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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-19-5683-2026</article-id><title-group><article-title>CRUX-1.0: an automatic GHG and Ozone observation system for inland Antarctica Plateau</article-title><alt-title>CRUX-1.0: GHG and Ozone observations on Antarctic Plateau</alt-title>
      </title-group>
      <contrib-group>
        <contrib contrib-type="author" corresp="no" rid="aff1 aff2">
          <name><surname>Tian</surname><given-names>Biao</given-names></name>
          
        </contrib>
        <contrib contrib-type="author" corresp="yes" rid="aff1 aff6">
          <name><surname>Ding</surname><given-names>Minghu</given-names></name>
          <email>dingminghu@foxmail.com</email>
        <ext-link>https://orcid.org/0000-0002-1142-6598</ext-link></contrib>
        <contrib contrib-type="author" corresp="no" rid="aff1">
          <name><surname>Zhu</surname><given-names>Kongju</given-names></name>
          
        </contrib>
        <contrib contrib-type="author" corresp="no" rid="aff3">
          <name><surname>Yao</surname><given-names>Xu</given-names></name>
          
        </contrib>
        <contrib contrib-type="author" corresp="no" rid="aff1">
          <name><surname>Zhao</surname><given-names>Yixi</given-names></name>
          
        </contrib>
        <contrib contrib-type="author" corresp="no" rid="aff1">
          <name><surname>Zhang</surname><given-names>Wenqian</given-names></name>
          
        </contrib>
        <contrib contrib-type="author" corresp="no" rid="aff4">
          <name><surname>Yang</surname><given-names>Diyi</given-names></name>
          
        <ext-link>https://orcid.org/0000-0002-1844-5900</ext-link></contrib>
        <contrib contrib-type="author" corresp="no" rid="aff5">
          <name><surname>Sun</surname><given-names>Weijun</given-names></name>
          
        </contrib>
        <contrib contrib-type="author" corresp="no" rid="aff1">
          <name><surname>Yu</surname><given-names>Yining</given-names></name>
          
        <ext-link>https://orcid.org/0000-0002-9197-995X</ext-link></contrib>
        <contrib contrib-type="author" corresp="no" rid="aff1">
          <name><surname>Zhao</surname><given-names>Shoudong</given-names></name>
          
        </contrib>
        <contrib contrib-type="author" corresp="no" rid="aff1">
          <name><surname>Cui</surname><given-names>Yige</given-names></name>
          
        </contrib>
        <contrib contrib-type="author" corresp="no" rid="aff3">
          <name><surname>Li</surname><given-names>Chuanjin</given-names></name>
          
        </contrib>
        <contrib contrib-type="author" corresp="no" rid="aff1">
          <name><surname>Tang</surname><given-names>Jie</given-names></name>
          
        </contrib>
        <contrib contrib-type="author" corresp="no" rid="aff6">
          <name><surname>Xiao</surname><given-names>Cunde</given-names></name>
          
        </contrib>
        <contrib contrib-type="author" corresp="no" rid="aff7">
          <name><surname>Zhu</surname><given-names>Tong</given-names></name>
          
        <ext-link>https://orcid.org/0000-0002-2752-7924</ext-link></contrib>
        <contrib contrib-type="author" corresp="no" rid="aff6">
          <name><surname>Zhang</surname><given-names>Renhe</given-names></name>
          
        </contrib>
        <aff id="aff1"><label>1</label><institution>State Key Laboratory of Disaster Weather Science and Technology, Chinese Academy of Meteorological Sciences, Beijing 100081, China</institution>
        </aff>
        <aff id="aff2"><label>2</label><institution>School of Earth and Space Sciences, Peking University, Beijing 100871, China</institution>
        </aff>
        <aff id="aff3"><label>3</label><institution>Polar Research Institute of China, Shanghai 200136, China</institution>
        </aff>
        <aff id="aff4"><label>4</label><institution>Haining Meteorological Bureau, Haining 314400, China</institution>
        </aff>
        <aff id="aff5"><label>5</label><institution>College of Geography and Environment, Shandong Normal University, Jinan 250014, China</institution>
        </aff>
        <aff id="aff6"><label>6</label><institution>Key Laboratory of Polar Atmosphere-ocean-ice System for Weather and Climate, Ministry of Education, Shanghai 200438, China</institution>
        </aff>
        <aff id="aff7"><label>7</label><institution>College of Environmental Sciences and Engineering, Peking University, Beijing 100871, China</institution>
        </aff>
      </contrib-group>
      <author-notes><corresp id="corr1">Minghu Ding (dingminghu@foxmail.com)</corresp></author-notes><pub-date><day>7</day><month>September</month><year>2026</year></pub-date>
      
      <volume>19</volume>
      <issue>17</issue>
      <fpage>5683</fpage><lpage>5695</lpage>
      <history>
        <date date-type="received"><day>4</day><month>March</month><year>2026</year></date>
           <date date-type="rev-request"><day>11</day><month>March</month><year>2026</year></date>
           <date date-type="rev-recd"><day>12</day><month>August</month><year>2026</year></date>
           <date date-type="accepted"><day>21</day><month>August</month><year>2026</year></date>
      </history>
      <permissions>
        <copyright-statement>Copyright: © 2026 Biao Tian et al.</copyright-statement>
        <copyright-year>2026</copyright-year>
      <license license-type="open-access"><license-p>This work is licensed under the Creative Commons Attribution 4.0 International License. To view a copy of this licence, visit <ext-link ext-link-type="uri" xlink:href="https://creativecommons.org/licenses/by/4.0/">https://creativecommons.org/licenses/by/4.0/</ext-link></license-p></license></permissions><self-uri xlink:href="https://amt.copernicus.org/articles/19/5683/2026/amt-19-5683-2026.html">This article is available from https://amt.copernicus.org/articles/19/5683/2026/amt-19-5683-2026.html</self-uri><self-uri xlink:href="https://amt.copernicus.org/articles/19/5683/2026/amt-19-5683-2026.pdf">The full text article is available as a PDF file from https://amt.copernicus.org/articles/19/5683/2026/amt-19-5683-2026.pdf</self-uri>
      <abstract><title>Abstract</title>

      <p id="d2e265">Antarctic inland regions, as critical hubs for global climate change monitoring, suffer from a lack of reliable long-term greenhouse gas (GHG) observation systems due to extremely low temperatures, strong winds, and limited logistical/energy support. To address this gap, the CRUX-1.0 automatic observation system was developed and deployed at Taishan Station (inland Antarctic Plateau) during the 39th and 40th CHINARE (Chinese National Antarctic Research Expedition), targeting simultaneous monitoring of <inline-formula><mml:math id="M1" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> and surface ozone (<inline-formula><mml:math id="M2" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">O</mml:mi><mml:mn mathvariant="normal">3</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>). Integrating four core subsystems – analysis, calibration, temperature control, and data communication – the system is specifically engineered for harsh polar environments with low power consumption (<inline-formula><mml:math id="M3" display="inline"><mml:mrow><mml:mo>&lt;</mml:mo><mml:mn mathvariant="normal">350</mml:mn></mml:mrow></mml:math></inline-formula> W) and autonomous operation capability. The operational analysis based on a 1-month continuous field experiment showed its stable performance: <inline-formula><mml:math id="M4" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> measurements achieved a coefficient of variation (CV) <inline-formula><mml:math id="M5" display="inline"><mml:mrow><mml:mo>&lt;</mml:mo><mml:mn mathvariant="normal">5.6</mml:mn></mml:mrow></mml:math></inline-formula> % (nearing 0 % post-calibration), while <inline-formula><mml:math id="M6" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">O</mml:mi><mml:mn mathvariant="normal">3</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> measurements maintained a CV <inline-formula><mml:math id="M7" display="inline"><mml:mrow><mml:mo>&lt;</mml:mo><mml:mn mathvariant="normal">5.6</mml:mn></mml:mrow></mml:math></inline-formula> %. The average mixing ratios (<inline-formula><mml:math id="M8" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>: 420.7 <inline-formula><mml:math id="M9" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> 0.7 ppm; <inline-formula><mml:math id="M10" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">O</mml:mi><mml:mn mathvariant="normal">3</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>: 20.1 <inline-formula><mml:math id="M11" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> 0.8 ppb) closely aligned with regional background levels and South Pole Station data, confirming high reliability. As an unattended system with synchronous <inline-formula><mml:math id="M12" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub><mml:mo>/</mml:mo><mml:msub><mml:mi mathvariant="normal">O</mml:mi><mml:mn mathvariant="normal">3</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> measurement, low-power temperature control and automatic calibration, CRUX-1.0 shows good potential for long-term deployment in data-scarce polar inland regions.</p>
  </abstract>
    
<funding-group>
<award-group id="gs1">
<funding-source>National Natural Science Foundation of China</funding-source>
<award-id>42201151</award-id>
</award-group>
</funding-group>
</article-meta>
  </front>
<body>
      

