Home Regularity for double-phase functionals with nearly linear growth and two modulating coefficients
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Regularity for double-phase functionals with nearly linear growth and two modulating coefficients

  • Bogi Kim and Jehan Oh EMAIL logo
Published/Copyright: July 2, 2025

Abstract

We deal with non-uniformly elliptic integral functionals

w c ( x ) D w log ( 1 + D w ) + a ( x ) ( D w 2 + s 2 ) q 2 + 1 d x ,

with s [ 0 , 1 ] , q > 1 , 0 c ( ) Λ , a ( ) 0 , and a ( x ) + c ( x ) 1 Λ for some Λ > 0 . In this article, we establish that the gradient of a local minimizer for the aforementioned functionals is locally Hölder continuous.

1 Introduction

In this article, we establish the first Schauder-type result for a local minimizer of non-uniformly elliptic integral functionals

(1.1) w ( w ; Ω ) Ω c ( x ) D w log ( 1 + D w ) + a ( x ) ( D w 2 + s 2 ) q 2 + 1 d x ,

where Ω R n is a bounded open subset, n 2 , s [ 0 , 1 ] , and q > 1 . Additionally, we may assume that two modulating coefficients a ( ) and c ( ) satisfy

(1.2) 0 a ( ) C loc 0 , α ( Ω ) , 1 < q < 1 + α n , 0 c ( ) C loc 0 , α 0 ( Ω ) , c ( x ) Λ , 1 Λ a ( x ) + c ( x ) , for all x Ω ,

where α , α 0 ( 0 , 1 ) , and Λ 1 . For simplicity, we denote

F ( x , z ) c ( x ) z log ( 1 + z ) + 1 , s ( z ) ( z 2 + s 2 ) 1 2 , g ( t ) log ( 1 + t ) + 1 ,

and

(1.3) H ( x , z ) = F ( x , z ) + a ( x ) [ s ( z ) ] q ,

for x Ω , z R n and t [ 0 , ) . Here, according to [18], g is a non-decreasing, concave, and unbounded function from [ 0 , ) into [ 1 , ) such that t t g ( t ) is convex and for every ε > 0 ,

(1.4) g ( t ) c g ( ε ) t ε , for every t 1 ,

holds for some constant c g ( ε ) .

We would like to show that the gradient of a local minimizer of (1.1) is Hölder continuous, when a ( ) and c ( ) are only Hölder continuous. In fact, this is implied to proving the nonlinear version of Schauder estimates originally established by Hopf and Caccioppoli. In [24] and [32], it is introduced that a local minimizer of the classical nearly linear functional

w Ω c ( x ) D w log ( 1 + D w ) d x

with c ( x ) 1 satisfies the Schauder estimate and is therefore Hölder continuous. According to [18], the term “nearly linear” refers to integrand where growth in the gradient variable is superlinear, but it is still slower than that of z z p for any p > 1 . The functional ( ) can be seen as a combination of such nearly linear growth integrand and q -power growth integrand and is derived from the well-studied double-phase functional

w P ( w ; Ω ) Ω ( c ( x ) D w p + a ( x ) D w q ) d x , 1 < p < q .

The functional P ( ) with c ( ) 1 was first introduced by Zhikov [3841] as an example of the Lavrentiev phenomenon (see [20,23] also) and as a model explaining strongly anisotropic materials in the context of homogenization. Writing the function

G ( x , z ) z p + a ( x ) z q , ( x Ω , z R n ) ,

the pointwise ellipticity ratio of G ( x , )

(1.5) G ( x , ) ( z ) highest eigenvalue of z z G ( x , z ) lowest eigenvalue of z z G ( x , z ) ,

and the global ellipticity ratio of G ( x , )

(1.6) G ( z ; B ) sup x B highest eigenvalue of z z G ( x , z ) inf x B lowest eigenvalue of z z G ( x , z ) ,

for any ball B Ω , we have

sup x Ω , z 1 G ( x , ) ( z ) c ( p , q )

and

G ( z ; B ) 1 + a L ( B ) z q p ,

provided that { a ( x ) 0 } B is nonempty, and hence, G ( z ; B ) is unbounded with respect to the gradient variable z . Therefore, the functional P ( ) is uniformly elliptic in the pointwise sense, but non-uniformly elliptic in the global sense. We refer to [34] for information on uniformly elliptic functionals and non-uniformly elliptic functionals. Such non-uniformly elliptic functional P has been well researched. To obtain sharp regularities for a local minimizer u of P , we may assume that

(1.7) a ( ) C 0 , α ( Ω ) , α ( 0 , 1 ] and q p 1 + α n ,

or

(1.8) u L ( Ω ) , a ( ) C 0 , α ( Ω ) , α ( 0 , 1 ] , and q p + α .

Indeed, they are optimal conditions for obtaining regularity results of minima [20,23]. Moreover, if either (1.7) or (1.8) holds, we can obtain from [6,12,13,28] that the gradient of minimizer u is Hölder continuous. Moreover, discussions on Harnack’s inequality and Hölder continuity can be found in [5,35,36], and Calderón-Zygmund estimates have been studied by Baasandorj et al. [2], De Filippis and Mingione [15], and Colombo and Mingione [14]. Additionally, global gradient estimates, gradient Hölder continuity, and gradient higher integrability have been discussed in [6,10,12,13]. Furthermore, looking at [8,9,11,21,22,26,27,37] provides various insights into the regularities of double-phase problems.

In this article, the main functional ( ) is different from the aforementioned situation because z G ( x , ) ( z ) is unbounded for G ( x , z ) = c ( x ) z log ( 1 + z ) + a ( x ) z q . In particular, the methods of De Giorgi and Moser cannot be used, and it is impossible to obtain gradient regularity by differentiating the Euler-Lagrange equation. For this reason, a new approach is needed to prove the Hopf-Caccioppoli-Schauder estimates. Indeed, De Filippis and Mingione [18] has proven the results by using a new approach involving nonlinear potentials and fractional Sobolev spaces. Furthermore, De Filippis and Piccinini [19] has recently studied multi-phase problems with nearly linear growth

ω Ω [ D w log ( 1 + D w ) + a ( x ) D w q + b ( x ) D w s ] d x ,

where 1 < q , s < and a ( ) , b ( ) are nonnegative bounded coefficients. We also plan to obtain the results in a similar manner. However, a key difference from [18] is that c ( ) can be zero. As a result, we may not be able to obtain the following ellipticity and growth conditions for F ( ) :

(1.9) ν z g ( z ) F ( x , z ) , F ( x , z ) L ( z g ( z ) + 1 ) , ν ξ 2 ( z 2 + 1 ) 1 2 z z F ( x , z ) ξ , ξ , z z F ( x , z ) L g ( z ) ( z 2 + 1 ) 1 2 ,

for every x Ω , z , ξ R n , with 0 < ν 1 L being fixed constants. Actually, (1.9)1 and (1.9)3 do not hold. For this reason, we consider the condition

1 Λ a ( x ) + c ( x ) , for all x Ω ,

in (1.2), and we prove the growth and ellipticity conditions of F ( ) (see Proposition 2.1). Before introducing the main theorem in this article, we state the definition of a local minimizer of ( ) .

