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<article xmlns:xlink="http://www.w3.org/1999/xlink">
  <front>
    <journal-meta />
    <article-meta>
      <title-group>
        <article-title>Sentinel-2 and MODIS Data Fusion for Generation Cloud-Free Images at the Sentinel Resolution Level of Daily</article-title>
      </title-group>
      <contrib-group>
        <contrib contrib-type="author">
          <string-name>Natalya Ivanchuk</string-name>
          <email>natalya.ivanchuk@eosda.com</email>
          <xref ref-type="aff" rid="aff0">0</xref>
          <xref ref-type="aff" rid="aff2">2</xref>
        </contrib>
        <contrib contrib-type="author">
          <string-name>Peter Kogut</string-name>
          <email>peter.kogut@eosda.com</email>
          <xref ref-type="aff" rid="aff1">1</xref>
          <xref ref-type="aff" rid="aff3">3</xref>
        </contrib>
        <contrib contrib-type="author">
          <string-name>Petro Martyniuk</string-name>
          <email>petro.martyniyk@eosda.com</email>
          <xref ref-type="aff" rid="aff2">2</xref>
          <xref ref-type="aff" rid="aff4">4</xref>
        </contrib>
        <aff id="aff0">
          <label>0</label>
          <institution>Department of Computer Sciences and Applied Mathematics, National University of Water and Environmental Engineering</institution>
          ,
          <addr-line>Soborna str., 11, Rivne, 33028</addr-line>
          ,
          <country country="UA">Ukraine</country>
        </aff>
        <aff id="aff1">
          <label>1</label>
          <institution>Department of Mathematical Analysis and Optimization, Oles Honchar Dnipro National University</institution>
          ,
          <addr-line>Gagarin av., 72, Dnipro, 49010</addr-line>
          ,
          <country country="UA">Ukraine</country>
        </aff>
        <aff id="aff2">
          <label>2</label>
          <institution>EOS Data Analytics Ukraine</institution>
          ,
          <addr-line>Desyatynny lane, 5, Kyiv, 01001</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, 49010</addr-line>
          ,
          <country country="UA">Ukraine</country>
        </aff>
        <aff id="aff4">
          <label>4</label>
          <institution>Institute of Automation, Cybernetics and Computer Engineering, National University of Water and Environmental Engineering</institution>
          ,
          <addr-line>Soborna str., 11, Rivne, 33028</addr-line>
          ,
          <country country="UA">Ukraine</country>
        </aff>
      </contrib-group>
      <abstract>
        <p>In this paperwe discuss a newvariational approach to the Date Fusion problem of multi-spectral satellite images from Sentinel-2 and MODIS that have been captureed at different resolution level and, arguably, on different days. The crucial assumption to our approach is that the MODIS image has to be cloud-free whereas the images from Sentinel-2 can be corrupted by clouds or noise. We formulate the data fusion problem as the two-level optimization problem. We discuss the well thoroughness and consistency of the proposed variational models. We also derive some optimality conditions and supply our approach by results of numerical simulations with the real satellite images.</p>
      </abstract>
      <kwd-group>
        <kwd>eol&gt;Data Fusion</kwd>
        <kwd>Variational Approach</kwd>
        <kwd>Image Reconstruction</kwd>
        <kwd>Optimization Problems</kwd>
        <kwd>Image restoration</kwd>
      </kwd-group>
    </article-meta>
  </front>
  <body>
    <sec id="sec-1">
      <title>Introduction</title>
      <p>It is well-known that the data fusion problem is often exacerbated by cloud contamination. In some
cloudy areas, researchers are fortunate to get 2–3 cloud-free satellite scenes per year, what is insufficient for
many applications that require dense temporal information, such as crop condition monitoring and
phenology studies. In view of this, we can indicate the following general requirements for the satellite
image fusion process: (i) The fused image should preserve all relevant information from the input images;
(ii) The image fusion should not introduce artifacts which can lead to wrong inferences.</p>
      <p>In spite of the fact that the first requirement (item (i)) sounds rather vague, we give a precise treatment
for it in Section 5, making use of a collection of special constrained minimization problems (see (22)). As
for the second item, it is important to emphasize that we are mainly interesting by satellite images that can
be useful from agricultural point of view (land cover change mapping, crop condition monitoring, yield
estimation, and many others).
