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<article xmlns:xlink="http://www.w3.org/1999/xlink">
  <front>
    <journal-meta />
    <article-meta>
      <title-group>
        <article-title>On Variational Problem with Nonstandard Growth Conditions for the Restoration of Clouds Corrupted Satellite Images</article-title>
      </title-group>
      <contrib-group>
        <contrib contrib-type="author">
          <string-name>Pavel Khanenko</string-name>
          <xref ref-type="aff" rid="aff2">2</xref>
          <xref ref-type="aff" rid="aff4">4</xref>
          <xref ref-type="aff" rid="aff5">5</xref>
        </contrib>
        <contrib contrib-type="author">
          <string-name>Peter I. Kogut</string-name>
          <xref ref-type="aff" rid="aff1">1</xref>
          <xref ref-type="aff" rid="aff3">3</xref>
          <xref ref-type="aff" rid="aff4">4</xref>
        </contrib>
        <contrib contrib-type="author">
          <string-name>Mykola Uvarov</string-name>
          <xref ref-type="aff" rid="aff0">0</xref>
          <xref ref-type="aff" rid="aff4">4</xref>
          <xref ref-type="aff" rid="aff5">5</xref>
        </contrib>
        <aff id="aff0">
          <label>0</label>
          <institution>Department of Computational Physics, G. V. Kurdyumov Institute for Metal Physics</institution>
          ,
          <addr-line>Kyiv</addr-line>
          ,
          <country country="UA">Ukraine</country>
        </aff>
        <aff id="aff1">
          <label>1</label>
          <institution>Department of Differential Equations, Oles Honchar Dnipro National University</institution>
        </aff>
        <aff id="aff2">
          <label>2</label>
          <institution>EOS Data Analytics Ukraine</institution>
          ,
          <addr-line>Desyatynny lane, 5, 01001 Kyiv</addr-line>
          ,
          <country country="UA">Ukraine</country>
        </aff>
        <aff id="aff3">
          <label>3</label>
          <institution>EOS Data Analytics Ukraine</institution>
          ,
          <addr-line>Gagarin av., 103a, Dnipro</addr-line>
          ,
          <country country="UA">Ukraine</country>
        </aff>
        <aff id="aff4">
          <label>4</label>
          <institution>Gagarin av.</institution>
          ,
          <addr-line>72, 49010 Dnipro</addr-line>
          ,
          <country country="UA">Ukraine</country>
        </aff>
        <aff id="aff5">
          <label>5</label>
          <institution>Max Planck Institute for Chemical Physics of Solids</institution>
          ,
          <addr-line>01187 Dresden</addr-line>
          ,
          <country country="DE">Germany</country>
        </aff>
      </contrib-group>
      <abstract>
        <p>Sensitivity to weather conditions, and specially to clouds, is a severe limiting factor to the use of optical remote sensing for Earth monitoring applications. Typically, the optical satellite images are often corrupted because of poor weather conditions. As a rule, the measure of degradation of optical images is such that one can not rely even on the brightness inside of the damaged regions. As a result, some subdomains of such images become absolutely invisible. So, there is a risk of information loss in optical remote sensing data. In view of this, we propose a new variational approach for exact restoration of multispectral satellite optical images. We discuss the consistency of the proposed variational model, give the scheme for its regularization, derive the corresponding optimality system, and discuss the algorithm for the practical implementation of the reconstruction procedure. Experimental results are very promising and they show a significant g ain o ver b aseline m ethods u sing t he r econstruction through linear interpolation between data available at temporally-close time instants.</p>
      </abstract>
      <kwd-group>
        <kwd>eol&gt;Risk of cloud distortion of satellite images</kwd>
        <kwd>Risk of information loss</kwd>
        <kwd>Image restoration</kwd>
        <kwd>Variational approach</kwd>
      </kwd-group>
    </article-meta>
  </front>
  <body>
    <sec id="sec-1">
      <title>1. Introduction</title>
      <p>is such that we can not rely even on the brightness inside of the damaged regions. As a result,
there is a risk of information loss, some subdomains of such images become absolutely invisible.
So, there is a great deal of missing information in optical remote sensing data, and a huge
gap still exists between the satellite data we acquire and the data we require. Therefore, the
reconstruction of missing information in remote sensing data becomes an active research field.</p>
      <p>Many solutions have been developed to remove the clouds from multispectral images. (for the
technical review, we refer to [2]). Formally, the present traditional algorithms can be primarily
classified into four categories: 1) spatial-based methods, without any other auxiliary information
source; 2) spectral-based methods, which extract the complementary information from other
spectra; 3) multitemporal-based methods, which extract the complementary information from
other data acquired at the same position and at diferent time periods; and 4) hybrid methods,
which extract the complementary information by a combination of the three previous approaches.
In parallel to the traditional approach, data-driven machine learning algorithms are actively
developing since 2014 [3]. However, the necessity of large datasets and volatility to errors in
input data limits its performance.</p>
      <p>Our main efort in this research is to develop a new variational model for the exact restoration
of the damaged multi-band optical satellite images that will meet demands from the agro
application, that is, it must be applicable for large areas in diferent climate zones, and preserves
the crop fields borders within damaged regions. In some sense, this model combines the
spacialbased method with the multitemporal one. Therefore, in contrast to the standard
variationalbased methods that are often optimased for a specific region or significantly blur textures, (see,
for instance, [4] and the references therein), we focus on the global texture reconstruction inside
damage regions. With that in mind we assume that the texture of a corrupted image can be
predicted through a number of past cloud-free images of the same region from the time series.
In order to describe the texture of background surface in the damage region, we follow the
paper [5], where the authors experimentally checked the hypothesis that the essential geometric
contents of a color image is contained in the level lines of the corresponding total spectral
energy of such image.</p>
      <p>We also pay much attention to the faithfulness of the reconstruction problem in the framework
of the proposed model and supply this approach by the rigorous mathematical substantiation.
The experiments undertaken in this study confirmed the eficacy of the proposed method and
revealed that it can acquire plausible visual performance and satisfactory quantitative accuracy
for agro scenes with rather complicated texture of background surface.</p>
    </sec>
    <sec id="sec-2">
