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  <front>
    <journal-meta>
<journal-id journal-id-type="publisher">AMT</journal-id>
<journal-title-group>
<journal-title>Atmospheric Measurement Techniques</journal-title>
<abbrev-journal-title abbrev-type="publisher">AMT</abbrev-journal-title>
<abbrev-journal-title abbrev-type="nlm-ta">Atmos. Meas. Tech.</abbrev-journal-title>
</journal-title-group>
<issn pub-type="epub">1867-8548</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/amt-10-2413-2017</article-id><title-group><article-title><?xmltex \hack{\vspace{3mm}}?>Improved pointing information for SCIAMACHY from in-flight measurements
of the viewing  directions towards sun and moon</article-title>
      </title-group><?xmltex \runningtitle{Improved pointing for SCIAMACHY}?><?xmltex \runningauthor{K. Bramstedt et al.}?>
      <contrib-group>
        <contrib contrib-type="author" corresp="yes" rid="aff1">
          <name><surname>Bramstedt</surname><given-names>Klaus</given-names></name>
          <email>klaus.bramstedt@uni-bremen.de</email>
        <ext-link>https://orcid.org/0000-0003-0941-6937</ext-link></contrib>
        <contrib contrib-type="author" corresp="no" rid="aff2">
          <name><surname>Stone</surname><given-names>Thomas C.</given-names></name>
          
        </contrib>
        <contrib contrib-type="author" corresp="no" rid="aff3">
          <name><surname>Gottwald</surname><given-names>Manfred</given-names></name>
          
        </contrib>
        <contrib contrib-type="author" corresp="no" rid="aff1">
          <name><surname>Noël</surname><given-names>Stefan</given-names></name>
          
        <ext-link>https://orcid.org/0000-0002-5216-9110</ext-link></contrib>
        <contrib contrib-type="author" corresp="no" rid="aff1">
          <name><surname>Bovensmann</surname><given-names>Heinrich</given-names></name>
          
        <ext-link>https://orcid.org/0000-0001-8882-4108</ext-link></contrib>
        <contrib contrib-type="author" corresp="no" rid="aff1">
          <name><surname>Burrows</surname><given-names>John P.</given-names></name>
          
        <ext-link>https://orcid.org/0000-0003-1547-8130</ext-link></contrib>
        <aff id="aff1"><label>1</label><institution>University of Bremen, Institute of Environmental Physics (IUP), Otto-Hahn-Allee 1, 28359 Bremen, Germany</institution>
        </aff>
        <aff id="aff2"><label>2</label><institution>US Geological Survey, 2255 North Gemini Drive, Flagstaff, AZ 86001, USA</institution>
        </aff>
        <aff id="aff3"><label>3</label><institution>German Aerospace Center, Remote Sensing Technology Institute, Münchner Str. 20, 82234 Wessling, Germany</institution>
        </aff>
      </contrib-group>
      <author-notes><corresp id="corr1">Klaus Bramstedt (klaus.bramstedt@uni-bremen.de)</corresp></author-notes><pub-date><day>5</day><month>July</month><year>2017</year></pub-date>
      
      <volume>10</volume>
      <issue>7</issue>
      <fpage>2413</fpage><lpage>2423</lpage>
      <history>
        <date date-type="received"><day>6</day><month>December</month><year>2016</year></date>
           <date date-type="rev-request"><day>9</day><month>January</month><year>2017</year></date>
           <date date-type="rev-recd"><day>29</day><month>May</month><year>2017</year></date>
           <date date-type="accepted"><day>29</day><month>May</month><year>2017</year></date>
      </history>
      <permissions>
<license license-type="open-access">
<license-p>This work is licensed under the Creative Commons Attribution 3.0 Unported License. To view a copy of this licence, visit <ext-link ext-link-type="uri" xlink:href="https://creativecommons.org/licenses/by/3.0/">https://creativecommons.org/licenses/by/3.0/</ext-link></license-p>
</license>
</permissions><self-uri xlink:href="https://amt.copernicus.org/articles/10/2413/2017/amt-10-2413-2017.html">This article is available from https://amt.copernicus.org/articles/10/2413/2017/amt-10-2413-2017.html</self-uri>
<self-uri xlink:href="https://amt.copernicus.org/articles/10/2413/2017/amt-10-2413-2017.pdf">The full text article is available as a PDF file from https://amt.copernicus.org/articles/10/2413/2017/amt-10-2413-2017.pdf</self-uri>


      <abstract>
    <p>The SCanning Imaging Absorption spectroMeter for Atmospheric
CHartographY
(SCIAMACHY) on Envisat (2002–2012) performed nadir, limb, solar/lunar
occultation and various monitoring measurements. The pointing information of
the instrument is determined by the attitude information of the Envisat
platform with its star trackers together with the encoder readouts of both
the azimuth and the elevation scanner of SCIAMACHY.</p>
    <p>In this work, we present additional sources of attitude information from the
SCIAMACHY measurements itself. The basic principle is the same as used by
the star tracker: we measure the viewing direction towards celestial
objects, i.e. sun and moon, to detect possible mispointings.</p>
    <p>In sun over limb port observations, we utilise the vertical scans over the
solar disk. In horizontal direction, SCIAMACHY's sun follower device (SFD)
is used to adjust the viewing direction. Moon over limb port measurements
use for both the vertical and the horizontal direction the adjustment by the
SFD. The viewing direction is steered towards the intensity centroid of the
illuminated part of the lunar disk. We use reference images from the USGS
Robotic Lunar Observatory (ROLO) to take into account the inhomogeneous
surface and the variations by lunar libration and phase to parameterise the
location of the intensity centroid from the observation geometry.
Solar observations through SCIAMACHY's so-called sub-solar port (with a
viewing direction closely to zenith) also use the
SFD in the vertical direction. In the horizontal direction the geometry of the port defines the viewing
direction.</p>
    <p>Using these three type of measurements, we fit improved mispointing
parameters by minimising the pointing offsets in elevation and azimuth. The
geolocation of all retrieved products will benefit from this; the
tangent heights are especially improved. The altitudes assigned to SCIAMACHY's solar
occultation measurements are changed in the range of <inline-formula><mml:math id="M1" display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>130 to <inline-formula><mml:math id="M2" display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>330 m, the lunar occultation
measurements are changed in the range of 0 to <inline-formula><mml:math id="M3" display="inline"><mml:mo>+</mml:mo></mml:math></inline-formula>130 m
and the limb measurements are changed in the range of <inline-formula><mml:math id="M4" display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>50 to
<inline-formula><mml:math id="M5" display="inline"><mml:mo>+</mml:mo></mml:math></inline-formula>60 m (depending on season, altitude and azimuth angle). The horizontal
location of the tangent point is changed by about
5 km for all measurements. These updates are implemented in version 9 of the SCIAMACHY Level 1b
products and Level 2 version 7 (based on L1b version 9).</p>
  </abstract>
    </article-meta>
  </front>
<body>
      

<sec id="Ch1.S1" sec-type="intro">
  <title>Introduction</title>
      <p>Satellite measurements allow global observations of atmospheric constituents.
Passive remote sensing instruments use three basic types of geometry:
nadir, limb and occultation.  Critical point in the latter two is always the
pointing knowledge, i.e. the precise knowledge of the viewing direction
and with that the altitude grid of the observations.</p>
      <p>SCIAMACHY (SCanning Imaging Absorption spectroMeter for Atmospheric CHartographY)
is a passive remote sensing moderate-resolution imaging
ultraviolet–visible–near-infrared
spectrometer on board the European Space Agency's (ESA) Environmental
Satellite (Envisat). Envisat was launched in March 2002 from Kourou, French
Guiana, to a sun-synchronous orbit, where it accomplished a successful 10-year
mission. In April 2012, the mission ended due to a platform malfunction.
SCIAMACHY observes Earth's atmosphere in nadir, limb and solar/lunar
occultation geometries and provides column and profile information of
atmospheric parameters of relevance to ozone chemistry, air pollution and
climate monitoring issues <xref ref-type="bibr" rid="bib1.bibx4 bib1.bibx2 bib1.bibx6" id="paren.1"/>.</p>
      <p>SCIAMACHY's solar occultation measurements are done in the Northern Hemisphere,
when the sun rises due to the orbital motion of the platform.
On the day side of the orbit, alternating limb and nadir measurements are
performed. The same air masses are probed first in limb and a few minutes
later in nadir. Lunar occultation is made in the Southern Hemisphere, if the
waxing moon with a phase larger than 0.5 is in the field of view and the moon
rise occurs after sunset. Dark current measurements are performed
during eclipse. Various types of monitoring measurements are executed in the
daily, weekly and monthly calibration periods.</p>
      <p>The pointing information for the instrument is derived from the attitude
information of the platform, which itself is calibrated using the three star
trackers of Envisat. Here, we use SCIAMACHY's own measurements to further improve
the pointing knowledge.  In <xref ref-type="bibr" rid="bib1.bibx3" id="text.2"/>, precise pointing knowledge
has been derived for SCIAMACHY's solar occultation measurements. It used the sun
over limb port measurements, which are the solar occultation measurements
continued above the atmosphere.  In this work, we will additionally use the
moon over limb port measurements and the sun over sub-solar port observations
to derive further pointing information. The viewing direction of the
instrument towards the sun or moon is derived from these measurements. From the
attitude information of the platform, the viewing direction towards sun or
moon is calculated. Systematic differences between the measured and the
calculated viewing directions indicate a mispointing.  Appropriate mispointing
parameters are needed, which improve the attitude information of the platform and
the SCIAMACHY line of sight information.</p>
      <p>The first set of in-flight mispointing parameters has been derived in 2007 by
<xref ref-type="bibr" rid="bib1.bibx7" id="text.3"/>, used in SCIAMACHY data products (re-)processed since
2010. Priority was minimising the large tangent height offsets of
about 1 km observed in the limb measurements. The sun over limb port and over
sub-solar port measurements were used for this. In <xref ref-type="bibr" rid="bib1.bibx3" id="text.4"/>, a
remaining systematic offset in tangent height of 280 m, a horizontal offset
of 5 km and seasonal pattern in both offsets have been shown for solar occultation
data.</p>
      <p>In this work, the combination of the pointing measurements from all three
measurement types listed above is used for fitting new mispointing parameters,
which further improve the pointing accuracy for all SCIAMACHY measurements.</p>
      <p>Section <xref ref-type="sec" rid="Ch1.S2"/> introduces the quantities and the parts of the instrument relevant
for this work. The relevant measurement types are described in
Sect. <xref ref-type="sec" rid="Ch1.S3"/>. The variability of the lunar disk needs special care as
described in Sect. <xref ref-type="sec" rid="Ch1.S4"/>. Finally, all measurements are utilised to
derive improved mispointing parameters in Sect. <xref ref-type="sec" rid="Ch1.S5"/>. Appendices A and C add technical details of the algorithm. Appendix B lists the
important abbreviations used throughout this paper for the reader's
convenience.</p>
</sec>
<sec id="Ch1.S2">
  <title>The instrument</title>
<sec id="Ch1.S2.SS1">
  <title>Coordinate systems</title>

      <?xmltex \floatpos{t}?><fig id="Ch1.F1"><caption><p>Sketch defining the attitude angles (roll, pitch, yaw) and the
viewing angles
(azimuth, elevation).</p></caption>
          <?xmltex \igopts{width=236.157874pt}?><graphic xlink:href="https://amt.copernicus.org/articles/10/2413/2017/amt-10-2413-2017-f01.pdf"/>

        </fig>

      <p>Envisat's orbit and viewing geometry can be described in various coordinate
systems, as defined in <xref ref-type="bibr" rid="bib1.bibx1" id="text.5"/>. The primary platform fixed
coordinate system is Envisat's Satellite Relative Reference coordinate
system. A possible misalignment between platform and instrument is described
by a set of three mispointing angles. They define the consecutive rotations in
roll, pitch and yaw to transform Satellite Relative Reference coordinate
system to the Satellite Relative Actual Reference (SRAR) coordinate
system. Initial mispointing angles for the SCIAMACHY instrument were already
determined in the on-ground calibration.</p>
      <p>The instrument's viewing direction is expressed as azimuth and elevation angle in the SRAR
coordinate system. Figure <xref ref-type="fig" rid="Ch1.F1"/> shows a sketch of these quantities.</p>
</sec>
<sec id="Ch1.S2.SS2">
  <title>The scanner unit</title>

      <?xmltex \floatpos{t}?><fig id="Ch1.F2"><caption><p>Schematic sketch of SCIAMACHY's scanner unit. The yellow beam
follows the
limb light path.</p></caption>
          <?xmltex \igopts{width=236.157874pt}?><graphic xlink:href="https://amt.copernicus.org/articles/10/2413/2017/amt-10-2413-2017-f02.pdf"/>

        </fig>

      <p>The scan mirror system comprises the elevation scan mechanism (ESM) and the azimuth
scan mechanism (ASM). Both scan mechanisms have on one side an aluminium
mirror and on the other side a diffuser for the nominal solar measurements.
Figure <xref ref-type="fig" rid="Ch1.F2"/> is a schematic sketch of the orientation
of the scanners. The ESM rotates parallel to the roll axis of the instrument,
whereas the ASM rotates parallel to the yaw axis. For the nominal nadir
measurements, only the ESM is used. For limb and occultation measurements,
both mirrors are needed, as shown in Fig. <xref ref-type="fig" rid="Ch1.F2"/>. The position of ESM
and ASM (if used) defines the actual viewing direction of the instrument.</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F3"><caption><p>Sun over limb port measurement sequence.  <bold>(b)</bold> In elevation, the
solar disk (yellow area) is scanned by movements of the ESM mirror (blue
line), which overall follows the rising sun. In total, 36 scans are usable
for the pointing investigations. <bold>(a)</bold> By fitting the maximum intensity in
each scan, the elevation angle of the centre of sun is measured for the
time of maximum intensity.</p></caption>
          <?xmltex \igopts{width=236.157874pt}?><graphic xlink:href="https://amt.copernicus.org/articles/10/2413/2017/amt-10-2413-2017-f03.pdf"/>