Definition 1.1

A function u W loc 1,1 ( Ω ) is a local minimizer of ( ) if for every ball B Ω , ( u ; B ) is finite and the minimality condition ( u ; B ) ( w ; B ) holds whenever w u W 0 1,1 ( B ) . In particular, this implies that ( u ; Ω 0 ) is finite whenever Ω 0 Ω is an open subset.

As we proceed with estimates, we are going to use constants that depend on various parameters. We denote these parameters using the notation “ data ”:

data data ( n , q , Λ , α , α 0 , a C 0 , α , c C 0 , α 0 , c g ( ) ) .

Now, the main theorem is as follows:

Theorem 1.2

Let u W loc 1,1 ( Ω ) be a local minimizer of the functional ( ) in (1.1) with (1.2). Then, the following statements hold:

  1. For every ball B B r Ω with r 1 ,

    (1.10) D u L ( B 2 ) c B [ F ( x , D u ) + a ( x ) ( D u 2 + s 2 ) q 2 ] d x ϑ + c ,

    where c c ( data ) and ϑ ϑ ( n , q , α , α 0 ) 1 . Furthermore, Du is locally Hölder continuous in Ω .

  2. When s > 0 , Du is locally Hölder continuous in Ω with the Hölder exponent α ˜ min { α , α 0 } .

Finally, we provide an overview of the remaining parts. In the next section, we introduce notations. Moreover, we obtain the growth and ellipticity conditions of F . In Section 3, we explain auxiliary functions and eigenvalues and obtain their properties. In Section 4, we consider the frozen functional of ( ) and prove the regularity for a minimizer of the frozen functional. Finally, in Section 5, after establishing the comparison estimate for frozen functionals and fractional Caccioppoli inequality, we prove the main theorem.

2 Preliminaries

2.1 Notation

We write a general constant larger than 1 by c . Although the constant may differ from line to line, we still denote it as c . Special constants may be denoted by c * , c ˜ , and so on. We write by B r ( x 0 ) { x R n : x x 0 < r } the open ball with center x 0 and radius r > 0 . Next, the open ball with center 0 and redius r > 0 is denoted as

r B r ( 0 ) = { x R n : x < r } .

For a ball B with radius r > 0 and a positive number γ , we denote by γ B the concentric ball with radius γ r and by B γ ( 1 γ ) B . Furthermore, Q inn Q inn ( B ) denotes the inner hypercube of B , i.e., Q inn B is the largest hypercube satisfying sides parallel to the coordinate axes and concentric to B . Then, the length of side of Q inn ( B ) equals 2 r n . The function spaces of vector-valued functions are denoted by L p ( Ω ; R k ) , W 1 , p ( Ω ; R k ) , and so on. But, when there is no ambiguity, they will still be denoted as L p ( Ω ) L p ( Ω ; R k ) , W 1 , p ( Ω ) W 1 , p ( Ω ; R k ) , and so on.

For a measurable subset U R n with 0 < U < , and for an integrable function f : U R k , k 1 , we write

( f ) U U f ( x ) d x 1 U U f ( x ) d x .

With a scalar function f and a number κ R , we write

( f κ ) + max { f κ , 0 } and ( f κ ) max { κ f , 0 } .

Next, whenever f : U R k and U is any set, we define

osc U f sup x , y U f ( x ) f ( y ) .

As usual, for β ( 0 , 1 ] , we write

f C 0 , β ( U ) f L ( U ) + [ f ] 0 , β ; U , [ f ] 0 , β ; U sup x , y U , x y f ( x ) f ( y ) x y β .

The finite difference operator τ h : L 1 ( Ω ; R k ) L 1 ( Ω h ; R k ) is defined as

τ h w ( x ) w ( x + h ) w ( x ) ,

for x Ω h and for any w L 1 ( Ω ; R k ) , where Ω h { x Ω : dist ( x , Ω ) > h } . For β ( 0 , 1 ) , s [ 1 , ) , k N , n 2 , and an open subset Ω R n , the space W β , s ( Ω ; R k ) is defined as the set of functions w : Ω R k such that

w W β , s ( Ω ; R k ) w L s ( Ω ; R k ) + [ w ] β , s ; Ω w L s ( Ω ; R k ) + Ω Ω w ( x ) w ( y ) s x y n + β s d x d y < .

2.2 Auxiliary results

For every 0 < p < and ω [ 0 , 1 ] , we define the vector fields V ω , p : R n R n by

V ω , p ( z ) ( z 2 + ω 2 ) ( p 2 ) 4 z , ( z R n ) .

By [18], we obtain

(2.1) V ω , p ( z 1 ) V ω , p ( z 2 ) n , p ( z 1 2 + z 2 2 + ω 2 ) ( p 2 ) 4 z 1 z 2 ,

whenever z 1 , z 2 R n , ω [ 0 , 1 ] and p > 0 , and

( z 1 2 + z 2 2 + ω 2 ) γ 2 0 1 ( z 2 + τ ( z 1 z 2 ) 2 + ω 2 ) γ 2 d τ ,

whenever γ 0 and z 1 + z 2 > 0 . In particular, if 0 γ < 1 and z 1 + z 2 > 0 ,

( z 1 2 + z 2 2 + ω 2 ) γ 2 n , γ 0 1 ( z 2 + τ ( z 1 z 2 ) 2 + ω 2 ) γ 2 d τ .

For a ball B Ω and σ ( 0 , 1 ) , we define

(2.2) a σ ( x ) a ( x ) + σ , a i ( B ) inf x B a ( x ) , and a σ , i ( B ) a i ( B ) + σ ,

and

(2.3) V ω , σ 2 ( x , z 1 , z 2 ) V 1,1 ( z 1 ) V 1,1 ( z 2 ) 2 + a σ ( x ) V ω , q ( z 1 ) V ω , q ( z 2 ) 2 , V ω , σ , i 2 ( z 1 , z 2 ; B ) V 1,1 ( z 1 ) V 1,1 ( z 2 ) 2 + a σ , i ( B ) V ω , q ( z 1 ) V ω , q ( z 2 ) 2 ,

where z 1 , z 2 R n , x Ω . In the rest of this section, we prove some properties of F ( ) such as the growth and ellipticity conditions.

Proposition 2.1

For any x , y Ω and z , ξ R n ,

(2.4) ν z g ( z ) H ( x , z ) , F ( x , z ) L ( z g ( z ) + 1 ) , ν ξ 2 ( 1 + z 2 ) 1 2 z z H ( x , z ) ξ , ξ , z z F ( x , z ) L g ( z ) ( 1 + z 2 ) 1 2 , z F ( x , z ) z F ( y , z ) L x y α 0 g ( z )

hold for some 0 < ν 1 L depending on q and Λ . Moreover, for z 1 ,

(2.5) z F ( x , z ) L z

is satisfied.

Proof

From [18, (1.11) and (1.13)], the inequalities (2.4) 2 , (2.4)4, (2.4) 5 , and (2.5) hold. Thus, we only need to prove (2.4)1 and (2.4)3. Since

lim t t log ( 1 + t ) ( s 2 + t 2 ) q 2 = 0 ,

there exists M = M ( q ) > 1 such that t log ( 1 + t ) ( s 2 + t 2 ) q 2 , whenever t M .

