<?xml version="1.0" encoding="UTF-8"?>
<!DOCTYPE article PUBLIC "-//NLM//DTD Journal Publishing with OASIS Tables v3.0 20080202//EN" "https://jats.nlm.nih.gov/nlm-dtd/publishing/3.0/journalpub-oasis3.dtd">
<article xmlns:xlink="http://www.w3.org/1999/xlink" xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:oasis="http://docs.oasis-open.org/ns/oasis-exchange/table" xml:lang="en" dtd-version="3.0" article-type="research-article">
  <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-17-893-2026</article-id><title-group><article-title>Overshoot and (ir)reversibility to 2300 in two CO<sub>2</sub>-emissions driven Earth System models</article-title><alt-title>Overshoot and (ir)reversibility to 2300</alt-title>
      </title-group>
      <contrib-group>
        <contrib contrib-type="author" corresp="yes" rid="aff1 aff2 aff3">
          <name><surname>Smith</surname><given-names>Chris</given-names></name>
          <email>smithc@iiasa.ac.at</email>
        <ext-link>https://orcid.org/0000-0003-0599-4633</ext-link></contrib>
        <contrib contrib-type="author" corresp="no" rid="aff4">
          <name><surname>Ramme</surname><given-names>Lennart</given-names></name>
          
        <ext-link>https://orcid.org/0000-0002-8307-2493</ext-link></contrib>
        <contrib contrib-type="author" corresp="no" rid="aff3">
          <name><surname>Wells</surname><given-names>Christopher D.</given-names></name>
          
        <ext-link>https://orcid.org/0000-0003-1958-0984</ext-link></contrib>
        <contrib contrib-type="author" corresp="no" rid="aff5">
          <name><surname>Gjermundsen</surname><given-names>Ada</given-names></name>
          
        <ext-link>https://orcid.org/0000-0002-2053-4689</ext-link></contrib>
        <contrib contrib-type="author" corresp="no" rid="aff6 aff4">
          <name><surname>Li</surname><given-names>Hongmei</given-names></name>
          
        <ext-link>https://orcid.org/0000-0003-2912-1837</ext-link></contrib>
        <contrib contrib-type="author" corresp="no" rid="aff4 aff6">
          <name><surname>Ilyina</surname><given-names>Tatiana</given-names></name>
          
        <ext-link>https://orcid.org/0000-0002-3475-4842</ext-link></contrib>
        <contrib contrib-type="author" corresp="no" rid="aff7">
          <name><surname>Muralidhar</surname><given-names>Adakudlu</given-names></name>
          
        </contrib>
        <contrib contrib-type="author" corresp="no" rid="aff8">
          <name><surname>Bourgeois</surname><given-names>Timothée</given-names></name>
          
        <ext-link>https://orcid.org/0000-0002-9367-464X</ext-link></contrib>
        <contrib contrib-type="author" corresp="no" rid="aff8">
          <name><surname>Schwinger</surname><given-names>Jörg</given-names></name>
          
        <ext-link>https://orcid.org/0000-0002-7525-6882</ext-link></contrib>
        <contrib contrib-type="author" corresp="no" rid="aff3">
          <name><surname>Romero-Prieto</surname><given-names>Alejandro</given-names></name>
          
        <ext-link>https://orcid.org/0009-0005-8522-7697</ext-link></contrib>
        <contrib contrib-type="author" corresp="no" rid="aff4">
          <name><surname>Li</surname><given-names>Chao</given-names></name>
          
        <ext-link>https://orcid.org/0000-0003-2556-0891</ext-link></contrib>
        <contrib contrib-type="author" corresp="no" rid="aff7">
          <name><surname>Mauritzen</surname><given-names>Cecilie</given-names></name>
          
        <ext-link>https://orcid.org/0000-0001-5956-8811</ext-link></contrib>
        <aff id="aff1"><label>1</label><institution>Department of Water and Climate, Vrije Universiteit Brussel, Brussels, Belgium</institution>
        </aff>
        <aff id="aff2"><label>2</label><institution>Energy, Climate and Environment Program, International Institute for Applied Systems Analysis (IIASA),  Laxenburg, Austria</institution>
        </aff>
        <aff id="aff3"><label>3</label><institution>School of Earth and Environment, University of Leeds, Leeds, UK</institution>
        </aff>
        <aff id="aff4"><label>4</label><institution>Max Planck Institute for Meteorology, Hamburg, Germany</institution>
        </aff>
        <aff id="aff5"><label>5</label><institution>Department of Geosciences, University of Oslo, Oslo, Norway</institution>
        </aff>
        <aff id="aff6"><label>6</label><institution>Helmholtz-Zentrum Hereon, Geesthacht, Germany</institution>
        </aff>
        <aff id="aff7"><label>7</label><institution>Norwegian Meteorological Institute, Oslo, Norway</institution>
        </aff>
        <aff id="aff8"><label>8</label><institution>NORCE Climate &amp; Environment and Bjerknes Centre for Climate Research, Bergen, Norway</institution>
        </aff>
      </contrib-group>
      <author-notes><corresp id="corr1">Chris Smith (smithc@iiasa.ac.at)</corresp></author-notes><pub-date><day>29</day><month>June</month><year>2026</year></pub-date>
      
      <volume>17</volume>
      <issue>3</issue>
      <fpage>893</fpage><lpage>911</lpage>
      <history>
        <date date-type="received"><day>25</day><month>October</month><year>2025</year></date>
           <date date-type="rev-request"><day>7</day><month>November</month><year>2025</year></date>
           <date date-type="rev-recd"><day>15</day><month>May</month><year>2026</year></date>
           <date date-type="accepted"><day>27</day><month>May</month><year>2026</year></date>
      </history>
      <permissions>
        <copyright-statement>Copyright: © 2026 Chris Smith 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/17/893/2026/esd-17-893-2026.html">This article is available from https://esd.copernicus.org/articles/17/893/2026/esd-17-893-2026.html</self-uri><self-uri xlink:href="https://esd.copernicus.org/articles/17/893/2026/esd-17-893-2026.pdf">The full text article is available as a PDF file from https://esd.copernicus.org/articles/17/893/2026/esd-17-893-2026.pdf</self-uri>
      <abstract><title>Abstract</title>

      <p id="d2e239">Future climate scenario projections are usually run with prescribed atmospheric <inline-formula><mml:math id="M2" 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> concentrations. However, by not allowing the carbon cycle to interactively respond to emissions in Earth System models, the role of carbon cycle feedbacks on contributions to differences in climate model projections may be undersampled. Here, we present the main findings of two Earth System Models (MPI-ESM1.2-LR and NorESM2-LM) run with <inline-formula><mml:math id="M3" 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> emissions to 2300 for three scenarios, two of which are climate overshoot scenarios, that were part of the Coupled Model Intercomparison Project Phase 6 (CMIP6). These experiments serve three important purposes: (i) an increasing focus on emissions driven runs, supplementing scenarios produced for the Coupled Climate-Carbon Cycle (C4MIP) and Carbon Dioxide Removal (CDRMIP) contributions to CMIP6; (ii) a focus on overshoot scenarios; and (iii) an extension of results beyond 2100, the timescales at which some of the most significant differences play out. Of the two models, NorESM2-LM shows more asymmetry in its climate response at the same global mean temperature levels before and after peak warming, particularly in terms of its regional pattern of warming and Atlantic Meridional Overturning Circulation (AMOC) response, with a substantially weakened AMOC persisting for decades after peak warming that takes more than a century to recover. In contrast, MPI-ESM1.2-LR shows reversibility with AMOC strength and regional warming more closely following surface temperature, but with some climate signals such as sea-level rise and ocean deoxygenation essentially irreversible. This diversity in model responses highlights the need for further research with a larger model ensemble that focuses on long-term emissions-driven model runs, particularly for overshoot scenarios, for CMIP7.</p>
  </abstract>
    
<funding-group>
<award-group id="gs1">
<funding-source>HORIZON EUROPE Climate, Energy and Mobility</funding-source>
<award-id>101081661</award-id>
</award-group>
<award-group id="gs2">
<funding-source>Natural Environment Research Council</funding-source>
<award-id>NE/S007458/1</award-id>
</award-group>
<award-group id="gs3">
<funding-source>HORIZON EUROPE Framework Programme</funding-source>
<award-id>101056939</award-id>
<award-id>101003536</award-id>
</award-group>
<award-group id="gs4">
<funding-source>Deutsche Forschungsgemeinschaft</funding-source>
<award-id>390683824</award-id>
</award-group>
</funding-group>
</article-meta>
  </front>
<body>
      

<sec id="Ch1.S1" sec-type="intro">
  <label>1</label><title>Introduction</title>
      <p id="d2e273">The Coupled Model Intercomparison Project (CMIP), for which CMIP phase 6 (CMIP6) is the most recent completed phase, provides the forum for state-of-the-art Earth System Models (ESMs) to submit results under carefully controlled climate model experimental protocols <xref ref-type="bibr" rid="bib1.bibx5 bib1.bibx54" id="paren.1"/>. One important component of CMIP is the Scenario Model Intercomparison Project (ScenarioMIP), which evaluates ESM projections into the future and provides insight into how human influences could affect climate due to greenhouse gases, aerosols and land use change <xref ref-type="bibr" rid="bib1.bibx32 bib1.bibx58" id="paren.2"/>. In ScenarioMIP, future socioeconomic projections (2015 onwards in CMIP6) are branched from the end of a historical hindcast (1850–2014) under a number of different pathways ranging from very high to very low climate forcing, resulting in a wide range of possible climate change trajectories over the 21st century <xref ref-type="bibr" rid="bib1.bibx55" id="paren.3"/>. ScenarioMIP experiments provide our best estimates of future climates resulting from these trajectories and are invaluable for informing climate impact models <xref ref-type="bibr" rid="bib1.bibx40" id="paren.4"/>. The climate impact models describe how climate change could affect human and natural systems such as crop productivity, biodiversity and human health <xref ref-type="bibr" rid="bib1.bibx59" id="paren.5"/>.</p>
      <p id="d2e291">In CMIP6, future climate projections are based upon the Shared Socioeconomic Pathway/Representative Concentration Pathway (SSP-RCP) matrix <xref ref-type="bibr" rid="bib1.bibx32" id="paren.6"/>. Scenarios run in ESMs are of the form SSP<inline-formula><mml:math id="M4" display="inline"><mml:mi>n</mml:mi></mml:math></inline-formula>-<inline-formula><mml:math id="M5" display="inline"><mml:mi>x</mml:mi></mml:math></inline-formula>, where <inline-formula><mml:math id="M6" display="inline"><mml:mrow><mml:mi>n</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">1</mml:mn><mml:mo>,</mml:mo><mml:mi mathvariant="normal">…</mml:mi><mml:mo>,</mml:mo><mml:mn mathvariant="normal">5</mml:mn></mml:mrow></mml:math></inline-formula> describes a specific socioeconomic storyline and <inline-formula><mml:math id="M7" display="inline"><mml:mi>x</mml:mi></mml:math></inline-formula> describes the approximate radiative forcing level (as a proxy for warming level and climate change mitigation effort) in the year 2100 in <inline-formula><mml:math id="M8" 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> (Gidden et al., 2019). A total of eight SSP-RCP combinations were chosen for running in ESMs for CMIP6, spanning radiative forcing targets from 1.9 to 8.5 <inline-formula><mml:math id="M9" 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> in 2100. For reference, present-day radiative forcing levels are around 3 <inline-formula><mml:math id="M10" 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> <xref ref-type="bibr" rid="bib1.bibx6" id="paren.7"/>.</p>
      <p id="d2e393">For each SSP-RCP, an emissions pathway is produced by an integrated assessment model (IAM). The IAM uses inputs of population, GDP, education and urbanization, and produces greenhouse gas (GHG) and short-lived climate forcer (SLCF) emissions projections as an output. IAMs are internally consistent representations of the economy, energy and land use system, which typically find cost- or welfare-optimising solutions from the input boundary conditions subject to technological, socioeconomic, physical, and climatic constraints (here, the 2100 radiative forcing level). Typically, as the radiative forcing constraint tightens (decreasing <inline-formula><mml:math id="M11" 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> target value), climate abatement costs increase and facilitate the requirement for negative emissions technologies. The ease of meeting particular radiative forcing levels depends on the SSP storyline which has different levels of challenges to mitigation and adaptation, with some RCP levels either above the no-mitigation baseline or not technologically feasible within given socioeconomic constraints in some SSPs <xref ref-type="bibr" rid="bib1.bibx37" id="paren.8"/>.</p>
      <p id="d2e416">IAMs produce time-varying emissions of <inline-formula><mml:math id="M12" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> and other forcers, but future climate experiments in ScenarioMIP and its earlier predecessors were driven by concentrations of <inline-formula><mml:math id="M13" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> and other GHGs. The concentrations in each SSP-RCP were calculated using a simple climate model, MAGICC, which uses a carbon cycle box model that is calibrated on full-complexity carbon cycle and Earth system models <xref ref-type="bibr" rid="bib1.bibx26 bib1.bibx27 bib1.bibx28" id="paren.9"/>. However, in addition to supplying the concentration-driven ScenarioMIP experiments, around a dozen ESMs in CMIP6 were set up to run with prescribed emissions of <inline-formula><mml:math id="M14" 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> <xref ref-type="bibr" rid="bib1.bibx20" id="paren.10"/>. Performing emissions-driven runs allows us to sample an additional dimension of uncertainty, namely the strengths of climate-carbon-cycle feedbacks that define the atmospheric airborne fraction and land and oceanic uptake of <inline-formula><mml:math id="M15" 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> emissions <xref ref-type="bibr" rid="bib1.bibx8" id="paren.11"/>. Since humans emit greenhouse gases rather than having direct control over atmospheric concentrations, an emissions-driven experimental design is also more appropriate for determining the levels of residual or negative emissions required to stabilize and reverse anthropogenic climate change <xref ref-type="bibr" rid="bib1.bibx22" id="paren.12"/>, as well as more clearly linking model responses to human efforts to reduce emissions.</p>
      <p id="d2e477">Under CMIP6, a handful of <inline-formula><mml:math id="M16" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> emissions-driven simulations were performed under the SSP5-8.5 (fossil-fuel driven, very high emissions) and SSP5-3.4-over (following SSP5-8.5 until 2040, with rapid emissions reductions after 2040 and high levels of net negative <inline-formula><mml:math id="M17" 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> emissions in the second half of the 21st century) under the Coupled Climate–Carbon Cycle Model Intercomparison Project (C4MIP) and Carbon Dioxide Removal Model Intercomparison Project (CDRMIP) components of CMIP6 respectively <xref ref-type="bibr" rid="bib1.bibx13 bib1.bibx14 bib1.bibx32" id="paren.13"/>. While scientifically interesting and useful for impact studies <xref ref-type="bibr" rid="bib1.bibx42" id="paren.14"/>, SSP5-8.5 has been criticised for being an unrealistically high emissions scenario <xref ref-type="bibr" rid="bib1.bibx12" id="paren.15"/>, which would require a global reversal of policy and shift back to fossil fuels <xref ref-type="bibr" rid="bib1.bibx11" id="paren.16"/> leading to warming projections at the end of the century in the region of 5 <inline-formula><mml:math id="M18" 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> above pre-industrial <xref ref-type="bibr" rid="bib1.bibx55" id="paren.17"/>. The ensuing climate damages from such a strong warming scenario would severely impact the economy and slow growth and ensuing emissions <xref ref-type="bibr" rid="bib1.bibx62 bib1.bibx44" id="paren.18"/>, making this scenario an unlikely reality. It has been argued that SSP5-3.4-over is also unrealistic given its abrupt turnaround and reliance on high levels of carbon dioxide removal <xref ref-type="bibr" rid="bib1.bibx43" id="paren.19"/>.</p>
      <p id="d2e534">The CMIP6 protocol allows for (concentration-driven) scenario projections to be extended beyond 2100 to 2300, but only a few models performed the extensions <xref ref-type="bibr" rid="bib1.bibx20" id="paren.20"/>. Beyond 2100, climate responses in models can differ substantially, and slow feedbacks and irreversibilities only become apparent on these timescales <xref ref-type="bibr" rid="bib1.bibx50" id="paren.21"/>. Furthermore, 2100 is now less than one human lifetime away <xref ref-type="bibr" rid="bib1.bibx21" id="paren.22"/>. Further studies using emissions-driven experiments have been undertaken in recent years, but realistic experiments may usually only be run to 2100 <xref ref-type="bibr" rid="bib1.bibx30 bib1.bibx9" id="paren.23"/>, with longer term experiments tending to be more idealized scenarios such as immediate zeroing of <inline-formula><mml:math id="M19" 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> emissions <xref ref-type="bibr" rid="bib1.bibx48 bib1.bibx15" id="paren.24"/>. For the reasons above, there is interest in running more plausible and policy-relevant climate scenarios in <inline-formula><mml:math id="M20" 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> emissions-driven ESMs, and these are intended to play a more important role in the upcoming CMIP7 phase beyond 2100 <xref ref-type="bibr" rid="bib1.bibx41 bib1.bibx58" id="paren.25"/>.</p>
      <p id="d2e578">These considerations motivate two research questions:</p>
      <p id="d2e581"><list list-type="order">
          <list-item>

      <p id="d2e586">how do overshoot and negative emissions manifest in responses in the global carbon cycle?</p>
          </list-item>
          <list-item>

      <p id="d2e592">to what extent are responses within the Earth system irreversible after a climate overshoot?</p>
          </list-item>
        </list></p>
      <p id="d2e597">Fully answering both research questions requires a longer time horizon than 2100 to analyse long-term impacts and reversibility, and an ensemble of simulations to account for internal variability in climate and the carbon cycle. <xref ref-type="bibr" rid="bib1.bibx34" id="text.26"/> explored the responses in regional and extreme climate in overshoot scenarios in a multi-model ensemble context to 2100, and found that there was asymmetry in the responses before and after peak warming. <xref ref-type="bibr" rid="bib1.bibx38 bib1.bibx39" id="text.27"/> used extended simulations to 2300 available for four models in <italic>ssp534-over</italic>, for which the longer term AMOC response exhibits a wide variety of behaviours. <xref ref-type="bibr" rid="bib1.bibx16" id="text.28"/> evaluated the global temperature, carbon stock and AMOC behaviour in five ESMs and one ESM of intermediate complexity in SSP5-3.4-over and SSP5-8.5 simulations run to 2300, noting substantial differences in AMOC and carbon uptake. However, these studies used simulations with prescribed concentrations, limiting the insight that changing emissions has on the carbon cycle and global climate.</p>
      <p id="d2e612">In this paper, we run two ESMs under SSP1-1.9 (very low emissions, consistent with the 1.5 <inline-formula><mml:math id="M21" 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> Paris Agreement goal), SSP2-4.5 (moderate emissions, most closely aligned to current policies with a projected warming in 2100 of around 2.5–3 <inline-formula><mml:math id="M22" 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>), as well as adding additional simulations of SSP5-3.4-over (included under the Carbon Dioxide Removal Model Intercomparison Project (CDRMIP; <xref ref-type="bibr" rid="bib1.bibx14" id="altparen.29"/>)) to 2300. Therefore, we fill in the emissions-driven scenario space at the low and moderate levels compared to the availability of CMIP6 simulations. These runs are primed to study this question because emission-driven ESM simulations give a more detailed representation of the carbon cycle compared to concentration-driven simulations, which take their prescribed concentration pathways from simpler climate models or emulators <xref ref-type="bibr" rid="bib1.bibx41" id="paren.30"/>. While emissions-driven experiments for net-zero and net negative pathways do exist, they have tended to be run with idealized, <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>-only trajectories <xref ref-type="bibr" rid="bib1.bibx46 bib1.bibx57" id="paren.31"/>. Running emissions-driven scenarios for a longer timeframe allows us to determine the carbon cycle, reversibility, and climate response to climate overshoot under negative emissions. These topics will become increasingly important as the 1.5 and 2 <inline-formula><mml:math id="M24" 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> warming thresholds are approached in the absence of robust mitigation <xref ref-type="bibr" rid="bib1.bibx43" id="paren.32"/>.</p>
</sec>
<sec id="Ch1.S2">
  <label>2</label><title>Experimental design</title>
      <p id="d2e677">We use two emissions-driven ESMs: the Norwegian Earth System Model (NorESM2-LM; <xref ref-type="bibr" rid="bib1.bibx47 bib1.bibx56" id="altparen.33"/>) and the Max-Planck-Institute Earth System Model (MPI-ESM1.2-LR; <xref ref-type="bibr" rid="bib1.bibx25" id="altparen.34"/>). These two ESMs are two of the best performing models with respect to reproducing observed atmospheric <inline-formula><mml:math id="M25" 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> concentrations in the historical period (Fig. <xref ref-type="fig" rid="F1"/>). Given their good correspondence to historical concentrations, the MPI-ESM1.2-LR and NorESM2-LM models are appropriate for the analysis of future <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> emissions-driven simulations.</p>