        </fig>

      <?xmltex \floatpos{t}?><fig id="Ch1.F4"><caption><p>Sun over sub-solar port measurement sequence. <bold>(b)</bold> After an
initial phase of waiting for the sun, the SFD tracks the sun in
elevation. <bold>(a)</bold> The ASM mirror is not in the light path. The azimuth angle
of the solar disk is changed by the orbital motion of the platform. At
maximum intensity, the azimuth angle is 270<inline-formula><mml:math id="M6" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> because that is the viewing
direction of the sub-solar port in azimuth.</p></caption>
          <?xmltex \igopts{width=236.157874pt}?><graphic xlink:href="https://amt.copernicus.org/articles/10/2413/2017/amt-10-2413-2017-f04.pdf"/>

        </fig>

      <?xmltex \floatpos{t}?><fig id="Ch1.F5"><caption><p>Moon over limb port measurement sequence. The moon is tracked for
2 s with the SFD in both elevation and azimuth
direction. The following scans over the lunar disk are not used here.</p></caption>
          <?xmltex \igopts{width=236.157874pt}?><graphic xlink:href="https://amt.copernicus.org/articles/10/2413/2017/amt-10-2413-2017-f05.pdf"/>

        </fig>

</sec>
<sec id="Ch1.S2.SS3">
  <title>The detectors</title>
      <p>The spectrometer has eight detector modules with 1024 detector pixels each,
covering the ultraviolet, visible and near-infrared spectral range.  Seven
broadband detectors, the polarisation measurement devices (PMDs), are used to
determine the polarisation state of the incoming light. PMDs 1–6 measure the
light polarised perpendicular to SCIAMACHY's optical plane. PMD 7 is sensitive to
the 45<inline-formula><mml:math id="M7" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> component in the visible spectral range.  The PMDs are sampling
devices, whereas the spectral detectors are integrating devices.  The PMDs
provide with 40 Hz the highest readout frequency.  Here, we use only PMD 4
(800–900 nm) to measure the intensity, as in <xref ref-type="bibr" rid="bib1.bibx3" id="text.6"/>.</p>
</sec>
<sec id="Ch1.S2.SS4">
  <title>The viewing ports</title>
      <p>The limb port is opened in flight direction towards Earth's
horizon. It is used for SCIAMACHY's limb and occultation
measurements. Both scan mirrors are used to adjust the viewing
direction in elevation and azimuth.</p>
      <p>The nadir port allows a downward viewing direction for SCIAMACHY's nadir
measurement. Only the ESM mirror is used for this viewing
direction.</p>
      <p>The so-called sub-solar port is directed upwards, about 29<inline-formula><mml:math id="M8" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> off the zenith. The
sun is observed through this port to monitor the nadir light path, and therefore
only the ESM is used in the sub-solar measurements. The azimuth of the viewing
direction is fixed at 270<inline-formula><mml:math id="M9" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> by the opening of the port.</p>
</sec>
<sec id="Ch1.S2.SS5">
  <title>SCIAMACHY's sun follower device (SFD)</title>
      <p>The SFD can be used to steer the instrument's line of
sight towards the central part of the intensity distribution of the sun or the
moon, referred to in the following as intensity centroid (IC).
The SFD is a four-quadrant sensor and detects the sun or the moon
in a 2.2<inline-formula><mml:math id="M10" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> <inline-formula><mml:math id="M11" display="inline"><mml:mo>×</mml:mo></mml:math></inline-formula> 2.2<inline-formula><mml:math id="M12" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> wide field. The image of the sun or moon is
reflected from the polished blades of the spectrometer entrance slit onto the
SFD. The SFD detector has a broadband sensitivity centred around 500 nm.</p>
</sec>
</sec>
<sec id="Ch1.S3">
  <title>Measurements</title>
      <p>Three types of measurements are used to derive additional pointing
information: the sun and moon observed through the limb port (the solar/lunar
occultation measurements at atmospheric tangent heights) and the sun observed
through the sub-solar port. Due to observing geometry defined by the orbit and
the viewing ports, sun over limb port is performed above the Northern Hemisphere,
moon over limb port above the Southern Hemisphere and the sun over sub-solar
port above the equatorial region.</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F6"><caption><p>The 15 ROLO reference images. The white lines mark the boundaries of the four
quadrants in the SFD simulation after adjustment. The images are listed
in Table <xref ref-type="table" rid="Ch1.T1"/> from top left to bottom right.</p></caption>
        <?xmltex \igopts{width=241.848425pt}?><graphic xlink:href="https://amt.copernicus.org/articles/10/2413/2017/amt-10-2413-2017-f06.pdf"/>

      </fig>

      <p>The sun over limb port measurement (Fig. <xref ref-type="fig" rid="Ch1.F3"/>) follows the rising
sun, performing vertical scans over the solar disk. The viewing direction
towards the centre of the sun in elevation is determined by fitting the
maximum intensity during the scan. In azimuth, the sun is tracked with the
SFD. Details are given in <xref ref-type="bibr" rid="bib1.bibx3" id="text.7"/>. Sun over limb port is the
upper part of the solar occultation measurement performed every orbit. Once
per day, a shortened solar occultation measurement is performed, which ends
with a 2 s period with tracking by the SFD also in elevation. The difference
between the two methods is below 1 mdeg <xref ref-type="bibr" rid="bib1.bibx3" id="paren.8"/>.</p>

