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  <front>
    <journal-meta><journal-id journal-id-type="publisher">ESD</journal-id><journal-title-group>
    <journal-title>Earth System Dynamics</journal-title>
    <abbrev-journal-title abbrev-type="publisher">ESD</abbrev-journal-title><abbrev-journal-title abbrev-type="nlm-ta">Earth Syst. Dynam.</abbrev-journal-title>
  </journal-title-group><issn pub-type="epub">2190-4987</issn><publisher>
    <publisher-name>Copernicus Publications</publisher-name>
    <publisher-loc>Göttingen, Germany</publisher-loc>
  </publisher></journal-meta>
    <article-meta>
      <article-id pub-id-type="doi">10.5194/esd-14-367-2023</article-id><title-group><article-title>The deployment length of solar radiation modification: an interplay of
mitigation, net-negative emissions<?xmltex \hack{\break}?> and climate uncertainty</article-title><alt-title>The deployment length of solar radiation modification</alt-title>
      </title-group><?xmltex \runningtitle{The deployment length of solar radiation modification}?><?xmltex \runningauthor{S.~Baur et al.}?>
      <contrib-group>
        <contrib contrib-type="author" corresp="yes" rid="aff1 aff2">
          <name><surname>Baur</surname><given-names>Susanne</given-names></name>
          <email>susanne.baur@cerfacs.fr</email>
        <ext-link>https://orcid.org/0000-0002-3711-0890</ext-link></contrib>
        <contrib contrib-type="author" corresp="no" rid="aff2 aff3">
          <name><surname>Nauels</surname><given-names>Alexander</given-names></name>
          
        <ext-link>https://orcid.org/0000-0003-1378-3377</ext-link></contrib>
        <contrib contrib-type="author" corresp="no" rid="aff3">
          <name><surname>Nicholls</surname><given-names>Zebedee</given-names></name>
          
        <ext-link>https://orcid.org/0000-0002-4767-2723</ext-link></contrib>
        <contrib contrib-type="author" corresp="no" rid="aff5">
          <name><surname>Sanderson</surname><given-names>Benjamin M.</given-names></name>
          
        </contrib>
        <contrib contrib-type="author" corresp="no" rid="aff2 aff4">
          <name><surname>Schleussner</surname><given-names>Carl-Friedrich</given-names></name>
          
        <ext-link>https://orcid.org/0000-0001-8471-848X</ext-link></contrib>
        <aff id="aff1"><label>1</label><institution>CECI, Université de Toulouse, CERFACS, CNRS, Toulouse, 31100,
France</institution>
        </aff>
        <aff id="aff2"><label>2</label><institution>Climate Analytics, 10969 Berlin, Germany</institution>
        </aff>
        <aff id="aff3"><label>3</label><institution>Australian-German Climate and Energy College, The University of
Melbourne,<?xmltex \hack{\break}?> Parkville, VIC 3010, Australia</institution>
        </aff>
        <aff id="aff4"><label>4</label><institution>Geography Department and IRI THESys, Humboldt-Universität zu
Berlin, Berlin, Germany</institution>
        </aff>
        <aff id="aff5"><label>5</label><institution>Centre for International Climate and Environmental Research (CICERO),
Oslo, Norway</institution>
        </aff>
      </contrib-group>
      <author-notes><corresp id="corr1">Susanne Baur (susanne.baur@cerfacs.fr)</corresp></author-notes><pub-date><day>28</day><month>March</month><year>2023</year></pub-date>
      
      <volume>14</volume>
      <issue>2</issue>
      <fpage>367</fpage><lpage>381</lpage>
      <history>
        <date date-type="received"><day>26</day><month>April</month><year>2022</year></date>
           <date date-type="rev-request"><day>29</day><month>April</month><year>2022</year></date>
           <date date-type="rev-recd"><day>8</day><month>March</month><year>2023</year></date>
           <date date-type="accepted"><day>8</day><month>March</month><year>2023</year></date>
      </history>
      <permissions>
        <copyright-statement>Copyright: © 2023 </copyright-statement>
        <copyright-year>2023</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/.html">This article is available from https://esd.copernicus.org/articles/.html</self-uri><self-uri xlink:href="https://esd.copernicus.org/articles/.pdf">The full text article is available as a PDF file from https://esd.copernicus.org/articles/.pdf</self-uri>
      <abstract><title>Abstract</title>

      <p id="d1e150">A growing body of literature investigates the effects of solar
radiation modification (SRM) on global and regional climates. Previous
studies have focused on the potentials and the side effects of SRM, with little
attention being given to possible deployment timescales and the levels of carbon
dioxide removal required for a phase out. Here, we investigate the
deployment timescales of SRM and how they are affected by different levels
of mitigation, net-negative emissions (NNEs) and climate uncertainty. We
generate a large dataset of 355 emission scenarios in which SRM is deployed
to keep warming levels at 1.5 <inline-formula><mml:math id="M1" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula>C global mean temperature.
Probabilistic climate projections from this ensemble result in a large range
of plausible future warming and cooling rates that lead to various SRM
deployment timescales. In all pathways consistent with extrapolated current
ambition, SRM deployment would exceed 100 years even under the most
optimistic assumptions regarding climate response. As soon as the temperature
threshold is exceeded, neither mitigation nor NNEs or climate sensitivity
alone can guarantee short deployment timescales. Since the evolution of
mitigation under SRM, the availability of carbon removal technologies and
the effects of climate reversibility will be mostly unknown at its
initialisation time, it is impossible to predict how temporary SRM
deployment would be. Any deployment of SRM therefore comes with the risk of
multi-century legacies of deployment, implying multi-generational
commitments of costs, risks and negative side effects of SRM and NNEs
combined.</p>
  </abstract>
    
