Application of atomic force microscopy and scaling analysis of images to predict the effect of current density, temperature and leveling agent on the morphology of electrolytically produced copper

2006 ◽  
Vol 51 (11) ◽  
pp. 2255-2260 ◽  
Author(s):  
T. Zhao ◽  
D. Zagidulin ◽  
G. Szymanski ◽  
J. Lipkowski
1994 ◽  
Vol 367 ◽  
Author(s):  
T. Yoshinobu ◽  
A. Iwamoto ◽  
K. Sudoh ◽  
H. Iwasaki

AbstractThe scaling behavior of the surface roughness of a-and poly-Si deposited on Si was investigated by atomic force microscopy (AFM). The interface width W(L), defined as the rms roughness as a function of the linear size of the surface area, was calculated from various sizes of AFM images. W(L) increased as a power of L with the roughness exponent ∝ on shorter length scales, and saturated at a constant value of on a macroscopic scale. The value of roughness exponent a was 0.48 and 0.90 for a-and poly-Si, respectively, and σ was 1.5 and 13.6nm for 350nm-thick a-Si and 500nm-thick poly-Si, respectively. The AFM images were compared with the surfaces generated by simulation.


1996 ◽  
Vol 428 ◽  
Author(s):  
A. H. Verbruggen ◽  
M. J. C. Van Den Homberg ◽  
A. J. Kalkman ◽  
J. R. Kraayeveld ◽  
A. W.-J. Willemsen ◽  
...  

AbstractChanges in the electrical resistance induced by electromigration in short (< 20 μm) Al lines show a rather well-defined behavior. For current densities j below a critical value jc the resistance change saturates with time and the resistance fully recovers when the current is switched off. Above the critical current density the induced resistance changes do not saturate and vary approximately linearly with time. In this case the resistance changes recover only partially after removal of the current. We report (i) measurements of the current dependence of the magnitude of the reversible resistance changes and (ii) the results of atomic force microscopy (AFM) inspection of the lines after stressing with current densities above jc. The resistance measurements were made with a high-resolution AC bridge technique. The samples were pure, unpassivated Al lines with a film thickness of 100 nm and a line width of 2 gm. The results show a linear dependence between the magnitude of the reversible changes and the current density. The linear dependence is predicted by two models. The first is based on a description of the vacancy flux and the second on a description of the build-up of mechanical stress during an electromigration experiment. To study the origin of the irreversible effects, samples were stressed at current densities above jc, and the induced irreversible changes in the resistance were recorded. Both negative and positive changes of the resistance were observed. After six hours the experiment was stopped and the lines were inspected by atomic force microscopy. It was always possible to observe a void, a hillock or a hillock/void pair that was created during the passage of the DC current. Moreover, lines with decreasing resistance during stress always showed a hillock and lines with an increased resistance always showed a void.


1994 ◽  
Vol 33 (Part 1, No. 1B) ◽  
pp. 383-387 ◽  
Author(s):  
Tatsuo Yoshinobu ◽  
Atsushi Iwamoto ◽  
Hiroshi Iwasaki

2002 ◽  
Vol 48 (2-3) ◽  
pp. 241-247
Author(s):  
R. Venugopal ◽  
B. Sundaravel ◽  
I.H. Wilson ◽  
J.B. Xu

2002 ◽  
Vol 16 (28n29) ◽  
pp. 4395-4400
Author(s):  
Y. CHOI ◽  
N. I. CHO ◽  
J. I. CHOE

Atomic force microscopy was applied to study the formation and growth mechanism of thin multilayers of chromium-molybdenum and chrome prepared by electro-pulse plating, respectively. The chromium-molybdenum and chrome layers were prepared using direct current density of 1.6 mA.mm -2 and pulse currents with on-off time from 5 to 2000 ms in the bath containing 300g l-1 of chromic acid and 75g l-1 ammonium molybdate, and 250g l-1 of chromic acid and 5g l-1 of sulfuric acid, respectively. The higher current density enhanced nucleation rate which resulted in refining grain size. The micro-hardness of the pulse plated chrome and chromium-molybdenum alloy layers increased with the duration of on-off time and pulse current density. The average surface roughness of chrome layer is increased with increasing on/off time ratio for a given peak current density and voltage because the growth and dissolution mainly occurs during on-time and off-time, respectively. However, the average surface roughness of chromium-molybdenum alloy layer is decreased with increasing on/off time ratio for a given peak current density and voltage because the alloying element in the layer.


1999 ◽  
Vol 605 ◽  
Author(s):  
Z. Moktadir ◽  
K. Sato ◽  
A. Matsumuro ◽  
K. Kayukawa ◽  
M. Shikida

AbstractWe have investigated the roughness of a silicon (110)-oriented surface after being etched with 20% TMAH (Tetra-methyl Ammonium Hydroxide). We have used an Atomic Force Microscope to determine the roughness exponent α using three different methods: fractal, power spectrum density and scaling analysis. The value of the parameter α was identified to be close to 1/2. This value is different from the KPZ value, which is 0.4 in 2+1 dimension


1996 ◽  
Vol 105 (13) ◽  
pp. 5542-5551 ◽  
Author(s):  
David J. Semin ◽  
Alan Lo ◽  
Shane E. Roark ◽  
Rex T. Skodje ◽  
Kathy L. Rowlen

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