Hardware Reference
In-Depth Information
Vn 1 is interpreted as a logic '0' if it is smaller than the gate 'c' logic threshold
Vth c .A defective effect appears on the output of gate 'c' and is propagated to the
primary output of the circuit.
Vn 1 is interpreted as a logic '1' if it is higher than the gate 'c' logic threshold
Vth c .A defect-free effect appears on the output of gate 'c' and is propagated to
the primary output of the circuit.
This small example highlights that the bridge defect may be detected or not by
a given test vector depending on the value of the intermediate potential Vn 1 .This
potential depends on the technological and topological transistor parameters of Gate
'a' (C ox ,V T , P ,W P ,L P :::) but also on the value of the bridge resistance Rsh. As
the bridge resistance value is obviously an unpredictable parameter, it is not possible
to compute the intermediate voltage Vn 1 . Consequently it is not possible to predict
the effect of the defect.
However, it is possible to analyze the impact of the bridge resistance value on
the effect of the defect. Figure 2.10 shows the Vn 1 vs. Rsh characteristics obtained
through electrical simulations. Two distinct regions can be distinguished according
to the Rsh value. In the high resistance range, the bridging defect does not modify
the logical behaviour and the circuit operates as a defect-free circuit. In the low resis-
tance range, the bridging defect induces a Vn 1 value smaller than the logic threshold
Vth c of the driven gate 'c' and this value is logically interpreted as a defective '0'.
The frontier between these two regions corresponds to a critical resistance value
R C . It is worth noting that although the bridge resistance value is an unpredictable
Vn 1
5
Vth c
0
R C
R C
Rsh
Vn 3
5
0
R C
R C
Rsh
Out
5
Fig. 2.10 Analogue
detectability interval
( Renovell et al. 1999 )
0
R C
R C
Rsh
 
 
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