<funding-group>
<award-group id="gs1">
<funding-source>Horizon 2020</funding-source>
<award-id>CONSTRAIN - Constraining uncertainty of multi decadal climate projections (820829)</award-id>
<award-id>PROVIDE (101003687)</award-id>
<award-id>ESM2025 (101003536)</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="d1e171">Emission pathways that reflect the level of climate ambition of current
nationally determined contributions (NDCs) until the end of the century are
estimated to lead to an average global warming of around 2.4 <inline-formula><mml:math id="M2" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula>C
(CAT, 2022). This is still a lot higher than the warming limit agreed upon in the
Paris Agreement of 2015 that entails holding warming to well below
2 <inline-formula><mml:math id="M3" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula>C and pursuing efforts of limiting warming to 1.5 <inline-formula><mml:math id="M4" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula>C
(UNFCCC, 2015). The growing concern around overshooting the Paris
Agreement's long-term temperature target has led to a discussion of solar
radiation modification (SRM), which could in theory halt global temperature
increase very rapidly but only as long as it is actively supported
(Irvine et al., 2016; Keith, 2000). SRM
techniques intend to artificially lower global mean surface air temperature
(GSAT) by modifying the radiative energy budget of the Earth system.
Proposed methods include stratospheric aerosol injection (SAI), cirrus cloud
thinning (CCT) and marine cloud brightening (MCB; Lawrence et al., 2018). SRM methods generally<?pagebreak page368?> operate on
one of the key impacts of climate change, temperature increase, without
addressing its cause, anthropogenic greenhouse gas (GHG) emissions, or its other
impacts, e.g. ocean acidification. Without explicit emission reductions, as
well as the removal of some of these climate forcers from the atmosphere in
the long term, i.e. through carbon dioxide removal (CDR; Fuss et al., 2018), GHG emissions commit
us to millennia of elevated temperature levels. Therefore, SRM deployment
would only be temporary if combined with emission reductions and CDR.</p>
      <p id="d1e201">Achieving the Paris Agreement's target of 1.5 <inline-formula><mml:math id="M5" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula>C relies on
stringent mitigation with large near-term emission reductions, as shown in
the 1.5 <inline-formula><mml:math id="M6" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula>C compatible pathways assessed by the Intergovernmental
Panel on Climate Change (IPCC; Rogelj et al., 2018; IPCC, 2021,
2022). It has been discussed that, in the absence of this strong near-term
mitigation, SRM could be a tool to avoid the impacts associated with
overshooting 1.5 <inline-formula><mml:math id="M7" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula>C until emission reductions and CDR are
sufficiently scaled up such that SRM is no longer needed to artificially lower
GSAT
(Belaia
et al., 2021; Buck et al., 2020; MacMartin et al., 2018; Neuber and Ott,
2020; Allen et al., 2018). This “buying-time” approach, although criticised
for relying on uncertain promises of SRM and CDR and increasing the risk of
“climate debt” (Asayama and Hulme, 2019),
currently remains the dominant framework  for any SRM deployment
(Neuber and Ott, 2020). Surprisingly little analysis,
however, has been done on the timescales this type of SRM deployment could
entail. Tilmes et al. (2016) analysed the climate
impacts of pathways whose temperatures would peak at 3 <inline-formula><mml:math id="M8" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula>C by the
end of the 21st century and used CDR and SRM to limit temperature
increases to 2.5 and 2 <inline-formula><mml:math id="M9" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula>C. Similarly,
MacMartin et al. (2018) chose an experimental
setup where mitigation, CDR and SRM are used to meet the 1.5 <inline-formula><mml:math id="M10" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula>C goal from a “business-as-usual” starting point. Both Tilmes et al. (2016)
and MacMartin et al. (2018) did not discuss the length of SRM deployment
and looked at selected illustrative pathways that cannot capture the many
possible futures where a buying-time approach to SRM could be embedded.</p>
      <p id="d1e259">In this study, we generate a large dataset of scenarios that use SRM to
avoid overshooting the 1.5 <inline-formula><mml:math id="M11" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula>C warming target. The underlying
emission scenarios reflect current NDCs until 2030 and subsequently diverge
to spread a wide range of conditions by the end of the century. We employ
this large scenario set to explore a large variety of futures of SRM
interlinkages with mitigation ambition and different magnitudes to which CDR
could be scaled up. There is large uncertainty regarding the evolution of
emissions under SRM, with some studies arguing that SRM could be deployed for
“peak shaving” under already ambitious mitigation scenarios (Coninck et al.,
2018) or that it does not negatively affect the public's willingness to engage in
mitigation behaviours
(Andrews
et al., 2022; Austin and Converse, 2021; Fairbrother, 2016; Kahan et al.,
2015; Merk et al., 2016), while others fear that it could undermine mitigation
ambition even further
(Baatz,
2016; Corner and Pidgeon, 2014; Pierrehumbert, 2019; Raimi et al., 2019)
and present a “moral hazard” risk
(Belaia
et al., 2021; Bellamy et al., 2016; Burns et al., 2016; Keith, 2000;
McLaren, 2016; Merk et al., 2016; Moreno-Cruz, 2015; Wibeck et al., 2015).
Here, we do not investigate to what extent SRM will or will not change
mitigation ambition and instead highlight what various emission reduction
assumptions could mean in terms of SRM deployment length. Thanks to the
large dataset underlying this study, we can analyse several other factors
that influence the length of SRM deployment, such as the amount of annual
net-negative emissions (NNEs) realised through large-scale CDR and climate
system uncertainty.</p>
      <p id="d1e271">There is a large body of literature dedicated to CDR and its application in
mitigation pathways
(Fuss
et al., 2014, 2018; Johansson et al., 2020; Rogelj et al., 2019; Schleussner
et al., 2016). Large uncertainties regarding overshoot pathways and CDR
remain, especially since the technology and the resulting temperature
declines are unproven at scale (Pathak et al., 2022). Uncertainties are
related to the response of the climate system to negative emissions, the
state of the climate system post overshoot in general, the environmental and
economic side effects of large-scale deployment, and the level to which CDR
can be scaled up
(Fuss
et al., 2018; Matthews et al., 2020; Rogelj et al., 2019; Schleussner et
al., 2016; Zickfeld et al., 2016). In this study, we do not account for
feasibility constraints or the potential side effects of CDR deployment;
rather, we explicitly assess the sensitivity of our results to any such
constraints being in place. As part of our sensitivity assessment, we
consider a wide range for maximum annual NNEs reaching up to 40 Gt CO<inline-formula><mml:math id="M12" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula> yr<inline-formula><mml:math id="M13" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula> (the highest potential the IPCC 6th Assessment Report (AR6)
assigns to any carbon removal technology that does not interfere with ocean
chemistry (IPCC, 2022)), as well as the uncertainty surrounding the
temperature decline in response to net-negative emissions.</p>
      <p id="d1e296">It is important to examine SRM deployment length in the context of climate
uncertainty. In contrast to mitigation and CDR, climate uncertainty is
beyond human control and, as this study demonstrates, would result in
greatly differing SRM deployment outcomes for the same levels of emissions.
We address climate uncertainty in two ways: firstly, by considering a large
range of plausible climate simulators, and secondly, by calculating two
climate metrics that relate emissions to temperature change and affect the
duration of the overshoot and therefore SRM deployment length.</p>
      <p id="d1e299">While many different methods for CDR (Fuss
et al., 2018) and SRM
(Boucher et
al., 2013; Lawrence et al., 2018) that come with different
specificities exist, this study does not differentiate between these specific
technological approaches, as our results are independent of the boundary
conditions for individual SRM and CDR techniques. We acknowledge that
forecasting technology this far into the future is highly speculative, and
this analysis is by no means intended to be a realistic representation of
SRM and CDR pathways. Therefore, this paper does not address issues of
feasibility or the<?pagebreak page369?> environmental side effects of SRM or CDR, of which there are
many (Lee et al., 2021; Canadell et al., 2021; Douville et al., 2021), nor does it propose potential implementation strategies and designs or
pose questions relating to economic, political or ethical concerns. With
this contribution, we aim to provide a conceptual framework for exploring
SRM deployment length in the context of scenarios that use the technology as
a temporary (albeit potentially multi-century) measure.</p>
</sec>
<sec id="Ch1.S2">
  <label>2</label><title>Methods</title>
<sec id="Ch1.S2.SS1">
  <label>2.1</label><title>Emissions data and pathway extension</title>
