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Non-occurrence of the Lavrentiev phenomenon for a class of convex nonautonomous Lagrangians

  • Carlo Mariconda ORCID logo EMAIL logo and Giulia Treu
Published/Copyright: February 17, 2020

Abstract

We consider the classical functional of the Calculus of Variations of the form

I(u)=ΩF(x,u(x),u(x))dx,

where Ω is a bounded open subset of ℝn and F : Ω × ℝ × ℝn → ℝ is a Carathéodory convex function; the admissible functions u coincide with a prescribed Lipschitz function ϕ on ∂Ω. We formulate some conditions under which a given function in ϕ + W01,p (Ω) with I(u) < +∞ can be approximated in the W1,p norm and in energy by a sequence of smooth functions that coincide with ϕ on ∂Ω. As a particular case we obtain that the Lavrentiev phenomenon does not occur when F(x, u, ξ) = f(x, u) + h(x, ξ) is convex and xF(x, 0, 0) is sufficiently smooth.

1 Introduction

In 1927, Lavrentiev [1] provided an example of the fact, later called the Lavrentiev phenomenon, that the infimum, over the set of absolutely continuous functions, of a one-dimensional functional of the calculus of variations may be strictly lower than the infimum of the same functional over the set of Lipschitz functions satisfying the same boundary conditions: the example was refined by Manià in [2] and, more recently, by Ball-Mizel in [3]. Finding the conditions that ensure the non-occurrence of the Lavrentiev phenomenon has some interest, if just for ensuring to catch the infimum of the functional via standard numerical methods. We point out that some authors refer to as the Lavrentiev phenomenon just the fact that the infima among the two aforementioned classes of functions differ without taking care the boundary datum. If one allows the boundary datum to vary, things change dramatically: in Lavrentiev’s celebrated example itself the infima among Lipschitz/absolutely functions are the same if one allows one boundary datum to be just arbitrarily close to the initial one. Some recent results concerning the study of this kind of “local” Lavrentiev phenomenon have been recently obtained in [4, Theorem 4].

Alberti and Serra Cassano proved in [5] that, when the integration set is an interval in ℝ, the phenomenon does not occur for autonomous Lagrangians. For scalar problems, where the domain is multi-dimensional, few results appeared in the literature. Of course, the problem becomes much easier if one imposes growth conditions of the Lagrangian from above, since approximations are facilitated by Lebesgue’s dominated convergence. A two-dimensional analogue of Manià’s example was provided in [6]. There are examples in [7] of functionals of the form F(x, ∇u) depending on the independent variable x of the space and on the gradient ∇u of the admissible functions that exhibit the Lavrentiev phenomenon; there are also cases in which the Lavrentiev phenomenon does not occur (see [8]). No example is known to the authors for scalar problems when the Lagrangian is autonomous.

It was conjectured by Buttazzo-Belloni in [9] that the phenomenon should not occur when the Lagrangian F(u, ∇u) is autonomous and convex in both variables, a fact that they proved in the case of a (strongly) star-shaped domain under the hidden growth assumption that F(u, 0) is summable and zero as a boundary datum. Other results that appeared aimed to prove the conjecture: we mention Ekeland-Temam who proved in [10] its validity for functionals of the gradient on a Lipschitz domain for a zero boundary datum; Bonfanti and Cellina in [6, 11] considered autonomous Lagrangians that are sum of a radial function of the gradient ∇u and a function of the variable u, under some smoothness assumptions on the boundary and on the boundary datum. A complete answer to the conjecture was given by Bousquet-Mariconda-Treu in [12], where they showed that whenever F(u, ∇u) is convex, given u W01,1 (Ω) with a Lipschitz boundary datum and finite energy (i.e., F(u, ∇u) ∈ L1(Ω)), there is no Lavrentiev gap at u: there exists a sequence (uk)k of Lipschitz functions that share the same boundary datum and converge to u both in W1,1 and in energy, no matter if u is a minimizer.

