Ultrafast and broadband photodetectors based on a perovskite/organic bulk heterojunction for large-dynamic-range imaging
Li et al. Light: Science & Applications (2020)9:31
https://doi.org/10.1038/s41377-020-0264-5
ARTICLE
Official journal of the CIOMP 2047-7538
www.nature.com/lsa
Open Access
Ultrafast and broadband photodetectors based
on a perovskite/organic bulk heterojunction for
large-dynamic-range imaging
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Chenglong Li1, Hailu Wang2,3, Fang Wang2,3, Tengfei Li4, Mengjian Xu2, Hao Wang2,3, Zhen Wang2,3, Xiaowei Zhan4,
Weida Hu 2,3 and Liang Shen1
Abstract
Organic-inorganic hybrid perovskite (OIHP) photodetectors that simultaneously achieve an ultrafast response and high
sensitivity in the near-infrared (NIR) region are prerequisites for expanding current monitoring, imaging, and optical
communication capbilities. Herein, we demonstrate photodetectors constructed by OIHP and an organic bulk
heterojunction (BHJ) consisting of a low-bandgap nonfullerene and polymer, which achieve broadband response
spectra up to 1 μm with a highest external quantum efficiency of approximately 54% at 850 nm, an ultrafast response
speed of 5.6 ns and a linear dynamic range (LDR) of 191 dB. High sensitivity, ultrafast speed and a large LDR are
preeminent prerequisites for the practical application of photodetectors. Encouragingly, due to the high-dynamicrange imaging capacity, high-quality visible-NIR actual imaging is achieved by employing the OIHP photodetectors.
We believe that state-of-the-art OIHP photodetectors can accelerate the translation of solution-processed
photodetector applications from the laboratory to the imaging market.
Introduction
Serving as technical functional components for the
translation of optical signals into electrical signals, photodetectors have received extensive attention and have
been applied in various fields, including industrial production, military affairs, biochemical detection, optical
communication, and scientific research1–10. The versatility
and availability of photodetectors always depend on a few
predominant factors: the photoresponse speed, sensitivity
to lower brightness, detection band in which photodetectors can efficaciously detect light and dynamic range
Correspondence: Fang Wang () or
Weida Hu () or Liang Shen ()
1
State Key Laboratory of Integrated Optoelectronics, College of Electronic
Science and Engineering, Jilin University, 2699 Qianjin Street, Changchun
130012, China
2
State Key Laboratory of Infrared Physics, Shanghai Institute of Technical
Physics, Chinese Academy of Sciences, 500 Yutian Road, Shanghai
200083, China
Full list of author information is available at the end of the article.
These author contributed equally: Chenglong Li, Hailu Wang
response11–16. Correspondingly, the key photodetector
parameters that are to used to evaluate these performance
factors are the response time or speed, spectral responsivity (R), noise current, external quantum efficiency
(EQE), specific detectivity (D*) and linear dynamic range
(LDR)17–20. Recently, the exploration of high-performance
photodetectors has gradually become a research focus in
the field of optoelectronics and high-quality imaging.
Organic-inorganic hybrid perovskites (OIHPs) are
emerging materials that have been progressively enabling
new thin-film optoelectronics, including solar cells21–27,
light-emitting diodes28,29 and photodetectors14,16,30–36.
The extensive application of hybrid perovskites can be
attributable to their excellent optical and electrical
properties, including a direct bandgap, large absorption
coefficient, high carrier mobility, and low trap density37–40.
Therefore, OIHP photodetectors have demonstrated high
R, high D*, an ultrafast response speed and a high LDR
when combined with device structure engineering11,18,41.
However, the detection range of MAPbI3 (either
© The Author(s) 2020
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Li et al. Light: Science & Applications (2020)9:31
Page 2 of 8
polycrystalline films or thin single crystals) is limited to
the wavelength region below 820 nm and does not cover
the near-infrared (NIR) range, which severely limits its
application, especially in biomedical imaging. To overcome this problem, an advantageous strategy has been
demonstrated: combining OIHP and an organic bulk
heterojunction (BHJ) consisting of donor-acceptor materials with light absorption in the NIR region16,35,36,42.
Shen et al. reported a composite photodetector based on
MAPbI3 and PDPPTDTPT/PCBM, which exhibited a
wider detection wavelength extending to 950 nm with a
5 ns ultrafast response time16. This work provided an
effective way of achieving both a wider and faster response
for next-generation photodetectors. However, the sole
flaw of the photodetectors was that the EQE value in the
NIR region failed to reach a similar value to that in the
UV-visible range, which resulted from the weak NIR
absorption of the low-bandgap polymer and a mismatched energy level alignment at the interface between
the OIHP and BHJ layers. Wang et al. reported photodetectors based on MAPbI3 and PDPP3T/PC71BM BHJ,
achieving a slightly higher EQE of 40% in the NIR region.
However, the achieved response time on the order of
microseconds cannot easily meet the application
requirements36. Recently, Wu et al. demonstrated a
broadband photodetector with an EQE of 70% in the NIR
region by coating PTB7-Th:IEICO-4F on MAPbI335.
However, the photodetectors did not display an inspiring
performance in terms of a lower noise current and an
extremely fast response time. State-of-the-art OIHP
broadband photodetectors should have a high EQE value
in the NIR region, high sensitivity and an ultrafast
response speed. However, no such results have been
reported to date. Compared with previously reported NIR
materials such as PDPPTDTPT, PDPP3T, and IEICO-4F,
a fused-ring electron acceptor named F8IC with a lower
bandgap and higher electron mobility has been successfully synthesized43. F8IC exhibits an extremely low
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