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  <front>
    <journal-meta>
<journal-id journal-id-type="publisher">NPG</journal-id>
<journal-title-group>
<journal-title>Nonlinear Processes in Geophysics</journal-title>
<abbrev-journal-title abbrev-type="publisher">NPG</abbrev-journal-title>
<abbrev-journal-title abbrev-type="nlm-ta">Nonlin. Processes Geophys.</abbrev-journal-title>
</journal-title-group>
<issn pub-type="epub">1607-7946</issn>
<publisher><publisher-name>Copernicus Publications</publisher-name>
<publisher-loc>Göttingen, Germany</publisher-loc>
</publisher>
</journal-meta>

    <article-meta>
      <article-id pub-id-type="doi">10.5194/npg-24-141-2017</article-id><title-group><article-title>Spatial and radiometric characterization of multi-spectrum satellite images
through multi-fractal analysis</article-title>
      </title-group><?xmltex \runningtitle{Spatial and radiometric characterization of multi-spectrum satellite images}?><?xmltex \runningauthor{C.~Alonso et al.}?>
      <contrib-group>
        <contrib contrib-type="author" corresp="no" rid="aff1 aff2">
          <name><surname>Alonso</surname><given-names>Carmelo</given-names></name>
          
        </contrib>
        <contrib contrib-type="author" corresp="yes" rid="aff2 aff3">
          <name><surname>Tarquis</surname><given-names>Ana M.</given-names></name>
          <email>anamaria.tarquis@upm.es</email>
        <ext-link>https://orcid.org/0000-0003-2336-5371</ext-link></contrib>
        <contrib contrib-type="author" corresp="no" rid="aff4">
          <name><surname>Zúñiga</surname><given-names>Ignacio</given-names></name>
          
        </contrib>
        <contrib contrib-type="author" corresp="no" rid="aff2">
          <name><surname>Benito</surname><given-names>Rosa M.</given-names></name>
          
        </contrib>
        <aff id="aff1"><label>1</label><institution>Earth Observation Systems, Indra Sistemas S.A., Madrid, Spain</institution>
        </aff>
        <aff id="aff2"><label>2</label><institution>Grupo de Sistemas Complejos, U.P.M, Madrid, Spain</institution>
        </aff>
        <aff id="aff3"><label>3</label><institution>CEIGRAM, E.T.S.I.A.A.B., U.P.M, Madrid, Spain</institution>
        </aff>
        <aff id="aff4"><label>4</label><institution>Dpt. Física Fundamental, Facultad de Ciencias, Universidad
Nacional de Educación a Distancia (UNED), Madrid, Spain</institution>
        </aff>
      </contrib-group>
      <author-notes><corresp id="corr1">Ana M. Tarquis (anamaria.tarquis@upm.es)</corresp></author-notes><pub-date><day>16</day><month>March</month><year>2017</year></pub-date>
      
      <volume>24</volume>
      <issue>2</issue>
      <fpage>141</fpage><lpage>155</lpage>
      <history>
        <date date-type="received"><day>20</day><month>May</month><year>2016</year></date>
           <date date-type="rev-request"><day>5</day><month>August</month><year>2016</year></date>
           <date date-type="rev-recd"><day>3</day><month>February</month><year>2017</year></date>
           <date date-type="accepted"><day>22</day><month>February</month><year>2017</year></date>
      </history>
      <permissions>
<license license-type="open-access">
<license-p>This work is licensed under a Creative Commons Attribution 3.0 Unported License. To view a copy of this license, visit <ext-link ext-link-type="uri" xlink:href="http://creativecommons.org/licenses/by/3.0/">http://creativecommons.org/licenses/by/3.0/</ext-link></license-p>
</license>
</permissions><self-uri xlink:href="https://npg.copernicus.org/articles/24/141/2017/npg-24-141-2017.html">This article is available from https://npg.copernicus.org/articles/24/141/2017/npg-24-141-2017.html</self-uri>
<self-uri xlink:href="https://npg.copernicus.org/articles/24/141/2017/npg-24-141-2017.pdf">The full text article is available as a PDF file from https://npg.copernicus.org/articles/24/141/2017/npg-24-141-2017.pdf</self-uri>


      <abstract>
    <p>Several studies have shown that vegetation indexes can be used to
estimate root zone soil moisture. Earth surface images, obtained by high-resolution satellites, presently give a lot of information on these
indexes, based on the data of several wavelengths. Because of the potential capacity for
systematic observations at various scales, remote sensing technology extends
the possible data archives from the present time to several decades back.
Because of this advantage, enormous efforts have been made by researchers and
application specialists to delineate vegetation indexes from local scale to
global scale by applying remote sensing imagery.</p>
    <p>In this work, four band images have been considered, which are involved in these
vegetation indexes, and were taken by satellites Ikonos-2 and Landsat-7 of the same
geographic location, to study the effect of both spatial (pixel size) and
radiometric (number of bits coding the image) resolution on these wavelength
bands as well as two vegetation indexes: the Normalized Difference
Vegetation Index (NDVI) and the Enhanced Vegetation Index (EVI).</p>
    <p>In order to do so, a multi-fractal analysis of these multi-spectral images
was applied in each of these bands and the two indexes derived. The results
showed that spatial resolution has a similar scaling effect in the four
bands, but radiometric resolution has a larger influence in blue and green
bands than in red and near-infrared bands. The NDVI showed a higher
sensitivity to the radiometric resolution than EVI. Both were equally
affected by the spatial resolution.</p>
    <p>From both factors, the spatial resolution has a major impact in the
multi-fractal spectrum for all the bands and the vegetation indexes. This
information should be taken in to account when vegetation indexes based on
different satellite sensors are obtained.</p>
  </abstract>
    </article-meta>
  </front>
<body>
      