Because of this an important option in the image data fusion is to preserve the precise geo-location of the
existing crop fields and avoid an appearance of the so-called false contours and pseudo-boundaries on a
given territory.</p>
      <p>In this paper we mainly focus on the image fusion problem coming from two satellites — Setnitel-2 and
Moderate Resolution Imaging Spectroradiometer (MODIS) [1]. Since each band (spectral channel) in
Sentinel images has 10, 20, or 60 meters in pixel size, it gives an ideal spatial resolution for vegetation
mapping at the field scale. Moreover, taking into account that Sentinel-2 has 3–5 revisit cycle over the
same territory, it makes its usage for studying global biophysical processes, which allows to evolve rapidly
during the growing season, essentially important. The unique problem that drastically restricts its practical
implementation, is the fact that the images from Sentinel-2, as a rule, are often contaminated by clouds,
shadows, dust, and other atmospheric artifacts.</p>
      <p>One of possible solutions for practical applications is to make use of frequent coarse-resolution data of
the MODIS. Taking into account that the MODIS data can be delivered with the daily repeat cycle and
500-m surface reflectance, the core idea is to use the Sentinel and MODIS data to generate synthetic ’daily’
surface reflectance products at Sentinel spatial resolution [2].</p>
      <p>The problem we consider in this paper can be briefly described as follows. We have a collection of
multi-band images { , ,… , : → ℝ } from Sentinel-2 that were captured at some time instances
{ , ,… , }, respectively, and we have a MODIS image : → ℝ from some day . It is assumed
that all of these images are well co-registered with respect to the unique geographic location. We also
suppose that the MODIS image is cloud-free and the day may does not coincide with any of time
instances { , ,… , }. Meanwhile, the Sentinel images { , ,… , : → ℝ } can be corrupted by
clouds. The main question is how to generate a new synthetic ’daily’ multi-band image of the same territory
from the day at the Sentinel-2 spatial resolution , utilizing for that the above mentioned data.</p>
      <p>In principle, this problem is not new in the literature [3, 4, 5]. For nowadays the spatial and temporal
adaptive reflectance fusion model (STARFM) is one of the most popular model where the idea to generate
a new synthetic ’daily’ satellite images at high resolution level has been realized [6, 7]. However, its
performance essentially depends on the characteristic patch size of the landscape and degrades somewhat
when used on extremely heterogeneous fine-grained landscapes [3].</p>
      <p>Instead of this, we mainly focus on the variational approach to the satellite image data fusion (see [8, 9,
10]). We formulate the data fusion problem as the two-level optimization problem. At the first level,
following a simple iterative procedure, we generate the so-called structural prototype for a synthetic
Sentinel image from the given day . The main characteristic feature of this prototype is the fact that, it
must have a similar geometrical structure (namely, precise location of contours and field boundaries) to the
nearest in time ’visible’ Sentinel images, albeit they may have rather different intensities in all bands. Since
the revisit cycle of Sentinel-2 is 2–3 days, such prototype can be easily generated. We consider the above
mentioned structural prototype as a reasonable input data for ’daily’ prediction problem that we formulate a
special constrained minimization problem, where the cost functional has a nonstandard growth and the edge
information for restoration of MODIS cloud-free images at the Sentinel resolution is accumulated both in
the variable exponent of nonlinearity and in the directional image gradients which we derive from the
predicted structural prototype. It is worth to emphasize that our model is considerably different from the
variational model for P+XS image fusion that was proposed in [11].</p>
    </sec>
    <sec id="sec-2">
      <title>Non-Formal Statement of the Problem</title>
      <p>Let Ω ⊂ ℝ be a bounded connected open set with a sufficiently smooth boundary Ω and nonzero
Lebesgue measure. In majority cases Ω can be interpreted as a rectangle domain. Let and be two
sample grids on Ω .</p>
      <p>Let [0, ] be a given time interval. Normally, by we mean a number of days. Let and { } be
moments in time (particular days) such that 0 ≤ &lt; &lt; ⋯ &lt; ≤ and &lt; &lt; . Let
{ , ,… , : → ℝ } be a collection of multispectral images of some territory, delivered from
Sentinel-2, that were taken at time instances , ,… , , respectively. Let : → ℝ be a MODIS
image of the same territory and this image has been captured at time = . It is assumed that:
1. The Sentinel-2 images { } can be corrupted by some noise, clouds and blur, whereas is
a cloud-free image;</p>
      <p>2. We divide the set of all bands for Sentinel images onto two parts and such that each
spectral channel of the MODIS image has the similar spectral characteristics to some channel of
-group;</p>
      <p>3. The MODIS image : → ℝ is not corrupted by clouds or its damage zone can be
neglected;</p>
      <p>4. The MODIS image and the images { , ,… , } from Sentinel-2 are rigidly co-registered
[12, 13]. This means that the MODIS image after arguably some affine transformation and each Sentinel
images after the resampling to the grid with low resolution , could be successfully matched according to
the unique geographic location [14, 15].
