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Oscillation of first order linear differential equations with several non-monotone delays

  • E.R. Attia , V. Benekas , H.A. El-Morshedy and I.P. Stavroulakis EMAIL logo
Published/Copyright: February 23, 2018

Abstract

Consider the first-order linear differential equation with several retarded arguments

x(t)+k=1npk(t)x(τk(t))=0,tt0,

where the functions pk, τkC([t0, ∞), ℝ+), τk(t) < t for tt0 and limt→∞τk(t) = ∞, for every k = 1, 2, …, n. Oscillation conditions which essentially improve known results in the literature are established. An example illustrating the results is given.

MSC 2010: 34K11; 34K06

1 Introduction

This paper is concerned with the oscillation of the first order differential equation with several delays of the form

x(t)+k=1npk(t)x(τk(t))=0,tt0,(1)

where pk, τkC([t0, ∞), [0, ∞)), such that τk(t)<tandlimtτk(t)=,k = 1, 2, …, n.

Let T0 ∈ [t0, ∞), τ (t) = min{τk(t) : k = 1, …, n} and τ(−1)(t) = inf{τ (s) : st}. By a solution of Eq. (1) we understand a function xC([t0, ∞), ℝ) continuously differentiable on [τ(−1)(t0), ∞) which satisfies (1) for tτ(−1)(t0). Such a solution is called oscillatory if it has arbitrarily large zeros, and otherwise it is called nonoscillatory.

We assume throughout this work that there exist t1t0, a family of nondecreasing continuous functions {gk(t)}k=1n and a nondecreasing continuous function g(t) such that

τk(t)gk(t)g(t)t,tt1,k=1,2,...,n.

To simplify the notations, we denote by λ (ξ) the smaller root of the equation eξλ = λ, ξ ≥ 0 and

c(ξ)=1ξ12ξξ22,0ξ1e.

Next, we mention some known oscillation criteria for Eq. (1).

In the case that the arguments τk(t) are monotone the following sufficient oscillation conditions have been established. In 1978, Ladde [1] and in 1982 Ladas and Stavroulakis [2] obtained the sufficient oscillatory criterion

lim inftτmax(t)tk=1npk(s)ds>1e,

where τmax(t)=max1kn{τk(t)}.

In 1984, Hunt and Yorke [3] established the condition

lim inftk=1npk(t)(tτk(t))>1e,

where (tτk(t)) ≤ τ0, for some τ0 > 0, 1 ≤ kn.

Also, in 1984, Fukagai and Kusano [4] established the following result.

Assume that there is a continuous nondecreasing functionτ (t)such thatτk(t) ≤ τ (t) ≤ tfortt0, 1 ≤ kn. If

lim inftτ(t)tk=1npk(s)ds>1e,(2)

then all solutions of Eq. (1)oscillate. If, on the other hand, there exists a continuous nondecreasing functionτ (t) such thatτ (t) ≤ τk(t) fortt0, 1 ≤ kn, limt→∞τ (t) = ∞ andfor all sufficiently larget,

τ(t)tk=1npk(s)ds1e,

thenEq.(1)has a non-oscillatory solution.

In 2003, Grammatikopoulos, Koplatadze and Stavroulakis [5] improved the above results as follows:

Assume that the functionsτkare nondecreasing for allk ∈ {1, …, n,

0pi(t)pj(t)dt<+,i,j=1,...,n,

and

lim inftτk(t)tpk(s)ds>0,k=1,...,n.

If

k=1nlim inftτk(t)tpk(s)ds>1e,

then all solutions of Eq. (1)oscillate.