<?xmltex \floatpos{t}?><table-wrap id="Ch1.T1" specific-use="star"><caption><p>The ROLO reference images with sub-observer and sub-solar point
coordinates and the lunar phase as illumination in percent. The intensity
centroid “IC image” is determined from the SFD simulation. The “IC parameter” is
calculated with the fitted parameters. The distance in degree between the two ICs
is given in the last two columns. The distance standard deviation in
latitude is 0.51<inline-formula><mml:math id="M13" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> and in longitude is 0.42<inline-formula><mml:math id="M14" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula>.</p></caption><oasis:table frame="topbot"><?xmltex \begin{scaleboxenv}{.9}[.9]?><oasis:tgroup cols="14">
     <oasis:colspec colnum="1" colname="col1" align="left"/>
     <oasis:colspec colnum="2" colname="col2" align="left"/>
     <oasis:colspec colnum="3" colname="col3" align="right" colsep="1"/>
     <oasis:colspec colnum="4" colname="col4" align="right"/>
     <oasis:colspec colnum="5" colname="col5" align="right" colsep="1"/>
     <oasis:colspec colnum="6" colname="col6" align="right"/>
     <oasis:colspec colnum="7" colname="col7" align="right"/>
     <oasis:colspec colnum="8" colname="col8" align="right"/>
     <oasis:colspec colnum="9" colname="col9" align="right"/>
     <oasis:colspec colnum="10" colname="col10" align="right" colsep="1"/>
     <oasis:colspec colnum="11" colname="col11" align="right"/>
     <oasis:colspec colnum="12" colname="col12" align="right" colsep="1"/>
     <oasis:colspec colnum="13" colname="col13" align="right"/>
     <oasis:colspec colnum="14" colname="col14" align="right"/>
     <oasis:thead>
       <oasis:row>  
         <oasis:entry colname="col1">Image</oasis:entry>  
         <oasis:entry rowsep="1" namest="col2" nameend="col3" align="center" colsep="1">Measurement time </oasis:entry>  
         <oasis:entry rowsep="1" namest="col4" nameend="col5" align="center" colsep="1">Sub-observer </oasis:entry>  
         <oasis:entry rowsep="1" namest="col6" nameend="col7" align="center">Sub-solar </oasis:entry>  
         <oasis:entry colname="col8">Illum.</oasis:entry>  
         <oasis:entry rowsep="1" namest="col9" nameend="col10" align="center" colsep="1">IC image </oasis:entry>  
         <oasis:entry rowsep="1" namest="col11" nameend="col12" align="center" colsep="1">IC parameter </oasis:entry>  
         <oasis:entry rowsep="1" namest="col13" nameend="col14" align="center">IC distance </oasis:entry>
       </oasis:row>
       <oasis:row rowsep="1">  
         <oasis:entry colname="col1"/>  
         <oasis:entry colname="col2"/>  
         <oasis:entry colname="col3"/>  
         <oasis:entry colname="col4">long</oasis:entry>  
         <oasis:entry colname="col5">lat</oasis:entry>  
         <oasis:entry colname="col6">long</oasis:entry>  
         <oasis:entry colname="col7">lat</oasis:entry>  
         <oasis:entry colname="col8">(%)</oasis:entry>  
         <oasis:entry colname="col9">long</oasis:entry>  
         <oasis:entry colname="col10">lat</oasis:entry>  
         <oasis:entry colname="col11">long</oasis:entry>  
         <oasis:entry colname="col12">lat</oasis:entry>  
         <oasis:entry colname="col13">long</oasis:entry>  
         <oasis:entry colname="col14">lat</oasis:entry>
       </oasis:row>
     </oasis:thead>
     <oasis:tbody>
       <oasis:row>  
         <oasis:entry colname="col1">mm194311</oasis:entry>  
         <oasis:entry colname="col2">10-May-1998</oasis:entry>  
         <oasis:entry colname="col3">08:46:21</oasis:entry>  
         <oasis:entry colname="col4"><inline-formula><mml:math id="M15" display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>2.04</oasis:entry>  
         <oasis:entry colname="col5"><inline-formula><mml:math id="M16" display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>4.89</oasis:entry>  
         <oasis:entry colname="col6">11.90</oasis:entry>  
         <oasis:entry colname="col7"><inline-formula><mml:math id="M17" display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>1.51</oasis:entry>  
         <oasis:entry colname="col8">98.448</oasis:entry>  
         <oasis:entry colname="col9">5.70</oasis:entry>  
         <oasis:entry colname="col10"><inline-formula><mml:math id="M18" display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>10.04</oasis:entry>  
         <oasis:entry colname="col11">5.87</oasis:entry>  
         <oasis:entry colname="col12"><inline-formula><mml:math id="M19" display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>9.58</oasis:entry>  
         <oasis:entry colname="col13"><inline-formula><mml:math id="M20" display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>0.16</oasis:entry>  
         <oasis:entry colname="col14"><inline-formula><mml:math id="M21" display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>0.45</oasis:entry>
       </oasis:row>
       <oasis:row>  
         <oasis:entry colname="col1">mm194403</oasis:entry>  
         <oasis:entry colname="col2">11-May-1998</oasis:entry>  
         <oasis:entry colname="col3">05:49:54</oasis:entry>  
         <oasis:entry colname="col4"><inline-formula><mml:math id="M22" display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>2.41</oasis:entry>  
         <oasis:entry colname="col5"><inline-formula><mml:math id="M23" display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>5.59</oasis:entry>  
         <oasis:entry colname="col6">1.21</oasis:entry>  
         <oasis:entry colname="col7"><inline-formula><mml:math id="M24" display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>1.52</oasis:entry>  
         <oasis:entry colname="col8">99.775</oasis:entry>  
         <oasis:entry colname="col9">1.44</oasis:entry>  
         <oasis:entry colname="col10"><inline-formula><mml:math id="M25" display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>10.04</oasis:entry>  
         <oasis:entry colname="col11">1.55</oasis:entry>  
         <oasis:entry colname="col12"><inline-formula><mml:math id="M26" display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>10.18</oasis:entry>  
         <oasis:entry colname="col13"><inline-formula><mml:math id="M27" display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>0.11</oasis:entry>  
         <oasis:entry colname="col14">0.14</oasis:entry>
       </oasis:row>
       <oasis:row>  
         <oasis:entry colname="col1">mm194407</oasis:entry>  
         <oasis:entry colname="col2">11-May-1998</oasis:entry>  
         <oasis:entry colname="col3">07:52:51</oasis:entry>  
         <oasis:entry colname="col4"><inline-formula><mml:math id="M28" display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>2.87</oasis:entry>  
         <oasis:entry colname="col5"><inline-formula><mml:math id="M29" display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>5.51</oasis:entry>  
         <oasis:entry colname="col6">0.17</oasis:entry>  
         <oasis:entry colname="col7"><inline-formula><mml:math id="M30" display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>1.52</oasis:entry>  
         <oasis:entry colname="col8">99.809</oasis:entry>  
         <oasis:entry colname="col9">1.06</oasis:entry>  
         <oasis:entry colname="col10"><inline-formula><mml:math id="M31" display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>10.33</oasis:entry>  
         <oasis:entry colname="col11">0.87</oasis:entry>  
         <oasis:entry colname="col12"><inline-formula><mml:math id="M32" display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>10.11</oasis:entry>  
         <oasis:entry colname="col13">0.20</oasis:entry>  
         <oasis:entry colname="col14"><inline-formula><mml:math id="M33" display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>0.22</oasis:entry>
       </oasis:row>
       <oasis:row>  
         <oasis:entry colname="col1">mm194411</oasis:entry>  
         <oasis:entry colname="col2">11-May-1998</oasis:entry>  
         <oasis:entry colname="col3">09:51:13</oasis:entry>  
         <oasis:entry colname="col4"><inline-formula><mml:math id="M34" display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>3.29</oasis:entry>  
         <oasis:entry colname="col5"><inline-formula><mml:math id="M35" display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>5.48</oasis:entry>  
         <oasis:entry colname="col6"><inline-formula><mml:math id="M36" display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>0.83</oasis:entry>  
         <oasis:entry colname="col7"><inline-formula><mml:math id="M37" display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>1.52</oasis:entry>  
         <oasis:entry colname="col8">99.834</oasis:entry>  
         <oasis:entry colname="col9">0.78</oasis:entry>  
         <oasis:entry colname="col10"><inline-formula><mml:math id="M38" display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>10.35</oasis:entry>  
         <oasis:entry colname="col11">0.22</oasis:entry>  
         <oasis:entry colname="col12"><inline-formula><mml:math id="M39" display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>10.09</oasis:entry>  
         <oasis:entry colname="col13">0.56</oasis:entry>  
         <oasis:entry colname="col14"><inline-formula><mml:math id="M40" display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>0.26</oasis:entry>
       </oasis:row>
       <oasis:row>  
         <oasis:entry colname="col1">mm197401</oasis:entry>  
         <oasis:entry colname="col2">10-Jun-1998</oasis:entry>  
         <oasis:entry colname="col3">05:54:53</oasis:entry>  
         <oasis:entry colname="col4"><inline-formula><mml:math id="M41" display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>4.11</oasis:entry>  
         <oasis:entry colname="col5"><inline-formula><mml:math id="M42" display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>5.64</oasis:entry>  
         <oasis:entry colname="col6"><inline-formula><mml:math id="M43" display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>5.28</oasis:entry>  
         <oasis:entry colname="col7"><inline-formula><mml:math id="M44" display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>1.53</oasis:entry>  
         <oasis:entry colname="col8">99.861</oasis:entry>  
         <oasis:entry colname="col9"><inline-formula><mml:math id="M45" display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>2.36</oasis:entry>  
         <oasis:entry colname="col10"><inline-formula><mml:math id="M46" display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>10.76</oasis:entry>  
         <oasis:entry colname="col11"><inline-formula><mml:math id="M47" display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>1.98</oasis:entry>  
         <oasis:entry colname="col12"><inline-formula><mml:math id="M48" display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>10.23</oasis:entry>  
         <oasis:entry colname="col13"><inline-formula><mml:math id="M49" display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>0.38</oasis:entry>  
         <oasis:entry colname="col14"><inline-formula><mml:math id="M50" display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>0.53</oasis:entry>
       </oasis:row>
       <oasis:row>  
         <oasis:entry colname="col1">mm197403</oasis:entry>  
         <oasis:entry colname="col2">10-Jun-1998</oasis:entry>  
         <oasis:entry colname="col3">06:52:47</oasis:entry>  
         <oasis:entry colname="col4"><inline-formula><mml:math id="M51" display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>4.31</oasis:entry>  
         <oasis:entry colname="col5"><inline-formula><mml:math id="M52" display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>5.60</oasis:entry>  
         <oasis:entry colname="col6"><inline-formula><mml:math id="M53" display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>5.77</oasis:entry>  
         <oasis:entry colname="col7"><inline-formula><mml:math id="M54" display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>1.53</oasis:entry>  
         <oasis:entry colname="col8">99.858</oasis:entry>  
         <oasis:entry colname="col9"><inline-formula><mml:math id="M55" display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>2.49</oasis:entry>  
         <oasis:entry colname="col10"><inline-formula><mml:math id="M56" display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>10.76</oasis:entry>  
         <oasis:entry colname="col11"><inline-formula><mml:math id="M57" display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>2.29</oasis:entry>  
         <oasis:entry colname="col12"><inline-formula><mml:math id="M58" display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>10.19</oasis:entry>  
         <oasis:entry colname="col13"><inline-formula><mml:math id="M59" display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>0.20</oasis:entry>  
         <oasis:entry colname="col14"><inline-formula><mml:math id="M60" display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>0.57</oasis:entry>
       </oasis:row>
       <oasis:row>  
         <oasis:entry colname="col1">mm212109</oasis:entry>  
         <oasis:entry colname="col2">04-Nov-1998</oasis:entry>  
         <oasis:entry colname="col3">06:42:59</oasis:entry>  
         <oasis:entry colname="col4">0.65</oasis:entry>  
         <oasis:entry colname="col5">6.74</oasis:entry>  
         <oasis:entry colname="col6"><inline-formula><mml:math id="M61" display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>0.15</oasis:entry>  
         <oasis:entry colname="col7">1.47</oasis:entry>  
         <oasis:entry colname="col8">99.784</oasis:entry>  
         <oasis:entry colname="col9">3.48</oasis:entry>  
         <oasis:entry colname="col10">0.14</oasis:entry>  
         <oasis:entry colname="col11">2.92</oasis:entry>  
         <oasis:entry colname="col12">0.69</oasis:entry>  
         <oasis:entry colname="col13">0.55</oasis:entry>  
         <oasis:entry colname="col14"><inline-formula><mml:math id="M62" display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>0.55</oasis:entry>
       </oasis:row>
       <oasis:row>  
         <oasis:entry colname="col1">mm215006</oasis:entry>  
         <oasis:entry colname="col2">03-Dec-1998</oasis:entry>  
         <oasis:entry colname="col3">11:26:07</oasis:entry>  
         <oasis:entry colname="col4">1.51</oasis:entry>  
         <oasis:entry colname="col5">6.69</oasis:entry>  
         <oasis:entry colname="col6">4.58</oasis:entry>  
         <oasis:entry colname="col7">1.47</oasis:entry>  
         <oasis:entry colname="col8">99.721</oasis:entry>  
         <oasis:entry colname="col9">6.06</oasis:entry>  
         <oasis:entry colname="col10">1.11</oasis:entry>  
         <oasis:entry colname="col11">5.26</oasis:entry>  
         <oasis:entry colname="col12">0.65</oasis:entry>  
         <oasis:entry colname="col13">0.80</oasis:entry>  
         <oasis:entry colname="col14">0.46</oasis:entry>
       </oasis:row>
       <oasis:row>  
         <oasis:entry colname="col1">mm218002</oasis:entry>  
         <oasis:entry colname="col2">02-Jan-1999</oasis:entry>  
         <oasis:entry colname="col3">09:45:45</oasis:entry>  
         <oasis:entry colname="col4">4.21</oasis:entry>  
         <oasis:entry colname="col5">4.42</oasis:entry>  
         <oasis:entry colname="col6">0.67</oasis:entry>  
         <oasis:entry colname="col7">1.02</oasis:entry>  
         <oasis:entry colname="col8">99.817</oasis:entry>  
         <oasis:entry colname="col9">5.43</oasis:entry>  
         <oasis:entry colname="col10"><inline-formula><mml:math id="M63" display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>1.93</oasis:entry>  
         <oasis:entry colname="col11">5.43</oasis:entry>  
         <oasis:entry colname="col12"><inline-formula><mml:math id="M64" display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>1.33</oasis:entry>  
         <oasis:entry colname="col13">0.00</oasis:entry>  
         <oasis:entry colname="col14"><inline-formula><mml:math id="M65" display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>0.60</oasis:entry>
       </oasis:row>
       <oasis:row>  
         <oasis:entry colname="col1">mm226801</oasis:entry>  
         <oasis:entry colname="col2">31-Mar-1999</oasis:entry>  
         <oasis:entry colname="col3">08:55:54</oasis:entry>  
         <oasis:entry colname="col4">3.51</oasis:entry>  
         <oasis:entry colname="col5"><inline-formula><mml:math id="M66" display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>3.96</oasis:entry>  
         <oasis:entry colname="col6">10.20</oasis:entry>  
         <oasis:entry colname="col7"><inline-formula><mml:math id="M67" display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>1.24</oasis:entry>  
         <oasis:entry colname="col8">99.604</oasis:entry>  
         <oasis:entry colname="col9">8.29</oasis:entry>  
         <oasis:entry colname="col10"><inline-formula><mml:math id="M68" display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>8.24</oasis:entry>  
         <oasis:entry colname="col11">8.64</oasis:entry>  
         <oasis:entry colname="col12"><inline-formula><mml:math id="M69" display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>8.76</oasis:entry>  
         <oasis:entry colname="col13"><inline-formula><mml:math id="M70" display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>0.35</oasis:entry>  
         <oasis:entry colname="col14">0.52</oasis:entry>
       </oasis:row>
       <oasis:row>  
         <oasis:entry colname="col1">mm244610</oasis:entry>  
         <oasis:entry colname="col2">25-Sep-1999</oasis:entry>  
         <oasis:entry colname="col3">08:45:19</oasis:entry>  
         <oasis:entry colname="col4"><inline-formula><mml:math id="M71" display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>5.15</oasis:entry>  
         <oasis:entry colname="col5">5.45</oasis:entry>  
         <oasis:entry colname="col6"><inline-formula><mml:math id="M72" display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>3.41</oasis:entry>  
         <oasis:entry colname="col7">1.19</oasis:entry>  
         <oasis:entry colname="col8">99.839</oasis:entry>  
         <oasis:entry colname="col9"><inline-formula><mml:math id="M73" display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>1.96</oasis:entry>  
         <oasis:entry colname="col10">0.14</oasis:entry>  
         <oasis:entry colname="col11"><inline-formula><mml:math id="M74" display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>1.91</oasis:entry>  
         <oasis:entry colname="col12"><inline-formula><mml:math id="M75" display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>0.44</oasis:entry>  
         <oasis:entry colname="col13"><inline-formula><mml:math id="M76" display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>0.06</oasis:entry>  
         <oasis:entry colname="col14">0.58</oasis:entry>
       </oasis:row>
       <oasis:row>  
         <oasis:entry colname="col1">mm250509</oasis:entry>  
         <oasis:entry colname="col2">23-Nov-1999</oasis:entry>  
         <oasis:entry colname="col3">06:23:57</oasis:entry>  
         <oasis:entry colname="col4"><inline-formula><mml:math id="M77" display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>1.08</oasis:entry>  
         <oasis:entry colname="col5">6.39</oasis:entry>  
         <oasis:entry colname="col6"><inline-formula><mml:math id="M78" display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>0.85</oasis:entry>  
         <oasis:entry colname="col7">1.40</oasis:entry>  
         <oasis:entry colname="col8">99.810</oasis:entry>  
         <oasis:entry colname="col9">1.70</oasis:entry>  
         <oasis:entry colname="col10">0.26</oasis:entry>  
         <oasis:entry colname="col11">1.58</oasis:entry>  
         <oasis:entry colname="col12">0.39</oasis:entry>  
         <oasis:entry colname="col13">0.12</oasis:entry>  
         <oasis:entry colname="col14"><inline-formula><mml:math id="M79" display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>0.13</oasis:entry>
       </oasis:row>
       <oasis:row>  
         <oasis:entry colname="col1">mm262206</oasis:entry>  
         <oasis:entry colname="col2">19-Mar-2000</oasis:entry>  
         <oasis:entry colname="col3">06:24:17</oasis:entry>  
         <oasis:entry colname="col4">4.31</oasis:entry>  
         <oasis:entry colname="col5"><inline-formula><mml:math id="M80" display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>4.37</oasis:entry>  
         <oasis:entry colname="col6">15.88</oasis:entry>  
         <oasis:entry colname="col7"><inline-formula><mml:math id="M81" display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>1.33</oasis:entry>  
         <oasis:entry colname="col8">98.917</oasis:entry>  
         <oasis:entry colname="col9">11.65</oasis:entry>  
         <oasis:entry colname="col10"><inline-formula><mml:math id="M82" display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>8.79</oasis:entry>  
         <oasis:entry colname="col11">11.31</oasis:entry>  
         <oasis:entry colname="col12"><inline-formula><mml:math id="M83" display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>9.12</oasis:entry>  
         <oasis:entry colname="col13">0.35</oasis:entry>  
         <oasis:entry colname="col14">0.33</oasis:entry>
       </oasis:row>
       <oasis:row>  
         <oasis:entry colname="col1">mm303606</oasis:entry>  
         <oasis:entry colname="col2">07-May-2001</oasis:entry>  
         <oasis:entry colname="col3">07:12:22</oasis:entry>  
         <oasis:entry colname="col4">5.07</oasis:entry>  
         <oasis:entry colname="col5"><inline-formula><mml:math id="M84" display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>4.72</oasis:entry>  
         <oasis:entry colname="col6">8.30</oasis:entry>  
         <oasis:entry colname="col7"><inline-formula><mml:math id="M85" display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>1.21</oasis:entry>  
         <oasis:entry colname="col8">99.827</oasis:entry>  
         <oasis:entry colname="col9">8.23</oasis:entry>  
         <oasis:entry colname="col10"><inline-formula><mml:math id="M86" display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>9.07</oasis:entry>  
         <oasis:entry colname="col11">8.88</oasis:entry>  
         <oasis:entry colname="col12"><inline-formula><mml:math id="M87" display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>9.39</oasis:entry>  
         <oasis:entry colname="col13"><inline-formula><mml:math id="M88" display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>0.65</oasis:entry>  
         <oasis:entry colname="col14">0.32</oasis:entry>
       </oasis:row>
       <oasis:row>  
         <oasis:entry colname="col1">mm303611</oasis:entry>  
         <oasis:entry colname="col2">07-May-2001</oasis:entry>  
         <oasis:entry colname="col3">09:53:02</oasis:entry>  
         <oasis:entry colname="col4">4.62</oasis:entry>  
         <oasis:entry colname="col5"><inline-formula><mml:math id="M89" display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>4.51</oasis:entry>  
         <oasis:entry colname="col6">6.94</oasis:entry>  
         <oasis:entry colname="col7"><inline-formula><mml:math id="M90" display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>1.21</oasis:entry>  
         <oasis:entry colname="col8">99.876</oasis:entry>  
         <oasis:entry colname="col9">7.44</oasis:entry>  
         <oasis:entry colname="col10"><inline-formula><mml:math id="M91" display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>8.24</oasis:entry>  
         <oasis:entry colname="col11">8.08</oasis:entry>  
         <oasis:entry colname="col12"><inline-formula><mml:math id="M92" display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>9.21</oasis:entry>  
         <oasis:entry colname="col13"><inline-formula><mml:math id="M93" display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>0.65</oasis:entry>  
         <oasis:entry colname="col14">0.97</oasis:entry>
       </oasis:row>
     </oasis:tbody>
   </oasis:tgroup><?xmltex \end{scaleboxenv}?></oasis:table></table-wrap>