      <fig id="F1"><label>Figure 1</label><caption><p id="d2e712">Atmospheric <inline-formula><mml:math id="M27" 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> concentrations reported from the emissions-driven historical simulations (esm-hist) from the C4MIP contribution to CMIP6 <xref ref-type="bibr" rid="bib1.bibx13" id="paren.35"/>. NorESM2-LM (red), MPI-ESM1.2-LR (blue), and the other 11 CMIP6 models (light grey) are compared to the best estimate concentration time series that was used to run concentration-driven scenarios (<xref ref-type="bibr" rid="bib1.bibx27" id="altparen.36"/>, black).</p></caption>
        <graphic xlink:href="https://esd.copernicus.org/articles/17/893/2026/esd-17-893-2026-f01.png"/>

      </fig>

      <p id="d2e738">The future scenarios are run from 2015 to 2300 and are labelled <italic>esm-ssp119</italic>, <italic>esm-ssp245</italic>, and <italic>esm-ssp534-over</italic> for SSP1-1.9, SSP2-4.5 and SSP5-3.4-over respectively. They are branched from <inline-formula><mml:math id="M28" 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> emissions-driven historical simulations (1850–2014) known as <italic>esm-hist</italic>. In this paper, we follow the CMIP convention of labelling scenarios, which disallows the period “.” symbol (so the radiative forcing target is multiplied by 10) and removes the dash “-” between the SSP and RCP part of the scenario name. For additional distinction we italicize the CMIP6 name, hence <italic>ssp119</italic> <inline-formula><mml:math id="M29" display="inline"><mml:mo>=</mml:mo></mml:math></inline-formula> SSP1-1.9. Furthermore, we again follow the CMIP6 convention of labelling <inline-formula><mml:math id="M30" 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> emissions-driven scenarios as run in “Earth system model” mode, so our emissions-driven scenarios are prepended with “esm-”, e.g. <italic>esm-ssp119</italic>. Table <xref ref-type="table" rid="T1"/> shows the ESM simulations performed within the project along with the number of ensemble members available for each model.</p>

<table-wrap id="T1" specific-use="star"><label>Table 1</label><caption><p id="d2e795">Number of ensemble members of the emission-driven simulations with the two ESMs used in this study, with the time periods supported by each ensemble size.</p></caption><oasis:table frame="topbot"><oasis:tgroup cols="5">
     <oasis:colspec colnum="1" colname="col1" align="left"/>
     <oasis:colspec colnum="2" colname="col2" align="right"/>
     <oasis:colspec colnum="3" colname="col3" align="right" colsep="1"/>
     <oasis:colspec colnum="4" colname="col4" align="right"/>
     <oasis:colspec colnum="5" colname="col5" align="right"/>
     <oasis:thead>
       <oasis:row>
         <oasis:entry colname="col1"/>
         <oasis:entry rowsep="1" namest="col2" nameend="col5" align="center">Model </oasis:entry>
       </oasis:row>
       <oasis:row rowsep="1">
         <oasis:entry colname="col1"/>
         <oasis:entry namest="col2" nameend="col3" align="center" colsep="1">MPI-ESM1.2-LR </oasis:entry>
         <oasis:entry namest="col4" nameend="col5" align="center">NorESM2-LM </oasis:entry>
       </oasis:row>
     </oasis:thead>
     <oasis:tbody>
       <oasis:row rowsep="1">
         <oasis:entry colname="col1">Experiment</oasis:entry>
         <oasis:entry colname="col2">2015–2100</oasis:entry>
         <oasis:entry colname="col3">2100–2300</oasis:entry>
         <oasis:entry colname="col4">2015–2100</oasis:entry>
         <oasis:entry colname="col5">2100–2300</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1"><italic>esm-ssp119</italic></oasis:entry>
         <oasis:entry colname="col2">10</oasis:entry>
         <oasis:entry colname="col3">10</oasis:entry>
         <oasis:entry colname="col4">10</oasis:entry>
         <oasis:entry colname="col5">3</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1"><italic>esm-ssp245</italic></oasis:entry>
         <oasis:entry colname="col2">30</oasis:entry>
         <oasis:entry colname="col3">10</oasis:entry>
         <oasis:entry colname="col4">10</oasis:entry>
         <oasis:entry colname="col5">3</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1"><italic>esm-ssp534-over</italic></oasis:entry>
         <oasis:entry colname="col2">10</oasis:entry>
         <oasis:entry colname="col3">10</oasis:entry>
         <oasis:entry colname="col4">10</oasis:entry>
         <oasis:entry colname="col5">3</oasis:entry>
       </oasis:row>
     </oasis:tbody>
   </oasis:tgroup></oasis:table></table-wrap>

      <p id="d2e914">The ESMs are forced with the <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> emission pathways used in the SSP scenarios, extended after the year 2100 as described in <xref ref-type="bibr" rid="bib1.bibx28" id="text.37"/>. Figure <xref ref-type="fig" rid="F2"/> shows the prescribed evolution of fossil fuel and industrial <inline-formula><mml:math id="M32" 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> emissions in both models. The original CMIP6 extension protocol mandates that positive levels of <inline-formula><mml:math id="M33" 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> emissions in 2100 are extended linearly to zero between 2100–2250, while negative emissions in 2100 are held constant for 40 <inline-formula><mml:math id="M34" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">years</mml:mi></mml:mrow></mml:math></inline-formula>. After that, <inline-formula><mml:math id="M35" 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> emissions linearly approach zero, which takes 30 <inline-formula><mml:math id="M36" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">years</mml:mi></mml:mrow></mml:math></inline-formula> in <italic>esm-ssp534-over</italic> and 45 <inline-formula><mml:math id="M37" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">years</mml:mi></mml:mrow></mml:math></inline-formula> in <italic>esm-ssp119</italic>. MPI-ESM1.2-LR implemented this protocol exactly, while NorESM2-LM implemented it differently such that negative emissions in <italic>esm-ssp119</italic> start to linearly approach zero from 2100 with no phase of constant negative emissions. <inline-formula><mml:math id="M38" 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> emissions from land use change are part of the terrestrial carbon cycle and are determined interactively by each ESMs. Land use transitions follow that of the underlying CMIP6 scenario, and no further land use transitions occur after 2100. Harvest rates are also held constant at 2100 levels for the post-2100 extensions. Non-<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> GHGs are prescribed using pre-calculated concentration time series from <xref ref-type="bibr" rid="bib1.bibx28" id="text.38"/>.</p>

      <fig id="F2"><label>Figure 2</label><caption><p id="d2e1028">Evolution of total <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> emissions for the <italic>esm-hist</italic>, <italic>esm-ssp119</italic>, <italic>esm-ssp245</italic> and <italic>esm-ssp534-over</italic> scenarios in MPI-ESM1.2-LR (solid) and NorESM2-LM (dashed).</p></caption>
        <graphic xlink:href="https://esd.copernicus.org/articles/17/893/2026/esd-17-893-2026-f02.png"/>

      </fig>

      <p id="d2e1060">In MPI-ESM1.2-LR, aerosols are prescribed using concentrations, in the form of the aerosol optical depth (AOD) from the MACv2-SP simulator <xref ref-type="bibr" rid="bib1.bibx52" id="paren.39"/>. AOD is reduced linearly to zero between 2100 and 2250 if aerosol emissions are mostly associated with industrial processes in a specific region. In contrast to that, they are held constant after 2100 if they are mostly associated with biomass burning. This matches the information given to the land modules of the ESMs. In NorESM2-LM, aerosols are emissions-driven, and emissions of black carbon, organic carbon and sulfur follow the extension pathways of <xref ref-type="bibr" rid="bib1.bibx28" id="text.40"/>.</p>
</sec>
<sec id="Ch1.S3">
  <label>3</label><title>Results</title>
<sec id="Ch1.S3.SS1">
  <label>3.1</label><title>Global surface temperature and <inline-formula><mml:math id="M41" 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> concentration</title>
      <p id="d2e1096">Figure <xref ref-type="fig" rid="F3"/> shows how MPI-ESM1.2-LR and NorESM2-LM simulate the evolution of the global-mean 2 <inline-formula><mml:math id="M42" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">m</mml:mi></mml:mrow></mml:math></inline-formula> surface air temperature (GSAT) anomaly compared to the 1850–1900 reference period (top row) and the atmospheric <inline-formula><mml:math id="M43" 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> concentration (bottom row) for <italic>esm-ssp119</italic>, <italic>esm-ssp245</italic>, and <italic>esm-ssp534-over</italic>. MPI-ESM1.2-LR shows an earlier warming over the historical period than NorESM2-LM. NorESM2-LM has a lower peak warming than MPI-ESM1.2-LR in the two overshoot <italic>esm-ssp119</italic> and <italic>esm-ssp534-over</italic> scenarios, and a lower 2100 warming in all three scenarios, but is equal to or above the temperature anomaly of MPI-ESM1.2-LR in 2300 in all three.</p>

      <fig id="F3" specific-use="star"><label>Figure 3</label><caption><p id="d2e1138">The evolution of the global mean temperature anomaly <bold>(a–c)</bold> and the atmospheric <inline-formula><mml:math id="M44" 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> concentration <bold>(d–f)</bold> in NorESM2-LM and MPI-ESM1.2-LR for <italic>esm-ssp119</italic> <bold>(a, d)</bold>, <italic>esm-ssp245</italic> <bold>(b, e)</bold>, and <italic>esm-ssp534-over</italic> <bold>(c, f)</bold>. Shown are the ensemble mean, as well as the full range spanned by the ensemble members for the emissions-driven simulations. Where available, the parallel data from the concentration-driven simulations is given with dotted lines (temperature for <italic>ssp119</italic> in MPI-ESM1.2-LR and for <italic>ssp534-over</italic> in NorESM2-LM, and <inline-formula><mml:math id="M45" 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> concentration time series from <xref ref-type="bibr" rid="bib1.bibx28" id="text.41"/> for all three scenarios).</p></caption>
          <graphic xlink:href="https://esd.copernicus.org/articles/17/893/2026/esd-17-893-2026-f03.png"/>

        </fig>

      <p id="d2e1204">The difference in future projected behaviour is driven by different responses in the models to zero and net negative <inline-formula><mml:math id="M46" 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> emissions phases. Both models have (150-year Gregory) equilibrium climate sensitivities (3.00 <inline-formula><mml:math id="M47" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">°</mml:mi><mml:mi mathvariant="normal">C</mml:mi></mml:mrow></mml:math></inline-formula> MPI-ESM1.2-LR; 2.54 <inline-formula><mml:math id="M48" 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> NorESM2-LM) and transient climate responses (1.84 <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> MPI-ESM1.2-LR; 1.48 <inline-formula><mml:math id="M50" 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> NorESM2-LM) that are not vastly different from each other <xref ref-type="bibr" rid="bib1.bibx49" id="paren.42"/>, therefore likely not accounting for the differences in model projections, particularly in the long term.  In <italic>esm-ssp119</italic> and <italic>esm-ssp534-over</italic>, NorESM2-LM shows an increasing temperature in the 22nd century following a temperature minimum before a stabilization in the 23rd century that is qualitatively different from the long-term stabilization in MPI-ESM1.2-LR. In the <italic>esm-ssp245</italic> scenario, NorESM2-LM continues to warm in the long term whereas MPI-ESM1.2-LR exhibits a peak temperature in the late 22nd century followed by a decline.</p>
      <p id="d2e1272">Differences in GSAT evolution in NorESM2-LM compared to MPI-ESM1.2-LR can be explained by differences in ocean circulation. Generally, a slow warming in NorESM2-LM is due to the delayed Southern Ocean response to climate forcing, whereby heat is transported downwards initially and re-emerges towards the surface later in the simulation <xref ref-type="bibr" rid="bib1.bibx10" id="paren.43"/>; note also that this behaviour is also observed in an Earth system model of intermediate complexity <xref ref-type="bibr" rid="bib1.bibx7" id="paren.44"/>. While a very different forcing profile, similar results are noted comparing 150-year and 500-year simulations of the <italic>abrupt-4xCO2</italic> idealized simulation in NorESM2-LM <xref ref-type="bibr" rid="bib1.bibx60" id="paren.45"/>. It is known that NorESM2-LM has a low climate sensitivity over timescales of 150 <inline-formula><mml:math id="M51" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">years</mml:mi></mml:mrow></mml:math></inline-formula>, roughly that of the CMIP6 historical period, but a much higher climate sensitivity when evaluated over 500 <inline-formula><mml:math id="M52" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">years</mml:mi></mml:mrow></mml:math></inline-formula> <xref ref-type="bibr" rid="bib1.bibx10 bib1.bibx47" id="paren.46"/>, caused by changes in the shortwave cloud feedback strength that are driven by the Southern Ocean surface temperature. A second factor, explaining the temperature minima after the GSAT peak in the NorESM2-LM <italic>esm-ssp119</italic> and <italic>esm-ssp534-over</italic> simulations is the decline and recovery of the Atlantic meridional overturning circulation (AMOC), which is much more pronounced in NorESM2-LM compared to MPI-ESM1.2-LR (Sect. 3.4). In overshoot scenarios, where atmospheric <inline-formula><mml:math id="M53" 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> is reduced at the same time as the northward heat transport is diminished, a strong northern high-latitude cooling followed by a warming has been described in NorESM2-LM <xref ref-type="bibr" rid="bib1.bibx45 bib1.bibx46" id="paren.47"/>. These differing long-term responses highlight the benefits of running climate scenarios beyond 2100.</p>
      <p id="d2e1327">As MPI-ESM1.2-LR ran <italic>ssp119</italic> and <italic>ssp245</italic> and NorESM2-LM ran <italic>ssp245</italic> and <italic>ssp534-over</italic> as part of CMIP6, both concentration-driven and only to 2100, it is possible to see the effects of the inclusion of the carbon cycle on the global mean temperature by comparing parallel emissions- and concentration-driven simulations. In all of the four cases, the 21st century warming projections are slightly lower for the emissions-driven runs than for the concentration-driven runs, because of lower atmospheric <inline-formula><mml:math id="M54" 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> concentrations resulting in a lower radiative forcing in the emissions-driven runs. This is because the ocean and land carbon sinks in these ESMs are stronger than in the MAGICC simple climate model used to derive the prescribed concentration time series. The differences are smallest between <italic>esm-ssp245</italic> and <italic>ssp245</italic>, where the concentrations deviate noticeably only after mid-century, and larger for the overshoot scenarios where the emissions-driven and concentration-driven runs diverge earlier. In the two overshoot scenarios, the divergence in atmospheric concentrations begins around the time of peak emissions, highlighting the need for a better calibration of simple climate models beyond 2100 and under overshoot conditions. More generally the need for better understanding of the behaviour of the carbon cycle in an at-yet unrealized post-peak world is necessary.</p>
      <p id="d2e1360">As the concentration-driven simulations end in the year 2100, it can be speculated that the increasing differences in atmospheric <inline-formula><mml:math id="M55" 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> would also cause substantial deviations in the global mean temperature in the 22nd and 23rd centuries between emissions- and concentration-driven scenarios. The post-2100 trajectory of concentrations in <italic>esm-ssp245</italic>, in which MPI-ESM1.2-LR has concentrations declining more rapidly than NorESM2-LM following their peak, would likely result in lower GSAT projections in both models compared to their <italic>ssp245</italic> counterparts.</p>
      <p id="d2e1380">By analysing global mean temperature anomaly as a function of cumulative <inline-formula><mml:math id="M56" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> emissions (Fig. <xref ref-type="fig" rid="F4"/>), we can first note that both ESMs follow the approximately linear relationship between cumulative <inline-formula><mml:math id="M57" 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> emissions and temperature <xref ref-type="bibr" rid="bib1.bibx1 bib1.bibx24" id="paren.48"/> between the start of the simulation and net zero <inline-formula><mml:math id="M58" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> emissions in both <italic>esm-ssp119</italic> and <italic>esm-ssp534-over</italic> (light coloured points in Fig. <xref ref-type="fig" rid="F4"/>). Both models imply a negative zero emissions commitment (ZEC) on the decadal timescale, evidenced by the cumulative emissions-temperature plot curving below the positive emissions phase in the first few decades after net zero <xref ref-type="bibr" rid="bib1.bibx17" id="paren.49"/>, highlighted by the darker points in Fig. <xref ref-type="fig" rid="F4"/>. The decadal timescale negative ZEC in these two models is also reported in idealized <inline-formula><mml:math id="M59" 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>-only experiments to zero emissions in <xref ref-type="bibr" rid="bib1.bibx22" id="text.50"/>, though it should be highlighted that the comparison is not directly applicable as our scenarios go to net negative carbon emissions and include non-<inline-formula><mml:math id="M60" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> forcers. However in NorESM2-LM the ZEC after 100 <inline-formula><mml:math id="M61" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">years</mml:mi></mml:mrow></mml:math></inline-formula> reverses sign and becomes positive, and warming is also reported during net negative carbon emissions phases in idealised overshoot scenarios in this model <xref ref-type="bibr" rid="bib1.bibx46" id="paren.51"/>. In <italic>esm-ssp119</italic> (Fig. <xref ref-type="fig" rid="F4"/>a), GSAT reaches a minimum around 2110, after which warming increases despite still being in a phase of net negative <inline-formula><mml:math id="M62" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> emissions, until stabilization around 2160. NorESM2-LM's response in <italic>esm-ssp534-over</italic> is more extreme (Fig. <xref ref-type="fig" rid="F4"/>b), showing a rapid warming of around 0.8 <inline-formula><mml:math id="M63" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">°</mml:mi><mml:mi mathvariant="normal">C</mml:mi></mml:mrow></mml:math></inline-formula> in the second half of the 22nd century. This is the period shortly after the scenario transitions from a constant negative emissions of <inline-formula><mml:math id="M64" display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>5.2 <inline-formula><mml:math id="M65" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">Gt</mml:mi><mml:mspace width="0.125em" linebreak="nobreak"/><mml:mi mathvariant="normal">C</mml:mi><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 2140 to zero in 2170.</p>

      <fig id="F4" specific-use="star"><label>Figure 4</label><caption><p id="d2e1533">Global-mean surface temperature anomaly as a function of cumulative emissions in MPI-ESM1.2-LR (blue) and NorESM2-LM (red). Light-coloured points show the phase before net zero emissions, dark-coloured points after net zero emissions. Scatter points represent 5-year means of ensemble means. Selected times of five-year means are marked for NorESM2-LM.</p></caption>
          <graphic xlink:href="https://esd.copernicus.org/articles/17/893/2026/esd-17-893-2026-f04.png"/>