2.1.</p>
    </sec>
    <sec id="sec-3">
      <title>Functional Spaces</title>
      <sec id="sec-3-1">
        <title>Let us recall some useful notations. For given 1 ≤</title>
        <p>where ∥ ∥ ( ;ℝ )= ∫ | ( )| for 1 ≤</p>
        <p>Given a real Banach space , we will denote by
[0, ] into . We recall that, for 1 ≤ &lt; ∞ ,
:[0, ]→ such that [16, 17]
(Ω ;ℝ ) =</p>
        <p>:Ω → ℝ
/
≤ + ∞ , the space
∶ ∥
∥ ( ;ℝ )&lt; + ∞ ,</p>
        <p>(Ω ;ℝ ) is defined by
&lt; + ∞ .
([0, ]; ) the space of all continuous functions from
(0, ; ) is the space of all measurable functions
∥ ∥ ( , ; )= ∫ ∥ ( ) ∥ &lt; ∞ ,
while (0, ; ) is the space of measurable functions such that ∥ ∥ ( , ; )= sup ∈[ , ] ∥
( ) ∥ &lt; ∞ .For more detailed presentation of the theory of these spaces and the Sobolev spaces with
variable exponents, we refer to [18, 19, 20, 21, 22, 23].
2.2.</p>
      </sec>
    </sec>
    <sec id="sec-4">
      <title>Topographic Maps and Geometry of Satillite Multispectral Images</title>
      <p>Following the main principle of the Mathematical Morphology, a scalar image :Ω → ℝ is a
representative of an equivalence class of images obtained from via a contrast change, i.e., = ( ),
where is a continuous strictly increasing function. Under this assumption, a scalar image can be
characterized by its upper level sets ( ) = { ∈ Ω ∶ ( ) ≥ }. Moreover, each image can be
recovered from its level sets by the reconstruction formula ( ) = sup{ ∶ ∈ ( )}. Thus, according
to the Mathematical Morphology Doctrine, we can suppose that the reliable geometric information about a
scalar image is contained in those level sets.</p>
      <p>In order to describe the level sets by their boundaries, ( ), we assume that ∈ , (Ω ), where
, (Ω ) stands for the standard Sobolev space of all functions ∈ (Ω ) with respect to the norm
∥ ∥ , ( )= ∥ ∥ ( ) + ∥ ∇ ∥ ( ) . Then at almost all points of almost all level sets of ∈ , (Ω )
we may define a unit normal vector ( ) [24]. This vector field formally satisfies the following relations
( ,∇ ) = |∇ | and | |≤ 1 a.e.in. In the sequel, we will refer to the vector field as the vector field
of unit normals to the topographic map of a function . So, we can associate with the geometry of the
scalar image [25, 26].</p>
      <p>Remark 2.1 In practice, a better choice for
some small value of
&gt; 0, where
( , , ) is a solution (for small value of
( , ) would be to compute it as the ration ∇ ( ,⋅) for</p>
      <p>|∇ ( ,⋅)|
&gt; 0) of the following
initial-boundary value problem with 1 -Laplace operator in the principle part</p>
      <p>∇
= div |∇ | , ∈ (0,+ ∞ ), ( , ) ∈ Ω ,
(0, , ) =
( , , )</p>
      <p>( , ), ( , ) ∈ Ω ,</p>
      <sec id="sec-4-1">
        <title>Let ∈ ([0, ]; (Ω )) be a given function. For each ∈ [0, ], we associate the real-valued ( ,⋅):Ω ↦ ℝ with a gray-scale image, and the mapping :(0, )× Ω → ℝ with an optical</title>
        <p>Definition 2.1 We say that a function
:(0, )× → ℝ if it is defined by the rule
:(0, )×</p>
        <p>→ ℝ is the texture index of a given optical
( , ):= 1 + ∫ |(∇ ∗ ( ,⋅))( )| ,
for all ( , ) ∈ , where denotes zero extension of from = (0, )× Ω to ℝ , stands for
the two-dimentional Gaussian of width (standard deviation) &gt; 0 :[0,∞ ) → (0,∞ ) is the
edge-stopping function which we take in the form of the Cauchy law ( ) = with &gt; 0 small
enough, and ℎ &gt; 0 is a small positive value.
