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  <front>
    <journal-meta><journal-id journal-id-type="publisher">AMT</journal-id><journal-title-group>
    <journal-title>Atmospheric Measurement Techniques</journal-title>
    <abbrev-journal-title abbrev-type="publisher">AMT</abbrev-journal-title><abbrev-journal-title abbrev-type="nlm-ta">Atmos. Meas. Tech.</abbrev-journal-title>
  </journal-title-group><issn pub-type="epub">1867-8548</issn><publisher>
    <publisher-name>Copernicus Publications</publisher-name>
    <publisher-loc>Göttingen, Germany</publisher-loc>
  </publisher></journal-meta>
    <article-meta>
      <article-id pub-id-type="doi">10.5194/amt-19-3151-2026</article-id><title-group><article-title>Impact of spectral aerosol radiative forcing at the Izaña observatory during the August 2023 extreme wildfires</article-title><alt-title>Impact of spectral aerosol radiative forcing</alt-title>
      </title-group>
      <contrib-group>
        <contrib contrib-type="author" corresp="no" rid="aff1 aff2 aff3">
          <name><surname>García</surname><given-names>Rosa D.</given-names></name>
          
        <ext-link>https://orcid.org/0000-0002-9451-1631</ext-link></contrib>
        <contrib contrib-type="author" corresp="yes" rid="aff2 aff3">
          <name><surname>Barreto</surname><given-names>África</given-names></name>
          <email>abarretov@aemet.es</email>
        </contrib>
        <contrib contrib-type="author" corresp="no" rid="aff3">
          <name><surname>Cachorro</surname><given-names>Victoria E.</given-names></name>
          
        <ext-link>https://orcid.org/0000-0002-4627-9444</ext-link></contrib>
        <contrib contrib-type="author" corresp="no" rid="aff1 aff2 aff3">
          <name><surname>González-Sicilia</surname><given-names>Pablo</given-names></name>
          
        <ext-link>https://orcid.org/0009-0009-2067-8517</ext-link></contrib>
        <contrib contrib-type="author" corresp="no" rid="aff1 aff2 aff5">
          <name><surname>Léon-Luis</surname><given-names>Sergio</given-names></name>
          
        </contrib>
        <contrib contrib-type="author" corresp="no" rid="aff1 aff2">
          <name><surname>Álvarez-Hernández</surname><given-names>Ayoze</given-names></name>
          
        <ext-link>https://orcid.org/0000-0002-0621-1293</ext-link></contrib>
        <contrib contrib-type="author" corresp="no" rid="aff2">
          <name><surname>Bustos</surname><given-names>Juan José</given-names></name>
          
        </contrib>
        <contrib contrib-type="author" corresp="no" rid="aff2">
          <name><surname>Ramos</surname><given-names>Ramón</given-names></name>
          
        </contrib>
        <contrib contrib-type="author" corresp="no" rid="aff4 aff2">
          <name><surname>Almansa</surname><given-names>Fernando</given-names></name>
          
        <ext-link>https://orcid.org/0000-0002-3674-3944</ext-link></contrib>
        <contrib contrib-type="author" corresp="no" rid="aff1 aff2">
          <name><surname>Álvarez-Losada</surname><given-names>Óscar</given-names></name>
          
        <ext-link>https://orcid.org/0000-0002-6693-5058</ext-link></contrib>
        <contrib contrib-type="author" corresp="no" rid="aff4 aff2">
          <name><surname>González</surname><given-names>Yenny</given-names></name>
          
        <ext-link>https://orcid.org/0000-0001-5153-3972</ext-link></contrib>
        <contrib contrib-type="author" corresp="no" rid="aff2">
          <name><surname>Rivas</surname><given-names>Pedro Pablo</given-names></name>
          
        </contrib>
        <contrib contrib-type="author" corresp="no" rid="aff2">
          <name><surname>Torres</surname><given-names>Carlos Javier</given-names></name>
          
