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<article xmlns:xlink="http://www.w3.org/1999/xlink" xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:oasis="http://docs.oasis-open.org/ns/oasis-exchange/table" dtd-version="3.0"><?xmltex \hack{\sloppy}?>
  <front>
    <journal-meta>
<journal-id journal-id-type="publisher">AMTD</journal-id>
<journal-title-group>
<journal-title>Atmospheric Measurement Techniques Discussions</journal-title>
<abbrev-journal-title abbrev-type="publisher">AMTD</abbrev-journal-title>
<abbrev-journal-title abbrev-type="nlm-ta">Atmos. Meas. Tech. Discuss.</abbrev-journal-title>
</journal-title-group>
<issn pub-type="epub">1867-8610</issn>
<publisher><publisher-name>Copernicus GmbH</publisher-name>
<publisher-loc>Göttingen, Germany</publisher-loc>
</publisher>
</journal-meta>

    <article-meta>
      <article-id pub-id-type="doi">10.5194/amtd-8-235-2015</article-id><title-group><article-title>Validation of merged MSU4 and AMSU9 temperature climate records with
a new 2002–2012 vertically resolved temperature record</article-title>
      </title-group><?xmltex \runningtitle{A~new vertically resolved temperature record}?><?xmltex \runningauthor{A.~A.~Penckwitt et~al.}?>
      <contrib-group>
        <contrib contrib-type="author" corresp="yes" rid="aff1">
          <name><surname>Penckwitt</surname><given-names>A. A.</given-names></name>
          <email>andreas@bodekerscientific.com</email>
        </contrib>
        <contrib contrib-type="author" corresp="no" rid="aff1">
          <name><surname>Bodeker</surname><given-names>G. E.</given-names></name>
          
        <ext-link>https://orcid.org/0000-0003-1094-5852</ext-link></contrib>
        <contrib contrib-type="author" corresp="no" rid="aff1">
          <name><surname>Stoll</surname><given-names>P.</given-names></name>
          
        </contrib>
        <contrib contrib-type="author" corresp="no" rid="aff1">
          <name><surname>Lewis</surname><given-names>J.</given-names></name>
          
        <ext-link>https://orcid.org/0000-0002-8155-8924</ext-link></contrib>
        <contrib contrib-type="author" corresp="no" rid="aff2">
          <name><surname>von Clarmann</surname><given-names>T.</given-names></name>
          
        </contrib>
        <contrib contrib-type="author" corresp="no" rid="aff3">
          <name><surname>Jones</surname><given-names>A.</given-names></name>
          
        </contrib>
        <aff id="aff1"><label>1</label><institution>Bodeker Scientific, Alexandra, New Zealand</institution>
        </aff>
        <aff id="aff2"><label>2</label><institution>Karlsruhe Institute of Technology, Institute for Meteorology and
Climate Research, Karlsruhe, Germany</institution>
        </aff>
        <aff id="aff3"><label>3</label><institution>Department of Physics, University of Toronto, Toronto, Ontario, Canada</institution>
        </aff>
      </contrib-group>
      <author-notes><corresp id="corr1">A. A. Penckwitt (andreas@bodekerscientific.com)</corresp></author-notes><pub-date><day>7</day><month>January</month><year>2015</year></pub-date>
      
      <volume>8</volume>
      <issue>1</issue>
      <fpage>235</fpage><lpage>267</lpage>
      <history>
        <date date-type="received"><day>14</day><month>November</month><year>2014</year></date>
           <date date-type="accepted"><day>12</day><month>December</month><year>2014</year></date>
           
      </history>
      <permissions>
<license license-type="open-access">
<license-p>This work is licensed under a Creative Commons Attribution 3.0 Unported License. To view a copy of this license, visit <ext-link ext-link-type="uri" xlink:href="http://creativecommons.org/licenses/by/3.0/">http://creativecommons.org/licenses/by/3.0/</ext-link></license-p>
</license>
</permissions><self-uri xlink:href="https://amt.copernicus.org/preprints/8/235/2015/amtd-8-235-2015.html">This article is available from https://amt.copernicus.org/preprints/8/235/2015/amtd-8-235-2015.html</self-uri>
<self-uri xlink:href="https://amt.copernicus.org/preprints/8/235/2015/amtd-8-235-2015.pdf">The full text article is available as a PDF file from https://amt.copernicus.org/preprints/8/235/2015/amtd-8-235-2015.pdf</self-uri>


      <abstract>
    <p>A new database of monthly mean zonal mean (5<inline-formula><mml:math display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> zones)
temperature time series spanning 17 pressure levels from 300 to
7 hPa and extending from 2002 to 2012 was created by merging
monthly mean time series from two satellite-based mid-infrared
spectrometers (ACE-FTS and MIPAS), a microwave sounder (SMR), and
from three satellite-based radio occultation experiments (GRACE,
CHAMP, and TSX). The primary intended use of this new temperature
data set is to validate the merging of the Microwave Sounding Unit
channel 4 (MSU4), and Advanced Microwave Sounding Unit channel 9
(AMSU9) temperature time series conducted in previous studies. The
six source data sets were merged by removing offsets and trends
between the different measurement series. Weighted means were
calculated of the six source data sets where the weights were
a function of the uncertainty on the original monthly mean data.
This new temperature data set of the upper troposphere and
stratosphere has been validated by comparing it to RATPAC-A, COSMIC
radio occultation data as well as the NCEPCFSR
reanalyses. Differences in all three cases were typically <inline-formula><mml:math display="inline"><mml:mrow><mml:mo>&lt;</mml:mo><mml:mn mathvariant="normal">2</mml:mn></mml:mrow></mml:math></inline-formula> K
in the upper troposphere and lower stratosphere, but could reach up
to 5 K in the mid-stratosphere.  The data across the 17 pressure
levels have then been vertically integrated, using the MSU4/AMSU9
weighting function, to provide a deep vertical layer temperature
proxy of the merged MSU4+AMSU9 series. Differences between this
vertically integrated data set and two different versions of the
MSU4+AMSU9 data set – one from Remote Sensing Systems and one from
the University of Alabama at Huntsville – were examined for
discontinuities.  No statistically significant discontinuities were
found in either of those two data sets suggesting that the
transition from the MSU4+AMSU9 data to AMSU9 data only does not
introduce any discontinuities in the MSU4+AMSU9 climate data records
that might compromise their use in temperature trend analyses.</p>
  </abstract>
    </article-meta>
  </front>
<body>
      