We consider here a convex nonautonomous Lagrangian F(x, u, ∇u), and establish a sufficient condition under which no Lavrentiev gap occurs at any admissible function. As a byproduct it turns out that the Lavrentiev phenomenon does not occur if the Lagrangian is of the form

F(x,u,u)=f(x,u)+h(x,u),

with f(⋅, 0) of class C1(Ω) and h(⋅, 0) of class C2(Ω). The methods used here are mainly based on [12, 13, 14]: we show that we can approximate a function (both in W1,1 and in energy) with a sequence of bounded functions that are Lipschitz in a neighbourhood of the boundary of the domain.

A partial motivation for studying these kind of functionals comes from minimization problems in the Heisenberg group where one wants to consider functionals that generalize those studied in [15] and in references therein.

We do not consider here the vectorial case for which, when the Lagrangian depends only on the gradient, there are both examples of the occurrence of the Lavrentiev phenomenon and cases where it does not occur [7].

The authors are grateful to Pierre Bousquet for his useful comments and to both the referees for having carefully read the manuscript.

2 Notation and assumptions

Notation

  1. The scalar product of x, y in ℝn is denoted by 〈x, y〉.

  2. The pointwise maximum (resp. minimum) of two functions u, v is denoted by uv (resp. uv), u+ = u ∨ 0 (resp u = (–u)∨ 0) is the positive (resp. negative) part of u.

  3. The convex subgradient of a function g : ℝm → ℝ at ξ0 ∈ ℝm is the set

    g(ξ0):={νRm:g(ξ)g(ξ0)ν,ξξ0ξRm}.
  4. The partial convex subgradient of F(x, s, ξ) with respect to x at (x0, s0, ξ0) is the convex subgradient of xF(x, s0, ξ0) at x = x0, it will denoted by xF(x0, s0, ξ0). Analogously we will denote by sF(x0, s0, ξ0) (resp. ξF(x0, s0, ξ0)) the partial convex subgradients of F(x, s, ξ) with respect to s (resp. ξ) at (x0, s0, ξ0). Also, the convex subgradient of (s, ξ) ↦ F(x, s, ξ) is denoted by s,ξF(x, s, ξ).

  5. For E ⊆ ℝn, |E| is the n-dimensional Lebesgue measure of E.

  6. 1E is the indicator function of a set E.

2.1 Assumptions

  1. Ω ⊂ ℝn is an open and bounded set.

  2. F : Ω × ℝ × ℝn → ℝ, (x, s, ξ) ↦ F(x, s, ξ) is a Carathéodory function, bounded below by 〈α(x), ξ〉 + β(x) for some αL1(Ω; ℝn), βL1(Ω).

  3. ϕ is a Lipschitz function on Ω.

  4. p ≥ 1, and for vϕ + W01,p (Ω) we define I(v) := Ω F(x, v, ∇ v) dx (the “energy”).

The following structure condition will be used, in alternative to the boundedness of the reference function u, in our main result.

2.2 Hypothesis (H)

Hypothesis (H)

  1. There are positive sequences (τk)k and (σk)k such that:

    1. limk+ τk = +∞, limk+ σk = +∞;

    2. For each k ∈ ℕ, there are selections (qτk(x), ζτk(x)) of s,ξF(x, τk, 0) and (qσk(x), ζσk(x)) of s,ξF(x, –σk, 0), and C ≥ 0 satisfying

      kNζτk(x),ζσk(x)W1,1(Ω),
      divζτk(x)C,divζσk(x)C. (2.1)

  2. There is a measurable and bounded selection q(x) of the subgradient sF(x, 0, 0) of F at (x, 0, 0) and, for all k ∈ ℕ,

    qσk(x)q(x)qτk(x)a.e. xΩ. (2.2)

Remark 2.1

  1. Condition (2.2) is satisfied if sF(x, s, ξ) is convex. Indeed the monotonicity of the subdifferential implies that, for a.e. xΩ,

    (qτk(x)q(x))(τk0)0,(qσk(x)q(x))(σk0)0.
  2. When F is of class C2(Ω) and (s, ξ) ↦ F(x, s, ξ) is convex for a.e. x, Hypothesis (H) reduces to Condition 1, namely that there are increasing, divergent sequences (τk)k and (σk)k such that

    kNdivξF(x,τk,0)C,divξF(x,σk,0)C

    for a suitable C ≥ 0.