If z < M , then H ( x , z ) 1 c ( M ) z ( log ( 1 + z ) + 1 ) , since z ( log ( 1 + z ) + 1 ) M log ( 1 + M ) + M . If z M , then

H ( x , z ) c ( x ) z log ( 1 + z ) + a ( x ) ( s 2 + z 2 ) q 2 ( c ( x ) + a ( x ) ) z log ( 1 + z ) 1 2 Λ z ( log ( 1 + z ) + log 2 ) c ( Λ ) z ( log ( 1 + z ) + 1 ) .

Thus, (2.4)1 holds.

Note that the first derivative and second derivative of [ s ( z ) ] q with respect to z are

z [ s ( z ) ] q = q ( z 2 + s 2 ) q 2 2 z

and

(2.6) z z [ s ( z ) ] q = q ( q 2 ) ( z 2 + 1 ) q 4 2 z z + q ( z 2 + 1 ) q 2 2 I n .

Hence, the first derivative and second derivative of H ( x , z ) with respect to z are

z H ( x , z ) = c ( x ) z z log ( 1 + z ) + c ( x ) z 1 + z + q a ( x ) ( z 2 + s 2 ) q 2 2 z

and

z z H ( x , z ) = c ( x ) I n z z z 2 log ( 1 + z ) z + c ( x ) I n 1 + z + c ( x ) z z z 2 ( 1 + z ) c ( x ) z z ( 1 + z ) 2 z + a ( x ) q ( q 2 ) ( z 2 + 1 ) q 4 2 z z + q a ( x ) ( z 2 + 1 ) q 2 2 I n ,

where I n is the n × n identity matrix. Since 0 < q 1 < 1 2 < 1 2 , ( 2 q ) 2 < 1 2 , z , ξ 2 z 2 ξ 2 , and

1 z 2 ( 1 + z ) 1 ( 1 + z ) 2 z = 1 z 2 ( 1 + z ) 2 0 ,

we obtain

z z H ( x , z ) ξ , ξ c ( x ) ξ 2 1 + z + a ( x ) ( q 2 2 q + 1 ) ( z 2 + 1 ) q 4 2 z , ξ 2 + a ( x ) ( q 1 ) ( z 2 + 1 ) q 2 2 ξ 2 1 2 c ( x ) ξ 2 ( 1 + z 2 ) 1 2 + ( q 1 ) a ( x ) ξ 2 ( 1 + z 2 ) 2 q 2 ( q 1 ) ( c ( x ) + a ( x ) ) ξ 2 ( 1 + z 2 ) 1 2 q 1 Λ ξ 2 ( 1 + z 2 ) 1 2 .

Thus, (2.4)3 holds.□

From [18], we obtain the growth condition of z F ( ) . Since this has nothing to do with c ( ) , it can be obtained through the same proof.

Lemma 2.2

[18] Let F : Ω × R n [ 0 , ) be as in (2.4). Then, there exists a constant c depending on q, Λ , and c g ( 1 ) such that z F ( x , z ) c g ( z ) holds for every ( x , z ) Ω × R n .

3 Auxiliary functions and their properties

We fix an arbitrary ball B Ω centered at x c and define

(3.1) H ω , σ ( x , z ) F ( x , z ) + a σ ( x ) [ ω ( z ) ] q , H ω , σ , i ( z ) H ω , σ , i ( z ; B ) F ( x c , z ) + a σ , i ( B ) [ ω ( z ) ] q , H ω , σ , i ( t ) H ω , σ , i ( t ; B ) t g ( t ) + a σ , i ( B ) ( t 2 + ω 2 ) q 2 + 1 , t 0 ,

for ω [ 0 , 1 ] and σ ( 0 , 1 ) . Then, t H ω , σ , i ( t ) is an increasing function. Next, we define two functions λ ω , σ , Λ ω , σ : Ω × [ 0 , ) [ 0 , ) by

λ ω , σ ( x , z ) ( z 2 + 1 ) 1 2 + ( q 1 ) a σ ( x ) [ ω ( z ) ] q 2 , Λ ω , σ ( x , z ) ( z 2 + 1 ) 1 2 g ( z ) + a σ ( x ) [ ω ( z ) ] q 2 ,

for z R n and x Ω . Then, we see that

(3.2) σ [ ω ( z ) ] q H ω , σ ( x , z ) c ( [ ω ( z ) ] q + 1 ) , λ ω , σ ( x , z ) ξ 2 c z z H ω , σ ( x , z ) ξ , ξ , z z H ω , σ ( x , z ) c Λ ω , σ ( x , z ) , V ω , σ 2 ( x , z 1 , z 2 ) c z H ω , σ ( x , z 1 ) z H ω , σ ( x , z 2 ) , z 1 z 2 , z H ω , σ ( x , z ) z H ω , σ ( y , z ) c x y α 0 g ( z ) + c x y α [ ω ( z ) ] q 1 ,

for all x , y Ω , z , z 1 , z 2 , ξ R n and for some c c ( data ) . First, (3.2)1 can be obtained from (2.4) 2 and (1.4) with ε = q 1 . Moreover, (3.2)3 and (3.2) 5 hold from (2.4)4 and (2.4) 5 , respectively. Similar to [18, Remark 2], we can show that if (3.2) 2 holds, then (3.2)4 is satisfied. Therefore, we only need to show that (3.2) 2 holds. Indeed, we obtain from (2.4)3 and (2.6) that for x Ω and z , ξ R n ,

z z H ω , σ ( x , z ) ξ , ξ 1 2 z z H ω , σ ( x , z ) ξ , ξ + 1 2 a σ ( x ) z z [ ω ( z ) ] q ξ , ξ 1 c λ ω , σ ( x , z ) ξ 2

holds for some constant c . Also, we easily check that when ω > 0 , the following properties are satisfied:

(3.3) σ ( q 1 ) [ 1 ( z ) ] q 2 ξ 2 c z z H ω , σ ( x , z ) ξ , ξ , z H ω , σ ( x , z ) 1 ( z ) + z z H ω , σ ( x , z ) [ 1 ( z ) ] 2 c [ 1 ( z ) ] q , z H ω , σ ( x , z ) z H ω , σ ( y , z ) c x y α ˜ [ 1 ( z ) ] q 1 ,

for all x , y Ω and z , ξ R n , where α ˜ = min { α , α 0 } and c c ( data , ω ) .

We similarly define

(3.4) λ ω , σ , i ( z ) ( z 2 + 1 ) 1 2 + ( q 1 ) a σ , i ( B ) [ ω ( z ) ] q 2 , Λ ω , σ , i ( z ) ( z 2 + 1 ) 1 2 g ( z ) + a σ , i ( B ) [ ω ( z ) ] q 2 .

Then, by following a similar proof for Proposition 2.1, (3.2) and (3.3), and using (1.2), we obtain

(3.5) σ [ ω ( z ) ] q H ω , σ , i ( z ) c ( [ ω ( z ) ] q + 1 ) , z H ω , σ , i ( z ) c g ( z ) + c a σ , i ( B ) [ ω ( z ) ] q 2 z , λ ω , σ , i ( z ) ξ 2 c z z H ω , σ , i ( z ) ξ , ξ , z z H ω , σ , i ( z ) c Λ ω , σ , i ( z ) , V ω , σ , i 2 ( z 1 , z 2 ; B ) c z H ω , σ , i ( z 1 ) z H ω , σ , i ( z 2 ) , z 1 z 2 , Λ ω , σ , i ( z ) λ ω , σ , i ( z ) g ( z ) + 1 q 1 c ( q ) g ( z ) ,

for some c c ( data ) whenever z , z 1 , z 2 , ξ R n . In particular, if ω > 0 , then there exists a constant c c ( data , ω ) such that

(3.6) σ ( q 1 ) [ 1 ( z ) ] q 2 ξ 2 c z z H ω , σ , i ( z ) ξ , ξ z H ω , σ , i ( z ) 1 ( z ) + z z H ω , σ , i ( z ) [ 1 ( z ) ] 2 c [ 1 ( z ) ] q ,

for all z , ξ R n . Two important quantities are defined as follows:

(3.7) E ω , σ ( x , t ) 0 t λ ω , σ ( x , s ) s d s , E ω , σ , i ( t ) E ω , σ , i ( t ; B ) 0 t λ ω , σ , i ( s ; B ) s d s .