      <p id="d1e317">As underlying data, we use all scenarios from the IPCC's 6th Assessment
Report's database that are in line with the 2030 NDCs (Riahi et al., 2022;
Byers et al., 2022) and have decreasing or stagnating emissions in the last
5 years of the 21st century. The policy categories we consider when
identifying the scenarios that pass through NDC emissions are P3b, P1c and
P0_3b (Riahi et al., 2022). This amounts to a total of 355
scenarios that cover the years 2015 to 2100 and that originate in a similar
climatic state in 2030 but diverge afterwards to cover a large variety of
emission levels in 2100. We employ this broad range of pathways to analyse
SRM under many different developments of mitigation ambition in relation to SRM, such
as large increases and decreases, as well as under the scrutiny of climate
change uncertainty, by running a probabilistic ensemble of 600 members (see
Sect. 2.2).</p>
      <p id="d1e320">To be able to estimate potential SRM timescales, we extend all pathways
until 2500. In order to explore a wide range of possible future developments,
we randomly sample three parameters for the extension of each scenario: the
change in rate of decarbonisation after 2100 (0 %–3 % increase), the maximum
net-negative fossil CO<inline-formula><mml:math id="M14" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula> emissions (log-normal distribution from 0–40 Gt CO<inline-formula><mml:math id="M15" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula> yr<inline-formula><mml:math id="M16" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula>) realised through large-scale CDR (Fig. 1c) and the floor
for CO<inline-formula><mml:math id="M17" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula> emissions from agriculture, forestry and other land use
(AFOLU CO<inline-formula><mml:math id="M18" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula>; normal distribution <inline-formula><mml:math id="M19" display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>1 to <inline-formula><mml:math id="M20" display="inline"><mml:mo>+</mml:mo></mml:math></inline-formula>1 Gt CO<inline-formula><mml:math id="M21" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula> yr<inline-formula><mml:math id="M22" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula>; Fig. 1f). For net fossil CO<inline-formula><mml:math id="M23" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula> we choose a positively skewed log-normal distribution of 0 to 40 Gt CO<inline-formula><mml:math id="M24" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula> yr<inline-formula><mml:math id="M25" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula>. The range depicts the maximum mitigation potential that
the IPCC AR6 assigns to industrial carbon removal technologies (direct air
carbon capture and storage – DACCS), while the distribution that is positively
skewed represents the tendency of limits to be at the lower rather than the higher
end of the chosen spectrum. The mean of the distribution is set to be 15 Gt CO<inline-formula><mml:math id="M26" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula> yr<inline-formula><mml:math id="M27" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula>, representing the rounded-up median potential experts assign
to DACCS in 2100 (Grant et al., 2021). The
storage capacity of technologically captured CO<inline-formula><mml:math id="M28" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula> is uncertain but is
likely in the range of 8000 to 55 000 Gt CO<inline-formula><mml:math id="M29" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula>
(Dooley, 2013; Kearns et al.,
2017). This capacity potential does not impact our results because even the
lower end is sufficient for the majority of our pathways (Fig. 4b). We
therefore choose no constraint on maximum negative cumulative
fossil CO<inline-formula><mml:math id="M30" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula> emissions. In contrast, nature-based CDR solutions
represented by AFOLU negative emissions are seriously limited in the total
amount they can remove. Current literature suggests that AFOLU-CDR is a
solution for the 21st century and that saturation could be hit soon
after (Fuss et al., 2018). Therefore, we
remove the need to make decisions about the role of AFOLU-CDR (which would
be a relatively small part of the picture over the timescales we are
considering) by setting the AFOLU long-term emissions level to be close to but
not exactly equal to 0 (<inline-formula><mml:math id="M31" display="inline"><mml:mo lspace="0mm">-</mml:mo></mml:math></inline-formula>1 to 1 Gt CO<inline-formula><mml:math id="M32" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula> yr<inline-formula><mml:math id="M33" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula> in line with the Global Carbon
Budget 2022;
Friedlingstein
et al., 2022). In the analysis of our results, we sum AFOLU and fossil
net-negative emissions into one variable which we call net-negative emissions
(NNEs).</p>
      <p id="d1e515">The modified decarbonisation rate of the last 10 years of the 21st
century is linearly extrapolated until meeting the maximum net-negative
fossil CO<inline-formula><mml:math id="M34" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula> emissions for the respective pathway (Fig. 1b, e). In the rare cases where scenarios have increasing AFOLU or fossil CO<inline-formula><mml:math id="M35" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula> emissions over the last 10 years (we only allow scenarios with stagnating or decreasing combined CO<inline-formula><mml:math id="M36" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula> emissions over the last few years, meaning fossil or AFOLU CO<inline-formula><mml:math id="M37" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula> can individually still have increasing emissions or decreasing negative emissions over the last decade) they are assigned decreasing emissions after 2100 with the rate of increasing emissions they had before plus the
change in rate that is randomly prescribed (0 %–3 %; see uppermost lines in
Fig. 1b, e). We assume that saturation for nature-based carbon removal is
hit in 2150 and that all pathways move linearly towards their randomly chosen
floor level after 2100 at a rate that allows the assigned floor to be reached
by 2150 (Fig. 1e). For simplicity, we hold non-CO<inline-formula><mml:math id="M38" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula> emissions constant
at 2100 emission levels until 2500, which gives some residual warming signal but is relatively small compared to the CO<inline-formula><mml:math id="M39" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula> contribution.</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F1" specific-use="star"><?xmltex \currentcnt{1}?><?xmltex \def\figurename{Figure}?><label>Figure 1</label><caption><p id="d1e576">Extension of emission pathways consistent with NDCs from the AR6 WG3 database to 2500. A distribution of extension options is used to sample the range of possible outcomes consistent with the current literature. For simplicity, in all cases, non-CO<inline-formula><mml:math id="M40" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula> emissions are kept constant after 2100. <bold>(a)</bold> Fossil CO<inline-formula><mml:math id="M41" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula> emissions from selected IPCC AR6 WG3 database scenarios (displayed: 5th–95th percentile). <bold>(b)</bold> Distribution of minimum fossil CO<inline-formula><mml:math id="M42" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula> emissions used in this study. <bold>(c)</bold> Illustration of extension algorithm used for fossil CO<inline-formula><mml:math id="M43" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula> emissions – each pathway is extended at a fixed rate of decline until it hits some prescribed value, after which emissions are held constant (see Sect. 2.1 for full description). <bold>(d)</bold> Land use CO<inline-formula><mml:math id="M44" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula> emissions from selected IPCC AR6 WG3 database scenarios (displayed: 5th–95th percentile). <bold>(e)</bold> Distribution of steady-state land use CO<inline-formula><mml:math id="M45" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula> emissions used in this study. <bold>(f)</bold> Illustration of extension algorithm used for land use CO<inline-formula><mml:math id="M46" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula> emissions – each pathway is extended so that it reaches a specific value by 2150, after which emissions are held constant (see Sect. 2.1 for full description). <bold>(g)</bold> Resulting temperature trajectories – the light-grey shading covers the 5th–95th percentiles over all scenarios with all 600 ensemble members, and the dark-grey shading covers the 5th–95th percentile of an exemplary scenario (MESSAGEix-GLOBIOM_1.1 EN_INDCi2030_1800f_NDCp), with the black line being the median of it. We cover a wide range of trajectories, from always remaining below 1.5 <inline-formula><mml:math id="M47" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula>C to never coming back below 1.5 <inline-formula><mml:math id="M48" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula>C after crossing 1.5 <inline-formula><mml:math id="M49" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula>C in the early 21st century.</p></caption>
          <?xmltex \igopts{width=503.61378pt}?><graphic xlink:href="https://esd.copernicus.org/articles/14/367/2023/esd-14-367-2023-f01.png"/>