In the case of non-monotone arguments we mention the following known oscillation results. In 2015 Infante, Koplatadze and Stavroulakis [6] obtained the following sufficient oscillation conditions:

lim suptj=1ni=1ngj(t)tpi(s)exp(τi(s)gi(t)k=1npk(u)exp(τk(u)u=1np(v)dv)du)ds1n>1nn,

and

lim supϵ0+lim suptj=1ni=1ngj(t)tpi(s)exp(τi(s)gi(t)k=1n(λ(qk)ϵ)pk(u)du)ds1n>1nn,(3)

where

qk=lim inftτk(t)tpk(s)ds>0,k=1,2,...,n.(4)

Also, in 2015 Koplatadze [7] derived the following three conditions. The first one takes the form

lim suptj=1ni=1ngj(t)tpi(s)exp(nτi(s)gi(t)=1np(ξ)1nψk(ξ)dξ)ds1n>1nn1i=1nc(βi),

where k ∈ ℕ and

ψ1(t)=0,ψi(t)=expk=1nτk(t)t=1np(s)1nψi1(s)ds,i=2,3,...,

and

βi=lim inftgi(t)tpi(s)ds,i=1,2,...,n.(5)

The second condition is

lim suptj=1ni=1ngj(t)tpi(s)exp(n(λ(p¯)ϵ)τi(s)gi(t)=1np(ξ)1ndξ)ds1n>1nn1=1nc(β),

where ϵ ∈ (0, λ ()), and

0<p¯:=lim infti=1nτi(t)t=1np(s)1nds1e.

The third condition is

lim suptj=1ni=1ngj(t)tpi(s)τi(s)gi(t)=1np(ξ)1ndξds1n>0,(6)

and p¯>1e.

In 2016, Braverman, Chatzarakis and Stavroulakis [8] obtained the sufficient condition

lim supth(t)ti=1npi(u)ar(h(t),τi(u))du>1,

where

h(t)=max1inhi(t),and hi(t)=supt0stτi(s),i=1,2,...,n,(7)

and

a1(t,s)=expsti=1npi(u)du,ar+1(t,s)=expsti=1npi(u)ar(u,τi(u))du,rN.

Also, in 2016 Akca, Chatzarakis and Stavroulakis [9] obtained the sufficient condition

lim supth(t)ti=1npi(u)ar(h(u),τi(u))du>1+ln(λ(α))λ(α),(8)

where

0<α:=lim inftτmax(t)ti=1npi(s)ds1e.

2 Main results

To obtain our main results we need the following lemmas:

Lemma 2.1

([6]). Let x(t) be an eventually positive solution of Eq. (1). Then

lim inftx(τk(t))x(t)λ(qk),k=1,2,...,n,

whereqkis defined by(4).

Lemma 2.2

([10]). Assume that

lim inftg(t)tP(s)ds=α,

andx(t) is an eventually positive solution of the first order delay differential inequality

x(t)+P(t)x(g(t))0,tt1,

wherePC([t1, ∞), [0, ∞)). If 0 ≤ α*1e, then

lim inftx(t)x(g(t))c(α).

Theorem 2.3

Assume that

ρ:=lim inftg(t)tk=1npk(s)ds,0<ρ1e,

and

lim supt(g(t)tQ(v)dv+c(ρ)eg(t)ti=1npi(s)ds)>1,(9)

where

Q(t)=k=1ni=1npi(t)τi(t)tpk(s)egk(t)tj=1npj(v)dv+λ(ρ)ϵτk(s)gk(t)=1np(u)duds,

andϵ ∈ (0, λ (ρ)). Then all solutions of Eq.(1)are oscillatory.

Proof

Assume the contrary, i.e., there exists a nonoscillatory solution x(t) of (1). Because of the linearity of (1), we assume that x(t) is eventually positive. Therefore, there exists a sufficiently large t2t1 such that x(τk(t)) > 0, for all tt2, k = 1, 2, …, n. Thus, equation (1) implies that x(t) is nonincreasing for all tt2. Integrating (1) from τi(t) to t, we obtain

x(t)x(τi(t))+k=1nτi(t)tpk(s)x(τk(s))ds=0.(10)

Also, dividing (1) by x(t) and integrating the resulting equation from τk(s) to gk(t), we get

x(τk(s))=x(gk(t))eτk(s)gk(t)=1np(u)x(τ(u))x(u)du.

Substituting this into (10),

x(t)x(τi(t))+k=1nx(gk(t))τi(t)tpk(s)eτk(s)gk(t)=1np(u)x(τ(u))x(u)duds=0.