Direct computations show that

E ω , σ ( x , t ) = ( 1 ( t ) 1 ) + ( 1 1 q ) a σ ( x ) ( [ ω ( t ) ] q ω q ) , E ω , σ , i ( t ) = ( 1 ( t ) 1 ) + ( 1 1 q ) a σ , i ( B ) ( [ ω ( t ) ] q ω q ) .

Through this, we define

(3.8) E ˜ ω , σ ( x , t ) 1 ( t ) + ( 1 1 q ) a σ ( x ) [ ω ( t ) ] q , E ˜ ω , σ , i ( t ) 1 ( t ) + ( 1 1 q ) a σ , i ( B ) [ ω ( t ) ] q .

Finally, we know from [18, Lemma 3.1] that they satisfy basic properties.

Lemma 3.1

Let B Ω be a ball. Then, the following properties hold:

  • For every s , t [ 0 , ) ,

    E ω , σ , i ( s ) E ω , σ , i ( t ) [ 1 + a σ , i ( B ) ( s 2 + t 2 + ω 2 ) ( q 1 ) 2 ] s t .

  • For all x B and t [ 0 , ) ,

    E ω , σ ( x , t ) E ω , σ , i ( t ) ( 1 1 q ) a ( x ) a i ( B ) ( [ ω ( t ) ] q ω q ) .

  • There exists a constant T 1 such that

    t 2 E ω , σ ( x , t ) and t 2 E ω , σ , i ( t )

    hold for all x Ω and t T .

  • There exists a constant c c ( q , Λ ) such that

    z + E ˜ ω , σ ( x , z ) c [ H ω , σ ( x , z ) + 1 ] , z + E ˜ ω , σ , i ( z ) c [ H ω , σ , i ( z ) + 1 ]

    hold for every x Ω and z R n .

4 Lipschitz estimates for frozen functionals

Let ω ( 0 , 1 ] . Let B τ B τ ( x c ) Ω be a ball with τ 1 , and fix u 0 W 1 , ( B τ ) . We now consider the unique solution v ω , σ u 0 + W 0 1 , q ( B τ ) to the Dirichlet problem

(4.1) v ω , σ min w u 0 + W 0 1 , q ( B τ ) B τ H ω , σ , i ( D w ) d x ,

where H ω , σ , i H ω . σ , i ( z ; B τ ) is defined in (3.1) 2 . Moreover, we obtain

B τ H ω , σ , i ( D v ω , σ ) d x B τ H ω , σ , i ( D u 0 ) d x .

Note that (3.3) and the direct method of the calculus of variations imply that such v ω , σ exists uniquely and the Euler-Lagrange equation of (4.1) is

B τ z H ω , σ , i ( D v ω , σ ) , D φ d x = 0 ,

for all φ W 0 1 , q ( B τ ) . Furthermore, we obtain from (3.3) that

(4.2) v ω , σ W loc 1 , ( B τ ) W loc 2,2 ( B τ ) , z H ω , σ , i ( D v ω , σ ) W loc 1,2 ( B τ ; R n )

(see [25, Chapter 8] and [18,30,31]). The following proposition is proven similar to the proof of [18, Proposition 4.1].

Proposition 4.1

Let v ω , σ u 0 + W 0 1 , q ( B τ ) be as in (4.1). Then, for any δ ( 0 , 1 ) , we have

(4.3) D v ω , σ L ( B 3 τ 4 ) c H ω , σ , i δ ( D u 0 L ( B τ ) ) D u 0 L ( B τ ) + c ,

for some c = c ( data , δ ) . Furthermore, whenever M is a number such that

(4.4) D v ω , σ L ( B ) + 1 M ,

for a ball B B τ , then there exists a constant c c ( data , δ ) such that the Caccioppoli-type inequality

(4.5) 3 B 4 D ( E ω , σ , i ( D v ω , σ ) κ ) + 2 d x c M δ B 2 n B ( E ω , σ , i ( D v ω , σ ) κ ) + 2 d x

holds for any κ 0 .

Proof

We simply write v v ω , σ , H i H ω , σ , i , H i H ω , σ , i , E i E ω , σ , i , and so forth, by omitting ω and σ . This is reasonable, since all the constants in this proposition are independent of ω and σ . Before proving this proposition, we choose χ ( 1 , ) and ε ( 0 , 1 ) such that

(4.6) χ = n n 2 , if n > 2 , 3 2 , if n = 2 ,

and

(4.7) ε < δ 4 + δ χ 1 2 χ .

As in the proof of [18, Proposition 4.1], we obtain

(4.8) s = 1 n B τ z z H i ( D v ) D D s v , D φ d x = 0 ,

for all φ W 1,2 ( B τ ) with supp φ B τ . Fix a ball B B τ and κ 0 . Let η C c 1 ( B ) be a cut-off function satisfying

η 1 in 3 B 4 , supp η 5 B 6 , and D η B 1 n .

By employing a method of the proof of [18, Proposition 4.1], using (1.4) and (3.5) 6 , and by recalling M 1 as in (4.4), we obtain

(4.9) B D [ η 2 ( E i ( D v ) κ ) + ] 2 d x c M 2 ε B 2 n B ( E i ( D v ) κ ) + 2 d x ,

with c depending on data and ε . By (4.7) and the fact 1 4 + δ χ 1 χ < 1 , we obtain 2 ε < δ , and hence, (4.5) holds.

Now, we prove (4.3). For T in Lemma 3.1, without loss of generality, we may assume

(4.10) D v ω , σ L ( B 3 τ 4 ) T 1 .

If not, clearly, (4.3) holds. For fixed constants τ 1 , τ 2 [ 3 τ 4 , 5 τ 6 ] with τ 1 < τ 2 , we consider the concentric balls

B 3 τ 4 B τ 1 B τ 2 B 5 τ 6 B τ B τ ( x c ) .

