. Introduction
Subextension of unbounded plurisubharmonic functions with estimation on total Monge–
Ampère mass of subextension was investigated by many authors in the last ten years.
Let " ⊂ "! be domains in Cn and let u be a plurisubharmonic function on " (briefly,
u ∈ P SH(")). A function !u ∈ P SH("!) is subextension of u if for all z ∈ ",!u(z) ≤ u(z).
On bounded hyperconvex domains in Cn, Cegrell and Zeriahi investigated the subextension problem for the class F(") ( for more details see Section 2). In [1], the authors
proved that if " ! "! are bounded hyperconvex domains in Cn and u ∈ F("), then there
exists !u ∈ F("!) such that !u ≤ u on " and
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Complex Variables and Elliptic Equations
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ISSN: 1747-6933 (Print) 1747-6941 (Online) Journal homepage:
Subextension of plurisubharmonic functions with
boundary values in weighted pluricomplex energy
classes
Le Mau Hai, Nguyen Xuan Hong & Trieu Van Dung
To cite this article: Le Mau Hai, Nguyen Xuan Hong & Trieu Van Dung (2015) Subextension
of plurisubharmonic functions with boundary values in weighted pluricomplex
energy classes, Complex Variables and Elliptic Equations, 60:11, 1580-1593, DOI:
10.1080/17476933.2015.1036244
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Complex Variables and Elliptic Equations, 2015
Vol. 60, No. 11, 1580–1593,
Subextension of plurisubharmonic functions with boundary values in
weighted pluricomplex energy classes
Le Mau Haia∗, Nguyen Xuan Honga and Trieu Van Dungb
aDepartment of Mathematics, Hanoi National University of Education, Hanoi, Vietnam;
bHung Vuong Gifted High School, Viettri City, Phutho, Vietnam
Communicated by S. Krantz
(Received 16 May 2014; accepted 27 March 2015)
In this paper, we investigate subextension of plurisubharmonic functions in the
weighted pluricomplex energy class Eχ (", f ). Moreover, we show the equality
of the weighted Monge–Ampère measures of subextension and the given function.
Keywords: weighted pluricomplex energy classes; complex Monge–Ampère
operator; subextension of plurisubharmonic functions
AMS Subject Classifications: 32U05; 32U15; 32W20
1. Introduction
Subextension of unbounded plurisubharmonic functions with estimation on total Monge–
Ampère mass of subextension was investigated by many authors in the last ten years.
Let " ⊂ "˜ be domains in Cn and let u be a plurisubharmonic function on " (briefly,
u ∈ P SH(")). A function u˜ ∈ P SH("˜) is subextension of u if for all z ∈ ", u˜(z) ≤ u(z).
On bounded hyperconvex domains in Cn , Cegrell and Zeriahi investigated the subex-
tension problem for the class F(") ( for more details see Section 2). In [1], the authors
proved that if " ! "˜ are bounded hyperconvex domains in Cn and u ∈ F("), then there
exists u˜ ∈ F("˜) such that u˜ ≤ u on " and∫
"˜
(ddcu˜)n ≤
∫
"
(ddcu)n .
In the class Ep("), p > 0, introduced and investigated early in [2], the subextension
problem was investigated by Hiep. He proved in [3] that if " ⊂ "˜ ! Cn are bounded
hyperconvex domains and u ∈ Ep("), then there exists a function u˜ ∈ Ep("˜) such that
u˜ ≤ u on " and ∫
"˜
(−u˜)p(ddcu˜)n ≤
∫
"
(−u)p(ddcu)n .