      <title>2. Preliminaries</title>
      <p>
        Let Ω ⊂ R2 be a bounded image domain with a Lipschitz boundary Ω . With each particular
image ⃗ = [1(), 2(), . . . ,  ()] : Ω → R , where each coordinate represents the
intensity of the corresponding spectral channel, we associate the panchromatic image  (the
so-called total spectral energy of ⃗)
() =  11() + . . .    ().
(
        <xref ref-type="bibr" rid="ref1">1</xref>
        )
Here,  1, . . . ,   are some weight coeficients.
      </p>
      <p>Let  ⊂ Ω be a Borel set with non empty interior and suficiently regular boundary and
such that |Ω ∖ | &gt; 0. We call  the damage region. Let ⃗0 ∈ 2(Ω ∖ ; R ) be an image of
interest which is assumed to be corrupted by clouds, and  is the zone of missing information.</p>
      <p>As it was mentioned before, we deal with the case where we have no information about
the original image ⃗0 inside . Instead of this, we assume that the texture of background
surface in the damage region  can be predicted with some accuracy by a number of past
cloud-free images of the same region from the time series of satellite images. Unlike the
wellknown ’chronochrome method’ [6] which essentially assumes that the background in  is
stationary in wide sense, we admit that the image time series follows smooth variations over land
(background), the time-series data are strictly chronological, and display regular fluctuations.</p>
      <p>
        Let {⃗−1 , . . . , ⃗− } be a given collection of past cloud-free images of the same region,
where we set ⃗ = ⃗0. We suppose that each cloud-free image of this time series should be well
co-registered with ⃗0 ∈ 2(Ω ∖ ; R ) in Ω ∖  [7]. With each particular image ⃗− in this
series, we associate its total spectral energy − using the standard rule (
        <xref ref-type="bibr" rid="ref1">1</xref>
        ). So, each element
of the time series {, −1 , . . . , − } is well-defined in Ω.
      </p>
      <p>Let * be a predicted total spectral energy of ⃗0 in the damage region . This prediction can
be done following the regularized regression model and the available information in the time
series {, −1 , . . . , − } (for the details we refer to [8]).</p>
      <p>ℒ() =
 1 ∫︁ [︁
|| 
−1 −</p>
      <p>∑︁ −1 − ]︁2 
=2
+
 1</p>
      <p>
        ∫︁
|Ω ∖ | Ω∖
[︁
 −
∑−1︁ − ]︁2  + ‖ ‖2R−1
=1
→ inf, (
        <xref ref-type="bibr" rid="ref2">2</xref>
        )
where  &gt; 0 is the regularization parameter,  1 &gt; 0 and  2 &gt; 0 are the parameters that control
the importance of the prediction and estimation terms, respectively. Seeing that the prediction
and estimation errors in (
        <xref ref-type="bibr" rid="ref2">2</xref>
        ) are normalized by the volume of samples contributing to each term,
we can constrain the values of  1 =  ∈ [0, 1] and  2 = 1 −  to control their relevance with a
single parameter  .
      </p>
      <p>As a result, setting 0 = Argmin ℒ(), the total spectral energy * in the damage region 
can be estimated as follows * =  in , where
̂︀</p>
      <p>−1
̂︀() = ∑︁ 0− (),
=1</p>
      <p>In order to reconstruct the texture (or geometry) of ⃗0 in the damage region , we assume
that predicted total energy * is a function of bounded variation, i.e. * ∈  (), and all
spectral channels of the damaged image should share the geometry of the panchromatic image
* ∈ 2() in . Hence, at most all points of almost all level sets of * ∈ () we can define
a normal vector  (), i.e., it formally satisfies (,  * ) = |∇* | and | | ≤ 1 a.e. in .</p>
    </sec>
    <sec id="sec-3">
      <title>3. Problem Statement</title>
      <p>say that a function ⃗ = [1, 2, . . . ,  ] : Ω
In view of the risk of cloud distortion, the problem is to reconstruct the original multi-band
image ⃗0 in the damage region  using the knowledge of its texture (geometry) on the subset
 together with the exact information about this image in Ω ∖  (the undamaged region). We
→ R is the result of restoration of a cloud
corrupted image ⃗0 :  → R if for given regularization parameters &gt;0 , &gt; 1, and   &gt;0,
 = 1, 2, each spectral component  is the solution of the following constrained minimization
problem with the nonstandard growth energy functional
()
(, ) :=</p>
      <p>Ω () |∇()|()  +
∫︁
∫︁
1
⃒
Ω∖ ⃒⃒ ∇ * ( − 0,)⃒⃒  +  2
Ω∖
|() − 0,()| 
Cauchy law () = 1+(1/)2 with an appropriate  &gt; 0;
and :[0, ∞) → (0, ∞) is the edge-stopping function which we take it in the form of the
•  ∈ ∞(, R2) is a given vector field such that</p>
      <p>| ()| ≤ 1 and ( (), ∇* ())R2 = |∇* ()| a.e. in ;
• ( * ) () determines the convolution of function  with the two-dimensional Gaussian
iflter kernel  , where the parameter &gt;0 determines the spatial size of the image details
which are removed by this 2D filter;</p>
      <p>By default we assume that the functions 0, and * are extended by zero outside of domains
Ω ∖  and , respectively.</p>
      <p>
        The proposed model (
        <xref ref-type="bibr" rid="ref3">3</xref>
        ) provides a completely new approach to restoration of non-smooth
multi-spectral images ⃗0 with the gap in damage region. The main characteristic feature of this
model is that we involve into consideration the energy functional with the nonstandard growth
condition. The variable character of the exponent () provides more flexibility in terms of
regularity for the recovered images. Since the first term in (
        <xref ref-type="bibr" rid="ref3">3</xref>
        ) is the regularization and the
second one is the so-called data fidelity, it is worth to emphasize the role of the rest terms in
(
        <xref ref-type="bibr" rid="ref3">3</xref>
        ). Taking into account the fact that the magnitude F(()) is close to one at those points,
where the spectral energy  is slowly varying, and this value is close to zero at the edges of ,
it follows that the edge information in the non-damage zone for the reconstruction is derived
from the given image ⃗0. So, in view of the estimate
|(∇ * )|2 − |(∇  * 0,)|
|(∇ * )| + |(∇ * 0,)| ⃒⃒ |(∇ * )| − |(∇  * 0,)| ⃒⃒ 
⃒
⃒
⃒
⃒
2 ⃒
︁) ⃒⃒ 
,
≤
      </p>
      <p>2
2‖ ‖1(Ω−Ω)  1|Ω| 23 (︃ ∫︁</p>
      <p>⃒
Ω∖ ⃒⃒ ∇ * ( − 0,)⃒⃒ 
the third term is also fidelity term which forces the texture (or topological map) of minimizer 
in domain Ω ∖  to stay close to the texture of a given spectral energy ⃗0,.</p>
      <p>
        As for the last term in (
        <xref ref-type="bibr" rid="ref3">3</xref>
        ), we notice that since  ∈ ∞(, R2) is a vector field with indicated
properties, it follows that  () has the direction of the normal to the level lines of * . Therefore,
the counterclockwise rotation of angle /2 , denoted by  ⊥, represents the tangent vector to the
level lines of * . In this case, if the spectral channels  share the geometry of the panchromatic
image * , we have
︁(
 ⊥, ∇
︁)
      </p>
      <p>R2</p>
      <p>= 0,  = 1, . . . ,  in .</p>
      <p>Therefore, we impose them in the energy functional  in the form of the last term.
to compute  (1, 2) by first regularizing  by the equation</p>
      <p>In practice, at the discrete level,  can be defined by the relation  (1, 2) = |∇∇̂̂︀︀((11,,22))| when
∇̂︀(1, 2) ̸= 0, and  (1, 2) = 0 when ∇̂︀(1, 2) = 0. However, a better choice would be


