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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-10-3589-2017</article-id><title-group><article-title>Tropospheric products of the second GOP European GNSS reprocessing (1996–2014)</article-title>
      </title-group><?xmltex \runningtitle{Tropospheric products of the second GOP European GNSS reprocessing (1996--2014)}?><?xmltex \runningauthor{J. Dousa et al.}?>
      <contrib-group>
        <contrib contrib-type="author" corresp="yes" rid="aff1">
          <name><surname>Dousa</surname><given-names>Jan</given-names></name>
          <email>jan.dousa@pecny.cz</email>
        <ext-link>https://orcid.org/0000-0002-6668-6207</ext-link></contrib>
        <contrib contrib-type="author" corresp="no" rid="aff1">
          <name><surname>Vaclavovic</surname><given-names>Pavel</given-names></name>
          
        </contrib>
        <contrib contrib-type="author" corresp="no" rid="aff1">
          <name><surname>Elias</surname><given-names>Michal</given-names></name>
          
        <ext-link>https://orcid.org/0000-0001-5661-4982</ext-link></contrib>
        <aff id="aff1"><institution>NTIS – New Technologies for the Information Society, Geodetic Observatory Pecný, RIGTC, 250 66 Zdiby, Czech Republic</institution>
        </aff>
      </contrib-group>
      <author-notes><corresp id="corr1">Jan Dousa (jan.dousa@pecny.cz)</corresp></author-notes><pub-date><day>29</day><month>September</month><year>2017</year></pub-date>
      
      <volume>10</volume>
      <issue>9</issue>
      <fpage>3589</fpage><lpage>3607</lpage>
      <history>
        <date date-type="received"><day>15</day><month>January</month><year>2017</year></date>
           <date date-type="rev-request"><day>2</day><month>February</month><year>2017</year></date>
           <date date-type="rev-recd"><day>14</day><month>August</month><year>2017</year></date>
           <date date-type="accepted"><day>28</day><month>August</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>
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</permissions><self-uri xlink:href="https://amt.copernicus.org/articles/10/3589/2017/amt-10-3589-2017.html">This article is available from https://amt.copernicus.org/articles/10/3589/2017/amt-10-3589-2017.html</self-uri>
<self-uri xlink:href="https://amt.copernicus.org/articles/10/3589/2017/amt-10-3589-2017.pdf">The full text article is available as a PDF file from https://amt.copernicus.org/articles/10/3589/2017/amt-10-3589-2017.pdf</self-uri>


      <abstract>
    <p>In this paper, we present results of the second reprocessing of all data from
1996 to 2014 from all stations in International Association of Geodesy (IAG)
Reference Frame Sub-Commission for Europe (EUREF) Permanent Network
(EPN) as performed at the Geodetic Observatory Pecný (GOP). While the original
goal of this research was to ultimately contribute to the realization of a
new European Terrestrial Reference System (ETRS), we also aim to provide a
new set of GNSS (Global Navigation Satellite System) tropospheric parameter
time series with possible applications to climate research. To achieve these
goals, we improved a strategy to guarantee the continuity of these
tropospheric parameters and we prepared several variants of troposphere
modelling. We then assessed all solutions in terms of the repeatability of
coordinates as an internal evaluation of applied models and strategies and in
terms of zenith tropospheric delays (ZTDs) and horizontal gradients with
those of the ERA-Interim numerical weather model (NWM) reanalysis. When
compared to the GOP Repro1 (first EUREF reprocessing) solution, the results
of the GOP Repro2 (second EUREF reprocessing) yielded improvements of
approximately 50 and 25 % in the repeatability of the horizontal and
vertical components, respectively, and of approximately 9 % in tropospheric
parameters. Vertical repeatability was reduced from 4.14 to 3.73 mm when
using the VMF1 mapping function, a priori ZHD (zenith hydrostatic delay), and
non-tidal atmospheric loading corrections from actual weather data. Raising
the elevation cut-off angle from 3 to 7<inline-formula><mml:math id="M1" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> and then to 10<inline-formula><mml:math id="M2" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula>
increased RMS from coordinates' repeatability, which was then confirmed by
independently comparing GNSS tropospheric parameters with the NWM reanalysis.
The assessment of tropospheric horizontal gradients with respect to the
ERA-Interim revealed a strong sensitivity of estimated gradients to the
quality of GNSS antenna tracking performance. This impact was demonstrated at
the Mallorca station, where gradients systematically grew up to 5 mm during
the period between 2003 and 2008, before this behaviour disappeared when the
antenna at the station was changed. The impact of processing variants on
long-term ZTD trend estimates was assessed at 172 EUREF stations with time
series longer than 10 years. The most significant site-specific impact was
due to the non-tidal atmospheric loading followed by the impact of changing
the elevation cut-off angle from 3 to 10<inline-formula><mml:math id="M3" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula>. The other processing
strategy had a very small or negligible impact on estimated trends.</p>
  </abstract>
    </article-meta>
  </front>
<body>
      

<sec id="Ch1.S1" sec-type="intro">
  <title>Introduction</title>
      <p>The US Global Positioning System (GPS) became operational in 1995 as the
first Global Navigation Satellite System (GNSS). Since that time, this
technology has been transformed into a fundamental technique for positioning
and navigation in everyday life. Hundreds of GPS permanent stations have
been deployed for scientific purposes throughout Europe and the world, and
the first stations have collected GPS data for approximately the last two
decades. In 1994, a science-driven global network of continuously operating
GPS stations was established by the International GNSS Service, IGS
(Dow et al.m 2009), of the International Association of
Geodesy (IAG) to support the determination of precise GPS/GNSS orbits, and
clock and earth rotation parameters, which are necessary for obtaining
high-accuracy GNSS analyses for scientific applications. A similar network,
but regional in its scope, was also organized by the IAG Reference Frame
Sub-Commission for Europe (EUREF) in 1996, which was called the EUREF
Permanent Network (EPN; Bruyninx et al.,
2012). Although its primary purpose was to maintain the European Terrestrial
Reference System (ETRS), the EPN also attempted to develop a pan-European
infrastructure for scientific projects and co-operations (Ihde et al., 2014).
Since 1996, the EPN has grown to include approximately 300 operating
stations, which are regularly distributed throughout Europe and its
surrounding areas. Today, EPN data are routinely analysed by 18 EUREF
analysis centres.</p>
      <p>Throughout the past two decades, GPS data analyses of both global and
regional networks have been affected by various changes in processing
strategy and updates of precise models and products, reference frames and
software packages. To reduce discontinuities in products, particularly
within coordinate time series, homogeneous reprocessing was initiated by the
IGS and EUREF on a global and regional scale, respectively. To exploit the
improvements in these IGS global products, the second European
reprocessing was performed in 2015–2016, with the ultimate goal of providing
a newly realized ETRS.</p>
      <p>Currently, station coordinate parameter time series from reprocessed
solutions are mainly used in the solid earth sciences as well as to maintain
global and regional terrestrial reference systems. Additionally, from an
analytical perspective, the long-term series of estimated parameters and
their residuals are useful for assessing the performances of applied models
and strategies over a given period. Moreover, tropospheric parameters
derived from this GNSS reanalysis could be useful for climate research (Yuan
et al., 1993), due to their high temporal resolution and unrivalled relative
accuracy for sensing water vapour when compared to other techniques, such as
radio sounding, water vapour radiometers and radio occultation (Ning,
2012). In this context, the GNSS zenith tropospheric delay (ZTD) represents
a site-specific parameter characterizing the total signal path delay in the
zenith due to both dry (hydrostatic) and wet contributions of the neutral
atmosphere, the latter of which is known to be proportional to precipitable
water (Bevis et al., 1994).</p>
      <p>With the second EUREF reprocessing, the secondary goal of the Geodetic
Observatory Pecný (GOP) was to support the activity of Working Group 3 of
the COST Action ES1206 (Guerova et al., 2016), which addresses the evaluation
of existing and future GNSS tropospheric products and assesses their
potential uses in climate research. For this purpose, the GOP provided
several solution variants, with a special focus on optimal tropospheric
estimates, including VMF1 vs. GMF mapping functions, the use of different
elevation cut-off angles and estimates of tropospheric horizontal gradients
using different time resolutions. Additionally, in order to enhance
tropospheric outputs, we improved the processing strategy in a variety of
ways compared to the GOP Repro1 (first EUREF reprocessing) solutions
(Douša and Václavovic, 2012): (1) by combining tropospheric
parameters during midnights and across GPS week breaks, (2) by checking
weekly coordinates before their substitutions in order to estimate
tropospheric parameters and (3) by filtering out problematic stations by
checking the consistency of daily coordinates. The results of this GOP
reprocessing, including all available variants, were assessed using internal
evaluations of applied models and strategy settings and using external
validations with independent tropospheric parameters derived from numerical
weather model (NWM) reanalyses.</p>
      <p>The processing strategy used in the second GOP reanalysis of the EUREF
Permanent Network is described in Sect. 2, and the new approach that is
developed to guarantee a continuity of estimated tropospheric parameters during midnights as well as between different GPS weeks is summarized in Sect. 3.
The relationship between mean tropospheric horizontal gradients and the
quality of low-elevation GNSS tracking is explained in Sect. 4. The
results of internal and external evaluations of GOP solution variants and
processing models are presented in Sect. 4, and the assessment of impacts
of specific variants on estimated ZTD trends are is presented in Sect. 5. The last section
concludes our findings and suggests avenues of future research.</p>
</sec>
<sec id="Ch1.S2">
  <title>GOP processing strategy and solution variants</title>
      <p>The EUREF GOP analysis centre was established in 1997 and contributed to
operational EUREF analyses until 2013 by providing final, rapid and near-real-time solutions. Recently, the GOP changed its contributions to that of a
long-term homogeneous reprocessing of all data from the EPN historical
archive. The GOP solution of the first EUREF reanalysis
(Völksen, 2011) comprised the processing of a subnetwork of 70 EPN
stations during the period of 1996–2008. In 2011, for the first time, the GOP
reprocessed the entire EPN network (spanning a period of 1996–2010) in order
to validate the European reference frame and to provide the first
homogeneous time series of tropospheric parameters for all EPN stations
(Douša and Václavovic, 2012).</p>
      <p>In the second EUREF reprocessing (Repro2), the GOP analysed data obtained from
the entire EPN network from a period of 1996–2014 using the Bernese GNSS
Software version 5.2 (Dach et al., 2015). The GOP strategy relies on a network
approach utilizing double-difference observations. Only GPS data from the
EPN stations were included according to official validity intervals provided
by the EPN Central Bureau (<uri>http://epncb.oma.be</uri>). Two products
were derived from the reprocessing campaign in order to contribute to a
combination at the EUREF level performed by the coordinator of analysis
centres and the coordinator of troposphere products: (1) site coordinates and
corresponding variance–covariance information in daily and weekly SINEX
files and (2) site tropospheric parameters in daily Solution (Software/technique) INdependent EXchange
Format for combination of TROpospheric estimates (SINEX_TRO) files.</p>

<?xmltex \floatpos{t}?><table-wrap id="Ch1.T1" specific-use="star"><caption><p>Characteristics of GOP reprocessing models.</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="justify" colwidth="398.338583pt"/>
     <oasis:thead>
       <oasis:row rowsep="1">  
         <oasis:entry colname="col1">Processing options</oasis:entry>  
         <oasis:entry colname="col2">Description</oasis:entry>
       </oasis:row>
     </oasis:thead>
     <oasis:tbody>
       <oasis:row>  
         <oasis:entry colname="col1">Products</oasis:entry>  
         <oasis:entry colname="col2">CODE precise orbit and earth rotation parameters from the second reprocessing.</oasis:entry>
       </oasis:row>
       <oasis:row>  
         <oasis:entry colname="col1">Observations</oasis:entry>  
         <oasis:entry colname="col2">Dual-frequency code and phase GPS observations from L1 and L2 carriers. Elevation cut-off angle 3<inline-formula><mml:math id="M4" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula>, elevation-dependent weighting <inline-formula><mml:math id="M5" display="inline"><mml:mrow><mml:mn mathvariant="normal">1</mml:mn><mml:mo>/</mml:mo><mml:msup><mml:mi>cos⁡</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msup></mml:mrow></mml:math></inline-formula> (zenith), double-difference observations and observations with 3 min sampling rate.</oasis:entry>
       </oasis:row>
       <oasis:row>  
         <oasis:entry colname="col1">Reference frame</oasis:entry>  
         <oasis:entry colname="col2">IGb08 realization – core stations set as fiducial after a consistency checking. Coordinates estimated using a minimum constraint.</oasis:entry>
       </oasis:row>
       <oasis:row>  
         <oasis:entry colname="col1">Antenna model</oasis:entry>  
         <oasis:entry colname="col2">GOP: IGS08_1832 model (receiver and satellite phase centre offsets and variations).</oasis:entry>
       </oasis:row>
       <oasis:row>  
         <oasis:entry colname="col1">Troposphere</oasis:entry>  
         <oasis:entry colname="col2">A priori zenith hydrostatic delay/mapping function: GPT/GMFh (GO0) and VMF1/VMF1h (GO1–GO6). Estimated ZWD corrections every hour using the VMF1 wet mapping function – 5  and 1 m for absolute and relative constraints, respectively. Estimated horizontal NS and EW tropospheric gradients every 6 h (GO0–GO5) or 24 h (GO6) without a priori tropospheric gradients and constraints.</oasis:entry>
       </oasis:row>
       <oasis:row>  
         <oasis:entry colname="col1">Ionosphere</oasis:entry>  
         <oasis:entry colname="col2">Eliminated using the ionosphere-free linear combination (GO0–GO6). Applying higher-order effects estimated using the CODE global ionosphere product (GO5).</oasis:entry>
       </oasis:row>
       <oasis:row>  
         <oasis:entry colname="col1">Loading effects</oasis:entry>  
         <oasis:entry colname="col2">Atmospheric tidal loading and hydrology loading not applied. Ocean tidal loading FES2004 used. Non-tidal atmospheric loading introduced in advanced variants from the model from TU Vienna (GO4–GO6).</oasis:entry>
       </oasis:row>
     </oasis:tbody>
   </oasis:tgroup></oasis:table></table-wrap>

      <?xmltex \floatpos{t}?><fig id="Ch1.F1"><caption><p>EUREF Permanent Network's clusters (designated by different
colours) in the second GOP reprocessing.</p></caption>
        <?xmltex \igopts{width=241.848425pt}?><graphic xlink:href="https://amt.copernicus.org/articles/10/3589/2017/amt-10-3589-2017-f01.pdf"/>

      </fig>

      <p>This GOP processing was clustered into eight subnetworks
(Fig. 1) and then stacked into daily network
solutions with pre-eliminated integer phase ambiguities when ensuring strong
ties to the IGS08 reference frame. This strategy introduced state-of-the-art
models (IERS Conventions, 2010) that are recommended as standards for highly
accurate GNSS analyses, particularly for the maintenance of the reference
frame. Additionally, the use of precise orbits obtained from the second
CODE (Centre of Orbit Determination in Europe) global reprocessing (Dach et al., 2014) guaranteed complete consistency
between all models on both the provider and user sides. Characteristics of
this GOP data reprocessing strategy and their models are summarized in
Table 1. Additionally, seven processing variants
were performed during the GOP Repro2 analysis for studying selected models
or settings: (a) applying the tropospheric mapping function model GMF (Böhm
et al., 2006a) vs. VMF1 (Böhm et al., 2006b), with the latter based on actual
weather information; (b) increasing the temporal resolution of tropospheric
linear horizontal gradients in the north and east directions; (c) using
three different elevation cut-off angles, namely 3, 7 and 10<inline-formula><mml:math id="M6" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula>; (d) modelling atmospheric loading
effects; and (e) modelling higher-order ionospheric effects.
Table 2 summarizes the settings and models of
solution variants selected for generating coordinate and troposphere
products, which are supplemented with variant rationales.</p>

<?xmltex \floatpos{t}?><table-wrap id="Ch1.T2" specific-use="star"><caption><p>GOP solution variants for the assessment of selected models and
settings.</p></caption><oasis:table frame="topbot"><oasis:tgroup cols="3">
     <oasis:colspec colnum="1" colname="col1" align="left"/>
     <oasis:colspec colnum="2" colname="col2" align="left"/>
     <oasis:colspec colnum="3" colname="col3" align="left"/>
     <oasis:thead>
       <oasis:row rowsep="1">  
         <oasis:entry colname="col1">Solution ID</oasis:entry>  
         <oasis:entry colname="col2">Specific settings and differences</oasis:entry>  
         <oasis:entry colname="col3">Remarks and rationales</oasis:entry>
       </oasis:row>
     </oasis:thead>
     <oasis:tbody>
       <oasis:row>  
         <oasis:entry colname="col1">GO0</oasis:entry>  
         <oasis:entry colname="col2">GMF and 3<inline-formula><mml:math id="M7" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> cut-off</oasis:entry>  
         <oasis:entry colname="col3">Legacy solution for Repro1</oasis:entry>
       </oasis:row>
       <oasis:row>  
         <oasis:entry colname="col1">GO1</oasis:entry>  
         <oasis:entry colname="col2">VMF1 and 3<inline-formula><mml:math id="M8" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> cut-off</oasis:entry>  
         <oasis:entry colname="col3">New candidate for Repro2</oasis:entry>
       </oasis:row>
       <oasis:row>  
         <oasis:entry colname="col1">GO2</oasis:entry>  
         <oasis:entry colname="col2">Same as GO1; 7<inline-formula><mml:math id="M9" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> cut-off</oasis:entry>  
         <oasis:entry colname="col3">Impact of elevation cut-off angle</oasis:entry>
       </oasis:row>
       <oasis:row>  
         <oasis:entry colname="col1">GO3</oasis:entry>  
         <oasis:entry colname="col2">Same as GO1; 10<inline-formula><mml:math id="M10" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> cut-off</oasis:entry>  
         <oasis:entry colname="col3">Impact of elevation cut-off angle</oasis:entry>
       </oasis:row>
       <oasis:row>  
         <oasis:entry colname="col1">GO4</oasis:entry>  
         <oasis:entry colname="col2">Same as GO1; atmospheric loading</oasis:entry>  
         <oasis:entry colname="col3">Non-tidal atmospheric loading applied</oasis:entry>
       </oasis:row>
       <oasis:row>  
         <oasis:entry colname="col1">GO5</oasis:entry>  
         <oasis:entry colname="col2">Same as GO4; higher-order ionosphere</oasis:entry>  
         <oasis:entry colname="col3">Higher-order ionosphere effect not applied</oasis:entry>
       </oasis:row>
       <oasis:row>  
         <oasis:entry colname="col1">GO6</oasis:entry>  
         <oasis:entry colname="col2">Same as GO4; 24 h gradients</oasis:entry>  
         <oasis:entry colname="col3">Stacking tropospheric gradients to 24 h sampling</oasis:entry>
       </oasis:row>
     </oasis:tbody>
   </oasis:tgroup></oasis:table></table-wrap>