<sec id="Ch1.S1" sec-type="intro">
  <title>Introduction</title>
      <p>Reliable long-term data records are necessary to detect and understand
climate change. Vertically resolved trends in temperature provide
a sensitive test of the mechanisms driving climate change
<xref ref-type="bibr" rid="bib1.bibx27 bib1.bibx13 bib1.bibx20" id="paren.1"/> which in turn are vital to
improving climate model projections of future climate. The National
Oceanic and Atmospheric Administration (NOAA) operated Microwave
Sounding Units (MSUs) on polar-orbiting satellite platforms from 1978
to 2005 and Advanced Microwave Sounding Units (AMSUs) from 1998
onwards. These nadir-looking instruments became the primary source of
long-term temperature climate records of the troposphere and
stratosphere even though their measurements were originally intended
for short-term weather forecasts, not climate applications.  To create
long-term homogeneous climate data records, measurements need to be
adjusted to account for inter-satellite biases, orbital changes and
calibration deficiencies, as well as small differences in radiometer
frequency and bandwidth between the MSU and AMSU instruments.  Three
such long-term records are currently maintained by independent groups
– Remote Sensing Systems (RSS) <xref ref-type="bibr" rid="bib1.bibx18 bib1.bibx19" id="paren.2"/>, the
University of Alabama at Hunstville (UAH) <xref ref-type="bibr" rid="bib1.bibx11" id="paren.3"/>, and the
Centre for Satellite Applications and Research (STAR) <xref ref-type="bibr" rid="bib1.bibx33" id="paren.4"/>.
While substantial differences in temperature trends were found between
the RSS and UAH data sets in the stratosphere <xref ref-type="bibr" rid="bib1.bibx20" id="paren.5"/>,
trends in the lower stratosphere between (A)MSU data sets are
generally comparable <xref ref-type="bibr" rid="bib1.bibx28" id="paren.6"/>.</p>
      <p>Satellite-based infrared sounders, as well as Global Positioning
System (GPS) radio occultation (RO) experiments, offer high vertical
resolution making them prime candidates to extend the MSU temperature
record and improve the monitoring of upper-air temperature
changes. Temperature measurements from infrared sounders typically
have a measurement uncertainty of <inline-formula><mml:math display="inline"><mml:mrow><mml:mo>&lt;</mml:mo><mml:mn mathvariant="normal">2</mml:mn></mml:mrow></mml:math></inline-formula> K with good horizontal
resolution. RO measurements have moderate horizontal resolution (<inline-formula><mml:math display="inline"><mml:mrow><mml:mo>∼</mml:mo><mml:mn>300</mml:mn></mml:mrow></mml:math></inline-formula> km), but good vertical resolution (<inline-formula><mml:math display="inline"><mml:mrow><mml:mo>∼</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:math></inline-formula> km) and are well
suited for high quality climatologies because of their low systematic
errors (<inline-formula><mml:math display="inline"><mml:mrow><mml:mo>&lt;</mml:mo><mml:mn>0.5</mml:mn></mml:mrow></mml:math></inline-formula> K) and high stability
<xref ref-type="bibr" rid="bib1.bibx9" id="paren.7"/>. <xref ref-type="bibr" rid="bib1.bibx16" id="text.8"/> found good agreement
between RO and radiosonde temperature anomalies, but statistically
significant differences in trend estimates from (A)MSU data compared
to RO measurements which they believed resulted mainly from the (A)MSU
data.</p>
      <p>In this study, monthly mean zonal mean (5<inline-formula><mml:math display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> zones) temperature
time series from six satellite-based instruments, including three RO
instruments, are merged to create a new time series of monthly mean
temperatures on 17 pressure levels from 300 hPa to 7 hPa.  This data
set is then vertically integrated using the (A)MSU vertical weighting
functions to create a (A)MSU proxy record suitable for assessing the
continuity of the merged (A)MSU temperature data sets by the RSS and
UAH groups, focusing on the Temperature Lower Stratosphere (TLS)
product. The TLS series spans altitudes from 13 to 22 km and results
from merging the MSU channel 4 (MSU4) and AMSU channel 9 (AMSU9)
temperature time series.</p>
      <p>Section <xref ref-type="sec" rid="Ch1.S2"/> describes the data sets used to compile our new
vertically resolved temperature data set. In
Sect. <xref ref-type="sec" rid="Ch1.S3"/>, the method used to merge the
six source data sets is described. The merged data set is then
validated against RATPAC (Radiosonde Atmospheric Temperature Products
for Assessing Climate) radiosonde data, COSMIC (Constellation
Observing System for Meteorology, Ionosphere, and Climate) RO data as
well as the NCEPCFSR (National Centers for Environmental Prediction
Climate Forecast System Reanalysis) reanalyses in
Sect. <xref ref-type="sec" rid="Ch1.S4"/>.  In
Sect. <xref ref-type="sec" rid="Ch1.S5"/>, the new data set is vertically
integrated using an appropriate weighting function to create an (A)MSU
proxy. The resulting temperature time series is then used to verify
the merging of MSU4 and AMSU9 temperature series.</p>
</sec>
<sec id="Ch1.S2">
  <title>Data</title>
      <p>Monthly mean zonal mean temperature records from satellite missions by
the European Space Agency (ESA) and Third Party Missions (TPMs), as
well as RO data, were created in collaboration with SPARC
(Stratosphere–troposphere Processes And their Role in Climate) as
a project of SPIN (ESA SPARC Initiative). In the following sections,
we briefly describe the characteristics of the different instruments,
and how the monthly mean zonal mean data sets used in this study were
produced from the individual temperature profiles.</p>
<sec id="Ch1.S2.SS1">
  <title>ESA and ESA-TPM temperature profiles</title>
      <p>Temperature measurements from three instruments of ESA/ESA-TPM were
used – the Michelson Interferometer for Passive Atmospheric Sounding
(MIPAS), the Atmospheric Chemistry Experiment – Fourier Transform
Spectrometer (ACE-FTS) and the Sub-Millimeter Radiometer (SMR).</p>
      <p>MIPAS is a mid-infrared limb emission Fourier transform spectrometer
on board the Environmental Satellite (Envisat). This study is based on
temperature data processed with the MIPAS research processor at the
Institute for Meteorology and Climate Research (IMK) at the Karlsruhe
Institute of Technology (KIT) in cooperation with the Institute de
Astrofìsica de Andalucìa (IAA-CSIC). In particular, the high
spectral resolution data V3O_T_8 were used from June 2002 to
March 2004 with an uncertainty of 0.4–0.8 K at <inline-formula><mml:math display="inline"><mml:mrow><mml:mo>∼</mml:mo><mml:mn mathvariant="normal">3</mml:mn></mml:mrow></mml:math></inline-formula> km vertical
resolution for stratospheric altitudes <xref ref-type="bibr" rid="bib1.bibx29" id="paren.9"/>. For the
time period from April 2004 to December 2004 no MIPAS data were
available. From January 2005 to April 2010 the reduced resolution data
V5R_T_220 were used with an uncertainty of 0.5–1.4 K and
a vertical resolution of 2–3.5 km <xref ref-type="bibr" rid="bib1.bibx31 bib1.bibx26" id="paren.10"/>.
The horizontal resolution of MIPAS temperatures is about 300 km for
the high resolution data pre 2004 and about 120 to 400 km for the
reduced resolution data post 2004 <xref ref-type="bibr" rid="bib1.bibx30" id="paren.11"/>.</p>
      <p>ACE-FTS is a Fourier transform spectrometer on the Canadian SCISAT
satellite using solar occultation mid-infrared spectra to retrieve
vertical profiles of temperature. The uncertainty on the ACE-FTS
measurements has not been published, but the systematic error of the
Version 2.2 data is estimated to be 2 K at 10–50 km
<xref ref-type="bibr" rid="bib1.bibx25" id="paren.12"/>. The vertical resolution of ACE-FTS measurements is
<inline-formula><mml:math display="inline"><mml:mrow><mml:mo>∼</mml:mo><mml:mn mathvariant="normal">3</mml:mn></mml:mrow></mml:math></inline-formula>–4 km <xref ref-type="bibr" rid="bib1.bibx5" id="paren.13"/>. As ACE-FTS makes no more than 30
measurements a day, its spatial and temporal resolutions are lower
than those of the other instruments used in this study. Furthermore,
ACE-FTS only measures certain latitudes for a given time of the year.</p>
      <p>Our temperature data set was created from Version 3.0 data covering
February 2004 to March 2011. The ACE-FTS product uses a priori
information for pressure and temperature at low altitudes from the
Canadian Meteorological Center (CMC). After our analysis was well
underway, it was discovered that Version 3.0 data should only be used
until the end of September 2010 because of problems with how the
pressure and temperature information was extracted from the CMC
models. These issues give inaccurate results for all of the retrievals
past this date <xref ref-type="bibr" rid="bib1.bibx8" id="paren.14"/>. In addition, quality flags were
recently introduced for all level 2 version 2.5 and 3.5 data
<xref ref-type="bibr" rid="bib1.bibx24" id="paren.15"/>, but no updated version of the monthly mean zonal
mean temperature data set used in this study has been made available
yet.</p>
      <p>SMR is a passive microwave sounder on the Odin satellite with four
tunable receivers in the <inline-formula><mml:math display="inline"><mml:mrow><mml:mo>∼</mml:mo><mml:mn>486</mml:mn></mml:mrow></mml:math></inline-formula>–581 GHz spectral range as well
as one mm-wave receiver. Temperature measurements in the stratosphere
are made in the 544.6 GHz band. Version 2.0 data from August 2001 to
April 2012 were used. The uncertainty of the temperature data is
estimated to be 1–3 K while the vertical resolution for the
544.6 GHz band is 4–6 km. No information on any systematic errors
is available.</p>
</sec>
<sec id="Ch1.S2.SS2">
  <title>RO temperature profiles</title>
      <p>The GPS RO limb sounding technique has many advantages compared to
infrared sounding measurements from space. The measurements are
self-calibrating and independent of the mission. Thus, there is
expected to be no satellite-to-satellite bias or instrumental
drift. RO observations achieve global coverage with high vertical
resolution of about 1 km in the lower stratosphere.  Measurements are
minimally affected by aerosols, clouds or precipitation, leading to
very small systematic biases (equivalent to <inline-formula><mml:math display="inline"><mml:mrow><mml:mo>&lt;</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:math></inline-formula> <inline-formula><mml:math display="inline"><mml:mi mathvariant="normal">K</mml:mi></mml:math></inline-formula>; average
systematic bias is <inline-formula><mml:math display="inline"><mml:mrow><mml:mo>&lt;</mml:mo><mml:mn>0.1</mml:mn></mml:mrow></mml:math></inline-formula> <inline-formula><mml:math display="inline"><mml:mi mathvariant="normal">K</mml:mi></mml:math></inline-formula>) and small measurement
uncertainties (0.02–0.05 <inline-formula><mml:math display="inline"><mml:mi mathvariant="normal">K</mml:mi></mml:math></inline-formula>) <xref ref-type="bibr" rid="bib1.bibx3" id="paren.16"/>.</p>
      <p>The CHAMP (CHAllenging Minisatellite Payload) satellite was launched
in 2000 <xref ref-type="bibr" rid="bib1.bibx32" id="paren.17"/>. It provided the first long-term continuous
GPS RO data set from May 2001 to October 2008. The temperature profiles
have a vertical resolution of 1.5 km and have a systematic bias
of <inline-formula><mml:math display="inline"><mml:mrow><mml:mo>∼</mml:mo><mml:mn>0.5</mml:mn></mml:mrow></mml:math></inline-formula> K between 5–20 km <xref ref-type="bibr" rid="bib1.bibx9" id="paren.18"/>.</p>
      <p>The GRACE (Gravity Recovery and Climate Experiment) is a twin
satellite configuration based on CHAMP heritage <xref ref-type="bibr" rid="bib1.bibx6" id="paren.19"/>
with similar resolution and uncertainty to CHAMP
<xref ref-type="bibr" rid="bib1.bibx32" id="paren.20"/>. The data set extends from January 2006 to
December 2011.</p>
      <p>The most recent RO data come from the Tracking, Occultation and
Ranging instrument package on board of the TerraSAR-X (hereafter
referred to as TSX) that was launched in 2007 <xref ref-type="bibr" rid="bib1.bibx7" id="paren.21"/>. The
vertical resolution in the upper troposphere/lower stratosphere is
about 500 m.  The data set spans July 2008 to March 2012.</p>
      <p>CHAMP, GRACE and TSX data were obtained directly from the
GeoForschungsZentrum (GFZ) Helmholtz Centre using Potsdam Occultation
Software version 6.0.</p>
</sec>
<sec id="Ch1.S2.SS3">
  <title>Monthly mean zonal mean temperature records</title>
      <p>The individual temperature profiles used to calculate the monthly mean
zonal mean data sets were carefully screened according to
recommendations given in relevant quality control documents, in
published literature, and/or according to best knowledge of the
instrument scientists. Linear interpolation in log pressure
coordinates was used to interpolate individual temperature profiles
onto the pressure grid 300, 250, 200, 170, 150, 130, 115, 100, 90, 80,
70, 50, 30, 20, 15, 10, 7, 5, 3, 2, 1.5, 1, 0.7, 0.5, 0.3, 0.2, 0.15,
and 0.1 hPa. For instruments providing data on an altitude grid,
conversion from altitude to pressure levels was done using retrieved
temperature/pressure profiles or meteorological analyses. Zonal means
were calculated as the average of all of the measurements on a given
pressure level within each 5<inline-formula><mml:math display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> latitude zone. The standard
error of the mean of the measurements was used as uncertainty on the
mean values within each latitude zone at each pressure level.</p>
      <p>Additionally, the RO data were screened such that temperatures below
150 K were omitted as were temperatures above 330 K. The
interpolated values were corrected for their zonal mean and monthly
mean representativeness using NCEPCFSR 6 hourly temperature fields on
pressure surfaces as

