
Citation: Tie-Hong Zhao, Zai-Yin He, Yu-Ming Chu. On some refinements for inequalities involving zero-balanced hypergeometric function[J]. AIMS Mathematics, 2020, 5(6): 6479-6495. doi: 10.3934/math.2020418
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Let a,b,c∈R with c≠0,−1,−2,⋯. Then the Gaussian hypergeometric function F(a,b;c;r) [1,2,3] is defined by
F(a,b;c;r)=2F1(a,b;c;r)=∞∑n=0(a)n(b)n(c)nn!rn(|r|<1), | (1.1) |
where (a)0=1, (a)n=a(a+1)(a+2)⋯(a+n−1)=Γ(a+n)/Γ(a) for n∈N={1,2,⋯} is the Pochhammer symbol and Γ(x)=∫∞0tx−1e−tdt is the classical Euler gamma function [4,5]. If c=a+b, then F(a,b;a+b;r) is said to be zero-balanced. In particular, the complete elliptic integral K(r) [6,7] and generalized complete elliptic integral Ka(r) (r∈(0,1),a∈(0,1/2]) [8] of the first kind are the special cases of the Gaussian hypergeometric function F(a,b;c;r). Indeed, K(r) and Ka(r) can be expressed by
K(r)=π2F(1/2,1/2;1;r2) |
and
Ka(r)=π2F(a,1−a;1;r2),r∈(0,1). | (1.2) |
In 2016, Takeuchi [9] introduced the complete p-elliptic integral Kp(r) of the first kind in terms of the Gaussian hypergeometric functions as follows
Kp(r)=πp2F(1/p;1−1/p;1;rp), |
where πp is given by
πp2=1pB(1/p,1−1/p)=πpsin(π/p) |
and
B(a,b)=∫10ta−1(1−t)b−1dt=Γ(a)Γ(b)Γ(a+b) |
is the Beta function.
Recently, the Gaussian hypergeometric function and its special cases have attracted the attention of many researchers [10,11,12,13,14,15,16,17,18,19,20,21,22,23,24,25] due to they have wide applications in pure and applied mathematics [26,27,28,29,30,31,32,33,34,35,36,37,38,39,40].
Anderson et al. [41] proved that the double inequality
K(r)K(√r)>11+r | (1.3) |
holds for all r∈(0,1).
Motivated by inequality (1.3), many researchers provided its improvements, variants, refinements and generalizations. For example, Alzer and Richards [42] proved that the double inequality
11+σ(a)r<Ka(r)Ka(√r)<11+τar | (1.4) |
holds for all a∈(0,1/2] and r∈(0,1) with the best possible factors σ(a)=a(1−a) and τa=0.
Recently, Yin et al. [43] generalized inequality (1.4) to the case of complete p-elliptic integral of the first kind Kp(r) and a sharp improvement of (1.4) was presented by Zhao et al. in [8]. Ismail [42, p. 1669] asked whether the inequality (1.4) can be extended to the zero-balanced hypergeometric function. Inspired by this question, Richards [44] proved the following result which is to answer the question by Ismail from another point of view.
Theorem A. (See [44]) Let a,b>0. Then the double inequality
1(1+r)λ(a,b)<F(a,b;a+b;r2)F(a,b;a+b;r)<1(1+r)μ(a,b) |
holds for all r∈(0,1) with the best possible exponents λ(a,b)=ab/(a+b) and μ(a,b)=0.
The main purpose of this paper is to generalize the inequality (1.4) to the case of zero-balanced hypergeometric function and also make some refinements of (1.4) and Theorem A under certain restriction of a,b, which gives an affirmative answer to the question by Ismail. Our main result is the following Theorem 1.1.
Throughout this paper, we mainly focus on the parameters satisfying a+b≥6ab/5 for a,b>0. By the symmetry, our parameters might be only consider as 0<a<b and a+b≥6ab/5, which is equivalent to
{(a,b)| 0<a≤56, b>0}∪{(a,b)| 56<a≤53, a<b≤5a6a−5}. | (1.5) |
For convenience, we denote σ(a,b) and τ(a,b) by σ and τ simply if no risk for confusion, where
σ(a,b)=aba+bandτ(a,b)=ab(a+b−ab+1)2(a+b)(a+b+1). |
Theorem 1.1. Let a,b>0 with a+b≥6ab/5. Then the double inequality
1+τr2+αr31+σr<F(a,b;a+b;r2)F(a,b;a+b;r)<1+τr2+βr31+σr | (1.6) |
holds for all r∈(0,1) if and only if α≤α0 and β≥β0, where
α0=α0(a,b)=−ab(a+1)(b+1)[a(2+a)+(1−a)(2+a)b+(1−a)b2]3(a+b)2(a+b+1)(a+b+2),β0=β0(a,b)=ab(a+1)(b+1)2(a+b)(1+a+b). |
Remark 1.2. For later use, we need discuss about the sign of α0 and α0+τ for a,b>0 with a+b≥6ab/5.
● Let ˆα(a,b)=a(2+a)+(1−a)(2+a)b+(1−a)b2. Then it is easy to see that ˆα(a,b)>0 for 0<a≤1 and b>0. Moreover, it follows from (1.5) that
ˆα(a,b)≥ˆα(a,5a6a−5)=3a2[(2a−3)2+1]2(6a−5)2>0 |
for 1<a≤5/3 and a<b≤5a/(6a−5). This yields α0<0.
● By calculations, we obtain
α0+τ=ab6(a+b)2(1+a+b)(2+a+b)[a(1+a)(2+a)+1125[(5−3a)(50+330a+223a2)+294a3]b+(1+a)(3−2a+2a2)b2+(2a−1)(a−1)b3]. |
From the above expression, we clearly see that α0+τ>0 for 0<a≤1/2 (or 1≤a≤5/3) and b>0, and α0+τ<0 for 1/2<a≤5/6 and sufficiently large b>0.
As mentioned in (1.2), if b=1−a, then F(a,b;a+b;r2)/F(a,b;a+b;r) reduces to the ratio of generalized complete elliptic integral of the first kind Ka(r)/Ka(√r) and a(1−a)≤1/4 for 0<a<1. That is to say Theorem 1.1 in [8] can be derived from our Theorem 1.1 as a corollary.
Corollary 1.3. Let a∈(0,1/2]. Then the double inequality
1+τ(a)r2+λ(a)r31+σ(a)r<Ka(r)Ka(√r)<1+τ(a)r2+μ(a)r31+σ(a)r | (1.7) |
holds for all r∈(0,1), where σ(a)=σ(a,1−a),τ(a)=τ(a,1−a) and λ(a)=α0(a,1−a), μ(a)=β0(a,1−a) are defined in the literature [8].
Remark 1.4. Corollary 1.3 gives an affirmative answer to the question by Ismail. Moreover, the bounds for inequality (1.7) are better than (1.4). Indeed, from λ(a)<0, σ(a)=τ(a)+μ(a) and τ(a)+λ(a)=a(1−a)[(1−2a)(6+13a+33a2)+2a3(25+4a)]/36>0 for a∈(0,1/2], we obtain
1+τ(a)r2+λ(a)r31+σ(a)r=11+σ(a)r+r21+σ(a)r[τ(a)+λ(a)r]>11+σ(a)r+r21+σ(a)r[τ(a)+λ(a)]>11+σ(a)r |
and
1+τ(a)r2+μ(a)r31+σ(a)r<1+τ(a)r+μ(a)r1+σ(a)r=1 |
for r∈(0,1) and a∈(0,1/2].
Remark 1.5. Under the assumption of Theorem 1.1, the upper bound of (1.6) is better than that in Theorem A due to
1+τr2+βr31+σr<1+τr+βr1+σr=1 |
from σ=τ+β0. On the other hand, in order to compare the lower bound of (1.6) and Theorem A, it suffices to take into account the sign of f(r):=(1+τr2+α0r3)(1+r)σ−(1+σr).
Differentiation yields
f′(r)=(1+r)σ−1[σ+2τr+(3α0+2τ+στ)r2+α0(3+σ)r3]−σ,f″(r)=(1+r)σ−2ˆf(r), | (1.8) |
where
ˆf(r)=2τ−σ+σ2+2(3α0+2τ+2στ)r+(2+σ)(6α0+τ+στ)r2+α0(σ+2)(σ+3)r3. |
It follows from
2τ−σ+σ2=a2b2(a+b)2(1+a+b),3α0+2τ+2στ=a2b2(5+3a+3b+ab)(a+b)2(1+a+b)(2+a+b) |
and α0<0 that ˆf(r) can be regarded as the special polynomial defined in Lemma 2.1. We can verify but miss the details that ˆf(1)<0 for a,b>0 with a+b≥6ab/5. This in conjunction with Lemma 2.1 implies that there exists r∗∈(0,1) such that ˆf(r)>0 for r∈(0,r∗) and ˆf(r)<0 for r∈(r∗,1). Combining this with (1.8) and f(0)=f′(0)=0, we conclude that f(r)>0 for r∈(0,r∗] and f(r) is strictly concave on (r∗,1).