        </fig>

</sec>
<sec id="Ch1.S3.SS2">
  <label>3.2</label><title>Carbon cycle response</title>
      <p id="d2e1550">Figure <xref ref-type="fig" rid="F5"/> shows how anthropogenic carbon is distributed between the three main reservoirs on Earth (atmosphere, ocean, land) in NorESM2-LM and MPI-ESM1.2-LR. Generally, both ESMs show a very similar distribution of carbon, in which initially most of the carbon from anthropogenic emissions remains in the atmosphere, with the ocean becoming the dominant sink of carbon in the long term. During the historical period, the land-use driven loss of carbon from the land reservoir is slightly stronger in NorESM2-LM than in MPI-ESM1.2-LR, but this is compensated by a slightly larger oceanic uptake of carbon, so that the atmospheric carbon reservoir remains approximately the same in both models. During the 21st century, the total land carbon uptake in NorESM2-LM catches up with that in MPI-ESM1.2-LR, and by the end of the century, more carbon is stored in the biosphere in NorESM2-LM than in MPI-ESM1.2-LR in all scenarios. At the same time, the total ocean carbon uptake is larger in NorESM2-LM, which explains the apparent reduction in the atmospheric <inline-formula><mml:math id="M66" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> concentration compared to MPI-ESM1.2-LR. After the year 2100, NorESM2-LM is forced with less negative emissions in <italic>esm-ssp119</italic> and has an apparent closure error in the carbon balance in <italic>esm-ssp534-over</italic>, which is an identified issue in many CMIP6 carbon-cycle enabled models <xref ref-type="bibr" rid="bib1.bibx53" id="paren.52"/>. Both cases can be interpreted as forcing NorESM2-LM with less negative <inline-formula><mml:math id="M67" 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> emissions after 2100, and in both cases this leads to roughly 40 <inline-formula><mml:math id="M68" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">GtC</mml:mi></mml:mrow></mml:math></inline-formula> that is added to the Earth system in NorESM2-LM compared to MPI-ESM1.2-LR at the end of the simulation, which complicates the comparison of the two models. Nevertheless, when accounting for this complication, some differences in the long-term carbon cycle response can still be analysed. First, the initially stronger land carbon sink in NorESM2-LM declines after 2100, leading to a cumulative land carbon sink that is smaller in NorESM2-LM than in MPI-ESM1.2-LR in the scenarios <italic>esm-ssp245</italic> and <italic>esm-ssp534-over</italic>. However, this is not the case in <italic>esm-ssp119</italic>, where the land carbon sink of NorESM2-LM still exceeds that of MPI-ESM1.2-LR by around 20 <inline-formula><mml:math id="M69" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">GtC</mml:mi></mml:mrow></mml:math></inline-formula> at the end of the simulation, which is potentially a consequence of the less negative emissions in this simulation in NorESM2-LM. The cumulative land carbon sink in NorESM2-LM shows an approximately similar behaviour in the <italic>esm-ssp119</italic> and <italic>esm-ssp534-over</italic> scenarios, whereas in MPI-ESM1.2-LR it is consistently weaker in <italic>esm-ssp119</italic> than in <italic>esm-ssp534-over</italic>, hence the difference comes mainly from a larger scenario-dependence in MPI-ESM1.2-LR. Many processes could be the cause of this, and a deeper analysis would be necessary for a comprehensive answer. One potential candidate is the smaller difference in global mean temperatures between the two scenarios, when using NorESM2-LM. Second, the generally larger cumulative ocean carbon uptake in NorESM2-LM is unlikely to be solely explainable by the (effectively) higher <inline-formula><mml:math id="M70" 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> emissions in NorESM2-LM, which could also have a range of possible explanations and require a deeper analysis for better understanding.</p>

      <fig id="F5" specific-use="star"><label>Figure 5</label><caption><p id="d2e1638">The distribution of <bold>(a, c, e)</bold> annual and <bold>(b, d, f)</bold> cumulative carbon stocks between atmosphere, ocean and land in the three scenarios <italic>esm-ssp119</italic> <bold>(a, b)</bold>, <italic>esm-ssp245</italic> <bold>(c, d)</bold>, and <italic>esm-ssp534-over</italic> <bold>(e, f)</bold>. The ensemble mean data are shown as a 5-year running mean to reduce interannual variability. Solid lines refer to MPI-ESM1.2-LR and dashed lines refer to NorESM2-LM. The apparent closure error in NorESM2-LM in esm-ssp534-over can be interpreted as less negative emissions of <inline-formula><mml:math id="M71" 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> after 2100, having a similar effect as the less negative emissions prescribed in <italic>esm-ssp119</italic> in NorESM2-LM (Fig. <xref ref-type="fig" rid="F2"/>).</p></caption>
          <graphic xlink:href="https://esd.copernicus.org/articles/17/893/2026/esd-17-893-2026-f05.png"/>

        </fig>

      <p id="d2e1688">In all scenarios, the higher atmospheric <inline-formula><mml:math id="M72" 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> concentrations between 2050–2150 in MPI-ESM1.2-LR can be explained by the weaker ocean and land sink strengths. The weaker land sink is particularly pronounced in <italic>esm-ssp119</italic>, and persists until the end of the simulation (Fig. <xref ref-type="fig" rid="F5"/>b). In both overshoot scenarios, the land and ocean both transition from a net sink to a net source of carbon around 2100 (Fig. <xref ref-type="fig" rid="F5"/>a and e). While the ocean returns to being a carbon sink after 2150, the land continues to emit carbon back to the atmosphere. The annual fluxes are small so these effects are best interpreted from the changes in stocks (Fig. <xref ref-type="fig" rid="F5"/>b and f).</p>
</sec>
<sec id="Ch1.S3.SS3">
  <label>3.3</label><title>Global signs of hysteresis and irreversibility</title>
      <p id="d2e1719">Next, we specifically look for signs of hysteresis and irreversibility in the climate and carbon cycles in the overshoot scenarios. We define hysteresis to mean a dependence on history (path-dependence) and irreversibility to mean an inability to return to a previous state.</p>
      <p id="d2e1722">The Atlantic Meridional Overturning Circulation (AMOC) is often considered to be one of the major tipping elements in the Earth system <xref ref-type="bibr" rid="bib1.bibx35 bib1.bibx63" id="paren.53"/>. Figure <xref ref-type="fig" rid="F6"/> shows that there is a major difference in the evolution of the AMOC between NorESM2-LM and MPI-ESM1.2-LR, with MPI-ESM1.2-LR showing much smaller variations over time. While both models show a reduction in the AMOC index during the warming period, NorESM2-LM also shows an initial increase during the 20th century, and a much stronger reduction during the first half of the 21st century. In contrast to NorESM2-LM, MPI-ESM1.2-LR exhibits a near-linear relationship between global warming and AMOC reduction, which also holds during the cooling periods in the overshoot scenarios. However, this AMOC weakening only starts at around 0.5 <inline-formula><mml:math id="M73" 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> above pre-industrial temperatures. There are also small deviations from the linear relationship in MPI-ESM1.2-LR. In the initially rapidly warming scenario <italic>esm-ssp534-over</italic>, the lowest AMOC indices are reached only after the peak warming period, when the climate has already started to cool. Furthermore, in <italic>esm-ssp245</italic>, there is some AMOC recovery in the late stages of the simulation, already before the warmest year is reached. Both of these effects are also present and even stronger in NorESM2-LM, which does not exhibit the same linear relationship between AMOC and temperature that MPI-ESM1.2-LR shows. In addition, NorESM2-LM also shows a much faster AMOC recovery than MPI-ESM1.2-LR and even an overshoot of the AMOC strength. This is concurrent with the second warming period unique to NorESM2-LM <xref ref-type="bibr" rid="bib1.bibx45" id="paren.54"/>, and may be implicated in the rapid warming in the late 22nd century in this model. The AMOC reduction causes an increased ocean heat uptake, which happens at the same time that atmospheric <inline-formula><mml:math id="M74" 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> is reduced by the negative emissions. When AMOC picks up again at that time atmospheric <inline-formula><mml:math id="M75" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> is approximately stabilized, ocean heat uptake decreases such that SAT increases again. It should be noted that a diversity of Atlantic Ocean heat transport (closely related to AMOC) profiles is seen in other models run with <inline-formula><mml:math id="M76" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> concentrations to 2300 in <italic>ssp534-over</italic>, including a persistent weakened state from the middle of the 21st century, and a continued weakening post-overshoot akin to an AMOC collapse <xref ref-type="bibr" rid="bib1.bibx39" id="paren.55"/>. This highlights the importance of running simulations longer than to 2100.</p>

      <fig id="F6" specific-use="star"><label>Figure 6</label><caption><p id="d2e1791">The evolution of the Atlantic Meridional Overturning Circulation (AMOC) index <bold>(a, d, g)</bold> over time and as a function of the global mean surface temperature (<bold>b, e, h</bold>: MPI-ESM1.2-LR; <bold>c, f, i</bold>: NorESM2-LM) in <bold>(a–c)</bold> <italic>esm-ssp119</italic>; <bold>(d–f)</bold> <italic>esm-ssp245</italic>; <bold>(g–i)</bold> <italic>esm-ssp534-over</italic>. In the left column, the years of peak warming are indicated for MPI-ESM1.2-LR and NorESM2-LM by a vertical line (in <italic>esm-ssp119</italic> the two lines overlap and <italic>esm-ssp245</italic> does not peak before 2300 in NorESM2-LM). In the temperature-AMOC plots, the color of the scatter points is changed after the year of the peak warming (green) compared to before (orange). The scatter plots use five-year averages for both variables.</p></caption>
          <graphic xlink:href="https://esd.copernicus.org/articles/17/893/2026/esd-17-893-2026-f06.png"/>

        </fig>

      <p id="d2e1835">NorESM2-LM shows a lag in its AMOC response rather than true irreversibility, but other components of the Earth system show true signs of irreversibility (Fig. <xref ref-type="fig" rid="F7"/>) on the timescale of our experiments. Although global mean surface temperature (GSAT) stabilizes in the long run in <italic>esm-ssp534-over</italic>, the ocean continues to take up heat. A warmer ocean leads to the thermal expansion of seawater, contributing to sea-level rise (<xref ref-type="bibr" rid="bib1.bibx61" id="altparen.56"/>; Fig. <xref ref-type="fig" rid="F7"/>a–c). A warmer ocean can also hold less dissolved oxygen (<xref ref-type="bibr" rid="bib1.bibx33" id="altparen.57"/>; Fig. <xref ref-type="fig" rid="F7"/>d–f) which can be detrimental to marine ecosystems.</p>

      <fig id="F7" specific-use="star"><label>Figure 7</label><caption><p id="d2e1856">Irreversible global quantities of the Earth system in MPI-ESM1.2-LR and NorESM2-LM, inferred from the overshoot scenario esm-ssp534-over. <bold>(a–c)</bold> thermosteric sea-level rise; <bold>(d–f)</bold> Mass of oxygen in the ocean. In <bold>(a)</bold>, <bold>(d)</bold>, the vertical lines mark the year of peak warming and plots thermosteric sea-level rise and ocean oxygen mass as a function of time. The other columns plot these variables as a function of temperature in <bold>(b, e)</bold> MPI-ESM1.2-LR and <bold>(c, f)</bold> NorESM2-LM.</p></caption>
          <graphic xlink:href="https://esd.copernicus.org/articles/17/893/2026/esd-17-893-2026-f07.png"/>

        </fig>

      <p id="d2e1884">As for the AMOC response, interesting differences between the two ESMs can be observed for sea-level rise and de-oxygenation. After the historical period, sea-level increases monotonically and oxygen mass decreases monotonically in both models, regardless of whether global mean temperature smoothly peaks, declines and stabilizes (in MPI-ESM1.2-LR) or reaches a post-peak minimum before a second warming and stabilization (NorESM2-LM). Continued sea-level rise in overshoot scenarios has also been noted in previous studies with ESMs <xref ref-type="bibr" rid="bib1.bibx19" id="paren.58"/> and sea-level emulators <xref ref-type="bibr" rid="bib1.bibx31" id="paren.59"/>.</p>
</sec>
<sec id="Ch1.S3.SS4">
  <label>3.4</label><title>Regional signs of hysteresis and irreversibility</title>
<sec id="Ch1.S3.SS4.SSS1">
  <label>3.4.1</label><title>Temperature</title>
      <p id="d2e1908">We determine the regional climate characteristics at the same global warming level (GWL) in the <italic>esm-ssp534-over</italic> scenarios in both models.</p>
      <p id="d2e1914">Firstly, we observe that NorESM2-LM has four distinct phases in its global temperature evolution: a warming up until 2060, a cooling from 2060 to 2150, another warming from 2150 to 2200 and a stabilization from 2200 to 2300 (Fig. <xref ref-type="fig" rid="F3"/>), qualitatively similar to the warming-cooling-warming cycles described in idealized NorESM2-LM overshoot simulations by <xref ref-type="bibr" rid="bib1.bibx45" id="text.60"/>. Taking the stabilization period as a 100-year mean GWL of 1.35 <inline-formula><mml:math id="M77" 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> above pre-industrial (yellow shaded period in Fig. <xref ref-type="fig" rid="F8"/>g), we apply this to the 31-year period around the crossing of this GWL in the warming (red shaded) and cooling (blue shaded) periods in Fig. <xref ref-type="fig" rid="F8"/>g.</p>

      <fig id="F8" specific-use="star"><label>Figure 8</label><caption><p id="d2e1939">Global and regional near-surface air temperature projections in <bold>(a–g)</bold> NorESM2-LM and <bold>(h–k)</bold> MPI-ESM1.2-LR in the <italic>esm-ssp534-over</italic> scenario. <bold>(a–c)</bold> regional changes in NorESM2-LM for <bold>(a)</bold> warming; <bold>(b)</bold> cooling; <bold>(c)</bold> long-term stabilization around a 1.35 <inline-formula><mml:math id="M78" 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> GWL. <bold>(d–f)</bold> Differences between <bold>(d)</bold> equilibrium and warming; <bold>(e)</bold> equilibrium and cooling; <bold>(f)</bold> cooling and warming in NorESM2-LM; <bold>(g, h)</bold> 31-year-smoothed timeseries of GSAT for <bold>(g)</bold> NorESM2-LM, showing times of warming (red), cooling (blue) and stabilization (yellow) at the 1.35 <inline-formula><mml:math id="M79" 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> GWL and <bold>(h)</bold> MPI-ESM1.2-LR showing warming (red) and cooling (blue). <bold>(i–k)</bold> regional temperature at 1.35 <inline-formula><mml:math id="M80" 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> GWL in MPI-ESM1.2-LR for <bold>(i)</bold> warming; <bold>(j)</bold> cooling, and <bold>(k)</bold> cooling minus warming. In <bold>(d–f)</bold> and <bold>(k)</bold>, stippling shows areas where the differences are more than twice the standard deviation of the ensemble mean. In <bold>(g)</bold> and <bold>(h)</bold>, red and blue shaded regions show the 31-year period around the ensemble mean 1.35 <inline-formula><mml:math id="M81" 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> GWL, and individual ensemble members may use data from slightly earlier or later periods.</p></caption>
            <graphic xlink:href="https://esd.copernicus.org/articles/17/893/2026/esd-17-893-2026-f08.png"/>

          </fig>

      <p id="d2e2059">MPI-ESM1.2-LR shows three phases, where the first two are similar to NorESM2-LM and the third is a stabilization starting around 2150. We choose to compare the warming and cooling phases at the same 1.35 <inline-formula><mml:math id="M82" 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> GWL used in NorESM2-LM, marked in red and blue respectively in  Fig. <xref ref-type="fig" rid="F8"/>h. Both Fig. <xref ref-type="fig" rid="F8"/>g and h show a 31-year running mean of GSAT, centred on the year in the <inline-formula><mml:math id="M83" display="inline"><mml:mi>x</mml:mi></mml:math></inline-formula> axis.</p>
      <p id="d2e2083">The rest of Fig. <xref ref-type="fig" rid="F8"/> shows the regional patterns of warming at the 1.35 <inline-formula><mml:math id="M84" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">°</mml:mi><mml:mi mathvariant="normal">C</mml:mi></mml:mrow></mml:math></inline-formula> GWL. Figure <xref ref-type="fig" rid="F8"/>a–c show the warming, cooling and stabilization periods in NorESM2-LM, and Fig. <xref ref-type="fig" rid="F8"/>i and j in MPI-ESM1.2-LR. In these plots, red colours show regions warmer than the 1.35 <inline-formula><mml:math id="M85" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">°</mml:mi><mml:mi mathvariant="normal">C</mml:mi></mml:mrow></mml:math></inline-formula> GWL and blue marks regions cooler than 1.35 <inline-formula><mml:math id="M86" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">°</mml:mi><mml:mi mathvariant="normal">C</mml:mi></mml:mrow></mml:math></inline-formula>. In both models and all periods, the Arctic amplification and North Atlantic cold pool are distinct features, as is the contrast between land and ocean, where most land areas, particularly in the Northern Hemisphere, tend to be warmer than the global mean and ocean areas cooler than the global mean. Aside from the North Pacific and the Arctic, the ocean is also cooler than the global mean during the stabilization period. The strong cooling in the North Atlantic (where some regions are cooler than pre-industrial, despite the global mean warming being <inline-formula><mml:math id="M87" display="inline"><mml:mrow><mml:mo>+</mml:mo><mml:mn mathvariant="normal">1.35</mml:mn></mml:mrow></mml:math></inline-formula> <inline-formula><mml:math id="M88" 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>) during the cooling phase of NorESM2-LM is consistent with the period of weakest AMOC (Fig. <xref ref-type="fig" rid="F6"/>), showing the profound influence of the overturning circulation on transporting heat towards Western Europe.</p>
      <p id="d2e2145">Comparing differences between periods, we see that there is a more distinct asymmetry in regional temperatures between the cooling and warming phases in NorESM2-LM compared to MPI-ESM1.2-LR (Fig. <xref ref-type="fig" rid="F8"/>f and k). NorESM2-LM loses heat from the Northern Hemisphere extratropics during the cooling phase, whereas the tropics and Southern Hemisphere are relatively warmer. In contrast, there are fewer regions of significant difference in MPI-ESM1.2-LR, suggesting that near-surface air temperature is more reversible in this model. While not directly comparable (analysing the stabilisation phase of an overshoot experiment relative to a zero-emissions commitment experiment), there is a diversity in hemispheric warming patterns post-net zero across the CMIP6 population <xref ref-type="bibr" rid="bib1.bibx3 bib1.bibx23" id="paren.61"/> and therefore it is not surprising that the regional responses of the two models may differ.</p>
      <p id="d2e2153">The equilibrium period in NorESM2-LM is qualitatively different to both the warming and cooling periods. In equilibrium, the AMOC has recovered to a strength exceeding that of the warming phase, with enhanced oceanic heat transport resulting in a distinctly warmer Northern Hemisphere ocean (Fig. <xref ref-type="fig" rid="F8"/>d). Other changes between equilibrium and warming are significant, but not as stark as the contrast between the equilibrium and cooling phases (Fig. <xref ref-type="fig" rid="F8"/>e), where large hemispheric differences are apparent.</p>
      <p id="d2e2160">In contrast to NorESM2-LM, other CMIP6 models in the multi-model mean under <italic>ssp534-over</italic> have a warmer Southern Hemisphere and cooler Northern Hemisphere in equilibrium compared with the warming phase at approximately the same GWL <xref ref-type="bibr" rid="bib1.bibx38" id="paren.62"/> as a consequence of a North-to-South transport of heat that commences at approximately the time of peak warming and persists into the 23rd century.</p>
</sec>
<sec id="Ch1.S3.SS4.SSS2">
  <label>3.4.2</label><title>Precipitation</title>
      <p id="d2e2177">Figure <xref ref-type="fig" rid="F9"/> shows the global and regional patterns of precipitation for the warming and cooling phases at the 1.35 <inline-formula><mml:math id="M89" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">°</mml:mi><mml:mi mathvariant="normal">C</mml:mi></mml:mrow></mml:math></inline-formula> GWL.</p>

      <fig id="F9" specific-use="star"><label>Figure 9</label><caption><p id="d2e2194">As Fig. <xref ref-type="fig" rid="F8"/>, for precipitation. In <bold>(a)</bold>–<bold>(c)</bold> and <bold>(i)</bold>, <bold>(j)</bold>, anomalies are shown relative to pre-industrial. In <bold>(g)</bold> and <bold>(h)</bold>, global means of both GSAT (green) and precipitation (purple) are shown.</p></caption>
            <graphic xlink:href="https://esd.copernicus.org/articles/17/893/2026/esd-17-893-2026-f09.png"/>