      <p>Within the processing, we screened station coordinate repeatabilities from
weekly combined solutions and we identified any problematic station for
which the north/east/up residuals exceeded 15/15/30 mm or RMS of the north/east/up
coordinate component exceeded values 10/10/20 mm. Such station was a priori
excluded from the tropospheric product for the corresponding day. There were
other standard control procedures within the processing when the individual
station could have been excluded, e.g. if (a) less than 60 % of GNSS data
were available, (b) code or phase data revealed poor quality, (c) station metadata
were found inconsistent with data file header information (receiver, antenna
and dome names, antenna eccentricities), and (d) phase residuals were too
large for all satellites in the processing period, indicating a problem with
the station. Tropospheric parameters were estimated practically without
constraints (a priori <inline-formula><mml:math id="M11" display="inline"><mml:mi mathvariant="italic">σ</mml:mi></mml:math></inline-formula> greater than 1 m); thus, parameter formal errors
reflect the relative uncertainties of estimates. Usually, large errors indicate
the lack of observations contributing to the parameter. During the
tropospheric parameter evaluations, we applied the filter for exceeding formal
errors of estimated parameters (ZTD <inline-formula><mml:math id="M12" display="inline"><mml:mi mathvariant="italic">σ</mml:mi></mml:math></inline-formula> greater than 3 mm, normal cases
stay below 1 mm).</p>
</sec>
<sec id="Ch1.S3">
  <title>Ensuring ZTD continuity during midnights</title>
      <p>When site tropospheric parameter time series generated from the second
EUREF reprocessing are applied to climate research, they should be free of
artificial offsets in order to avoid misinterpretations (Bock et al., 2014).
However, GNSS processing is commonly performed on a daily basis according to
adopted standards for data and product dissemination. Thus far, EUREF
analysis centres have provided independent daily solutions, although precise
IGS products are combined and distributed on a weekly basis. Station
coordinates are estimated on a daily basis and are later combined to form
more stable weekly solutions. According to the EUREF analysis centre
guidelines (<uri>http://www.epncb.oma.be/_documentation/guidelines/guidelines_analysis_centres.pdf</uri>), weekly coordinates should be used to estimate tropospheric
parameters on a daily basis, but there are no requirements with which to
guarantee the continuity of tropospheric parameters during midnights.
Additionally, there are also discontinuities on a weekly basis, as neither
daily coordinates nor hourly tropospheric parameters are combined across
midnights between corresponding adjacent GPS weeks.</p>
      <p>The impact of a 3-day combination was previously studied when assessing the
tropospheric parameters stemming from the second IGS reprocessing campaign
2016 in the GOP-TropDB database (Győri and Douša, 2016). We compared two
global tropospheric products provided by the analysis centre CODE differing only in the procedure of combining
tropospheric parameters from the daily original solutions. The first
product, COF, was based purely on a single-day solution while the second
product, COD, was based on a 3-day combination (Dach et al., 2014). Sub-daily
statistics were calculated by comparing 2 h ZTD estimates from both
products during 2013. There were no significant biases observed, but mean
standard deviation estimated from differences reached 0.8 mm in ZTD over a
day and almost 1.8 mm close to the day boundaries. Similarly, a dispersion
characterized by 1<inline-formula><mml:math id="M13" display="inline"><mml:mi mathvariant="italic">σ</mml:mi></mml:math></inline-formula> over all stations reached 0.5 mm for the former but up to 1.2 mm for the latter. Actual differences in ZTDs could even be
larger, because this case used approximations leading to smooth
low-resolution values close to the day boundaries.</p>
      <p>During the first GOP reprocessing, there was no way to guarantee
tropospheric parameter continuity at midnight, as the troposphere was
modelled by applying a piecewise constant model. In these cases,
tropospheric parameters with a temporal resolution of 1 h were reported
in the middle of the hour, as was originally estimated. In the second GOP
reprocessing, using again hourly estimates, we applied a piecewise linear
model for the tropospheric parameters. The parameter continuities during midnights were not guaranteed implicitly, but only by an explicit
combination of parameters at daily boundaries. For the combination procedure
we used 3 consecutive days while the tropospheric product stems from the
middle day. The procedure is done again for 3 consecutive days shifted
by 1 day. A similar procedure, using the piecewise constant model, was
applied for estimating weekly coordinates which aimed to minimize remaining
effects in consistency at the breaks of GPS weeks (on Saturday at midnight).
The coordinates of the weekly solution corresponding to the middle day of a
3-day combination were fixed for the tropospheric parameter estimates.
In the last step, we transformed the piecewise linear model to the piecewise
constant model expressed in the middle of each hourly interval (HR:30),
which was saved in the SINEX_TRO format to support the EUREF combination
procedure requiring such sampling. The original piecewise linear parameter
model was thus lost, and, to retain this information in the official product
in the SINEX_TRO format, we additionally stored values for full hours
(HR:00). Figure 2 summarizes four plots displaying
tropospheric solutions with discontinuities in the left panels (a, c) and
enforcing tropospheric continuities in the right panels (b, d). While the
upper plots (a, b) display the piecewise constant model, bottom plots (c, d) indicate the solution representing the piecewise linear model. The GOP
Repro1 implementation is thus represented by the Fig. 2a plot while the GOP Repro2 solution corresponds to
Fig. 2d and, alternatively, Fig. 2b.</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F2" specific-use="star"><caption><p>Charts of four variants of representation of tropospheric parameters
in time (<inline-formula><mml:math id="M14" display="inline"><mml:mi>x</mml:mi></mml:math></inline-formula> axis, with no specific dates). Right <bold>(b, d)</bold> and left
<bold>(a, c)</bold> panels display estimates made with and without midnight
combinations, respectively. Top <bold>(a, b)</bold> and bottom <bold>(c, d)</bold>
panels display the piecewise constant and the linear model, respectively. Ok
vs. not ok indicates a consistency vs. inconsistency, respectively, at
daily or GPS week boundaries, the latter representing a specific case of the
former.</p></caption>
        <?xmltex \igopts{width=355.659449pt}?><graphic xlink:href="https://amt.copernicus.org/articles/10/3589/2017/amt-10-3589-2017-f02.png"/>

      </fig>

      <p>These theoretical concepts were practically tested using a limited dataset
in 1996 (Fig. 3). The panels in Fig. 3 follow the organization of the
theoretical plots shown in Fig. 2; corresponding
formal errors are also plotted along with estimated ZTDs. Discontinuities
are visible in the left-hand plots and are usually accompanied by increasing
formal errors for parameters close to data interval boundaries. As expected,
discontinuities disappear in the right-hand plots. Although the values
between 23:30 and 00:30 on 2 adjacent days are not connected by a line in
the top-right plot, continuity was enforced for midnight parameters anyway,
as seen in the bottom-right plot. Formal errors also became smooth near day
boundaries, thus characterizing the contribution of data from both days and
demonstrating that the concept behaves as expected in its practical
implementation.</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F3" specific-use="star"><caption><p>Four variants of representation of tropospheric parameters.
Right <bold>(b, d)</bold> and left <bold>(a, c)</bold> panels display estimates with and without
midnight combinations, respectively. Top <bold>(a, b)</bold> and bottom <bold>(c, d)</bold> panels
display the piecewise constant and the piecewise linear model, respectively.</p></caption>
        <?xmltex \igopts{width=412.564961pt}?><graphic xlink:href="https://amt.copernicus.org/articles/10/3589/2017/amt-10-3589-2017-f03.png"/>

      </fig>

</sec>
<sec id="Ch1.S4">
  <title>Quality of the observations and impact on tropospheric gradients</title>
      <p>Recently, we have developed a new interactive web interface to conduct
tropospheric parameter comparisons in the GOP-TropDB (Győri and
Douša, 2016), which is being prepared for the IGS Tropospheric Working
Group web (<uri>http://twg.igs.org/</uri>; Dousa et al., 2017). Using the
interface, we observed large systematic tropospheric gradients during
specific years at several EPN stations. Generally, from GNSS data, we can
only estimate total tropospheric horizontal gradients without being able to
distinguish between dry and wet contributions. The former is mostly due to
horizontal asymmetry in atmospheric pressure, and the latter is due to
asymmetry in the water vapour content. The latter is thus more variable in
time and space than the former (Li et al., 2015). Regardless, mean gradients
should be close to zero, whereas dry gradients may tend to point slightly
more to the equator, corresponding to latitudinal changes in atmosphere
thickness (Meindl et al., 2004). Similarly, orography-triggered horizontal
gradients can appear due to the presence of high mountain ranges in the
vicinity of the station (Morel et al., 2015). Such systematic effects can
reach the maximum submillimetre level, while a higher long-term gradient
(i.e. that above 1 mm) is likely more indicative of issues with site
instrumentation, the environment or modelling effects. Therefore, in order to
clearly identify these systematic effects, we also compared our gradients
with those calculated from the ERA-Interim.</p>
      <p>It is beyond the scope of this paper to investigate in detail the correlation
between tropospheric horizontal gradients and effects such as antenna
tracking performance. However, we do observe a strong impact in the most
extreme case identified when comparing gradients from the GNSS and the
ERA-Interim for all EPN stations. Figure 4 shows the monthly means of
differences in the north and east tropospheric gradients from the MALL
station (Mallorca, Spain). These differences increase from 0 mm up to
<inline-formula><mml:math id="M15" display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>4 mm and 2 mm for the east and north gradients, respectively, within the
period of June 2003–October 2008. Such large monthly differences in GNSS and
NWM gradients are not realistic and were attributed to data processing when
long-term increasing biases dropped down to zero on 1 November 2008,
immediately after the antenna and receiver were changed at the station.
During the same period, yearly mean ZTD differences in the ERA-Interim
steadily changed from about 3 mm to about <inline-formula><mml:math id="M16" display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>12 mm and immediately dropped
down to <inline-formula><mml:math id="M17" display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>2 mm in 2008 after the antenna change.</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F4" specific-use="star"><caption><p>MALL station – monthly mean differences in tropospheric horizontal
gradients with respect to the ERA-Interim.</p></caption>
        <?xmltex \igopts{width=355.659449pt}?><graphic xlink:href="https://amt.copernicus.org/articles/10/3589/2017/amt-10-3589-2017-f04.pdf"/>

      </fig>

      <p>The EPN Central Bureau (<uri>http://epncb.oma.be</uri>), operating at the Royal
Observatory of Belgium (ROB), provides a web service for monitoring GNSS
data quality and includes monthly snapshots of the tracking characteristics
of all stations. The sequence of plots displayed in
Fig. 5, representing the interval of interest
(2002, 2004, 2006 and 2008), reveals a slow but systematic and horizontally
asymmetric degradation of the capability of the antenna to track
low-elevation observations at the station. Therefore, we analysed days of
the year (DoY) 302 and 306 (corresponding to 28 October and 1 November 2008) with the in-house G-Nut/Anubis software (Václavovic and Douša,
2016) and observed differences in the sky plots of these 2 days. The
left-hand plot in Fig. 6 depicts the severe loss
of dual-frequency observations up to a 25<inline-formula><mml:math id="M18" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> elevation cut-off angle
in the southeast direction (with an azimuth of 90–180<inline-formula><mml:math id="M19" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula>), which causes the tropospheric linear gradient of
approximately 5 mm to point in the opposite direction. Figure 10 also
demonstrates that an increasing loss of second frequency observations
appears to occur in the east (represented as black dots). The right-hand
plot in this figure demonstrates that both of these effects fully
disappeared after the antenna was replaced on 30 October 2008 (DoY 304),
resulting in the appearance of normal sky plot characteristics and a GLONASS
constellation with one satellite providing only single-frequency
observations (represented as black lines).</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F5" specific-use="star"><caption><p>Low-elevation tracking problems at the MALL station during the
period of 2003–2008. From top-left to bottom-right: January 2002, 2004, 2006
and 2008 (courtesy of the EPN Central Bureau, ROB).</p></caption>
        <?xmltex \igopts{width=412.564961pt}?><graphic xlink:href="https://amt.copernicus.org/articles/10/3589/2017/amt-10-3589-2017-f05.png"/>

      </fig>

      <?xmltex \floatpos{t}?><fig id="Ch1.F6" specific-use="star"><caption><p>Sky plots before <bold>(a)</bold> and after <bold>(b)</bold> replacing the
malfunctioning antenna at the MALL site (30 October 2008). Blue and green
dots represent GPS and GLONASS (GLO), respectively, while black dots indicate
single-frequency observations.</p></caption>
        <?xmltex \igopts{width=355.659449pt}?><graphic xlink:href="https://amt.copernicus.org/articles/10/3589/2017/amt-10-3589-2017-f06.png"/>

      </fig>

      <p>This situation demonstrates the high sensitivity of the estimated gradients
on data asymmetry, particularly at low-elevation angles. The systematic
behaviour of these monthly mean gradients, their variations from independent
data and a profound progress over time seem to be useful indicators of
instrumentation-related issues at permanent GNSS stations. It is also
considered that gradient parameters can be a valuable method as a part of ZTD
data screening procedure (Bock et al., 2016).</p>
      <p>Although the station MALL represented an extreme case, biases at other
stations were observed too, e.g. GOPE (1996–2002), TRAB (1999–2008), CREU
(2000–2002), HERS (1999–2001), GAIA (2008–2014) and others. Site-specific,
spatially or temporally correlated biases suggest different possible reasons
such as site-instrumentation effects including the tracking quality and
phase centre variation (PCV) models, site-environment effects including multipath
and seasonal variation (e.g. winter snow–ice coverage), edge-network effects
when processing double-difference observations, spatially correlated effects
in reference frame realization and possibly others. The problematic stations
and periods mentioned above were however still included in comparisons and
trend analysis because of the lack of objective criteria for their
identification, which should be studied in future.</p>
</sec>
<sec id="Ch1.S5">
  <title>Assessment of reprocessing solutions</title>
      <p>The GOP variants and reprocessing models were assessed by a number of criteria,
including those of the internal evaluations of repeatability of station
coordinates, residuals at reference stations and the external validation of
ZTDs and tropospheric horizontal gradients with data from numerical weather
model reanalyses.</p>
<sec id="Ch1.S5.SS1">
  <title>Repeatability of station coordinates</title>
      <p>We used coordinate repeatability to assess the quality of models applied in
GNSS analysis. To be as thorough as possible, we not only assessed all GOP
Repro2 variants but also assessed two GOP Repro1 solutions in order to
discern improvements within the new reanalyses. The two Repro1 solutions
differed in their used reference frames and PCV models: IGS05 and IGS08.</p>

<?xmltex \floatpos{t}?><table-wrap id="Ch1.T3"><caption><p>Comparison of GOP solution variants for north, east and up
coordinate repeatability.</p></caption><oasis:table frame="topbot"><?xmltex \begin{scaleboxenv}{.95}[.95]?><oasis:tgroup cols="4">
     <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:thead>
       <oasis:row>  
         <oasis:entry colname="col1">Solution</oasis:entry>  
         <oasis:entry colname="col2">North RMS</oasis:entry>  
         <oasis:entry colname="col3">East RMS</oasis:entry>  
         <oasis:entry colname="col4">Up RMS</oasis:entry>
       </oasis:row>
       <oasis:row rowsep="1">  
         <oasis:entry colname="col1"/>  
         <oasis:entry colname="col2">(mm)</oasis:entry>  
         <oasis:entry colname="col3">(mm)</oasis:entry>  
         <oasis:entry colname="col4">(mm)</oasis:entry>
       </oasis:row>
     </oasis:thead>
     <oasis:tbody>
       <oasis:row>  
         <oasis:entry colname="col1">GOP Repro1/IGS05</oasis:entry>  
         <oasis:entry colname="col2">3.01</oasis:entry>  
         <oasis:entry colname="col3">2.40</oasis:entry>  
         <oasis:entry colname="col4">5.08</oasis:entry>
       </oasis:row>
       <oasis:row>  
         <oasis:entry colname="col1">GOP Repro1/IGS08</oasis:entry>  
         <oasis:entry colname="col2">2.64</oasis:entry>  
         <oasis:entry colname="col3">2.21</oasis:entry>  
         <oasis:entry colname="col4">4.94</oasis:entry>
       </oasis:row>
       <oasis:row>  
         <oasis:entry colname="col1">GO0</oasis:entry>  
         <oasis:entry colname="col2">1.20</oasis:entry>  
         <oasis:entry colname="col3">1.30</oasis:entry>  
         <oasis:entry colname="col4">4.14</oasis:entry>
       </oasis:row>
       <oasis:row>  
         <oasis:entry colname="col1">GO1</oasis:entry>  
         <oasis:entry colname="col2">1.23</oasis:entry>  
         <oasis:entry colname="col3">1.33</oasis:entry>  
         <oasis:entry colname="col4">3.97</oasis:entry>
       </oasis:row>
       <oasis:row>  
         <oasis:entry colname="col1">GO2</oasis:entry>  
         <oasis:entry colname="col2">1.24</oasis:entry>  
         <oasis:entry colname="col3">1.33</oasis:entry>  
         <oasis:entry colname="col4">4.01</oasis:entry>
       </oasis:row>
       <oasis:row>  
         <oasis:entry colname="col1">GO3</oasis:entry>  
         <oasis:entry colname="col2">1.26</oasis:entry>  
         <oasis:entry colname="col3">1.34</oasis:entry>  
         <oasis:entry colname="col4">4.07</oasis:entry>
       </oasis:row>
       <oasis:row>  
         <oasis:entry colname="col1">GO4</oasis:entry>  
         <oasis:entry colname="col2">1.14</oasis:entry>  
         <oasis:entry colname="col3">1.24</oasis:entry>  
         <oasis:entry colname="col4">3.73</oasis:entry>
       </oasis:row>
       <oasis:row>  
         <oasis:entry colname="col1">GO5</oasis:entry>  
         <oasis:entry colname="col2">1.14</oasis:entry>  
         <oasis:entry colname="col3">1.24</oasis:entry>  
         <oasis:entry colname="col4">3.73</oasis:entry>
       </oasis:row>
       <oasis:row>  
         <oasis:entry colname="col1">GO6</oasis:entry>  
         <oasis:entry colname="col2">1.14</oasis:entry>  
         <oasis:entry colname="col3">1.24</oasis:entry>  
         <oasis:entry colname="col4">3.73</oasis:entry>
       </oasis:row>
     </oasis:tbody>
   </oasis:tgroup><?xmltex \end{scaleboxenv}?></oasis:table></table-wrap>

