2022
DOI: 10.1021/acs.jpclett.2c03642
|View full text |Cite
|
Sign up to set email alerts
|

A-Site Cation Engineering of Ruddlesden–Popper Perovskites for Stable, Sensitive, and Portable Direct Conversion X-ray Imaging Detectors

Abstract: Perovskite flat-panel X-ray detectors are promising products for realizing low-dose medical imaging, a nondestructive test, and security inspection. However, the perovskite X-ray imager still faces intractable problems such as severe baseline drift, a low signal-to-noise ratio, and rapid performance degradation, which were involved by the notorious intrinsic ion migration of the perovskite functional layer. In this work, sensitive, stable, and portable pixel quasi-two-dimensional (2D) Ruddlesden–Popper (RP) pe… Show more

Help me understand this report

Search citation statements

Order By: Relevance

Paper Sections

Select...
2
1
1

Citation Types

0
17
0
2

Year Published

2023
2023
2024
2024

Publication Types

Select...
8

Relationship

2
6

Authors

Journals

citations
Cited by 15 publications
(19 citation statements)
references
References 38 publications
0
17
0
2
Order By: Relevance
“…Reproduced with permission. 97 Copyright 2022, American Chemical Society. (e) Photograph (left) and X-ray image (right) of a standard Pb phantom acquired by the MAPb(I 0.9 Cl 0.1 ) 3 detector.…”
Section: Membrane Fillingmentioning
confidence: 99%
See 1 more Smart Citation
“…Reproduced with permission. 97 Copyright 2022, American Chemical Society. (e) Photograph (left) and X-ray image (right) of a standard Pb phantom acquired by the MAPb(I 0.9 Cl 0.1 ) 3 detector.…”
Section: Membrane Fillingmentioning
confidence: 99%
“…Reproduced with permission. 97 Copyright 2022, American Chemical Society. (h) X-ray imaging of the BA 2 MA 9 Pb 10 I 31 X-ray detector.…”
Section: Membrane Fillingmentioning
confidence: 99%
“…MA3Bi2I9 单晶具有优异的探测性能,为进一步 实现该材料的应用,2020 年,Tie 等 [77] 采用等静压 制备工艺,将 MA3Bi2I9 晶体粉末压制成型,制备了 毫米级厚度的 MA3Bi2I9 多晶片。该 多晶 片 具有 6 Quasi-2D polycrystalline X-ray detector (a) Preparing of RP perovskite -nylon matrix by a lamination process [26] ; (b) Photograph and corresponding X-ray image of a copper Chinese characters pattern [26] ; (c) A-site cation engineering to prepare RP perovskite X-ray detectors [22] ; (d) Microstructure of the TFT substrate and 12×12 pixel perovskite X-ray detector [22] ; (e) Images of visible light and X-rays based on BA2MA9Pb10I31 detector [22] ; (f) X-ray image based on (BA2PbBr4)0.5-FAPbI3 device [83] ; (g) Dark current uniformity of MAPbI3 device (left) and quasi-2D PEA2MA8Pb9I28 device (right) [84] 子的尺寸对离子迁移及电子传输存在直接影响。阳 [85] 。同时,利用 钙钛矿材料的铁电性质也可以达到类似的效果,值 得探索。电极结构设计对器件性能影响显著。通过 设计具有暗电流分流作用的电极结构,可以有效降 低 X 射线探测器的暗电流,同时减少噪声和基线漂 移 [86] 。通过设计更先进的器件结构实现高性能探测 器,是值得研究的重要方向。 (3)…”