<sec id="Ch1.S1" sec-type="intro">
  <title>Introduction</title>
      <p>Soil moisture is a critical condition affecting interaction of land surface
and atmosphere. Remotely sensed data are an important source of information
and can indirectly measure soil moisture in space and time. However, the
signal only penetrates the top few centimetres, and soil moisture at deeper
layers must be estimated. One method to estimate soil moisture at deeper
layers is through vegetation indexes. Several authors have investigated the
potential of vegetation indexes to estimate root zone soil moisture. The
Normalized Difference Vegetation Index (NDVI) and Enhanced Vegetation Index
(EVI) have been used by several authors (Wang et al., 2007; Ben-Ze'ev et
al., 2006; Deng et al., 2007) in different conditions to find significant
estimations with root zone soil moisture. For the estimation of these
indexes near-infrared (NIR), red and blue wavelengths are needed (Huete et al., 2014).</p>
      <p>The images provided by the satellites show the land surface in a wide range
of wavelengths (from visible to thermal infrared or microwaves) and also
with a great variety of spatial resolutions (from a few kilometres to tens
of centimetres). The analysis of these varied images and their synergic
possibilities are a challenging problem, especially with new sensors, which
have small spatial resolution and a large range of radiometric
quantification. Fractal analysis offers significant potential for
improvement in the measurement and analysis of spatially and radiometrically
complex remote sensing data. This analysis also provides quantitative
insight on the spatial complexity in the information of the landscape
contained within these data.</p>
      <p>In the general mathematical framework of fractal geometry, many analytical
methods have been developed, including the following: textural homogeneity, which has been
characterized using the fractal dimension (Fioravanti, 1994) (it has also
been used as a spatial measure for describing the complexity of remote
sensing imagery; Lam and De Cola, 1993)); and changes in the image complexity,
which have been detected through the spectral range of hyperspectral images
affecting the fractal dimension (Qiu et al., 1999). Similarly, De Cola (1989)
and Lam (1990) have found that fractal dimension also depends on the
spectral bands of Landsat-7 TM imagery.</p>
      <p>Motivated by the fractal geometry of sets (Mandelbrot, 1983), the
development of multi-fractal theory, introduced in the context of turbulence,
has been applied in many areas, such as earthquake distribution analysis
(Hirata and Imoto, 1991), soil pore characterization (Kravchenko et al., 1999; Tarquis et al., 2003), image analysis (Sánchez et al., 1992) or
remote sensing (Tessier et al., 1993; Cheng and Agterberg, 1996; Schmitt et
al., 1997; Laferrière and Gaonac'h, 1999; Cheng, 2004; Lovejoy et al.,
2001b; Du and Yeo, 2002; Parrinello and Vaughan, 2002; Harvey et al., 2002;
Turiel et al., 2005).</p>
      <p>The acquisition of remotely sensed multiple spectral images is thus a unique
source of data for determining the scale-invariant characteristics of the
radiance fields related to many factors, such as soil and bedrock chemical
composition, humidity content and surface temperature (e.g. Laferrière
and Gaonac'h, 1999; Maìtre and Pinciroli, 1999; Lovejoy et al., 2001a,
b; Harvey et al., 2002; Beaulieu and Gaonac'h, 2002; Gaonac'h et al., 2003).
In one of the schemes used in the multi-fractal analysis, the satellite image
is considered as a mass distribution of a statistical measure on the space
domain studied, and it is analysed through a multi-fractal (MF) spectrum
(Cheng, 2004; Mao-Gui Hu, 2009; Tarquis et al., 2014), which gives either
geometrical or probabilistic information about the pixel distribution with
the same singularity. Other techniques focus on the
variations of a measure analysing the moments of the absolute differences of
their values at different scales, e.g. the Generalized Structure Function and the
Universal Multi-fractal model (Lovejoy et al., 2001a, 2008; Renosh et al.,
2015)</p>
      <p>The aim of this work is to characterize by MF analysis the image patterns in the wavelength range for the common bands of the satellites used, as well as both NDVI and EVI indexes. In order to investigate how the image information is
affected by the sampling with different spatial and radiometric resolutions,
we have also analysed images of the same site but acquired by two different
satellites: Landsat-7 and Ikonos-2.</p>
      <p>We present a comparative analysis of multi-fractal (MF) tools applied to
multi-spectral images obtained by Ikonos-2 and LANDSAT-7. Both satellites
have several bands in visible and near-infrared spectral regions in common
that can be used in vegetation-index estimation. However, the bands have
different spatial resolution (4 m for Ikonos-2 and 30 m for LANDSAT-7), and
radiometric resolution (11 bits for Ikonos-2 and 8 bits for LANDSAT-7). The bands we have chosen
are red, green, blue and near infrared. For each of those
bands, the MF spectrum has been calculated directly from the Hölder
exponents <inline-formula><mml:math id="M1" display="inline"><mml:mi mathvariant="italic">α</mml:mi></mml:math></inline-formula> and the singularity spectrum f(<inline-formula><mml:math id="M2" display="inline"><mml:mrow><mml:mi mathvariant="italic">α</mml:mi><mml:mo>)</mml:mo></mml:mrow></mml:math></inline-formula>. The same
calculations were applied for NDVI and EVI estimated on red, blue and near-infrared bands
for each image.</p>
</sec>
<sec id="Ch1.S2">
  <title>Materials and methods</title>
<sec id="Ch1.S2.SS1">
  <title>Images</title>
      <p>As already noted, in this work we have analysed two images of the same site
acquired from different satellites, Landsat-7 and Ikonos-2. Both are
multi-spectral images with several bands that cover several regions of the
electromagnetic spectrum in the visible and near-infrared wavelength.</p>
      <p>Landsat-7 was put in orbit in April 1999. This satellite follows a
sun-synchronous orbit at 705 km of altitude, with an equatorial crossing
time of 10:00 LT in the descending node. It requires 98.8 min to circle
the Earth, tracing a worldwide reference system (WRS) of just over 230
ground paths. Over at least three decades, Landsat-7 orbits over each of
these paths once every 16 days in a repetitive cycle (Mika, 1997).</p>
      <p>The main Landsat-7 sensor for Earth observation is the Enhanced Thematic
Mapper Plus (ETM<inline-formula><mml:math id="M3" display="inline"><mml:mrow><mml:mo>+</mml:mo><mml:mo>)</mml:mo></mml:mrow></mml:math></inline-formula>. The ETM<inline-formula><mml:math id="M4" display="inline"><mml:mo>+</mml:mo></mml:math></inline-formula> operates as a whiskbroom scanner and
acquires data for seven spectral bands: visible (ETM<inline-formula><mml:math id="M5" display="inline"><mml:mo>+</mml:mo></mml:math></inline-formula>#1, from 0.45 to
0.52 <inline-formula><mml:math id="M6" display="inline"><mml:mi mathvariant="normal">µ</mml:mi></mml:math></inline-formula>m; ETM<inline-formula><mml:math id="M7" display="inline"><mml:mo>+</mml:mo></mml:math></inline-formula>#2, from 0.53 to 0.61 <inline-formula><mml:math id="M8" display="inline"><mml:mi mathvariant="normal">µ</mml:mi></mml:math></inline-formula>m; ETM<inline-formula><mml:math id="M9" display="inline"><mml:mo>+</mml:mo></mml:math></inline-formula>#3, from 0.63
to 0.69 <inline-formula><mml:math id="M10" display="inline"><mml:mi mathvariant="normal">µ</mml:mi></mml:math></inline-formula>m), near infrared (ETM<inline-formula><mml:math id="M11" display="inline"><mml:mo>+</mml:mo></mml:math></inline-formula>#4, from 0.78 to 0.9 <inline-formula><mml:math id="M12" display="inline"><mml:mi mathvariant="normal">µ</mml:mi></mml:math></inline-formula>m),
shortwave infrared (ETM<inline-formula><mml:math id="M13" display="inline"><mml:mo>+</mml:mo></mml:math></inline-formula>#5, from 1.55 to 1.75 <inline-formula><mml:math id="M14" display="inline"><mml:mi mathvariant="normal">µ</mml:mi></mml:math></inline-formula>m, and ETM<inline-formula><mml:math id="M15" display="inline"><mml:mo>+</mml:mo></mml:math></inline-formula>#7,
from 2.09 to 2.35 <inline-formula><mml:math id="M16" display="inline"><mml:mi mathvariant="normal">µ</mml:mi></mml:math></inline-formula>m) and thermal infrared (ETM<inline-formula><mml:math id="M17" display="inline"><mml:mo>+</mml:mo></mml:math></inline-formula>#6, from 10.4 to
12.5 <inline-formula><mml:math id="M18" display="inline"><mml:mi mathvariant="normal">µ</mml:mi></mml:math></inline-formula>m). The ETM<inline-formula><mml:math id="M19" display="inline"><mml:mo>+</mml:mo></mml:math></inline-formula> ground sampling distance (pixel size in the
images) is 30 m for the six reflective bands and 60 m for the thermal band.
The ETM<inline-formula><mml:math id="M20" display="inline"><mml:mo>+</mml:mo></mml:math></inline-formula> also acquires images for a panchromatic band (ETM<inline-formula><mml:math id="M21" display="inline"><mml:mo>+</mml:mo></mml:math></inline-formula>#8, from
0.52 to 0.9 <inline-formula><mml:math id="M22" display="inline"><mml:mi mathvariant="normal">µ</mml:mi></mml:math></inline-formula>m) with a 15 m ground sampling distance. The radiometric
resolution of the Landsat-7 data is 8 bits per pixel or 256 grey levels for the
pixel digital value.</p>
      <p>Ikonos-2 was launched in September 1999. Its panchromatic sensor, with a
resolution of 0.82 m, provided the first very high-resolution images of the
Earth's surface from earth observation satellites (EOS). The Ikonos-2 orbiting altitude is approximately 681 km; it is inclined 98.1<inline-formula><mml:math id="M23" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> to the equator and it provides
sun-synchronous operation. The equatorial crossing time of Ikonos-2 is 10:30 LT in the descending node. The orbit provides daily access to sites within
45<inline-formula><mml:math id="M24" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> of nadir (Dial et al., 2003).</p>
      <p>The multi-spectral sensor simultaneously collects blue (IK#1, from 0.445
to 0.516 <inline-formula><mml:math id="M25" display="inline"><mml:mi mathvariant="normal">µ</mml:mi></mml:math></inline-formula>m), green (IK#2, from 0.506 to 0.595 <inline-formula><mml:math id="M26" display="inline"><mml:mi mathvariant="normal">µ</mml:mi></mml:math></inline-formula>m), red
(IK#3, from 0.632 to 0.698 <inline-formula><mml:math id="M27" display="inline"><mml:mi mathvariant="normal">µ</mml:mi></mml:math></inline-formula>m) and near-infrared (IK#4, from
0.757 to 0.853 <inline-formula><mml:math id="M28" display="inline"><mml:mi mathvariant="normal">µ</mml:mi></mml:math></inline-formula>m) bands with 3.28 m resolution at nadir. Both
images, panchromatic and multi-spectral, have a radiometric resolution of 11
bits per pixel or 2048 grey levels for the pixel digital value.</p>
      <p>The Landsat-7 multi-spectral image used in this study was acquired on 6 August
2000 at 10:46 LT. and it corresponds to the scene with WRS
coordinates: path and row 201 and 32, respectively. This scene is located in the central
region of Spain and it covers a square surface of approximately 180 km
side length, located around Madrid. Solar azimuth and elevation angles for
this scene are 132.44 and 58.62<inline-formula><mml:math id="M29" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> respectively.</p>
      <p>The Ikonos-2 datum used in this study is a multi-spectral image acquired on
8 August  2000 at 11:03 LT. It covers an area of 11 km<inline-formula><mml:math id="M30" display="inline"><mml:msup><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msup></mml:math></inline-formula>
located near Aranjuez, south of Madrid, in the central region of Spain.
Solar azimuth and elevation angles for this scene are 139.5 and 60.79<inline-formula><mml:math id="M31" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> respectively. Both images were corrected geometrically to the same
cartographic projection: Universal Transverse Mercatorprojection (UTM), zone 30<inline-formula><mml:math id="M32" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> N, by a co-registration process.</p>
      <p>The analysis has been carried out on a subset that covers (approximately)
the same area in both the Landsat-7 and the Ikonos-2 images, corresponding
to a region located north of the town of Aranjuez. The representative elements
of the land used in the selected area are irrigation crops, pastures, heaths,
unirrigated land cultivations and olive groves. The Landsat-7 subset image
is a square of <inline-formula><mml:math id="M33" display="inline"><mml:mrow><mml:mn mathvariant="normal">512</mml:mn><mml:mo>×</mml:mo><mml:mn mathvariant="normal">512</mml:mn></mml:mrow></mml:math></inline-formula> pixels with a resolution of 30 m covering a somewhat
larger surface than the Ikonos-2 image. The Ikonos-2 image consists of a
square subset with <inline-formula><mml:math id="M34" display="inline"><mml:mrow><mml:mn mathvariant="normal">2048</mml:mn><mml:mo>×</mml:mo><mml:mn mathvariant="normal">2048</mml:mn></mml:mrow></mml:math></inline-formula> pixels and 4 m resolution.</p>
</sec>
<sec id="Ch1.S2.SS2">
  <title>Vegetation indexes</title>
      <p>Vegetation is one of the landscape elements that has received the most
attention in the field of image analysis. Therefore, there are many
parameters that can be used to obtain information on vegetation from remote
sensing imagery.</p>
      <p>One of the main parameters is made up of the vegetation indexes. These
indexes allow to detect the presence of vegetation in an area and its
activity, since its values are related to this activity. For this, we can
use the reflectance values corresponding to the different wavelengths,
interpreting these in relation to the photosynthetic activity. Of these
indexes, the most commonly used is the NDVI.</p>
      <p>The NDVI is defined by
            <disp-formula id="Ch1.E1" content-type="numbered"><mml:math id="M35" display="block"><mml:mrow><mml:mi mathvariant="normal">NDVI</mml:mi><mml:mo>=</mml:mo><mml:mstyle displaystyle="true"><mml:mfrac style="display"><mml:mrow><mml:mi mathvariant="normal">NIR</mml:mi><mml:mo>-</mml:mo><mml:mi mathvariant="normal">R</mml:mi></mml:mrow><mml:mrow><mml:mi mathvariant="normal">NIR</mml:mi><mml:mo>+</mml:mo><mml:mi mathvariant="normal">R</mml:mi></mml:mrow></mml:mfrac></mml:mstyle><mml:mo>,</mml:mo></mml:mrow></mml:math></disp-formula>
          where NIR is the pixel value in the near-infrared band and R the pixel value
in the red band. The values of this index are within the range (<inline-formula><mml:math id="M36" display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>1, 1) and
their positive values are sensitive to the proportion of soil and vegetation
in each pixel (Carlson and Ripley, 1997). Pixels with NDVI &lt; 0.2 are
considered without vegetation or bare soil. Pixels with NDVI &gt; 0.5 are considered as fully covered by vegetation.</p>
      <p>EVI, the other vegetation index, is defined by
            <disp-formula id="Ch1.E2" content-type="numbered"><mml:math id="M37" display="block"><mml:mrow><mml:mi mathvariant="normal">EVI</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">2.5</mml:mn><mml:mstyle displaystyle="true"><mml:mfrac style="display"><mml:mrow><mml:mfenced open="(" close=")"><mml:mi mathvariant="normal">NIR</mml:mi><mml:mo>-</mml:mo><mml:mi mathvariant="normal">R</mml:mi></mml:mfenced></mml:mrow><mml:mrow><mml:mfenced open="(" close=")"><mml:mi>L</mml:mi><mml:mo>+</mml:mo><mml:mi mathvariant="normal">NIR</mml:mi><mml:mo>+</mml:mo><mml:msub><mml:mi>C</mml:mi><mml:mn mathvariant="normal">1</mml:mn></mml:msub><mml:mi mathvariant="normal">R</mml:mi><mml:mo>-</mml:mo><mml:msub><mml:mi>C</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub><mml:mi mathvariant="normal">B</mml:mi></mml:mfenced></mml:mrow></mml:mfrac></mml:mstyle><mml:mo>,</mml:mo></mml:mrow></mml:math></disp-formula>
          where NIR is the pixel value in the near-infrared band, R the pixel value in
the red band and B the pixel value in the blue band. <inline-formula><mml:math id="M38" display="inline"><mml:mi>L</mml:mi></mml:math></inline-formula>, <inline-formula><mml:math id="M39" display="inline"><mml:mrow><mml:msub><mml:mi>C</mml:mi><mml:mn mathvariant="normal">1</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> and
<inline-formula><mml:math id="M40" display="inline"><mml:mrow><mml:msub><mml:mi>C</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> are constants with the values 1, 6 and 7.5 respectively. The main
characteristic of this index is that it corrects some distortions caused by
the light dispersion from aerosols, as well as the background soil (Huete et
al., 2014).</p>
</sec>
<sec id="Ch1.S2.SS3">
  <title>Multi-fractal image analysis</title>
      <p>A monofractal object can be measured by counting the number <inline-formula><mml:math id="M41" display="inline"><mml:mi>N</mml:mi></mml:math></inline-formula> of <inline-formula><mml:math id="M42" display="inline"><mml:mi mathvariant="italic">δ</mml:mi></mml:math></inline-formula>
size boxes needed to cover the object. The measure depends on the box size
as
            <disp-formula id="Ch1.E3" content-type="numbered"><mml:math id="M43" display="block"><mml:mrow><mml:mi>N</mml:mi><mml:mo>(</mml:mo><mml:mi mathvariant="italic">δ</mml:mi><mml:mo>)</mml:mo><mml:mo>∝</mml:mo><mml:msup><mml:mi mathvariant="italic">δ</mml:mi><mml:mrow><mml:mo>-</mml:mo><mml:msub><mml:mi>D</mml:mi><mml:mn mathvariant="normal">0</mml:mn></mml:msub></mml:mrow></mml:msup><mml:mo>,</mml:mo></mml:mrow></mml:math></disp-formula>
          where
            <disp-formula id="Ch1.E4" content-type="numbered"><mml:math id="M44" display="block"><mml:mrow><mml:msub><mml:mi>D</mml:mi><mml:mn mathvariant="normal">0</mml:mn></mml:msub><mml:mo>=</mml:mo><mml:munder><mml:mo movablelimits="false">lim⁡</mml:mo><mml:mrow><mml:mi mathvariant="italic">δ</mml:mi><mml:mo>→</mml:mo><mml:mn mathvariant="normal">0</mml:mn></mml:mrow></mml:munder><mml:mstyle displaystyle="true"><mml:mfrac style="display"><mml:mrow><mml:mi>log⁡</mml:mi><mml:mi>N</mml:mi><mml:mo>(</mml:mo><mml:mi mathvariant="italic">δ</mml:mi><mml:mo>)</mml:mo></mml:mrow><mml:mrow><mml:mi>log⁡</mml:mi><mml:mstyle displaystyle="false"><mml:mfrac style="text"><mml:mn mathvariant="normal">1</mml:mn><mml:mi mathvariant="italic">δ</mml:mi></mml:mfrac></mml:mstyle></mml:mrow></mml:mfrac></mml:mstyle></mml:mrow></mml:math></disp-formula>
          is the fractal dimension. <inline-formula><mml:math id="M45" display="inline"><mml:mrow><mml:msub><mml:mi>D</mml:mi><mml:mn mathvariant="normal">0</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> is calculated from slope of a log–log
plot. However, many examples are found where a single scaling law cannot be
applied and it is necessary to do a multi-scaling analysis.</p>
      <p>There are several methods for implementing multi-fractal analysis. The
universal multi-fractal (UM) model assumes that multi-fractals are generated
from a random variable with an exponentiated extreme Levy distribution
(Lavallée et al., 1991; Tessier et al., 1993). In UM analysis, the
scaling exponent <inline-formula><mml:math id="M46" display="inline"><mml:mrow><mml:mi>K</mml:mi><mml:mo>(</mml:mo><mml:mi>q</mml:mi><mml:mo>)</mml:mo></mml:mrow></mml:math></inline-formula> is highly relevant. This function for the moments <inline-formula><mml:math id="M47" display="inline"><mml:mi>q</mml:mi></mml:math></inline-formula> of
a cascade conserved process is obtained according to Schertzer and Lovejoy (1987), as follows:
            <disp-formula id="Ch1.E5" content-type="numbered"><mml:math id="M48" display="block"><mml:mrow><mml:mi>K</mml:mi><mml:mfenced open="(" close=")"><mml:mi>q</mml:mi></mml:mfenced><mml:mo>=</mml:mo><mml:mfenced open="{" close="}"><mml:mtable class="array" columnalign="left"><mml:mtr><mml:mtd><mml:mrow><mml:mstyle displaystyle="true"><mml:mfrac style="display"><mml:mrow><mml:msub><mml:mi>C</mml:mi><mml:mn mathvariant="normal">1</mml:mn></mml:msub><mml:mfenced open="(" close=")"><mml:msup><mml:mi>q</mml:mi><mml:mrow><mml:msub><mml:mi mathvariant="italic">α</mml:mi><mml:mi mathvariant="normal">L</mml:mi></mml:msub></mml:mrow></mml:msup><mml:mo>-</mml:mo><mml:mi>q</mml:mi></mml:mfenced></mml:mrow><mml:mrow><mml:msub><mml:mi mathvariant="italic">α</mml:mi><mml:mi mathvariant="normal">L</mml:mi></mml:msub><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:mfrac></mml:mstyle><mml:mspace width="0.25em" linebreak="nobreak"/><mml:mspace linebreak="nobreak" width="0.25em"/><mml:mtext>if</mml:mtext><mml:mspace width="0.25em" linebreak="nobreak"/><mml:mspace width="0.25em" linebreak="nobreak"/><mml:msub><mml:mi mathvariant="italic">α</mml:mi><mml:mi mathvariant="normal">L</mml:mi></mml:msub><mml:mo>≠</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:mtd></mml:mtr><mml:mtr><mml:mtd><mml:mrow><mml:msub><mml:mi>C</mml:mi><mml:mn mathvariant="normal">1</mml:mn></mml:msub><mml:mi>q</mml:mi><mml:mi>log⁡</mml:mi><mml:mfenced close=")" open="("><mml:mi>q</mml:mi></mml:mfenced><mml:mspace width="0.25em" linebreak="nobreak"/><mml:mspace width="0.25em" linebreak="nobreak"/><mml:mtext>if</mml:mtext><mml:mspace width="0.25em" linebreak="nobreak"/><mml:mspace width="0.25em" linebreak="nobreak"/><mml:msub><mml:mi mathvariant="italic">α</mml:mi><mml:mi mathvariant="normal">L</mml:mi></mml:msub><mml:mo>=</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:mtd></mml:mtr></mml:mtable></mml:mfenced><mml:mo>,</mml:mo></mml:mrow></mml:math></disp-formula>
          where <inline-formula><mml:math id="M49" display="inline"><mml:mrow><mml:msub><mml:mi>C</mml:mi><mml:mn mathvariant="normal">1</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> is the mean intermittency codimension and <inline-formula><mml:math id="M50" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="italic">α</mml:mi><mml:mi mathvariant="normal">L</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> is the
Levy index. These are known as the UM parameters.</p>
      <p>Other method is the moment method developed by Halsey et al. (1986) and
applied to this case study. This method mainly uses three functions: <inline-formula><mml:math id="M51" display="inline"><mml:mrow><mml:mi mathvariant="italic">τ</mml:mi><mml:mo>(</mml:mo><mml:mi>q</mml:mi><mml:mo>)</mml:mo></mml:mrow></mml:math></inline-formula>, known as the mass exponent function; <inline-formula><mml:math id="M52" display="inline"><mml:mi mathvariant="italic">α</mml:mi></mml:math></inline-formula>, the coarse Hölder
exponent; and <inline-formula><mml:math id="M53" display="inline"><mml:mrow><mml:mi>f</mml:mi><mml:mo>(</mml:mo><mml:mi mathvariant="italic">α</mml:mi><mml:mo>)</mml:mo></mml:mrow></mml:math></inline-formula>, multi-fractal spectrum (MFS). A measure (or field),
defined in two-dimensional image embedding space (<inline-formula><mml:math id="M54" display="inline"><mml:mrow><mml:mi>n</mml:mi><mml:mo>×</mml:mo><mml:mi>n</mml:mi></mml:mrow></mml:math></inline-formula> pixels) and
with values based on grey tones (for 8 bits, from 0 to 255), cannot be
considered as a geometrical set and therefore cannot be characterized by a
single fractal dimension.</p>
      <p>To characterize the scaling property of a variable measured on the spatial
domain of the studied area, it divides the image into a number of self-similar
boxes. Applying disjoint covering by boxes in an “up-scaling” partitioning
process we obtain the partition function <inline-formula><mml:math id="M55" display="inline"><mml:mrow><mml:mi mathvariant="italic">χ</mml:mi><mml:mo>(</mml:mo><mml:mi>q</mml:mi><mml:mo>,</mml:mo><mml:mi mathvariant="italic">δ</mml:mi><mml:mo>)</mml:mo></mml:mrow></mml:math></inline-formula> (Feder,
1989) defined as follows:
            <disp-formula id="Ch1.E6" content-type="numbered"><mml:math id="M56" display="block"><mml:mrow><mml:mi mathvariant="italic">χ</mml:mi><mml:mo>(</mml:mo><mml:mi>q</mml:mi><mml:mo>,</mml:mo><mml:mi mathvariant="italic">δ</mml:mi><mml:mo>)</mml:mo><mml:mo>=</mml:mo><mml:munderover><mml:mo movablelimits="false">∑</mml:mo><mml:mrow><mml:mi>i</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow><mml:mrow><mml:mi>N</mml:mi><mml:mo>(</mml:mo><mml:mi mathvariant="italic">δ</mml:mi><mml:mo>)</mml:mo></mml:mrow></mml:munderover><mml:msubsup><mml:mi mathvariant="italic">μ</mml:mi><mml:mi>i</mml:mi><mml:mi>q</mml:mi></mml:msubsup><mml:mo>(</mml:mo><mml:mi mathvariant="italic">δ</mml:mi><mml:mo>)</mml:mo><mml:mo>=</mml:mo><mml:munderover><mml:mo movablelimits="false">∑</mml:mo><mml:mrow><mml:mi>i</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow><mml:mrow><mml:mi>N</mml:mi><mml:mo>(</mml:mo><mml:mi mathvariant="italic">δ</mml:mi><mml:mo>)</mml:mo></mml:mrow></mml:munderover><mml:msubsup><mml:mi>m</mml:mi><mml:mi>i</mml:mi><mml:mi>q</mml:mi></mml:msubsup><mml:mo>,</mml:mo></mml:mrow></mml:math></disp-formula>
          where <inline-formula><mml:math id="M57" display="inline"><mml:mi>m</mml:mi></mml:math></inline-formula> is the mass of the measure, <inline-formula><mml:math id="M58" display="inline"><mml:mi>q</mml:mi></mml:math></inline-formula> is the mass exponent, <inline-formula><mml:math id="M59" display="inline"><mml:mi mathvariant="italic">δ</mml:mi></mml:math></inline-formula> is the
length size of the box and <inline-formula><mml:math id="M60" display="inline"><mml:mrow><mml:mi>N</mml:mi><mml:mo>(</mml:mo><mml:mi mathvariant="italic">δ</mml:mi><mml:mo>)</mml:mo></mml:mrow></mml:math></inline-formula> is the number of boxes in
which <inline-formula><mml:math id="M61" display="inline"><mml:mrow><mml:msub><mml:mi>m</mml:mi><mml:mi>i</mml:mi></mml:msub><mml:mo>&gt;</mml:mo><mml:mn mathvariant="normal">0</mml:mn></mml:mrow></mml:math></inline-formula>. Based on this, the mass exponent function <inline-formula><mml:math id="M62" display="inline"><mml:mrow><mml:mi mathvariant="italic">τ</mml:mi><mml:mo>(</mml:mo><mml:mi>q</mml:mi><mml:mo>)</mml:mo></mml:mrow></mml:math></inline-formula> shows
how the moments of the measure scales with the box size:
            <disp-formula id="Ch1.E7" content-type="numbered"><mml:math id="M63" display="block"><mml:mrow><mml:mi mathvariant="italic">τ</mml:mi><mml:mo>(</mml:mo><mml:mi>q</mml:mi><mml:mo>)</mml:mo><mml:mo>=</mml:mo><mml:munder><mml:mo movablelimits="false">lim⁡</mml:mo><mml:mrow><mml:mi mathvariant="italic">δ</mml:mi><mml:mo>→</mml:mo><mml:mn mathvariant="normal">0</mml:mn></mml:mrow></mml:munder><mml:mstyle displaystyle="true"><mml:mfrac style="display"><mml:mrow><mml:mi>log⁡</mml:mi><mml:mo>&lt;</mml:mo><mml:mi mathvariant="italic">χ</mml:mi><mml:mo>(</mml:mo><mml:mi>q</mml:mi><mml:mo>,</mml:mo><mml:mi mathvariant="italic">δ</mml:mi><mml:mo>)</mml:mo><mml:mo>&gt;</mml:mo></mml:mrow><mml:mrow><mml:mi>log⁡</mml:mi><mml:mo>(</mml:mo><mml:mi mathvariant="italic">δ</mml:mi><mml:mo>)</mml:mo></mml:mrow></mml:mfrac></mml:mstyle><mml:mo>=</mml:mo><mml:munder><mml:mo movablelimits="false">lim⁡</mml:mo><mml:mrow><mml:mi mathvariant="italic">δ</mml:mi><mml:mo>→</mml:mo><mml:mn mathvariant="normal">0</mml:mn></mml:mrow></mml:munder><mml:mstyle displaystyle="true"><mml:mfrac style="display"><mml:mrow><mml:mi>log⁡</mml:mi><mml:mo>&lt;</mml:mo><mml:munderover><mml:mo movablelimits="false">∑</mml:mo><mml:mrow><mml:mi>i</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow><mml:mrow><mml:mi>N</mml:mi><mml:mo>(</mml:mo><mml:mi mathvariant="italic">δ</mml:mi><mml:mo>)</mml:mo></mml:mrow></mml:munderover><mml:msubsup><mml:mi>m</mml:mi><mml:mi>i</mml:mi><mml:mi>q</mml:mi></mml:msubsup><mml:mo>&gt;</mml:mo></mml:mrow><mml:mrow><mml:mi>log⁡</mml:mi><mml:mo>(</mml:mo><mml:mi mathvariant="italic">δ</mml:mi><mml:mo>)</mml:mo></mml:mrow></mml:mfrac></mml:mstyle><mml:mo>,</mml:mo></mml:mrow></mml:math></disp-formula>
          where <inline-formula><mml:math id="M64" display="inline"><mml:mrow><mml:mo>&lt;</mml:mo><mml:mspace width="0.25em" linebreak="nobreak"/><mml:mo>&gt;</mml:mo></mml:mrow></mml:math></inline-formula> represents a statistical moment of the measure
<inline-formula><mml:math id="M65" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="italic">μ</mml:mi><mml:mi>i</mml:mi></mml:msub><mml:mo>(</mml:mo><mml:mi mathvariant="italic">δ</mml:mi><mml:mo>)</mml:mo></mml:mrow></mml:math></inline-formula> defined on a group of non-overlapping boxes of the same
size partitioning as the area studied.</p>
      <p>The singularity index, <inline-formula><mml:math id="M66" display="inline"><mml:mi mathvariant="italic">α</mml:mi></mml:math></inline-formula>, can be determined by the Legendre
transformation of the <inline-formula><mml:math id="M67" display="inline"><mml:mrow><mml:mi mathvariant="italic">τ</mml:mi><mml:mo>(</mml:mo><mml:mi>q</mml:mi><mml:mo>)</mml:mo></mml:mrow></mml:math></inline-formula> curve (Halsey et al., 1986) as follows:
            <disp-formula id="Ch1.E8" content-type="numbered"><mml:math id="M68" display="block"><mml:mrow><mml:mi mathvariant="italic">α</mml:mi><mml:mo>(</mml:mo><mml:mi>q</mml:mi><mml:mo>)</mml:mo><mml:mo>=</mml:mo><mml:mstyle displaystyle="true"><mml:mfrac style="display"><mml:mrow><mml:mi mathvariant="normal">d</mml:mi><mml:mi mathvariant="italic">τ</mml:mi><mml:mo>(</mml:mo><mml:mi>q</mml:mi><mml:mo>)</mml:mo></mml:mrow><mml:mrow><mml:mi mathvariant="normal">d</mml:mi><mml:mi>q</mml:mi></mml:mrow></mml:mfrac></mml:mstyle><mml:mo>.</mml:mo></mml:mrow></mml:math></disp-formula>
          The number of cells of size <inline-formula><mml:math id="M69" display="inline"><mml:mi mathvariant="italic">δ</mml:mi></mml:math></inline-formula> with the same <inline-formula><mml:math id="M70" display="inline"><mml:mi mathvariant="italic">α</mml:mi></mml:math></inline-formula>, <inline-formula><mml:math id="M71" display="inline"><mml:mrow><mml:msub><mml:mi>N</mml:mi><mml:mi mathvariant="italic">α</mml:mi></mml:msub><mml:mo>(</mml:mo><mml:mi mathvariant="italic">δ</mml:mi><mml:mo>)</mml:mo></mml:mrow></mml:math></inline-formula>, is related to the cell size as <inline-formula><mml:math id="M72" display="inline"><mml:mrow><mml:msub><mml:mi>N</mml:mi><mml:mi mathvariant="italic">α</mml:mi></mml:msub><mml:mo>(</mml:mo><mml:mi mathvariant="italic">δ</mml:mi><mml:mo>)</mml:mo><mml:mo>∝</mml:mo><mml:msup><mml:mi mathvariant="italic">δ</mml:mi><mml:mrow><mml:mo>-</mml:mo><mml:mi>f</mml:mi><mml:mo>(</mml:mo><mml:mi mathvariant="italic">α</mml:mi><mml:mo>)</mml:mo></mml:mrow></mml:msup></mml:mrow></mml:math></inline-formula>, where <inline-formula><mml:math id="M73" display="inline"><mml:mrow><mml:mi>f</mml:mi><mml:mo>(</mml:mo><mml:mi mathvariant="italic">α</mml:mi><mml:mo>)</mml:mo></mml:mrow></mml:math></inline-formula> is a scaling exponent of
the cells with common <inline-formula><mml:math id="M74" display="inline"><mml:mi mathvariant="italic">α</mml:mi></mml:math></inline-formula>. Parameter <inline-formula><mml:math id="M75" display="inline"><mml:mrow><mml:mi>f</mml:mi><mml:mo>(</mml:mo><mml:mi mathvariant="italic">α</mml:mi><mml:mo>)</mml:mo></mml:mrow></mml:math></inline-formula> can be
calculated as follows:
            <disp-formula id="Ch1.E9" content-type="numbered"><mml:math id="M76" display="block"><mml:mrow><mml:mi>f</mml:mi><mml:mo>(</mml:mo><mml:mi mathvariant="italic">α</mml:mi><mml:mo>)</mml:mo><mml:mo>=</mml:mo><mml:mi>q</mml:mi><mml:mi mathvariant="italic">α</mml:mi><mml:mo>(</mml:mo><mml:mi>q</mml:mi><mml:mo>)</mml:mo><mml:mo>-</mml:mo><mml:mi mathvariant="italic">τ</mml:mi><mml:mo>(</mml:mo><mml:mi>q</mml:mi><mml:mo>)</mml:mo><mml:mo>.</mml:mo></mml:mrow></mml:math></disp-formula>
          MFS, shown as plot of <inline-formula><mml:math id="M77" display="inline"><mml:mi mathvariant="italic">α</mml:mi></mml:math></inline-formula> versus <inline-formula><mml:math id="M78" display="inline"><mml:mrow><mml:mi>f</mml:mi><mml:mo>(</mml:mo><mml:mi mathvariant="italic">α</mml:mi><mml:mo>)</mml:mo></mml:mrow></mml:math></inline-formula>,
quantitatively characterizes variability of the measure studied with
asymmetry to the right and left indicating domination of small and large
values respectively (Evertsz and Mandelbrot, 1992). There are three
characteristic values obtained from MFS, the singularity <inline-formula><mml:math id="M79" display="inline"><mml:mrow><mml:mi mathvariant="italic">α</mml:mi><mml:mo>(</mml:mo><mml:mi>q</mml:mi><mml:mo>)</mml:mo></mml:mrow></mml:math></inline-formula> values
for <inline-formula><mml:math id="M80" display="inline"><mml:mrow><mml:mi>q</mml:mi><mml:mo>=</mml:mo><mml:mfenced open="{" close="}"><mml:mn mathvariant="normal">0</mml:mn><mml:mo>,</mml:mo><mml:mn mathvariant="normal">1</mml:mn><mml:mo>,</mml:mo><mml:mn mathvariant="normal">2</mml:mn></mml:mfenced></mml:mrow></mml:math></inline-formula>. The first value (<inline-formula><mml:math id="M81" display="inline"><mml:mrow><mml:mi mathvariant="italic">α</mml:mi><mml:mfenced open="(" close=")"><mml:mn mathvariant="normal">0</mml:mn></mml:mfenced><mml:mo>)</mml:mo></mml:mrow></mml:math></inline-formula>
corresponds to the maximum of MFS and it is related to the box-counting
dimension of the measure support; the second value is related to information
or entropy dimension <inline-formula><mml:math id="M82" display="inline"><mml:mrow><mml:mo>(</mml:mo><mml:mi mathvariant="italic">α</mml:mi><mml:mfenced open="(" close=")"><mml:mn mathvariant="normal">1</mml:mn></mml:mfenced><mml:mo>)</mml:mo></mml:mrow></mml:math></inline-formula> and the third with the
correlation dimension. The entropy dimension quantifies the degree of
disorder present in a distribution. According to Andraud et al. (1994) and
Gouyet (1996), a <inline-formula><mml:math id="M83" display="inline"><mml:mrow><mml:mi mathvariant="italic">α</mml:mi><mml:mfenced close=")" open="("><mml:mn mathvariant="normal">1</mml:mn></mml:mfenced></mml:mrow></mml:math></inline-formula> value close to 2.0 characterizes a
system uniformly distributed throughout all scales, whereas a <inline-formula><mml:math id="M84" display="inline"><mml:mrow><mml:mi mathvariant="italic">α</mml:mi><mml:mfenced open="(" close=")"><mml:mn mathvariant="normal">1</mml:mn></mml:mfenced></mml:mrow></mml:math></inline-formula> close to 0 reflects a subset of the scale in which the
irregularities are concentrated. These three values will be shown from each
calculation of MFS.</p>
      <p>The width of the MF spectrum (<inline-formula><mml:math id="M85" display="inline"><mml:mrow><mml:mi mathvariant="normal">Δ</mml:mi><mml:mo>)</mml:mo></mml:mrow></mml:math></inline-formula> indicates overall variability
(Tarquis et al., 2001, 2014) and we have split it in two sections. Section I
correspond to values <inline-formula><mml:math id="M86" display="inline"><mml:mrow><mml:mi mathvariant="italic">α</mml:mi><mml:mo>(</mml:mo><mml:mi>q</mml:mi><mml:mo>)</mml:mo><mml:mo>&lt;</mml:mo><mml:mi mathvariant="italic">α</mml:mi><mml:mo>(</mml:mo><mml:mn mathvariant="normal">0</mml:mn><mml:mo>)</mml:mo></mml:mrow></mml:math></inline-formula> or <inline-formula><mml:math id="M87" display="inline"><mml:mrow><mml:mi>q</mml:mi><mml:mo>&gt;</mml:mo><mml:mn mathvariant="normal">0</mml:mn></mml:mrow></mml:math></inline-formula> and section II to
values with <inline-formula><mml:math id="M88" display="inline"><mml:mrow><mml:mi mathvariant="italic">α</mml:mi><mml:mo>(</mml:mo><mml:mi>q</mml:mi><mml:mo>)</mml:mo><mml:mo>&gt;</mml:mo><mml:mi mathvariant="italic">α</mml:mi><mml:mo>(</mml:mo><mml:mn mathvariant="normal">0</mml:mn><mml:mo>)</mml:mo></mml:mrow></mml:math></inline-formula> or <inline-formula><mml:math id="M89" display="inline"><mml:mrow><mml:mi>q</mml:mi><mml:mo>&lt;</mml:mo><mml:mn mathvariant="normal">0</mml:mn></mml:mrow></mml:math></inline-formula>. In section I the amplitude, or
semi-width, was calculated with differences <inline-formula><mml:math id="M90" display="inline"><mml:mrow><mml:msup><mml:mi mathvariant="normal">Δ</mml:mi><mml:mo>+</mml:mo></mml:msup><mml:mo>=</mml:mo><mml:mi mathvariant="italic">α</mml:mi><mml:mo>(</mml:mo><mml:mn mathvariant="normal">0</mml:mn><mml:mo>)</mml:mo><mml:mo>-</mml:mo><mml:mi mathvariant="italic">α</mml:mi><mml:mo>(</mml:mo><mml:mo>+</mml:mo><mml:mn mathvariant="normal">5</mml:mn><mml:mo>)</mml:mo></mml:mrow></mml:math></inline-formula>, and in section II with <inline-formula><mml:math id="M91" display="inline"><mml:mrow><mml:msup><mml:mi mathvariant="normal">Δ</mml:mi><mml:mo>-</mml:mo></mml:msup><mml:mo>=</mml:mo><mml:mi mathvariant="italic">α</mml:mi><mml:mo>(</mml:mo><mml:mo>-</mml:mo><mml:mn mathvariant="normal">5</mml:mn><mml:mo>)</mml:mo><mml:mo>-</mml:mo><mml:mi mathvariant="italic">α</mml:mi><mml:mo>(</mml:mo><mml:mn mathvariant="normal">0</mml:mn><mml:mo>)</mml:mo></mml:mrow></mml:math></inline-formula>.</p>
      <p>To study the asymmetry of the MFS we have chosen the
asymmetry index (AI) estimated as follows (Xie et al., 2010):
            <disp-formula id="Ch1.E10" content-type="numbered"><mml:math id="M92" display="block"><mml:mrow><mml:mi mathvariant="normal">AI</mml:mi><mml:mo>=</mml:mo><mml:mstyle displaystyle="true"><mml:mfrac style="display"><mml:mrow><mml:mi mathvariant="normal">Δ</mml:mi><mml:msub><mml:mi mathvariant="italic">α</mml:mi><mml:mi mathvariant="normal">L</mml:mi></mml:msub><mml:mo>-</mml:mo><mml:mi mathvariant="normal">Δ</mml:mi><mml:msub><mml:mi mathvariant="italic">α</mml:mi><mml:mi mathvariant="normal">R</mml:mi></mml:msub></mml:mrow><mml:mrow><mml:mi mathvariant="normal">Δ</mml:mi><mml:msub><mml:mi mathvariant="italic">α</mml:mi><mml:mi mathvariant="normal">L</mml:mi></mml:msub><mml:mo>+</mml:mo><mml:mi mathvariant="normal">Δ</mml:mi><mml:msub><mml:mi mathvariant="italic">α</mml:mi><mml:mi mathvariant="normal">R</mml:mi></mml:msub></mml:mrow></mml:mfrac></mml:mstyle><mml:mspace linebreak="nobreak" width="1em"/><mml:mtable class="array" columnalign="left"><mml:mtr><mml:mtd><mml:mrow><mml:mi mathvariant="normal">Δ</mml:mi><mml:msub><mml:mi mathvariant="italic">α</mml:mi><mml:mi mathvariant="normal">L</mml:mi></mml:msub><mml:mo>=</mml:mo><mml:msub><mml:mi mathvariant="italic">α</mml:mi><mml:mn mathvariant="normal">0</mml:mn></mml:msub><mml:mo>-</mml:mo><mml:msub><mml:mi mathvariant="italic">α</mml:mi><mml:mi mathvariant="normal">min</mml:mi></mml:msub></mml:mrow></mml:mtd></mml:mtr><mml:mtr><mml:mtd><mml:mrow><mml:mi mathvariant="normal">Δ</mml:mi><mml:msub><mml:mi mathvariant="italic">α</mml:mi><mml:mi mathvariant="normal">R</mml:mi></mml:msub><mml:mo>=</mml:mo><mml:msub><mml:mi mathvariant="italic">α</mml:mi><mml:mi mathvariant="normal">max</mml:mi></mml:msub><mml:mo>-</mml:mo><mml:msub><mml:mi mathvariant="italic">α</mml:mi><mml:mn mathvariant="normal">0</mml:mn></mml:msub></mml:mrow></mml:mtd></mml:mtr></mml:mtable><mml:mo>.</mml:mo></mml:mrow></mml:math></disp-formula>
          In our case, <inline-formula><mml:math id="M93" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="italic">α</mml:mi><mml:mn mathvariant="normal">0</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> is the singularity for <inline-formula><mml:math id="M94" display="inline"><mml:mrow><mml:mi>q</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">0</mml:mn></mml:mrow></mml:math></inline-formula> or <inline-formula><mml:math id="M95" display="inline"><mml:mrow><mml:mi mathvariant="italic">α</mml:mi><mml:mo>(</mml:mo><mml:mn mathvariant="normal">0</mml:mn><mml:mo>)</mml:mo></mml:mrow></mml:math></inline-formula>,
<inline-formula><mml:math id="M96" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="italic">α</mml:mi><mml:mi mathvariant="normal">min</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> is <inline-formula><mml:math id="M97" display="inline"><mml:mrow><mml:mi mathvariant="italic">α</mml:mi><mml:mo>(</mml:mo><mml:mo>+</mml:mo><mml:mn mathvariant="normal">5</mml:mn><mml:mo>)</mml:mo></mml:mrow></mml:math></inline-formula> and <inline-formula><mml:math id="M98" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="italic">α</mml:mi><mml:mi mathvariant="normal">max</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> is <inline-formula><mml:math id="M99" display="inline"><mml:mrow><mml:mi mathvariant="italic">α</mml:mi><mml:mo>(</mml:mo><mml:mo>-</mml:mo><mml:mn mathvariant="normal">5</mml:mn><mml:mo>)</mml:mo></mml:mrow></mml:math></inline-formula>.
Therefore, we can rewrite the AI as follows:
            <disp-formula id="Ch1.E11" content-type="numbered"><mml:math id="M100" display="block"><mml:mrow><mml:mi mathvariant="normal">AI</mml:mi><mml:mo>=</mml:mo><mml:mstyle displaystyle="true"><mml:mfrac style="display"><mml:mrow><mml:msup><mml:mi mathvariant="normal">Δ</mml:mi><mml:mo>+</mml:mo></mml:msup><mml:mo>-</mml:mo><mml:msup><mml:mi mathvariant="normal">Δ</mml:mi><mml:mo>-</mml:mo></mml:msup></mml:mrow><mml:mrow><mml:msup><mml:mi mathvariant="normal">Δ</mml:mi><mml:mo>+</mml:mo></mml:msup><mml:mo>+</mml:mo><mml:msup><mml:mi mathvariant="normal">Δ</mml:mi><mml:mo>-</mml:mo></mml:msup></mml:mrow></mml:mfrac></mml:mstyle><mml:mo>.</mml:mo></mml:mrow></mml:math></disp-formula>
          Expressing AI as Eq. (11), we can see that it is a normalized index
based on the amplitudes <inline-formula><mml:math id="M101" display="inline"><mml:mrow><mml:msup><mml:mi mathvariant="normal">Δ</mml:mi><mml:mo>+</mml:mo></mml:msup></mml:mrow></mml:math></inline-formula> and <inline-formula><mml:math id="M102" display="inline"><mml:mrow><mml:msup><mml:mi mathvariant="normal">Δ</mml:mi><mml:mo>-</mml:mo></mml:msup></mml:mrow></mml:math></inline-formula>.</p>
      <p>There are several works relating the UM model and the multi-fractal formalism
based on <inline-formula><mml:math id="M103" display="inline"><mml:mrow><mml:mi mathvariant="italic">τ</mml:mi><mml:mo>(</mml:mo><mml:mi>q</mml:mi><mml:mo>)</mml:mo></mml:mrow></mml:math></inline-formula> (Gagnon et al., 2003; Aguado et al., 2014; Morató et
al., 2017, among others) through the following equations:

                <disp-formula specific-use="align" content-type="numbered"><mml:math id="M104" display="block"><mml:mtable displaystyle="true"><mml:mlabeledtr id="Ch1.E12"><mml:mtd/><mml:mtd><mml:mstyle displaystyle="true" class="stylechange"/></mml:mtd><mml:mtd><mml:mrow><mml:mstyle displaystyle="true" class="stylechange"/><mml:mi>f</mml:mi><mml:mfenced open="(" close=")"><mml:mi mathvariant="italic">α</mml:mi></mml:mfenced><mml:mo>=</mml:mo><mml:mi>E</mml:mi><mml:mo>-</mml:mo><mml:mi>c</mml:mi><mml:mfenced open="(" close=")"><mml:mi mathvariant="italic">γ</mml:mi></mml:mfenced><mml:mo>;</mml:mo><mml:mspace linebreak="nobreak" width="0.125em"/><mml:mi mathvariant="italic">α</mml:mi><mml:mo>=</mml:mo><mml:mi>E</mml:mi><mml:mo>-</mml:mo><mml:mi mathvariant="italic">γ</mml:mi><mml:mo>,</mml:mo></mml:mrow></mml:mtd></mml:mlabeledtr><mml:mlabeledtr id="Ch1.E13"><mml:mtd/><mml:mtd><mml:mstyle displaystyle="true" class="stylechange"/></mml:mtd><mml:mtd><mml:mrow><mml:mstyle displaystyle="true" class="stylechange"/><mml:mi mathvariant="italic">τ</mml:mi><mml:mfenced close=")" open="("><mml:mi>q</mml:mi></mml:mfenced><mml:mo>=</mml:mo><mml:mi>E</mml:mi><mml:mfenced open="(" close=")"><mml:mi>q</mml:mi><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mfenced><mml:mo>-</mml:mo><mml:mi>K</mml:mi><mml:mfenced close=")" open="("><mml:mi>q</mml:mi></mml:mfenced><mml:mo>,</mml:mo></mml:mrow></mml:mtd></mml:mlabeledtr></mml:mtable></mml:math></disp-formula>