For a,b>0 with a+b≥6ab/5, we have the following two conclusion:
● if f(1)≥0, then f(r)>min{f(r∗),f(1)}≥0 for r∈(r∗,1). This yields the lower bound of (1.6) is better than that in Theorem A for r∈(0,1) and we refer to see the domain of a,b illustrated in Figure 1;
● if f(1)<0, then there exists r′∈(r∗,1) such that the lower bound of (1.6) is better than that in Theorem A for r∈(0,r′).
In this section, we introduce some notations and present some technical lemmas, which will be used in proving our main result.
Let a,b>0 and
Δn:=Δn(a,b)=(a)n(b)nn!(a+b)n. |
Then we clearly see from (1.1) that F(a,b;a+b;r) can be expressed simply as
F(a,b;a+b;r)=∞∑n=0Δnrn. | (2.1) |
It is easy to verify that Δn satisfies the recurrence relation
Δn+1Δn=(n+a)(n+b)(a+b+n)(n+1) | (2.2) |
and also Δn is strictly decreasing for n≥0 if a+b≥ab.
The following lemma provides a simple criterion to determine the sign of a class of special polynomial.
Lemma 2.1. (See [45, Lemma 7) Let n,m∈N∪{0} with n>m and Pn(t) be the polynomial of degree n defined by
Pn(t)=m∑i=0aiti−n∑i=m+1aiti, |
where am,an>0 and ai≥0 for 0≤i≤n−1 with i≠m. Then there exist t0∈(0,∞) such that Pn(t0)=0 and Pn(t)>0 for t∈(0,t0) and Pn(t)<0 for t∈(t0,∞).
Lemma 2.2. (1) For a,b>0, then nΔn(a,b) is strictly increasing for n≥1. In particular,
Δn(a,b)Δm(a,b)<mn | (2.3) |
for m>n≥1.
(2) For a,b>0 with a+b≥6ab/5, then Δn+1/Δn is strictly increasing for n≥1.
(3) For a,b>0 with a+b≥ab, then Δn+1/Δn>Δ2n+2/Δ2n holds for n≥0.
Proof. (1) From the recurrence relation (2.2) of Δn, we clearly see that
(n+1)Δn+1nΔn=n+1n⋅(a+n)(b+n)(a+b+n)(n+1)=1+abn(a+b+n)>1 |
for a,b>0 and n≥1. This yields the monotonicity of nΔn(a,b) with respect to n and inequality (2.3) follows directly from the monotonicity of nΔn(a,b).
(2) Taking the differentiation of (2.2) with respect to n yields
∂(Δn+1/Δn)∂n=δ1(n;a,b)(n+1)2(a+b+n)2, | (2.4) |
where
δ1(n;a,b)=a2+a(1−a)b+(1−a)b2+2(a+b−ab)n+n2. |
● If 0<a≤1 and b>0, then we clearly see that δ1(n;a,b)>0 for n≥1.
● If 1<a≤5/3, then it follows from (1.5) that
δ1(n;a,b)≥δ(1;a,b)=(a+1)2−(a−1)(a+2)b−(a−1)b2≥(a+1)2−(a−1)(a+2)⋅5a6a−5−(a−1)(5a6a−5)2=4+3(a−1)[4+(a−1)(10+(a−1)2+a2)](6a−5)2>0 |
for n≥1.
Therefore, the proof is completed from (2.4) and δ1(n;a,b)>0.
(3) From (2.2) we clearly see that
Δn+1Δn−Δ2n+2Δ2n=(n+a)(n+b)(a+b+n)(n+1)−(2n+a)(2n+b)(2n+1+a)(2n+1+b)(a+b+2n)(2n+1)(a+b+2n+1)(2n+2)=abδ2(n;a,b)2(n+1)(2n+1)(a+b+n)(a+b+2n)(1+a+b+2n), | (2.5) |
where
δ2(n;a,b)=(a+b)(1+a+b−ab)+[3(1+2a+2b)+a+b−ab]n+4(3+a+b)n2+8n3. |
Combining this with a+b≥ab and (2.5) yields the desired result.
Lemma 2.3. Let a,b>0 with a+b≥6ab/5 and ρn(a,b)=(1+σ)Δn+2−2(α0+τ)Δ2n+2−2Δ2n+4. Then ρn(a,b)>0 for n≥2.
Proof. Let ˆρn(a,b)=(1+σ)Δn+2−2Δ2n+4. Then Remark 1.2 makes us to know that the sign of α0+τ can not be determined. We divide into two cases to complete the proof by mathematical induction.
Case 1 α0+τ≤0. It suffices to show that ˆρn(a,b)>0 for n≥0.
From the definition of Δn, we compute that
ˆρ0(a,b)=a2(a+1)b2(b+1)η(a,b)12(a+b)2(1+a+b)(2+a+b)(3+a+b), | (2.6) |
where
η(a,b)=36+17a+a2+(17+2a−a2)b+(1−a)b2. |
It follows from 0<a≤1 that η(a,b)>0. For a>1, we clearly see that η(a,b)>0 from (1.5) and Lemma 2.1 together with
η(a,5a6a−5)=6[24+212(a−1)+(a−1)2(338+104a+a2)](6a−5)2>0. |
This in conjunction with (2.6) yields ˆρ0(a,b)>0.
We assume that ˆρk(a,b)>0, namely, (1+σ)Δk+2>2Δ2k+4 for k≥0. By the induction hypothesis, it follows from Lemma 2.2(3) and n=k+2 that
ˆρk+1(a,b)=(1+σ)Δk+2⋅Δk+3Δk+2−2Δ2k+6>2Δ2k+4⋅Δk+3Δk+2−2Δ2k+6=2Δ2k+4(Δk+3Δk+2−Δ2k+6Δ2k+4)>0. |
This completes the proof of Case 1.
Case 2 α0+τ>0.
By simple calculations, ρ2(a,b) can be simplified as
ρ2(a,b)=ab∏3i=0(a+i)∏3j=0(b+j)60480(a+b)∏2i=0(a+b+i)∏7j=0(a+b+j)7∑k=0ϵk(a)bk, | (2.7) |
where
ϵ0(a)=2a(1+a)(2+a)(823200+465754a+87277a2+5546a3+23a4),ϵ1(a)=3292800+10782032a+13070784a2+7204178a3+2041437a4+313859a5+25539a6+891a7,ϵ2(a)=6802216+13070784a+8341952a2+1941253a3+2474a4−67079a5−9902a6−458a7,ϵ3(a)=4790032+7204178a+1941253a2−896662a3−577922a4−121105a5−11511a6−423a7,ϵ4(a)=1477354+2041437a+2474a2−577922a3−227680a4−36779a5−2588a6−56a7,ϵ5(a)=207922+313859a−67079a2−121105a3−36779a4−4330a5−168a6,ϵ6(a)=11230+25539a−9902a2−11511a3−2588a4−168a5,ϵ7(a)=(1−a)(46+937a+479a2+56a3). |
Obviously, it follows that ϵ0(a)>0,ϵ1(a)>0 for a>0 and ϵ7(a)≥0 for 0<a≤1 and ϵ7(a)<0 for 1<a≤5/3. Moreover, ϵk(a) (k=2,3,⋯,6) is the special polynomial defined in Lemma 2.1. It follows from Lemma 2.1 and
ϵ2(5/3)=1305072134722187,ϵ3(5/3)=95252967281,ϵ4(5/3)=−1666165122187,ϵ5(5/3)=−87250384243,ϵ6(5/3)=−132656027 |
that ϵ2(a)>0,ϵ3(a)>0 for 0<a≤5/3 and there exits ak∈(0,5/3) (k=4,5,6) such that ϵk(a)>0 for 0<a<ak and ϵk(a)<0 for ak<a≤5/3. The roots ak can be computed numerically as follows a4=1.65774⋯>a5=1.41613⋯>a6=1.22785⋯>1. So
● for 0<a≤1, then it follows that ∑7k=0ϵk(a)bk>0;
● for 1<a≤5/3, then we can consider the following intervals (1,a6], (a6,a5], (a5,a4], (a4,5/3] and ∑7k=0ϵk(a)bk can be regarded as the special polynomial defined in Lemma 2.1 on each such interval, which yields ∑7k=0ϵk(a)bk>0 following from (1.5) and Lemma 2.1 together with
7∑k=0ϵk(a)(5a6a−5)k=72a2(6a−5)7[48(295386449(a−1)2+15384558(a2−1)+1526700a2)+(a−1)3(12215090768+17108173200a+8769780982a2+3825548386a3(a−1)+10871964835a4+18178058803a5+6741509385a6+1047476909a7+64085484a8+772338a9)]>0. |
This in conjunction with (2.7) implies ρ2(a,b)>0.