      <p>Table 3 summarizes mean coordinate repeatability in
the north, east and up components of all stations from their weekly
combinations. All GOP Repro2 solution variants reached approximately 50
and 25 % of the lower mean RMS of coordinate repeatability when compared
to the GOP Repro1/IGS08 solution in its horizontal and vertical components,
respectively. These values represent even greater improvements when compared
to the GOP Repro1/IGS05 solution. Comparing these two Repro1 solutions
clearly demonstrates the beneficial impact of the new PCV models and
reference frames. The observed differences between Repro2 and Repro1 also
indicate an overall improvement of the processing software from version 5.0 to
5.2 and the enhanced quality of global precise orbit and earth orientation
products.</p>
      <p>Various GOP Repro2 solutions were also used to assess the selected models.
Variants GO0 and GO1 differ in their mapping functions (GMF vs. VMF1) used to
project ZTDs into slant path delays. These comparisons demonstrate that
vertical component repeatability improved from 4.14 to 3.97 mm, whereas
horizontal component repeatability decreased slightly. By increasing the
elevation cut-off angle from 3 to 7<inline-formula><mml:math id="M20" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> (GO2) and
10<inline-formula><mml:math id="M21" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> (GO3), we observed a slight increase in RMS from repeatability
of all coordinates. This can be explained by the positive impact of
low-elevation observations on the decorrelation of height and tropospheric
parameters, despite the fact that applied models (such as
elevation-dependent weighting, PCVs, multipath) are still not optimal for
including observations at very low-elevation angles. On the other hand, it
should be noted that the VMF1 mapping function is particularly tuned to
observations at 3<inline-formula><mml:math id="M22" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> elevation angle, which leads to biases at higher
elevation angles (Zus et al., 2015).</p>
      <p>The GO4 solution represents an official GOP contribution to EUREF combined
products. It is identical to the variant GO1 but applies a non-tidal
atmospheric loading. Steigenberger et al. (2009) discussed the importance of
applying non-tidal atmospheric loading corrections together with a precise a
priori ZHD (zenith hydrostatic
delay) model. It has been concluded that using mean, or slowly varying,
empirical pressure values for estimating a priori ZHD instead of true
pressure values results in a partial compensation of atmospheric loading
effects, which is the case of the GO1 solution. A positive 10 % improvement in
height repeatability was observed for the GO4 solution. Our improvement was
slightly lower than in a global scope reported by Dach et al. (2011) with an
improvement of 10–20 % over all stations. As the effect depends on
the selected stations, a slightly higher impact in a global scale might be
attributed to the station distribution, particularly differences in terms of
latitude and altitude.
<?xmltex \hack{\newpage}?>
No impact was observed from the higher-order ionospheric effects (GO4 vs.
GO5) in terms of coordinate repeatability. As the effect is systematic within
the regional network (Fritsche et al., 2005), it was mostly eliminated by
using reference stations in the domains of interest. The combination of
tropospheric horizontal gradients from 6 to 24 h time resolution (GO4 vs.
GO6), using the piecewise linear model, had a negligible impact on the
repeatability of station coordinates too.</p>
</sec>
<sec id="Ch1.S5.SS2">
  <title>Reference frame – residuals at fiducial stations</title>
      <p>The terrestrial reference frame (Altamimi et al., 2001) is a realization of
a geocentric system of coordinates used by space geodetic techniques. To
avoid a degradation of GNSS products, differential GNSS analysis methods
require a proper referencing of the solution to the system applied in the
generation of precise GNSS orbit products. For this purpose, we often use
the concept of fiducial stations with precise coordinates well known in the
requested system. Such stations are used to define the geodetic datum while
their actual position can be readjusted by applying a condition minimizing
coordinate residuals. No station is able to guarantee a stable
position
and unchanged instrumentation during the whole reprocessing
period. Thus a set of about 50 stations, with more than 100 time periods for
reference coordinates, was carefully prepared for datum definition in the
GOP reprocessing. An iterative procedure was then applied for every day by
comparing a priori reference coordinates with actually estimated ones and
excluding fiducial stations exceeding differences by 5, 5 and 15 mm in the north,
east and up components.</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F7" specific-use="star"><caption><p>Statistics of the daily reference system realization: <bold>(a)</bold> RMS of
residuals at fiducial stations (representing the total, height and
position); <bold>(b)</bold> number of stations (all and accepted after an iterative
control).</p></caption>
          <?xmltex \igopts{width=355.659449pt}?><graphic xlink:href="https://amt.copernicus.org/articles/10/3589/2017/amt-10-3589-2017-f07.png"/>

        </fig>

      <p>Figure 7 shows the evolution of the number of
actually used fiducial stations (represented as red dots) from all
configured fiducial sites (represented as black dots) after applying an
iterative procedure of validation on a daily basis. This reprocessing began
with the use of 16–20 fiducial stations in 1996, and this number increased
to reach a maximum of over 50 during the period from 2003 to 2011. After 2011,
this number decreased, due to a common loss of reference stations available
from the last realization of the global terrestrial reference frame without
changes in its instrumentation. In most cases, only 2 or 3 stations were
excluded from the total number; however, this number is lower for some daily
solutions, indicating the removal of even more stations. The lowest number
of fiducial sites (12) was identified on day 209 of the year 1999, while
low numbers were generally observed at the beginning of the reprocessing
period, in 1996. We observed consistent mean RMS errors for horizontal,
vertical and total residuals of 6.47, 10.22 and 12.25 mm and 4.83, 7.94 and
9.35 mm for daily and weekly solutions, respectively, which demonstrate the
stability of the reference system in the reprocessing. The seasonality in
height coordinate estimates characterized by the RMS of residuals from the
reference frame realization is dominated by errors due to modelling of the
troposphere. We believe the main contribution stems from the
insufficiencies in modelling of wet tropospheric delay, as the effect has
the most pronounced seasonal signal within the GNSS data analysis.
Additionally, the estimated station ZTD parameters and height are difficult
to decorrelate. In the next section, the strong seasonal variation in
comparing zenith total delays estimated from GNSS and NWM data is clearly
visible.</p>
</sec>
<sec id="Ch1.S5.SS3">
  <title>Zenith total delays</title>
      <p>We compared all reprocessed tropospheric parameters with respect to
independent data from the ERA-Interim global reanalysis (Dee et al., 2011)
provided by the European Centre for Medium-Range Weather Forecasts
from 1969 to the present. For the period of 1996–2014, we calculated
tropospheric parameters (namely ZTD and tropospheric horizontal linear
gradients) from the NWM for all EPN stations using the GFZ (German Research
Centre for Geosciences) ray-tracing software (Zus et al., 2014). The
comparison of tropospheric parameters was performed by applying the linear
interpolation of GNSS parameters to the original NWM 6 h representation,
using the GOP-TropoDB (Győri and Douša, 2016). For monthly
statistics discussed in this section, we applied an iterative procedure for
outlier detection using the 3<inline-formula><mml:math id="M23" display="inline"><mml:mi mathvariant="italic">σ</mml:mi></mml:math></inline-formula> criteria calculated from the compared
ZTD or gradient differences.</p>

<?xmltex \floatpos{t}?><table-wrap id="Ch1.T4" specific-use="star"><caption><p>Statistics (bias and standard deviations) of ZTD and tropospheric
gradients from the seven reprocessing variants compared to those obtained
from the ERA-Interim NWM reanalysis. In addition to the statistics, the 1<inline-formula><mml:math id="M24" display="inline"><mml:mi mathvariant="italic">σ</mml:mi></mml:math></inline-formula>
range over the ensemble of stations is provided.</p></caption><oasis:table frame="topbot"><oasis:tgroup cols="7">
     <oasis:colspec colnum="1" colname="col1" align="left"/>
     <oasis:colspec colnum="2" colname="col2" align="center"/>
     <oasis:colspec colnum="3" colname="col3" align="center"/>
     <oasis:colspec colnum="4" colname="col4" align="center"/>
     <oasis:colspec colnum="5" colname="col5" align="center"/>
     <oasis:colspec colnum="6" colname="col6" align="center"/>
     <oasis:colspec colnum="7" colname="col7" align="center"/>
     <oasis:thead>
       <oasis:row>  
         <oasis:entry colname="col1">Solution</oasis:entry>  
         <oasis:entry colname="col2">ZTD bias</oasis:entry>  
         <oasis:entry colname="col3">ZTD SD</oasis:entry>  
         <oasis:entry colname="col4">EGRD bias</oasis:entry>  
         <oasis:entry colname="col5">EGRD SD</oasis:entry>  
         <oasis:entry colname="col6">NGRD bias</oasis:entry>  
         <oasis:entry colname="col7">NGRD SD</oasis:entry>
       </oasis:row>
       <oasis:row rowsep="1">  
         <oasis:entry colname="col1"/>  
         <oasis:entry colname="col2">(mm)</oasis:entry>  
         <oasis:entry colname="col3">(mm)</oasis:entry>  
         <oasis:entry colname="col4">(mm)</oasis:entry>  
         <oasis:entry colname="col5">(mm)</oasis:entry>  
         <oasis:entry colname="col6">(mm)</oasis:entry>  
         <oasis:entry colname="col7">(mm)</oasis:entry>
       </oasis:row>
     </oasis:thead>
     <oasis:tbody>
       <oasis:row>  
         <oasis:entry colname="col1">GO0</oasis:entry>  
         <oasis:entry colname="col2"><inline-formula><mml:math id="M25" display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>1.5 <inline-formula><mml:math id="M26" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> 2.1</oasis:entry>  
         <oasis:entry colname="col3">8.8 <inline-formula><mml:math id="M27" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> 2.0</oasis:entry>  
         <oasis:entry colname="col4"><inline-formula><mml:math id="M28" display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>0.04 <inline-formula><mml:math id="M29" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> 0.08</oasis:entry>  
         <oasis:entry colname="col5">0.39 <inline-formula><mml:math id="M30" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> 0.10</oasis:entry>  
         <oasis:entry colname="col6"><inline-formula><mml:math id="M31" display="inline"><mml:mrow><mml:mo>+</mml:mo><mml:mn mathvariant="normal">0.01</mml:mn><mml:mo>±</mml:mo><mml:mn mathvariant="normal">0.09</mml:mn></mml:mrow></mml:math></inline-formula></oasis:entry>  
         <oasis:entry colname="col7">0.43 <inline-formula><mml:math id="M32" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> 0.12</oasis:entry>
       </oasis:row>
       <oasis:row>  
         <oasis:entry colname="col1">GO1</oasis:entry>  
         <oasis:entry colname="col2"><inline-formula><mml:math id="M33" display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>2.0 <inline-formula><mml:math id="M34" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> 2.1</oasis:entry>  
         <oasis:entry colname="col3">8.3 <inline-formula><mml:math id="M35" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> 2.2</oasis:entry>  
         <oasis:entry colname="col4"><inline-formula><mml:math id="M36" display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>0.04 <inline-formula><mml:math id="M37" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> 0.08</oasis:entry>  
         <oasis:entry colname="col5">0.39 <inline-formula><mml:math id="M38" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> 0.10</oasis:entry>  
         <oasis:entry colname="col6"><inline-formula><mml:math id="M39" display="inline"><mml:mrow><mml:mo>+</mml:mo><mml:mn mathvariant="normal">0.01</mml:mn><mml:mo>±</mml:mo><mml:mn mathvariant="normal">0.09</mml:mn></mml:mrow></mml:math></inline-formula></oasis:entry>  
         <oasis:entry colname="col7">0.42 <inline-formula><mml:math id="M40" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> 0.13</oasis:entry>
       </oasis:row>
       <oasis:row>  
         <oasis:entry colname="col1">GO2</oasis:entry>  
         <oasis:entry colname="col2"><inline-formula><mml:math id="M41" display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>1.9 <inline-formula><mml:math id="M42" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> 2.2</oasis:entry>  
         <oasis:entry colname="col3">8.4 <inline-formula><mml:math id="M43" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> 2.2</oasis:entry>  
         <oasis:entry colname="col4"><inline-formula><mml:math id="M44" display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>0.05 <inline-formula><mml:math id="M45" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> 0.10</oasis:entry>  
         <oasis:entry colname="col5">0.41 <inline-formula><mml:math id="M46" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> 0.10</oasis:entry>  
         <oasis:entry colname="col6"><inline-formula><mml:math id="M47" display="inline"><mml:mrow><mml:mo>+</mml:mo><mml:mn mathvariant="normal">0.00</mml:mn><mml:mo>±</mml:mo><mml:mn mathvariant="normal">0.12</mml:mn></mml:mrow></mml:math></inline-formula></oasis:entry>  
         <oasis:entry colname="col7">0.45 <inline-formula><mml:math id="M48" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> 0.12</oasis:entry>
       </oasis:row>
       <oasis:row>  
         <oasis:entry colname="col1">GO3</oasis:entry>  
         <oasis:entry colname="col2"><inline-formula><mml:math id="M49" display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>1.8 <inline-formula><mml:math id="M50" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> 2.3</oasis:entry>  
         <oasis:entry colname="col3"><inline-formula><mml:math id="M51" display="inline"><mml:mn mathvariant="normal">8</mml:mn></mml:math></inline-formula>.5 <inline-formula><mml:math id="M52" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> 2.1</oasis:entry>  
         <oasis:entry colname="col4"><inline-formula><mml:math id="M53" display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>0.08 <inline-formula><mml:math id="M54" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> 0.13</oasis:entry>  
         <oasis:entry colname="col5">0.43 <inline-formula><mml:math id="M55" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> 0.11</oasis:entry>  
         <oasis:entry colname="col6"><inline-formula><mml:math id="M56" display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>0.01 <inline-formula><mml:math id="M57" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> 0.14</oasis:entry>  
         <oasis:entry colname="col7">0.49 <inline-formula><mml:math id="M58" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> 0.12</oasis:entry>
       </oasis:row>
       <oasis:row>  
         <oasis:entry colname="col1">GO4</oasis:entry>  
         <oasis:entry colname="col2"><inline-formula><mml:math id="M59" display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>1.8 <inline-formula><mml:math id="M60" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> 2.4</oasis:entry>  
         <oasis:entry colname="col3">8.1 <inline-formula><mml:math id="M61" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> 2.1</oasis:entry>  
         <oasis:entry colname="col4"><inline-formula><mml:math id="M62" display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>0.04 <inline-formula><mml:math id="M63" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> 0.09</oasis:entry>  
         <oasis:entry colname="col5">0.38 <inline-formula><mml:math id="M64" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> 0.10</oasis:entry>  
         <oasis:entry colname="col6"><inline-formula><mml:math id="M65" display="inline"><mml:mrow><mml:mo>+</mml:mo><mml:mn mathvariant="normal">0.00</mml:mn><mml:mo>±</mml:mo><mml:mn mathvariant="normal">0.09</mml:mn></mml:mrow></mml:math></inline-formula></oasis:entry>  
         <oasis:entry colname="col7">0.40 <inline-formula><mml:math id="M66" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> 0.12</oasis:entry>
       </oasis:row>
       <oasis:row>  
         <oasis:entry colname="col1">GO5</oasis:entry>  
         <oasis:entry colname="col2"><inline-formula><mml:math id="M67" display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>1.8 <inline-formula><mml:math id="M68" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> 2.4</oasis:entry>  
         <oasis:entry colname="col3">8.1 <inline-formula><mml:math id="M69" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> 2.1</oasis:entry>  
         <oasis:entry colname="col4"><inline-formula><mml:math id="M70" display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>0.05 <inline-formula><mml:math id="M71" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> 0.09</oasis:entry>  
         <oasis:entry colname="col5">0.38 <inline-formula><mml:math id="M72" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> 0.10</oasis:entry>  
         <oasis:entry colname="col6"><inline-formula><mml:math id="M73" display="inline"><mml:mrow><mml:mo>+</mml:mo><mml:mn mathvariant="normal">0.01</mml:mn><mml:mo>±</mml:mo><mml:mn mathvariant="normal">0.08</mml:mn></mml:mrow></mml:math></inline-formula></oasis:entry>  
         <oasis:entry colname="col7">0.40 <inline-formula><mml:math id="M74" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> 0.12</oasis:entry>
       </oasis:row>
       <oasis:row>  
         <oasis:entry colname="col1">GO6</oasis:entry>  
         <oasis:entry colname="col2"><inline-formula><mml:math id="M75" display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>1.8 <inline-formula><mml:math id="M76" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> 2.4</oasis:entry>  
         <oasis:entry colname="col3">8.2 <inline-formula><mml:math id="M77" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> 2.1</oasis:entry>  
         <oasis:entry colname="col4"><inline-formula><mml:math id="M78" display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>0.04 <inline-formula><mml:math id="M79" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> 0.08</oasis:entry>  
         <oasis:entry colname="col5">0.29 <inline-formula><mml:math id="M80" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> 0.06</oasis:entry>  
         <oasis:entry colname="col6"><inline-formula><mml:math id="M81" display="inline"><mml:mrow><mml:mo>+</mml:mo><mml:mn mathvariant="normal">0.01</mml:mn><mml:mo>±</mml:mo><mml:mn mathvariant="normal">0.09</mml:mn></mml:mrow></mml:math></inline-formula></oasis:entry>  
         <oasis:entry colname="col7">0.28 <inline-formula><mml:math id="M82" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> 0.06</oasis:entry>
       </oasis:row>
     </oasis:tbody>
   </oasis:tgroup></oasis:table></table-wrap>