          </fig>

      <p id="d2e2224">In Fig. <xref ref-type="fig" rid="F9"/>g and h, the global mean precipitation (purple curves) is shown superimposed on the GSAT anomaly (green curves). In both models, there is a lag in the response of global mean precipitation to global mean temperature, noting that precipitation response depends on the combination of climate forcers in addition to GSAT <xref ref-type="bibr" rid="bib1.bibx2" id="paren.63"/>. Both models project global mean precipitation in the cooling period to be higher than in the warming period, and in NorESM2-LM's case, the stabilization period is wetter still.</p>
      <p id="d2e2233">In both models during the warming phase, the inter-tropical convergence zone (ITCZ) shifts northward (Fig. <xref ref-type="fig" rid="F9"/>a and i), which is consistent with the general hypothesis that the ITCZ moves towards the hemisphere with greater warming (refer to Fig. <xref ref-type="fig" rid="F8"/>a and i), and other (concentration-driven) overshoot simulations from CMIP6 models <xref ref-type="bibr" rid="bib1.bibx4 bib1.bibx18" id="text.64"/>. These differences persist in the cooling and stabilization phases (Fig. <xref ref-type="fig" rid="F9"/>b, c, and j). Further analysing the differences in the phases, it can be noted that the ITCZ is northward shifted in the stabilization relative to warming, which also shows a generally wetter Northern Hemisphere (Fig. <xref ref-type="fig" rid="F9"/>d). This is also true, though less clear, in the cooling minus warming differences in both models (Fig. <xref ref-type="fig" rid="F9"/>f and k). Again, the equilibrium minus cooling phase in NorESM2-LM is interesting (Fig. <xref ref-type="fig" rid="F9"/>e), with the ITCZ shifted southwards reflecting the relatively cooler Northern Hemisphere when comparing these two periods due to the weakened AMOC <xref ref-type="bibr" rid="bib1.bibx29" id="paren.65"/>. This results in a larger interhemispheric temperature gradient in the cooling phase in NorESM2-LM. This behaviour is consistent with the results of <xref ref-type="bibr" rid="bib1.bibx51" id="text.66"/> for NorESM2-LM. Owing to the greater variability in precipitation, the regional changes are significant in a smaller proportion of the globe than for temperature.</p>
      <p id="d2e2258">Comparisons can again be drawn with other (concentration-driven) CMIP6 models for NorESM2-LM. In general, owing to the warmer Northern Hemisphere in the stabilization phase compared to warming phase, the ITCZ is more northerly located during the stabilization period (Fig. <xref ref-type="fig" rid="F9"/>d), which is in contrast to the CMIP6 model mean <xref ref-type="bibr" rid="bib1.bibx38" id="paren.67"/>. However, NorESM2-LM shares the feature of increased precipitation in the eastern Pacific south of the equator with the CMIP6 model mean.</p>
</sec>
<sec id="Ch1.S3.SS4.SSS3">
  <label>3.4.3</label><title>Net primary productivity</title>
      <p id="d2e2274">Finally, we demonstrate one aspect of the regional terrestrial carbon cycle response, the net primary productivity (NPP), which describes the amount of carbon taken up by photosynthesis minus the carbon loss through vegetation respiration.</p>
      <p id="d2e2277">In both models there is an overall net uptake in carbon in the land system relative to pre-industrial over all three future time periods (Fig. <xref ref-type="fig" rid="F10"/>a–c and g–j), which is likely due to the <inline-formula><mml:math id="M90" 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> fertilisation effect. Nevertheless, some areas show a net carbon loss, including the region south-east of the Amazon (both models) and eastern North America (MPI-ESM1.2-LR).</p>

      <fig id="F10" specific-use="star"><label>Figure 10</label><caption><p id="d2e2295">As Fig. <xref ref-type="fig" rid="F9"/>, for net primary productivity. In <bold>(a)</bold>–<bold>(c)</bold> and <bold>(i)</bold>, <bold>(j)</bold>, anomalies are shown relative to pre-industrial. In <bold>(g)</bold> and <bold>(h)</bold>, global mean GSAT anomaly (green) and total net primary productivity (purple) are shown.</p></caption>
            <graphic xlink:href="https://esd.copernicus.org/articles/17/893/2026/esd-17-893-2026-f10.png"/>

          </fig>

      <p id="d2e2326">Furthermore, analysis of the global NPP shows that in the long term carbon sinks are not as productive at the same warming levels than they are in periods close to the start of the simulation (Fig. <xref ref-type="fig" rid="F10"/>g and h). NPP more closely follows the evolution of atmospheric <inline-formula><mml:math id="M91" 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> than temperature (Fig. <xref ref-type="fig" rid="FA1"/>) which is related to the fertilisation effect, but this correspondence is not exact. There are also differences between the cooling and warming phases in both models. On the global scale, NorESM2-LM has higher NPP during the cooling phase than the warming phase, but MPI-ESM1.2-LR has lower NPP in the cooling phase relative to the warming phase. At the regional scale, NorESM2-LM (Fig. <xref ref-type="fig" rid="F10"/>f) is taking up more carbon in North America but less in boreal Europe, whereas MPI-ESM1.2-LR is showing a reduced carbon uptake in the Amazon, eastern North America and sub-Saharan Africa, and an increase in Siberia (Fig. <xref ref-type="fig" rid="F10"/>k).</p>
</sec>
</sec>
</sec>
<sec id="Ch1.S4" sec-type="conclusions">
  <label>4</label><title>Discussion and conclusions</title>
      <p id="d2e2358">We present two <inline-formula><mml:math id="M92" 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> emissions-driven ESMs run to 2300 under three different emissions scenarios: <italic>esm-ssp119</italic> (a scenario designed to limit long-term warming to 1.5 <inline-formula><mml:math id="M93" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">°</mml:mi><mml:mi mathvariant="normal">C</mml:mi></mml:mrow></mml:math></inline-formula> with a small and temporary overshoot), <italic>esm-ssp245</italic> (a roughly “current policies” scenario leading to around 2.5–3 <inline-formula><mml:math id="M94" 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> warming in 2100) and <italic>esm-ssp534-over</italic> (a “high overshoot” scenario with very high greenhouse gas emissions in the short term and large amounts of carbon removal in the longer term). Each ESM has run multiple ensemble members for each scenario, which enables us to separate the forced signal from internal variability. The number of ensemble members required depends on the phenomenon being investigated: for global and regional mean state variables reported in this paper (temperature, precipitation, NPP, carbon fluxes and stocks, AMOC strength, thermosteric sea-level rise and ocean oxygen content) three members is likely sufficient to determine significant differences, though extremes (not evaluated in this paper) would benefit from a larger ensemble.  We note several similarities and differences between the models. The two models have very different temperature responses, due to differences in the response of ocean circulation to climate forcing, especially for scenarios <italic>esm-ssp119</italic> and <italic>esm-ssp534-over</italic>. Both NorESM2-LM and MPI-ESM1.2-LR peak in temperature in the 21st century, but while MPI-ESM1.2-LR declines and stabilizes thereafter, NorESM2-LM goes into a new warming phase that stabilizes in the 23rd century. Despite these differences, there are many responses that are similar in the two models. Considering <italic>esm-ssp534-over</italic> specifically we find that both models show:</p>
      <p id="d2e2411"><list list-type="order">
          <list-item>

      <p id="d2e2416">a similar global distribution of anthropogenic carbon emissions among the atmosphere, ocean, and land. At the beginning of the simulations, most of the carbon remains in the atmosphere, but in the long term, the ocean becomes the dominant carbon reservoir;</p>
          </list-item>
          <list-item>

      <p id="d2e2422">a transition from carbon sink to carbon source: In both overshoot scenarios, both the land and ocean systems transition from being net carbon sinks to carbon sources around the year 2100. After 2150, the ocean resumes absorbing carbon, while the land continues to release carbon to the atmosphere;</p>
          </list-item>
          <list-item>

      <p id="d2e2428">a similar global response of precipitation to temperature changes, where global precipitation is higher during the cooling phase than during the warming phase;</p>
          </list-item>
          <list-item>

      <p id="d2e2434">a northward shift of the ITCZ during the warming phase, with similar patterns being observed during the cooling and stabilization phases;</p>
          </list-item>
          <list-item>

      <p id="d2e2440">long-term irreversibility in sea level and ocean deoxygenation, which are largely irreversible even after temperatures decline on the timescales of these simulations.</p>
          </list-item>
        </list></p>
      <p id="d2e2445">In contrast, there are differences in the global and regional responses to <inline-formula><mml:math id="M95" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> emissions between the models resulting from varying sink strengths in the global carbon cycle and patterns of ocean warming. NorESM2-LM shows substantial hysteresis in its AMOC strength and regional patterns of warming when comparing periods before and after peak warming. MPI-ESM1.2-LR is more reversible in its AMOC and regional pattern of warming. While the main focus of our analysis of irreversibility was the <italic>esm-ssp534-over</italic> simulations, we note qualitatively similar behaviour for the smaller overshoot <italic>esm-ssp119</italic> scenario for global temperature as a function of emissions. We find a similar pattern of regional temperature and precipitation response to periods before and after peak warming in the MPI-ESM1.2-LR model to concentration-driven scenarios in <xref ref-type="bibr" rid="bib1.bibx34" id="text.68"/>, indicating that physical climate responses are likely not sensitive to whether scenarios are run with prescribed emissions or concentrations.</p>
      <p id="d2e2468">While <italic>esm-ssp534-over</italic> was designed as a relatively extreme narrative to test the responses of ESMs to negative emissions, a large class of emissions scenarios that peak warming in the 1.5–2.0 <inline-formula><mml:math id="M96" 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> range before declining towards the end of the 21st century were submitted by IAM teams to the IPCC Sixth Assessment Report <xref ref-type="bibr" rid="bib1.bibx36" id="paren.69"/>. It is very likely that overshoot is required to limit global mean warming to 1.5 <inline-formula><mml:math id="M97" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">°</mml:mi><mml:mi mathvariant="normal">C</mml:mi></mml:mrow></mml:math></inline-formula> in the long term due to a lack of action on greenhouse gas emissions reductions in the last decade <xref ref-type="bibr" rid="bib1.bibx43" id="paren.70"/>. Therefore, given the diversity of the responses of these two models to these scenarios, further investigation should target a larger set of models and additional overshoot pathways.</p>
      <p id="d2e2501">From a peak global mean temperature perspective, the results presented in this paper probably represent a “best case” scenario. Both models have a (150-year Gregory regression-derived) climate sensitivity on the low side of the CMIP6 range, and have a strongly negative ZEC meaning that temperatures are expected to cool after net zero <inline-formula><mml:math id="M98" 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> is reached <xref ref-type="bibr" rid="bib1.bibx22" id="paren.71"/>, notwithstanding the influence of non-<inline-formula><mml:math id="M99" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> forcers. The <italic>esm-ssp119</italic> simulations peak below 1.5 <inline-formula><mml:math id="M100" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">°</mml:mi><mml:mi mathvariant="normal">C</mml:mi></mml:mrow></mml:math></inline-formula> in both models and are likely biased cool relative to historical GSAT change. The combination of low (Gregory) climate sensitivity, strong negative ZEC, and potential low-biased ensemble mean warming levels mean that the outcomes presented in the paper may underestimate the risks and challenges associated with overshoot scenarios. In addition, while on the cool side in terms of GSAT, the projections from NorESM2-LM suggest that large abrupt changes in AMOC, rapid phase of warming during the late 22nd century, and substantial regional changes such as cooling in Europe during the slowdown phase may pose more severe adaptation challenges than a model with higher peak warming but a more reversible regional climate profile. In reality, the Earth system's response could be more severe, with greater irreversibility and fewer opportunities for recovery. In order to sample the full range of plausible futures in response to <inline-formula><mml:math id="M101" 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> emissions, more participating models running several different <inline-formula><mml:math id="M102" 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> emissions-driven scenarios, with and without overshoot, are required <xref ref-type="bibr" rid="bib1.bibx41" id="paren.72"/>. Even within our two-model ensemble we see very different long-term behaviours, and NorESM2-LM suggests that the risks of AMOC slowdown and regional cooling over Europe, as well as an unexpected warming rebound once negative emissions cease, cannot be ruled out.</p>
</sec>

      
      </body>
    <back><app-group>

<app id="App1.Ch1.S1">
  <label>Appendix A</label><title/>

      <fig id="FA1"><label>Figure A1</label><caption><p id="d2e2582">As Fig. <xref ref-type="fig" rid="F10"/>g and h, showing the global total net primary productivity (purple) compared to the global mean <inline-formula><mml:math id="M103" 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> concentration (green) in NorESM2-LM (left) and MPI-ESM1.2-LR (right).</p></caption>
        
        <graphic xlink:href="https://esd.copernicus.org/articles/17/893/2026/esd-17-893-2026-f11.png"/>

      </fig>

</app>
  </app-group><notes notes-type="dataavailability"><title>Data availability</title>

      <p id="d2e2610">The MPI-ESM1.2-LR output data is available on the DKRZ node of the Earth System Grid Federation at <uri>https://esgf-metagrid.cloud.dkrz.de/search</uri> (last access: 22 June 2026) under project MPI-Edriven-LE. NorESM2-LM data is accessed through creating an account on the Norwegian Supercomputing Centre sigma2 service at <uri>https://www.sigma2.no/</uri> (last access: 22 June 2026) and requesting access to project NS10013K.</p>
  </notes><notes notes-type="authorcontribution"><title>Author contributions</title>

      <p id="d2e2622">Conceptualisation: CS, AG, CL, CM. Funding acquisition: CS, CL, CM. Investigation: LR, AG, HL, TI, TB, JS, ARP. Methodology: LR, CDW, AM. Supervision: CS, CL. Visualisation: CS, LR, CDW, AM. Writing  –  original draft: CS, LR, CDW. Writing  –  review and editing: CS, LR, CDW, AM, TI, AG, TB, JS, CL, CM</p>
  </notes><notes notes-type="competinginterests"><title>Competing interests</title>

      <p id="d2e2628">The contact author has declared that none of the authors has any competing interests.</p>
  </notes><notes notes-type="disclaimer"><title>Disclaimer</title>

      <p id="d2e2634">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="d2e2640">Computational resources were provided by the German Climate Computing Center (DKRZ).</p></ack><notes notes-type="financialsupport"><title>Financial support</title>

      <p id="d2e2647">This research has been supported by the HORIZON EUROPE Climate, Energy and Mobility (grant no. 101081661).  ARP was supported by the Leeds-York-Hull Natural Environment Research Council (NERC) Doctoral Training Partnership (DTP) Panorama under grant NE/S007458/1. JS and TB have received funding from the European Union's Horizon Europe research and innovation programme under grant agreement no. 101056939 (project RESCUE). TI and CL were supported by the German Research Foundation (DFG) under Germany's Excellence Strategy–EXC 2037 “CLICCS–Climate, Climatic Change, and Society” – Project Number 390683824, as well as by the EU Horizon 2020 research and innovation program under grant agreement 101003536 (project ESM2025–Earth System Models for the Future).</p>
  </notes><notes notes-type="reviewstatement"><title>Review statement</title>

      <p id="d2e2653">This paper was edited by Kirsten Zickfeld and reviewed by Mitchell Dickau and one anonymous referee.</p>
  </notes><ref-list>
    <title>References</title>

