NEWDYNAMICINEQUALITIES FORDECREASING FUNCTIONS AND THEOREMS OF HIGHER INTEGRABILITY∗
2018-07-06SakerReganOsmanAgarwal
S.H.Saker,D.O’Regan,M.M.Osman,R.P.Agarwal
(1.Dept.of Math.,Faculty of Science,Mansoura University,Mansoura-Egypt;2.School of Math.,Statistics and Applied Math.,National University of Ireland,Galway,Ireland;3.Dept.of Math.,Texas A&M University-Kingsvilie,Texas,78363,USA)
1 Introduction
The classical integral Hölder inequality states that if f and g are positive measurable functions defined on
For generalizations and extensions in the literature we refer the reader to the papers[6–9,12–15].In this paper we establish some new dynamic inequalities on time scales.For related dynamic inequalities on time scales,we refer the reader to the books[1,2]and the papers[16,17].
The paper is organized as follows.In Section 2 we give a brief overview on time scales.In Section 3,we prove some new dynamic inequalities via convexity functions which contain inequalities given by Hardy,Littlewood and Pólya.We also establish some new dynamic inequalities on time scales for decreasing functions.These inequalities contain in particular generalizations of integral inequalities due to Hardy,D’Apuzzo and Sbordone and Popoli.We apply also these inequalities to prove a higher integrability theorem for monotone decreasing function on time scales.
2 Preliminaries on Time Scales
For a good introduction on time scales we refer the reader to the book[4].The forward jump operator and the backward jump operator are defined byσ(t):=inf{s∈T:s>t},andρ(t):=sup{s∈T:s
One chain rule is
which is a simple consequence of Keller’s chain rule[4,Theorem 1.90].Another chain rule is as follows:Let f:R→R be continuously differentiable and suppose g:T→R is delta differentiable,then f◦g:T→R is delta differentiable and
In this paper we will consider the(delta)integral which we can be defined as follows.If F∆(t)=f(t),then the Cauchy(delta)integral of f is defined byf(s)∆s:=F(t)−F(t0).It can be shown(see[4])that if f∈Crd(T),then the Cauchy integralAn infinite integral is defined asIntegration on discrete time scales is defined by
The integration by parts formula on time scales is given by
Hölder’s inequality[4,Theorem 6.13]states that two rd-continuous functions f,g:T→R satisfy
where p>1,1/p+1/q=1 and a,b∈T.
Throughout this paper,we will assume that the functions in the statements of the theorems are positive and the integrals considered are assumed to exist and are finite.
Next we present a weighted Hardy type inequality[16]on time scales which is useful in the proof of our main results.Without loss of generality,we assume that sup T=∞,and define the time scale interval[a,b]Tby[a,b]T:=[a,b]∩T.
Theorem 2.1LetTbe a time scale witha,b∈T(a
3 Main Results
In our next two results we will assume thatϕis a differentiable convex function.
Theorem 3.1LetTbe a time scale with0,a∈T(a>0).Iffis decreasing then
ProofLet x∈(0,a)T.Since f is a decreasing function,
Let F(x)=so F is increasing.Note thatis a convex function,then
From the chain rule(2.3)note
Since F is increasing,
Now from(3.2)and(3.3)we obtain
so integration from 0 to a yields
From this inequality we have(3.1).The proof is complete.
A special case of Theorem 3.1 is given as follows whenϕ(u)=up,p>1.
Corollary 3.1LetTbe a time scale with0,a∈T(a>0).Iffis decreasing then
Remark 3.1Applying Hölder’s inequality on the right hand side of(3.6)we get the inequality
Remark 3.2We consider the interval[a,b]Tand immediately we have
Note if f is decreasing then xγ−1f(with γ ≤ 1)is decreasing.Use xγ−1f in(3.6)to obtain the following result.
