R E S E A R C H
Open Access
Parameterized discrete Hilbert-type
inequalities with intermediate variables
Ricai Luo
1*and Bicheng Yang
2*Correspondence:
1School of Mathematics and
Statistics, Hechi University, Yizhou, P.R. China
Full list of author information is available at the end of the article
Abstract
By means of the weight coefficients and the idea of introducing parameters, a discrete Hilbert-type inequality with the general homogeneous kernel and the intermediate variables is given. The equivalent form is obtained. The equivalent statements of the best possible constant factor related to some parameters, the operator expressions, and a few particular cases are considered.
MSC: 26D15
Keywords: Weight coefficient; Hilbert-type inequality; Equivalent statement; Parameter; Operator expression
1 Introduction
Assuming thatp> 1, 1
p +
1
q= 1,am,bn≥0, 0 <
∞
m=1a
p
m<∞, and 0 <
∞
n=1b
q
n<∞, we have the following Hardy–Hilbert inequality with the best possible constant sin(ππ/p) (cf. [1], Theorem 315):
∞
m=1
∞
n=1 ambn
m+n< π
sin(π/p)
∞
m=1 apm
1
p∞
n=1 bqn
1 q
. (1)
Forp=q= 2, inequality (1) reduces to the well-known Hilbert inequality. Iff(x),g(y)≥0, 0 <0∞fp(x)dx<∞and 0 <∞
0 gq(y)dy<∞, then we have the following
Hardy–Hilbert integral inequality:
∞
0 ∞
0
f(x)g(y)
x+y dx dy< π
sin(π/p)
∞
0
fp(x)dx 1
p ∞
0
gq(y)dy 1 q
(2)
with the best possible constant factor π
sin(π/p)(cf. [1], Theorem 316).
In 1998, by introducing an independent parameterλ> 0, Yang [2,3] gave an extension of (2) (forp=q= 2) with the best possible constant factorB(λ
2,
λ
2) as follows:
∞
0 ∞
0
f(x)g(y)
(x+y)λ dx dy<B
λ
2,
λ
2
∞
0
x1–λf2(x)dx ∞
0
y1–λg2(y)dy 1 2
. (3)
Inequalities (1), (2), (3) and their extensions are important in analysis and its applications (cf. [4–15]).
The following half-discrete Hilbert-type inequality was provided (cf. [1], Theorem 351): IfK(x) (x> 0) is a decreasing function,p> 1, 1p +1q= 1, 0 <φ(s) =0∞K(x)xs–1dx<∞,
then
∞
0 xp–2
∞
n=1
K(nx)an
p
dx<φp
1
q
∞
n=1
apn. (4)
Some new extensions of (4) with their applications were provided by [16–21].
In 2016, by the use of the technique of real analysis, Hong [22] considered some equiv-alent statements of the extensions of (1) with the best possible constant factor related to a few parameters. The other similar works about the extensions of (2) and (3) were given by [23–27].
In this paper, following the way of [22], by means of the weight functions and the idea of introducing parameters, a discrete Hilbert-type inequality with the general homogeneous kernel and the intermediate variables is given, which is an extension of (1). The equivalent form is obtained. The equivalent statements of the best possible constant factor related to parameters, the operator expressions, and a few particular cases are considered.
2 Some lemmas
In what follows, we suppose thatp> 1,1p+1q= 1,α,β> 0,λ∈R,λ2,λ–λ1≤β1,λ1,λ–λ2≤
1
α,kλ(x,y) is a positive homogeneous function of degree –λsatisfying, for anyu,x,y> 0,
kλ(ux,uy) =u–λkλ(x,y).
Also,kλ(x,y) is strictly decreasing with respect tox,y> 0 such that, forγ =λ1,λ–λ2,
kλ(γ) :=
∞
0
kλ(u, 1)uγ–1du∈R+= (0,∞). (5)
We still assume thatam,bn≥0 (m,n∈N ={1, 2, . . .}) such that
0 <
∞
m=1 mp[1–α(
λ–λ2
p +
λ1
q)]–1ap
m<∞ and 0 <
∞
n=1 nq[1–β(
λ–λ1
q +
λ2
p)]–1bq
n<∞.