Suppose that ρk(a,b)>0 for k≥2. We now prove that ρk+1(a,b)>0.
The induction hypothesis enables us to know that
(1+σ)Δk+2>2(α0+τ)Δ2k+2+2Δ2k+4. | (2.8) |
It follows from Lemma 2.2(2) and (3) with n=k+2 that
Δk+3Δk+2−Δ2k+4Δ2k+2>Δk+3Δk+2−Δ2k+6Δ2k+4>0. |
This in conjunction with (2.8) yields
ρk+1(a,b)=(1+σ)Δk+2⋅Δk+3Δk+2−2(α0+τ)Δ2k+4−2Δ2k+6>[2(α0+τ)Δ2k+2+2Δ2k+4]⋅Δk+3Δk+2−2(α0+τ)Δ2k+4−2Δ2k+6=2Δ2k+4[(α0+τ)Δ2k+2Δ2k+4(Δk+3Δk+2−Δ2k+4Δ2k+2)+(Δk+3Δk+2−Δ2k+6Δ2k+4)]>0. |
Lemma 2.4. Let a,b>0 with a+b≥6ab/5 and
An=Δn+2−α0Δ2n+1−τΔ2n+2−Δ2n+4,Bn=σΔn+2−α0Δ2n+2−τΔ2n+3−Δ2n+5. |
Then (i) An>0; (ii) An+Bn>0 for n≥0.
Proof. (ⅰ) By Lemma 2.2(2) and Bernoulli's inequality we know that
Δn+2Δ2n+1=Δn+2Δn+3⋅Δn+3Δn+4⋯Δ2nΔ2n+1≥(Δ2nΔ2n+1)n−1=[1+a+b−ab+2n(a+2n)(b+2n)]n−1≥1+(n−1)(a+b−ab+2n)(a+2n)(b+2n) |
for n≥2. This in conjunction with (2.2) and the monotonicity of Δn with respect to n gives
AnΔ2n+1=Δn+2Δ2n+1−α0−τΔ2n+2Δ2n+1−Δ2n+4Δ2n+1≥Δn+2Δ2n+1−α0−(τ+1)Δ2n+2Δ2n+1≥1+(n−1)(a+b−ab+2n)(a+2n)(b+2n)−α0−(τ+1)(a+2n+1)(b+2n+1)(a+b+2n+1)(2n+2)≥1+(n−1)(a+b−ab+2n)(a+b+2n+1)(2n+2)−α0−(τ+1)(a+2n+1)(b+2n+1)(a+b+2n+1)(2n+2)=δ3(n;a,b)12(a+b)2(1+a+b)(2+a+b)(1+n)(1+a+b+2n), | (2.9) |
where δ3(n;a,b)=ζ0(a,b)+ζ1(a,b)n+ζ2(a,b)n2 and ζ0(a,b)=∑5k=0ε0k(a)bk, ζ1(a,b)=∑5k=0ε1k(a)bk, ζ2(a,b)=∑4k=0ε2k(a)bk, and
ε00(a)=6a2(1+a)(2+a),ε01(a)=a(24+56a+29a2+4a3+a4),ε02(a)=2(6+28a+17a2−4a3−2a4),ε03(a)=18+29a−8a2−22a3−10a4−a5,ε04(a)=2(3+2a−2a2−5a3−a4),ε05(a)=a(1−a)(1+a),ε10(a)=6a3(1+a)(2+a),ε11(a)=2a2(18+28a+3a2−4a3),ε12(a)=2a(18+20a−12a2−8a3+3a4),ε13(a)=2(6+28a−12a2−26a3−3a4−2a5),ε14(a)=2(9+3a−8a2−3a3−4a4),ε15(a)=2(1−a)(3−a+2a2),ε20(a)=12a2(1+a)(2+a),ε21(a)=4a[12+25a+a2(9−a)],ε22(a)=4[6+25a+a2(3a2−a+6)],ε23(a)=49(3+a+a2)[7+2(5−3a)(2+3a)],ε24(a)=4125[(5−3a)(75+20a+87a2)+11a3]. |
From the above expressions, we clearly see that ζ2(a,b)>0 for 0<a≤5/3 and b>0. Moreover,
2ζ2(a,b)+ζ1(a,b)=6a2(1+a)(2+a)(4+a)+2a[48+118a+46a2+a2(2−a)+4a2(4−a2)]b+2[24+118a+12a2+16a2(2−a)+4a4+3a5]b2+2(42+64a−16a2−26a3−11a4−2a5)b3+2(21−a+4a2−11a3−4a4)b4+2(1−a)(3−a+2a2)b5, |
which gives 2ζ2(a,b)+ζ1(a,b)>0 for 0<a≤1. By the same argument as in Case 2 of Lemma 2.3, 2ζ2(a,b)+ζ1(a,b) can be regarded as the special polynomial of b defined in Lemma 2.1 for 1<a≤5/3, which implies 2ζ2(a,b)+ζ1(a,b)>0 from Lemma 2.1 and
2ζ2(a,5a6a−5)+ζ1(a,5a6a−5)=12a4(6a−5)5[23168(a−1)+2940a+(a−1)2(32043+6028a+20528a2+14472a3+768a4)]>0. |
From the above discussion, we clearly see that for n≥2,
δ3(n;a,b)≥n[2ζ2(a,b)+ζ1(a,b)]+ζ0(a,b)≥2[2ζ2(a,b)+ζ1(a,b)]+ζ0(a,b)=6a2(1+a)(2+a)(9+2a)+3a[72+176a+75a2+5a2(4−a2)]b+6[18+88a+11a2+12a2(2−a)+2a4+2a5]b2+3(62+95a−24a2−42a3−18a4−3a5)b3+6(15+2a2−9a3−3a4)b4+3(1−a)(4−a+3a2)b5:=ˆζ(a,b). | (2.10) |
Similarly, it follows from (2.10) that ˆζ(a,b)>0 for 0<a≤1 and ˆζ(a,b)>0 for 1<a≤5/3 from Lemma 2.1 and
ˆζ(a,5a6a−5)=108a4(6a−5)5[652+(a−1)(1098(a3−1)+5202a+2908a2(a2−1)+338a3+11a4+189a5)]>0. |
This in conjunction with (2.9) and (2.10) implies that An>0 for n≥2.
It remains to verify the sign of A0 and A1. We only give the details of calculations for A0 and similar for A1.
By the definition of Δn, A0 can be rewritten as
A0=a(1+a)b(1+b)ˆζ0(a,b)8(a+b)3(1+a+b)2(2+a+b)(3+a+b), |
where
ˆζ0(a,b)=2a2(1+a)(2+a)(3+a)+a[24+70a+51a2+6a3+a3(2−a)]b+[2(6−a)+2a2+a(18+13a+a2)(4−a2)]b2+(22+51a−14a2−24a3−3a4)b3+(12+8a−13a2−3a3)b4+(1−a)(2+a)b5. |
The same argument as in (2.10) enables us to know that ˆζ0(a,b)>0 for 0<a≤1 and ˆζ0(a,b)>0 for 1<a≤5/3 from Lemma 2.1 and
ˆζ0(a,5a6a−5)=12a4(6a−5)5[834+(a−1)(334+2134a+2301a2(a−1)+1722a3+2952a4+306a5)]>0. |
(ⅱ) We first verify the sign of A0+B0 and A1+B1. Since the method is similar as above, we only give some necessary expression for A0+B0 and then similar for A1+B1.
