TY - JOUR
T1 - Predicted THz-wave absorption properties observed in all-inorganic perovskite CsPbI3 thin films
T2 - Integrity at the grain boundary
AU - Maeng, Inhee
AU - Chen, Shi
AU - Lee, Seungjun
AU - Wang, Shenghao
AU - Kwon, Young Kyun
AU - Jung, Min Cherl
N1 - Publisher Copyright:
© 2022 The Author(s)
PY - 2023/1
Y1 - 2023/1
N2 - The realization of terahertz (THz) detectors using organic-inorganic hybrid perovskite (OHP) materials presents a challenge because of the high real conductivities and broad THz absorption spectra required. The control of phonon vibration modes in OHPs depends on the control of defect states such as the defect-incorporated perovskite structure and the δ/α-mixed interfacial structure observed in MAPbI3 and δ/α-mixed FAPbI3, respectively. Difficulties with defect control in particular materials may amplify relative risk factors and invite strong resistance to commercialization. As an alternative to OHPs, the all-inorganic perovskite material CsPbI3 (lacking the hydrophobic organic cations that generate structural defects) constitutes a good candidate for THz detectors. We investigated the phonon vibration modes of thin films of the all-inorganic perovskite γ-CsPbI3 containing no atomic or chemical defect states. We observed the three expected major phonon vibration modes at 0.9, 1.5, and 1.8 THz that originate from the transverse I–Pb–I frame, the Cs–I–Cs optical vibration, and the longitudinal I–Pb–I frame, respectively, finding good agreement with theoretical simulations. Significantly, the real conductivity of these all-inorganic perovskite thin films ranged from approximately 10–40 S/cm across a broad frequency range of 0.5–3.0 THz, demonstrating the material's considerable potential for application as a THz-band detector.
AB - The realization of terahertz (THz) detectors using organic-inorganic hybrid perovskite (OHP) materials presents a challenge because of the high real conductivities and broad THz absorption spectra required. The control of phonon vibration modes in OHPs depends on the control of defect states such as the defect-incorporated perovskite structure and the δ/α-mixed interfacial structure observed in MAPbI3 and δ/α-mixed FAPbI3, respectively. Difficulties with defect control in particular materials may amplify relative risk factors and invite strong resistance to commercialization. As an alternative to OHPs, the all-inorganic perovskite material CsPbI3 (lacking the hydrophobic organic cations that generate structural defects) constitutes a good candidate for THz detectors. We investigated the phonon vibration modes of thin films of the all-inorganic perovskite γ-CsPbI3 containing no atomic or chemical defect states. We observed the three expected major phonon vibration modes at 0.9, 1.5, and 1.8 THz that originate from the transverse I–Pb–I frame, the Cs–I–Cs optical vibration, and the longitudinal I–Pb–I frame, respectively, finding good agreement with theoretical simulations. Significantly, the real conductivity of these all-inorganic perovskite thin films ranged from approximately 10–40 S/cm across a broad frequency range of 0.5–3.0 THz, demonstrating the material's considerable potential for application as a THz-band detector.
KW - All-inorganic perovskite thin film
KW - Clean grain boundary
KW - THz-wave absorption
KW - Three major THz absorptions
KW - γ-CsPbI
UR - http://www.scopus.com/inward/record.url?scp=85145781078&partnerID=8YFLogxK
U2 - 10.1016/j.mtphys.2022.100960
DO - 10.1016/j.mtphys.2022.100960
M3 - Article
AN - SCOPUS:85145781078
SN - 2542-5293
VL - 30
JO - Materials Today Physics
JF - Materials Today Physics
M1 - 100960
ER -