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https://doi.org/10.26637/MJM0504/0005

Random variable inequalities involving

(k,s)-integration

M. Houas

1

* and Z. Dahmani

2

Abstract

In this paper, we use the(k,s)−Riemann-Liouville operator to establish new results on integral inequalities by

using fractional moments of continuous random variables. Keywords

(k,s)−Riemann-Liouville integral, random variable, (k,s)−fractional expectation, (k,s)−fractional variance, (k,s)−fractional moment.

AMS Subject Classification

26D15, 26A33, 60E15.

1Laboratory FIMA, UDBKM, University of Khemis Miliana, Algeria. 2Laboratory LPAM, UMAB, University of Mostaganem, Algeria.

*Corresponding author[email protected];ı2[email protected]

Article History: Received6June2017; Accepted7August2017 c2017 MJM.

Contents

1 Introduction. . . 641

2 Preliminaries. . . 641

3 Inequalities for(k,s)−operator. . . 643

References. . . 645

1. Introduction

The study of integral inequalities is an important research subject in mathematical analysis. These inequalities have many applications in differential equations, probability theory and statistical problems, but one of the most useful appli-cations is to establish uniqueness of solutions in fractional boundary value problems. For detailed applications on the subject, one may refer to [9–12], and the references cited therein. Moreover, the integral inequalities involving frac-tional integration are also of great importance. For some earlier work on the topic, we refer to [2–5,7,8,14,16,17]. In [9], P. Kumar presented new results involving higher moments for continuous random variables. Also the author established some estimations for the central moments. Other results based on Gruss inequality and some applications of the truncated exponential distribution have been also discussed by the au-thor. In [10], Ostrowski type integral inequalities involving moments of a continuous random variable defined on a finite interval, is established. In [3], the author established several inequalities for the fractional dispersion and the fractional

variance functions of continuous random variables. Recently, A. Akkurt et al. [1] proposed new generalizations of the re-sults in [3]. Very recently, Z. Dahmani [4,6] presented new fractional integral results for the fractional moments of contin-uous random variables by correcting some results in [3]. In a very recent work, M. Tomar et al. [17] proposed new integral inequalities for the(k,s)−fractional expectation and variance functions of a continuous random variable.

Motivated by the results presented in [3,4,6,14,17], in this paper, we present some random variable integral inequalities for the(k,s)−fractional operator.

2. Preliminaries

We recall the notations and definitions of the(k,s)−fractional integration theory [13,14,17].

Definition 2.1. The Riemann–Liouville fractional integral of orderα≥0, for a continuous function f on[a,b]is defined by

a[f(t)] =Γ(1α)

Rt

a(t−τ) α−1

f(τ)dτ;α≥0,a<t≤b ,

(2.1)

whereΓ(α) =R∞

0 e

−uuα−1du.

(2)

by

kJaα[f(t)] =kΓk1(α) Rt

a(t−τ)

α

k−1f(τ)dτ; α>0, a<tb ,

(2.2)

whereΓk(α) =

R∞

0 e −uk

kuα−1du.

Definition 2.3. The(k,s)−Riemann-Liouville fractional in-tegral of orderα>0, for a continuous function f on[a,b]is defined as

k

sJaα[f(t)] =

(s+1)1−αk kΓk(α)

Rt

a ts+1−τs+1 αk−1

τsf(τ)dτ;α>0,a<t≤b ,

(2.3)

where k>0,s∈R\ {−1}.

Theorem 2.4. Let f be continuous on[a,b],k>0,and s∈ R\ {−1}.Then,

k sJaα

h k sJ

β a[f(t)]

i

= ksJaα+β[f(t)] = ksJ β a

k

sJaα[f(t)]

,k>0,s∈R\ {−1} ,

(2.4)

for allα>0,β>0,a<t≤b.

Theorem 2.5. Let α >0,β >0,k>0 and s∈R\ {−1}. Then, we have

k sJaα

ts+1−as+1βk−1

= Γk(β) (s+1)αkΓk(α+β) t

s+1as+1β+αk −1

,

(2.5)

Remark 2.6. (i):Taking s=0,k>0in(5),we obtain

kJaα

(t−a)βk−1

= Γk(β)

Γk(α+β)(t−a)

β+α

k −1,α,β>0,a>0,k>0 .