Recently a weighted pluricomplex energy class Eχ ("), which is generalization of the
classes Ep(") and F(") was introduced and investigated by Benelkourchi, Guedj and
∗Corresponding author. Email: mauhai@fpt.vn
© 2015 Taylor & Francis
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Complex Variables and Elliptic Equations 1581
Zeriahi [4]. In [5], Benelkourchi studied subextension for the class Eχ ("). Theorem 6.2
in [5] claimed that if " ⊂ "˜ are hyperconvex domains in Cn and χ : R− −→ R+ is a
decreasing function with χ(−∞) = +∞ then for every u ∈ Eχ (") there exists u˜ ∈ Eχ ("˜)
such that u˜ ≤ u on " and (ddcu˜)n ≤ (ddcu)n on " and∫
"˜
χ (˜u)(ddcu˜)n ≤
∫
"
χ(u)(ddcu)n .
The subextension problem in the classes with boundary values was considered in recent
years. Namely, in 2008, in [6], the authors showed that if " and "˜ are two bounded
hyperconvex domains such that" ⊂ "˜ ⊂ Cn, n ≥ 1 and u ∈ F(", f ) with f ∈ E(") has
subextension v ∈ F("˜, g) with g ∈ E("˜) ∩ M P SH("˜), and∫
"˜
(ddcv)n ≤
∫
"
(ddcu)n,
under the assumption that f ≥ g on ", where M P SH("˜) denotes the set of maximal
plurisubharmonic functions on "˜.
It should be noticed that in results above only estimation of total Monge–Ampère mass
of subextension was obtained. In our recent paper (see [7]), we investigated subextension
in the classF(", f ) and we proved that the Monge–Ampère measure of subextension does
not change. Namely, let " ⊂ "˜ be bounded hyperconvex domains in Cn and let f ∈ E(")
and g ∈ E("˜) ∩ M P SH("˜) with f ≥ g on ", then for every u ∈ F(", f ) with∫
"
(ddcu)n < +∞,
there exists u˜ ∈ F("˜, g) such that u˜ ≤ u on " and (ddcu˜)n = 1"(ddcu)non "˜.
In this paper, we extend this result to the class Eχ (", f ). Our main theorem is the
following.
Theorem 3.3 Let " ! "˜ be bounded hyperconvex domains in Cn and let f ∈ E(")∩
M P SH("), g ∈ E("˜) ∩ M P SH("˜) with f ≥ g on ". Assume that χ : R− −→ R+
is a decreasing continuous function such that χ(t) > 0 for all t < 0. Then for every
u ∈ Eχ (", f ) such that ∫
"
[χ(u)− ρ](ddcu)n < +∞,
for some ρ ∈ E0("), there exists u˜ ∈ Eχ ("˜, g) such that u˜ ≤ u on " and
χ (˜u)(ddcu˜)n = 1"χ(u)(ddcu)n on "˜.
Note that the proof of the above theorem is different than traditional proofs of the
subextension problem in the other classes, for example, F(", f ) or Eχ (") because the
class Eχ (", f ) does not have good properties as the class F(", f ) and the comparison
between the measure 1"χ(u)(ddcu)n , u ∈ Eχ (", f ) with the measure of subextension is
not simple. Hence, in order to prove the above result we have to find a new approach for
the subextension problem in the class Eχ (", f ).
The paper is organized as follows. Beside the introduction, the paper has two sections.
In Section 2, we recall some elements of pluripotential theory needed for the proof of the
main result. Section 3 is devoted to proving the main result of the paper.
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2. Preliminairies
Some elements of pluripotential theory that will be used throughout the paper can be found in
[8–12]. Now, we recall some Cegrell classes of plurisubharmonic functions (see [13–15])
and classes of plurisubharmonic functions with generalized boundary values concerning
Cegrell classes. Let " be an open set in Cn . By P SH−("), we denote the set of negative
plurisubharmonic functions on ".