= div
︂(
̂︀
∇ )︂
|∇|
in (0, ∞) × Ω,
coupled with the initial and Neumann boundary conditions
Then, for any  ≥
[9, 10] for the details)
(0, 1, 2) = ̂︀(1, 2), for a.a. (1, 2) ∈ Ω,


= 0 on Ω.
0, there is a vector field  () ∈ ∞(Ω)</p>
      <p>with ‖ ()‖∞(Ω) ≤ 1 such that (see
and


( (), ∇()) = |∇()| in Ω,</p>
      <p>( (),  ) = 0 on Ω,
= div ( ()) in the sense of distributions in (0, ∞) × Ω.</p>
      <p>As a result, in order to characterize the texture of the cloud contaminated image ⃗0 in the
damage region , we may take  =  () for some small value of  &gt; 0. As was mentioned in
[9], following this way, we do not not distort the geometry of  in an essential way.</p>
      <p>So, the novelty of the model that we propose, is that the edge information for the
multispectral restoration in Ω is accumulated in the variable exponent () which we derive from
̂︀
the time series and initial data.</p>
    </sec>
    <sec id="sec-4">
      <title>4. Existence Result</title>
      <p>
        In this section we show that constrained minimization problem (
        <xref ref-type="bibr" rid="ref3">3</xref>
        ) is consistent and admits at
least one solution (, ) ∈ Ξ , where () = F(()) in Ω . We note that because of
the specific form of the energy functional (, ) in (
        <xref ref-type="bibr" rid="ref3">3</xref>
        ), the standard approaches are no longer
applicable in its study, especially with respect to the existence of minimizers and their basic
properties. It makes the minimization problem (
        <xref ref-type="bibr" rid="ref3">3</xref>
        ) rather challenging.
      </p>
      <p>We begin with some auxiliary results which will play a crucial role in the sequel.</p>
      <p>Lemma 4.1. Let {}∈N be a sequence of measurable non-negative functions  : Ω →
[ 0, ∞) such that {}∈N are uniformly bounded in 1(Ω) and () → () almost
everywhere in Ω for some  ∈ 1(Ω). Let { = 1 +  (|(∇ * )|)}∈N be the corresponding
sequence of variable exponents. Then
(·) → (·) = 1 +  (|(∇ * ) (·)|)
 := 1 +  ≤ () ≤  := 2,</p>
      <p>|∇ ( − )| ()  ≤ ‖  ‖1(Ω−Ω) ‖‖1(Ω),
() = 1 +
∫︁
,</p>
      <p>
        Then 1-boundedness of {}∈N guarantees the existence of a positive value  ∈ (
        <xref ref-type="bibr" rid="ref1">0, 1</xref>
        ) such
that estimate (
        <xref ref-type="bibr" rid="ref4">4</xref>
        ) holds true for all  ∈ N.
      </p>
      <p>Moreover, as follows from the estimate</p>
      <p>⃒⃒ |(∇ * ) ()|2 − |(∇  * ) ()|2
|() − ()| ≤ 2 ⃒⃒⃒⃒ (︁ 2 + |(∇ * ) ()|2︁) (︁
⃒⃒⃒
2 + |(∇ * ) ()|2︁) ⃒⃒⃒
Ω
and smoothness of the function ∇ (·) , there exists a positive constant  &gt; 0 independent
of  such that</p>
      <p>|∇ ( − ) − ∇  ( − )| , ∀ ,  ∈ Ω
|() − ()| ≤</p>
      <p>
        ||(∇ * ) ()| − |(∇  * ) ()||
non-negative value  ≥ 0 such that  =
sequence to the problem (
        <xref ref-type="bibr" rid="ref3">3</xref>
        ), i.e.
      </p>
      <p>inf
Since max∈Ω |()| ≤  and each element of the sequence {}∈N has the same modulus of
continuity, it follows that this sequence is uniformly bounded and equi-continuous. Hence, by
Arzelà–Ascoli Theorem the sequence {}∈N is relatively compact with respect to the strong
topology of (Ω) . Taking into account that the set S is closed with respect to the uniform
convergence and () → () almost everywhere in Ω , we deduce: (·)
Ω as  →</p>
      <p>∞, where () = 1 +  (|(∇ * ) ()|) in Ω. The proof is complete.</p>
      <p>
        Following in many aspects the resent studies [11, 12], we give the following existence result.
0, ∈ 2(Ω ∖ ), the minimization problem (
        <xref ref-type="bibr" rid="ref3">3</xref>
        ) admits at least one solution (, 
Theorem 4.2. For each  = 1, . . . ,  and given &gt;0,  1&gt;0,  2&gt;0,  ∈ ∞(, R2), and
) ∈ Ξ.