Multiplying the above equation by pi(t), and taking the sum over i, it follows that

x(t)+x(t)i=1npi(t)+k=1nx(gk(t))i=1npi(t)τi(t)tpk(s)eτk(s)gk(t)=1np(u)x(τ(u))x(u)duds=0.

The substitution y(t)=et0t=1np(s)dsx(t), reduces this equation to

y(t)+k=1ny(gk(t))egk(t)t=1np(s)dsi=1npi(t)τi(t)tpk(s)eτk(s)gk(t)=1np(u)x(τ(u))x(u)duds=0,(11)

which in turn, by integrating from g(t) to t, leads to

y(t)y(g(t))+g(t)tk=1ny(gk(v))egk(v)v=1np(s)dsi=1npi(v)τi(v)vpk(s)eτk(s)gk(v)=1np(u)x(τ(u))x(u)dudsdv=0.

Hence, the nonincreasing nature of y(t) implies that

y(t)y(g(t))+y(g(t))g(t)tk=1negk(v)v=1np(s)dsi=1npi(v)τi(v)vpk(s)eτk(s)gk(v)=1np(u)x(τ(u))x(u)dudsdv0,(12)

for all tt3 and some t3t2.

On the other hand, using the nonincreasing nature of x(t), equation (1) implies that

x(t)+x(g(t))k=1npk(t)0, for all tt3.(13)

Therefore, from [11, Lemma 2.1.2], we obtain lim inftx(g(t))x(t)λ(ρ). Thus, for sufficiently small ϵ > 0, we have

x(τ(t))x(t)x(g(t))x(t)>λ(ρ)ϵ, for all tt4,1n,(14)

for some t4t3. This together with (12) implies that

y(t)y(g(t))+y(g(t))g(t)tk=1negk(v)v=1np(s)dsi=1npi(v)τi(v)vpk(s)eλ(ρ)ϵτk(s)gk(v)=1np(u)dudsdv0,

for all tt5, where t5t4. That is

g(t)tk=1negk(v)v=1np(s)dsi=1npi(v)τi(v)vpk(s)eλ(ρ)ϵτk(s)gk(v)=1np(u)dudsdv1y(t)y(g(t)),(15)

for all tt5. Also, in view of Lemma 2.2, for sufficiently small ϵ > 0 and some t6t5, inequality (13) leads to

x(t)x(g(t))>c(ρ)ϵ, for all tt6.

Therefore,

y(t)y(g(t))=x(t)x(g(t))eg(t)ti=1npi(s)ds>c(ρ)ϵeg(t)ti=1npi(s)ds, for all tt6.

Combining this inequality with (15), it follows that

g(t)tQ(v)dv1c(ρ)ϵeg(t)ti=1npi(s)ds, for all tt6.

Then

lim suptg(t)tQ(v)dv+c(ρ)eg(t)ti=1npi(s)ds1+ϵlim supteg(t)ti=1npi(s)ds.(16)

Notice that, by integrating (13) from g(t) to t and using the nonincreasing nature of x(t), we obtain

g(t)tk=1npk(s)ds1x(t)x(g(t))1, for all tt3.

Now, letting ϵ → 0 in (16), we arrive at a contradiction with (9). The proof is complete. □

Remark 2.4

Theorem 2.3 is proved using the core idea of the proof of [12, Theorem 2.1] which is given for Equation (1) when n = 1. However, Theorem 2.3 produces a new oscillation criterion even for equations with only one non-monotone delay.

Using Lemma 2.1 instead of [11, Lemma 2.1.2], similar reasoning as in the proof of Theorem 2.3 implies the following result:

Theorem 2.5

Assume that

lim supt(g(t)tQ1(v)dv+c(ρ)eg(t)ti=1npi(s)ds)>1,

where

Q1(t)=k=1ni=1npi(t)τi(t)tpk(s)egk(t)tj=1npj(v)dv+τk(s)gk(t)=1nλ(q)ϵp(u)duds,

q is defined by (4), ρ is defined as in Theorem 2.3 and ϵ ∈ (0, λ (q)). Then all solutions of Equation (1) oscillate.