      <p>Three different sequences for sun over sub-solar port measurement are done.
In the sequence used here, the sun is tracked in
elevation by the SFD (Fig. <xref ref-type="fig" rid="Ch1.F4"/>). The ASM is not involved in this light
path. The sun moves in azimuth direction through the field of view because of
the orbital motion of the satellite. At the maximum intensity during the
measurement, the sun is at 270<inline-formula><mml:math id="M94" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> azimuth angle (the opening direction of the
sub-solar port). This sun over sub-solar port measurement is part of the
monthly calibration. After October 2006, it was scheduled every 3 days.</p>
      <p>The moon over limb port measurement (Fig. <xref ref-type="fig" rid="Ch1.F5"/>) used here is a
monitoring measurement, which is performed well above the atmosphere. In its
first phase, the moon is tracked in azimuth and elevation by the SFD. This
phase is used here. The SFD adjusts the viewing direction towards the
IC of the actual lunar disk. The location of the IC is
discussed in Sect. <xref ref-type="sec" rid="Ch1.S4"/>. This monitoring measurement is performed once
per day, if the moon appears in the field of view. This is the case for about 1 week
per month during the phase of the waxing moon with a lunar phase larger than
0.5. Note: the regular lunar occultation measurements are performed every orbit with
the same restrictions. Additionally, the tangent point has to be at local
night time, limiting the usable period to about 6 months per year.</p>
</sec>
<sec id="Ch1.S4">
  <title>Lunar variability</title>
<sec id="Ch1.S4.SS1">
  <title>Robotic Lunar Observatory (ROLO) reference images</title>
      <p>The ROLO of US Geological Survey (USGS) is located in Flagstaff, Arizona, in
the United States. In 6 years of operation (1997–2003), the observatory has
acquired over 110 000 lunar images. Twin telescopes cover the visible and
near-infrared range (350–950 nm) in 23 bands and the shortwave infrared
(950–2350 nm) in 9 bands <xref ref-type="bibr" rid="bib1.bibx10" id="paren.9"/>. We use the calibrated images
of the 550 nm band, which is the closest band to the sensitivity of the SFD
at 500 nm. Size of the images is 512 <inline-formula><mml:math id="M95" display="inline"><mml:mo>×</mml:mo></mml:math></inline-formula> 512 pixel.</p>
      <p>We simulate the control loop of the SFD to determine the IC for the lunar
images. The image is separated in four quadrants (representing the sectors of
the SFD). The boundaries between the left and right and the upper and lower
part of the images are adjusted until the difference between the left and
right part on the one hand and the upper and lower part on the other hand is
minimised. After this adjustment, the sums over the intensities of the pixels
in each quadrant are equal within the limits of the discretisation. The
determined IC is independent from rotations of the image. After a 90<inline-formula><mml:math id="M96" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula>
rotation, the geometry is repeated because of the sensor symmetry. Taking into
account the mirror symmetry of the sensor at the 45<inline-formula><mml:math id="M97" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> axis, we have to check
only rotations between 0 and 45<inline-formula><mml:math id="M98" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula>. We rotated a high-resolution lunar image
in 5<inline-formula><mml:math id="M99" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> steps from 0 to 45<inline-formula><mml:math id="M100" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> and determined in all cases the same IC
location.</p>
      <p>We determined the IC for 15 ROLO images close to full moon. Figure <xref ref-type="fig" rid="Ch1.F6"/>
shows the images with the boundaries of the quadrants after adjustment. The
cross of the boundaries marks the intensity centre of the moon, where the SFD
will adjust the line of sight.</p>
      <p>From the SFD simulation, we get the location of the IC as pixel position on
the ROLO image. The corresponding lunar coordinates are derived by visual
inspection of a high-resolution lunar image. We used the program
Virtual Moon Atlas Pro V6.0 <xref ref-type="bibr" rid="bib1.bibx11 bib1.bibx12" id="paren.10"/> for
this purpose. Figure <xref ref-type="fig" rid="Ch1.F7"/> shows an example: the
green dot marks the identified location in the Ptolemaeus crater region.</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F7" specific-use="star"><caption><p>An example of the determination of the IC lunar coordinates
with the program Virtual Moon. <bold>(a)</bold> Clipping of the ROLO image “mm194407” including the adjusted boundaries
of the four quadrants in the SFD simulation. <bold>(b)</bold> is panel <bold>(a)</bold> rotated by about 70<inline-formula><mml:math id="M101" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> counter-clockwise to match the orientation of
the moon in Virtual Moon. <bold>(c)</bold> The same area as the
image in Virtual Moon.  The intensity centre in the Ptolemaeus crater
region is marked by the green dot. The shown region in <bold>(b)</bold> and <bold>(a)</bold> corresponds to the one used in Fig. <xref ref-type="fig" rid="Ch1.F8"/>.</p></caption>
          <?xmltex \igopts{width=341.433071pt}?><graphic xlink:href="https://amt.copernicus.org/articles/10/2413/2017/amt-10-2413-2017-f07.pdf"/>

        </fig>

      <?xmltex \floatpos{t}?><fig id="Ch1.F8"><caption><p>Illustration of the IC parameterisation. For each ROLO reference
image, the sub-observer point <inline-formula><mml:math id="M102" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="bold-italic">P</mml:mi><mml:mi mathvariant="normal">sobs</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula>, the sub-solar point <inline-formula><mml:math id="M103" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="bold-italic">P</mml:mi><mml:mi mathvariant="normal">ssol</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> and the IC
location in the ROLO images <inline-formula><mml:math id="M104" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="bold-italic">P</mml:mi><mml:mi mathvariant="normal">icen</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> are plotted onto a grid of lunar
coordinates. The parameterised IC (shown as a cross) is in all
cases close to the observed intensity centre.</p></caption>
          <?xmltex \igopts{width=236.157874pt}?><graphic xlink:href="https://amt.copernicus.org/articles/10/2413/2017/amt-10-2413-2017-f08.pdf"/>

        </fig>

</sec>
<sec id="Ch1.S4.SS2">
  <title>Parameterisation of the lunar intensity centroid</title>
      <p>The observing geometry is defined by the sub-observer point
<inline-formula><mml:math id="M105" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="bold-italic">P</mml:mi><mml:mi mathvariant="normal">sobs</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula>, the intersection of the straight line from the
observer (here Envisat or the ROLO telescope) to the centre of the moon with
the lunar surface. This point defines the visible part of the lunar surface;
its change with time is called the libration of the moon.</p>
      <p>The lunar illumination is defined by the sub-solar point
<inline-formula><mml:math id="M106" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="bold-italic">P</mml:mi><mml:mi mathvariant="normal">ssol</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula>, the intersection of the straight line from the centre of
the sun to the centre of the moon with the lunar surface. The distance between
the  sub-solar point and the sub-observer point determines the illumination of
the visible part of the lunar surface: the lunar phase.</p>
      <p>For the 15 ROLO images, we have calculated  <inline-formula><mml:math id="M107" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="bold-italic">P</mml:mi><mml:mi mathvariant="normal">sobs</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula>,
<inline-formula><mml:math id="M108" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="bold-italic">P</mml:mi><mml:mi mathvariant="normal">ssol</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> (using the HORIZONS software; see Appendix Sect. <xref ref-type="sec" rid="App1.Ch1.S1.SS2"/>)
and determined <inline-formula><mml:math id="M109" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="bold-italic">P</mml:mi><mml:mi mathvariant="normal">icen</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula>. The lunar
coordinates in latitude and longitude of these points are given in
Table <xref ref-type="table" rid="Ch1.T1"/>.</p>
      <p>In Fig. <xref ref-type="fig" rid="Ch1.F8"/> these points are plotted in a Cartesian coordinate
system. We neglected the in principal spherical nature of the problem, because
the deviation to the Cartesian approach is small for regions near the
Equator. The directions and distances between <inline-formula><mml:math id="M110" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="bold-italic">P</mml:mi><mml:mi mathvariant="normal">sobs</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> and <inline-formula><mml:math id="M111" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="bold-italic">P</mml:mi><mml:mi mathvariant="normal">ssol</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> are similar in all
cases and varies depending on the location of <inline-formula><mml:math id="M112" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="bold-italic">P</mml:mi><mml:mi mathvariant="normal">ssol</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula>.  With the following
equation, the location of the <inline-formula><mml:math id="M113" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="bold-italic">P</mml:mi><mml:mi mathvariant="normal">icen</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> can be parameterised:
            <disp-formula id="Ch1.E1" content-type="numbered"><mml:math id="M114" display="block"><mml:mrow><mml:msub><mml:mi mathvariant="bold-italic">P</mml:mi><mml:mi mathvariant="normal">icen</mml:mi></mml:msub><mml:mo>=</mml:mo><mml:msub><mml:mi mathvariant="bold-italic">P</mml:mi><mml:mi mathvariant="normal">sobs</mml:mi></mml:msub><mml:mo>+</mml:mo><mml:mi mathvariant="bold-italic">d</mml:mi><mml:mo>+</mml:mo><mml:mi mathvariant="bold-italic">a</mml:mi><mml:mo>(</mml:mo><mml:msub><mml:mi mathvariant="bold-italic">P</mml:mi><mml:mi mathvariant="normal">ssol</mml:mi></mml:msub><mml:mo>-</mml:mo><mml:msub><mml:mi mathvariant="bold-italic">P</mml:mi><mml:mi mathvariant="normal">sobs</mml:mi></mml:msub><mml:mo>)</mml:mo><mml:mo>.</mml:mo></mml:mrow></mml:math></disp-formula></p>
      <p><inline-formula><mml:math id="M115" display="inline"><mml:mi mathvariant="bold-italic">d</mml:mi></mml:math></inline-formula> is the distance between <inline-formula><mml:math id="M116" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="bold-italic">P</mml:mi><mml:mi mathvariant="normal">sobs</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> and <inline-formula><mml:math id="M117" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="bold-italic">P</mml:mi><mml:mi mathvariant="normal">ssol</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> for full moon, and <inline-formula><mml:math id="M118" display="inline"><mml:mi mathvariant="bold-italic">a</mml:mi></mml:math></inline-formula>
parameterises the movement of the IC due to the lunar phase.
All terms in Eq. (<xref ref-type="disp-formula" rid="Ch1.E1"/>) are two-element vectors with the lunar coordinates
in longitude and latitude.</p>
      <p><inline-formula><mml:math id="M119" display="inline"><mml:mi mathvariant="bold-italic">d</mml:mi></mml:math></inline-formula> and <inline-formula><mml:math id="M120" display="inline"><mml:mi mathvariant="bold-italic">a</mml:mi></mml:math></inline-formula> are fitted by minimising the distances between the
parameterised and the observed ICs. The fitted parameters are given in
Table <xref ref-type="table" rid="Ch1.T2"/>. In Fig. <xref ref-type="fig" rid="Ch1.F8"/>, the crosses show the
parameterised ICs. With the parameterisation of Eq. (<xref ref-type="disp-formula" rid="Ch1.E1"/>), we can
calculate the IC for all lunar observations close to full moon from the observing geometry only.</p>
      <p>The uncertainty of the IC location depends on three components. First, the
ROLO reference images have a resolution of 512 <inline-formula><mml:math id="M121" display="inline"><mml:mo>×</mml:mo></mml:math></inline-formula> 512 pixels.
Each image pixel has an instantaneous field of view of 1.13 mdeg (measured
precisely from astrometry of star fields). This pixel width is the uncertainty
for the location of the IC.  Second, the
parameterised IC matches not exactly the IC of the image. The standard
deviation of the distances between these two ICs in lunar longitude and latitude
is 0.43<inline-formula><mml:math id="M122" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> and 0.51<inline-formula><mml:math id="M123" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula>, respectively. This lunar coordinate's standard
deviation corresponds to a 2.3 mdeg standard deviation of the viewing angle at the satellite.
Third, we have the pointing precision of the SFD of
1 mdeg as estimated in <xref ref-type="bibr" rid="bib1.bibx3" id="text.11"/>. Adding up the three error
sources as root of the summed squares of the error, we roughly
estimate the uncertainty in the viewing angle to 2.8 mdeg. In elevation, this
corresponds to a tangent height uncertainty of about 160 m.</p>
</sec>
</sec>
<sec id="Ch1.S5">
  <title>Mispointing analysis</title>
      <p>Mispointing of SCIAMACHY can have two main causes. First, the assumed mispointing
angles to determine the SRAR coordinate system may not be correct, either
because the SCIAMACHY misalignment is not well described or because the platform
attitude knowledge is inaccurate. The SRAR coordinate system can be aligned by appropriate
roll, pitch and yaw mispointing angles.</p>
      <p>Second, the scan mirror positions might have an offset. As the ASM rotates in
the yaw axis, an ASM offset corresponds to a yaw mispointing if the ASM
mirror is used in the measurement. An ESM offset corresponds to a roll
mispointing. However, if  the ASM is also used (limb light path), an ESM
offset corresponds to a mispointing in pitch; see  Figs. <xref ref-type="fig" rid="Ch1.F1"/>
and <xref ref-type="fig" rid="Ch1.F2"/>.</p>
      <p>In summary, we have five parameters to minimise the mispointing: the three
mispointing angles and two offsets for the mirror positions.</p>