                <disp-formula id="Ch1.E1" content-type="numbered"><mml:math display="block"><mml:mrow><mml:msub><mml:mi>T</mml:mi><mml:mtext>corr</mml:mtext></mml:msub><mml:mo>=</mml:mo><mml:msub><mml:mi>T</mml:mi><mml:mtext>RO</mml:mtext></mml:msub><mml:mo>(</mml:mo><mml:mi mathvariant="italic">θ</mml:mi><mml:mo>,</mml:mo><mml:mi mathvariant="italic">ϕ</mml:mi><mml:mo>,</mml:mo><mml:mi>P</mml:mi><mml:mo>,</mml:mo><mml:mi>t</mml:mi><mml:mo>)</mml:mo><mml:mo>×</mml:mo><mml:mfrac><mml:mrow><mml:msub><mml:mover accent="true"><mml:mi>T</mml:mi><mml:mo mathvariant="normal">‾</mml:mo></mml:mover><mml:mtext>CFSR</mml:mtext></mml:msub><mml:mo>(</mml:mo><mml:msup><mml:mn mathvariant="normal">5</mml:mn><mml:mo>∘</mml:mo></mml:msup><mml:mo>,</mml:mo><mml:mi>P</mml:mi><mml:mo>,</mml:mo><mml:mspace width="0.25em" linebreak="nobreak"/><mml:mtext>month</mml:mtext><mml:mo>)</mml:mo></mml:mrow><mml:mrow><mml:msub><mml:mi>T</mml:mi><mml:mtext>CFSR</mml:mtext></mml:msub><mml:mo>(</mml:mo><mml:mi mathvariant="italic">θ</mml:mi><mml:mo>,</mml:mo><mml:mi mathvariant="italic">ϕ</mml:mi><mml:mo>,</mml:mo><mml:mi>P</mml:mi><mml:mo>,</mml:mo><mml:mi>t</mml:mi><mml:mo>)</mml:mo></mml:mrow></mml:mfrac><mml:mo>,</mml:mo></mml:mrow></mml:math></disp-formula>

          where <inline-formula><mml:math display="inline"><mml:mrow><mml:msub><mml:mi>T</mml:mi><mml:mtext>corr</mml:mtext></mml:msub></mml:mrow></mml:math></inline-formula> is the bias corrected temperature value,
<inline-formula><mml:math display="inline"><mml:mrow><mml:msub><mml:mi>T</mml:mi><mml:mtext>RO</mml:mtext></mml:msub></mml:mrow></mml:math></inline-formula> is the RO temperature measurement interpolated onto
pressure <inline-formula><mml:math display="inline"><mml:mi>P</mml:mi></mml:math></inline-formula> at latitude <inline-formula><mml:math display="inline"><mml:mi mathvariant="italic">θ</mml:mi></mml:math></inline-formula>, longitude <inline-formula><mml:math display="inline"><mml:mi mathvariant="italic">ϕ</mml:mi></mml:math></inline-formula> at time <inline-formula><mml:math display="inline"><mml:mi>t</mml:mi></mml:math></inline-formula>,
<inline-formula><mml:math display="inline"><mml:mrow><mml:msub><mml:mover accent="true"><mml:mi>T</mml:mi><mml:mo mathvariant="normal">‾</mml:mo></mml:mover><mml:mtext>CFSR</mml:mtext></mml:msub><mml:mo>(</mml:mo><mml:msup><mml:mn mathvariant="normal">5</mml:mn><mml:mo>∘</mml:mo></mml:msup><mml:mo>,</mml:mo><mml:mi>P</mml:mi><mml:mo>,</mml:mo><mml:mspace width="0.25em" linebreak="nobreak"/><mml:mtext>month</mml:mtext><mml:mo>)</mml:mo></mml:mrow></mml:math></inline-formula> is the
NCEPCFSR 5<inline-formula><mml:math display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> monthly mean zonal mean temperature at pressure
<inline-formula><mml:math display="inline"><mml:mi>P</mml:mi></mml:math></inline-formula>, and <inline-formula><mml:math display="inline"><mml:mrow><mml:msub><mml:mi>T</mml:mi><mml:mtext>CFSR</mml:mtext></mml:msub></mml:mrow></mml:math></inline-formula> is the NCEPCFSR temperature at the same
time and location as <inline-formula><mml:math display="inline"><mml:mrow><mml:msub><mml:mi>T</mml:mi><mml:mtext>RO</mml:mtext></mml:msub></mml:mrow></mml:math></inline-formula>. Applying Eq. (<xref ref-type="disp-formula" rid="Ch1.E1"/>)
corrects the RO measurements for their sampling bias both in terms of
geographical coverage and temporal coverage within the month of
interest.</p>
      <p>It may be noted that this mean representative correction was only
applied to the RO measurements though it might also have
been a useful correction for the other three instruments, especially
in the case of ACE-FTS with its low sampling rate. For this reason,
monthly mean temperatures that were obtained from only a small number
of measurements are excluded from the merging process as described in
the next section.</p>
</sec>
</sec>
<sec id="Ch1.S3">
  <title>Constructing a single merged temperature climate data record</title>
      <p>The monthly mean zonal mean temperature data sets from the three
ESA/ESA-TPM instruments and the three RO experiments described in
Sect. <xref ref-type="sec" rid="Ch1.S2"/> were merged to create new zonal mean monthly mean
temperature time series in 5<inline-formula><mml:math display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> latitude zones, henceforth
referred to as the vertically resolved temperature (VRT) climate
record or data set.  As not all of the six source data sets had
measurements at all 27 pressure levels mentioned in
Sect. <xref ref-type="sec" rid="Ch1.S2.SS3"/>, only the first 17 pressure
levels were used. RO measurements have been shown to be an effective
climate benchmark below <inline-formula><mml:math display="inline"><mml:mrow><mml:mo>∼</mml:mo><mml:mn>25</mml:mn></mml:mrow></mml:math></inline-formula> km altitude
<xref ref-type="bibr" rid="bib1.bibx15 bib1.bibx1" id="paren.22"/>. Comparisons of the annual mean zonal
mean temperatures calculated from the three RO data sets show
agreement within 0.5 K in the lower stratosphere (<inline-formula><mml:math display="inline"><mml:mrow><mml:mo>∼</mml:mo><mml:mn>20</mml:mn></mml:mrow></mml:math></inline-formula> km) but
there is a robust bias that increases in magnitude with height,
reaching 3–5 K in the upper stratosphere, near 40 km. GRACE is
consistently warmer than both CHAMP and TSX in the Southern Hemisphere
and consistently colder in the Northern Hemisphere. Because of the
systematic bias of GRACE against both CHAMP and TSX, we exclude GRACE
as a suitable benchmark data set for the construction of the merged
product. Choosing between CHAMP and TSX as an initial data set, CHAMP
provides a longer data record.</p>
      <p>Figure <xref ref-type="fig" rid="App1.Ch1.F1"/> shows graphically the process of how,
starting with CHAMP as the benchmark data set, the remaining data sets
are successively merged. At each latitude zone and pressure level, the
data set with the biggest temporal overlap with CHAMP is chosen as the
first candidate to be merged with CHAMP. In the example of
Fig. <xref ref-type="fig" rid="App1.Ch1.F1"/>, MIPAS is found to have the biggest
overlap with CHAMP. Thus, differences are calculated between the CHAMP
and MIPAS monthly mean temperatures and these are then modelled
statistically using a regression model that includes an offset and
drift where the offset fit coefficient is expanded in Fourier pairs to
also account for seasonality in the differences, i. e.:

              <disp-formula id="Ch1.E2" content-type="numbered"><mml:math display="block"><mml:mrow><mml:mi>f</mml:mi><mml:mo>(</mml:mo><mml:mi>t</mml:mi><mml:mo>)</mml:mo><mml:mo>=</mml:mo><mml:msub><mml:mi>a</mml:mi><mml:mn mathvariant="normal">1</mml:mn></mml:msub><mml:mo>+</mml:mo><mml:msub><mml:mi>a</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub><mml:mi>t</mml:mi><mml:mo>+</mml:mo><mml:msub><mml:mi>a</mml:mi><mml:mn mathvariant="normal">3</mml:mn></mml:msub><mml:mi>sin⁡</mml:mi><mml:mo>(</mml:mo><mml:mn mathvariant="normal">2</mml:mn><mml:mi mathvariant="italic">π</mml:mi><mml:mi>t</mml:mi><mml:mo>)</mml:mo><mml:mo>+</mml:mo><mml:msub><mml:mi>a</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub><mml:mi>cos⁡</mml:mi><mml:mo>(</mml:mo><mml:mn mathvariant="normal">2</mml:mn><mml:mi mathvariant="italic">π</mml:mi><mml:mi>t</mml:mi><mml:mo>)</mml:mo><mml:mo>+</mml:mo><mml:msub><mml:mi>a</mml:mi><mml:mn mathvariant="normal">5</mml:mn></mml:msub><mml:mi>sin⁡</mml:mi><mml:mo>(</mml:mo><mml:mn mathvariant="normal">4</mml:mn><mml:mi mathvariant="italic">π</mml:mi><mml:mi>t</mml:mi><mml:mo>)</mml:mo><mml:mo>+</mml:mo><mml:msub><mml:mi>a</mml:mi><mml:mn mathvariant="normal">6</mml:mn></mml:msub><mml:mi>cos⁡</mml:mi><mml:mo>(</mml:mo><mml:mn mathvariant="normal">4</mml:mn><mml:mi mathvariant="italic">π</mml:mi><mml:mi>t</mml:mi><mml:mo>)</mml:mo><mml:mo>.</mml:mo></mml:mrow></mml:math></disp-formula>

        The uncertainty of the difference function <inline-formula><mml:math display="inline"><mml:mrow><mml:mi>f</mml:mi><mml:mo>(</mml:mo><mml:mi>t</mml:mi><mml:mo>)</mml:mo></mml:mrow></mml:math></inline-formula> takes into account
possible correlations between the coefficients

              <disp-formula id="Ch1.E3" content-type="numbered"><mml:math display="block"><mml:mrow><mml:msubsup><mml:mi mathvariant="italic">σ</mml:mi><mml:mi>f</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msubsup><mml:mo>(</mml:mo><mml:mi>t</mml:mi><mml:mo>)</mml:mo><mml:mo>=</mml:mo><mml:munderover><mml:mo movablelimits="false">∑</mml:mo><mml:mrow><mml:mi>i</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow><mml:mn mathvariant="normal">6</mml:mn></mml:munderover><mml:msup><mml:mfenced open="(" close=")"><mml:mfrac><mml:mrow><mml:mo>∂</mml:mo><mml:mi>f</mml:mi><mml:mo>(</mml:mo><mml:mi>t</mml:mi><mml:mo>)</mml:mo></mml:mrow><mml:mrow><mml:mo>∂</mml:mo><mml:msub><mml:mi>a</mml:mi><mml:mi>i</mml:mi></mml:msub></mml:mrow></mml:mfrac></mml:mfenced><mml:mn mathvariant="normal">2</mml:mn></mml:msup><mml:mo>⋅</mml:mo><mml:msubsup><mml:mi mathvariant="italic">σ</mml:mi><mml:mrow><mml:msub><mml:mi>a</mml:mi><mml:mi>i</mml:mi></mml:msub></mml:mrow><mml:mn mathvariant="normal">2</mml:mn></mml:msubsup><mml:mo>+</mml:mo><mml:mn mathvariant="normal">2</mml:mn><mml:munderover><mml:mo movablelimits="false">∑</mml:mo><mml:mrow><mml:mi>i</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow><mml:mn mathvariant="normal">5</mml:mn></mml:munderover><mml:munderover><mml:mo movablelimits="false">∑</mml:mo><mml:mrow><mml:mi>k</mml:mi><mml:mo>=</mml:mo><mml:mi>i</mml:mi><mml:mo>+</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow><mml:mn mathvariant="normal">6</mml:mn></mml:munderover><mml:mfrac><mml:mrow><mml:mo>∂</mml:mo><mml:mi>f</mml:mi><mml:mo>(</mml:mo><mml:mi>t</mml:mi><mml:mo>)</mml:mo></mml:mrow><mml:mrow><mml:mo>∂</mml:mo><mml:msub><mml:mi>a</mml:mi><mml:mi>i</mml:mi></mml:msub></mml:mrow></mml:mfrac><mml:mfrac><mml:mrow><mml:mo>∂</mml:mo><mml:mi>f</mml:mi><mml:mo>(</mml:mo><mml:mi>t</mml:mi><mml:mo>)</mml:mo></mml:mrow><mml:mrow><mml:mo>∂</mml:mo><mml:msub><mml:mi>a</mml:mi><mml:mi>k</mml:mi></mml:msub></mml:mrow></mml:mfrac><mml:mo>⋅</mml:mo><mml:mtext>cov</mml:mtext><mml:mo>(</mml:mo><mml:msub><mml:mi>a</mml:mi><mml:mi>i</mml:mi></mml:msub><mml:mo>,</mml:mo><mml:msub><mml:mi>a</mml:mi><mml:mi>k</mml:mi></mml:msub><mml:mo>)</mml:mo></mml:mrow></mml:math></disp-formula>

        The statistical model fit from Eq. (<xref ref-type="disp-formula" rid="Ch1.E2"/>) is then used to
correct the MIPAS data

              <disp-formula id="Ch1.E4" content-type="numbered"><mml:math display="block"><mml:mrow><mml:msub><mml:mi>T</mml:mi><mml:mtext>MIPAS,corr</mml:mtext></mml:msub><mml:mo>(</mml:mo><mml:mi>t</mml:mi><mml:mo>)</mml:mo><mml:mo>=</mml:mo><mml:msub><mml:mi>T</mml:mi><mml:mtext>MIPAS</mml:mtext></mml:msub><mml:mo>(</mml:mo><mml:mi>t</mml:mi><mml:mo>)</mml:mo><mml:mo>+</mml:mo><mml:mi>f</mml:mi><mml:mo>(</mml:mo><mml:mi>t</mml:mi><mml:mo>)</mml:mo><mml:mo>,</mml:mo></mml:mrow></mml:math></disp-formula>

        and the model's uncertainty is used to recalculate the uncertainty
estimate of the corrected MIPAS data

              <disp-formula id="Ch1.E5" content-type="numbered"><mml:math display="block"><mml:mrow><mml:msub><mml:mi mathvariant="italic">σ</mml:mi><mml:mtext>MIPAS,corr</mml:mtext></mml:msub><mml:mo>(</mml:mo><mml:mi>t</mml:mi><mml:mo>)</mml:mo><mml:mo>=</mml:mo><mml:msqrt><mml:mrow><mml:msubsup><mml:mi mathvariant="italic">σ</mml:mi><mml:mtext>MIPAS</mml:mtext><mml:mn mathvariant="normal">2</mml:mn></mml:msubsup><mml:mo>(</mml:mo><mml:mi>t</mml:mi><mml:mo>)</mml:mo><mml:mo>+</mml:mo><mml:msubsup><mml:mi mathvariant="italic">σ</mml:mi><mml:mi>f</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msubsup><mml:mo>(</mml:mo><mml:mi>t</mml:mi><mml:mo>)</mml:mo></mml:mrow></mml:msqrt><mml:mo>,</mml:mo></mml:mrow></mml:math></disp-formula>

        where <inline-formula><mml:math display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="italic">σ</mml:mi><mml:mtext>MIPAS</mml:mtext></mml:msub></mml:mrow></mml:math></inline-formula> is the uncertainty on the MIPAS mean
temperatures. A new benchmark time series is created by merging the
original CHAMP time series with the corrected MIPAS time series by
calculating a weighted average

