BiO(IO <sub>3</sub> ) with Ultrahigh Effective Atomic Number and Density for Sensitive and Stable Hard X‐Ray Detection

H Haiyu Ren (School of Physical Science and Technology Lanzhou Center for Theoretical Physics Key Laboratory of Theoretical Physics of Gansu Province Key Laboratory of Quantum Theory and Applications of MoE and Gansu Provincial Research Center For Basic Disciplines of Quantum Physics Lanzhou University Lanzhou Gansu China) Y Youkui Xu (School of Physical Science and Technology &amp; Lanzhou Center for Theoretical Physics Key Laboratory of Theoretical Physics of Gansu Province and Key Laboratory of Quantum Theory and Applications of MoE Lanzhou University Lanzhou Gansu 730000 China) F Feifei Chai (College of Mechanical and Electrical Engineering Henan Agricultural University Zhengzhou China) Z Zhenhua Li (State Key Laboratory of Forage Breeding-by-Design and Utilization, Key Laboratory of Photobiology, Institute of Botany, Chinese Academy of Sciences) Y Yutian Lei G Guoqiang Peng (School of Physical Science and Technology &amp; Lanzhou Center for Theoretical Physics &amp; Key Laboratory of Theoretical Physics of Gansu Province &amp; Key Laboratory of Quantum Theory and Applications of MOE Lanzhou University Lanzhou China) T Tengfei Yu Z Zhiwen Jin (School of Physical Science and Technology &amp; Lanzhou Center for Theoretical Physics &amp; Key Laboratory of Theoretical Physics of Gansu Province &amp; Key Laboratory of Quantum Theory and Applications of MOE Lanzhou University Lanzhou China)

Abstract

ABSTRACT Bismuth halide perovskites are promising materials for hard X‐ray detection owing to their high effective atomic number (Z eff ) and excellent optoelectronic properties. However, the reported A‐site cations or pseudohalides to address chemical stability issues inevitably reduce material Z eff /density and aggravate electron localization. These changes significantly degrade X‐ray absorption and charge transport, ultimately undermining detection performance. Herein, we chose the oxidized I 5+ to replace I − , and designed 2D BiO(IO 3 ). This substitution yields a significantly more compact crystal lattice while retaining two high‐Z elements (Bi and I), affording the material an ultrahigh Z eff (72.29) and density (7.399 g/cm 3 ), which greatly enhances hard X‐ray absorption. Concurrently, the small effective mass of the material facilitates efficient carrier transport, resulting in a high device sensitivity of 4563 µC Gy air −1  cm −2 for ∼25 keV X‐ray photons. Furthermore, the formation of strong Bi–O and I–O bonds endows the material with excellent stability, leading to a high ion migration activation energy of 0.73 eV. Specifically, polycrystalline wafers with a thickness of 1 mm were successfully fabricated and showed no performance degradation after long time continuous aging test (160 kV X‐ray, high voltage, temperature, etc.). This work provides a promising solution for developing high‐performance hard X‐ray detection materials.

Article Details

Volume / Issue Vol. 38, Issue 13
Published March 01, 2026
ISSN 0935-9648
Publisher Unknown Publisher

Journal Info

Advanced Materials

Unknown Publisher

ISSN: 0935-9648 Physical Sciences

Authors (8)

H

Haiyu Ren

School of Physical Science and Technology Lanzhou Center for Theoretical Physics Key Laboratory of Theoretical Physics of Gansu Province Key Laboratory of Quantum Theory and Applications of MoE and Gansu Provincial Research Center For Basic Disciplines of Quantum Physics Lanzhou University Lanzhou Gansu China

Y

Youkui Xu

School of Physical Science and Technology &amp; Lanzhou Center for Theoretical Physics Key Laboratory of Theoretical Physics of Gansu Province and Key Laboratory of Quantum Theory and Applications of MoE Lanzhou University Lanzhou Gansu 730000 China

F

Feifei Chai

College of Mechanical and Electrical Engineering Henan Agricultural University Zhengzhou China

Z

Zhenhua Li

State Key Laboratory of Forage Breeding-by-Design and Utilization, Key Laboratory of Photobiology, Institute of Botany, Chinese Academy of Sciences

Y

Yutian Lei

G

Guoqiang Peng

School of Physical Science and Technology &amp; Lanzhou Center for Theoretical Physics &amp; Key Laboratory of Theoretical Physics of Gansu Province &amp; Key Laboratory of Quantum Theory and Applications of MOE Lanzhou University Lanzhou China

T

Tengfei Yu

Z

Zhiwen Jin

School of Physical Science and Technology &amp; Lanzhou Center for Theoretical Physics &amp; Key Laboratory of Theoretical Physics of Gansu Province &amp; Key Laboratory of Quantum Theory and Applications of MOE Lanzhou University Lanzhou China