(2.6)

(ii):The formula(5),for s=0and k=1becomes Jα

a h

(t−a)β−1i= Γ(β)

Γ(α+β)(t−a) β+α−1

. (2.7)

Corollary 2.7. Let k>0and s∈R\ {−1}.Then, for any α>0,we have

k

sJaα[1] = 1

(s+1)αkΓk(α+k) t

s+1as+1αk−2

. (2.8)

Remark 2.8. (i):For s=0,k>0in(8),we get

kJaα[1] =Γk(α1+k)(t−a)

α

k−2 . (2.9) (ii):For s=0,k=1in(8),we have

a [1] =Γ(α1+1)(t−a)

β−2 . (2.10) For more details on(k,s)−fractional integral, we refer the reader to [14,17].

We recall also the following definitions [3,4,17]

Definition 2.9. The(k,s)−fractional expectation function of orderα>0, for a random variable X with a positive p.d.f.

f defined on[a,b]is defined as

k

sEX,α(t):=

(s+1)1−αk kΓk(α)

t

Z

a

ts+1−τs+1

α

k−1

τs+1f(τ)dτ,

(2.11)

α>0,k>0,s∈R\ {−1}and a<t≤b.

Definition 2.10. The(k,s)−fractional expectation function of orderα >0for the random variable X−E(X) with a positive probability density function f defined on [a,b] is defined as

k

sEX−E(X),α(t):=

(s+1)1−αk kΓk(α)

t

Z

a

ts+1−τs+1αk−1

τs(τ−E(X))f(τ)dτ,

(2.12)

α>0,k>0,s∈R\ {−1}and a<t≤b.

Definition 2.11. The(k,s)−fractional variance function of orderα>0for a random variable X having a positive p.d.f.

f on[a,b]is defined as

k

sσX2,α(t):=

(s+1)1−αk kΓk(α)

t

Z

a

ts+1−τs+1

α

k−1τsE(X))2f(τ),

(2.13)

α>0,k>0,s∈R\ {−1}and a<t≤b.

We introduce also the following definition.

Definition 2.12. The(k,s)−fractional moment function of orders r>0,α >0 for a continuous random variable X having a p.d.f. f defined on[a,b]is defined as

k

sMr,α(t):=

(s+1)1−αk kΓk(α)

t

Z

a

ts+1−τs+1

α

k−1

τs+rf(τ)dτ,

(2.14)

α>0,k>0,s∈R\ {−1}and a<t≤b.

Remark 2.13. If we take s=0,α=k=1in Definition 12, we obtain the classical moment of order r>0given by Mr:= b

R

a

τrf(τ)dτ.

We define the quantities that will be used later:

H(τ,ρ):= (g(τ)−g(ρ)) (h(τ)−h(ρ)), τ,ρ∈(a,t),a<t≤b,

(3)

and

ϕkα,s(t,τ):=(s+1) 1−α

k

Γk(α)

ts+1−τs+1

α

k−1

τsp(τ),k>0,s∈R/{−1} τ∈(a,t),

(2.16) wherep:[a,b]→R+is a continuous function.

3. Inequalities for

(k

,

s)

operator

We prove:

Theorem 3.1. Let X be a continuous random variable having a p.d.f. f:[a,b]→R+.

(i):If f ∈L∞[a,b], then for all a<t≤b andα>0,k>

0,s∈R\ {−1}, k

sJaα[f(t)] ksEXr−1(X−E(X))(t)− ksEX−E(X)(t)ksMr−1,α(t)

≤ kfk2hk

sJaα[1] ksJaα[tr]−ksJaα[t)]ksJaα

tr−1i, (3.1)

(ii):for all a<t≤b,the inequality k

sJaα[f(t)] ksEXr−1(X−E(X))(t)− ksEX−E(X)(t)ksMr−1,α(t)

≤ 1

2(t−a) t

r−1−ar−1k

sJaα[f(t)] 2

, (3.2)

is also valid forα>0,k>0,s∈R/{−1}.

Proof. Using (2.15) and (2.16), we can write

t

Z

a

ϕkα,s(t,τ)H(τ,ρ)dτ= t

Z

a

ϕkα,s(t,τ) (g(τ)−g(ρ)) (h(τ)−h(ρ))dτ.

(3.3) Then Z t a Z t a

ϕkα,s(t,τ)ϕkα,s(t,ρ)H(τ,ρ)dτdρ (3.4) =

Z t

a

Z t

a

ϕkα,s(t,τ)ϕkα,s(t,τ) (g(τ)−g(ρ)) (h(τ)−h(ρ))dτdρ.