        <ext-link>https://orcid.org/0000-0002-5382-8835</ext-link></contrib>
        <aff id="aff1"><label>1</label><institution>TRAGSATEC, 28037, Madrid, Spain</institution>
        </aff>
        <aff id="aff2"><label>2</label><institution>Izaña Atmospheric Research Center (IARC), State Meteorological Agency of Spain (AEMET), 38108, Santa Cruz de Tenerife, Spain</institution>
        </aff>
        <aff id="aff3"><label>3</label><institution>Atmospheric Optics Group of Valladolid University (GOA-UVA), Valladolid University, Valladolid, Spain</institution>
        </aff>
        <aff id="aff4"><label>4</label><institution>Scientific department, CIMEL Electronique, Paris, 75011, France</institution>
        </aff>
        <aff id="aff5"><label>a</label><institution>now at: Department of Physics, La Laguna University, San Cristóbal de La Laguna, 38206, Spain</institution>
        </aff>
      </contrib-group>
      <author-notes><corresp id="corr1">África Barreto (abarretov@aemet.es)</corresp></author-notes><pub-date><day>13</day><month>May</month><year>2026</year></pub-date>
      
      <volume>19</volume>
      <issue>9</issue>
      <fpage>3151</fpage><lpage>3167</lpage>
      <history>
        <date date-type="received"><day>19</day><month>January</month><year>2026</year></date>
           <date date-type="rev-request"><day>2</day><month>February</month><year>2026</year></date>
           <date date-type="rev-recd"><day>20</day><month>March</month><year>2026</year></date>
           <date date-type="accepted"><day>2</day><month>April</month><year>2026</year></date>
      </history>
      <permissions>
        <copyright-statement>Copyright: © 2026 Rosa D. García et al.</copyright-statement>
        <copyright-year>2026</copyright-year>
      <license license-type="open-access"><license-p>This work is licensed under the Creative Commons Attribution 4.0 International License. To view a copy of this licence, visit <ext-link ext-link-type="uri" xlink:href="https://creativecommons.org/licenses/by/4.0/">https://creativecommons.org/licenses/by/4.0/</ext-link></license-p></license></permissions><self-uri xlink:href="https://amt.copernicus.org/articles/19/3151/2026/amt-19-3151-2026.html">This article is available from https://amt.copernicus.org/articles/19/3151/2026/amt-19-3151-2026.html</self-uri><self-uri xlink:href="https://amt.copernicus.org/articles/19/3151/2026/amt-19-3151-2026.pdf">The full text article is available as a PDF file from https://amt.copernicus.org/articles/19/3151/2026/amt-19-3151-2026.pdf</self-uri>
      <abstract><title>Abstract</title>

      <p id="d2e219">Extreme wildfires represent a highly variable source of atmospheric aerosols with potentially strong impacts on surface solar radiation. In August 2023, an exceptional wildfire on Tenerife (Canary Islands, Spain) reached the neighbourhoods of the Izaña Observatory (IZO, 2400 m a.s.l.). This near-source configuration enabled a rare observational characterisation of the spectral radiative effects of biomass-burning aerosols. During the most intense phases of the event (17–18 August), aerosol optical depth (AOD) at 500 nm reached extreme values of 3.63 and 2.25, respectively, with Ångström Exponent (AE) above 2, indicating a strong dominance of fine-mode smoke particles. Spectral measurements of global-horizontal, direct-normal and diffuse-horizontal solar irradiance (300–1100 nm) show a pronounced attenuation of direct and global irradiances, particularly in the visible range, together with a strong enhancement of diffuse radiation. Relative to clean-sky conditions, daily global irradiance decreased by 21 %–27 %, while direct-normal irradiance was reduced by 72 %–99 %. Spectral aerosol radiative forcing and radiative forcing efficiency at the surface were quantified using radiative transfer simulations under pristine atmospheric conditions as a reference. The integrated spectral radiative forcing (300–1100 nm) for global irradiance reached <inline-formula><mml:math id="M1" display="inline"><mml:mrow><mml:mi mathvariant="normal">−</mml:mi><mml:mn mathvariant="normal">395</mml:mn></mml:mrow></mml:math></inline-formula> and <inline-formula><mml:math id="M2" display="inline"><mml:mrow><mml:mi mathvariant="normal">−</mml:mi><mml:mn mathvariant="normal">299</mml:mn></mml:mrow></mml:math></inline-formula> W m<sup>−2</sup> on 17 and 18 August, respectively, indicating strong surface cooling dominated by scattering processes. Maximum forcing and efficiency occurred in the visible spectral range, consistent with the optical properties of freshly emitted smoke aerosols. At the same time, increases in the amount of present particles, equivalent black carbon (eBC) and greenhouse gases (CO<sub>2</sub>, CH<sub>4</sub> and CO) confirm the direct influence of the wildfire plume on atmospheric composition at IZO. These observations provide one of the few detailed spectral assessments of surface radiative forcing by extreme biomass-burning aerosols at a high-altitude site and highlight the need to accurately represent fine-mode smoke aerosols in radiative transfer and climate models.</p>
  </abstract>
    </article-meta>
  </front>
<body>
      

