2022
DOI: 10.1016/j.na.2022.112891
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Gradient estimates for Orlicz double phase problems with variable exponents

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Cited by 7 publications
(7 citation statements)
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“…Then (3.5) holds for any θ > 0 in Cases ( 1)-( 2) and for θ = s * q−p in Case (3). The constant b 0 depends only on n, p, q, L, L ω and b.…”
Section: Model and Functionmentioning
confidence: 90%
See 1 more Smart Citation
“…Then (3.5) holds for any θ > 0 in Cases ( 1)-( 2) and for θ = s * q−p in Case (3). The constant b 0 depends only on n, p, q, L, L ω and b.…”
Section: Model and Functionmentioning
confidence: 90%
“…See Corollary 1.1 for the corresponding expressions F and Table 1 for examples of our assumptions in some of these cases. We refer to [41] for references up to 2020 and [3,4,18,20,30,32,45,49] for some more recent advances on variants of the variable exponent and double phase models.…”
Section: Introductionmentioning
confidence: 99%
“…In recent years, there are many results of differential equations in Musielak-Orlicz-Sobolev spaces. For example, Fan [17] and we [18] proved the existence of weak solutions of a class of differential equations of divergence form by using a subsupersolution method in reflexive Musielak-Orlicz-Sobolev spaces and nonreflexive Musielak-Orlicz-Sobolev spaces, respectively; Li et al [19] proved the existence and uniqueness of entropy solutions and the uniqueness of renormalized solutions to the nonlinear elliptic equations in Musielak-Orlicz-Sobolev spaces; we [20] proved the existence of barrier solutions of elliptic differential equations in Musielak-Orlicz-Sobolev spaces; and Baasandorj et al [21] established optimal regularity estimates for the gradient of solutions to nonuniformly elliptic equations of the Orlicz double phase with variable exponent types. Musielak-Orlicz functions (described in Section 2) have many applications such as non-Newtonian fluids (see, e.g., [22]), thermistor problem (see, e.g., [23]), and image restoration (see, e.g., [24]).…”
Section: Introductionmentioning
confidence: 95%
“…On the other hand, since (1.1) features purely nonlocal behaviors on the set {a(x) = 0}, we could not compare (1.1) with a local problem as in [26]. We thus develop a different method motivated from the ones in [1,3,23], whose crucial tools include the expansion of positivity results described in Lemmas 4.2 and 4.3 below. For fractional p-Laplacian type problems, analogous results are proved in [23,Lemma 6.3], but their proofs are not directly applicable to our double phase setting.…”
Section: Introductionmentioning
confidence: 99%