<?xmltex \floatpos{t}?><table-wrap id="Ch1.T2"><caption><p>The fitted parameters <inline-formula><mml:math id="M124" display="inline"><mml:mi mathvariant="bold-italic">d</mml:mi></mml:math></inline-formula> and <inline-formula><mml:math id="M125" display="inline"><mml:mi mathvariant="bold-italic">a</mml:mi></mml:math></inline-formula> to determine the
location of the lunar intensity centroid from the observing
geometry with Eq. (<xref ref-type="disp-formula" rid="Ch1.E1"/>).</p></caption><oasis:table frame="topbot"><oasis:tgroup cols="2">
     <oasis:colspec colnum="1" colname="col1" align="left"/>
     <oasis:colspec colnum="2" colname="col2" align="left"/>
     <oasis:tbody>
       <oasis:row>  
         <oasis:entry colname="col1"><inline-formula><mml:math id="M126" display="inline"><mml:mrow><mml:msub><mml:mi>d</mml:mi><mml:mi mathvariant="normal">long</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> <inline-formula><mml:math id="M127" display="inline"><mml:mo>=</mml:mo></mml:math></inline-formula> 2.575 <inline-formula><mml:math id="M128" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> 0.151</oasis:entry>  
         <oasis:entry colname="col2"><inline-formula><mml:math id="M129" display="inline"><mml:mrow><mml:msub><mml:mi>a</mml:mi><mml:mi mathvariant="normal">long</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> <inline-formula><mml:math id="M130" display="inline"><mml:mo>=</mml:mo></mml:math></inline-formula> 0.382 <inline-formula><mml:math id="M131" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> 0.028</oasis:entry>
       </oasis:row>
       <oasis:row>  
         <oasis:entry colname="col1"><inline-formula><mml:math id="M132" display="inline"><mml:mrow><mml:msub><mml:mi>d</mml:mi><mml:mi mathvariant="normal">lat</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> <inline-formula><mml:math id="M133" display="inline"><mml:mo>=</mml:mo></mml:math></inline-formula> <inline-formula><mml:math id="M134" display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>5.223 <inline-formula><mml:math id="M135" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> 0.129</oasis:entry>  
         <oasis:entry colname="col2"><inline-formula><mml:math id="M136" display="inline"><mml:mrow><mml:msub><mml:mi>a</mml:mi><mml:mi mathvariant="normal">lat</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> <inline-formula><mml:math id="M137" display="inline"><mml:mo>=</mml:mo></mml:math></inline-formula> 0.156 <inline-formula><mml:math id="M138" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> 0.032</oasis:entry>
       </oasis:row>
     </oasis:tbody>
   </oasis:tgroup></oasis:table></table-wrap>

      <?xmltex \floatpos{t}?><fig id="Ch1.F9" specific-use="star"><caption><p>The elevation/azimuth angle offsets (<inline-formula><mml:math id="M139" display="inline"><mml:mrow><mml:mi>d</mml:mi><mml:mi mathvariant="italic">λ</mml:mi></mml:mrow></mml:math></inline-formula>/<inline-formula><mml:math id="M140" display="inline"><mml:mrow><mml:mi>d</mml:mi><mml:mi mathvariant="italic">φ</mml:mi></mml:mrow></mml:math></inline-formula>) for
the measurements used in the fit of the new mispointing parameters. <bold>(a, b)</bold> The elevation angle offset using the mispointing
parameters from 2007 and the newly fitted parameters (2016). <bold>(c, d)</bold> The azimuth angle offset for both cases. With the new
parameters, the offsets are strongly reduced.</p></caption>
        <?xmltex \igopts{width=341.433071pt}?><graphic xlink:href="https://amt.copernicus.org/articles/10/2413/2017/amt-10-2413-2017-f09.pdf"/>

      </fig>

      <p>Sub-solar measurements are available once per month, and therefore we selected
roundabout one measurement per type and month during the mission. Excluded is
the year 2002, because the first sub-solar measurements failed due to a timing
problem. In total 96 moon over limb port, 96 sun over limb port and 90 sun
over sub-solar measurements are used.</p>
      <p>A non-linear Levenberg–Marquardt  fit is used to minimise elevation and azimuth
angle offsets by varying the five mispointing parameters. Initial guesses are
the currently used final values from 2007. The newly fitted mispointing
parameters are listed in Table <xref ref-type="table" rid="Ch1.T3"/>. For completeness,  the
previously used mispointing parameters are also given as explained in the table
caption.</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F10" specific-use="star"><caption><p>Solar occultation mispointing with mispointing parameters as
defined in 2007 (grey) and with the newly fitted mispointing parameters
(labelled 2016). <bold>(a)</bold> Elevation angle offset <inline-formula><mml:math id="M141" display="inline"><mml:mrow><mml:mi>d</mml:mi><mml:mi mathvariant="italic">λ</mml:mi></mml:mrow></mml:math></inline-formula>. <bold>(b)</bold> Azimuth angle
offset <inline-formula><mml:math id="M142" display="inline"><mml:mrow><mml:mi>d</mml:mi><mml:mi mathvariant="italic">φ</mml:mi></mml:mrow></mml:math></inline-formula>. The lines are a function with a constant, a linear
and an annual and semiannual sinusoidal term, fitted to the datasets (for details
see <xref ref-type="bibr" rid="bib1.bibx3" id="altparen.12"/>). With the newly fitted parameters,
offsets for both angles are close to zero.</p></caption>
        <?xmltex \igopts{width=398.338583pt}?><graphic xlink:href="https://amt.copernicus.org/articles/10/2413/2017/amt-10-2413-2017-f10.pdf"/>

      </fig>

<?xmltex \floatpos{t}?><table-wrap id="Ch1.T3" specific-use="star"><caption><p>Envisat and SCIAMACHY mispointing parameters.
“AOCS”: these mispointing parameters are part of Attitude and Orbit
Control System (AOCS) of Envisat and describe the initial platform mispointing, here
only shown for comparison. “Scanner control”: SCIAMACHY mispointing
as determined before launch. These mispointing angles are also used in the
scanner control of SCIAMACHY. “Extra mispointing”: in the analysis
<xref ref-type="bibr" rid="bib1.bibx7" id="normal.13"/>, the mispointing was derived relative to
the mispointing already implemented in the scanner control. “SCIAMACHY
mispointing”: these four columns describe the mispointing parameters as
used in the L0-1 processing. “Launch”: for the first processor
versions since launch, no mispointing was assumed. “First 2007”:
first attempt to recognise the 2007 analysis. “Final 2007”: final
settings from the 2007 analysis, which should be the sum of scanner
control and extra mispointing. “New fit”: mispointing
parameters as determined by this work. Beyond mispointing angles in pitch,
roll and yaw, also offsets to the scanner positions (dpos<inline-formula><mml:math id="M143" display="inline"><mml:msub><mml:mi/><mml:mi mathvariant="normal">ESM</mml:mi></mml:msub></mml:math></inline-formula>, dpos<inline-formula><mml:math id="M144" display="inline"><mml:msub><mml:mi/><mml:mi mathvariant="normal">ASM</mml:mi></mml:msub></mml:math></inline-formula>)
are determined. Version 9 is the proposed processor version to implement
the new mispointing parameters.</p></caption><oasis:table frame="topbot"><oasis:tgroup cols="8">
     <oasis:colspec colnum="1" colname="col1" align="left"/>
     <oasis:colspec colnum="2" colname="col2" align="right"/>
     <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:colspec colnum="8" colname="col8" align="right"/>
     <oasis:thead>
       <oasis:row>  
         <oasis:entry colname="col1"/>  
         <oasis:entry namest="col2" nameend="col4" align="center"/>  
         <oasis:entry rowsep="1" namest="col5" nameend="col8" align="center">SCIAMACHY mispointing </oasis:entry>
       </oasis:row>
       <oasis:row>  
         <oasis:entry colname="col1"/>  
         <oasis:entry colname="col2"/>  
         <oasis:entry colname="col3">Scanner</oasis:entry>  
         <oasis:entry colname="col4">Extra mis-</oasis:entry>  
         <oasis:entry colname="col5"/>  
         <oasis:entry colname="col6">First</oasis:entry>  
         <oasis:entry colname="col7">Final</oasis:entry>  
         <oasis:entry colname="col8"/>
       </oasis:row>
       <oasis:row rowsep="1">  
         <oasis:entry colname="col1"/>  
         <oasis:entry colname="col2">AOCS</oasis:entry>  
         <oasis:entry colname="col3">control</oasis:entry>  
         <oasis:entry colname="col4">pointing</oasis:entry>  
         <oasis:entry colname="col5">launch</oasis:entry>  
         <oasis:entry colname="col6">2007</oasis:entry>  
         <oasis:entry colname="col7">2007</oasis:entry>  
         <oasis:entry colname="col8">New fit</oasis:entry>
       </oasis:row>
     </oasis:thead>
     <oasis:tbody>
       <oasis:row rowsep="1">  
         <oasis:entry colname="col1">L0-1b processor version</oasis:entry>  
         <oasis:entry colname="col2">all</oasis:entry>  
         <oasis:entry colname="col3">all</oasis:entry>  
         <oasis:entry colname="col4">–</oasis:entry>  
         <oasis:entry colname="col5"><inline-formula><mml:math id="M145" display="inline"><mml:mo>&lt;</mml:mo></mml:math></inline-formula> 6.0</oasis:entry>  
         <oasis:entry colname="col6"><inline-formula><mml:math id="M146" display="inline"><mml:mo>≥</mml:mo></mml:math></inline-formula> 6.03</oasis:entry>  
         <oasis:entry colname="col7"><inline-formula><mml:math id="M147" display="inline"><mml:mo>≥</mml:mo></mml:math></inline-formula> 7.0</oasis:entry>  
         <oasis:entry colname="col8"><inline-formula><mml:math id="M148" display="inline"><mml:mo>≥</mml:mo></mml:math></inline-formula> 9.0</oasis:entry>
       </oasis:row>
       <oasis:row>  
         <oasis:entry colname="col1">Pitch    (mdeg)</oasis:entry>  
         <oasis:entry colname="col2"><inline-formula><mml:math id="M149" display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>167.074</oasis:entry>  
         <oasis:entry colname="col3">0.630</oasis:entry>  
         <oasis:entry colname="col4"><inline-formula><mml:math id="M150" display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>26 <inline-formula><mml:math id="M151" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> 3</oasis:entry>  
         <oasis:entry colname="col5">0.0</oasis:entry>  
         <oasis:entry colname="col6"><inline-formula><mml:math id="M152" display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>26.0</oasis:entry>  
         <oasis:entry colname="col7"><inline-formula><mml:math id="M153" display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>25.4</oasis:entry>  
         <oasis:entry colname="col8"><inline-formula><mml:math id="M154" display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>17.06 <inline-formula><mml:math id="M155" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> 0.63</oasis:entry>
       </oasis:row>
       <oasis:row>  
         <oasis:entry colname="col1">Roll     (mdeg)</oasis:entry>  
         <oasis:entry colname="col2">50.233</oasis:entry>  
         <oasis:entry colname="col3">1.662</oasis:entry>  
         <oasis:entry colname="col4"><inline-formula><mml:math id="M156" display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>20 <inline-formula><mml:math id="M157" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> 1</oasis:entry>  
         <oasis:entry colname="col5">0.0</oasis:entry>  
         <oasis:entry colname="col6"><inline-formula><mml:math id="M158" display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>20.0</oasis:entry>  
         <oasis:entry colname="col7"><inline-formula><mml:math id="M159" display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>18.3</oasis:entry>  
         <oasis:entry colname="col8"><inline-formula><mml:math id="M160" display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>25.18 <inline-formula><mml:math id="M161" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> 0.48</oasis:entry>
       </oasis:row>
       <oasis:row>  
         <oasis:entry colname="col1">Yaw      (mdeg)</oasis:entry>  
         <oasis:entry colname="col2">391.987</oasis:entry>  
         <oasis:entry colname="col3"><inline-formula><mml:math id="M162" display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>227.464</oasis:entry>  
         <oasis:entry colname="col4">9 <inline-formula><mml:math id="M163" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> 8</oasis:entry>  
         <oasis:entry colname="col5">0.0</oasis:entry>  
         <oasis:entry colname="col6"><inline-formula><mml:math id="M164" display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>218.46</oasis:entry>  
         <oasis:entry colname="col7"><inline-formula><mml:math id="M165" display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>218.5</oasis:entry>  
         <oasis:entry colname="col8"><inline-formula><mml:math id="M166" display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>227.61 <inline-formula><mml:math id="M167" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> 1.26</oasis:entry>
       </oasis:row>
       <oasis:row>  
         <oasis:entry colname="col1">dpos<inline-formula><mml:math id="M168" display="inline"><mml:msub><mml:mi/><mml:mi mathvariant="normal">ESM</mml:mi></mml:msub></mml:math></inline-formula> (mdeg)</oasis:entry>  
         <oasis:entry colname="col2"/>  
         <oasis:entry colname="col3"/>  
         <oasis:entry colname="col4"/>  
         <oasis:entry colname="col5"/>  
         <oasis:entry colname="col6"/>  
         <oasis:entry colname="col7"/>  
         <oasis:entry colname="col8"><inline-formula><mml:math id="M169" display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>8.11 <inline-formula><mml:math id="M170" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> 0.54</oasis:entry>
       </oasis:row>
       <oasis:row>  
         <oasis:entry colname="col1">dpos<inline-formula><mml:math id="M171" display="inline"><mml:msub><mml:mi/><mml:mi mathvariant="normal">ASM</mml:mi></mml:msub></mml:math></inline-formula> (mdeg)</oasis:entry>  
         <oasis:entry colname="col2"/>  
         <oasis:entry colname="col3"/>  
         <oasis:entry colname="col4"/>  
         <oasis:entry colname="col5"/>  
         <oasis:entry colname="col6"/>  
         <oasis:entry colname="col7"/>  
         <oasis:entry colname="col8"><inline-formula><mml:math id="M172" display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>102.02 <inline-formula><mml:math id="M173" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> 1.43</oasis:entry>
       </oasis:row>
     </oasis:tbody>
   </oasis:tgroup></oasis:table></table-wrap>