∥
∥ ([ , ]; ( )) such that</p>
        <p>
          Since ∈ (ℝ ) , it follows from (
          <xref ref-type="bibr" rid="ref4">4</xref>
          ) that 1 &lt; ( , ) ≤ 2 in and
∈ ([0, ]; (ℝ )) even if is just an absolutely integrable function in . Moreover, for each
∈ [0, ], ( , ) ≈ 1 in those places of Ω where some edges or discontinuities are present in the image
( ,⋅), and ( , ) ≈ 2 in places where ( , ) is smooth or contains homogeneous features. In view of
this, ( , ) can be interpreted as a characteristic of the sparse texture of the function that can change
with time.
        </p>
        <p>Lemma 2.1 Let ∈ ([0, ]; ( )) be a measurable function extended by zero outside of .
Let be the corresponding texture index. Then there exists a constant &gt; 0 depending on , , and
:= 1 +
≤
( , ) ≤
∈
, (
:= 2, ∀ ( , ) ∈
),
,
where
= ℎ
ℎ+ ∥
∥ (
) |Ω |∥
∥ ( , ; ( ))
.</p>
      </sec>
    </sec>
    <sec id="sec-5">
      <title>Data Fusion Problem. Main Requirements to the Formal Statement</title>
      <p>Let { , ,… , : → ℝ } be a collection of multispectral images of some territory from Sentinel-2
that were taken at time instances { , ,… , }⊂ [0, ], respectively. Let { , ,… , }⊂ 2 be a
collection of damage regions for the corresponding Sentinel-images. So, in fact, we deal with the set of
images { : \ → ℝ }, = 1,..., . Let : → ℝ be a MODIS image of the same territory and
this image has been captured at time = ∈ ( , ).</p>
      <p>We begin with the following assumption: = ∅ and the damage zones for the rest images from
Sentinel-2 are such that each , = 2,… , , is a measurable closed subset of Ω with property ℒ ( ) ≤
0.6 ℒ (Ω ), where ℒ ( ) stands for the 2-D Lebesgue measure of .</p>
      <p>
        We say that multi-band images
cloud-corrupted ones { :
\
→ ℝ
if they are defined as follows:
are structural prototypes of the corresponding
(
        <xref ref-type="bibr" rid="ref1">1</xref>
        )
(
        <xref ref-type="bibr" rid="ref2">2</xref>
        )
(
        <xref ref-type="bibr" rid="ref3">3</xref>
        )
(
        <xref ref-type="bibr" rid="ref4">4</xref>
        )
(
        <xref ref-type="bibr" rid="ref5">5</xref>
        )
(
        <xref ref-type="bibr" rid="ref6">6</xref>
        )
=
, ( ),
, ( ),
      </p>
      <p>, = [
[ , ] \ := ℒ ( \ )∑ ∈ \ , ( ).</p>
      <sec id="sec-5-1">
        <title>Moreover, each structural prototype : → ℝ is rigidly related to the corresponding day the image : \ → ℝ had been taken.</title>
        <p>
          Remark 3.1 As follows from the rule (
          <xref ref-type="bibr" rid="ref7">7</xref>
          ), this iterative procedure should be applied to each spectral
channel of all multi-band images from Sentinel-2. Since the revisit time for Sentinel-2 is 3 − 5 days and
the collection of images { } is rigidly co-registered, it follows from (
          <xref ref-type="bibr" rid="ref7">7</xref>
          ) that the structural prototypes
are also well co-registered and they have the similar topographic maps with respect to their precise
space location, albeit some false contours can appear along the boundaries of the damage zones . In
fact, in order to avoid the appearance of the false contours, the weight coefficients , have been
introduced.