Here are some Lagrangians that satisfy Hypothesis (H).

Proposition 2.2

(Validity of Hypothesis (H)). Assume that the map (s, ξ) ↦ F(x, s, ξ) is convex for a.e. x and that

  1. Either F(x, s, ξ) = F(s, ξ), i.e., F is autonomous, or

  2. F(x, s, ξ) = f(x, s) + h(x, ξ) for some Carathéodory functions f : Ω × ℝ → ℝ and h : Ω × ℝn → ℝ with xxf(x, 0) bounded and xh(x, 0) of class C2(Ω).

Then F fulfills Hypothesis (H).

Proof

Let (τk)k, (σk)k be arbitrary positive divergent sequences.

  1. Since ζτk, ζσk do not depend on x it turns out that their divergence is zero. Similarly, Point 2 of Hypothesis (H) is fulfilled since any qsF(0, 0) does not depend on x and F is convex.

  2. Assume now that F(x, s, ξ) = f(x, s) + h(x, ξ). Then, for each k,

    ξF(x,τk,0)=ξF(x,σk,0)=ξh(x,0)

    and div ∇ξh(x, 0) is continuous, thus bounded on Ω. Moreover, any element of sF(x, 0, 0) is an element of xf(x, 0) and is thus bounded. Condition (2.2) follows from the convexity of sF(x, s, ξ), proving the validity of Hypothesis (H).□

3 Approximation lemmas

In this section, we establish two preliminary results that will be used in the proof of Theorem 4.2.

As a first step, we give a sufficient condition under which there is no Lavrentiev gap between Wϕ1,p (Ω) and Wϕ1,p (Ω) ∩ L(Ω). We have defined the space Wϕ1,p (Ω) as the set of those functions uW1,p(Ω) such that the extension of u by ϕ on ℝnΩ belongs to Wloc1,p (ℝn). We still denote by u this extension. In particular, (uϕ) belongs to W1,p(ℝn) and has compact support.

Lemma 3.1

Let F : Ω × ℝ × ℝn → ℝ satisfy Hypothesis (H). Then for every u in Wϕ1,p (Ω) such that F(x, u, ∇u) ∈ L1(Ω), there exists a sequence (uk)k in Wϕ1,p (Ω) ∩ L(Ω) such that (uk)k converges to u in Wϕ1,p (Ω) and

limk+I(uk)=I(u). (3.1)

Proof

Let (τk)k and (σk)k satisfy the conditions formulated in Hypothesis (H). For k large enough such that both τk > |ϕ|L(Ω) and σk > |ϕ|L(Ω), we define uk by

uk(x)=(u+τk)(x)(uσk)(x)=u(x)if σku(x)τk,τkif u(x)τk,σkif u(x)σk.

It is clear that uk Wϕ1,p (Ω) ∩ L(Ω) and that uk converges to u in Wϕ1,p (Ω). Moreover,

I(uk)={σkuτk}F(x,u,u)dx+{uτk}F(x,τk,0)dx+{uσk}F(x,σk,0)dx. (3.2)

Let q(x) and (qτk(x), ζτk(x)) be as in Hypothesis (H). We have

F(x,u,u)F(x,τk,0)+qτk(x)(uτk)+ζτk(x)(uτk) a.e..

Moreover, from Point 2 of Hypothesis (H) we get

F(x,u,u)F(x,τk,0)+q(x)(uτk)+ζτk(x)(uk) a.e. on {uτk}.

Since (uτk)+ W01,1 (Ω), integration on {uτk} then gives

{uτk}F(x,u,u)dx{uτk}F(x,τk,0)qudx+{uτk}ζτk(x)(uτk)+dx{uτk}F(x,τk,0)qudxΩdivζτk(x)(uτk)+dx.