Theorem 2.6

Assume that

lim suptj=1nk=1ngj(t)tRk(s)ds1n+k=1nc(βk)nnek=1ngk(t)t=1np(s)ds>1nn,

where βk is defined by (5) with 0 < βk1eand

Rk(s)=egk(s)sj=1npj(u)dui=1npi(s)τi(s)spk(u)e(λ(ρ)ϵ)τk(u)gk(s)=1np(v)dvdu,

ρ is defined as in Theorem 2.3 and ϵ ∈ (0, λ(ρ )). Then all solutions of Equation (1) oscillate.

Proof

Let x(t) be a nonoscillatory solution of (1). As usual, we assume that x(t) is an eventually positive solution. Substituting (14) into (11), we obtain

y(t)+k=1ny(gk(t))egk(t)tj=1npj(s)dsi=1npi(t)τi(t)tpk(s)e(λ(ρ)ϵ)τk(s)gk(t)=1np(u)duds0,

for all tt2 and some t2t1 where ϵ ∈ (0, λ (ρ)) and y(t)=et0t=1np(s)dsx(t) Integrating from gj(t) to t and using the nonincreasing nature of y(t), we obtain

y(t)y(gj(t))+k=1ny(gk(t))gj(t)tRk(s)ds0, for all tt3,

and some t3t2. Using the relation between arithmetic and geometric mean, it follows that

y(gj(t))nk=1ny(gk(t))1nk=1ngj(t)tRk(s)ds1n+y(t), for all tt3.

Taking the product on both sides,

j=1ny(gj(t))nnk=1ny(gk(t))j=1nk=1ngj(t)tRk(s)ds1n+y(t)n, for all tt3.

Therefore,

j=1nk=1ngj(t)tRk(s)ds1n+y(t)nnnk=1ny(gk(t))1nn, for all tt3.(17)

Since y(t)=et0t=1np(s)dsx(t), then

y(t)nk=1ny(gk(t))=ek=1ngk(t)t=1np(s)dsx(t)nk=1nx(gk(t)).

Substituting in (17),

j=1nk=1ngj(t)tRk(s)ds1n+ek=1ngk(t)t=1np(s)dsx(t)nnnk=1nx(gk(t))1nn, for all tt3.(18)

On the other hand, the nonincreasing nature of x(t) and (1) imply that

x(t)+pk(t)x(gk(t))0, for all tt3,k=1,2,...,n,(19)

and hence, by Lemma 2.2, it follows that

x(t)nk=1nx(gk(t))>k=1nc(βk)ϵ, for all tt4,

for some t4t3 and sufficiently small ϵ > 0. This together with (18) leads to

j=1nk=1ngj(t)tRk(s)ds1n+k=1nc(βk)nnek=1ngk(t)t=1np(s)ds1nn+ϵnnek=1ngk(t)t=1np(s)ds,

for all tt4. Consequently,

lim suptj=1nk=1ngj(t)tRk(s)ds1n+k=1nc(βk)nnek=1ngk(t)t=1np(s)ds1nn+ϵnnlim suptek=1ngk(t)t=1np(s)ds.(20)

On the other hand, integrating (1) from gk(t) to t, we get

x(t)x(gk(t))+gk(t)t=1nx(τ(s))p(s)ds=0,k=1,2,...,n.

Then, using the nonincreasing nature of x(t), we obtain

gk(t)t=1np(s)dsx(gk(t))x(t)1, for all tt3,k=1,2,...,n.

But applying Lemma 2.2 to (19), we obtain

lim suptx(gk(t))x(t)<+,k=1,2,...,n.

Therefore, ek=1ngk(t)t=1np(s)ds is bounded. Now, allowing ϵ → 0 in (20), it follows that

lim suptj=1nk=1ngj(t)tRk(s)ds1n+k=1nc(βk)nnek=1ngk(t)t=1np(s)ds1nn.

