The properties of radio frequency sputtered transparent and conducting ZnO:F films on polyethylene naphthalate substrate

被引:28
作者
Bowen, A. [1 ]
Li, J. [1 ]
Lewis, J. [2 ,4 ]
Sivaramakrishnan, K. [3 ,4 ]
Alford, T. L. [3 ]
Iyer, S. [1 ]
机构
[1] N Carolina Agr & Tech State Univ, Dept Elect & Comp Engn, Greensboro, NC 27411 USA
[2] RT1 Int Inc, Res Triangle Pk, NC 27709 USA
[3] Arizona State Univ, Dept Chem & Mat Engn, Tempe, AZ 85287 USA
[4] Arizona State Univ, Flexible Display Ctr, Tempe, AZ 85287 USA
基金
美国国家科学基金会;
关键词
Rutherford Backscattering Spectroscopy; Polyethylene naphthalate; Flexible electronics; Thin films; Zinc Oxide; Sputtering; ZnO:F; Transparent conducting oxide; Electrical properties and measurements; Optical properties; ZINC-OXIDE FILMS; CHEMICAL-VAPOR-DEPOSITION; THIN-FILMS; PHYSICAL-PROPERTIES; SURFACE-MORPHOLOGY; OPTICAL-PROPERTIES; ROOM-TEMPERATURE; GROWTH; RESISTIVITY;
D O I
10.1016/j.tsf.2010.10.019
中图分类号
T [工业技术];
学科分类号
08 ;
摘要
We report on the properties of ZnO:F films deposited by RF sputtering on polyethylene naphthalate (PEN) substrates and compared them with films deposited on glass. Detailed and systematic investigations of various properties of films were deposited on PEN substrates were carried out as functions of thickness and annealing ambient. The films were deposited at room temperature and annealed at 150 degrees C in either Ar or 7% H-2/Ar ambients. These films exhibited carrier concentrations between 2 x 10(18)/cm(3) and 9.5 x 10(19)/cm(3), mobility between 3 and 11 cm(2)/V-s, and resistivity between 10(-1) and 10(-2) Omega-cm. Hall mobility variation with concentration has been explained assuming ionized impurity and lattice scattering to be the dominant mechanisms. The transmission of the films varied from 68 to 80% with increasing thickness and the absorption edge was limited by the absorption of the PEN substrate. The mechanical flexibility of the films was measured in terms of its critical radius of bending which was determined from the onset of a sharp increase in electrical resistance. The critical radius varied between 6.5 and 17 mm for film thicknesses varying from 20 to 200 nm. The thickness dependence of critical strain and critical radius can be explained by Griffith defect theory. (C) 2010 Elsevier B.V. All rights reserved.
引用
收藏
页码:1809 / 1816
页数:8
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