By calculations, we obtain
A0+B0=a(1+a)b(1+b)ˆζ1(a,b)120(a+b)3(1+a+b)2(2+a+b)(3+a+b)(4+a+b), |
where
ˆζ1(a,b)=6a2(1+a)(2+a)(3+a)(4+a)+a(288+2580a+3836a2+1919a3+358a4+19a5)b+(2+a)(3+a)[24+410a+431a2+2a2(2−a)(18+7a)]b2+(300+3836a+2877a2−666a3−869a4−187a5−11a6)b3+(210+1919a+379a2−869a3−346a4−33a5)b4+(60+358a−78a2−187a3−33a4)b5+(1−a)(2+a)(3+11a)b6. |
We can compute easily that ˆζ1(a,b)>0 for 0<a≤1 and ˆζ1(a,b)>0 for 1<a≤5/3 from Lemma 2.1 and
ˆζ1(a,5a6a−5)=36a4(6a−5)6[59520+(a−1)(32020+164020a+367670a2+a3(a−1)(1030750+709949a)+42672a5+179016a6+7446a7))]>0. |
For n≥2, it follows from α0<0 and Lemma 2.3 together with the monotonicity of Δn with respect to n that
An+Bn=(1+σ)Δn+2−α0(Δ2n+1+Δ2n+2)−τ(Δ2n+2+Δ2n+3)−(Δ2n+4+Δ2n+5)≥(1+σ)Δn+2−2(α0+τ)Δ2n+2−2Δ2n+4=ρn(a,b)>0. |
Lemma 2.5. Let a,b>0 with a+b≥ab and
Cn=σΔn+1−β0Δ2n−τΔ2n+1−Δ2n+3,Dn=Δn+2−β0Δ2n+1−τΔ2n+2−Δ2n+4. |
Then (i) Cn<0; (ii) Cn+Dn<0 for n≥0.
Proof. (ⅰ) By calculations, we obtain
C0=−a(1+a)b(1+b)[(a+b)(4+3a+3b)+2(a+b+3)(a+b−ab)]6(a+b)2(1+a+b)(2+a+b)<0. | (2.11) |
The relation σ=β0+τ allows us to rewrite Cn as
Cn=(β0+τ)Δn+1−β0Δ2n−τΔ2n+1−Δ2n+3=β0(Δn+1−2nn+1Δ2n)+τ(Δn+1−2n+1n+1Δ2n+1)+ˆCn, |
where
ˆCn=n−1n+1β0Δ2n+nn+1τΔ2n+1−Δ2n+3. |
From Lemma 2.2(1) it suffices to show ˆCn<0 for n≥1.
For n≥1, Lemma 2.2(1) and τ,β0>0 together with the monotonicity of Δn with respect to n lead to
ˆCn<(n−1n+1β0+nn+1τ)Δ2n−Δ2n+3<Δ2n+3[(n−1n+1β0+nn+1τ)2n+32n−1]:=Δ2n+3ˆC∗n. | (2.12) |
Simplifying ˆC∗n gives rise to
ˆC∗n=−14(a+b)(1+a+b)n(1+n)[3a(1+a)b(1+b)+2(2(a+b+1)(a+b−ab)+a2b2)n+4(1+a+b)(a+b−ab)n2]<0. |
This in conjunction with (2.11) and (2.12) completes the proof of (ⅰ).
(ⅱ) For n≥0, it follows from Lemma 2.2(1) and σ=τ+β0 together with the monotonicity of Δn with respect to n that
Cn+Dn=σΔn+1+Δn+2−β0(Δ2n+Δ2n+1)−τ(Δ2n+1+Δ2n+2)−(Δ2n+3+Δ2n+4)<σΔn+1+Δn+2−2(τ+β0)Δ2n+2−2Δ2n+4=σ(Δn+1−2Δ2n+2)+Δn+2−2Δ2n+4<0. |
This completes the proof.
Proof. Define
φa,b(r)=(1+σr)F(a,b;a+b;r2)−(1+τr2+α0r3)F(a,b;a+b;r) |
and
ϕa,b(r)=(1+σr)F(a,b;a+b;r2)−(1+τr2+β0r3)F(a,b;a+b;r). |
In order to prove the inequalities (1.6) is valid, it suffices to show φa,b(r)>0 and ϕa,b(r)<0 for r∈(0,1).
From (2.1), we can rewrite φa,b(r) and ϕa,b(r), in terms of power series, as
φa,b(r)=(1+σr)∞∑n=0Δnr2n−(1+τr2+α0r3)∞∑n=0Δnrn=r4[∞∑n=0(An+Bnr)r2n], | (3.1) |
ϕa,b(r)=(1+σr)∞∑n=0Δnr2n−(1+τr2+β0r3)∞∑n=0Δnrn=r3[∞∑n=0(Cn+Dnr)r2n], | (3.2) |
where An,Bn and Cn,Dn are defined in Lemma 2.4 and Lemma 2.5, respectively.
From (3.1) and (3.2), we only need to prove that An+Bnr>0 and Cn+Dnr<0 for r∈(0,1) and n≥0.
Case 1 An+Bnr>0.
● If Bn≥0, then it follows from Lemma 2.4(i) that An+Bnr≥An>0 for r∈(0,1);
● If Bn<0, then Lemma 2.4(ii) enables us to know that An+Bnr>An+Bn>0 for r∈(0,1).
Case 2 Cn+Dnr<0.
● If Dn≤0, then it follows from Lemma 2.5(i) that Cn+Dnr≤Cn<0 for r∈(0,1);
● If Dn>0, then from Lemma 2.5(ii) we clearly see that Cn+Dnr<Cn+Dn<0 for r∈(0,1).
We are now in a position to prove α0 and β0 are the best possible constants.
Let
Φa,b(r)=(1+σr)F(a,b;a+b;r2)−(1+τr2)F(a,b;a+b;r)r3F(a,b;a+b;r). | (3.3) |
Then we clearly see that
{limr→0+Φa,b(r)=−ab(a+1)(b+1)[a(2+a)+(1−a)(2+a)b+(1−a)b2]3(a+b)2(a+b+1)(a+b+2)=α0,limr→1−Φa,b(r)=ab(a+1)(b+1)2(a+b)(1+a+b)=β0. | (3.4) |
For α0<c<β0, then it follows from (3.4) that there exist sufficiently small r1,r2∈(0,1) such that Φa,b(r)<c for r∈(0,r1) and Φa,b(r)>c for r∈(1−r2,1). In other words,
F(a,b;a+b;r2)F(a,b;a+b;r)<1+τr2+cr31+σr,r∈(0,r1) |
and
F(a,b;a+b;r2)F(a,b;a+b;r)>1+τr2+cr31+σr,r∈(1−r2,1). |
This completes the proof of Theorem 1.1.
Remark 3.1. In the proof of Theorem A [44], the parameters a and b are required to meet the condition that a+b>ab, although this is still more relaxed than our parameter's condition a+b≥6ab/5 in Theorem 1.1.
It is natural to ask that can our parameter's condition be relaxed to a+b>ab? From Lemma 2.5, we clearly see that the upper bound in Theorem 1.1 still holds for a+b≥ab but the lower bound is not true. The reason is that A0(a,b)<0 for 3/2≤a≤3 and a+b=ab. More precisely,
A0(a,aa−1)=−(1−a2)(2a−1)[(3−a)(2a−3)(43a2+72a−72)+5a4]648(a2+a−1)2(a2+2a−2)(a2+3a−3)<0 |
for 3/2≤a≤3. By the continuity, it follows from (3.1) that there exists a sufficiently small ra,b∈(0,1) such that φa,b(r)<0 for r∈(0,ra,b) when a and b lie in a very narrow strip near the curve segment {(a,b)| 3/2≤a≤3,a+b=ab}. We focus on the condition that a+b≥6ab/5 just to make the calculation simpler. Of course, one can give some refinements for our parameter condition.
To this end, numerical experiment results allow us to pose the following conjecture.
Conjecture. Let a,b>0 with a+b≥6ab/5 and Φa,b(r) be defined as in (3.3). Then Φa,b(r) is strictly increasing from (0,1) onto (α0,β0).
This paper deals with the zero-balanced hypergeometric function 2F1(a,b;a+b;r). In this study, we present an elegant double inequality for 2F1(a,b;a+b;r2)/2F1(a,b;a+b;r), which gives some refinements for some previously known results and also answers to the question by Ismail in the affirmative.
In this paper, we have established a sharp double inequality involving the ratio of zero-balanced hypergeometric function 2F1(a,b;a+b;r2)/2F1(a,b;a+b;r). More precisely, the double inequality
1+τr2+α0r31+σr<F(a,b;a+b;r2)F(a,b;a+b;r)<1+τr2+β0r31+σr |
holds for all r∈(0,1) with the best possible constants α0 and β0, where
σ=aba+b,τ=ab(a+b−ab+1)2(a+b)(a+b+1),α0=−ab(a+1)(b+1)[a(2+a)+(1−a)(2+a)b+(1−a)b2]3(a+b)2(a+b+1)(a+b+2),β0=ab(a+1)(b+1)2(a+b)(1+a+b). |
The authors would like to thank the anonymous referees for their valuable comments and suggestions, which led to considerable improvement of the article.
