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  <front>
    <journal-meta><journal-id journal-id-type="publisher">ESD</journal-id><journal-title-group>
    <journal-title>Earth System Dynamics</journal-title>
    <abbrev-journal-title abbrev-type="publisher">ESD</abbrev-journal-title><abbrev-journal-title abbrev-type="nlm-ta">Earth Syst. Dynam.</abbrev-journal-title>
  </journal-title-group><issn pub-type="epub">2190-4987</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/esd-17-415-2026</article-id><title-group><article-title>Large-scale atmospheric circulation and its impact on the Baltic Sea region: controls, predictability and consequences</article-title><alt-title>Large-Scale atmospheric circulation and the Baltic Sea Region</alt-title>
      </title-group>
      <contrib-group>
        <contrib contrib-type="author" corresp="yes" rid="aff1">
          <name><surname>Börgel</surname><given-names>Florian</given-names></name>
          <email>florian.boergel@iow.de</email>
        <ext-link>https://orcid.org/0000-0003-3294-667X</ext-link></contrib>
        <contrib contrib-type="author" corresp="yes" rid="aff8">
          <name><surname>Ruvalcaba Baroni</surname><given-names>Itzel</given-names></name>
          <email>itzel.ruvalcababaroni@smhi.se</email>
        </contrib>
        <contrib contrib-type="author" corresp="no" rid="aff1">
          <name><surname>Barghorn</surname><given-names>Leonie</given-names></name>
          
        <ext-link>https://orcid.org/0000-0002-1907-7353</ext-link></contrib>
        <contrib contrib-type="author" corresp="no" rid="aff2">
          <name><surname>Borchert</surname><given-names>Leonard</given-names></name>
          
        <ext-link>https://orcid.org/0000-0002-3232-7409</ext-link></contrib>
        <contrib contrib-type="author" corresp="no" rid="aff1">
          <name><surname>Cahill</surname><given-names>Bronwyn</given-names></name>
          
        <ext-link>https://orcid.org/0000-0003-3782-2553</ext-link></contrib>
        <contrib contrib-type="author" corresp="no" rid="aff3">
          <name><surname>Dutheil</surname><given-names>Cyril</given-names></name>
          
        <ext-link>https://orcid.org/0000-0001-6891-2389</ext-link></contrib>
        <contrib contrib-type="author" corresp="no" rid="aff4">
          <name><surname>Esters</surname><given-names>Leonie</given-names></name>
          
        </contrib>
        <contrib contrib-type="author" corresp="no" rid="aff5">
          <name><surname>Falarz</surname><given-names>Małgorzata</given-names></name>
          
        </contrib>
        <contrib contrib-type="author" corresp="no" rid="aff6">
          <name><surname>Filipsson</surname><given-names>Helena L.</given-names></name>
          
        <ext-link>https://orcid.org/0000-0001-7200-8608</ext-link></contrib>
        <contrib contrib-type="author" corresp="no" rid="aff1">
          <name><surname>Gröger</surname><given-names>Matthias</given-names></name>
          
        <ext-link>https://orcid.org/0000-0002-9927-5164</ext-link></contrib>
        <contrib contrib-type="author" corresp="no" rid="aff7">
          <name><surname>Hänninen</surname><given-names>Jari</given-names></name>
          
        </contrib>
        <contrib contrib-type="author" corresp="no" rid="aff8">
          <name><surname>Hieronymus</surname><given-names>Magnus</given-names></name>
          
        </contrib>
        <contrib contrib-type="author" corresp="no" rid="aff9">
          <name><surname>Jakobson</surname><given-names>Erko</given-names></name>
          
        </contrib>
        <contrib contrib-type="author" corresp="no" rid="aff8">
          <name><surname>Karami</surname><given-names>Mehdi Pasha</given-names></name>
          
        <ext-link>https://orcid.org/0000-0003-0390-2889</ext-link></contrib>
        <contrib contrib-type="author" corresp="no" rid="aff10">
          <name><surname>Kuliński</surname><given-names>Karol</given-names></name>
          
        <ext-link>https://orcid.org/0000-0002-5403-6629</ext-link></contrib>
        <contrib contrib-type="author" corresp="no" rid="aff11">
          <name><surname>Liblik</surname><given-names>Taavi</given-names></name>
          
        </contrib>
        <contrib contrib-type="author" corresp="no" rid="aff1">
          <name><surname>Meier</surname><given-names>H. E. Markus</given-names></name>
          
        <ext-link>https://orcid.org/0000-0001-5855-4645</ext-link></contrib>
        <contrib contrib-type="author" corresp="no" rid="aff12 aff13 aff14">
          <name><surname>Messori</surname><given-names>Gabriele</given-names></name>
          
        <ext-link>https://orcid.org/0000-0002-2032-5211</ext-link></contrib>
        <contrib contrib-type="author" corresp="no" rid="aff1">
          <name><surname>Naumov</surname><given-names>Lev</given-names></name>
          
        <ext-link>https://orcid.org/0000-0002-2891-4766</ext-link></contrib>
        <contrib contrib-type="author" corresp="no" rid="aff1">
          <name><surname>Neumann</surname><given-names>Thomas</given-names></name>
          
        <ext-link>https://orcid.org/0000-0002-5653-906X</ext-link></contrib>
        <contrib contrib-type="author" corresp="no" rid="aff15">
          <name><surname>Post</surname><given-names>Piia</given-names></name>
          
        <ext-link>https://orcid.org/0000-0002-3537-3005</ext-link></contrib>
        <contrib contrib-type="author" corresp="no" rid="aff1">
          <name><surname>Rehder</surname><given-names>Gregor</given-names></name>
          
        <ext-link>https://orcid.org/0000-0002-0597-9989</ext-link></contrib>
        <contrib contrib-type="author" corresp="no" rid="aff12">
          <name><surname>Rutgersson</surname><given-names>Anna</given-names></name>
          
        <ext-link>https://orcid.org/0000-0001-7656-1881</ext-link></contrib>
        <contrib contrib-type="author" corresp="no" rid="aff1">
          <name><surname>Voelker</surname><given-names>Georg Sebastian</given-names></name>
          
        <ext-link>https://orcid.org/0000-0003-3658-8515</ext-link></contrib>
        <aff id="aff1"><label>1</label><institution>Leibniz Institute for Baltic Sea Research Warnemünde, Rostock, Germany</institution>
        </aff>
        <aff id="aff2"><label>2</label><institution>Center for Earth System Research and Sustainability, Universität Hamburg, Hamburg, Germany</institution>
        </aff>
        <aff id="aff3"><label>3</label><institution>MARBEC, University of Montpellier, CNRS, IFREMER, IRD, Sète, France</institution>
        </aff>
        <aff id="aff4"><label>4</label><institution>Institute of Geosciences, University of Bonn, Bonn, Germany</institution>
        </aff>
        <aff id="aff5"><label>5</label><institution>Institute of Earth Sciences, Faculty of Natural Sciences, University of Silesia in Katowice, Katowice, Poland</institution>
        </aff>
        <aff id="aff6"><label>6</label><institution>Department of Earth and Environmental Sciences, Lund University, Lund, Sweden</institution>
        </aff>
        <aff id="aff7"><label>7</label><institution>Archipelago Research Institute, Biodiversity Unit, University of Turku, 20014, Finland</institution>
        </aff>
        <aff id="aff8"><label>8</label><institution>Department of Research and Development, Swedish Meteorological and Hydrological Institute, Norrköping, Sweden</institution>
        </aff>
        <aff id="aff9"><label>9</label><institution>Tartu Observatory, University of Tartu, Töravere, Estonia</institution>
        </aff>
        <aff id="aff10"><label>10</label><institution>Institute of Oceanology Polish Academy of Sciences, Sopot, Poland</institution>
        </aff>
        <aff id="aff11"><label>11</label><institution>Department of Marine Systems, Tallinn University of Technology, Tallinn, Estonia</institution>
        </aff>
        <aff id="aff12"><label>12</label><institution>Department of Earth Sciences, Uppsala University, Uppsala, Sweden</institution>
        </aff>
        <aff id="aff13"><label>13</label><institution>Swedish Centre for Impact of Climate Extremes (climes), Uppsala University, Uppsala, Sweden</institution>
        </aff>
        <aff id="aff14"><label>14</label><institution>Department of Meteorology, Stockholm University, Stockholm, Sweden</institution>
        </aff>
        <aff id="aff15"><label>15</label><institution>Institute of Physics, University of Tartu, Tartu, Estonia</institution>
        </aff>
      </contrib-group>
      <author-notes><corresp id="corr1">Florian Börgel (florian.boergel@iow.de) and Itzel Ruvalcaba Baroni (itzel.ruvalcababaroni@smhi.se)</corresp></author-notes><pub-date><day>5</day><month>May</month><year>2026</year></pub-date>
      
      <volume>17</volume>
      <issue>3</issue>
      <fpage>415</fpage><lpage>450</lpage>
      <history>
        <date date-type="received"><day>5</day><month>November</month><year>2025</year></date>
           <date date-type="rev-request"><day>14</day><month>November</month><year>2025</year></date>
           <date date-type="rev-recd"><day>1</day><month>April</month><year>2026</year></date>
           <date date-type="accepted"><day>17</day><month>April</month><year>2026</year></date>
      </history>
      <permissions>
        <copyright-statement>Copyright: © 2026 Florian Börgel 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://esd.copernicus.org/articles/17/415/2026/esd-17-415-2026.html">This article is available from https://esd.copernicus.org/articles/17/415/2026/esd-17-415-2026.html</self-uri><self-uri xlink:href="https://esd.copernicus.org/articles/17/415/2026/esd-17-415-2026.pdf">The full text article is available as a PDF file from https://esd.copernicus.org/articles/17/415/2026/esd-17-415-2026.pdf</self-uri>
      <abstract><title>Abstract</title>

      <p id="d2e392">Large-scale Euro-Atlantic variability, shaped by the polar jet stream, governs weather and climate in the Baltic Sea region, thereby impacting the physical and biogeochemical properties of the Baltic Sea ecosystem. This review synthesizes how key atmospheric circulation features and modes of climate variability, including the North Atlantic Oscillation, atmospheric blocking and the Atlantic Multidecadal Variability, influence the Baltic Sea region. By integrating evidence from the published literature, observational datasets, and both global and regional climate model simulations, we assess established as well as potential linkages to key climatic variables, including temperature, precipitation, and storm activity, across temporal scales ranging from synoptic events to multidecadal variability. We then evaluate how these climate controls cascade into ecosystem-relevant processes, namely oxygen dynamics, primary productivity and ocean acidification. Although physical links are already established, the pathways connecting large-scale atmospheric patterns to biogeochemistry are still poorly constrained, partly because dedicated field studies and targeted model experiments are limited. We outline priority research needs to enhance near-term predictability and reduce uncertainty in future projections for the Baltic Sea.</p>
  </abstract>
    </article-meta>
  </front>
<body>
      

<sec id="Ch1.S1" sec-type="intro">
  <label>1</label><title>Introduction</title>
      <p id="d2e404">Home to more than 85 million people in its catchment area (see Fig. <xref ref-type="fig" rid="F1"/>) and bordered by nine countries, the Baltic Sea faces intense anthropogenic pressures and ranks among the most socio-economically exploited and polluted marine systems in the world <xref ref-type="bibr" rid="bib1.bibx112" id="paren.1"/>. It is the second-largest brackish water body in the world with an average salinity of approximately 7.4 <inline-formula><mml:math id="M1" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">g</mml:mi><mml:mspace width="0.125em" linebreak="nobreak"/><mml:msup><mml:mi mathvariant="normal">kg</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> <xref ref-type="bibr" rid="bib1.bibx184" id="paren.2"/>. Many resident species already live close to species-specific salinity tolerance limits and are simultaneously exposed to multiple human stressors, making them highly sensitive to environmental change <xref ref-type="bibr" rid="bib1.bibx99" id="paren.3"><named-content content-type="pre">e.g.,</named-content></xref>. Even small shifts in physical or biogeochemical conditions can substantially influence species abundance and growth. Superimposed onto these pressures, atmospheric variability in the Euro-Atlantic region further modulates the Baltic Sea's ecosystem across synoptic to multidecadal time scales <xref ref-type="bibr" rid="bib1.bibx126" id="paren.4"><named-content content-type="pre">e.g.,</named-content></xref>.</p>

      <fig id="F1" specific-use="star"><label>Figure 1</label><caption><p id="d2e445">Geographic extent of the Baltic Sea catchment (green) and schematic representation of the large-scale modes of climate variability influencing the Baltic Sea region: Atlantic Multidecadal Variability (AMV; purple), the North Atlantic Oscillation (NAO; blue/black), Scandinavian Blocking (SB; red), and jet-stream dynamics (black).</p></caption>
        <graphic xlink:href="https://esd.copernicus.org/articles/17/415/2026/esd-17-415-2026-f01.png"/>