2.1. Cegrell classes
Now, we assume that " is a bounded hyperconvex domain in Cn . This means that " is a
bounded domain in Cn and there exists a plurisubharmonic function ϕ : " −→ (−∞, 0)
such that for every c < 0 the set "c = {z ∈ " : ϕ(z) < c} ! ". As in [13], we define the
following subclasses of P SH−("):
E0(") =
{
ϕ ∈ P SH−(") ∩ L∞(") : lim
z→∂"ϕ(z) = 0,
∫
"
(ddcϕ)n <∞
}
,
F(") =
{
ϕ ∈ P SH−(") : ∃ E0(") ∋ ϕ j ↘ ϕ, sup
j
∫
"
(
ddcϕ j
)n
<∞
}
,
and
E(") =
{
ϕ ∈ P SH−(") : ∀z0 ∈ ", ∃ a neighbourhood U ∋ z0,
E0(") ∋ ϕ j ↘ ϕ on U, sup
j
∫
"
(
ddcϕ j
)n
<∞
}
.
The following inclusions are obvious: E0(") ⊂ F(") ⊂ E(").
2.2. Maximal plurisubharmonic functions
Since in this paper we also need the class of maximal plurisubharmonic functions, we recall
the following definition given in [16].
Definition 2.1 A plurisubharmonic function u on " is said to be maximal (briefly, u ∈
M P SH(")) if for every compact et K ! " and for every v ∈ P SH("), if v ≤ u on"\ K
then v ≤ u on ".
It is well known (see, e.g. [10]) that locally bounded plurisubharmonic functions are
maximal if and only if they satisfy the homogeneous Monge–Ampère equation (ddcu)n = 0.
In [17], Błocki extended the above result for the class E(").
2.3. The classN (!)
We recall the class N (") introduced in [14]. Let " be a hyperconvex domain in Cn
and {" j } j≥1 a fundamental sequence of ". This is an increasing sequence of strictly
pseudoconvex subsets {" j } j≥1 of " such that " j ! " j+1 and ⋃+∞j=1 " j = ". Let
ϕ ∈ P SH−("). For each j ≥ 1, put
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Complex Variables and Elliptic Equations 1583
ϕ j = sup {u : u ∈ P SH("), u ≤ ϕ on "\" j} .
As in [14], the function (lim j→∞ ϕ j )∗ ∈ M P SH("). Set
N (") =
{
ϕ ∈ E(") : ϕ j ↑ 0
}
.
It is easy to see that F(") ⊂ N (") ⊂ E(").
2.4. The class Eχ (!)
Next, we recall the class Eχ (") (see Definition 3.1 in [4]) and the relation between this
class and the classes Ep("),F(") and N (").
Definition 2.2 Let χ : R− −→ R+ be a decreasing function and " be a hyperconvex
domain in Cn . We say that the function u ∈ P SH−(") belongs to Eχ (") if there exists a
sequence {u j } ⊂ E0(") decreasing to u on " and satisfying
sup
j
∫
"
χ(u j )(ddcu j )n < +∞.
If we take χ(t) = (−t)p, p > 0 then the class Eχ (") coincides with the class Ep(").
If χ(t) is bounded and χ(0) > 0 then Eχ (") is the class F("). Proposition A in [5] and,
more generally, Corollary 3.3 in [18] claims that if χ ̸≡ 0 then Eχ (") ⊂ E(") and, hence,
in this case the Monge–Ampère operator is well defined on Eχ ("). Corollary 3.3 in [18]
shows that if χ(t) > 0 for t < 0 then Eχ (") ⊂ N ("). Moreover, Theorem 2.7 in [19]
implies that
Eχ (") =
⎧⎨⎩u ∈ N (") :
∫
"
χ(u)(ddcu)n < +∞
⎫⎬⎭ .
Below we need the following result.
Proposition 2.3 Let χ : R− −→ R+ be a decreasing continuous function such that
χ(t) > 0 for all t < 0 and " be a bounded hyperconvex domain in Cn. Assume that µ is a
positive Radon measure which vanishes on pluripolar sets of " and u, v ∈ E(") are such
that χ(u)(ddcu)n ≥ µ and χ(v)(ddcv)n ≥ µ. Then
χ(max(u, v))(ddc max(u, v))n ≥ µ.
Proof From the hypothesis, we have
(ddcu)n ≥ 1{u=v} µ
χ(u)
= 1{u=v} µ
χ(max(u, v))
.