            where <inline-formula><mml:math id="M105" display="inline"><mml:mi>E</mml:mi></mml:math></inline-formula> is the Euclidean dimension in which the measure is embedded, in this
case <inline-formula><mml:math id="M106" display="inline"><mml:mrow><mml:mi>E</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">2</mml:mn></mml:mrow></mml:math></inline-formula>, and <inline-formula><mml:math id="M107" display="inline"><mml:mrow><mml:mi>c</mml:mi><mml:mo>(</mml:mo><mml:mi mathvariant="italic">γ</mml:mi><mml:mo>)</mml:mo></mml:mrow></mml:math></inline-formula> is the codimension of the singularity of the
density of the multi-fractal measure <inline-formula><mml:math id="M108" display="inline"><mml:mi mathvariant="italic">γ</mml:mi></mml:math></inline-formula>.</p>
</sec>
</sec>
<sec id="Ch1.S3">
  <title>Results and discussion</title>
<sec id="Ch1.S3.SS1">
  <title>Radiometric influence in the multi-fractal spectrum</title>
      <p>To study the influence of radiometric resolution on Ikonos-2 image
information complexity, the original pixel code (11 bits) has been
transformed to 8 bits through a rescaling based on minimum and maximum values between 0
and 255, with the aim of preserving the initial histogram shape.</p>
      <p>We first discuss the results obtained for the <inline-formula><mml:math id="M109" display="inline"><mml:mrow><mml:mn mathvariant="normal">2048</mml:mn><mml:mo>×</mml:mo><mml:mn mathvariant="normal">2048</mml:mn></mml:mrow></mml:math></inline-formula> pixel Ikonos-2
image shown in Fig. 1, in bands combination of false colour (IK#4,
IK#3, IK#2 band combination in RGB visualization). In Fig. 2 IK#1,
IK#2, IK#3 and IK#4 band histograms are shown. In the right column
are histograms with the original radiometric resolution and in the left
column the corresponding histograms are rescaled to 8 bits. The histograms
present a bimodal structure with a narrow peak of low-value pixels (dark
grey) showing a sharp maximum and a wider peak around a second lower
maximum. For bands IK#1, IK#2 and IK#3, the narrow peak maximum
corresponds to vegetation, mainly irrigation crops, showing strong water
absorption. This effect is particularly important in band IK#3. High-value pixels (lighter grey) correspond to ground zones with lower vegetation
content. However, as vegetation shows high reflectivity in the near-infrared, IK#4 band histogram shows a predominance of high-value pixels
(lighter grey pixels) corresponding to dense vegetation parts. For both
radiometric resolutions the shapes of the histograms are very similar, as it
was our intention (see Fig. 2).</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F1"><caption><p>The Ikonos-2 image in band combinations of false colour (IK#4,
IK#3 and IK#2 in RGB). The image has a size of <inline-formula><mml:math id="M110" display="inline"><mml:mrow><mml:mn mathvariant="normal">2048</mml:mn><mml:mo>×</mml:mo><mml:mn mathvariant="normal">2048</mml:mn></mml:mrow></mml:math></inline-formula> pixels,
each area unit corresponding to <inline-formula><mml:math id="M111" display="inline"><mml:mrow><mml:mn mathvariant="normal">4</mml:mn><mml:mo>×</mml:mo><mml:mn mathvariant="normal">4</mml:mn></mml:mrow></mml:math></inline-formula> m. The coordinates UTM (zone 30) of the
upper left and lower right pixel in the image are: ULX <inline-formula><mml:math id="M112" display="inline"><mml:mo>=</mml:mo></mml:math></inline-formula> 446 037 m, ULY <inline-formula><mml:math id="M113" display="inline"><mml:mo>=</mml:mo></mml:math></inline-formula>
4 441 684 m, LRX <inline-formula><mml:math id="M114" display="inline"><mml:mo>=</mml:mo></mml:math></inline-formula> 454 229 m and LRY <inline-formula><mml:math id="M115" display="inline"><mml:mo>=</mml:mo></mml:math></inline-formula> 4 433 492 m.</p></caption>
          <?xmltex \igopts{width=236.157874pt}?><graphic xlink:href="https://npg.copernicus.org/articles/24/141/2017/npg-24-141-2017-f01.jpg"/>

        </fig>

      <p>We cover the image with boxes of size <inline-formula><mml:math id="M116" display="inline"><mml:mrow><mml:mi mathvariant="italic">δ</mml:mi><mml:mo>=</mml:mo><mml:msup><mml:mn mathvariant="normal">2</mml:mn><mml:mrow><mml:mo>-</mml:mo><mml:mi>n</mml:mi></mml:mrow></mml:msup></mml:mrow></mml:math></inline-formula> and we change the box
size from 2048 to 2 pixels, that is, <inline-formula><mml:math id="M117" display="inline"><mml:mrow><mml:mi mathvariant="italic">δ</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">2048</mml:mn><mml:mo>/</mml:mo><mml:msup><mml:mn mathvariant="normal">2</mml:mn><mml:mi>n</mml:mi></mml:msup></mml:mrow></mml:math></inline-formula> with <inline-formula><mml:math id="M118" display="inline"><mml:mrow><mml:mi>n</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">0</mml:mn></mml:mrow></mml:math></inline-formula>, 1, 2, …, 10. For each
value of the parameter <inline-formula><mml:math id="M119" display="inline"><mml:mi>q</mml:mi></mml:math></inline-formula>, from <inline-formula><mml:math id="M120" display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>5 to <inline-formula><mml:math id="M121" display="inline"><mml:mo>+</mml:mo></mml:math></inline-formula>5 with increments of 0.5, the
partition function (Eq. 6) is computed and log <inline-formula><mml:math id="M122" display="inline"><mml:mrow><mml:mi mathvariant="italic">χ</mml:mi><mml:mo>(</mml:mo><mml:mi>q</mml:mi><mml:mo>,</mml:mo><mml:mi mathvariant="italic">δ</mml:mi><mml:mo>)</mml:mo></mml:mrow></mml:math></inline-formula> versus
<inline-formula><mml:math id="M123" display="inline"><mml:mrow><mml:mi>log⁡</mml:mi><mml:mi mathvariant="italic">δ</mml:mi></mml:mrow></mml:math></inline-formula> is plotted in Fig. 3. Each graph contains 11 points and from
these a range of scales are selected for the least-square linear fit
reaching the maximum possible scales and with a standard error in the slope,
the estimated values of <inline-formula><mml:math id="M124" display="inline"><mml:mrow><mml:mi mathvariant="italic">τ</mml:mi><mml:mo>(</mml:mo><mml:mi>q</mml:mi><mml:mo>)</mml:mo></mml:mrow></mml:math></inline-formula>, less than 0.01. Then, using Eqs. (7)–(8),
<inline-formula><mml:math id="M125" display="inline"><mml:mrow><mml:mi mathvariant="italic">α</mml:mi><mml:mo>(</mml:mo><mml:mi>q</mml:mi><mml:mo>)</mml:mo></mml:mrow></mml:math></inline-formula> and <inline-formula><mml:math id="M126" display="inline"><mml:mrow><mml:mi>f</mml:mi><mml:mo>(</mml:mo><mml:mi mathvariant="italic">α</mml:mi><mml:mo>)</mml:mo></mml:mrow></mml:math></inline-formula> are obtained. Comparing the range of
scales used in both radiometric resolutions, the bands using the original
data (11 bits) showed a wider range of scales for the linear fit, up to 4
pixels, whereas in the 8-bit radiometric resolution were required up to 32
pixels (see arrows in Fig. 3).</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F2" specific-use="star"><caption><p>Histograms of the four bands of the Ikonos-2 image for the original
radiometric resolution, 11 bits (right), and the minimum–maximum rescaled 8-bit radiometric resolution (left).</p></caption>
          <?xmltex \igopts{width=426.791339pt}?><graphic xlink:href="https://npg.copernicus.org/articles/24/141/2017/npg-24-141-2017-f02.jpg"/>

        </fig>

<?xmltex \floatpos{t}?><table-wrap id="Ch1.T1" specific-use="star"><caption><p>Parameters obtained from the multi-fractal spectrum from each band
of the Ikonos-2 image, and the vegetation indexes (VIs) estimated, with a pixel
size of 4 m and a radiometric resolution of 11 bits. The amplitudes of
<inline-formula><mml:math id="M127" display="inline"><mml:mi mathvariant="italic">α</mml:mi></mml:math></inline-formula> values are presented as <inline-formula><mml:math id="M128" display="inline"><mml:mrow><mml:msup><mml:mi mathvariant="normal">Δ</mml:mi><mml:mo>+</mml:mo></mml:msup></mml:mrow></mml:math></inline-formula> and <inline-formula><mml:math id="M129" display="inline"><mml:mrow><mml:msup><mml:mi mathvariant="normal">Δ</mml:mi><mml:mo>-</mml:mo></mml:msup></mml:mrow></mml:math></inline-formula>
corresponding to <inline-formula><mml:math id="M130" display="inline"><mml:mrow><mml:mi mathvariant="italic">α</mml:mi><mml:mo>(</mml:mo><mml:mn mathvariant="normal">0</mml:mn><mml:mo>)</mml:mo><mml:mo>-</mml:mo><mml:mi mathvariant="italic">α</mml:mi><mml:mo>(</mml:mo><mml:mn mathvariant="normal">5</mml:mn><mml:mo>)</mml:mo></mml:mrow></mml:math></inline-formula> and <inline-formula><mml:math id="M131" display="inline"><mml:mrow><mml:mi mathvariant="italic">α</mml:mi><mml:mo>(</mml:mo><mml:mo>-</mml:mo><mml:mn mathvariant="normal">5</mml:mn><mml:mo>)</mml:mo><mml:mo>-</mml:mo><mml:mi mathvariant="italic">α</mml:mi><mml:mo>(</mml:mo><mml:mn mathvariant="normal">0</mml:mn><mml:mo>)</mml:mo></mml:mrow></mml:math></inline-formula>
respectively. The asymmetry index (AI) corresponds to
<inline-formula><mml:math id="M132" display="inline"><mml:mstyle displaystyle="false"><mml:mfrac style="text"><mml:mrow><mml:msup><mml:mi mathvariant="normal">Δ</mml:mi><mml:mo>+</mml:mo></mml:msup><mml:mo>-</mml:mo><mml:msup><mml:mi mathvariant="normal">Δ</mml:mi><mml:mo>-</mml:mo></mml:msup></mml:mrow><mml:mrow><mml:msup><mml:mi mathvariant="normal">Δ</mml:mi><mml:mo>+</mml:mo></mml:msup><mml:mo>+</mml:mo><mml:msup><mml:mi mathvariant="normal">Δ</mml:mi><mml:mo>-</mml:mo></mml:msup></mml:mrow></mml:mfrac></mml:mstyle></mml:math></inline-formula>.</p></caption><oasis:table frame="topbot"><oasis:tgroup cols="7">
     <oasis:colspec colnum="1" colname="col1" align="left"/>
     <oasis:colspec colnum="2" colname="col2" align="left"/>
     <oasis:colspec colnum="3" colname="col3" align="right"/>
     <oasis:colspec colnum="4" colname="col4" align="right"/>
     <oasis:colspec colnum="5" colname="col5" align="right"/>
     <oasis:colspec colnum="6" colname="col6" align="right"/>
     <oasis:colspec colnum="7" colname="col7" align="right"/>
     <oasis:thead>
       <oasis:row rowsep="1">

         <oasis:entry colname="col1"/>

         <oasis:entry colname="col2">Band</oasis:entry>

         <oasis:entry colname="col3"><inline-formula><mml:math id="M133" display="inline"><mml:mi>q</mml:mi></mml:math></inline-formula></oasis:entry>

         <oasis:entry colname="col4"><inline-formula><mml:math id="M134" display="inline"><mml:mrow><mml:mi mathvariant="italic">α</mml:mi><mml:mo>(</mml:mo><mml:mi>q</mml:mi><mml:mo>)</mml:mo></mml:mrow></mml:math></inline-formula></oasis:entry>

         <oasis:entry colname="col5"><inline-formula><mml:math id="M135" display="inline"><mml:mrow><mml:msup><mml:mi mathvariant="normal">Δ</mml:mi><mml:mo>+</mml:mo></mml:msup></mml:mrow></mml:math></inline-formula></oasis:entry>

         <oasis:entry colname="col6"><inline-formula><mml:math id="M136" display="inline"><mml:mrow><mml:msup><mml:mi mathvariant="normal">Δ</mml:mi><mml:mo>-</mml:mo></mml:msup></mml:mrow></mml:math></inline-formula></oasis:entry>

         <oasis:entry colname="col7">AI</oasis:entry>

       </oasis:row>
     </oasis:thead>
     <oasis:tbody>
       <oasis:row>

         <oasis:entry rowsep="1" colname="col1" morerows="11">Ikonos-2 (11 bits)</oasis:entry>

         <oasis:entry rowsep="1" colname="col2" morerows="2">IK#1</oasis:entry>

         <oasis:entry colname="col3">0</oasis:entry>

         <oasis:entry colname="col4">2.001 <inline-formula><mml:math id="M137" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> 0.001</oasis:entry>

         <oasis:entry rowsep="1" colname="col5" morerows="2">0.418</oasis:entry>

         <oasis:entry rowsep="1" colname="col6" morerows="2">0.256</oasis:entry>

         <oasis:entry rowsep="1" colname="col7" morerows="2">0.240</oasis:entry>

       </oasis:row>
       <oasis:row>

         <oasis:entry colname="col3">1</oasis:entry>

         <oasis:entry colname="col4">1.938 <inline-formula><mml:math id="M138" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> 0.005</oasis:entry>

       </oasis:row>
       <oasis:row rowsep="1">

         <oasis:entry colname="col3">2</oasis:entry>

         <oasis:entry colname="col4">1.865 <inline-formula><mml:math id="M139" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> 0.009</oasis:entry>

       </oasis:row>
       <oasis:row>

         <oasis:entry rowsep="1" colname="col2" morerows="2">IK#2</oasis:entry>

         <oasis:entry colname="col3">0</oasis:entry>

         <oasis:entry colname="col4">2.001 <inline-formula><mml:math id="M140" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> 0.001</oasis:entry>

         <oasis:entry rowsep="1" colname="col5" morerows="2">0.377</oasis:entry>

         <oasis:entry rowsep="1" colname="col6" morerows="2">0.313</oasis:entry>

         <oasis:entry rowsep="1" colname="col7" morerows="2">0.093</oasis:entry>

       </oasis:row>
       <oasis:row>

         <oasis:entry colname="col3">1</oasis:entry>

         <oasis:entry colname="col4">1.936 <inline-formula><mml:math id="M141" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> 0.005</oasis:entry>

       </oasis:row>
       <oasis:row rowsep="1">

         <oasis:entry colname="col3">2</oasis:entry>

         <oasis:entry colname="col4">1.871 <inline-formula><mml:math id="M142" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> 0.007</oasis:entry>

       </oasis:row>
       <oasis:row>

         <oasis:entry rowsep="1" colname="col2" morerows="2">IK#3</oasis:entry>

         <oasis:entry colname="col3">0</oasis:entry>

         <oasis:entry colname="col4">2.001 <inline-formula><mml:math id="M143" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> 0.001</oasis:entry>

         <oasis:entry rowsep="1" colname="col5" morerows="2">0.348</oasis:entry>

         <oasis:entry rowsep="1" colname="col6" morerows="2">0.382</oasis:entry>

         <oasis:entry rowsep="1" colname="col7" morerows="2"><inline-formula><mml:math id="M144" display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>0.047</oasis:entry>

       </oasis:row>
       <oasis:row>

         <oasis:entry colname="col3">1</oasis:entry>

         <oasis:entry colname="col4">1.937 <inline-formula><mml:math id="M145" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> 0.005</oasis:entry>

       </oasis:row>
       <oasis:row rowsep="1">

         <oasis:entry colname="col3">2</oasis:entry>

         <oasis:entry colname="col4">1.878 <inline-formula><mml:math id="M146" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> 0.006</oasis:entry>

       </oasis:row>
       <oasis:row>

         <oasis:entry rowsep="1" colname="col2" morerows="2">IK#4</oasis:entry>

         <oasis:entry colname="col3">0</oasis:entry>

         <oasis:entry colname="col4">2.001 <inline-formula><mml:math id="M147" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> 0.001</oasis:entry>

         <oasis:entry rowsep="1" colname="col5" morerows="2">0.290</oasis:entry>

         <oasis:entry rowsep="1" colname="col6" morerows="2">0.470</oasis:entry>

         <oasis:entry rowsep="1" colname="col7" morerows="2"><inline-formula><mml:math id="M148" display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>0.237</oasis:entry>

       </oasis:row>
       <oasis:row>

         <oasis:entry colname="col3">1</oasis:entry>

         <oasis:entry colname="col4">1.959 <inline-formula><mml:math id="M149" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> 0.005</oasis:entry>

       </oasis:row>
       <oasis:row rowsep="1">

         <oasis:entry colname="col3">2</oasis:entry>

         <oasis:entry colname="col4">1.908 <inline-formula><mml:math id="M150" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> 0.009</oasis:entry>

       </oasis:row>
       <oasis:row rowsep="1">

         <oasis:entry colname="col1"/>

         <oasis:entry colname="col2">VI</oasis:entry>

         <oasis:entry colname="col3"><inline-formula><mml:math id="M151" display="inline"><mml:mi>q</mml:mi></mml:math></inline-formula></oasis:entry>

         <oasis:entry colname="col4"><inline-formula><mml:math id="M152" display="inline"><mml:mrow><mml:mi mathvariant="italic">α</mml:mi><mml:mo>(</mml:mo><mml:mi>q</mml:mi><mml:mo>)</mml:mo></mml:mrow></mml:math></inline-formula></oasis:entry>

         <oasis:entry colname="col5"><inline-formula><mml:math id="M153" display="inline"><mml:mrow><mml:msup><mml:mi mathvariant="normal">Δ</mml:mi><mml:mo>+</mml:mo></mml:msup></mml:mrow></mml:math></inline-formula></oasis:entry>

         <oasis:entry colname="col6"><inline-formula><mml:math id="M154" display="inline"><mml:mrow><mml:msup><mml:mi mathvariant="normal">Δ</mml:mi><mml:mo>-</mml:mo></mml:msup></mml:mrow></mml:math></inline-formula></oasis:entry>