      </fig>

      <p id="d2e454">The Baltic Sea is shallow, with a mean depth of 53 m and a maximum depth of 459 m <xref ref-type="bibr" rid="bib1.bibx115" id="paren.5"><named-content content-type="pre">e.g.,</named-content></xref>. It is shaped by a unique topography comprising several sub-basins and is connected to the North Sea only via the narrow and shallow Danish straits, which severely restrict water exchange between the two seas <xref ref-type="bibr" rid="bib1.bibx188" id="paren.6"><named-content content-type="pre">e.g.,</named-content></xref>. The result is an estuarine-like circulation with a fresher upper layer – sustained mainly by river runoff and, to a lesser extent, excess precipitation – that overlies more saline bottom waters which are renewed by intermittent saline inflows from the North Sea. This stratification suppresses vertical mixing and ventilation, increasing the vulnerability to hypoxic and eutrophic conditions.</p>
      <p id="d2e468">Given this strongly stratified, weakly ventilated system, local atmospheric forcing dominates the Baltic Sea's hydrodynamic variability on short time scales. On longer time scales, however, large-scale Euro-Atlantic circulation variability shapes the statistics of that forcing, most clearly in winter, by modulating the prevalence and persistence of westerlies, cold-air outbreaks, and storm-track activity <xref ref-type="bibr" rid="bib1.bibx270" id="paren.7"/>. The regional climate reflects a sensitive balance between moist, relatively mild marine air from the North Atlantic and the Eurasian continental influence, resulting in transitions between maritime and subarctic conditions. Accordingly, the southern and western parts of the Baltic Sea belong to the central European mild climate zone governed by westerly winds, whereas the northern part is typically located north of the polar front with a winter climate that is cold and dry due to Arctic air outbreaks from the east <xref ref-type="bibr" rid="bib1.bibx188" id="paren.8"/>.</p>
      <p id="d2e477">Key large-scale modes influencing the Baltic Sea include the North Atlantic Oscillation <xref ref-type="bibr" rid="bib1.bibx111" id="paren.9"><named-content content-type="pre">NAO;</named-content></xref>, atmospheric blocking <xref ref-type="bibr" rid="bib1.bibx300" id="paren.10"/> and, on longer time scales, their interplay with the Atlantic Multidecadal Variability <xref ref-type="bibr" rid="bib1.bibx23" id="paren.11"><named-content content-type="pre">AMV;</named-content></xref>. These modes are widely used because they can be linked to variability in the North Atlantic atmosphere (i.e., pressure and wind fields) and are associated with jet shifts. Together they explain a substantial fraction of observed variability over the Baltic Sea region <xref ref-type="bibr" rid="bib1.bibx184 bib1.bibx271 bib1.bibx136 bib1.bibx24" id="paren.12"><named-content content-type="pre">e.g.,</named-content></xref>. Changes in the jet's position and strength shape storm-track activity and thereby influence regional atmospheric forcing over the Baltic Sea including the frequency and persistence of local circulation states. For example, <xref ref-type="bibr" rid="bib1.bibx153" id="text.13"/> relate the large-scale NAO to a Baltic Sea pressure-gradient pattern (their Baltic Sea Index) that co-varies with Baltic Sea filling level and exchange through the Danish Straits, illustrating how remote modes project onto the local forcing that directly drives Baltic Sea dynamics.</p>
      <p id="d2e501">Together with high anthropogenic pressure (e.g., human-induced warming and nutrient inputs) and complex interactions among physical and biogeochemical processes across multiple spatiotemporal scales, variability in large-scale atmospheric circulation and the local atmospheric forcing contribute to the deterioration of the Baltic Sea's water quality <xref ref-type="bibr" rid="bib1.bibx121 bib1.bibx187 bib1.bibx141 bib1.bibx188 bib1.bibx203 bib1.bibx60" id="paren.14"/>. While episodic large saltwater inflows from the North Sea (so-called “Major Baltic Inflows”; MBIs) can temporarily oxygenate bottom waters <xref ref-type="bibr" rid="bib1.bibx200" id="paren.15"><named-content content-type="pre">e.g.,</named-content></xref>, anoxia intensified in the deep basins of the central Baltic Sea during the 20th century, driven by increased anthropogenic nutrient loads and subsequent eutrophication. Since the 1980s, when nutrient levels were at their peak, anoxia has become largely permanent <xref ref-type="bibr" rid="bib1.bibx87 bib1.bibx34 bib1.bibx185 bib1.bibx187 bib1.bibx223 bib1.bibx33 bib1.bibx163" id="paren.16"><named-content content-type="pre">e.g.,</named-content></xref>. Despite substantial efforts to reduce nutrient inputs since the 1980s, the Baltic Sea has shown little improvement in its eutrophication status, and deep-water oxygen conditions have continued to deteriorate <xref ref-type="bibr" rid="bib1.bibx87 bib1.bibx4 bib1.bibx96 bib1.bibx141" id="paren.17"/>.</p>
      <p id="d2e520">Large-scale Euro-Atlantic circulation variability has been shown to impact the Baltic Sea ecosystem by modulating the statistics of local forcing <xref ref-type="bibr" rid="bib1.bibx93 bib1.bibx54 bib1.bibx86" id="paren.18"><named-content content-type="pre">e.g.,</named-content></xref>. However, the effects vary regionally as coastal and sub-basin dynamics respond differently to changes in local forcing (e.g., winds, heat fluxes, freshwater input, or vertical mixing) <xref ref-type="bibr" rid="bib1.bibx64 bib1.bibx157 bib1.bibx53 bib1.bibx83 bib1.bibx272 bib1.bibx169 bib1.bibx232 bib1.bibx46" id="paren.19"/>. In the Baltic Sea, such differences can emerge as changes in coastal upwelling and cross-shore transport, shifts in riverine freshwater and nutrient supply, or altered stratification, deep-water ventilation, and oxygen depletion in the central basins. Disentangling these sources of internal variability from anthropogenic trends is therefore essential for understanding how regional biogeochemistry is linked to large-scale circulation variability. This review represents a first attempt to synthesize these links for the Baltic Sea region, identify key knowledge gaps, and clarify how large-scale circulation patterns and their variability influence both physical processes in the Baltic Sea and biogeochemical responses. Improved understanding of these links may also support future advances in predictability, although this prospect is currently much more developed for physical variables than for biogeochemical processes.</p>
      <p id="d2e531">Despite being one of the most thoroughly studied basins in the world with exceptionally long-term observations, direct empirical evidence from field studies that link large-scale atmospheric and oceanic patterns to Baltic Sea variability is rare, and many implications remain theoretical, especially for biogeochemistry.</p>
      <p id="d2e534">This review synthesizes current understanding of how large-scale atmospheric Euro-Atlantic circulation variability relates to local forcing over the Baltic Sea region (here defined as the Baltic Sea and its surrounding catchment area; Fig. <xref ref-type="fig" rid="F1"/>) across time scales ranging from synoptic to multidecadal. It also examines how the resulting hydrodynamic variability is linked to oxygen dynamics, primary productivity and ocean acidification. We focus specifically on the recent evolution of the Baltic Sea, during which anthropogenic climate change has become the dominant long-term external driver. Against this background, we examine how variability in Euro-Atlantic circulation patterns governs local forcing over the region and critically assess how these large-scale atmospheric influences interact with ongoing climate change.</p>
</sec>
<sec id="Ch1.S2">
  <label>2</label><title>Atmosphere and Ocean Dynamics</title>
<sec id="Ch1.S2.SS1">
  <label>2.1</label><title>Atmospheric features originating in the North Atlantic and impacting the Baltic Sea region</title>
<sec id="Ch1.S2.SS1.SSS1">
  <label>2.1.1</label><title>North Atlantic Jet Stream, Baroclinicity and Planetary Waves</title>
      <p id="d2e561">The dynamics of the tropospheric polar jet stream are a key control of weather and climate in the mid-latitudes. These dynamics arise from the interplay of baroclinic instability and large-scale wave patterns known as Rossby waves <xref ref-type="bibr" rid="bib1.bibx1 bib1.bibx164" id="paren.20"/>. To zeroth order, these components are driven by meridional temperature gradients, the thermal wind relation and the Earth's rotation. In the North Atlantic region, the polar jet is often referred to as the North Atlantic jet.</p>
      <p id="d2e567">The North Atlantic jet influences regional weather across Europe and the Baltic Sea region by modulating pressure systems, temperature advection, cloud cover, radiative processes and precipitation patterns <xref ref-type="bibr" rid="bib1.bibx300 bib1.bibx302 bib1.bibx91" id="paren.21"/>. More specifically, jet variability in the North Atlantic can be organized by time scale. On synoptic time scales, it primarily reflects baroclinic wave growth and downstream development that is tightly coupled with the storm track. On longer intraseasonal time scales, the dominant variability is captured by persistent flow patterns (weather regimes) <xref ref-type="bibr" rid="bib1.bibx285 bib1.bibx37 bib1.bibx36 bib1.bibx79 bib1.bibx66" id="paren.22"/>. On seasonal to interannual scales, anomalies in the jet latitude and strength project onto canonical modes of climate variability such as the NAO or the East Atlantic pattern <xref ref-type="bibr" rid="bib1.bibx109 bib1.bibx15 bib1.bibx301 bib1.bibx299 bib1.bibx303 bib1.bibx227" id="paren.23"/>. On decadal and longer time scales, coupled ocean-atmosphere variability in the North Atlantic can modulate the jet and storm track, providing a pathway for low-frequency variability to influence Northern Europe and the Baltic Sea region <xref ref-type="bibr" rid="bib1.bibx216 bib1.bibx266 bib1.bibx10 bib1.bibx247 bib1.bibx24" id="paren.24"/>.</p>
      <p id="d2e582">It should be noted that several localized processes further modulate this large-scale circulation and form the basis for typical synoptic-scale weather phenomena and dominant modes of climate variability affecting the Baltic Sea region. Factors such as orography, seasonal snow, ice cover, radiative processes, ocean heat transport and differences between land and ocean surfaces all contribute to a distinct thermal structure that drives a seasonal cycle. As a consequence, the jet stream follows a seasonally varying pattern with locally modified characteristics <xref ref-type="bibr" rid="bib1.bibx91 bib1.bibx300" id="paren.25"/>.</p>
      <p id="d2e588">Because the jet's latitude and strength vary seasonally, upstream Pacific circulation anomalies <xref ref-type="bibr" rid="bib1.bibx97 bib1.bibx192 bib1.bibx71" id="paren.26"/> as well as the state of the North Atlantic Ocean <xref ref-type="bibr" rid="bib1.bibx247" id="paren.27"/>, affect the jet differently in different seasons. Consequently, their downstream impacts over Europe and the Baltic Sea region are also season-dependent <xref ref-type="bibr" rid="bib1.bibx300 bib1.bibx302 bib1.bibx266 bib1.bibx24 bib1.bibx193 bib1.bibx275 bib1.bibx247" id="paren.28"/>.</p>
      <p id="d2e601">Changes in the structure, latitude and strength of the North Atlantic jet not only drive extreme weather in the mid-latitudes, such as heat waves, cold-air outbreaks and droughts, but also regulate moisture and precipitation <xref ref-type="bibr" rid="bib1.bibx74" id="paren.29"/>. Close to 90 % of the poleward moisture transport occurs within atmospheric rivers <xref ref-type="bibr" rid="bib1.bibx75 bib1.bibx74" id="paren.30"/>, long, narrow corridors in the atmosphere characterized by strong horizontal water vapor transport. Atmospheric rivers are typically in the warm conveyor belt ahead of extratropical cyclones. By influencing cyclone growth and storm tracks, the North Atlantic jet sets the preferred corridors and landfall latitudes. Accordingly, atmospheric river occurrence, intensity and associated precipitation patterns over the Baltic Sea region are sensitive to shifts in the North Atlantic jet as well.</p>
      <p id="d2e610">Pattern-based dimensionality reduction approaches are commonly used to assess this complexity, including canonical large-scale circulation patterns such as the NAO <xref ref-type="bibr" rid="bib1.bibx109" id="paren.31"/> or the Euro-Atlantic weather regimes <xref ref-type="bibr" rid="bib1.bibx285" id="paren.32"/>, which collapse jet and storm-track variability, Rossby-wave dynamics, and related regional modulation into a small number of reference states and display a systematic connection to jet characteristics <xref ref-type="bibr" rid="bib1.bibx176" id="paren.33"/>. These approaches provide an interpretable link between large-scale atmospheric circulation and its regional importance in the Baltic Sea region and allow a more detailed description of the local dynamics by describing their patterns and statistical properties. They are less suited to describe phenomena that are controlled by specific synoptic sequences rather than low-dimensional modes, such as MBIs, which depend on particular wind and pressure patterns <xref ref-type="bibr" rid="bib1.bibx182" id="paren.34"><named-content content-type="pre">e.g.,</named-content></xref>.</p>
</sec>
<sec id="Ch1.S2.SS1.SSS2">
  <label>2.1.2</label><title>Blocking patterns in the mid-latitudes</title>
      <p id="d2e635">An atmospheric block is a long-lasting (days to a few weeks) weather pattern that occurs when persistent and quasi-stationary highs hinder the climatological westerly winds in the mid-latitudes <xref ref-type="bibr" rid="bib1.bibx167" id="paren.35"/>. Dynamically, blocking is closely tied to the jet-stream and Rossby wave variability discussed in the previous section, as it reflects amplified planetary-wave patterns and is often accompanied by wave breaking and a deformation or splitting of the jet. This commonly leads to a deflected and strong zonal flow north and south of the blocking system <xref ref-type="bibr" rid="bib1.bibx194" id="paren.36"/> and prevents the usual progression of synoptic weather systems across large areas <xref ref-type="bibr" rid="bib1.bibx239 bib1.bibx269" id="paren.37"/>. Blocking systems typically extend vertically across the whole troposphere and are associated with large high pressure systems at the surface. As a consequence of their tight coupling to the background flow, changes in the large-scale circulation states (and modes of climate variability) can modulate blocking statistics by shifting the jet and storm track and therefore also the region of dominant wave amplification and breaking.</p>
      <p id="d2e647">In the mid-latitudes, blocking is frequently associated with extreme weather conditions, including heat waves <xref ref-type="bibr" rid="bib1.bibx230 bib1.bibx257 bib1.bibx246" id="paren.38"/>, cold spells <xref ref-type="bibr" rid="bib1.bibx31 bib1.bibx28 bib1.bibx245" id="paren.39"/>, heavy rainfall <xref ref-type="bibr" rid="bib1.bibx158" id="paren.40"/> and compound weather events <xref ref-type="bibr" rid="bib1.bibx134" id="paren.41"/>. The type of extreme event also depends on the exact location of the blocking pattern. Moreover, a single blocking event can cause different surface extremes at different locations (Fig. <xref ref-type="fig" rid="F2"/>). In general, blocking events are 7–10 d long and the most extreme events last 2–3 weeks. However, the societal relevance of these events is not solely defined by their persistence but also by the number of total blocking days and their seasonality <xref ref-type="bibr" rid="bib1.bibx29 bib1.bibx256 bib1.bibx134" id="paren.42"/>.</p>

      <fig id="F2" specific-use="star"><label>Figure 2</label><caption><p id="d2e670">Schematic illustration of the omega pattern (i.e., a blocking system) over the Baltic Sea region (black line, indicating a geopotential height or PV contour) and some associated surface extremes during <bold>(a)</bold> the warm season and <bold>(b)</bold> the cold season. Rossby wave breaking occurs on the flanks of the block, leading to (persistent) cutoff systems in this area. Areas with heavy precipitation are marked in light blue (poleward edge of the ridge and at both flanks). Areas with high integrated water vapor transport (IVT) are illustrated in orange. Thunderstorm activity is marked by yellow lightning bolt symbols. The position of a warm conveyor belt (WCB) appears in purple. Areas with temperature extremes are marked with dashed lines (red for heat waves and blue for cold spells) <xref ref-type="bibr" rid="bib1.bibx134" id="paren.43"><named-content content-type="pre">after</named-content></xref>.</p></caption>
            <graphic xlink:href="https://esd.copernicus.org/articles/17/415/2026/esd-17-415-2026-f02.png"/>

          </fig>

      <p id="d2e691">Figure <xref ref-type="fig" rid="F2"/> illustrates the potential extreme surface weather conditions in the Baltic Sea region associated with the Omega pattern: a blocking high with two cutoff lows on either side, with a high-pressure system squeezed in between. Panels (a) and (b) separate the impacts between the cold season (October to March) and the warm season (April to September), respectively. During the colder months, the eastern side of the blocking system may exhibit low-temperature anomalies. In contrast, the warmer months are prone to heat waves beneath the blocking system, occasionally coinciding with drought conditions. Additionally, the probability of thunderstorms increases at both the eastern and western flanks of the blocking system. Regardless of the season, heavy rainfall events – potentially leading to floods and associated with high integrated water vapor concentrations – are observed at the edges and near the poleward boundary of the blocking ridge.</p>
</sec>
</sec>
<sec id="Ch1.S2.SS2">
  <label>2.2</label><title>Natural variability from synoptic to multidecadal time scales</title>
      <p id="d2e705">Natural variability refers to climatic fluctuations that occur without any human influence, that is, internal variability (i.e. chaotically generated within the system) in isolation or in combination with natural external forcings such as volcanic eruptions or changes in solar activity <xref ref-type="bibr" rid="bib1.bibx8" id="paren.44"/>. The natural variability of the North Atlantic climate system affects the Baltic Sea region across multiple temporal and spatial scales, ranging from individual extreme events such as storms and heat waves <xref ref-type="bibr" rid="bib1.bibx82 bib1.bibx84 bib1.bibx59 bib1.bibx251" id="paren.45"/> to multi-decadal shifts in precipitation intensity <xref ref-type="bibr" rid="bib1.bibx25" id="paren.46"/>. The impacts on society span various sectors, for instance affecting energy production, agriculture, forestry, traffic, biodiversity, fisheries, maritime activities and the livelihood of coastal communities (HELCOM, 2023). This section focuses on linking our current knowledge of natural variability and its impact at different time scales, unfolding from days to decades. More specifically, we address synoptic (1–7 d), intraseasonal (10–90 d), seasonal (1 year), interannual (1 to 9 years), decadal and multidecadal (10 years and longer) time scales.</p>
      <p id="d2e717">In this review, we distinguish between different statistical methods to describe large-scale circulation patterns, such as the NAO derived from EOF-based analyses of sea-level pressure or geopotential-height anomalies, or weather regimes, which describe recurrent, quasi-stationary circulation patterns diagnosed from clustering methods on daily to sub-seasonal time scales. While these frameworks are related, weather regimes often project onto leading modes, and are not interchangeable.</p>
<sec id="Ch1.S2.SS2.SSS1">
  <label>2.2.1</label><title>Synoptic, intraseasonal and seasonal time scales</title>
      <p id="d2e727">Atmospheric circulation variability over the Baltic Sea region spans a broad range of time scales, from synoptic to multidecadal, and reflects the interplay of atmospheric, oceanic, and terrestrial factors. At shorter time scales, departures from the climatological reference state often take the form of large-scale geopotential height anomalies that persist from several days to about two weeks <xref ref-type="bibr" rid="bib1.bibx134" id="paren.47"/>.</p>
      <p id="d2e733">These recurrent disturbances are modulated by variations in the Euro-Atlantic atmospheric circulation and are well classified by the Euro-Atlantic weather regimes <xref ref-type="bibr" rid="bib1.bibx285 bib1.bibx66 bib1.bibx37" id="paren.48"/>. At their core, weather regimes represent a statistical description of persistent and recurrent circulation patterns, similar to attractors in non-linear dynamical systems <xref ref-type="bibr" rid="bib1.bibx43 bib1.bibx221" id="paren.49"/> that can be described in terms of their quasi-stationarity and frequency of occurrence. The regimes are identified objectively from daily large-scale circulation anomalies over the Euro-Atlantic sector: the seasonal cycle is removed and anomaly fields are normalized by their standard deviation, dimensionality is reduced using the leading EOFs (principal components), and k-means clustering is applied in this reduced phase space. This yields a daily sequence of regime occurrence, with some days assigned to one of the recurrent regimes and others classified as transition or “no regime” days <xref ref-type="bibr" rid="bib1.bibx79" id="paren.50"/>. The regimes affect the Baltic Sea region by shaping the synoptic-scale pressure gradient over Northern Europe. They are closely linked to jet-stream variability and the associated characteristic flow patterns <xref ref-type="bibr" rid="bib1.bibx176" id="paren.51"/>. As a result, they modulate the prevalence and intensity of westerly flow into the Baltic Sea catchment versus blocking situations, as well as the position and strength of the storm tracks affecting the region.</p>
      <p id="d2e748">Traditionally, the canonical Euro-Atlantic weather-regime classification refers to the four recurrent large-scale circulation regimes most robustly identified in boreal winter <xref ref-type="bibr" rid="bib1.bibx285 bib1.bibx36 bib1.bibx16 bib1.bibx66" id="paren.52"/>. In this manuscript, weather regimes refer to statistically identified, recurrent large-scale circulation states, rather than to individual synoptic weather patterns. The Zonal and Greenland-Blocking regimes are often described as NAO-like, in the sense that they project strongly onto the positive and negative phases of the NAO, respectively. Hence, the Zonal pattern (NAO+) corresponds to a central North Atlantic jet which brings mild and wet air masses as well as Atlantic cyclones into Northern Europe <xref ref-type="bibr" rid="bib1.bibx78" id="paren.53"/>. In contrast, Greenland Blocking (NAO-) represents a more southerly jet position, weakening the westerlies, favoring colder, drier conditions. The Atlantic Ridge describes a high pressure system over the Atlantic with a northward shift of the jet, leading to stable weather and potentially blocking the eastward progression of wet and windy conditions. The Scandinavian Blocking is a high pressure system over Scandinavia featuring a jet structure that tilts from southwest to northeast (Fig. <xref ref-type="fig" rid="F3"/>).</p>

      <fig id="F3"><label>Figure 3</label><caption><p id="d2e762">Atlantic-European weather regimes in winter and their relative frequency of occurrence (in percent). <bold>(a–g)</bold> 500 hPa geopotential height mean composites (contours, every 80 geopotential meters (gpm)) and their anomalies (shading, every 20 gpm) with respect to the seasonal climatology <bold>(h)</bold> during active regime life cycles (the onset to decay period) in December, January, February of 1979–2019. The weather regimes considered are: <bold>(a)</bold> Atlantic Trough, <bold>(b)</bold> Zonal Regime (NAO+), <bold>(c)</bold> Scandinavian Trough, <bold>(d)</bold> Atlantic Ridge, <bold>(e)</bold> European Blocking, <bold>(f)</bold> Scandinavian Blocking, <bold>(g)</bold> Greenland Blocking (NAO-). Numbers in the subfigure titles indicate the frequencies of winter days attributed to the respective regime <bold>(a–g)</bold>. The frequency of “no regime” days is 24.1 % <xref ref-type="bibr" rid="bib1.bibx106" id="paren.54"><named-content content-type="post">their Fig. 1</named-content></xref>.</p></caption>
            <graphic xlink:href="https://esd.copernicus.org/articles/17/415/2026/esd-17-415-2026-f03.png"/>