        </fig>

</sec>
<sec id="Ch1.S2.SS2">
  <label>2.2</label><title>MAGICC setup and SRM pathway construction</title>
      <p id="d1e706">All global climate model simulations are conducted with the climate emulator
MAGICC7.5.3 (Meinshausen et al., 2020). This emulator is commonly used in
several leading integrated assessment models and consecutively in the IPCC
assessments, including the most recent sixth assessment cycle. The model
includes a simplified terrestrial and ocean carbon cycle
(Meinshausen
et al., 2009, 2011a, 2020). We apply a probabilistic setup with an ensemble
of 600 runs derived from a Markov chain Monte Carlo approach, and we display all
ensemble members except if indicated otherwise. The range of the ensemble
members depicts the equilibrium climate sensitivity uncertainty range of the
IPCC 6th Assessment Report (Forster et al., 2021) and the C4MIP carbon cycle
ranges (Forster et al., 2021) and as a consequence offers good coverage of
climate system and model uncertainty. The ensemble members span a transient
climate response to cumulative carbon emissions (TCRE) range of 0.87 to 3.47
[K/1000 PgC] (the 17 %–83 % range is from 1.37 to 2.19).</p>
      <?pagebreak page370?><p id="d1e709">The purpose of SRM in our scenario setup is to cool the temperature
overshoot pathways down to the global average warming of 1.5 <inline-formula><mml:math id="M50" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula>C,
starting in 2030. Because SRM is implemented in the model by modifying the
effective radiative forcing (ERF), it is necessary to determine what forcing
pathway is equivalent to following a 1.5 <inline-formula><mml:math id="M51" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula>C compliant trajectory
for each member of the ensemble (Fig. 2). This 1.5 <inline-formula><mml:math id="M52" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula>C trajectory
represents the SRM pathway. Due to the computational efficiency and the close
resemblance to WG3 NDC pathways, we choose an SSP2-4.5 pathway as a starting
point for this SRM pathway construction (Fig. 2a). This reduces the
required computing time by a factor of 10 while still retaining sufficient
accuracy to make useful quantifications of the required SRM deployment times.
Using 2030 NDC emission levels as the starting point for our analysis, we
also assume that radiative forcing can be modified no sooner than 2030.
Depending on the ensemble member, this leads to either a smooth approach to
1.5 <inline-formula><mml:math id="M53" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula>C where an overshoot is avoided in the SRM pathway (Fig. 2b) or to an overshoot that is subsequently brought down to 1.5 <inline-formula><mml:math id="M54" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula>C
(Fig. 2c). Whether the SRM pathway for a given ensemble member overshoots
is determined by its SSP2-4.5 2035 warming level had it followed its 10-year
gradient from 2030 to 2040 for 5 more years after 2030. If this 2035
warming level is higher than 1.5 <inline-formula><mml:math id="M55" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula>C, the pathway will overshoot to
the respective 2035 level and subsequently descend to 1.5 <inline-formula><mml:math id="M56" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula>C in a
sigmoidal pattern, reaching 1.5 <inline-formula><mml:math id="M57" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula>C in 2050.</p>
      <?pagebreak page371?><p id="d1e785">Since each of the 355 scenarios is prescribed different assumptions (see
Sect. 2.1) and since each ensemble member in MAGICC's probabilistic distribution has
different physics, we must calculate the SRM on a scenario–ensemble member
basis where the SRM required is the difference between the 1.5 <inline-formula><mml:math id="M58" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula>C pathway and the extended NDC scenario without SRM (NDC extension described
in Sect. 2.1). The start date of SRM is determined by the date where the extended
NDC scenario exceeds the designed SRM pathway for the respective ensemble
member. SRM termination is assumed to happen once 1.5 <inline-formula><mml:math id="M59" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula>C global
mean warming is reattained in the NDC scenario.</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F2" specific-use="star"><?xmltex \currentcnt{2}?><?xmltex \def\figurename{Figure}?><label>Figure 2</label><caption><p id="d1e809">Calculating required SRM. <bold>(a)</bold> Calculating warming to 2035 using an NDC-like pathway (in this case, SSP2-4.5). <bold>(b)</bold> Determining a 1.5 <inline-formula><mml:math id="M60" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula>C temperature trajectory for ensemble members that have not already overshot 1.5 <inline-formula><mml:math id="M61" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula>C by 2035. <bold>(c)</bold> Determining a 1.5 <inline-formula><mml:math id="M62" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula>C temperature trajectory for ensemble members that have already overshot 1.5 <inline-formula><mml:math id="M63" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula>C by 2035. <bold>(d, e)</bold> Calculating required solar radiation modification (SRM) for each scenario–ensemble member combination, whether it overshoots 1.5 <inline-formula><mml:math id="M64" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula>C <bold>(e)</bold> or remains below 1.5 <inline-formula><mml:math id="M65" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula>C at all times <bold>(d)</bold>.</p></caption>
          <?xmltex \igopts{width=503.61378pt}?><graphic xlink:href="https://esd.copernicus.org/articles/14/367/2023/esd-14-367-2023-f02.png"/>

        </fig>

      <p id="d1e892">To address climate uncertainty and to depict the whole range of possible
outcomes, we use all members of our ensemble instead of only focusing on
medians. Additionally, we calculate the uncertainty surrounding the rise in
temperature for a specific amount of CO<inline-formula><mml:math id="M66" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula> emissions and non-CO<inline-formula><mml:math id="M67" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula>
forcing, referred to as the effective transient response to cumulative CO<inline-formula><mml:math id="M68" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula> emissions (eTCRE, subsequently called eTCRE-up; Gregory
et al., 2009; Matthews et al., 2009, 2020; Vakilifard et al., 2022). We also
consider uncertainty in the temperature change as a result of reducing the
concentrations of CO<inline-formula><mml:math id="M69" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula> and associated non-CO<inline-formula><mml:math id="M70" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula> gases in the
atmosphere (subsequently called eTCRE-down). Due to uncertain Earth system
feedbacks such as a lagged ocean response, it is possible that eTCRE-up and
eTCRE-down are not identical (Matthews
et al., 2020; Zickfeld et al., 2016) and that this asymmetry is reflected in the
MAGICC ensemble. eTCRE-up informs us whether temperature targets are exceeded
for a specific amount of cumulative emissions and therefore whether SRM is
deployed in our scenarios or not, as well as the point at which peak warming is hit.
eTCRE-down informs us how effective NNEs are at cooling, indicating how many
cumulative NNEs we need and how long it would take to return to our target
temperature increase of 1.5 <inline-formula><mml:math id="M71" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula>C.</p>
      <p id="d1e950">We define eTCRE-up and eTCRE-down as follows:

                <disp-formula specific-use="gather" content-type="numbered"><mml:math id="M72" display="block"><mml:mtable displaystyle="true"><mml:mlabeledtr id="Ch1.E1"><mml:mtd><mml:mtext>1</mml:mtext></mml:mtd><mml:mtd><mml:mrow><mml:mstyle class="stylechange" displaystyle="true"/><?xmltex \hack{\hbox\bgroup\fontsize{9.5}{9.5}\selectfont$\displaystyle}?><mml:msub><mml:mi mathvariant="normal">eTCRE</mml:mi><mml:mi mathvariant="normal">up</mml:mi></mml:msub><mml:mo>=</mml:mo><mml:mstyle displaystyle="true"><mml:mfrac style="display"><mml:mrow><mml:mi mathvariant="normal">Δ</mml:mi><mml:msub><mml:mi>T</mml:mi><mml:mrow><mml:mn mathvariant="normal">2030</mml:mn><mml:mo>→</mml:mo><mml:mi mathvariant="normal">peak</mml:mi><mml:mi mathvariant="normal">_</mml:mi><mml:mi mathvariant="normal">warming</mml:mi></mml:mrow></mml:msub></mml:mrow><mml:mrow><mml:msubsup><mml:mo>∑</mml:mo><mml:mn mathvariant="normal">2030</mml:mn><mml:mrow><mml:mi mathvariant="normal">peak</mml:mi><mml:mi mathvariant="normal">_</mml:mi><mml:mi mathvariant="normal">warming</mml:mi></mml:mrow></mml:msubsup><mml:msub><mml:mi mathvariant="normal">CO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub><mml:mspace linebreak="nobreak" width="0.125em"/><mml:mi mathvariant="normal">emissions</mml:mi></mml:mrow></mml:mfrac></mml:mstyle><mml:mspace linebreak="nobreak" width="0.125em"/><mml:mo>[</mml:mo><mml:mrow class="unit"><mml:mi mathvariant="normal">K</mml:mi><mml:mspace width="0.125em" linebreak="nobreak"/><mml:mn mathvariant="normal">1000</mml:mn><mml:mspace linebreak="nobreak" width="0.125em"/><mml:msup><mml:mi mathvariant="normal">PgC</mml:mi><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:mrow><mml:mo>]</mml:mo><?xmltex \hack{$\egroup}?><mml:mo>,</mml:mo></mml:mrow></mml:mtd></mml:mlabeledtr><mml:mlabeledtr id="Ch1.E2"><mml:mtd><mml:mtext>2</mml:mtext></mml:mtd><mml:mtd><mml:mrow><mml:mstyle class="stylechange" displaystyle="true"/><mml:mtable class="split" rowspacing="0.2ex" displaystyle="true" columnalign="right left"><mml:mtr><mml:mtd><mml:mrow><mml:msub><mml:mi mathvariant="normal">eTCRE</mml:mi><mml:mi mathvariant="normal">down</mml:mi></mml:msub><mml:mo>=</mml:mo></mml:mrow></mml:mtd><mml:mtd><mml:mrow><mml:mstyle displaystyle="true"><mml:mfrac style="display"><mml:mrow><mml:mi mathvariant="normal">Δ</mml:mi><mml:msub><mml:mi>T</mml:mi><mml:mrow><mml:mn mathvariant="normal">1.5</mml:mn><mml:mspace linebreak="nobreak" width="0.125em"/><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup><mml:mrow class="unit"><mml:mi mathvariant="normal">C</mml:mi></mml:mrow><mml:mo>→</mml:mo><mml:mi mathvariant="normal">peak</mml:mi><mml:mi mathvariant="normal">_</mml:mi><mml:mi mathvariant="normal">warming</mml:mi></mml:mrow></mml:msub></mml:mrow><mml:mrow><mml:msubsup><mml:mo>∑</mml:mo><mml:mrow><mml:mi mathvariant="normal">peak</mml:mi><mml:mi mathvariant="normal">_</mml:mi><mml:mi mathvariant="normal">warming</mml:mi></mml:mrow><mml:mrow><mml:mi mathvariant="normal">year</mml:mi><mml:mi mathvariant="normal">_</mml:mi><mml:mi mathvariant="normal">of</mml:mi><mml:mi mathvariant="normal">_</mml:mi><mml:mi mathvariant="normal">return</mml:mi><mml:mi mathvariant="normal">_</mml:mi><mml:mi mathvariant="normal">to</mml:mi><mml:mi mathvariant="normal">_</mml:mi><mml:mn mathvariant="normal">1.5</mml:mn><mml:mspace linebreak="nobreak" width="0.125em"/><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup><mml:mrow class="unit"><mml:mi mathvariant="normal">C</mml:mi></mml:mrow></mml:mrow></mml:msubsup><mml:msub><mml:mi mathvariant="normal">CO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub><mml:mspace linebreak="nobreak" width="0.125em"/><mml:mi mathvariant="normal">emissions</mml:mi></mml:mrow></mml:mfrac></mml:mstyle></mml:mrow></mml:mtd></mml:mtr><mml:mtr><mml:mtd/><mml:mtd><mml:mrow><mml:mspace linebreak="nobreak" width="0.25em"/><mml:mspace linebreak="nobreak" width="0.25em"/><mml:mo>[</mml:mo><mml:mrow class="unit"><mml:mi mathvariant="normal">K</mml:mi><mml:mspace linebreak="nobreak" width="0.125em"/><mml:mn mathvariant="normal">1000</mml:mn><mml:mspace linebreak="nobreak" width="0.125em"/><mml:msup><mml:mi mathvariant="normal">PgC</mml:mi><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:mrow><mml:mo>]</mml:mo><mml:mo>.</mml:mo></mml:mrow></mml:mtd></mml:mtr></mml:mtable></mml:mrow></mml:mtd></mml:mlabeledtr></mml:mtable></mml:math></disp-formula>