         <oasis:entry colname="col7">AI</oasis:entry>

       </oasis:row>
       <oasis:row>

         <oasis:entry colname="col1" morerows="5">Ikonos-2 (11 bits)</oasis:entry>

         <oasis:entry rowsep="1" colname="col2" morerows="2">NDVI</oasis:entry>

         <oasis:entry colname="col3">0</oasis:entry>

         <oasis:entry colname="col4">2.000 <inline-formula><mml:math id="M155" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> 0.001</oasis:entry>

         <oasis:entry rowsep="1" colname="col5" morerows="2">0.516</oasis:entry>

         <oasis:entry rowsep="1" colname="col6" morerows="2">1.166</oasis:entry>

         <oasis:entry rowsep="1" colname="col7" morerows="2"><inline-formula><mml:math id="M156" display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>0.386</oasis:entry>

       </oasis:row>
       <oasis:row>

         <oasis:entry colname="col3">1</oasis:entry>

         <oasis:entry colname="col4">1.886 <inline-formula><mml:math id="M157" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> 0.008</oasis:entry>

       </oasis:row>
       <oasis:row rowsep="1">

         <oasis:entry colname="col3">2</oasis:entry>

         <oasis:entry colname="col4">1.779 <inline-formula><mml:math id="M158" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> 0.010</oasis:entry>

       </oasis:row>
       <oasis:row>

         <oasis:entry colname="col2" morerows="2">EVI</oasis:entry>

         <oasis:entry colname="col3">0</oasis:entry>

         <oasis:entry colname="col4">2.000 <inline-formula><mml:math id="M159" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> 0.001</oasis:entry>

         <oasis:entry colname="col5" morerows="2">0.270</oasis:entry>

         <oasis:entry colname="col6" morerows="2">0.877</oasis:entry>

         <oasis:entry colname="col7" morerows="2"><inline-formula><mml:math id="M160" display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>0.533</oasis:entry>

       </oasis:row>
       <oasis:row>

         <oasis:entry colname="col3">1</oasis:entry>

         <oasis:entry colname="col4">1.948 <inline-formula><mml:math id="M161" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> 0.002</oasis:entry>

       </oasis:row>
       <oasis:row>

         <oasis:entry colname="col3">2</oasis:entry>

         <oasis:entry colname="col4">1.897 <inline-formula><mml:math id="M162" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> 0.004</oasis:entry>

       </oasis:row>
     </oasis:tbody>
   </oasis:tgroup></oasis:table></table-wrap>

      <p>The MF spectra <inline-formula><mml:math id="M163" display="inline"><mml:mrow><mml:mi>f</mml:mi><mml:mo>(</mml:mo><mml:mi mathvariant="italic">α</mml:mi><mml:mo>)</mml:mo></mml:mrow></mml:math></inline-formula> corresponding to the four bands of multi-spectral
Ikonos images are shown in Fig. 4. These differences found in the
multi-scaling behaviour of each band are in agreement with previous works
(Cheng, 2004; Lovejoy et al., 2008). Just by visual observation, there is a remarkable difference between the bands #3 and #4, and red and
NIR, between 8 and 11 bits respectively. Higher radiometric resolution gives a
higher range of possible grey values per pixel. Note that this radiometric
resolution effect is manifested in both sections of the MF spectra (for
<inline-formula><mml:math id="M164" display="inline"><mml:mrow><mml:mi>q</mml:mi><mml:mo>&gt;</mml:mo><mml:mn mathvariant="normal">0</mml:mn></mml:mrow></mml:math></inline-formula> and for <inline-formula><mml:math id="M165" display="inline"><mml:mrow><mml:mi>q</mml:mi><mml:mo>&lt;</mml:mo><mml:mn mathvariant="normal">0</mml:mn><mml:mo>)</mml:mo></mml:mrow></mml:math></inline-formula>.</p>

<?xmltex \floatpos{t}?><table-wrap id="Ch1.T2" specific-use="star"><caption><p>Parameters obtained from the multi-fractal spectrum from each band
of the Ikonos-2 image, and the vegetation indexes (VIs) estimated, with a pixel
size of 4 m and a radiometric resolution of 8 bits. The amplitudes of
<inline-formula><mml:math id="M166" display="inline"><mml:mi mathvariant="italic">α</mml:mi></mml:math></inline-formula> values are presented as <inline-formula><mml:math id="M167" display="inline"><mml:mrow><mml:msup><mml:mi mathvariant="normal">Δ</mml:mi><mml:mo>+</mml:mo></mml:msup></mml:mrow></mml:math></inline-formula> and <inline-formula><mml:math id="M168" display="inline"><mml:mrow><mml:msup><mml:mi mathvariant="normal">Δ</mml:mi><mml:mo>-</mml:mo></mml:msup></mml:mrow></mml:math></inline-formula>
corresponding to <inline-formula><mml:math id="M169" display="inline"><mml:mrow><mml:mi mathvariant="italic">α</mml:mi><mml:mo>(</mml:mo><mml:mn mathvariant="normal">0</mml:mn><mml:mo>)</mml:mo><mml:mo>-</mml:mo><mml:mi mathvariant="italic">α</mml:mi><mml:mo>(</mml:mo><mml:mn mathvariant="normal">5</mml:mn><mml:mo>)</mml:mo></mml:mrow></mml:math></inline-formula> and <inline-formula><mml:math id="M170" display="inline"><mml:mrow><mml:mi mathvariant="italic">α</mml:mi><mml:mo>(</mml:mo><mml:mo>-</mml:mo><mml:mn mathvariant="normal">5</mml:mn><mml:mo>)</mml:mo><mml:mo>-</mml:mo><mml:mi mathvariant="italic">α</mml:mi><mml:mo>(</mml:mo><mml:mn mathvariant="normal">0</mml:mn><mml:mo>)</mml:mo></mml:mrow></mml:math></inline-formula>
respectively. The asymmetry index (AI) corresponds to
<inline-formula><mml:math id="M171" display="inline"><mml:mstyle displaystyle="false"><mml:mfrac style="text"><mml:mrow><mml:msup><mml:mi mathvariant="normal">Δ</mml:mi><mml:mo>+</mml:mo></mml:msup><mml:mo>-</mml:mo><mml:msup><mml:mi mathvariant="normal">Δ</mml:mi><mml:mo>-</mml:mo></mml:msup></mml:mrow><mml:mrow><mml:msup><mml:mi mathvariant="normal">Δ</mml:mi><mml:mo>+</mml:mo></mml:msup><mml:mo>+</mml:mo><mml:msup><mml:mi mathvariant="normal">Δ</mml:mi><mml:mo>-</mml:mo></mml:msup></mml:mrow></mml:mfrac></mml:mstyle></mml:math></inline-formula>.</p></caption><oasis:table frame="topbot"><oasis:tgroup cols="7">
     <oasis:colspec colnum="1" colname="col1" align="left"/>
     <oasis:colspec colnum="2" colname="col2" align="left"/>
     <oasis:colspec colnum="3" colname="col3" align="right"/>
     <oasis:colspec colnum="4" colname="col4" align="right"/>
     <oasis:colspec colnum="5" colname="col5" align="right"/>
     <oasis:colspec colnum="6" colname="col6" align="right"/>
     <oasis:colspec colnum="7" colname="col7" align="right"/>
     <oasis:thead>
       <oasis:row rowsep="1">

         <oasis:entry colname="col1"/>

         <oasis:entry colname="col2">Band</oasis:entry>

         <oasis:entry colname="col3"><inline-formula><mml:math id="M172" display="inline"><mml:mi>q</mml:mi></mml:math></inline-formula></oasis:entry>

         <oasis:entry colname="col4"><inline-formula><mml:math id="M173" display="inline"><mml:mrow><mml:mi mathvariant="italic">α</mml:mi><mml:mo>(</mml:mo><mml:mi>q</mml:mi><mml:mo>)</mml:mo></mml:mrow></mml:math></inline-formula></oasis:entry>

         <oasis:entry colname="col5"><inline-formula><mml:math id="M174" display="inline"><mml:mrow><mml:msup><mml:mi mathvariant="normal">Δ</mml:mi><mml:mo>+</mml:mo></mml:msup></mml:mrow></mml:math></inline-formula></oasis:entry>

         <oasis:entry colname="col6"><inline-formula><mml:math id="M175" display="inline"><mml:mrow><mml:msup><mml:mi mathvariant="normal">Δ</mml:mi><mml:mo>-</mml:mo></mml:msup></mml:mrow></mml:math></inline-formula></oasis:entry>

         <oasis:entry colname="col7">AI</oasis:entry>

       </oasis:row>
     </oasis:thead>
     <oasis:tbody>
       <oasis:row>

         <oasis:entry rowsep="1" colname="col1" morerows="11">Ikonos-2 (8 bits)</oasis:entry>

         <oasis:entry rowsep="1" colname="col2" morerows="2">IK#1</oasis:entry>

         <oasis:entry colname="col3">0</oasis:entry>

         <oasis:entry colname="col4">2.000 <inline-formula><mml:math id="M176" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> 0.001</oasis:entry>

         <oasis:entry rowsep="1" colname="col5" morerows="2">0.231</oasis:entry>

         <oasis:entry rowsep="1" colname="col6" morerows="2">0.192</oasis:entry>

         <oasis:entry rowsep="1" colname="col7" morerows="2">0.092</oasis:entry>

       </oasis:row>
       <oasis:row>

         <oasis:entry colname="col3">1</oasis:entry>

         <oasis:entry colname="col4">1.971 <inline-formula><mml:math id="M177" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> 0.003</oasis:entry>

       </oasis:row>
       <oasis:row rowsep="1">

         <oasis:entry colname="col3">2</oasis:entry>

         <oasis:entry colname="col4">1.930 <inline-formula><mml:math id="M178" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> 0.006</oasis:entry>

       </oasis:row>
       <oasis:row>

         <oasis:entry rowsep="1" colname="col2" morerows="2">IK#2</oasis:entry>

         <oasis:entry colname="col3">0</oasis:entry>

         <oasis:entry colname="col4">2.000 <inline-formula><mml:math id="M179" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> 0.001</oasis:entry>

         <oasis:entry rowsep="1" colname="col5" morerows="2">0.270</oasis:entry>

         <oasis:entry rowsep="1" colname="col6" morerows="2">0.287</oasis:entry>

         <oasis:entry rowsep="1" colname="col7" morerows="2"><inline-formula><mml:math id="M180" display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>0.031</oasis:entry>

       </oasis:row>
       <oasis:row>

         <oasis:entry colname="col3">1</oasis:entry>

         <oasis:entry colname="col4">1.963 <inline-formula><mml:math id="M181" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> 0.004</oasis:entry>

       </oasis:row>
       <oasis:row rowsep="1">

         <oasis:entry colname="col3">2</oasis:entry>

         <oasis:entry colname="col4">1.914 <inline-formula><mml:math id="M182" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> 0.006</oasis:entry>

       </oasis:row>
       <oasis:row>

         <oasis:entry rowsep="1" colname="col2" morerows="2">IK#3</oasis:entry>

         <oasis:entry colname="col3">0</oasis:entry>

         <oasis:entry colname="col4">2.000 <inline-formula><mml:math id="M183" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> 0.001</oasis:entry>

         <oasis:entry rowsep="1" colname="col5" morerows="2">0.323</oasis:entry>

         <oasis:entry rowsep="1" colname="col6" morerows="2">0.614</oasis:entry>

         <oasis:entry rowsep="1" colname="col7" morerows="2"><inline-formula><mml:math id="M184" display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>0.311</oasis:entry>

       </oasis:row>
       <oasis:row>

         <oasis:entry colname="col3">1</oasis:entry>

         <oasis:entry colname="col4">1.945 <inline-formula><mml:math id="M185" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> 0.005</oasis:entry>

       </oasis:row>
       <oasis:row rowsep="1">

         <oasis:entry colname="col3">2</oasis:entry>

         <oasis:entry colname="col4">1.887 <inline-formula><mml:math id="M186" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> 0.006</oasis:entry>

       </oasis:row>
       <oasis:row>

         <oasis:entry rowsep="1" colname="col2" morerows="2">IK#4</oasis:entry>

         <oasis:entry colname="col3">0</oasis:entry>

         <oasis:entry colname="col4">2.000 <inline-formula><mml:math id="M187" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> 0.001</oasis:entry>

         <oasis:entry rowsep="1" colname="col5" morerows="2">0.248</oasis:entry>

         <oasis:entry rowsep="1" colname="col6" morerows="2">0.512</oasis:entry>

         <oasis:entry rowsep="1" colname="col7" morerows="2"><inline-formula><mml:math id="M188" display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>0.347</oasis:entry>

       </oasis:row>
       <oasis:row>

         <oasis:entry colname="col3">1</oasis:entry>

         <oasis:entry colname="col4">1.966 <inline-formula><mml:math id="M189" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> 0.004</oasis:entry>

       </oasis:row>
       <oasis:row rowsep="1">

         <oasis:entry colname="col3">2</oasis:entry>

         <oasis:entry colname="col4">1.923 <inline-formula><mml:math id="M190" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> 0.008</oasis:entry>

       </oasis:row>
       <oasis:row rowsep="1">

         <oasis:entry colname="col1"/>

         <oasis:entry colname="col2">VI</oasis:entry>

         <oasis:entry colname="col3"><inline-formula><mml:math id="M191" display="inline"><mml:mi>q</mml:mi></mml:math></inline-formula></oasis:entry>

         <oasis:entry colname="col4"><inline-formula><mml:math id="M192" display="inline"><mml:mrow><mml:mi mathvariant="italic">α</mml:mi><mml:mo>(</mml:mo><mml:mi>q</mml:mi><mml:mo>)</mml:mo></mml:mrow></mml:math></inline-formula></oasis:entry>

         <oasis:entry colname="col5"><inline-formula><mml:math id="M193" display="inline"><mml:mrow><mml:msup><mml:mi mathvariant="normal">Δ</mml:mi><mml:mo>+</mml:mo></mml:msup></mml:mrow></mml:math></inline-formula></oasis:entry>

         <oasis:entry colname="col6"><inline-formula><mml:math id="M194" display="inline"><mml:mrow><mml:msup><mml:mi mathvariant="normal">Δ</mml:mi><mml:mo>-</mml:mo></mml:msup></mml:mrow></mml:math></inline-formula></oasis:entry>

         <oasis:entry colname="col7">AI</oasis:entry>

       </oasis:row>
       <oasis:row>

         <oasis:entry colname="col1" morerows="5">Ikonos-2 (8 bits)</oasis:entry>

         <oasis:entry rowsep="1" colname="col2" morerows="2">NDVI</oasis:entry>

         <oasis:entry colname="col3">0</oasis:entry>

         <oasis:entry colname="col4">2.000 <inline-formula><mml:math id="M195" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> 0.002</oasis:entry>

         <oasis:entry rowsep="1" colname="col5" morerows="2">0.337</oasis:entry>

         <oasis:entry rowsep="1" colname="col6" morerows="2">0.984</oasis:entry>

         <oasis:entry rowsep="1" colname="col7" morerows="2"><inline-formula><mml:math id="M196" display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>0.490</oasis:entry>

       </oasis:row>
       <oasis:row>

         <oasis:entry colname="col3">1</oasis:entry>

         <oasis:entry colname="col4">1.932 <inline-formula><mml:math id="M197" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> 0.005</oasis:entry>

       </oasis:row>
       <oasis:row rowsep="1">

         <oasis:entry colname="col3">2</oasis:entry>

         <oasis:entry colname="col4">1.855 <inline-formula><mml:math id="M198" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> 0.008</oasis:entry>

       </oasis:row>
       <oasis:row>

         <oasis:entry colname="col2" morerows="2">EVI</oasis:entry>

         <oasis:entry colname="col3">0</oasis:entry>

         <oasis:entry colname="col4">2.000 <inline-formula><mml:math id="M199" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> 0.002</oasis:entry>

         <oasis:entry colname="col5" morerows="2">0.300</oasis:entry>

         <oasis:entry colname="col6" morerows="2">0.874</oasis:entry>

         <oasis:entry colname="col7" morerows="2"><inline-formula><mml:math id="M200" display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>0.488</oasis:entry>

       </oasis:row>
       <oasis:row>

         <oasis:entry colname="col3">1</oasis:entry>

         <oasis:entry colname="col4">1.940 <inline-formula><mml:math id="M201" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> 0.004</oasis:entry>

       </oasis:row>
       <oasis:row>

         <oasis:entry colname="col3">2</oasis:entry>

         <oasis:entry colname="col4">1.873 <inline-formula><mml:math id="M202" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> 0.006</oasis:entry>

       </oasis:row>
     </oasis:tbody>
   </oasis:tgroup></oasis:table></table-wrap>

      <?xmltex \floatpos{t}?><fig id="Ch1.F3" specific-use="star"><caption><p>Bi-log plots of the partition function <inline-formula><mml:math id="M203" display="inline"><mml:mrow><mml:mi mathvariant="italic">χ</mml:mi><mml:mo>(</mml:mo><mml:mi>q</mml:mi><mml:mo>,</mml:mo><mml:mi mathvariant="italic">δ</mml:mi><mml:mo>)</mml:mo></mml:mrow></mml:math></inline-formula> versus
<inline-formula><mml:math id="M204" display="inline"><mml:mi mathvariant="italic">δ</mml:mi></mml:math></inline-formula> for the first four bands of the Ikonos-2 satellite and for <inline-formula><mml:math id="M205" display="inline"><mml:mrow><mml:mi>q</mml:mi><mml:mo>&lt;</mml:mo><mml:mn mathvariant="normal">0</mml:mn></mml:mrow></mml:math></inline-formula>
values. From top to bottom we show the results for IK#1, IK#2, IK#3
and IK#4. The left column correspond to the 8-bit image and the right column
to the 11-bit image. The arrows marked the range of scales used for the fit and
to calculate the slope for different values of <inline-formula><mml:math id="M206" display="inline"><mml:mi>q</mml:mi></mml:math></inline-formula> (7 points in the left
column and 10 points in the right column).</p></caption>
          <?xmltex \igopts{width=398.338583pt}?><graphic xlink:href="https://npg.copernicus.org/articles/24/141/2017/npg-24-141-2017-f03.png"/>

        </fig>

      <?xmltex \floatpos{t}?><fig id="Ch1.F4" specific-use="star"><caption><p>Multi-fractal spectrum of Ikonos-2 images for the original pixel
values coded in 11 bits (lower) and the minimum–maximum rescaled to 8 bits (upper).
Left column corresponds to each band analysed: IK#1 in blue colour,
IK#2 in green colour, IK#3 in red colour and IK#4 in black. Right
column corresponds to vegetation indexes: NDVI in green colour and EVI in
brown.</p></caption>
          <?xmltex \igopts{width=398.338583pt}?><graphic xlink:href="https://npg.copernicus.org/articles/24/141/2017/npg-24-141-2017-f04.png"/>