      <ref id="bib1.bibx1"><label>Allen et al.(2009)</label><mixed-citation> Allen, M. R., Frame, D. J., Huntingford, C., Jones, C. D., Lowe, J. A., Meinshausen, M., and Meinshausen, N.: Warming caused by cumulative carbon emissions towards the trillionth tonne, Nature, 458, 1163, 2009.</mixed-citation></ref>
      <ref id="bib1.bibx2"><label>Andrews et al.(2010)</label><mixed-citation>Andrews, T., Forster, P. M., Boucher, O., Bellouin, N., and Jones, A.: Precipitation, radiative forcing and global temperature change, Geophys. Res. Lett., 37, 2010GL043991, <ext-link xlink:href="https://doi.org/10.1029/2010GL043991" ext-link-type="DOI">10.1029/2010GL043991</ext-link>, 2010.</mixed-citation></ref>
      <ref id="bib1.bibx3"><label>Cassidy et al.(2024)</label><mixed-citation>Cassidy, L. J., King, A. D., Brown, J. R., MacDougall, A. H., Ziehn, T., Min, S.-K., and Jones, C. D.: Regional temperature extremes and vulnerability under net zero <inline-formula><mml:math id="M104" 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> emissions, Environ. Res. Lett., 19, 014051, <ext-link xlink:href="https://doi.org/10.1088/1748-9326/ad114a" ext-link-type="DOI">10.1088/1748-9326/ad114a</ext-link>, 2024.</mixed-citation></ref>
      <ref id="bib1.bibx4"><label>Douglas et al.(2025)</label><mixed-citation>Douglas, H. C., Revell, L. E., King, A., Harrington, L. J., and Frame, D. J.: Effects of temperature overshoot amplitude on regional climate, Environ. Res. Lett., 20, 114043, <ext-link xlink:href="https://doi.org/10.1088/1748-9326/ae114f" ext-link-type="DOI">10.1088/1748-9326/ae114f</ext-link>, 2025.</mixed-citation></ref>
      <ref id="bib1.bibx5"><label>Eyring et al.(2016)</label><mixed-citation>Eyring, V., Bony, S., Meehl, G. A., Senior, C. A., Stevens, B., Stouffer, R. J., and Taylor, K. E.: Overview of the Coupled Model Intercomparison Project Phase 6 (CMIP6) experimental design and organization, Geosci. Model Dev., 9, 1937–1958, <ext-link xlink:href="https://doi.org/10.5194/gmd-9-1937-2016" ext-link-type="DOI">10.5194/gmd-9-1937-2016</ext-link>, 2016.</mixed-citation></ref>
      <ref id="bib1.bibx6"><label>Forster et al.(2025)</label><mixed-citation>Forster, P. M., Smith, C., Walsh, T., Lamb, W. F., Lamboll, R., Cassou, C., Hauser, M., Hausfather, Z., Lee, J.-Y., Palmer, M. D., von Schuckmann, K., Slangen, A. B. A., Szopa, S., Trewin, B., Yun, J., Gillett, N. P., Jenkins, S., Matthews, H. D., Raghavan, K., Ribes, A., Rogelj, J., Rosen, D., Zhang, X., Allen, M., Aleluia Reis, L., Andrew, R. M., Betts, R. A., Borger, A., Broersma, J. A., Burgess, S. N., Cheng, L., Friedlingstein, P., Domingues, C. M., Gambarini, M., Gasser, T., Gütschow, J., Ishii, M., Kadow, C., Kennedy, J., Killick, R. E., Krummel, P. B., Liné, A., Monselesan, D. P., Morice, C., Mühle, J., Naik, V., Peters, G. P., Pirani, A., Pongratz, J., Minx, J. C., Rigby, M., Rohde, R., Savita, A., Seneviratne, S. I., Thorne, P., Wells, C., Western, L. M., van der Werf, G. R., Wijffels, S. E., Masson-Delmotte, V., and Zhai, P.: Indicators of Global Climate Change 2024: annual update of key indicators of the state of the climate system and human influence, Earth Syst. Sci. Data, 17, 2641–2680, <ext-link xlink:href="https://doi.org/10.5194/essd-17-2641-2025" ext-link-type="DOI">10.5194/essd-17-2641-2025</ext-link>, 2025.</mixed-citation></ref>
      <ref id="bib1.bibx7"><label>Frenger et al.(2025)</label><mixed-citation>Frenger, I., Frey, S., Oschlies, A., Getzlaff, J., Martin, T., and Koeve, W.: Southern Ocean heat burp in a cooling world, AGU Advances, 6, e2025AV001700, <ext-link xlink:href="https://doi.org/10.1029/2025AV001700" ext-link-type="DOI">10.1029/2025AV001700</ext-link>, 2025.</mixed-citation></ref>
      <ref id="bib1.bibx8"><label>Friedlingstein et al.(2006)</label><mixed-citation>Friedlingstein, P., Cox, P., Betts, R., Bopp, L., Von Bloh, W., Brovkin, V., Cadule, P., Doney, S., Eby, M., Fung, I., Bala, G., John, J., Jones, C., Joos, F., Kato, T., Kawamiya, M., Knorr, W., Lindsay, K., Matthews, H. D., Raddatz, T., Rayner, P., Reick, C., Roeckner, E., Schnitzler, K.-G., Schnur, R., Strassmann, K., Weaver, A. J., Yoshikawa, C., and Zeng, N.: Climate–carbon cycle feedback analysis: results from the C4MIP model intercomparison, J. Climate, 19, 3337–3353, <ext-link xlink:href="https://doi.org/10.1175/JCLI3800.1" ext-link-type="DOI">10.1175/JCLI3800.1</ext-link>, 2006.</mixed-citation></ref>
      <ref id="bib1.bibx9"><label>Fyfe et al.(2021)</label><mixed-citation>Fyfe, J. C., Kharin, V. V., Swart, N., Flato, G. M., Sigmond, M., and Gillett, N. P.: Quantifying the influence of short-term emission reductions on climate, Science Advances, 7, eabf7133, <ext-link xlink:href="https://doi.org/10.1126/sciadv.abf7133" ext-link-type="DOI">10.1126/sciadv.abf7133</ext-link>, 2021.</mixed-citation></ref>
      <ref id="bib1.bibx10"><label>Gjermundsen et al.(2021)</label><mixed-citation>Gjermundsen, A., Nummelin, A., Olivié, D., Bentsen, M., Seland, Ø., and Schulz, M.: Shutdown of Southern Ocean convection controls long-term greenhouse gas-induced warming, Nat. Geosci., 14, 724–731, <ext-link xlink:href="https://doi.org/10.1038/s41561-021-00825-x" ext-link-type="DOI">10.1038/s41561-021-00825-x</ext-link>, 2021.</mixed-citation></ref>
      <ref id="bib1.bibx11"><label>Hausfather(2025)</label><mixed-citation>Hausfather, Z.: An assessment of current policy scenarios over the 21st century and the reduced plausibility of high-emissions pathways, Dialogues on Climate Change, 29768659241304854, <ext-link xlink:href="https://doi.org/10.1177/29768659241304854" ext-link-type="DOI">10.1177/29768659241304854</ext-link>, 2025.</mixed-citation></ref>
      <ref id="bib1.bibx12"><label>Hausfather and Peters(2020)</label><mixed-citation>Hausfather, Z. and Peters, G. P.: Emissions – the `business as usual' story is misleading, Nature, 577, 618–620, <ext-link xlink:href="https://doi.org/10.1038/d41586-020-00177-3" ext-link-type="DOI">10.1038/d41586-020-00177-3</ext-link>, 2020.</mixed-citation></ref>
      <ref id="bib1.bibx13"><label>Jones et al.(2016)</label><mixed-citation>Jones, C. D., Arora, V., Friedlingstein, P., Bopp, L., Brovkin, V., Dunne, J., Graven, H., Hoffman, F., Ilyina, T., John, J. G., Jung, M., Kawamiya, M., Koven, C., Pongratz, J., Raddatz, T., Randerson, J. T., and Zaehle, S.: C4MIP – The Coupled Climate–Carbon Cycle Model Intercomparison Project: experimental protocol for CMIP6, Geosci. Model Dev., 9, 2853–2880, <ext-link xlink:href="https://doi.org/10.5194/gmd-9-2853-2016" ext-link-type="DOI">10.5194/gmd-9-2853-2016</ext-link>, 2016.</mixed-citation></ref>
      <ref id="bib1.bibx14"><label>Keller et al.(2018)</label><mixed-citation>Keller, D. P., Lenton, A., Scott, V., Vaughan, N. E., Bauer, N., Ji, D., Jones, C. D., Kravitz, B., Muri, H., and Zickfeld, K.: The Carbon Dioxide Removal Model Intercomparison Project (CDRMIP): rationale and experimental protocol for CMIP6, Geosci. Model Dev., 11, 1133–1160, <ext-link xlink:href="https://doi.org/10.5194/gmd-11-1133-2018" ext-link-type="DOI">10.5194/gmd-11-1133-2018</ext-link>, 2018.</mixed-citation></ref>
      <ref id="bib1.bibx15"><label>King et al.(2024)</label><mixed-citation>King, A. D., Ziehn, T., Chamberlain, M., Borowiak, A. R., Brown, J. R., Cassidy, L., Dittus, A. J., Grose, M., Maher, N., Paik, S., Perkins-Kirkpatrick, S. E., and Sengupta, A.: Exploring climate stabilisation at different global warming levels in ACCESS-ESM-1.5, Earth Syst. Dynam., 15, 1353–1383, <ext-link xlink:href="https://doi.org/10.5194/esd-15-1353-2024" ext-link-type="DOI">10.5194/esd-15-1353-2024</ext-link>, 2024.</mixed-citation></ref>
      <ref id="bib1.bibx16"><label>Koven et al.(2022)</label><mixed-citation>Koven, C. D., Arora, V. K., Cadule, P., Fisher, R. A., Jones, C. D., Lawrence, D. M., Lewis, J., Lindsay, K., Mathesius, S., Meinshausen, M., Mills, M., Nicholls, Z., Sanderson, B. M., Séférian, R., Swart, N. C., Wieder, W. R., and Zickfeld, K.: Multi-century dynamics of the climate and carbon cycle under both high and net negative emissions scenarios, Earth Syst. Dynam., 13, 885–909, <ext-link xlink:href="https://doi.org/10.5194/esd-13-885-2022" ext-link-type="DOI">10.5194/esd-13-885-2022</ext-link>, 2022.</mixed-citation></ref>
      <ref id="bib1.bibx17"><label>Koven et al.(2023)</label><mixed-citation>Koven, C. D., Sanderson, B. M., and Swann, A. L. S.: Much of zero emissions commitment occurs before reaching net zero emissions, Environ. Res. Lett., 18, 014017, <ext-link xlink:href="https://doi.org/10.1088/1748-9326/acab1a" ext-link-type="DOI">10.1088/1748-9326/acab1a</ext-link>, 2023.</mixed-citation></ref>
      <ref id="bib1.bibx18"><label>Kug et al.(2022)</label><mixed-citation>Kug, J.-S., Oh, J.-H., An, S.-I., Yeh, S.-W., Min, S.-K., Son, S.-W., Kam, J., Ham, Y.-G., and Shin, J.: Hysteresis of the intertropical convergence zone to <inline-formula><mml:math id="M105" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> forcing, Nat. Clim. Change, 12, 47–53, <ext-link xlink:href="https://doi.org/10.1038/s41558-021-01211-6" ext-link-type="DOI">10.1038/s41558-021-01211-6</ext-link>, 2022.</mixed-citation></ref>
      <ref id="bib1.bibx19"><label>Lacroix et al.(2024)</label><mixed-citation>Lacroix, F., Burger, F. A., Silvy, Y., Schleussner, C., and Frölicher, T. L.: Persistently elevated high latitude ocean temperatures and global sea level following temporary temperature overshoots, Earths Future, 12, e2024EF004862, <ext-link xlink:href="https://doi.org/10.1029/2024EF004862" ext-link-type="DOI">10.1029/2024EF004862</ext-link>, 2024.</mixed-citation></ref>
      <ref id="bib1.bibx20"><label>Lee et al.(2021)</label><mixed-citation>Lee, J.-Y., Marotzke, J., Bala, G., Cao, L., Corti, S., Dunne, J., Engelbrecht, F., Fischer, E., Fyfe, J., Jones, C., Maycock, A., Mutemi, J., Ndiaye, O., Panickal, S., and Zhou, T.: Future global climate: scenario-based projections and near-term information, in: Climate Change 2021: The Physical Science Basis. Contribution of Working Group I to the Sixth Assessment Report of the Intergovernmental Panel on Climate Change, edited by: Masson-Delmotte, V., Zhai, P., Pirani, A., Connors, S. L., Péan, C., Berger, S., Caud, N., Chen, Y., Goldfarb, L., Gomis, M. I., Huang, M., Leitzell, K., Lonnoy, E., Matthews, J. B. R., Maycock, T. K., Waterfield, T., Yelekçi, O., Yu, R., and Zhou, B., Sect. 4, Cambridge University Press, Cambridge, UK and New York, NY, USA, <ext-link xlink:href="https://doi.org/10.1017/9781009157896.006" ext-link-type="DOI">10.1017/9781009157896.006</ext-link>, 553–672, 2021.</mixed-citation></ref>
      <ref id="bib1.bibx21"><label>Lyon et al.(2022)</label><mixed-citation>Lyon, C., Saupe, E. E., Smith, C. J., Hill, D. J., Beckerman, A. P., Stringer, L. C., Marchant, R., McKay, J., Burke, A., O'Higgins, P., Dunhill, A. M., Allen, B. J., Riel Salvatore, J., and Aze, T.: Climate change research and action must look beyond 2100, Glob. Change Biol., 28, 349–361, <ext-link xlink:href="https://doi.org/10.1111/gcb.15871" ext-link-type="DOI">10.1111/gcb.15871</ext-link>, 2022.</mixed-citation></ref>
      <ref id="bib1.bibx22"><label>MacDougall et al.(2020)</label><mixed-citation>MacDougall, A. H., Frölicher, T. L., Jones, C. D., Rogelj, J., Matthews, H. D., Zickfeld, K., Arora, V. K., Barrett, N. J., Brovkin, V., Burger, F. A., Eby, M., Eliseev, A. V., Hajima, T., Holden, P. B., Jeltsch-Thömmes, A., Koven, C., Mengis, N., Menviel, L., Michou, M., Mokhov, I. I., Oka, A., Schwinger, J., Séférian, R., Shaffer, G., Sokolov, A., Tachiiri, K., Tjiputra , J., Wiltshire, A., and Ziehn, T.: Is there warming in the pipeline? A multi-model analysis of the Zero Emissions Commitment from <inline-formula><mml:math id="M106" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub><mml:mo>,</mml:mo></mml:mrow></mml:math></inline-formula> Biogeosciences, 17, 2987–3016, <ext-link xlink:href="https://doi.org/10.5194/bg-17-2987-2020" ext-link-type="DOI">10.5194/bg-17-2987-2020</ext-link>, 2020.</mixed-citation></ref>
      <ref id="bib1.bibx23"><label>MacDougall et al.(2022)</label><mixed-citation>MacDougall, A. H., Mallett, J., Hohn, D., and Mengis, N.: Substantial regional climate change expected following cessation of <inline-formula><mml:math id="M107" 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> emissions, Environ. Res. Lett., 17, 114046, <ext-link xlink:href="https://doi.org/10.1088/1748-9326/ac9f59" ext-link-type="DOI">10.1088/1748-9326/ac9f59</ext-link>, 2022.</mixed-citation></ref>
      <ref id="bib1.bibx24"><label>Matthews et al.(2009)</label><mixed-citation>Matthews, H. D., Gillett, N. P., Stott, P. A., and Zickfeld, K.: The proportionality of global warming to cumulative carbon emissions, Nature, 459, 829–832, <ext-link xlink:href="https://doi.org/10.1038/nature08047" ext-link-type="DOI">10.1038/nature08047</ext-link>, 2009.</mixed-citation></ref>
      <ref id="bib1.bibx25"><label>Mauritsen et al.(2019)</label><mixed-citation>Mauritsen, T., Bader, J., Becker, T., Behrens, J., Bittner, M., Brokopf, R., Brovkin, V., Claussen, M., Crueger, T., Esch, M., Fast, I., Fiedler, S., Fläschner, D., Gayler, V., Giorgetta, M., Goll, D. S., Haak, H., Hagemann, S., Hedemann, C., Hohenegger, C., Ilyina, T., Jahns, T., Jimenéz de la Cuesta, D., Jungclaus, J., Kleinen, T., Kloster, S., Kracher, D., Kinne, S., Kleberg, D., Lasslop, G., Kornblueh, L., Marotzke, J., Matei, D., Meraner, K., Mikolajewicz, U., Modali, K., Möbis, B., Müller, W. A., Nabel, J. E. M. S., Nam, C. C. W., Notz, D., Nyawira, S., Paulsen, H., Peters, K., Pincus, R., Pohlmann, H., Pongratz, J., Popp, M., Raddatz, T. J., Rast, S., Redler, R., Reick, C. H., Rohrschneider, T., Schemann, V., Schmidt, H., Schnur, R., Schulzweida, U., Six, K. D., Stein, L., Stemmler, I., Stevens, B., Von Storch, J., Tian, F., Voigt, A., Vrese, P., Wieners, K., Wilkenskjeld, S., Winkler, A., and Roeckner, E.: Developments in the MPI M Earth system model version 1.2 (MPI ESM1.2) and its response to increasing <inline-formula><mml:math id="M108" 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>, J. Adv. Model. Earth Sy., 11, 998–1038, <ext-link xlink:href="https://doi.org/10.1029/2018MS001400" ext-link-type="DOI">10.1029/2018MS001400</ext-link>, 2019.</mixed-citation></ref>
      <ref id="bib1.bibx26"><label>Meinshausen et al.(2011)</label><mixed-citation>Meinshausen, M., Raper, S. C. B., and Wigley, T. M. L.: Emulating coupled atmosphere-ocean and carbon cycle models with a simpler model, MAGICC6 – Part 1: Model description and calibration, Atmos. Chem. Phys., 11, 1417–1456, <ext-link xlink:href="https://doi.org/10.5194/acp-11-1417-2011" ext-link-type="DOI">10.5194/acp-11-1417-2011</ext-link>, 2011.</mixed-citation></ref>
      <ref id="bib1.bibx27"><label>Meinshausen et al.(2017)</label><mixed-citation>Meinshausen, M., Vogel, E., Nauels, A., Lorbacher, K., Meinshausen, N., Etheridge, D. M., Fraser, P. J., Montzka, S. A., Rayner, P. J., Trudinger, C. M., Krummel, P. B., Beyerle, U., Canadell, J. G., Daniel, J. S., Enting, I. G., Law, R. M., Lunder, C. R., O'Doherty, S., Prinn, R. G., Reimann, S., Rubino, M., Velders, G. J. M., Vollmer, M. K., Wang, R. H. J., and Weiss, R.: Historical greenhouse gas concentrations for climate modelling (CMIP6), Geosci. Model Dev., 10, 2057–2116, <ext-link xlink:href="https://doi.org/10.5194/gmd-10-2057-2017" ext-link-type="DOI">10.5194/gmd-10-2057-2017</ext-link>, 2017.</mixed-citation></ref>
      <ref id="bib1.bibx28"><label>Meinshausen et al.(2020)</label><mixed-citation>Meinshausen, M., Nicholls, Z. R. J., Lewis, J., Gidden, M. J., Vogel, E., Freund, M., Beyerle, U., Gessner, C., Nauels, A., Bauer, N., Canadell, J. G., Daniel, J. S., John, A., Krummel, P. B., Luderer, G., Meinshausen, N., Montzka, S. A., Rayner, P. J., Reimann, S., Smith, S. J., van den Berg, M., Velders, G. J. M., Vollmer, M. K., and Wang, R. H. J.: The shared socio-economic pathway (SSP) greenhouse gas concentrations and their extensions to 2500, Geosci. Model Dev., 13, 3571–3605, <ext-link xlink:href="https://doi.org/10.5194/gmd-13-3571-2020" ext-link-type="DOI">10.5194/gmd-13-3571-2020</ext-link>, 2020.</mixed-citation></ref>
      <ref id="bib1.bibx29"><label>Moreno-Chamarro et al.(2020)</label><mixed-citation>Moreno-Chamarro, E., Marshall, J., and Delworth, T. L.: Linking ITCZ migrations to the AMOC and North Atlantic/Pacific SST decadal variability, J. Climate, 33, 893–905, <ext-link xlink:href="https://doi.org/10.1175/JCLI-D-19-0258.1" ext-link-type="DOI">10.1175/JCLI-D-19-0258.1</ext-link>, 2020.</mixed-citation></ref>
      <ref id="bib1.bibx30"><label>Murphy et al.(2014)</label><mixed-citation>Murphy, J. M., Booth, B. B. B., Boulton, C. A., Clark, R. T., Harris, G. R., Lowe, J. A., and Sexton, D. M. H.: Transient climate changes in a perturbed parameter ensemble of emissions-driven earth system model simulations, Clim. Dynam., 43, 2855–2885, <ext-link xlink:href="https://doi.org/10.1007/s00382-014-2097-5" ext-link-type="DOI">10.1007/s00382-014-2097-5</ext-link>, 2014.</mixed-citation></ref>
      <ref id="bib1.bibx31"><label>Nauels et al.(2025)</label><mixed-citation>Nauels, A., Nicholls, Z., Möller, T., Hermans, T. H. J., Mengel, M., Kloenne, U., Smith, C., Slangen, A. B. A., and Palmer, M. D.: Multi-century global and regional sea-level rise commitments from cumulative greenhouse gas emissions in the coming decades, Nat. Clim. Change, <ext-link xlink:href="https://doi.org/10.1038/s41558-025-02452-5" ext-link-type="DOI">10.1038/s41558-025-02452-5</ext-link>, 2025.</mixed-citation></ref>
      <ref id="bib1.bibx32"><label>O'Neill et al.(2016)</label><mixed-citation>O'Neill, B. C., Tebaldi, C., van Vuuren, D. P., Eyring, V., Friedlingstein, P., Hurtt, G., Knutti, R., Kriegler, E., Lamarque, J.-F., Lowe, J., Meehl, G. A., Moss, R., Riahi, K., and Sanderson, B. M.: The Scenario Model Intercomparison Project (ScenarioMIP) for CMIP6, Geosci. Model Dev., 9, 3461–3482, <ext-link xlink:href="https://doi.org/10.5194/gmd-9-3461-2016" ext-link-type="DOI">10.5194/gmd-9-3461-2016</ext-link>, 2016.</mixed-citation></ref>
      <ref id="bib1.bibx33"><label>Oschlies et al.(2018)</label><mixed-citation>Oschlies, A., Brandt, P., Stramma, L., and Schmidtko, S.: Drivers and mechanisms of ocean deoxygenation, Nat. Geosci., 11, 467–473, <ext-link xlink:href="https://doi.org/10.1038/s41561-018-0152-2" ext-link-type="DOI">10.1038/s41561-018-0152-2</ext-link>, 2018.</mixed-citation></ref>
      <ref id="bib1.bibx34"><label>Pfleiderer et al.(2024)</label><mixed-citation>Pfleiderer, P., Schleussner, C.-F., and Sillmann, J.: Limited reversal of regional climate signals in overshoot scenarios, Environmental Research: Climate, 3, 015005, <ext-link xlink:href="https://doi.org/10.1088/2752-5295/ad1c45" ext-link-type="DOI">10.1088/2752-5295/ad1c45</ext-link>, 2024.</mixed-citation></ref>
      <ref id="bib1.bibx35"><label>Rahmstorf(1995)</label><mixed-citation>Rahmstorf, S.: Bifurcations of the Atlantic thermohaline circulation in response to changes in the hydrological cycle, Nature, 378, 145–149, <ext-link xlink:href="https://doi.org/10.1038/378145a0" ext-link-type="DOI">10.1038/378145a0</ext-link>, 1995.</mixed-citation></ref>
      <ref id="bib1.bibx36"><label>Riahi et al.(2022)</label><mixed-citation>Riahi, K., Schaeffer, R., Arango, J., Calvin, K., Guivarch, C., Hasegawa, T., Jiang, K., Kriegler, E., Matthews, R., Peters, G. P., Rao, A., Robertson, S., Sebbit, A. M., Steinberger, J., Tavoni, M., and Van Vuuren, D. P.: Mitigation pathways compatible with long-term goals., in: IPCC, 2022: Climate Change 2022: Mitigation of Climate Change. Contribution of Working Group III to the Sixth Assessment Report of the Intergovernmental Panel on Climate Change, edited by: Shukla, P. R., Skea, J., Slade, R., Khourdajie, A. A., van Diemen, R., McCollum, D., Pathak, M., Some, S., Vyas, P., Fradera, R., Belkacemi, M., Hasija, A., Lisboa, G., Luz, S., and Malley, J., Cambridge University Press, Cambridge, UK and New York, NY, USA, <ext-link xlink:href="https://doi.org/10.1017/9781009157926.005" ext-link-type="DOI">10.1017/9781009157926.005</ext-link>, 2022.</mixed-citation></ref>
      <ref id="bib1.bibx37"><label>Rogelj et al.(2018)</label><mixed-citation>Rogelj, J., Popp, A., Calvin, K. V., Luderer, G., Emmerling, J., Gernaat, D., Fujimori, S., Strefler, J., Hasegawa, T., Marangoni, G., Krey, V., Kriegler, E., Riahi, K., van Vuuren, D. P., Doelman, J., Drouet, L., Edmonds, J., Fricko, O., Harmsen, M., Havlík, P., Humpenöder, F., Stehfest, E., and Tavoni, M.: Scenarios towards limiting global mean temperature increase below 1.5 <inline-formula><mml:math id="M109" 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>, Nat. Clim. Change, 8, 325–332, <ext-link xlink:href="https://doi.org/10.1038/s41558-018-0091-3" ext-link-type="DOI">10.1038/s41558-018-0091-3</ext-link>, 2018.</mixed-citation></ref>
      <ref id="bib1.bibx38"><label>Roldán-Gómez et al.(2025a)</label><mixed-citation>Roldán-Gómez, P. J., De Luca, P., Bernardello, R., and Donat, M. G.: Regional irreversibility of mean and extreme surface air temperature and precipitation in CMIP6 overshoot scenarios associated with interhemispheric temperature asymmetries, Earth Syst. Dynam., 16, 1–27, <ext-link xlink:href="https://doi.org/10.5194/esd-16-1-2025" ext-link-type="DOI">10.5194/esd-16-1-2025</ext-link>, 2025a.</mixed-citation></ref>
      <ref id="bib1.bibx39"><label>Roldán-Gómez et al.(2025b)</label><mixed-citation>Roldán-Gómez, P. J., Ortega, P., and Donat, M. G.: Contribution of meridional overturning circulation and sea ice changes to large-scale temperature asymmetries in CMIP6 overshoot scenarios, Ocean Sci., 21, 2283–2303, <ext-link xlink:href="https://doi.org/10.5194/os-21-2283-2025" ext-link-type="DOI">10.5194/os-21-2283-2025</ext-link>, 2025b.</mixed-citation></ref>
      <ref id="bib1.bibx40"><label>Rosenzweig et al.(2017)</label><mixed-citation>Rosenzweig, C., Arnell, N. W., Ebi, K. L., Lotze-Campen, H., Raes, F., Rapley, C., Smith, M. S., Cramer, W., Frieler, K., Reyer, C. P. O., Schewe, J., Van Vuuren, D., and Warszawski, L.: Assessing inter-sectoral climate change risks: the role of ISIMIP, Environ. Res. Lett., 12, 010301, <ext-link xlink:href="https://doi.org/10.1088/1748-9326/12/1/010301" ext-link-type="DOI">10.1088/1748-9326/12/1/010301</ext-link>, 2017.</mixed-citation></ref>
      <ref id="bib1.bibx41"><label>Sanderson et al.(2024)</label><mixed-citation>Sanderson, B. M., Booth, B. B. B., Dunne, J., Eyring, V., Fisher, R. A., Friedlingstein, P., Gidden, M. J., Hajima, T., Jones, C. D., Jones, C. G., King, A., Koven, C. D., Lawrence, D. M., Lowe, J., Mengis, N., Peters, G. P., Rogelj, J., Smith, C., Snyder, A. C., Simpson, I. R., Swann, A. L. S., Tebaldi, C., Ilyina, T., Schleussner, C.-F., Séférian, R., Samset, B. H., van Vuuren, D., and Zaehle, S.: The need for carbon-emissions-driven climate projections in CMIP7, Geosci. Model Dev., 17, 8141–8172, <ext-link xlink:href="https://doi.org/10.5194/gmd-17-8141-2024" ext-link-type="DOI">10.5194/gmd-17-8141-2024</ext-link>, 2024.</mixed-citation></ref>
      <ref id="bib1.bibx42"><label>Sarofim et al.(2024)</label><mixed-citation>Sarofim, M. C., Smith, C. J., Malek, P., McDuffie, E. E., Hartin, C. A., Lay, C. R., and McGrath, S.: High radiative forcing climate scenario relevance analyzed with a ten-million-member ensemble, Nat. Commun., 15, 8185, <ext-link xlink:href="https://doi.org/10.1038/s41467-024-52437-9" ext-link-type="DOI">10.1038/s41467-024-52437-9</ext-link>, 2024.</mixed-citation></ref>
      <ref id="bib1.bibx43"><label>Schleussner et al.(2024)</label><mixed-citation>Schleussner, C.-F., Ganti, G., Lejeune, Q., Zhu, B., Pfleiderer, P., Prütz, R., Ciais, P., Frölicher, T. L., Fuss, S., Gasser, T., Gidden, M. J., Kropf, C. M., Lacroix, F., Lamboll, R., Martyr, R., Maussion, F., McCaughey, J. W., Meinshausen, M., Mengel, M., Nicholls, Z., Quilcaille, Y., Sanderson, B., Seneviratne, S. I., Sillmann, J., Smith, C. J., Steinert, N. J., Theokritoff, E., Warren, R., Price, J., and Rogelj, J.: Overconfidence in climate overshoot, Nature, 634, 366–373, <ext-link xlink:href="https://doi.org/10.1038/s41586-024-08020-9" ext-link-type="DOI">10.1038/s41586-024-08020-9</ext-link>, 2024.</mixed-citation></ref>
      <ref id="bib1.bibx44"><label>Schoenberg et al.(2025)</label><mixed-citation>Schoenberg, W., Blanz, B., Rajah, J. K., Callegari, B., Wells, C., Breier, J., Grimeland, M. B., Lindqvist, A. N., Ramme, L., Smith, C., Li, C., Mashhadi, S., Muralidhar, A., and Mauritzen, C.: An overview of FRIDA v2.1: a feedback-based, fully coupled, global integrated assessment model of climate and humans, Geosci. Model Dev., 18, 8047–8069, <ext-link xlink:href="https://doi.org/10.5194/gmd-18-8047-2025" ext-link-type="DOI">10.5194/gmd-18-8047-2025</ext-link>, 2025.</mixed-citation></ref>
      <ref id="bib1.bibx45"><label>Schwinger et al.(2022a)</label><mixed-citation>Schwinger, J., Asaadi, A., Goris, N., and Lee, H.: Possibility for strong northern hemisphere high-latitude cooling under negative emissions, Nat. Commun., 13, 1095, <ext-link xlink:href="https://doi.org/10.1038/s41467-022-28573-5" ext-link-type="DOI">10.1038/s41467-022-28573-5</ext-link>, 2022a.</mixed-citation></ref>
      <ref id="bib1.bibx46"><label>Schwinger et al.(2022b)</label><mixed-citation>Schwinger, J., Asaadi, A., Steinert, N. J., and Lee, H.: Emit now, mitigate later? Earth system reversibility under overshoots of different magnitudes and durations, Earth Syst. Dynam., 13, 1641–1665, <ext-link xlink:href="https://doi.org/10.5194/esd-13-1641-2022" ext-link-type="DOI">10.5194/esd-13-1641-2022</ext-link>, 2022b.</mixed-citation></ref>
      <ref id="bib1.bibx47"><label>Seland et al.(2020)</label><mixed-citation>Seland, Ø., Bentsen, M., Olivié, D., Toniazzo, T., Gjermundsen, A., Graff, L. S., Debernard, J. B., Gupta, A. K., He, Y.-C., Kirkevåg, A., Schwinger, J., Tjiputra, J., Aas, K. S., Bethke, I., Fan, Y., Griesfeller, J., Grini, A., Guo, C., Ilicak, M., Karset, I. H. H., Landgren, O., Liakka, J., Moseid, K. O., Nummelin, A., Spensberger, C., Tang, H., Zhang, Z., Heinze, C., Iversen, T., and Schulz, M.: Overview of the Norwegian Earth System Model (NorESM2) and key climate response of CMIP6 DECK, historical, and scenario simulations, Geosci. Model Dev., 13, 6165–6200, <ext-link xlink:href="https://doi.org/10.5194/gmd-13-6165-2020" ext-link-type="DOI">10.5194/gmd-13-6165-2020</ext-link>, 2020.</mixed-citation></ref>
      <ref id="bib1.bibx48"><label>Sigmond et al.(2020)</label><mixed-citation>Sigmond, M., Fyfe, J. C., Saenko, O. A., and Swart, N. C.: Ongoing AMOC and related sea-level and temperature changes after achieving the Paris targets, Nat. Clim. Change, 10, 672–677, <ext-link xlink:href="https://doi.org/10.1038/s41558-020-0786-0" ext-link-type="DOI">10.1038/s41558-020-0786-0</ext-link>, 2020.</mixed-citation></ref>
      <ref id="bib1.bibx49"><label>Smith et al.(2021)</label><mixed-citation>Smith, C., Nicholls, Z. R. J., Armour, K., Collins, W., Forster, P., Meinshausen, M., Palmer, M. D., and Watanabe, M.: The Earth's energy budget, climate feedbacks, and climate sensitivity supplementary material, in: Climate Change 2021: The Physical Science Basis. Contribution of Working Group I to the Sixth Assessment Report of the Intergovernmental Panel on Climate Change, edited by: Masson-Delmotte, V., Zhai, P., Pirani, A., Connors, S. L., Péan, C., Berger, S., Caud, N., Chen, Y., Goldfarb, L., Gomis, M. I., Huang, M., Leitzell, K., Lonnoy, E., Matthews, J. B. R., Maycock, T. K., Waterfield, T., Yelekçi, O., Yu, R., and Zhou, B., Sect. 7.SM, Cambridge University Press, Cambridge, UK and New York, NY, USA, <uri>https://www.ipcc.ch/report/ar6/wg1/downloads/report/IPCC_AR6_WGI_Chapter07_SM.pdf</uri> (last access: 22 June 2026), 1–35, 2021.</mixed-citation></ref>
      <ref id="bib1.bibx50"><label>Solomon et al.(2009)</label><mixed-citation>Solomon, S., Plattner, G.-K., Knutti, R., and Friedlingstein, P.: Irreversible climate change due to carbon dioxide emissions, P. Natl. Acad. Sci. USA, 106, 1704–1709, <ext-link xlink:href="https://doi.org/10.1073/pnas.0812721106" ext-link-type="DOI">10.1073/pnas.0812721106</ext-link>, 2009.</mixed-citation></ref>
      <ref id="bib1.bibx51"><label>Steinert et al.(2025)</label><mixed-citation>Steinert, N. J., Schwinger, J., Chadwick, R., Kug, J., and Lee, H.: Irreversible land water availability changes from a potential ITCZ shift during temperature overshoot, Earths Future, 13, e2024EF005787, <ext-link xlink:href="https://doi.org/10.1029/2024EF005787" ext-link-type="DOI">10.1029/2024EF005787</ext-link>, 2025.</mixed-citation></ref>
      <ref id="bib1.bibx52"><label>Stevens et al.(2017)</label><mixed-citation>Stevens, B., Fiedler, S., Kinne, S., Peters, K., Rast, S., Müsse, J., Smith, S. J., and Mauritsen, T.: MACv2-SP: a parameterization of anthropogenic aerosol optical properties and an associated Twomey effect for use in CMIP6, Geosci. Model Dev., 10, 433–452, <ext-link xlink:href="https://doi.org/10.5194/gmd-10-433-2017" ext-link-type="DOI">10.5194/gmd-10-433-2017</ext-link>, 2017.</mixed-citation></ref>
      <ref id="bib1.bibx53"><label>Tang et al.(2025)</label><mixed-citation>Tang, G., Nicholls, Z., Jones, C., Gasser, T., Norton, A., Ziehn, T., Romero-Prieto, A., and Meinshausen, M.: Investigating carbon and nitrogen conservation in reported CMIP6 Earth system model data, Geosci. Model Dev., 18, 2111–2136, <ext-link xlink:href="https://doi.org/10.5194/gmd-18-2111-2025" ext-link-type="DOI">10.5194/gmd-18-2111-2025</ext-link>, 2025.</mixed-citation></ref>
      <ref id="bib1.bibx54"><label>Taylor et al.(2012)</label><mixed-citation>Taylor, K. E., Stouffer, R. J., and Meehl, G. A.: An Overview of CMIP5 and the experiment design, B. Am. Meteorol. Soc., 93, 485–498, <ext-link xlink:href="https://doi.org/10.1175/BAMS-D-11-00094.1" ext-link-type="DOI">10.1175/BAMS-D-11-00094.1</ext-link>, 2012.</mixed-citation></ref>
      <ref id="bib1.bibx55"><label>Tebaldi et al.(2021)</label><mixed-citation>Tebaldi, C., Debeire, K., Eyring, V., Fischer, E., Fyfe, J., Friedlingstein, P., Knutti, R., Lowe, J., O'Neill, B., Sanderson, B., van Vuuren, D., Riahi, K., Meinshausen, M., Nicholls, Z., Tokarska, K. B., Hurtt, G., Kriegler, E., Lamarque, J.-F., Meehl, G., Moss, R., Bauer, S. E., Boucher, O., Brovkin, V., Byun, Y.-H., Dix, M., Gualdi, S., Guo, H., John, J. G., Kharin, S., Kim, Y., Koshiro, T., Ma, L., Olivié, D., Panickal, S., Qiao, F., Rong, X., Rosenbloom, N., Schupfner, M., Séférian, R., Sellar, A., Semmler, T., Shi, X., Song, Z., Steger, C., Stouffer, R., Swart, N., Tachiiri, K., Tang, Q., Tatebe, H., Voldoire, A., Volodin, E., Wyser, K., Xin, X., Yang, S., Yu, Y., and Ziehn, T.: Climate model projections from the Scenario Model Intercomparison Project (ScenarioMIP) of CMIP6, Earth Syst. Dynam., 12, 253–293, <ext-link xlink:href="https://doi.org/10.5194/esd-12-253-2021" ext-link-type="DOI">10.5194/esd-12-253-2021</ext-link>, 2021.</mixed-citation></ref>
      <ref id="bib1.bibx56"><label>Tjiputra et al.(2020)</label><mixed-citation>Tjiputra, J. F., Schwinger, J., Bentsen, M., Morée, A. L., Gao, S., Bethke, I., Heinze, C., Goris, N., Gupta, A., He, Y.-C., Olivié, D., Seland, Ø., and Schulz, M.: Ocean biogeochemistry in the Norwegian Earth System Model version 2 (NorESM2), Geosci. Model Dev., 13, 2393–2431, <ext-link xlink:href="https://doi.org/10.5194/gmd-13-2393-2020" ext-link-type="DOI">10.5194/gmd-13-2393-2020</ext-link>, 2020.</mixed-citation></ref>
      <ref id="bib1.bibx57"><label>Tokarska and Zickfeld(2015)</label><mixed-citation>Tokarska, K. B. and Zickfeld, K.: The effectiveness of net negative carbon dioxide emissions in reversing anthropogenic climate change, Environ. Res. Lett., 10, 094013, <ext-link xlink:href="https://doi.org/10.1088/1748-9326/10/9/094013" ext-link-type="DOI">10.1088/1748-9326/10/9/094013</ext-link>, 2015.</mixed-citation></ref>
      <ref id="bib1.bibx58"><label>Van Vuuren et al.(2026)</label><mixed-citation>Van Vuuren, D. P., O'Neill, B. C., Tebaldi, C., Sanderson, B. M., Chini, L. P., Friedlingstein, P., Hasegawa, T., Riahi, K., Govindasamy, B., Bauer, N., Eyring, V., Fall, C. M. N., Frieler, K., Gidden, M. J., Gohar, L. K., Högner, A., Jones, A. D., Kikstra, J., King, A., Knutti, R., Kriegler, E., Lawrence, P., Lennard, C., Lowe, J., Mathison, C., Mehmood, S., Nicholls, Z., Prado, L. F., Zhang, Q., Rose, S. K., Ruane, A. C., Sandstad, M., Schleussner, C.-F., Seferian, R., Sillmann, J., Smith, C., Sörensson, A. A., Panickal, S., Tachiiri, K., Vaughan, N., Vishwanathan, S. S., Yokohata, T., Zecchetto, M., and Ziehn, T.: The Scenario Model Intercomparison Project for CMIP7 (ScenarioMIP-CMIP7), Geosci. Model Dev., 19, 2627–2656, <ext-link xlink:href="https://doi.org/10.5194/gmd-19-2627-2026" ext-link-type="DOI">10.5194/gmd-19-2627-2026</ext-link>, 2026.</mixed-citation></ref>
      <ref id="bib1.bibx59"><label>Wells et al.(2026a)</label><mixed-citation>Wells, C. D., Blanz, B., Ramme, L., Breier, J., Callegari, B., Muralidhar, A., Rajah, J. K., Lindqvist, A. N., Eriksson, A. E., Schoenberg, W. A., Köberle, A. C., Wang-Erlandsson, L., Mauritzen, C., Grimeland, M. B., and Smith, C.: The representation of climate impacts in the FRIDAv2.1 Integrated Assessment Model, Geosci. Model Dev., 19, 1229–1260, <ext-link xlink:href="https://doi.org/10.5194/gmd-19-1229-2026" ext-link-type="DOI">10.5194/gmd-19-1229-2026</ext-link>, 2026a.</mixed-citation></ref>
      <ref id="bib1.bibx60"><label>Wells et al.(2026b)</label><mixed-citation>Wells, C. D., Cummins, D. P., He, H., and Smith, C.: Long run emulator calibration increases warming and sea-level rise projections, Environ. Res. Lett., 21, 034008, <ext-link xlink:href="https://doi.org/10.1088/1748-9326/ae3847" ext-link-type="DOI">10.1088/1748-9326/ae3847</ext-link>, 2026b. </mixed-citation></ref>
      <ref id="bib1.bibx61"><label>Wigley and Raper(1987)</label><mixed-citation>Wigley, T. M. L. and Raper, S. C. B.: Thermal expansion of sea water associated with global warming, Nature, 330, 127–131, <ext-link xlink:href="https://doi.org/10.1038/330127a0" ext-link-type="DOI">10.1038/330127a0</ext-link>, 1987.</mixed-citation></ref>
      <ref id="bib1.bibx62"><label>Woodard et al.(2019)</label><mixed-citation>Woodard, D. L., Davis, S. J., and Randerson, J. T.: Economic carbon cycle feedbacks may offset additional warming from natural feedbacks, P. Natl. Acad. Sci. USA, 116, 759–764, <ext-link xlink:href="https://doi.org/10.1073/pnas.1805187115" ext-link-type="DOI">10.1073/pnas.1805187115</ext-link>, 2019.</mixed-citation></ref>
      <ref id="bib1.bibx63"><label>Wunderling et al.(2024)</label><mixed-citation>Wunderling, N., von der Heydt, A. S., Aksenov, Y., Barker, S., Bastiaansen, R., Brovkin, V., Brunetti, M., Couplet, V., Kleinen, T., Lear, C. H., Lohmann, J., Roman-Cuesta, R. M., Sinet, S., Swingedouw, D., Winkelmann, R., Anand, P., Barichivich, J., Bathiany, S., Baudena, M., Bruun, J. T., Chiessi, C. M., Coxall, H. K., Docquier, D., Donges, J. F., Falkena, S. K. J., Klose, A. K., Obura, D., Rocha, J., Rynders, S., Steinert, N. J., and Willeit, M.: Climate tipping point interactions and cascades: a review, Earth Syst. Dynam., 15, 41–74, <ext-link xlink:href="https://doi.org/10.5194/esd-15-41-2024" ext-link-type="DOI">10.5194/esd-15-41-2024</ext-link>, 2024.</mixed-citation></ref>