<sec id="Ch1.S1" sec-type="intro">
  <label>1</label><title>Introduction</title>
      <p id="d2e281">Wildfires are increasingly recognised as key agents of changes on the atmosphere, influencing air quality, the planetary radiation budget, and the climate system. According to the IPCC Sixth Assessment Report <xref ref-type="bibr" rid="bib1.bibx38" id="paren.1"/>, the total anthropogenic effective radiative forcing in 2019 relative to preindustrial conditions is estimated at 2.72 [1.96–3.48] W m<sup>−2</sup> (medium confidence) <xref ref-type="bibr" rid="bib1.bibx25" id="paren.2"/>. This positive forcing arises mainly from the continuous accumulation of greenhouse gases (GHGs), partially offset by the cooling effect due to anthropogenic aerosols. <xref ref-type="bibr" rid="bib1.bibx38" id="text.3"/> also reports a <inline-formula><mml:math id="M7" display="inline"><mml:mo>∼</mml:mo></mml:math></inline-formula> 0.43 W m<sup>−2</sup> (<inline-formula><mml:math id="M9" display="inline"><mml:mo lspace="0mm">∼</mml:mo></mml:math></inline-formula> 19 %) increase in the total radiative forcing since the Fifth Assessment Report <xref ref-type="bibr" rid="bib1.bibx37" id="paren.4"/>. Most of this increment, around 0.34 W m<sup>−2</sup>, is attributed to additional GHG emissions since 2011, while the remaining increase, around 0.09 W m<sup>−2</sup>, reflects improved estimates of aerosol contributions, owing to enhanced observational datasets and progress in representing aerosol–radiation and aerosol–cloud interactions in climate models.</p>
      <p id="d2e359">Among the different aerosol sources, biomass burning stands out as one of the most variable and least predictable in terms of emissions and radiative effects. Aerosols produced by wildfires encompass a heterogeneous mixture of absorbing components (e.g., black carbon, brown carbon) and scattering species (organic and inorganic matter). Their radiative influence depends strongly on their optical and microphysical characteristics, vertical distribution within the atmosphere, and interactions with clouds and underlying surfaces. These complexities generate significant uncertainty when assessing the radiative forcing associated with wildfire emissions.</p>
      <p id="d2e362">In recent decades, wildfire activity has intensified across many regions of the globe, a trend strongly linked to rising global temperatures, a higher frequency of extreme heat events, and widespread transformations in land use and droughts <xref ref-type="bibr" rid="bib1.bibx18 bib1.bibx21 bib1.bibx66" id="paren.5"/>. Current estimates indicate that wildfires burn 3.5–4.6 million km<sup>2</sup> each year, equivalent to about 2 %–3 % of Earth's land surface <xref ref-type="bibr" rid="bib1.bibx32" id="paren.6"/>. Beyond their ecological impacts, these events represent a major atmospheric source of trace gases and aerosols, with significant implications for air quality and climate. Areas with Mediterranean-type climates – such as southern Europe, California, central Chile, southwestern Australia, and parts of South Africa – are particularly prone to suffer large and intense fires due to their hot and dry summers, and strong interannual climatic variability. Within Europe, Mediterranean countries account for nearly 85 % of the total burned area <xref ref-type="bibr" rid="bib1.bibx58 bib1.bibx3 bib1.bibx67 bib1.bibx57" id="paren.7"/>. Recent high-impact fire seasons, including the 2016 Madeira fires <xref ref-type="bibr" rid="bib1.bibx47" id="paren.8"/> and the 2023 wildfire crisis in Greece <xref ref-type="bibr" rid="bib1.bibx43 bib1.bibx45 bib1.bibx40" id="paren.9"/>, have highlighted the growing societal exposure to fire hazards, often resulting in mass evacuations, severe damage to infrastructures, and major economic losses <xref ref-type="bibr" rid="bib1.bibx39 bib1.bibx21" id="paren.10"/>. At the same time, shifts in atmospheric circulation – particularly the increased frequency and intensity of extreme heatwaves and droughts – together with the desiccation of continental air masses, such as Saharan advection episodes, create highly favourable conditions for fire ignition and rapid fire spread. This is the case for one of the most frequent types of heatwaves over Europe, which often occur in the presence of intrusions of desert dust particles originating from North Africa <xref ref-type="bibr" rid="bib1.bibx66" id="paren.11"/>. The Canary Islands (Spain) are regularly influenced by such Saharan intrusions, which constitute a prominent and recurrent component of the regional atmospheric dynamics <xref ref-type="bibr" rid="bib1.bibx14 bib1.bibx7" id="paren.12"/>. These air masses are typically characterised by exceptionally low humidity and temperatures well above climatological values <xref ref-type="bibr" rid="bib1.bibx10" id="paren.13"/>.</p>