              <disp-formula id="Ch1.E6" content-type="numbered"><mml:math display="block"><mml:mrow><mml:msub><mml:mi>T</mml:mi><mml:mtext>merged</mml:mtext></mml:msub><mml:mo>=</mml:mo><mml:mfrac><mml:mrow><mml:msub><mml:mi>w</mml:mi><mml:mtext>CHAMP</mml:mtext></mml:msub><mml:mo>⋅</mml:mo><mml:msub><mml:mi>T</mml:mi><mml:mtext>CHAMP</mml:mtext></mml:msub><mml:mo>+</mml:mo><mml:msub><mml:mi>w</mml:mi><mml:mtext>MIPAS,corr</mml:mtext></mml:msub><mml:mo>⋅</mml:mo><mml:msub><mml:mi>T</mml:mi><mml:mtext>MIPAS,corr</mml:mtext></mml:msub></mml:mrow><mml:mrow><mml:msub><mml:mi>w</mml:mi><mml:mtext>CHAMP</mml:mtext></mml:msub><mml:mo>+</mml:mo><mml:msub><mml:mi>w</mml:mi><mml:mtext>MIPAS,corr</mml:mtext></mml:msub></mml:mrow></mml:mfrac><mml:mo>,</mml:mo></mml:mrow></mml:math></disp-formula>

        where the weights are given by <inline-formula><mml:math display="inline"><mml:mrow><mml:msub><mml:mi>w</mml:mi><mml:mi>x</mml:mi></mml:msub><mml:mo>=</mml:mo><mml:mn mathvariant="normal">1</mml:mn><mml:mo>/</mml:mo><mml:msubsup><mml:mi mathvariant="italic">σ</mml:mi><mml:mi>x</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msubsup></mml:mrow></mml:math></inline-formula>. The
uncertainty in the correction applied to the MIPAS monthly means is
incorporated into a new estimate of the uncertainty on the monthly
mean

              <disp-formula id="Ch1.E7" content-type="numbered"><mml:math display="block"><mml:mrow><mml:msub><mml:mi mathvariant="italic">σ</mml:mi><mml:mtext>merged</mml:mtext></mml:msub><mml:mo>=</mml:mo><mml:mfrac><mml:mn mathvariant="normal">1</mml:mn><mml:msqrt><mml:mrow><mml:msub><mml:mi>w</mml:mi><mml:mtext>CHAMP</mml:mtext></mml:msub><mml:mo>+</mml:mo><mml:msub><mml:mi>w</mml:mi><mml:mtext>MIPAS,corr</mml:mtext></mml:msub></mml:mrow></mml:msqrt></mml:mfrac></mml:mrow></mml:math></disp-formula>

        The process is then repeated using each remaining data set in the
order of decreasing temporal overlap with the iteratively revised
benchmark data set. For the example in Fig. <xref ref-type="fig" rid="App1.Ch1.F1"/>,
after merging MIPAS with CHAMP, this is found to be GRACE. Differences
between the GRACE monthly mean temperatures and those of the new
benchmark data set of CHAMP merged with corrected MIPAS are then used
as input to a new statistical model to derive corrections to be
applied to the GRACE monthly means. This process is repeated,
consecutively folding the MIPAS, GRACE, TSX, ACE-FTS and SMR into the
original CHAMP data to successively extend the CHAMP data set. The
order in which the data sets are merged can be different for each
latitude zone and pressure level depending on the availability of
data.</p>
      <p>The inclusion of each additional data set reduces the uncertainty on
the final product (as long as they are appropriately corrected).  The
monthly mean data from an instrument are excluded from this merging
process if there are fewer than 4 measurements in a particular month
or less than 5 % of measurements of the month with the highest
number of measurements within that year. The new VRT climate record
consists of such a temperature time series for every 5<inline-formula><mml:math display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula>
latitude zone and on the following 17 pressure levels: 300, 250, 200,
170, 150, 130, 115, 100, 90, 80, 70, 50, 30, 20, 15, 10, and 7 hPa.</p>
</sec>
<sec id="Ch1.S4">
  <title>Validation of the VRT climate record</title>
      <p>The merged temperature database described above was validated against
the following three independent data sets:
<list list-type="order"><list-item>
      <p>The radiosonde-based RATPAC-A <xref ref-type="bibr" rid="bib1.bibx12" id="paren.23"/> database.</p></list-item><list-item>
      <p>A COSMIC <xref ref-type="bibr" rid="bib1.bibx4" id="paren.24"/> RO zonal mean monthly mean
temperature data set.</p></list-item><list-item>
      <p>A NCEPCFSR <xref ref-type="bibr" rid="bib1.bibx23" id="paren.25"/> monthly mean zonal mean temperature data set.</p></list-item></list>
The comparison of the vertically integrated temperature data set
against the merged MSU4+AMSU9 data set (presented in
Sect. <xref ref-type="sec" rid="Ch1.S5"/>) also provides a partial validation of
the VRT data set.</p>
<sec id="Ch1.S4.SS1">
  <title>Validation against RATPAC-A</title>
      <p>The RATPAC-A data set provides annual anomalies on pressure levels and
is aggregated over seven large geographical regions, namely a global
data set, the Northern and Southern Hemispheres, the tropics
(30<inline-formula><mml:math display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> S to 30<inline-formula><mml:math display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> N) and extra-tropics, as well as
a narrower tropical zone from 20<inline-formula><mml:math display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> S to 20<inline-formula><mml:math display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> N.
Area-weighted annual means were calculated for those seven
geographical regions from our VRT database for comparison. Because
RATPAC-A data are only provided as anomalies, and because the period
over which the anomalies are calculated could not be ascertained from
the available RATPAC-A documentation (nor from e.g. D. Seidel,
personal communication, 2013), the
RATPAC-A anomalies were first subtracted from the VRT annual time
series at each pressure level and then the mean of the resultant time
series was subtracted. If the inter-annual variability in our merged
data set and RATPAC-A were identical, the resultant time series would
be uniformly zero, i. e. we compare the ability of the two databases
to track inter-annual variability in the temperature signals.</p>
      <p>Figure <xref ref-type="fig" rid="App1.Ch1.F2"/> shows the comparison of the inter-annual
variability for the Southern (a) and Northern (b) Hemispheres as
a function of pressure and time. At 250 hPa and at 300 hPa
differences in inter-annual variability can exceed 1 K while at lower
pressures, differences are generally less than <inline-formula><mml:math display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula>0.5 K.</p>
      <p>Differences in the inter-annual variability are smaller on all
pressure levels in the tropics (Fig. <xref ref-type="fig" rid="App1.Ch1.F2"/>c and d). In
extra-tropical regions (Fig. <xref ref-type="fig" rid="App1.Ch1.F2"/>e and f), the anomalies
are in general also small at all pressure levels, but can be as large
as <inline-formula><mml:math display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula>1.5 K at low pressure levels of 30 to 5 hPa in 2004/05 as
well as at 300 hPa in 2011. Similar comparisons are also available
for the whole globe (not shown here). The ability of the VRT data set
to track year-to-year variability over most of the upper troposphere
and stratosphere at the <inline-formula><mml:math display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula>0.5 K level indicates that this database
includes a valid representation of inter-annual variability in
temperatures over this region.</p>
</sec>
<sec id="Ch1.S4.SS2">
  <title>Validation against a COSMIC radio occultation data set</title>
      <p>The COSMIC RO data set used for this validation was created in the
same way as the other RO data sets used in the construction of the VRT
climate record described in Sect. <xref ref-type="sec" rid="Ch1.S2.SS3"/>.
The COSMIC RO data set was retained as a means of validating the VRT
data set, rather than being used in the construction of the data set.
Comparisons between the VRT and COSMIC RO data sets were made at all
17 pressure levels for which the databases are available. Examples of
comparisons at four different pressure levels are shown in
Fig. <xref ref-type="fig" rid="App1.Ch1.F3"/>.  In general, temperature differences are more
pronounced from 2009 onwards after the end of the CHAMP record that
was used as an initial benchmark. At 10 hPa the VRT values tend to be
up to 3 K lower than the COSMIC temperatures south of <inline-formula><mml:math display="inline"><mml:mrow><mml:mo>∼</mml:mo><mml:mn>20</mml:mn></mml:mrow></mml:math></inline-formula><inline-formula><mml:math display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> S and up to 3 K higher than the COSMIC temperatures
north of <inline-formula><mml:math display="inline"><mml:mrow><mml:mo>∼</mml:mo><mml:mn>20</mml:mn></mml:mrow></mml:math></inline-formula><inline-formula><mml:math display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> S.  At 100 hPa the differences are
smaller, typically within 1 K, with merged temperatures being lower
than COSMIC temperatures at higher latitudes and higher than COSMIC
temperatures at lower latitudes.</p>
      <p>The latitude zone over the tropics where merged temperatures are
higher than those of COSMIC diminishes in width with increasing
pressure and at around 200 hPa the pattern reverses, i. e. merged
temperatures in the extra-tropics are higher than COSMIC and lower in
the tropics (see Fig. <xref ref-type="fig" rid="App1.Ch1.F3"/>c and d).</p>
      <p>The temperature differences relative to the COSMIC data set are
typically of the order of 1 K at lower altitudes up to a pressure
level of 50 hPa, but can become relatively large, reaching about 4 K
at lower pressure levels of 7 hPa. There is also a distinct
difference apparent between the tropics and extra-tropics. At low
altitudes (up to 200 hPa) merged temperatures are typically lower in
the tropics and higher in the extra-tropics, but the opposite in sign
at higher altitudes (<inline-formula><mml:math display="inline"><mml:mrow><mml:mo>&lt;</mml:mo><mml:mn>200</mml:mn></mml:mrow></mml:math></inline-formula> hPa).</p>
</sec>
<sec id="Ch1.S4.SS3">
  <title>Validation against NCEPCFSR reanalyses</title>
      <p>NCEPCFSR reanalyses were linearly interpolated onto the log pressure
levels of the VRT data set and then area weighted monthly mean zonal
means were calculated for all pressure levels.</p>
      <p>Figure <xref ref-type="fig" rid="App1.Ch1.F4"/> shows differences in temperature between the
VRT and the NCEPCFSR data sets. The VRT data set can be up to 5 K
warmer than NCEPCFSR at 10 hPa with a larger bias in the Northern
Hemisphere than in the Southern Hemisphere. At 90 hPa, differences
over the tropics are close to zero but with a clear seasonal cycle.
These differences grow to 1.5–2 K over higher latitudes. At 250 hPa
the differences are generally between zero and 2 K. The left-hand
column of Fig. <xref ref-type="fig" rid="App1.Ch1.F4"/> shows the mean difference for each
latitude zone averaged over all months. A clear latitudinal bias can
be seen with temperature differences increasing from about 20<inline-formula><mml:math display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula>
out to the poles, and also larger temperature differences over the
equator with some seasonal variations over the tropics. There is no
discernible trend in the difference fields.</p>
      <p>As opposed to other months in the year, VRT temperatures in December
seem to be consistently lower than NCEPCFSR temperatures as indicated
by the vertical stripes in the right hand column of
Fig. <xref ref-type="fig" rid="App1.Ch1.F4"/>b and c.</p>
      <p>The results from these three validations suggest that the use of the
ESA/ESA-TPM data together with the RO temperature data in the
construction of the VRT data set results in a temperature time series
that, with sufficient extension, is likely to be suitable for analyses
of temperature trends in the upper troposphere and stratosphere.</p>
</sec>
</sec>
<sec id="Ch1.S5">
  <title>Validation of merged MSU4 and AMSU9 data sets</title>
      <p>One of the purposes of constructing the VRT data record was to assess
the quality of the merging of the MSU4 and AMSU9 temperature time
series in the lower stratosphere (the TLS product) by both the RSS and
UAH group. Of particular interest is whether the transition from the
period of overlap between MSU4 and AMSU9 (from 1998 to 2006) to
coverage by AMSU9 only after 2006 introduces any discontinuity in the
climate data record. A statistical model is used that accounts for any
systematic biases between the VRT time series and the MSU4+AMSU9 data
sets. The residuals are examined for any anomalies, in particular
a step function around the transition to the AMSU9 only measurements
around 2006.</p>
<sec id="Ch1.S5.SS1">
  <title>Merged MSU4 and AMSU9 temperature time series</title>
      <p>Microwave sounders retrieve vertical temperature profiles by measuring
the thermal emission from oxygen molecules at different frequencies.
The MSUs operating on a number of polar-orbiting NOAA satellites from
1978 to 2006 had four channels ranging from 50.3 to 57.95 GHz,
measuring the atmospheric temperature in four thick layers from the
surface through to the lower stratosphere. Reliable operation of the
MSU ceased in 2005, but there was already a significant number of
missing data beginning in 2004 <xref ref-type="bibr" rid="bib1.bibx18" id="paren.26"/>.</p>
      <p>A series of follow-on instruments, the AMSUs, began operation in 1998
using a larger number of channels that not only improved the vertical
resolution, but also extended measurements into the upper stratosphere
not covered by MSU channels. By using the AMSU channels most closely
matching the channels of the MSU instruments, MSU-based temperature
series were extended to the present.</p>
      <p>The temperature in the lower stratosphere (TLS) is measured by MSU
channel 4 and is closely matched by AMSU channel 9. The amalgamated
TLS product of MSU4+AMSU9 by RSS version 3.2 is described in
<xref ref-type="bibr" rid="bib1.bibx18" id="text.27"/>.  While the version 2.3 data set uses data only
from one AMSU instrument, NOAA-15, in our study the updated version
3.3 data set is used that includes data from AMSU instruments on Aqua,
NOAA-18, and METOP. Data from NOAA-16 are not used because of an
unexplained drift during its lifetime.</p>
      <p>Version 5.0 of the UAH data set contains AMSU data from both NOAA-15
and NOAA-16 <xref ref-type="bibr" rid="bib1.bibx11" id="paren.28"/>. Subsequent versions improve the
correction due to diurnal drift between the satellites
<xref ref-type="bibr" rid="bib1.bibx17 bib1.bibx10" id="paren.29"/>, convert AMSU data to mimic MSU, and add
additional AMSU measurements from AQUA, NOAA-18, NOAA-19, and
METOP. In our study, we use the UAH version 5.6.</p>
</sec>
<sec id="Ch1.S5.SS2">
  <title>Vertically weighted layer mean temperature series for comparison
with MSU4+AMSU9</title>
      <p>As the nadir-looking microwave sounders measure the temperature in
thick layers, our VRT time series needs to be integrated across the 17
pressure levels to obtain a single zonal mean monthly mean temperature
series (iVRT) comparable to the MSU4+AMSU9 data sets. Usually the
averaging kernel of the temperature retrieval is used for this purpose
<xref ref-type="bibr" rid="bib1.bibx22" id="paren.30"/>. In the case of the MSU and AMSU data products,
however, no profile retrieval involving any constrained generalized
inversion is performed, but the temperatures obtained from the
microwave channels are directly assigned to the altitude range to
which the particular channel is sensitive. Thus, the weighting
function of the related radiative transfer problem of this channel,
which describes which fraction of the measured signal originates from
which altitude, can be used directly in place of the averaging kernel.</p>
      <p>RSS provides text files of vertical weighting functions for the
different MSU channels on their ftp-server based on the US Standard
Atmosphere <xref ref-type="bibr" rid="bib1.bibx21" id="paren.31"/>. While the exact form of the weighting
function depends on the temperature, humidity, and liquid water
content of the atmospheric column, the representative weighting
function based on the mean state of the atmosphere for MSU4+AMSU9 is
given in the file.</p>
      <p>As this weighting function <inline-formula><mml:math display="inline"><mml:mrow><mml:mi mathvariant="italic">ω</mml:mi><mml:mo>(</mml:mo><mml:mi>p</mml:mi><mml:mo>)</mml:mo></mml:mrow></mml:math></inline-formula> is normalized to unity, the
weighted means of our temperature time series are given by