Therefore, Hypothesis (H) yields

{uτk}F(x,u,u)dx{uτk}F(x,τk,0)(q+C)udx. (3.3)

Analogously we get

{uσk}F(x,u,u)dx{uσk}F(x,σk,0)+(q+C)udx. (3.4)

It follows from (3.2), (3.3) and (3.4) that

I(uk){σkuτk}F(x,u,u)dx+{uτk}F(x,u,u)dx+{uσk}F(x,u,u)dx+(q+C){uσk}{uτk}|u|dxI(u)+(q+C){uσk}{uτk}|u|dx. (3.5)

Since uL1(Ω), Lebesgue’s Theorem implies that

lim supk+I(uk)I(u).

By Fatou lemma,

lim infk+I(uk)I(u)

and (3.1) follows.□

We now prove that there is no Lavrentiev gap at u Wϕ1,p (Ω) if u is Lipschitz continuous on a neighborhood of ∂Ω.

Lemma 3.2

Assume that F : Ω × ℝ × ℝn → ℝ is convex with respect to its three variables. Let u in Wϕ1,p (Ω) be such that F(x, u, ∇u) ∈ L1(Ω). Assume, moreover, that either u is bounded or that F fulfils Hypothesis (H). If u is Lipschitz continuous on a neighborhood of ∂Ω, then there exists a sequence (uk)k in Lipϕ(Ω) such that (uk)k converges to u in Wϕ1,p (Ω) and

limk+I(uk)=I(u).

Moreover, if u is bounded in L(Ω), then the sequence (uk)k may be taken to be bounded in L(Ω).

Proof

From Lemma 3.1 it is not restrictive to assume that u is bounded. We may consider u as extended by ϕ out of Ω. By assumption, there exists an open set V ⊂ ℝn such that ∂ΩV and u is Lipschitz continuous on VΩ. In particular u and ∇u are in L(VΩ).

Let ρ Cc (B1, ℝ+) be even, Rn ρ dx = 1 and for k = 1, 2, ..., (ρk)k be the sequence of mollifiers defined by ρk(x) := knρ(kx). Let also θ Cc (Ω, [0, 1]) be such that θ = 1 on a neighborhood of ΩV. We then define

uk=θ(uρk)+(1θ)u.

Notice first that uk ∈ Lipϕ(Ω). Indeed, if θ = 1 then uk = u * ρk, otherwise {0 ≤ θ < 1} ⊂ VΩ where ∇u is bounded. Clearly, (uk)k converges to u in Wϕ1,p (Ω). This implies

lim infk+I(uk)I(u).

It remains to show that

lim supk+I(uk)I(u). (3.6)

For this purpose, we decompose I(uk) = Ω F(x, uk, ∇uk)dx as the sum

I(uk)={θ=1}F(x,uk,uk)dx+{0θ<1}F(x,uk,uk)dx. (3.7)

On the set {0 ≤ θ < 1} ⊂ VΩ, ∇uL(VΩ) and

uk=θ(uρk)+(1θ)u+(θ)(uρku).

Let k be such that

kk¯{0θ<1}+B1/kVΩ.

Then, for kk and x ∈ {0 ≤ θ < 1} we have

|uk(x)|2uL(VΩ);|uk(x)|2uL(VΩ)+2θL(VΩ)uL(VΩ)

which in turn means that under the above assumptions both uk and ∇uk are bounded by a constant that does not depend on k. Since (uk)k converges to u in W1,p(Ω) we may assume, by taking a subsequence, that (uk, ∇uk)k converges a.e. to (u, ∇u). Now, since F is bounded on bounded sets, by Lebesgue’s Theorem we have

limk+{0θ<1}F(x,uk,uk)dx={0θ<1}F(x,u,u)dx. (3.8)

On the set {θ = 1} we have

uk=uρk,uk=uρk.

It remains to show that

lim supk0{θ=1}F(x,uρk,uρk)dx{θ=1}F(x,u,u)dx; (3.9)

afterwards, in view of (3.7) and (3.8), we get (3.6). Notice that, since ρ is even,

ρkx=xkN.