            While the change in temperature is related to both CO<inline-formula><mml:math id="M73" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula> and non-CO<inline-formula><mml:math id="M74" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula>
gases, the cumulative emissions are only related to CO<inline-formula><mml:math id="M75" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula>. Due to a few
extreme outliers, both metrics are constrained to their 1st–99th percentiles.</p>
</sec>
</sec>
<sec id="Ch1.S3">
  <label>3</label><title>Results</title>
      <p id="d1e1194">The 355 NDC scenarios, including extensions and probabilistic MAGICC7
simulations, lead to 213 000 different realisations with a large range of
warming outcomes throughout the centuries (Fig. 1g). While few
realisations peak at or below 1.5 <inline-formula><mml:math id="M76" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula>C, the vast majority of the
baseline simulations without SRM overshoot the temperature target
temporarily. Others do not return back to 1.5 <inline-formula><mml:math id="M77" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula>C before 2500 at
all. The 5th–95th percentile range of peak warming in our dataset ranges from
1.60  to 3.91 <inline-formula><mml:math id="M78" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula>C, with the median at 2.14 <inline-formula><mml:math id="M79" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula>C.
Therefore, even though all realisations originate in 2030 NDC levels, due to
the range of possible developments of mitigation and NNEs under SRM, the
resulting SRM deployment length ranges from 0 to <inline-formula><mml:math id="M80" display="inline"><mml:mrow><mml:mi mathvariant="italic">&gt;</mml:mi><mml:mn mathvariant="normal">470</mml:mn></mml:mrow></mml:math></inline-formula> years
(Fig. 3), with 5 % of realisations not requiring SRM to limit warming to
1.5 <inline-formula><mml:math id="M81" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula>C and 15 % having deployment times that exceed 470 years.
In the following analysis, we only include realisations that fall into the
1–470 year range.</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F3" specific-use="star"><?xmltex \currentcnt{3}?><?xmltex \def\figurename{Figure}?><label>Figure 3</label><caption><p id="d1e1255">SRM deployment length for all scenarios and all ensemble members. One bar spans a range of 50 years. Marked in black are pathways consistent with current 2100 warming projections for NDCs (2.4 <inline-formula><mml:math id="M82" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula>C; CAT, 2022).</p></caption>
        <?xmltex \igopts{width=426.791339pt}?><graphic xlink:href="https://esd.copernicus.org/articles/14/367/2023/esd-14-367-2023-f03.png"/>

      </fig>

      <p id="d1e1273">Figure 4 breaks down the three indicators – mitigation, negative emissions and
climate uncertainty – and their interlinkages with SRM deployment length. The
relationship between the emission pathway, i.e. the cumulative emissions
from 2030 until net zero, and the SRM deployment length is weak (Fig. 4a). The
triangular shape of the data points towards a tendency for very high
cumulative emissions (<inline-formula><mml:math id="M83" display="inline"><mml:mrow><mml:mi mathvariant="italic">&gt;</mml:mi><mml:mn mathvariant="normal">3000</mml:mn></mml:mrow></mml:math></inline-formula> Gt CO<inline-formula><mml:math id="M84" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula> at time of net zero) to
lead to longer SRM timescales, whereas scenarios with lower cumulative
emissions are spread across the whole range of SRM deployment times, with a
skewing towards the shorter end. Realisations above 1500 Gt CO<inline-formula><mml:math id="M85" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula> (apart from
a few exceptions) require at least a few decades of deployment to keep
warming at 1.5 <inline-formula><mml:math id="M86" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula>C, no matter the climate uncertainty. The plot
looks stratified because the cumulative emissions value is
member independent and therefore stays equal across all ensemble members of
each scenario.</p>
      <p id="d1e1314">The way our scenarios are set up, the choice of maximum-potential NNEs is
random and therefore independent of the amount of cumulative emissions.
However, average annual NNEs are not entirely arbitrarily spread: shorter
deployment timescales are constrained to lower annual NNEs because of the
limited time these scenarios have to scale up their net-negative emissions.
Similarly, high-emission scenarios take longer to reach high net-negative
emissions. This is demonstrated by scenarios with cumulative emissions above
3500 Gt CO<inline-formula><mml:math id="M87" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula>, almost all of which reach annual NNEs above 15 Gt CO<inline-formula><mml:math id="M88" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula> yr<inline-formula><mml:math id="M89" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula> by
2500 (see Fig. S01 in the Supplement), but most never reach this level on average
terms because of the time required to scale up.</p>
      <p id="d1e1347">Focussing on the interlinkages with negative emissions, Fig. 4b shows
cumulative emissions between net zero and the reattainment of 1.5 <inline-formula><mml:math id="M90" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula>C
against SRM deployment. The relationship is much clearer, and the triangle
shape of Fig. 4b is considerably more defined; low cumulative negative
emissions are represented across the whole range of SRM deployment length,
but high cumulative negative emissions are constrained to long SRM
time frames. For example, cumulative negative-emission requirements above
<inline-formula><mml:math id="M91" display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>2000 Gt CO<inline-formula><mml:math id="M92" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula> imply more than 100 years of SRM deployment. Similarly,
<inline-formula><mml:math id="M93" display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>6000 Gt CO<inline-formula><mml:math id="M94" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula> leads to more than 200 years of SRM deployment, and <inline-formula><mml:math id="M95" display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>10 000 Gt CO<inline-formula><mml:math id="M96" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula> leads to more than 300 years of SRM deployment. Part of this effect is the simple fact
that you only get very large amounts of cumulative negative emissions if
you are deploying SRM for long time periods.</p>
      <p id="d1e1408">Whereas in Fig. 4a the annual average NNEs are partly random, a clear
pattern becomes visible in Fig. 4b. The higher the annual average NNEs, the
shorter the SRM timescale for the same amount of cumulative emissions. For
higher total negative-emission requirements, low NNEs are not sufficient in
limiting the deployment to 470 years<?pagebreak page372?> and are thus not shown. Very small
amounts of NNEs (<inline-formula><mml:math id="M97" display="inline"><mml:mrow><mml:mi mathvariant="italic">&lt;</mml:mi><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:math></inline-formula> Gt CO<inline-formula><mml:math id="M98" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula> yr<inline-formula><mml:math id="M99" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula>) are constrained to pathways with
no or very small amounts of the negative emissions required to get down to
1.5 <inline-formula><mml:math id="M100" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula>C of warming.</p>
      <p id="d1e1451">Regarding climate uncertainty, the calculated 5th–95th percentile range of
eTCRE-up is 1.0–6.0 [K/1000 PgC], and that of eTCRE-down is <inline-formula><mml:math id="M101" display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>6.9–12.4 [K/1000 PgC].
Figure 4c sets the eTCRE ratio (defined as eTCRE-up <inline-formula><mml:math id="M102" display="inline"><mml:mo>/</mml:mo></mml:math></inline-formula> eTCRE-down) against
the SRM time frames. The spread in uncertainty increases with SRM deployment
length. Realisations with an absolute eTCRE ratio of <inline-formula><mml:math id="M103" display="inline"><mml:mrow><mml:mi mathvariant="italic">&gt;</mml:mi><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:math></inline-formula> have a
lower sensitivity to negative emissions than to positive ones, causing them to
deploy SRM for longer periods even though net zero is reached earlier than for
other scenarios (see Fig. S02). Negative eTCRE ratios (dark-purple
data points) are the result of negative eTCRE-down values, all of which
arise in realisations that<?pagebreak page373?> have positive cumulative emissions in the cooling
phase. This could be due to a highly negative zero-emissions commitment (ZEC; Jenkins
et al., 2022; Jones et al., 2019; MacDougall et al., 2020) or non-CO<inline-formula><mml:math id="M104" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula>
effects that allow temperatures to drop despite cumulative positive CO<inline-formula><mml:math id="M105" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula> emissions.</p>