Definition 1 We define the following weight coefficients:
ωλ(λ2,m) :=mα(λ–λ2)
∞
n=1 kλ
mα,nβnβλ2–1 (m∈N), (6)
λ(λ1,n) :=nβ(λ–λ1)
∞
m=1 kλ
mα,nβmαλ1–1 (n∈N). (7)
Lemma 1 We have the following inequalities:
ωλ(λ2,m) <
1
βkλ(λ–λ2) (m∈N), (8)
λ(λ1,n) <
1
Proof Forβλ2– 1≤0, it is evident thatkλ(mα,yβ)yβλ2–1is strictly decreasing with respect toy> 0. By the decreasingness property, settingu=mα
yβ, we find that
ωλ(λ2,m) <mα(λ–λ2) ∞
0 kλ
mα,yβyβλ2–1dy
= 1
β ∞
0
kλ(u, 1)u(λ–λ2)–1du= 1
βkλ(λ–λ2).
Hence, we have (8).
Forαλ1– 1≤0, it is evident thatkλ(xα,nβ)xαλ1–1is strictly decreasing with respect to
x> 0. By the decreasingness property, settingu=xα
nβ, we find that
λ(λ1,n) <nβ(λ–λ1) ∞
0 kλ
xα,nβxαλ1–1dx
=1
α ∞
0
kλ(u, 1)uλ1–1du= 1
αkλ(λ1).
Hence, we have (9).
Lemma 2 We have the following inequality:
I:=
∞
n=1
∞
m=1 kλ
mα,nβa
mbn
< 1
β1/pα1/qk
1 p
λ(λ–λ2)k
1 q
λ(λ1)
∞
m=1
mp[1–α(λ –λ2
p +
λ1 q)]–1ap
m
1 p
.
× ∞
n=1 nq[1–β(λ
–λ1 q +
λ2 p)]–1bq
n
1 q
. (10)
Proof By Hölder’s inequality with weight (cf. [28]), we obtain
I=
∞
n=1
∞
m=1 kλ
mα,nβn (βλ2–1)/p
m(αλ1–1)/qam
m(αλ1–1)/q n(βλ2–1)/pbn
≤ ∞
m=1
∞
n=1 kλ
mα,nβ n
βλ2–1
m(αλ1–1)(p–1)a
p m
1
p∞
n=1
∞
m=1 kλ
mα,nβ m
αλ1–1
n(βλ2–1)(q–1)b
q n
1 q
=
∞
m=1
ωλ(λ2,m)mp[1–α(
λ–λ2 p +
λ1 q)]–1ap
m
1
p∞
n=1
λ(λ1,n)nq[1–β(
λ–λ1 q +
λ2 p)]–1bq
n
1 q
.
Then, by (8) and (9), we have (10).
Remark1 (i) By (10), forλ1+λ2=λ, we find
0 <
∞
m=1
mp(1–αλ1)–1ap
m<∞ and 0 <
∞
n=1
nq(1–βλ2)–1bq
and the following inequality:
∞
n=1
∞
m=1 kλ
mα,nβa
mbn
< 1
β1/pα1/qkλ(λ1)
∞
m=1
mp(1–αλ1)–1ap
m
1
p∞
n=1
nq(1–βλ2)–1bq
n
1 q
. (11)
In particular, forα=β= 1, we have
∞
n=1
∞
m=1
kλ(m,n)ambn<kλ(λ1) ∞
m=1
mp(1–λ1)–1ap m
1
p∞
n=1
nq(1–λ2)–1bq n
1 q
. (12)
(ii) Forλ= 1,k1(x,y) = x1+y,λ1=1q,λ2=1p, (12) reduces to (1). Hence, (11) is an extension
of (12) and (1).
Lemma 3 The constant factor β1/p1α1/qkλ(λ1)in(11)is the best possible.
Proof For anyε> 0, we set
˜
am:=mα(λ1– ε
p)–1, b˜
n:=nβ(λ2– ε
q)–1 (m,n∈N).
If there exists a constant M (≤ 1
β1/pα1/qkλ(λ1)) such that (11) is valid when replacing 1
β1/pα1/qkλ(λ1) byM, then, in particular, we have
˜ I:=
∞
n=1
∞
m=1 kλ
mα,nβa˜
mb˜n<M
∞
m=1
mp(1–αλ1)–1a˜p
m
1
p∞
n=1
nq(1–βλ2)–1b˜q
n
1 q
.
By the decreasingness property, we obtain
˜ I<M
∞
m=1
mp(1–αλ1)–1mpαλ1–αε–p 1
p∞
n=1
nq(1–βλ2)–1nqβλ2–βε–q 1
q
=M
1 +
∞
m=2 m–αε–1
1
p
1 +
∞
n=2 n–βε–1
1 q
<M
1 +
∞
1
t–αε–1dt 1
p
1 +
∞
1
t–βε–1dt 1 q
=M
ε
ε+1
α 1
p
ε+1
β 1 q
.