        </p>
        <p>
          Since the MODIS image has been taken at a time instance
cases:
∈ ( , ), we can have three possible
(А1) there exists an index ∗ ∈ {1,..., } such that = ∗;
(А2) there exists an index ∗ ∈ {1,..., − 1} such that ∗ &lt;
(А3) &lt; &lt; .
&lt;
∗ ;
In view of this, we will distinguish three different statements of the data fusion problem:
(Restoration Problem) The problem (A1) consists in restoration of the damaged multi-band optical
image ∗: \ ∗ → ℝ using result of its fusion with the cloud-free MODIS image : → ℝ of the
same territory. It means that, we have to create a new image ∗ : → ℝ , which would be well defined
on the entire grid , such that
∗ ( ) =
∗( ), ∀
= ( , ) ∈
\ ∗,
(
          <xref ref-type="bibr" rid="ref8">8</xref>
          )
∑ ∈ ∩ ∗ ( ∗ , ( )− ( )) = i∈nℐf∑ ∈ ∩ ∗ (( ∗ )( )− ( )) ,∀ ∈ , (
          <xref ref-type="bibr" rid="ref9">9</xref>
          )
∗, ( ) = ∗, ( ), ∀ ∈ , ∀ ∈ . (
          <xref ref-type="bibr" rid="ref10">10</xref>
          )
        </p>
        <p>The precise description of the class of admissible (or feasible) images ℐ will be given in the next
section.</p>
        <p>(Interpolation Problem) The problem (A2) consists in generation of a new multi-band optical image
: → ℝ at the Sentinel-level of resolution using result of the fusion of cloud-free MODIS image
: → ℝ with the predicted structural prototype : → ℝ from the given day . In fact, in this
case we deal with the two-level problem. At the first level, having the collection of structural prototypes
: → ℝ which is associated with the time instances { , ,… , }⊂ [0, ], we create a new
’intermediate’ image : → ℝ that can be considered as daily prediction of the topographical map of
a given territory from the day . Then, at the second level, we realize the fusion procedure of this
predicted image with the cloud-free MODIS image : → ℝ of the same territory.</p>
        <p>(Extrapolation Problem) The problem (A3) consists in generation of a new multi-band optical image
: → ℝ using result of the data assimilation from the cloud-free MODIS image : → ℝ into
the structural prototype : → ℝ of the Sentinel-image : \ → ℝ .</p>
      </sec>
    </sec>
    <sec id="sec-6">
      <title>The Model for Prediction of Structural Prototypes</title>
      <p>Let ∗, and ∗ , be structural prototypes of the corresponding images from given days ∗ and
∗ . Since ∗, and ∗ , are well co-registered images, it is reasonable to assume that they have the
similar geometric structure albeit they may have very different intensities.</p>
      <p>The main question we are going to discuss in this section is: how to correctly define the ’intermediate’
image : → ℝ that can be considered as daily prediction of the topographical map of a given
territory from the day . With that in mind, for each spectral channel ∈ {1,2,… , }, we make use of the
following model
− div|∇ | ( , ) ∇
=</p>
      <p>in ( ∗, ∗ )× Ω ,
= 0 on ( ∗, ∗ )× Ω ,
( ∗,⋅)= ∗, (⋅) in Ω ,
where ( , ) stands for the texture index of the scalar image (see Definition 2.1), and ∈
( ∗, ∗ ; (Ω )) is an unknown source term that should be defined in the way to guarantee the
fulfillment (with some accuracy) of the relation</p>
      <p>( ∗ ,⋅)≈ ∗ , (⋅) in Ω .</p>
      <p>
        Here, in (
        <xref ref-type="bibr" rid="ref13">13</xref>
        ) and (
        <xref ref-type="bibr" rid="ref14">14</xref>
        ), by default, we assume that the images
the entire domain Ω .