This contradiction completes the proof. □

The following example shows that Theorem 2.3 can be applied but conditions (2), (3) and (6) fail to apply as well as (8) when r = 1.

Example 2.7

Consider the first order delay differential equation

x(t)+a(b+sin(t))xtπ2+a(b+cos(t))xτ¯(t)=0,t0,(21)

wherea=0.41.137π+2,b=1.784and

τ¯(t)=tπ2σsin2(300t),σ=1150.

Clearly

tπ2στ¯(t)tπ2.
Fig. 1
Fig. 1

Equation (21) has the form (1) with p1(t) = a(b + sin (t)), p2(t) = a(b + cos (t)), τ1(t) = tπ2and τ2(t) = tπ2σ sin2(300t). Therefore, we can choose g1(t) = g2(t) = g(t) = tπ2and ϵ = 0.001. Then

g(t)tk=12pk(s)ds=abπ+2asin(t).

Consequently,

ρ=lim inftg(t)tk=12pk(s)ds=abπ2a0.2891659465,c(ρ)=1ρ12ρρ220.06470619,andλ(ρ)ϵ1.577422807.

LetI(t)=g(t)tQ(v)dv+c(ρ)eg(t)ti=12pi(s)ds.Then, the property that ex ≥ ex for x ≥ 0 leads to

I(t)eg(t)ti=12pi(v)g(v)vk=12pk(s)(g(v)v=12p(s)ds+λ(ρ)ϵg(s)g(v)l=12pl(u)du)dsdv+c(ρ)eg(t)ti=12pi(s)ds.

Now, using Maple, we get

I(t)0.49727+0.0029516sin(t)cos2(t)+0.27514sin(t)0.23059cos(t)0.015664cos2(t)0.083083cos(t)sin(t)+0.0037423cos3(t)+0.10144e0.16044sin(t).

ChooseTk=3π4+2πk,then

I(Tk)1.0019>1,forallkN,

which means that

lim supt(g(t)tQ(v)dv+c(ρ)eg(t)ti=12pi(s)ds)>1.

That is, condition (9) of Theorem 2.3 is satisfied and therefore all solutions of Eq. (21) oscillate.

We will show, however, that none of the conditions (2), (3), (6), and (8) (with r = 1) is satisfied. Indeed, notice that

τ(t)tk=12pk(s)dstπ2tk=12pk(s)ds=abπ+2asin(t).

Hence,

lim inftτ(t)tk=12pk(s)dsabπ2a0.2891659465<1e.

On the other hand, since h(t) = g(t), pi(t) ≤ a(b+1) for i = 1, 2, where h(t) is defined by (7), we have

a1(h(s),τi(s))=expτi(s)g(s)i=12pi(u)duexpsπ2σsπ2i=12pi(u)duexpsπ2σsπ22a(b+1)du=exp(2a(b+1)σ).

Therefore,

h(t)ti=12pi(s)a1(h(s),τi(s))dstπ2ta(b+sin(s)+b+cos(s))exp2a(b+1)σds=tπ2t2abds+tπ2tasin(s)ds+tπ2tacos(s)dsexp2a(b+1)σ=[abπ+2asin(t)]exp2a(b+1)σabπ+2aexp2a(b+1)σ<0.61188.

Since λ (ρ) ≈ 1.578422807, then

1+ln(λ(ρ))λ(ρ)>0.92.

Therefore, none of conditions (2) and (8) (with r = 1) is satisfied.

Also, since

g(t)ta(b+sin(s))ds=abπ2+a(sin(t)cos(t)),

and

τ¯(t)ta(b+cos(s))dstπ2σta(b+cos(s))dsa(b+1)tπ2σtπ2ds+tπ2ta(b+cos(s))ds=aσ(b+1)+abπ2+a(cos(t)+sin(t)).

Then, q1=abπ2a2andq2abπ2a2+aσ(b+1),where qi is defined by (4), i = 1, 2. Therefore, λ (q1) ≈ 1.134680932 and λ (q2) ≈ 1.136881841. Let

I1(t)=j=12i=12gj(t)tpi(s)exp(τi(s)gi(t)k=12(λ(qk)ϵ)pk(u)du)ds12.