      <p id="d2e402">In August 2023, a large-scale wildfire on Tenerife (Canary Islands) allowed researchers to investigate, as an exceptional natural experiment, the atmospheric impacts of intense biomass burning. It was the second largest wildfire on Tenerife and the third in the Canary Islands since systematic monitoring began in 1983 <xref ref-type="bibr" rid="bib1.bibx10" id="paren.14"/>. The fire burned more than 13.000 ha across 12 municipalities and advanced, reaching the close vicinity of the Izaña Observatory (IZO), a high-mountain research station operated by the Spanish State Meteorological Agency (AEMET) through the Izaña Atmospheric Research Center (IARC). Although the observatory infrastructure was not damaged, the extreme closeness of the fire enabled direct observations of its impact in the low free troposphere. This unusual scenario provided a unique opportunity to examine how intense wildfire emissions affect a wide range of atmospheric parameters routinely measured at IZO. As part of the World Meteorological Organization (WMO) Global Atmosphere Watch (GAW) programme, and of the European Research Infrastructure Consortia ACTRIS (Aerosols, Clouds and Trace Gases Research Infrastructure) and ICOS (Integrated Carbon Observation System), IZO maintains long-term records of greenhouse gases, aerosols, solar radiation, and reactive gases, among other variables <xref ref-type="bibr" rid="bib1.bibx41 bib1.bibx16 bib1.bibx17" id="paren.15"/>. During the wildfire episode, pronounced anomalies were detected across these datasets, offering valuable insights into the radiative and compositional impacts of smoke intrusions at this remote high-elevated site.</p>
      <p id="d2e412">This study aims to characterise the spectral aerosol radiative forcing and efficiency exerted by wildfire aerosols. Such spectral studies are very scarce, and most existing works focus on the impact of wildfires on irradiance without considering their effects on radiative forcing or efficiency. The extreme 2023 fire episode occurred only a <inline-formula><mml:math id="M13" display="inline"><mml:mo>≈</mml:mo></mml:math></inline-formula> 280 m north and 620 m east of the spectroradiometer operating at IZO, providing a unique opportunity to directly observe the spectral radiative signal of fresh smoke under near-source conditions.</p>
      <p id="d2e422">The measurements used in this study were conducted within the framework of the WMO Measurement Lead Centre (MLC) for Aerosols and Water Vapour Remote Sensing Instruments. The structure of the paper is as follows: Sect. <xref ref-type="sec" rid="Ch1.S2"/> presents the main features of the Izaña Observatory and the instrumentation used in this work. Section <xref ref-type="sec" rid="Ch1.S3"/> describes the methodology applied to quantify aerosol spectral radiative forcing and radiative efficiency. Section <xref ref-type="sec" rid="Ch1.S4"/> provides an overview of the wildfire event and presents the key results. Finally, Sect. <xref ref-type="sec" rid="Ch1.S5"/> summarises the main conclusions of the study.</p>
</sec>
<sec id="Ch1.S2">
  <label>2</label><title>Site description and instruments</title>
<sec id="Ch1.S2.SS1">
  <label>2.1</label><title>Site description</title>
      <p id="d2e448">The datasets analysed in this study were obtained at the Izaña Observatory (IZO), operated by the Izaña Atmospheric Research Center (IARC) of the Spanish State Meteorological Agency (AEMET) (<uri>http://izana.aemet.es</uri>, last access: 15 April 2025). IZO is located on the island of Tenerife (Canary Islands, Spain (28.3° N, 16.5° W)), at an altitude of 2400 m a.s.l. (Fig. <xref ref-type="fig" rid="F1"/>a), and is typically situated above a quasi-permanent temperature inversion layer. This persistent atmospheric feature limits the vertical transport of locally generated pollutants from lower altitudes, ensuring that the measurements collected at the site are mostly representative of free-tropospheric conditions <xref ref-type="bibr" rid="bib1.bibx13" id="paren.16"/>. Consequently, IZO offers an exceptional environment for both in situ and remote sensing observations of trace gases and aerosols. The combination of a stable total ozone column, extremely low water vapour content, reduced aerosol loading, and the frequent occurrence of clean, cloud-free skies makes the observatory an ideal reference site for calibration and validation activities (more details in <xref ref-type="bibr" rid="bib1.bibx17" id="altparen.17"/>).</p>