          </fig>

      <p id="d2e807">A year-round classification adds three more regimes (Fig. <xref ref-type="fig" rid="F3"/>): the Scandinavian Trough, a low pressure system over Scandinavia, the Atlantic Trough, associated with a low pressure system over the North Atlantic, and European Blocking, marked by a high pressure system over western Europe that blocks the North Atlantic jet <xref ref-type="bibr" rid="bib1.bibx79" id="paren.55"/>. In total, the seven weather regimes represent different types of zonal regimes (Atlantic Trough, Zonal, and Scandinavian Trough), responsible for the advection of warm (or cold) air masses from the North Atlantic region into the Baltic Sea region, as well as four regional blocking regimes (Atlantic Ridge, European Blocking, Scandinavian Blocking, and Greenland Blocking).</p>
      <p id="d2e815">Depending on the season, zonal regimes are associated with wet and cool (warm) conditions in northern Europe during summer (winter). In contrast, the blocked regimes interrupt the mean flow and are often associated with hot and dry spells during summer and cold spells on their eastern flank during winter <xref ref-type="bibr" rid="bib1.bibx79 bib1.bibx19 bib1.bibx55 bib1.bibx195 bib1.bibx276" id="paren.56"/>.</p>
      <p id="d2e821">The seven regimes (Fig. <xref ref-type="fig" rid="F3"/>) occur with a similar frequency but have strong seasonal preferences. Zonal regimes (i.e. Atlantic Trough, Zonal/NAO+ and Scandinavian Trough) are more common in winter (November–March), with Zonal being particularly frequent. Summer (May–September) is dominated by blocked regimes (i.e. Atlantic Ridge, European Blocking, Scandinavian Blocking and Greenland Blocking), with Scandinavian Blocking occurring most often. Atlantic Trough occurs year round and European Blocking is the leading winter blocking pattern, while Scandinavian Blocking dominates summer <xref ref-type="bibr" rid="bib1.bibx79" id="paren.57"/>.</p>
      <p id="d2e829">Seasonal circulation variability over the Baltic Sea region differs markedly between winter and summer. Winter is dominated by zonal (NAO-like) patterns, enhanced baroclinicity and high internal variability. The latter is often weaker, with a poleward-shifted jet and a more barotropic background. Thermodynamic processes such as land-sea contrasts, soil-moisture feedbacks, and diabatic heating then play a larger role in shaping circulation variability and extremes <xref ref-type="bibr" rid="bib1.bibx114 bib1.bibx165 bib1.bibx86 bib1.bibx59" id="paren.58"/>. This suggests that large-scale atmospheric circulation variability exerts a stronger control on the Baltic Sea region in winter than in summer.</p>
</sec>
<sec id="Ch1.S2.SS2.SSS2">
  <label>2.2.2</label><title>Interannual time scales</title>
      <p id="d2e843">Interannual variability can be understood through the lens of the jet stream. Specifically, anomalies in the location and intensity of the jet stream during the winter season drive climate variability that can explain much of the observed interannual variability <xref ref-type="bibr" rid="bib1.bibx97" id="paren.59"/>. Good examples are the winters of 2009/10 and 2011/12 (Fig. <xref ref-type="fig" rid="F4"/>), which exhibited opposite jet regimes: the former displayed an anomalously southerly, zonal jet, while the latter displayed an anomalously northerly jet <xref ref-type="bibr" rid="bib1.bibx254" id="paren.60"/>. The first led to an anomalously cold winter in the Baltic Sea region, while the second led to an unusually warm winter.</p>

      <fig id="F4" specific-use="star"><label>Figure 4</label><caption><p id="d2e856">North Atlantic Oscillation (NAO) index, monthly values (thin gray) with 12 month centered running mean (thick black). Months with <inline-formula><mml:math id="M2" display="inline"><mml:mrow><mml:mtext>NAO</mml:mtext><mml:mo>&gt;</mml:mo><mml:mn mathvariant="normal">0</mml:mn></mml:mrow></mml:math></inline-formula> are shaded red; <inline-formula><mml:math id="M3" display="inline"><mml:mrow><mml:mtext>NAO</mml:mtext><mml:mo>&lt;</mml:mo><mml:mn mathvariant="normal">0</mml:mn></mml:mrow></mml:math></inline-formula> are shaded blue. Vertical dashed lines mark winters 2009/10 and 2011/12. Data: NOAA CPC monthly standardized NAO (<inline-formula><mml:math id="M4" display="inline"><mml:mrow><mml:msub><mml:mi>z</mml:mi><mml:mn mathvariant="normal">500</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>-based).</p></caption>
            <graphic xlink:href="https://esd.copernicus.org/articles/17/415/2026/esd-17-415-2026-f04.png"/>

          </fig>

      <p id="d2e900">The NAO reflects a leading mode of observed interannual wintertime variability in North Atlantic-European atmospheric circulation and is tightly coupled to the zonal jet. Notably, both the intensity (NAO+ or NAO-; Fig. <xref ref-type="fig" rid="F4"/>) and the geographic positioning of the NAO centers of action vary substantially year-to-year <xref ref-type="bibr" rid="bib1.bibx104 bib1.bibx110 bib1.bibx228 bib1.bibx229 bib1.bibx171 bib1.bibx172 bib1.bibx173 bib1.bibx24" id="paren.61"/>. These spatial shifts of the NAO modify how strongly the NAO affects the Baltic Sea region, as changes in the pressure gradient orientation alter prevailing wind patterns <xref ref-type="bibr" rid="bib1.bibx154 bib1.bibx24" id="paren.62"/>. This dynamic is likely linked to the interaction between the NAO and the jet stream <xref ref-type="bibr" rid="bib1.bibx303" id="paren.63"/>, which due to the zonal shift of the Icelandic Low aligns the westerly winds directly toward the Baltic Sea.</p>
      <p id="d2e915">To relate this interannual perspective to the synoptic-to-intraseasonal weather-regime framework introduced above, we compare the characteristic circulation patterns associated with the main interannual climate-variability indices to the circulation patterns of the weather regimes. The positive East Atlantic pattern <xref ref-type="bibr" rid="bib1.bibx15" id="paren.64"/> corresponds to a quasi-stationary ridge over the North Atlantic aligning with the Atlantic Ridge regime, while the negative East Atlantic pattern corresponds to the Atlantic Trough <xref ref-type="bibr" rid="bib1.bibx35" id="paren.65"/>. Together with the NAO, the East Atlantic pattern can be used as a combined framework describing both climatological changes and interannual and multidecadal variability in the North Atlantic jet <xref ref-type="bibr" rid="bib1.bibx301 bib1.bibx299 bib1.bibx227" id="paren.66"/>. However, the NAO primarily describes shifts in the jet latitude, which tends to be more relevant for interannual time scales <xref ref-type="bibr" rid="bib1.bibx303" id="paren.67"/>. For the Baltic Sea region, this distinction implies that NAO-driven jet-latitude shifts dominate year-to-year variability in winter temperature, sea-ice and storminess, whereas changes linked with the East Atlantic pattern modulate multidecadal variability.</p>
      <p id="d2e930">While the positive phase of the Scandinavian pattern <xref ref-type="bibr" rid="bib1.bibx132" id="paren.68"><named-content content-type="pre">e.g.,</named-content></xref> resembles  Scandinavian Blocking, its negative phase aligns with the Scandinavian Trough. After the NAO and East Atlantic pattern, it is the third most important winter sea level pressure pattern over the North Atlantic domain <xref ref-type="bibr" rid="bib1.bibx41" id="paren.69"/> and in the Baltic Sea region, specifically, it is considered the second most important pattern <xref ref-type="bibr" rid="bib1.bibx132" id="paren.70"/>.</p>
      <p id="d2e944">Since the Scandinavian pattern resembles the positive Scandinavian Blocking regime <xref ref-type="bibr" rid="bib1.bibx41" id="paren.71"/>, the question arises how it might be connected to the interannual variability of blocking occurrences. According to <xref ref-type="bibr" rid="bib1.bibx30" id="text.72"/>, the anticyclonic center of the Scandinavian pattern lies in a region where the potential vorticity gradients are generally very low during the winter months, possibly favoring the development of a block. However, <xref ref-type="bibr" rid="bib1.bibx240" id="text.73"/> found that the dominant winter blocking patterns are connected to different large-scale circulation patterns, the Scandinavian pattern only being one of them. This could be different in the summer season where Scandinavian Blocking occurs more often. However, studies on summer modes of interannual variability are still scarce.</p>
      <p id="d2e956">In summary, these interannual modes systematically alter the direction and strength of the flow over Northern Europe/Scandinavia, modulating winter advection, storminess, temperature, and sea-ice. Multiple other interannual circulation patterns in the Euro-Atlantic sector have been identified, for example the East Atlantic/West Russia pattern <xref ref-type="bibr" rid="bib1.bibx15 bib1.bibx132 bib1.bibx45" id="paren.74"/> or the Barents Sea Oscillation <xref ref-type="bibr" rid="bib1.bibx267 bib1.bibx280" id="paren.75"/>. They all represent a statistical description of characteristic jet features. However, there is little literature specifically addressing their role in modulating the climate of the Baltic Sea region on interannual time scales.</p>
</sec>
<sec id="Ch1.S2.SS2.SSS3">
  <label>2.2.3</label><title>Decadal and multidecadal time scales</title>
      <p id="d2e974">On decadal time scales, atmospheric variability in Northern Europe is modulated by an interplay of the aforementioned atmospheric modes with the North Atlantic Ocean, shaping the statistics of local climate in the Baltic Sea region. The ocean's memory, especially through the Atlantic Meridional Overturning Circulation (AMOC), drives much of this decadal variability as it transports heat into higher latitudes, altering sea surface temperature (SST) patterns <xref ref-type="bibr" rid="bib1.bibx150" id="paren.76"><named-content content-type="pre">e.g.,</named-content></xref>.</p>
      <p id="d2e982">One central component of this variability is the AMV, which refers to basin-wide fluctuations in the North Atlantic SSTs over multidecadal periods <xref ref-type="bibr" rid="bib1.bibx63 bib1.bibx139" id="paren.77"><named-content content-type="pre">e.g.,</named-content></xref>. The main driver of these fluctuations is likely a combination of internal variability that is coupled to AMOC variability <xref ref-type="bibr" rid="bib1.bibx241 bib1.bibx298 bib1.bibx50" id="paren.78"/> and a response to external forcing <xref ref-type="bibr" rid="bib1.bibx178" id="paren.79"/>. For the Baltic Sea region, large ensembles of global climate simulations suggest that the response to external forcing is more relevant than internal variability <xref ref-type="bibr" rid="bib1.bibx13" id="paren.80"/>.</p>
      <p id="d2e999">Sea surface temperature anomalies that are advected along the North Atlantic current influence temperature variations in the Norwegian Sea <xref ref-type="bibr" rid="bib1.bibx148 bib1.bibx67" id="paren.81"/> and over Norway <xref ref-type="bibr" rid="bib1.bibx9" id="paren.82"/>. These anomalies can often be traced back to oceanic advection of signals from the North Atlantic subpolar gyre (SPG) <xref ref-type="bibr" rid="bib1.bibx67" id="paren.83"/>, which is one of the most predictable regions in the world on decadal to multidecadal time scales <xref ref-type="bibr" rid="bib1.bibx306 bib1.bibx22" id="paren.84"/>. This connection indicates a potential for successful near-term predictions of decadal climate variability in the Baltic Sea region.</p>
      <p id="d2e1014">Multidecadal SST variations in the North Atlantic have been shown to alter the atmospheric circulation in the North Atlantic and climate variability across Europe <xref ref-type="bibr" rid="bib1.bibx57 bib1.bibx49 bib1.bibx248 bib1.bibx268 bib1.bibx216 bib1.bibx247 bib1.bibx218" id="paren.85"/> with further impacts on the Nordic Seas <xref ref-type="bibr" rid="bib1.bibx9 bib1.bibx140 bib1.bibx67" id="paren.86"/> and the Baltic Sea <xref ref-type="bibr" rid="bib1.bibx23 bib1.bibx24 bib1.bibx25 bib1.bibx26 bib1.bibx13 bib1.bibx191 bib1.bibx137" id="paren.87"/>. One example of this influence is the modulation of a subpolar wave train, a large-scale atmospheric pattern that responds to SST anomalies and projects onto the European climate <xref ref-type="bibr" rid="bib1.bibx21 bib1.bibx199" id="paren.88"/>. This wave train is often centered over Northern Europe and transports oceanic signals from the North Atlantic into the Baltic Sea region.</p>
      <p id="d2e1030">Similar to the interannual time scale, in Northern Europe, decadal atmospheric variability in wintertime over the North Atlantic is dominated by the NAO <xref ref-type="bibr" rid="bib1.bibx222 bib1.bibx225" id="paren.89"><named-content content-type="pre">e.g.,</named-content></xref>. More specifically, the decadal to multidecadal SST anomalies, linked to the AMV, influence both the position and strength of the NAO <xref ref-type="bibr" rid="bib1.bibx24" id="paren.90"/> and the jet stream <xref ref-type="bibr" rid="bib1.bibx247 bib1.bibx10" id="paren.91"/>. Hence, during wintertime, the AMV influences the advection of air masses from the North Atlantic, weakening the westerlies during its positive states. Negative AMV states are associated with increased westerlies, transporting moist air masses into the Baltic Sea region <xref ref-type="bibr" rid="bib1.bibx25" id="paren.92"/>. This coupling between the ocean and the atmosphere has been linked to the relative importance of the NAO for the Baltic Sea region <xref ref-type="bibr" rid="bib1.bibx213" id="paren.93"/> on multidecadal time scales <xref ref-type="bibr" rid="bib1.bibx24" id="paren.94"/>. During summer, subtropical North Atlantic SSTs excite an atmospheric Rossby wave which connects to decadal surface air temperature fluctuations in Europe, with an imprint on the Baltic Sea region <xref ref-type="bibr" rid="bib1.bibx202" id="paren.95"><named-content content-type="pre">e.g.,</named-content></xref>.</p>
      <p id="d2e1059">On decadal to multidecadal time scales, the relevance of modes of climate variability such as the NAO arises from changes in the frequency and persistence of large-scale circulation states and from their coupling to slowly varying boundary conditions, especially North Atlantic SSTs and ocean circulation, rather than from direct analogies with individual synoptic systems <xref ref-type="bibr" rid="bib1.bibx202" id="paren.96"/>. For example, besides its interplay with the AMV, one key feedback loop involves the NAO and the North Atlantic SST tripole pattern <xref ref-type="bibr" rid="bib1.bibx51" id="paren.97"/>. The direction of this interaction is still under debate with studies illustrating an SST influence on the NAO <xref ref-type="bibr" rid="bib1.bibx242 bib1.bibx237" id="paren.98"/> and some showing NAO influence on SST <xref ref-type="bibr" rid="bib1.bibx10" id="paren.99"/>. It was also shown that the location of the Gulf Stream front may imprint onto NAO on these time scales <xref ref-type="bibr" rid="bib1.bibx122" id="paren.100"/>. Recent research proposes a negative feedback loop: NAO-induced SST anomalies affect the AMOC, which in turn alters the SSTs which influence the NAO in the opposite direction <xref ref-type="bibr" rid="bib1.bibx226" id="paren.101"/>. Some studies also indicate that a vertical component in the atmosphere is included in this feedback loop <xref ref-type="bibr" rid="bib1.bibx212" id="paren.102"/>. This feedback loop acts on decadal-to-multidecadal time scales and may give rise to important variability in Northern Europe as well <xref ref-type="bibr" rid="bib1.bibx24" id="paren.103"/>.</p>
      <p id="d2e1087">In this context, the representation of coupled North Atlantic ocean-atmosphere variability in global climate models has recently been questioned. In particular, <xref ref-type="bibr" rid="bib1.bibx35" id="text.104"/> showed that the observed link between spring North Atlantic SST variability and summer Euro-Atlantic circulation is temporally non-stationary and is generally not reproduced, or is too weakly reproduced, in the evaluated global model. More broadly, persistent deficiencies in the simulation of Euro-Atlantic jet and regime dynamics, including blocking, further limit the realism of atmosphere-ocean coupling pathways in models. This is also relevant for the Baltic Sea region, because many regional Baltic Sea models are still forced by prescribed atmospheric boundary conditions and therefore inherit biases in the large-scale circulation from their driving models.</p>
      <p id="d2e1093">Freshwater anomalies in the subpolar North Atlantic (SPG) may also influence European, and potentially Baltic Sea, climate through downstream circulation anomalies. <xref ref-type="bibr" rid="bib1.bibx211" id="text.105"/> linked such anomalies – likely related to anomalous Arctic/sub-Arctic runoff and meltwater input – to a sharper winter SST front between the subpolar and subtropical North Atlantic and to associated large-scale atmospheric circulation anomalies. Overall, these hydrographic anomalies, modulated by SPG variability, contribute to multiyear predictability in both oceanic and atmospheric conditions <xref ref-type="bibr" rid="bib1.bibx140 bib1.bibx107 bib1.bibx67 bib1.bibx211" id="paren.106"/>.</p>
      <p id="d2e1102">Longer-range teleconnections which can modulate the North Atlantic climate, particularly from the Indian and Pacific Oceans, add further complexity to European climate variability <xref ref-type="bibr" rid="bib1.bibx36 bib1.bibx69 bib1.bibx68" id="paren.107"/>. One notable mode of Pacific variability is the Pacific Decadal Oscillation (PDO), the leading mode of North Pacific SST variability (EOF1 of SSTs over 20–70° N) <xref ref-type="bibr" rid="bib1.bibx179 bib1.bibx207" id="paren.108"/>. While direct studies on the PDO's influence on the Baltic climate remain limited, its impact on the region is often mediated through its interactions with other modes of climate variability such as the NAO, El Niño-Southern Oscillation (ENSO) and Arctic sea ice variability. For instance, <xref ref-type="bibr" rid="bib1.bibx265" id="text.109"/> report PDO-related anomalies over the Baltic region, though they emphasize its modulation of broader sea ice effects. Additionally, the PDO has been shown to modulate ENSO's influence on the North Atlantic <xref ref-type="bibr" rid="bib1.bibx291 bib1.bibx130" id="paren.110"/>, further underscoring its indirect role in shaping atmospheric circulation patterns that can affect Northern Europe. This is because PDO-related shifts in the Aleutian Low and North Pacific jet reshape the North Pacific waveguide, steering ENSO-forced Rossby waves and altering their downstream projection into the North Atlantic <xref ref-type="bibr" rid="bib1.bibx177" id="paren.111"/>. More broadly, such extratropical teleconnections are dependent on the climatological background flow <xref ref-type="bibr" rid="bib1.bibx217" id="paren.112"/>. This interconnectedness highlights the PDO's potential contribution to (multi)decadal variability in European climate.</p>
</sec>
</sec>
<sec id="Ch1.S2.SS3">
  <label>2.3</label><title>Large-scale atmosphere–ocean controls on regional climate variability</title>
      <p id="d2e1133">The climate of the Baltic Sea region can be perceived as an interplay between the aforementioned large-scale circulation variability and regional features. In particular, one should recall the unique bathymetry of the Baltic Sea (see Fig. <xref ref-type="fig" rid="F5"/>) which is characterized by a shallow mean depth, a suite of sub-basins and narrow and shallow connections to the open ocean.</p>

