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Strongly convex functions and extensions of related inequalities with applications to entropy

  • We extended the Mercer inequlaity, Fejér-Hermite-Hadamard, and Jensen inequalities for strongly convex functions. Moreover, we obtained several results in information theory and mathematical analysis using obtained inequalities.

    Citation: Yamin Sayyari, Mana Donganont, Mehdi Dehghanian, Morteza Afshar Jahanshahi. Strongly convex functions and extensions of related inequalities with applications to entropy[J]. AIMS Mathematics, 2024, 9(5): 10997-11006. doi: 10.3934/math.2024538

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  • We extended the Mercer inequlaity, Fejér-Hermite-Hadamard, and Jensen inequalities for strongly convex functions. Moreover, we obtained several results in information theory and mathematical analysis using obtained inequalities.



    For a,bR,a<b, and I:=[a,b], the function φ:IR is convex if

    φ(tx1+(1t)x2)tφ(x1)+(1t)φ(x2)

    and φ is named strongly convex (S-C) with modulus k if

    φ(tx1+(1t)x2)tφ(x1)+(1t)φ(x2)kt(1t)(x1x2)2,

    for all x1,x2I and all t[0,1]

    Mercer inequality [8], Hermite-Hadamard inequality (H-H inequality) [6], and Jensen's inequality [7] are some types of important inequalities in different fields of mathematical analysis and optimization.

    In [4], Fejér investigated an extension of the H-H inequality. Azócar et al. [1] obtained the following Fejér inequality for the S-C function.

    Because of the comprehensive results of the Jensen's, Mercer, and H-H inequalities, some researchers exteneded their studies via mappings of various types (see [2,3,10,17,18]).

    The theory of convex function is significant in entropy estimation and optimization [11,12,13,14,15,16].

    An equivalent condition for the convexity of a continuous function is given in [21]. Also, in [22], S. Zlobec generalized some of the basic integral properties of convex functions.

    Throughout this article, suppose that x={xi}[a,b] and t={ti},0ti with ni=1ti=1.

    Theorem 1.1. [9] Suppose that φ:IR is an S-C function with modulus k, then

    φ(ni=1tixi)ni=1tiφ(xi)kV(x),

    for all x1,x2,,xn[a,b],ti0(i=1,,n) with ni=1ti=1,ˉx=ni=1tixi, and V(x):=ni=1ti(xiˉx)2.

    Definition 1.1. The Shannon entropy of a probability distribution t is defined by

    H(t):=ni=1tilog(ti).

    Proposition 1.1. [19] Let η:=min{ti:i=1,,n} and ϑ:=max{ti:i=1,,n}, then

    m(η,ϑ):=ηlog(2ηη+ϑ)+ϑlog(2ϑη+ϑ)lognH(t)log((η+ϑ)24ηϑ):=M(η,ϑ).

    Our main goal is to obtain some intersting Jensen, Mercer, and Fejér-Hermite-Hadamard inequalities for S-C functions. Furthermore, we use those inequalities in mathematical analysis and the Shannon entropy to obtain a strong bound for entropy of a probability distribution.

    In this section, we generelize the Mercer, Jensen type, and Fejér-Hermite-Hadamard inequalities for S-C functions.

    Lemma 2.1. Suppose that φ:IR is an S-C function with modulus k. If w1,w2,w3I, and w1<w2<w3, then

    (i) φ(w2)φ(w1)2φ(w2+w32)φ(w1+w32)k4(w2w1)(2w3w2w1),

    (ii) φ(w3)φ(w2)2φ(w1+w32)φ(w1+w22)+k4(w3+w22w1)(w3w2).

    Proof. Since w1<w2<w2+w32<w3, there are s,t[0,1], s+t=1 such that w2=s(w2+w32)+tw1. Therefore,

    φ(w1)φ(w2)2+φ(w2+w32)=12[φ(w1)φ(tw1+s(w2+w32))]+φ(w2+w32)12[φ(w1)(tφ(w1)+sφ(w2+w32)kts(w2+w32w1)2)]+φ(w2+w32)=s2φ(w1)+2s2φ(w2+w32)+k2ts(w2+w32w1)2φ(s2w1+2s2(w2+w32))+(ks(2s)4+k2ts)(w2+w32w1)2=φ(s2w1+(w2+w32)12(w2tw1))+k4(4s3s2)(w2+w32w12)2=φ(w1+w32)+k4(4(w2w1)(2w3w2w1)(w2+w32w1)2)(w2+w32w12)2=φ(w1+w32)+k4(w2w1)(2w3w2w1).

