Abstract
The past decade has witnessed remarkable progress in the device efficiency of quantum dot light-emitting diodes based on the framework of organic-inorganic hybrid device structure. The striking improvement notwithstanding, the following conundrum remains underexplored: state-of-the-art devices with seemingly unfavorable energy landscape exhibit barrierless hole injection initiated even at sub-band gap voltages. Here, we unravel that the cause of barrierless hole injection stems from the Fermi level alignment derived by the surface states. The reorganized energy landscape provides macroscopic electrostatic potential gain to promote hole injection to quantum dots. The energy level alignment surpasses the Coulombic attraction induced by a charge employed in quantum dots which adjust the local carrier injection barrier of opposite charges by a relatively small margin. Our finding elucidates how quantum dots accommodate barrierless carrier injection and paves the way to a generalized design principle for efficient electroluminescent devices employing nanocrystal emitters.
Highlights
The past decade has witnessed remarkable progress in the device efficiency of quantum dot light-emitting diodes based on the framework of organic-inorganic hybrid device structure
In the case of hole transport layers (HTLs) with a larger E1Sh − EHOMO, HTL value, both VJ and VJ and luminance thresholds (VL) are lower than what would correspond to the bandgap of quantum dots (QDs) (Eg/e = 1.97 eV) (Fig. 1b, c)
One would attribute the sub-Eg thresholds to the recombination of charge transfer complex because VJ coincides with built-in potential, ECBM, ZnO − EHOMO, HTLs (Fig. 1d)
Summary
The past decade has witnessed remarkable progress in the device efficiency of quantum dot light-emitting diodes based on the framework of organic-inorganic hybrid device structure. We can make better sense of the sub-Eg turn-on in the hybrid QLEDs. First, the band bending at the QD–organic HTL junction reduces the energy level offset for the hole injection, E1Sh − EHOMO, HTL, in the way of large electrostatic potential gain.
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