By Jensen’s inequality,

F(x,uρk,uρk)=F(xρk,uρk,uρk)F(x,u,u)ρk.

Whence

{θ=1}F(x,uρk,uρk)dx{θ=1}F(x,u,u)ρkdx.

Since F(x, u, ∇u) ∈ L1(Ω), we get (3.9).□

4 Main result

We consider here domains Ω that are locally strongly star-shaped in the sense of [12, Definition 2.9]. These include Lipschitz ones and allow even some cusps at some boundary points.

Definition 4.1

An open and bounded set Ω is called locally strongly star-shaped if for every p∂Ω, there exists an open set H ⊂ ℝn such that pH and HΩ is strongly star-shaped, i.e., there is zHHΩ such that zH + λ(ΩzH) is relatively compact in Ω for every λ ∈ [0, 1[.

Theorem 4.2

(Non-occurrence of the Lavrentiev gap). Assume that Ω is locally strongly star-shaped and that F : Ω × ℝ × ℝn → ℝ is convex. Let u Wϕ1,p (Ω) be such that F(x, u, ∇u) ∈ L1(Ω). Assume, moreover, that either u is bounded or that F satisfies the structure Hypothesis (H). Then the Lavrentiev gap for I does not occur at u, i.e. there exists a sequence (uk)k in Lipϕ(Ω) converging to u in W1,p(Ω) and such that

limk+I(uk)=I(u). (4.1)

Moreover, if u is bounded in L(Ω), the sequence (uk)k may be taken to be bounded in L(Ω).

Proof

In view of Lemma 3.2 it is enough to provide a sequence (uk)k in Wϕ1,p (Ω) satisfying the conditions of the claim with the exception that it is just Lipschitz continuous in a neighborhood of ∂Ω (instead of Lipschitz on Ω). We may consider u to be extended by ϕ out of Ω. Also, in view of Lemma 3.1, it is not restrictive to assume that u is bounded.

Without loss of generality, we can assume that F ≥ 0. Indeed, since F is convex with respect to its variables, if x0Ω and (a, q, ζ) ∈ ∂F(x0, 0, 0) then

G(x,s,ξ):=F(x,s,ξ)a¯xq¯sζ¯ξF(x0,0,0)0.

Moreover additive affine terms do not perturb our convergence results: if a sequence (uk)k converges to u in W1,p(Ω) then (I(uk))k converges to I(u) if and only if Ω G(x, uk, ∇uk)dx converges to Ω G(x, u, ∇u)dx.

Consider first the case where Ω is strongly star-shaped with respect to the origin, i.e., for every h ∈ [0, 1[, is relatively compact in Ω. Given λ, h ∈ ]1/2, 1[, set

uhλ:=ϕ(x)+λhuϕxh.

Notice that uhλ converges to u in W1,1 as λ, h → 1 and that uhλ = ϕ on ℝn. We then write

x,uhλ,uhλ=x,ϕ(x)+λhuϕxh,ϕ(x)+λuϕxh

as a convex combination in λ, namely

x,uhλ,uhλ=λxh,uxh,λuxh+(1λ)x1λ/h1λ,ξhλ(x),ϕ(x)λϕxh1λ, (4.2)

where

ξhλ(x):=uhλλuxh=11λϕ(x)hλϕxh+(h1)λuxh.

The convexity of F yields

I(uhλ)λΩFxh,uxh,uxhdx+(1λ)ΩFx1λ/h1λ,ξhλ(x),ϕ(x)λϕxh1λdx (4.3)

Since F ≥ 0, we get

ΩFxh,uxh,uxhdx=hnhΩF(x,u(x),u(x)dxΩF(x,u(x),u(x))dx.

Fix λ ∈ ]1/2, 1[; we then study the second term of the right hand side of (4.3). Since h ≥ 1/2, we have

x1λ/h1λsup{|x|:xΩ}1λ,ξhλ11λ2ϕ+u

and

ϕ(x)λϕxh1λ2ϕ1λ.