This work was supported by the National Natural Science Foundation of China (Grant Nos. 11971142, 61673169, 11701176, 11871202) and the Natural Science Foundation of Zhejiang Province (Grant No. LY19A010012).
The authors declare that they have no competing interests.
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4. | Tie-Hong Zhao, Zai-Yin He, Yu-Ming Chu, Sharp Bounds for the Weighted Hölder Mean of the Zero-Balanced Generalized Complete Elliptic Integrals, 2020, 1617-9447, 10.1007/s40315-020-00352-7 | |
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93. | Muhammad Bilal Khan, Jorge E. Macías-Díaz, Savin Treanțǎ, Mohamed S. Soliman, Some Fejér-Type Inequalities for Generalized Interval-Valued Convex Functions, 2022, 10, 2227-7390, 3851, 10.3390/math10203851 | |
94. | Zhenping Zhou, Xin Liu, Ping Li, B24N24 nanocage as an electronic sensor for metronidazole drug: density functional theory studies, 2022, 28, 1610-2940, 10.1007/s00894-022-05127-6 | |
95. | Ali A Rajhi, Sagr Alamri, Ghaffar Ebadi, Retracted: A density functional theory investigation on the Au-decorated zinc oxide nanosheet as a chemical sensor for mesalamine drug detection, 2022, 97, 0031-8949, 045401, 10.1088/1402-4896/ac51c7 | |
96. | Amjad Ali Pasha, Nazrul Islam, Wasim Jamshed, Mohammad Irfan Alam, Abdul Gani Abdul Jameel, Khalid A. Juhany, Radi Alsulami, Statistical analysis of viscous hybridized nanofluid flowing via Galerkin finite element technique, 2022, 137, 07351933, 106244, 10.1016/j.icheatmasstransfer.2022.106244 | |
97. | Li-E Yan, Nidal H. Abu-Hamdeh, Rashad A.R. Bantan, Mahmoud M. Selim, Heat storage unit for melting of paraffin considering hybrid nanomaterial and helical tubes, 2021, 44, 2352152X, 103427, 10.1016/j.est.2021.103427 | |
98. | Ali Rostamian, Keivan Fallah, Yasser Rostamiyan, Javad Alinejad, Application of computational fluid dynamics for detection of high risk region in middle cerebral artery (MCA) aneurysm, 2023, 34, 0129-1831, 10.1142/S0129183123500195 | |
99. | Tie-Hong Zhao, Barkat Ali Bhayo, Yu-Ming Chu, Inequalities for Generalized Grötzsch Ring Function, 2022, 22, 1617-9447, 559, 10.1007/s40315-021-00415-3 | |
100. | Yahya Ali Rothan, Simulation of physical behavior of nanomaterial during freezing within a container, 2022, 36, 0217-9849, 10.1142/S0217984922501184 | |
101. | Xinglong Liu, Zahir Shah, Mohammed R. Alzahrani, Numerical modeling of nanofluid exergy loss within tube with multi-helical tapes, 2022, 137, 2190-5444, 10.1140/epjp/s13360-021-02327-6 | |
102. | Saade Abdalkareem Jasim, Ahmed M. Mohsen, Usama S. Altimari, Mustafa Z. Mahmoud, Yehya M. Ahmed, Maryam Derakhshandeh, The CH3F and CH3Cl detection by the BeO nanotube in the presence of environmental gases, 2022, 153, 0026-9247, 331, 10.1007/s00706-022-02907-x | |
103. | Tie-Hong Zhao, Zhong-Hua Shen, Yu-Ming Chu, Sharp power mean bounds for the lemniscate type means, 2021, 115, 1578-7303, 10.1007/s13398-021-01117-0 | |
104. | Nastaran Chokhachi Zadeh Moghadam, Saade Abdalkareem Jasim, Fuad Ameen, Dalal H. Alotaibi, Marcos A. L. Nobre, Hanen Sellami, Mehrdad Khatami, Nickel oxide nanoparticles synthesis using plant extract and evaluation of their antibacterial effects on Streptococcus mutans, 2022, 45, 1615-7591, 1201, 10.1007/s00449-022-02736-6 | |
105. | Tie-Hong Zhao, Wei-Mao Qian, Yu-Ming Chu, On approximating the arc lemniscate functions, 2022, 53, 0019-5588, 316, 10.1007/s13226-021-00016-9 | |
106. | Adel Almarashi, Irreversibility and thermal analysis of ferrofluid with numerical modeling, 2021, 136, 2190-5444, 10.1140/epjp/s13360-021-02106-3 | |
107. | Mohammed N. Ajour, Muhyaddin J. H. Rawa, Ahmad H. Milyani, Meicheng Li, Mahmoud M. Selim, RETRACTED ARTICLE: Nanomaterial heat transfer through a complex shaped solar system considering variable magnetic field, 2022, 2190-5509, 10.1007/s13204-021-02319-z | |
108. | Firoozeh Abolhasani Zadeh, Saade Abdalkareem Jasim, Mohammad Javed Ansari, Dmitry Olegovich Bokov, Ghulam Yasin, Lakshmi Thangavelu, Maryam Derakhshandeh, Boron carbide nanotube as targeted drug delivery system for melphalan anticancer drug, 2022, 354, 01677322, 118796, 10.1016/j.molliq.2022.118796 | |
109. | Zhongliang Shen, Shuaixian Yu, Shichuang Zheng, Taher A. Nofal, Awad Musa, Z. Li, Numerical study of multi-jet with upstream divergent ramp at supersonic cross flow, 2022, 127, 12709638, 107689, 10.1016/j.ast.2022.107689 | |
110. | Yahya Ali Rothan, Numerical investigation for augmentation of performance of solar absorber utilizing perforated tape and nanomaterial, 2022, 102, 0044-2267, 10.1002/zamm.202100542 | |
111. | Muhammad Bilal Khan, Gustavo Santos-García, Muhammad Aslam Noor, Mohamed S. Soliman, New Class of Preinvex Fuzzy Mappings and Related Inequalities, 2022, 10, 2227-7390, 3753, 10.3390/math10203753 | |
112. | Guangli Fan, Adel Almarashi, Peixi Guo, Nidal H. Abu-Hamdeh, Abdullah M. Abusorrah, R. Moradi, Comparison of convergent/divergent ramp on fuel mixing of single jet at supersonic crossflow, 2022, 120, 12709638, 107236, 10.1016/j.ast.2021.107236 | |
113. | Yahya Ali Rothan, Modeling approach for nanomaterial convective migration with inclusion of Lorentz force, 2022, 102, 0044-2267, 10.1002/zamm.202100204 | |
114. | Yinghong Qin, Numerical modeling of energy storage unit during freezing of paraffin utilizing Al2O3 nanoparticles and Y-shape fin, 2021, 44, 2352152X, 103452, 10.1016/j.est.2021.103452 | |
115. | Yahya Ali Rothan, Physical features of ferrofluid under the impact of magnetic force inside a complex domain, 2022, 36, 0217-9849, 10.1142/S0217984922500026 | |
116. | Syed Modassir Hussain, Wasim Jamshed, Amjad Ali Pasha, Mohammad Adil, Mohammad Akram, Galerkin finite element solution for electromagnetic radiative impact on viscid Williamson two-phase nanofluid flow via extendable surface, 2022, 137, 07351933, 106243, 10.1016/j.icheatmasstransfer.2022.106243 | |
117. | Musaad S. Aldhabani, Kamsing Nonlaopon, S. Rezaei, Fatimah S.Bayones, S.K. Elagan, Sobhy A.A. El-Marouf, Abundant solitary wave solutions to a perturbed Schrödinger equation with Kerr law nonlinearity via a novel approach, 2022, 35, 22113797, 105385, 10.1016/j.rinp.2022.105385 | |
118. | Xiujun Zhang, Ghulam Farid, Ayşe Kübra Demirel, Chahn Yong Jung, Muhammad Arif, ( p , h )-Convex Functions Associated with Hadamard and Fejér-Hadamard Inequalities via k -Fractional Integral Operators, 2022, 2022, 2314-8888, 1, 10.1155/2022/3832330 | |
119. | Muhammad Adil Khan, Hidayat Ullah, Tareq Saeed, Some estimations of the Jensen difference and applications, 2023, 46, 0170-4214, 5863, 10.1002/mma.8873 | |