<sec id="Ch1.S1" sec-type="intro">
  <label>1</label><title>Introduction</title>
      <p id="d2e407">Observing atmospheric composition and greenhouse gases is a critical global issue, as it serves as a key benchmark for assessing global changes and formulating policies such as the Paris Agreement and Conference of the Parties (COP) negotiations. Currently, global atmospheric background stations provide a significant amount of observational data, but their distribution remains uneven. In fact, there are notable disparities in greenhouse gas mixing ratios across different regions.For example, high-latitude and polar regions, including Antarctica, suffer from a lack of observation stations, making it difficult to monitor the atmospheric composition in these areas (Das et al., 2016; Liu et al., 2024). The absence of sufficient observation capacity in these regions highlights the need for enhanced monitoring systems. In particular, the challenging environmental conditions and logistical difficulties in these regions necessitate advancements in observation technologies and improved support for maintaining such systems. Given these challenges, there is a growing demand for increasing the capacity of remote, unattended observation systems to better capture the atmospheric background in these critical areas (Köne and Büke, 2010).</p>
      <p id="d2e410">Autonomous and unattended atmospheric observation technology has achieved initial applications across multiple global spheres. Its core technologies (low-power hardware, automated quality control, and remote data transmission) provide a feasible solution for long-term monitoring in remote/extreme regions.In the marine boundary layer, the autonomous ozone measurement system (equipped with PSI and 2B Technologies sensors) developed by the Woods Hole Oceanographic Institution has successfully operated for over one month in an unattended mode on Atlantic buoys and the Chesapeake Bay Lighthouse Tower, thanks to its waterproof packaging, automatic valve protection (to cope with high winds and sea fog), and fault self-correcting controller. Among them, the 2B sensor consumes less than 4 W of power, which is compatible with the energy constraints of marine platforms (Hintsa et al., 2004). In the atmospheric background monitoring at fixed terrestrial stations, the 300 m tall tower station in Bialystok, Poland, has implemented quasi-continuous observations of multiple species such as <inline-formula><mml:math id="M13" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>, <inline-formula><mml:math id="M14" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">O</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub><mml:mo>/</mml:mo><mml:msub><mml:mi mathvariant="normal">N</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>, and <inline-formula><mml:math id="M15" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CH</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> since 2005. By automatically calibrating the <inline-formula><mml:math id="M16" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub><mml:mo>/</mml:mo><mml:msub><mml:mi mathvariant="normal">O</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> sensors every 40 h, the gas chromatography module every 5 d, and conducting weekly flask sampling for quality control, the station has ensured data continuity for more than 3 years. Additionally, multi-height sampling has enabled effective differentiation between local and regional GHG signals (Popa et al., 2010). In the field of mobile observation, the MPAL vehicle-mounted monitoring platform of the University of Michigan achieves 6.5 h of continuous operation of all instruments relying on <inline-formula><mml:math id="M17" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">LiFeMnPO</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> battery packs. Through automatic PM sampling loss correction and weekly comparison with fixed stations, it completed 84 d of observations with over 260 000 1 s resolution data points in Detroit, verifying the spatiotemporal coverage advantages of mobile unattended platforms (Xia et al., 2023). Furthermore, the REA-FTIR flux system at the Shoalhaven Farm in Australia completed 3 weeks of unattended simultaneous flux observations of <inline-formula><mml:math id="M18" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>, <inline-formula><mml:math id="M19" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CH</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>, and <inline-formula><mml:math id="M20" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">N</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub><mml:mi mathvariant="normal">O</mml:mi></mml:mrow></mml:math></inline-formula> relying on 3G remote monitoring and automatic sampling bag switching, and also proposed an innovative method for estimating <inline-formula><mml:math id="M21" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">N</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub><mml:mi mathvariant="normal">O</mml:mi></mml:mrow></mml:math></inline-formula> background fluxes via <inline-formula><mml:math id="M22" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> tracer (Griffith et al., 2009).</p>
      <p id="d2e542">The observation of greenhouse gases and other atmospheric components in Antarctica presents significant challenges, particularly regarding conducting unattended monitoring. The extreme environmental conditions, including low temperatures, strong winds, and long periods of darkness, pose technical difficulties for maintaining continuous observation systems (Griffiths et al., 2020). Moreover, logistical support in such a remote region is limited, making it hard to deploy and maintain equipment effectively. Over the years, targeted efforts have been made to address these challenges, with some advances in equipment adaptation, energy management, and data reliability: <list list-type="custom"><list-item><label>1.</label>
      <p id="d2e547">British Antarctic Survey (BAS) Autonomous Ozone Network (2007–present). BAS deployed a network of 2B Technologies ozone monitors (ultraviolet photometry, 5 min sampling interval, 11–13 W power consumption) across 8 sites, from the southeastern coast of the Weddell Sea to the Antarctic Plateau (Bauguitte et al., 2011). The system relied on “solar-wind hybrid power + lead-acid batteries” (10–14 d of backup) and passive insulation with intake heating to avoid icing. It delivered 5 years of continuous data (2007–2012), with spring ozone mixing ratios averaging 28 <inline-formula><mml:math id="M23" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> 3 ppb along the coast (vs. 35 <inline-formula><mml:math id="M24" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> 2 ppb on the plateau) and a data continuity rate of 85 %. This work first confirmed that ozone depletion rates were higher at polar vortex edges (0.8 <inline-formula><mml:math id="M25" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">ppb</mml:mi><mml:mspace linebreak="nobreak" width="0.125em"/><mml:msup><mml:mi mathvariant="normal">d</mml:mi><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:mrow></mml:math></inline-formula>) than inland (0.3 <inline-formula><mml:math id="M26" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">ppb</mml:mi><mml:mspace linebreak="nobreak" width="0.125em"/><mml:msup><mml:mi mathvariant="normal">d</mml:mi><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:mrow></mml:math></inline-formula>). However, limitations emerged: passive insulation failed at <inline-formula><mml:math id="M27" display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">60</mml:mn></mml:mrow></mml:math></inline-formula> <inline-formula><mml:math id="M28" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">°</mml:mi><mml:mi mathvariant="normal">C</mml:mi></mml:mrow></mml:math></inline-formula> (causing 15 % winter data loss), wind turbine blade icing halted power supply for 12 consecutive days in 2009, and the lack of automatic calibration required manual on-site zero-checks, increasing operational costs (Bauguitte et al., 2011).</p></list-item><list-item><label>2.</label>
      <p id="d2e620">Chinese Kunlun Station (Dome A) Ozone Monitoring (2016). During the 2016 Chinese National Antarctic Research Expedition (CHINARE), Ding et al. (2020a) deployed a 2B Technologies Model 205 ozone monitor (10 min sampling interval, 5 W power consumption) at Dome A (80.25° S), leveraging the PLATO astronomical observatory module’s shared diesel generator and 50 kWh battery for power. The instrument operated continuously for 1 year, capturing the first annual ozone dataset for Antarctica’s highest-latitude inland region – with polar night mixing ratios averaging 32 <inline-formula><mml:math id="M29" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> 4 ppb and summer mixing ratios 29 <inline-formula><mml:math id="M30" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> 2 ppb (15 % lower than at Dome C). Data continuity reached 99.5 %, validating the Model 205’s suitability for extreme cold. Nevertheless, the system suffered from energy dependency (Ding et al., 2020a).</p></list-item><list-item><label>3.</label>
