Abstract:All‐inorganic halide perovskites (CsPbX3, X = Cl−, Br−, and I−) are brought to the forefront of research focus in the field of modern lighting technology. However, due to the toxic element (Pb2+), environmentally friendly white‐light emissions are difficult to achieve, thus limiting their practical applications. Herein, high‐quality Mg2+‐alloyed CsPb1−x
Mgx
X3 (up to 20%) nanocrystals (NCs) are synthesized. The structural and optical properties are investigated. The application of these NCs in white‐light‐emit… Show more
“…The increased doping concentration also leads to peak broadening and splitting at 30.7°, which indicates a symmetry-lowering tilt and distortion of the [BX 6 ] 4− octahedron. [17,29] Such distortions are also predicted by our first principles calculations, but they are below 1.5°. It has been reported that doping can induce structural evolution, especially when the size mismatch between the dopant and substituted atoms is large, [29,31,36] but the calculated small distortion here indicates the lattice contraction and octahedral tilting are not strong enough to induce a distinct structural change.…”
Section: Resultssupporting
confidence: 83%
“…[13] B-site cations also play a critical role in determining the electronic band structure of perovskites and consequently their emission properties. Recent studies have demonstrated successful B-site doping using alkaline-earth metal ions (Mg 2+ , Ba 2+ , Sr 2+ ), [14][15][16][17] transition metal ions (Cu 2+ , Cd 2+ , Ag + , Zn 2+ ), [18][19][20][21] metalloid ions (Sn 2+ , Bi 3+ ), [22][23][24] and lanthanide ions (Ce 3+ , Tb 3+ , Yb 3+ ). [25][26][27] Despite these advantages, dopants may also lead to negative effects on the properties of NCs.…”
Colloidal CsPbX 3 (X = Br, Cl, and I) perovskite nanocrystals exhibit tunable bandgaps over the entire visible spectrum and high photoluminescence quantum yields in the green and red regions. However, the lack of highly efficient blue-emitting perovskite nanocrystals limits their development for optoelectronic applications. Herein, neodymium (III) (Nd 3+) doped CsPbBr 3 nanocrystals are prepared through the ligand-assisted reprecipitation method at room temperature with tunable photoemission from green to deep blue. A blue-emitting nanocrystal with a central wavelength at 459 nm, an exceptionally high photoluminescence quantum yield of 90%, and a spectral width of 19 nm is achieved. First principles calculations reveal that the increase in photoluminescence quantum yield upon doping is driven by an enhancement of the exciton binding energy due to increased electron and hole effective masses and an increase in oscillator strength due to shortening of the Pb-Br bond. Putting these results together, an all-perovskite white light-emitting diode is successfully fabricated, demonstrating that B-site composition engineering is a reliable strategy to further exploit the perovskite family for wider optoelectronic applications.