Proof. Since Ξ ̸
= ∅ and 0 ≤ (, ) &lt; +∞ for all (, ) ∈ Ξ , it follows that there exists a
→ (·) uniformly in
(, ). Let {(, )}∈N ⊂ Ξ be a minimizing
(, ) ∈ Ξ,  () = 1 +  (|(∇ * ) ()|) in Ω ∀  ∈ N, and lim  (, ) = .
→∞
and the initial assumptions, we deduce
So, without lost of generality, we can suppose that  (, ) ≤  + 1 for all  ∈ N. From this
⃒⃒ |ℎ() − ℎ()| ≤ | − |, ∀ , , ∈ Ω,
      </p>
      <p>}︃
⃒
⃒
1 &lt;  ≤ ℎ(·) ≤  in Ω.</p>
      <p>
        (
        <xref ref-type="bibr" rid="ref5">5</xref>
        )
(7)
(8)
where
∫︁
Utilizing the fact that () ≤  1 for almost all  ∈ Ω, we infer the following estimate
Then arguing as in Lemma 4.1 it can be shown that  ∈ 0,1(Ω) and
sup
∈N ∈Ω
      </p>
      <p>sup () ≤ 2.
‖‖1(Ω) ≤  1|Ω|,</p>
      <p>
        ∀  ∈ N.
 := 1 +  ≤ () ≤  := 2,
|()|  ≤
 1  ≤  1 |Ω|,
∀  ∈ N,
|∇()|()  ≤ 2
Ω () |∇()|()  &lt; 2( + 1),
∀  ∈ N,
(
        <xref ref-type="bibr" rid="ref6">6</xref>
        )
∫︁
Taking this fact into account, we deduce from (
        <xref ref-type="bibr" rid="ref6">6</xref>
        ), (7), and (??) that
‖‖ 1, (Ω) =
︂( ∫︁
uniformly with respect to  ∈ N. Therefore, there exists a subsequence of {}∈N, still denoted
by the same index, and a function  ∈  1, (Ω) such that
 →  strongly in (Ω) for all  ∈ [1,  * ),
 ⇀  weakly in  1, (Ω)
as  → ∞,
where, by Sobolev embedding theorem,  * = 22 = 21+2 &gt; 2.
      </p>
      <p>Moreover, passing to a subsequence if necessa r−y, we ha− ve (see Proposition A.3 and Lemma 4.1):
() → () a.e. in Ω.
 ⇀  weakly in (·) (Ω),</p>
      <p>weakly in (·) (Ω;
∇ ⇀ ∇</p>
      <p>R2),
(·) → (·) = 1 +  (|(∇ * ) (·)|)
uniformly in Ω as  → ∞,
where  ∈  1,(·) (Ω) with () = 1 +  (|(∇ * ) ()|) in Ω.</p>
      <p>
        Since  0 ≤ () ≤  1 a.a. in Ω for all  ∈ N, it follows from (9) that the limit function 
 is a feasible solution to minimization problem
is also subjected the same restriction. Thus, 
(
        <xref ref-type="bibr" rid="ref3">3</xref>
        ).
      </p>
      <p>Let us show that (, ) is a minimizer of this problem. With that in mind we note that
in view of the obvious inequality
|() − 0,()| ≤
2−1
(|()| + |0,()| )
and the fact that 0, ∈ 2(Ω ∖ ), we have: the sequence {() − 0,()}∈N is bounded in
 (Ω ∖ ) and converges weakly in  (Ω ∖ ) to  − 0,. Hence, by Proposition A.3 (see
(32)),  − 0, ∈ (·) (Ω ∖ ) and
lim inf
→∞
∫︁
Ω∖
∫︁</p>
      <p>Ω∖
|() − 0,()|  ≥</p>
      <p>
        () − 0,()| .
|
(10)
As for the rest terms in (
        <xref ref-type="bibr" rid="ref3">3</xref>
        ), in view of the strong convergence  →  in (Ω)
we have
with  &gt; 2,
(9)
≤
∫︁
Ω
      </p>
      <p>Ω
⃒

