Show simple item record

dc.contributor.authorVladimir A. Makagonov
dc.contributor.authorKonstantin S. Gabriel’s
dc.contributor.authorYuri E. Kalinin
dc.contributor.authorArtem Yu. Lopatin
dc.contributor.authorLudmila A. Bliznyuk
dc.contributor.authorAlexander K. Fedotov
dc.contributor.otherVoronezh State Technical University
dc.contributor.otherVoronezh State Technical University
dc.contributor.otherVoronezh State Technical University
dc.contributor.otherVoronezh State Technical University
dc.contributor.otherScientific-Practical Materials Research Centre of the National Academy of Sciences of Belarus
dc.contributor.otherBelarusian State University
dc.date.accessioned2025-10-09T04:54:01Z
dc.date.available2025-10-09T04:54:01Z
dc.date.issued01-10-2024
dc.identifier.urihttps://moem.pensoft.net/article/140732/download/pdf/
dc.identifier.urihttp://digilib.fisipol.ugm.ac.id/repo/handle/15717717/40832
dc.description.abstractA method of measuring the thermovoltaic effect in heterogeneous media with gradient doping impurity distributions producing gradient carrier distributions has been proposed. Iron doped zinc oxide specimens have been produced using ion beam sputtering on thin foil tantalum substrates for thermovoltaic effect measurements, glass-ceramic substrates for Hall measurements and silicon substrates for structural study. The doping impurity concentration хFe in the specimens has been varied from 0.34 to 4.18 at.%. X-ray phase analysis has shown that all the specimens have a hexagonal zinc oxide crystal structure. The films have preferential [002] orientation. The carrier concentration in the experimental specimen layers according Hall data obtained on an ECOPIA 5500 measurement system in a 0.5 T DC magnetic field has varied in the 1016–1020 cm-3 range. The specimens have an n-type conductivity. Thermovoltaic measurements have been carried out for two-layered iron doped zinc oxide specimens with different carrier and iron doping impurity concentrations using the method proposed. The maximum thermovoltaic response (U ~ 80 μV) has been observed in the two-layered thin-film specimen with the carrier concentration difference between the layers (Δn ≈ 2∙103 cm-3). The observed saturation of the thermovoltaic response has been attributed to the establishment of dynamic equilibrium between carrier diffusion from the high carrier concentration layer to the low carrier concentration layer and carrier drift due to internal electric field.
dc.language.isoEN
dc.publisherPensoft Publishers
dc.subject.lccElectronics
dc.titleThermovoltaic response in two-layered thin-film zinc oxide structures
dc.typeArticle
dc.description.pages159-165
dc.description.doi10.3897/j.moem.10.3.140732
dc.title.journalModern Electronic Materials
dc.identifier.e-issn2452-1779
dc.identifier.oaioai:doaj.org/journal:179a84ed1dca46aa979d3d022a2c70b5
dc.journal.infoVolume 10, Issue 3


This item appears in the following Collection(s)

Show simple item record