      <p id="d2e638">Terra Nova Bay Station Stratospheric <inline-formula><mml:math id="M31" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">NO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> Monitoring (2000). Bortoli and Kostadinov (2002) deployed a GASCOD UV-Visible spectrometer (423–460 nm wavelength, 0.5 nm resolution) at Terra Nova Bay Station for unattended <inline-formula><mml:math id="M32" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">NO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> observations. Key adaptations included a 30° inclined quartz window to reduce snow accumulation, 24 h continuous measurement (with integration time auto-adjusted from 2–5 s at noon to 5–10 min at twilight), and a built-in mercury lamp for daily grating calibration (spectral accuracy <inline-formula><mml:math id="M33" display="inline"><mml:mrow><mml:mo>&lt;</mml:mo><mml:mn mathvariant="normal">0.2</mml:mn></mml:mrow></mml:math></inline-formula> nm). Invalid data were screened via the “Flux Index (FI)” (values <inline-formula><mml:math id="M34" display="inline"><mml:mrow><mml:mo>&lt;</mml:mo><mml:mn mathvariant="normal">5</mml:mn><mml:mo>×</mml:mo><mml:msup><mml:mn mathvariant="normal">10</mml:mn><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">5</mml:mn></mml:mrow></mml:msup></mml:mrow></mml:math></inline-formula> <inline-formula><mml:math id="M35" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">mV</mml:mi><mml:mspace linebreak="nobreak" width="0.125em"/><mml:msup><mml:mi mathvariant="normal">ms</mml:mi><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:mrow></mml:math></inline-formula> rejected). The system yielded 1996 data showing <inline-formula><mml:math id="M36" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">NO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> slant column densities (sc) dropping from <inline-formula><mml:math id="M37" display="inline"><mml:mrow><mml:mn mathvariant="normal">1.2</mml:mn><mml:mo>×</mml:mo><mml:msup><mml:mn mathvariant="normal">10</mml:mn><mml:mn mathvariant="normal">17</mml:mn></mml:msup></mml:mrow></mml:math></inline-formula> to <inline-formula><mml:math id="M38" display="inline"><mml:mrow><mml:mn mathvariant="normal">4</mml:mn><mml:mo>×</mml:mo><mml:msup><mml:mn mathvariant="normal">10</mml:mn><mml:mn mathvariant="normal">16</mml:mn></mml:msup></mml:mrow></mml:math></inline-formula> <inline-formula><mml:math id="M39" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">molec</mml:mi><mml:mo>.</mml:mo><mml:mspace width="0.125em" linebreak="nobreak"/><mml:msup><mml:mi mathvariant="normal">cm</mml:mi><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">2</mml:mn></mml:mrow></mml:msup></mml:mrow></mml:math></inline-formula> in austral autumn and rebounding in spring – confirming coupling between photochemical loss and dynamic transport. It also quantified temperature-dependent errors: <inline-formula><mml:math id="M40" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">NO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> sc increased by 3.5 %–4 % for every 10 K rise in cross-section temperature. However, heavy snow in August 1996 covered the quartz window, causing a 7 d data gap, and mercury lamp intensity declined at <inline-formula><mml:math id="M41" display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">10</mml:mn></mml:mrow></mml:math></inline-formula> <inline-formula><mml:math id="M42" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">°</mml:mi><mml:mi mathvariant="normal">C</mml:mi></mml:mrow></mml:math></inline-formula>, leading to two failed calibrations.</p></list-item></list> The Antarctic inland plateau faces unique challenges including ultra-low temperatures (below <inline-formula><mml:math id="M43" display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">40</mml:mn></mml:mrow></mml:math></inline-formula> <inline-formula><mml:math id="M44" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">°</mml:mi><mml:mi mathvariant="normal">C</mml:mi></mml:mrow></mml:math></inline-formula>), polar night (over 3 months without effective illumination), and extremely low logistical accessibility. Existing global unattended monitoring schemes (such as solar-powered supply for marine platforms, mains-powered calibration for terrestrial tall towers, and 3G communication for farmland systems) cannot be directly adapted to this region. Therefore, developing a fully automated greenhouse gases and surface ozone observation system tailored to the Antarctic inland plateau, which fills the gap in unattended monitoring of the atmospheric background in the polar inland, is of crucial significance for understanding the polar feedback of the global climate system. Building on these experiences, a new system to monitor greenhouse gases and surface ozone was developed in 2022–2023 and deployed at the Antarctic inland Taishan Station. The preliminary system only operated for 3 d due to excessive power consumption: the temperature control module accounted for 70 % of the total power (peak 3 kW), which overloaded the power supply. The power allocation was 2.1 kW for temperature control and 0.9 kW for analysis/calibration/communication modules. As a result, an improved system named CRUX-1.0 (the name “CRUX” is inspired by constellation of Crux is one of the most prominent and easily recognizable constellations in the southern hemisphere sky) was developed with 350 W power limitation and tested at Tulihe, China, during cold season (<inline-formula><mml:math id="M45" display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">20</mml:mn></mml:mrow></mml:math></inline-formula> to <inline-formula><mml:math id="M46" display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">40</mml:mn></mml:mrow></mml:math></inline-formula> <inline-formula><mml:math id="M47" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">°</mml:mi><mml:mi mathvariant="normal">C</mml:mi></mml:mrow></mml:math></inline-formula>). Then in February 2024, it was deployed at Taishan Station on the Antarctic ice sheet. This system successfully operated for one month before the power supply broke down, providing valuable data on the atmospheric composition in this extreme environment. Here in this paper, we will introduce the detailed design of the system and its performance in Antarctica.</p>
</sec>
<sec id="Ch1.S2">
  <label>2</label><title>Site Descriptions</title>
      <p id="d2e863">Atmospheric <inline-formula><mml:math id="M48" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> and <inline-formula><mml:math id="M49" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">O</mml:mi><mml:mn mathvariant="normal">3</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> observational data in this study were obtained from one self-developed unattended monitoring system and four WMO-certified long-term monitoring stations with mature observation networks. The authoritative sources and verification channels for 2024 observational data are specified as follows: <inline-formula><mml:math id="M50" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> data were retrieved from the World Data Centre for Greenhouse Gases (WDCGG) of the World Meteorological Organization/Global Atmosphere Watch (WMO/GAW, <uri>https://gaw.kishou.go.jp/search/summary</uri>, last access: 14 December 2025), while surface ozone data were derived from the European Database for Atmospheric Sounding (EBAS, <uri>https://ebas-data.nilu.no/Pages/DataSetList.aspx</uri>, last access: 14 December 2025). All datasets were verified via the WMO/GAW quality control system to ensure cross-station consistency and comparability (Global Atmosphere Watch [GAW], 2001).</p>
<sec id="Ch1.S2.SS1">
  <label>2.1</label><title>Taishan Station</title>
      <p id="d2e912">Taishan Station (72.01° S, 92.08° E; 2621 m a.s.l.) is located on the Antarctic ice sheet (Fig. 1). It is situated on the high Antarctic Plateau, an area characterized by extreme environmental conditions. The station experiences strong katabatic winds and is positioned in a region with limited access to logistics and power resources, making it a challenging site for long-term atmospheric monitoring. The climate at Taishan Station is typical of the high Antarctic interior, where temperatures are consistently low throughout the year. The long-term data from September 2012 to July 2021 revealed an annual average air temperature of <inline-formula><mml:math id="M51" display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">35.4</mml:mn></mml:mrow></mml:math></inline-formula> <inline-formula><mml:math id="M52" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">°</mml:mi><mml:mi mathvariant="normal">C</mml:mi></mml:mrow></mml:math></inline-formula>, with a relative humidity of 67 %, an air pressure of 699 hPa, and an average wind speed of 10.9 <inline-formula><mml:math id="M53" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">m</mml:mi><mml:mspace width="0.125em" linebreak="nobreak"/><mml:msup><mml:mi mathvariant="normal">s</mml:mi><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:mrow></mml:math></inline-formula> (Ding et al., 2022). The temperature exhibits significant seasonal variation, with a clear “coreless” winter, meaning that there is no distinct temperature minimum, which is common in the interior of Antarctica due to the unique seasonal sunlight patterns (Fig. 2). Furthermore, temperature variability is much greater during the austral winter (2.46 <inline-formula><mml:math id="M54" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">°</mml:mi><mml:mi mathvariant="normal">C</mml:mi></mml:mrow></mml:math></inline-formula>) than during the austral summer (1.67 <inline-formula><mml:math id="M55" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">°</mml:mi><mml:mi mathvariant="normal">C</mml:mi></mml:mrow></mml:math></inline-formula>), reflecting the greater frequency of weather events and atmospheric disturbances during the colder months (Ding et al., 2020b, 2022).</p>