      <p>Table 4 summarizes comparisons of GNSS ZTDs, and
tropospheric horizontal gradients, from all GOP processing variants with
those obtained from the ERA-Interim. Mean biases and standard deviations
were first calculated for each station and each month and then the mean and
standard deviation of these values were computed, characterizing dispersions
of all statistical values over the ensemble of stations.</p>
      <p>The results in the table indicate a mean ZTD bias <inline-formula><mml:math id="M83" display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>1.8 mm for all
comparisons (GNSS–NWM) suggesting ZTDs achieved from the NWM reanalysis
are drier than those obtained from GNSS reprocessing. Similar biases have
been observed for all other European GNSS reprocessing products during the
period of 1996–2014 (Pacione et al., 2017). On the other hand, when
processing the ERA-Interim using two different software and methodologies
within the GNSS4SWEC Benchmark campaign (Douša et al., 2016) during May and
June of 2013 in Central Europe, and by their comparison to two GNSS reference
products based on different processing methods, we observed bias differences
within <inline-formula><mml:math id="M84" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula>0.4 mm in ZTD. As neither GNSS nor NWM is able to sense the
troposphere with an absolute accuracy better than the bias that we observed,
we cannot make any conclusion, except for its independence from the GNSS software. A
mixture of common processing aspects such as the scale of the GNSS network, applied
tropospheric model, precise orbit product and others could still cause such
small biases in GNSS analysis at least.</p>
      <p>Comparing the results of the official GOP Repro2 solution (GO4) to those of
the legacy solution (GO0) demonstrates an overall improvement of 9 % in
terms of accuracy, which corresponds to a similar comparison between the
EUREF Repro1 and Repro2 products (Pacione et al., 2017). The improvement is
assumed to be even larger (indicated by the coordinate repeatability) since
the comparison of tropospheric parameters is limited by a lower quality of
reference products derived from NWM data (Douša et al., 2016;
Kačmařík et al., 2017; Bock and Nuret, 2009).</p>
      <p>Comparing the GO1 and GO0 variants demonstrates that the VMF1 mapping
function outperforms GMF in terms of the standard deviation if the elevation
cut-off angle of 3<inline-formula><mml:math id="M85" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> is used. The change of mapping function
together with the use of more accurate a priori ZHD resulted in the ZTD
standard deviation improving from 8.8 mm (GO0) to 8.3 mm (GO1). However,
bias was slightly increased, which could be partly attributed to the use of
the mean pressure model compensating for part of
the non-tidal atmospheric loading (see Sect. 5.1).
Using non-tidal atmospheric loading
corrections along with precise modelling of a priori ZHD contributed to a
small reduction of the bias from <inline-formula><mml:math id="M86" display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>2.0 to <inline-formula><mml:math id="M87" display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>1.8 mm and, mainly, to the
improvement by reducing this ZTD accuracy to 8.1 mm (GO4). This corresponds
with the previous assessment of the repeatability of station coordinates.
Degradation in ZTD precision was also observed when the elevation cut-off
angle was raised from 3 to 7<inline-formula><mml:math id="M88" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> (GO2) or 10<inline-formula><mml:math id="M89" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula>
(GO3). No impacts on ZTD were visible from additional
modelling of high-order ionospheric effects (GO5) or from stacking of
6 h horizontal gradients into daily piecewise linear estimates (GO6).</p>
      <p>Figure 8 displays the time series of statistics
from comparisons of the GOP official ZTD product (GO4) with respect to the
results of the ERA-Interim reanalysis. Mean bias and standard deviation were
derived from the monthly statistics of the 6-hourly GNSS–ERA-Interim ZTD differences. A
1<inline-formula><mml:math id="M90" display="inline"><mml:mi mathvariant="italic">σ</mml:mi></mml:math></inline-formula> range of the mean values, represented by error bars, are
additionally derived from all stations on a monthly basis. Although the time
series show homogeneous results over the given time span, a small increase
in the mean standard deviation over time likely corresponds with the increasing
number of EPN sites, rising from approximately 30 to 300. The early years
(1996–2001) also display a worse overall agreement in the 1<inline-formula><mml:math id="M91" display="inline"><mml:mi mathvariant="italic">σ</mml:mi></mml:math></inline-formula> range of mean
values over all stations, which can be attributed to the varying quality of
historical observations and precise orbit products. The mean bias varies
from <inline-formula><mml:math id="M92" display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>3 to 1 mm during the period of 1996–2014, with a long-term mean of
<inline-formula><mml:math id="M93" display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>1.8 mm (Table 4). The long-term mean is also
relatively small compared to the ZTD mean 1<inline-formula><mml:math id="M94" display="inline"><mml:mi mathvariant="italic">σ</mml:mi></mml:math></inline-formula> range of 3–5 mm.</p>
</sec>
<sec id="Ch1.S5.SS4">
  <title>Tropospheric horizontal linear gradients</title>
      <p>Additional GNSS signal delay due to the tropospheric gradients were
developed by MacMillan (1995). The complete tropospheric model for the
line-of-sight delay (<inline-formula><mml:math id="M95" display="inline"><mml:mrow><mml:mi mathvariant="normal">Δ</mml:mi><mml:msub><mml:mi>D</mml:mi><mml:mi mathvariant="normal">T</mml:mi></mml:msub><mml:mo>)</mml:mo></mml:mrow></mml:math></inline-formula> using the parameters zenith hydrostatic
delay, zenith wet delay (ZWD), and first-order horizontal tropospheric
gradients <inline-formula><mml:math id="M96" display="inline"><mml:mrow><mml:msub><mml:mi>G</mml:mi><mml:mi>N</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> and <inline-formula><mml:math id="M97" display="inline"><mml:mrow><mml:msub><mml:mi>G</mml:mi><mml:mi>E</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula>, all expressed in units of length, is
described as follows:

                <disp-formula specific-use="align" content-type="numbered"><mml:math id="M98" display="block"><mml:mtable displaystyle="true"><mml:mtr><mml:mtd><mml:mrow><mml:mstyle class="stylechange" displaystyle="true"/><mml:mi mathvariant="normal">Δ</mml:mi><mml:msub><mml:mi>D</mml:mi><mml:mi mathvariant="normal">T</mml:mi></mml:msub></mml:mrow></mml:mtd><mml:mtd><mml:mrow><mml:mstyle displaystyle="true" class="stylechange"/><mml:mo>=</mml:mo><mml:msub><mml:mi mathvariant="normal">mf</mml:mi><mml:mi mathvariant="normal">h</mml:mi></mml:msub><mml:mo>(</mml:mo><mml:mi>e</mml:mi><mml:mo>)</mml:mo><mml:mi mathvariant="normal">ZHD</mml:mi><mml:mo>+</mml:mo><mml:msub><mml:mi mathvariant="normal">mf</mml:mi><mml:mi mathvariant="normal">w</mml:mi></mml:msub><mml:mo>(</mml:mo><mml:mi>e</mml:mi><mml:mo>)</mml:mo><mml:mi mathvariant="normal">ZWD</mml:mi></mml:mrow></mml:mtd></mml:mtr><mml:mlabeledtr id="Ch1.E1"><mml:mtd/><mml:mtd><mml:mstyle class="stylechange" displaystyle="true"/></mml:mtd><mml:mtd><mml:mrow><mml:mstyle displaystyle="true" class="stylechange"/><mml:mo>+</mml:mo><mml:msub><mml:mi mathvariant="normal">mf</mml:mi><mml:mi mathvariant="normal">g</mml:mi></mml:msub><mml:mo>(</mml:mo><mml:mi>e</mml:mi><mml:mo>)</mml:mo><mml:mi>cot⁡</mml:mi><mml:mo>(</mml:mo><mml:mi>e</mml:mi><mml:mo>)</mml:mo><mml:mo>[</mml:mo><mml:msub><mml:mi>G</mml:mi><mml:mi>N</mml:mi></mml:msub><mml:mi>cos⁡</mml:mi><mml:mo>(</mml:mo><mml:mi>A</mml:mi><mml:mo>)</mml:mo><mml:mo>+</mml:mo><mml:msub><mml:mi>G</mml:mi><mml:mi>E</mml:mi></mml:msub><mml:mi>sin⁡</mml:mi><mml:mo>(</mml:mo><mml:mi>A</mml:mi><mml:mo>)</mml:mo><mml:mo>]</mml:mo><mml:mo>,</mml:mo></mml:mrow></mml:mtd></mml:mlabeledtr></mml:mtable></mml:math></disp-formula>

            where <inline-formula><mml:math id="M99" display="inline"><mml:mi>e</mml:mi></mml:math></inline-formula> and <inline-formula><mml:math id="M100" display="inline"><mml:mi>A</mml:mi></mml:math></inline-formula> are observation elevation and azimuth angles and mf<inline-formula><mml:math id="M101" display="inline"><mml:msub><mml:mi/><mml:mi mathvariant="normal">h</mml:mi></mml:msub></mml:math></inline-formula>, mf<inline-formula><mml:math id="M102" display="inline"><mml:msub><mml:mi/><mml:mi mathvariant="normal">w</mml:mi></mml:msub></mml:math></inline-formula>, mf<inline-formula><mml:math id="M103" display="inline"><mml:msub><mml:mi/><mml:mi mathvariant="normal">g</mml:mi></mml:msub></mml:math></inline-formula>
are hydrostatic, wet and gradient mapping functions, respectively, representing the
projection from an elevation to the zenith. Horizontal gradients should
optimally represent a ZTD change in north and east
directions characterized by terms <inline-formula><mml:math id="M104" display="inline"><mml:mrow><mml:msub><mml:mi>G</mml:mi><mml:mi>N</mml:mi></mml:msub><mml:mi>cot⁡</mml:mi><mml:mo>(</mml:mo><mml:mi>e</mml:mi><mml:mo>)</mml:mo></mml:mrow></mml:math></inline-formula> and <inline-formula><mml:math id="M105" display="inline"><mml:mrow><mml:msub><mml:mi>G</mml:mi><mml:mi>E</mml:mi></mml:msub><mml:mi>cot⁡</mml:mi><mml:mo>(</mml:mo><mml:mi>e</mml:mi><mml:mo>)</mml:mo></mml:mrow></mml:math></inline-formula> in the equation. However, the gradients need to be parameterized
practically with respect to observation elevation angle instead of the
distance theoretically applicable to the tropospheric effect at various
elevation angles. The interpretation of the tropospheric horizontal
gradients in the Bernese software represents the north and east components of
angle applied for the tilting the zenith direction in the mapping function
with gradients representing (in unit of length) the tilting angle multiplied
by the delay in zenith (Meindl et al., 2004).</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F8" specific-use="star"><caption><p>Monthly means of bias and standard deviation of the official GOP ZTD
products compared to those of the ERA-Interim. Error bars indicate standard
errors of mean values over all compared stations.</p></caption>
          <?xmltex \igopts{width=355.659449pt}?><graphic xlink:href="https://amt.copernicus.org/articles/10/3589/2017/amt-10-3589-2017-f08.pdf"/>

        </fig>

      <?xmltex \floatpos{t}?><fig id="Ch1.F9" specific-use="star"><caption><p>Monthly means of bias and standard deviation of tropospheric
horizontal north (N-GRD) and east (E-GRD) gradients compared to those
obtained by the ERA-Interim. Note that similar products are almost superposed. Error
bars indicate standard errors of mean values over all compared stations
plotted from the zero <inline-formula><mml:math id="M106" display="inline"><mml:mi>y</mml:mi></mml:math></inline-formula> axis to emphasize seasonal variations and trends.
Error bars are displayed for north gradients only; however, they are
representative for the east gradients too.</p></caption>
          <?xmltex \igopts{width=355.659449pt}?><graphic xlink:href="https://amt.copernicus.org/articles/10/3589/2017/amt-10-3589-2017-f09.png"/>

        </fig>

      <p>Similarly as in the case of the ZTD and coordinate assessment, Table 4 shows that
tropospheric gradients became worse when raising the elevation cut-off angle
from 3  to 7<inline-formula><mml:math id="M107" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> (GO2) or 10<inline-formula><mml:math id="M108" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> (GO3). Mean
standard deviations of the GO2 and GO3 solutions increased by 8 and
12 %, respectively, which is valid for the whole period of monthly time
series (not shown). No significant differences in temporal variations of
mean biases of the north and east tropospheric gradient variants were
identified while they shared a higher variability during the years
1996–2001. No impact of modelling of high-order ionospheric effects (GO5)
was observed. Statistics of GO4 and GO6 solutions compared to the ERA-Interim
revealed that standard deviations dropped from 0.38  to 0.28 mm and from
0.40  to 0.29 mm for the east and north gradients, respectively. The worse
performance of the GO4 solution is attributed to the fact that tropospheric
horizontal gradients were estimated with a 6 h sampling interval using the
piecewise linear model by applying practically no absolute or relative
constraints. In such cases, increased correlations of the gradients with
other parameters can cause instabilities in processing certain stations at
specific times; the gradients absorb some remaining errors in the GNSS
analysis model. The mean biases of the tropospheric gradients are considered
to be negligible, but it was demonstrated in Sect. 4 that some large systematic effects were indeed
discovered and attributed to the quality of GNSS signal tracking.</p>

<?xmltex \floatpos{t}?><table-wrap id="Ch1.T5" specific-use="star"><caption><p>Median, minimum (min) and maximum (max) values of total ZTD biases
and standard deviation (SD) over all stations. Units are millimetres.</p></caption><oasis:table frame="topbot"><oasis:tgroup cols="7">
     <oasis:colspec colnum="1" colname="col1" align="left"/>
     <oasis:colspec colnum="2" colname="col2" align="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:thead>
       <oasis:row>  
         <oasis:entry colname="col1">Compared</oasis:entry>  
         <oasis:entry colname="col2">ZTD bias</oasis:entry>  
         <oasis:entry colname="col3">ZTD bias</oasis:entry>  
         <oasis:entry colname="col4">ZTD bias</oasis:entry>  
         <oasis:entry colname="col5">ZTD SD</oasis:entry>  
         <oasis:entry colname="col6">ZTD SD</oasis:entry>  
         <oasis:entry colname="col7">ZTD SD</oasis:entry>
       </oasis:row>
       <oasis:row rowsep="1">  
         <oasis:entry colname="col1">variants</oasis:entry>  
         <oasis:entry colname="col2">median</oasis:entry>  
         <oasis:entry colname="col3">min</oasis:entry>  
         <oasis:entry colname="col4">max</oasis:entry>  
         <oasis:entry colname="col5">median</oasis:entry>  
         <oasis:entry colname="col6">min</oasis:entry>  
         <oasis:entry colname="col7">max</oasis:entry>
       </oasis:row>
     </oasis:thead>
     <oasis:tbody>
       <oasis:row>  
         <oasis:entry colname="col1">GO1–GO0</oasis:entry>  
         <oasis:entry colname="col2"><inline-formula><mml:math id="M109" display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>0.36</oasis:entry>  
         <oasis:entry colname="col3"><inline-formula><mml:math id="M110" display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>1.52</oasis:entry>  
         <oasis:entry colname="col4"><inline-formula><mml:math id="M111" display="inline"><mml:mrow><mml:mo>+</mml:mo><mml:mn mathvariant="normal">0.70</mml:mn></mml:mrow></mml:math></inline-formula></oasis:entry>  
         <oasis:entry colname="col5">2.01</oasis:entry>  
         <oasis:entry colname="col6">0.69</oasis:entry>  
         <oasis:entry colname="col7">3.82</oasis:entry>
       </oasis:row>
       <oasis:row>  
         <oasis:entry colname="col1">GO2–GO1</oasis:entry>  
         <oasis:entry colname="col2"><inline-formula><mml:math id="M112" display="inline"><mml:mrow><mml:mo>+</mml:mo><mml:mn mathvariant="normal">0.03</mml:mn></mml:mrow></mml:math></inline-formula></oasis:entry>  
         <oasis:entry colname="col3"><inline-formula><mml:math id="M113" display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>0.81</oasis:entry>  
         <oasis:entry colname="col4"><inline-formula><mml:math id="M114" display="inline"><mml:mrow><mml:mo>+</mml:mo><mml:mn mathvariant="normal">1.66</mml:mn></mml:mrow></mml:math></inline-formula></oasis:entry>  
         <oasis:entry colname="col5">0.66</oasis:entry>  
         <oasis:entry colname="col6">0.15</oasis:entry>  
         <oasis:entry colname="col7">1.29</oasis:entry>
       </oasis:row>
       <oasis:row>  
         <oasis:entry colname="col1">GO3–GO1</oasis:entry>  
         <oasis:entry colname="col2"><inline-formula><mml:math id="M115" display="inline"><mml:mrow><mml:mo>+</mml:mo><mml:mn mathvariant="normal">0.03</mml:mn></mml:mrow></mml:math></inline-formula></oasis:entry>  
         <oasis:entry colname="col3"><inline-formula><mml:math id="M116" display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>2.22</oasis:entry>  
         <oasis:entry colname="col4"><inline-formula><mml:math id="M117" display="inline"><mml:mrow><mml:mo>+</mml:mo><mml:mn mathvariant="normal">2.66</mml:mn></mml:mrow></mml:math></inline-formula></oasis:entry>  
         <oasis:entry colname="col5">1.10</oasis:entry>  
         <oasis:entry colname="col6">0.31</oasis:entry>  
         <oasis:entry colname="col7">2.04</oasis:entry>
       </oasis:row>
       <oasis:row>  
         <oasis:entry colname="col1">GO4–GO1</oasis:entry>  
         <oasis:entry colname="col2"><inline-formula><mml:math id="M118" display="inline"><mml:mrow><mml:mo>+</mml:mo><mml:mn mathvariant="normal">0.05</mml:mn></mml:mrow></mml:math></inline-formula></oasis:entry>  
         <oasis:entry colname="col3"><inline-formula><mml:math id="M119" display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>3.29</oasis:entry>  
         <oasis:entry colname="col4"><inline-formula><mml:math id="M120" display="inline"><mml:mrow><mml:mo>+</mml:mo><mml:mn mathvariant="normal">5.55</mml:mn></mml:mrow></mml:math></inline-formula></oasis:entry>  
         <oasis:entry colname="col5">1.37</oasis:entry>  
         <oasis:entry colname="col6">0.68</oasis:entry>  
         <oasis:entry colname="col7">4.72</oasis:entry>
       </oasis:row>
       <oasis:row>  
         <oasis:entry colname="col1">GO5–GO4</oasis:entry>  
         <oasis:entry colname="col2"><inline-formula><mml:math id="M121" display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>0.02</oasis:entry>  
         <oasis:entry colname="col3"><inline-formula><mml:math id="M122" display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>0.31</oasis:entry>  
         <oasis:entry colname="col4"><inline-formula><mml:math id="M123" display="inline"><mml:mrow><mml:mo>+</mml:mo><mml:mn mathvariant="normal">0.07</mml:mn></mml:mrow></mml:math></inline-formula></oasis:entry>  
         <oasis:entry colname="col5">0.07</oasis:entry>  
         <oasis:entry colname="col6">0.04</oasis:entry>  
         <oasis:entry colname="col7">0.30</oasis:entry>
       </oasis:row>
       <oasis:row>  
         <oasis:entry colname="col1">GO6–GO4</oasis:entry>  
         <oasis:entry colname="col2"><inline-formula><mml:math id="M124" display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>0.02</oasis:entry>  
         <oasis:entry colname="col3"><inline-formula><mml:math id="M125" display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>0.23</oasis:entry>  
         <oasis:entry colname="col4"><inline-formula><mml:math id="M126" display="inline"><mml:mrow><mml:mo>+</mml:mo><mml:mn mathvariant="normal">0.16</mml:mn></mml:mrow></mml:math></inline-formula></oasis:entry>  
         <oasis:entry colname="col5">1.24</oasis:entry>  
         <oasis:entry colname="col6">0.76</oasis:entry>  
         <oasis:entry colname="col7">2.46</oasis:entry>
       </oasis:row>
     </oasis:tbody>
   </oasis:tgroup></oasis:table></table-wrap>