By the decreasingness property and Fubini theorem (cf. [29]), we find
˜ I=
∞
n=1
∞
m=1 kλ
mα,nβm
αλ1–1
mεα/p ·
nβλ2–1 nεβ/q
≥ ∞
1
∞
1 kλ
xα,yβx
αλ1–1
xεα/p ·
yβλ2–1 yεβ/q dx
dy
u=x
α
=1
α ∞
1 y–βε–1
∞
1 yβ
kλ(u, 1)u
λ1–εp–1du dy
=1
α ∞
1 y–βε–1
1
1 yβ
kλ(u, 1)u
λ1–εp–1du dy
+ 1
α ∞
1
y–βε–1dy ∞
1
kλ(u, 1)u
λ1–pε–1du
=1
α 1
0
∞
u–1/β
y–βε–1dy k
λ(u, 1)u
λ1–pε–1du
+ 1
αβε ∞
1
kλ(u, 1)uλ1– ε
p–1du
= 1
αβε 1
0
kλ(u, 1)uλ1+ ε
q–1du+ ∞
1
kλ(u, 1)uλ1– ε
p–1du .
Then we have
1
αβ 1
0
kλ(u, 1)u
λ1+εq–1du+ ∞
1
kλ(u, 1)u
λ1–εp–1du
<M
ε+1
α 1
p
ε+ 1
β 1 q
.
Forε→0+, by Fatou’s lemma (cf. [29]), we find
1
αβkλ(λ1) =
1
αβ 1
0
lim
ε→0+kλ(u, 1)u
λ1+qε–1du+ ∞
1
lim
ε→0+kλ(u, 1)u
λ1–εp–1du
≤ 1
αβεlim→0+ 1
0
kλ(u, 1)uλ1+ ε
q–1du+ ∞
1
kλ(u, 1)uλ1– ε
p–1du
≤M lim
ε→0+
ε+1
α 1
p
ε+1
β 1 q
=M
1
α 1 p1
β 1 q
,
namely 1
β1/pα1/qkλ(λ1)≤M. Hence,M=β1/p1α1/qkλ(λ1) is the best possible constant factor
of (11).
Remark2 Settingλˆ1:=λ–pλ2 +λq1,λˆ2:=λ–qλ1 +λp2, we find
ˆ λ1+λˆ2=
λ–λ2 p +
λ1 q +
λ–λ1 q +
λ2 p =
λ p+
λ q =λ,
ˆ λ1≤
1
pα+
1
qα =
1
α, λˆ2≤
1
qβ +
1
pβ =
1
β,
and by Hölder’s inequality (cf. [28]), we obtain
0 <kλ(λ–λˆ2) =kλ(λˆ1) =kλ
λ–λ2
p + λ1
q
=
∞ 0
kλ(u, 1)u λ–λ2
p +
λ1
q–1du= ∞
0
kλ(u, 1)
u
λ–λ2–1
p u
λ1–1
≤ ∞ 0
kλ(u, 1)uλ–λ2–1du
1
p ∞
0
kλ(u, 1)uλ1–1du
1 q
=k 1 p
λ(λ–λ2)k
1 q
λ(λ1) <∞. (13)
We can reduce (10) as follows:
I< 1
β1/pα1/qk
1 p
λ(λ–λ2)k 1 q
λ(λ1) ∞
m=1
mp(1–αλˆ1)–1ap
m
1
p∞
n=1
nq(1–βλˆ2)–1bq
n
1 q
. (14)
Lemma 4 If the constant factor β1/p1α1/qk 1 p
λ(λ–λ2)k 1 q
λ(λ1)in(10)is the best possible,then λ1+λ2=λ.
Proof If the constant factor β1/p1α1/qk 1 p
λ(λ–λ2)k
1 q
λ(λ1) in (10) is the best possible, then by (14) and (11) the unique best possible constant factor must beβ1/p1α1/qkλ(λˆ1) (∈R+), namely
kλ(λˆ1) =k 1 p
λ(λ–λ2)k 1 q
λ(λ1).
We observe that (13) keeps the form of equality if and only if there exist constantsAand
Bsuch that they are not all zero and (cf. [28])
Auλ–λ2–1=Buλ1–1 a.e. in R +.
Assuming thatA= 0 (otherwise,B=A= 0), it follows thatuλ–λ2–λ1=B
Aa.e. in R+, and then
λ–λ2–λ1= 0, namelyλ1+λ2=λ.