      <fig id="F1"><label>Figure 1</label><caption><p id="d2e974">Geographical distributions of Taishan station.</p></caption>
          <graphic xlink:href="https://amt.copernicus.org/articles/19/5683/2026/amt-19-5683-2026-f01.jpg"/>

        </fig>

      <fig id="F2" specific-use="star"><label>Figure 2</label><caption><p id="d2e985">Multiyear monthly average temperature <bold>(a)</bold>, relative humidity <bold>(b)</bold>, atmospheric pressure <bold>(c)</bold>, wind speed, and wind direction <bold>(d, e)</bold> at Taishan Station.</p></caption>
          <graphic xlink:href="https://amt.copernicus.org/articles/19/5683/2026/amt-19-5683-2026-f02.png"/>

        </fig>

      <p id="d2e1007">The CRUX-1.0 fully automated unattended observation system was deployed at Taishan Station from 10 February to 9 March 2024. This system has achieved simultaneous monitoring of <inline-formula><mml:math id="M56" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> and <inline-formula><mml:math id="M57" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">O</mml:mi><mml:mn mathvariant="normal">3</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> and obtained continuous observation data. Specifically, the CRUX-1.0 system is installed in a yellow observation cabin, which is located approximately 100 m to the southeast of the green-colored unattended generator cabin (Fig. 1). Given that easterly winds prevail at Taishan Station, the air inlet of the observation cabin is positioned on the upwind side of the generator cabin, which effectively minimizes the potential interference of the monitoring results from the exhaust emissions of the generator cabin. Detailed technical parameters and operational mechanisms of this system will be elaborated in Sect. 3.</p>
</sec>
<sec id="Ch1.S2.SS2">
  <label>2.2</label><title>Other Observation Stations</title>
      <p id="d2e1040">This study adopts four representative Global Atmosphere Watch (GAW) background stations covering polar, mid-latitude coastal and alpine regions for atmospheric comparative analysis. The Amundsen-Scott South Pole Station (SPO; 90° S, 24.8° W; 2837 m a.s.l.) is a NOAA-operated Antarctic background station, performing hourly in situ <inline-formula><mml:math id="M58" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> and <inline-formula><mml:math id="M59" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">O</mml:mi><mml:mn mathvariant="normal">3</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> observations with biweekly flask sampling and weekly NOAA-2016 scale calibration (Mahesh et al., 2003). It maintains a 98.8 % data continuity rate and provides benchmark Antarctic atmospheric background data (Prinn et al., 2018). Barrow Station (BRW; 71.32° N, 156.61° W; 11 m a.s.l.), a key NOAA GMCC Arctic coastal station, conducts hourly <inline-formula><mml:math id="M60" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> and <inline-formula><mml:math id="M61" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">O</mml:mi><mml:mn mathvariant="normal">3</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> monitoring and biweekly flask cross-validation. Influenced by North American emissions and Arctic atmospheric circulation, BRW captures both pristine Arctic background air masses and regional pollution episodes, with all data standardized to 10 min intervals via NOAA quality control protocols (Heintzenberg, 1989). The long-term NOAA-operated Mauna Loa Station (MLO; 19.54° N, 155.58° W; 3397 m a.s.l.), established in 1958, hosts the world’s longest continuous greenhouse gas observation records. It implements hourly WMO GAW-calibrated <inline-formula><mml:math id="M62" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> and <inline-formula><mml:math id="M63" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">O</mml:mi><mml:mn mathvariant="normal">3</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> monitoring and daily flask sampling, and its remote marine location minimizes anthropogenic interference to ensure reliable mid-latitude baseline observations (Keeling, 1976). As a high-altitude alpine background station under the ACTRIS network, Jungfraujoch Station (JFJ; 46.54° N, 7.96° E; 3580 m a.s.l.) monitors <inline-formula><mml:math id="M64" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> and <inline-formula><mml:math id="M65" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">O</mml:mi><mml:mn mathvariant="normal">3</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> at 6 min intervals, with weekly flask sampling and monthly systematic calibration, effectively reflecting mid-latitude European atmospheric trace gas variations. The station maintains a long-term data completeness of approximately 92 % under routine quality assurance (Sturm et al., 2012). Notably, systematic biases between NOAA and AGAGE datasets are less than 1 % for <inline-formula><mml:math id="M66" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> and 3 % for <inline-formula><mml:math id="M67" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">O</mml:mi><mml:mn mathvariant="normal">3</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>, which are sufficiently small to be negligible for regional and global comparative analyses (Prinn et al., 2018).</p>
</sec>
</sec>
<sec id="Ch1.S3">
  <label>3</label><title>Design of the observation system</title>
      <p id="d2e1163">The preliminary version of the unmanned automatic observation system, CRUX-1.0, is designed with 4 main modules: a sampling and calibration module, an analysis module, a temperature control module and a data communication module.</p>
<sec id="Ch1.S3.SS1">
  <label>3.1</label><title>Sampling and Calibration Module</title>
<sec id="Ch1.S3.SS1.SSS1">
  <label>3.1.1</label><title>Sampling</title>
      <p id="d2e1180">The sampling module is responsible for collecting atmospheric gas samples and ensuring their consistent flow into the analysis module for evaluation (see Fig. 3-I). It consists of several key components that work together to maintain a stable and reliable system. The intake port, positioned at a height of 2.9 m (see Fig. 3-IIa), ensures that the air samples are representative of the surrounding atmosphere and not influenced by local pollutants or snow. Furthermore, the inlet is installed with a Thermo-5030i pre-filter matched with a 47 mm-diameter, 5.0 <inline-formula><mml:math id="M68" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">µ</mml:mi><mml:mi mathvariant="normal">m</mml:mi></mml:mrow></mml:math></inline-formula> MILLIPORE PTFE membrane filter. This filter can efficiently block blown snow particles and coarse dust, effectively avoiding pipeline clogging induced by frequent blowing snow in Antarctica and enhancing the environmental suitability of the sampling setup. This elevated position and filter are crucial for ensuring that the collected data are as accurate as possible.</p>