      <fig id="F5" specific-use="star"><label>Figure 5</label><caption><p id="d2e1140">Bathymetry of the Baltic Sea with labels indicating major sub-basins.</p></caption>
          <graphic xlink:href="https://esd.copernicus.org/articles/17/415/2026/esd-17-415-2026-f05.jpg"/>

        </fig>

      <p id="d2e1149">In this section, we describe the impacts of the large-scale atmosphere-ocean patterns on the natural variability of regional processes in the Baltic Sea, without assessing the effect of anthropogenic climate change.</p>
<sec id="Ch1.S2.SS3.SSS1">
  <label>2.3.1</label><title>Precipitation</title>
      <p id="d2e1160">Precipitation in the Baltic Sea region varies across time scales, with different mechanisms dominating at each scale. The best-established link is for wintertime variability, when large-scale North Atlantic circulation exerts a strong control on moisture transport and cyclone pathways into Northern Europe. On synoptic and intraseasonal time scales, precipitation anomalies are primarily associated with variations in the latitude and strength of the North Atlantic jet and the resulting shifts in storm-track activity, rather than with any specific weather regime. When the jet is stronger and displaced northward, cyclones and moisture transport more frequently reach Northern Europe and parts of the Baltic Sea catchment, favoring wetter conditions. In contrast, a more southerly jet or blocked circulation over Scandinavia tends to suppress precipitation over large parts of the region, while enhancing it along the flanks and poleward side of the block, where moisture transport and warm conveyor belts are concentrated <xref ref-type="bibr" rid="bib1.bibx134 bib1.bibx158" id="paren.113"/>. On interannual time scales, the NAO is the most widely used index for precipitation variability in the Baltic Sea region, especially in winter, but its influence is not spatially uniform across the region <xref ref-type="bibr" rid="bib1.bibx109 bib1.bibx111 bib1.bibx304" id="paren.114"/>. Positive NAO conditions are generally associated with strong westerly flow and wetter-than-average conditions over the northern and western parts of the Baltic Sea region, whereas negative NAO conditions tend to favor reduced precipitation there. However, the strength and even the sign of the precipitation response can vary within the Baltic catchment depending on the longitudinal position of the NAO centers of action and on the state of other circulation patterns <xref ref-type="bibr" rid="bib1.bibx24" id="paren.115"/>. In particular, the East Atlantic and Scandinavian patterns modulate both the spatial structure and the magnitude of precipitation anomalies over the Baltic Sea region <xref ref-type="bibr" rid="bib1.bibx36 bib1.bibx45 bib1.bibx154" id="paren.116"/>. On multidecadal time scales, the influence is more indirect. North Atlantic sea-surface temperature variability can alter the mean position of the jet and the associated sea-level pressure patterns, thereby changing the background likelihood of wet and dry conditions in the Baltic Sea region. Available evidence suggests relatively drier conditions during positive AMV phases and wetter conditions during negative AMV phases, although these relationships are less robust and more weakly constrained than the wintertime interannual links associated with the NAO <xref ref-type="bibr" rid="bib1.bibx247 bib1.bibx25" id="paren.117"/>. Potential influences from Arctic or Pacific sea-ice variability on Baltic precipitation remain uncertain, and their net effect on the region has not yet been robustly established <xref ref-type="bibr" rid="bib1.bibx264 bib1.bibx183" id="paren.118"/>.</p>
</sec>
<sec id="Ch1.S2.SS3.SSS2">
  <label>2.3.2</label><title>Storms</title>
      <p id="d2e1190">Variability in storminess in the Baltic Sea region is closely connected to the location and strength of the North Atlantic storm track, but the relative importance of associated large-scale circulation and locally driven dynamics depends on the time scale. On synoptic to intraseasonal time scales, the NAO and jet-stream configuration provide a useful framework for describing the regional likelihood, pathways, and clustering of storms reaching the Baltic Sea region <xref ref-type="bibr" rid="bib1.bibx154 bib1.bibx24 bib1.bibx250" id="paren.119"/>. In this sense, large-scale circulation exerts a strong control on the statistics of storminess, especially in winter, whereas the realized near-surface winds and local impacts of individual events remain strongly shaped by local factors such as coastline orientation, basin geometry, bathymetry, and land-sea contrasts. Generally, a stronger and northward-shifted jet – such as during NAO+ or a positive East Atlantic pattern – favors enhanced storm-track activity and increased storminess over the Baltic Sea region. In contrast, blocked regimes (Atlantic Ridge and European/Scandinavian Blocking) tend to suppress storms locally beneath the ridge, while enhancing activity along the flanks. A positive NAO also increases extreme wind return levels along the southern Baltic Sea and downstream, indicating an elevated risk of storm surges <xref ref-type="bibr" rid="bib1.bibx235" id="paren.120"/>.</p>
      <p id="d2e1199">On interannual time scales, the influence of large-scale atmospheric variability is spatially heterogeneous across the Baltic region. The Scandinavian Pattern appears to be the strongest modulator of winter storm activity in the Baltic region, followed by the NAO and the Polar/Eurasian pattern – a pattern projecting onto a zonal/NAO+ regime during its positive phase, while the negative phase projects onto blocked regimes, mainly Greenland Blocking (NAO-) and sometimes Scandinavian Blocking. The East Atlantic pattern also plays an important role, especially for the forecasting skill of storm tracks into the Baltic Sea region <xref ref-type="bibr" rid="bib1.bibx48 bib1.bibx290" id="paren.121"/>.  Moreover, the positioning of the jet stream and the strength of the meridional pressure gradient in the North Atlantic can explain a large part of the decadal changes in 10 m wind speeds in northern Europe, with low windiness in winters of the 1980s and 2010s and high windiness in the 1990s <xref ref-type="bibr" rid="bib1.bibx152" id="paren.122"/>. On multidecadal time scales, the warm phase of the AMV corresponds to an equatorward-shifted jet and a storm track that is less extended poleward compared to the AMV cold phase <xref ref-type="bibr" rid="bib1.bibx247" id="paren.123"/>, favoring reduced storminess in the Baltic region.</p>
</sec>
<sec id="Ch1.S2.SS3.SSS3">
  <label>2.3.3</label><title>Sea level</title>
      <p id="d2e1219">Sea level variability in the Baltic Sea is predominantly driven by the large-scale atmospheric circulation owing to small tidal amplitudes. On synoptic time scales, the Baltic Sea sea level is mainly driven by wind stress inside the basin, whereas on seasonal to multidecadal time scales the controlling signal originates from the adjacent basin Kattegat and thus ultimately from the North Atlantic <xref ref-type="bibr" rid="bib1.bibx252" id="paren.124"/>. This is because the Danish straits separating the Baltic Sea from the Kattegat act as a physical low-pass filter, essentially damping synoptic scale variability, while allowing seasonal and longer time scales to pass <xref ref-type="bibr" rid="bib1.bibx102" id="paren.125"/>.</p>
      <p id="d2e1228">Sea level in the Baltic Sea exhibits a seasonal cycle, with higher levels in autumn and winter than in spring and summer <xref ref-type="bibr" rid="bib1.bibx274" id="paren.126"/>. Against this seasonal background, interannual sea-level variability has been found to correlate with the NAO, especially in winter, although the strength of the relationship varies in time and across the Baltic Sea region. For example, <xref ref-type="bibr" rid="bib1.bibx6" id="text.127"/> reported a correlation of <inline-formula><mml:math id="M5" display="inline"><mml:mrow><mml:mi>r</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">0.63</mml:mn></mml:mrow></mml:math></inline-formula> between the winter (JFM) NAO index and the winter mean Baltic Sea level over 1825–1997, increasing to <inline-formula><mml:math id="M6" display="inline"><mml:mrow><mml:mi>r</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">0.74</mml:mn></mml:mrow></mml:math></inline-formula> for 1902–1997. Westerly winds over the area are typically stronger during the positive phase of the NAO which pushes water into the Baltic and raises the sea level <xref ref-type="bibr" rid="bib1.bibx119 bib1.bibx120" id="paren.128"/>. The strength of the correlation between the NAO and mean sea level, however, varies between different basins and in time. The temporal variability can partly be explained by the interplay between the NAO, the East Atlantic and the Scandinavian patterns <xref ref-type="bibr" rid="bib1.bibx132 bib1.bibx38" id="paren.129"/>.</p>
      <p id="d2e1268">An index based on the sea level pressure difference between the Bay of Biscay and Tromsø has also been suggested as an alternative to the NAO <xref ref-type="bibr" rid="bib1.bibx129" id="paren.130"/>. This Baltic Sea and North Sea Oscillation (BANOS) index was introduced because the NAO–Baltic sea-level relationship is non-stationary in time and spatially heterogeneous, whereas BANOS is more stably linked to Baltic and North Sea sea-level variability. <xref ref-type="bibr" rid="bib1.bibx129" id="text.131"/> showed that it explained locally up to 90 % of interannual sea-level variance in winter and up to 79 % in summer during 1993–2013. Decadal and multidecadal sea level variability is much less explored than interannual variability. <xref ref-type="bibr" rid="bib1.bibx128" id="text.132"/> reported statistically significant links between decadal sea level variability and variations in sea level pressure and precipitation. In contrast, they found no robust connection to the AMV, as the strongest correlation reported for any season was only 0.2.</p>
      <p id="d2e1280">Not only mean sea level, but also sea level extremes in the Baltic Sea are correlated to the NAO <xref ref-type="bibr" rid="bib1.bibx180 bib1.bibx101" id="paren.133"><named-content content-type="pre">e.g.,</named-content></xref>. However, this relationship is regionally heterogeneous and generally weaker than for mean sea level. In part, the relationship can be explained as a preconditioning, where storm surges occur from a higher baseline during positive NAO phases owing to its effect on the mean sea level, but there is likely an effect also on the surges themselves <xref ref-type="bibr" rid="bib1.bibx295" id="paren.134"/>. Yet, the magnitude of individual storm-surge events depends strongly on regional and event-specific wind forcing, coastline orientation, fetch, and basin geometry. This indicates that multiple time scales from synoptic to at least interannual could be contributing to this effect. Moreover, NAO variability extends to other flooding-relevant drivers. For example, along the southern coast of Sweden, total annual wave energy is positively correlated with the winter NAO (<inline-formula><mml:math id="M7" display="inline"><mml:mrow><mml:mi>r</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">0.51</mml:mn></mml:mrow></mml:math></inline-formula>) offshore, and this relationship is even stronger closer to the coast <xref ref-type="bibr" rid="bib1.bibx2" id="paren.135"/>. Runoff has likewise been reported to show seasonally significant NAO correlations in parts of the Baltic catchment, although these relationships are more regionally heterogeneous than for mean sea level <xref ref-type="bibr" rid="bib1.bibx304" id="paren.136"/>. Together, these links suggest that the risk of compound flooding may also be modulated by the NAO <xref ref-type="bibr" rid="bib1.bibx103" id="paren.137"><named-content content-type="pre">e.g.,</named-content></xref>.</p>
</sec>
<sec id="Ch1.S2.SS3.SSS4">
  <label>2.3.4</label><title>Surface Air Temperature and Sea Temperatures</title>
      <p id="d2e1323">Surface air temperature (SAT) and sea-surface temperature (SST) in the Baltic Sea are tightly coupled. In summer, the surface mixed layer is typically 15–20 m deep, while in autumn-winter it often reaches the seabed in shallow areas or deepens to the halocline (40–80 m) in deeper basins. Consequently, daily SAT anomalies are reflected in SST with a lag of only a few days; in summer the lag rarely exceeds two weeks. Hence, more than 80 % of the monthly SST variance is explained by the combined sensible and latent heat fluxes that depend on SAT and incoming shortwave radiation <xref ref-type="bibr" rid="bib1.bibx137" id="paren.138"/>.</p>
      <p id="d2e1329">Anomalously low winter SSTs in the Baltic Sea are associated with negative NAO phases and severe winters, whereas anomalously high SSTs are linked to positive NAO phases and mild winters <xref ref-type="bibr" rid="bib1.bibx262 bib1.bibx137" id="paren.139"/>, closely following the winter NAO-SAT relationship <xref ref-type="bibr" rid="bib1.bibx279" id="paren.140"/>. Most of the interannual winter SAT variability (87 % at Stockholm) is explained by the NAO <xref ref-type="bibr" rid="bib1.bibx184" id="paren.141"/>.</p>
      <p id="d2e1341">The properties of the cold intermediate layer are established during winter mixing, and this water mass persists in the water column until the following winter. Consequently, the interannual variability of cold intermediate layer temperature is strongly correlated with the severity of the preceding winter, which is largely determined by the winter NAO <xref ref-type="bibr" rid="bib1.bibx160 bib1.bibx105 bib1.bibx197" id="paren.142"/>.</p>
      <p id="d2e1347">On decadal and longer time scales, positive AMV phases are associated with higher Baltic Sea SSTs, but this response is strongly seasonal and spatially heterogeneous rather than uniform throughout the year. Previous work estimated that about 58 % of the decadal Baltic SST variability can be linked to the AMV after removing the global warming signal <xref ref-type="bibr" rid="bib1.bibx137" id="paren.143"/>. More recent work further showed that the linear annual-mean SST response to the AMV is relatively weak, on the order of 0.2 <inline-formula><mml:math id="M8" 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>, whereas the influence is strongest in winter, when up to 40 % of regional SST variability can be associated with multidecadal variability closely linked to the AMV, corresponding locally to about 1.2 <inline-formula><mml:math id="M9" 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> per standard deviation of the AMV<xref ref-type="bibr" rid="bib1.bibx26" id="paren.144"/>. This influence is thought to be mediated partly through the NAO and partly through a subpolar atmospheric wave train that links North Atlantic SST anomalies to Northern European climate <xref ref-type="bibr" rid="bib1.bibx21 bib1.bibx199 bib1.bibx24" id="paren.145"/>. In the Baltic Sea region, this influence appears to be expressed primarily through changes in large-scale pressure patterns, westerly flow, and oceanic inertia <xref ref-type="bibr" rid="bib1.bibx26" id="paren.146"/> and aerosol forcing <xref ref-type="bibr" rid="bib1.bibx13" id="paren.147"/>.</p>
      <p id="d2e1387">Temperature variability on all time scales provides the baseline for marine heat waves (MHWs) in the Baltic Sea, which are predominantly linked to atmospheric modes <xref ref-type="bibr" rid="bib1.bibx86 bib1.bibx17" id="paren.148"/>. These MHWs very likely coincide with atmospheric heat waves although a dedicated comparison is missing. <xref ref-type="bibr" rid="bib1.bibx86" id="text.149"/> identified the dominant preconditions for MHWs on seasonal time scales. During summer, a prevailing stable high pressure system over Scandinavia supports anomalously high shortwave absorption and thus heat uptake in the upper water layer. The associated weak-wind regime further delimits mixing of heated surface waters with colder water from below resulting in a stable and shallow thermocline. Winter MHWs are mainly caused by external warm and humid air masses advected from the North Atlantic via the westerly wind regime <xref ref-type="bibr" rid="bib1.bibx86" id="paren.150"/>. Consequently, atmospheric conditions resembling the positive phase of the NAO elevate the risk for winter MHWs in the Baltic Sea. The local processes are characterized by an anomalously low heat flux out of the sea. Here, reduced latent heat fluxes (due to the humid air masses) and reduced sensible heat fluxes (due to anomalously warm air) play the dominant roles.</p>
</sec>
<sec id="Ch1.S2.SS3.SSS5">
  <label>2.3.5</label><title>Sea ice cover</title>
      <p id="d2e1407">Sea ice in the Baltic Sea shows pronounced interannual variability <xref ref-type="bibr" rid="bib1.bibx80" id="paren.151"/>. Over the past century, a shift toward milder ice winters has been observed, with reductions in both ice extent and thickness expected to continue in the present century <xref ref-type="bibr" rid="bib1.bibx188 bib1.bibx90" id="paren.152"/>.</p>
      <p id="d2e1416">The variability is influenced by the NAO and the Arctic Oscillation <xref ref-type="bibr" rid="bib1.bibx287 bib1.bibx286 bib1.bibx90 bib1.bibx282" id="paren.153"/>. Statistical modelling shows that zonal flow is the dominant circulation control on Baltic Sea ice extent, with the winter NAO accounting for about 29 % of the year-to-year variance in annual maximum ice extent, while meridional flow also contributes, particularly in November and January <xref ref-type="bibr" rid="bib1.bibx213" id="paren.154"/>. Winters dominated by strong westerlies (NAO+) are typically associated with reduced sea ice cover in the Baltic Sea. Between January and March, negative NAO phases (<inline-formula><mml:math id="M10" display="inline"><mml:mrow><mml:mtext>NAO</mml:mtext><mml:mo>&lt;</mml:mo><mml:mo>-</mml:mo><mml:mn mathvariant="normal">0.5</mml:mn></mml:mrow></mml:math></inline-formula>) are linked to substantially larger mean annual ice extent (259 000 <inline-formula><mml:math id="M11" display="inline"><mml:mrow class="unit"><mml:msup><mml:mi mathvariant="normal">km</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msup></mml:mrow></mml:math></inline-formula>), while positive phases (<inline-formula><mml:math id="M12" display="inline"><mml:mrow><mml:mtext>NAO</mml:mtext><mml:mo>&gt;</mml:mo><mml:mo>+</mml:mo><mml:mn mathvariant="normal">0.5</mml:mn></mml:mrow></mml:math></inline-formula>) are associated with reduced ice extent <xref ref-type="bibr" rid="bib1.bibx287" id="paren.155"><named-content content-type="pre">121 000 <inline-formula><mml:math id="M13" display="inline"><mml:mrow class="unit"><mml:msup><mml:mi mathvariant="normal">km</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msup></mml:mrow></mml:math></inline-formula>,</named-content></xref>. The relationship between NAO and annual maximum ice extent is non-stationary and can vary across different time periods <xref ref-type="bibr" rid="bib1.bibx213 bib1.bibx39" id="paren.156"/>, possibly linked to shifts in the NAO centers of action <xref ref-type="bibr" rid="bib1.bibx24" id="paren.157"/>.</p>
      <p id="d2e1487">In addition to the NAO and Arctic Oscillation, interannual variations in Baltic Sea ice parameters have also been found to correlate with the PDO <xref ref-type="bibr" rid="bib1.bibx282" id="paren.158"/>. The physical mechanisms underlying this connection remain unclear, but correlations can be of comparable magnitude to those of the North Atlantic Oscillation, although they are not temporally persistent <xref ref-type="bibr" rid="bib1.bibx286" id="paren.159"/>.</p>
</sec>
<sec id="Ch1.S2.SS3.SSS6">
  <label>2.3.6</label><title>Salinity and Stratification</title>
      <p id="d2e1504">Salinity variations in the Baltic Sea are controlled by the interplay of freshwater input, mainly through river runoff and irregular saltwater inflows from the North Sea. The river runoff lowers the salinity in the surface layer of the Baltic Sea via direct dilution, accounting for 27 % of the salinity variations <xref ref-type="bibr" rid="bib1.bibx236" id="paren.160"/>. Consequently, the outflowing water through the Danish straits becomes fresher. This water partly mixes with the underlying saltier layer which decreases the salinity of subsequent saltwater inflows <xref ref-type="bibr" rid="bib1.bibx191" id="paren.161"/>.</p>
      <p id="d2e1513">Saltwater inflows that shape the salinity of the deeper parts in the Baltic Sea occur under specific synoptic wind conditions and are connected to the passage of deep cyclones over the region <xref ref-type="bibr" rid="bib1.bibx182 bib1.bibx260 bib1.bibx155" id="paren.162"><named-content content-type="pre">e.g.,</named-content></xref>. Wind variations on synoptic time scales are reflected in salinity fluctuations in the rather shallow western Baltic Sea whereas the deeper basins of the central Baltic Sea act as a low-pass filter  <xref ref-type="bibr" rid="bib1.bibx81 bib1.bibx190" id="paren.163"><named-content content-type="pre">e.g.,</named-content></xref>. Depending on their density, inflows spread at intermediate depths or form a deep layer that propagates along the bottom. Only large inflows (MBIs) can reach the deep basins of the Baltic Proper and settle at the bottom. While MBIs occur mainly in winter and only roughly a few times per decade, smaller inflows can happen throughout the year <xref ref-type="bibr" rid="bib1.bibx182 bib1.bibx198 bib1.bibx196" id="paren.164"/>. MBIs are modulated by the accumulated freshwater supply over multidecadal time scales <xref ref-type="bibr" rid="bib1.bibx191" id="paren.165"/>, whereas smaller inflows <xref ref-type="bibr" rid="bib1.bibx61 bib1.bibx189" id="paren.166"/> show a strong dependence on interannual atmospheric forcing.</p>
      <p id="d2e1535">Directly linking NAO and salinity variations is challenging <xref ref-type="bibr" rid="bib1.bibx236 bib1.bibx259" id="paren.167"/> due to their differing dominant time scales: the NAO fluctuates mainly on 4–10 year periods <xref ref-type="bibr" rid="bib1.bibx191" id="paren.168"/>, while the water balance of the Baltic Sea is characterized by multidecadal 30 year fluctuations <xref ref-type="bibr" rid="bib1.bibx184 bib1.bibx137 bib1.bibx191 bib1.bibx271" id="paren.169"><named-content content-type="pre">e.g.,</named-content></xref>. Longer periods with predominant NAO+ (i.e., persistent strong westerlies) elevate the mean sea level in the Baltic Sea, suppressing saltwater inflows and lowering bottom salinities <xref ref-type="bibr" rid="bib1.bibx149 bib1.bibx260 bib1.bibx155 bib1.bibx191 bib1.bibx184" id="paren.170"/>.</p>
      <p id="d2e1552">On a multidecadal scale, the salinity of the Baltic Sea is correlated with the AMV. During the course of the last millennium, the dominant time scales were above 120 and 60–90 years during the Little Ice Age <xref ref-type="bibr" rid="bib1.bibx23" id="paren.171"><named-content content-type="post">their Fig. 2</named-content></xref> and were linked to salinity changes of about 0.7 <inline-formula><mml:math id="M14" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">g</mml:mi><mml:mspace linebreak="nobreak" width="0.125em"/><mml:msup><mml:mi mathvariant="normal">kg</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 the 20th century, common spectral power was also found between 20 and 30 years <xref ref-type="bibr" rid="bib1.bibx236" id="paren.172"/>, resulting in changes of about 0.2 <inline-formula><mml:math id="M15" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">g</mml:mi><mml:mspace width="0.125em" linebreak="nobreak"/><mml:msup><mml:mi mathvariant="normal">kg</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>. The dominance of 30 year fluctuations in the water cycle of the Baltic Sea has been a matter of discussion for a long time, given that neither the NAO nor the AMV have high spectral power in that period band. Recently, <xref ref-type="bibr" rid="bib1.bibx191" id="text.173"/> argued that the superposition of 60 year temperature fluctuations in the North Atlantic related to the AMV and the 60 year periodicity in the displacement of the NAO's centers of action evoked by, again, the AMV <xref ref-type="bibr" rid="bib1.bibx24" id="paren.174"/> causes the 30 year variability in the water balance of the Baltic Sea.</p>
</sec>
<sec id="Ch1.S2.SS3.SSS7">
  <label>2.3.7</label><title>Solar radiation</title>
      <p id="d2e1613">Changes in solar radiation, more specifically, shortwave irradiance, are affected by atmospheric processes altering the amount of sunlight which can be absorbed, reflected or scattered by atmospheric transparency, water vapour, cloud cover and albedo. In the 1950s to 1980s a decrease in shortwave irradiance (dimming) has been detected in many regions in Europe, followed by an increase (brightening) until present <xref ref-type="bibr" rid="bib1.bibx297 bib1.bibx208 bib1.bibx249 bib1.bibx253 bib1.bibx224 bib1.bibx233" id="paren.175"/>.</p>
      <p id="d2e1619">Several studies attribute brightening in Europe to a decline in aerosols <xref ref-type="bibr" rid="bib1.bibx208 bib1.bibx296" id="paren.176"/>. However, a recent investigation found a more subtle shift in attribution over the last four decades <xref ref-type="bibr" rid="bib1.bibx258" id="paren.177"/> supporting earlier results <xref ref-type="bibr" rid="bib1.bibx188" id="paren.178"/>. While the aerosol effect was primarily responsible for brightening between 1983 and 2002, variability in cloud cover emerged as the predominant driver of observed brightening between 2001 and 2020. <xref ref-type="bibr" rid="bib1.bibx234" id="text.179"/> found a significant increase in solar radiation accompanied by a decrease in cloud cover in the Baltic Sea during the past half-century. They show that while anticyclonic (clear) circulation patterns have become more frequent, zonal (overcast) patterns are occurring less often with a significant negative trend. This can be partially explained by variations in the synoptic patterns over Scandinavia (Sect. <xref ref-type="sec" rid="Ch1.S2.SS3.SSS7"/>) likely linked to a northward shift in the North Atlantic storm tracks which enter the Arctic, without passing Scandinavia, and promote the blocking over northwestern Europe <xref ref-type="bibr" rid="bib1.bibx138 bib1.bibx70 bib1.bibx57 bib1.bibx224" id="paren.180"/>.</p>
      <p id="d2e1640">The increase in surface solar radiation may also explain shifts in seasonality, especially to longer and earlier summers in the Baltic Sea <xref ref-type="bibr" rid="bib1.bibx234" id="paren.181"/>. <xref ref-type="bibr" rid="bib1.bibx124" id="text.182"/> detected important seasonal shifts in a variety of physical and biological parameters, with e.g. the cumulative sum of 30 000 <inline-formula><mml:math id="M16" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">W</mml:mi><mml:mspace width="0.125em" linebreak="nobreak"/><mml:msup><mml:mi mathvariant="normal">m</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> of surface incoming shortwave irradiance being reached 23 d earlier in 2013 compared to 1983. The shift is highly correlated with earlier warming and later cooling of SST, which in turn also affects the availability of light in the water column  (see also Sect. <xref ref-type="sec" rid="Ch1.S2.SS2.SSS1"/>).</p>
      <p id="d2e1668">A recent modeling study suggested that the PDO accounts for about 20 %–40 % of the unforced year-to-year shortwave-flux variability in Northern Hemisphere continental averages, mainly through cloud redistribution. For Europe, the modeled response is weaker, with anomalies of about <inline-formula><mml:math id="M17" display="inline"><mml:mrow><mml:mo>±</mml:mo><mml:mn mathvariant="normal">2</mml:mn></mml:mrow></mml:math></inline-formula> <inline-formula><mml:math id="M18" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">W</mml:mi><mml:mspace linebreak="nobreak" width="0.125em"/><mml:msup><mml:mi mathvariant="normal">m</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>, and negative PDO phases are associated with reduced atmospheric shortwave reflectivity. However, the signal is strongest in spatially aggregated averages and is difficult to distinguish from atmospheric noise over most of Europe, so its relevance for the Baltic Sea region remains uncertain <xref ref-type="bibr" rid="bib1.bibx40" id="paren.183"/>.</p>
</sec>
</sec>
</sec>
<sec id="Ch1.S3">
  <label>3</label><title>Biogeochemistry</title>
<sec id="Ch1.S3.SS1">
  <label>3.1</label><title>Main biogeochemical processes</title>
      <p id="d2e1718">Although the biogeochemical functioning of the Baltic Sea system has been widely investigated – an extensive review is given by <xref ref-type="bibr" rid="bib1.bibx144" id="paren.184"/> – its modulation by the large-scale circulation variability remains understudied. As a first step towards linking biogeochemical processes to large-scale circulation patterns, we focus on three major biogeochemical processes, namely deoxygenation, primary productivity and ocean acidification in the Baltic Sea <xref ref-type="bibr" rid="bib1.bibx190 bib1.bibx144 bib1.bibx288" id="paren.185"><named-content content-type="pre">e.g.,</named-content></xref>. During the last decades, all three processes have undergone major changes primarily driven by regional pressures, in particular eutrophication. Here, however, we focus on the potential links between large-scale circulation variability and local biogeochemical functioning on different time scales. We start by briefly introducing the three key biogeochemical processes.</p>
<sec id="Ch1.S3.SS1.SSS1">
  <label>3.1.1</label><title>Deoxygenation</title>
      <p id="d2e1736">Oxygen concentrations in surface waters are determined by the exchange with the atmosphere, oxygen production during photosynthesis, sea surface temperatures, sea surface salinity and the supply of oxygen through vertical and lateral transport. Surface oxygen is then distributed to the rest of the water column. In the Baltic Sea, mechanisms controlling oxygenation in the interior differ per subbasin (hereafter following the subbasin names of Savchuk, 2018), largely depending on the presence/absence of a permanent halocline.</p>
      <p id="d2e1739">In the central and western Baltic Proper, below its permanent halocline, oxygen levels are controlled by MBIs, smaller inflows (both are often referred to as “intrusions” of oxygen-rich waters) <xref ref-type="bibr" rid="bib1.bibx198 bib1.bibx196 bib1.bibx186 bib1.bibx108 bib1.bibx11 bib1.bibx14" id="paren.186"><named-content content-type="pre">e.g.,</named-content></xref>, vertical mixing <xref ref-type="bibr" rid="bib1.bibx238" id="paren.187"><named-content content-type="pre">e.g.,</named-content></xref>, and oxygen consumption due to organic matter degradation. The latter is related to the temperature-dependent remineralization in both the water column and the sediments, and the supply of degradable organic matter <xref ref-type="bibr" rid="bib1.bibx168 bib1.bibx151 bib1.bibx255 bib1.bibx27" id="paren.188"><named-content content-type="pre">e.g.,</named-content></xref>. Only large MBIs can ventilate the deeper parts of the central and western Baltic Proper <xref ref-type="bibr" rid="bib1.bibx145 bib1.bibx181" id="paren.189"/>. These subbasins are therefore prone to develop permanent bottom anoxia which has spread due to the rise of anthropogenic nutrient loads in the 1960s (Fig. <xref ref-type="fig" rid="F6"/>).</p>