Moreover

limh1x1λ/h1λ=x,limh1ξhλ(x)=ϕ(x) a.e.

and

limh1ϕ(x)λϕxh1λ=ϕ(x)x.

The function F being bounded on bounded sets, by means of the dominated convergence theorem we get

limh1ΩFx1λ/h1λ,ξhλ(x),ϕ(x)λϕxh1λdx=ΩF(x,ϕ,ϕ)dx,

so that

lim suph1I(uhλ)λI(u)+(1λ)I(ϕ).

The right-hand side term of the latter inequality tends to I(u) as λ tends to 1. Hence, for every i ∈ ℕ, i ≥ 1, there are sequences λi and ki ∈ ℕ with kii such that ukiλi u in W1,p(Ω) as i → +∞, ukiλi are Lipschitz in a neighbourhood of ∂Ω, and

I(ukiλi)I(u)+1ii1.

In particular we get

lim supi+I(ukiλi)I(u).

Also, Fatou’s lemma gives

lim infi+I(ukiλi)I(u),

and thus limi+ I( ukiλi ) = I(u), proving the claim.

The case of a general locally strongly star-shaped domain follows with the obvious changes as in the proof of [12, Theorem 4.1].□

Remark 4.3

Assume that F(x, u, ∇u) = f(x, u) + h(∇u) with f convex and superlinear. In Theorem 4.2 the (alternative) assumption that u is bounded is satisfied if, for instance, for every constant boundary datum k ∈ ℤ, the minimizers of I among the functions that are equal to k in the boundary of Ω are bounded. Indeed, the fact that ϕ is bounded and the comparison principles of [16, 17] show that u is bounded too.

Acknowledgement

This research is partially supported by the Padua University grant SID 2018 “Controllability, stabilizability and infimum gaps for control systems”, prot. BIRD 187147.

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Received: 2020-01-02
Accepted: 2020-01-10
Published Online: 2020-02-17

© 2020 Carlo Mariconda and Giulia Treu, published by De Gruyter

This work is licensed under the Creative Commons Attribution 4.0 International License.