      <fig id="F3" specific-use="star"><label>Figure 3</label><caption><p id="d2e1195">Functional and structural layout (I) and onsite installation and layout (II) of the unmanned automated <inline-formula><mml:math id="M69" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> and surface ozone observation system at Taishan Station.</p></caption>
            <graphic xlink:href="https://amt.copernicus.org/articles/19/5683/2026/amt-19-5683-2026-f03.jpg"/>

          </fig>

      <p id="d2e1215">The gas flow controller, which includes a vacuum pump (Kamoer KZP-PE model: low rate <inline-formula><mml:math id="M70" display="inline"><mml:mo>≥</mml:mo></mml:math></inline-formula> 7 <inline-formula><mml:math id="M71" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">L</mml:mi><mml:mspace width="0.125em" linebreak="nobreak"/><mml:msup><mml:mi mathvariant="normal">min</mml:mi><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:mrow></mml:math></inline-formula>; power <inline-formula><mml:math id="M72" display="inline"><mml:mo>≤</mml:mo></mml:math></inline-formula> 12 W; positive pressure <inline-formula><mml:math id="M73" display="inline"><mml:mo>≥</mml:mo></mml:math></inline-formula> 0.2 MPa), standard gas cylinder pressure-reducing valve, and flow controller, ensures that the gas is drawn into the system at a constant rate (see Fig. 3-IIb and c). The vacuum pump helps maintain a positive pressure airflow, whereas the flow controller regulates the gas flow for consistent sampling. Additionally, the system incorporates three-way and electromagnetic valves to allow the sampling system to switch between different sampling points or introduce calibration gases as needed. The overall design of the sampling module considers the dominant wind direction at Taishan Station, with the intake positioned in the upwind direction of the energy bin to minimize contamination from emissions. This thoughtful design ensures that the sampling module operates efficiently, even in harsh Antarctic environments.</p>
</sec>
<sec id="Ch1.S3.SS1.SSS2">
  <label>3.1.2</label><title>Calibration</title>
      <p id="d2e1264">The calibration module is designed to eliminate instrument drift through standard gas calibration, ensuring the accuracy and stability of the observation data. The standard gas cylinder pressure-reducing valve controls the output pressure of the standard air, with the secondary gauge set to 2 psi. This setting ensures that the instrument's intake pressure is met while conserving the standard air as much as possible, thereby extending its usage duration. Each standard gas cylinder is certified for high precision and traceability and is equipped with a single-stage pressure-reducing valve. The cylinders are connected to the electromagnetic valve via <inline-formula><mml:math id="M74" display="inline"><mml:mrow><mml:mn mathvariant="normal">1</mml:mn><mml:mo>/</mml:mo><mml:mn mathvariant="normal">8</mml:mn></mml:mrow></mml:math></inline-formula> in. stainless steel tubing, ensuring the stability of the gas mixing ratios during transmission.</p>
      <p id="d2e1279">The electromagnetic valve is powered and controlled by the CR1000 data logger, which operates the valve at scheduled intervals through a prewritten control program. This program switches between external air and standard air intake, ensuring a consistent and controlled flow. To maintain a constant airflow through the instrument, a flow controller is installed downstream of the electromagnetic valve, preset to a constant flow rate. This ensures precise control over the gas flow entering the monitoring sensors, improving the accuracy of the measurements.</p>
      <p id="d2e1282">To prevent instrument drift from affecting the observation data, the system incorporates a standard gas calibration system, following the atmospheric background observation guidelines. The data logger sends instructions to the electromagnetic valve to allow standard air to flow into the system twice daily – every 11 h and 10 min for a 10 min period. This calibration process ensures that the sensor is calibrated and that any drift is corrected while considering the limitations of energy consumption and the unmanned operating conditions at Taishan Station.</p>
</sec>
</sec>
<sec id="Ch1.S3.SS2">
  <label>3.2</label><title>Analysis Module</title>
<sec id="Ch1.S3.SS2.SSS1">
  <label>3.2.1</label><title><inline-formula><mml:math id="M75" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> Monitor</title>
      <p id="d2e1312">To meet the energy consumption requirements at Taishan Station (where the atmospheric composition monitoring system needs to maintain a power consumption of less than 0.5 kW), a low-power LICOR-830 <inline-formula><mml:math id="M76" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> analyzer (see Fig. 3-IIc) is used in this experimental system. This device operates via the nondispersive infrared (NDIR) method, which consumes approximately 20 W of power. The NDIR method is considered one of the simplest yet effective technologies for gas detection because of its moderate sensitivity and fast response time. The LICOR-830 is widely used in various research fields, including agronomy, ecology, global carbon cycling, and climate change studies (Griffiths, 1983; Ekeberg et al., 2004; Chen et al., 2010).</p>
      <p id="d2e1326">The core components of the analyzer include an infrared light source, a light chamber, filters, and a detector. The working principle is as follows: infrared radiation emitted by the light source passes through the target gas in the light chamber. If the spectrum of the radiation overlaps with the absorption spectrum of the target gas, the gas absorbs photons at specific wavelengths according to the Beer–Lambert law (Kwon et al., 2009). After passing through the gas, the infrared radiation is filtered so that only the wavelengths absorbed by the gas are retained. These specific photons, which contain mixing ratio information, are detected by the sensor, and the signal is processed to display the mixing ratio of the greenhouse gas (Xu et al., 2022).</p>
      <p id="d2e1329">Prior to deployment at Taishan Station, a preexpedition laboratory experiment was conducted to quantify the precision differences between the LICOR-830 and the Picarro G2301 greenhouse gas analyzers. This experiment aimed to assess the performance of observation systems based on different principles for measuring greenhouse gases (Nan et al., 2024). Through repeatability tests, drift tests, and target gas calibration tests, it was found that the accuracy of the LICOR-830, after calibration, met the WMO requirement of less than 0.1 ppm and was comparable to the advanced international accuracy level of the Picarro G2301, demonstrating its significant application potential in greenhouse gas monitoring.</p>
</sec>
<sec id="Ch1.S3.SS2.SSS2">
  <label>3.2.2</label><title>Ozone Monitor</title>
      <p id="d2e1340">For ozone monitoring, a Model 205 ozone monitor from 2B Technologies (see Fig. 3-IIc) was used in this experiment. This model was previously deployed in a year-long ground-based ozone observation experiment at Kunlun Station in Antarctica in 2016, where it successfully collected comprehensive observational data (Ding et al., 2022). Model 205 has demonstrated excellent applicability in ozone mixing ratio monitoring, both domestically and internationally. It is energy efficient, highly accurate, compact, and lightweight, making it an ideal tool for monitoring atmospheric ozone mixing ratios in outdoor or field environments (Ollison et al., 2013; DiGangi et al., 2018; Tian et al., 2022).</p>
      <p id="d2e1343">The Model 205 ozone monitor operates via ultraviolet photometry (Williams et al., 2006). The ozone mixing ratio was measured by detecting its maximum absorption at a UV wavelength of 253.7 nm. When an air sample enters the instrument's gas flow system at a constant flow rate, two electromagnetic valves alternate in directing the sample either into the absorption chamber or through an ozone filter before entering the absorption chamber. The absorption chamber concentrates stable UV light produced by the UV light source. Owing to the absorption characteristics of ozone at 254 nm, the intensity of transmitted light as the gas passes through the chamber is detected, providing accurate and stable measurements of the ozone mixing ratio. Instruments based on this method are widely used in pollution monitoring, including atmospheric and water pollution (Tanimoto et al., 2006).</p>
      <p id="d2e1346">Calibration of the ozone monitor requires an ozone calibration instrument that meets international traceability standards. Therefore, cross-mixing ratio calibrations are performed every three months according to observation protocols. However, the calibration procedures for Antarctic ice sheet instruments differ from those at manned stations. For instance, in 2011, after the BAS team retrieved all instruments from the observation network to Halley Station, they validated them using the newly calibrated TE-Model 49C. Upon returning to Cambridge, the instruments were re-calibrated using the NPL-certified TE-Model 49iPS, confirming that the calibration parameters of the 10 instruments remained stable throughout the year's deployment, with data deviations not exceeding the initial accuracy range of 2 % (Bauguitte et al., 2011). In 2016, testing at Antarctic Dome A confirmed the stable operation of the instrument in the field, and reliable observations can be obtained by conducting calibrations twice per year (Ding et al., 2020a). Owing to the overall energy consumption limitations and unattended conditions at Taishan Station, we conducted calibrations before deployment and after retrieval. This strategy is sufficient for the 1-month experiment, because the 2B Model 205 monitor features ultra-low intrinsic drift (<inline-formula><mml:math id="M77" display="inline"><mml:mrow><mml:mo>&lt;</mml:mo><mml:mn mathvariant="normal">3</mml:mn></mml:mrow></mml:math></inline-formula> <inline-formula><mml:math id="M78" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">ppb</mml:mi><mml:mspace width="0.125em" linebreak="nobreak"/><mml:msup><mml:mi mathvariant="normal">yr</mml:mi><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:mrow></mml:math></inline-formula> for baseline drift, <inline-formula><mml:math id="M79" display="inline"><mml:mrow><mml:mo>&lt;</mml:mo><mml:mn mathvariant="normal">3</mml:mn></mml:mrow></mml:math></inline-formula> % <inline-formula><mml:math id="M80" display="inline"><mml:mrow class="unit"><mml:msup><mml:mi mathvariant="normal">yr</mml:mi><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:mrow></mml:math></inline-formula> for sensitivity drift). The drift over one month was verified to be <inline-formula><mml:math id="M81" display="inline"><mml:mrow><mml:mo>&lt;</mml:mo><mml:mn mathvariant="normal">2</mml:mn></mml:mrow></mml:math></inline-formula> % in laboratory tests and Antarctic field applications (Wang et al., 2017), meeting the WMO/GAW accuracy requirement.</p>
</sec>
</sec>
<sec id="Ch1.S3.SS3">
  <label>3.3</label><title>Temperature Control Module</title>
      <p id="d2e1419">The temperature control module is designed to ensure the stable operation of the monitoring equipment under extreme Antarctic conditions, especially the freezing temperatures at Taishan Station. This module includes a temperature control cabinet, a gas flow controller, and an uninterruptible power supply (UPS) (see Fig. 3-IIb-➃, ➄). The temperature control cabinet is equipped with precise sensors and adjustment mechanisms that maintain a stable internal temperature range for the equipment, protecting it from extreme cold at the station.</p>
      <p id="d2e1422">To meet the appropriate temperature range for the operation of <inline-formula><mml:math id="M82" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> and ozone monitoring while reducing the energy consumption of temperature control, the temperature control accuracy is <inline-formula><mml:math id="M83" display="inline"><mml:mrow><mml:mo>±</mml:mo><mml:mn mathvariant="normal">1.0</mml:mn></mml:mrow></mml:math></inline-formula> <inline-formula><mml:math id="M84" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">°</mml:mi><mml:mi mathvariant="normal">C</mml:mi></mml:mrow></mml:math></inline-formula>, and the heating response time is 5 min, and the minimum heating temperature of the temperature control cabinet is preset to 10 <inline-formula><mml:math id="M85" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">°</mml:mi><mml:mi mathvariant="normal">C</mml:mi></mml:mrow></mml:math></inline-formula>. When the internal temperature drops below 10 <inline-formula><mml:math id="M86" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">°</mml:mi><mml:mi mathvariant="normal">C</mml:mi></mml:mrow></mml:math></inline-formula>, the system begins to heat; when the temperature exceeds 15 <inline-formula><mml:math id="M87" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">°</mml:mi><mml:mi mathvariant="normal">C</mml:mi></mml:mrow></mml:math></inline-formula>, heating stops, ensuring that the equipment remains within a safe and optimal operating temperature range. This design ensures that the monitoring instruments are effectively protected in the extremely low-temperature environment of Taishan Station (which can reach as low as <inline-formula><mml:math id="M88" display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">40</mml:mn></mml:mrow></mml:math></inline-formula> <inline-formula><mml:math id="M89" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">°</mml:mi><mml:mi mathvariant="normal">C</mml:mi></mml:mrow></mml:math></inline-formula>). The environmental monitoring and control system, which includes temperature regulation, is the highest power-consuming component in the entire system, with a peak power consumption of 250 W. Given the power constraints at Taishan Station, energy efficiency is a crucial consideration in the design of the temperature control system. This is balanced with the need to maintain a stable environment for the equipment.</p>
      <p id="d2e1507">Since the experimental system is powered by Taishan Station's external energy cabin, an uninterruptible power supply (UPS) system is installed to prevent sudden power outages or voltage instability from negatively impacting the system's operation (Fig. 3-IId). The UPS provides stable and reliable power to the entire monitoring system (see Fig. 3-IId). In the event of an external power failure, the UPS can quickly switch to backup power. The battery backup can last up to 48 h, ensuring the continuous operation of the monitoring system and uninterrupted data collection. This design significantly enhances the system's reliability and fault tolerance, providing a safeguard against power disruptions in the remote environment.</p>
</sec>
<sec id="Ch1.S3.SS4">
  <label>3.4</label><title>Data Communication Module</title>
      <p id="d2e1519">The satellite communication system consists of a customized bracket (with a height of 3 m) and an integrated transmitting antenna (Fig. 3-IIa-➀), enabling high-speed and stable data transmission to a remote data center. This module uses ARGOS (full system: Argos Data Collection System, named after the all-seeing giant Argus from Greek mythology) satellite communication technology, with a data transmission interval of 1 h, ensuring the real-time transmission of monitored data processed by the data logger in the harsh Antarctic environment, which can avoid potential interruptions and delays that could arise with traditional ground communication methods. The stable applicability of this satellite communication module in Antarctica has been verified through testing at the Prydz Bay-Amery Ice Shelf-Dome A (PANDA) profile automatic weather station (Ding et al., 2022).</p>
      <p id="d2e1522">The data processing and storage system uses the CR1000X measurement and control data logger (see Fig. 3-IIc), a low-power device primarily used for sensor measurements, direct/remote communication connections, data analysis, external device control, and storage of data and programs. It features a sealed design to shield against radio frequency interference and a stainless steel housing. Equipped with a precise clock, it supports the BASIC-like programming language commonly used by Campbell Scientific data loggers, which includes data processing and analysis capabilities.</p>
      <p id="d2e1525">The CR1000X connection panel has two 12 V terminals, 16 analog measurement terminals, and detachable connectors. It is responsible for receiving raw data from two monitoring sensors, performing preprocessing, analysis, and storage. This module has powerful data processing capabilities, enabling it to filter out and correct anomalous data points in real time, ensuring the reliability of the data quality. Additionally, the module supports remote data access and download functions, allowing researchers to retrieve and analyze monitoring data at any time.</p>
</sec>
</sec>
<sec id="Ch1.S4">
  <label>4</label><title>Experimental analysis</title>
<sec id="Ch1.S4.SS1">
  <label>4.1</label><title>Observational results</title>
      <p id="d2e1544">From 10 February to 12 March 2024, the observation system at Taishan Station operated autonomously under unattended low-temperature conditions, with good performance, and satellite remote data transmission was normal. By analyzing the transmitted data, we found the following: in the environment at Taishan Station, where the average temperature was below <inline-formula><mml:math id="M90" display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">25</mml:mn></mml:mrow></mml:math></inline-formula> <inline-formula><mml:math id="M91" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">°</mml:mi><mml:mi mathvariant="normal">C</mml:mi></mml:mrow></mml:math></inline-formula> in February, the internal temperature of the equipment cabinet was able to be stably maintained at 13.9 <inline-formula><mml:math id="M92" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> 2.5 <inline-formula><mml:math id="M93" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">°</mml:mi><mml:mi mathvariant="normal">C</mml:mi></mml:mrow></mml:math></inline-formula> (Fig. 4a), meeting the environmental temperature requirements for both types of optical cavity equipment used in this experiment.</p>

