TY - JOUR
T1 - Pure Cs4PbBr6: Highly Luminescent Zero-Dimensional Perovskite Solids
AU - Saidaminov, Makhsud I.
AU - Almutlaq, Jawaher
AU - Sarmah, Smritakshi P.
AU - Dursun, Ibrahim
AU - Zhumekenov, Ayan A.
AU - Begum, Raihana
AU - Pan, Jun
AU - Cho, Nam Chul
AU - Mohammed, Omar F.
AU - Bakr, Osman
N1 - KAUST Repository Item: Exported on 2020-10-01
Acknowledgements: The authors acknowledge the support of King Abdullah University of Science and Technology (KAUST).
PY - 2016/9/29
Y1 - 2016/9/29
N2 - So-called zero-dimensional perovskites, such as Cs4PbBr6, promise outstanding emissive properties. However, Cs4PbBr6 is mostly prepared by melting of precursors that usually leads to a coformation of undesired phases. Here, we report a simple low-temperature solution-processed synthesis of pure Cs4PbBr6 with remarkable emission properties. We found that pure Cs4PbBr6 in solid form exhibits a 45% photoluminescence quantum yield (PLQY), in contrast to its three-dimensional counterpart, CsPbBr3, which exhibits more than 2 orders of magnitude lower PLQY. Such a PLQY of Cs4PbBr6 is significantly higher than that of other solid forms of lower-dimensional metal halide perovskite derivatives and perovskite nanocrystals. We attribute this dramatic increase in PL to the high exciton binding energy, which we estimate to be ∼353 meV, likely induced by the unique Bergerhoff–Schmitz–Dumont-type crystal structure of Cs4PbBr6, in which metal-halide-comprised octahedra are spatially confined. Our findings bring this class of perovskite derivatives to the forefront of color-converting and light-emitting applications.
AB - So-called zero-dimensional perovskites, such as Cs4PbBr6, promise outstanding emissive properties. However, Cs4PbBr6 is mostly prepared by melting of precursors that usually leads to a coformation of undesired phases. Here, we report a simple low-temperature solution-processed synthesis of pure Cs4PbBr6 with remarkable emission properties. We found that pure Cs4PbBr6 in solid form exhibits a 45% photoluminescence quantum yield (PLQY), in contrast to its three-dimensional counterpart, CsPbBr3, which exhibits more than 2 orders of magnitude lower PLQY. Such a PLQY of Cs4PbBr6 is significantly higher than that of other solid forms of lower-dimensional metal halide perovskite derivatives and perovskite nanocrystals. We attribute this dramatic increase in PL to the high exciton binding energy, which we estimate to be ∼353 meV, likely induced by the unique Bergerhoff–Schmitz–Dumont-type crystal structure of Cs4PbBr6, in which metal-halide-comprised octahedra are spatially confined. Our findings bring this class of perovskite derivatives to the forefront of color-converting and light-emitting applications.
UR - http://hdl.handle.net/10754/623102
UR - http://pubs.acs.org/doi/full/10.1021/acsenergylett.6b00396
UR - http://www.scopus.com/inward/record.url?scp=85011333921&partnerID=8YFLogxK
U2 - 10.1021/acsenergylett.6b00396
DO - 10.1021/acsenergylett.6b00396
M3 - Article
SN - 2380-8195
VL - 1
SP - 840
EP - 845
JO - ACS Energy Letters
JF - ACS Energy Letters
IS - 4
ER -