3 Main results
Theorem 1 Inequality(10)is equivalent to
J:=
∞
n=1 npβ(
λ–λ1
q +
λ2
p)–1 ∞
m=1 kλ
mα,nβam
p1p
< 1
β1/pα1/qk
1 p
λ(λ–λ2)k 1 q
λ(λ1) ∞
m=1 mp[1–α(
λ–λ2
p +
λ1
q)]–1ap
m
1 p
. (15)
If the constant factor in(10)is the best possible,then so is the constant factor in(15).
Proof Suppose that (15) is valid. By Hölder’s inequality (cf. [28]), we find
I=
∞
n=1
n–1p+β(
λ–λ1
q +
λ2
p)
∞
m=1 kλ
mα,nβam
n1p–β(
λ–λ1
q +
λ2
p)b
n
≤J ∞
n=1 nq[1–β(
λ–λ1
q +
λ2
p)]–1bq
n
1 q
. (16)
On the other hand, assuming that (10) is valid, we set
bn:=npβ( λ–λ1
q +
λ2 p)–1
∞
m=1 kλ
mα,nβam
p–1
, n∈N.
IfJ= 0, then (15) is naturally valid; ifJ=∞, then it is impossible to make (15) valid, namely
J<∞. Suppose that 0 <J<∞. By (10), it follows that
∞
n=1 nq[1–β(
λ–λ1
q +
λ2 p)]–1bq
n
=Jp=I< 1
β1/pα1/qk
1 p
λ(λ–λ2)k 1 q
λ(λ1)
× ∞
m=1 mp[1–α(
λ–λ2
p +
λ1
q)]–1ap
m
1
p∞
n=1 nq[1–β(
λ–λ1
q +
λ2
p)]–1bq
n
1 q
,
J=
∞
n=1 nq[1–β(
λ–λ1 q +
λ2 p)]–1bq
n
1 p
< 1
β1/pα1/qk
1 p
λ(λ–λ2)k 1 q
λ(λ1) ∞
m=1 mp[1–α(
λ–λ2 p +
λ1 q)]–1ap
m
1 p
,
namely (15) follows, which is equivalent to (10).
If the constant factor in (10) is the best possible, then so is constant factor in (15). Oth-erwise, by (16), we would reach a contradiction that the constant factor in (10) is not the
best possible.
Theorem 2 The following statements(i), (ii), (iii),and(iv)are equivalent:
(i) k 1 p
λ(λ–λ2)k 1 q
λ(λ1)is independent ofp,q;
(ii) k 1 p
λ(λ–λ2)k 1 q
λ(λ1)is expressible as a single integral;
(iii) β1/p1α1/qk 1 p
λ(λ–λ2)k 1 q
λ(λ1)is the best possible constant factor of(10); (iv) λ1+λ2=λ.
If the statement (iv)follows,namely λ1+λ2=λ, then we have(11)and the following equivalent inequality with the best possible constant factor β1/p1α1/qkλ(λ1):
∞
n=1 npβλ2–1
∞
m=1 kλ
mα,nβam
p1p < 1
β1/pα1/qkλ(λ1)
∞
m=1
mp(1–αλ1)–1ap
m
1 p
. (17)
Proof (i)⇒(ii). Sincek 1 p
λ(λ–λ2)k 1 q
λ(λ1) is independent ofp,q, we find
k 1 p
λ(λ–λ2)k 1 q
λ(λ1) = lim
p→∞qlim→1+k 1 p
λ(λ–λ2)k 1 q
λ(λ1) =kλ(λ1),
namelyk 1 p
λ(λ–λ2)k
1 q
λ(λ1) is expressible as a single integral
kλ(λ1) = ∞
0
(ii)⇒(iv). In (13), ifk 1 p
λ(λ–λ2)k 1 q
λ(λ1) is expressible as a single integralkλ(λ–pλ2 +λq1), then (13) keeps the form of equality, from which it follows thatλ1+λ2=λ.
(iv)⇒(i). Ifλ1+λ2=λ, thenk 1 p
λ(λ–λ2)k 1 q
λ(λ1) =kλ(λ1), which is independent ofp,q.
Hence, we have (i)⇔(ii)⇔(iv).
(iii)⇒(iv). By Lemma4, we haveλ1+λ2=λ.
(iv)⇒(iii). By Lemma3, forλ1+λ2=λ,
1
β1/pα1/qk
1 p
λ(λ–λ2)k 1 q
λ(λ1)
= 1
β1/pα1/qkλ(λ1)
is the best possible constant factor of (10). Therefore, we find (iii)⇔(iv).
