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Impact of proton irradiation on photoluminescent properties of C-doped ZrO2 films prepared by ALD

Anna SytchkovaOptical Coatings Group, Department for Energy Technologies and Renewable Sources, ENEA C.R. Casaccia, via Anguillarese 301, Rome, 00123, ItalyMaria Lucia ProtopapaDepartment for Sustainability, ENEA C.R. Brindisi, SS 7 Appia Km 706, 72100, Brindisi, ItalyHristo KolevInstitute of Catalysis, Bulgarian Academy of Sciences, Acad. G. Bonchev St., Bldg. 11, 1113, Sofia, BulgariaEmiliano BurresiDepartment for Sustainability, ENEA C.R. Brindisi, SS 7 Appia Km 706, 72100, Brindisi, ItalyP. OliveroPhysics Department and “NIS” inter-departmental centre, University of Torino, via P. Giuria 1, 10125, Torino, ItalyToni DunatovLaboratory for ion beam interaction, Institut Ruđer Bosković, Bijenička cesta 54, 10000, Zagreb, CroatiaZdravko SiketićLaboratory for ion beam interaction, Institut Ruđer Bosković, Bijenička cesta 54, 10000, Zagreb, CroatiaL. TapferDepartment for Sustainability, ENEA C.R. Brindisi, SS 7 Appia Km 706, 72100, Brindisi, ItalyZhihao WangCenter of Materials Science and Optoelectronics Engineering, University of Chinese Academy of Sciences, Beijing, 100049, ChinaHongbo HeKey Laboratory of Materials for High Power Laser, Shanghai Institute of Optics and Fine Mechanics, No. 390 Qinghe Road, Jiading District, Shanghai, 201800, ChinaYanzhi WangLaboratory of Thin Film Optics, Shanghai Institute of Optics and Fine Mechanics, No. 390 Qinghe Road, Jiading District, Shanghai, 201800, China
2024en
ABI

Abstract

Amorphous C-doped zirconia thin films grown by ALD technique on fused silica substrates have high transmittance and significant photoluminescence (PL) capacity suitable for application as a transparent material to convert high energy into lower energy photons as well as an optical sensor of radiation. Due to carbon doping, zirconia films present three main PL transitions: Transition I and II at λem = 450 nm (λexc = 200 and 270 nm), related to sp3 and sp2 C–C bonds, and Transition III at λem = 450 nm (λexc = 300 nm) that can be assigned to CO bonds which introduce n levels in the π- π* gap. Protons with energy of 100 keV and two values of fluence (1∙1012 p+/cm2 and 5∙1014 p+/cm2) were used to modify the film properties. The changes induced by the radiation in the chemical composition of the films have been monitored as a function of irradiation dose using in-depth resolved XPS analysis which evidenced modification of C–Zr, Zr–O, C–H, C–C/CC and CO bonds. We demonstrate that C–Zr bonds formed in the film depth are cleaved by protonation in favor of Zr–O, C–H and CO bonds establishment. As a consequence, more defect levels are formed in the π- π* gap of carbon. Consequently, the emission due to Transitions III becomes more intense for high energy doses, getting intensity values close to Transitions I/II.

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