  </ref-list></back>
    <!--<article-title-html>Overshoot and (ir)reversibility to 2300 in two CO<sub>2</sub>-emissions driven Earth System models</article-title-html>
<abstract-html/>
<ref-html id="bib1.bib1"><label>Allen et al.(2009)</label><mixed-citation>
       Allen, M. R., Frame, D. J., Huntingford, C., Jones, C. D., Lowe, J. A., Meinshausen, M., and Meinshausen, N.: Warming caused by cumulative carbon emissions towards the trillionth tonne, Nature, 458, 1163, 2009.

    </mixed-citation></ref-html>
<ref-html id="bib1.bib2"><label>Andrews et al.(2010)</label><mixed-citation>
       Andrews, T., Forster, P. M., Boucher, O., Bellouin, N., and Jones, A.: Precipitation, radiative forcing and global temperature change, Geophys. Res. Lett., 37, 2010GL043991, <a href="https://doi.org/10.1029/2010GL043991" target="_blank">https://doi.org/10.1029/2010GL043991</a>, 2010.

    </mixed-citation></ref-html>
<ref-html id="bib1.bib3"><label>Cassidy et al.(2024)</label><mixed-citation>
       Cassidy, L. J., King, A. D., Brown, J. R., MacDougall, A. H., Ziehn, T., Min, S.-K., and Jones, C. D.: Regional temperature extremes and vulnerability under net zero CO<sub>2</sub> emissions, Environ. Res. Lett., 19, 014051, <a href="https://doi.org/10.1088/1748-9326/ad114a" target="_blank">https://doi.org/10.1088/1748-9326/ad114a</a>, 2024.

    </mixed-citation></ref-html>
<ref-html id="bib1.bib4"><label>Douglas et al.(2025)</label><mixed-citation>
       Douglas, H. C., Revell, L. E., King, A., Harrington, L. J., and Frame, D. J.: Effects of temperature overshoot amplitude on regional climate, Environ. Res. Lett., 20, 114043, <a href="https://doi.org/10.1088/1748-9326/ae114f" target="_blank">https://doi.org/10.1088/1748-9326/ae114f</a>, 2025.

    </mixed-citation></ref-html>
<ref-html id="bib1.bib5"><label>Eyring et al.(2016)</label><mixed-citation>
       Eyring, V., Bony, S., Meehl, G. A., Senior, C. A., Stevens, B., Stouffer, R. J., and Taylor, K. E.: Overview of the Coupled Model Intercomparison Project Phase 6 (CMIP6) experimental design and organization, Geosci. Model Dev., 9, 1937–1958, <a href="https://doi.org/10.5194/gmd-9-1937-2016" target="_blank">https://doi.org/10.5194/gmd-9-1937-2016</a>, 2016.