∗, and
∗ , are well defined onto
∈
and the integral identity
      </p>
      <p>∗
∫ ∗ ∫</p>
      <p>−
holds true for any function
+ (|∇ | ∇ ,∇ )</p>
      <p>∗
= ∫ ∗</p>
      <p>∫
∈ Φ, where Φ =
+ ∫
∈
∗, |</p>
      <p>∗
([ ∗, ∗ ]× Ω ) ∶ |
∗
= 0 .</p>
      <p>
        (
        <xref ref-type="bibr" rid="ref11">11</xref>
        )
(
        <xref ref-type="bibr" rid="ref14">14</xref>
        )
(
        <xref ref-type="bibr" rid="ref15">15</xref>
        )
(
        <xref ref-type="bibr" rid="ref16">16</xref>
        )
      </p>
      <p>Utilizing the perturbation technique and the classical fixed point theorem of Schauder, it has been
recently proven the following existence result.</p>
      <p>
        Remark 4.1 The main characteristic feature of the proposed initial-boundary value problem (IBVP) is
the fact that the exponent depend not only on ( , ) but also on ( , ). It is well-known that the
variable character of exponent causes a gap between the monotonicity and coercivity conditions.
Because of this gap, equations of the type (
        <xref ref-type="bibr" rid="ref11">11</xref>
        ) can be termed equations with nonstandard growth
conditions. So, in fact, we deal with the Cauchy-Neumann IBVP for parabolic equation of =
( , , )-Laplacian type with variable exponent of nonlinearity. It was recently shown that the model (
        <xref ref-type="bibr" rid="ref11">11</xref>
        )–
(
        <xref ref-type="bibr" rid="ref13">13</xref>
        ) naturally appears as the Euler-Lagrange equation in the problem of restoration of cloud contaminated
satellite optical images [27]. In particular, this model has been proposed in [2] in order to avoid the
blurring of edges and other localization problems presented by linear diffusion models in images
processing.
      </p>
      <p>∗, (⋅) and</p>
      <p>∗ , (⋅).</p>
      <p>
        We note that the distributed control in the right hand side of (
        <xref ref-type="bibr" rid="ref11">11</xref>
        ) describes the fictitious sources or
sinks of the intensity that may have a tendency to change at most pixels even for co-registered structural
prototypes
      </p>
      <p>
        Definition 4.1 We say that, for given
to the problem (
        <xref ref-type="bibr" rid="ref11">11</xref>
        )–(
        <xref ref-type="bibr" rid="ref13">13</xref>
        ) if, for a.a.
      </p>
      <p>∈ ( ) and
∈ [ ∗, ∗ ],
∗, ∈
( ), a function
is a weak solution
( ∗, ∗ ; (Ω )), ( ,⋅)∈</p>
      <p>∗
, (Ω ) , ∫ ∗
∫ |∇ | ( , )
&lt; + ∞ ,</p>
      <p>
        Theorem 4.1 [28] Let ∈ ( ) and ∗, ∈ ( ) be given distributions. Then initial-boundary
value problem (
        <xref ref-type="bibr" rid="ref11">11</xref>
        )–(
        <xref ref-type="bibr" rid="ref13">13</xref>
        ) admits at least one weak solution = ( , ) with the following higher
inegrability properties
      </p>
      <p>
        ∈ ( ∗, ∗ ; (Ω )), ∈ , (( ∗, ∗ )× Ω ), ∈ ( ∗, ∗ ; (Ω )),
where the exponent is given by the rule
(
        <xref ref-type="bibr" rid="ref17">17</xref>
        )
=
∥ ∥ (
)| | ∥ ∥ ( ) ∥ ∗,∥ ( )
.
      </p>
      <p>
        In order to satisfy the condition (
        <xref ref-type="bibr" rid="ref14">14</xref>
        ) and define an appropriate source term = ( , ), we utilize some
issues coming from the well-known method of Horn and Schunck that has been developed in order to
compute optical flow velocity from spatiotemporal derivatives of image intensity. Following this approach,
we define the function ∗ as a solution of the problem
∫ − div(|∇ | ∇ )| − + ∫ |∇ | → inf ,
∈ ( )
where ̂ = ( ∗ + ∗ )/2, &gt; 0 is tuning parameter (for numerical simulations we take
and the spatiotemporal derivatives are computed by the rules
(
        <xref ref-type="bibr" rid="ref18">18</xref>
        )
= 0.5),
=
∗
∗
∗ , −
      </p>
      <p>∗, ,
div(|∇ | ∇ )| =
[div |∇ ∗, |
∗, ∇ ∗, + div |∇ ∗ , |
∗ , ∇ ∗ , ].</p>
      <p>
        It is clear that a minimum point ∗ ∈ (Ω ) to unconstrained minimization problem (
        <xref ref-type="bibr" rid="ref18">18</xref>
        ) is unique and
satisfies necessarily the Euler-Lagrange equation
Δ ∗ +
− div(|∇ | ∇ )| −
∗ = 0
with the Nuemann boundary condition ∗ = 0 on Ω .