    Similarly, we obtain (ⅱ) by putting w2=t(w1+w22)+sw3, where w1<w1+w22<w2<w3.

    Theorem 2.1. Assume that φ:[a,b]R is an S-C function with modulus k and

    Δk(p,q)=φ(p)+φ(q)2φ(p+q2)k2(pq)2,

    where ap,qb, then

    maxp,qΔk(p,q)=Δk(a,b). (2.1)

    Proof. Taking w1=a,w2=p, and w3=b in the part (ⅰ) of Lemma 2.1 and w1=p,w2=q, and w3=b in the part (ⅱ) of Lemma 2.1, we gain

    φ(p)φ(a)2φ(p+b2)φ(a+b2)k4(pa)(2bpa), (2.2)
    φ(b)φ(q)2φ(p+b2)φ(p+q2)+k4(bq)(b+q2p), (2.3)

    respectively.

    By (2.3), we get

    φ(q)φ(b)2φ(p+q2)φ(p+b2)k4(bq)(b+q2p). (2.4)

    Now, from (2.2) and (2.4), we conclude (2.1).

    Corollary 2.1. Assume that φ:[a,b]R is an S-C function with modulus k and x[a,b], then

    φ(a+bx)k2(a+b2x)2φ(a)+φ(b)φ(x)k2(ba)2. (2.5)

    Proof. Replacing p by x and q by a+bx in Theorem 2.1 gives the desired result.

    Lemma 2.2. Let λ,μ0 and λ+μ=1 and let φ:[a,b]R be an S-C function with modulus k, then

    φ(λ(a+b)+(μλ)ni=1tixi)λφ(a)+λφ(b)+(μλ)ni=1tiφ(xi)k[ni=1ti(xiˉx)2+λ2(ba)2+λμ(a+b2ˉx)2λ2ni=1ti(a+b2xi)2], (2.6)

    for all x1,x2,,xn[a,b],ti0(1in) with ni=1ti=1 and ˉx=ni=1tixi.

    Proof. By applying Theorem 1.1 and (2.5), we obtain

    φ(λ(a+b)+(μλ)ni=1tixi)=φ(λni=1ti(a+bxi)+μni=1tixi)λφ(ni=1ti(a+bxi))+μφ(ni=1tixi)kλμ(a+b2ni=1tixi)2λ(ni=1tiφ(a+bxi)kni=1ti(xiˉx)2)+μφ(ni=1tixi)kλμ(a+b2ni=1tixi)2λ(φ(a)+φ(b)ni=1tiφ(xi)k2(ba)2+k2ni=1ti(a+b2xi)2)kλni=1ti(xiˉx)2+μni=1tiφ(xi)kμni=1ti(xiˉx)2kλμ(a+b2ˉx)2=λφ(a)+λφ(b)+(μλ)ni=1tiφ(xi)+kλ2ni=1ti(a+b2xi)2k[ni=1ti(xiˉx)2+λ2(ba)2+λμ(a+b2ˉx)2].

    Corollary 2.2. Let λ,μ[0,1] with λ+μ=1, and let φ be an S-C function with modulus k on [a,b] and x[a,b], then

    φ(λ(a+b)+(μλ)x)kλ2(a+b2x)2λφ(a)+λφ(b)+(μλ)φ(x)kλ[12(ba)2+μ(a+b2x)2].

    Corollary 2.3. Let φ be an S-C function with modulus k on [a,b] and s,t,λ,μ[0,1] with s+t=1 and λ+μ=1, then

    φ(λ(a+b)+(μλ)(sa+tb))+(λμ)φ(sa+tb)kλ2(st)2(ba)2λφ(a)+λφ(b)kλ[12(ba)2+λμ(a+b2sa2tb)2].

    Proof. Substitute x by sa+tb in Corollary 2.2 to get the inequality.

    Corollary 2.4. Let φ be an S-C function with modulus k on [a,b] and s,t[0,1],s+t=1, then

    2φ(a+b2)φ(sa+tb)+φ(ta+sb)k2(st)2(ba)2φ(a)+φ(b)k2(ba)2.

    Proof. Set λ=1 in Corollary 2.3 to get the righthand side of the inequality. On the other hand, by definition, we have

    φ(a+b2)=φ(sa+tb2+ta+sb2)12φ(sa+tb)+12φ(ta+sb)k4(st)2(ab)2.

    The Corollary 2.4 shows a kind of pre-H-H inequalities.

    Next, we prove a generalization of the H-H type inequality for S-C functions.