      <fig id="F6" specific-use="star"><label>Figure 6</label><caption><p id="d2e1764"><bold>(a)</bold> Observed oxygen concentrations in intermediate and bottom waters at BY15 (in the Baltic Proper) for the period 1960 to 2023, where <inline-formula><mml:math id="M19" 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">S</mml:mi></mml:mrow></mml:math></inline-formula> concentrations were converted to negative oxygen equivalent (<inline-formula><mml:math id="M20" display="inline"><mml:mrow><mml:mn mathvariant="normal">1</mml:mn><mml:mo>[</mml:mo><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">S</mml:mi></mml:mrow><mml:mspace width="0.33em" linebreak="nobreak"/><mml:mo>(</mml:mo><mml:mrow class="chem"><mml:mi mathvariant="normal">mL</mml:mi><mml:mspace width="0.125em" linebreak="nobreak"/><mml:msup><mml:mi mathvariant="normal">L</mml:mi><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:mrow><mml:mo>)</mml:mo><mml:mo>]</mml:mo><mml:mo>=</mml:mo><mml:mo>-</mml:mo><mml:mn mathvariant="normal">2</mml:mn><mml:mo>[</mml:mo><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">O</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow><mml:mspace width="0.33em" linebreak="nobreak"/><mml:mo>(</mml:mo><mml:mrow class="unit"><mml:mi mathvariant="normal">mL</mml:mi><mml:mspace linebreak="nobreak" width="0.125em"/><mml:msup><mml:mi mathvariant="normal">L</mml:mi><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:mrow><mml:mo>)</mml:mo><mml:mo>]</mml:mo></mml:mrow></mml:math></inline-formula>). <bold>(b)</bold> Areal extent of anoxic (<inline-formula><mml:math id="M21" display="inline"><mml:mrow><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">O</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow><mml:mo>&lt;</mml:mo><mml:mn mathvariant="normal">0</mml:mn><mml:mspace linebreak="nobreak" width="0.125em"/><mml:mrow class="unit"><mml:mi mathvariant="normal">mL</mml:mi><mml:mspace linebreak="nobreak" width="0.125em"/><mml:msup><mml:mi mathvariant="normal">L</mml:mi><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:mrow></mml:mrow></mml:math></inline-formula>) and hypoxic (<inline-formula><mml:math id="M22" display="inline"><mml:mrow><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">O</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow><mml:mo>&lt;</mml:mo><mml:mn mathvariant="normal">2</mml:mn><mml:mspace linebreak="nobreak" width="0.125em"/><mml:mrow class="unit"><mml:mi mathvariant="normal">mL</mml:mi><mml:mspace width="0.125em" linebreak="nobreak"/><mml:msup><mml:mi mathvariant="normal">L</mml:mi><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:mrow></mml:mrow></mml:math></inline-formula>) conditions in the central Baltic Sea (Baltic Proper, Gulf of Finland and Gulf of Riga) from 1960 to 2023 estimated from observations <xref ref-type="bibr" rid="bib1.bibx95" id="paren.190"><named-content content-type="pre">adapted from</named-content></xref>. <bold>(c)</bold> Maps showing the extent of hypoxic and anoxic waters for the years 1906 and 2023, adapted from <xref ref-type="bibr" rid="bib1.bibx34" id="text.191"/> and Hansson and Viktorsson (2024).</p></caption>
            <graphic xlink:href="https://esd.copernicus.org/articles/17/415/2026/esd-17-415-2026-f06.png"/>

