6.5 Fixed Modes of Decentralized Systems 397
done in O(|E|) time and the potential function of (6.110) for a strong com-
ponent
ˆ
G =(
ˆ
V,
ˆ
E), if any, can be found in time of O(|
ˆ
E|) by the procedure
of Remark 6.4.19. It should be emphasized here that the whole algorithm
involves only pivoting operations on the matrix Q(1), the entries of which
are rational numbers (simple numbers such as ±1 in practical applications).
Remark 6.5.16. The graph-theoretic criterion in Theorem 6.5.7 can be
derived from Theorem 6.5.12 and Theorem 6.5.15 applied to the matrix
D(s)=Q(s)+T (s)+K defined by (6.96) in Remark 6.5.10. Recall (cf. (6.88))
that both Row(D) and Col(D) have a natural one-to-one correspondence
with X ∪ U ∪ Y , to be denoted by ν
R
:Row(D) → X ∪ U ∪ Y and
ν
C
: Col(D) → X ∪ U ∪ Y . Note also that Q(s) satisfies (MP-Q2) with
r
i
=
1(ν
R
(i) ∈ X)
0(ν
R
(i) ∈ U ∪ Y ),
c
j
=0 (j ∈ Col(D)).
In considering nonzero fixed modes we may take (
ˆ
I,
ˆ
J)=(∅, ∅) since Q(s)is
nonsingular. The auxiliary network N =(G, γ)for(
ˆ
I,
ˆ
J)=(∅, ∅)iseasyto
identify. We have
E
TQ
= {(ϕ
T
(j),ϕ
Q
(j)) | j ∈ Col(D)},
E
QT
= {(ϕ
Q
(i),ϕ
T
(i)) | i ∈ Row(D)},
E
Q
= {(ϕ
Q
(j),ϕ
Q
(i)) | ν
R
(i)=ν
C
(j),i∈ Row(D),j ∈ Col(D)},
E
T
= {(ϕ
T
(i),ϕ
T
(j)) | T
ij
=0},
E
K
= {(ϕ
T
(i),ϕ
T
(j)) | K
ij
=0},
E
M
= ∅,
and γ(a)=1ifa =(ϕ
Q
(i),ϕ
T
(i)) ∈ E
QT
with ν
R
(i) ∈ X,andγ(a)=0
otherwise. Let us call an arc a with γ(a)=1acritical arc. A critical arc
corresponds to an element of X. It is easy to see that a strong component of
G (of N) containing a critical arc cannot admit a potential function.
We mean by (M1) the condition that each strong component of G either
contains an arc of E
K
or admits a potential function π such that (6.110)
holds, and by (M2) the condition of nonsingularity of D(0). We also refer to
the conditions (G1) and (G2) in Theorem 6.5.7.
The equivalence of (G2) and (M2) is easy to see. Also the implication,
(G1) =⇒ (M1), is easy to see. The converse is not always true (see Example
6.5.18). Under the condition (M2), however, every critical arc is contained in
a strong component of G, and consequently, the converse, (M1) =⇒ (G1), is
also true. Thus we have shown [(M2) ⇐⇒ (G2)], [(G1) =⇒ (M1)], and [(M1),
(M2) =⇒ (G1)], proving [(M1), (M2) ⇐⇒ (G1), (G2)]. It is emphasized,
however, that (G1) alone does not correspond to the nonexistence of nonzero
fixed modes, as we have seen in Example 6.5.8. 2