Similarly,
(ddcv)n ≥ 1{u=v} µ
χ(v)
= 1{u=v} µ
χ(max(u, v))
.
Proposition 4.3 in [20] implies that
(ddc(max(u, v))n ≥ 1{u=v} µ
χ(max(u, v))
,
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1584 L.M. Hai et al.
or
χ(max(u, v))(ddc(max(u, v))n ≥ 1{u=v}µ.
The above inequality together with Theorem 4.1 in [20] give us that
χ(max(u, v))(ddc max(u, v))n
= 1{u>v}χ(max(u, v))(ddc max(u, v))n
+ 1{u=v}χ(max(u, v))(ddc max(u, v))n + 1{u<v}χ(max(u, v))(ddc max(u, v))n
= 1{u>v}χ(u)(ddcu)n + 1{u=v}χ(max(u, v))(ddc max(u, v))n
+ 1{u<v}χ(v)(ddcv)n
≥ 1{u>v}µ+ 1{u=v}µ+ 1{u<v}µ = µ,
and the proof is complete. "
2.5. Cegrell classes with boundary values
We recall classes of plurisubharmonic functions with generalized boundary values in the
class E(").
Definition 2.4 LetK ∈ {E0("),F("),N ("), Eχ ("), E(")} and let f ∈ E("). Then we
say that a plurisubharmonic function u defined on" is inK(", f ) if there exists a function
ϕ ∈ K such that
ϕ + f ≤ u ≤ f,
on ". By Ka(", f ), we denote the set of plurisubharmonic functions u ∈ K(", f ) such
that (ddcu)n vanishes on all pluripolar sets of ".
For systematic and complete study of classes of plurisubharmonic functions with gen-
eralized boundary values in other classes, we refer readers to the paper of [21]. Note that
functions in K(", f ) not necessarily have finite total Monge–Ampère mass (see [22]).
We need the following proposition which will be used in the main result of the paper.
Proposition 2.5 Let " be a bounded hyperconvex domain in Cn and let f ∈ E(") ∩
M P SH("). Then for every u ∈ N (", f ) such that∫
{u=−∞}∩"
(ddcu)n < +∞,
there exists v ∈ F(", f ) such that v ≥ u and
(ddcv)n = 1{u=−∞}(ddcu)n .
Proof Let ϕ ∈ N (") such that ϕ + f ≤ u ≤ f on ". We may assume that ϕ ≥ u
on ". Indeed, put ψ = max(ϕ, u). Then ψ ∈ N ("),ψ ≥ u on ". It is easy to see that
ψ+ f ≤ u ≤ f on". By replacing ϕ byψ , the desired conclusion follows. Since (ddc f )n
vanishes on pluripolar sets of " and 0 ≤ ϕ − u ≤ − f so by Lemma 4.12 in [8], we get
1{u=−∞}(ddcu)n = 1{ϕ=−∞}(ddcϕ)n
≤ (ddcϕ)n .
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Complex Variables and Elliptic Equations 1585
Hence, Theorem 4.14 in [8] implies that there existsw ∈ N (", f ) such thatϕ+ f ≤ w ≤ f
on " and
(ddcw)n = 1{u=−∞}(ddcu)n .
We have
∫
"(dd
cw)n = ∫{u=−∞}∩"(ddcu)n < +∞ then Proposition 2.2 in [6] implies
that w ∈ F(", f ). Put
ψ1 =
(
sup{ψ ∈ P SH−(") : ψ + f ≤ w on "}
)∗
.
Then ψ1 ∈ P SH−("), ϕ ≤ ψ1 and ψ1 + f ≤ w on ". From Theorem 2.1 in [14], we
have ∫
"
(ddcψ1)n ≤
∫
"
(ddcw)n . (2.1)
Since ψ1 + f ≤ w on " then by Lemma 4.1 in [8], we have
1{w=−∞}(ddcw)n ≤ 1{ψ1+ f =−∞}(ddc(ψ1 + f ))n = 1{ψ1=−∞}
(
ddcψ1
)n
,
where the second equality follows from |ψ1 + f − ψ1| = − f by Lemma 4.12 in [8]. But
(ddcw)n is carried by a pluripolar set then we have the following:
(ddcw)n = 1{w=−∞}(ddcw)n ≤ 1{ψ1+ f =−∞}
(
ddc (ψ1 + f ))n (2.2)
= 1{ψ1=−∞}(ddcψ1)n ≤
(
ddcψ1
)n
.