      <fig id="F4"><label>Figure 4</label><caption><p id="d2e1586">Compares synchronous in-cabinet temperature (black, left axis) and outdoor ambient temperature (pink, right axis) <bold>(a)</bold>, hourly average mixing ratio of observed <inline-formula><mml:math id="M94" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>, hourly average mixing ratio of calibrated <inline-formula><mml:math id="M95" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> and <inline-formula><mml:math id="M96" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">O</mml:mi><mml:mn mathvariant="normal">3</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> mixing ratio transmitted from the unattended automated observation system at Taishan Station <bold>(b)</bold>.</p></caption>
          <graphic xlink:href="https://amt.copernicus.org/articles/19/5683/2026/amt-19-5683-2026-f04.png"/>

        </fig>

      <p id="d2e1634">The hourly average <inline-formula><mml:math id="M97" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> mixing ratio observed at Taishan Station was 422.6 <inline-formula><mml:math id="M98" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> 2.8 ppm (Fig. 4b). To ensure the accuracy of observational data, we first analyzed concurrent meteorological parameters including wind speed and wind direction, and verified that generator exhaust exerted no direct interference on the monitoring data (Fig. S1 in the Supplement). To constrain instrumental drift under unattended field conditions, the system executes an automatic 10 min standard gas calibration every 11 h; this customized calibration interval comprehensively balances drift correction efficiency, limited on-site power supply and automatic operation requirements. All <inline-formula><mml:math id="M99" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> raw datasets underwent standardized multi-step QA/QC procedures sequentially: exhaust interference exclusion based on sampling layout and field wind rose statistics, wind-speed-dependent pollution screening, quantitative mixing ratio calibration, and final 48 h moving average smoothing for noise reduction. The daily-averaged calibrated <inline-formula><mml:math id="M100" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> mixing ratio was determined as 420.7 <inline-formula><mml:math id="M101" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> 0.7 ppm. The ozone raw datasets were calibrated using the five-point cross-mixing ratio formula (<inline-formula><mml:math id="M102" display="inline"><mml:mrow><mml:mi>y</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">0.994</mml:mn><mml:mo>⋅</mml:mo><mml:mi>x</mml:mi><mml:mo>-</mml:mo><mml:mn mathvariant="normal">0.495</mml:mn></mml:mrow></mml:math></inline-formula>, <inline-formula><mml:math id="M103" display="inline"><mml:mrow><mml:msup><mml:mi>R</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msup><mml:mo>=</mml:mo><mml:mn mathvariant="normal">0.9998</mml:mn></mml:mrow></mml:math></inline-formula>). This calibration function was established in laboratory before instrument shipment via systematic calibration on the Model 205 ozone analyzer with a Thermo 49ips standard ozone calibrator. Upon completion of the QA/QC procedures, the daily-averaged calibrated surface ozone mixing ratio at Taishan Station was 20.1 <inline-formula><mml:math id="M104" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> 0.8 ppb. Full technical details of each QA/QC step are provided in the Supplement.</p>
</sec>
<sec id="Ch1.S4.SS2">
  <label>4.2</label><title>Accuracy evaluation</title>
      <p id="d2e1735">We evaluated system performance using WMO/GAW required indicators: <inline-formula><mml:math id="M105" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> (zero drift <inline-formula><mml:math id="M106" display="inline"><mml:mrow><mml:mo>≤</mml:mo><mml:mn mathvariant="normal">0.1</mml:mn></mml:mrow></mml:math></inline-formula> ppm per month, span drift <inline-formula><mml:math id="M107" display="inline"><mml:mrow><mml:mo>≤</mml:mo><mml:mn mathvariant="normal">0.2</mml:mn></mml:mrow></mml:math></inline-formula> % FS, accuracy <inline-formula><mml:math id="M108" display="inline"><mml:mrow><mml:mo>±</mml:mo><mml:mn mathvariant="normal">1.5</mml:mn></mml:mrow></mml:math></inline-formula> ppm); <inline-formula><mml:math id="M109" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">O</mml:mi><mml:mn mathvariant="normal">3</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> (zero drift <inline-formula><mml:math id="M110" display="inline"><mml:mrow><mml:mo>≤</mml:mo><mml:mn mathvariant="normal">0.5</mml:mn></mml:mrow></mml:math></inline-formula> ppb per month, span drift <inline-formula><mml:math id="M111" display="inline"><mml:mrow><mml:mo>≤</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:math></inline-formula> % FS, accuracy <inline-formula><mml:math id="M112" display="inline"><mml:mrow><mml:mo>±</mml:mo><mml:mn mathvariant="normal">0.8</mml:mn></mml:mrow></mml:math></inline-formula> ppb), plus standard deviation and coefficient of variation (CV) (Global Atmosphere Watch [GAW], 2001). The standard deviation provides insight into the dispersion of measurement data, reflecting the precision and stability of the system. On the other hand, CV, which normalizes the standard deviation by the mean value, allows for a comparison of variability across different parameters and conditions, regardless of their magnitude. Using these two metrics, we evaluated the precision of <inline-formula><mml:math id="M113" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">O</mml:mi><mml:mn mathvariant="normal">3</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> and <inline-formula><mml:math id="M114" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> mixing ratios, as well as the cabinet temperature, over time.</p>
      <p id="d2e1843">Prior to the Antarctic field campaign, we had been completed laboratory performance intercomparison between the LICOR-830 analyzer used in this work and Picarro G2301 by means of repeatability, long-term drift and three-point cross-mixing ratio calibration with traceable <inline-formula><mml:math id="M115" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> standard gases, with related test plots (Figs. S2–S5) attached in the Supplement. The test results indicated that LICOR-830 had a repeatability of 0.4 ppm versus 0.04 ppm for Picarro G2301, alongside drift biases of <inline-formula><mml:math id="M116" display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">4.22</mml:mn></mml:mrow></mml:math></inline-formula> % and 0.82 % respectively; after three-mixing ratio standard gas calibration for 1 h, LICOR-830’s precision was markedly optimized to 0.026 ppm (bias: <inline-formula><mml:math id="M117" display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">0.11</mml:mn></mml:mrow></mml:math></inline-formula> %), while Picarro G2301’s precision changed slightly to 0.0341 ppm with an accuracy of 0.03 %.</p>
      <p id="d2e1877">In addition, for the ozone measurement module equipped with a 2B Model 205 dual-beam UV analyzer, multi-point calibration conducted before and after field deployment meets the data quality requirement for 1-year Antarctic observation (Bauguitte et al., 2011; Ding et al., 2020a). The laboratory comparison test (Fig. S6) between Model 205 and WMO reference Thermo Model 49i proved excellent measurement consistency (<inline-formula><mml:math id="M118" display="inline"><mml:mrow><mml:msup><mml:mi>R</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msup><mml:mo>=</mml:mo><mml:mn mathvariant="normal">0.9998</mml:mn></mml:mrow></mml:math></inline-formula>), with most absolute deviations below 4 ppb, and regular mixing ratio-dependent bias can be fully corrected by linear fitting using pre- and post-campaign calibration results. Laboratory aging experiments demonstrate the intrinsic monthly zero drift of Model 205 is less than 0.6 ppb; after adding extra thermal drift from periodic cabinet temperature fluctuation, the total monthly drift remains below 0.7 ppb, within the WMO/GAW allowed total uncertainty of <inline-formula><mml:math id="M119" display="inline"><mml:mrow><mml:mo>±</mml:mo><mml:mn mathvariant="normal">0.8</mml:mn></mml:mrow></mml:math></inline-formula> ppb for <inline-formula><mml:math id="M120" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">O</mml:mi><mml:mn mathvariant="normal">3</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>.</p>
      <p id="d2e1916">The <inline-formula><mml:math id="M121" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">O</mml:mi><mml:mn mathvariant="normal">3</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> mixing ratio (black line) consistently has a low standard deviation and minimal fluctuations, indicating high measurement stability. In contrast, the original <inline-formula><mml:math id="M122" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> mixing ratio (yellow line) displays substantial variation, with a peak standard deviation of 1.8, suggesting lower precision (Fig. 5a). The cabinet temperature (blue line) maintains a stable standard deviation, although a stepwise decrease over time suggests some control, albeit with potential for further improvement. In terms of the CV, the <inline-formula><mml:math id="M123" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">O</mml:mi><mml:mn mathvariant="normal">3</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> mixing ratio remains low (<inline-formula><mml:math id="M124" display="inline"><mml:mrow><mml:mo>&lt;</mml:mo><mml:mn mathvariant="normal">6</mml:mn></mml:mrow></mml:math></inline-formula> %) and continues to decrease over time, reflecting enhanced measurement consistency. As illustrated in Fig. 4, the ambient surface temperature at Taishan Station fluctuates widely between <inline-formula><mml:math id="M125" display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">45.0</mml:mn></mml:mrow></mml:math></inline-formula> and <inline-formula><mml:math id="M126" display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">20.5</mml:mn></mml:mrow></mml:math></inline-formula> <inline-formula><mml:math id="M127" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">°</mml:mi><mml:mi mathvariant="normal">C</mml:mi></mml:mrow></mml:math></inline-formula> with prominent diurnal cycles, whereas the active thermal cabinet limits internal instrument temperature within 8.0–19.0 <inline-formula><mml:math id="M128" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">°</mml:mi><mml:mi mathvariant="normal">C</mml:mi></mml:mrow></mml:math></inline-formula> with a CV of 16 %–20 % (<inline-formula><mml:math id="M129" display="inline"><mml:mrow><mml:mo>±</mml:mo><mml:mn mathvariant="normal">2.5</mml:mn></mml:mrow></mml:math></inline-formula> <inline-formula><mml:math id="M130" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">°</mml:mi><mml:mi mathvariant="normal">C</mml:mi></mml:mrow></mml:math></inline-formula> fluctuation). Comparative time-series analysis of <inline-formula><mml:math id="M131" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> and <inline-formula><mml:math id="M132" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">O</mml:mi><mml:mn mathvariant="normal">3</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> in Fig. 4b confirms that such cabinet temperature variation only yields tiny measurement drift (<inline-formula><mml:math id="M133" display="inline"><mml:mrow><mml:mo>≤</mml:mo><mml:mn mathvariant="normal">0.2</mml:mn></mml:mrow></mml:math></inline-formula> <inline-formula><mml:math id="M134" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">ppm</mml:mi><mml:mspace width="0.125em" linebreak="nobreak"/><mml:msup><mml:mi mathvariant="normal">h</mml:mi><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:mrow></mml:math></inline-formula> for <inline-formula><mml:math id="M135" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>, <inline-formula><mml:math id="M136" display="inline"><mml:mrow><mml:mo>≤</mml:mo><mml:mn mathvariant="normal">0.1</mml:mn></mml:mrow></mml:math></inline-formula> <inline-formula><mml:math id="M137" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">ppb</mml:mi><mml:mspace linebreak="nobreak" width="0.125em"/><mml:msup><mml:mi mathvariant="normal">h</mml:mi><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:mrow></mml:math></inline-formula> for <inline-formula><mml:math id="M138" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">O</mml:mi><mml:mn mathvariant="normal">3</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>), with no significant impact on measurement results (Fig. 5b). Postcalibration, the <inline-formula><mml:math id="M139" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> mixing ratio (red line) significantly decreases in CV, approaching 0 %, demonstrating the effectiveness of calibration in improving measurement accuracy.</p>

      <fig id="F5"><label>Figure 5</label><caption><p id="d2e2137">Evaluation of the Precision of <inline-formula><mml:math id="M140" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">O</mml:mi><mml:mn mathvariant="normal">3</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> and <inline-formula><mml:math id="M141" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> mixing ratios and Cabinet Temperatures through Standard Deviation and Coefficient of Variation Analysis Standard Deviation <bold>(a)</bold> Coefficient of Variation <bold>(b)</bold>.</p></caption>
          <graphic xlink:href="https://amt.copernicus.org/articles/19/5683/2026/amt-19-5683-2026-f05.png"/>