      <p>Figure <xref ref-type="fig" rid="Ch1.F9"/> shows the improvement. For the measurements used in the fit,
the observed elevation/azimuth angle offset (<inline-formula><mml:math id="M174" display="inline"><mml:mrow><mml:mi>d</mml:mi><mml:mi mathvariant="italic">λ</mml:mi></mml:mrow></mml:math></inline-formula>/<inline-formula><mml:math id="M175" display="inline"><mml:mrow><mml:mi>d</mml:mi><mml:mi mathvariant="italic">φ</mml:mi></mml:mrow></mml:math></inline-formula>) is
plotted, once using the mispointing parameters from 2007 and once using the
new parameters (marked as 2016).  The elevation and azimuth angle offsets for
all three measurement types are clearly reduced for the full time series.  In
elevation, the offsets with opposite signs for the lunar and solar
measurements over limb port have been corrected. In azimuth, the large
horizontal offset for the measurements over the limb light path has been
removed.</p>
      <p>The new parameters briefly have the following impact on the pointing:</p>
      <p><list list-type="bullet">
          <list-item>

      <p>The ASM mirror offset fixes the large azimuth angle offset.</p>
          </list-item>
          <list-item>

      <p>The yaw mispointing is almost unchanged because the sub-solar
azimuth angle had no offset.</p>
          </list-item>
          <list-item>

      <p>The changed roll mispointing angle fixes the elevation offsets with
opposite signs for solar and lunar occultation, because these two
measurement have different viewing directions in azimuth. Whereas the solar
occultation is performed at <inline-formula><mml:math id="M176" display="inline"><mml:mrow><mml:mo>∼</mml:mo><mml:mo>-</mml:mo><mml:msup><mml:mn mathvariant="normal">30</mml:mn><mml:mo>∘</mml:mo></mml:msup></mml:mrow></mml:math></inline-formula> azimuth angle, the lunar occultation
azimuth angle is up to <inline-formula><mml:math id="M177" display="inline"><mml:mrow><mml:mo>∼</mml:mo><mml:mo>+</mml:mo><mml:msup><mml:mn mathvariant="normal">40</mml:mn><mml:mo>∘</mml:mo></mml:msup></mml:mrow></mml:math></inline-formula>.</p>
          </list-item>
          <list-item>

      <p>The pitch mispointing angle results in an overall adjustment of the
elevation angle offset.</p>
          </list-item>
        </list></p>
<sec id="Ch1.S5.SS1">
  <title>Impact of new parameters</title>
      <p>In <xref ref-type="bibr" rid="bib1.bibx3" id="text.14"/>, the mispointing for the solar occultation
measurements has been investigated in detail. With the new mispointing
parameters, we repeated this analysis. Figure <xref ref-type="fig" rid="Ch1.F10"/> shows the viewing
angles offsets for the previous and the new parameters. The mean tangent
height/horizontal offset has been reduced from 276 m/5031 m to 29 m/71 m.
The encoder readouts of the scanner unit are discretized in mdeg steps,
corresponding to about 56 m at the tangent point. The remaining offsets are
at the noise level of these readouts. The amplitude of the seasonal
variation of the elevation angle offset has been reduced from 122 to
48 m. Because of the roll mispointing, the elevation angle offset was
azimuth dependent. Therefore, the fixed seasonal pattern of the azimuth of the
solar occultation measurement contributed strongly to the seasonal pattern in
the elevation offsets. The offsets and seasonal variations are summarised in
Table <xref ref-type="table" rid="Ch1.T4"/>.</p>
      <p>The impact on the limb and occultation tangent heights is shown for orbit
15 193  (25 January 2005) in Fig. <xref ref-type="fig" rid="Ch1.F11"/>.  Given is the difference in
tangent heights (elevation angles) between the configuration derived in this
paper and the previous one.  The solar occultation tangent heights are changed
by about <inline-formula><mml:math id="M178" display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">290</mml:mn></mml:mrow></mml:math></inline-formula> m (<inline-formula><mml:math id="M179" display="inline"><mml:mrow><mml:mo>+</mml:mo><mml:mn mathvariant="normal">5</mml:mn></mml:mrow></mml:math></inline-formula> mdeg); for lunar occultation we observe about
<inline-formula><mml:math id="M180" display="inline"><mml:mrow><mml:mo>+</mml:mo><mml:mn mathvariant="normal">140</mml:mn></mml:mrow></mml:math></inline-formula> m (<inline-formula><mml:math id="M181" display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">2.5</mml:mn></mml:mrow></mml:math></inline-formula> mdeg). The SCIAMACHY limb measurements have a horizontal
swath of about 960 km, for a large part of the spectral range divided into
four vertical profiles. Depending on the profile (and therefore the azimuth
angle), the changes are in the range of <inline-formula><mml:math id="M182" display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>50 to <inline-formula><mml:math id="M183" display="inline"><mml:mo>+</mml:mo></mml:math></inline-formula>60 m (<inline-formula><mml:math id="M184" display="inline"><mml:mrow><mml:mo>+</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:math></inline-formula> to
<inline-formula><mml:math id="M185" display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1.2</mml:mn></mml:mrow></mml:math></inline-formula> mdeg). An east–west asymmetry in the tangent height offset has been
observed in former tangent height retrievals from the limb measurements. The
limb tangent height retrieval method is described in <xref ref-type="bibr" rid="bib1.bibx9" id="text.15"/> and
<xref ref-type="bibr" rid="bib1.bibx14" id="text.16"/>. The corrections derived in this paper confirm an
east–west asymmetry. Depending on season, the solar occultation tangent
heights changes are in the range of <inline-formula><mml:math id="M186" display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>330 to <inline-formula><mml:math id="M187" display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>130 m. The range for solar
occultation is 0 to <inline-formula><mml:math id="M188" display="inline"><mml:mo>+</mml:mo></mml:math></inline-formula>130 m. Limb tangent heights are changed in the range of
<inline-formula><mml:math id="M189" display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>60 to <inline-formula><mml:math id="M190" display="inline"><mml:mo>+</mml:mo></mml:math></inline-formula>70 m, with a fixed pattern in the horizontal direction.  For all
tangent points, the horizontal location is moved by about 5 km.</p>

<?xmltex \floatpos{t}?><table-wrap id="Ch1.T4"><caption><p>The offset and amplitudes of the seasonal cycles of the functions
fitted to the occultation mispointing angle with the mispointing parameters as
defined in 2007 and with the newly fitted mispointing parameters (see
Fig. <xref ref-type="fig" rid="Ch1.F10"/>). The values for the 2007
mispointing very slightly differ from the ones given in <xref ref-type="bibr" rid="bib1.bibx3" id="text.17"/>
because of the update in the orbit parameters (see Sect. <xref ref-type="sec" rid="App1.Ch1.S1.SS1"/>) and a
slightly changed set of available orbits in the Level 1b product version
8.</p></caption><oasis:table frame="topbot"><?xmltex \begin{scaleboxenv}{.84}[.84]?><oasis:tgroup cols="5">
     <oasis:colspec colnum="1" colname="col1" align="left"/>
     <oasis:colspec colnum="2" colname="col2" align="right"/>
     <oasis:colspec colnum="3" colname="col3" align="right" colsep="1"/>
     <oasis:colspec colnum="4" colname="col4" align="right"/>
     <oasis:colspec colnum="5" colname="col5" align="right"/>
     <oasis:thead>
       <oasis:row>  
         <oasis:entry colname="col1"/>  
         <oasis:entry rowsep="1" namest="col2" nameend="col3" align="center" colsep="1">Amplitude </oasis:entry>  
         <oasis:entry rowsep="1" namest="col4" nameend="col5" align="center">Mean offset </oasis:entry>
       </oasis:row>
       <oasis:row rowsep="1">  
         <oasis:entry colname="col1"/>  
         <oasis:entry colname="col2">(mdeg)</oasis:entry>  
         <oasis:entry colname="col3">(m)</oasis:entry>  
         <oasis:entry colname="col4">(mdeg)</oasis:entry>  
         <oasis:entry colname="col5">(m)</oasis:entry>
       </oasis:row>
     </oasis:thead>
     <oasis:tbody>
       <oasis:row>  
         <oasis:entry colname="col1">Elevation 2007</oasis:entry>  
         <oasis:entry colname="col2">2.158 <inline-formula><mml:math id="M191" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> 0.011</oasis:entry>  
         <oasis:entry colname="col3">122 <inline-formula><mml:math id="M192" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> 1</oasis:entry>  
         <oasis:entry colname="col4"><inline-formula><mml:math id="M193" display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>4.89 <inline-formula><mml:math id="M194" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> 0.013</oasis:entry>  
         <oasis:entry colname="col5">276 <inline-formula><mml:math id="M195" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> 1</oasis:entry>
       </oasis:row>
       <oasis:row>  
         <oasis:entry colname="col1">Elevation 2016</oasis:entry>  
         <oasis:entry colname="col2">0.849 <inline-formula><mml:math id="M196" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> 0.012</oasis:entry>  
         <oasis:entry colname="col3">48 <inline-formula><mml:math id="M197" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> 1</oasis:entry>  
         <oasis:entry colname="col4"><inline-formula><mml:math id="M198" display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>0.51 <inline-formula><mml:math id="M199" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> 0.013</oasis:entry>  
         <oasis:entry colname="col5">29 <inline-formula><mml:math id="M200" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> 1</oasis:entry>
       </oasis:row>
       <oasis:row>  
         <oasis:entry colname="col1">Azimuth 2007</oasis:entry>  
         <oasis:entry colname="col2">2.230 <inline-formula><mml:math id="M201" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> 0.017</oasis:entry>  
         <oasis:entry colname="col3">126 <inline-formula><mml:math id="M202" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> 1</oasis:entry>  
         <oasis:entry colname="col4">89.04 <inline-formula><mml:math id="M203" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> 0.019</oasis:entry>  
         <oasis:entry colname="col5"><inline-formula><mml:math id="M204" display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>5031 <inline-formula><mml:math id="M205" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> 1</oasis:entry>
       </oasis:row>
       <oasis:row>  
         <oasis:entry colname="col1">Azimuth 2016</oasis:entry>  
         <oasis:entry colname="col2">2.257 <inline-formula><mml:math id="M206" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> 0.017</oasis:entry>  
         <oasis:entry colname="col3">128 <inline-formula><mml:math id="M207" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> 1</oasis:entry>  
         <oasis:entry colname="col4">1.25 <inline-formula><mml:math id="M208" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> 0.019</oasis:entry>  
         <oasis:entry colname="col5"><inline-formula><mml:math id="M209" display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>71 <inline-formula><mml:math id="M210" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> 1</oasis:entry>
       </oasis:row>
     </oasis:tbody>
   </oasis:tgroup><?xmltex \end{scaleboxenv}?></oasis:table></table-wrap>