120. | Guangli Fan, Hassan Abdulwahab Anjal, Raed Qahiti, Nidal H. Abu-Hamdeh, Abdullah M. Abusorrah, Jin Xu, Hailong Zhang, Zhixiong Li, Comparison of different lobe-injectors on fuel mixing characteristics of single jet at the supersonic combustion chamber, 2021, 119, 12709638, 107193, 10.1016/j.ast.2021.107193 | |
121. | Yahya Ali Rothan, Modeling for freezing of PCM enhanced with nano-powders within a duct, 2022, 137, 2190-5444, 10.1140/epjp/s13360-022-02505-0 | |
122. | Hamdi Ayed, Modeling of nanomaterial transportation within an enclosure with imposing external magnetic source, 2022, 2190-5509, 10.1007/s13204-021-02136-4 | |
123. | Xiaoqing Xu, Weiqi Wang, Lu Lu, Jingzheng Zhang, Jia Luo, Magnesium oxide nanotube as a promising material for detection of methamphetamine drug: theoretical study, 2022, 28, 1610-2940, 10.1007/s00894-022-05151-6 | |
124. | Muhammad Bilal Khan, Savin Treanțǎ, Mohamed S. Soliman, Generalized Preinvex Interval-Valued Functions and Related Hermite–Hadamard Type Inequalities, 2022, 14, 2073-8994, 1901, 10.3390/sym14091901 | |
125. | Li Xu, Lu Chen, Ti-Ren Huang, Monotonicity, convexity and inequalities involving zero-balanced Gaussian hypergeometric function, 2022, 7, 2473-6988, 12471, 10.3934/math.2022692 | |
126. | Bardia Mortezagholi, Emad Movahed, Amirhossein Fathi, Milad Soleimani, Armita Forutan Mirhosseini, Negar Zeini, Mehrdad Khatami, Mahin Naderifar, Bahman Abedi Kiasari, Mehran Zareanshahraki, Plant‐mediated synthesis of silver‐doped zinc oxide nanoparticles and evaluation of their antimicrobial activity against bacteria cause tooth decay, 2022, 85, 1059-910X, 3553, 10.1002/jemt.24207 | |
127. | Murad Ali Shah, Kejia Pan, Muhammad Ibrahim, Tareq Saeed, Use of neural network and machine learning in optimizing heat transfer and entropy generated in a cavity filled with nanofluid under the influence of magnetic field: A numerical study, 2022, 139, 09557997, 113, 10.1016/j.enganabound.2022.03.012 | |
128. | Ying Lai, Peng Liu, Potential application of BC3 nanotube for removal of bisphenol from water; density functional theory study, 2022, 357, 01677322, 119147, 10.1016/j.molliq.2022.119147 | |
129. | Ghassan Fadhil Smaisim, Azher M. Abed, Hayder Al-Madhhachi, Salema K. Hadrawi, Hasan Mahdi M. Al-Khateeb, Ehsan Kianfar, Graphene-Based Important Carbon Structures and Nanomaterials for Energy Storage Applications as Chemical Capacitors and Supercapacitor Electrodes: a Review, 2023, 13, 2191-1630, 219, 10.1007/s12668-022-01048-z | |
130. | Mohammed Zwawi, Treatment of ferrofluid through a sinusoidal cavity with impose of magnetic source, 2022, 2190-5509, 10.1007/s13204-022-02361-5 | |
131. | Xiao-Yong Shen, Hong-Qin Xu, M. Barzegar Gerdroodbary, S. Valiallah Mousavi, Amir Musa Abazari, S. Misagh Imani, Numerical simulation of blood flow effects on rupture of aneurysm in middle cerebral artery, 2022, 33, 0129-1831, 10.1142/S0129183122500309 | |
132. | Haiwei Yang, Yahya Ali Rothan, Saad Althobaiti, Mahmoud M. Selim, Simulation for influence of Y-shape fin on phase change of paraffin inside triplex pipe with using Al2O3 nanoparticles, 2022, 46, 2352152X, 103878, 10.1016/j.est.2021.103878 | |
133. | Menglin Qin, Sajjad Haider, Shaukat Khan, Alibek Issakhov, Mahmoud M. Selim, RETRACTED ARTICLE: Study for Lorentz force impact on irreversibility of nanomaterial with considering the permeable zone, 2022, 2190-5509, 10.1007/s13204-021-02183-x | |
134. | Menglin Qin, Bandar Almohsen, M. Sabershahraki, Alibek Issakhov, Investigation of water freezing with inclusion of nanoparticle within a container with fins, 2022, 2190-5509, 10.1007/s13204-021-02139-1 | |
135. | Saade Abdalkareem Jasim, Moaed E. Al-Gazally, Hasan Sh. Majdi, Yasir Salam Karim, Maria Jade Catalan Opulencia, Mustafa M. Kadhim, Ali Thaeer Hammid, Yasser Fakri Mustafa, Parvaneh Delir Kheirollahi Nezhad, Gallium and scandium doping effect on the sensing performance of aluminum phosphide nanotubes toward toxic ethylene oxide gas, 2022, 441, 03759601, 128145, 10.1016/j.physleta.2022.128145 | |
136. | Masoome Sadeghi, Asal Yousefi Siavoshani, Mahdiye Bazargani, Abduladheem Turki Jalil, Mojtaba Ramezani, Mohammad Reza Poor Heravi, Dichlorosilane adsorption on the Al, Ga, and Zn-doped fullerenes, 2022, 153, 0026-9247, 427, 10.1007/s00706-022-02926-8 | |
137. | Muhammad Bilal Khan, Aleksandr Rakhmangulov, Najla Aloraini, Muhammad Aslam Noor, Mohamed S. Soliman, Generalized Harmonically Convex Fuzzy-Number-Valued Mappings and Fuzzy Riemann–Liouville Fractional Integral Inequalities, 2023, 11, 2227-7390, 656, 10.3390/math11030656 | |
138. | Sagr Alamri, Ali A. Rajhi, M. Derakhshande, Potential detection of C2N2 gas by the pure, Al, and Cu-doped graphynes: a DFT study, 2022, 48, 0892-7022, 574, 10.1080/08927022.2022.2036338 | |
139. | Chuan-Yu Cai, Lu Chen, Ti-Ren Huang, Yuming Chu, New properties for the Ramanujan R-function, 2022, 20, 2391-5455, 724, 10.1515/math-2022-0045 | |
140. | Ahmad Banji Jafar, Sharidan Shafie, Imran Ullah, Rabia Safdar, Wasim Jamshed, Amjad Ali Pasha, Mustafa Mutiur Rahman, Syed M. Hussain, Aysha Rehman, El Sayed M. Tag El Din, Mohamed R. Eid, Mixed convection flow of an electrically conducting viscoelastic fluid past a vertical nonlinearly stretching sheet, 2022, 12, 2045-2322, 10.1038/s41598-022-18761-0 | |
141. | Xue-De Luan, Yi-Peng Xu, Hamdi Ayed, Mahmoud M. Selim, Heat transfer treatment of nanomaterial with considering turbulator effects, 2022, 131, 07351933, 105787, 10.1016/j.icheatmasstransfer.2021.105787 | |
142. | Yahya Ali Rothan, Investigation of hybrid nanomaterial application in melting process of paraffin enhanced with nanoparticles, 2021, 96, 0031-8949, 125253, 10.1088/1402-4896/ac3877 | |
143. | Daniyal Irfan, Maria Jade Catalan Opulencia, Saade Abdalkareem Jasim, Odilkhon R. Salimov, Ahmed B. Mahdi, Azher M. Abed, A. Sarkar, Systematically theoretical investigation the effect of nitrogen and iron-doped graphdiyne on the oxygen reduction reaction mechanism in proton exchange membrane fuel cells, 2022, 47, 03603199, 17341, 10.1016/j.ijhydene.2022.03.209 | |
144. | Menglin Qin, Adel Almarashi, Ziyad Jamil Talabany, Sajjad Haider, Shaukat Khan, Mahmoud M. Selim, Charging of phase change material layers though air heat exchanger considering TiO2 nanomaterial, 2022, 47, 2352152X, 103652, 10.1016/j.est.2021.103652 | |
145. | Xinrui Qi, Maawiya Ould Sidi, Iskander Tlili, Talib K. Ibrahim, Mohamed Abdelghany Elkotb, M.A. El-Shorbagy, Zhixiong Li, Optimization and sensitivity analysis of extended surfaces during melting and freezing of phase changing materials in cylindrical Lithium-ion battery cooling, 2022, 51, 2352152X, 104545, 10.1016/j.est.2022.104545 | |