      <p>Figure 9 displays monthly time series of statistics
from comparisons of the GNSS and NWM tropospheric horizontal gradients in
the north and east directions. Two solutions are highlighted in order to
demonstrate the impact of different parameter temporal resolutions: a 6 h
resolution is used for GO4 and a 24 h resolution is used for GO6.
Seasonal variations are mainly pronounced when observing mean standard
deviations (top plot), whereas gradual improvement is more pronounced for
mean biases (bottom plot). The reduction of the initial mean biases in
horizontal gradients, and the corresponding 1<inline-formula><mml:math id="M127" display="inline"><mml:mi mathvariant="italic">σ</mml:mi></mml:math></inline-formula> ranges over the values
from the ensemble of stations, can be attributed to the improved
availability and quality of low-elevation observation tracking. Elevation
cut-off angles for collecting GNSS observations were initially configured
station by station, ranging from 0 to 15<inline-formula><mml:math id="M128" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula>, until 2008
when the elevation cut-off angle 0<inline-formula><mml:math id="M129" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> was recommended for all the
stations.</p>
      <p>Mean standard deviations and their 1<inline-formula><mml:math id="M130" display="inline"><mml:mi mathvariant="italic">σ</mml:mi></mml:math></inline-formula> ranges over all stations
(Fig. 9, top plot) are lower by a factor of 1.3
for the solution with 24 h resolution (GO6) compared to the 6 h
resolution (GO4); the impact is also especially pronounced in the early
years of the dataset. The improvement factor ranges from 1.03 to 1.65 with
the mean value of 1.35 overall stations and it is usually higher for years
before 2001. Theoretically, with 4 times more observations in GO6, the
standard deviation was expected to be divided by a factor of 2. This
discrepancy indicates serial correlations in errors which, among others,
stem from the errors in precise products and models. Significant
improvements, however, indicate possible correlations between tropospheric
gradients and other estimated parameters, such as ambiguities, height and
zenith total delays, and suggest a careful handling, particularly when
applying a sub-daily temporal resolution.</p>
</sec>
<sec id="Ch1.S5.SS5">
  <title>Spatial and temporal ZTD analysis</title>
      <p>We performed spatial and temporal analyses of all processed variants in
order to assess the impact of different settings on tropospheric products.
Zenith tropospheric delays from all variants were compared in such a way to
enable the assessment of the impact of any single processing change: (1) GO1–GO0 for
mapping function and a more precise a priori ZHD model, (2) GO2–GO1 and GO3–GO1
for different elevation cut-off angle, (3) GO4–GO1 for non-tidal atmospheric
corrections, (4) GO5–GO4 for higher-order ionospheric corrections and (5) GO6–GO4 for temporal resolution tropospheric horizontal gradients.
Station-specific behaviour will be studied in future.</p>
      <p>Geographical maps of spatially distributed biases and standard deviations in
ZTDs from all compared variants for the whole network are shown in
Figs. 10 and 11.
Additionally, median, minimum and maximum values of station-wise total
statistics are provided in Table 5.
Figures 12,  13 and
14 illustrate ZTD statistics with respect to
the station latitude, ellipsoidal height and time, respectively.</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F10" specific-use="star"><caption><p>Geographic visualization of biases from inter-comparisons of the GOP
second reprocessing variants.</p></caption>
          <?xmltex \igopts{width=412.564961pt}?><graphic xlink:href="https://amt.copernicus.org/articles/10/3589/2017/amt-10-3589-2017-f10.png"/>

        </fig>

      <?xmltex \floatpos{t}?><fig id="Ch1.F11" specific-use="star"><caption><p>Geographic visualization of standard deviations from
inter-comparisons of the GOP second reprocessing variants.</p></caption>
          <?xmltex \igopts{width=412.564961pt}?><graphic xlink:href="https://amt.copernicus.org/articles/10/3589/2017/amt-10-3589-2017-f11.png"/>

        </fig>

      <?xmltex \floatpos{t}?><fig id="Ch1.F12" specific-use="star"><caption><p>Dependence of ZTD biases (blue) and standard deviations (red)
from inter-comparisons of the GOP second reprocessing solution variants on
station latitude. Note the different <inline-formula><mml:math id="M131" display="inline"><mml:mi>y</mml:mi></mml:math></inline-formula> range for the GO5 vs. GO4 comparison.</p></caption>
          <?xmltex \igopts{width=312.980315pt}?><graphic xlink:href="https://amt.copernicus.org/articles/10/3589/2017/amt-10-3589-2017-f12.pdf"/>

        </fig>

      <?xmltex \floatpos{t}?><fig id="Ch1.F13" specific-use="star"><caption><p>Dependence of ZTD biases (blue) and standard deviations (red)
from inter-comparisons of the GOP second reprocessing solution variants on
station ellipsoidal height. Note the different <inline-formula><mml:math id="M132" display="inline"><mml:mi>y</mml:mi></mml:math></inline-formula> range for the GO5 vs. GO4
comparison.</p></caption>
          <?xmltex \igopts{width=312.980315pt}?><graphic xlink:href="https://amt.copernicus.org/articles/10/3589/2017/amt-10-3589-2017-f13.pdf"/>

        </fig>

      <?xmltex \floatpos{t}?><fig id="Ch1.F14" specific-use="star"><caption><p>Dependence of ZTD biases (blue), mean biases (unfilled black
circles), standard deviations (red) and mean standard deviations (filled
black circles) from inter-comparisons of the GOP second reprocessing solution
variants per year. Note the different <inline-formula><mml:math id="M133" display="inline"><mml:mi>y</mml:mi></mml:math></inline-formula> range for the GO5 vs. GO4 comparison.</p></caption>
          <?xmltex \igopts{width=312.980315pt}?><graphic xlink:href="https://amt.copernicus.org/articles/10/3589/2017/amt-10-3589-2017-f14.pdf"/>

        </fig>

      <p>Using the VMF1 mapping function together with precise a priori ZHD from VMF1
instead of the GMF and GPT models, respectively (see GO1 vs. GO0), we observe
biases ranging from <inline-formula><mml:math id="M134" display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>1.52 to 0.70 mm, the median value of <inline-formula><mml:math id="M135" display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>0.36 mm,
and, according to Table 5, all biases indicated a moderate latitudinal
dependence, see Fig. 12. Standard deviations range from 0.69 to 3.82 mm in Table 5, with a
marked increase along with the latitude, Fig. 12, indicating the GPT performs
worse at higher latitudes. This is consistent with Steigenberger et
al. (2009) demonstrating a partial compensation of the atmospheric loading
effect by using the GPT model. In cases where the atmospheric loading effect
is not corrected for, the errors are mostly assimilated to the zenith total
delay parameters if station coordinates are fixed on a weekly basis.
Additionally, Fig. 14 shows that the standard deviation grows with time,
which might be explained by the increased number of low-elevation
observations with time in the EUREF Permanent Network as demonstrated for the
WTZR (Wettzell) station in Fig. 15.</p>
      <p>Biases obtained from the comparison of different elevation cut-off angles,
i.e. variants 3 to 7<inline-formula><mml:math id="M136" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> (GO2–GO1) and 3 to 10<inline-formula><mml:math id="M137" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> (GO3–GO1), range from <inline-formula><mml:math id="M138" display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>0.81 to 1.66 mm and from <inline-formula><mml:math id="M139" display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>2.22 to
2.66 mm, respectively, and standard deviations range from 0.15 to 1.29 mm  and
from 0.31 to 2.04 mm, see Table 5. Generally, the impact of the different elevation
cut-off angle does not reveal any biases with respect to the latitude
(Fig. 12) or the station height (Fig. 13). As expected, the impact is larger
for the GO3–GO1 differences and particularly affected some stations. Yearly
biases exceeding <inline-formula><mml:math id="M140" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula>2.5 mm were identified for the BELL, DENT, MLVL, MOPS,
POLV RAMO and SBG2 stations. Temporal dependencies in the GO2–GO1 and GO3–GO1
comparisons, Fig. 14, show that the scatter of station-specific biases
steadily grows in time, which is assumed to be related to the higher
availability of low-elevation observations. On the other hand, a small impact
is observed for the standard deviation compared to the other studied effects.
This indicates the elevation cut-off angle affects mainly ZTD biases, which
has been also reported by Ning and Elgered (2012).</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F15" specific-use="star"><caption><p>Availability of observations at low-elevation angles (below
5, 10, 15, 20 and
30<inline-formula><mml:math id="M141" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula>) for the WTZR station.</p></caption>
          <?xmltex \igopts{width=355.659449pt}?><graphic xlink:href="https://amt.copernicus.org/articles/10/3589/2017/amt-10-3589-2017-f15.pdf"/>

        </fig>

      <?xmltex \floatpos{t}?><fig id="Ch1.F16" specific-use="star"><caption><p>Long-term ZTD trend estimates and their formal errors (error
bars) for all processing variants.</p></caption>
          <?xmltex \igopts{width=355.659449pt}?><graphic xlink:href="https://amt.copernicus.org/articles/10/3589/2017/amt-10-3589-2017-f16.pdf"/>

        </fig>

      <p>Table 5 shows that biases due to the non-tidal atmospheric loading (GO4–GO1)
range from <inline-formula><mml:math id="M142" display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>2.29 to 5.55 mm, which is one of the largest impacts compared
to other comparison variants, and standard deviations range from 0.68 to
4.72 mm, which represents the second largest impact compared to all other
variants. A standard deviation larger than 3 mm was observed at some stations,
such as JOZE, MAD2, MADR, MDVO, MOPI, NYAL, SBG2, VENE and WETT. It should be
emphasized this comparison reflects differences due to the modelling of
atmospheric loading corrections in GO4 and a partial compensation of the
loading effect by zenith tropospheric delay estimates in the GO1 solution
variant. The differences are strongly station dependent, but they did not reveal
any dependence on latitude, see Fig. 12. This shows, however, some degradation
in standard deviation during the first years of the reprocessing, see
Fig. 14. Since a similar degradation in terms of standard deviations has not been observed for other
comparison variants, it can be related to the quality of pressure data used
to compute atmospheric loading.</p>
      <p>The impact of the higher-order ionospheric effect (GO5–GO4) is negligible at all
stations, demonstrating total statistics for all stations within <inline-formula><mml:math id="M143" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula>0.3 mm
when applying the <inline-formula><mml:math id="M144" display="inline"><mml:mi>y</mml:mi></mml:math></inline-formula> range about 10 times smaller than in other panels of
Figs. 12, 13 and 14. A strong latitudinal dependence is clearly
visible in Fig. 12 as well as a temporal variability showing peaks up to
<inline-formula><mml:math id="M145" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula>0.4 mm, Fig. 14. Both dependencies are due to the changing magnitude of
ionospheric corrections, generally increasing towards the equator along with
quasi-periodic cycles of the solar magnetic activity, reaching peaks around
years 2001 and 2014.</p>
      <p>The impact of stacking tropospheric gradients from 6 h to daily estimates
(GO6–GO4) is almost negligible in terms of biases which stay below <inline-formula><mml:math id="M146" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula>1 mm,
Table 5 and Fig. 10. However, standard deviations range from 0.76 to 2.46 mm
and grow towards the equator, Fig. 12. That can be certainly attributed to
the more difficult modelling of a local asymmetry in the troposphere, which
generally increases together with the increasing of the water vapour
content. No significant temporal variation is visible for the bias,
but a small decrease is observed for the standard deviation (Fig. 14).
This can be attributed to a
higher stability of the gradient estimates with time, see Fig. 9, when
supported with an increased number of available low-elevation observations.</p>
</sec>
</sec>
<sec id="Ch1.S6">
  <title>Impact of variants on long-term ZTD trend estimates</title>
      <p>We assessed the impact of solution variants on long-term ZTD trend estimates
by analysing 172 EUREF stations providing a time series of data longer than
10 years. For each station, the trend analysis was performed without any data
homogenization or outlier rejection as our focus was only on assessing the
impact of solution variants on the trend estimates. The ZTD trends were
estimated using the least squares regression method applied on the model
(Weatherhead et al., 1998):
          <disp-formula id="Ch1.E2" content-type="numbered"><mml:math id="M147" display="block"><mml:mrow><mml:msub><mml:mi>Y</mml:mi><mml:mi mathvariant="normal">t</mml:mi></mml:msub><mml:mo>=</mml:mo><mml:mi mathvariant="italic">μ</mml:mi><mml:mo>+</mml:mo><mml:mi mathvariant="italic">β</mml:mi><mml:msub><mml:mi>X</mml:mi><mml:mi mathvariant="normal">t</mml:mi></mml:msub><mml:mo>+</mml:mo><mml:msub><mml:mi>S</mml:mi><mml:mi mathvariant="normal">t</mml:mi></mml:msub><mml:mo>+</mml:mo><mml:msub><mml:mi mathvariant="italic">ε</mml:mi><mml:mi mathvariant="normal">t</mml:mi></mml:msub><mml:mo>,</mml:mo></mml:mrow></mml:math></disp-formula>
        <?xmltex \hack{\newpage}?>where <inline-formula><mml:math id="M148" display="inline"><mml:mi mathvariant="italic">μ</mml:mi></mml:math></inline-formula> is the constant term of the model; <inline-formula><mml:math id="M149" display="inline"><mml:mrow><mml:mi mathvariant="italic">β</mml:mi><mml:msub><mml:mi>X</mml:mi><mml:mi mathvariant="normal">t</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> is the
linear trend function, with <inline-formula><mml:math id="M150" display="inline"><mml:mi mathvariant="italic">β</mml:mi></mml:math></inline-formula> representing the trend magnitude;
<inline-formula><mml:math id="M151" display="inline"><mml:mrow><mml:msub><mml:mi>S</mml:mi><mml:mi mathvariant="normal">t</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> represents the term modelled by the sine wave function of
time <inline-formula><mml:math id="M152" display="inline"><mml:mrow><mml:msub><mml:mi>X</mml:mi><mml:mi mathvariant="normal">t</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> including annual, second harmonics and daily variations; and
finally <inline-formula><mml:math id="M153" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="italic">ε</mml:mi><mml:mi mathvariant="normal">t</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> is the noise in the data.</p>
      <p>Site-by-site-estimated ZTD trends from all the variants are provided in the
Supplement completed by time span information, number of records
and estimated mean formal errors calculated over all variants. In total,
trends range from <inline-formula><mml:math id="M154" display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>0.99 to 0.96 mm year<inline-formula><mml:math id="M155" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula>. Although the individual
station trend provided in the Supplement could be compared to other studies
– e.g. Baldysz et al. (2016), Klos et al. (2016), or Nilsson and
Elgered (2008) –
it should be strongly emphasized here that our trends are estimated
without any preceding time-series homogenization and the formal errors of the
trend estimates are underestimated by a factor 2–4 (Nilsson and Elgered,
2008).</p>