lim inf
→∞</p>
      <p>Ω∖ ⃒⃒ ∇ * ( − 0,)⃒⃒  =
lim inf
→∞
Ω∖ ⃒⃒ ∇ * ( − 0,)⃒⃒ ,
As a result, utilizing relations (10), (11), (12), and the lower semicontinuity property (32), we
 =</p>
      <p>inf
(, ) = lim  (, ) = lim inf (, ) ≥ (
, 
).</p>
      <p>
        ) is a minimizer to the problem (
        <xref ref-type="bibr" rid="ref3">3</xref>
        ), whereas its uniqueness remains as an
Hence,
ifnally obtain
      </p>
      <p>Thus, (,</p>
      <p>open question.
ℎ()| ≤ | − |, ∀ ,  ∈ Ω,
ℎ() ≤  := 2,</p>
    </sec>
    <sec id="sec-5">
      <title>5. On Relaxation of the Restoration Problem</title>
      <p>
        It is clear that because of the nonstandard energy functional and its non-convexity, constrained
minimization problem (
        <xref ref-type="bibr" rid="ref3">3</xref>
        ) is not trivial in its practical implementation. The main dificulty in its
study comes from the state constraints
1 ≤  0 ≤ () ≤  1 a.a. in Ω,
() = 1 +
 (|(∇ * ) ()|)
that we impose on the set of feasible solutions Ξ . This motivates us to pass to some relaxation.
In view of this, we propose the following iteration procedure which is based on the concept of
relaxation of extremal problems and their variational convergence [13, 14, 15, 16]. At the first
step we set up
0() =
︂{
1 +  (|(∇ * 0,) ()|) , if ∈Ω ∖ , }︂
1 +  (|(∇ * * ) ()|) , if ∈,
      </p>
      <p>∈ℬ0(·)
0 = Argmin (, 0(·)).
  = Argmin (, (·)).</p>
      <p>(13)
∈ℬ(·)
︁( ⃒ (︁</p>
      <p>⃒
︂{
Then, for each  ≥</p>
      <p>1, we set
() = 1 +  ⃒
∇ * −1 )︁
()⃒ ,
⃒
⃒ )︁
Here, ℬ(·) = {︀  ∈  1,(·) (Ω) : 1≤</p>
      <p>Before proceeding further, we set</p>
      <p>
        0 ≤ () ≤  1 a.a. in Ω }︀ .
where  &gt; 0 and  &gt; 0 are defined by (
        <xref ref-type="bibr" rid="ref5">5</xref>
        ) and (8), respectively.
      </p>
      <p>
        Arguing as in the proof of Theorem 1 and using the convexity arguments, it can be shown
that, for each (·)
Argmin∈ℬ(·)
∈ S, there exists a unique element 
0,(·)
∈ ℬ(·) such that 
0,(·)
(, (·)) . Moreover, it can be shown that, for given  = 1, . . . ,  ,  &gt;
compact with respect to the strong topology of (Ω).
 1&gt;0,  2 &gt; 0, * ∈  1, (), and ⃗0 ∈ 2(Ω ∖ , R ), the sequence {︀ 
∈  1,(·) (Ω) }︀
is compact with respect to the weak topology of  1, (Ω) , whereas the exponents {}∈N are
∈N
=
0,
We say that a pair (̂︀, ) is a weak solution to the original problem (
        <xref ref-type="bibr" rid="ref3">3</xref>
        ) if
      </p>
      <p>̂︀
∈ℬ̂︀(·)
̂︀ = Argmin (, ̂︀(·)), ̂︀ ∈ ℬ̂︀(·) ,
() = 1 +  (|(∇ * ̂︀) ()|) , ∀  ∈ Ω.</p>
      <p>̂︀
the asymptotic properties:
Our main result can be stated as follows:</p>
      <sec id="sec-5-1">
        <title>Theorem 5.2.</title>
        <p>
          Then, for each  ∈ {1, . . . ,  }, the sequence of approximated solutions {︀ (, ) ∈N
︀}
possesses
Let &gt;0,  1&gt;0,  2&gt;0, * ∈ (), and ⃗0∈2(Ω∖,
R ) be given data.
where (̃︀, ̃︀) is a weak solution to the original problem (
          <xref ref-type="bibr" rid="ref3">3</xref>
          ), that is,
        </p>
        <p>() → ̃︀() a.e. in Ω,
 ⇀ ̃︀ in  (Ω),</p>
        <p>and ∇ ⇀ ∇̃︀ in  (Ω; R2),
 → ̃︀ = F(()) strongly in (Ω) as  → ∞,</p>
        <p>̃︀
̃︀ ∈ ℬ̃︀(·) , ̃︀ = Argmin (, ̃︀(·)),
and, in addition, the following variational property holds true</p>
        <p>[︃
→∞
lim (, (·)) = lim
→∞ ∈ℬ(·)
inf
(, (·))
= inf</p>
        <p>Proof. Let’s assume the converse — namely, there is a function ∙ ∈ ℬ̃︀(·) such that
inf</p>
        <p>(, ̃︀(·)) &lt; (̃︀, ̃︀(·)).</p>
        <p>Using the procedure of the direct smoothing, we set
where  &gt; 0 is a small parameter,  is a positive compactly supported smooth function with
properties
 ∈ 0∞(R2),</p>
        <p>()  = 1, and () = (− ),
and ̃︁∙ is zero extension of ∙ outside of Ω.
by the classical properties of smoothing operators (see [17]). From this we deduce that
() → ∙ () a.e. in Ω.</p>
        <p>Moreover, taking into account the estimates
→∞
∫︁
∫︁
⃒
1
̃︀
1
∫︁
∫︁</p>
        <p>R2
∈ ()−1 (−Ω)
(16)
(17)
(18)
(19)
(21)
we see that each element  is subjected to the pointwise constraints
 0 ≤ () ≤  1 a.a. in Ω,
∀  &gt; 0.
⟨
inf∈ℬ(·)</p>
        <p>(, (·)) . Hence,
Since, for each  &gt; 0,  ∈  1,(·) (Ω)
for all  ∈</p>
        <p>N, it follows that  ∈
ℬ(·) , i.e.,
each element of the sequence {}&gt;0 is a feasible solution to all approximating problems
(, (·)) ≤ (, (·)),
∀  &gt; 0, ∀  = 0, 1, . . .</p>
        <p>Further we notice that
by Proposition A.3 and Fatou’s lemma, and
→∞
lim inf (, (·)) ≥ (̃︀, ̃︀(·))
→∞
lim (, (·)) = lim
Ω () |∇()|()  +</p>
        <p>Ω∖ ⃒⃒ ∇ * ( − 0,)⃒⃒  +  2
Ω∖
∫︁ ⃒ (︁
 ⃒
⃒  ⊥, ∇ ⃒⃒
() |∇()|()
→ () |∇()|̃︀()
it follows from the Lebesgue dominated convergence theorem and (20) that
→∞
lim (, (·)) = (, ̃︀(·)),
∀ &gt; 0.</p>
        <p>As a result, passing to the limit in (18) and utilizing properties (19)–(21), we obtain
(̃︀, ̃︀(·)) ≤ (, ̃︀(·)) =
∫︁</p>
        <p>1
Ω ̃︀() |∇()|̃︀
()  +