We let x 0 B τ 1 arbitrary and put r 0 ( τ 2 τ 1 ) 8 . Take

B ϱ ( x 0 ) B r 0 ( x 0 ) B τ 2 ,

and choose M 2 D v L ( B τ 2 ) . Then, we obtain from (4.10) that, for any ball B B τ 2 , (4.4) holds. Thus, by (4.9) and Sobolev embedding theorem, we obtain

B ϱ 2 ( x 0 ) ( E i ( D v ) κ ) + 2 χ d x 1 χ c M 2 ε B ϱ ( x 0 ) ( E i ( D v ) κ ) + 2 d x ,

where χ is defined in (4.6) and c c ( data , ε ) . Then, by [18, Lemma 2.5] with κ 0 = 0 , M 0 M ε and M 1 = M 2 = M 3 0 , we obtain that

E i ( D v ( x 0 ) ) c M ε χ χ 1 B r 0 [ E i ( D v ) ] 2 d x 1 2 ,

with c depending only on n and q . Then, in the same way as [18, Proposition 4.1], we have

E i ( D v L ( B τ 1 ) ) c ( τ 2 τ 1 ) n 2 E i ( D v L ( B τ 2 ) ) ( 2 ε + 1 ) χ 1 2 ( χ 1 ) B 5 τ 6 [ H i ( D v ) + 1 ] d x 1 2 ,

with c depending on data and ε . Note that, by (4.7),

ε < δ 4 + δ χ 1 2 χ χ 1 2 χ 2 ε χ < χ 1 2 ε χ + χ 1 < 2 ( χ 1 ) ( 2 ε + 1 ) χ 1 2 ( χ 1 ) < 1 .

By the aforementioned facts and Young’s inequality, we obtain that

E i ( D v L ( B τ 1 ) ) 1 2 E i ( D v L ( B τ 2 ) ) + c ( τ 2 τ 1 ) n γ * B 5 τ 6 [ H i ( D v ) + 1 ] d x γ * 1 2 E i ( D v L ( B τ 2 ) ) + c ( 5 τ ) n γ * [ 6 ( τ 2 τ 1 ) ] n γ * B 5 τ 6 [ H i ( D v ) + 1 ] d x γ * ,

with

γ * χ 1 ( 1 2 ε ) χ 1 .

Note that

( 4.7 ) 2 ε ( 4 + δ ) χ δ ( χ 1 ) δ ( χ 1 ) + ( 4 + δ ) ( χ 1 ) ( 4 + δ ) ( 2 ε χ ) + ( 4 + δ ) ( χ 1 ) 4 ( χ 1 ) ( 4 + δ ) ( ( 1 2 ε ) χ 1 ) χ 1 ( 1 2 ε ) χ 1 1 + δ 4 .

Moreover, since 0 < τ 2 τ 1 τ 3 , we obtain

5 τ 6 ( τ 2 τ 1 ) 5 2 1 .

Hence, we arrive at

E i ( D v L ( B τ 1 ) ) 1 2 E i ( D v L ( B τ 2 ) ) + c ( 5 τ ) n ( 1 + δ 4 ) [ 6 ( τ 2 τ 1 ) ] n ( 1 + δ 4 ) B 5 τ 6 [ H i ( D v ) + 1 ] d x 1 + δ 4 1 2 E i ( D v L ( B τ 2 ) ) + c ( τ 2 τ 1 ) n ( 1 + δ 4 ) B 5 τ 6 [ H i ( D v ) + 1 ] d x 1 + δ 4 ,

and then, we can easily obtain (4.3) by proving the remaining part similar to [18, Proposition 4.1].□

5 Proof of Theorem 1.2

First, we shall focus on the case s = 0 , and we will explain the case s > 0 at the end of this section.

5.1 Auxiliary convergence results

We first show that the function H ( ) defined in (1.3) indicates the absence of Laverentiev phenomenon. To do this, we have the following lemma regarding energy approximation. The proof proceeds in a manner similar to the proofs of [16, Section 5] and [20, Lemma 13].

Lemma 5.1

(Absence of Lavrentiev phenomenon) For H ( ) defined in (1.3) with (1.2), let v W loc 1.1 ( Ω ) be any function such that H ( , D v ) L loc 1 ( Ω ) . For every ball B Ω , there exists a sequence { v ε } W 1 , ( B ) such that v ε v in W 1,1 ( B ) and H ( , D v ε ) H ( , D v ) in L 1 ( B ) .

For other related results, we refer to the previous studies [1,3,4,7,29].

Now, we prove the existence of a sequence weakly converging to a local minimizer u in the W 1,1 -sense. Before that, we define by ( ε ) a quantity that satisfies ( ε ) 0 as ε 0 . Moreover, for fixed ε > 0 , we define by ε ( ω ) a quantity such that ε ( ω ) 0 as ω 0 . The property of these quantities converging to 0 is the only important factor, and their exact values may vary each time.

Lemma 5.2

Let u W loc 1,1 ( Ω ) be a local minimizer of ( ) in (1.1) with (1.2). Then, for any open ball B r Ω with 0 < r 1 , there exist a decreasing sequence { ε k } k = 1 in ( 0 , 1 ] with lim k ε k = 0 and a sequence { u ε k } k = 1 in W loc 1 , q ( B r ) such that

(5.1) u ε k u , weakly i n W 1,1 ( B r ) .

Proof

As in [18, Section 5.2], we simply write ω , ε { ω } , { ε } { ω k } k , { ε k } k , where { ω k } k and { ε k } k are two decreasing sequences of ω k , ε k ( 0 , 1 ] with ω k , ε k 0 . Furthermore, we will also write their subsequences as ω and ε .

By Lemma 5.1, there exists a sequence { u ˜ ε } in W 1 , ( B r ) so that

(5.2) u ˜ ε u in W 1,1 ( B r ) and ( u ˜ ε ; B r ) = ( u ; B r ) + ( ε ) .

We define the sequence

σ ε ( 1 + ε 1 + D u ˜ ε L q ( B r ) 2 q ) 1 .

Then, σ ε B r [ ω ( D u ˜ ε ) ] q d x 0 uniformly with respect to ω . Referring to [18], if we consider a unique solution u ω , ε u ˜ ε + W 0 1 , q ( B r ) to the Dirichlet problem

(5.3) u ω , ε min w u ˜ ε + W 0 1 , q ( B r ) ω , ε ( w ; B r ) min w u ˜ ε + W 0 1 , q ( B r ) B r H ω , σ ε ( x , D w ) d x ,

where H ω , σ ε was defined in (3.1) with σ σ ε , then we obtain

(5.4) u ω , ε C loc 1 , β ( B r ) , for some β ( 0 , 1 ) ,

(see also [25,30,31]). Note that z q 1 z + 1 c H ( x , z ) + c by (2.4)1 and q < 3 2 . Then, according to [18], we have the following two inequalities:

(5.5) ω , ε ( u ω , ε ; B r ) ( u ; B r ) + ε ( ω ) + ( ε )

and

(5.6) ( u ω , ε ; B r ) + σ ε B r [ ω ( D u ω , ε ) ] q d x ω , ε ( u ω , ε ; B r ) + ε ( ω ) + ( ε ) + c ω .

Then, we obtain from (5.5) and (3.2)1 that for any ε ( 0 , 1 ) , the sequence { u ω , ε } ω is uniformly bounded in W 1 , q ( B r ) . Then, up to not relabeled subsequences, we see that

(5.7) u ω , ε u ε , weakly in W 1 , q ( B r ) ,

as ω 0 and u ε u ˜ ε W 0 1 , q ( B r ) . Therefore, by completing the proof in the same manner as [18, Section 5.2], we obtain (5.1).□

5.2 Comparison estimates for frozen functionals

Fix ω , ε ( 0 , 1 ] , and consider u ω , ε as in (5.3). Let B ϱ ( x 0 ) B r be a ball. Here, the center of B r may differ from x 0 . Next, we take M such that

(5.8) M E ˜ ω , σ ε ( , D u ω , ε ) L ( B ϱ ( x 0 ) ) + 1 ,

where E ˜ ω , σ ε ( ) is defined in (3.8) with σ σ ε . By (5.4), the quantity M is finite.