<?xmltex \floatpos{t}?><table-wrap id="Ch1.T6" specific-use="star"><caption><p>Mean statistics of ZTD trend differences estimated between
variants for 172 stations. Units are mm year<inline-formula><mml:math id="M156" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula>.</p></caption><oasis:table frame="topbot"><oasis:tgroup cols="7">
     <oasis:colspec colnum="1" colname="col1" align="left"/>
     <oasis:colspec colnum="2" colname="col2" align="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:thead>
       <oasis:row rowsep="1">  
         <oasis:entry colname="col1">Statistics</oasis:entry>  
         <oasis:entry colname="col2">GO1–GO0</oasis:entry>  
         <oasis:entry colname="col3">GO2–GO1</oasis:entry>  
         <oasis:entry colname="col4">GO3–GO1</oasis:entry>  
         <oasis:entry colname="col5">GO4–GO1</oasis:entry>  
         <oasis:entry colname="col6">GO5–GO4</oasis:entry>  
         <oasis:entry colname="col7">GO6–GO4</oasis:entry>
       </oasis:row>
     </oasis:thead>
     <oasis:tbody>
       <oasis:row>  
         <oasis:entry colname="col1">Min</oasis:entry>  
         <oasis:entry colname="col2"><inline-formula><mml:math id="M157" display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>0.118</oasis:entry>  
         <oasis:entry colname="col3"><inline-formula><mml:math id="M158" display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>0.141</oasis:entry>  
         <oasis:entry colname="col4"><inline-formula><mml:math id="M159" display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>0.308</oasis:entry>  
         <oasis:entry colname="col5"><inline-formula><mml:math id="M160" display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>0.547</oasis:entry>  
         <oasis:entry colname="col6"><inline-formula><mml:math id="M161" display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>0.017</oasis:entry>  
         <oasis:entry colname="col7"><inline-formula><mml:math id="M162" display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>0.038</oasis:entry>
       </oasis:row>
       <oasis:row>  
         <oasis:entry colname="col1">Max</oasis:entry>  
         <oasis:entry colname="col2">0.045</oasis:entry>  
         <oasis:entry colname="col3">0.179</oasis:entry>  
         <oasis:entry colname="col4">0.331</oasis:entry>  
         <oasis:entry colname="col5">0.452</oasis:entry>  
         <oasis:entry colname="col6">0.031</oasis:entry>  
         <oasis:entry colname="col7">0.036</oasis:entry>
       </oasis:row>
       <oasis:row>  
         <oasis:entry colname="col1">Mean</oasis:entry>  
         <oasis:entry colname="col2">0.036</oasis:entry>  
         <oasis:entry colname="col3">0.018</oasis:entry>  
         <oasis:entry colname="col4">0.012</oasis:entry>  
         <oasis:entry colname="col5"><inline-formula><mml:math id="M163" display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>0.048</oasis:entry>  
         <oasis:entry colname="col6">0.007</oasis:entry>  
         <oasis:entry colname="col7">0.001</oasis:entry>
       </oasis:row>
       <oasis:row>  
         <oasis:entry colname="col1">SD</oasis:entry>  
         <oasis:entry colname="col2">0.081</oasis:entry>  
         <oasis:entry colname="col3">0.160</oasis:entry>  
         <oasis:entry colname="col4">0.319</oasis:entry>  
         <oasis:entry colname="col5">0.499</oasis:entry>  
         <oasis:entry colname="col6">0.024</oasis:entry>  
         <oasis:entry colname="col7">0.037</oasis:entry>
       </oasis:row>
     </oasis:tbody>
   </oasis:tgroup></oasis:table></table-wrap>

      <p>Table 6 summarizes the statistics of estimated trend differences at all
172 stations, always between particular variants as defined in Sect. 5.5.
Interestingly, the most significant impact is observed due to the non-tidal
atmospheric loading effects reaching differences below
<inline-formula><mml:math id="M164" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula>0.55 mm year<inline-formula><mml:math id="M165" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula> in ZTD trends for some extreme cases from the
ensemble of 172 stations and an overall 1<inline-formula><mml:math id="M166" display="inline"><mml:mi mathvariant="italic">σ</mml:mi></mml:math></inline-formula> scatter of
0.50 mm year<inline-formula><mml:math id="M167" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula> from the ensemble of stations. Changes in elevation
cut-off angle, particularly from 3 to 10<inline-formula><mml:math id="M168" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula>, also reveal a significant
impact characterized by differences below <inline-formula><mml:math id="M169" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula>0.34 mm year<inline-formula><mml:math id="M170" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula> and the
scatter of 0.32 mm year<inline-formula><mml:math id="M171" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula>. The impact of mapping function on trend
estimates remains small, with a maximum difference of 0.12 mm year<inline-formula><mml:math id="M172" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula>
and the 1<inline-formula><mml:math id="M173" display="inline"><mml:mi mathvariant="italic">σ</mml:mi></mml:math></inline-formula> scatter below 0.08 mm year<inline-formula><mml:math id="M174" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula>, while other strategy
changes, due to time resolution of tropospheric gradients and higher-order
ionospheric effects, remain negligible, always below
<inline-formula><mml:math id="M175" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula>0.04 mm year<inline-formula><mml:math id="M176" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula> for all 172 stations, with the scatter of the same
magnitude. All mean biases over differences also stay below
0.05 mm year<inline-formula><mml:math id="M177" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula>. These results are consistent with a study performed by
Ning and Elgered (2012) spanning a broader span of cut-off angles. They
demonstrated a significant impact of this parameter on integrated water vapour
trend estimates.</p>
      <p>Finally, we selected 12 stations available over the entire second reprocessing
period. All estimated trends are displayed in Fig. 16, ranging from <inline-formula><mml:math id="M178" display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>0.05
to 0.38 mm year<inline-formula><mml:math id="M179" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula>. Consistent with the overall results reported in
Table 5, the most significant impact for the selected 12 stations is observed
in the change of elevation cut-off angle (GO2 and GO3 vs. GO1) and atmospheric
loading (GO4 vs. GO1) when reaching differences up to 0.1 mm year<inline-formula><mml:math id="M180" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula> in
estimated ZTD trends. Impacts of other strategies are generally below
0.05 mm year<inline-formula><mml:math id="M181" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula> – variants GO4, GO5 and GO6 are very similar, but not
consistent again with GO1, meaning the non-tidal atmospheric loading has a
significant impact on trend estimates for selected stations with the longest
data time series.</p>
</sec>
<sec id="Ch1.S7" sec-type="conclusions">
  <title>Conclusions</title>
      <p>In this paper, we present results of the new GOP reanalysis of all stations
within the EUREF Permanent Network during the period of 1996–2014. This
reanalysis was completed during the second EUREF reprocessing to support the
realization of a new European Terrestrial Reference System. In the second
reprocessing, we focused on analysing a new product – the GNSS tropospheric
parameter time series for applications to climate research. To achieve this
goal, we improved our strategy for combining tropospheric parameters during midnights and week breaks.
We also performed seven solution
variants to study optimal troposphere modelling; we assessed each of these
variants in terms of their coordinate repeatability by using internal
evaluations of the applied models and strategies. We also compared
tropospheric ZTD and tropospheric horizontal gradients with independent
evaluations obtained by numerical weather reanalysis via the ERA-Interim.</p>
      <p>Results of the GOP Repro2 yielded improvements of approximately 50 and 25 %
for their horizontal and vertical component repeatability, respectively, when
compared to those of the GOP Repro1 solution. Vertical repeatability was
reduced from 4.14 to 3.73 mm when using the VMF1 mapping function, a priori
ZHD, and non-tidal atmospheric loading corrections from actual weather data.
Increasing the elevation cut-off angle from 3 to 7<inline-formula><mml:math id="M182" display="inline"><mml:mrow><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup><mml:mo>/</mml:mo><mml:msup><mml:mn mathvariant="normal">10</mml:mn><mml:mo>∘</mml:mo></mml:msup></mml:mrow></mml:math></inline-formula>
increased RMS errors of residuals from these coordinates' repeatability. All
of these factors were also confirmed by the independent assessment of
tropospheric parameters using NWM reanalysis data.</p>
      <p>We particularly recommend using low-elevation observations along with the
VMF1 mapping function as well as using precise a priori ZHD values together
with the consistent model of non-tidal atmospheric loading. While estimating
tropospheric horizontal linear gradients improves coordinates' repeatability,
6 h sampling without any absolute or relative constraints revealed a loss of
stability due to their correlations with other parameters. On the other hand,
24 h piecewise linear gradients did not indicate a worse repeatability of
coordinates estimates. For saving the time needed for the processing of
4 times fewer gradient parameters, we could recommend
using the unconstrained 24 h piecewise model for the modelling of the
first-order tropospheric asymmetry.</p>
      <p>The impact of processing variants on long-term ZTD trend estimates was
assessed at 172 EUREF stations with time series longer than 10 years. The
most significant impact was observed due to the non-tidal atmospheric loading
effect reaching differences below <inline-formula><mml:math id="M183" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula>0.55 mm year<inline-formula><mml:math id="M184" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula> in ZTD trends
for some extreme cases from the ensemble of 172 stations. Changes in
elevation cut-off angle, particularly from 3 to 10<inline-formula><mml:math id="M185" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula>, also revealed a
significant impact reaching differences below <inline-formula><mml:math id="M186" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula>0.35 mm year<inline-formula><mml:math id="M187" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula>.
The change of mapping function was observed to be rather small, with a maximum
difference of 0.12 mm year<inline-formula><mml:math id="M188" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula>, while other strategy changes, due to
time resolution of tropospheric gradients and higher-order ionospheric
effects, remained negligible, always below <inline-formula><mml:math id="M189" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula>0.04 mm year<inline-formula><mml:math id="M190" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula> for
all 172 stations.</p>
      <p>Assessing the tropospheric horizontal gradients with respect to the
ERA-Interim reanalysis data revealed some long-term systematic behaviour
linked to degradation in antenna tracking quality. We presented an extreme
case at the Mallorca station, in which gradients systematically
increased up to 5 mm from 2003 to 2008 while pointing in the direction of
prevailing observations at low-elevation angles. However, these biases
disappeared when the malfunctioning antenna was replaced. More cases similar
to this, although less extreme, have indicated that estimated tropospheric
gradients are extremely sensitive to the quality of GNSS antenna tracking,
thus suggesting that these gradients can be used to identify problems with
GNSS data tracking in historical archives.</p>
      <p>One of the main difficulties faced during the second reprocessing was that of
the quality of the historical data, which contains a large variety of
problems. We removed data that caused significant problems in network
processing when these could not be pre-eliminated from normal equations
during the combination process without still affecting daily solutions. To
provide high-accuracy, high-resolution GNSS tropospheric products, the
elimination of such problematic data or stations is even more critical
considering the targeting static coordinates on a daily or weekly basis for
the maintenance of the reference frame or the derivation of a velocity field.
Before undertaking the third EUREF reprocessing, which is expected to begin
after significant improvements have been made to state-of-the-art models,
products and software, we need to improve data quality control and clean the
EUREF historical archive in order to optimize any future reprocessing efforts
and to increase the quality of tropospheric products. These efforts should
also include the collection and documentation of all available information
from each step of the second EUREF reprocessing, including individual
contributions, EUREF combinations, time-series analyses and coordinates, and
independent evaluations of tropospheric parameters.</p>
</sec>

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

      <p>All processed reprocessed GNSS data are available at
<uri>ftp://epncb.oma.be/pub/obs/</uri>, where they are maintained by the historical EPN
archive of the Royal Observatory of Belgium. The official second GOP EUREF
reprocessing solution (GO4) in SINEX and SINEX_TRO formats are publicly
available at <uri>ftp://igs.bkg.bund.de/EPNrepro2/products/</uri>. Additionally,
the tropospheric parameters for all EPN stations are available via the
GOP-TropDB download service at
<uri>http://www.pecny.cz/GOP-TropDB/data-download</uri>.</p>
  </notes><app-group>
        <supplementary-material position="anchor"><p><bold>The Supplement related to this article is available online at <inline-supplementary-material xlink:href="https://doi.org/10.5194/amt-10-3589-2017-supplement" xlink:title="pdf">https://doi.org/10.5194/amt-10-3589-2017-supplement</inline-supplementary-material>.</bold></p></supplementary-material>
        </app-group><notes notes-type="authorcontribution">

      <p>JD and PV performed the second
GOP European GNSS reprocessing. ME performed a long-term trend analysis for
all the variants of the reprocessing. JD prepared the manuscript with the support
of PV and ME, who particularly contributed to Sect. 6. All authors approved
the final manuscript before its submission.</p>
  </notes><notes notes-type="competinginterests">

      <p>The authors declare that they have no conflict of
interest.</p>
  </notes><notes notes-type="sistatement">

      <p>This article is part of the special issue “Advanced Global Navigation Satellite Systems tropospheric products for monitoring severe weather events and climate (GNSS4SWEC) (AMT/ACP/ANGEO inter-journal SI)”.
It is not associated with a conference.</p>
  </notes><ack><title>Acknowledgements</title><p>The reprocessing effort and its evaluations were supported by the Ministry of
Education, Youth and Science, the Czech Republic (projects LD14102 and
LO1506). We thank two anonymous reviewers and Olivier Bock for their comments and
suggestions which helped us to improve the
manuscript.<?xmltex \hack{\newline}?><?xmltex \hack{\newline}?>Edited by: Olivier Bock
<?xmltex \hack{\newline}?> Reviewed by: two anonymous referees</p></ack><ref-list>
    <title>References</title>