</sec>
</sec>
<sec id="Ch1.S6" sec-type="conclusions">
  <title>Conclusions</title>
      <p>We provide a method to determine improved mispointing parameters for SCIAMACHY
on board ENVISAT from in-flight measurements. The viewing direction
towards sun or moon is derived for three types of measurements and compared to
the expected viewing direction. These types are sun
and moon over limb port and sun over sub-solar port measurements.</p>
      <p><?xmltex \hack{\newpage}?>SCIAMACHY's sun follower device adjusts the azimuth direction in sun over limb
port, the elevation direction in sun over sub-solar port and both directions
in moon over limb port observations. Sun over limb port elevation offset are
derived from the scans over the solar disk: at maximum intensity the
instrument points to the solar centre. Similarly, the solar disk moves in
azimuth over the field of view of the sub-solar port by the orbital motion;
again the maximum intensity defines the direction towards the solar centre.</p>
      <p>The moon is an inhomogeneous and variable target, and the SFD points to the
IC of the moon instead of the lunar centre. We
investigated reference images from the USGS ROLO
and derived a parameterisation for the location of the IC from the observation
geometry only.</p>
      <p>The viewing directions are compared to the ones according to the attitude
information of the platform to derive azimuth and elevation angle
offsets. Mispointing angle in pitch, roll and yaw for the platform can correct
the assumed attitude. Zero offsets for the positions of the scan mirrors can
improve the pointing of the instrument.</p>
      <p>With a suitable subset of the available pointing measurements, we minimise the
mispointing for the whole mission by varying the five mispointing parameters
in a non-linear Levenberg–Marquardt  fit.</p>
      <p>The azimuth and elevation angle offsets observed with the previous set of
mispointing parameters are clearly reduced by the newly derived set. For sun
over limb port measurements, the mean offset in tangent height is reduced from
276 m to negligible 29 m. The amplitude of the seasonal cycle of the tangent
height offset is reduced from 122  to 48 m. The previously observed
horizontal offset of 5 km is reduced to 71 m.</p>
      <p>The tangent height altitudes of SCIAMACHY's solar occultation measurements are
changed by <inline-formula><mml:math id="M211" display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>130 to <inline-formula><mml:math id="M212" display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>330 m, lunar occultation is altered by 0 to <inline-formula><mml:math id="M213" display="inline"><mml:mo>+</mml:mo></mml:math></inline-formula>130 m.  The
limb measurements are changed by <inline-formula><mml:math id="M214" display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>50 to <inline-formula><mml:math id="M215" display="inline"><mml:mo>+</mml:mo></mml:math></inline-formula>60 m, including the removal of an
east–west asymmetry in the limb tangent height offsets.  The horizontal
location of the tangent point is for all three cases changed by about 5 km.</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F11"><caption><p>Tangent height changes for the limb and occultation
measurements of orbit 15 193 (25 January 2005) from the previous
mispointing parameters to the ones derived here.</p></caption>
        <?xmltex \igopts{width=241.848425pt}?><graphic xlink:href="https://amt.copernicus.org/articles/10/2413/2017/amt-10-2413-2017-f11.pdf"/>

      </fig>

      <p><?xmltex \hack{\newpage}?>The new mispointing angles and the mirror position offsets according to
Table <xref ref-type="table" rid="Ch1.T3"/> will be used
in the next release of the SCIAMACHY data processor (Level 1b version 9 and
Level 2 version 7) and improve the geolocation for all measurements. Most
important is the better knowledge of the tangent heights for SCIAMACHY's limb
and occultation measurements.</p>
</sec>

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

      <p>SCIAMACHY Level 1b data are available from ESA
(<uri>https://earth.esa.int</uri>) and require only a short, quick registration.
The ROLO images used in this study were supplied by the USGS Lunar
Calibration project. Readers wishing to utilise these images may contact
co-author T. Stone (for contact details see <uri>http://www.moon-cal.org</uri>).</p>
  </notes><?xmltex \hack{\clearpage}?><app-group>

<app id="App1.Ch1.S1">
  <title>Software packages</title>
<sec id="App1.Ch1.S1.SS1">
  <title>Envisat-1 mission CFI software</title>
      <p>All calculations necessary for orbit propagation and pointing issues for
Envisat are combined in the Envisat-1 mission CFI software <xref ref-type="bibr" rid="bib1.bibx13" id="paren.18"/>.
The software needs as input the orbit information of the satellite. In
<xref ref-type="bibr" rid="bib1.bibx3" id="normal.19"/>, the orbit state vector from the main product header in
the SCIAMACHY Level 1b product has been propagated along the orbit. In this
work, we use the DORIS precise orbit product files for Envisat, which are
more accurate and also used for the re-processing campaigns of SCIAMACHY
data. The DORIS system <xref ref-type="bibr" rid="bib1.bibx8" id="paren.20"/> provides accurate orbit
information; for Envisat the radial orbit precision is 2 cm
<xref ref-type="bibr" rid="bib1.bibx15" id="paren.21"/>.</p>
</sec>
<sec id="App1.Ch1.S1.SS2">
  <title>HORIZONS</title>
      <p>The JPL HORIZONS online solar system data and ephemeris computation
service of the Solar System Dynamics (SSD) group of NASA's Jet Propulsion
Laboratory (JPL) <xref ref-type="bibr" rid="bib1.bibx5 bib1.bibx16" id="paren.22"/> provides access to key solar
system data and flexible production of highly accurate ephemerides for solar
system objects. It is needed for the specific requirements of the lunar target,
which are not covered by the CFIs. Specifically, the system can calculate the
sub-solar and sub-observer point on the moon for each viewing point in space
and time. It can also calculate observation parameters for target points
on the moon specified by lunar coordinates.</p><?xmltex \hack{\vspace*{3mm}}?>
</sec>
</app>

<app id="App1.Ch1.S2">
  <title>Abbreviations</title>
      <p><table-wrap id="Taba" position="anchor"><oasis:table><oasis:tgroup cols="2">
     <oasis:colspec colnum="1" colname="col1" align="left"/>
     <oasis:colspec colnum="2" colname="col2" align="left"/>
     <oasis:tbody>
       <oasis:row>  
         <oasis:entry colname="col1">SCIAMACHY</oasis:entry>  
         <oasis:entry colname="col2">SCanning Imaging Absorption spectroMeter for Atmospheric CHartographY (on board Envisat)</oasis:entry>
       </oasis:row>
       <oasis:row>  
         <oasis:entry colname="col1">ESM</oasis:entry>  
         <oasis:entry colname="col2">SCIAMACHY's elevation scan mechanism</oasis:entry>
       </oasis:row>
       <oasis:row>  
         <oasis:entry colname="col1">ASM</oasis:entry>  
         <oasis:entry colname="col2">SCIAMACHY's azimuth scan mechanism</oasis:entry>
       </oasis:row>
       <oasis:row>  
         <oasis:entry colname="col1">SFD</oasis:entry>  
         <oasis:entry colname="col2">SCIAMACHY's sun follower device</oasis:entry>
       </oasis:row>
       <oasis:row>  
         <oasis:entry colname="col1">PMD</oasis:entry>  
         <oasis:entry colname="col2">SCIAMACHY's polarisation measurement device</oasis:entry>
       </oasis:row>
       <oasis:row>  
         <oasis:entry colname="col1">ROLO</oasis:entry>  
         <oasis:entry colname="col2">The Robotic Lunar Observatory of US Geological Survey (USGS)</oasis:entry>
       </oasis:row>
       <oasis:row>  
         <oasis:entry colname="col1">IC</oasis:entry>  
         <oasis:entry colname="col2">Intensity centroid (of the actual lunar disk)</oasis:entry>
       </oasis:row>
       <oasis:row>  
         <oasis:entry colname="col1">SRAR</oasis:entry>  
         <oasis:entry colname="col2">Satellite Relative Actual Reference (Envisat coordinate system)</oasis:entry>
       </oasis:row>
     </oasis:tbody>
   </oasis:tgroup></oasis:table></table-wrap></p><?xmltex \hack{\newpage}?>
</app>

<app id="App1.Ch1.S3">
  <title>Detailed algorithm for lunar measurements</title>
      <p>The CFI software does not provide all quantities necessary for determining the
viewing direction toward the IC on the moon. The sequence is therefore as follows:
<list list-type="bullet"><list-item>
      <p>The orbital positions of the satellite during the lunar measurement is
calculated using the CFIs.</p></list-item><list-item>
      <p>The sub-observer point from this satellite position and the sub-solar
point in lunar coordinates are derived with the HORIZONS system.</p></list-item><list-item>
      <p>Using the parameterisation of Eq. (<xref ref-type="disp-formula" rid="Ch1.E1"/>), the lunar coordinates of
the IC is derived.</p></list-item><list-item>
      <p>The HORIZONS system calculates for the coordinates the right ascension
and the declination of the IC for the satellite position.</p></list-item><list-item>
      <p>These astronomical coordinates are used in the CFIs to derive the actual
azimuth and elevation angle of the IC.</p></list-item></list></p><?xmltex \hack{\clearpage}?>
</app>
  </app-group><notes notes-type="competinginterests">

      <p>The authors declare that they have no conflict of
interest.</p>
  </notes><ack><title>Acknowledgements</title><p>SCIAMACHY is a national contribution to the ESA Envisat project, funded by
Germany, the Netherlands and Belgium. SCIAMACHY data have been provided by
ESA.  This work has been funded by DLR Space Agency (Germany), by ESA via
the SCIAMACHY Quality Working Group (SQWG) and by the state and the
University of Bremen.<?xmltex \hack{\newline}?><?xmltex \hack{\newline}?>
The article processing charges for this open-access <?xmltex \hack{\newline}?> publication were covered by the University of Bremen.<?xmltex \hack{\newline}?><?xmltex \hack{\newline}?>
Edited by: Alexander Kokhanovsky<?xmltex \hack{\newline}?>
Reviewed by: three anonymous referees</p></ack><ref-list>
    <title>References</title>

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Rep. PO-IS-ESA-GS-0561, Issue 2.0, ESA, GMV, S.A., Madrid,
<uri>http://eop-cfi.esa.int/index.php/docs-and-mission-data/cfi-docs</uri> (last access: 27 June 2017),
1997.</mixed-citation></ref>
      <ref id="bib1.bibx2"><label>Bovensmann et al.(1999)</label><mixed-citation>Bovensmann, H., Burrows, J. P., Buchwitz, M., Frerick, J., Noël, S.,
Rozanov, V. V., Chance, K. V., and Goede, A. P. H.: SCIAMACHY: Mission
Objectives and Measurement Modes, J. Atmos. Sci., 56, 127–150,
<ext-link xlink:href="https://doi.org/10.1175/1520-0469(1999)056&lt;0127:SMOAMM&gt;2.0.CO;2" ext-link-type="DOI">10.1175/1520-0469(1999)056&lt;0127:SMOAMM&gt;2.0.CO;2</ext-link>, 1999.</mixed-citation></ref>
      <ref id="bib1.bibx3"><label>Bramstedt et al.(2012)</label><mixed-citation>Bramstedt, K., Noël, S., Bovensmann, H., Gottwald, M., and Burrows, J.
P.: Precise pointing knowledge for SCIAMACHY solar occultation measurements,
Atmos. Meas. Tech., 5, 2867–2880, <ext-link xlink:href="https://doi.org/10.5194/amt-5-2867-2012" ext-link-type="DOI">10.5194/amt-5-2867-2012</ext-link>, 2012.</mixed-citation></ref>
      <ref id="bib1.bibx4"><label>Burrows et al.(1995)</label><mixed-citation>Burrows, J., Hözle, E., Goede, A., Visser, H., and Fricke, W.:
SCIAMACHY – scanning imaging absorption spectrometer for atmospheric
chartography, Acta Astronaut., 35, 445–451,
<ext-link xlink:href="https://doi.org/10.1016/0094-5765(94)00278-T" ext-link-type="DOI">10.1016/0094-5765(94)00278-T</ext-link>,
1995.</mixed-citation></ref>
      <ref id="bib1.bibx5"><label>Giorgini et al.(1996)</label><mixed-citation>Giorgini, J. D., Yeomans, D. K., Chamberlin, A. B., Chodas, P. W., Jacobson,
R. A., Keesey, M. S., Lieske, J. H., Ostro, S. J., Standish, E. M., and
Wimberly, R. N.: JPL's On-Line Solar System Data Service, in: Bulletin of
the American Astronomical Society, vol. 28, p. 1158, 1996.
 </mixed-citation></ref><?xmltex \hack{\newpage}?>
      <ref id="bib1.bibx6"><label>Gottwald and Bovensmann(2011)</label><mixed-citation>
Gottwald, M. and Bovensmann, H. (Eds.): SCIAMACHY – Exploring the Changing
Earth's Atmosphere, Springer, Dordrecht, Heidelberg, London, New York, 2011.</mixed-citation></ref>
      <ref id="bib1.bibx7"><label>Gottwald et al.(2007)</label><mixed-citation>
Gottwald, M., Krieg, E., von Savigny, C., Noël, S., Bovensmann, H., and
Bramstedt, K.: Determination of SCIAMACHY Line-of-Sight Misalignments,
Proc. Envisat Symposium, Montreux Switzerland 23–27 April, SP-636, 2007.</mixed-citation></ref>
      <ref id="bib1.bibx8"><label>Jayles et al.(2006)</label><mixed-citation>Jayles, C., Nhun-Fat, B., and Tourain, C.: DORIS: System Description and
Control of the Signal Integrity, J. Geodesy, 80, 457–472,
<ext-link xlink:href="https://doi.org/10.1007/s00190-006-0046-8" ext-link-type="DOI">10.1007/s00190-006-0046-8</ext-link>, 2006.</mixed-citation></ref>
      <ref id="bib1.bibx9"><label>Kaiser et al.(2004)</label><mixed-citation>Kaiser, J. W., von Savigny, C., Eichmann, K. U., Noël, S., Bovensmann,
H., Frerick, J., and Burrows, J. P.: Satellite-pointing retrieval from
atmospheric limb-scattering of solar UV-B radiation, Can. J.
Phys., 82, 1041–1052, <ext-link xlink:href="https://doi.org/10.1139/p04-071" ext-link-type="DOI">10.1139/p04-071</ext-link>,
2004.</mixed-citation></ref>
      <ref id="bib1.bibx10"><label>Kieffer and Stone(2005)</label><mixed-citation>Kieffer, H. H. and Stone, T. C.: The Spectral Irradiance of the Moon,
Astron. J., 129, 2887, <ext-link xlink:href="https://doi.org/10.1086/430185" ext-link-type="DOI">10.1086/430185</ext-link>, 2005.</mixed-citation></ref>
      <ref id="bib1.bibx11"><label>Legrand and Chevalley(2013a)</label><mixed-citation>
Legrand, C. and Chevalley, P.: Virtual Moon Atlas ”Pro 6” Freeware, in:
Lunar and Planetary Science Conference, vol. 44 of Lunar and Planetary
Inst. Technical Report, p. 1021, 2013a.</mixed-citation></ref>
      <ref id="bib1.bibx12"><label>Legrand and Chevalley(2013b)</label><mixed-citation>Legrand, C. and Chevalley, P.: Virtual Moon Atlas “Pro” Version 6.0,
<uri>http://www.ap-i.net/avl/en/start</uri> (last access: 1 June 2015),
2013b.</mixed-citation></ref>
      <ref id="bib1.bibx13"><label>Muñoz(2011)</label><mixed-citation>Muñoz, C. V.: Re-Engineering of Mission Analysis Software for Envisat-1,
General Software User Manual, Tech. Rep. PO-IS-DMS-GS-0556, Issue 5.9, ESA,
DEIMOS Space S.L.U, Madrid,
<uri>http://eop-cfi.esa.int/index.php/docs-and-mission-data/cfi-docs</uri> (last access: 27 June 2017),
2011.</mixed-citation></ref>
      <ref id="bib1.bibx14"><label>von Savigny et al.(2005)</label><mixed-citation>von Savigny, C., Kaiser, J. W., Bovensmann, H., Burrows, J. P., McDermid, I.
S., and Leblanc, T.: Spatial and temporal characterization of SCIAMACHY limb
pointing errors during the first three years of the mission, Atmos. Chem.
Phys., 5, 2593–2602, <ext-link xlink:href="https://doi.org/10.5194/acp-5-2593-2005" ext-link-type="DOI">10.5194/acp-5-2593-2005</ext-link>, 2005.</mixed-citation></ref>
      <ref id="bib1.bibx15"><label>Willis et al.(2006)</label><mixed-citation>Willis, P., Jayles, C., and Bar-Sever, Y.: DORIS: From orbit determination for
altimeter missions to geodesy, C. R. Geosci., 338, 968–979,
<ext-link xlink:href="https://doi.org/10.1016/j.crte.2005.11.013" ext-link-type="DOI">10.1016/j.crte.2005.11.013</ext-link>,  2006.</mixed-citation></ref>
      <ref id="bib1.bibx16"><label>Yeomans et al.(1996)</label><mixed-citation>Yeomans, D., Chamberlin, A., Giorgini, J., Chodas, P., Jacobson, R., Keesey,
M., Lieske, J., Ostro, S., Standish, E., and Wimberly, R.: The JPL HORIZONS
on-line solar system data and ephemeris computation service,
<uri>http://ssd.jpl.nasa.gov/?horizons</uri> (last access: 1 September 2016),
1996.</mixed-citation></ref>