Now, we rescale u and H ( ) on B ϱ ( x 0 ) defining

(5.9) u ω , ε , ϱ ( x ) u ω , ε ( x 0 + ϱ x ) ϱ , F ϱ ( x , z ) F ( x 0 + ϱ x , z ) , a ϱ ( x ) a ( x 0 + ϱ x ) , ϱ ( x , z ) H ( x 0 + ϱ x , z ) = F ϱ ( x , z ) + a ϱ ( x ) z q ,

with ( x , z ) 1 × R n . Next, as in (2.2) and (3.1) 2 , we define

(5.10) ( a ϱ ) σ ε ( x ) = a ϱ ( x ) + σ ε = a ( x 0 + ϱ x ) + σ ε , ( ϱ ) ω , σ ε ( x , z ) = F ϱ ( x , z ) + ( a ϱ ) σ ε ( x ) [ ω ( z ) ] q ,

with ( x , z ) 1 × R n . Since ϱ ( ) and ( ϱ ) ω , σ ε ( x , z ) are functions of the type in (1.3) and (3.1) 2 , respectively, the content of Section 3 is satisfied as well. By (5.3), u ω , ε , ϱ W 1 , q ( 1 ) is a local minimizer of the functional

W 1 , q ( 1 ) w 1 ( ϱ ) ω , σ ε ( x , D w ) d x .

From this point onward, we will keep the initial choices of ω and ε fixed. To simplify the notation, we will omit specifying the dependence on these parameters and simply abbreviate it as

(5.11) u ϱ ( x ) u ω , ε , ϱ ( x ) , H ϱ ( x , z ) ( ϱ ) ω , σ ε ( x , z ) ,

for ( x , z ) 1 × R n . By minimality of u ϱ , we obtain the Euler-Lagrange equation

(5.12) 1 z H ϱ ( x , D u ϱ ) , D ϕ d x = 0 , for all ϕ W 0 1 , q ( 1 ) .

Moreover, we obtain from (3.2) that

λ ϱ ( x , z ) ξ 2 c z z H ϱ ( x , z ) ξ , ξ , z z H ϱ ( x , z ) c Λ ϱ ( x , z ) , z H ϱ ( x , z ) z H ϱ ( y , z ) c ϱ α 0 x y α 0 g ( z ) + c ϱ α x y α [ ω ( z ) ] q 1

hold for any x , y 1 , z , ξ R n and for some c c ( data ) , where

λ ϱ ( x , z ) λ ω , σ ε ( x 0 + ϱ x , z ) , Λ ϱ ( x , z ) Λ ω , σ ε ( x 0 + ϱ x , z ) .

Now, we take a number β 0 ( 0 , 1 ) to be chosen later, and a vector h R n \ { 0 } satisfying

(5.13) 0 < h 1 2 8 β 0 .

Then, we let x c 1 2 + 2 h β 0 and fix a ball B h B h β 0 ( x c ) . Note that 8 B h 1 . We denote

(5.14) m m ( 8 B h ) D u ϱ L ( 8 B h ) + 1 .

As in (2.2), (2.3), (3.1), (3.4), (3.7), (3.8), (5.10), and (5.11), we denote the following notation:

a ˜ ϱ , i ( 8 B h ) ( a ϱ ) σ ε , i ( 8 B h ) = inf x 8 B h ( a ϱ ) σ ε ( x ) = inf x 8 B h a ( x 0 + ϱ x ) + σ ε , H ϱ , i ( z ) ( ϱ ) ω , σ ε , i ( z ; 8 B h ) F ϱ ( x c , z ) + a ˜ ϱ , i ( 8 B h ) [ ω ( z ) ] q , H ϱ , i ( t ) t g ( t ) + a ˜ ϱ , i ( 8 B h ) ( t 2 + ω 2 ) q 2 + 1 , λ ϱ , i ( z ) λ ϱ , i ( z ; 8 B h ) ( z 2 + 1 ) 1 2 + ( q 1 ) a ˜ ϱ , i ( 8 B h ) [ ω ( z ) ] q 2 , Λ ϱ , i ( z ) Λ ϱ , i ( z ; 8 B h ) ( z 2 + 1 ) 1 2 g ( z ) + a ˜ ϱ , i ( 8 B h ) [ ω ( z ) ] q 2 , E ϱ ( x , t ) 0 t λ ϱ ( x , s ) s d s , E ϱ , i ( t ) E ϱ , i ( t ; 8 B h ) 0 t λ ϱ , i ( s ; 8 B h ) s d s , E ˜ ϱ ( x , t ) 1 ( t ) + ( 1 1 q ) ( a ϱ ) σ ε ( x ) [ ω ( t ) ] q , E ˜ ϱ , i ( t ) 1 ( t ) + ( 1 1 q ) a ˜ ϱ , i ( 8 B h ) [ ω ( t ) ] q , V ϱ , i 2 ( z 1 , z 2 ; 8 B h ) V 1,1 ( z 1 ) V 1,1 ( z 2 ) 2 + a ˜ ϱ , i ( 8 B h ) V ω , q ( z 1 ) V ω , q ( z 2 ) 2 ,

for any x Ω , z , z 1 , z 2 R n , and t 0 . By (1.4), (3.5), and the second inequality of Lemma 3.1, we have

(5.15) σ ε [ ω ( z ) ] q H ϱ , i ( z ) c ( [ ω ( z ) ] q + 1 ) , z H ϱ , i ( z ) c ( [ ω ( z ) ] q 1 + 1 ) , λ ϱ , i ( z ) ξ 2 c z z H ϱ , i ( z ) ξ , ξ , z z H ϱ , i ( z ) c Λ ϱ , i ( z ) , V ϱ , i 2 ( z 1 , z 2 ; 8 B h ) c z H ϱ , i ( z 1 ) z H ϱ , i ( z 2 ) , z 1 z 2 ,

for all z , z 1 , z 2 , ξ R n , and

(5.16) E ϱ ( x , t ) E ϱ , i ( t ) c h α β 0 ϱ α [ ω ( t ) ] q ,

for every x 8 B h and t 0 , with c c ( data ) . Moreover, (5.8) and (5.14) imply that

(5.17) M E ˜ ϱ ( , D u ϱ ) L ( 1 ) + 1

and

(5.18) a ˜ ϱ , i ( 8 B h ) [ ω ( m ) ] q c ( a ϱ ) σ ε ( ) [ ω ( D u ϱ ) ] q L ( 8 B h ) + c c M , m ω ( m ) c M ,

hold for some constant c c ( q , a L ) . By (5.15), the direct methods of the calculus of variations, and strict convexity, we obtain a unique minimizer v u ϱ + W 0 1 , q ( 8 B h ) of the functional

(5.19) u ϱ + W 0 1 , q ( 8 B h ) w 8 B h H ϱ , i ( D w ) d x .