        </fig>

</sec>
</sec>
<sec id="Ch1.S5">
  <label>5</label><title>Discussion</title>
<sec id="Ch1.S5.SS1">
  <label>5.1</label><title>Performance Comparison</title>
      <p id="d2e2191">Traditional manned stations (e.g., South Pole Station) have irreplaceable advantages: real-time troubleshooting, flexible parameter adjustment, and weekly on-site calibration (measurement uncertainty <inline-formula><mml:math id="M142" display="inline"><mml:mrow><mml:mo>&lt;</mml:mo><mml:mn mathvariant="normal">0.5</mml:mn></mml:mrow></mml:math></inline-formula> ppm, better than CRUX's <inline-formula><mml:math id="M143" display="inline"><mml:mrow><mml:mo>±</mml:mo><mml:mn mathvariant="normal">1.0</mml:mn></mml:mrow></mml:math></inline-formula> ppm for <inline-formula><mml:math id="M144" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>). However, manned observations face high logistics costs and data gaps due to extreme weather evacuations. CRUX compensates for these shortcomings: its unattended operation mode eliminates the need for resident staff and frequent resupply, substantially reducing routine logistical costs; its 48 h UPS backup also ensures data continuity during short-term power outages. The good consistency with South Pole Station data  (<inline-formula><mml:math id="M145" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>: 420.7 ppm vs. 418.2 ppm; <inline-formula><mml:math id="M146" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">O</mml:mi><mml:mn mathvariant="normal">3</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>: 20.1 ppb vs. 20.5 ppb) indicates reliable measurement quality under the current short-term stable deployment, providing supporting evidence for its potential to complement manned observations in the future.</p>
      <p id="d2e2247">As shown in Table 1, CRUX's strengths lie in integrated optimization for Antarctic inland conditions: (1) Balanced performance: it reduces power consumption by 92 % compared to the initial 3 kW version, achieving <inline-formula><mml:math id="M147" display="inline"><mml:mrow><mml:mo>&lt;</mml:mo><mml:mn mathvariant="normal">350</mml:mn></mml:mrow></mml:math></inline-formula> W operation while maintaining multi-parameter detection, adapting to polar green energy constraints. (2) Extreme cold reliability: active temperature control isolates <inline-formula><mml:math id="M148" display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">25</mml:mn></mml:mrow></mml:math></inline-formula> to <inline-formula><mml:math id="M149" display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">40</mml:mn></mml:mrow></mml:math></inline-formula> <inline-formula><mml:math id="M150" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">°</mml:mi><mml:mi mathvariant="normal">C</mml:mi></mml:mrow></mml:math></inline-formula> external temperatures, and upwind intake with particle filters mitigates blowing snow interference. (3) High autonomy and accuracy: twice-daily auto-calibration reduces <inline-formula><mml:math id="M151" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> CV to near 0 %. Field tests revealed minor limitation flaws: (1) Temperature control lag: A 5 min heating response delay leads to 16 %–20 % cabinet temperature CV, potentially causing 0.2 <inline-formula><mml:math id="M152" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">ppm</mml:mi><mml:mspace width="0.125em" linebreak="nobreak"/><mml:msup><mml:mi mathvariant="normal">h</mml:mi><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:mrow></mml:math></inline-formula> drift of the LICOR-830 analyzer. (2) Insufficient long-term power: 48 h UPS backup. (3) Limited adaptability: fixed-time calibration cannot respond to sudden sensor drift; only two parameters are monitored.</p>

<table-wrap id="T1" specific-use="star"><label>Table 1</label><caption><p id="d2e2321">Comparison of the Polar Automatic GHG or Ozone Observation Systems.</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="left"/>
     <oasis:colspec colnum="3" colname="col3" align="left"/>
     <oasis:colspec colnum="4" colname="col4" align="left"/>
     <oasis:thead>
       <oasis:row>
         <oasis:entry colname="col1">Key Techniques</oasis:entry>
         <oasis:entry colname="col2">CRUX-1.0</oasis:entry>
         <oasis:entry colname="col3">BAS Ozone Network</oasis:entry>
         <oasis:entry colname="col4">Kunlun Station</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1"/>
         <oasis:entry colname="col2">(2024)</oasis:entry>
         <oasis:entry colname="col3">(2011)</oasis:entry>
         <oasis:entry colname="col4">Ozone  Monitor</oasis:entry>
       </oasis:row>
       <oasis:row rowsep="1">
         <oasis:entry colname="col1"/>
         <oasis:entry colname="col2"/>
         <oasis:entry colname="col3"/>
         <oasis:entry colname="col4">(2016)</oasis:entry>
       </oasis:row>
     </oasis:thead>
     <oasis:tbody>
       <oasis:row rowsep="1">
         <oasis:entry colname="col1">Monitoring Parameters</oasis:entry>
         <oasis:entry colname="col2"><inline-formula><mml:math id="M153" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> / <inline-formula><mml:math id="M154" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">O</mml:mi><mml:mn mathvariant="normal">3</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col3"><inline-formula><mml:math id="M155" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">O</mml:mi><mml:mn mathvariant="normal">3</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col4"><inline-formula><mml:math id="M156" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">O</mml:mi><mml:mn mathvariant="normal">3</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula></oasis:entry>
       </oasis:row>
       <oasis:row rowsep="1">
         <oasis:entry colname="col1">Power Consumption</oasis:entry>
         <oasis:entry colname="col2"><inline-formula><mml:math id="M157" display="inline"><mml:mrow><mml:mo>&lt;</mml:mo><mml:mn mathvariant="normal">350</mml:mn></mml:mrow></mml:math></inline-formula> W</oasis:entry>
         <oasis:entry colname="col3">11–13 W</oasis:entry>
         <oasis:entry colname="col4">5 W</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">Temperature Control Method</oasis:entry>
         <oasis:entry colname="col2">Auto-temperature control</oasis:entry>
         <oasis:entry colname="col3">Passive Insulation</oasis:entry>
         <oasis:entry colname="col4">Passive</oasis:entry>
       </oasis:row>
       <oasis:row rowsep="1">
         <oasis:entry colname="col1"/>
         <oasis:entry colname="col2">(10–15 <inline-formula><mml:math id="M158" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">°</mml:mi><mml:mi mathvariant="normal">C</mml:mi></mml:mrow></mml:math></inline-formula>)</oasis:entry>
         <oasis:entry colname="col3">with intake heater</oasis:entry>
         <oasis:entry colname="col4">Insulation</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">Calibration Method</oasis:entry>
         <oasis:entry colname="col2"><inline-formula><mml:math id="M159" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>: automatic (Single standard</oasis:entry>
         <oasis:entry colname="col3">On-site zero-check with</oasis:entry>
         <oasis:entry colname="col4">Periodic</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1"/>
         <oasis:entry colname="col2">gas mode, twice daily);</oasis:entry>
         <oasis:entry colname="col3">manual intervention and</oasis:entry>
         <oasis:entry colname="col4">calibration</oasis:entry>
       </oasis:row>
       <oasis:row rowsep="1">
         <oasis:entry colname="col1"/>
         <oasis:entry colname="col2"><inline-formula><mml:math id="M160" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">O</mml:mi><mml:mn mathvariant="normal">3</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>: periodic calibration</oasis:entry>
         <oasis:entry colname="col3">Periodic calibration</oasis:entry>
         <oasis:entry colname="col4"/>
       </oasis:row>
       <oasis:row rowsep="1">
         <oasis:entry colname="col1">Single Battery Backup Duration</oasis:entry>
         <oasis:entry colname="col2">48 h (UPS Backup Battery)</oasis:entry>
         <oasis:entry colname="col3">10–14 d (Lead-Acid Batteries)</oasis:entry>
         <oasis:entry colname="col4">Not applicable</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">Data Continuity Rate</oasis:entry>
         <oasis:entry colname="col2">99.2 %</oasis:entry>
         <oasis:entry colname="col3">85 % (Affected by</oasis:entry>
         <oasis:entry colname="col4">99.5 %</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1"/>
         <oasis:entry colname="col2"/>
         <oasis:entry colname="col3">power/communication)</oasis:entry>
         <oasis:entry colname="col4"/>
       </oasis:row>
     </oasis:tbody>
   </oasis:tgroup></oasis:table></table-wrap>

</sec>
<sec id="Ch1.S5.SS2">
  <label>5.2</label><title>Site Comparison</title>
      <p id="d2e2614">To verify the global representativeness of measurements from CRUX-1.0 at Taishan Station, quantify the regional differences in atmospheric <inline-formula><mml:math id="M161" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> and <inline-formula><mml:math id="M162" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">O</mml:mi><mml:mn mathvariant="normal">3</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> between polar and mid-latitude background regions,</p>
      <p id="d2e2639">To present the latitudinal gradient of global atmospheric background concentrations and verify the reliability of CRUX-1.0 data against the same-region reference station, comparative analysis was conducted on concurrent <inline-formula><mml:math id="M163" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> and <inline-formula><mml:math id="M164" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">O</mml:mi><mml:mn mathvariant="normal">3</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> datasets from five stations. It should be noted that stations with different latitudes and environments are not used to directly validate system performance, but to provide a global background context. The selected stations cover distinct geographical locations (polar vs. mid-latitude) and operational modes (unattended vs. manned), including Taishan Station (Antarctic inland, unattended), South Pole Station (Antarctic coastal, manned), Barrow Station (Arctic coastal, manned), Mauna Loa Station (mid-latitude marine, manned), and Jungfraujoch Station (mid-latitude alpine, manned) (Fig. 6a).</p>

      <fig id="F6"><label>Figure 6</label><caption><p id="d2e2666"><bold>(a)</bold> Global distribution of selected atmospheric background stations; <bold>(b)</bold> time series of hourly <inline-formula><mml:math id="M165" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> mixing ratios and <bold>(c)</bold> time series of hourly surface <inline-formula><mml:math id="M166" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">O</mml:mi><mml:mn mathvariant="normal">3</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> mixing ratios observed at these stations during the concurrent period (10 February–12 March 2024). This figure aims to validate the reliability and global representativeness of CRUX-1.0 measurements at Antarctic Taishan Station, reveal the distinct regional differences in atmospheric <inline-formula><mml:math id="M167" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> and <inline-formula><mml:math id="M168" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">O</mml:mi><mml:mn mathvariant="normal">3</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> between polar and mid-latitude background regions, and confirm the role of the unattended system in complementing the global atmospheric observation network.</p></caption>
          <graphic xlink:href="https://amt.copernicus.org/articles/19/5683/2026/amt-19-5683-2026-f06.png"/>