    Theorem 2.2. Assume that φ:[a,b]R is an S-C function with modulus k and ω is a nonnegative function on [a,b], then

    2φ(a+b2)baω(u)duba(ω(u)+ω(a+bu))φ(u)duk2ba(a+b2u)2ω(u)du(φ(a)+φ(b)k2(ba)2)baω(u)du.

    Proof. By multiplying the two-sided inequality in Corollary 2.4 with ω(a+t(ba)), integrating with respect to variable t from 0 to 1, and by interchanging u=a+t(ba), we get

    2φ(a+b2)baω(u)duba(φ(u)+φ(a+bu))ω(u)duk2ba(a+b2u)2ω(u)du(φ(a)+φ(b)k2(ba)2)baω(u)du,

    since

    ba(ω(u)+ω(a+bu))φ(u)du=ba(φ(u)+φ(a+bu))ω(u)du.

    Corollary 2.5. Let φ:[a,b]R be an S-C function with modulus k, then

    φ(a+b2)+k12(ba)21babaφ(u)duφ(a)+φ(b)2k6(ba)2.

    Proof. Putting ω1 in Theorem 2.2 and after some calculations, the desired inequality follows.

    If we consider ω(u)=uα1 in Theorem 2.2, then we have the following result.

    Corollary 2.6. Let α>0, 0<a<b, and φ:[a,b]R be an S-C function with modulus k, then

    2φ(a+b2)αbαaαba(uα1+(a+bu)α1)φ(u)dukα2(bαaα)ba(a+b2u)2uα1duφ(a)+φ(b)k2(ba)2.

    If α0+ in Corollary 2.6, then we get the next corollary.

    Corollary 2.7. Let 0<a<b and φ:[a,b]R be an S-C function with modulus k, then

    2φ(a+b2)log(ba)a+bbaφ(u)u(a+bu)duk2((a+b)2log(ba)2b2+2a2)(φ(a)+φ(b)k2(ba)2)log(ba)a+b.

    Let φ:[a,b]R be an S-C function with modulus k and 0s,t1 such that s+t=1. We define

    Δk(s,t,x,y)=sφ(x)+tφ(y)φ(sx+ty)kst(xy)2,

    for all x,y[a,b].

    Theorem 2.3. Let φ:[a,b]R be an S-C function with modulus k, then

    maxs,tt;x,y[a,b]Δk(s,t,x,y)Δk(a,b).

    Proof. First, we prove that

    Δk(s,t,x,y)Δk(x,y),

    for all s,tt and x,y[a,b].

    Now,

    Δk(x,y)Δk(s,t,x,y)=tφ(x)+sφ(y)+φ(sx+ty)+kst(xy)22φ(x+y2)k2(xy)2φ(tx+sy)+φ(sx+ty)+2kst(xy)2k2(xy)22φ(x+y2)=φ(tx+sy)+φ(sx+ty)k2(st)2(xy)22φ(x+y2)2φ((tx+sy)+(sx+ty)2)2φ(x+y2)=0.

    The remains of the proof is an application of Theorem 2.1.

    Theorem 2.4. Suppose that φ:[a,b]R is an S-C function with modulus k, then

    Jφ(t,x):=ni=1tiφ(xi)φ(ni=1tixi)φ(a)+φ(b)2φ(a+b2)k4(ba)2k(bxr)(xra),

    where (bxr)(xra)=mini{(bxi)(xia)}.

    Proof. Since xi[a,b], there is a sequence {λi},λi[0,1] with xi=λia+(1λi)b for i=1,2,. Thus,

    ni=1tiφ(xi)φ(ni=1tixi)=ni=1tiφ(λia+(1λi)b)φ(ni=1ti(λia+(1λi)b))ni=1ti(λiφ(a)+(1λi)φ(b)kλi(1λi)(ba)2)φ(ani=1tiλi+bni=1ti(1λi)).

    Setting λ:=ni=1tiλi and μ:=1ni=1tiλi, by the use of Theorem 2.3, we gain

    Jφ(t,x)λφ(a)+μφ(b)φ(λa+μb)k(ba)2ni=1tiλi(1λi)φ(a)+φ(b)2φ(a+b2)k2(ba)2+kλμ(ba)2kλr(1λr)(ba)2,

    because

    λr(1λr)=(bxr)(xra)(ba)2(bxi)(xia)(ba)2=λi(1λi),

    for all i=1,2,,n. Hence,

    Jφ(t,x)φ(a)+φ(b)2φ(a+b2)k4(ba)2k(bxr)(xra).

    In the following, we obtain an application of Lemma 2.2, which improves the results from [8].