        </fig>

      <?xmltex \floatpos{t}?><fig id="Ch1.F5" specific-use="star"><caption><p>Bi-log plots of the partition function <inline-formula><mml:math id="M207" display="inline"><mml:mrow><mml:mi mathvariant="italic">χ</mml:mi><mml:mo>(</mml:mo><mml:mi>q</mml:mi><mml:mo>,</mml:mo><mml:mi mathvariant="italic">δ</mml:mi><mml:mo>)</mml:mo></mml:mrow></mml:math></inline-formula> versus
<inline-formula><mml:math id="M208" display="inline"><mml:mi mathvariant="italic">δ</mml:mi></mml:math></inline-formula> for the vegetation indexes estimated from blue, red and NIR bands of
the Ikonos-2 satellite and for <inline-formula><mml:math id="M209" display="inline"><mml:mrow><mml:mi>q</mml:mi><mml:mo>&lt;</mml:mo><mml:mn mathvariant="normal">0</mml:mn></mml:mrow></mml:math></inline-formula> values. From top to bottom we show the
results for NDVI and EVI respectively. The left column corresponds to the 8-bit
image and the right column to the 11-bit image. The arrows marked the range of
scales used for the fit and to calculate the slope for different values of
<inline-formula><mml:math id="M210" display="inline"><mml:mi>q</mml:mi></mml:math></inline-formula> (7 points).</p></caption>
          <?xmltex \igopts{width=398.338583pt}?><graphic xlink:href="https://npg.copernicus.org/articles/24/141/2017/npg-24-141-2017-f05.png"/>

        </fig>

      <?xmltex \floatpos{t}?><fig id="Ch1.F6" specific-use="star"><caption><p>The Landsat-7 image and the histograms for the first four bands:
blue (ETM<inline-formula><mml:math id="M211" display="inline"><mml:mo>+</mml:mo></mml:math></inline-formula>#1), green (ETM<inline-formula><mml:math id="M212" display="inline"><mml:mo>+</mml:mo></mml:math></inline-formula>#2), red (ETM<inline-formula><mml:math id="M213" display="inline"><mml:mo>+</mml:mo></mml:math></inline-formula>#3) and near
infrared (ETM<inline-formula><mml:math id="M214" display="inline"><mml:mo>+</mml:mo></mml:math></inline-formula>#4). The image has a size of <inline-formula><mml:math id="M215" display="inline"><mml:mrow><mml:mn mathvariant="normal">512</mml:mn><mml:mo>×</mml:mo><mml:mn mathvariant="normal">512</mml:mn></mml:mrow></mml:math></inline-formula> pixels, each area
unit corresponds to <inline-formula><mml:math id="M216" display="inline"><mml:mrow><mml:mn mathvariant="normal">30</mml:mn><mml:mo>×</mml:mo><mml:mn mathvariant="normal">30</mml:mn></mml:mrow></mml:math></inline-formula> m. The coordinates UTM (zone 30) of the upper-left
and lower-right pixel in the image are ULX <inline-formula><mml:math id="M217" display="inline"><mml:mo>=</mml:mo></mml:math></inline-formula> 442 185 m, ULY <inline-formula><mml:math id="M218" display="inline"><mml:mo>=</mml:mo></mml:math></inline-formula> 4 445 568 m,
LRX <inline-formula><mml:math id="M219" display="inline"><mml:mo>=</mml:mo></mml:math></inline-formula> 457 545 m and LRY <inline-formula><mml:math id="M220" display="inline"><mml:mo>=</mml:mo></mml:math></inline-formula> 4 430 208 m.</p></caption>
          <?xmltex \igopts{width=398.338583pt}?><graphic xlink:href="https://npg.copernicus.org/articles/24/141/2017/npg-24-141-2017-f06.jpg"/>

        </fig>

      <p>Some characteristic parameters obtained from these MF spectra are shown in
Table 1 and Table 2. As expected, in both radiometric resolutions and in
each band the <inline-formula><mml:math id="M221" display="inline"><mml:mrow><mml:mi mathvariant="italic">α</mml:mi><mml:mfenced close=")" open="("><mml:mn mathvariant="normal">0</mml:mn></mml:mfenced></mml:mrow></mml:math></inline-formula> is practically 2, as the measure is
defined in the entire plane and it has an Euclidean dimension of 2. With respect
to the <inline-formula><mml:math id="M222" display="inline"><mml:mrow><mml:mi mathvariant="italic">α</mml:mi><mml:mfenced open="(" close=")"><mml:mn mathvariant="normal">1</mml:mn></mml:mfenced></mml:mrow></mml:math></inline-formula> value, certain differences are found.
Comparing the bands in  8 bits to the same ones in 11 bits, the entropy
dimension was always higher. However, considering the standard errors, only IK#1
(B) and IK#2 (G) bands were significantly different, with the blue band showing
the highest difference. Meanwhile, red and NIR bands are not significantly
different. This shows that a more spatially uniform distribution for
the bands of Ikonos-2 8 bits than in 11 bits. The same behaviour is observed
in the <inline-formula><mml:math id="M223" display="inline"><mml:mrow><mml:mi mathvariant="italic">α</mml:mi><mml:mfenced close=")" open="("><mml:mn mathvariant="normal">2</mml:mn></mml:mfenced></mml:mrow></mml:math></inline-formula>.</p>
      <p>The amplitudes calculated (<inline-formula><mml:math id="M224" display="inline"><mml:mrow><mml:msup><mml:mi mathvariant="normal">Δ</mml:mi><mml:mo>+</mml:mo></mml:msup></mml:mrow></mml:math></inline-formula> and <inline-formula><mml:math id="M225" display="inline"><mml:mrow><mml:msup><mml:mi mathvariant="normal">Δ</mml:mi><mml:mo>-</mml:mo></mml:msup><mml:mo>)</mml:mo></mml:mrow></mml:math></inline-formula> in Ikonos-2 11-bit
bands present opposite trends (Table 1). Note that amplitude <inline-formula><mml:math id="M226" display="inline"><mml:mrow><mml:msup><mml:mi mathvariant="normal">Δ</mml:mi><mml:mo>+</mml:mo></mml:msup></mml:mrow></mml:math></inline-formula>
decreases as band wavelength grows, whereas the other amplitude <inline-formula><mml:math id="M227" display="inline"><mml:mrow><mml:msup><mml:mi mathvariant="normal">Δ</mml:mi><mml:mo>-</mml:mo></mml:msup></mml:mrow></mml:math></inline-formula> diminishes. Observing these parameters in Ikonos-2 8-bit bands (Table 2) a different trend and behaviour are found. In this case both <inline-formula><mml:math id="M228" display="inline"><mml:mrow><mml:msup><mml:mi mathvariant="normal">Δ</mml:mi><mml:mo>+</mml:mo></mml:msup></mml:mrow></mml:math></inline-formula> and <inline-formula><mml:math id="M229" display="inline"><mml:mrow><mml:msup><mml:mi mathvariant="normal">Δ</mml:mi><mml:mo>-</mml:mo></mml:msup></mml:mrow></mml:math></inline-formula> increase as the wavelength increases for the three
visible bands, but decrease for the near-infrared band (IK#4).</p>
      <p>The AI estimated on these MFS amplitudes on each radiometric resolution
are shown in the last column of Table 1 and Table 2. Comparing the bands in
8 bits to the same ones in 11 bits, the behaviour is similar: there is a
decreasing trend from IK#1 to IK#4, although the range of values is
different. At a resolution of 11 bits from a positive <inline-formula><mml:math id="M230" display="inline"><mml:mrow><mml:mi mathvariant="normal">AI</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">0.240</mml:mn></mml:mrow></mml:math></inline-formula> at blue band
goes to a negative <inline-formula><mml:math id="M231" display="inline"><mml:mrow><mml:mi mathvariant="normal">AI</mml:mi><mml:mo>=</mml:mo><mml:mo>-</mml:mo><mml:mn mathvariant="normal">0.237</mml:mn></mml:mrow></mml:math></inline-formula> at NIR band. On the other hand, at a
resolution of 8 bits, an <inline-formula><mml:math id="M232" display="inline"><mml:mrow><mml:mi mathvariant="normal">AI</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">0.092</mml:mn></mml:mrow></mml:math></inline-formula> goes to a negative <inline-formula><mml:math id="M233" display="inline"><mml:mrow><mml:mi mathvariant="normal">AI</mml:mi><mml:mo>=</mml:mo><mml:mo>-</mml:mo><mml:mn mathvariant="normal">0.347</mml:mn></mml:mrow></mml:math></inline-formula>. The
more symmetric MFS are found in green and red bands at a resolution of 11 bits and
in blue and green bands at a resolution of 8 bits.</p>
      <p>Doing the same study for the vegetation indexes we found the following. The
bi-log plot of the partition function (<inline-formula><mml:math id="M234" display="inline"><mml:mrow><mml:mi mathvariant="italic">χ</mml:mi><mml:mo>(</mml:mo><mml:mi>q</mml:mi><mml:mo>,</mml:mo><mml:mi mathvariant="italic">δ</mml:mi><mml:mo>)</mml:mo><mml:mo>)</mml:mo></mml:mrow></mml:math></inline-formula> versus <inline-formula><mml:math id="M235" display="inline"><mml:mi mathvariant="italic">δ</mml:mi></mml:math></inline-formula> is
plotted in Fig. 5 for both vegetation indexes at both radiometric resolutions. Each graph
contains 11 points as the bands from where they were estimated. The linear
fit was done with the same methodology as that for the four bands. In this case
only the EVI at 8 bits shows a better linear trend in a wider range of scales.
However, to better compare both vegetation indexes, from both radiometric resolutions, a
range achieving 32 pixels (128 m) was selected as shown by arrows in Fig. 5.</p>
      <p>The MF spectra <inline-formula><mml:math id="M236" display="inline"><mml:mrow><mml:mi>f</mml:mi><mml:mo>(</mml:mo><mml:mi mathvariant="italic">α</mml:mi><mml:mo>)</mml:mo></mml:mrow></mml:math></inline-formula> of EVI and NDVI estimated for both radiometric
resolutions of Ikonos images are shown in Fig. 4. Both vegetation indexes
show differences due to the transformation from 11  to 8 bits. However,
NDVI shows higher differences in the MFS, mainly in the part corresponding
to <inline-formula><mml:math id="M237" display="inline"><mml:mi>q</mml:mi></mml:math></inline-formula> negative values (right side). Even EVI presents changes; its MFS is
closer at both radiometric resolutions. Comparing the range of <inline-formula><mml:math id="M238" display="inline"><mml:mrow><mml:mi>f</mml:mi><mml:mo>(</mml:mo><mml:mi mathvariant="italic">α</mml:mi><mml:mo>)</mml:mo></mml:mrow></mml:math></inline-formula>
values in the vegetation indexes to the range obtained in the four bands (left column in
Fig. 4), there is a remarkable contrast. Meanwhile the NIR band of 8 bits
achieves a <inline-formula><mml:math id="M239" display="inline"><mml:mrow><mml:mi>f</mml:mi><mml:mo>(</mml:mo><mml:mi mathvariant="italic">α</mml:mi><mml:mo>)</mml:mo></mml:mrow></mml:math></inline-formula> value close to 0.5; EVI and NDVI achieve values closer
to 0.2. These differences are higher in the 11-bit image; the red band achieves
a <inline-formula><mml:math id="M240" display="inline"><mml:mrow><mml:mi>f</mml:mi><mml:mo>(</mml:mo><mml:mi mathvariant="italic">α</mml:mi><mml:mo>)</mml:mo></mml:mrow></mml:math></inline-formula> value close to 0.9 and vegetation indexes again achieve values of <inline-formula><mml:math id="M241" display="inline"><mml:mo>∼</mml:mo></mml:math></inline-formula>0.2.
The same characteristic parameters obtained from the band MF spectra were
calculated for the vegetation indexes and are shown in Table 1 and Table 2.</p>
      <p>With respect to the <inline-formula><mml:math id="M242" display="inline"><mml:mrow><mml:mi mathvariant="italic">α</mml:mi><mml:mfenced open="(" close=")"><mml:mn mathvariant="normal">1</mml:mn></mml:mfenced></mml:mrow></mml:math></inline-formula> values, certain differences are
found between the vegetation indexes. Comparing the NDVI in 8 bits to the
same ones in 11 bits, the entropy dimension was always higher than it was found
to be in the bands. However, EVI shows the contrary: entropy values of the 11-bit
image are higher than the 8-bit image, although the differences are not
significant. Therefore, the radiometric resolution affects NDVI
more than EVI. The former presents a more uniform space distribution in
8 bits than in the 11-bit image. The same behaviour is observed in <inline-formula><mml:math id="M243" display="inline"><mml:mrow><mml:mi mathvariant="italic">α</mml:mi><mml:mfenced open="(" close=")"><mml:mn mathvariant="normal">2</mml:mn></mml:mfenced></mml:mrow></mml:math></inline-formula>.</p>
      <p>The amplitudes calculated (<inline-formula><mml:math id="M244" display="inline"><mml:mrow><mml:msup><mml:mi mathvariant="normal">Δ</mml:mi><mml:mo>+</mml:mo></mml:msup></mml:mrow></mml:math></inline-formula> and <inline-formula><mml:math id="M245" display="inline"><mml:mrow><mml:msup><mml:mi mathvariant="normal">Δ</mml:mi><mml:mo>-</mml:mo></mml:msup><mml:mo>)</mml:mo></mml:mrow></mml:math></inline-formula> in Ikonos-2 11-bit
vegetation indexes present a similar situation (Table 1). The amplitude <inline-formula><mml:math id="M246" display="inline"><mml:mrow><mml:msup><mml:mi mathvariant="normal">Δ</mml:mi><mml:mo>+</mml:mo></mml:msup></mml:mrow></mml:math></inline-formula> is
lower than amplitude <inline-formula><mml:math id="M247" display="inline"><mml:mrow><mml:msup><mml:mi mathvariant="normal">Δ</mml:mi><mml:mo>-</mml:mo></mml:msup></mml:mrow></mml:math></inline-formula> and therefore the AI estimated is
negative. This is visually perceived in Fig. 4 (right column). Observing
these parameters in Ikonos-2 8 bits vegetation indexes (Table 2), similar
situations are found but the values are lower. In both images (11  and
8 bits) NDVI shows higher values for both amplitudes, <inline-formula><mml:math id="M248" display="inline"><mml:mrow><mml:msup><mml:mi mathvariant="normal">Δ</mml:mi><mml:mo>+</mml:mo></mml:msup></mml:mrow></mml:math></inline-formula> and
<inline-formula><mml:math id="M249" display="inline"><mml:mrow><mml:msup><mml:mi mathvariant="normal">Δ</mml:mi><mml:mo>-</mml:mo></mml:msup></mml:mrow></mml:math></inline-formula>.</p>

<?xmltex \floatpos{t}?><table-wrap id="Ch1.T3" specific-use="star"><caption><p>Parameters obtained from the multi-fractal spectrum from each band
of the Landsat-7 image, and the vegetation indexes (VIs) estimated, with a pixel
size of 4 m and a radiometric resolution of 8 bits. The amplitudes of
<inline-formula><mml:math id="M250" display="inline"><mml:mi mathvariant="italic">α</mml:mi></mml:math></inline-formula> values are presented as <inline-formula><mml:math id="M251" display="inline"><mml:mrow><mml:msup><mml:mi mathvariant="normal">Δ</mml:mi><mml:mo>+</mml:mo></mml:msup></mml:mrow></mml:math></inline-formula> and <inline-formula><mml:math id="M252" display="inline"><mml:mrow><mml:msup><mml:mi mathvariant="normal">Δ</mml:mi><mml:mo>-</mml:mo></mml:msup></mml:mrow></mml:math></inline-formula>
corresponding to <inline-formula><mml:math id="M253" display="inline"><mml:mrow><mml:mi mathvariant="italic">α</mml:mi><mml:mo>(</mml:mo><mml:mn mathvariant="normal">0</mml:mn><mml:mo>)</mml:mo><mml:mo>-</mml:mo><mml:mi mathvariant="italic">α</mml:mi><mml:mo>(</mml:mo><mml:mn mathvariant="normal">5</mml:mn><mml:mo>)</mml:mo></mml:mrow></mml:math></inline-formula> and <inline-formula><mml:math id="M254" display="inline"><mml:mrow><mml:mi mathvariant="italic">α</mml:mi><mml:mo>(</mml:mo><mml:mo>-</mml:mo><mml:mn mathvariant="normal">5</mml:mn><mml:mo>)</mml:mo><mml:mo>-</mml:mo><mml:mi mathvariant="italic">α</mml:mi><mml:mo>(</mml:mo><mml:mn mathvariant="normal">0</mml:mn><mml:mo>)</mml:mo></mml:mrow></mml:math></inline-formula>
respectively. The asymmetry index (AI) corresponds to
<inline-formula><mml:math id="M255" display="inline"><mml:mstyle displaystyle="false"><mml:mfrac style="text"><mml:mrow><mml:msup><mml:mi mathvariant="normal">Δ</mml:mi><mml:mo>+</mml:mo></mml:msup><mml:mo>-</mml:mo><mml:msup><mml:mi mathvariant="normal">Δ</mml:mi><mml:mo>-</mml:mo></mml:msup></mml:mrow><mml:mrow><mml:msup><mml:mi mathvariant="normal">Δ</mml:mi><mml:mo>+</mml:mo></mml:msup><mml:mo>+</mml:mo><mml:msup><mml:mi mathvariant="normal">Δ</mml:mi><mml:mo>-</mml:mo></mml:msup></mml:mrow></mml:mfrac></mml:mstyle></mml:math></inline-formula>.</p></caption><oasis:table frame="topbot"><oasis:tgroup cols="7">
     <oasis:colspec colnum="1" colname="col1" align="left"/>
     <oasis:colspec colnum="2" colname="col2" align="left"/>
     <oasis:colspec colnum="3" colname="col3" align="right"/>
     <oasis:colspec colnum="4" colname="col4" align="right"/>
     <oasis:colspec colnum="5" colname="col5" align="right"/>
     <oasis:colspec colnum="6" colname="col6" align="right"/>
     <oasis:colspec colnum="7" colname="col7" align="right"/>
     <oasis:thead>
       <oasis:row rowsep="1">