Combining (2.1) and (2.2) we get
(ddcw)n = 1{ψ1=−∞}(ddcψ1)n .
Hence 1{ψ1=−∞}(ddcψ1)n = 1{u=−∞}(ddcu)n .
Put v = max(w, u). We have ϕ + f ≤ u ≤ v ≤ f . Hence, v ∈ N (", f ), v ≥ u. We
shall prove that (ddcv)n = 1{u=−∞}(ddcu)n and v ∈ F(", f ) and the proof of Proposition
2.5 will be finished. First, we note that v ≤ ψ1 on ". Indeed, because u + f ≤ ϕ + f ≤ w
andw+ f ≤ w then v+ f = max(w+ f, u+ f ) ≤ w and by the definition ofψ1 the desired
conclusion follows. On the other hand, since v,w ∈ N (", f ), v ≥ w, ∫"(ddcw)n < +∞
then Lemma 3.3 in [8] implies that∫
"
(ddcv)n ≤
∫
"
(ddcw)n . (2.3)
From u ≤ v ≤ ψ1 then by Lemma 4.1 in [8], we have
1{ψ1=−∞}(ddcψ1)n ≤ 1{v=−∞}(ddcv)n ≤ 1{u=−∞}(ddcu)n .
But we have proved that 1{ψ1=−∞}(ddcψ1)n = 1{u=−∞}(ddcu)n then
1{v=−∞}(ddcv)n = 1{u=−∞}(ddcu)n = (ddcw)n .
Hence,
(ddcv)n ≥ (ddcw)n . (2.4)
Now (2.3) and (2.4) give us that∫
"
(ddcw)n ≤
∫
"
(ddcv)n ≤
∫
"
(ddcw)n =
∫
{u=−∞}∩"
(ddcu)n < +∞.
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Therefore,
(ddcv)n = (ddcw)n = 1{u=−∞}(ddcu)n .
Moreover, by Proposition 2.2 in [6] we infer that v ∈ F(", f ). The proof is
complete. "
3. Proof of the main theorem
In this section, we give the proof of the main result of the paper. However, to arrive at the
desired result we need some auxiliary lemmas.
Lemma 3.1 Let " ⊂ "˜ be bounded hyperconvex domains in Cn and let f ∈ E("),
g ∈ E("˜) ∩ M P SH("˜) with f ≥ g on ". Assume that u ∈ F(", f ) is such that
(a) (ddcu)n is carried by a pluripolar set.
(b) ∫"(ddcu)n < +∞.
Then the function
u˜ := (sup {ϕ ∈ F("˜, g) : ϕ ≤ u on "})∗
belongs to F("˜, g) and (ddcu˜)n = 1"(ddcu)n on "˜.
Proof Without loss of generality we may assume that (ddcu)n is carried by the set {u =
−∞}. By [6], there exists v ∈ F ("˜, g) such that v ≤ u on " and∫
"˜
(ddcv)n ≤
∫
"
(ddcu)n .
Since v ≤ u˜ ≤ g in "˜ so u˜ ∈ F("˜, g). By Lemma 3.3 in [8], we have∫
"˜
(
ddcu˜
)n ≤ ∫
"˜
(ddcv)n ≤
∫
"
(ddcu)n .
Moreover, since u˜ ≤ u in " so Lemma 4.1 in [8] implies that
1{˜u=−∞}
(
ddcu˜
)n ≥ 1{u=−∞}(ddcu)n on ".
Therefore, since (ddcu)n is carried by the set {u = −∞} so(
ddcu˜
)n ≥ 1"(ddcu)n on "˜.