  </ref-list><app-group content-type="float"><app><title/>

    </app></app-group></back>
    <!--<article-title-html>Improved pointing information for SCIAMACHY from in-flight measurements of the viewing  directions towards sun and moon</article-title-html>
<abstract-html><p class="p">The SCanning Imaging Absorption spectroMeter for Atmospheric
CHartographY
(SCIAMACHY) on Envisat (2002–2012) performed nadir, limb, solar/lunar
occultation and various monitoring measurements. The pointing information of
the instrument is determined by the attitude information of the Envisat
platform with its star trackers together with the encoder readouts of both
the azimuth and the elevation scanner of SCIAMACHY.</p><p class="p">In this work, we present additional sources of attitude information from the
SCIAMACHY measurements itself. The basic principle is the same as used by
the star tracker: we measure the viewing direction towards celestial
objects, i.e. sun and moon, to detect possible mispointings.</p><p class="p">In sun over limb port observations, we utilise the vertical scans over the
solar disk. In horizontal direction, SCIAMACHY's sun follower device (SFD)
is used to adjust the viewing direction. Moon over limb port measurements
use for both the vertical and the horizontal direction the adjustment by the
SFD. The viewing direction is steered towards the intensity centroid of the
illuminated part of the lunar disk. We use reference images from the USGS
Robotic Lunar Observatory (ROLO) to take into account the inhomogeneous
surface and the variations by lunar libration and phase to parameterise the
location of the intensity centroid from the observation geometry.
Solar observations through SCIAMACHY's so-called sub-solar port (with a
viewing direction closely to zenith) also use the
SFD in the vertical direction. In the horizontal direction the geometry of the port defines the viewing
direction.</p><p class="p">Using these three type of measurements, we fit improved mispointing
parameters by minimising the pointing offsets in elevation and azimuth. The
geolocation of all retrieved products will benefit from this; the
tangent heights are especially improved. The altitudes assigned to SCIAMACHY's solar
occultation measurements are changed in the range of −130 to −330 m, the lunar occultation
measurements are changed in the range of 0 to +130 m
and the limb measurements are changed in the range of −50 to
+60 m (depending on season, altitude and azimuth angle). The horizontal
location of the tangent point is changed by about
5 km for all measurements. These updates are implemented in version 9 of the SCIAMACHY Level 1b
products and Level 2 version 7 (based on L1b version 9).</p></abstract-html>
<ref-html id="bib1.bib1"><label>Alvarez(1997)</label><mixed-citation>
Alvarez, L.: Envisat-1 Mission CFI Software Mission Conventions Document, Tech.
Rep. PO-IS-ESA-GS-0561, Issue 2.0, ESA, GMV, S.A., Madrid,
<a href="http://eop-cfi.esa.int/index.php/docs-and-mission-data/cfi-docs" target="_blank">http://eop-cfi.esa.int/index.php/docs-and-mission-data/cfi-docs</a> (last access: 27 June 2017),
1997.
</mixed-citation></ref-html>
<ref-html id="bib1.bib2"><label>Bovensmann et al.(1999)</label><mixed-citation>
Bovensmann, H., Burrows, J. P., Buchwitz, M., Frerick, J., Noël, S.,
Rozanov, V. V., Chance, K. V., and Goede, A. P. H.: SCIAMACHY: Mission
Objectives and Measurement Modes, J. Atmos. Sci., 56, 127–150,
<a href="https://doi.org/10.1175/1520-0469(1999)056&lt;0127:SMOAMM&gt;2.0.CO;2" target="_blank">https://doi.org/10.1016/10.1175/1520-0469(1999)056&lt;0127:SMOAMM&gt;2.0.CO;2</a>, 1999.
</mixed-citation></ref-html>
<ref-html id="bib1.bib3"><label>Bramstedt et al.(2012)</label><mixed-citation>
Bramstedt, K., Noël, S., Bovensmann, H., Gottwald, M., and Burrows, J.
P.: Precise pointing knowledge for SCIAMACHY solar occultation measurements,
Atmos. Meas. Tech., 5, 2867–2880, <a href="https://doi.org/10.5194/amt-5-2867-2012" target="_blank">https://doi.org/10.1016/10.5194/amt-5-2867-2012</a>, 2012.
</mixed-citation></ref-html>
<ref-html id="bib1.bib4"><label>Burrows et al.(1995)</label><mixed-citation>
Burrows, J., Hözle, E., Goede, A., Visser, H., and Fricke, W.:
SCIAMACHY – scanning imaging absorption spectrometer for atmospheric
chartography, Acta Astronaut., 35, 445–451,
<a href="https://doi.org/10.1016/0094-5765(94)00278-T" target="_blank">https://doi.org/10.1016/10.1016/0094-5765(94)00278-T</a>,
1995.
</mixed-citation></ref-html>
<ref-html id="bib1.bib5"><label>Giorgini et al.(1996)</label><mixed-citation>
Giorgini, J. D., Yeomans, D. K., Chamberlin, A. B., Chodas, P. W., Jacobson,
R. A., Keesey, M. S., Lieske, J. H., Ostro, S. J., Standish, E. M., and
Wimberly, R. N.: JPL's On-Line Solar System Data Service, in: Bulletin of
the American Astronomical Society, vol. 28, p. 1158, 1996.

</mixed-citation></ref-html>
<ref-html id="bib1.bib6"><label>Gottwald and Bovensmann(2011)</label><mixed-citation>
Gottwald, M. and Bovensmann, H. (Eds.): SCIAMACHY – Exploring the Changing
Earth's Atmosphere, Springer, Dordrecht, Heidelberg, London, New York, 2011.
</mixed-citation></ref-html>
<ref-html id="bib1.bib7"><label>Gottwald et al.(2007)</label><mixed-citation>
Gottwald, M., Krieg, E., von Savigny, C., Noël, S., Bovensmann, H., and
Bramstedt, K.: Determination of SCIAMACHY Line-of-Sight Misalignments,
Proc. Envisat Symposium, Montreux Switzerland 23–27 April, SP-636, 2007.
</mixed-citation></ref-html>
<ref-html id="bib1.bib8"><label>Jayles et al.(2006)</label><mixed-citation>
Jayles, C., Nhun-Fat, B., and Tourain, C.: DORIS: System Description and
Control of the Signal Integrity, J. Geodesy, 80, 457–472,
<a href="https://doi.org/10.1007/s00190-006-0046-8" target="_blank">https://doi.org/10.1016/10.1007/s00190-006-0046-8</a>, 2006.
</mixed-citation></ref-html>
<ref-html id="bib1.bib9"><label>Kaiser et al.(2004)</label><mixed-citation>
Kaiser, J. W., von Savigny, C., Eichmann, K. U., Noël, S., Bovensmann,
H., Frerick, J., and Burrows, J. P.: Satellite-pointing retrieval from
atmospheric limb-scattering of solar UV-B radiation, Can. J.
Phys., 82, 1041–1052, <a href="https://doi.org/10.1139/p04-071" target="_blank">https://doi.org/10.1016/10.1139/p04-071</a>,
2004.
</mixed-citation></ref-html>
<ref-html id="bib1.bib10"><label>Kieffer and Stone(2005)</label><mixed-citation>
Kieffer, H. H. and Stone, T. C.: The Spectral Irradiance of the Moon,
Astron. J., 129, 2887, <a href="https://doi.org/10.1086/430185" target="_blank">https://doi.org/10.1016/10.1086/430185</a>, 2005.
</mixed-citation></ref-html>
<ref-html id="bib1.bib11"><label>Legrand and Chevalley(2013a)</label><mixed-citation>
Legrand, C. and Chevalley, P.: Virtual Moon Atlas ”Pro 6” Freeware, in:
Lunar and Planetary Science Conference, vol. 44 of Lunar and Planetary
Inst. Technical Report, p. 1021, 2013a.
</mixed-citation></ref-html>
<ref-html id="bib1.bib12"><label>Legrand and Chevalley(2013b)</label><mixed-citation>
Legrand, C. and Chevalley, P.: Virtual Moon Atlas “Pro” Version 6.0,
<a href="http://www.ap-i.net/avl/en/start" target="_blank">http://www.ap-i.net/avl/en/start</a> (last access: 1 June 2015),
2013b.
</mixed-citation></ref-html>
<ref-html id="bib1.bib13"><label>Muñoz(2011)</label><mixed-citation>
Muñoz, C. V.: Re-Engineering of Mission Analysis Software for Envisat-1,
General Software User Manual, Tech. Rep. PO-IS-DMS-GS-0556, Issue 5.9, ESA,
DEIMOS Space S.L.U, Madrid,
<a href="http://eop-cfi.esa.int/index.php/docs-and-mission-data/cfi-docs" target="_blank">http://eop-cfi.esa.int/index.php/docs-and-mission-data/cfi-docs</a> (last access: 27 June 2017),
2011.
</mixed-citation></ref-html>
<ref-html id="bib1.bib14"><label>von Savigny et al.(2005)</label><mixed-citation>
von Savigny, C., Kaiser, J. W., Bovensmann, H., Burrows, J. P., McDermid, I.
S., and Leblanc, T.: Spatial and temporal characterization of SCIAMACHY limb
pointing errors during the first three years of the mission, Atmos. Chem.
Phys., 5, 2593–2602, <a href="https://doi.org/10.5194/acp-5-2593-2005" target="_blank">https://doi.org/10.1016/10.5194/acp-5-2593-2005</a>, 2005.
</mixed-citation></ref-html>
<ref-html id="bib1.bib15"><label>Willis et al.(2006)</label><mixed-citation>
Willis, P., Jayles, C., and Bar-Sever, Y.: DORIS: From orbit determination for
altimeter missions to geodesy, C. R. Geosci., 338, 968–979,
<a href="https://doi.org/10.1016/j.crte.2005.11.013" target="_blank">https://doi.org/10.1016/10.1016/j.crte.2005.11.013</a>,  2006.
</mixed-citation></ref-html>
<ref-html id="bib1.bib16"><label>Yeomans et al.(1996)</label><mixed-citation>
Yeomans, D., Chamberlin, A., Giorgini, J., Chodas, P., Jacobson, R., Keesey,
M., Lieske, J., Ostro, S., Standish, E., and Wimberly, R.: The JPL HORIZONS
on-line solar system data and ephemeris computation service,
<a href="http://ssd.jpl.nasa.gov/?horizons" target="_blank">http://ssd.jpl.nasa.gov/?horizons</a> (last access: 1 September 2016),
1996.
</mixed-citation></ref-html>--></article>