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  16. Metric completions, the Heine-Borel property, and approachability
  17. Functional identities on upper triangular matrix rings
  18. Uniqueness on entire functions and their nth order exact differences with two shared values
  19. The adaptive finite element method for the Steklov eigenvalue problem in inverse scattering
  20. Existence of a common solution to systems of integral equations via fixed point results
  21. Fixed point results for multivalued mappings of Ćirić type via F-contractions on quasi metric spaces
  22. Some inequalities on the spectral radius of nonnegative tensors
  23. Some results in cone metric spaces with applications in homotopy theory
  24. On the Malcev products of some classes of epigroups, I
  25. Self-injectivity of semigroup algebras
  26. Cauchy matrix and Liouville formula of quaternion impulsive dynamic equations on time scales
  27. On the symmetrized s-divergence
  28. On multivalued Suzuki-type θ-contractions and related applications
  29. Approximation operators based on preconcepts
  30. Two types of hypergeometric degenerate Cauchy numbers
  31. The molecular characterization of anisotropic Herz-type Hardy spaces with two variable exponents
  32. Discussions on the almost 𝒵-contraction
  33. On a predator-prey system interaction under fluctuating water level with nonselective harvesting
  34. On split involutive regular BiHom-Lie superalgebras
  35. Weighted CBMO estimates for commutators of matrix Hausdorff operator on the Heisenberg group
  36. Inverse Sturm-Liouville problem with analytical functions in the boundary condition
  37. The L-ordered L-semihypergroups
  38. Global structure of sign-changing solutions for discrete Dirichlet problems
  39. Analysis of F-contractions in function weighted metric spaces with an application
  40. On finite dual Cayley graphs
  41. Left and right inverse eigenpairs problem with a submatrix constraint for the generalized centrosymmetric matrix
  42. Controllability of fractional stochastic evolution equations with nonlocal conditions and noncompact semigroups
  43. Levinson-type inequalities via new Green functions and Montgomery identity
  44. The core inverse and constrained matrix approximation problem
  45. A pair of equations in unlike powers of primes and powers of 2
  46. Miscellaneous equalities for idempotent matrices with applications
  47. B-maximal commutators, commutators of B-singular integral operators and B-Riesz potentials on B-Morrey spaces
  48. Rate of convergence of uniform transport processes to a Brownian sheet
  49. Curves in the Lorentz-Minkowski plane with curvature depending on their position
  50. Sequential change-point detection in a multinomial logistic regression model
  51. Tiny zero-sum sequences over some special groups
  52. A boundedness result for Marcinkiewicz integral operator
  53. On a functional equation that has the quadratic-multiplicative property
  54. The spectrum generated by s-numbers and pre-quasi normed Orlicz-Cesáro mean sequence spaces
  55. Positive coincidence points for a class of nonlinear operators and their applications to matrix equations
  56. Asymptotic relations for the products of elements of some positive sequences
  57. Jordan {g,h}-derivations on triangular algebras
  58. A systolic inequality with remainder in the real projective plane
  59. A new characterization of L2(p2)
  60. Nonlinear boundary value problems for mixed-type fractional equations and Ulam-Hyers stability
  61. Asymptotic normality and mean consistency of LS estimators in the errors-in-variables model with dependent errors
  62. Some non-commuting solutions of the Yang-Baxter-like matrix equation
  63. General (p,q)-mixed projection bodies
  64. An extension of the method of brackets. Part 2
  65. A new approach in the context of ordered incomplete partial b-metric spaces
  66. Sharper existence and uniqueness results for solutions to fourth-order boundary value problems and elastic beam analysis
  67. Remark on subgroup intersection graph of finite abelian groups
  68. Detectable sensation of a stochastic smoking model
  69. Almost Kenmotsu 3-h-manifolds with transversely Killing-type Ricci operators
  70. Some inequalities for star duality of the radial Blaschke-Minkowski homomorphisms
  71. Results on nonlocal stochastic integro-differential equations driven by a fractional Brownian motion
  72. On surrounding quasi-contractions on non-triangular metric spaces
  73. SEMT valuation and strength of subdivided star of K 1,4
  74. Weak solutions and optimal controls of stochastic fractional reaction-diffusion systems
  75. Gradient estimates for a weighted nonlinear parabolic equation and applications
  76. On the equivalence of three-dimensional differential systems
  77. Free nonunitary Rota-Baxter family algebras and typed leaf-spaced decorated planar rooted forests
  78. The prime and maximal spectra and the reticulation of residuated lattices with applications to De Morgan residuated lattices
  79. Explicit determinantal formula for a class of banded matrices
  80. Dynamics of a diffusive delayed competition and cooperation system
  81. Error term of the mean value theorem for binary Egyptian fractions
  82. The integral part of a nonlinear form with a square, a cube and a biquadrate
  83. Meromorphic solutions of certain nonlinear difference equations
  84. Characterizations for the potential operators on Carleson curves in local generalized Morrey spaces
  85. Some integral curves with a new frame
