Unoccupied Electron States and the Formation of Interface between Films of Dimethyl-Substituted Thiophene–Phenylene Coolygomers and Oxidized Silicon Surface
- Authors: Ponomarenko S.A.1,2, Handke B.3, Komolov A.S.4, Lazneva E.F.4, Gerasimova N.B.4, Panina Y.A.4, Zashikhin G.D.4, Pshenichnyuk S.A.5, Borshchev O.V.1
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Affiliations:
- Enikopolov Institute of Synthetic Polymeric Materials
- Moscow State University
- Faculty of Material Science and Ceramics
- St. Petersburg State University
- Institute of Molecules and Crystals
- Issue: Vol 60, No 5 (2018)
- Pages: 1029-1034
- Section: Polymers
- URL: https://journal-vniispk.ru/1063-7834/article/view/202991
- DOI: https://doi.org/10.1134/S1063783418050128
- ID: 202991
Cite item
Abstract
The unoccupied electron states and the boundary potential barrier during deposition of ultrathin films of dimethyl-substituted thiophene–phenylene coolygomers of the type of CH3–phenylene–thiophene–thiophene–phenylene–CH3 (CH3–PTTP–CH3) on an oxidized silicon surface have been studied. The electronic characteristics have been measured in the energy range from 5 to 20 eV above the Fermi level using total current spectroscopy (TCS). The structure of the CH3–PTTP–CH3 film surfaces has been studied by atomic force microscopy (AFM), and the atomic compositions of the films have been studied by X-ray photoelectron spectroscopy (XPS). The changes in the maximum intensities measured by the TCS method obtained from the deposited CH3–PTTP–CH3 film and from the substrate during increasing in the organic coating thickness to 6 nm is discussed. The formation of the boundary potential barrier in the n-Si/SiO2/CH3–PTTP–CH3 is accompanied by the decrease in the surface work function from 4.2 ± 0.1 to 4.0 ± 0.1 eV as the organic coating thickness increases to 3 nm. The ratio of atomic concentrations C: S in the CH3–PTTP–CH3 films well corresponds to the chemical formula of CH3–PTTP–CH3 molecules. The roughness of the CH3–PTTP–CH3 coating surface was not higher than 10 nm on the ~10 × 10 μm areas as the total CH3–PTTP–CH3-layer thickness was about 100 nm.
About the authors
S. A. Ponomarenko
Enikopolov Institute of Synthetic Polymeric Materials; Moscow State University
Email: a.komolov@spbu.ru
Russian Federation, Moscow, 117393; Moscow, 119991
B. Handke
Faculty of Material Science and Ceramics
Email: a.komolov@spbu.ru
Poland, Kraków
A. S. Komolov
St. Petersburg State University
Author for correspondence.
Email: a.komolov@spbu.ru
Russian Federation, St. Petersburg, 199034
E. F. Lazneva
St. Petersburg State University
Email: a.komolov@spbu.ru
Russian Federation, St. Petersburg, 199034
N. B. Gerasimova
St. Petersburg State University
Email: a.komolov@spbu.ru
Russian Federation, St. Petersburg, 199034
Yu. A. Panina
St. Petersburg State University
Email: a.komolov@spbu.ru
Russian Federation, St. Petersburg, 199034
G. D. Zashikhin
St. Petersburg State University
Email: a.komolov@spbu.ru
Russian Federation, St. Petersburg, 199034
S. A. Pshenichnyuk
Institute of Molecules and Crystals
Email: a.komolov@spbu.ru
Russian Federation, pr. Oktyabrya 151, Ufa, Bashkortostan, 450075
O. V. Borshchev
Enikopolov Institute of Synthetic Polymeric Materials
Email: a.komolov@spbu.ru
Russian Federation, Moscow, 117393
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