146. | Kamsing Nonlaopon, Shahram Rezapour, Musaad S. Aldhabani, Samirah H. Alsulami, S.K. Elagan, On an efficient approach to solutions of a perturbed nonlinear Schrödinger’s equation, 2022, 39, 22113797, 105738, 10.1016/j.rinp.2022.105738 | |
147. | Syed M. Hussain, B. Shankar Goud, Prakash Madheshwaran, Wasim Jamshed, Amjad Ali Pasha, Rabia Safdar, Misbah Arshad, Rabha W. Ibrahim, Mohammad Kalimuddin Ahmad, Effectiveness of Nonuniform Heat Generation (Sink) and Thermal Characterization of a Carreau Fluid Flowing across a Nonlinear Elongating Cylinder: A Numerical Study, 2022, 7, 2470-1343, 25309, 10.1021/acsomega.2c02207 | |
148. | Omar Dheyauldeen Salahdin, Hamidreza Sayadi, Reena Solanki, Rosario Mireya Romero Parra, Mohaimen Al-Thamir, Abduladheem Turki Jalil, Samar Emad Izzat, Ali Thaeer Hammid, Luis Andres Barboza Arenas, Ehsan Kianfar, Graphene and carbon structures and nanomaterials for energy storage, 2022, 128, 0947-8396, 10.1007/s00339-022-05789-2 | |
149. | Fuzhang Wang, Rebwar Nasir Dara, Ahmed Msmali, Taher A. Nofal, Awad Musa, Nidal H. Abu-Hamdeh, Simulation for discharging of phase change material within a porous duct utilizing multi layers, 2022, 213, 09204105, 110305, 10.1016/j.petrol.2022.110305 | |
150. | Jian Wang, Wissam H. Alawee, Hayder A. Dhahad, Taher A. Nofal, Awad Musa, Ping Xu, Numerical study for solidification of water inside a storage tank considering copper oxide nanoparticles, 2022, 52, 2352152X, 104683, 10.1016/j.est.2022.104683 | |
151. | Saima Rashid, Rehana Ashraf, Fahd Jarad, Strong interaction of Jafari decomposition method with nonlinear fractional-order partial differential equations arising in plasma via the singular and nonsingular kernels, 2022, 7, 2473-6988, 7936, 10.3934/math.2022444 | |
152. | Hamed Sadeghi, Hajar Q. Alijani, Shahla Hashemi-Shahraki, Mahin Naderifar, Seyedeh-Sharifeh Rahimi, Firoozeh Abolhasani Zadeh, Siavash Iravani, Mojtaba Haghighat, Mehrdad Khatami, Iron oxyhydroxide nanoparticles: green synthesis and their cytotoxicity activity against A549 human lung adenocarcinoma cells, 2022, 33, 2037-4631, 461, 10.1007/s12210-022-01065-w | |
153. | Abeer S. Alnahdi, Saleem Nasir, Taza Gul, Couple stress ternary hybrid nanofluid flow in a contraction channel by means of drug delivery function, 2023, 03784754, 10.1016/j.matcom.2023.02.021 | |
154. | Murad Ali Shah, Kejia Pan, Muhammad Ibrahim, Tareq Saeed, Syed Ibrahim, Numerical study and optimization of important parameters of non-Newtonian nanofluid turbulent flow in a channel with triangular vortex generators using artificial neural network, 2022, 139, 09557997, 94, 10.1016/j.enganabound.2022.03.022 | |
155. | Muhammad Bilal Khan, Gustavo Santos-García, Savin Treanțǎ, Mohamed S. Soliman, New Class Up and Down Pre-Invex Fuzzy Number Valued Mappings and Related Inequalities via Fuzzy Riemann Integrals, 2022, 14, 2073-8994, 2322, 10.3390/sym14112322 | |
156. | Menglin Qin, Hamdi Ayed, Alibek Issakhov, Mahmoud M. Selim, RETRACTED ARTICLE: Modeling of nanomaterial transportation over a sheet with involving MHD effect, 2022, 2190-5509, 10.1007/s13204-021-02168-w | |
157. | Xuexiao You, Muhammad Adil Khan, Hidayat Ullah, Tareq Saeed, Improvements of Slater’s Inequality by Means of 4-Convexity and Its Applications, 2022, 10, 2227-7390, 1274, 10.3390/math10081274 | |
158. | Saade Abdalkareem Jasim, Hawraz Ibrahim M. Amin, Ahmad Rajabizadeh, Marcos Augusto Lima Nobre, Fariba Borhani, Abduladheem Turki Jalil, Marwan Mahmood Saleh, Mustafa M. Kadhim, Mehrdad Khatami, Synthesis characterization of Zn-based MOF and their application in degradation of water contaminants, 2022, 86, 0273-1223, 2303, 10.2166/wst.2022.318 | |
159. | Jun Song, Didi Wu, Mohammad Arefi, Modified couple stress and thickness-stretching included formulation of a sandwich micro shell subjected to electro-magnetic load resting on elastic foundation, 2022, 18, 22149147, 1935, 10.1016/j.dt.2022.04.015 | |
160. | Hui-Zuo Xu, Wei-Mao Qian, Yu-Ming Chu, Sharp bounds for the lemniscatic mean by the one-parameter geometric and quadratic means, 2022, 116, 1578-7303, 10.1007/s13398-021-01162-9 | |
161. | JunRu Liu, Hadi jabbari, Mustafa M. Kadhim, Mohammad Javed Ansari, Abdol Ghaffar Ebadi, Design organic material with acceptor-π-donor configuration for high performance solar cells, 2022, 1212, 2210271X, 113729, 10.1016/j.comptc.2022.113729 | |
162. | Ahmad El Askary, Basem H. Elesawy, Nasser S. Awwad, Hala A. Ibrahium, Mohd. Shkir, Different metal-decorated aluminum phosphide nanotubes as hydrazine sensors for biomedical applications, 2022, 28, 1610-2940, 10.1007/s00894-022-05102-1 | |
163. | Hamad Hassan Awan, Arshad Hussain, Muhammad Faisal Javed, Yanjun Qiu, Raid Alrowais, Abdeliazim Mustafa Mohamed, Dina Fathi, Abdullah Mossa Alzahrani, Predicting Marshall Flow and Marshall Stability of Asphalt Pavements Using Multi Expression Programming, 2022, 12, 2075-5309, 314, 10.3390/buildings12030314 | |
164. | Muhammad Bilal Khan, Hakeem A. Othman, Aleksandr Rakhmangulov, Mohamed S. Soliman, Alia M. Alzubaidi, Discussion on Fuzzy Integral Inequalities via Aumann Integrable Convex Fuzzy-Number Valued Mappings over Fuzzy Inclusion Relation, 2023, 11, 2227-7390, 1356, 10.3390/math11061356 | |
165. | Hamdi Ayed, Couple stress and Darcy Forchheimer hybrid nanofluid flow on a vertical plate by means of double diffusion Cattaneo–Christov analysis, 2023, 32, 1674-1056, 040205, 10.1088/1674-1056/ac7bfb | |
166. | Muhammad Bilal Khan, Jorge E. Macías-Díaz, Saeid Jafari, Abdulwadoud A. Maash, Mohamed S. Soliman, Pre-Invexity and Fuzzy Fractional Integral Inequalities via Fuzzy Up and Down Relation, 2023, 15, 2073-8994, 862, 10.3390/sym15040862 | |
167. | Muhammad Bilal Khan, Aziz Ur Rahman, Abdulwadoud A. Maash, Savin Treanțǎ, Mohamed S. Soliman, Some New Estimates of Fuzzy Integral Inequalities for Harmonically Convex Fuzzy-Number-Valued Mappings via up and down Fuzzy Relation, 2023, 12, 2075-1680, 365, 10.3390/axioms12040365 | |
168. | Sharif Ullah, Ikram Ullah, Amir Ali, Soret and Dufour effects on dissipative Jeffrey nanofluid flow over a curved surface with nonlinear slip, activation energy and entropy generation, 2023, 1745-5030, 1, 10.1080/17455030.2022.2164380 | |
169. | BoAn Xiao, Electrochemical sensor based on Bimetallic phosphosulfide Zn–Ni–P–S Nanocomposite -reduced graphene oxide for determination of Paraoxon Ethyl in agriculture wastewater, 2022, 17, 14523981, 220672, 10.20964/2022.06.72 | |