 ∫︁
Ω∖
|() − 0,()| 
Ω∖

⃒</p>
        <p>⃒
0,)⃒  +  2
⃒  ⊥, ∇ ⃒
,
for all  &gt; 0. Taking into account the pointwise convergence (see (17) and property (16))
0,(·) ()() 
as  → 0, and the fact that, for  small enough,
|∇()|̃︀
[︁
2 (1 + |∙ (·)|)</p>
        <p>+ 2 (1 + |0,(·)|)
2
 ‖1(Ω−Ω) ||
Ω 2 02 = const,
∈ 1(Ω)
a.e. in Ω</p>
        <p>∖ ,
we can pass to the limit in (22) as  → 0 by the Lebesgue dominated convergence theorem. This
(̃︀, ̃︀(·)) ≤
→0
lim (, ̃︀(·)) = (∙ , ̃︀(·)).</p>
        <p>
          Combining this inequality with (22) and (15), we finally get
that leads us into conflict with the initial assumption. Thus,
(̃︀, ̃︀(·)) =
inf
and, therefore, (, ) is a weak solution to the original problem (
          <xref ref-type="bibr" rid="ref3">3</xref>
          ). As for the variational
property (14), it is a direct consequence of (23) and (21).
        </p>
        <p>|∇()|̃︀</p>
      </sec>
    </sec>
    <sec id="sec-6">
      <title>6. Optimality Conditions</title>
      <p>To characterize the solution 0,(·)
⟨
lim
→0
⟩
+

∫︁
Ω∖
⃒
⃒⃒ 0,(·) () −
=
∫︁ (︁</p>
      <p>Ω
0,()⃒
⃒</p>
      <p>of the approximating optimization problem
inf∈ℬ(·)</p>
      <p>(, (·)) , we check that the functional (·) is Gâteaux diferentiable, that is,
(0,(·) + , (·)) −
(0,(·) , (·))
|∇0,(·) ()|()−2
︁)

for all 
∈
 1,(·) (Ω), where
∫︁
Ω
⃒
 ⊥, ∇0,(·) )︁ ⃒⃒ −1
︁(
 ⊥, ∇
︁)
,
Λ() =
(∇ ( −
), ∇ ( −
))
0,(·) ()
0,() 
︁)
Ω∖ ()  .</p>
      <p>To this end, we note that
|∇0,(·) () + ∇()|()
− |∇</p>
      <p>0,(·) ()|()
()
almost everywhere in Ω. Since, by convexity,
it follows that
⃒
⃒
⃒
⃒
⃒ |∇0,(·) () + ∇()|()
− |∇</p>
      <p>0,(·) ()|() ⃒⃒
()
→
|∇0,(·) ()|
()−2
∇0,(·) (), ∇()
as 
→</p>
      <p>0
︁)