                <disp-formula id="Ch1.E8" content-type="numbered"><mml:math display="block"><mml:mrow><mml:msub><mml:mi>T</mml:mi><mml:mtext>weighted</mml:mtext></mml:msub><mml:mo>=</mml:mo><mml:mo movablelimits="false">∫</mml:mo><mml:mi mathvariant="italic">ω</mml:mi><mml:mo>(</mml:mo><mml:mi>ln⁡</mml:mi><mml:mo>(</mml:mo><mml:mi>p</mml:mi><mml:mo>)</mml:mo><mml:mo>)</mml:mo><mml:mo>⋅</mml:mo><mml:mi>T</mml:mi><mml:mo>(</mml:mo><mml:mi>ln⁡</mml:mi><mml:mo>(</mml:mo><mml:mi>p</mml:mi><mml:mo>)</mml:mo><mml:mo>)</mml:mo><mml:mspace width="0.125em" linebreak="nobreak"/><mml:mi mathvariant="normal">d</mml:mi><mml:mi>ln⁡</mml:mi><mml:mo>(</mml:mo><mml:mi>p</mml:mi><mml:mo>)</mml:mo><mml:mo>.</mml:mo></mml:mrow></mml:math></disp-formula>

          The uncertainty on the weighted mean is calculated as a weighted
average of the measurement uncertainties

                <disp-formula id="Ch1.E9" content-type="numbered"><mml:math display="block"><mml:mrow><mml:msub><mml:mi mathvariant="italic">σ</mml:mi><mml:mtext>weighted</mml:mtext></mml:msub><mml:mo>=</mml:mo><mml:mo movablelimits="false">∫</mml:mo><mml:mi mathvariant="italic">ω</mml:mi><mml:mo>(</mml:mo><mml:mi>ln⁡</mml:mi><mml:mo>(</mml:mo><mml:mi>p</mml:mi><mml:mo>)</mml:mo><mml:mo>)</mml:mo><mml:mo>⋅</mml:mo><mml:mi mathvariant="italic">σ</mml:mi><mml:mo>(</mml:mo><mml:mi>ln⁡</mml:mi><mml:mo>(</mml:mo><mml:mi>p</mml:mi><mml:mo>)</mml:mo><mml:mo>)</mml:mo><mml:mspace linebreak="nobreak" width="0.125em"/><mml:mi mathvariant="normal">d</mml:mi><mml:mi>ln⁡</mml:mi><mml:mo>(</mml:mo><mml:mi>p</mml:mi><mml:mo>)</mml:mo><mml:mo>.</mml:mo></mml:mrow></mml:math></disp-formula>