Then

I1(t)<j=12i=12gj(t)tpi(s)exp(λ(q2)τi(s)gi(t)l=12pl(u)du)ds12j=12i=12gj(t)tpi(s)exp(2aλ(q2)(1+b)(ts+σ))ds12i=12tπ2σtpi(s)exp(2aλ(q2)(1+b)(ts+σ))dsi=12[tπ2σtπ2a(b+1)exp(2aλ(q2)(1+b)(ts+σ))ds+tπ2tpi(s)exp(2aλ(q2)(1+b)(ts+σ))ds]0.1363159006+0.08561813338sin(t)0.00925235722cos(t)0.02983977134cos2(t)0.00652549885sin(t)cos(t)<0.23771189<14.

Therefore, lim supϵ0+lim suptI1(t)<14,which implies that condition (3) is not satisfied.

Finally, since

i=12τi(t)tl=12pl(s)12dsi=1212τi(t)tl=12pl(s)ds12tπ2tl=12pl(s)ds+12tπ2σtl=12pl(s)ds=12tπ2tl=12pl(s)ds+12tπ2σtπ2l=12pl(s)ds+tπ2tl=12pl(s)dstπ2tl=12pl(s)ds+tπ2σtπ2a(b+1)dstπ2tl=12pl(s)ds+aσ(b+1),

then

p¯=lim infti=12τi(t)tl=12pl(s)12dsabπ2a+aσ(b+1)<0.2906549<1e.

Therefore, condition (6) fails to apply.

Acknowledgement

The authors would like to thank the referees for their valuable comments and suggestions.

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Received: 2017-05-30
Accepted: 2018-01-17
Published Online: 2018-02-23

© 2018 Attia et al., published by De Gruyter

This work is licensed under the Creative Commons Attribution-NonCommercial-NoDerivatives 4.0 License.