      </p>
      <p>
        Setting = ∗ in (
        <xref ref-type="bibr" rid="ref11">11</xref>
        ), we can define a function ∗ = ∗( , ) as the weak solution of the IBVP (
        <xref ref-type="bibr" rid="ref11">11</xref>
        )–
(
        <xref ref-type="bibr" rid="ref13">13</xref>
        ). Numerical experiments show that, following this way, we obtain a function ∗ with properties (
        <xref ref-type="bibr" rid="ref15">15</xref>
        )
and (
        <xref ref-type="bibr" rid="ref17">17</xref>
        ) such that ∗( ∗, ) = ∗, ( ) and ∗( ∗ , ) ≈ ∗ , ( ) in Ω , where the peak
signal-to-noise ratio (PSNR) between images ∗( ∗ , ) and ∗ , ( ) is sufficiently large, &gt;
46.
      </p>
      <p>This observation leads us to the following conclusion: the ’intermediate’ image
defined as follow:
:
→ ℝ
can be
( ) =
∗( , ), ∀
∈
.</p>
    </sec>
    <sec id="sec-7">
      <title>Variational Statements of the Data Fusion Problems (A1)–(A3)</title>
      <p>
        Coming back to the principle cases (A1)–(A3), that have been described in Section 3, we can suppose
that a structural prototype from the given day is well defined. As it was pointed out in Section 3,
this prototype coincides either with one of the images in cases (A1) and (A3), or it should be defined
using the solutions of the problem (
        <xref ref-type="bibr" rid="ref11">11</xref>
        )–(
        <xref ref-type="bibr" rid="ref13">13</xref>
        ), (19) for each = 1,..., in the case (A2)-problem (see the
rule (20)).
      </p>
      <p>
        Let ∈ {1,..., } be a fixed index value (the number of spectral channel). Let :Ω → ℝ be the
texture index of the -th band for the structural prototype : → ℝ . Let ∈ (
        <xref ref-type="bibr" rid="ref1">0,1</xref>
        ) be a given
threshold. Let = [ , be a vector field such that | ( )|ℝ ≤ 1 and
      </p>
      <p>We define the linear operator
( ),∇</p>
      <p>, ( ) ℝ
, :ℝ → ℝ
, ∇ := ∇ −</p>
      <p>= |∇
as follows
,∇</p>
      <p>,
= ∫ \ ∗ | ∗, ( )| − ∫ \ ∗ | , ( )|
is a solutions of the following constrained minimization problem
ℱ ( ) = ∫
( )
| , ∇ ( )| ( )
+ ∫
∇ ( )− ∇
, ( )
(22)
(23)
+ ∫ Π ( ∗ − , ) → i∈nf,
Ξ = ∈ , (⋅)(Ω ) ∶ 0 ≤ ( ) ≤ a.e.in Ω stands for the set of feasible solutions, and
, (⋅)(Ω ) denotes the Sobolev space with variable exponent. As for the constants , their choice
depends on the format of signed integer numbers in which the corresponding intensities , ( ) are
represented. In particular, it can be = 2 − 1, = 2 − 1, and so on.</p>
      <sec id="sec-7-1">
        <title>2. A multi-band image</title>
        <p>Problem, if it is given by the rule
:
→ ℝ , with
∗ &lt;
&lt;
∗ , is a solution of the Interpolation
,
∀
∈
= ∫ | , ( )| − ∫ | , ( )|
is a solutions of the constrained minimization problem (22).</p>
      </sec>
      <sec id="sec-7-2">
        <title>Here,</title>
        <p>and
where
and</p>
      </sec>
      <sec id="sec-7-3">
        <title>3. A multi-band image</title>
        <p>Problem, if it is given by the rule
:
→ ℝ , with
&lt;
&lt;</p>
        <p>, is a solution of the Extrapolation</p>
        <p>, ( ) , ∀ ∈ ,
is a solutions of the constrained minimization problem (22), and
∀
∈
, ∀ ∈
,</p>
        <p>Let us briefly discuss the relevance of the proposed minimization problem. The first term in (22) can be
considered as the regularization in the Sobolev-Orlicz space , (⋅)(Ω ) [29]. As for the second term in
(22), it reflects the fact that the topographic map of the retrieved image should be as close as possible to the
topographic map of predicted structural prototype : → ℝ . We interpret this closedness in its
simplified form, namely, in the sense of -norm of the difference of the corresponding gradients [6, 30,
