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dc.contributor.authorTuleushev, A. Z.en
dc.contributor.authorHarrison, F. E.en
dc.contributor.authorKozlovskiy, A. L.en
dc.contributor.authorZdorovets, M. V.en
dc.date.accessioned2022-05-12T08:13:11Z-
dc.date.available2022-05-12T08:13:11Z-
dc.date.issued2022-
dc.identifier.citationUrbach Rule in the Red-Shifted Absorption Edge of PET Films Irradiated with Swift Heavy Ions / A. Z. Tuleushev, F. E. Harrison, A. L. Kozlovskiy et al. // Polymers. — 2022. — Vol. 14. — Iss. 5. — 923.en
dc.identifier.issn2073-4360-
dc.identifier.otherAll Open Access, Gold, Green3
dc.identifier.urihttp://elar.urfu.ru/handle/10995/111116-
dc.description.abstractThis paper presents a new analysis of the experimental transmission spectra of polyethylene terephthalate (PET) films before and after irradiation with swift heavy ions (SHI) films, as reported previously by the authors. It is shown that the absorption edge red shift for irradiated films contains two regions of exponential form, one of which is located in the UV region and the other at lower energy, mainly in the visible part of the spectrum. The behaviour of the transmission curves under different irradiating fluences demonstrates that these two regions reflect respectively the electron-enriched core of the latent track and its electron-depleted peripheral halo. The focal point method yields a bandgap energy of 4.1 eV for the electron-enriched core of the latent track, which is similar to n-doped semiconductors, and a bandgap of about 1.3–1.5 eV for the electron-depleted halo, similar to p-doped semiconductors. The boundary between the latent track cores and halos corresponds to a conventional semiconductor p-n junction. The values of the characteristic Urbach energy determined from experimental data correspond to the nonradiative transition energy between the excited singlet and triplet levels of benzene-carboxyl complexes in repeat units of the PET chain molecule. A parallel is drawn between the SHI-induced redistribution of electrons held in structural traps in the PET film and chemical redox reactions, which involve the redistribution of electrons in chemical bonds. It is suggested that alkali etching triggers the release of excess electrons in the latent track cores, which act as a catalyst for the fragmentation of PET chain molecules along the latent tracks of the SHI irradiation. © 2022 by the authors. Licensee MDPI, Basel, Switzerland.en
dc.format.mimetypeapplication/pdfen
dc.language.isoenen
dc.publisherMDPIen1
dc.publisherMDPI AGen
dc.rightsinfo:eu-repo/semantics/openAccessen
dc.sourcePolym.2
dc.sourcePolymersen
dc.subjectBANDGAP ENERGYen
dc.subjectLATENT TRACKen
dc.subjectPOLYETHYLENE TEREPHTHALATEen
dc.subjectSHI IRRADIATIONen
dc.subjectURBACH ENERGYen
dc.subjectABSORPTION SPECTROSCOPYen
dc.subjectELECTRONSen
dc.subjectENERGY GAPen
dc.subjectETCHINGen
dc.subjectHEAVY IONSen
dc.subjectIRRADIATIONen
dc.subjectLIGHT ABSORPTIONen
dc.subjectMOLECULESen
dc.subjectPLASTIC BOTTLESen
dc.subjectPOLYETHYLENE TEREPHTHALATESen
dc.subjectRED SHIFTen
dc.subjectSEMICONDUCTOR DOPINGen
dc.subjectSEMICONDUCTOR JUNCTIONSen
dc.subjectABSORPTION EDGESen
dc.subjectBAND GAP ENERGYen
dc.subjectCHAIN MOLECULESen
dc.subjectHEAVY IONS IRRADIATIONSen
dc.subjectLATENT TRACKSen
dc.subjectPOLYETHYLENE-TEREPHTHALATE FILMSen
dc.subjectSWIFT HEAVY ION IRRADIATIONen
dc.subjectSWIFT HEAVY IONSen
dc.subjectTRACK CORESen
dc.subjectURBACH ENERGYen
dc.subjectREDOX REACTIONSen
dc.titleUrbach Rule in the Red-Shifted Absorption Edge of PET Films Irradiated with Swift Heavy Ionsen
dc.typeArticleen
dc.typeinfo:eu-repo/semantics/articleen
dc.typeinfo:eu-repo/semantics/publishedVersionen
dc.identifier.doi10.3390/polym14050923-
dc.identifier.scopus85125588753-
local.contributor.employeeTuleushev, A.Z., Flerov Laboratory of Nuclear Reactions, Joint Institute for Nuclear Research, Dubna, 141980, Russian Federation; Harrison, F.E., Engineering Profile Laboratory, L.N. Gumilyov Eurasian National University, Nur-Sultan, 010008, Kazakhstan; Kozlovskiy, A.L., Engineering Profile Laboratory, L.N. Gumilyov Eurasian National University, Nur-Sultan, 010008, Kazakhstan, Laboratory of Solid-State Physics, The Institute of Nuclear Physics, Almaty, 050032, Kazakhstan; Zdorovets, M.V., Engineering Profile Laboratory, L.N. Gumilyov Eurasian National University, Nur-Sultan, 010008, Kazakhstan, Laboratory of Solid-State Physics, The Institute of Nuclear Physics, Almaty, 050032, Kazakhstan, Department of Intelligent Information Technologies, Ural Federal University, Yekaterinburg, 620075, Russian Federationen
local.issue5-
local.volume14-
dc.identifier.wos000769242600001-
local.contributor.departmentFlerov Laboratory of Nuclear Reactions, Joint Institute for Nuclear Research, Dubna, 141980, Russian Federation; Engineering Profile Laboratory, L.N. Gumilyov Eurasian National University, Nur-Sultan, 010008, Kazakhstan; Laboratory of Solid-State Physics, The Institute of Nuclear Physics, Almaty, 050032, Kazakhstan; Department of Intelligent Information Technologies, Ural Federal University, Yekaterinburg, 620075, Russian Federationen
local.identifier.pure29721957-
local.description.order923-
local.identifier.eid2-s2.0-85125588753-
local.identifier.wosWOS:000769242600001-
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