Young’s modulus and density of nanocrystalline cubic boron nitride films determined by dispersion of surface acoustic waves

被引:0
|
作者
G. Lehmann
P. Hess
S. Weissmantel
G. Reisse
P. Scheible
A. Lunk
机构
[1] Institute of Physical Chemistry,
[2] University of Heidelberg,undefined
[3] Im Neuenheimer Feld 253,undefined
[4] 69120 Heidelberg,undefined
[5] Germany (Fax: +49-6221/54-4255,undefined
[6] E-mail: Peter.Hess@urz.uni-heidelberg.de),undefined
[7] Hochschule Mittweida,undefined
[8] University of Applied Sciences,undefined
[9] Technikumplatz 17,undefined
[10] 09648 Mittweida,undefined
[11] Germany (Fax: +49-3727/58-1379,undefined
[12] E-mail: GReisse@htwm.de),undefined
[13] Institut für Plasmaforschung,undefined
[14] University of Stuttgart,undefined
[15] Pfaffenwaldring 31,undefined
[16] 70569 Stuttgart,undefined
[17] Germany (Fax: +49-711/685-3102,undefined
[18] E-mail: lunk@ipf.uni-stuttgart.de),undefined
来源
Applied Physics A | 2002年 / 74卷
关键词
PACS: 43.35; 68.35; 68.60; 81.05;
D O I
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学科分类号
摘要
Cubic boron nitride (c-BN) films of 200–420 nm thickness and high phase purity were deposited on silicon (100) substrates by ion-assisted pulsed laser deposition (IA PLD)from a boron nitride target using a KrF-excimer laser, and by plasma-enhanced physical vapor deposition (PE PVD)with a hollow-cathode arc evaporation device. In order to improve the c-BNfilm adhesion, hexagonal boron nitride (h-BN) films with 25–50 nm thickness were used as buffer layers. The density and Young’s modulus of the c-BNfilms were obtained by investigating the dispersion of surface acoustic waves. In data analysis a two-layer model was applied in order to take the influence of the h-BNlayer into consideration. The values for the density vary from 2.95±0.25 g/cm3to 3.35±0.3 g/cm3, and those for the Young’s modulus from 420±40 GPa to 505±30 GPa. The results are compared with literature values reported for nanocrystalline films, polycrystalline disks and single crystal c-BN.
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页码:41 / 45
页数:4
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