Hence, statements (i), (ii), (iii), and (iv) are equivalent.
Remark3 (i) Forλ=α=β= 1,λ1= q1,λ2= 1p in (11) and (17), we have the following
equivalent inequalities with the best possible constant factork1(1q):
∞
n=1
∞
m=1
k1(m,n)ambn<k1
1
q
∞
m=1 apm
1
p∞
n=1 bqn
1 q
, (18)
∞
n=1 ∞
m=1
k1(m,n)am
p1p <k1
1
q
∞
m=1 apm
1 p
. (19)
(ii) Forλ=α=β= 1,λ1=p1,λ2=1q in (11) and (17), we have the following equivalent
inequalities with the best possible constant factork1(1p):
∞
n=1
∞
m=1
k1(m,n)ambn<k1
1
p
∞
m=1 mp–2apm
1
p∞
n=1 nq–2bqn
1 q
, (20)
∞
n=1 np–2
∞
m=1
k1(m,n)am
p1p <k1
1
p
∞
m=1 mp–2apm
1 p
. (21)
(iii) Forp=q= 2, both (18) and (20) reduce to
∞
n=1
∞
m=1
k1(m,n)ambn<k1
1 2
∞
m=1 a2m
∞
n=1 b2n
1 2
, (22)
and both (19) and (21) reduce to the equivalent form of (22) as follows:
∞
n=1 ∞
m=1
k1(m,n)am
212
<k1
1 2
∞
m=1 a2m
1 2
. (23)
4 Operator expressions and some particular cases
We set functions
φ(m) :=mp[1–α(
λ–λ2
p +
λ1
q)]–1, ψ(n) :=nq[1–β(
λ–λ1 q +
from which
ψ1–p(n) =npβ(
λ–λ1
q +
λ2
p)–1 (m,n∈N).
Define the following real normed spaces:
lp,φ:=
a={am}∞m=1;ap,φ:=
∞
m=1
φ(m)|am|p
1 p
<∞
,
lq,ψ:=
b={bn}∞n=1;bq,ψ:=
∞
n=1
ψ(n)|bn|q
1 q
<∞
,
lp,ψ1–p:=
c={cn}∞n=1;cp,ψ1–p:=
∞
n=1
ψ1–p(n)|bn|p
1 p
<∞
.
Assuming thata∈lp,φ, setting
c={cn}∞n=1, cn:=
∞
m=1 kλ
mα,nβa
m, n∈N,
we can rewrite (15) as follows:
cp,ψ1–p<
1
β1/pα1/qk
1 p
λ(λ–λ2)k 1 q
λ(λ1)ap,φ<∞,
namelyc∈lp,ψ1–p.
Definition 2 Define a Hilbert-type operator T :lp,φ→lp,ψ1–p as follows: For anya∈
lp,φ,there exists a unique representationc∈lp,ψ1–p. Define the formal inner product of Taandb∈lq,ψ, and the norm ofT as follows:
(Ta,b) :=
∞
n=1 ∞
m=1 kλ
mα,nβa
m
bn,
T:= sup
a(=θ)∈lp,φ
Tap,ψ1–p ap,φ
.
By Theorem1and Theorem2, we have the following.
Theorem 3 If a∈lp,φ,b∈lq,ψ,ap,φ,bq,ψ > 0,then we have the following equivalent
inequalities:
(Ta,b) < 1
β1/pα1/qk
1 p
λ(λ–λ2)k 1 q
λ(λ1)ap,φbq,ψ, (24)
Tap,ψ1–p<
1
β1/pα1/qk
1 p
λ(λ–λ2)k 1 q
λ(λ1)ap,φ. (25)
Moreover,λ1+λ2=λif and only if the constant factor
1
β1/pα1/qk
1 p
λ(λ–λ2)k 1 q
λ(λ1) =
1
in(24)and(25)is the best possible,namely
T= 1
β1/pα1/qkλ(λ1). (26)
Example1 We setkλ(x,y) :=(cx+1y)λ (c,λ> 0;x,y> 0). Then we find
kλ
mα,nβ= 1 (cmα+nβ)λ.
For 0 <λ1,λ–λ2≤ α1, 0 <λ2, λ–λ1≤
1
β,kλ(x,y) is a positive homogeneous function of degree –λsuch thatkλ(x,y) is strictly decreasing with respect tox,y> 0, and forγ =
λ1,λ–λ2,
kλ(γ) =
∞
0
uγ–1
(cu+ 1)λdu= 1
cγ
∞
0
vγ–1
(v+ 1)λdv= 1
cγB(γ,λ–γ)∈R+.
