학술논문
Tissue Equivalent Curved Organic X‐ray Detectors Utilizing High Atomic Number Polythiophene Analogues.
Document Type
Article
Author
Nanayakkara, M. Prabodhi A.; He, Qiao; Ruseckas, Arvydas; Karalasingam, Anushanth; Matjacic, Lidija; Masteghin, Mateus G.; Basiricò, Laura; Fratelli, Ilaria; Ciavatti, Andrea; Kilbride, Rachel C.; Jenatsch, Sandra; Parnell, Andrew J.; Fraboni, Beatrice; Nisbet, Andrew; Heeney, Martin; Jayawardena, K. D. G. Imalka; Silva, S. Ravi P.
Source
Subject
*ATOMIC number
*BUTYRATES
*DETECTORS
*ORGANIC semiconductors
*POLYTHIOPHENES
*CHARGE transfer
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Language
ISSN
2198-3844
Abstract
Organic semiconductors are a promising material candidate for X‐ray detection. However, the low atomic number (Z) of organic semiconductors leads to poor X‐ray absorption thus restricting their performance. Herein, the authors propose a new strategy for achieving high‐sensitivity performance for X‐ray detectors based on organic semiconductors modified with high –Z heteroatoms. X‐ray detectors are fabricated with p‐type organic semiconductors containing selenium heteroatoms (poly(3‐hexyl)selenophene (P3HSe)) in blends with an n‐type fullerene derivative ([6,6]‐Phenyl C71 butyric acid methyl ester (PC70BM). When characterized under 70, 100, 150, and 220 kVp X‐ray radiation, these heteroatom‐containing detectors displayed a superior performance in terms of sensitivity up to 600 ± 11 nC Gy−1 cm−2 with respect to the bismuth oxide (Bi2O3) nanoparticle (NP) sensitized organic detectors. Despite the lower Z of selenium compared to the NPs typically used, the authors identify a more efficient generation of electron‐hole pairs, better charge transfer, and charge transport characteristics in heteroatom‐incorporated detectors that result in this breakthrough detector performance. The authors also demonstrate flexible X‐ray detectors that can be curved to a radius as low as 2 mm with low deviation in X‐ray response under 100 repeated bending cycles while maintaining an industry‐standard ultra‐low dark current of 0.03 ± 0.01 pA mm−2. [ABSTRACT FROM AUTHOR]