          Vertically integrated values are considered to be valid only if data
from all 17 pressure levels are available.</p>
      <p>Figure <xref ref-type="fig" rid="App1.Ch1.F5"/> illustrates the calculation of
the vertically integrated temperature for the latitude zone 35 to
40<inline-formula><mml:math display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> N in May 2002 as an example.</p>
</sec>
<sec id="Ch1.S5.SS3">
  <title>Break-point analysis of the merged MSU4 and AMSU9 data</title>
      <p>Vertically integrating our VRT data set creates a proxy for the merged
MSU4+AMSU9 temperature series. This proxy was then compared to the two
MSU4+AMSU9 data sets available from the RSS and UAH groups in each
5<inline-formula><mml:math display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> latitude zone (see Fig. <xref ref-type="fig" rid="App1.Ch1.F6"/> for an
example). Our primary interest is not the absolute difference between
our iVRT data set and the MSU4+AMSU9 data sets but rather whether
there are any discontinuities in the differences that might be
indicative of steps in the MSU4+AMSU9 data resulting from imperfect
merging of the source data. To this end a regression model consisting
of an offset term and linear trend term was fitted to the difference
time series (panel b of Fig. <xref ref-type="fig" rid="App1.Ch1.F6"/>). Both the
offset and linear trend fit coefficients were expanded in three
Fourier terms to account for seasonality. In this way the regression
model accounts for any systematic biases between the vertically
integrated database and the merged MSU4+AMSU9 databases. Any steps in
the residuals from those regression model fits would be indicative of
problems either with the merging of the MSU4 and AMSU9 time series or
with the construction of our iVRT data set.</p>
      <p>Since it was not possible to determine definitively when the switch
from using MSU to using AMSU data in the combined databases happened,
the Standard Normal Homogeneity Test (SNHT) <xref ref-type="bibr" rid="bib1.bibx2" id="paren.32"/>
was used to statistically test for any break-points in the residuals
from the start of 2005 to the end of 2007 in all 36 latitude zones.
Two variants of the SNHT were applied. In the first variant, the standard deviation (SD) of
the time series is assumed to be the same before and after a potential
break. Critical values from <xref ref-type="bibr" rid="bib1.bibx14" id="text.33"/> at a 95 % level of
significance were used (linearly interpolated to the exact number of
data points). In the second variant, the SDs within the two parts of
the series, before and after a possible break, were allowed to differ
from each other. For this test, critical values were taken from the
original <xref ref-type="bibr" rid="bib1.bibx2" id="text.34"/> publication.</p>
      <p>Assuming a constant SD, the SNHT did not detect any break-points in
either the RSS or UAH data sets. However, when the SD is allowed to
change after the break-point, the three latitude zones shown in
Fig. <xref ref-type="fig" rid="App1.Ch1.F7"/> exhibited a break-point in
the residuals for the UAH data set (indicated by the vertical dashed
lines).</p>
      <p>While there are no discernible steps in the residuals for any of the
three depicted zones, the SDs change after the break-point.  For the
zone from 60 to 65<inline-formula><mml:math display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> N, the SD appears to decrease
after the break-point in September 2006
(Fig. <xref ref-type="fig" rid="App1.Ch1.F7"/>b). However, the critical
value of 16.88 is only barely exceeded by the test value of 17.54 at
a 5 % level of significance (Table <xref ref-type="table" rid="App1.Ch1.T1"/>). In the
absence of break-points across a number of neighbouring latitude
zones, this break-point can be considered a statistical artefact.</p>
      <p>For the zones close to the poles
(Fig. <xref ref-type="fig" rid="App1.Ch1.F7"/>a and c), the SDs increase
considerably in 2005.  As the number of measurements close to the
poles is generally small, an increase in the variability does not
necessarily indicate an anomaly with the merging process. Unlike the
UAH database, the RSS merged data set does not report any monthly mean
temperatures for either polar zone. To establish whether the detected
increase in variability of the residuals comes from the UAH or iVRT
data set, the break-point analysis was repeated, but the iVRT data
were averaged by month over all years (i.e. the same climatology was
used for all years). Compared to this repeated climatology, the
residuals of the UAH data set showed no increase in variability in the
polar zones where break-points were detected previously indicating
that the change in the SDs observed in
Fig. <xref ref-type="fig" rid="App1.Ch1.F7"/>a and c are likely caused by
the iVRT data set.</p>
      <p>As there are no steps found in the residuals we can conclude that the
merged MSU4+AMSU9 temperature series of both the RSS and UAH group are
homogeneous in time and provide climate data records devoid of
discontinuities that are suitable for long-term trend detection. The
changes in the SDs of the residuals in the polar zones for the UAH
database are likely caused by an increase in variability in the iVRT
data set.</p>
</sec>
</sec>
<sec id="Ch1.S6" sec-type="conclusions">
  <title>Discussion and conclusions</title>
      <p>A new database of monthly mean zonal mean temperatures spanning the
upper troposphere and stratosphere was created by merging monthly mean
zonal mean temperature measurements from the mid-infrared
spectrometers ACE-FTS and MIPAS, the microwave sounder SMR, and the RO
experiments GRACE, CHAMP and TSX. The new temperature data record is
aggregated in 5<inline-formula><mml:math display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> latitudinal zones and is vertically resolved
on pressure levels from 300 to 7 hPa.</p>
      <p>Systematic biases between different instruments were corrected by
statistically modelling the differences allowing for an offset and
drift as well as temporal periodic fluctuations. The merging process
was initiated with the CHAMP temperature time series as RO
measurements are known to provide an effective climate benchmark. As
the merging algorithm mainly removes systematic biases relative to the
initial data set, it is crucial to choose this initial benchmark data
set carefully. The sensitivity to the initial benchmark data set was
tested by using the same merging algorithm, but starting the process
with MIPAS, GRACE and TSX, respectively, rather than
CHAMP. A comparison of these latter three temperature time series to
that initiated with CHAMP shows all resultant merged data sets being
in very good agreement.  The main differences between the different
data sets is an offset of similar magnitude to the offset seen in the
right hand column of Fig. <xref ref-type="fig" rid="App1.Ch1.F1"/>. The merged
temperature set starting with CHAMP typically lies somewhere in the
middle of the three comparative data sets. However, for some latitude
zones and pressure levels, especially in the Southern Hemisphere, the
other three temperature time series show a trend relative to the one
started with CHAMP. A trend in the differences is more problematic
because one intended use of our merged data set is to detect
relatively small warming or cooling trends in the atmosphere. This
trend is relatively small for TSX, but bigger for MIPAS and
GRACE. Nevertheless, the comparison shows that CHAMP remains the best
choice as an initial benchmark data set in the merging process.</p>
      <p>The merged VRT climate record was validated against three different
databases. The first validation was done against RATPAC-A which
provides annual mean temperature anomalies from radiosonde
measurements aggregated over seven large geographical regions. The
inter-annual variability in temperatures is well represented by our
VRT data set over most of the upper troposphere and stratosphere at
the <inline-formula><mml:math display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula>0.5 K level, but can exceed 1 K at the 250 and 300 hPa
levels. The comparison with the COSMIC RO database showed more
divergent results. Temperature differences were typically up to 1 K
at most pressure levels (<inline-formula><mml:math display="inline"><mml:mrow><mml:mo>≥</mml:mo><mml:mn>50</mml:mn></mml:mrow></mml:math></inline-formula> hPa), but could reach up to 4 K at
lower pressure levels. There were also clear spatial differences
between tropical and extra-tropical zones depending on altitude. The
temperatures from our VRT database were consistently lower in the
tropics than in the extra-tropics above 200 hPa, but this pattern
reversed below 200 hPa. The third validation was performed against
NCEPCFSR reanalyses. Differences were typically less than 2 K over
most pressure levels, but could reach 5 K at the highest altitudes
(<inline-formula><mml:math display="inline"><mml:mrow><mml:mo>≤</mml:mo><mml:mn>10</mml:mn></mml:mrow></mml:math></inline-formula> hPa). Seasonal variations, on the other hand, were more
pronounced than in the other two validations.</p>
      <p>As a major application, the VRT temperature record was used to verify
the quality of the merging process of the MSU4 and AMSU9 channels of
both the RSS and UAH groups. After removing systematic biases, the
residuals relative to our iVRT data set were examined for
statistically significant break-points. No statistically significant
steps were found in the residuals around the switch from MSU4 to
AMSU9, confirming that both groups made appropriate adjustments in the
merging process to assure a continuous temperature time series that is
not affected by calibration errors between the two types of
instruments or other systematic biases due to satellite drifts. Only
in the two polar 5<inline-formula><mml:math display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> latitude zones did our iVRT temperature
record show an increase in variability in 2005 relative to the UAH
temperature series.</p>
      <p>The VRT climate record can also be seen as a contribution to establish
long-term vertically resolved temperature records to enable updated
knowledge of long-term changes in temperatures across different
altitude ranges. To date, the microwave sounding measurements have
been a de-facto standard for temperature climate data records. With
the increased use of satellite infrared-sounders as well as highly
accurate RO measurements, more finely vertically-resolved data records
are available. Our VRT record is, to the best of our knowledge, the
first that merged temperature measurements from selected ESA/ESA-TPM
missions with RO measurements.  It has been shown that the uncertainty
on the monthly mean zonal mean temperatures decreases with an
increased number of instruments used in the merging. The VRT climate
record thus provides a useful data set for long-term temperature trend
analyses.</p>
</sec>