         <oasis:entry colname="col1"/>

         <oasis:entry colname="col2">Band</oasis:entry>

         <oasis:entry colname="col3"><inline-formula><mml:math id="M256" display="inline"><mml:mi>q</mml:mi></mml:math></inline-formula></oasis:entry>

         <oasis:entry colname="col4"><inline-formula><mml:math id="M257" display="inline"><mml:mrow><mml:mi mathvariant="italic">α</mml:mi><mml:mo>(</mml:mo><mml:mi>q</mml:mi><mml:mo>)</mml:mo></mml:mrow></mml:math></inline-formula></oasis:entry>

         <oasis:entry colname="col5"><inline-formula><mml:math id="M258" display="inline"><mml:mrow><mml:msup><mml:mi mathvariant="normal">Δ</mml:mi><mml:mo>+</mml:mo></mml:msup></mml:mrow></mml:math></inline-formula></oasis:entry>

         <oasis:entry colname="col6"><inline-formula><mml:math id="M259" display="inline"><mml:mrow><mml:msup><mml:mi mathvariant="normal">Δ</mml:mi><mml:mo>-</mml:mo></mml:msup></mml:mrow></mml:math></inline-formula></oasis:entry>

         <oasis:entry colname="col7">AI</oasis:entry>

       </oasis:row>
     </oasis:thead>
     <oasis:tbody>
       <oasis:row>

         <oasis:entry rowsep="1" colname="col1" morerows="11">Landsat-7</oasis:entry>

         <oasis:entry rowsep="1" colname="col2" morerows="2">ETM<inline-formula><mml:math id="M260" display="inline"><mml:mo>+</mml:mo></mml:math></inline-formula>#1</oasis:entry>

         <oasis:entry colname="col3">0</oasis:entry>

         <oasis:entry colname="col4">2.001 <inline-formula><mml:math id="M261" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> 0.001</oasis:entry>

         <oasis:entry rowsep="1" colname="col5" morerows="2">0.160</oasis:entry>

         <oasis:entry rowsep="1" colname="col6" morerows="2">0.119</oasis:entry>

         <oasis:entry rowsep="1" colname="col7" morerows="2">0.147</oasis:entry>

       </oasis:row>
       <oasis:row>

         <oasis:entry colname="col3">1</oasis:entry>

         <oasis:entry colname="col4">1.985 <inline-formula><mml:math id="M262" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> 0.005</oasis:entry>

       </oasis:row>
       <oasis:row rowsep="1">

         <oasis:entry colname="col3">2</oasis:entry>

         <oasis:entry colname="col4">1.960 <inline-formula><mml:math id="M263" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> 0.010</oasis:entry>

       </oasis:row>
       <oasis:row>

         <oasis:entry rowsep="1" colname="col2" morerows="2">ETM<inline-formula><mml:math id="M264" display="inline"><mml:mo>+</mml:mo></mml:math></inline-formula>#2</oasis:entry>

         <oasis:entry colname="col3">0</oasis:entry>

         <oasis:entry colname="col4">2.003 <inline-formula><mml:math id="M265" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> 0.001</oasis:entry>

         <oasis:entry rowsep="1" colname="col5" morerows="2">0.119</oasis:entry>

         <oasis:entry rowsep="1" colname="col6" morerows="2">0.119</oasis:entry>

         <oasis:entry rowsep="1" colname="col7" morerows="2">0.000</oasis:entry>

       </oasis:row>
       <oasis:row>

         <oasis:entry colname="col3">1</oasis:entry>

         <oasis:entry colname="col4">1.988 <inline-formula><mml:math id="M266" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> 0.004</oasis:entry>

       </oasis:row>
       <oasis:row rowsep="1">

         <oasis:entry colname="col3">2</oasis:entry>

         <oasis:entry colname="col4">1.970 <inline-formula><mml:math id="M267" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> 0.008</oasis:entry>

       </oasis:row>
       <oasis:row>

         <oasis:entry rowsep="1" colname="col2" morerows="2">ETM<inline-formula><mml:math id="M268" display="inline"><mml:mo>+</mml:mo></mml:math></inline-formula>#3</oasis:entry>

         <oasis:entry colname="col3">0</oasis:entry>

         <oasis:entry colname="col4">2.001 <inline-formula><mml:math id="M269" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> 0.001</oasis:entry>

         <oasis:entry rowsep="1" colname="col5" morerows="2">0.095</oasis:entry>

         <oasis:entry rowsep="1" colname="col6" morerows="2">0.110</oasis:entry>

         <oasis:entry rowsep="1" colname="col7" morerows="2"><inline-formula><mml:math id="M270" display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>0.073</oasis:entry>

       </oasis:row>
       <oasis:row>

         <oasis:entry colname="col3">1</oasis:entry>

         <oasis:entry colname="col4">1.989 <inline-formula><mml:math id="M271" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> 0.004</oasis:entry>

       </oasis:row>
       <oasis:row rowsep="1">

         <oasis:entry colname="col3">2</oasis:entry>

         <oasis:entry colname="col4">1.974 <inline-formula><mml:math id="M272" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> 0.007</oasis:entry>

       </oasis:row>
       <oasis:row>

         <oasis:entry rowsep="1" colname="col2" morerows="2">ETM<inline-formula><mml:math id="M273" display="inline"><mml:mo>+</mml:mo></mml:math></inline-formula>#4</oasis:entry>

         <oasis:entry colname="col3">0</oasis:entry>

         <oasis:entry colname="col4">2.017 <inline-formula><mml:math id="M274" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> 0.001</oasis:entry>

         <oasis:entry rowsep="1" colname="col5" morerows="2">0.106</oasis:entry>

         <oasis:entry rowsep="1" colname="col6" morerows="2">0.104</oasis:entry>

         <oasis:entry rowsep="1" colname="col7" morerows="2">0.010</oasis:entry>

       </oasis:row>
       <oasis:row>

         <oasis:entry colname="col3">1</oasis:entry>

         <oasis:entry colname="col4">1.989 <inline-formula><mml:math id="M275" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> 0.004</oasis:entry>

       </oasis:row>
       <oasis:row rowsep="1">

         <oasis:entry colname="col3">2</oasis:entry>

         <oasis:entry colname="col4">1.973 <inline-formula><mml:math id="M276" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> 0.008</oasis:entry>

       </oasis:row>
       <oasis:row rowsep="1">

         <oasis:entry colname="col1"/>

         <oasis:entry colname="col2">VI</oasis:entry>

         <oasis:entry colname="col3"><inline-formula><mml:math id="M277" display="inline"><mml:mi>q</mml:mi></mml:math></inline-formula></oasis:entry>

         <oasis:entry colname="col4"><inline-formula><mml:math id="M278" display="inline"><mml:mrow><mml:mi mathvariant="italic">α</mml:mi><mml:mo>(</mml:mo><mml:mi>q</mml:mi><mml:mo>)</mml:mo></mml:mrow></mml:math></inline-formula></oasis:entry>

         <oasis:entry colname="col5"><inline-formula><mml:math id="M279" display="inline"><mml:mrow><mml:msup><mml:mi mathvariant="normal">Δ</mml:mi><mml:mo>+</mml:mo></mml:msup></mml:mrow></mml:math></inline-formula></oasis:entry>

         <oasis:entry colname="col6"><inline-formula><mml:math id="M280" display="inline"><mml:mrow><mml:msup><mml:mi mathvariant="normal">Δ</mml:mi><mml:mo>-</mml:mo></mml:msup></mml:mrow></mml:math></inline-formula></oasis:entry>

         <oasis:entry colname="col7">AI</oasis:entry>

       </oasis:row>
       <oasis:row>

         <oasis:entry colname="col1" morerows="5">Landsat-7</oasis:entry>

         <oasis:entry rowsep="1" colname="col2" morerows="2">NDVI</oasis:entry>

         <oasis:entry colname="col3">0</oasis:entry>

         <oasis:entry colname="col4">2.001 <inline-formula><mml:math id="M281" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> 0.001</oasis:entry>

         <oasis:entry rowsep="1" colname="col5" morerows="2">0.028</oasis:entry>

         <oasis:entry rowsep="1" colname="col6" morerows="2">0.353</oasis:entry>

         <oasis:entry rowsep="1" colname="col7" morerows="2"><inline-formula><mml:math id="M282" display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>0.852</oasis:entry>

       </oasis:row>
       <oasis:row>

         <oasis:entry colname="col3">1</oasis:entry>

         <oasis:entry colname="col4">1.996 <inline-formula><mml:math id="M283" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> 0.001</oasis:entry>

       </oasis:row>
       <oasis:row rowsep="1">

         <oasis:entry colname="col3">2</oasis:entry>

         <oasis:entry colname="col4">1.992 <inline-formula><mml:math id="M284" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> 0.001</oasis:entry>

       </oasis:row>
       <oasis:row>

         <oasis:entry colname="col2" morerows="2">EVI</oasis:entry>

         <oasis:entry colname="col3">0</oasis:entry>

         <oasis:entry colname="col4">2.001 <inline-formula><mml:math id="M285" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> 0.001</oasis:entry>

         <oasis:entry colname="col5" morerows="2">0.022</oasis:entry>

         <oasis:entry colname="col6" morerows="2">0.288</oasis:entry>

         <oasis:entry colname="col7" morerows="2"><inline-formula><mml:math id="M286" display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>0.859</oasis:entry>

       </oasis:row>
       <oasis:row>

         <oasis:entry colname="col3">1</oasis:entry>

         <oasis:entry colname="col4">1.997 <inline-formula><mml:math id="M287" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> 0.001</oasis:entry>

       </oasis:row>
       <oasis:row>

         <oasis:entry colname="col3">2</oasis:entry>

         <oasis:entry colname="col4">1.994 <inline-formula><mml:math id="M288" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> 0.001</oasis:entry>

       </oasis:row>
     </oasis:tbody>
   </oasis:tgroup></oasis:table></table-wrap>

      <?xmltex \floatpos{t}?><fig id="Ch1.F7"><caption><p>Bi-log plots of the partition function <inline-formula><mml:math id="M289" display="inline"><mml:mrow><mml:mi mathvariant="italic">χ</mml:mi><mml:mo>(</mml:mo><mml:mi>q</mml:mi><mml:mo>,</mml:mo><mml:mi mathvariant="italic">δ</mml:mi><mml:mo>)</mml:mo></mml:mrow></mml:math></inline-formula> versus
<inline-formula><mml:math id="M290" display="inline"><mml:mi mathvariant="italic">δ</mml:mi></mml:math></inline-formula> for the first four bands of the Landsat-7 satellite and for <inline-formula><mml:math id="M291" display="inline"><mml:mrow><mml:mi>q</mml:mi><mml:mo>&lt;</mml:mo><mml:mn mathvariant="normal">0</mml:mn></mml:mrow></mml:math></inline-formula>
values. From top to bottom we show the results for ETM<inline-formula><mml:math id="M292" display="inline"><mml:mo>+</mml:mo></mml:math></inline-formula>#1, ETM<inline-formula><mml:math id="M293" display="inline"><mml:mo>+</mml:mo></mml:math></inline-formula>#2,
ETM<inline-formula><mml:math id="M294" display="inline"><mml:mo>+</mml:mo></mml:math></inline-formula>#3 and ETM<inline-formula><mml:math id="M295" display="inline"><mml:mo>+</mml:mo></mml:math></inline-formula>#4. The arrows marked the range of scales used for
the fit and to calculate the slope for different values of <inline-formula><mml:math id="M296" display="inline"><mml:mi>q</mml:mi></mml:math></inline-formula> (8 points).</p></caption>
          <?xmltex \igopts{width=236.157874pt}?><graphic xlink:href="https://npg.copernicus.org/articles/24/141/2017/npg-24-141-2017-f07.png"/>

        </fig>

      <?xmltex \floatpos{t}?><fig id="Ch1.F8" specific-use="star"><caption><p>Multi-fractal spectrum of the Landsat-7 image for the original pixel
values coded in 8 bits. Left plot corresponds to each band analysed:
ETM<inline-formula><mml:math id="M297" display="inline"><mml:mo>+</mml:mo></mml:math></inline-formula>#1 in blue colour, ETM<inline-formula><mml:math id="M298" display="inline"><mml:mo>+</mml:mo></mml:math></inline-formula>#2 in green colour, ETM<inline-formula><mml:math id="M299" display="inline"><mml:mo>+</mml:mo></mml:math></inline-formula>#3 in red
colour and ETM<inline-formula><mml:math id="M300" display="inline"><mml:mo>+</mml:mo></mml:math></inline-formula>#4 in black. Right plot corresponds to vegetation
indexes: NDVI in green colour and EVI in brown.</p></caption>
          <?xmltex \igopts{width=398.338583pt}?><graphic xlink:href="https://npg.copernicus.org/articles/24/141/2017/npg-24-141-2017-f08.png"/>

        </fig>

      <?xmltex \floatpos{t}?><fig id="Ch1.F9"><caption><p>Bi-log plots of the partition function <inline-formula><mml:math id="M301" display="inline"><mml:mrow><mml:mi mathvariant="italic">χ</mml:mi><mml:mo>(</mml:mo><mml:mi>q</mml:mi><mml:mo>,</mml:mo><mml:mi mathvariant="italic">δ</mml:mi><mml:mo>)</mml:mo></mml:mrow></mml:math></inline-formula> versus
<inline-formula><mml:math id="M302" display="inline"><mml:mi mathvariant="italic">δ</mml:mi></mml:math></inline-formula> for the vegetation indexes estimated from blue, red and NIR bands of
the Landsat-7 satellite and for <inline-formula><mml:math id="M303" display="inline"><mml:mrow><mml:mi>q</mml:mi><mml:mo>&lt;</mml:mo><mml:mn mathvariant="normal">0</mml:mn></mml:mrow></mml:math></inline-formula> values. From top to bottom we show the
results for NDVI and EVI. The arrows marked the range of scales used for the
fit and to calculate the slope for different values of <inline-formula><mml:math id="M304" display="inline"><mml:mi>q</mml:mi></mml:math></inline-formula> (7 points).</p></caption>
          <?xmltex \igopts{width=236.157874pt}?><graphic xlink:href="https://npg.copernicus.org/articles/24/141/2017/npg-24-141-2017-f09.png"/>