Hence

(s+1)2(1−αk) k2Γ2

k(α) t Z a t Z a

ts+1−τs+1

α

k−1 ts+1ρs+1αk−1 τsρs

(3.5)

×p(τ)p(ρ) (g(τ)−g(ρ)) (h(τ)−h(ρ))dτdρ = 2ks

a[p(t)] ksJ α

a[pgh(t)]−2ksJ α

a[pg(t)]ksJ α

a [ph(t)].

In (3.5), we choosep(t) =f(t),g(t) =t−E(X)andh(t) = tr−1,t∈(a,b), we obtain

(s+1)2(1−αk) k2Γ2

k(α) t Z a t Z a

ts+1−τs+1

α

k−1 ts+1 ρs+1

α

k−1

τsρs (3.6)

×(τ−ρ) τr−1−ρr−1f(τ)f(ρ)dτdρ

= 2ks

a[f(t)]ksJaα

tr−1(t−E(X))f(t) −2ks

a[(t−E(X))f(t)]ksJaα

tr−1f(t)

= 2ks

a[f(t)]ksEXr−1(X−E(X))(t)−2

k

sEX−E(X),α(t)

k

sMr−1,α(t).

Using the factf ∈L∞([a,b]), we can write

(s+1)2(1−αk) k2Γ2

k(α) t Z a t Z a

ts+1−τs+1αk−1

ts+1−ρs+1αk−1

τsρs (3.7)

×(τ−ρ) τr−1−ρr−1f(τ)f(ρ)dτdρ

≤ kfk2(s+1) 2(α

k−1)

k2Γ2) t Z a t Z a

ts+1−τs+1αk−1 ts+1−ρs+1αk−1 τsρs

×(τ−ρ) τr−1−ρr−1dτdρ

= kfk2h2ks

a [1] ksJaα[tr]−2ksJaα[t] ksJaα

tr−1i

.

By (3.6) and (3.7), we have

k

sJaα[f(t)]skEXr−1(X−E(X))(t)−

k

sEX−E(X),α(t)

k

sMr−1,α(t)

≤ kfk2hk

sJaα[1] ksJaα[tr]−ksJaα[t] ksJaα

tr−1 i

. (3.8)

Since sup

τ,ρ∈[a,t]

|τ−ρ|

τr−1−ρr−1

= (t−a) tr−1−ar−1

, then we observe that

(s+1)2(1−αk) k2Γ2)

t Z a t Z a

ts+1−τs+1αk−1 ts+1−ρs+1αk−1 τsρs

×(τ−ρ) τr−1−ρr−1f(τ)f(ρ)dτdρ (3.9)

≤ sup

τ,ρ∈[a,t]

|τ−ρ|

τr−1−ρr−1

(s+1) 2(α

k−1)

k2Γ2) t Z a t Z a

ts+1−τs+1αk−1

× ts+1−ρs+1

α

k−1τsρsf(τ)f(ρ)dτdρ

= (t−a) tr−1−ar−1 (ks

a[f(t)])2.

Thanks to (3.6) and (3.9), we obtain

k

sJaα[f(t)]skEXr−1(X−E(X))(t)−

k

sEX−E(X),α(t)

k

sMr−1,α(t)

≤ (t−a) tr−1−ar−1 (ks

a[f(t)])2. (3.10)

We prove also the following result:

Theorem 3.2. Let X be a continuous random variable having a p.d.f. f :[a,b]→R+. Then we have:

(i∗)For any k>0,s∈R/{−1}andα>0,β>0, k

sJaα[f(t)]ksEXr−1(X−E(X))(t) + skJaβ[f(t)]skEXr−1(X−E(X))(t)

−k

sEX,α(t)ksMr−1,β(t)−skEX,β(t) ksMr−1,α(t) (3.11) ≤ kfk2hk

sJaα[1]ksJaβ[tr] +ksJaβ[1]ksJaα[tr] −ks

a [t]ksJaβ

tr−1−ksJβ a[t] skJ

α a

tr−1i,a<t≤b,

(4)

(ii∗)The inequality

k

sJaα[f(t)]ksEXr−1(X−E(X))(t) + ksJaβ[f(t)]ksEXr−1(X−E(X))(t)

−k

sEX,α(t)ksMr−1,β(t)− ksEX,β(t)ksMr−1,α(t) (3.12) ≤ (t−a) tr−1−ar−1k

sJaα[f(t)]ksJaβ[f(t)],a<t≤b

is also valid for any k>0,s∈R/{−1}andα>0,β >0. Proof. Multiplying both sides of (3.4) byϕkβ,s(t,ρ),where

ϕkβ,s(t,ρ):=(s+1) 1−α

k

Γk(α)

ts+1−ρs+1

α

k−1

τsp(τ),ρ∈(a,t), a<t≤b,

(3.13) we can obtain

Z t

a

Z t

a

ϕkα,s(t,τ)ϕkβ,s(t,ρ)H(τ,ρ)dτdρ (3.14) =

Z t

a

Z t

a

ϕkα,s(t,τ)ϕkβ,s(t,ρ) (g(τ)−g(ρ)) (h(τ)−h(ρ))dτdρ.