    </mixed-citation></ref-html>
<ref-html id="bib1.bib6"><label>Forster et al.(2025)</label><mixed-citation>
       Forster, P. M., Smith, C., Walsh, T., Lamb, W. F., Lamboll, R., Cassou, C., Hauser, M., Hausfather, Z., Lee, J.-Y., Palmer, M. D., von Schuckmann, K., Slangen, A. B. A., Szopa, S., Trewin, B., Yun, J., Gillett, N. P., Jenkins, S., Matthews, H. D., Raghavan, K., Ribes, A., Rogelj, J., Rosen, D., Zhang, X., Allen, M., Aleluia Reis, L., Andrew, R. M., Betts, R. A., Borger, A., Broersma, J. A., Burgess, S. N., Cheng, L., Friedlingstein, P., Domingues, C. M., Gambarini, M., Gasser, T., Gütschow, J., Ishii, M., Kadow, C., Kennedy, J., Killick, R. E., Krummel, P. B., Liné, A., Monselesan, D. P., Morice, C., Mühle, J., Naik, V., Peters, G. P., Pirani, A., Pongratz, J., Minx, J. C., Rigby, M., Rohde, R., Savita, A., Seneviratne, S. I., Thorne, P., Wells, C., Western, L. M., van der Werf, G. R., Wijffels, S. E., Masson-Delmotte, V., and Zhai, P.: Indicators of Global Climate Change 2024: annual update of key indicators of the state of the climate system and human influence, Earth Syst. Sci. Data, 17, 2641–2680, <a href="https://doi.org/10.5194/essd-17-2641-2025" target="_blank">https://doi.org/10.5194/essd-17-2641-2025</a>, 2025.

    </mixed-citation></ref-html>
<ref-html id="bib1.bib7"><label>Frenger et al.(2025)</label><mixed-citation>
       Frenger, I., Frey, S., Oschlies, A., Getzlaff, J., Martin, T., and Koeve, W.: Southern Ocean heat burp in a cooling world, AGU Advances, 6, e2025AV001700, <a href="https://doi.org/10.1029/2025AV001700" target="_blank">https://doi.org/10.1029/2025AV001700</a>, 2025.

    </mixed-citation></ref-html>
<ref-html id="bib1.bib8"><label>Friedlingstein et al.(2006)</label><mixed-citation>
       Friedlingstein, P., Cox, P., Betts, R., Bopp, L., Von Bloh, W., Brovkin, V., Cadule, P., Doney, S., Eby, M., Fung, I., Bala, G., John, J., Jones, C., Joos, F., Kato, T., Kawamiya, M., Knorr, W., Lindsay, K., Matthews, H. D., Raddatz, T., Rayner, P., Reick, C., Roeckner, E., Schnitzler, K.-G., Schnur, R., Strassmann, K., Weaver, A. J., Yoshikawa, C., and Zeng, N.: Climate–carbon cycle feedback analysis: results from the C4MIP model intercomparison, J. Climate, 19, 3337–3353, <a href="https://doi.org/10.1175/JCLI3800.1" target="_blank">https://doi.org/10.1175/JCLI3800.1</a>, 2006.

    </mixed-citation></ref-html>
<ref-html id="bib1.bib9"><label>Fyfe et al.(2021)</label><mixed-citation>
       Fyfe, J. C., Kharin, V. V., Swart, N., Flato, G. M., Sigmond, M., and Gillett, N. P.: Quantifying the influence of short-term emission reductions on climate, Science Advances, 7, eabf7133, <a href="https://doi.org/10.1126/sciadv.abf7133" target="_blank">https://doi.org/10.1126/sciadv.abf7133</a>, 2021.

    </mixed-citation></ref-html>
<ref-html id="bib1.bib10"><label>Gjermundsen et al.(2021)</label><mixed-citation>
       Gjermundsen, A., Nummelin, A., Olivié, D., Bentsen, M., Seland, Ø., and Schulz, M.: Shutdown of Southern Ocean convection controls long-term greenhouse gas-induced warming, Nat. Geosci., 14, 724–731, <a href="https://doi.org/10.1038/s41561-021-00825-x" target="_blank">https://doi.org/10.1038/s41561-021-00825-x</a>, 2021.

    </mixed-citation></ref-html>
<ref-html id="bib1.bib11"><label>Hausfather(2025)</label><mixed-citation>
       Hausfather, Z.: An assessment of current policy scenarios over the 21st century and the reduced plausibility of high-emissions pathways, Dialogues on Climate Change, 29768659241304854, <a href="https://doi.org/10.1177/29768659241304854" target="_blank">https://doi.org/10.1177/29768659241304854</a>, 2025.

    </mixed-citation></ref-html>
<ref-html id="bib1.bib12"><label>Hausfather and Peters(2020)</label><mixed-citation>
       Hausfather, Z. and Peters, G. P.: Emissions – the `business as usual' story is misleading, Nature, 577, 618–620, <a href="https://doi.org/10.1038/d41586-020-00177-3" target="_blank">https://doi.org/10.1038/d41586-020-00177-3</a>, 2020.

    </mixed-citation></ref-html>
<ref-html id="bib1.bib13"><label>Jones et al.(2016)</label><mixed-citation>
       Jones, C. D., Arora, V., Friedlingstein, P., Bopp, L., Brovkin, V., Dunne, J., Graven, H., Hoffman, F., Ilyina, T., John, J. G., Jung, M., Kawamiya, M., Koven, C., Pongratz, J., Raddatz, T., Randerson, J. T., and Zaehle, S.: C4MIP – The Coupled Climate–Carbon Cycle Model Intercomparison Project: experimental protocol for CMIP6, Geosci. Model Dev., 9, 2853–2880, <a href="https://doi.org/10.5194/gmd-9-2853-2016" target="_blank">https://doi.org/10.5194/gmd-9-2853-2016</a>, 2016.

    </mixed-citation></ref-html>
<ref-html id="bib1.bib14"><label>Keller et al.(2018)</label><mixed-citation>
       Keller, D. P., Lenton, A., Scott, V., Vaughan, N. E., Bauer, N., Ji, D., Jones, C. D., Kravitz, B., Muri, H., and Zickfeld, K.: The Carbon Dioxide Removal Model Intercomparison Project (CDRMIP): rationale and experimental protocol for CMIP6, Geosci. Model Dev., 11, 1133–1160, <a href="https://doi.org/10.5194/gmd-11-1133-2018" target="_blank">https://doi.org/10.5194/gmd-11-1133-2018</a>, 2018.

    </mixed-citation></ref-html>
<ref-html id="bib1.bib15"><label>King et al.(2024)</label><mixed-citation>
       King, A. D., Ziehn, T., Chamberlain, M., Borowiak, A. R., Brown, J. R., Cassidy, L., Dittus, A. J., Grose, M., Maher, N., Paik, S., Perkins-Kirkpatrick, S. E., and Sengupta, A.: Exploring climate stabilisation at different global warming levels in ACCESS-ESM-1.5, Earth Syst. Dynam., 15, 1353–1383, <a href="https://doi.org/10.5194/esd-15-1353-2024" target="_blank">https://doi.org/10.5194/esd-15-1353-2024</a>, 2024.

    </mixed-citation></ref-html>
<ref-html id="bib1.bib16"><label>Koven et al.(2022)</label><mixed-citation>
       Koven, C. D., Arora, V. K., Cadule, P., Fisher, R. A., Jones, C. D., Lawrence, D. M., Lewis, J., Lindsay, K., Mathesius, S., Meinshausen, M., Mills, M., Nicholls, Z., Sanderson, B. M., Séférian, R., Swart, N. C., Wieder, W. R., and Zickfeld, K.: Multi-century dynamics of the climate and carbon cycle under both high and net negative emissions scenarios, Earth Syst. Dynam., 13, 885–909, <a href="https://doi.org/10.5194/esd-13-885-2022" target="_blank">https://doi.org/10.5194/esd-13-885-2022</a>, 2022.

    </mixed-citation></ref-html>
<ref-html id="bib1.bib17"><label>Koven et al.(2023)</label><mixed-citation>
       Koven, C. D., Sanderson, B. M., and Swann, A. L. S.: Much of zero emissions commitment occurs before reaching net zero emissions, Environ. Res. Lett., 18, 014017, <a href="https://doi.org/10.1088/1748-9326/acab1a" target="_blank">https://doi.org/10.1088/1748-9326/acab1a</a>, 2023.

    </mixed-citation></ref-html>
<ref-html id="bib1.bib18"><label>Kug et al.(2022)</label><mixed-citation>
       Kug, J.-S., Oh, J.-H., An, S.-I., Yeh, S.-W., Min, S.-K., Son, S.-W., Kam, J., Ham, Y.-G., and Shin, J.: Hysteresis of the intertropical convergence zone to CO<sub>2</sub> forcing, Nat. Clim. Change, 12, 47–53, <a href="https://doi.org/10.1038/s41558-021-01211-6" target="_blank">https://doi.org/10.1038/s41558-021-01211-6</a>, 2022.

    </mixed-citation></ref-html>
<ref-html id="bib1.bib19"><label>Lacroix et al.(2024)</label><mixed-citation>
       Lacroix, F., Burger, F. A., Silvy, Y., Schleussner, C., and Frölicher, T. L.: Persistently elevated high latitude ocean temperatures and global sea level following temporary temperature overshoots, Earths Future, 12, e2024EF004862, <a href="https://doi.org/10.1029/2024EF004862" target="_blank">https://doi.org/10.1029/2024EF004862</a>, 2024.

    </mixed-citation></ref-html>
<ref-html id="bib1.bib20"><label>Lee et al.(2021)</label><mixed-citation>
       Lee, J.-Y., Marotzke, J., Bala, G., Cao, L., Corti, S., Dunne, J., Engelbrecht, F., Fischer, E., Fyfe, J., Jones, C., Maycock, A., Mutemi, J., Ndiaye, O., Panickal, S., and Zhou, T.: Future global climate: scenario-based projections and near-term information, in: Climate Change 2021: The Physical Science Basis. Contribution of Working Group I to the Sixth Assessment Report of the Intergovernmental Panel on Climate Change, edited by: Masson-Delmotte, V., Zhai, P., Pirani, A., Connors, S. L., Péan, C., Berger, S., Caud, N., Chen, Y., Goldfarb, L., Gomis, M. I., Huang, M., Leitzell, K., Lonnoy, E., Matthews, J. B. R., Maycock, T. K., Waterfield, T., Yelekçi, O., Yu, R., and Zhou, B., Sect. 4, Cambridge University Press, Cambridge, UK and New York, NY, USA, <a href="https://doi.org/10.1017/9781009157896.006" target="_blank">https://doi.org/10.1017/9781009157896.006</a>, 553–672, 2021.

    </mixed-citation></ref-html>
<ref-html id="bib1.bib21"><label>Lyon et al.(2022)</label><mixed-citation>
       Lyon, C., Saupe, E. E., Smith, C. J., Hill, D. J., Beckerman, A. P., Stringer, L. C., Marchant, R., McKay, J., Burke, A., O'Higgins, P., Dunhill, A. M., Allen, B. J., Riel Salvatore, J., and Aze, T.: Climate change research and action must look beyond 2100, Glob. Change Biol., 28, 349–361, <a href="https://doi.org/10.1111/gcb.15871" target="_blank">https://doi.org/10.1111/gcb.15871</a>, 2022.

    </mixed-citation></ref-html>
<ref-html id="bib1.bib22"><label>MacDougall et al.(2020)</label><mixed-citation>
       MacDougall, A. H., Frölicher, T. L., Jones, C. D., Rogelj, J., Matthews, H. D., Zickfeld, K., Arora, V. K., Barrett, N. J., Brovkin, V., Burger, F. A., Eby, M., Eliseev, A. V., Hajima, T., Holden, P. B., Jeltsch-Thömmes, A., Koven, C., Mengis, N., Menviel, L., Michou, M., Mokhov, I. I., Oka, A., Schwinger, J., Séférian, R., Shaffer, G., Sokolov, A., Tachiiri, K., Tjiputra , J., Wiltshire, A., and Ziehn, T.: Is there warming in the pipeline? A multi-model analysis of the Zero Emissions Commitment from CO<sub>2</sub>,  Biogeosciences, 17, 2987–3016, <a href="https://doi.org/10.5194/bg-17-2987-2020" target="_blank">https://doi.org/10.5194/bg-17-2987-2020</a>, 2020.

    </mixed-citation></ref-html>
<ref-html id="bib1.bib23"><label>MacDougall et al.(2022)</label><mixed-citation>
       MacDougall, A. H., Mallett, J., Hohn, D., and Mengis, N.: Substantial regional climate change expected following cessation of CO<sub>2</sub> emissions, Environ. Res. Lett., 17, 114046, <a href="https://doi.org/10.1088/1748-9326/ac9f59" target="_blank">https://doi.org/10.1088/1748-9326/ac9f59</a>, 2022.

    </mixed-citation></ref-html>
<ref-html id="bib1.bib24"><label>Matthews et al.(2009)</label><mixed-citation>
       Matthews, H. D., Gillett, N. P., Stott, P. A., and Zickfeld, K.: The proportionality of global warming to cumulative carbon emissions, Nature, 459, 829–832, <a href="https://doi.org/10.1038/nature08047" target="_blank">https://doi.org/10.1038/nature08047</a>, 2009.

    </mixed-citation></ref-html>
<ref-html id="bib1.bib25"><label>Mauritsen et al.(2019)</label><mixed-citation>
       Mauritsen, T., Bader, J., Becker, T., Behrens, J., Bittner, M., Brokopf, R., Brovkin, V., Claussen, M., Crueger, T., Esch, M., Fast, I., Fiedler, S., Fläschner, D., Gayler, V., Giorgetta, M., Goll, D. S., Haak, H., Hagemann, S., Hedemann, C., Hohenegger, C., Ilyina, T., Jahns, T., Jimenéz de la Cuesta, D., Jungclaus, J., Kleinen, T., Kloster, S., Kracher, D., Kinne, S., Kleberg, D., Lasslop, G., Kornblueh, L., Marotzke, J., Matei, D., Meraner, K., Mikolajewicz, U., Modali, K., Möbis, B., Müller, W. A., Nabel, J. E. M. S., Nam, C. C. W., Notz, D., Nyawira, S., Paulsen, H., Peters, K., Pincus, R., Pohlmann, H., Pongratz, J., Popp, M., Raddatz, T. J., Rast, S., Redler, R., Reick, C. H., Rohrschneider, T., Schemann, V., Schmidt, H., Schnur, R., Schulzweida, U., Six, K. D., Stein, L., Stemmler, I., Stevens, B., Von Storch, J., Tian, F., Voigt, A., Vrese, P., Wieners, K., Wilkenskjeld, S., Winkler, A., and Roeckner, E.: Developments in the MPI M Earth system model version 1.2 (MPI ESM1.2) and its response to increasing CO<sub>2</sub>, J. Adv. Model. Earth Sy., 11, 998–1038, <a href="https://doi.org/10.1029/2018MS001400" target="_blank">https://doi.org/10.1029/2018MS001400</a>, 2019.

    </mixed-citation></ref-html>
<ref-html id="bib1.bib26"><label>Meinshausen et al.(2011)</label><mixed-citation>
       Meinshausen, M., Raper, S. C. B., and Wigley, T. M. L.: Emulating coupled atmosphere-ocean and carbon cycle models with a simpler model, MAGICC6 – Part 1: Model description and calibration, Atmos. Chem. Phys., 11, 1417–1456, <a href="https://doi.org/10.5194/acp-11-1417-2011" target="_blank">https://doi.org/10.5194/acp-11-1417-2011</a>, 2011.

    </mixed-citation></ref-html>
<ref-html id="bib1.bib27"><label>Meinshausen et al.(2017)</label><mixed-citation>
       Meinshausen, M., Vogel, E., Nauels, A., Lorbacher, K., Meinshausen, N., Etheridge, D. M., Fraser, P. J., Montzka, S. A., Rayner, P. J., Trudinger, C. M., Krummel, P. B., Beyerle, U., Canadell, J. G., Daniel, J. S., Enting, I. G., Law, R. M., Lunder, C. R., O'Doherty, S., Prinn, R. G., Reimann, S., Rubino, M., Velders, G. J. M., Vollmer, M. K., Wang, R. H. J., and Weiss, R.: Historical greenhouse gas concentrations for climate modelling (CMIP6), Geosci. Model Dev., 10, 2057–2116, <a href="https://doi.org/10.5194/gmd-10-2057-2017" target="_blank">https://doi.org/10.5194/gmd-10-2057-2017</a>, 2017.

    </mixed-citation></ref-html>
<ref-html id="bib1.bib28"><label>Meinshausen et al.(2020)</label><mixed-citation>
       Meinshausen, M., Nicholls, Z. R. J., Lewis, J., Gidden, M. J., Vogel, E., Freund, M., Beyerle, U., Gessner, C., Nauels, A., Bauer, N., Canadell, J. G., Daniel, J. S., John, A., Krummel, P. B., Luderer, G., Meinshausen, N., Montzka, S. A., Rayner, P. J., Reimann, S., Smith, S. J., van den Berg, M., Velders, G. J. M., Vollmer, M. K., and Wang, R. H. J.: The shared socio-economic pathway (SSP) greenhouse gas concentrations and their extensions to 2500, Geosci. Model Dev., 13, 3571–3605, <a href="https://doi.org/10.5194/gmd-13-3571-2020" target="_blank">https://doi.org/10.5194/gmd-13-3571-2020</a>, 2020.

    </mixed-citation></ref-html>
<ref-html id="bib1.bib29"><label>Moreno-Chamarro et al.(2020)</label><mixed-citation>
       Moreno-Chamarro, E., Marshall, J., and Delworth, T. L.: Linking ITCZ migrations to the AMOC and North Atlantic/Pacific SST decadal variability, J. Climate, 33, 893–905, <a href="https://doi.org/10.1175/JCLI-D-19-0258.1" target="_blank">https://doi.org/10.1175/JCLI-D-19-0258.1</a>, 2020.

    </mixed-citation></ref-html>
<ref-html id="bib1.bib30"><label>Murphy et al.(2014)</label><mixed-citation>
       Murphy, J. M., Booth, B. B. B., Boulton, C. A., Clark, R. T., Harris, G. R., Lowe, J. A., and Sexton, D. M. H.: Transient climate changes in a perturbed parameter ensemble of emissions-driven earth system model simulations, Clim. Dynam., 43, 2855–2885, <a href="https://doi.org/10.1007/s00382-014-2097-5" target="_blank">https://doi.org/10.1007/s00382-014-2097-5</a>, 2014.

    </mixed-citation></ref-html>
<ref-html id="bib1.bib31"><label>Nauels et al.(2025)</label><mixed-citation>
       Nauels, A., Nicholls, Z., Möller, T., Hermans, T. H. J., Mengel, M., Kloenne, U., Smith, C., Slangen, A. B. A., and Palmer, M. D.: Multi-century global and regional sea-level rise commitments from cumulative greenhouse gas emissions in the coming decades, Nat. Clim. Change, <a href="https://doi.org/10.1038/s41558-025-02452-5" target="_blank">https://doi.org/10.1038/s41558-025-02452-5</a>, 2025.

    </mixed-citation></ref-html>
<ref-html id="bib1.bib32"><label>O'Neill et al.(2016)</label><mixed-citation>
       O'Neill, B. C., Tebaldi, C., van Vuuren, D. P., Eyring, V., Friedlingstein, P., Hurtt, G., Knutti, R., Kriegler, E., Lamarque, J.-F., Lowe, J., Meehl, G. A., Moss, R., Riahi, K., and Sanderson, B. M.: The Scenario Model Intercomparison Project (ScenarioMIP) for CMIP6, Geosci. Model Dev., 9, 3461–3482, <a href="https://doi.org/10.5194/gmd-9-3461-2016" target="_blank">https://doi.org/10.5194/gmd-9-3461-2016</a>, 2016.

    </mixed-citation></ref-html>
<ref-html id="bib1.bib33"><label>Oschlies et al.(2018)</label><mixed-citation>
       Oschlies, A., Brandt, P., Stramma, L., and Schmidtko, S.: Drivers and mechanisms of ocean deoxygenation, Nat. Geosci., 11, 467–473, <a href="https://doi.org/10.1038/s41561-018-0152-2" target="_blank">https://doi.org/10.1038/s41561-018-0152-2</a>, 2018.

    </mixed-citation></ref-html>
<ref-html id="bib1.bib34"><label>Pfleiderer et al.(2024)</label><mixed-citation>
       Pfleiderer, P., Schleussner, C.-F., and Sillmann, J.: Limited reversal of regional climate signals in overshoot scenarios, Environmental Research: Climate, 3, 015005, <a href="https://doi.org/10.1088/2752-5295/ad1c45" target="_blank">https://doi.org/10.1088/2752-5295/ad1c45</a>, 2024.

    </mixed-citation></ref-html>
<ref-html id="bib1.bib35"><label>Rahmstorf(1995)</label><mixed-citation>
       Rahmstorf, S.: Bifurcations of the Atlantic thermohaline circulation in response to changes in the hydrological cycle, Nature, 378, 145–149, <a href="https://doi.org/10.1038/378145a0" target="_blank">https://doi.org/10.1038/378145a0</a>, 1995.