      <?xmltex \floatpos{p}?><fig id="Ch1.F4" specific-use="star"><?xmltex \currentcnt{4}?><?xmltex \def\figurename{Figure}?><label>Figure 4</label><caption><p id="d1e1498">Interdependencies of mitigation, negative emissions and climate uncertainty with SRM deployment length. <bold>(a)</bold> Relationship between cumulative CO<inline-formula><mml:math id="M106" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula> emissions from 2030 until net-zero CO<inline-formula><mml:math id="M107" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula> and SRM deployment length. Colour coding is according to annual average NNEs in Gt CO<inline-formula><mml:math id="M108" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula> yr<inline-formula><mml:math id="M109" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula>. <bold>(b)</bold> Relationship between cumulative CO<inline-formula><mml:math id="M110" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula> emissions from net-zero CO<inline-formula><mml:math id="M111" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula> until the reattainment of 1.5 <inline-formula><mml:math id="M112" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula>C and SRM deployment length. Colour coding is according to annual average NNEs in Gt CO<inline-formula><mml:math id="M113" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula> yr<inline-formula><mml:math id="M114" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula>. <bold>(c)</bold> Relationship between eTCRE ratio and SRM deployment length. Colour coding is according to cumulative CO<inline-formula><mml:math id="M115" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula> emissions from the time of peak warming until the reattainment of 1.5 <inline-formula><mml:math id="M116" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula>C. Plot shows data points that fall in the 1st–99th percentile range.</p></caption>
        <?xmltex \igopts{width=398.338583pt}?><graphic xlink:href="https://esd.copernicus.org/articles/14/367/2023/esd-14-367-2023-f04.png"/>

      </fig>

</sec>
<sec id="Ch1.S4">
  <label>4</label><title>Discussion</title>
      <p id="d1e1631">In current literature, SRM is often framed in the context of a stopgap
measure (Asayama
and Hulme, 2019; Buck et al., 2020; Neuber and Ott, 2020). Our study
focuses on the question of what range of time frames would be consistent with
an intended temporary SRM deployment due to the uncertainty in mitigation
ambition, negative emissions and climate uncertainty.</p>
      <p id="d1e1634">We show that the range of possible deployment timescales is vast even for
pathways that have similar conditions at the start of SRM deployment – in our
case, in 2030 (Fig. 3). This is due to the uncertain evolution of
mitigation ambition and annual NNEs under SRM and the effects of climate
uncertainty. We find that neither of these three indicators (mitigation,
net-negative emissions or climate uncertainty) alone can determine SRM
deployment length. Mitigation and negative emissions represent a bounding
condition on SRM deployment length rather than a linear correlation, to some
degree due to the climate sensitivity of increasing and decreasing emissions
(Fig. 4c). This means that positive emissions after SRM initialisation on
the medium to lower end could imply both short- and long-term SRM deployment
(Fig. 4a). Similarly, low cumulative negative-emission requirements are no
guarantee for short SRM time frames (Fig. 4b). However, the faster and
higher annual NNEs are scaled up, the shorter the time-wise commitment to SRM
(Figs. 4b, 5a). Our data suggest that, for the range of emission pathways,
NNEs and, in particular, the limited analysis length of 470 years in our
experiments, it might be easier to determine a lower limit of deployment
length rather than an upper limit.</p>
      <p id="d1e1637">The relationship between the eTCRE ratio and SRM deployment length versus
cumulative emissions that results from our data is complex and requires
further study (Figs. 4c, 5b). Several aspects play into the variables used
to calculate the two climate uncertainty metrics. For example, the
temperature change in the eTCRE calculation is related to CO<inline-formula><mml:math id="M117" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula> and non-CO<inline-formula><mml:math id="M118" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula> gases, while the cumulative emissions are only a function of
CO<inline-formula><mml:math id="M119" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula>. Additionally, the experimental setup of this study is such that
CO<inline-formula><mml:math id="M120" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula> and non-CO<inline-formula><mml:math id="M121" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula> emissions are not linearly related: non-CO<inline-formula><mml:math id="M122" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula>
emissions vary between 2030 and 2100 and then stay constant at the 2100
level, while CO<inline-formula><mml:math id="M123" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula> emissions fall consistently after 2100.</p>
      <p id="d1e1704">Our calculated eTCRE-up is higher than the pure range of TCRE that the
MAGICC7 ensemble members have, i.e. the TCRE range in the AR6 of the IPCC
(0.87–3.47). This is expected and has been observed before because of the
impact of non-CO<inline-formula><mml:math id="M124" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula> climate forcers
(Matthews et al., 2020;
Damon Matthews et al., 2021). Assumptions regarding the constant ratio of cumulative emissions of
CO<inline-formula><mml:math id="M125" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula> to temperature (TCRE) are suggested to go up to at least 3000 PgC
of positive cumulative CO<inline-formula><mml:math id="M126" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula> emissions
(Leduc et al., 2015; Tokarska
et al., 2016). Our values exceed this limit. However, this might not be
directly transferable to our eTCRE-up metric, especially since these values
are expectedly higher than TCRE (Matthews et al.,
2020). Studies with intermediate-complexity climate models have found a
higher TCRE-up compared to TCRE-down, suggesting a greater impact of positive
CO<inline-formula><mml:math id="M127" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula> emissions than negative emissions on temperatures
(Zickfeld et al., 2016). This can be explained by a lagged
ocean response that leads to continued warming after the start of carbon
removal (Zickfeld et al., 2016). However, ocean effects
might differ in cases where SRM is deployed and where complex Earth system models
show a range of responses after emissions are halted
(Jenkins
et al., 2022; MacDougall et al., 2020), let alone when they are negative for a sustained
period.</p>
      <p id="d1e1744">The inconclusive relationship of the eTCRE ratio and negative emissions
against SRM deployment length (Fig. 5) emphasises the fact that, while
ending SRM hinges fundamentally on the decline of temperatures (when SRM is
used for the purposes described in this paper), climate reversibility is
currently marked by large uncertainties.</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F5" specific-use="star"><?xmltex \currentcnt{5}?><?xmltex \def\figurename{Figure}?><label>Figure 5</label><caption><p id="d1e1749">Relationship between cumulative CO<inline-formula><mml:math id="M128" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula> emissions from net-zero CO<inline-formula><mml:math id="M129" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula> until the reattainment of 1.5 <inline-formula><mml:math id="M130" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula>C and SRM deployment length. <bold>(a)</bold> Colour coding is according to the maximum deployed annual NNEs. <bold>(b)</bold> Colour coding is according to the eTCRE ratio. See the clean figure without descriptions in the Supplement (Fig. S03).</p></caption>
        <?xmltex \igopts{width=503.61378pt}?><graphic xlink:href="https://esd.copernicus.org/articles/14/367/2023/esd-14-367-2023-f05.png"/>