          </fig>

      <p id="d2e1933">The basins without permanent halocline, such as the eastern Gulf of Finland, Gulf of Bothnia, and Gulf of Riga, are largely impacted by atmospheric conditions which control the local stratification/mixing regime <xref ref-type="bibr" rid="bib1.bibx146 bib1.bibx64 bib1.bibx272 bib1.bibx162 bib1.bibx232" id="paren.192"/>. These basins are generally more oxygenated, but are not exempt from developing prolonged periods of deoxygenation and bottom anoxia.</p>
      <p id="d2e1939">Coastal deoxygenation in the Baltic Sea is also affected by additional processes, such as marine heat waves (MHWs; Sect. <xref ref-type="sec" rid="Ch1.S2.SS3.SSS4"/>) <xref ref-type="bibr" rid="bib1.bibx251" id="paren.193"/>. The gradual decline of oxygen, the expansion (both vertically and horizontally) of oxygen deficit, and the increasing hydrogen sulfide inventory adding to the “oxygen debt” in the Baltic Proper (Fig. <xref ref-type="fig" rid="F6"/>) increase the risk of exporting hypoxic waters to the Bothnian Sea and shallow coastal areas <xref ref-type="bibr" rid="bib1.bibx244 bib1.bibx231" id="paren.194"/>.</p>
</sec>
<sec id="Ch1.S3.SS1.SSS2">
  <label>3.1.2</label><title>Primary Productivity</title>
      <p id="d2e1960">Primary productivity – the rate at which marine autotrophs, mainly phytoplankton, convert inorganic carbon (<inline-formula><mml:math id="M23" 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>) into organic matter through photosynthesis – is heterogeneous in space and consistently enhanced by nutrient inputs in the Baltic Sea (Fig. <xref ref-type="fig" rid="F7"/>). The high nutrient concentrations result from human-induced nutrient enrichment, long water residence times due to limited exchange with the North Sea, vertical mixing, and efficient benthic nutrient recycling <xref ref-type="bibr" rid="bib1.bibx34 bib1.bibx33" id="paren.195"><named-content content-type="pre">e.g.,</named-content></xref>.</p>

      <fig id="F7" specific-use="star"><label>Figure 7</label><caption><p id="d2e1983">Primary productivity (PP) in the Baltic Sea: <bold>(a)</bold> Daily PP of the Baltic Sea, the mean from the period of 2010–2019. The numbers represent mean values determined for the analyzed basins: the Bornholm Basin, the Eastern Gotland Basin (EGB), the Gdańsk Basin and for the entire Baltic Sea. <bold>(b)</bold> Anomalies of the Baltic Sea primary production determined as the difference between PP in 2019 and the average PP value from 2010 to 2019. The total yearly primary production for <bold>(c)</bold> the entire Baltic Sea and the Bornholm Basin and <bold>(d)</bold> the Eastern Gotland Basin and the Gdańsk Basin together with the trend line; determined based on the monthly means for particular years for the period 2010–2019 (data source: SatBałtyk System) <xref ref-type="bibr" rid="bib1.bibx219" id="paren.196"/>.</p></caption>
            <graphic xlink:href="https://esd.copernicus.org/articles/17/415/2026/esd-17-415-2026-f07.jpg"/>

          </fig>

      <p id="d2e2007">Natural fluctuations in nutrient and organic matter supply, closely linked to the hydrological cycle, regulate primary productivity. Other physical factors, such as the availability of incoming surface solar radiation, the penetration of light into the water column, the spectral quality of light in the euphotic zone, changes in freshwater supply, ocean mixing, sea surface temperature, and winds, likewise play a role in primary production. While the averaged primary productivity shows consistent patterns (an example for the period 2010–2019 is shown in Fig. <xref ref-type="fig" rid="F7"/>a), significant differences can be found from year-to-year and from region to region. For example, anomaly analysis shows considerably elevated productivity in relation to the 10 year average in the Baltic Proper in 2019 <xref ref-type="bibr" rid="bib1.bibx219" id="paren.197"><named-content content-type="pre">Fig. <xref ref-type="fig" rid="F7"/>b;</named-content></xref>.</p>
      <p id="d2e2020">Since phytoplankton forms the dominant group of primary producers in the Baltic Sea, its growth directly reflects the combined effects of the aforementioned drivers. Light availability, which is further decreased by the presence of organic particles in the water column, is the main limiting factor for phytoplankton growth during autumn in the Baltic Sea <xref ref-type="bibr" rid="bib1.bibx209" id="paren.198"/>. In contrast, during spring and summer, light is not a limiting factor and allows phytoplankton growth, leading to seasonal peaks in primary production. While yearly primary production in the Baltic Sea shows a general slight increasing trend due to the response of phytoplankton to local drivers, primary productivity trends differ per basin <xref ref-type="bibr" rid="bib1.bibx219" id="paren.199"><named-content content-type="pre">Fig. <xref ref-type="fig" rid="F7"/>c and d;</named-content></xref>.</p>
      <p id="d2e2033">In winter, both temperature and light limit phytoplankton growth. In summer, thermal stratification is an additional factor regulating production dynamics as it forms a stable upper mixed layer that is shallower than the euphotic zone. Phytoplankton is then confined within this lighted surface layer allowing blooms to develop. However, stratification also suppresses mixing with deeper layers, gradually limiting the upward transport of nutrients to the surface and thus phytoplankton growth. Nitrate is usually fully depleted down to the halocline after the spring bloom period <xref ref-type="bibr" rid="bib1.bibx263" id="paren.200"/>. A second bloom of nitrogen-fixing primary producers (cyanobacteria) develops in summer, with timing of the onset and intensity subject to large interannual variability <xref ref-type="bibr" rid="bib1.bibx126 bib1.bibx127" id="paren.201"/>.</p>
      <p id="d2e2042">In early spring, diatoms – a major group of phytoplankton characterized by their capacity of building silica-based cell walls – are the first to bloom, particularly in the southern Baltic Sea. In the central Baltic Sea (Baltic Proper, Gulf of Finland and Gulf of Riga), cold-water dinoflagellates may be dominant, especially after warmer winters, while mixotrophic dinoflagellates and occasionally ciliates are dominant in summer <xref ref-type="bibr" rid="bib1.bibx135" id="paren.202"><named-content content-type="pre">e.g.,</named-content></xref>. Cyanobacteria in the Baltic Sea, which grow in low salinity (<inline-formula><mml:math id="M24" display="inline"><mml:mrow><mml:mo>&lt;</mml:mo><mml:mn mathvariant="normal">10</mml:mn></mml:mrow></mml:math></inline-formula> <inline-formula><mml:math id="M25" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">g</mml:mi><mml:mspace linebreak="nobreak" width="0.125em"/><mml:msup><mml:mi mathvariant="normal">kg</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>; <xref ref-type="bibr" rid="bib1.bibx204" id="altparen.203"/>) and are capable of fixing atmospheric nitrogen, form blooms in summer after nitrogen depletion in surface waters <xref ref-type="bibr" rid="bib1.bibx292 bib1.bibx293 bib1.bibx135 bib1.bibx210" id="paren.204"/>. However, phytoplankton dynamics in the Baltic Sea are changing, potentially due to changing seasonality of the cumulative surface incoming solar radiation <xref ref-type="bibr" rid="bib1.bibx124" id="paren.205"/>, reduced light penetration in the water column (so-called darkening), water temperatures and stratification <xref ref-type="bibr" rid="bib1.bibx113 bib1.bibx58 bib1.bibx214 bib1.bibx294" id="paren.206"/>.</p>
</sec>
<sec id="Ch1.S3.SS1.SSS3">
  <label>3.1.3</label><title>Ocean acidification</title>
      <p id="d2e2098">Ocean acidification is a core indicator of the Global Climate Observing System, as rising surface-ocean <inline-formula><mml:math id="M26" 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> partial pressure (<inline-formula><mml:math id="M27" display="inline"><mml:mrow><mml:mi>p</mml:mi><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:mrow></mml:math></inline-formula>) levels closely track rising atmospheric <inline-formula><mml:math id="M28" display="inline"><mml:mrow><mml:mi>p</mml:mi><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:mrow></mml:math></inline-formula>. When <inline-formula><mml:math id="M29" 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> dissolves in seawater, it forms carbonic acid, releases hydrogen ions (<inline-formula><mml:math id="M30" display="inline"><mml:mrow class="chem"><mml:msup><mml:mi mathvariant="normal">H</mml:mi><mml:mo>+</mml:mo></mml:msup></mml:mrow></mml:math></inline-formula>), and lowers pH <xref ref-type="bibr" rid="bib1.bibx56 bib1.bibx18" id="paren.207"><named-content content-type="pre">e.g.,</named-content></xref>. In the open ocean, ocean acidification is traceable as a decreasing long-term pH trend since at least the 1980s (i.e., since observations have been available), clearly revealing against the background of seasonal pH variability related to photosynthesis and respiration  <xref ref-type="bibr" rid="bib1.bibx174" id="paren.208"/>. In the Baltic Sea (similar to most coastal and shelf waters), ocean acidification trends are less clear (Fig. <xref ref-type="fig" rid="F8"/>), mainly due to changes related to eutrophication and variable total alkalinity which, next to <inline-formula><mml:math id="M31" 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> dynamics, is a key driver for seawater pH <xref ref-type="bibr" rid="bib1.bibx33 bib1.bibx144" id="paren.209"/>.</p>

      <fig id="F8" specific-use="star"><label>Figure 8</label><caption><p id="d2e2189"><bold>(a)</bold> Long-term spatial distribution of pH in surface waters in the Baltic Sea showing the long-term mean over the period of 1911–2003 <xref ref-type="bibr" rid="bib1.bibx98" id="paren.210"/>. <bold>(b)</bold> The rate of total alkalinity (TA) increases in surface waters of 4 different basins in the Baltic Sea, averaged over the period 1995 to 2021 (colored dots). The black line represents a third order polynomial regression <xref ref-type="bibr" rid="bib1.bibx44" id="paren.211"/>. <bold>(c)</bold> Changes of pH with time in 4 basins of the Baltic Sea (from <xref ref-type="bibr" rid="bib1.bibx144" id="altparen.212"/>, based on <xref ref-type="bibr" rid="bib1.bibx33" id="altparen.213"/>). <bold>(d)</bold> Monthly profiles of pH and oxygen in the Gotland Basin  during 2008 (after <xref ref-type="bibr" rid="bib1.bibx281" id="altparen.214"/>). Negative oxygen values show how much oxygen would be required to reoxidize the hydrogen sulphide to sulphate.</p></caption>
            <graphic xlink:href="https://esd.copernicus.org/articles/17/415/2026/esd-17-415-2026-f08.png"/>

          </fig>

      <p id="d2e2225">Total alkalinity is defined as an excess of proton acceptors over proton donors (or bases over acids) and is a measure of buffer capacity against ocean acidification <xref ref-type="bibr" rid="bib1.bibx52" id="paren.215"/>. Although total alkalinity is a conservative salinity-dependent parameter, its surface distribution in the Baltic Sea is complex. This is due to significant differences in the total alkalinity concentrations in river water across the Baltic Sea catchment, a phenomenon closely linked to variations in the geological structure of the surrounding land <xref ref-type="bibr" rid="bib1.bibx92 bib1.bibx143" id="paren.216"/>. Generally, the Scandinavian rivers drain catchments underlain by granite bedrock and therefore have low total alkalinity concentrations. Rivers entering the Baltic Sea from the south and south-east flow through a catchment area rich in limestone and heavily agriculturally transformed, which makes these rivers an important net source of total alkalinity. Finally, the Baltic Proper acts as a mixing chamber where these various freshwater types mix with the salty (and therefore alkalinity-rich) water flowing into the Baltic from the North Sea <xref ref-type="bibr" rid="bib1.bibx144" id="paren.217"/>.</p>
      <p id="d2e2238">The overall low alkalinity suggests that the Baltic Sea is prone to ocean acidification. However, total alkalinity in the Baltic Sea has shown an increase over the past three decades <xref ref-type="bibr" rid="bib1.bibx201" id="paren.218"/>. The most recent data analysis by <xref ref-type="bibr" rid="bib1.bibx44" id="text.219"/> shows that this increase is  between 3.2 <inline-formula><mml:math id="M32" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">µ</mml:mi><mml:mi mathvariant="normal">mol</mml:mi><mml:mspace width="0.125em" linebreak="nobreak"/><mml:msup><mml:mi mathvariant="normal">kg</mml:mi><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup><mml:mspace linebreak="nobreak" width="0.125em"/><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> in the Gulf of Bothnia and 5.3 <inline-formula><mml:math id="M33" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">µ</mml:mi><mml:mi mathvariant="normal">mol</mml:mi><mml:mspace linebreak="nobreak" width="0.125em"/><mml:msup><mml:mi mathvariant="normal">kg</mml:mi><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup><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> in the Bornholm Basin, which partially mitigates the pH drop in the Baltic Sea due to increasing <inline-formula><mml:math id="M34" display="inline"><mml:mrow><mml:mi>p</mml:mi><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:mrow></mml:math></inline-formula> (Fig. <xref ref-type="fig" rid="F8"/>b). The source of this increase remains unclear, but it is likely the result of a combination of different processes, such as a rise in total alkalinity loads from rivers, enhanced erosion, dissolution of carbonate deposits, and total alkalinity input due to the expansion of bottom anoxia and low redox conditions <xref ref-type="bibr" rid="bib1.bibx201 bib1.bibx89 bib1.bibx289" id="paren.220"/>.</p>
      <p id="d2e2323">Because both <inline-formula><mml:math id="M35" display="inline"><mml:mrow><mml:mi>p</mml:mi><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:mrow></mml:math></inline-formula> and total alkalinity are key parameters to understand pH variability and ocean acidification, any processes and mechanisms affecting either of them should be considered in the context of teleconnections. This makes correlations between acidification and natural variability, large-scale atmospheric, and oceanic patterns difficult to detect in the Baltic Sea, leaving the response to changes across different time scales poorly understood.</p>
</sec>
</sec>
<sec id="Ch1.S3.SS2">
  <label>3.2</label><title>Linkages between large-scale circulation patterns, physical drivers and biogeochemical processes across time scales</title>
      <p id="d2e2349">While dedicated studies assessing the effects of large-scale circulation variability on biogeochemical processes in the Baltic Sea are rare (see <xref ref-type="bibr" rid="bib1.bibx206" id="altparen.221"/> and references therein), important links – often local – between biogeochemical and physical processes have been suggested in the literature. One example assessing the relative roles of physical parameters in modulating a biogeochemical parameter across different time scales is that of <xref ref-type="bibr" rid="bib1.bibx126" id="text.222"/>. Using Partial Least Squares analysis, they show that, in addition to biogeochemical properties (such as nutrient inputs), the temperature is a key driver for surface cyanobacteria accumulation (FCA) on decadal time scales (with <inline-formula><mml:math id="M36" display="inline"><mml:mrow><mml:msup><mml:mi>R</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msup><mml:mo>&gt;</mml:mo><mml:mn mathvariant="normal">0.2</mml:mn></mml:mrow></mml:math></inline-formula>). They also identify temperature, solar radiation and wind as major contributors on interannual time scales (Fig. <xref ref-type="fig" rid="F9"/>). The occurrence and development of cyanobacterial blooms are thus among the few examples in the field of biogeochemistry where attempts have been made to explain natural variability on different time scales through physical drivers.</p>

      <fig id="F9"><label>Figure 9</label><caption><p id="d2e2377">Influence of various environmental factors on cyanobacteria surface accumulations (FCA) expressed as coefficient of determination (<inline-formula><mml:math id="M37" display="inline"><mml:mrow><mml:msup><mml:mi>R</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msup></mml:mrow></mml:math></inline-formula>) on decadal (blue) and interannual (orange) time scales for the central Baltic Proper. The environmental categories include sea surface temperature derived from satellite (sat T) and measured in situ (In situ T) for 0 to 15 m, surface incoming shortwave radiation (Solar), various biogeochemical properties (BGC) and wind (Wind). Error bars highlight the variability within each category. The figure is adapted from <xref ref-type="bibr" rid="bib1.bibx126" id="text.223"/>.</p></caption>
          <graphic xlink:href="https://esd.copernicus.org/articles/17/415/2026/esd-17-415-2026-f09.png"/>