170. | Muhammad Bilal Khan, Eze R. Nwaeze, Cheng-Chi Lee, Hatim Ghazi Zaini, Der-Chyuan Lou, Khalil Hadi Hakami, Weighted Fractional Hermite–Hadamard Integral Inequalities for up and down Ԓ-Convex Fuzzy Mappings over Coordinates, 2023, 11, 2227-7390, 4974, 10.3390/math11244974 | |
171. | Shanhe Wu, Muhammad Adil Khan, Shah Faisal, Tareq Saeed, Eze R. Nwaeze, Derivation of Hermite-Hadamard-Jensen-Mercer conticrete inequalities for Atangana-Baleanu fractional integrals by means of majorization, 2024, 57, 2391-4661, 10.1515/dema-2024-0024 | |
172. | H.M. Srivastava, Shakir Malik, M.I. Qureshi, Bilal Bhat, Some zero-balanced terminating hypergeometric series and their applications, 2023, 37, 0354-5180, 7367, 10.2298/FIL2322367S | |
173. | Tareq Saeed, Adriana Cătaș, Muhammad Bilal Khan, Ahmed Mohammed Alshehri, Some New Fractional Inequalities for Coordinated Convexity over Convex Set Pertaining to Fuzzy-Number-Valued Settings Governed by Fractional Integrals, 2023, 7, 2504-3110, 856, 10.3390/fractalfract7120856 | |
174. | Saade Abdalkareem Jasim, Andrés Alexis Ramírez-Coronel, Ameer A. Alameri, I.B. Sapaev, Yasser Fakri Mustafa, Abduladheem Turki Jalil, Qutaiba A. Qasim, Munther Abosaooda, Phenytoin drug detection study through the B24N24 and Al24N24 nano-clusters in gas and solvent phase: DFT, TD-DFT, and thermodynamic study, 2023, 153, 13877003, 110887, 10.1016/j.inoche.2023.110887 | |
175. | Tareq Saeed, Muhammad Bilal Khan, Savin Treanță, Hamed H. Alsulami, Mohammed Sh. Alhodaly, Study of Log Convex Mappings in Fuzzy Aunnam Calculus via Fuzzy Inclusion Relation over Fuzzy-Number Space, 2023, 11, 2227-7390, 2043, 10.3390/math11092043 | |
176. | Ling Zhu, A new upper bound for the complete elliptic integral of the first kind, 2023, 117, 1578-7303, 10.1007/s13398-023-01453-3 | |
177. | Ebrahem A. Algehyne, Izharul Haq, Zehba Raizah, Fuad S. Alduais, Anwar Saeed, Ahmed M. Galal, Heat transport phenomenon of the MHD water-based hybrid nanofluid flow over a rotating disk with velocity slips, 2024, 38, 0217-9792, 10.1142/S0217979224501005 | |
178. | Chao Luo, Wanhe Yao, Xu Gao, Degradation of a Reactive Orange 16 in textile wastewater treatment using CuO/ZnO nanocomposite as photocatalyst, 2022, 17, 14523981, 220732, 10.20964/2022.07.26 | |
179. | Yajun Chen, Jiahui Wu, Tiehong Zhao, On the absolute monotonicity of generalized elliptic integral of the first kind, 2023, 117, 1578-7303, 10.1007/s13398-023-01472-0 | |
180. | Wei-Dong Jiang, Sharp inequalities for the complete elliptic integrals of the first and second kinds, 2023, 17, 1452-8630, 388, 10.2298/AADM200613020J | |
181. | Mohamed J. Saadh, Durgesh Singh, Diego Mayorga, Anjan Kumar, María Albuja, Ahmad Ismael Saber, Mohammed Ahmed Mustafa, Yasser Elmasry, Noubu Sun, The potential of 2D carbon nitride monolayer as an efficient adsorbent for capturing mercury: A DFT study, 2024, 141, 09259635, 110566, 10.1016/j.diamond.2023.110566 | |
182. | Chaoran Li, Yongjun Xiao, Jianfang Liu, Guangzhou Li, Yugao Zhu, Determination of Anabolic Steroid as Doping Agent in Serum and Urine of Athletes by Using an Electrochemical Sensor Based on the Graphene-Gold Hybrid Nanostructure, 2022, 17, 14523981, 220766, 10.20964/2022.07.70 | |
183. | Muhammad Adil Khan, Asadullah Sohail, Hidayat Ullah, Tareq Saeed, Estimations of the Jensen Gap and Their Applications Based on 6-Convexity, 2023, 11, 2227-7390, 1957, 10.3390/math11081957 | |
184. | Jiahui Wu, Tiehong Zhao, On the Absolute Monotonicity of the Logarithmic of Gaussian Hypergeometric Function, 2024, 50, 1017-060X, 10.1007/s41980-024-00889-6 | |
185. | Tie-hong Zhao, Yu-ming Chu, Sharp power-type Heronian and Lehmer means inequalities for the complete elliptic integrals, 2023, 38, 1005-1031, 467, 10.1007/s11766-023-4223-9 | |
186. | Tie-Hong Zhao, Miao-Kun Wang, Sharp double-exponent type bounds for the lemniscate sine function, 2024, 18, 1452-8630, 148, 10.2298/AADM230417005Z | |
187. | Abdul Basir, Muhammad Adil Khan, Hidayat Ullah, Yahya Almalki, Saowaluck Chasreechai, Thanin Sitthiwirattham, Derivation of Bounds for Majorization Differences by a Novel Method and Its Applications in Information Theory, 2023, 12, 2075-1680, 885, 10.3390/axioms12090885 | |
188. | Zhiyang Liu, Yan Liu, Zhongyu Tan, Ying Liu, Linglong Meng, Sheng Yang, Electrochemical Determination of Rutin in Herbal Samples Using CuO/CNT composite Modified Glassy Carbon Electrode, 2022, 17, 14523981, 220724, 10.20964/2022.07.22 | |
189. | Ziyi Wang, Yumang Zhang, Synthesis of Pt/GO composite as an electrochemical sensor for determination of synthetic corticosteroid triamcinolone as doping agents in sports, 2022, 17, 14523981, 220769, 10.20964/2022.07.67 | |
190. | Muhammad Bilal Khan, Ali Althobaiti, Cheng-Chi Lee, Mohamed S. Soliman, Chun-Ta Li, Some New Properties of Convex Fuzzy-Number-Valued Mappings on Coordinates Using Up and Down Fuzzy Relations and Related Inequalities, 2023, 11, 2227-7390, 2851, 10.3390/math11132851 | |
191. | Zaid Mohammed Mohammed Mahdi Sayed, Muhammad Adil Khan, Shahid Khan, Josip Pecaric, Refinement of the classical Jensen inequality using finite sequences, 2024, 53, 2651-477X, 608, 10.15672/hujms.1270585 | |
192. | Fenzhao Liu, Hydrothermal Synthesis and Electrochemical Properties of LiNi0.8Co0.2-xMgxO2 Cathode Material for Lithium Ion Batteries, 2022, 17, 14523981, 220742, 10.20964/2022.07.36 | |
193. | Tareq Saeed, Muhammad Adil Khan, Shah Faisal, Hamed H. Alsulami, Mohammed Sh. Alhodaly, New conticrete inequalities of the Hermite-Hadamard-Jensen-Mercer type in terms of generalized conformable fractional operators via majorization, 2023, 56, 2391-4661, 10.1515/dema-2022-0225 | |
194. | Chen Hai-sheng, Zhu Ye-cheng, Optimal power-type Heronian and Lehmer means inequalities for the complete elliptic integrals, 2024, 1065-2469, 1, 10.1080/10652469.2024.2392281 | |
195. | Muhammad Adil Khan, Hidayat Ullah, Tareq Saeed, Zaid M. M. M. Sayed, Salha Alshaikey, Emad E. Mahmoud, Daniel Maria Busiello, Determination of Novel Estimations for the Slater Difference and Applications, 2024, 2024, 1099-0526, 1, 10.1155/2024/8481103 | |
196. | Muhammad Bilal Khan, Jorge E. Macías-Díaz, Ali Althobaiti, Saad Althobaiti, Some New Properties of Exponential Trigonometric Convex Functions Using up and down Relations over Fuzzy Numbers and Related Inequalities through Fuzzy Fractional Integral Operators Having Exponential Kernels, 2023, 7, 2504-3110, 567, 10.3390/fractalfract7070567 | |
197. | Jiahui Wu, Tiehong Zhao, On the power series related to zero-balanced hypergeometric function, 2025, 0019-5588, 10.1007/s13226-025-00768-8 |