      </fig>

      <p id="d1e1791">The shape of the triangle in Figs. 4a, b and  5a, b is partly due to
the effects of climate uncertainty and partly due to the experimental setup
with a limit of yearly NNEs at 40 Gt CO<inline-formula><mml:math id="M131" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula> yr<inline-formula><mml:math id="M132" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula>. However, the area of the
plot with short SRM deployment under around a century would not be covered
even for higher amounts of annual NNEs because the scaling up requires time.
To contextualise, a yearly removal of 40 Gt CO<inline-formula><mml:math id="M133" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula> equates to today's
yearly fossil CO<inline-formula><mml:math id="M134" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula> emissions
(Friedlingstein
et al., 2022) and would entail a massive industrial effort by itself, which
would take decades to build up. So even though very high NNEs could shorten
SRM timescales, it likely would not be available for short SRM deployments.
In those cases, the best bet is to require a small amount of total
net-negative emissions to return back down to 1.5 <inline-formula><mml:math id="M135" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula>C. This would
imply low cumulative positive emissions and a high eTCRE-down.</p>
      <?pagebreak page375?><p id="d1e1842">The upper limit of NNEs goes to the heart of concerns regarding CDR: the
magnitude of yearly removal to which it can be scaled up. Because it is
impossible to predict technological development this far into the future, we
reflect all plausible options by assuming NNEs that range from barely being
able to compensate residual positive emissions to being consistent with
current sustainable levels to much larger amounts that future technological
development could enable but that far exceed many estimates in the current literature
(Fuss et al., 2018;
Grant et al., 2021; Coninck et al., 2018; Pathak et al., 2022). It needs to
be highlighted that this study looks at net-negative emissions and not CDR.
This means that our estimates of net-negative emissions are a lower bound in terms of
the amount of CDR needed. There is a broad discussion in the current literature
regarding the negative side effects and sustainability concerns of CDR in mitigation
scenarios
(Brack
and King, 2020; Fuss et al., 2018; Smith et al., 2015), as well as the
question of equity in the allocation of CDR burden
(Fyson et al., 2020). Major concerns are the
considerable land, water, energy and financial requirements and constraints
in long-term storage of removed CO<inline-formula><mml:math id="M136" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula> that increase for higher yearly
removal rates. These recognised environmental and social concerns of CDR are
at least as applicable for pathways where CDR exceeds current sustainable
ranges and needs to be sustained for decades up to centuries. This paper
quantifies the importance of decades-long large-scale CDR for peak-shaving
SRM scenarios, which has previously been pointed out by Asayama and Hulme (2019) and others. In addition, we find that initialisation and commitment
to SRM happen under the promise that CDR can be scaled up high enough to end
SRM again. Belaia et al. (2021) even demonstrate that a cost-optimal
portfolio to meet a 2 <inline-formula><mml:math id="M137" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula>C GSAT increase would first consist of SRM and
mitigation and then, later, CDR deployment. With CDR being unproven at scale
and with peak-and-decline scenarios being marked by large uncertainties, this is a
risky promise. Our scenarios show what happens if the scalability of CDR is
not as high as assumed or if TCRE-down is low: SRM deployment will have to be
extended for a much longer period of time (Fig. 4b).</p>
      <p id="d1e1863">In scenarios where the level of warming in 2100 follows the level of
mitigation ambition reflected in 2030 NDC commitments until the end of the
century (CAT, 2022), no pathway deploys SRM for a shorter period than 100 years, while most require 150–300 years in order to return to a 1.5 <inline-formula><mml:math id="M138" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula>C GSAT increase (black bars in Fig. 3; the 25 %–75 % percentile range is from 159 to 294 years,  excluding all pathways that exceed 470 years in the statistic). Even
for scenarios with a somewhat smaller overshoot above 1.5 <inline-formula><mml:math id="M139" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula>C,
potential deployment length remains considerable. Half of all the scenario
realisations that would peak around 1.8 <inline-formula><mml:math id="M140" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula>C require SRM deployment
for 96–195 years to stay at 1.5 <inline-formula><mml:math id="M141" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula>C. Therefore, short
peak-shaving SRM deployment perhaps implies a length on the order of 100–200 years rather than 10–50 years. These time frames are much longer than the hotly
debated CDR deployment lengths in GHG emission reduction pathways for
limiting warming to 1.5 <inline-formula><mml:math id="M142" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula>C in 2100 after a high or no/limited
overshoot assessed in the IPCC SR1.5 (Rogelj et al., 2018) or the IPCC AR6 WG3
(Riahi et al, 2022).</p>
      <p id="d1e1912">MacMartin et al. (2018) created an exemplary scenario where emissions would
lead to a peak warming of 2.7 <inline-formula><mml:math id="M143" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula>C without SRM and would deploy 15 Gt CDR
per year. Their scenario requires around 235 years of SRM deployment to
limit warming to 1.5 <inline-formula><mml:math id="M144" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula>C. Constraining our dataset to<?pagebreak page376?> their
benchmark data results in an SRM deployment of 99–404 years, with a mean of
221 years – a range that encompasses their result with a mean that is not far off
from their estimate. Tilmes et al. (2016) constructed a scenario that peaks
at 3 <inline-formula><mml:math id="M145" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula>C and uses SRM to cool down to 2.0 <inline-formula><mml:math id="M146" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula>C with 18.5
GtCO<inline-formula><mml:math id="M147" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula> CDR per year. Simulated with the CESM Earth system model, they
indicate a deployment time of 160 years to compensate for the overshoot over
2 <inline-formula><mml:math id="M148" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula>C. While these results are not fully comparable, compensating for
1 <inline-formula><mml:math id="M149" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula>C of overshoot with NNEs of 18.5 Gt CO<inline-formula><mml:math id="M150" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula> per year in our
scenarios results in an average deployment length of 204 years and a full
range of 98–393 years. Our results thus compare well with previous
explorations of this question documented in the literature, yet they also provide a
much more holistic perspective on the uncertainties involved. As we
demonstrate, these are just few of the many possible future outcomes of SRM
deployment, and including climate uncertainty shows where the limits of our
control lie.</p>
      <p id="d1e1988">The challenge in defining SRM deployment length at its initialisation poses
a clear risk, as there are several issues that might arise with a
multi-century SRM deployment. One of the arguably biggest difficulties of
SRM deployment is international cooperation and coordination
(Möller, 2020; Reynolds, 2019;
Shepherd et al., 2009). Maintaining international cooperation will be even
more difficult if deployment needs to be sustained over many decades, as the
priorities and interests of countries and their leaders might change.
Furthermore, long-lasting SRM deployment would require substantial financial
resources; due to the difficulty in predicting SRM deployment length, as
pointed out in this study, costs could end up being much higher than
originally anticipated if deployment ends up being longer than planned. This
needs to be put into context with the overall cost of responding to climate
change and the avoided costs of climate change damages by means of SRM
(Arino
et al., 2016; Belaia et al., 2021). Moreover, a key risk of SRM is the
so-called “termination shock”, a rapid warming response to a sudden stop of
SRM deployment (Parker and Irvine, 2018). The longer
the deployment, the longer the risk of such an occurrence. And lastly,
long-term deployment would bind future generations to SRM, which raises
substantial ethical and moral questions
(Flegal et
al., 2019; Goeschl et al., 2013; Svoboda et al., 2011). The idea of imposing
a technology on individuals who have not yet been born and do not have a say
in the matter can be considered to be a violation of their rights and
autonomy. This ethical risk needs be considered in conjunction with the
additional climate-change-related risks from ongoing warming that may also be imposed on
future generations who did not contribute to the problem to begin with.</p>
      <p id="d1e1991">In addition to all the risks, costs and potential side effects that come
with SRM, due to the dependency, future generations would be burdened by
large-scale deployment of CDR, which might compete with efforts to secure
their own requirements by increasing the risks of biodiversity loss and food and
water scarcity (Dooley and Kartha, 2018; Shue, 2017; Asayama and Hulme,
2019; Svoboda et al., 2011). With this study, we add quantitative data to the
literature calling for precautionary and ethical approaches to technology
development. The identified risks need to be weighed against the risk of not
deploying SRM. Our research highlights the substantial dependencies of SRM
and CDR deployment, which imply the side effects, risks, costs and uncertainties
of both SRM and CDR.</p>
      <p id="d1e1994">In this analysis, we use SRM for the prevention of overshooting the
1.5 <inline-formula><mml:math id="M151" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula>C target, and the deployment lengths we indicate only hold
under the stated conditions of the analysis. Possible avenues for prior
phase outs have been discussed in
Keith and MacMartin (2015), MacMartin et al. (2018, 2022) and Parker and
Irvine (2018). However, these avenues would violate the 1.5 <inline-formula><mml:math id="M152" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula>C target and, as suggested by Parker and Irvine (2018), depending on the
amount of Wm<inline-formula><mml:math id="M153" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">2</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula> compensated for, could take several decades. Therefore, even
if SRM was, due to technical and/or environmental considerations, phased
out earlier, the phase out itself could become a multi-decadal undertaking.</p>
      <p id="d1e2027">Being a reduced-complexity model, MAGICC7 has its caveats and constraints
related to the physical and spatial resolution of relevant climate and
carbon cycle processes. Nevertheless, MAGICC has been used successfully in
many instances to robustly analyse long-term perspectives
(Meinshausen
et al., 2011b, 2020;  Nauels et al., 2017).
Therefore, we also consider it to be appropriate for this first quantification of
hypothetical SRM deployment length, which could motivate further study in
more complex models.</p>
      <p id="d1e2030">It is important to highlight that, even if global temperature was stabilised
with the help of SRM, this will not provide a solution with respect to the
regional impacts (Jones et al.,
2018) and the other impacts of high GHG concentration levels, such as ocean
acidification (Tjiputra et al., 2016). In
our study, however, we do not aim to provide a comprehensive analysis of the
impacts or side effects of such a climate intervention, nor do we provide a
likely or desirable implementation strategy; rather, we explore a concept to
determine hypothetical SRM deployment lengths.</p>
</sec>
<sec id="Ch1.S5" sec-type="conclusions">
  <label>5</label><title>Conclusions</title>
      <p id="d1e2042">In this paper, we generate a large dataset of pathways to analyse SRM
deployment length in scenarios that are consistent with 2030 NDC levels and
use SRM to cool down to 1.5 <inline-formula><mml:math id="M154" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula>C of warming. We find a large spread
of SRM deployment lengths, ranging from no NNE and SRM requirements at all
to massive NNE and SRM requirements past 2500 to limit global warming to
1.5 <inline-formula><mml:math id="M155" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula>C. Most of our simulations require around 150–300 years of
SRM. Deployment time frames are considerably dependent on mitigation,
negative emissions and climate uncertainty, yet none of these factors alone
can predict their length. Large cumulative positive<?pagebreak page377?> emissions lead to long SRM
deployments. However, small cumulative emissions are no guarantee for short
deployment timescales. Similarly, realisations that require large cumulative
negative emissions lead to long SRM deployments. However, small cumulative
negative-emission requirements do not necessarily imply short SRM
time frames. A large part of this uncertainty can be attributed to the
uncertainty surrounding eTCRE-up and eTCRE-down.</p>
      <p id="d1e2063">For all realisations that follow current NDC median 2100 warming projections
(2.4 <inline-formula><mml:math id="M156" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula>C), none deploy SRM for a shorter period than 100 years, even
under the most optimistic assumptions regarding the eTCRE ratio. For SRM deployment
to truly be temporary, carbon removal technologies need to be massively
scaled up within a relatively short time frame, except in cases of very low
emission requirements and extremely high negative ZEC. Larger average annual
NNEs do generally imply shorter SRM timescales.</p>
      <p id="d1e2075">Our study shows that the range of possible deployment timescales is vast
even if pathways start at a similar point at the beginning of SRM deployment
because the evolution of mitigation under SRM, the availability of carbon
removal technologies and the effects of climate reversibility are not
precisely known. Since these effects will be mostly uncertain at the time of
SRM initialisation, a precedent prediction of deployment length seems
unlikely, with possibilities ranging from decades to multiple centuries. This
is a knowledge gap that must be considered before any SRM proposal is
seriously considered.</p>
</sec>