Corollary 3.2LetTbe a time scale with0,a∈T(a>0),p>1andγ≤1.Iffis decreasing then
Remark 3.3Consider the interval[a,b]Tand assume that there exist positive numbers r and s with r In our next results we will assume that there exists an m>0 such that We apply now the weighted Hardy inequality(2.6)to prove a dynamic inequality. Theorem 3.2SupposeTis a time scale anda,b∈T(b>a),and assume(3.11)holds.Let Ifα≤1andβ>1,then where In particular ProofApplying inequality(2.6)with p=q= β,u(x)=(x − a)α−β−1and υ(x)=(x − a)α−1,we obtain here A=Cpand so Let t∈(a,σ(b))T.From the chain rule(2.2)we see that(noteα≤1 andβ>1) and as a result Let t∈(a,b)T.Apply the chain rule(2.2)and(3.11),then we have(noteα<β) and as a result From(3.15),(3.16)and(3.17)we have Putting(3.18)into(3.14),we obtain(3.13).The proof is complete. Letα=q/p andβ=q with p≥q>1 in(3.13)and we obtain the following Hardy-type inequality. Corollary 3.3SupposeTis a time scale anda,b∈T(b>a),p≥q>1,and assume(3.11)holds.Then wheremandGare defined in(3.11)and(3.12)respectively. Remark 3.4As a special case of Theorem 3.2 when T=R(note m=1),we have the inequality in[15,Theorem 2.1](note in our caseα≤1 andβ>1) where In particular when a=0 andα=1 we have Remark 3.5As a special case of Theorem 3.2 when T=N,a,b∈N,noting σ(x)=x+1 andwe have the discrete inequality Now we prove some lemmas that will be needed below. Lemma 3.1Suppose0<λ≤1and assume(3.11)holds.Let ProofFrom the definition of H and(3.11)we have Let u(x)=.Integrating the right hand side of(3.22),using formula(2.4)with u∆(x)=(x − a)λ−1and υσ(x)=h(t)∆t,we obtain(note Let t∈(a,b)T.Apply the chain rule(2.2)and we see that(note 0<λ≤1) and as a result The proof is complete. Lemma 3.2Letλ<0and suppose(3.11)holds.In addition assume Then whereHis defined in Lemma3.1. ProofProceed as in Lemma 3.1 and we obtain(note(3.23)) Let t∈(a,b)T.Apply the chain rule(2.2),and we see that(noteλ<0) and as a result The proof is complete. Lemma 3.3Letλ>1and assume(3.11)holds.Then whereHis defined in Lemma3.1. ProofFrom the definition of H(x)and(3.11)we have Let u(x)=Integrating the right hand side of(3.26),using formula(2.4)with u∆(x)=(σ(x)−a)λ−1and υσ(x)=∆t,we obtain(note Let t∈(a,b)T.Apply the chain rule(2.2),and we see that(noteλ>1) and as a result The proof is complete. In our next result we assume the nonnegative function f satisfies the reverse Hölder inequality,that is for x ∈ (a,b)Tthere exist some constants p,q with p Theorem 3.3LetTbe a time scale witha,b∈T(b>a),α<1and assume(3.11)holds.Suppose there exist constantsp,qwithp and hold.Then ProofLet where we let r=p and r=q.From(3.27)we have Apply Lemma 3.2 on the left-hand side of(3.29)withλ=α−1<0,h=fq(x),then we have Apply Theorem 3.2 on the right-hand side of(3.29)withβ=q/p(note p Substituting this into(3.29),we obtain Thus The proof is complete. Remark 3.6Consider the special case whenα=(and assume r>q)and p=1.Then we have see[7,Lemma 3.2]when T=R. Now we prove a higher integrability theorem for a monotone decreasing function on time scales. Theorem 3.4SupposeTis a time scale anda,b∈T(b>a),and assume(3.11)holds.Letfbe a decreasing function and suppose there exist constantsp,qwithp and holds.Then ProofFrom Theorem 3.3(withα=)we obtain Apply inequality(3.10)with r=q(note r=q Thus The proof is complete. Remark 3.7Since f is decreasing,we have f(σ(x))≤ f(x),so inequality(3.31)becomes [1]R.P.Agarwal,D.O’Regan and S.H.Saker,Dynamic Inequalities on Time Scales,Springer Cham Heidlelberg New York Drodrechet London,2014. [2]R.P.Agarwal,D.O’Regan and S.H.Saker,Hardy Type Inequalities on Time Scales,Springer International Publishing,Cham Heidlelberg New York Drodrechet London,2016. [3]R.Bibi,M.Bohner,J.Pecaric and S.Varošanec,Minkowski and Beckenbach-Dresher inequalities and functionals on time scales,Journal of Mathematical Inequalities,7:3(2013),299-312. 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