      <fig id="F1" specific-use="star"><label>Figure 1</label><caption><p id="d2e464"><bold>(a, b)</bold> Copernicus Sentinel-2 image acquired on 18 August over Tenerife. The red dot marks the location of the Izaña Observatory (Canary Islands, Spain). <bold>(c, d)</bold> Images of Teide National Park captured on 17 and 18 August 2023 from Izaña Observatory  (Teide Cloud Laboratory Project, project from Izaña Observatory by Daniel López).</p></caption>
          <graphic xlink:href="https://amt.copernicus.org/articles/19/3151/2026/amt-19-3151-2026-f01.jpg"/>

        </fig>

</sec>
<sec id="Ch1.S2.SS2">
  <label>2.2</label><title>Instruments</title>
<sec id="Ch1.S2.SS2.SSS1">
  <label>2.2.1</label><title>EKO RSB spectroradiometer</title>
      <p id="d2e493">In this study, global (GHI<sub><italic>λ</italic></sub>), direct-normal (DNI<sub><italic>λ</italic></sub>), and diffuse (DHI<sub><italic>λ</italic></sub>) spectral irradiance were measured using an EKO MS-711 spectroradiometer equipped with a rotating shadow band (hereafter EKO RSB; Fig. <xref ref-type="fig" rid="F2"/>a). The instrument operates over the 300–1100 nm range, with a spectral step of approximately 0.4 nm and a nominal full width at half maximum (FWHM) of less than 7 nm. It acquires one spectrum per minute, with exposure times automatically adjusted between 10 ms and 5 s according to irradiance levels and sky conditions. Each measurement cycle consists of four sequential acquisitions at different shadow band positions (Fig. <xref ref-type="fig" rid="F2"/>b), completed in less than one minute <xref ref-type="bibr" rid="bib1.bibx54 bib1.bibx60" id="paren.18"/>. Thus, at the 1st position the shadow band rests outside the instrument's field of view (FOV);  at the 2nd position the shadow band stops at <inline-formula><mml:math id="M17" display="inline"><mml:mrow><mml:mi mathvariant="normal">−</mml:mi><mml:mn mathvariant="normal">5</mml:mn><mml:mi mathvariant="italic">°</mml:mi></mml:mrow></mml:math></inline-formula> from the solar disk; at the 3rd position the EKO RSB covers the solar disk to perform the diffuse measurement and finally at the 4th position the shadow band stops at <inline-formula><mml:math id="M18" display="inline"><mml:mrow><mml:mo>+</mml:mo><mml:mn mathvariant="normal">5</mml:mn><mml:mi mathvariant="italic">°</mml:mi></mml:mrow></mml:math></inline-formula> beyond the solar disk. The spectral GHI<sub><italic>λ</italic></sub> and DHI<sub><italic>λ</italic></sub> irradiances are measured in the 1st and 3rd positions, respectively. From these two measurements, the DNI<sub><italic>λ</italic></sub> spectral irradiance is derived as follows:

              <disp-formula id="Ch1.E1" content-type="numbered"><label>1</label><mml:math id="M22" display="block"><mml:mrow><mml:msub><mml:mi mathvariant="normal">DNI</mml:mi><mml:mi mathvariant="italic">λ</mml:mi></mml:msub><mml:mo>=</mml:mo><mml:mstyle displaystyle="true"><mml:mfrac style="display"><mml:mrow><mml:mo>(</mml:mo><mml:msub><mml:mi mathvariant="normal">GHI</mml:mi><mml:mi mathvariant="italic">λ</mml:mi></mml:msub><mml:mo>-</mml:mo><mml:msub><mml:mi mathvariant="normal">DHI</mml:mi><mml:mi mathvariant="italic">λ</mml:mi></mml:msub><mml:mo>)</mml:mo></mml:mrow><mml:mrow><mml:mi>cos⁡</mml:mi><mml:mo>(</mml:mo><mml:mi mathvariant="normal">SZA</mml:mi><mml:mo>)</mml:mo></mml:mrow></mml:mfrac></mml:mstyle></mml:mrow></mml:math></disp-formula>

            where SZA is the solar zenith angle. The 2nd (IRR<sub>2<italic>λ</italic></sub>) and 4th (IRR<sub>4<italic>λ</italic></sub>) positions are used to estimate the amount of diffuse irradiance lost due to the EKO RSB's partial obstruction of the sky, and a correction is applied to DHI<sub><italic>λ</italic></sub> as follows:

              <disp-formula id="Ch1.E2" content-type="numbered"><label>2</label><mml:math id="M26" display="block"><mml:mrow><mml:msub><mml:mi mathvariant="normal">DHI</mml:mi><mml:mrow><mml:mi mathvariant="italic">λ</mml:mi><mml:mi mathvariant="normal">corr</mml:mi></mml:mrow></mml:msub><mml:mo>=</mml:mo><mml:msub><mml:mi mathvariant="normal">DHI</mml:mi><mml:mi mathvariant="italic">λ</mml:mi></mml:msub><mml:mo>+</mml:mo><mml:mfenced close=")" open="("><mml:mrow><mml:msub><mml:mi mathvariant="normal">GHI</mml:mi><mml:mi mathvariant="italic">λ</mml:mi></mml:msub><mml:mo>-</mml:mo><mml:mstyle displaystyle="true"><mml:mfrac style="display"><mml:mrow><mml:msub><mml:mi mathvariant="normal">IRR</mml:mi><mml:mrow><mml:mn mathvariant="normal">2</mml:mn><mml:mi mathvariant="italic">λ</mml:mi></mml:mrow></mml:msub><mml:mo>+</mml:mo><mml:msub><mml:mi mathvariant="normal">IRR</mml:mi><mml:mrow><mml:mn mathvariant="normal">4</mml:mn><mml:mi mathvariant="italic">λ</mml:mi></mml:mrow></mml:msub></mml:mrow><mml:mn mathvariant="normal">2</mml:mn></mml:mfrac></mml:mstyle></mml:mrow></mml:mfenced></mml:mrow></mml:math></disp-formula></p>

      <fig id="F2"><label>Figure 2</label><caption><p id="d2e713"><bold>(a)</bold> The EKO RSB grating spectroradiometer installed at Izaña station. <bold>(b)</bold> EKO RSB band sweeping positions (Figure adapted from <xref ref-type="bibr" rid="bib1.bibx54" id="altparen.19"/>).</p></caption>
            <graphic xlink:href="https://amt.copernicus.org/articles/19/3151/2026/amt-19-3151-2026-f02.png"/>