    Proposition 3.1. Let 0<axib, ti0(i=1,2,,n) with ni=1ti=1,λ,μ0, and λ+μ=1, then

    ˜Gλ˜Aλe12b2(V(x)+12(ba)2λ2ˉy)˜Aλ, (3.1)

    where ˜Aλ:=λ(a+b)+(μλ)ˉx,˜Gλ:=(ab)λni=1xti(λμ)i,yi:=(a+b2xi)2, and y:={yi}.

    Proof. Letting φ(x):=log(x) and k=12b2 in Lemma 2.2, the desired inequality follows.

    Remark 3.1. Putting λ=1 in (3.1), we obtain

    ˜G˜Ae12b2(V(x)+12(ba)212ˉy)˜A,

    where ˜A=a+bˉx and ˜G=abni=1xtii (see [8]).

    Example 3.1. Assume that β2 and 0<a<b, then φ(x)=xβ is an S-C function with modulus k:=β(β1)2aβ2 on [a,b]. Further, if β=2n(n=1,2,), then φ(x)=xβ is an S-C function with modulus k on arbitrary interval [a,b].

    Proof. Let x,y[a,b]. Define the following functions on [0,1]:

    g(t):=(tx+(1t)y)β+β(β1)2aβ2t(1t)(xy)2

    and

    h(t):=txβ+(1t)yβ.

    Since g(0)=h(0), g(1)=h(1), h0, and

    g(t)=β(β1)(xy)2((tx+(1t)y)β2aβ2)0,

    g(t)h(t) for every t[0,1]. Therefore, xβ is an S-C function with modulus β(β1)2aβ2 on [a,b].

    In the next proposition, we give an extension of the pre-Grüss inequality (see [5,20]):

    ni=1tix2i(ni=1tixi)214(ba)2.

    Proposition 3.2. Assume that xi[a,b] and {ti}t, then

    ni=1tix2i(ni=1tixi)214(ba)2(bxr)(xra),

    where (bxr)(xra)=mini{(bxi)(xia)}.

    Proof. It follows from Example 3.1 and Theorem 2.4 with φ(x)=x2.

    In this subsection, new Shannon entropy bounds are found, that improve the entropy bounds from [19].

    Proposition 3.3. Assume that η:=min{ti:i=1,,n} and ϑ:=max{ti:i=1,,n}, then

    0lognH(t)log((η+ϑ)24ηϑ)(ϑη)28ϑ2:=Γ(η,ϑ)M(η,ϑ).

    Proof. Replace φ(x) by log(x) in Theorem 2.4 and consider k=12b2,xi:=1ti for all i=1,,n.

    Proposition 3.4. Assume that φ:[a,b]R is an S-C function with modulus k, then

    1nni=1φ(xi)φ(ni=1xin)φ(a)+φ(b)2φ(a+b2)k4(ba)2k(bxr)(xra),

    where (bxr)(xra)=mini{(bxi)(xia)}.

    Proof. Set ti=1n for every i=1,,n in Theorem 2.4.

    Proposition 3.5. Assume that η:=min{ti:i=1,,n} and ϑ:=max{ti:i=1,,n}, then

    0lognH(t)n{ηlog(2ηη+ϑ)+ϑlog(2ϑη+ϑ)18ϑ(ϑη)2}:=Λ(η,ϑ).

    Proof. Replace φ(x) by xlog(x) in Proposition 3.4 and modulus k=12b,xi:=ti for all i=1,,n.

    Example 3.2. Let j2 be an integer, n=10j, η=10j1, and ϑ=10j+1, then

    M(η,ϑ)Γ(η,ϑ)0.1225

    and

    n.m(η,ϑ)Λ(η,ϑ)12.25.

    In this work, we have stablished some new inequalities such as the Mercer, Fejér-Hermite-Hadamard, and Jensen inequalities for strongly convex functions. Next, using these inequalities, we get some applications in analysis and entropy of probability distributions.

    The authors declare they have not used Artificial Intelligence (AI) tools in the creation of this article.

    The authors declare that they have no competing interests.