Hence,

(s+1)2

1−α+βk

k2Γ

k(α)Γk(β) t Z a t Z a

ts+1−τs+1αk−1

ts+1−ρs+1βk−1

(3.15)

×τsρsp(τ)p(ρ) (g(τ)−g(ρ)) (h(τ)−h(ρ))dτdρ

= ks

a [p(t)]ksJaβ[pgh(t)] +ksJaβ[p(t)] ksJaα[pgh(t)] −k

sJaα[ph(t)]ksJaβ[pg(t)]−ksJaβ[ph(t)]ksJaα[pg(t)].

In (3.15), we takep(t) = f(t),g(t) =t−E(X),h(t) =tr−1. So, we get

(s+1)2

1−α+β k

k2Γ

k(α)Γk(β) t Z a t Z a

ts+1−τs+1αk−1 ts+1−ρs+1βk−1 τsρs

×(τ−ρ) τr−1−ρr−1)f(τ)f(ρ)dτdρ (3.16)

= ks

a [f(t)]ksJaβ

tr−1(t−E(X))f(t) +ks

a[f(t)] ksJaα

tr−1(t−E(X))f(t)

−ks

a[(t−E(X))f(t)] ksJaβ

tr−1f(t)− ks

a[(t−E(X))f(t)]ksJaα

tr−1f(t)

= ks

a [f(t)]ksEXr−1(X−E(X))(t) + ksJaβ[f(t)]ksEXr−1(X−E(X))(t)

−k

sEX,α(t)ksMr−1,β(t)− ksEX,β(t)ksMr−1,α(t).

We have also

(s+1)2

1−α+β k

k2Γ

k(α)Γk(β) t Z a t Z a

ts+1−τs+1αk−1 ts+1−ρs+1βk−1 τsρs

×(τ−ρ) τr−1−ρr−1f(τ)f(ρ)dτdρ (3.17)

≤ kfk2(s+1) 21−α+β

k

k2Γ

k(α)Γk(β) t Z a t Z a

ts+1−τs+1αk−1 ts+1 ρs+1

β

k−1 τsρs

×(τ−ρ) τr−1−ρr−1dτdρ

= kfk2hk sJ

α a[1]ksJ

β

a[tr] + ksJ β a[1]ksJ

α a [tr]

− k

sJaα[t]ksJaβ

tr−1−k

sJaβ[t] ksJaα

tr−1i.

By (3.16) and (3.17), we obtain (3.11). To prove (3.12), we remark that

(s+1)2

1−α+βk

k2Γ

k(α)Γk(β) t Z a t Z a

ts+1−τs+1

α

k−1 ts+1ρs+1βk−1 τsρs

×(τ−ρ) τr−1−ρr−1f(τ)f(ρ)dτdρ (3.18)

≤ sup

τ,ρ∈[a,t]

|(τ−ρ|

τr−1−ρr−1 (s+1)2

1−α+βk

k2Γ

k(α)Γk(β) t Z a t Z a

ts+1−τs+1αk−1

ts+1−ρs+1βk−1

×τsρsf(τ)f(ρ)dτdρ

= (t−a) tr−1−ar−1k

sJaα[f(t)] ksJaβ[f(t)].

Therefore, by (3.16) and (3.18), we get (3.12).

Remark 3.3. If we takeα =β in Theorem 15, we obtain Theorem 14.

We give also the following(k,s)−fractional integral in-equality:

Theorem 3.4. Let X be a continuous random variable hav-ing a p.d.f. f :[a,b]→R+. Assume that there exist con-stantsϕ,φ such thatϕ≤ f(t)≤φ.Then, for all k>0,s∈ R/{−1},α>0,we have

k

sJaα[f(t)] ksM2r,α(t)−ksMr2,α(t)≤

1 4(b

rar)2k

sJaα[f(t)] 2

, a<t≤b.