      
      </body>
    <back><notes notes-type="codedataavailability"><title>Code and data availability</title>

      <p id="d1e2082">The code is publicly available at <ext-link xlink:href="https://doi.org/10.5281/zenodo.7707967" ext-link-type="DOI">10.5281/zenodo.7707967</ext-link> (Baur and Nicholls, 2023).
Raw data have been taken from the IPCC AR6 WGIII database <ext-link xlink:href="https://doi.org/10.5281/zenodo.7197970" ext-link-type="DOI">10.5281/zenodo.7197970</ext-link> (Byers et al., 2022).</p>
  </notes><app-group>
        <supplementary-material position="anchor"><p id="d1e2091">The supplement related to this article is available online at: <inline-supplementary-material xlink:href="https://doi.org/10.5194/esd-14-367-2023-supplement" xlink:title="pdf">https://doi.org/10.5194/esd-14-367-2023-supplement</inline-supplementary-material>.</p></supplementary-material>
        </app-group><notes notes-type="authorcontribution"><title>Author contributions</title>

      <p id="d1e2100">All the authors designed the experiments, and SB and ZN carried them out. SB
prepared the paper with contributions from all the authors.</p>
  </notes><notes notes-type="competinginterests"><title>Competing interests</title>

      <p id="d1e2106">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="d1e2112">Publisher's note: Copernicus Publications remains neutral with regard to jurisdictional claims in published maps and institutional affiliations.</p>
  </notes><ack><title>Acknowledgements</title><p id="d1e2118">Susanne Baur is supported by CERFACS through the project MIRAGE. Alexander Nauels, Zebedee Nicholls, Benjamin M. Sanderson  and Carl-Friedrich Schleussner
acknowledge support by the European Union's Horizon 2020 Research and
Innovation Programme; the respective Horizon 2020 projects are PROVIDE
(grant no. 101003687) for Carl-Friedrich Schleussner and Benjamin M. Sanderson, the project ESM2025 (grant no.
101003536) for  Zebedee Nicholls and Benjamin M. Sanderson, and the project CONSTRAIN (grant no. 820829) for
Alexander Nauels and Carl-Friedrich Schleussner.</p></ack><notes notes-type="financialsupport"><title>Financial support</title>

      <p id="d1e2123">This research has been supported by CERFACS (MIRAGE) and the Horizon 2020 projects PROVIDE (grant no. 101003687), CONSTRAIN (grant no. 820829) and ESM2025 (grant no. 101003536).</p>
  </notes><notes notes-type="reviewstatement"><title>Review statement</title>

      <p id="d1e2129">This paper was edited by Ben Kravitz and reviewed by Daniele Visioni and two anonymous referees.</p>
  </notes><ref-list>
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