          </fig>

</sec>
</sec>
<sec id="Ch1.S2.SS3">
  <label>2.3</label><title>Ancillary instruments</title>
<sec id="Ch1.S2.SS3.SSS1">
  <label>2.3.1</label><title>AERONET Cimel Sun Photometer</title>
      <p id="d2e746">The aerosol columnar optical properties (aerosol optical depth (AOD), Ångström Exponent (AE), and fine/coarse AOD) used in this study were obtained from measurements performed with a Cimel CE318-T sun–sky–lunar photometer, the reference instrument of the AErosol RObotic NETwork (AERONET), a global federated network established in 1993 for the long-term monitoring and characterization of atmospheric aerosols <xref ref-type="bibr" rid="bib1.bibx36 bib1.bibx49 bib1.bibx50 bib1.bibx6 bib1.bibx30" id="paren.20"/>. This instrument is an automatic scanning filter radiometer operating at nine nominal wavelengths (340, 380, 440, 500, 675, 870, 937, 1020, and 1640 nm), with a FOV of 1.3° <xref ref-type="bibr" rid="bib1.bibx36 bib1.bibx62" id="paren.21"/> and a FWHM of 10 nm, except for 340, 380, and 1640 nm, which have bandwidths of 2, 4, and 25 nm, respectively. Izaña Observatory is an AERONET calibration site for reference instruments <xref ref-type="bibr" rid="bib1.bibx61" id="paren.22"/>.</p>
      <p id="d2e758">In this study, Level 2.0 AERONET direct-sun products (AOD, AE, and fine/coarse AOD) were used to retrieve aerosol properties for 17 August. However, for 18 August, Level 1.0 AOD data were employed because the extreme intensity of the event caused most photometric measurements to be misclassified as cloudy by the AERONET quality-control algorithms, as previously reported for the February 2020 desert dust outbreak <xref ref-type="bibr" rid="bib1.bibx15" id="paren.23"/>. To ensure retrievals under clear-sky conditions, only measurements identified as clear sky by the procedure of <xref ref-type="bibr" rid="bib1.bibx42" id="text.24"/>, as adapted for Izaña by <xref ref-type="bibr" rid="bib1.bibx26" id="text.25"/>, were considered. Furthermore, inversion products (such as single scattering albedo and asymmetry parameter) were not used because the available data were insufficient for this study.</p>
</sec>
<sec id="Ch1.S2.SS3.SSS2">
  <label>2.3.2</label><title>Micro-Pulse Lidar</title>
      <p id="d2e778">Relative attenuated backscatter profiles and volume depolarization ratios were measured with a Micro-Pulse Lidar (MPL, model MPL-4B) operating at IZO during the forest fire outbreak at the station. This type of lidar is an eye-safe elastic lidar operating continuously (24/7) at 532 nm with a low-pulse energy laser (5–6 <inline-formula><mml:math id="M27" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">µ</mml:mi></mml:mrow></mml:math></inline-formula>J) and a repetition rate of 2.5 kHz <xref ref-type="bibr" rid="bib1.bibx65 bib1.bibx9" id="paren.26"/>. The MPL-4B version features depolarization capability, which is useful for identifying depolarizing particles <xref ref-type="bibr" rid="bib1.bibx24" id="paren.27"/>. As the reference instrument of the National Aeronautics and Space Administration Micro-Pulse Lidar Network (NASA-MPLNet), signal processing and retrieval products are centralised at the network level <xref ref-type="bibr" rid="bib1.bibx64" id="paren.28"/>. According to <xref ref-type="bibr" rid="bib1.bibx9" id="text.29"/> and <xref ref-type="bibr" rid="bib1.bibx64" id="text.30"/>, this processing includes corrections for detector deadtime and dark current, laser–detector after-pulse, overlap, and polarization calibrations. MPLNet Version 3, Level 1.5 aerosol products were used in this study.</p>
</sec>
<sec id="Ch1.S2.SS3.SSS3">
  <label>2.3.3</label><title>TEOM</title>
      <p id="d2e813">Surface measurements of bulk mass concentrations were measured using the TEOM 1405-DF instrument (Thermo Fisher Scientific™). This instrument operates by collecting particles onto a vibrating substrate maintained at constant amplitude. As particles accumulate on the filter, the increasing mass causes a decrease in the vibration frequency. The total particle concentration (PM, Particulate Matter) is then calculated from this frequency change as a function of aerosol mass accumulation over time <xref ref-type="bibr" rid="bib1.bibx51" id="paren.31"/>.</p>
      <p id="d2e819">The TEOM 1405-DF measures the coarse PM and PM<sub>2.5</sub> fractions of PM<sub>10</sub>, which are separated by a virtual impactor and collected on two dedicated filters. PM<sub>10</sub> concentration is obtained by summing the PM<sub>2.5</sub> and coarse PM fractions. The instrument has a resolution of approximately <inline-formula><mml:math id="M32" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> 5 <inline-formula><mml:math id="M33" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">µ</mml:mi></mml:mrow></mml:math></inline-formula>g m<sup>−3</sup> for 10 min sampling intervals <xref ref-type="bibr" rid="bib1.bibx56" id="paren.32"/>.</p>
</sec>
<sec id="Ch1.S2.SS3.SSS4">
  <label>2.3.4</label><title>MAAP</title>
      <p id="d2e897">Surface Equivalent Black Carbon (eBC) mass concentrations were obtained from two Multi-Angle Absorption Photometer instruments (MAAP; Thermo™) with separated sampling lines for PM<sub>10</sub> and PM<sub>1</sub> using virtual impactors. MAAP instruments measure the change in transmittance of a 637 nm light source through a filter tape as particles are deposited. Additionally, the instrument measures backscattered light from the sample and filters using two detectors positioned at different angles. This configuration enables determination of the absorption of the aerosol sample through a radiative transfer scheme with a relative uncertainty of <inline-formula><mml:math id="M37" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> 12 % <xref ref-type="bibr" rid="bib1.bibx52" id="paren.33"/>. The measured absorption is then converted to eBC mass concentration using a mass absorption cross-section of 6.6 m<sup>2</sup> g<sup>−1</sup>, defined in the instrument firmware following ACTRIS guidelines <xref ref-type="bibr" rid="bib1.bibx46 bib1.bibx53" id="paren.34"/>. </p>
</sec>
<sec id="Ch1.S2.SS3.SSS5">
  <label>2.3.5</label><title>Integrating Nephelometer</title>
      <p id="d2e963">Surface total scattering coefficient data (<inline-formula><mml:math id="M40" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="italic">σ</mml:mi><mml:mi mathvariant="normal">scat</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> (<inline-formula><mml:math id="M41" display="inline"><mml:mi mathvariant="italic">λ</mml:mi></mml:math></inline-formula>)) were collected with a TSI™ integrating nephelometer (model 3563) at three wavelengths (450, 550, and 700 nm). From that, the Scattering Ångström Exponent (SAE; <xref ref-type="bibr" rid="bib1.bibx5" id="altparen.35"/>) was calculated using the 450 (<inline-formula><mml:math id="M42" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="italic">λ</mml:mi><mml:mn mathvariant="normal">1</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>) nm and 700  (<inline-formula><mml:math id="M43" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="italic">λ</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>) nm total scattering values according to the following relation:

