106 J. Li et al. / Discrete Applied Mathematics 171 (2014) 104–115
Fig. 2. Separating an edge uv.
uv (see Fig. 2). In this paper, we study how the second smallest normalized Laplacian eigenvalue behaves when the graph is
perturbed by separating an edge. This result can be used to determine all trees and unicyclic graphs with λ
2
(G) ≥ 1 −
√
2
2
.
Moreover, the trees and unicyclic graphs with λ
2
(G) = 1 −
√
2
2
are also determined, respectively.
2. An edge-separating theorem on λ
2
(G)
In this section, we consider how the second smallest normalized Laplacian eigenvalue behaves when the graph is
perturbed by separating an edge. Similar problem has been studied for the algebraic connectivity [5]. Before giving our
main result, the following lemmas are needed.
Lemma 2.1 ([8]). Let G = (V, E) be a connected graph and L be its normalized Laplacian matrix. Let f be a harmonic
eigenfunction associated with λ
2
(G). Let v be a cut vertex of G such that G
0
, G
1
, . . . , G
s
are the connected components of the
graph G − v. Then
(1) If f (v) > 0, then exactly one of the components G
i
contains a vertex negatively valuated by f . For all vertices u in the remaining
components f (u) > f (v).
(2) If f (v) = 0 and there exists a component G
i
containing both positively and negatively valuated vertices, then there is exactly
one such component, all remaining components being zero valuated.
(3) If f (v) = 0 and no component contains both positively and negatively valuated vertices, then each component contains either
only positively valuated, or negatively valuated, or zero valuated vertices.
Lemma 2.2 ([6]). Let G be a connected graph with a cutpoint v and α(G) be the algebraic connectivity of G. Then α(G) ≤ 1, the
equality holds if and only if v is adjacent to every vertex of G.
Combined with Proposition 1.3, we have the following:
Lemma 2.3. Let G be a connected graph with a cutpoint v. Then λ
2
(G) ≤ 1. Moreover, if λ
2
(G) = 1 then v is adjacent to every
vertex of G and δ(G) = 1.
Proof. From Proposition 1.3 and Lemma 2.2, we have λ
2
(G) ≤
α(G)
δ(G)
≤
1
δ(G)
≤ 1. Moreover, if λ
2
(G) = 1, then we have
α(G) = 1 and δ(G) = 1. Lemma 2.2 implies that v is adjacent to every vertex of G.
Theorem 2.4. Let e = uv be a cut edge of a connected graph G and suppose that G − uv = G
1
∪ G
2
(|V (G
1
)|, |V (G
2
)| ≥ 2),
where G
1
and G
2
are two components of G − uv, u ∈ V (G
1
) and v ∈ V (G
2
). Let G
′
be the graph obtained from G by separating
the edge uv. Then λ
2
(G) ≤ λ
2
(G
′
), and the inequality is strict if f (v
e
) = 0, where f is a harmonic eigenfunction associated with
λ
2
(G
′
).
Proof. Let V (G
1
) = {u, u
1
, u
2
, . . . , u
n
1
} and V (G
2
) = {v, v
1
, v
2
, . . . , v
n
2
}, f be a harmonic eigenfunction associated with
λ
2
(G
′
). Then V (G
′
) = {u
e
, v
e
, u
1
, u
2
, . . . , u
n
1
, v
1
, v
2
, . . . , v
n
2
}. Let d(x) and d
′
(x) be the degrees of x in G and G
′
, respectively.
Let D
′
and D be the diagonal degree matrices of G
′
and G, respectively. Then d
′
(u
e
) = d(u) + d(v) − 1, d
′
(v
e
) = 1, d
′
(u
i
) =
d(u
i
) for i = 1, . . . , n
1
and d
′
(v
i
) = d(v
i
) for i = 1, . . . , n
2
. From Proposition 1.2, we have λ
2
(G
′
) ≤ 1 since G
′
= K
n
. If
λ
2
(G
′
) = 1, from Lemma 2.3, we have λ
2
(G) < 1 since u (or v) is a cutpoint of G and |V (G
2
)| ≥ 2 (or |V (G
1
)| ≥ 2). Then
the result follows. Now we suppose that λ
2
(G
′
) < 1. Note that −f is also a harmonic eigenfunction associated with λ
2
(G
′
).
We may assume that f (v
e
) ≥ 0. From Proposition 1.1, we have (1 − λ
2
(G
′
))f (v
e
) = f (u
e
). Assume that f (v
e
) = 0. Then
f (u
e
) = 0.
Let h be a vector such that
h(u) = f (u
e
) = 0;
h(v) = f (v
e
) = 0;
h(u
i
) = f (u
i
) for i = 1, 2, . . . , n
1
;
h(v
i
) = f (v
i
) for i = 1, 2, . . . , n
2
.
Then ⟨h, De⟩ =
n
1
i=1
d(u
i
)h(u
i
) +
n
2
i=1
d(v
i
)h(v
i
) =
n
1
i=1
d
′
(u
i
)f (u
i
) +
n
2
i=1
d
′
(v
i
)f (v
i
) = ⟨f , D
′
e⟩ = 0. Moreover,
⟨h, L(G)h⟩ =
xy∈E(G)
(h(x) − h(y))
2
=
xy∈E(G
′
)
(f (x) − f (y))
2
= ⟨f , L(G
′
)f ⟩ and ⟨h, Dh⟩ =
n
1
i=1
d(u
i
)h(u
i
)
2
+
n
2
i=1
d(v
i
)h(v
i
)
2
=
n
1
i=1
d
′
(u
i
)f (u
i
)
2
+
n
2
i=1
d
′
(v
i
)f (v
i
)
2
= ⟨f , D
′
f ⟩.