    [1] A. Azócar, K. Nikodem, G. Roa, Fejér-type inequalities for strongly convex functions, Annales Mathematicae Silesianae, 26 (2012), 43–54.
    [2] M. Dehghanian, Y. Sayyari, On cubic convex functions and applications in information theory, Int. J. Nonlinear Anal. Appl., 14 (2023), 77–83. http://dx.doi.org/10.22075/ijnaa.2023.28880.4010 doi: 10.22075/ijnaa.2023.28880.4010
    [3] S. Dragomir, C. Goh, Some bounds on entropy measures in information theory, Appl. Math. Lett., 10 (1997), 23–28. http://dx.doi.org/10.1016/S0893-9659(97)00028-1 doi: 10.1016/S0893-9659(97)00028-1
    [4] L. Fejér, Uber die Fourierreihen (Hungarian), Math. Naturwise. Anz. Ungar. Akad. Wiss, 24 (1906), 369–390.
    [5] G. Grüss, Über das maximum des absoluten Betrages von, Math. Z., 39 (1935), 215–226.
    [6] J. Hadamard, Etude sur les proprietes des fonctions entieres et en particulier dune fonction consideree par Riemann, J. Math. Pure. Appl., 9 (1893), 171–215.
    [7] J. Jensen, Sur les fonctions convexes et les inégalités entre les valeurs moyennes, Acta Math., 30 (1906), 175–193. http://dx.doi.org/10.1007/BF02418571 doi: 10.1007/BF02418571
    [8] A. Mercer, A variant of Jensen's inequality, J. Inequal. Pure Appl. Math., 4 (2003), 73.
    [9] N. Merentes, K. Nikodem, Remarks on strongly convex functions, Aequat. Math., 80 (2010), 193–199. http://dx.doi.org/10.1007/s00010-010-0043-0 doi: 10.1007/s00010-010-0043-0
    [10] Y. Sayyari, New entropy bounds via uniformly convex functions, Chaos Soliton. Fract., 141 (2020), 110360. http://dx.doi.org/10.1016/j.chaos.2020.110360 doi: 10.1016/j.chaos.2020.110360
    [11] Y. Sayyari, A refinement of the Jensen-Simic-Mercer inequality with applications to entropy, J. Korean Soc. Math. Educ. B: Pure Appl. Math., 29 (2022), 51–57. http://dx.doi.org/10.7468/jksmeb.2022.29.1.51 doi: 10.7468/jksmeb.2022.29.1.51
    [12] Y. Sayyari, New refinements of Shannon's entropy upper bounds, J. Inform. Optim. Sci., 42 (2021), 1869–1883. http://dx.doi.org/10.1080/02522667.2021.1966947 doi: 10.1080/02522667.2021.1966947
    [13] Y. Sayyari, An improvement of the upper bound on the entropy of information sources, J. Math. Ext., 15 (2021), 1–12. http://dx.doi.org/10.30495/JME.SI.2021.1976 doi: 10.30495/JME.SI.2021.1976
    [14] Y. Sayyari, Remarks on uniformly convexity with applications in A-G-H inequality and entropy, Int. J. Nonlinear Anal., 13 (2022), 131–139. http://dx.doi.org/10.22075/IJNAA.2022.24133.2678 doi: 10.22075/IJNAA.2022.24133.2678
    [15] Y. Sayyari, An extension of Jensen-Mercer inequality with applications to entropy, Honam Math. J., 44 (2022), 513–520. http://dx.doi.org/10.5831/HMJ.2022.44.4.513 doi: 10.5831/HMJ.2022.44.4.513
    [16] Y. Sayyari, H. Barsam, A. Sattarzadeh, On new refinement of the Jensen inequality using uniformly convex functions with applications, Appl. Anal., 102 (2023), 5215–5223. http://dx.doi.org/10.1080/00036811.2023.2171873 doi: 10.1080/00036811.2023.2171873
    [17] Y. Sayyari, M. Dehghanian, fgh-convex functions and entropy bounds, Numer. Func. Anal. Opt., 44 (2023), 1428–1442. http://dx.doi.org/10.1080/01630563.2023.2261742 doi: 10.1080/01630563.2023.2261742
    [18] Y. Sayyari, M. Dehghanian, C. Park, S. Paokanta, An extension of the Hermite-Hadamard inequality for a power of a convex function, Open Math., 21 (2023), 20220542. http://dx.doi.org/10.1515/math-2022-0542 doi: 10.1515/math-2022-0542
    [19] S. Simic, Jensen's inequality and new entropy bounds, Appl. Math. Lett., 22 (2009), 1262–1265. http://dx.doi.org/10.1016/j.aml.2009.01.040 doi: 10.1016/j.aml.2009.01.040
    [20] S. Simic, Sharp global bounds for Jensen's inequality, Rocky MT J. Math., 41 (2011), 2021–2031.
    [21] S. Zlobec, Characterization of convexifiable functions, Optimization, 55 (2006), 251–261. http://dx.doi.org/10.1080/02331930600711968 doi: 10.1080/02331930600711968
    [22] S. Zlobec, Convexifiable functions in integral calculus, Glas. Mat., 40 (2005), 241–247.
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