    </mixed-citation></ref-html>
<ref-html id="bib1.bib36"><label>Riahi et al.(2022)</label><mixed-citation>
       Riahi, K., Schaeffer, R., Arango, J., Calvin, K., Guivarch, C., Hasegawa, T., Jiang, K., Kriegler, E., Matthews, R., Peters, G. P., Rao, A., Robertson, S., Sebbit, A. M., Steinberger, J., Tavoni, M., and Van Vuuren, D. P.: Mitigation pathways compatible with long-term goals., in: IPCC, 2022: Climate Change 2022: Mitigation of Climate Change. Contribution of Working Group III to the Sixth Assessment Report of the Intergovernmental Panel on Climate Change, edited by: Shukla, P. R., Skea, J., Slade, R., Khourdajie, A. A., van Diemen, R., McCollum, D., Pathak, M., Some, S., Vyas, P., Fradera, R., Belkacemi, M., Hasija, A., Lisboa, G., Luz, S., and Malley, J., Cambridge University Press, Cambridge, UK and New York, NY, USA, <a href="https://doi.org/10.1017/9781009157926.005" target="_blank">https://doi.org/10.1017/9781009157926.005</a>, 2022.

    </mixed-citation></ref-html>
<ref-html id="bib1.bib37"><label>Rogelj et al.(2018)</label><mixed-citation>
       Rogelj, J., Popp, A., Calvin, K. V., Luderer, G., Emmerling, J., Gernaat, D., Fujimori, S., Strefler, J., Hasegawa, T., Marangoni, G., Krey, V., Kriegler, E., Riahi, K., van Vuuren, D. P., Doelman, J., Drouet, L., Edmonds, J., Fricko, O., Harmsen, M., Havlík, P., Humpenöder, F., Stehfest, E., and Tavoni, M.: Scenarios towards limiting global mean temperature increase below 1.5&thinsp;°C, Nat. Clim. Change, 8, 325–332, <a href="https://doi.org/10.1038/s41558-018-0091-3" target="_blank">https://doi.org/10.1038/s41558-018-0091-3</a>, 2018.

    </mixed-citation></ref-html>
<ref-html id="bib1.bib38"><label>Roldán-Gómez et al.(2025a)</label><mixed-citation>
       Roldán-Gómez, P. J., De Luca, P., Bernardello, R., and Donat, M. G.: Regional irreversibility of mean and extreme surface air temperature and precipitation in CMIP6 overshoot scenarios associated with interhemispheric temperature asymmetries, Earth Syst. Dynam., 16, 1–27, <a href="https://doi.org/10.5194/esd-16-1-2025" target="_blank">https://doi.org/10.5194/esd-16-1-2025</a>, 2025a.

    </mixed-citation></ref-html>
<ref-html id="bib1.bib39"><label>Roldán-Gómez et al.(2025b)</label><mixed-citation>
       Roldán-Gómez, P. J., Ortega, P., and Donat, M. G.: Contribution of meridional overturning circulation and sea ice changes to large-scale temperature asymmetries in CMIP6 overshoot scenarios, Ocean Sci., 21, 2283–2303, <a href="https://doi.org/10.5194/os-21-2283-2025" target="_blank">https://doi.org/10.5194/os-21-2283-2025</a>, 2025b.

    </mixed-citation></ref-html>
<ref-html id="bib1.bib40"><label>Rosenzweig et al.(2017)</label><mixed-citation>
       Rosenzweig, C., Arnell, N. W., Ebi, K. L., Lotze-Campen, H., Raes, F., Rapley, C., Smith, M. S., Cramer, W., Frieler, K., Reyer, C. P. O., Schewe, J., Van Vuuren, D., and Warszawski, L.: Assessing inter-sectoral climate change risks: the role of ISIMIP, Environ. Res. Lett., 12, 010301, <a href="https://doi.org/10.1088/1748-9326/12/1/010301" target="_blank">https://doi.org/10.1088/1748-9326/12/1/010301</a>, 2017.

    </mixed-citation></ref-html>
<ref-html id="bib1.bib41"><label>Sanderson et al.(2024)</label><mixed-citation>
       Sanderson, B. M., Booth, B. B. B., Dunne, J., Eyring, V., Fisher, R. A., Friedlingstein, P., Gidden, M. J., Hajima, T., Jones, C. D., Jones, C. G., King, A., Koven, C. D., Lawrence, D. M., Lowe, J., Mengis, N., Peters, G. P., Rogelj, J., Smith, C., Snyder, A. C., Simpson, I. R., Swann, A. L. S., Tebaldi, C., Ilyina, T., Schleussner, C.-F., Séférian, R., Samset, B. H., van Vuuren, D., and Zaehle, S.: The need for carbon-emissions-driven climate projections in CMIP7, Geosci. Model Dev., 17, 8141–8172, <a href="https://doi.org/10.5194/gmd-17-8141-2024" target="_blank">https://doi.org/10.5194/gmd-17-8141-2024</a>, 2024.

    </mixed-citation></ref-html>
<ref-html id="bib1.bib42"><label>Sarofim et al.(2024)</label><mixed-citation>
       Sarofim, M. C., Smith, C. J., Malek, P., McDuffie, E. E., Hartin, C. A., Lay, C. R., and McGrath, S.: High radiative forcing climate scenario relevance analyzed with a ten-million-member ensemble, Nat. Commun., 15, 8185, <a href="https://doi.org/10.1038/s41467-024-52437-9" target="_blank">https://doi.org/10.1038/s41467-024-52437-9</a>, 2024.

    </mixed-citation></ref-html>
<ref-html id="bib1.bib43"><label>Schleussner et al.(2024)</label><mixed-citation>
       Schleussner, C.-F., Ganti, G., Lejeune, Q., Zhu, B., Pfleiderer, P., Prütz, R., Ciais, P., Frölicher, T. L., Fuss, S., Gasser, T., Gidden, M. J., Kropf, C. M., Lacroix, F., Lamboll, R., Martyr, R., Maussion, F., McCaughey, J. W., Meinshausen, M., Mengel, M., Nicholls, Z., Quilcaille, Y., Sanderson, B., Seneviratne, S. I., Sillmann, J., Smith, C. J., Steinert, N. J., Theokritoff, E., Warren, R., Price, J., and Rogelj, J.: Overconfidence in climate overshoot, Nature, 634, 366–373, <a href="https://doi.org/10.1038/s41586-024-08020-9" target="_blank">https://doi.org/10.1038/s41586-024-08020-9</a>, 2024.

    </mixed-citation></ref-html>
<ref-html id="bib1.bib44"><label>Schoenberg et al.(2025)</label><mixed-citation>
       Schoenberg, W., Blanz, B., Rajah, J. K., Callegari, B., Wells, C., Breier, J., Grimeland, M. B., Lindqvist, A. N., Ramme, L., Smith, C., Li, C., Mashhadi, S., Muralidhar, A., and Mauritzen, C.: An overview of FRIDA v2.1: a feedback-based, fully coupled, global integrated assessment model of climate and humans, Geosci. Model Dev., 18, 8047–8069, <a href="https://doi.org/10.5194/gmd-18-8047-2025" target="_blank">https://doi.org/10.5194/gmd-18-8047-2025</a>, 2025.

    </mixed-citation></ref-html>
<ref-html id="bib1.bib45"><label>Schwinger et al.(2022a)</label><mixed-citation>
       Schwinger, J., Asaadi, A., Goris, N., and Lee, H.: Possibility for strong northern hemisphere high-latitude cooling under negative emissions, Nat. Commun., 13, 1095, <a href="https://doi.org/10.1038/s41467-022-28573-5" target="_blank">https://doi.org/10.1038/s41467-022-28573-5</a>, 2022a.

    </mixed-citation></ref-html>
<ref-html id="bib1.bib46"><label>Schwinger et al.(2022b)</label><mixed-citation>
       Schwinger, J., Asaadi, A., Steinert, N. J., and Lee, H.: Emit now, mitigate later? Earth system reversibility under overshoots of different magnitudes and durations, Earth Syst. Dynam., 13, 1641–1665, <a href="https://doi.org/10.5194/esd-13-1641-2022" target="_blank">https://doi.org/10.5194/esd-13-1641-2022</a>, 2022b.

    </mixed-citation></ref-html>
<ref-html id="bib1.bib47"><label>Seland et al.(2020)</label><mixed-citation>
       Seland, Ø., Bentsen, M., Olivié, D., Toniazzo, T., Gjermundsen, A., Graff, L. S., Debernard, J. B., Gupta, A. K., He, Y.-C., Kirkevåg, A., Schwinger, J., Tjiputra, J., Aas, K. S., Bethke, I., Fan, Y., Griesfeller, J., Grini, A., Guo, C., Ilicak, M., Karset, I. H. H., Landgren, O., Liakka, J., Moseid, K. O., Nummelin, A., Spensberger, C., Tang, H., Zhang, Z., Heinze, C., Iversen, T., and Schulz, M.: Overview of the Norwegian Earth System Model (NorESM2) and key climate response of CMIP6 DECK, historical, and scenario simulations, Geosci. Model Dev., 13, 6165–6200, <a href="https://doi.org/10.5194/gmd-13-6165-2020" target="_blank">https://doi.org/10.5194/gmd-13-6165-2020</a>, 2020.

    </mixed-citation></ref-html>
<ref-html id="bib1.bib48"><label>Sigmond et al.(2020)</label><mixed-citation>
       Sigmond, M., Fyfe, J. C., Saenko, O. A., and Swart, N. C.: Ongoing AMOC and related sea-level and temperature changes after achieving the Paris targets, Nat. Clim. Change, 10, 672–677, <a href="https://doi.org/10.1038/s41558-020-0786-0" target="_blank">https://doi.org/10.1038/s41558-020-0786-0</a>, 2020.

    </mixed-citation></ref-html>
<ref-html id="bib1.bib49"><label>Smith et al.(2021)</label><mixed-citation>
       Smith, C.,
Nicholls, Z. R. J., Armour, K., Collins, W., Forster, P., Meinshausen, M.,
Palmer, M. D., and Watanabe, M.: The Earth's energy budget, climate
feedbacks, and climate sensitivity supplementary material, in:
Climate Change 2021: The Physical Science Basis. Contribution of
Working Group I to the Sixth Assessment Report of the
Intergovernmental Panel on Climate Change, edited by:
Masson-Delmotte, V., Zhai, P., Pirani, A., Connors, S. L., Péan, C.,
Berger, S., Caud, N., Chen, Y., Goldfarb, L., Gomis, M. I., Huang, M.,
Leitzell, K., Lonnoy, E., Matthews, J. B. R., Maycock, T. K., Waterfield, T.,
Yelekçi, O., Yu, R., and Zhou, B., Sect. 7.SM, Cambridge University Press, Cambridge,
UK and New York, NY, USA,
<a href="https://www.ipcc.ch/report/ar6/wg1/downloads/report/IPCC_AR6_WGI_Chapter07_SM.pdf" target="_blank"/> (last access: 22 June 2026), 1–35, 2021.

    </mixed-citation></ref-html>
<ref-html id="bib1.bib50"><label>Solomon et al.(2009)</label><mixed-citation>
       Solomon, S., Plattner, G.-K., Knutti, R., and Friedlingstein, P.: Irreversible climate change due to carbon dioxide emissions, P. Natl. Acad. Sci. USA, 106, 1704–1709, <a href="https://doi.org/10.1073/pnas.0812721106" target="_blank">https://doi.org/10.1073/pnas.0812721106</a>, 2009.

    </mixed-citation></ref-html>
<ref-html id="bib1.bib51"><label>Steinert et al.(2025)</label><mixed-citation>
       Steinert, N. J., Schwinger, J., Chadwick, R., Kug, J., and Lee, H.: Irreversible land water availability changes from a potential ITCZ shift during temperature overshoot, Earths Future, 13, e2024EF005787, <a href="https://doi.org/10.1029/2024EF005787" target="_blank">https://doi.org/10.1029/2024EF005787</a>, 2025.

    </mixed-citation></ref-html>
<ref-html id="bib1.bib52"><label>Stevens et al.(2017)</label><mixed-citation>
       Stevens, B., Fiedler, S., Kinne, S., Peters, K., Rast, S., Müsse, J., Smith, S. J., and Mauritsen, T.: MACv2-SP: a parameterization of anthropogenic aerosol optical properties and an associated Twomey effect for use in CMIP6, Geosci. Model Dev., 10, 433–452, <a href="https://doi.org/10.5194/gmd-10-433-2017" target="_blank">https://doi.org/10.5194/gmd-10-433-2017</a>, 2017.

    </mixed-citation></ref-html>
<ref-html id="bib1.bib53"><label>Tang et al.(2025)</label><mixed-citation>
      
Tang, G., Nicholls, Z., Jones, C., Gasser, T., Norton, A., Ziehn, T., Romero-Prieto, A., and Meinshausen, M.: Investigating carbon and nitrogen conservation in reported CMIP6 Earth system model data, Geosci. Model Dev., 18, 2111–2136, <a href="https://doi.org/10.5194/gmd-18-2111-2025" target="_blank">https://doi.org/10.5194/gmd-18-2111-2025</a>, 2025.

    </mixed-citation></ref-html>
<ref-html id="bib1.bib54"><label>Taylor et al.(2012)</label><mixed-citation>
       Taylor, K. E., Stouffer, R. J., and Meehl, G. A.: An Overview of CMIP5 and the experiment design, B. Am. Meteorol. Soc., 93, 485–498, <a href="https://doi.org/10.1175/BAMS-D-11-00094.1" target="_blank">https://doi.org/10.1175/BAMS-D-11-00094.1</a>, 2012.

    </mixed-citation></ref-html>
<ref-html id="bib1.bib55"><label>Tebaldi et al.(2021)</label><mixed-citation>
       Tebaldi, C., Debeire, K., Eyring, V., Fischer, E., Fyfe, J., Friedlingstein, P., Knutti, R., Lowe, J., O'Neill, B., Sanderson, B., van Vuuren, D., Riahi, K., Meinshausen, M., Nicholls, Z., Tokarska, K. B., Hurtt, G., Kriegler, E., Lamarque, J.-F., Meehl, G., Moss, R., Bauer, S. E., Boucher, O., Brovkin, V., Byun, Y.-H., Dix, M., Gualdi, S., Guo, H., John, J. G., Kharin, S., Kim, Y., Koshiro, T., Ma, L., Olivié, D., Panickal, S., Qiao, F., Rong, X., Rosenbloom, N., Schupfner, M., Séférian, R., Sellar, A., Semmler, T., Shi, X., Song, Z., Steger, C., Stouffer, R., Swart, N., Tachiiri, K., Tang, Q., Tatebe, H., Voldoire, A., Volodin, E., Wyser, K., Xin, X., Yang, S., Yu, Y., and Ziehn, T.: Climate model projections from the Scenario Model Intercomparison Project (ScenarioMIP) of CMIP6, Earth Syst. Dynam., 12, 253–293, <a href="https://doi.org/10.5194/esd-12-253-2021" target="_blank">https://doi.org/10.5194/esd-12-253-2021</a>, 2021.

    </mixed-citation></ref-html>
<ref-html id="bib1.bib56"><label>Tjiputra et al.(2020)</label><mixed-citation>
       Tjiputra, J. F., Schwinger, J., Bentsen, M., Morée, A. L., Gao, S., Bethke, I., Heinze, C., Goris, N., Gupta, A., He, Y.-C., Olivié, D., Seland, Ø., and Schulz, M.: Ocean biogeochemistry in the Norwegian Earth System Model version 2 (NorESM2), Geosci. Model Dev., 13, 2393–2431, <a href="https://doi.org/10.5194/gmd-13-2393-2020" target="_blank">https://doi.org/10.5194/gmd-13-2393-2020</a>, 2020.

    </mixed-citation></ref-html>
<ref-html id="bib1.bib57"><label>Tokarska and Zickfeld(2015)</label><mixed-citation>
       Tokarska, K. B. and Zickfeld, K.: The effectiveness of net negative carbon dioxide emissions in reversing anthropogenic climate change, Environ. Res. Lett., 10, 094013, <a href="https://doi.org/10.1088/1748-9326/10/9/094013" target="_blank">https://doi.org/10.1088/1748-9326/10/9/094013</a>, 2015.

    </mixed-citation></ref-html>
<ref-html id="bib1.bib58"><label>Van Vuuren et al.(2026)</label><mixed-citation>
       Van Vuuren, D. P., O'Neill, B. C., Tebaldi, C., Sanderson, B. M., Chini, L. P., Friedlingstein, P., Hasegawa, T., Riahi, K., Govindasamy, B., Bauer, N., Eyring, V., Fall, C. M. N., Frieler, K., Gidden, M. J., Gohar, L. K., Högner, A., Jones, A. D., Kikstra, J., King, A., Knutti, R., Kriegler, E., Lawrence, P., Lennard, C., Lowe, J., Mathison, C., Mehmood, S., Nicholls, Z., Prado, L. F., Zhang, Q., Rose, S. K., Ruane, A. C., Sandstad, M., Schleussner, C.-F., Seferian, R., Sillmann, J., Smith, C., Sörensson, A. A., Panickal, S., Tachiiri, K., Vaughan, N., Vishwanathan, S. S., Yokohata, T., Zecchetto, M., and Ziehn, T.: The Scenario Model Intercomparison Project for CMIP7 (ScenarioMIP-CMIP7), Geosci. Model Dev., 19, 2627–2656, <a href="https://doi.org/10.5194/gmd-19-2627-2026" target="_blank">https://doi.org/10.5194/gmd-19-2627-2026</a>, 2026.

    </mixed-citation></ref-html>
<ref-html id="bib1.bib59"><label>Wells et al.(2026a)</label><mixed-citation>
       Wells, C. D., Blanz, B., Ramme, L., Breier, J., Callegari, B., Muralidhar, A., Rajah, J. K., Lindqvist, A. N., Eriksson, A. E., Schoenberg, W. A., Köberle, A. C., Wang-Erlandsson, L., Mauritzen, C., Grimeland, M. B., and Smith, C.: The representation of climate impacts in the FRIDAv2.1 Integrated Assessment Model, Geosci. Model Dev., 19, 1229–1260, <a href="https://doi.org/10.5194/gmd-19-1229-2026" target="_blank">https://doi.org/10.5194/gmd-19-1229-2026</a>, 2026a.

    </mixed-citation></ref-html>
<ref-html id="bib1.bib60"><label>Wells et al.(2026b)</label><mixed-citation>
       Wells, C. D., Cummins, D. P., He, H., and Smith, C.: Long run emulator calibration increases warming and sea-level rise projections, Environ. Res. Lett., 21, 034008, <a href="https://doi.org/10.1088/1748-9326/ae3847" target="_blank">https://doi.org/10.1088/1748-9326/ae3847</a>, 2026b.


    </mixed-citation></ref-html>
<ref-html id="bib1.bib61"><label>Wigley and Raper(1987)</label><mixed-citation>
       Wigley, T. M. L. and Raper, S. C. B.: Thermal expansion of sea water associated with global warming, Nature, 330, 127–131, <a href="https://doi.org/10.1038/330127a0" target="_blank">https://doi.org/10.1038/330127a0</a>, 1987.

    </mixed-citation></ref-html>
<ref-html id="bib1.bib62"><label>Woodard et al.(2019)</label><mixed-citation>
       Woodard, D. L., Davis, S. J., and Randerson, J. T.: Economic carbon cycle feedbacks may offset additional warming from natural feedbacks, P. Natl. Acad. Sci. USA, 116, 759–764, <a href="https://doi.org/10.1073/pnas.1805187115" target="_blank">https://doi.org/10.1073/pnas.1805187115</a>, 2019.

    </mixed-citation></ref-html>
<ref-html id="bib1.bib63"><label>Wunderling et al.(2024)</label><mixed-citation>
       Wunderling, N., von der Heydt, A. S., Aksenov, Y., Barker, S., Bastiaansen, R., Brovkin, V., Brunetti, M., Couplet, V., Kleinen, T., Lear, C. H., Lohmann, J., Roman-Cuesta, R. M., Sinet, S., Swingedouw, D., Winkelmann, R., Anand, P., Barichivich, J., Bathiany, S., Baudena, M., Bruun, J. T., Chiessi, C. M., Coxall, H. K., Docquier, D., Donges, J. F., Falkena, S. K. J., Klose, A. K., Obura, D., Rocha, J., Rynders, S., Steinert, N. J., and Willeit, M.: Climate tipping point interactions and cascades: a review, Earth Syst. Dynam., 15, 41–74, <a href="https://doi.org/10.5194/esd-15-41-2024" target="_blank">https://doi.org/10.5194/esd-15-41-2024</a>, 2024.

    </mixed-citation></ref-html>--></article>
