electrodes.…”
Section: Introductionmentioning
confidence: 99%
“…For inorganic bulk materials, in which the Bohr radius is larger than the lattice spacing, Wannier–Mott excitons with a weak binding energy are generated. For inorganic NCs, however, the exciton Bohr radius is comparable to the NC size, and the photogenerated electron–hole pairs are bound by Coulomb force, leading to the formation of Frenkel excitons. , These Frenkel excitons need to be dissociated by the energy offset between the highest occupied molecular orbital (HOMO) of the CP donor and the ionization potential (i.e., the valence band edge) of the NC acceptor at the donor/acceptor interface . Therefore, the PCE of organic–inorganic hybrid solar cells relies largely on the electronic band structures of both donor and acceptor materials, as well as the energy-level alignment at the donor/acceptor interface.…”
mentioning
confidence: 99%