Also, we obtain its Euler-Lagrange equation

8 B h z H ϱ , i ( D v ) , D ϕ d x = 0 for all ϕ W 0 1 , q ( 8 B h )

and the minimality condition

8 B h H ϱ , i ( D v ) d x 8 B h H ϱ , i ( D u ϱ ) d x .

We use Proposition 4.1 and refer [18, Lemma 5.2] to obtain the following lemma:

Lemma 5.3

Let δ 1 ( 0 , 1 ) . Then, we have the inequalities

D v L ( 6 B h ) c m 1 + δ 1

and

2 B h D ( E ϱ , i ( D v ) κ ) + 2 d x c m δ 1 h 2 β 0 4 B h ( E ϱ . i ( D v ) κ ) + 2 d x ,

where c depends on data and δ 1 .

Also, we may obtain a comparison estimate in the same way as [18, Lemma 5.3].

Lemma 5.4

Let u ϱ W 1 , q ( 1 ) be as in (5.9) and v u ϱ + W 0 1 , q ( 8 B h ) be a minimizer of (5.19). For any δ 2 ( 0 , 1 2 ) , we obtain the inequality

8 B h V ϱ , i 2 ( D u ϱ , D v ; 8 B h ) d x c h β 0 α ˜ M 1 δ 2 2 ϱ α 8 B h ( D u ϱ + 1 ) q 1 + δ 2 d x + c h β 0 α ˜ M 1 δ 2 2 ϱ α 0 8 B h ( D u ϱ + 1 ) 3 δ 2 d x ,

where c c ( data , δ 2 ) and α ˜ = min { α , α 0 } . Here, M is a number satisfying (5.8), and hence, (5.17).

5.3 Fractional Caccioppoli inequality

Lemma 5.5

Let u ω , ε W 1 , q ( B r ) be as in (5.3). For any δ 1 , δ 2 ( 0 , 1 ) and for a ball B ϱ ( x 0 ) B r , the inequality

(5.20) B ϱ 2 ( x 0 ) ( E ω , σ ε ( x , D u ω , ε ) κ ) + 2 χ d x 1 χ + ϱ 2 β n [ ( E ω , σ ε ( , D u ω , ε ) κ ) + ] β , 2 ; B ϱ 2 ( x 0 ) 2 c M 2 s 1 B ϱ ( x 0 ) ( E ω , σ ε ( , D u ω , ε ) κ ) + 2 d x + c M 2 s 2 ϱ 2 α B ϱ ( x 0 ) ( D u ω , ε + 1 ) 2 ( q 1 + δ 2 ) d x + c M 2 s 3 ϱ α B ϱ ( x 0 ) ( D u ω , ε + 1 ) q 1 + δ 2 d x + c M 2 s 3 ϱ α 0 B ϱ ( x 0 ) ( D u ω , ε + 1 ) 3 δ 2 d x

holds provided

(5.21) β ( 0 , α * ) with α * α ˜ α ˜ + 2 , χ χ ( β ) n n 2 β ,

and

(5.22) E ˜ ω , σ ε ( , D u ω , ε ) L ( B ϱ ( x 0 ) ) + 1 M ,

where c c ( data , δ 1 , δ 2 , β ) and

(5.23) s 1 s 1 ( δ 1 ) δ 1 2 , s 2 s 2 ( δ 2 ) 1 δ 2 , s 3 s 3 ( δ 1 , δ 2 ) 2 + ( q + 1 ) δ 1 δ 2 2 2 .

Proof

First, our goal is to prove the inequality

(5.24) B h τ h ( E ϱ ( D u ϱ ) κ ) + 2 d x c ˜ h 2 α * M 2 s 1 4 B h ( E ϱ ( x , D u ϱ ) κ ) + 2 d x + c ˜ h 2 α * M 2 s 2 ϱ 2 α 8 B h ( D u ϱ + 1 ) 2 ( q 1 + δ 2 ) d x + c ˜ h 2 α * M 2 s 3 ϱ α 8 B h ( D u ϱ + 1 ) q 1 + δ 2 d x + c ˜ h 2 α * M 2 s 3 ϱ α 0 8 B h ( D u ϱ + 1 ) 3 δ 2 d x ,

with c ˜ c ˜ ( data , δ 1 , δ 2 ) .

Recall that basic properties of difference quotients yield

B h τ h ( E ϱ , i ( D v ) κ ) + 2 d x h 2 2 B h D ( E ϱ , i ( D v ) κ ) + 2 d x ,

where κ 0 is any number (recall that h h β 0 ). We obtain from this and the second inequality in Lemma 5.3 that

(5.25) B h τ h ( E ϱ , i ( D v ) κ ) + 2 d x c h 2 ( 1 β 0 ) m δ 1 4 B h ( E ϱ , i ( D v ) κ ) + 2 d x ,

with c c ( data , δ 1 ) . Recall that E ϱ , i ( z ) E ϱ , i ( z ; 8 B h ) .

We now write down a few auxiliary estimates. First, we obtain from (5.16), (5.14), and (5.18) 2 that

(5.26) 4 B h E ϱ ( x , D u ϱ ) E ϱ , i ( D u ϱ ) 2 d x c h 2 α β 0 ϱ 2 α 4 B h [ ω ( D u ϱ ) ] 2 q d x c h 2 α β 0 m 2 ( 1 δ 2 ) ϱ 2 α 4 B h D u ϱ 2 ( q 1 + δ 2 ) d x c h α β 0 M 2 ( 1 δ 2 ) ϱ 2 α 4 B h D u ϱ 2 ( q 1 + δ 2 ) d x ,

for c c ( n , q ) . To obtain the second auxiliary inequality, we obtain from (5.17) and Lemma 3.1 that

4 B h E ϱ , i ( D u ϱ ) E ϱ , i ( D v ) 2 d x c 4 B h D u ϱ D v 2 d x + c [ a ˜ ϱ , i ( 8 B h ) ] 2 4 B h ( D u ϱ 2 + D v 2 + ω 2 ) q 1 D u ϱ D v 2 d x = c 4 B h ( D u ϱ 2 + D v 2 + 1 ) 1 2 ( D u ϱ 2 + D v 2 + 1 ) 1 2 D u ϱ D v 2 d x + c [ a ˜ ϱ , i ( 8 B h ) ] 2 4 B h ( D u ϱ 2 + D v 2 + ω 2 ) q 1 D u ϱ D v 2 d x c m 1 + δ 1 4 B h ( D u ϱ 2 + D v 2 + 1 ) 1 2 2 D u ϱ D v 2 d x + c [ a ˜ ϱ , i ( 8 B h ) ] 2 m q ( 1 + δ 1 ) 4 B h ( D u ϱ 2 + D v 2 + ω 2 ) ( q 2 ) 2 D u ϱ D v 2 d x ( 2.1 ) c m 1 + δ 1 4 B h V 1,1 ( D u ϱ ) V 1,1 ( D v ) 2 d x + c a ˜ ϱ , i ( 8 B h ) [ ω ( m ) ] q m q δ 1 4 B h a ˜ ϱ , i ( 8 B h ) V ω , q ( D u ϱ ) V ω , q ( D v ) 2 d x c ( m 1 + δ 1 + M m q δ 1 ) 4 B h V ϱ , i 2 ( D u ϱ , D v ; 8 B h ) d x ,

where c depends on data and δ 1 . Here, the last line is obtained by using (5.18)1. Applying (5.18) 2 , we have

4 B h E ϱ , i ( D u ϱ ) E ϱ , i ( D v ) 2 d x c M 1 + q δ 1 4 B h V ϱ , i 2 ( D u ϱ , D v ; 8 B h ) d x .

Using Lemma 5.4, we obtain the second auxiliary estimate

(5.27) 4 B h E ϱ , i ( D u ϱ ) E ϱ , i ( D v ) 2 d x c h β 0 α ˜ M 2 + q δ 1 δ 2 2 ϱ α 8 B h ( D u ϱ + 1 ) q 1 + δ 2 d x + c h β 0 α ˜ M 2 + q δ 1 δ 2 2 ϱ α 0 8 B h ( D u ϱ + 1 ) 3 δ 2 d x ,

for some c c ( data , δ 1 , δ 2 ) .

