TY - JOUR
T1 - High-temperature self-grown Zr O2 layer against Cu diffusion at Cu (2.5 at. % Zr) Si O2 interface
AU - Liu, C. J.
AU - Chen, J. S.
N1 - Funding Information:
The authors gratefully acknowledge the financial support from the National Science Council of Taiwan, R.O.C. (Grant No. NSC-92-2623-7-006-015).
Copyright:
Copyright 2008 Elsevier B.V., All rights reserved.
PY - 2005
Y1 - 2005
N2 - Films of pure Cu and of Cu alloy containing 2.5 at. % of Zr [abbreviated as Cu (2.5 at. % Zr)] were deposited on Si O2 Si substrates by magnetron sputtering. Samples were subsequently annealed at temperatures ranging from 500 to 800 °C in vacuum (2× 10-5 Torr) for 30 min and analyzed by Rutherford backscattering spectrometry, x-ray photoelectron spectroscopy, and glancing incident angle x-ray diffraction. Resistivity of both pure Cu and Cu alloy films, before and after annealing, was measured at room temperature by using a standard four-point probe technique. Upon annealing, the added Zr atoms in Cu (2.5 at. % Zr) diffuse to both the free surface and the alloySi O2 interface and react with the residual oxygen in the vacuum system and with the Si O2 to form a Zr O2 layer. At the interface, a self-grown Zr O2 layer forms upon annealing at 700 °C that hinders Cu from diffusion into the Si O2, while Cu diffusion into Si O2 is apparent for pure Cu on Si O2 at this temperature. The room-temperature resistivity of the as-deposited Cu (2.5 at. % Zr) film is 21.8 μΩ cm and decreases to about 6.2 μΩ cm upon vacuum annealing at 700 °C for 30 min. This value is still thrice that of the pure Cu film similarly treated. The relation between the diffusion of the added Zr and the characteristics of Cu (2.5 at. % Zr) Si O2 interface, self-formed surface layer, and the resistivity change, is discussed.
AB - Films of pure Cu and of Cu alloy containing 2.5 at. % of Zr [abbreviated as Cu (2.5 at. % Zr)] were deposited on Si O2 Si substrates by magnetron sputtering. Samples were subsequently annealed at temperatures ranging from 500 to 800 °C in vacuum (2× 10-5 Torr) for 30 min and analyzed by Rutherford backscattering spectrometry, x-ray photoelectron spectroscopy, and glancing incident angle x-ray diffraction. Resistivity of both pure Cu and Cu alloy films, before and after annealing, was measured at room temperature by using a standard four-point probe technique. Upon annealing, the added Zr atoms in Cu (2.5 at. % Zr) diffuse to both the free surface and the alloySi O2 interface and react with the residual oxygen in the vacuum system and with the Si O2 to form a Zr O2 layer. At the interface, a self-grown Zr O2 layer forms upon annealing at 700 °C that hinders Cu from diffusion into the Si O2, while Cu diffusion into Si O2 is apparent for pure Cu on Si O2 at this temperature. The room-temperature resistivity of the as-deposited Cu (2.5 at. % Zr) film is 21.8 μΩ cm and decreases to about 6.2 μΩ cm upon vacuum annealing at 700 °C for 30 min. This value is still thrice that of the pure Cu film similarly treated. The relation between the diffusion of the added Zr and the characteristics of Cu (2.5 at. % Zr) Si O2 interface, self-formed surface layer, and the resistivity change, is discussed.
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U2 - 10.1116/1.1839911
DO - 10.1116/1.1839911
M3 - Article
AN - SCOPUS:31144476488
SN - 1071-1023
VL - 23
SP - 90
EP - 95
JO - Journal of Vacuum Science and Technology B: Microelectronics and Nanometer Structures
JF - Journal of Vacuum Science and Technology B: Microelectronics and Nanometer Structures
IS - 1
ER -