Now, we have ∫
"˜
(ddcu˜)n ≤
∫
"
(ddcu)n =
∫
"∩{u=−∞}
(ddcu)n
≤
∫
"∩{˜u=−∞}
(ddcu˜)n ≤
∫
"˜
(ddcu˜)n,
and it follows that (ddcu˜)n = 1"(ddcu)n on "˜. The proof is complete. "
The following lemma is an essential tool in the proof of the main result.
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Complex Variables and Elliptic Equations 1587
Lemma 3.2 Let" be a bounded hyperconvex domain inCn and letµ be a positive Radon
measure which vanishes on pluripolar sets of" with µ(") < +∞. Let χ : R− → R+ be a
bounded decreasing continuous function such that χ(t) > 0 for all t < 0 and χ(−∞) = 1.
Assume that f ∈ E(") ∩ M P SH(") and v ∈ F(", f ) such that (ddcv)n is carried by a
pluripolar set and ∫
"
(ddcv)n < +∞.
Then the function u defined by
u := (sup {ϕ ∈ E(") : ϕ ≤ v and χ(ϕ)(ddcϕ)n ≥ µ})∗
belongs to N (", f ) and
χ(u)(ddcu)n ≥ µ+ (ddcv)n .
Moreover, if supp(ddcv)n ! " and ∫"(−ρ)(ddcu)n < +∞ for some ρ ∈ E0(") then
χ(u)(ddcu)n = µ+ (ddcv)n .
Proof First, we prove that u ∈ N (", f ). Indeed, since µ vanishes on all pluripolar sets
of " and µ(") < +∞ so Theorem 4.10 in [18] implies that there exists '0 ∈ N (") such
that
χ('0)(ddc'0)n = µ.
We have '1 := '0 + v ∈ N (", f ) and
χ('1)(ddc'1)n ≥ χ('0)(ddc'0)n = µ.
Hence, we have u ≥ '1 and the desired conclusion follows. Next, we claim that
χ(u)(ddcu)n ≥ µ. Indeed, by Choquet’s lemma and Proposition 2.3 we can choose a
sequence {ϕ j } ⊂ E(") such that ϕ j ≥ '1, ϕ j ↗ u a.e. in " and
χ(ϕ j )(ddcϕ j )n ≥ µ.
Fix k and let j ≥ k. Since χ(ϕ j ) ≤ χ(ϕk) so
χ(ϕk)(ddcϕ j )n ≥ χ(ϕ j )(ddcϕ j )n ≥ µ.
It follows that
(ddcϕ j )n ≥ 1
χ(ϕk)
µ
for every j ≥ k. Letting j → +∞, by [23] we get
(ddcu)n ≥ 1
χ(ϕk)
µ.
Since ϕk ↗ u as k ↗∞ outside a pluripolar set of " and µ vanishes on pluripolar sets of
" so by letting k → +∞, we get
(ddcu)n ≥ 1
χ(u)
µ,
as we wanted.
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1588 L.M. Hai et al.
Next, we prove thatχ(u)(ddcu)n ≥ µ+(ddcv)n . Indeed, sinceµ vanishes on pluripolar
sets of " and χ(u)(ddcu)n ≥ µ so
1{u ̸=−∞}χ(u)(ddcu)n ≥ µ.
Moreover, since u ≤ v so Lemma 4.1 in [8] implies that
1{u=−∞}χ(u)(ddcu)n = 1{u=−∞}(ddcu)n ≥ 1{v=−∞}(ddcv)n .
Therefore,
χ(u)(ddcu)n ≥ µ+ (ddcv)n .
Now, assume that supp(ddcv)n ! U ! " and ∫"(−ρ)(ddcu)n < +∞. Note that by
Theorem 2.4 in [8] we can assume that ρ ∈ E0(") ∩ C("). By Proposition 2.5 in [8] we
can choose a sequence {v j } ∈ E0(", f ) such that supp(ddcv j )n ! U ! " and v j ↘ v as
j ↗∞. Since 0 ≤ χ ≤ 1 and v ≤ v j so by Lemma 3.3 in [8], we have∫
"
χ(v j )(ddcv j )n ≤
∫
"
(ddcv j )n ≤
∫
"
(ddcv)n < +∞.