  86. Meromorphic exact solutions of the (2 + 1)-dimensional generalized Calogero-Bogoyavlenskii-Schiff equation
  87. Towards a homological generalization of the direct summand theorem
  88. A standard form in (some) free fields: How to construct minimal linear representations
  89. On the determination of the number of positive and negative polynomial zeros and their isolation
  90. Perturbation of the one-dimensional time-independent Schrödinger equation with a rectangular potential barrier
  91. Simply connected topological spaces of weighted composition operators
  92. Generalized derivatives and optimization problems for n-dimensional fuzzy-number-valued functions
  93. A study of uniformities on the space of uniformly continuous mappings
  94. The strong nil-cleanness of semigroup rings
  95. On an equivalence between regular ordered Γ-semigroups and regular ordered semigroups
  96. Evolution of the first eigenvalue of the Laplace operator and the p-Laplace operator under a forced mean curvature flow
  97. Noetherian properties in composite generalized power series rings
  98. Inequalities for the generalized trigonometric and hyperbolic functions
  99. Blow-up analyses in nonlocal reaction diffusion equations with time-dependent coefficients under Neumann boundary conditions
  100. A new characterization of a proper type B semigroup
  101. Constructions of pseudorandom binary lattices using cyclotomic classes in finite fields
  102. Estimates of entropy numbers in probabilistic setting
  103. Ramsey numbers of partial order graphs (comparability graphs) and implications in ring theory
  104. S-shaped connected component of positive solutions for second-order discrete Neumann boundary value problems
  105. The logarithmic mean of two convex functionals
  106. A modified Tikhonov regularization method based on Hermite expansion for solving the Cauchy problem of the Laplace equation
  107. Approximation properties of tensor norms and operator ideals for Banach spaces
  108. A multi-power and multi-splitting inner-outer iteration for PageRank computation
  109. The edge-regular complete maps
  110. Ramanujan’s function k(τ)=r(τ)r2(2τ) and its modularity
  111. Finite groups with some weakly pronormal subgroups
  112. A new refinement of Jensen’s inequality with applications in information theory
  113. Skew-symmetric and essentially unitary operators via Berezin symbols
  114. The limit Riemann solutions to nonisentropic Chaplygin Euler equations
  115. On singularities of real algebraic sets and applications to kinematics
  116. Results on analytic functions defined by Laplace-Stieltjes transforms with perfect ϕ-type
  117. New (p, q)-estimates for different types of integral inequalities via (α, m)-convex mappings
  118. Boundary value problems of Hilfer-type fractional integro-differential equations and inclusions with nonlocal integro-multipoint boundary conditions
  119. Boundary layer analysis for a 2-D Keller-Segel model
  120. On some extensions of Gauss’ work and applications
  121. A study on strongly convex hyper S-subposets in hyper S-posets
  122. On the Gevrey ultradifferentiability of weak solutions of an abstract evolution equation with a scalar type spectral operator on the real axis
  123. Special Issue on Graph Theory (GWGT 2019), Part II
  124. On applications of bipartite graph associated with algebraic structures
  125. Further new results on strong resolving partitions for graphs
  126. The second out-neighborhood for local tournaments
  127. On the N-spectrum of oriented graphs
  128. The H-force sets of the graphs satisfying the condition of Ore’s theorem
  129. Bipartite graphs with close domination and k-domination numbers
  130. On the sandpile model of modified wheels II
  131. Connected even factors in k-tree
  132. On triangular matroids induced by n3-configurations
  133. The domination number of round digraphs
  134. Special Issue on Variational/Hemivariational Inequalities
  135. A new blow-up criterion for the Nabc family of Camassa-Holm type equation with both dissipation and dispersion
  136. On the finite approximate controllability for Hilfer fractional evolution systems with nonlocal conditions
  137. On the well-posedness of differential quasi-variational-hemivariational inequalities
  138. An efficient approach for the numerical solution of fifth-order KdV equations
  139. Generalized fractional integral inequalities of Hermite-Hadamard-type for a convex function
  140. Karush-Kuhn-Tucker optimality conditions for a class of robust optimization problems with an interval-valued objective function
  141. An equivalent quasinorm for the Lipschitz space of noncommutative martingales
  142. Optimal control of a viscous generalized θ-type dispersive equation with weak dissipation
  143. Special Issue on Problems, Methods and Applications of Nonlinear analysis
  144. Generalized Picone inequalities and their applications to (p,q)-Laplace equations
  145. Positive solutions for parametric (p(z),q(z))-equations
  146. Revisiting the sub- and super-solution method for the classical radial solutions of the mean curvature equation
  147. (p,Q) systems with critical singular exponential nonlinearities in the Heisenberg group
  148. Quasilinear Dirichlet problems with competing operators and convection
  149. Hyers-Ulam-Rassias stability of (m, n)-Jordan derivations
  150. Special Issue on Evolution Equations, Theory and Applications
  151. Instantaneous blow-up of solutions to the Cauchy problem for the fractional Khokhlov-Zabolotskaya equation
  152. Three classes of decomposable distributions
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