| | − |


| ≤
2 (︀ | |
1
−
+ | |
−1 )︀
| −</p>
      <p>|,
︁(
︁(
≤
≤
≤
by the Lebesgue dominated convergence theorem.</p>
      <p>Taking into account that
‖0,(·) ()|
()−1</p>
      <p>‖′(·) (Ω)
∫︁
|∇0,(·) () + ∇()|
()−1
+ |∇0,(·) ()|</p>
      <p>()−1 )︁
≤
const
|∇0,(·) ()|
()−1
+ |∇()|
|∇()|.</p>
      <p>(25)
by (33) (︂ ∫︁
by (??) (︁
by (33)
Ω
‖0,(·) ()|</p>
      <p>()
‖0,(·)
2
|(·) (Ω)
+ 2
 + 1</p>
      <p>1
︁)  ′
,
Ω |
()|() 
by (??)
≤
‖</p>
      <p>2
‖(·) (Ω)
function. Therefore,
|∇0,(·) () + ∇()|()
− |∇
0,(·) ()|()</p>
      <p>()
→
∫︁
︁(
+ 1, we see that the right hand side of inequality (25) is
|∇0,(·) ()|
()−2
︁)
inf
∈ℬ(·)</p>
      <p>
        Utilizing the similar arguments to the rest terms in (
        <xref ref-type="bibr" rid="ref3">3</xref>
        ), we deduce that the representation
(24) for the Gâteaux diferential of (·, (·)) at the point 0,(·) ∈ ℬ(·) is valid.
      </p>
      <p>Thus, in order to derive some optimality conditions for the minimizing element 0,(·) ∈
ℬ(·) to the problem</p>
      <p>(, (·)) , we note that ℬ(·) is a nonempty convex subset of
 1,(·) (Ω) and the objective functional (·, (·)) :
ℬ(·) → R is strictly convex. Hence, the
well known classical result (see [18, Theorem 1.1.3]) and representation (24) lead us to the
following conclusion.</p>
      <p>Theorem 6.1. Let (·) ∈ S be an exponent given by the iterative rule (13). Then the unique
minimizer  ∈ ℬ(·) to the approximating problem inf∈ℬ(·)
(, (·)) is characterized by
∫︁ (︂ ⃒
Ω ⃒⃒ ∇()⃒⃒
⃒ ()−2
∇(), ∇() − ∇ ()  + 2 1
︂)
∫︁
Ω
Λ() (︁
() − ()
︁) 
+</p>
      <p>∫︁
+  2
Ω∖ ⃒</p>
    </sec>
    <sec id="sec-7">
      <title>7. Numerical Experiments</title>
      <p>In order to illustrate the proposed algorithm for the restoration of satellite multi-spectral images
we have provided some numerical experiments. As input data we have used a series of Sentinel-2
L2A images over the Dnipro Airport area, Ukraine (see Fig. 1, 2). This region represents a typical
agricultural area with medium sides fields of various shapes.
As a final result, we obtain in Fig. 3. Comparing the restored image and the contaminated
one we could see that the texture of original image is well preserved. However, overall colors
of different fields are shifted due to colorization part of algorithm. This problem has to be
addressed in the following research.</p>
    </sec>
    <sec id="sec-8">
      <title>8. Conclusion</title>
      <p>We propose a novel model for the restoration of satellite multi-spectral images. This model
is based on the solutions of special variational problems with nonstandard growth objective
functional. Because of the risk of information loss in optical images (see [19] for the details),
we do not impose any information about such images inside the damage region, but instead we
assume that the texture of these images can be predicted through a number of past cloud-free
images of the same region from the time series. So, the characteristic feature of variational
problems, which we formulate for each spectral channel separately, is the structure of their
objective functionals. On the one hand, we involve into consideration the energy functionals
with the nonstandard growth (), where the variable exponent () is unknown a priori and
it directly depends on the texture of an image that we are going to restore. On the other hand,
the texture of an image ⃗, we are going to restore, can have rather rich structure in the damage
region . In order to identify it, we push forward the following hypothesis: the geometry of
each spectral channels of a cloud corrupted image in the damage region is topologically close to
the geometry of the total spectral energy that can be predicted with some accuracy by a number
of past cloud-free images of the same region. As a result, we impose this requirement in each
objective functional in the form of a special fidelity term. In order to study the consistency of
the proposed collection of non-convex minimization problems, we develop a special technique
and supply this approach by the rigorous mathematical substantiation.</p>
    </sec>
    <sec id="sec-9">
      <title>Appendix A. On Orlicz Spaces</title>
      <p>Let (·) be a measurable exponent function on Ω such that 1 ≤  ≤ () ≤  &lt;
where  and  are given constants. Let ′(·) = (·)−1
be the corresponding conjugate exponent.
measurable functions  () on Ω such that ∫︀
Ω | ()|()  &lt; ∞. Then (·) (Ω)
is a reflexive
where  ′ and  ′ stand for the conjugates of constant exponents. Denote by (·) (Ω) the set of all
separable Banach space with respect to the Luxemburg norm (see [20] for the details)
1 ≤  − 1
≤ ′() ≤  − 1
‖ ‖(·) (Ω) = inf {︀  &gt; 0 :  ( −1  ) ≤ 1︀} ,
(26)

⏟
 ′⏞
∫︁</p>
      <p>Ω
∫︁
∫︁
Ω
Ω
∫︁
Ω
∫︁
‖ ‖(·) (Ω) − 1 ≤
| ()|()  ≤ ‖  ‖(·) (Ω)
+ 1,</p>
      <p>∀  ∈ (·) (Ω),
‖ ‖(·) (Ω) =</p>
      <p>| ()|() , if ‖ ‖(·) (Ω) = 1.
1 ∫︁


*
Ω
| ()|()  ≤
1 ∫︁


*
Ω</p>
      <p>| ()|() ,
∫︁ ⃒⃒  () ⃒⃒ ()
Ω ⃒⃒ 
* ⃒
⃒
 ≤</p>
      <p>*
1 ∫︁
Ω
1 ∫︁</p>
      <p>Ω
| ()|()  ≤ 1 ≤</p>
      <p>| ()|() .</p>
      <p>| ()|()  ≤ ‖ ‖(·) (Ω), if ‖ ‖(·) (Ω) &gt; 1,
| ()|()  ≤ ‖ ‖(·) (Ω), if ‖ ‖(·) (Ω) &lt; 1,