Moreover, since µ(") < +∞ so by Theorem 4.10 in [18] there exists a function w j ∈
N (", f ) such that
χ(w j )(ddcw j )n = µ+ χ(v j )(ddcv j )n . (3.1)
Since χ(w j )(ddcw j )n ≥ χ(v j )(ddcv j )n so Theorem 4.8 in [18] implies that w j ≤ v j on
". Put
u j := (sup {ϕ ∈ E(") : ϕ ≤ v j and χ(ϕ)(ddcϕ)n ≥ µ})∗ .
We have u j ≥ w j on ". Since u j+1 ≤ u j so u j+k ≤ u j for every k ≥ 0. Hence,
w j ≤ ψ j :=
(
sup
k∈N
w j+k
)∗
≤ u j .
Therefore, ψ := lim j→+∞ ψ j ≤ u := lim j→+∞ u j . Moreover, since
(ddc('0 + v j ))n ≥ (ddc'0)n + (ddcv j )n,
and χ('0 + v j ) ≥ χ('0),χ('0 + v j ) ≥ χ(v j ) and by (3.1) we infer that
χ('0 + v j ) (ddc ('0 + v j ))n ≥ χ('0 + v j ) ((ddc'0)n + (ddcv j )n)
= χ('0 + v j ) (ddc'0)n + χ('0 + v j ) (ddcv j )n
≥ χ('0) (ddc'0)n + χ(v j ) (ddcv j )n
= µ+ χ(v j ) (ddcv j )n = χ(w j ) (ddcw j )n
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Complex Variables and Elliptic Equations 1589
so by Theorem 4.8 in [18] we havew j ≥ '0+v j ≥ '0+v. It follows thatψ,ψ j ∈ N (", f )
and ψ j ↘ ψ as j −→∞. Hence, by Lemma 3.3 and Corollary 3.4 in [8], we have∫
"
(−ρ)(ddcu)n ≤
∫
"
(−ρ)(ddcψ)n = lim
j→∞
∫
"
(−ρ)(ddcψ j )n (3.2)
≤ lim sup
j→∞
∫
"
(−ρ)(ddcw j )n
≤ lim sup
j→∞
∫
"
−ρ
χ(ψ j )
[µ+ (ddcv j )n]
≤ lim sup
j→∞
∫
"
−ρ
χ(ψ j )
µ+ lim sup
j→∞
∫
"
−ρ
χ(ψ j )
(ddcv j )n
≤
∫
"
−ρ
χ(ψ)
µ+ lim sup
j→∞
∫
U
−ρ
χ(ψ j )
(ddcv j )n,
where the first term in the (3.2) follows from the monotone convergence theorem and for
the second by invoking supp(ddcv j )n ! U ! ". We have v j ↘ v ∈ E(") then Corollary
3.3 in [23] implies that−ρ(ddcv j )n is convergent weakly to−ρ(ddcv)n . Moreover, 1χ(ψ j )
is upper-semicontinuous and decreasing to 1χ(ψ) . Hence, we have the following estimation
for the second term of (3.2):
lim sup
j→∞
∫
U
−ρ
χ(ψ j )
(ddcv j )n ≤
∫
U
−ρ
χ(ψ)
(ddcv)n (3.3)
≤
∫
"
−ρ
χ(ψ)
(ddcv)n ≤
∫
"
−ρ
χ(u)
(ddcv)n .
Combining (3.2) and (3.3) we get∫
"
(−ρ)(ddcu)n ≤
∫
"
−ρ
χ(u)
[µ+ (ddcv)n].
On the other hand, since
∫
"(−ρ)(ddcu)n < +∞ and
−ρ(ddcu)