31]. The last term in (22) represents an -distortion between a -th spectral channel in the MODIS image
and the corresponding channel of the retrieved image which is resampled to the grid of low resolution</p>
        <p>Existence Result and Optimality Conditions for Constrained Minimization
Problem ( )</p>
      </sec>
      <sec id="sec-7-4">
        <title>Following in many aspects the recent studies [28], we give the following existence result.</title>
        <p>Theorem 6.1 Let :
Sentinel-2. Then for any given
a unique solution ∈ .</p>
        <p>
          → ℝ
∈ ,
be a given structural prototype for unknown image from
&gt; 0, &gt; 0, and ∈ (
          <xref ref-type="bibr" rid="ref1">0,1</xref>
          ), the minimization problem (22) admits
In order to derive some optimality conditions to the problem (22) and characterize its solution
∈ , (⋅)(Ω ), we note that the cost functional ℱ :Ξ → ℝ is Gâteaux differentiable. Since Ξ is a
nonempty convex subset of , (⋅)(Ω )∩ (Ω ) and the objective functional ℱ :Ξ → ℝ is strictly
convex, the well known classical approach leads us to the following conclusion.
        </p>
        <p>Theorem 6.2 Let : → ℝ be a given structural prototype for unknown image from
Sentinel-2. Let : → ℝ be a given MODIS image. Let stands for the texture index of the -th band
for the predicted structural prototype . Then the unique minimizer ∈ to the minimization
problem ℱ ( ) is characterized by the following variational inequality
∈
∫ | , ∇</p>
        <p>( )| ( )
+
∫ Π
+ ∫
∗ ∗</p>
        <p>, ∇
∇</p>
        <p>( ), , ∇ ( )− , ∇
( )− ∇ , ( ),∇ ( )
∗ − , ≥ 0, ∀
( )
∈ Ξ .</p>
        <p>Remark 6.1 In practical implementation, it is reasonable to define an optimal solution ∈ using a
’gradient descent’ strategy. Indeed, following the standard procedure and starting from the initial image
, , we can pass to the following initial value problem for the quasi-linear parabolic equations with
Nuemann boundary conditions</p>
        <p>− div | , ∇
= −
div | , ∇
( )| ( )
( )| ( )
, ∇</p>
        <p>( )
, ∇
+ div∇ ( )− ∇
( )| ( )
, ( ) −
,</p>
        <p>Π
= 0 on
( ),
∗ ∗
∗
−
| , ∇ , ∇ Ω ,
0 ≤ ( ) ≤ a.a.in Ω ,</p>
        <p>(0, ) = , ( ), ∀ ∈ Ω . (24)
In principle, instead of the initial condition (24) we may consider other image that can be generated
from , and the bicubic interpolation of the MODIS band , onto the entire domain Ω following
one of well-known simple data fusion methods [32].</p>
      </sec>
    </sec>
    <sec id="sec-8">
      <title>Numerical Experiments</title>
      <p>In order to illustrate the proposed approach for the restoration of satellite multi-spectral images we have
used two Sentinel-2 images (610 × 699 in pixels) over the Dnipro Airport area, Ukraine (see Fig. 1) that
were captured at different time instances. What is the most important, it was a growing season when the
global biophysical processes are rapid enough. This region represents a typical agricultural area with
medium sides fields of various shapes.
Figure</p>
      <p>2: MODIS image with the date of generation 2019/07/01</p>
      <p>We also have a cloud-free MODIS image (67 × 77 in pixels) from 2019/07/01 (see Fig. 2). We solve
the interpolation problem (A2). As a result, a new image from the date 2019/07/01 at the Sentinel-level of
resolution is depicted in Fig. 3. These numerical simulations have been supplied by a detailed analysis of
the obtained results using the special validation metrics.
8. References
[19] D. Cruz-Uribe, A. Fiorenza, Variable Lebesgue Spaces: Foundations and Harmonic Analysis,</p>
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[22] V. Zhikov, Solvability of the three-dimensional thermistor problem, Proceedings of the Steklov</p>
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