Section: 零维钙钛矿多晶探测器unclassified
“…国亟待攻克的"卡脖子"技术之一。因此,研发先进 的探测材料及技术为打破探测器领域自身的技术限 制及国外技术封锁均具有十分重要的意义。 X 射线探测器分为直接型和间接型两种。 相比 于间接型,直接型探测器的像素串扰问题较少,理 论空间分辨率更高 [4] 。 非晶硒 (a-Se) [5] , 碲锌镉 (CZT) [6] 等是直接型 X 射线探测器的典型代表。目前,a-Se 与薄膜晶体管(TFT)阵列结合,实现了大面积 二维 X 射线成像。 然而, a-Se 对射线的吸收能力差, 载流子迁移率低, 以及易晶化导致了工作不稳定性, 极大地限制了其应用范围。CZT 的基本性质十分契 合 X 射线探测的需求,然而大尺寸、高质量的 CZT 制备困难, 只有少数几个国家和地区掌握相关技术。 CZT 单晶的高温(>1000 ℃)制备工艺限制了其在 商业 TFT 基板直接沉积的可能性。其他常见的直接 型 X 射线探测材料:硅 [7] 、锗 [8] 、碘化汞 [9] 等存在 X 射线吸收能力和稳定性差等问题,应用也受到极大 限制。 近年来,卤化物钙钛矿由于光电性质优异、带 隙可调、制备简单、成本低等优点,在材料科学、 光电子领域引起了广泛关注 [10] 。钙钛矿的高原子序 数 (Z) 和高载流子迁移率使其适用于 X 射线检测。 与传统的 a-Se、CZT 相比,钙钛矿材料的主要优势 如下: (1)缺陷容忍度高,载流子迁移率高和载流 子寿命长。 (2)组分和结构可调,为材料性质调变 提供了丰富的操作平台。 (3)制备方法简单多样, 包括刮刀涂布 [11] 、旋涂 [12] 、喷涂 [13] 、热压 [14] 、模板 辅助生长法 [15] 以及数字喷墨打印 [16] 等。 根据八面体结构基元在不同方向上的连接方式, 钙钛矿被分为三维(3D) 、2D、1D 和 0D 结构 [17] 。 自 2015 年 Yakunin 等首次报道了基于 3D MAPbI3 多晶膜 X 射线探测器之后, 钙钛矿 X 射线探测器取 得了引人瞩目的进展,灵敏度>10 4 µC • Gyair −1 • cm −2 , 远优于商业化 a-Se 探测器 [18][19][20][21] 。然而,由于 3D 钙 钛矿存在较严重的离子迁移,导致噪声大和基线漂 移严重等问题,不利于获取低检测下限及高稳定性 器件 [22] 。2021 年,Liu 等 [23] 发现具有复合 A 位阳离 子的三维钙钛矿单晶可以在一定程度上抑制离子迁 移。如何进一步抑制钙钛矿离子迁移是获得具有高 稳定性 X 射线探测器的关键。 研究发现, 低维 (2D、 1D、0D)钙钛矿材料在微观结构上可以隔断离子迁 移 通 道 , 进而更好地 抑制离 子 迁 移 [24] 。 例如, MA3Bi2I9、Cs3Bi2I9、(NH4)3Bi2I9、Ruddlesden-Popper (RP)钙钛矿等低维材料的离子迁移激活能(Ea) 较大 [24][25][26][27][28][29]…”
unclassified
“…X-ray imaging has become increasingly prominent as the auxiliary evidence for the chest diagnosis and treatment. However, frequent radiation often increases the risk of cancer in the human body. To increase the frequency and fidelity of diagnostic technologies for early diagnosis of diseases without sacrificing imaging quality, high-performance X-ray detectors for low-dose detection are urgently needed. Direct X-ray detection has obvious advantages over the indirect ones in resolution and simpler system configuration. For direct X-ray detection, electron–hole pairs (EHPs) are generated in the photoconductive layer after absorbing incident X-ray photons and are collected by the electrodes in opposite direction under external bias. , Therefore, the efficiency of carrier separation and extraction in the photoconductive layer influences the performance of direct X-ray detectors. Though high bias voltages can provide a large driving force to ensure a sufficient separation of EHPs, large dark current is introduced as well, which is an unpleasant source of noise. , Noise is a random component added to the image signal, existing as white dots appearing randomly in the image.…”
Section: Introductionmentioning
confidence: 99%