      <ref id="bib1.bib1"><label>1</label><mixed-citation>
Altamimi, Z., Angermann, D., Argus, D., Blewitt, G., Boucher, C., Chao, B., Drewes, H.,
Eanes, R., Feissel, M., Ferland, R.,  Herring, T., Holt, M., Johannson, J., Larson, K., Ma, C.,
Manning, J., Meertens, C.,  Nothnagel, A., Pavlis, E., Petit, G., Ray, J., Ries, J., Scherneck, H.-G., Sillard, P., and Watkins, M.: The terrestrial reference frame and the dynamic Earth, EOS,
Transacttions, American Geophysical Union, 82, 273–279, 2001.</mixed-citation></ref>
      <ref id="bib1.bib2"><label>2</label><mixed-citation>Baldysz, Z., Nykiel, G., Araszkiewicz, A., Figurski, M., and Szafranek, K.:
Comparison of GPS tropospheric delays derived from two consecutive EPN
reprocessing campaigns from the point of view of climate monitoring, Atmos.
Meas. Tech., 9, 4861–4877, <ext-link xlink:href="https://doi.org/10.5194/amt-9-4861-2016" ext-link-type="DOI">10.5194/amt-9-4861-2016</ext-link>, 2016.</mixed-citation></ref>
      <ref id="bib1.bib3"><label>3</label><mixed-citation>Bevis, M., Businger, S., Chiswell, S., Herring, T. A., Anthes, R. A.,
Rocken,
C., and Ware R. H.: GPS Meteorology: Mapping Zenith Wet Delays onto
Precipitable Water, J. Appl. Meteorol., 33, 379–386, <ext-link xlink:href="https://doi.org/10.1175/1520-0450" ext-link-type="DOI">10.1175/1520-0450</ext-link>, 1994.</mixed-citation></ref>
      <ref id="bib1.bib4"><label>4</label><mixed-citation>Bock, O. and Nuret, M.: Verification of NWP model analyses and radiosonde
humidity data with GPS precipitable water vapor estimates during AMMA,
Weather Forecast., 24, 1085–1101,  <ext-link xlink:href="https://doi.org/10.1175/2009WAF2222239.1" ext-link-type="DOI">10.1175/2009WAF2222239.1</ext-link>,  2009.</mixed-citation></ref>
      <ref id="bib1.bib5"><label>5</label><mixed-citation>Bock, O., Willis, P., Wang, J., and Mears, C.: A high-quality, homogenized,
global, long-term (1993–2008) DORIS precipitable water data set for climate
monitoring and model verification, J. Geophys. Res.-Atmos., 119, 7209–7230,
<ext-link xlink:href="https://doi.org/10.1002/2013JD021124" ext-link-type="DOI">10.1002/2013JD021124</ext-link>,
2014.</mixed-citation></ref>
      <ref id="bib1.bib6"><label>6</label><mixed-citation>Bock, O., Bosser, P., Pacione, R., Nuret, M., Fourrié, N., and Parracho,
A.: A high-quality reprocessed ground-based GPS dataset for atmospheric
process studies, radiosonde and model evaluation, and reanalysis of HyMeX
Special Observing Period, Q. J. Roy. Meteor. Soc., 142, 56–71,  <ext-link xlink:href="https://doi.org/10.1002/qj.2701" ext-link-type="DOI">10.1002/qj.2701</ext-link>,  2016.</mixed-citation></ref>
      <ref id="bib1.bib7"><label>7</label><mixed-citation>Böhm, J., Niell, A. E., Tregoning, P., and Schuh, H.: 2006, Global
Mapping Functions (GMF): A new empirical mapping function based on numerical
weather model data, Geophys. Res. Lett., 33, L07304,  <ext-link xlink:href="https://doi.org/10.1029/2005GL025546" ext-link-type="DOI">10.1029/2005GL025546</ext-link>, 2006a.</mixed-citation></ref>
      <ref id="bib1.bib8"><label>8</label><mixed-citation>Böhm, J., Werl, B., and Schuh, H.: Troposphere mapping functions for GPS
and very long baseline interferometry from European Centre for Medium-Range
Weather Forecasts operational analysis data. J. Geophys. Res., 111, B02406,
<ext-link xlink:href="https://doi.org/10.1029/2005JB003629" ext-link-type="DOI">10.1029/2005JB003629</ext-link>,
2006b.</mixed-citation></ref>
      <ref id="bib1.bib9"><label>9</label><mixed-citation>Bruyninx, C., Habrich, H., Söhne, W., Kenyeres, A.,
Stangl, G., and Völksen, C.: Enhancement of the EUREF Permanent Network
Services and Products, Geodesy for Planet Earth, IAG Symposia Series, 136,
27–35,  <ext-link xlink:href="https://doi.org/10.1007/978-3-642-20338-1_4" ext-link-type="DOI">10.1007/978-3-642-20338-1_4</ext-link>, 2012.</mixed-citation></ref>
      <ref id="bib1.bib10"><label>10</label><mixed-citation>Dach, R., Böhm, J., Lutz, S., Steigenberger, P., and Beutler, G.:
Evaluation of the impact of atmospheric pressure loading modeling on GNSS
data analysis, J. Geodynam., 85, 75–91, <ext-link xlink:href="https://doi.org/10.1007/s00190-010-0417-z" ext-link-type="DOI">10.1007/s00190-010-0417-z</ext-link>, 2011.</mixed-citation></ref>
      <ref id="bib1.bib11"><label>11</label><mixed-citation>Dach, R., Schaer, S., Lutz, S., Baumann, C., Bock, H., Orliac, E., Prange,
L., Thaller, D., Mervart, L., Jäggi, A., Beutler, G., Brockmann, E.,
Ineichen, D., Wiget, A., Weber, G., Habrich, H., Söhne, W., Ihde, J.,
Steigenberger, P., and Hugentobler, U.: CODE IGS Analysis Center Technical
Report 2013, edited by: Dach, R. and Jean, Y., IGS 2013 Tech. Rep., 21–34,
2014.</mixed-citation></ref>
      <ref id="bib1.bib12"><label>12</label><mixed-citation>Dach, R., Lutz, S., Walser, P., and Fridez, P. (Eds.): Bernese GNSS Software
Version 5.2. User manual, Astronomical Institute, University of Bern, Bern
Open Publishing, 2015.</mixed-citation></ref>
      <ref id="bib1.bib13"><label>13</label><mixed-citation>Dee, D. P., Uppala, S. M., Simmons, A. J., Berrisford, P., Poli, P.,
Kobayashi, S., Andrae, U., Balmaseda, M. A., Balsamo, G., Bauer, P.,
Bechtold, P., Beljaars, A. C. M., van de Berg, L., Bidlot, J., Bormann, N.,
Delsol, C., Dragani, R., Fuentes, M., Geer, A. J., Haimberger, L., Healy, S.
B., Hersbach, H., Hólm, E. V., Isaksen, L., Kållberg, P., Köhler, M.,
Matricardi, M., McNally, A. P., Monge-Sanz, B. M., Morcrette, J.-J., Park,
B.-K., Peubey, C., de Rosnay, P., Tavolato, C., Thépaut, J.-N., and Vitart,
F.: The ERA-Interim reanalysis: Configuration and performance of the data
assimilation system, Q. J. Roy. Meteorol. Soc., 137, 553–597,
<ext-link xlink:href="https://doi.org/10.1002/qj.828" ext-link-type="DOI">10.1002/qj.828</ext-link>, 2011.</mixed-citation></ref>
      <ref id="bib1.bib14"><label>14</label><mixed-citation>Douša, J.  and Václavovic, P.: Results of GPS Reprocessing campaign
(1996–2011) provided by Geodetic observatory Pecný, Geoinformatics, FCE
CTU, 9, 77–89, <ext-link xlink:href="https://doi.org/10.14311/gi.9.7" ext-link-type="DOI">10.14311/gi.9.7</ext-link>,  2012.</mixed-citation></ref>
      <ref id="bib1.bib15"><label>15</label><mixed-citation>Douša, J., Dick, G., Kacmarík, M., Brožková, R., Zus, F., Brenot,
H., Stoycheva, A., Möller, G., and Kaplon, J.: Benchmark campaign and case
study episode in central Europe for development and assessment of advanced
GNSS tropospheric models and products, Atmos. Meas. Tech., 9, 2989–3008,
<ext-link xlink:href="https://doi.org/10.5194/amt-9-2989-2016" ext-link-type="DOI">10.5194/amt-9-2989-2016</ext-link>, 2016.</mixed-citation></ref>
      <ref id="bib1.bib16"><label>16</label><mixed-citation>Douša, J., Böhm, O., Byram, S., Hackman, C., Deng Z., Zus, F., Dach,
R., and Steigenberger, P.: Evaluation of GNSS reprocessing tropospheric
products using GOP-TropDB, IGS Workshop 2016, Sydney, 8–12 February 2017,
available at: <uri>http://www.igs.org/assets/pdf/W2016 - PS0303 - Dousa.pdf</uri>,
last access: September 2017 2017.</mixed-citation></ref>
      <ref id="bib1.bib17"><label>17</label><mixed-citation>Dow, J. M., Neilan, R. E., and Rizos, C.: The International GNSS Service in a changing landscape of Global Navigation Satellite Systems, J.  Geod., 83, 191–198,
<ext-link xlink:href="https://doi.org/10.1007/s00190-008-0300-3" ext-link-type="DOI">10.1007/s00190-008-0300-3</ext-link>, 2009.</mixed-citation></ref>
      <ref id="bib1.bib18"><label>18</label><mixed-citation>Fritsche, M., Dietrich, R., Knofel, C., Rlke, A., Vey, S., Rothacher, M.,
and Steigenberger, P.: Impact of higher-order ionospheric terms on GPS
estimates. Geophys. Res. Lett., 32, L23311,  <ext-link xlink:href="https://doi.org/10.1029/2005GL024342" ext-link-type="DOI">10.1029/2005GL024342</ext-link>, 2005.</mixed-citation></ref>
      <ref id="bib1.bib19"><label>19</label><mixed-citation>Guerova, G., Jones, J., Douša, J., Dick, G., de Haan, S., Pottiaux, E.,
Bock, O., Pacione, R., Elgered, G., Vedel, H.,
and Bender, M.: Review of the state of the art and future prospects of the ground-based GNSS meteorology in Europe, Atmos. Meas. Tech., 9, 5385–5406,  <ext-link xlink:href="https://doi.org/10.5194/amt-9-5385-2016" ext-link-type="DOI">10.5194/amt-9-5385-2016</ext-link>, 2016.</mixed-citation></ref>
      <ref id="bib1.bib20"><label>20</label><mixed-citation>Győri, G.  and Douša, J.: GOP-TropDB developments for tropospheric
product evaluation and monitoring – design, functionality and initial
results, IAG Symposia Series, Springer, 143, 595–602, 2016.</mixed-citation></ref>
      <ref id="bib1.bib21"><label>21</label><mixed-citation>IERS Conventions: Gérard, P., and Luzum, B. (Eds.): IERS Technical Note
No. 36, Frankfurt am Main, Verlag des Bundesamts für Kartographie und
Geodäsie, 179 pp., 2010.</mixed-citation></ref>
      <ref id="bib1.bib22"><label>22</label><mixed-citation>Ihde, J., Habrich, H., Sacher, M., Sohne, W., Altamimi, Z., Brockmann, E.,
Bruyninx, C., Caporali, A., Dousa, J., Fernandes, R., Hornik, H., Kenyeres,
A., Lidberg, M., Makinen, J., Poutanen, M., Stangl, G., Torres, J. A., and
Volksen, C.: EUREF's Contribution to National, European and Global Geodetic
Infrastructures, in: Earth on the Edge: Science for a Sustainable Planet,
edited by: Rizos, C. and Willis, P., IAG Symposia Series, Springer, 139,
189–196, <ext-link xlink:href="https://doi.org/10.1007/978-3-642-37222-3_24" ext-link-type="DOI">10.1007/978-3-642-37222-3_24</ext-link>, 2014.</mixed-citation></ref>
      <ref id="bib1.bib23"><label>23</label><mixed-citation>Kacmarík, M., Douša, J., Dick, G., Zus, F., Brenot, H., Möller, G.,
Pottiaux, E., Kaplon, J., Hordyniec, P., Václavovic, P., and Morel, L.:
Inter-technique validation of tropospheric slant total delays, Atmos. Meas.
Tech., 10, 2183–2208, <ext-link xlink:href="https://doi.org/10.5194/amt-10-2183-2017" ext-link-type="DOI">10.5194/amt-10-2183-2017</ext-link>, 2017.</mixed-citation></ref>
      <ref id="bib1.bib24"><label>24</label><mixed-citation>Klos, A., Hunegnaw, A., Teferle, F. N., Abraha, K. E., Ahmed, F., and Bogusz,
J.: Noise characteristics in Zenith Total Delay from homogeneously
reprocessed GPS time series, Atmos. Meas. Tech. Discuss.,
<ext-link xlink:href="https://doi.org/10.5194/amt-2016-385" ext-link-type="DOI">10.5194/amt-2016-385</ext-link>, 2016.</mixed-citation></ref>
      <ref id="bib1.bib25"><label>25</label><mixed-citation>Li, X., Zus, F., Lu, C., Ning, T., Dick, G., Ge, M., Wickert, J., and Schuh,
H.: Retrieving high-resolution tropospheric gradients from multiconstellation
GNSS observations, Geophys. Res. Lett., 42, 4173–4181,  <ext-link xlink:href="https://doi.org/10.1002/2015GL063856" ext-link-type="DOI">10.1002/2015GL063856</ext-link>, 2015.</mixed-citation></ref>
      <ref id="bib1.bib26"><label>26</label><mixed-citation>MacMillan, D. S.: Atmospheric gradients from very long baseline
interferometry observations, Geophys. Res. Lett., 22, 1041–1044, <ext-link xlink:href="https://doi.org/10.1029/95GL00887" ext-link-type="DOI">10.1029/95GL00887</ext-link>, 1995.</mixed-citation></ref>
      <ref id="bib1.bib27"><label>27</label><mixed-citation>Meindl, M., Schaer, S., Hugentobler, U., and Beutler, G.: Tropospheric
Gradient Estimation at CODE: Results from Global Solutions, J. Meteorol. Soc.
Jpn., 82, 331–338, 2004.</mixed-citation></ref>
      <ref id="bib1.bib28"><label>28</label><mixed-citation>Morel, L., Pottiaux, E., Durand, F., Fund, F., Follin, J. M., Durand, S.,
Bonifac, K., Oliveira, P. S., van Baelen, J., Montibert, C., Cavallo, T.,
Escaffit, R., and Fragnol, L.: Global validity and behaviour of tropospheric
gradients estimated by GPS, presentation at the 2nd GNSS4SWEC Workshop held
in Thessaloniki, Greece, 11–14 May 2015.</mixed-citation></ref>
      <ref id="bib1.bib29"><label>29</label><mixed-citation>Nilsson, T. and Elgered, G., Long-term trends in the atmospheric water
vapor content estimated from ground-based GPS data, J. Geophys. Res., 113,
D19101, <ext-link xlink:href="https://doi.org/10.1029/2008JD010110" ext-link-type="DOI">10.1029/2008JD010110</ext-link>,  2008.</mixed-citation></ref>
      <ref id="bib1.bib30"><label>30</label><mixed-citation>Ning, T.: GPS Meteorology: With Focus on Climate Applications, PhD Thesis,
Dept. Earth and Space Sciences, Chalmers University of Technology, 2012.</mixed-citation></ref>
      <ref id="bib1.bib31"><label>31</label><mixed-citation>Ning, T. and Elgered, E.: Trends in the atmospheric water vapor content
from ground-based GPS: The impact of the elevation cutoff angle, IEEE J. Sel.
Top. Appl., 5, 744–751,  <ext-link xlink:href="https://doi.org/10.1109/JSTARS.2012.2191392" ext-link-type="DOI">10.1109/JSTARS.2012.2191392</ext-link>, 2012.
</mixed-citation></ref><?xmltex \hack{\newpage}?>
      <ref id="bib1.bib32"><label>32</label><mixed-citation>Pacione, R., Araszkiewicz, A., Brockmann, E., and Dousa, J.: EPN-Repro2: A
reference GNSS tropospheric data set over Europe, Atmos. Meas. Tech., 10,
1689–1705, <ext-link xlink:href="https://doi.org/10.5194/amt-10-1689-2017" ext-link-type="DOI">10.5194/amt-10-1689-2017</ext-link>, 2017.</mixed-citation></ref>
      <ref id="bib1.bib33"><label>33</label><mixed-citation>Steigenberger, P., Böhm, J., and Tesmer, V.: Comparison of GMF/GPT with
VMF1/ECMWF and implications for atmospheric loading, J. Geodynam., 83, 943,
<ext-link xlink:href="https://doi.org/10.1007/s00190-009-0311-8" ext-link-type="DOI">10.1007/s00190-009-0311-8</ext-link>,
2009.</mixed-citation></ref>
      <ref id="bib1.bib34"><label>34</label><mixed-citation>Václavovic, P.  and Douša, J.: G-Nut/Anubis – open-source tool for
multi-GNSS data monitoring, in: IAG 150 Years, edited by: Rizos, Ch. and
Willis, P., IAG Symposia Series, Springer, 143, 775–782,  <ext-link xlink:href="https://doi.org/10.1007/1345_2015_97" ext-link-type="DOI">10.1007/1345_2015_97</ext-link>, 2016.</mixed-citation></ref>
      <ref id="bib1.bib35"><label>35</label><mixed-citation>Völksen, C.: An update on the EPN Reprocessing Project: Current
Achievements and Status, Presented at the EUREF 2011 Symposium, Chisinau,
Republic of Moldova, 25–28 May, available at: <uri>http://www.epncb.oma.be/_
documentation/papers/eurefsymposium2011/an_update_on_epn_
reprocessing_project_current_achievement_and_status</uri> (last access: September 2017),
2011.</mixed-citation></ref>
      <ref id="bib1.bib36"><label>36</label><mixed-citation>Weatherhead, E. C., Reinsel, G. C., Tiao, G. C., Meng, X.-L., Choi, D.,
Cheang, W.-K., Keller, T., DeLuisi, J., Wuebbles, D. J., Kerr, J. B., Miller,
A. J., Oltmans, S. J., and Frederick J. E.: Factors affecting the detection
of trends: Statistical considerations and applications to environmental data,
J. Geophys. Res., 103, 17149–17161, <ext-link xlink:href="https://doi.org/10.1029/98JD00995" ext-link-type="DOI">10.1029/98JD00995</ext-link>, 1998.</mixed-citation></ref>
      <ref id="bib1.bib37"><label>37</label><mixed-citation>Yuan, L. L., Anthes, R. A., Ware, R. H., Rocken, C., Bonner, W. D., Bevis, M. G.,
and Businger, S.: Sensing Climate Change Using the Global Positioning System,
J. Geophys. Res., 98, 14925–14937, 1993.</mixed-citation></ref>
      <ref id="bib1.bib38"><label>38</label><mixed-citation>Zus, F., Dick, G., Heise, S., Dousa, J., and Wickert, J.: The rapid and
precise computation of GPS slant total delays and mapping factors utilizing a
numerical weather model, Radio Sci., 49, 207–216,  <ext-link xlink:href="https://doi.org/10.1002/2013RS005280" ext-link-type="DOI">10.1002/2013RS005280</ext-link>, 2014.</mixed-citation></ref>
      <ref id="bib1.bib39"><label>39</label><mixed-citation>Zus, F., Dick, G., Dousa, J., and Wickert, J.: Systematic errors of mapping
functions which are based on the VMF1 concept, GPS Solut., 19, 277–286,
<ext-link xlink:href="https://doi.org/10.1007/s10291-014-0386-4" ext-link-type="DOI">10.1007/s10291-014-0386-4</ext-link>,
2015.</mixed-citation></ref>

