The Improvement of Immunity to Electromigration by Means of Microstructural Design

1996 ◽  
Vol 428 ◽  
Author(s):  
O. V. Kononenko ◽  
V. N. Matveev

AbstractIt is known from literature that the properties of thin films greatly depend on their structuare. Therefore, the microstructural design is attractive for control over the properties of thin metal films used for interconnect metallization.In this paper we discuss the potentialities of the self-ion assisted deposition technique for control over the grain and grain boundary structures of thin metal films and their properties such as resistivity and immunity to electromigration.It was found that resistivity of aluminum films deposited at the 6 kV bias was virtually equal to resistivity of bulk aluminum. Films deposited at the less bias or without it had higher resistivities. Abnormal grain growth was found in 6 kV-films. In films prepared without bias normal grain growth proceeds.

1990 ◽  
Vol 67 (9) ◽  
pp. 4099-4104 ◽  
Author(s):  
C. V. Thompson ◽  
J. Floro ◽  
Henry I. Smith

1999 ◽  
Vol 47 (10) ◽  
pp. 2865-2878 ◽  
Author(s):  
H. Gao ◽  
L. Zhang ◽  
W.D. Nix ◽  
C.V. Thompson ◽  
E. Arzt

Author(s):  
H. P. Singh ◽  
L. E. Murr

This paper reports observations of nucleation and growth characteristics of thin metal films vapor deposited onto heated sodium chloride substrates. An attempt is made to explain the differences in nucleation and growth characteristics on the basis of classical nucleation theory.Thin metal films were prepared by vapor deposition onto heated NaCl (001) substrates in a commercial vacuum unit using a constant evaporation rate of approximately 1000 Å/sec. In the case of discontinuous thin films, approximately 200 Å of carbon was deposited for support. Samples for electron microscopy were prepared by standard techniques and were observed at 125 kV. Figs. 1(a) to (c) show a growth sequence of gold thin films characterized by 1) the formation of random, three dimensional, isolated nuclei at initial deposition, and their growth with further deposition predominantly by surface diffusion; 2) coalescence of these nuclei forming bigger islands; 3) the flattening of islands and formation of network structure : and 4) the filling up of these network structures with further deposition forming a continuous film.


2010 ◽  
Vol 58 (16) ◽  
pp. 5232-5241 ◽  
Author(s):  
D.V. Bachurin ◽  
D. Weygand ◽  
P. Gumbsch

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