(3.19)

Proof. Using Theorem 2.4 of [17], we can write

k

sJaα[p(t)] ksJaα[phg(t)]−ksJaα[ph(t)] ksJaα[pg(t)] ≤ 1 4 k

sJaα[p(t)] 2

(φ−ϕ)2.

(3.20) In (3.20), we replacehbyg,we will have

k

sJaα[p(t)]ksJaα

pg2(t)−(ks

a[pg(t)])2 ≤ 1 4 k

sJaα[p(t)] 2

(φ−ϕ)2.

(3.21) Takingp(t) = f(t),g(t) =tr,a<t≤bin (3.21), we obtain

k

sJaα[f(t)]ksJaα

t2rf(t) −(k

sJaα[trf(t)])2 ≤ 1 4 k

sJaα[f(t)] 2

(φ−ϕ)2.

(3.22) In (3.22), we takeφ=brandϕ=ar, then we have

0≤ks

a[f(t)]ksJaα

t2rf(t)−(ks

a[trf(t)])2≤

1 4(b

rar)2k

sJaα[f(t)] 2

.

(3.23) This implies that

k

sJaα[f(t)]ksM2r,α(t)−ksMr2,α(t)≤

1 4(b

r−ar)2k

sJaα[f(t)] 2

.

(5)

Finally, we present the following result:

Theorem 3.5. Let X be a continuous random variable hav-ing a p.d.f. f :[a,b]→R+. Assume that there exist con-stantsϕ,φ such thatϕ≤ f(t)≤φ.Then, for all k>0,s∈ R/{−1},α>0,β>0,we have

k

sJaα[f(t)] ksM2r,β(t) + ksJaβ[f(t)]ksM2r,α(t) (3.25) +2arbr ks

a[f(t)]ksJaβ[f(t)] ≤ (ar+br)ks

a[f(t)]ksMr,β(t) + (ar+br)ksJaβ[f(t)] ksMr,α(t),a<t≤b.

Proof. We takep(t) =f(t),g(t) =tr,a<t≤band by The-orem 2.5 of [17], we can write

h k

sJaα[f(t)] ksJaβ

t2rf(t)+ks

a[f(t)]ksJaα

t2rf(t) (3.26)

−2ks

a [trf(t)]ksJaβ[trf(t)] i2

≤ hφks

a[f(t)]−ksJaα[trf(t)] ksJaβ[trf(t)]−ϕksJaβ[f(t)]

+ks

a [trf(t)]−ϕskJaα[f(t)] φskJaβ[f(t)]−ksJaβ[trf(t)] i2

.

Combining (3.21) and (3.26) and taking into account the fact that the left-hand side of (3.21) is positive, we can write

k

sJaα[f(t)] ksJaβ

t2rf(t) +ks

a[f(t)]skJaα

t2rf(t)

−2sk

a [trf(t))]ksJ β

a[trf(t)] (3.27) ≤ φ ksJaα[f(t)]− ksJaα[trf(t)] ksJaβ[trf(t)]−ϕksJaβ[f(t)]

+ks

a[trf(t)]−ϕksJaα[f(t)] φskJaβ[f(t)]−ksJaβ[trf(t)]

.

Therefore

k

sJaα[f(t)] ksM2r,β(t) + ksJaβ[f(t)]ksM2r,α(t)−2ksMr,β(t)ksMr,α(t) ≤ φ ks

a[f(t)]− ksMr,α(t) ksMr,β(t)−ϕksJaβ[f(t)]

(3.28)

+ksMr,α(t)−ϕksJaα[f(t)] φ ksJaβ[f(t)]−ksMr,β(t)

.

This implies that

k

sJaα[f(t)] ksM2r,β(t) + ksJaβ[f(t)]ksM2r,α(t) +2ϕ φskJaα[f(t)]ksJaβ[f(t)] ≤ (φ+ϕ)ks

a[f(t)]ksMr,β(t) + ksJaβ[f(t)] ksMr,α(t)

. (3.29)

In (3.29), we takeφ=br,ϕ=ar, then we have

k

sJaα[f(t)]ksM2r,β(t) + ksJaβ[f(t)] ksM2r,α(t) +2arbr skJaα[f(t)] ksJaβ[f(t)] ≤ (ar+br)ks

a[f(t)]ksMr,β(t) + skJaβ[f(t)] ksMr,α(t)

. (3.30)

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ISSN(P):2319−3786 Malaya Journal of Matematik

ISSN(O):2321−5666

References

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