        </fig>

      <p id="d2e2400">In this section, we present a synthesis and analysis from relevant information found in the literature on how remote and local physical processes drive natural variability in deoxygenation, primary productivity, and ocean acidification, classifying their potential impacts across the time scales defined in Sect. <xref ref-type="sec" rid="Ch1.S2.SS2"/>.</p>
<sec id="Ch1.S3.SS2.SSS1">
  <label>3.2.1</label><title>Synoptic, intraseasonal and seasonal time scales</title>
      <p id="d2e2413">Most of the available biogeochemical observational data do not cover long-term periods with the time resolution to capture synoptic (1–7 d) and intraseasonal (10–90 d) time scales. In addition, atmospheric or oceanic data do not always have the same period, the same frequency or spatial coverage. Only due to the recent availability of satellite observations together with improved measurement techniques and numerical modeling has it become possible to obtain biogeochemical data with higher spatiotemporal resolution. Therefore, it is not surprising that biogeochemical parameters are not typically linked to weather systems on synoptic or intraseasonal time scales. However, the need for early warnings and short-term predictions for biogeochemical parameters (e.g., for risk assessments) demands more studies on the biogeochemistry responses to weather regimes or short-term events like storms.</p>
      <p id="d2e2416">A study by Post and Aun (2024) about solar radiation on synoptic time scales (Sect. <xref ref-type="sec" rid="Ch1.S2.SS3.SSS7"/>) potentially explains the observed earlier onset of phytoplankton growth reported for the Baltic Sea (see Sect. 3.1.2). <xref ref-type="bibr" rid="bib1.bibx127" id="text.224"/> recently suggested that the main controlling factors for the initiation of cyanobacteria blooms are the rate of change in SST due to surface irradiance and reduced vertical mixing due to lower wind speed, while SST itself was not correlated with bloom initiation. Similarly, <xref ref-type="bibr" rid="bib1.bibx202" id="text.225"/> observed the vertical carbon removal from the surface layer during a cyanobacterial event, and related the integrated cyanobacterial production to the heat uptake in the surface layer. Increased wind speed and resulting mixed layer deepening ended this productive episode. These findings link both the onset of cyanobacterial blooms and integrated production of individual bloom events to meteorological conditions with persistent low wind speed and reduced cloud cover. This parallels conditions fostering summer heat waves, with an apparent link to blocking regimes (Sect. <xref ref-type="sec" rid="Ch1.S2.SS1.SSS2"/>). Yet, for the most part, a clear correlation between phytoplankton variability and weather regimes is still missing.</p>
      <p id="d2e2429">The shallow and brackish Baltic Sea is affected by marine heat waves (MHWs) on synoptic time scales (Sect. <xref ref-type="sec" rid="Ch1.S2.SS3.SSS4"/>). Their impact can last from a couple of days to a few months and can reach the seabed at water depths of less than 20 m <xref ref-type="bibr" rid="bib1.bibx32" id="paren.226"/>, which has been shown to have led to a significant decrease in oxygen concentration during summer <xref ref-type="bibr" rid="bib1.bibx251 bib1.bibx76 bib1.bibx283" id="paren.227"/>. As MHWs are projected to increase in intensity, duration and frequency in the future <xref ref-type="bibr" rid="bib1.bibx85" id="paren.228"/>, the risk of hypoxic events in Baltic coastal waters is of growing concern <xref ref-type="bibr" rid="bib1.bibx251 bib1.bibx133 bib1.bibx162" id="paren.229"/>. <xref ref-type="bibr" rid="bib1.bibx126" id="text.230"/> suggested that MHWs can trigger extreme surface accumulations of cyanobacteria which, in turn, will further increase heating in the uppermost water layer due to increased light absorption and thus modulated air-sea heat fluxes. <xref ref-type="bibr" rid="bib1.bibx133" id="text.231"/> studied the effect of MHWs on benthic ecosystems in the Baltic Sea and found that the seafloor functioning responds differently depending on the intensity of the heatwave. They suggest that a prolonged, moderate MHW enhances nutrient recycling by boosting benthic activity, while a strong heatwave reduces organic matter degradation and the nutrient cycling. Over time, both can lead to a build-up of organic matter on the seafloor and cause oxygen depletion <xref ref-type="bibr" rid="bib1.bibx133" id="paren.232"/>. As bioturbation and related benthic fluxes alter the nutrient recycling and organic matter remineralization, benthic processes can also alter primary productivity.</p>
      <p id="d2e2456">Most physical parameters in the Baltic Sea, such as temperature, wind speed, cloudiness, runoff, evaporation, and precipitation have pronounced intraseasonal/seasonal variations, whose influence decreases with depth according to the bathymetry of each basin. Consequently, such signals are also reflected in most biogeochemical processes, but can be mitigated by other regional effects. For example, while intraseasonal/seasonal variations in oxygen are weak in most of the stratified areas of the Baltic Sea <xref ref-type="bibr" rid="bib1.bibx271" id="paren.233"/>, in the Gulf of Finland, bottom water conditions are dominated by seasonal variability as seasonal westerly winds can reverse the estuarine circulation, which deepens the halocline and increases the oxygen content in the near-bottom layer <xref ref-type="bibr" rid="bib1.bibx62 bib1.bibx161 bib1.bibx166" id="paren.234"/>.</p>
      <p id="d2e2466">Primary productivity in the entire Baltic Sea has a clear seasonal cycle mainly driven by temperature, light and nutrient availability (Sect. <xref ref-type="sec" rid="Ch1.S3.SS1.SSS2"/>). Following changes in <inline-formula><mml:math id="M38" display="inline"><mml:mrow><mml:mi>p</mml:mi><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:mrow></mml:math></inline-formula> caused by seasonal changes in the production and remineralization of organic matter, the pH of the Baltic surface waters also changes seasonally, with higher values observed in summer than in winter. Thus, natural variability of ocean acidification is closely related to that of primary production, but also to the buffering capacity, given by the total alkalinity. In addition, the <inline-formula><mml:math id="M39" 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> flux at the air-sea interface is largely controlled by temperature, salinity and winds <xref ref-type="bibr" rid="bib1.bibx278 bib1.bibx277" id="paren.235"/>, which are directly impacted by the large-scale atmospheric variability across different time scales (Sect. <xref ref-type="sec" rid="Ch1.S2.SS2"/>). In deeper waters, the seasonal influence of teleconnections is less evident but may follow that of deoxygenation (Fig. <xref ref-type="fig" rid="F6"/>), since pH is primarily controlled by <inline-formula><mml:math id="M40" 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> accumulation and alkalinity release during redox processes <xref ref-type="bibr" rid="bib1.bibx143" id="paren.236"/>. In the end, all of these processes are linked to seasonally affected physical parameters. The relative roles of such parameters in controlling the intraseasonal to seasonal variability of primary production and ocean acidification remain unclear and likely vary regionally.</p>
</sec>
<sec id="Ch1.S3.SS2.SSS2">
  <label>3.2.2</label><title>Interannual time scales</title>
      <p id="d2e2527">Interannual variability (1–9 years) in Baltic Sea oxygen deficiency is strongly driven by atmospheric forcing through its effects on circulation, stratification, and vertical exchange, leading to changes in oxygen content.</p>
      <p id="d2e2530">Interannual variability below the halocline in the western and southern Baltic depends largely on the inflow of oxygenated water from the North Sea <xref ref-type="bibr" rid="bib1.bibx261 bib1.bibx14 bib1.bibx170" id="paren.237"/>. In between MBI events, oxygen concentrations in the near bottom layer decline continuously although the frequent smaller inflows <xref ref-type="bibr" rid="bib1.bibx61 bib1.bibx189" id="paren.238"/> oxygenate the subhalocline layer (<inline-formula><mml:math id="M41" display="inline"><mml:mrow><mml:mo>≈</mml:mo><mml:mn mathvariant="normal">100</mml:mn></mml:mrow></mml:math></inline-formula> m depth) at an interannual time scale. Consequently, year-to-year variability in the subhalocline layer is more closely linked to the large-scale atmospheric circulation than the deeper bottom layers in the central Baltic Sea.</p>
      <p id="d2e2549">The influence of atmospheric variability is particularly pronounced in the shallower basins of the Baltic Sea. A positive NAO with accompanying winds from southwest can alter or even reverse the advection of oxygen-depleted saline waters from the Baltic Proper to the Gulf of Finland and remove hypoxia in the whole gulf <xref ref-type="bibr" rid="bib1.bibx64 bib1.bibx161 bib1.bibx166 bib1.bibx157" id="paren.239"/>. A negative NAO, on the other hand, supports estuarine circulation and stronger oxygen deficiency. <xref ref-type="bibr" rid="bib1.bibx159" id="text.240"/> and <xref ref-type="bibr" rid="bib1.bibx100" id="text.241"/> showed that oxygen depletion  in the case of a warmer upper layer is not  only intensified due to stronger stratification, but that enhanced oxygen consumption in higher temperatures also contributes to the interannual variability of deoxygenation in the shallow southern Baltic Sea.</p>
      <p id="d2e2561">Wind patterns and heat fluxes associated with high pressure systems during the European Blocking regime support the seasonal oxygen depletion occurring from year-to-year in the Gulf of Riga <xref ref-type="bibr" rid="bib1.bibx162 bib1.bibx272" id="paren.242"/>. North-easterly winds cause dense water transport from the Baltic Proper to the Gulf of Riga. Although this water is oxygenated, it also causes strong stratification and reduces oxygen transport by vertical mixing in the gulf. Strong heat fluxes during the prevailing European Blocking regime cause higher sea surface temperature and stratification, which could reduce downward oxygen transport and enhance deoxygenation of the deep layer <xref ref-type="bibr" rid="bib1.bibx272" id="paren.243"/>.</p>
      <p id="d2e2572">Besides low oxygen concentrations, seasonally increasing near-bottom water temperature seems to be the main factor controlling denitrification rates <xref ref-type="bibr" rid="bib1.bibx3" id="paren.244"/>. In turn, intensive denitrification and organic matter degradation under anoxic conditions are an important source of alkalinity and thus can affect the year-to-year acid-base system of the Baltic Proper <xref ref-type="bibr" rid="bib1.bibx88" id="paren.245"/>. Although the effect is usually reversed upon re-oxygenation, denitrification and the formation of vivianite and pyrite are permanent sources of alkalinity <xref ref-type="bibr" rid="bib1.bibx143" id="paren.246"/>, potentially acting on longer time scales.</p>
      <p id="d2e2584">During 1860–1880 and 1980–2000, negative wavelet coherence between surface and bottom salinity at Gotland Deep and the NAO index is found in the period band between 5 and 10 years <xref ref-type="bibr" rid="bib1.bibx236" id="paren.247"/>, very likely affecting bottom oxygen concentration dynamics <xref ref-type="bibr" rid="bib1.bibx156" id="paren.248"><named-content content-type="pre">e.g.,</named-content></xref>. <xref ref-type="bibr" rid="bib1.bibx271" id="text.249"/> found strong correlation between the positive phase of winter NAO and negative salinity and positive oxygen anomalies in the Baltic Proper during the period 1983 to 1990. This suggest that the positive phase of winter NAO (west wind anomaly) causes a salinity decline in the Gotland Basin and improved oxygen conditions. The mechanism is explained by <xref ref-type="bibr" rid="bib1.bibx142" id="text.250"/> and confirmed by dynamic modeling <xref ref-type="bibr" rid="bib1.bibx184" id="paren.251"/> and statistics (Zorita and Laine, 2000). Correlations between the NAO and the main factors controlling primary productivity, such as air/sea surface temperature, light and sea ice at interannual time scales are large (Sect. <xref ref-type="sec" rid="Ch1.S2.SS3"/>; <xref ref-type="bibr" rid="bib1.bibx213 bib1.bibx137" id="altparen.252"/>). Therefore, strong interannual signals are expected to modulate primary productivity in the Baltic Sea. Indeed, a study on primary productivity in the northeastern Baltic Sea and large-scale atmospheric variability found significant correlations between chlorophyll and the winter values of NAO, Scandinavian pattern and the annual Polar/Eurasian index, which suggests a potential effect on primary productivity <xref ref-type="bibr" rid="bib1.bibx77" id="paren.253"/>. Solar radiation has been shown to affect cyanobacteria on interannual time scales rather than on decadal time scales. Wind conditions did not show a strong relationship with how often cyanobacteria blooms occurred, although winds mainly influenced variations from year-to-year <xref ref-type="bibr" rid="bib1.bibx126" id="paren.254"><named-content content-type="post">their Fig. <xref ref-type="fig" rid="F9"/></named-content></xref>.</p>
</sec>
<sec id="Ch1.S3.SS2.SSS3">
  <label>3.2.3</label><title>Decadal and multidecadal time scale</title>
      <p id="d2e2627">The Baltic Sea exhibits complex decadal to multidecadal-scale variability in oxygen dynamics, primary productivity and ocean acidification. By examining paleoenvironmental archives from sediment records, we can better understand shifts in core biogeochemical processes under conditions of no or minimal anthropogenic influence. Past widespread hypoxia in the Baltic Sea has occurred during the Holocene Thermal Maximum (8000–4800 years before present) and the Medieval Climate Anomaly (1000–700 years before present) <xref ref-type="bibr" rid="bib1.bibx309 bib1.bibx117 bib1.bibx27" id="paren.255"/>. These past hypoxic intervals generally coincided with warmer climatic conditions <xref ref-type="bibr" rid="bib1.bibx123" id="paren.256"/> and elevated salinity, both of which favored higher primary productivity and increased organic matter flux to the seafloor. Sediment record studies show that, before major human influence, hypoxia in the Baltic Sea was largely a natural response to climate variability and changes in water exchange with the North Sea <xref ref-type="bibr" rid="bib1.bibx42 bib1.bibx116" id="paren.257"/>.</p>
      <p id="d2e2639">Proxy records of hypoxia showed strong multidecadal oscillations likely driven by both the internal iron-phosphorus cycling and the Atlantic Multidecadal Variability (AMV) <xref ref-type="bibr" rid="bib1.bibx118" id="paren.258"/>, in which temperature and salinity played a major role in modulating the remineralization of organic matter <xref ref-type="bibr" rid="bib1.bibx27" id="paren.259"/> and the timing of massive blooms <xref ref-type="bibr" rid="bib1.bibx7" id="paren.260"/>. In addition, oxygen concentration variations at multidecadal time scales have been identified to be negatively correlated with salinity in the major part of the water column, indicating improved ventilation during a fresher state of the Baltic Sea <xref ref-type="bibr" rid="bib1.bibx94" id="paren.261"><named-content content-type="pre">e.g.,</named-content></xref>. Reduced salinity and consequent improved oxygen conditions have been linked to stronger zonal atmospheric circulation <xref ref-type="bibr" rid="bib1.bibx310" id="paren.262"/>.</p>
      <p id="d2e2659">Modern bottom oxygen concentrations in both the Baltic Proper and the western Gulf of Finland show strong decadal signals, mainly controlled by runoff and zonal wind stress <xref ref-type="bibr" rid="bib1.bibx284" id="paren.263"/>. Similarly, <xref ref-type="bibr" rid="bib1.bibx147" id="text.264"/> reported an increase in oxygen concentrations in the late 1980s and early 1990s which they attributed to a decrease in salinity due to high runoff and a loss of stratification, thus related to more humid weather conditions.</p>
      <p id="d2e2668">Primary production has fluctuated over a range of spatial and temporal scales, increasing approximately 2–3-fold since the early-to-mid 20th century as a direct result of nutrient enrichment <xref ref-type="bibr" rid="bib1.bibx255" id="paren.265"/>. However, multidecadal variability persists, superimposed on the anthropogenic trend. Model and field data show that wind forcing and shifts in atmospheric circulation play a crucial role in regulating primary production and biogeochemical regimes in the Baltic Sea <xref ref-type="bibr" rid="bib1.bibx5" id="paren.266"/>. For example, the AMV has been shown to account for a significant fraction (over 50 %) of decadal-scale variability in sea surface temperature in the Baltic Sea, indirectly influencing primary productivity through impacts on thermal stratification and nutrient availability <xref ref-type="bibr" rid="bib1.bibx136" id="paren.267"/>.</p>
      <p id="d2e2681">Paleoceanographic evidence demonstrates that during the Medieval Climate Anomaly, periods of warmer temperatures promoted abundant cyanobacteria blooms in the Baltic Sea <xref ref-type="bibr" rid="bib1.bibx73" id="paren.268"/> and increased diatom production, boosting organic matter export and contributing to hypoxia in deep basins <xref ref-type="bibr" rid="bib1.bibx20" id="paren.269"/>. Furthermore, significant changes have occurred in net primary productivity from 1993 to the present (Fig. <xref ref-type="fig" rid="F7"/>), which cannot solely be explained by nutrient distribution <xref ref-type="bibr" rid="bib1.bibx219" id="paren.270"/>. Still, nutrient loads from rivers, especially after industrialization, and nutrient recycling from sediments have become the dominant control on primary productivity <xref ref-type="bibr" rid="bib1.bibx255" id="paren.271"/>, amplifying and modulating its magnitude rather than overriding its natural, climate-driven variability.</p>
      <p id="d2e2698">Long-term trends and variations of primary productivity in the Baltic Sea are difficult to study due to the lack of observations in both space and time, especially before the year 1996 <xref ref-type="bibr" rid="bib1.bibx219" id="paren.272"/>. Nevertheless, long seasonal trends in primary productivity have been identified in the Baltic Sea, especially in the Gulf of Gdansk <xref ref-type="bibr" rid="bib1.bibx308" id="paren.273"><named-content content-type="pre">e.g.,</named-content></xref>. As large-scale temperature, shortwave radiation, and cloudiness changes have been shown to affect phytoplankton growth, large-scale circulation variability on multidecadal time scales likely impacts primary productivity.</p>
      <p id="d2e2709"><xref ref-type="bibr" rid="bib1.bibx126" id="text.274"/> showed that the frequency of cyanobacteria in the Baltic Proper at decadal time scales is primarily correlated with phosphorus abundance and bottom-water anoxia (Fig. <xref ref-type="fig" rid="F9"/>). However, sea surface temperature and wind speed also play a significant role in modulating decadal cyanobacteria blooms and their initiation <xref ref-type="bibr" rid="bib1.bibx125 bib1.bibx127" id="paren.275"/>. Yet, in the Baltic Sea, the links between large-scale circulation patterns and primary productivity remain poorly understood and largely unquantified; consequently, the relative importance of these links and the future response of productivity to accelerated warming are even less certain.</p>
      <p id="d2e2719">The recent multidecadal increase in total alkalinity has also been partially explained by changes in precipitation patterns and continental weathering driven by acidic rain <xref ref-type="bibr" rid="bib1.bibx201" id="paren.276"/> which are closely linked to the NAO and AMV (Sect. <xref ref-type="sec" rid="Ch1.S2.SS3.SSS1"/>). The latter are expected to change by the end of the 21st century, likely leading to wetter conditions in the northern part of the Baltic Sea, mostly composed of granite, and drier conditions in the southern, limestone-rich Baltic Sea <xref ref-type="bibr" rid="bib1.bibx188 bib1.bibx144" id="paren.277"/>. The sources of the alkalinity  increase are neither well understood nor quantified and are also highly linked to eutrophication and alkalinity production from anaerobic processes <xref ref-type="bibr" rid="bib1.bibx201 bib1.bibx44" id="paren.278"/>. The teleconnections for total alkalinity production through anaerobic processes, though not yet directly investigated, should be similar to those for primary production and hypoxia/anoxia.</p>
</sec>
</sec>
<sec id="Ch1.S3.SS3">
  <label>3.3</label><title>Large-scale circulation patterns and physical controls in key biogeochemical processes: Roles and knowledge gaps</title>
      <p id="d2e2742">Disentangling climate change from natural variability is essential for correctly attributing observed changes in the Earth system. Without separating internally generated fluctuations from externally forced trends, long-term shifts may be misinterpreted as short-term variability, or vice versa. Clear attribution improves projections, strengthens confidence in model simulations, and supports effective policy and management decisions by distinguishing persistent climate change-driven trends from temporary natural fluctuations. This is particularly valid for biogeochemical processes, as in the Baltic Sea achieving good environmental status is crucial and a priority in EU conventions. This requires up-to-date environmental information and improved predictability of key processes.</p>
      <p id="d2e2745">We have reviewed and gathered evidence from the literature linking the potential effects of large-scale circulation variability and local physical controls on three key biogeochemical processes. In this section, we synthesize relevant evidence from Sect. <xref ref-type="sec" rid="Ch1.S3.SS2"/>, placing it in the context of anthropogenic climate change and remaining knowledge gaps. We also identify, where possible, the relative roles and importance of remote and local physical controls for these biogeochemical processes. Our analysis, consistent with <xref ref-type="bibr" rid="bib1.bibx206" id="text.279"/>, shows that ecosystem dynamics are influenced not only by temperature and salinity, but by a broader range of atmospheric and oceanic drivers.</p>
      <p id="d2e2753">The main causes of the recent oxygen decline in the Baltic Sea are the anthropogenic nutrient load from land <xref ref-type="bibr" rid="bib1.bibx187" id="paren.280"/>, warming, and inflowing North Sea waters driven by climate change, which decreases oxygen solubility, increases mineralization rates and strengthens stratification <xref ref-type="bibr" rid="bib1.bibx12 bib1.bibx205 bib1.bibx231" id="paren.281"/>. However, the variability of oxygen is heavily modulated by regional effects of natural variability at different time scales (Sect. <xref ref-type="sec" rid="Ch1.S3.SS2"/>), but relative roles remain unclear.</p>
      <p id="d2e2764">The same is true for primary productivity. However, there are a number of uncertainties associated with changes in primary production. For example, the consequences of climate change <xref ref-type="bibr" rid="bib1.bibx288" id="paren.282"/> or possible shifts in species diversity, patterns of species succession or responses to changes in hydrological patterns are largely unknown <xref ref-type="bibr" rid="bib1.bibx288 bib1.bibx175 bib1.bibx308 bib1.bibx273 bib1.bibx219" id="paren.283"><named-content content-type="pre">e.g.,</named-content></xref>. Further changes affecting primary productivity in the Baltic Sea are expected to continue but the specific phytoplankton response to the combined complexity of physical drivers and the related time scales, especially the contribution of natural variability, remains understudied and difficult to detect. In addition, harmful algal blooms (such as blooms of the prymesiophyte Prymnesium polylepis; <xref ref-type="bibr" rid="bib1.bibx131" id="altparen.284"/>) are recurrent phenomena, especially along the coast and the Kattegat-Skagerrak. Most of the harmful (toxic) phytoplankton species only constitute a small fraction of the phytoplankton biomass. However, they affect the composition and the spatio-seasonal distribution of the phytoplankton community. Their drivers are complex and not well understood, but they are clearly impacted by weather conditions <xref ref-type="bibr" rid="bib1.bibx243" id="paren.285"/>. Because primary productivity forms the base of the marine food web, understanding its link to natural variability and large-scale patterns is important to better predict its future and implications.</p>
      <p id="d2e2782">In addition, there is growing concern over the ecological impacts of coastal ocean darkening <xref ref-type="bibr" rid="bib1.bibx214 bib1.bibx72 bib1.bibx47" id="paren.286"/>, given that some of the highest rates of darkening since 2003 have been recently observed in the Baltic Sea, in particular in the Gulf of Bothnia (Davies and Smyth, 2025). Climate change-driven alterations in precipitation, land use, and runoff are projected to intensify this darkening phenomenon through increased input of organic material and particulates, altering the penetration and spectral quality of light in the water column, with unknown consequences for photosynthesis, primary production, and species behavior <xref ref-type="bibr" rid="bib1.bibx58 bib1.bibx215" id="paren.287"/>. Identifying connections between North European precipitation patterns, temperature variability and decadal changes in underwater lightscapes is an emerging research topic.</p>
      <p id="d2e2791">Ocean acidification is the result of multiple combined drivers and there is still limited knowledge on several key processes and their relative contribution in the Baltic Sea. It is also poorly known how the ecosystems will respond to a combination of changing factors (e.g. nutrient loads, mixing/stagnation, and precipitation/evaporation), especially in the coastal ocean. <xref ref-type="bibr" rid="bib1.bibx98" id="text.288"/> identified as key priorities in future research to quantify the responses to dominant drivers (notably warming, eutrophication, hypoxia) and to determine the effects of diurnal and seasonal environmental fluctuations. In addition, to better understand the complex acid-base system of the Baltic Sea and its future, it is important to improve estimates of the relative contributions between seasonal/interannual and long-term atmospheric and hydrodynamic variability affecting carbon fixation rates, pH, and total alkalinity sinks and sources. Future research on this matter should at least include alterations in precipitation and runoff together with a good understanding of changes in the land use and in the rate of <inline-formula><mml:math id="M42" 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>-induced weathering of carbonate and silicate rocks.</p>
      <p id="d2e2808">A summary of confirmed remote and regional/local physical drivers directly affecting oxygen concentrations, primary productivity, and ocean acidification across the analyzed time scales is presented in Fig. <xref ref-type="fig" rid="F10"/>. All regional physical effects on natural variability mentioned in Sect. 2.3 affect in some way these three main biogeochemical processes. However, most of the impacts remain poorly constrained or quantified and are therefore difficult to accurately implement in models, hindering the possibility of reducing uncertainties. The temperature (including SST), salinity and ocean stratification are likely the major factors modulating natural variability of deoxygenation. While natural variability of primary productivity is also largely affected by temperature, solar radiation and wind regimes also play major roles, likely also in determining the timing of the blooms. Links between physical drivers and ocean acidification are complex and may be more indirect than for other processes. For example, variations in runoff directly affect the nutrient supply, the salinity distribution, and the alkalinity.</p>