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  2. Algebraic proofs for shallow water bi–Hamiltonian systems for three cocycle of the semi-direct product of Kac–Moody and Virasoro Lie algebras
  3. On a viscous two-fluid channel flow including evaporation
  4. Generation of pseudo-random numbers with the use of inverse chaotic transformation
  5. Singular Cauchy problem for the general Euler-Poisson-Darboux equation
  6. Ternary and n-ary f-distributive structures
  7. On the fine Simpson moduli spaces of 1-dimensional sheaves supported on plane quartics
  8. Evaluation of integrals with hypergeometric and logarithmic functions
  9. Bounded solutions of self-adjoint second order linear difference equations with periodic coeffients
  10. Oscillation of first order linear differential equations with several non-monotone delays
  11. Existence and regularity of mild solutions in some interpolation spaces for functional partial differential equations with nonlocal initial conditions
  12. The log-concavity of the q-derangement numbers of type B
  13. Generalized state maps and states on pseudo equality algebras
  14. Monotone subsequence via ultrapower
  15. Note on group irregularity strength of disconnected graphs
  16. On the security of the Courtois-Finiasz-Sendrier signature
  17. A further study on ordered regular equivalence relations in ordered semihypergroups
  18. On the structure vector field of a real hypersurface in complex quadric
  19. Rank relations between a {0, 1}-matrix and its complement
  20. Lie n superderivations and generalized Lie n superderivations of superalgebras
  21. Time parallelization scheme with an adaptive time step size for solving stiff initial value problems
  22. Stability problems and numerical integration on the Lie group SO(3) × R3 × R3
  23. On some fixed point results for (s, p, α)-contractive mappings in b-metric-like spaces and applications to integral equations
  24. On algebraic characterization of SSC of the Jahangir’s graph 𝓙n,m
  25. A greedy algorithm for interval greedoids
  26. On nonlinear evolution equation of second order in Banach spaces
  27. A primal-dual approach of weak vector equilibrium problems
  28. On new strong versions of Browder type theorems
  29. A Geršgorin-type eigenvalue localization set with n parameters for stochastic matrices
  30. Restriction conditions on PL(7, 2) codes (3 ≤ |𝓖i| ≤ 7)
  31. Singular integrals with variable kernel and fractional differentiation in homogeneous Morrey-Herz-type Hardy spaces with variable exponents
  32. Introduction to disoriented knot theory
  33. Restricted triangulation on circulant graphs
  34. Boundedness control sets for linear systems on Lie groups
  35. Chen’s inequalities for submanifolds in (κ, μ)-contact space form with a semi-symmetric metric connection
  36. Disjointed sum of products by a novel technique of orthogonalizing ORing
  37. A parametric linearizing approach for quadratically inequality constrained quadratic programs
  38. Generalizations of Steffensen’s inequality via the extension of Montgomery identity
  39. Vector fields satisfying the barycenter property
  40. On the freeness of hypersurface arrangements consisting of hyperplanes and spheres
  41. Biderivations of the higher rank Witt algebra without anti-symmetric condition
  42. Some remarks on spectra of nuclear operators
  43. Recursive interpolating sequences
  44. Involutory biquandles and singular knots and links
  45. Constacyclic codes over 𝔽pm[u1, u2,⋯,uk]/〈 ui2 = ui, uiuj = ujui
  46. Topological entropy for positively weak measure expansive shadowable maps
  47. Oscillation and non-oscillation of half-linear differential equations with coeffcients determined by functions having mean values
  48. On 𝓠-regular semigroups
  49. One kind power mean of the hybrid Gauss sums
  50. A reduced space branch and bound algorithm for a class of sum of ratios problems
  51. Some recurrence formulas for the Hermite polynomials and their squares
  52. A relaxed block splitting preconditioner for complex symmetric indefinite linear systems
  53. On f - prime radical in ordered semigroups
  54. Positive solutions of semipositone singular fractional differential systems with a parameter and integral boundary conditions
  55. Disjoint hypercyclicity equals disjoint supercyclicity for families of Taylor-type operators
  56. A stochastic differential game of low carbon technology sharing in collaborative innovation system of superior enterprises and inferior enterprises under uncertain environment
  57. Dynamic behavior analysis of a prey-predator model with ratio-dependent Monod-Haldane functional response
  58. The points and diameters of quantales
  59. Directed colimits of some flatness properties and purity of epimorphisms in S-posets
  60. Super (a, d)-H-antimagic labeling of subdivided graphs
  61. On the power sum problem of Lucas polynomials and its divisible property
  62. Existence of solutions for a shear thickening fluid-particle system with non-Newtonian potential
  63. On generalized P-reducible Finsler manifolds
  64. On Banach and Kuratowski Theorem, K-Lusin sets and strong sequences
  65. On the boundedness of square function generated by the Bessel differential operator in weighted Lebesque Lp,α spaces
  66. On the different kinds of separability of the space of Borel functions
  67. Curves in the Lorentz-Minkowski plane: elasticae, catenaries and grim-reapers
  68. Functional analysis method for the M/G/1 queueing model with single working vacation