where  ( ) := ∫︀Ω | ()|() .</p>
      <p>It is well-known that (·) (Ω) is reflexive provided  &gt;
1, and its dual is ′(·) (Ω) , that is,
any continuous functional  =  ( ) on (·) (Ω)
has the form (see [21, Lemma 13.2])
 ( ) =
  ,</p>
      <p>with  ∈ ′(·) (Ω).</p>
      <p>if  * := ‖ ‖(·) (Ω) &gt; 0, then  ( −*1  ) = 1.</p>
      <p>As for the infimum in (26), we have the following result.</p>
      <p>Proposition A.1. The infimum in (26) is attained if  ( ) &gt; 0. Moreover</p>
      <p>Taking this result and condition 1 ≤  ≤ () ≤  into account, we see that
Hence, (see [20] for the details)
and, therefore,
‖ ‖(·) (Ω) ≤
‖ ‖(·) (Ω) ≤
The following estimates are well-known: if  ∈ (·) (Ω) then</p>
      <p>‖ ‖ (Ω) ≤ (1 + |Ω|) 1/ ‖ ‖(·) (Ω),
‖ ‖(·) (Ω) ≤ (1 + |Ω|) 1/ ′ ‖ ‖ (Ω),  ′ =
∀  ∈  (Ω).</p>
      <p>− 1
,
in this subsection we assume that</p>
      <p>Let {}∈N ⊂</p>
      <p>0, (Ω) , with some  ∈ (0, 1], be a given sequence of exponents. Hereinafter
1 ≤  ≤ () ≤  &lt;</p>
      <p>∞ a.e. in Ω for  = 1, 2, . . . , and (·) → (·) in (Ω) as  → ∞.
(·) (Ω). We say that the sequence {︀  ∈ (·) (Ω) }︀
We associate with this sequence the following collection {︀  ∈ (·) (Ω) }︀
tic feature of this set of functions is that each element  lives in the corresponding Orlicz space
∈N. The
characteris∈N is bounded if (see [22, Section 6.2])
(27)
(28)
(29)</p>
      <sec id="sec-9-1">
        <title>Definition A.2.</title>
        <p>A bounded sequence {︀  ∈ (·) (Ω) }︀
∈N is weakly convergent in the
{}∈N ⊂ 0, (Ω) in the uniform topology of (Ω), if
variable Orlicz space (·) (Ω) to a function  ∈ (·) (Ω), where  ∈ 0, (Ω) is the limit of
∫︁
lim</p>
        <p>For our further analysis, we need some auxiliary results (we refer to [21, Lemma 13.3] for
comparison). We begin with the lower semicontinuity property of the variable (·) -norm
with respect to the weak convergence in (·) (Ω).</p>
        <p>Proposition A.3. If a bounded sequence {︀  ∈ (·) (Ω) }︀
to  for some  &gt;
1, then  ∈ (·) (Ω),  ⇀  in variable (·) (Ω), and</p>
        <p>∈N converges weakly in  (Ω)
lim inf
→∞
∫︁
Ω
∫︁
Proof. In view of the fact that
⃒
⃒
⃒ ∫︁
⃒ Ω
|()|()  −
lim inf
→∞
∫︁
|()|()  = lim inf
→∞</p>
        <p>Ω () |()|() .</p>
        <p>∫︁
lim
Using the Young inequality  ≤ | |/ + ||′/′, we have
for ′() = ()/(() − 1) and any  ∈ 0∞(R2).</p>
        <p>Then passing to the limit in (30) as  → ∞ and utilizing property (27) and the fact that
()()  =
 ()()  for all  ∈  ′(Ω),
(31)
Since the last inequality is valid for all 
it follows that this relation holds true for 
∈ 0∞(R2) and the set 0∞(R2) is dense in ′(·) (Ω) ,
∈ ′(·) (Ω) . So, taking 
= | ()|()−2  (), we
arrive at the announced inequality (29). As an consequence of (29) and estimate (??), we get:</p>
        <p>To end of the proof, it remains to observe that relation (31) holds true for 
well. From this the weak convergence  ⇀  in the variable Orlicz space (·) (Ω)
∈ 0∞(R2) as
follows.</p>
        <p>Remark A.4. Arguing in a similar manner and using, instead of (30), the estimate
∫︁</p>
        <p>1
lim inf
→∞
Ω () |()|()  ≥
∫︁
Ω
() ()()  −
∫︁</p>
        <p>1
Ω ′() |( )|′() ,
it is easy to show that the lower semicontinuity property (29) can be generalized as follows
∫︁</p>
        <p>1
lim inf
→∞
Ω () |()|()  ≥
∫︁</p>
        <p>1
Ω () | ()|() .</p>
        <p>We need the following result that leads to the analog of the Hölder inequality in Lebesgue
spaces with variable exponents (for the details we refer to [20]).</p>
        <p>Proposition A.6. If  ∈ (·) (Ω)  and  ∈ ′(·) (Ω)  , then (, ) ∈ 1(Ω) and
∫︁
Ω</p>
        <p>(, )  ≤ 2‖ ‖(·) (Ω) ‖‖′(·) (Ω) .
|()|()  ≥
() ()()  −</p>
        <p>Appendix B. Sobolev Spaces with Variable Exponent
We recall here the well-known facts concerning the Sobolev spaces with variable exponent.
Let (·) be a measurable exponent function on Ω such that 1 &lt;  ≤ () ≤  &lt;
where  and  are given constants. We associate with it the so-called Sobolev-Orlicz space
 ∈  1,1(Ω) :
︂}
∫︁ [︁|()|() + |∇()|()]︁  &lt; +∞
Ω
(32)
(33)
and equip it with the norm ‖‖01,(·) (Ω) = ‖‖(·) (Ω) + ‖∇‖(·) (Ω;R2).</p>
        <p>It is well-known that, in general, unlike classical Sobolev spaces, smooth functions are not
necessarily dense in  = 01,(·) (Ω) . Hence, with the given variable exponent  = ()
(1 &lt;  ≤  ≤  ) it can be associated another Sobolev space,</p>
        <p>= 1,(·) (Ω) as the closure of the set ∞(Ω) in  1,(·) (Ω)-norm.</p>
        <p>Since the identity  =  is not always valid, it makes sense to say that an exponent () is
regular if ∞(Ω) is dense in  1,(·) (Ω).</p>
        <p>The following result reveals an important property ensuring the regularity of exponent ().</p>
        <p>Proposition B.1. Assume that there exists  ∈ (0, 1] such that  ∈ 0, (Ω). Then the set
∞(Ω) is dense in  1,(·) (Ω), and, therefore,  = .</p>
        <p>Proof. Let  ∈ 0, (Ω) be a given exponent. Since
lim || log(||) = 0
→0
with an arbitrary  ∈ (0, 1],
(34)
it follows from the Hölder continuity of (·) that
|() − ()| ≤ | − | ≤
[︃</p>
        <p>| − |
sup
,∈Ω log(| − |−1 )
]︃
(| − |),
∀ ,  ∈ Ω,
where () = / log(||−1 ), and  &gt; 0 is some positive constant.</p>
        <p>Then property (34) implies that (·) is a log-Hölder continuous function. So, to deduce the
density of ∞(Ω) in  1,(·) (Ω) it is enough to refer to Theorem 13.10 in [21].
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