Abstract:As
effective light absorbers in solar cells, CsPbI3 all-inorganic
perovskite quantum dots (QDs) have received increasing attention,
benefitting from their suitable optical band gap and thermal stability.
However, the easy cubic to yellow orthorhombic phase transition hinders
their further application in stable photovoltaic devices. CsPbBr3 QDs have been targeted as a promising material for ultrahigh
voltage and stable solar cells. In this work, we first develop a simple
yet efficient post-treatment method usin… Show more
“…1d ), consistent with the distance between the (200) planes indexed in the XRD measurement. Notably, the dimensions of CsPbBr 3 QDs with high crystallization are similar to the grain size of the perovskite films produced by the precursor solution with post-annealing treatment 26 – 28 , suggesting that the CsPbBr 3 QDs are suitable not only for the LEM device active layer, but also for many other perovskite optoelectronic devices 35 , 36 . A sharp emission peak centered at λ = 526 nm with a comparable photoluminescence (PL) intensity is observed in both the CsPbBr 3 QDs and PMMA/CsPbBr 3 QDs samples (Fig.…”
Field-induced ionic motions in all-inorganic CsPbBr3 perovskite quantum dots (QDs) strongly dictate not only their electro-optical characteristics but also the ultimate optoelectronic device performance. Here, we show that the functionality of a single Ag/CsPbBr3/ITO device can be actively switched on a sub-millisecond scale from a resistive random-access memory (RRAM) to a light-emitting electrochemical cell (LEC), or vice versa, by simply modulating its bias polarity. We then realize for the first time a fast, all-perovskite light-emitting memory (LEM) operating at 5 kHz by pairing such two identical devices in series, in which one functions as an RRAM to electrically read the encoded data while the other simultaneously as an LEC for a parallel, non-contact optical reading. We further show that the digital status of the LEM can be perceived in real time from its emission color. Our work opens up a completely new horizon for more advanced all-inorganic perovskite optoelectronic technologies.
“…1d ), consistent with the distance between the (200) planes indexed in the XRD measurement. Notably, the dimensions of CsPbBr 3 QDs with high crystallization are similar to the grain size of the perovskite films produced by the precursor solution with post-annealing treatment 26 – 28 , suggesting that the CsPbBr 3 QDs are suitable not only for the LEM device active layer, but also for many other perovskite optoelectronic devices 35 , 36 . A sharp emission peak centered at λ = 526 nm with a comparable photoluminescence (PL) intensity is observed in both the CsPbBr 3 QDs and PMMA/CsPbBr 3 QDs samples (Fig.…”
Field-induced ionic motions in all-inorganic CsPbBr3 perovskite quantum dots (QDs) strongly dictate not only their electro-optical characteristics but also the ultimate optoelectronic device performance. Here, we show that the functionality of a single Ag/CsPbBr3/ITO device can be actively switched on a sub-millisecond scale from a resistive random-access memory (RRAM) to a light-emitting electrochemical cell (LEC), or vice versa, by simply modulating its bias polarity. We then realize for the first time a fast, all-perovskite light-emitting memory (LEM) operating at 5 kHz by pairing such two identical devices in series, in which one functions as an RRAM to electrically read the encoded data while the other simultaneously as an LEC for a parallel, non-contact optical reading. We further show that the digital status of the LEM can be perceived in real time from its emission color. Our work opens up a completely new horizon for more advanced all-inorganic perovskite optoelectronic technologies.
“…1e), consistent with the distance between the (200) planes indexed in the XRD measurement. Notably, the dimensions of CsPbBr 3 QDs with high crystallization are similar to the grain size of the perovskite films produced by the precursor solution with post-annealing treatment 26−28 , suggesting that the CsPbBr 3 QDs are suitable not only for the LEM device active layer, but also for many other perovskite optoelectronic devices 32,33 . The elemental composition of the CsPbBr 3 QDs is also analyzed by using the energy dispersive Xray spectroscopy (EDS), as shown in homojunctions 34 .…”
Field-induced ionic motions in all-inorganic CsPbBr3 perovskite quantum dots (QDs) strongly dictate not only their electro-optical characteristics but also the ultimate device performance of the CsPbBr3 optoelectronics. Novel device concepts with multiple functionalities can as a result be achieved based on CsPbBr3 by carefully controlling the ionic flow under different bias conditions. Here, we show that by manipulating the ion migrations in two nominally identical, series-connected Ag/CsPbBr3/ITO devices, one device can operate as a resistive random-access memory (RRAM) while the other simultaneously as a light-emitting electrochemical cell (LEC), or vice versa, simply through the polarity switching of the external bias across the entire structure. We further show that this electrically switchable, series-connected perovskite memories and light emitters can be employed as a novel all-perovskite light-emitting memory (LEM) device for simultaneous electronic and optical reading of the encoded information in communication and computation applications. We present a physical picture that clearly depicts the movements of each ionic species and their reduction or oxidation processes in the perovskite LEM responsible for the observed electronic and optical characteristics. The demonstrated bifunctionality of the simple metal-perovskite-metal structures and the novel device concept derived from their creative synergy opens up a completely new horizon for more advanced all-inorganic perovskite optoelectronics with novel functionalities.
“…Unfortunately, the temperature is still about 160 °C, which is disadvantageous for flexible PSCs. Although the formation temperature can be reduced to room temperature by coating the CsPbBr 3 quantum dots (QDs) on the polymer based flexible substrates, [18] the slow charge transfer between QDs undoubtedly drags the efficiency. Therefore, the finding of heat‐resistant substrates is a persistent objective to make flexible, all‐inorganic CsPbBr 3 PSCs and even other flexible electronics.…”
All‐inorganic CsPbBr3 perovskite solar cells (PSCs) have attracted tremendous attention, owing to their excellent stability and rising power conversion efficiency. However, the mechanical flexibility of these solar cells has ground to a standstill because of the high‐temperature requirement for ideal CsPbBr3 perovskite films. In this study, a flexible CsPbBr3 PSC with an efficiency of 5.71 % has been made by means of fabricating a heat‐resistant conductive muscovite substrate, which demonstrates very high mechanical flexibility with nearly unchanged resistance even after 4000 bending cycles (12000 cycles of concave and convex bending for PSCs), owing to the weak van der Waals force and layered structure. Implementation of the muscovite substrate enables the fabrication of flexible PSCs under high‐temperature conditions, providing a new path to increase the efficiency without lowering the crystallization temperature of state‐of‐the‐art electron‐transporting materials and perovskite films in the future.
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