        </fig>

      <p id="d2e2729">Comparative results revealed distinct regional and operational differences in both <inline-formula><mml:math id="M169" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> and <inline-formula><mml:math id="M170" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">O</mml:mi><mml:mn mathvariant="normal">3</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> observations. For <inline-formula><mml:math id="M171" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>, polar stations (Taishan and South Pole; mean: 420.7 and 418.2 ppm; hereafter means) exhibited significantly lower baseline mixing ratios than mid-latitude counterparts (Mauna Loa: 424.9 ppm; Jungfraujoch: 427.6 ppm), primarily due to the absence of anthropogenic emissions in the Antarctic inland. Taishan Station also showed smaller fluctuation amplitude (<inline-formula><mml:math id="M172" display="inline"><mml:mrow><mml:mo>±</mml:mo><mml:mn mathvariant="normal">1.5</mml:mn></mml:mrow></mml:math></inline-formula> ppm), attributed to the homogeneous air masses in the Antarctic inland circulation and interference-free operation of the unattended system, whereas mid-latitude stations displayed larger fluctuations driven by regional emission transport and diurnal cycles. For <inline-formula><mml:math id="M173" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">O</mml:mi><mml:mn mathvariant="normal">3</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>, polar stations (Taishan: 20.1 ppb; South Pole: 20.5 ppb) had much lower mixing ratios than mid-latitude stations (Mauna Loa: 48.9 ppb; Jungfraujoch: 47.1 ppb), which was associated with weak photochemical activity in the Antarctic late summer., which was associated with the low mixing ratios of ozone precursors in Antarctica (due to the dual scarcity of natural and anthropogenic sources) impair the ozone formation potential, while the intense sunlight in summer, chemical depletion triggered by trace amounts of NO, and stable boundary layer conditions jointly lead to surface ozone in Antarctica being dominated by depletion during summer (Tian et al., 2022).</p>
</sec>
<sec id="Ch1.S5.SS3">
  <label>5.3</label><title>Long-term deployment challenges</title>
      <p id="d2e2794">The 1-month validation in this study only confirms the short-term feasibility of CRUX-1.0, which is a common constraint for proof-of-concept polar observation systems. From a broader perspective, long-term autonomous atmospheric observation in Antarctica generally faces three core common challenges: energy supply limitations under polar nights, long-term data quality assurance via autonomous calibration, and extreme environmental adaptability (e.g., blowing snow and ultra-low temperature).</p>
      <p id="d2e2797">For energy supply, CRUX-1.0 currently relies on Taishan Station’s diesel power infrastructure, which is limited by seasonal manual fuel replenishment. For long-term measurement accuracy, the single-point calibration of CRUX-1.0 is sufficient for short campaigns but has limited drift correction capacity over multi-month deployments.Targeting these challenges, we are conducting iterative upgrades of the CRUX-2.0 system, including a standalone PV-battery-methanol hybrid power system and autonomous multi-concentration calibration capability. The prototype is currently undergoing field validation at Saishiteng Mountain (Qinghai), with detailed parameters and test progress provided in the Supplement (Figs. S7 to S10).</p>
</sec>
</sec>
<sec id="Ch1.S6" sec-type="conclusions">
  <label>6</label><title>Summary</title>
      <p id="d2e2809">To fill the gap in unattended multi-parameter atmospheric observation in the Antarctic inland plateau, this study developed the CRUX-1.0 fully automated observation system. It is the first system of its kind in this region to achieve synchronous <inline-formula><mml:math id="M174" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> and surface <inline-formula><mml:math id="M175" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">O</mml:mi><mml:mn mathvariant="normal">3</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> monitoring with low-power design and automatic calibration. Integrating four core modules – sampling and calibration, analysis, temperature control, and data communication – the system is specifically optimized for polar conditions, featuring key characteristics such as total power consumption below 350 W, active cabinet temperature regulation maintaining 10–15 <inline-formula><mml:math id="M176" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">°</mml:mi><mml:mi mathvariant="normal">C</mml:mi></mml:mrow></mml:math></inline-formula>, twice-daily automatic single-point calibration for <inline-formula><mml:math id="M177" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>, and a 48 h UPS backup, making it well suited for remote sites with limited logistic support.</p>
      <p id="d2e2855">Deployed and operated continuously at Taishan Station (72.01° S, 92.08° E) from 10 February to 9 March 2024, the system achieved outstanding operational stability with a 99.2 % data recovery rate. Observed calibrated <inline-formula><mml:math id="M178" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> and <inline-formula><mml:math id="M179" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">O</mml:mi><mml:mn mathvariant="normal">3</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> mixing ratios (420.7 <inline-formula><mml:math id="M180" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> 0.7 ppm and 20.1 <inline-formula><mml:math id="M181" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> 0.8 ppb, respectively) show excellent consistency with synchronous reference measurements from South Pole Station; post-calibration CV values reach nearly 0 % for <inline-formula><mml:math id="M182" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> and below 5.6 % for <inline-formula><mml:math id="M183" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">O</mml:mi><mml:mn mathvariant="normal">3</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>, which validates the reliability of the CRUX-1.0 unattended observation framework under harsh Antarctic conditions. Compared with conventional manned observation platforms, CRUX-1.0 features an unattended operation mode that eliminates the need for resident staff and frequent resupply, substantially reducing routine logistical costs, offering a promising technical reference for filling observational gaps in the East Antarctic inland and supporting the construction of long-term polar monitoring networks.</p>
      <p id="d2e2917">Nevertheless, CRUX-1.0 still has limitations that restrict long-term year-round deployment in polar regions: continuous PTC heating results in relatively high power consumption; only single-point automatic calibration is available, with limited capacity to constrain span drift over multi-month operation; no reserved hardware interfaces for expanding additional gas species; and the current energy configuration cannot sustain prolonged polar-night operation. Targeting these four prominent bottlenecks (temperature control optimization, long-duration power supply, multi-parameter synchronous measurement, and dynamic calibration), we will carry out with targeted improvements: <list list-type="custom"><list-item><label>a.</label>
      <p id="d2e2922">Temperature control and power consumption optimization. Building on heating scheme comparisons in this study, follow-up upgrades will test a combination of self-limiting heating tapes and aerogel thermal wrapping to implement intermittent intelligent temperature control, cutting continuous heating power demand without compromising the thermal stability of internal instruments.</p></list-item><list-item><label>b.</label>
      <p id="d2e2926">Long-term energy supply improvement. Future deployments will adopt an optimized PV-battery-methanol hybrid power configuration to alleviate power shortage risks during multi-month polar nights.</p></list-item><list-item><label>c.</label>
      <p id="d2e2930">Multi-parameter coordinated monitoring. The next-generation CRUX-2.0 platform reserves modular expansion interfaces to sequentially add <inline-formula><mml:math id="M184" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CH</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>, <inline-formula><mml:math id="M185" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">H</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub><mml:mi mathvariant="normal">O</mml:mi></mml:mrow></mml:math></inline-formula> and other trace gas sensors, enabling synchronous multi-component atmospheric observation.</p></list-item><list-item><label>d.</label>
      <p id="d2e2958">Dynamic automatic calibration upgrade. Following laboratory intercomparison between the ABB GLA131-GGA analyzer and the Picarro G4301, we have selected the ABB GLA131-GGA configuration; paired with multi-channel solenoid valves, this design supports automatic multi-point standard gas calibration.</p></list-item></list> The CRUX-2.0 prototype is under field validation at Saishiteng Mountain (Lenghu, Qinghai), with completion scheduled for July 2026 to further enhance the sustainability and performance of polar autonomous atmospheric monitoring.</p>
</sec>

      
      </body>
    <back><notes notes-type="dataavailability"><title>Data availability</title>

      <p id="d2e2966">The in situ <inline-formula><mml:math id="M186" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> and surface ozone observation data collected at Taishan Station from 10 February to 12 March 2024 are archived and publicly available at the National Tibetan Plateau/Third Pole Environment Data Center (<ext-link xlink:href="https://doi.org/10.11888/Atmos.tpdc.303486" ext-link-type="DOI">10.11888/Atmos.tpdc.303486</ext-link>, Tian et al., 2026). The reference <inline-formula><mml:math id="M187" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> datasets for global background stations were retrieved from the World Data Centre for Greenhouse Gases (WDCGG) of WMO/GAW (<uri>https://gaw.kishou.go.jp/data/</uri>, last access: 14 December 2025), and the surface ozone datasets were obtained from the European Database for Atmospheric Sounding (EBAS, <uri>https://ebas-data.nilu.no/Pages/DataSetList.aspx</uri>, last access: 14 December 2025). Both public datasets are accessible in compliance with their respective official data policies.</p>
  </notes><app-group>
        <supplementary-material position="anchor"><p id="d2e3000">The supplement related to this article is available online at <inline-supplementary-material xlink:href="https://doi.org/10.5194/amt-19-5683-2026-supplement" xlink:title="pdf">https://doi.org/10.5194/amt-19-5683-2026-supplement</inline-supplementary-material>.</p></supplementary-material>
        </app-group><notes notes-type="authorcontribution"><title>Author contributions</title>

      <p id="d2e3009">Biao Tian was responsible for funding acquisition, field experiment, writing of the original draft, experimental design, and formal analysis. Minghu Ding was responsible for project administration, supervision, resources coordination, and review and editing. Kongju Zhu and Xu Yao were responsible for on-site field experiment. Yixi Zhao was responsible for formal analysis and data visualization. Wenqian Zhang was responsible for system software debugging and remote data acquisition. Diyi Yang, Weijun Sun, Yining Yu, Shoudong Zhao, Yige Cui, Chuanjin Li, Jie Tang, Cunde Xiao, Tong Zhu, and Renhe Zhang were responsible for review and editing.</p>
  </notes><notes notes-type="competinginterests"><title>Competing interests</title>

      <p id="d2e3015">The contact author has declared that none of the authors has any competing interests.</p>
  </notes><notes notes-type="disclaimer"><title>Disclaimer</title>

      <p id="d2e3021">Publisher's note: Copernicus Publications remains neutral with regard to jurisdictional claims made in the text, published maps, institutional affiliations, or any other geographical representation in this paper. The authors bear the ultimate responsibility for providing appropriate place names. Views expressed in the text are those of the authors and do not necessarily reflect the views of the publisher.</p>
  </notes><ack><title>Acknowledgements</title><p id="d2e3027">This study was made possible with the support and assistance of the 39th and 40th Chinese National Antarctic Research Expeditions (CHINARE) team. We would like to express our heartfelt gratitude for their invaluable contributions during the data collection process.</p></ack><notes notes-type="financialsupport"><title>Financial support</title>

      <p id="d2e3032">This work is financially supported by the National Natural Science Foundation of China (42201151) and the Basic Research Fund of Chinese Academy of Meteorological Sciences (2023Z004, 2024Z007).</p>
  </notes><notes notes-type="reviewstatement"><title>Review statement</title>

      <p id="d2e3039">This paper was edited by Keding Lu and reviewed by three anonymous referees.</p>
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