        </fig>

      <p>All the AI estimated for both vegetation indexes on each radiometric
resolution are negative (Table 1 and Table 2), indicating a high asymmetry on
the right part of the MFS, as shown in Fig. 4. Comparing the AI values in
8 bits to the same ones in 11 bits, they are similar which shows that the
shape of the MFS is similar as this index is a normalized index. However, the
values of the amplitudes mark a higher change in NDVI than in EVI.</p>
</sec>
<sec id="Ch1.S3.SS2">
  <title>Spatial resolution influence in the multi-fractal spectrum</title>
      <p>A comparison is made between Landsat, with an original pixel code of 8 bits, and the
rescaled histograms from Ikonos, with an original pixel code of 11 bits. In this section, we discuss the results obtained in the MF analysis on
the <inline-formula><mml:math id="M305" display="inline"><mml:mrow><mml:mn mathvariant="normal">512</mml:mn><mml:mo>×</mml:mo><mml:mn mathvariant="normal">512</mml:mn></mml:mrow></mml:math></inline-formula> pixel Landsat-7 image shown in Fig. 6, in bands combination of
false colour (ETM<inline-formula><mml:math id="M306" display="inline"><mml:mo>+</mml:mo></mml:math></inline-formula>#3, ETM<inline-formula><mml:math id="M307" display="inline"><mml:mo>+</mml:mo></mml:math></inline-formula>#2 and ETM<inline-formula><mml:math id="M308" display="inline"><mml:mo>+</mml:mo></mml:math></inline-formula>#1 band combination in
RGB visualization).</p>
      <p>In the right column of Fig. 6, the histograms of the Landsat-7 image for the
first four bands are shown. The histograms present a bimodal structure,
except for ETM<inline-formula><mml:math id="M309" display="inline"><mml:mo>+</mml:mo></mml:math></inline-formula>#4 (NIR), in which there is only one peak. Comparing these
histograms with those obtained for Ikonos-2 8-bit image (Fig. 2), the peaks
are not so abrupt and narrow. At the same time, ETM<inline-formula><mml:math id="M310" display="inline"><mml:mo>+</mml:mo></mml:math></inline-formula>#1, ETM<inline-formula><mml:math id="M311" display="inline"><mml:mo>+</mml:mo></mml:math></inline-formula>#2 and
ETM<inline-formula><mml:math id="M312" display="inline"><mml:mo>+</mml:mo></mml:math></inline-formula>#3 bands show the absolute maximum peak at high-value pixels (light
grey) and a second one at lower-value pixels (dark grey). These bands are
more centred and do not show a shift to the left as the Ikonos-2 8-bit bands
(IK#1, IK#2 and IK#3. In the case of the NIR band, Landsat-7 and
Ikonos-2 8 bits are quite similar except for the absence of a second peak.</p>
      <p>In the calculations, box sizes range from 512 to 2 pixels, that is, <inline-formula><mml:math id="M313" display="inline"><mml:mrow><mml:mi mathvariant="italic">δ</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">512</mml:mn><mml:mo>/</mml:mo><mml:msup><mml:mn mathvariant="normal">2</mml:mn><mml:mi>n</mml:mi></mml:msup></mml:mrow></mml:math></inline-formula> with <inline-formula><mml:math id="M314" display="inline"><mml:mrow><mml:mi>n</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">0</mml:mn></mml:mrow></mml:math></inline-formula>, 1, …, 8. For each value of the parameters <inline-formula><mml:math id="M315" display="inline"><mml:mi>q</mml:mi></mml:math></inline-formula>, from <inline-formula><mml:math id="M316" display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>5 to <inline-formula><mml:math id="M317" display="inline"><mml:mo>+</mml:mo></mml:math></inline-formula>5
with increments of 0.5, we compute the partition function, and the bi-log
<inline-formula><mml:math id="M318" display="inline"><mml:mrow><mml:mi mathvariant="italic">χ</mml:mi><mml:mo>(</mml:mo><mml:mi>q</mml:mi><mml:mo>,</mml:mo><mml:mi mathvariant="italic">δ</mml:mi><mml:mo>)</mml:mo></mml:mrow></mml:math></inline-formula> versus <inline-formula><mml:math id="M319" display="inline"><mml:mi mathvariant="italic">δ</mml:mi></mml:math></inline-formula> is plotted in Fig. 7. In this case each
linear fits contains only 9 points as the size of the image is <inline-formula><mml:math id="M320" display="inline"><mml:mrow><mml:mn mathvariant="normal">512</mml:mn><mml:mo>×</mml:mo><mml:mn mathvariant="normal">512</mml:mn></mml:mrow></mml:math></inline-formula>
pixels. The same method was applied to select the range of scales used in
the linear fit, achieving a scale of 4 pixels. Changing from pixels to
metres, the scale achieved, used in Landsat-7 in the MF analysis, was <inline-formula><mml:math id="M321" display="inline"><mml:mo>∼</mml:mo></mml:math></inline-formula>120 m. In the case of the Ikonos-2 8 bits the scale was 32 pixels or 128 m, very
close to Landsat-7.</p>
      <p>The MF spectra, <inline-formula><mml:math id="M322" display="inline"><mml:mrow><mml:mi>f</mml:mi><mml:mo>(</mml:mo><mml:mi mathvariant="italic">α</mml:mi><mml:mo>)</mml:mo></mml:mrow></mml:math></inline-formula>, corresponding to the first four bands of
multi-spectral Landsat-7 images are shown in Fig. 8. From a comparison of
Figs. 4 and 8 we see that Landsat-7 image MF spectra are always located
inside the corresponding Ikonos-2 MF spectra. For a given value of
Hölder exponent <inline-formula><mml:math id="M323" display="inline"><mml:mi mathvariant="italic">α</mml:mi></mml:math></inline-formula>, the relation <inline-formula><mml:math id="M324" display="inline"><mml:mrow><mml:msub><mml:mi>f</mml:mi><mml:mi mathvariant="normal">Landsat</mml:mi></mml:msub><mml:mo>(</mml:mo><mml:mi mathvariant="italic">α</mml:mi><mml:mo>)</mml:mo><mml:mo>≤</mml:mo><mml:msub><mml:mi>f</mml:mi><mml:mi mathvariant="normal">Ikonos</mml:mi></mml:msub><mml:mo>(</mml:mo><mml:mi mathvariant="italic">α</mml:mi><mml:mo>)</mml:mo></mml:mrow></mml:math></inline-formula> is always satisfied. This result means that Landsat-7
images show lower complexity than Ikonos-2 8-bit images. As stated in
Sect. 2.1 Ikonos-2 satellite data are coded in 11 bits in contrast with
Landsat-7 8-bit-coded data. To compare both sensors, with different spatial
resolution, we pass Ikonos-2 from 11 to 8 bits, observing that the latter
shows more complexity than Landsat.</p>
      <p>The MF-spectra parameters from Landsat-7 are shown in Table 3. In this section we will
compare the MF spectra and the vegetation indexes of the Ikonos-2 8 bits (Table 2). The <inline-formula><mml:math id="M325" display="inline"><mml:mrow><mml:mi mathvariant="italic">α</mml:mi><mml:mfenced open="(" close=")"><mml:mn mathvariant="normal">1</mml:mn></mml:mfenced></mml:mrow></mml:math></inline-formula> values from the four bands of Landsat-7 are higher than the ones
presented by Ikonos-2 8 bits, indicating a more uniform space
distribution. Comparing between the bands, there are not significant
differences, contrary to the trend we observed among them in Ikonos-2
8 bits. The <inline-formula><mml:math id="M326" display="inline"><mml:mrow><mml:mi mathvariant="italic">α</mml:mi><mml:mfenced open="(" close=")"><mml:mn mathvariant="normal">2</mml:mn></mml:mfenced></mml:mrow></mml:math></inline-formula> shows the same behaviour.</p>
      <p>The amplitudes calculated (<inline-formula><mml:math id="M327" display="inline"><mml:mrow><mml:msup><mml:mi mathvariant="normal">Δ</mml:mi><mml:mo>+</mml:mo></mml:msup></mml:mrow></mml:math></inline-formula> and <inline-formula><mml:math id="M328" display="inline"><mml:mrow><mml:msup><mml:mi mathvariant="normal">Δ</mml:mi><mml:mo>-</mml:mo></mml:msup><mml:mo>)</mml:mo></mml:mrow></mml:math></inline-formula> in Landsat-7 bands
present few variations (Table 3). The amplitude <inline-formula><mml:math id="M329" display="inline"><mml:mrow><mml:msup><mml:mi mathvariant="normal">Δ</mml:mi><mml:mo>+</mml:mo></mml:msup></mml:mrow></mml:math></inline-formula> decreases from
ETM<inline-formula><mml:math id="M330" display="inline"><mml:mo>+</mml:mo></mml:math></inline-formula>#1 to ETM<inline-formula><mml:math id="M331" display="inline"><mml:mo>+</mml:mo></mml:math></inline-formula>#3 and then presents an increase in ETM<inline-formula><mml:math id="M332" display="inline"><mml:mo>+</mml:mo></mml:math></inline-formula>#4
(NIR) whereas the other amplitude <inline-formula><mml:math id="M333" display="inline"><mml:mrow><mml:msup><mml:mi mathvariant="normal">Δ</mml:mi><mml:mo>-</mml:mo></mml:msup></mml:mrow></mml:math></inline-formula> remains practically constant.
Observing these parameters in Ikonos-2 8-bit bands (Table 2), there are
variations in value and behaviour for the four bands. In this case, both
<inline-formula><mml:math id="M334" display="inline"><mml:mrow><mml:msup><mml:mi mathvariant="normal">Δ</mml:mi><mml:mo>+</mml:mo></mml:msup></mml:mrow></mml:math></inline-formula> and <inline-formula><mml:math id="M335" display="inline"><mml:mrow><mml:msup><mml:mi mathvariant="normal">Δ</mml:mi><mml:mo>-</mml:mo></mml:msup></mml:mrow></mml:math></inline-formula> increase as the wavelength increases for the
three visible bands, but decrease for the NIR band (IK#4).</p>
      <p>The AIs estimated on these MFS amplitudes on each Landsat-7 bands are
positive, except for ETM<inline-formula><mml:math id="M336" display="inline"><mml:mo>+</mml:mo></mml:math></inline-formula>#3 (red band). For the green band (ETM<inline-formula><mml:math id="M337" display="inline"><mml:mo>+</mml:mo></mml:math></inline-formula>#3) the
symmetry of the MFS is complete. The band that shows certain asymmetry is
the blue band (ETM<inline-formula><mml:math id="M338" display="inline"><mml:mo>+</mml:mo></mml:math></inline-formula>#1).</p>
      <p>Regarding the vegetation indexes, estimated on Landsat-7 bands, we found the
following. The bi-log plot of the partition function (<inline-formula><mml:math id="M339" display="inline"><mml:mrow><mml:mi mathvariant="italic">χ</mml:mi><mml:mo>(</mml:mo><mml:mi>q</mml:mi><mml:mo>,</mml:mo><mml:mi mathvariant="italic">δ</mml:mi><mml:mo>)</mml:mo><mml:mo>)</mml:mo></mml:mrow></mml:math></inline-formula>
versus <inline-formula><mml:math id="M340" display="inline"><mml:mi mathvariant="italic">δ</mml:mi></mml:math></inline-formula> is plotted in Fig. 9 for both vegetation indexes. Each graph contains 9 points corresponding to the bands from which they were estimated. The linear fit was done with
the same methodology as that for the four bands. EVI and NDVI show the same
behaviour, and the same range of scale was selected achieving 8 pixels, as
shown by arrows in Fig. 9.</p>
      <p>The MF spectra <inline-formula><mml:math id="M341" display="inline"><mml:mrow><mml:mi>f</mml:mi><mml:mo>(</mml:mo><mml:mi mathvariant="italic">α</mml:mi><mml:mo>)</mml:mo></mml:mrow></mml:math></inline-formula> of EVI and NDVI, estimated based on the Landsat-7
image, are shown in Fig. 8. Both vegetation indexes show differences mainly
in the right side of the MFS (for <inline-formula><mml:math id="M342" display="inline"><mml:mi>q</mml:mi></mml:math></inline-formula> negative values). Comparing the range of
<inline-formula><mml:math id="M343" display="inline"><mml:mrow><mml:mi>f</mml:mi><mml:mo>(</mml:mo><mml:mi mathvariant="italic">α</mml:mi><mml:mo>)</mml:mo></mml:mrow></mml:math></inline-formula> values in the vegetation indexes to the range obtained in the four bands (left
column in Fig. 8), there is a remarkable contrast. Meanwhile the NIR band of
8 bits achieves <inline-formula><mml:math id="M344" display="inline"><mml:mrow><mml:mi>f</mml:mi><mml:mo>(</mml:mo><mml:mi mathvariant="italic">α</mml:mi><mml:mo>)</mml:mo></mml:mrow></mml:math></inline-formula> value close to 1.6, EVI and NDVI achieve values
closer to 1. A similar situation was found with both images of Ikonos-2.</p>
      <p>We are going to study the parameters obtained from the MF spectra for the
vegetation indexes (Table 3). The results are quite similar to those
found for the Landsat-7 bands, showing even higher values: 1.996 in NDVI
and 1.997 in EVI.</p>
      <p>The amplitude <inline-formula><mml:math id="M345" display="inline"><mml:mrow><mml:msup><mml:mi mathvariant="normal">Δ</mml:mi><mml:mo>+</mml:mo></mml:msup></mml:mrow></mml:math></inline-formula> is quite low compared with the bands and to the
vegetation indexes of Ikonos-2 8 bits. On the other hand, the amplitude <inline-formula><mml:math id="M346" display="inline"><mml:mrow><mml:msup><mml:mi mathvariant="normal">Δ</mml:mi><mml:mo>-</mml:mo></mml:msup></mml:mrow></mml:math></inline-formula> is
higher than Landsat-7 bands but by only a third of the values shown by
Ikonos-2 8-bit vegetation indexes (Table 2). The AI estimated for both vegetation indexes
are negative, indicating a high asymmetry on the right part of the MFS, as
shown in Fig. 8. Comparing the AI values of Landsat-7 vegetation indexes with the ones
of both Ikonos-2 images, these are the highest, indicating that the most
unbalanced MFS shifted totally on the right side of the spectrum.</p>
</sec>
</sec>
<sec id="Ch1.S4" sec-type="conclusions">
  <title>Conclusions</title>
      <p>In this work, we have used MF spectra as a successful technique for
analysing common information contained in multi-spectral images of the site
of the Earth surface acquired by two satellites, Landsat-7 and Ikonos, in
four common bands in the visible (blue, green and red) and near-infrared wavelength regions used in several vegetation indexes.</p>
      <p>The radiometric resolution has been studied by comparing MF spectra of the
images acquired by Ikonos-2 coded in 11 bits and transformed into 8-bit code.
The results obtained after the histogram transformation in the blue and
green bands were those one would expect after the simplification
applied from 11 to 8 bits, i.e. higher frequency in all the histogram bin
values (see Fig. 2). In contrast, red and infrared bands showed no
sensitivity at all to this transformation, keeping similar MF spectra. To our
knowledge, this is the first time these differences among bands have been
reported.</p>
      <p>In order to analyse the effect of spatial resolution in each band at 4 m (Ikonos-2 with 8 bits) pixel size and 30 m (Landsat-7 with 8 bits) pixel size
are compared. Obviously, the higher the spatial resolution, the higher the
Hölder spectrum amplitudes in the green and blue bands are. In fact,
observing the graphics of the three cases studied (Ikonos-2 11 bits,
Ikonos-2 8 bits and Landsat-7 8 bits) both bands gradually reduce their
<inline-formula><mml:math id="M347" display="inline"><mml:mrow><mml:mi mathvariant="italic">α</mml:mi><mml:mo>(</mml:mo><mml:mi>q</mml:mi><mml:mo>)</mml:mo></mml:mrow></mml:math></inline-formula> amplitude in the negative as well as in the positive <inline-formula><mml:math id="M348" display="inline"><mml:mi>q</mml:mi></mml:math></inline-formula> values.
However, this is not the case for red and NIR bands that present a much higher
difference between Ikonos-2 8 bits and Landsat-7 curves of the MF spectra
than between Ikonos-2 11 and 8 bits.</p>
      <p>In the <inline-formula><mml:math id="M349" display="inline"><mml:mrow><mml:mi>q</mml:mi><mml:mi mathvariant="italic">&gt;</mml:mi><mml:mn mathvariant="normal">0</mml:mn></mml:mrow></mml:math></inline-formula> MFS region for blue and green bands the sensitivity to both factors is very
similar, the blue band ratio being slightly higher. The other two bands, red
and NIR, for the same region, mainly present sensitivity to spatial
resolution, showing a similar rate to blue and green bands. Observing the
<inline-formula><mml:math id="M350" display="inline"><mml:mrow><mml:mi>q</mml:mi><mml:mi mathvariant="italic">&lt;</mml:mi><mml:mn mathvariant="normal">0</mml:mn></mml:mrow></mml:math></inline-formula> region for blue and green, the behaviour is similar to the positive one but
with a lower ratio (between 1 and 2) and, once more, the red and infrared
bands show slight sensitivity to radiometric resolution. Nevertheless, in
the spatial resolution the red band has a ratio similar to blue and green, and NIR
shows the highest ratio (<inline-formula><mml:math id="M351" display="inline"><mml:mo>∼</mml:mo></mml:math></inline-formula>8), showing the extreme influence of the
lowest values contained; see histograms in Fig. 2 (Ikonos-2 8 and 11 bits)
and Fig. 6 (Landsat-7).</p>
      <p>The implications of these variations in the blue, red and NIR in the
multi-scaling behaviour of two vegetation indexes, NDVI and EVI, have been
also studied. The radiometric resolution showed a higher influence in the
MFS of the NDVI than in EVI. This implies that the use of the blue band in the
latter has a steady effect on the scaling behaviour. As was noted for the
bands, the spatial resolution had a major impact in both vegetation indexes.</p>
      <p>Further research will be conducted to establish a qualitative and
quantitative comparison of these conclusions among several multi-fractal
methodologies applied on these images.</p><?xmltex \hack{\newpage}?>
</sec>

      
      </body>
    <back><notes notes-type="dataavailability">

      <p>Data are available by email request to the corresponding author.</p>
  </notes><notes notes-type="competinginterests">

      <p>The authors declare that they have no conflict of interest.</p>
  </notes><ack><title>Acknowledgements</title><p>Thanks are due to the anonymous referees and the editor for their interest
in and patience with this work. Discussion and comments suggested by  Jose Manuel Redondo are highly appreciated. This work has been supported by the
Ministerio de Economía y Competitividad (MINECO) under contract nos.
MTM2012-39101 and MTM2015-63914-P.<?xmltex \hack{\newline}?><?xmltex \hack{\newline}?>
Edited by: Asim Biswas<?xmltex \hack{\newline}?>
Reviewed by: two anonymous referees</p></ack><ref-list>
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  </ref-list><app-group content-type="float"><app><title/>

    </app></app-group></back>
    <!--<article-title-html>Spatial and radiometric characterization of multi-spectrum satellite images through multi-fractal analysis</article-title-html>
<abstract-html><p class="p">Several studies have shown that vegetation indexes can be used to
estimate root zone soil moisture. Earth surface images, obtained by high-resolution satellites, presently give a lot of information on these
indexes, based on the data of several wavelengths. Because of the potential capacity for
systematic observations at various scales, remote sensing technology extends
the possible data archives from the present time to several decades back.
Because of this advantage, enormous efforts have been made by researchers and
application specialists to delineate vegetation indexes from local scale to
global scale by applying remote sensing imagery.</p><p class="p">In this work, four band images have been considered, which are involved in these
vegetation indexes, and were taken by satellites Ikonos-2 and Landsat-7 of the same
geographic location, to study the effect of both spatial (pixel size) and
radiometric (number of bits coding the image) resolution on these wavelength
bands as well as two vegetation indexes: the Normalized Difference
Vegetation Index (NDVI) and the Enhanced Vegetation Index (EVI).</p><p class="p">In order to do so, a multi-fractal analysis of these multi-spectral images
was applied in each of these bands and the two indexes derived. The results
showed that spatial resolution has a similar scaling effect in the four
bands, but radiometric resolution has a larger influence in blue and green
bands than in red and near-infrared bands. The NDVI showed a higher
sensitivity to the radiometric resolution than EVI. Both were equally
affected by the spatial resolution.</p><p class="p">From both factors, the spatial resolution has a major impact in the
multi-fractal spectrum for all the bands and the vegetation indexes. This
information should be taken in to account when vegetation indexes based on
different satellite sensors are obtained.</p></abstract-html>
<ref-html id="bib1.bib1"><label>1</label><mixed-citation>
Aguado, P. L., Del Monte, J. P., Moratiel, R., and Tarquis, A. M.: Spatial
Characterization of Landscapes through Multifractal Analysis of DEM, The
Scientific World Journal, 2014, 563038, <a href="http://dx.doi.org/10.1155/2014/563038" target="_blank">doi:10.1155/2014/563038</a>, 2014.
</mixed-citation></ref-html>
<ref-html id="bib1.bib2"><label>2</label><mixed-citation>
Andraud, C., Beghdadi, A., and Lafait, J.: Entropic analysis of morphologies,
Physica A, 207, 208–212, 1994.
</mixed-citation></ref-html>
<ref-html id="bib1.bib3"><label>3</label><mixed-citation>
Beaulieu, A. and Gaonac'h, H.: Scaling of differentially eroded surfaces in
the drainage network of the Ethiopian plateau, Remote Sens. Environ., 82,
111–122, 2002.
</mixed-citation></ref-html>
<ref-html id="bib1.bib4"><label>4</label><mixed-citation>
Ben-Ze'ev, E., Karnieli, A., Agam, N., Kaufman, Y., and Holben, B.: Assessing
Vegetation Condition In The Presence Of Biomass Burning Smoke By Applying
The Aerosol-Free Vegetation Index (AFRI) On MODIS Images, Int.
J. Remote Sens., 27, 3203–3221, 2006.
</mixed-citation></ref-html>
<ref-html id="bib1.bib5"><label>5</label><mixed-citation>
Carlson, T. N. and Ripley, D. A.: On the relation between NDVI, Fractional
Vegetation Cover, and Leaf Area Index, Remote Sens. Environ., 62,
241–252, 1997.
</mixed-citation></ref-html>
<ref-html id="bib1.bib6"><label>6</label><mixed-citation>
Cheng, Q.: A new model for quantifying anisotropic scale invariance and for
decomposition of mixing patterns, Math. Geol., 36, 345–360, 2004.
</mixed-citation></ref-html>
<ref-html id="bib1.bib7"><label>7</label><mixed-citation>
Cheng, Q. and Agterberg, F. P.: Multifractal modelling and spatial
statistics, Mathematical Geology, 28, 1–16, 1996.
</mixed-citation></ref-html>
<ref-html id="bib1.bib8"><label>8</label><mixed-citation>
De Cola, L.: Fractal analysis of a classified Landsat-7 scene,
Photogrammetric Engineering and Remote Sensing, 55, 601–610, 1989.
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