      <fig id="F10" specific-use="star"><label>Figure 10</label><caption><p id="d2e2815">Simplified diagram summarizing identified connections between physical patterns and deoxygenation, primary productivity, and ocean acidification acting in the Baltic Sea across the time scales examined in this study. Arrows only show confirmed links from the literature that are addressed in Sect. <xref ref-type="sec" rid="Ch1.S3.SS2"/>. Potential (unconfirmed) links are not shown. <inline-formula><mml:math id="M43" display="inline"><mml:mi>P</mml:mi></mml:math></inline-formula>/<inline-formula><mml:math id="M44" display="inline"><mml:mi>E</mml:mi></mml:math></inline-formula>, <inline-formula><mml:math id="M45" display="inline"><mml:mi>S</mml:mi></mml:math></inline-formula>, <inline-formula><mml:math id="M46" display="inline"><mml:mi>T</mml:mi></mml:math></inline-formula> and OM denote precipitation/evaporation, salinity, temperature, and organic matter, respectively.</p></caption>
          <graphic xlink:href="https://esd.copernicus.org/articles/17/415/2026/esd-17-415-2026-f10.png"/>

        </fig>

</sec>
</sec>
<sec id="Ch1.S4" sec-type="conclusions">
  <label>4</label><title>Conclusions</title>
      <p id="d2e2863">The Baltic Sea is located at the confluence of Atlantic, Arctic and continental influences, with variability controlled primarily by large-scale atmospheric circulation over the North Atlantic-European sector, especially the North Atlantic jet and associated circulation patterns such as the NAO, East Atlantic, and Scandinavian patterns <xref ref-type="bibr" rid="bib1.bibx38 bib1.bibx41" id="paren.289"><named-content content-type="pre">e.g.,</named-content></xref>. Their impacts on the Baltic Sea region are substantial <xref ref-type="bibr" rid="bib1.bibx250" id="paren.290"><named-content content-type="pre">e.g.,</named-content></xref>. For example, in winter the NAO explains about 87 % of the surface air temperature variability at Stockholm <xref ref-type="bibr" rid="bib1.bibx184" id="paren.291"/>, accounts for about 29 % of the year-to-year variance in annual maximum Baltic Sea ice extent <xref ref-type="bibr" rid="bib1.bibx213" id="paren.292"/>, and correlates strongly with winter mean Baltic Sea level (<inline-formula><mml:math id="M47" display="inline"><mml:mrow><mml:mi>r</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">0.63</mml:mn></mml:mrow></mml:math></inline-formula> for 1825–1997 and <inline-formula><mml:math id="M48" display="inline"><mml:mrow><mml:mi>r</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">0.74</mml:mn></mml:mrow></mml:math></inline-formula> for 1902–1997; <xref ref-type="bibr" rid="bib1.bibx6" id="altparen.293"/>). On longer time scales, coupled ocean–atmosphere interactions linked to the AMOC, the SPG, and the AMV exert additional control <xref ref-type="bibr" rid="bib1.bibx9 bib1.bibx26 bib1.bibx305" id="paren.294"/>: for instance, about 58 % of decadal Baltic Sea SST variability has been linked to the AMV after removing the long-term warming trend <xref ref-type="bibr" rid="bib1.bibx137" id="paren.295"/>, and local winter SST responses can reach about 1.2 <inline-formula><mml:math id="M49" 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> per standard deviation of AMV-related multidecadal variability <xref ref-type="bibr" rid="bib1.bibx26" id="paren.296"/>. However, quantifying the effect of the NAO on the past and future climate of the Baltic Sea region remains a challenge <xref ref-type="bibr" rid="bib1.bibx111" id="paren.297"/>.</p>
      <p id="d2e2933">Across time scales, the literature uses different frameworks to describe large-scale circulation patterns and their variability, but many of these can be related to the weather-regime framework. For example, the Zonal and Greenland Blocking regimes are commonly interpreted as NAO-like states <xref ref-type="bibr" rid="bib1.bibx36 bib1.bibx285 bib1.bibx16 bib1.bibx65" id="paren.298"/>. Similarly, the East Atlantic pattern has been linked to Atlantic Ridge and Atlantic Trough-like circulation anomalies <xref ref-type="bibr" rid="bib1.bibx15 bib1.bibx35" id="paren.299"/>, while the Scandinavian pattern resembles Scandinavian Blocking in its positive phase and Scandinavian Trough in its negative phase <xref ref-type="bibr" rid="bib1.bibx132 bib1.bibx41" id="paren.300"/>. Thus, apparent differences across studies often arise from the framework and time scale used, rather than from entirely distinct circulation dynamics <xref ref-type="bibr" rid="bib1.bibx285 bib1.bibx79" id="paren.301"/>.</p>
      <p id="d2e2948">Our literature review highlights that, although still greatly underexplored, all three key biogeochemical parameters in the Baltic Sea are influenced by large-scale circulation patterns across all previously discussed time scales. These patterns affect biogeochemistry primarily by shaping the statistics of local physical processes such as stratification, water exchange, heat flux and advection, which then regulate nutrient availability, oxygen concentrations, species distributions, and phytoplankton abundance. However, quantitative and basin-wide evidence directly linking large-scale circulation variability to oxygenation, primary production, and ocean acidification in the Baltic Sea remains scarce. Important knowledge gaps persist, particularly regarding the spatial and temporal dynamics of total alkalinity <xref ref-type="bibr" rid="bib1.bibx143" id="paren.302"/>. Likewise, although the physical controls on primary-production variability, especially for the summer cyanobacterial bloom, are partly linked to large-scale variability <xref ref-type="bibr" rid="bib1.bibx126 bib1.bibx127" id="paren.303"/>, a substantial fraction of the annual variability remains unexplained <xref ref-type="bibr" rid="bib1.bibx127" id="paren.304"/>.</p>
      <p id="d2e2960">Similar to the physical controls, the NAO, the East Atlantic, and the Scandinavian pattern were identified as relevant. For example, a positive NAO can reverse the advection of oxygen-depleted water and remove hypoxia on interannual time scales in the Gulf of Finland, whereas strong heat fluxes during European Blocking can enhance stratification and exacerbate deep-water deoxygenation in the Gulf of Riga. Wind speed, light, and cloud cover have also been identified as potential triggers for initiating or ending phytoplankton blooms on synoptic scales. Importantly, the relative influence of these physical drivers varies with time scale. These findings underscore that understanding and predicting regional biogeochemical states requires explicit consideration of both large-scale atmospheric forcing and its time scale-dependent effects on the local physics.</p>
      <p id="d2e2964">This results in a system where large-scale circulation shapes the statistics of local processes. Yet, the attribution of their quantitative contributions, especially for biogeochemistry, remains challenging and understudied. Large-scale circulation patterns are non-stationary: their spatial structure and strength evolve with changes in the background climate, including, for example, Arctic amplification <xref ref-type="bibr" rid="bib1.bibx307" id="paren.305"/>, likely altering their relative importance for the Baltic Sea in the future. Thus, anthropogenic climate change as well as legacy nutrient loads set the stage for the biogeochemistry in the Baltic Sea upon which large-scale circulation patterns superimpose variability. Based on our review, we encourage future studies, in particular those on biogeochemistry, to include a more systematic quantification of dominant drivers, robust statistical assessments of relationships between connected processes, and a detailed analysis of time-scale dependence.</p>
      <p id="d2e2970">Robust attribution and causal disentanglement of large-scale circulation impacts on the Baltic Sea region remain difficult because externally forced signals and internal variability cannot easily be separated <xref ref-type="bibr" rid="bib1.bibx50" id="paren.306"><named-content content-type="pre">e.g.,</named-content></xref>. In addition, summer circulation patterns that drive variability on decadal and longer time scales are either less well resolved over Northern Europe or remain insufficiently studied. Possible predictability arising from the North Atlantic (e.g., SPG, AMV, AMOC) has not yet been systematically researched for the Baltic Sea region, as regional downscalings of decadal predictability experiments are not available. Finally, model fidelity is a limiting factor: common biases in jets, storm tracks, sea ice, subpolar gyre and the AMOC variability and likely incomplete coupling of physics and biogeochemistry do not yet allow for robust results <xref ref-type="bibr" rid="bib1.bibx220" id="paren.307"><named-content content-type="pre">e.g.,</named-content></xref>.</p>
      <p id="d2e2983">To advance our understanding of links between large-scale circulation patterns and local processes, we highlight the need for: <list list-type="bullet"><list-item>
      <p id="d2e2988">Regime-based diagnostics paired with in-depth process analysis to move beyond correlation. In addition, the nonstationarity of large-scale circulation patterns must be addressed, because their spatial structure and regional impacts may evolve over time. This can be investigated with coordinated multi-model ensembles, ideally complemented by initial-condition large ensembles which make it possible to separate internally generated variability from the externally forced response and to test the robustness of circulation–impact relationships across models and realizations.</p></list-item><list-item>
      <p id="d2e2992">Fully coupled regional Earth-system models that resolve the complex topography of the Baltic Sea and can represent regional feedbacks among atmosphere, ocean, sea ice, and biogeochemistry more consistently.</p></list-item><list-item>
      <p id="d2e2996">Targeted evaluation of the large-scale circulation and ocean state in the global parent model – including jets, storm tracks, the subpolar gyre, and the AMOC – because biases in these features can propagate into the regional model through the imposed boundary conditions and thereby affect the simulated Baltic Sea variability.</p></list-item><list-item>
      <p id="d2e3000">Event-based observing and modeling approaches for storms, atmospheric rivers and marine heat waves to quantify the biogeochemical responses on short time scales.</p></list-item><list-item>
      <p id="d2e3004">Sustained high-frequency measurements of temperature, salinity, oxygen and other biogeochemical variables from coasts to deep basins to understand the impact of large-scale circulation patterns on biogeochemistry.</p></list-item></list></p>
      <p id="d2e3007">The main barriers to robust attributions and predictions are their non-stationary nature and the limitation of currently available observations and models. Targeted observational, process-focused methods and fully coupled regional models together provide a credible route to near-term gains in understanding and to actionable guidance for the Baltic Sea region.</p>
</sec>

      
      </body>
    <back><notes notes-type="codeavailability"><title>Code availability</title>

      <p id="d2e3015">No proprietary software was used. The code used to generate the figure(s) in this paper is available from the authors upon reasonable request and relies exclusively on publicly available datasets.</p>
  </notes><notes notes-type="dataavailability"><title>Data availability</title>

      <p id="d2e3021">The data analyzed in this study are derived from previously published, publicly available materials. No new measurements were generated as part of this work. Details on data access are provided through the corresponding references.</p>
  </notes><notes notes-type="authorcontribution"><title>Author contributions</title>

      <p id="d2e3027">The co-corresponding authorship FB and IRB were responsible for designing, conceptualizing, coordinating, supervising and writing the manuscript. HEMM, LBa, LN, TL, GR and BC contributed in ensuring relevance and consistency. Each author contributed to discussions and writing, focusing on their areas of expertise.</p>
  </notes><notes notes-type="competinginterests"><title>Competing interests</title>

      <p id="d2e3033">At least one of the (co-)authors is a member of the editorial board of <italic>Earth System Dynamics</italic>. The peer-review process was guided by an independent editor, and the authors also have no other competing interests to declare.</p>
  </notes><notes notes-type="disclaimer"><title>Disclaimer</title>

      <p id="d2e3042">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="d2e3048">We sincerely thank the two anonymous reviewers for their thoughtful and constructive comments, which greatly helped us improve the manuscript.</p><p id="d2e3050">The research presented in this study is part of the Baltic Earth program (Earth System Science for the Baltic Sea region; <uri>https://www.baltic.earth</uri>, last access: 30 April 2026) and contributes to the Baltic Earth Working Groups on (i) Teleconnections between the North Atlantic, Northern Europe and the Baltic Sea region, and (ii) Land-Sea Biogeochemical Linkages in the Baltic Sea region.</p></ack><notes notes-type="financialsupport"><title>Financial support</title>

      <p id="d2e3058">Lev Naumov is paid through funding by the grant number 67KIA4017A, belonging to the SEAGUARD, funded by the Federal Ministry for the Environment, Climate Action, Nature Conservation and Nuclear Safety (BMUNKN) on the basis of a resolution of the German Bundestag.</p>
  </notes><notes notes-type="reviewstatement"><title>Review statement</title>

      <p id="d2e3064">This paper was edited by Ira Didenkulova and reviewed by Ulrike Löptien and one anonymous referee.</p>
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