      
      </body>
    <back><ack><title>Acknowledgements</title><p>This work was funded in large part through the Support to Science
Element ESA (European Space Agency) SPARC (Stratosphere–troposphere
Processes And their Role in Climate) Initiative (ESA Contract No.
4000105291/12/I-NB) and we take this opportunity to acknowledge ESA
for this support. We acknowledge the individual instrument teams
(GRACE, CHAMP, TSX, ACE-FTS, MIPAS, and SMR) and the respective
space agencies for making their measurements available, and the ESA
SPARC Initiative (SPIN) for organizing and coordinating the
compilation of the monthly mean zonal mean temperature data sets
used in this work. ACE is a Canadian-led mission mainly supported by
the Canadian Space Agency (CSA). Development of the ACE-FTS
temperature climatology was supported by a grant from the
CSA. Special thanks go to  Bernd Funke and  Kaley Walker for
helpful comments on an early draft of this paper.  We also
acknowledge NOAA (National Oceanic and Atmospheric Administration)
for full and open data access to RATPAC temperature anomalies
through their National Climatic Data Center (NCDC). We would like to
thank  Torsten Schmidt from GeoForschungsZentrum (GFZ) Potsdam for
providing the COSMIC radio occultation data, and Chi-Fan Shih from
the National Center for Atmospheric Research in Boulder, CO, for
providing the NCEPCFSR reanalyses. Last but not least, we would like
to acknowledge  Joachim Urban, not only for his work on the SMR
data set used in this article, but also his general contribution to
the scientific community. Sadly, he passed away in August 2014.</p></ack><ref-list>
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  </ref-list><app-group content-type="float"><app><title/>

<table-wrap id="App1.Ch1.T1"><caption><p>Break-points detected in UAH database. The month shown in the table
is the last month before the break-point.</p></caption><oasis:table frame="topbot"><oasis:tgroup cols="4">
     <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:thead>
       <oasis:row rowsep="1">  
         <oasis:entry colname="col1">Zone</oasis:entry>  
         <oasis:entry colname="col2">Month</oasis:entry>  
         <oasis:entry colname="col3"><inline-formula><mml:math display="inline"><mml:mi>T</mml:mi></mml:math></inline-formula> value</oasis:entry>  
         <oasis:entry colname="col4">Crit. value</oasis:entry>
       </oasis:row>
     </oasis:thead>
     <oasis:tbody>
       <oasis:row>  
         <oasis:entry colname="col1">85–90<inline-formula><mml:math display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> S</oasis:entry>  
         <oasis:entry colname="col2">Apr 2005</oasis:entry>  
         <oasis:entry colname="col3">61.54</oasis:entry>  
         <oasis:entry colname="col4">16.88</oasis:entry>
       </oasis:row>
       <oasis:row>  
         <oasis:entry colname="col1">60–65<inline-formula><mml:math display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> N</oasis:entry>  
         <oasis:entry colname="col2">Sep 2006</oasis:entry>  
         <oasis:entry colname="col3">17.54</oasis:entry>  
         <oasis:entry colname="col4">16.88</oasis:entry>
       </oasis:row>
       <oasis:row>  
         <oasis:entry colname="col1">85–90<inline-formula><mml:math display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> N</oasis:entry>  
         <oasis:entry colname="col2">Sep 2005</oasis:entry>  
         <oasis:entry colname="col3">60.10</oasis:entry>  
         <oasis:entry colname="col4">16.88</oasis:entry>
       </oasis:row>
     </oasis:tbody>
   </oasis:tgroup></oasis:table></table-wrap>

      <?xmltex \floatpos{h}?><fig id="App1.Ch1.F1" position="anchor"><caption><p>An example of the generation of the VRT database, in this
case showing the time series at 100 hPa and between 50
and 55<inline-formula><mml:math display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> N.  The upper left panel shows the CHAMP monthly
means and their 1<inline-formula><mml:math display="inline"><mml:mi mathvariant="italic">σ</mml:mi></mml:math></inline-formula> uncertainties which form the initial
benchmark data set for the merging.  The second row of panels show
the uncorrected MIPAS monthly mean temperatures (green) in the
leftmost panel and their differences against the CHAMP data in the
rightmost panel. The regression model fit to these differences is
shown as a black line in the rightmost panel together with the
uncertainty on the regression model fit (grey shaded area). The
regression model fit is then used to correct the MIPAS data which
is then shown as the red line in the leftmost panel. The black line
and grey shaded region in the leftmost panel show what a merged
CHAMP and (corrected) MIPAS data set would look like. The remaining
data sets are then successively folded in as described in the
text. The final resultant data set is displayed as a black line and
grey shaded region in the bottom left panel.</p></caption>
      <?xmltex \igopts{width=199.169291pt}?><graphic xlink:href="https://amt.copernicus.org/preprints/8/235/2015/amtd-8-235-2015-f01.png"/>

    </fig>

      <fig id="App1.Ch1.F2"><caption><p>Differences between VRT anomalies and those from the
RATPAC-A database for <bold>(a)</bold> the Southern Hemisphere,
<bold>(b)</bold> the Northern Hemisphere, <bold>(c)</bold> the tropics from
30<inline-formula><mml:math display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> S to 30<inline-formula><mml:math display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> N, <bold>(d)</bold> the tropics from
20<inline-formula><mml:math display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> S to 20<inline-formula><mml:math display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> N, <bold>(e)</bold> the extra-tropics in
the Southern Hemisphere, and <bold>(f)</bold> the extra-tropics in the
Northern Hemisphere.</p></caption>
      <?xmltex \igopts{width=341.433071pt}?><graphic xlink:href="https://amt.copernicus.org/preprints/8/235/2015/amtd-8-235-2015-f02.png"/>

    </fig>

      <fig id="App1.Ch1.F3"><caption><p>Temperature differences between the COSMIC RO and the VRT
data sets at 10, 100, 150 and 200 hPa.</p></caption>
      <?xmltex \igopts{width=256.074803pt}?><graphic xlink:href="https://amt.copernicus.org/preprints/8/235/2015/amtd-8-235-2015-f03.png"/>

    </fig>

      <fig id="App1.Ch1.F4"><caption><p>Differences between monthly mean zonal mean (5<inline-formula><mml:math display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula>
zones) temperatures from the VRT data set and from the NCEPCFSR data
set.  Results are shown for three different pressure levels
viz. 10 hPa (upper panel), 90 hPa (middle panel) and 250 hPa
(lower panel).  The left hand column shows the mean differences for
each latitude zone averaged over all months.</p></caption>
      <?xmltex \igopts{width=256.074803pt}?><graphic xlink:href="https://amt.copernicus.org/preprints/8/235/2015/amtd-8-235-2015-f04.png"/>

    </fig>

      <?xmltex \floatpos{h}?><fig id="App1.Ch1.F5" position="anchor"><caption><p>Calculation of weighted temperature in latitude zone
35 to 40<inline-formula><mml:math display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> N in May 2002. <bold>(a)</bold>
Normalized weighting function of MSU4+AMSU9. <bold>(b)</bold>
Temperature profile. <bold>(c)</bold> Weighted temperature profile
<inline-formula><mml:math display="inline"><mml:mrow><mml:mi mathvariant="italic">ω</mml:mi><mml:mo>(</mml:mo><mml:mi>p</mml:mi><mml:mo>)</mml:mo><mml:mo>⋅</mml:mo><mml:mi>T</mml:mi><mml:mo>(</mml:mo><mml:mi>p</mml:mi><mml:mo>)</mml:mo></mml:mrow></mml:math></inline-formula> and the integrated temperature
<inline-formula><mml:math display="inline"><mml:mrow><mml:msub><mml:mi>T</mml:mi><mml:mtext>weighted</mml:mtext></mml:msub></mml:mrow></mml:math></inline-formula> in the shaded region.</p></caption>
      <?xmltex \igopts{width=284.527559pt}?><graphic xlink:href="https://amt.copernicus.org/preprints/8/235/2015/amtd-8-235-2015-f05.png"/>

    </fig>

      <fig id="App1.Ch1.F6"><caption><p>An example of the comparison of the weighted iVRT data set
and the two merged MSU4+AMSU9 data sets. <bold>(a)</bold> The original
raw monthly mean time series, <bold>(b)</bold> regression model fits
(lines) to the differences between the RSS and iVRT time series
(cyan dots and blue line showing the regression model fit) and
between the UAH and iVRT time series (orange dots and red line
showing the regression model fit), <bold>(c)</bold> the residuals from
the regression model fits shown in panel <bold>(b)</bold>.</p></caption>
      <?xmltex \igopts{width=341.433071pt}?><graphic xlink:href="https://amt.copernicus.org/preprints/8/235/2015/amtd-8-235-2015-f06.png"/>

    </fig>

      <fig id="App1.Ch1.F7"><caption><p>Latitudinal zones of the UAH merged MSU4 and AMSU9 database
with break-points in the residuals relative to the iVRT data
set. The residuals from the regression model for the zones from
<bold>(a)</bold> 85 to 90<inline-formula><mml:math display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> S, <bold>(b)</bold> 60
to 65<inline-formula><mml:math display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> N, and <bold>(c)</bold> 85 to 90<inline-formula><mml:math display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> N
are shown. The vertical dashed lines indicate where the SNHT
detected break-points.</p></caption>
      <?xmltex \igopts{width=284.527559pt}?><graphic xlink:href="https://amt.copernicus.org/preprints/8/235/2015/amtd-8-235-2015-f07.png"/>

    </fig>

    </app></app-group></back>
    </article>