In view of Theorem3, it follows thatλ1+λ2=λif and only if
T= 1
β1/pα1/qkλ(λ1) = 1
β1/pα1/q · 1
cλ1B(λ1,λ2).
Example2 We setkλ(x,y) :=(cxln()cxλ–/yy)λ (c,λ> 0;x,y> 0). Then we find
kλ
mα,nβ= ln(cm α/nβ)
cλmλα–nλβ.
For 0 <λ1,λ–λ2≤α1, 0 <λ2,λ–λ1≤
1
β,kλ(x,y) is a positive homogeneous function of degree –λsuch thatkλ(x,y) is strictly decreasing with respect tox,y> 0 (cf. [4], Exam-ple 2.2.1), and forγ =λ1,λ–λ2,
kλ(γ) =
∞
0
uγ–1ln(cu)
(cu)λ– 1 du= 1
cγλ2 ∞
0
v(γ/λ)–1lnv v– 1 dv=
1
cγ
π λsin(π γ/λ)
2 ∈R+.
In view of Theorem3, it follows thatλ1+λ2=λif and only if
T= 1
β1/pα1/qkλ(λ1) = 1
β1/pα1/q · 1
cλ1
π λsin(π λ1/λ)
2
.
Example3 Fors∈N, we setkλ(x,y) := s 1
k=1(xλ/s+ckyλ/s) (0 <c1≤ · · · ≤cs,λ> 0;x,y> 0).
Then we find
kλ
mα,nβ=s 1
k=1(mαλ/s+cknβλ/s) .
For 0 <λ1,λ–λ2≤ α1, 0 <λ2, λ–λ1≤
1
β,kλ(x,y) is a positive homogeneous function of degree –λsuch thatkλ(x,y) is strictly decreasing with respect tox,y> 0, and forγ =
λ1,λ–λ2, by Example 1 of [30], we have
kλ(s)(γ) =
∞
0
tγ–1 s
k=1(tλ/s+ck)
dt= πs
λsin(πλsγ) s
k=1 c
sγ λ–1 k
s
j=1(j=k)
1
In view of Theorem3, it follows thatλ1+λ2=λif and only if
T= 1
β1/pα1/qk
(s)
λ (λ1) =
1
β1/pα1/q·
πs
λsin(πsλ1
λ )
s
k=1 c
sλ1
λ –1 k
s
j=1(j=k)
1
cj–ck .
In particular, forc1=· · ·=cs=c, we havekλ(x,y) =(xλ/s+1cyλ/s)s and
˜
kλ(s)(λ1) := ∞
0
tλ1–1
(tλ/s+c)sdt
= s
λc(1–λλ1)s
∞
0
vsλλ1–1 (v+ 1)sdv=
s
λc(1–λλ1)s
B
sλ1 λ ,
sλ2 λ .
Ifs= 1, then we havekλ(x,y) =xλ+1cyλ and
T= 1
β1/pα1/qk˜
(1)
λ (λ1) =
1
β1/pα1/q · 1
λc1–λλ1
π
sin(π λ1
λ ) .
5 Conclusions
In this paper, by means of the weight coefficients and the idea of introducing parameters, a discrete Hilbert-type inequality with the general homogeneous kernel and the interme-diate variables is obtained which is an extension of (1). The equivalent forms are given in Lemma2and Theorem1. The equivalent statements of the best possible constant fac-tor related to some parameters are considered in Theorem2. The operator expressions, some particular cases, and examples are given in Theorem3, Remark1, Remark3, and Examples1–3. The lemmas and theorems provide an extensive account of this type of inequalities.
Funding
This work is supported by the National Natural Science Foundation (No. 61772140) and Guangxi Natural Science Foundation (No. 2016GXNSFAA380125).
Competing interests
The authors declare that they have no competing interests.
Authors’ contributions
BY carried out the mathematical studies, participated in the sequence alignment, and drafted the manuscript. RL participated in the design of the study and performed the numerical analysis. All authors read and approved the final manuscript.
Author details
1School of Mathematics and Statistics, Hechi University, Yizhou, P.R. China.2Department of Mathematics, Guangdong
University of Education, Guangzhou, China.
Publisher’s Note
Springer Nature remains neutral with regard to jurisdictional claims in published maps and institutional affiliations.
Received: 17 February 2019 Accepted: 10 May 2019
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