  69. Existence of asymptotically periodic solutions for semilinear evolution equations with nonlocal initial conditions
  70. The existence of solutions to certain type of nonlinear difference-differential equations
  71. Domination in 4-regular Knödel graphs
  72. Stepanov-like pseudo almost periodic functions on time scales and applications to dynamic equations with delay
  73. Algebras of right ample semigroups
  74. Random attractors for stochastic retarded reaction-diffusion equations with multiplicative white noise on unbounded domains
  75. Nontrivial periodic solutions to delay difference equations via Morse theory
  76. A note on the three-way generalization of the Jordan canonical form
  77. On some varieties of ai-semirings satisfying xp+1x
  78. Abstract-valued Orlicz spaces of range-varying type
  79. On the recursive properties of one kind hybrid power mean involving two-term exponential sums and Gauss sums
  80. Arithmetic of generalized Dedekind sums and their modularity
  81. Multipreconditioned GMRES for simulating stochastic automata networks
  82. Regularization and error estimates for an inverse heat problem under the conformable derivative
  83. Transitivity of the εm-relation on (m-idempotent) hyperrings
  84. Learning Bayesian networks based on bi-velocity discrete particle swarm optimization with mutation operator
  85. Simultaneous prediction in the generalized linear model
  86. Two asymptotic expansions for gamma function developed by Windschitl’s formula
  87. State maps on semihoops
  88. 𝓜𝓝-convergence and lim-inf𝓜-convergence in partially ordered sets
  89. Stability and convergence of a local discontinuous Galerkin finite element method for the general Lax equation
  90. New topology in residuated lattices
  91. Optimality and duality in set-valued optimization utilizing limit sets
  92. An improved Schwarz Lemma at the boundary
  93. Initial layer problem of the Boussinesq system for Rayleigh-Bénard convection with infinite Prandtl number limit
  94. Toeplitz matrices whose elements are coefficients of Bazilevič functions
  95. Epi-mild normality
  96. Nonlinear elastic beam problems with the parameter near resonance
  97. Orlicz difference bodies
  98. The Picard group of Brauer-Severi varieties
  99. Galoisian and qualitative approaches to linear Polyanin-Zaitsev vector fields
  100. Weak group inverse
  101. Infinite growth of solutions of second order complex differential equation
  102. Semi-Hurewicz-Type properties in ditopological texture spaces
  103. Chaos and bifurcation in the controlled chaotic system
  104. Translatability and translatable semigroups
  105. Sharp bounds for partition dimension of generalized Möbius ladders
  106. Uniqueness theorems for L-functions in the extended Selberg class
  107. An effective algorithm for globally solving quadratic programs using parametric linearization technique
  108. Bounds of Strong EMT Strength for certain Subdivision of Star and Bistar
  109. On categorical aspects of S -quantales
  110. On the algebraicity of coefficients of half-integral weight mock modular forms
  111. Dunkl analogue of Szász-mirakjan operators of blending type
  112. Majorization, “useful” Csiszár divergence and “useful” Zipf-Mandelbrot law
  113. Global stability of a distributed delayed viral model with general incidence rate
  114. Analyzing a generalized pest-natural enemy model with nonlinear impulsive control
  115. Boundary value problems of a discrete generalized beam equation via variational methods
  116. Common fixed point theorem of six self-mappings in Menger spaces using (CLRST) property
  117. Periodic and subharmonic solutions for a 2nth-order p-Laplacian difference equation containing both advances and retardations
  118. Spectrum of free-form Sudoku graphs
  119. Regularity of fuzzy convergence spaces
  120. The well-posedness of solution to a compressible non-Newtonian fluid with self-gravitational potential
  121. On further refinements for Young inequalities
  122. Pretty good state transfer on 1-sum of star graphs
  123. On a conjecture about generalized Q-recurrence
  124. Univariate approximating schemes and their non-tensor product generalization
  125. Multi-term fractional differential equations with nonlocal boundary conditions
  126. Homoclinic and heteroclinic solutions to a hepatitis C evolution model
  127. Regularity of one-sided multilinear fractional maximal functions
  128. Galois connections between sets of paths and closure operators in simple graphs
  129. KGSA: A Gravitational Search Algorithm for Multimodal Optimization based on K-Means Niching Technique and a Novel Elitism Strategy
  130. θ-type Calderón-Zygmund Operators and Commutators in Variable Exponents Herz space
  131. An integral that counts the zeros of a function
  132. On rough sets induced by fuzzy relations approach in semigroups
  133. Computational uncertainty quantification for random non-autonomous second order linear differential equations via adapted gPC: a comparative case study with random Fröbenius method and Monte Carlo simulation
  134. The fourth order strongly noncanonical operators
  135. Topical Issue on Cyber-security Mathematics
  136. Review of Cryptographic Schemes applied to Remote Electronic Voting systems: remaining challenges and the upcoming post-quantum paradigm
  137. Linearity in decimation-based generators: an improved cryptanalysis on the shrinking generator
  138. On dynamic network security: A random decentering algorithm on graphs
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