Now, as in [18, Lemma 5.4], we deduce from (5.25) that

B h τ h ( E ϱ ( x , D u ϱ ) κ ) + 2 d x c h 2 ( 1 β 0 ) m δ 1 4 B h ( E ϱ ( x , D u ϱ ) κ ) + 2 d x + c 4 B h E ϱ ( x , D u ϱ ) E ϱ , i ( D u ϱ ) 2 d x + c m δ 1 4 B h E ϱ , i ( D u ϱ ) E ϱ , i ( D v ) 2 d x ,

for some c c ( data , δ 1 ) . Take

β 0 2 α ˜ + 2 .

Then, we have

(5.28) β 0 α ˜ = 2 ( 1 β 0 ) = 2 α * .

Using (5.26), (5.27), (5.28), and (5.18) 2 , we conclude with (5.24).

By patching up estimates (5.24) from a dyadic covering argument as in Step 2 in the proof of [18, Lemma 5.4], (5.20) holds.□

5.4 Proof of Theorem 1.2 (i)

First, we take δ 1 and δ 2 in Lemma 5.5 to satisfy the following conditions:

s 1 ( δ 1 ) χ χ 1 + 1 2 = n δ 1 4 β + 1 2 < 1 , s 1 ( δ 1 ) χ 1 + s 2 ( δ 2 ) = ( n 2 β ) δ 1 4 β + 1 δ 2 < 1 , s 1 ( δ 1 ) χ 1 + s 3 ( δ 1 , δ 2 ) = ( n 2 β ) δ 1 4 β + 1 + ( q + 1 ) δ 1 δ 2 2 2 < 1 ,

and

0 < δ 2 1 2 min 1 + α n q , α 0 3 n < 1 2 .

Then, we obtain the C 0 , 1 -bounds for u ω , ε using nonlinear potentials in the same way as in [18, Proposition 5.5]. We refer to [17,33] and [18, Section 2.4] for details on nonlinear potentials.

Lemma 5.6

Let u ω , ε W 1 , q ( B r ) be as in (5.3). Then, the inequality

(5.29) E ˜ ω , σ ε ( , D u ω , ε ) L ( B t ) c ( s t ) n ϑ H ω , σ ε ( , D u ω , ε ) + 1 L 1 ( B s ) ϑ + c

holds for any concentric balls B t B s B r with r 1 . Here, c c ( data ) and ϑ ϑ ( n , q , α , α 0 ) 1 .

Proof of Theorem 1.2 (i)

By (5.5) and (5.29), we obtain

E ˜ ω , σ ε ( , D u ω , ε ) L ( B t ) c ( r t ) n ϑ [ ( u ; B r ) + ε ( ω ) + ( ε ) + B r ] ϑ + c .

Recalling (3.8), we have

(5.30) D u ω , ε L ( B t ) c ( r t ) n ϑ [ ( u ; B r ) + ε ( ω ) + ( ε ) + B r ] ϑ + c .

Then, passing to not relabeled subsequences, we can upgrade the convergence of (5.7) to u ω , ε * u ε in W 1 , ( B t ) as ω 0 for every ε > 0 . Letting ω 0 in (5.30), we obtain

(5.31) D u ε L ( B t ) c ( r t ) n ϑ [ ( u ; B r ) + ( ε ) + B r ] ϑ + c ,

for every ε > 0 . Then, we can also upgrade the convergence of (5.1) to u ε * u in W 1 , ( B t ) as ε 0 . Thus, letting ε 0 in (5.31), taking t = r 2 , and renaming 2 ϑ into ϑ yield (1.10). Finally, by referencing [18, Subsections 5.9 and 5.10], we obtain

B ϱ D u ( D u ) B ϱ 2 d x c ϱ 2 α ˜ β ˜ n + 2 β ˜ + α ˜ ,

for some c 1 and β ˜ ( 0 , 1 ) depending only on data , dist ( Ω 0 , Ω ) and ( u ; Ω ) . Hence, Du is locally Hölder continuous when s = 0 .

Now, we briefly explain how to obtain Theorem 1.2(i) in the non-singular case s > 0 . To reach the conclusion, we use the functional s , ε as in (5.3), and all subsequent estimates remain independent of s and ε . Additionally, the approximation and the convergence occur only with respect to ε , which implies (1.10). By employing the same reasoning and setting ω to s , we conclude the proof of this subsection.□

5.5 Proof of Theorem 1.2 (ii)

This proof follows from [18, Section 5.11]. Additionally, we refer to [17]. Through the above steps, we already know that Du is locally Hölder continuous with exponent β . As in [18], we set M D u L ( Ω ) + [ D u ] 0 , β ; Ω + 1 < and take

A r ( z ) z H r α ˜ , i ( z ) = z F ( x c , z ) + q a r α ˜ , i ( B r ) [ s ( z ) ] q 2 z ,

for z R n . Then, we obtain from (3.2)4 that

z H r α ˜ , i ( z ) z H ( x , z ) c r α ˜ [ 1 ( z ) ] q 1

holds for any x B r and z R n . Also, for a solution v u + W 0 1 , q ( B r ) of the equation div A r ( D v ) = 0 in B r , we have

(5.32) D v L ( B r 2 ) c M 2 ,

as in [18, (5.61)], where c depends on data. Then, we obtain from these and [18, (5.65)] that

D u D v L 2 ( B r 2 ) 2 c r n + α ˜

holds for some c c ( data ) (see also [17, (10.3)]). Next, defining the matrix [ A ( x ) ] i j z j A r i ( D v ( x ) ) implies that there exists λ λ ( data , s , M ) > 0 , independent of r , such that λ I A ( x ) ( 1 λ ) I holds for a.e. x B r 2 , where I is the identity matrix. Indeed, we see from (2.4) 2 , (2.4)3, and (5.32) that there exists a constant c c ( data , M ) such that

ξ 2 ( M 4 + 1 ) 1 2 c A ( x ) ξ , ξ , A ( x ) c [ g ( M 2 ) + s q 2 ] ,

for a.e. x B r 2 and ξ R n . This is the most crucial part of this proof. The remaining part proceeds with the proof in the same way as in [17, (10.6)], and hence, the proof is complete.

Acknowledgments

The authors would like to express their sincere gratitude to the anonymous referees who provided valuable comments and suggestions on the earlier version, which have greatly improved the quality and clarity of the manuscript.

  1. Funding information: This work was supported by National Research Foundation of Korea (NRF) grant funded by the Korea government [Grant Nos. RS-2023-00217116 and RS-2025-00555316].

  2. Author contributions: All authors contributed equally to the manuscript and read and approved the final manuscript.

  3. Conflict of interest: The authors state no conflict of interest.

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Received: 2024-07-28
Revised: 2025-03-24
Accepted: 2025-05-02
Published Online: 2025-07-02

© 2025 the author(s), published by De Gruyter

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

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