Hardware Reference
In-Depth Information
Fig. 1.7
Weak
open defects
(
Rodrıguez-Monta nes et al.
2002
)
. (
a
) Metal cavity and formation of
a
weak
open defect due to the Ti barrier and (
b
) resistive via
Weak opens
Strong opens
100
Metal 1
Metal 2
Metal 3
Metal 4
Metal 5
Metal 6
80
60
40
20
0
< 100 k
Ω
Ω
to 1 M
Ω
100 k
Ω
to10 M
Ω
1M
10M
to
100 M
Ω
Ω
100 M
Ω
to1G
Ω
> 1 G
Ω
Fig. 1.8
Distribution of resistances for an open metal line
(
Rodrıguez-Monta nes et al.
2002
)
Delay Model of
Resistive
Opens
Special attention has been paid to interconnect
resistive
opens. They can be modeled
like interconnect
full
opens, but replacing the complete disconnection by an open
open, apart from the defect-free delay caused by the equivalent on resistance .R
ON
/
of the driving network and the total capacitance of the line (C), there is an extra
delay caused by the open. This delay depends on the open resistance .R
o
/ and its
exact location along the defective line .'/, which determines the capacitance located
after the open ..1
'/ C/.