“…The increased doping concentration also leads to peak broadening and splitting at 30.7°, which indicates a symmetry-lowering tilt and distortion of the [BX 6 ] 4− octahedron. [17,29] Such distortions are also predicted by our first principles calculations, but they are below 1.5°. It has been reported that doping can induce structural evolution, especially when the size mismatch between the dopant and substituted atoms is large, [29,31,36] but the calculated small distortion here indicates the lattice contraction and octahedral tilting are not strong enough to induce a distinct structural change.…”
Section: Resultssupporting
confidence: 83%
“…[13] B-site cations also play a critical role in determining the electronic band structure of perovskites and consequently their emission properties. Recent studies have demonstrated successful B-site doping using alkaline-earth metal ions (Mg 2+ , Ba 2+ , Sr 2+ ), [14][15][16][17] transition metal ions (Cu 2+ , Cd 2+ , Ag + , Zn 2+ ), [18][19][20][21] metalloid ions (Sn 2+ , Bi 3+ ), [22][23][24] and lanthanide ions (Ce 3+ , Tb 3+ , Yb 3+ ). [25][26][27] Despite these advantages, dopants may also lead to negative effects on the properties of NCs.…”
Colloidal CsPbX 3 (X = Br, Cl, and I) perovskite nanocrystals exhibit tunable bandgaps over the entire visible spectrum and high photoluminescence quantum yields in the green and red regions. However, the lack of highly efficient blue-emitting perovskite nanocrystals limits their development for optoelectronic applications. Herein, neodymium (III) (Nd 3+) doped CsPbBr 3 nanocrystals are prepared through the ligand-assisted reprecipitation method at room temperature with tunable photoemission from green to deep blue. A blue-emitting nanocrystal with a central wavelength at 459 nm, an exceptionally high photoluminescence quantum yield of 90%, and a spectral width of 19 nm is achieved. First principles calculations reveal that the increase in photoluminescence quantum yield upon doping is driven by an enhancement of the exciton binding energy due to increased electron and hole effective masses and an increase in oscillator strength due to shortening of the Pb-Br bond. Putting these results together, an all-perovskite white light-emitting diode is successfully fabricated, demonstrating that B-site composition engineering is a reliable strategy to further exploit the perovskite family for wider optoelectronic applications.
“…To overcome the toxicity problem, more endeavors should be taken in the development of heavy-metal-free impurity-doped nanocrystal LEDs [ 353 , 354 , 355 ], otherwise it will be difficult to enter the mainstream display, lighting, and signaling markets. For the lifetime issue, no impurity-doped nanocrystal LEDs with satisfactory operational stability have been reported.…”
In recent years, impurity-doped nanocrystal light-emitting diodes (LEDs) have aroused both academic and industrial interest since they are highly promising to satisfy the increasing demand of display, lighting, and signaling technologies. Compared with undoped counterparts, impurity-doped nanocrystal LEDs have been demonstrated to possess many extraordinary characteristics including enhanced efficiency, increased luminance, reduced voltage, and prolonged stability. In this review, recent state-of-the-art concepts to achieve high-performance impurity-doped nanocrystal LEDs are summarized. Firstly, the fundamental concepts of impurity-doped nanocrystal LEDs are presented. Then, the strategies to enhance the performance of impurity-doped nanocrystal LEDs via both material design and device engineering are introduced. In particular, the emergence of three types of impurity-doped nanocrystal LEDs is comprehensively highlighted, namely impurity-doped colloidal quantum dot LEDs, impurity-doped perovskite LEDs, and impurity-doped colloidal quantum well LEDs. At last, the challenges and the opportunities to further improve the performance of impurity-doped nanocrystal LEDs are described.
“…For instance, by blending blue CsPbBrxCl3-x QDs with orange polymer of poly[2-methoxy-5-(2-ethylhexyloxy)1,4-phenylenevinylene] (MEH:PPV) with the ratio of 9 : 1, a single-EML white LED with CIE chromaticity coordinates of (0.33, 0.34) was demonstrated ( Figure 5.3). [179] Other additional emitters, like rare-earth ion Sm 3+ , [180] alkali metal Mg 2+ , [181] also show good compatibilities with perovskites. Adapted from reference.…”
Section: Perovskite-based Hybrid White Ledsmentioning
Metal halide perovskites (MHPs) are recognized as promising semiconductor materials for a variety of optical and electrical device applications due to their cost-effective and outstanding optoelectronic properties. As one of the most significant applications, perovskite light-emitting diodes (PeLEDs) hold promise for future lighting and display technologies, attributed to their high photoluminescence quantum yield (PLQY), high color purity, and tunable emission color. The emission colors of PeLEDs can be tuned by mixing the halide anions, adjusting the size of perovskite nanocrystals, or changing the dimensionality of perovskites. However, in practice, all these different approaches have their own advantages and challenges. This thesis centres around the color tunability of perovskites, aiming to develop PeLEDs with different colors using different approaches.
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