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

    </app></app-group></back>
    <!--<article-title-html>Tropospheric products of the second GOP European GNSS reprocessing (1996–2014)</article-title-html>
<abstract-html><p class="p">In this paper, we present results of the second reprocessing of all data from
1996 to 2014 from all stations in International Association of Geodesy (IAG)
Reference Frame Sub-Commission for Europe (EUREF) Permanent Network
(EPN) as performed at the Geodetic Observatory Pecný (GOP). While the original
goal of this research was to ultimately contribute to the realization of a
new European Terrestrial Reference System (ETRS), we also aim to provide a
new set of GNSS (Global Navigation Satellite System) tropospheric parameter
time series with possible applications to climate research. To achieve these
goals, we improved a strategy to guarantee the continuity of these
tropospheric parameters and we prepared several variants of troposphere
modelling. We then assessed all solutions in terms of the repeatability of
coordinates as an internal evaluation of applied models and strategies and in
terms of zenith tropospheric delays (ZTDs) and horizontal gradients with
those of the ERA-Interim numerical weather model (NWM) reanalysis. When
compared to the GOP Repro1 (first EUREF reprocessing) solution, the results
of the GOP Repro2 (second EUREF reprocessing) yielded improvements of
approximately 50 and 25 % in the repeatability of the horizontal and
vertical components, respectively, and of approximately 9 % in tropospheric
parameters. Vertical repeatability was reduced from 4.14 to 3.73 mm when
using the VMF1 mapping function, a priori ZHD (zenith hydrostatic delay), and
non-tidal atmospheric loading corrections from actual weather data. Raising
the elevation cut-off angle from 3 to 7° and then to 10°
increased RMS from coordinates' repeatability, which was then confirmed by
independently comparing GNSS tropospheric parameters with the NWM reanalysis.
The assessment of tropospheric horizontal gradients with respect to the
ERA-Interim revealed a strong sensitivity of estimated gradients to the
quality of GNSS antenna tracking performance. This impact was demonstrated at
the Mallorca station, where gradients systematically grew up to 5 mm during
the period between 2003 and 2008, before this behaviour disappeared when the
antenna at the station was changed. The impact of processing variants on
long-term ZTD trend estimates was assessed at 172 EUREF stations with time
series longer than 10 years. The most significant site-specific impact was
due to the non-tidal atmospheric loading followed by the impact of changing
the elevation cut-off angle from 3 to 10°. The other processing
strategy had a very small or negligible impact on estimated trends.</p></abstract-html>
<ref-html id="bib1.bib1"><label>1</label><mixed-citation>
Altamimi, Z., Angermann, D., Argus, D., Blewitt, G., Boucher, C., Chao, B., Drewes, H.,
Eanes, R., Feissel, M., Ferland, R.,  Herring, T., Holt, M., Johannson, J., Larson, K., Ma, C.,
Manning, J., Meertens, C.,  Nothnagel, A., Pavlis, E., Petit, G., Ray, J., Ries, J., Scherneck, H.-G., Sillard, P., and Watkins, M.: The terrestrial reference frame and the dynamic Earth, EOS,
Transacttions, American Geophysical Union, 82, 273–279, 2001.
</mixed-citation></ref-html>
<ref-html id="bib1.bib2"><label>2</label><mixed-citation>
Baldysz, Z., Nykiel, G., Araszkiewicz, A., Figurski, M., and Szafranek, K.:
Comparison of GPS tropospheric delays derived from two consecutive EPN
reprocessing campaigns from the point of view of climate monitoring, Atmos.
Meas. Tech., 9, 4861–4877, <a href="https://doi.org/10.5194/amt-9-4861-2016" target="_blank">https://doi.org/10.5194/amt-9-4861-2016</a>, 2016.
</mixed-citation></ref-html>
<ref-html id="bib1.bib3"><label>3</label><mixed-citation>Bevis, M., Businger, S., Chiswell, S., Herring, T. A., Anthes, R. A.,
Rocken,
C., and Ware R. H.: GPS Meteorology: Mapping Zenith Wet Delays onto
Precipitable Water, J. Appl. Meteorol., 33, 379–386, <a href="https://doi.org/10.1175/1520-0450" target="_blank">https://doi.org/10.1175/1520-0450</a>, 1994.
</mixed-citation></ref-html>
<ref-html id="bib1.bib4"><label>4</label><mixed-citation>Bock, O. and Nuret, M.: Verification of NWP model analyses and radiosonde
humidity data with GPS precipitable water vapor estimates during AMMA,
Weather Forecast., 24, 1085–1101,  <a href="https://doi.org/10.1175/2009WAF2222239.1" target="_blank">https://doi.org/10.1175/2009WAF2222239.1</a>,  2009.
</mixed-citation></ref-html>
<ref-html id="bib1.bib5"><label>5</label><mixed-citation>Bock, O., Willis, P., Wang, J., and Mears, C.: A high-quality, homogenized,
global, long-term (1993–2008) DORIS precipitable water data set for climate
monitoring and model verification, J. Geophys. Res.-Atmos., 119, 7209–7230,
<a href="https://doi.org/10.1002/2013JD021124" target="_blank">https://doi.org/10.1002/2013JD021124</a>,
2014.
</mixed-citation></ref-html>
<ref-html id="bib1.bib6"><label>6</label><mixed-citation>Bock, O., Bosser, P., Pacione, R., Nuret, M., Fourrié, N., and Parracho,
A.: A high-quality reprocessed ground-based GPS dataset for atmospheric
process studies, radiosonde and model evaluation, and reanalysis of HyMeX
Special Observing Period, Q. J. Roy. Meteor. Soc., 142, 56–71,  <a href="https://doi.org/10.1002/qj.2701" target="_blank">https://doi.org/10.1002/qj.2701</a>,  2016.
</mixed-citation></ref-html>
<ref-html id="bib1.bib7"><label>7</label><mixed-citation>Böhm, J., Niell, A. E., Tregoning, P., and Schuh, H.: 2006, Global
Mapping Functions (GMF): A new empirical mapping function based on numerical
weather model data, Geophys. Res. Lett., 33, L07304,  <a href="https://doi.org/10.1029/2005GL025546" target="_blank">https://doi.org/10.1029/2005GL025546</a>, 2006a.
</mixed-citation></ref-html>
<ref-html id="bib1.bib8"><label>8</label><mixed-citation>Böhm, J., Werl, B., and Schuh, H.: Troposphere mapping functions for GPS
and very long baseline interferometry from European Centre for Medium-Range
Weather Forecasts operational analysis data. J. Geophys. Res., 111, B02406,
<a href="https://doi.org/10.1029/2005JB003629" target="_blank">https://doi.org/10.1029/2005JB003629</a>,
2006b.
</mixed-citation></ref-html>
<ref-html id="bib1.bib9"><label>9</label><mixed-citation>Bruyninx, C., Habrich, H., Söhne, W., Kenyeres, A.,
Stangl, G., and Völksen, C.: Enhancement of the EUREF Permanent Network
Services and Products, Geodesy for Planet Earth, IAG Symposia Series, 136,
27–35,  <a href="https://doi.org/10.1007/978-3-642-20338-1_4" target="_blank">https://doi.org/10.1007/978-3-642-20338-1_4</a>, 2012.
</mixed-citation></ref-html>
<ref-html id="bib1.bib10"><label>10</label><mixed-citation>Dach, R., Böhm, J., Lutz, S., Steigenberger, P., and Beutler, G.:
Evaluation of the impact of atmospheric pressure loading modeling on GNSS
data analysis, J. Geodynam., 85, 75–91, <a href="https://doi.org/10.1007/s00190-010-0417-z" target="_blank">https://doi.org/10.1007/s00190-010-0417-z</a>, 2011.
</mixed-citation></ref-html>
<ref-html id="bib1.bib11"><label>11</label><mixed-citation>Dach, R., Schaer, S., Lutz, S., Baumann, C., Bock, H., Orliac, E., Prange,
L., Thaller, D., Mervart, L., Jäggi, A., Beutler, G., Brockmann, E.,
Ineichen, D., Wiget, A., Weber, G., Habrich, H., Söhne, W., Ihde, J.,
Steigenberger, P., and Hugentobler, U.: CODE IGS Analysis Center Technical
Report 2013, edited by: Dach, R. and Jean, Y., IGS 2013 Tech. Rep., 21–34,
2014.
</mixed-citation></ref-html>
<ref-html id="bib1.bib12"><label>12</label><mixed-citation>Dach, R., Lutz, S., Walser, P., and Fridez, P. (Eds.): Bernese GNSS Software
Version 5.2. User manual, Astronomical Institute, University of Bern, Bern
Open Publishing, 2015.
</mixed-citation></ref-html>
<ref-html id="bib1.bib13"><label>13</label><mixed-citation>
Dee, D. P., Uppala, S. M., Simmons, A. J., Berrisford, P., Poli, P.,
Kobayashi, S., Andrae, U., Balmaseda, M. A., Balsamo, G., Bauer, P.,
Bechtold, P., Beljaars, A. C. M., van de Berg, L., Bidlot, J., Bormann, N.,
Delsol, C., Dragani, R., Fuentes, M., Geer, A. J., Haimberger, L., Healy, S.
B., Hersbach, H., Hólm, E. V., Isaksen, L., Kållberg, P., Köhler, M.,
Matricardi, M., McNally, A. P., Monge-Sanz, B. M., Morcrette, J.-J., Park,
B.-K., Peubey, C., de Rosnay, P., Tavolato, C., Thépaut, J.-N., and Vitart,
F.: The ERA-Interim reanalysis: Configuration and performance of the data
assimilation system, Q. J. Roy. Meteorol. Soc., 137, 553–597,
<a href="https://doi.org/10.1002/qj.828" target="_blank">https://doi.org/10.1002/qj.828</a>, 2011.
</mixed-citation></ref-html>
<ref-html id="bib1.bib14"><label>14</label><mixed-citation>Douša, J.  and Václavovic, P.: Results of GPS Reprocessing campaign
(1996–2011) provided by Geodetic observatory Pecný, Geoinformatics, FCE
CTU, 9, 77–89, <a href="https://doi.org/10.14311/gi.9.7" target="_blank">https://doi.org/10.14311/gi.9.7</a>,  2012.
</mixed-citation></ref-html>
<ref-html id="bib1.bib15"><label>15</label><mixed-citation>
Douša, J., Dick, G., Kacmarík, M., Brožková, R., Zus, F., Brenot,
H., Stoycheva, A., Möller, G., and Kaplon, J.: Benchmark campaign and case
study episode in central Europe for development and assessment of advanced
GNSS tropospheric models and products, Atmos. Meas. Tech., 9, 2989–3008,
<a href="https://doi.org/10.5194/amt-9-2989-2016" target="_blank">https://doi.org/10.5194/amt-9-2989-2016</a>, 2016.
</mixed-citation></ref-html>
<ref-html id="bib1.bib16"><label>16</label><mixed-citation>Douša, J., Böhm, O., Byram, S., Hackman, C., Deng Z., Zus, F., Dach,
R., and Steigenberger, P.: Evaluation of GNSS reprocessing tropospheric
products using GOP-TropDB, IGS Workshop 2016, Sydney, 8–12 February 2017,
available at: <a href="http://www.igs.org/assets/pdf/W2016 - PS0303 - Dousa.pdf" target="_blank">http://www.igs.org/assets/pdf/W2016 - PS0303 - Dousa.pdf</a>,
last access: September 2017 2017.
</mixed-citation></ref-html>
<ref-html id="bib1.bib17"><label>17</label><mixed-citation>
Dow, J. M., Neilan, R. E., and Rizos, C.: The International GNSS Service in a changing landscape of Global Navigation Satellite Systems, J.  Geod., 83, 191–198,
<a href="https://doi.org/10.1007/s00190-008-0300-3" target="_blank">https://doi.org/10.1007/s00190-008-0300-3</a>, 2009.
</mixed-citation></ref-html>
<ref-html id="bib1.bib18"><label>18</label><mixed-citation>Fritsche, M., Dietrich, R., Knofel, C., Rlke, A., Vey, S., Rothacher, M.,
and Steigenberger, P.: Impact of higher-order ionospheric terms on GPS
estimates. Geophys. Res. Lett., 32, L23311,  <a href="https://doi.org/10.1029/2005GL024342" target="_blank">https://doi.org/10.1029/2005GL024342</a>, 2005.
</mixed-citation></ref-html>
<ref-html id="bib1.bib19"><label>19</label><mixed-citation>
Guerova, G., Jones, J., Douša, J., Dick, G., de Haan, S., Pottiaux, E.,
Bock, O., Pacione, R., Elgered, G., Vedel, H.,
and Bender, M.: Review of the state of the art and future prospects of the ground-based GNSS meteorology in Europe, Atmos. Meas. Tech., 9, 5385–5406,  <a href="https://doi.org/10.5194/amt-9-5385-2016" target="_blank">https://doi.org/10.5194/amt-9-5385-2016</a>, 2016.
</mixed-citation></ref-html>
<ref-html id="bib1.bib20"><label>20</label><mixed-citation>Győri, G.  and Douša, J.: GOP-TropDB developments for tropospheric
product evaluation and monitoring – design, functionality and initial
results, IAG Symposia Series, Springer, 143, 595–602, 2016.
</mixed-citation></ref-html>
<ref-html id="bib1.bib21"><label>21</label><mixed-citation>IERS Conventions: Gérard, P., and Luzum, B. (Eds.): IERS Technical Note
No. 36, Frankfurt am Main, Verlag des Bundesamts für Kartographie und
Geodäsie, 179 pp., 2010.
</mixed-citation></ref-html>
<ref-html id="bib1.bib22"><label>22</label><mixed-citation>Ihde, J., Habrich, H., Sacher, M., Sohne, W., Altamimi, Z., Brockmann, E.,
Bruyninx, C., Caporali, A., Dousa, J., Fernandes, R., Hornik, H., Kenyeres,
A., Lidberg, M., Makinen, J., Poutanen, M., Stangl, G., Torres, J. A., and
Volksen, C.: EUREF's Contribution to National, European and Global Geodetic
Infrastructures, in: Earth on the Edge: Science for a Sustainable Planet,
edited by: Rizos, C. and Willis, P., IAG Symposia Series, Springer, 139,
189–196, <a href="https://doi.org/10.1007/978-3-642-37222-3_24" target="_blank">https://doi.org/10.1007/978-3-642-37222-3_24</a>, 2014.
</mixed-citation></ref-html>
<ref-html id="bib1.bib23"><label>23</label><mixed-citation>
Kacmarík, M., Douša, J., Dick, G., Zus, F., Brenot, H., Möller, G.,
Pottiaux, E., Kaplon, J., Hordyniec, P., Václavovic, P., and Morel, L.:
Inter-technique validation of tropospheric slant total delays, Atmos. Meas.
Tech., 10, 2183–2208, <a href="https://doi.org/10.5194/amt-10-2183-2017" target="_blank">https://doi.org/10.5194/amt-10-2183-2017</a>, 2017.
</mixed-citation></ref-html>
<ref-html id="bib1.bib24"><label>24</label><mixed-citation>
Klos, A., Hunegnaw, A., Teferle, F. N., Abraha, K. E., Ahmed, F., and Bogusz,
J.: Noise characteristics in Zenith Total Delay from homogeneously
reprocessed GPS time series, Atmos. Meas. Tech. Discuss.,
<a href="https://doi.org/10.5194/amt-2016-385" target="_blank">https://doi.org/10.5194/amt-2016-385</a>, 2016.
</mixed-citation></ref-html>
<ref-html id="bib1.bib25"><label>25</label><mixed-citation>Li, X., Zus, F., Lu, C., Ning, T., Dick, G., Ge, M., Wickert, J., and Schuh,
H.: Retrieving high-resolution tropospheric gradients from multiconstellation
GNSS observations, Geophys. Res. Lett., 42, 4173–4181,  <a href="https://doi.org/10.1002/2015GL063856" target="_blank">https://doi.org/10.1002/2015GL063856</a>, 2015.
</mixed-citation></ref-html>
<ref-html id="bib1.bib26"><label>26</label><mixed-citation>MacMillan, D. S.: Atmospheric gradients from very long baseline
interferometry observations, Geophys. Res. Lett., 22, 1041–1044, <a href="https://doi.org/10.1029/95GL00887" target="_blank">https://doi.org/10.1029/95GL00887</a>, 1995.
</mixed-citation></ref-html>
<ref-html id="bib1.bib27"><label>27</label><mixed-citation>Meindl, M., Schaer, S., Hugentobler, U., and Beutler, G.: Tropospheric
Gradient Estimation at CODE: Results from Global Solutions, J. Meteorol. Soc.
Jpn., 82, 331–338, 2004.
</mixed-citation></ref-html>
<ref-html id="bib1.bib28"><label>28</label><mixed-citation>Morel, L., Pottiaux, E., Durand, F., Fund, F., Follin, J. M., Durand, S.,
Bonifac, K., Oliveira, P. S., van Baelen, J., Montibert, C., Cavallo, T.,
Escaffit, R., and Fragnol, L.: Global validity and behaviour of tropospheric
gradients estimated by GPS, presentation at the 2nd GNSS4SWEC Workshop held
in Thessaloniki, Greece, 11–14 May 2015.
</mixed-citation></ref-html>
<ref-html id="bib1.bib29"><label>29</label><mixed-citation>Nilsson, T. and Elgered, G., Long-term trends in the atmospheric water
vapor content estimated from ground-based GPS data, J. Geophys. Res., 113,
D19101, <a href="https://doi.org/10.1029/2008JD010110" target="_blank">https://doi.org/10.1029/2008JD010110</a>,  2008.
</mixed-citation></ref-html>
<ref-html id="bib1.bib30"><label>30</label><mixed-citation>Ning, T.: GPS Meteorology: With Focus on Climate Applications, PhD Thesis,
Dept. Earth and Space Sciences, Chalmers University of Technology, 2012.
</mixed-citation></ref-html>
<ref-html id="bib1.bib31"><label>31</label><mixed-citation>Ning, T. and Elgered, E.: Trends in the atmospheric water vapor content
from ground-based GPS: The impact of the elevation cutoff angle, IEEE J. Sel.
Top. Appl., 5, 744–751,  <a href="https://doi.org/10.1109/JSTARS.2012.2191392" target="_blank">https://doi.org/10.1109/JSTARS.2012.2191392</a>, 2012.

</mixed-citation></ref-html>
<ref-html id="bib1.bib32"><label>32</label><mixed-citation>
Pacione, R., Araszkiewicz, A., Brockmann, E., and Dousa, J.: EPN-Repro2: A
reference GNSS tropospheric data set over Europe, Atmos. Meas. Tech., 10,
1689–1705, <a href="https://doi.org/10.5194/amt-10-1689-2017" target="_blank">https://doi.org/10.5194/amt-10-1689-2017</a>, 2017.
</mixed-citation></ref-html>
<ref-html id="bib1.bib33"><label>33</label><mixed-citation>Steigenberger, P., Böhm, J., and Tesmer, V.: Comparison of GMF/GPT with
VMF1/ECMWF and implications for atmospheric loading, J. Geodynam., 83, 943,
<a href="https://doi.org/10.1007/s00190-009-0311-8" target="_blank">https://doi.org/10.1007/s00190-009-0311-8</a>,
2009.
</mixed-citation></ref-html>
<ref-html id="bib1.bib34"><label>34</label><mixed-citation>Václavovic, P.  and Douša, J.: G-Nut/Anubis – open-source tool for
multi-GNSS data monitoring, in: IAG 150 Years, edited by: Rizos, Ch. and
Willis, P., IAG Symposia Series, Springer, 143, 775–782,  <a href="https://doi.org/10.1007/1345_2015_97" target="_blank">https://doi.org/10.1007/1345_2015_97</a>, 2016.
</mixed-citation></ref-html>
<ref-html id="bib1.bib35"><label>35</label><mixed-citation>Völksen, C.: An update on the EPN Reprocessing Project: Current
Achievements and Status, Presented at the EUREF 2011 Symposium, Chisinau,
Republic of Moldova, 25–28 May, available at: <a href="http://www.epncb.oma.be/_&#xA;documentation/papers/eurefsymposium2011/an_update_on_epn_&#xA;reprocessing_project_current_achievement_and_status" target="_blank">http://www.epncb.oma.be/_
documentation/papers/eurefsymposium2011/an_update_on_epn_
reprocessing_project_current_achievement_and_status</a> (last access: September 2017),
2011.
</mixed-citation></ref-html>
<ref-html id="bib1.bib36"><label>36</label><mixed-citation>
Weatherhead, E. C., Reinsel, G. C., Tiao, G. C., Meng, X.-L., Choi, D.,
Cheang, W.-K., Keller, T., DeLuisi, J., Wuebbles, D. J., Kerr, J. B., Miller,
A. J., Oltmans, S. J., and Frederick J. E.: Factors affecting the detection
of trends: Statistical considerations and applications to environmental data,
J. Geophys. Res., 103, 17149–17161, <a href="https://doi.org/10.1029/98JD00995" target="_blank">https://doi.org/10.1029/98JD00995</a>, 1998.
</mixed-citation></ref-html>
<ref-html id="bib1.bib37"><label>37</label><mixed-citation>Yuan, L. L., Anthes, R. A., Ware, R. H., Rocken, C., Bonner, W. D., Bevis, M. G.,
and Businger, S.: Sensing Climate Change Using the Global Positioning System,
J. Geophys. Res., 98, 14925–14937, 1993.
</mixed-citation></ref-html>
<ref-html id="bib1.bib38"><label>38</label><mixed-citation>Zus, F., Dick, G., Heise, S., Dousa, J., and Wickert, J.: The rapid and
precise computation of GPS slant total delays and mapping factors utilizing a
numerical weather model, Radio Sci., 49, 207–216,  <a href="https://doi.org/10.1002/2013RS005280" target="_blank">https://doi.org/10.1002/2013RS005280</a>, 2014.
</mixed-citation></ref-html>
<ref-html id="bib1.bib39"><label>39</label><mixed-citation>Zus, F., Dick, G., Dousa, J., and Wickert, J.: Systematic errors of mapping
functions which are based on the VMF1 concept, GPS Solut., 19, 277–286,
<a href="https://doi.org/10.1007/s10291-014-0386-4" target="_blank">https://doi.org/10.1007/s10291-014-0386-4</a>,
2015.
</mixed-citation></ref-html>--></article>