              <disp-formula id="Ch1.E3" content-type="numbered"><label>3</label><mml:math id="M44" display="block"><mml:mrow><mml:mi mathvariant="normal">SAE</mml:mi><mml:mo>=</mml:mo><mml:mo>-</mml:mo><mml:mstyle displaystyle="true"><mml:mfrac style="display"><mml:mrow><mml:mi>ln⁡</mml:mi><mml:mo>(</mml:mo><mml:msub><mml:mi mathvariant="italic">σ</mml:mi><mml:mi mathvariant="normal">scat</mml:mi></mml:msub><mml:mo>(</mml:mo><mml:msub><mml:mi mathvariant="italic">λ</mml:mi><mml:mn mathvariant="normal">1</mml:mn></mml:msub><mml:mo>)</mml:mo><mml:mo>/</mml:mo><mml:msub><mml:mi mathvariant="italic">σ</mml:mi><mml:mi mathvariant="normal">scat</mml:mi></mml:msub><mml:mo>(</mml:mo><mml:msub><mml:mi mathvariant="italic">λ</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub><mml:mo>)</mml:mo><mml:mo>)</mml:mo></mml:mrow><mml:mrow><mml:mi>ln⁡</mml:mi><mml:mo>(</mml:mo><mml:msub><mml:mi mathvariant="italic">λ</mml:mi><mml:mn mathvariant="normal">1</mml:mn></mml:msub><mml:mo>/</mml:mo><mml:msub><mml:mi mathvariant="italic">λ</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub><mml:mo>)</mml:mo></mml:mrow></mml:mfrac></mml:mstyle></mml:mrow></mml:math></disp-formula>

            The instrument is calibrated annually using CO<sub>2</sub> as the high span gas and filtered air as the low span gas. The averaging time is set to 1 min, and the instrument performs routine 5 min zero checks every hour. Additional corrections for truncation and non-Lambertian illumination were applied to the data following the method described by <xref ref-type="bibr" rid="bib1.bibx4" id="text.36"/>, which gives a reported uncertainty of approximately 7 % for scattering values <xref ref-type="bibr" rid="bib1.bibx35" id="paren.37"/>. Sampling is performed through an inlet assembly with a PM<sub>10</sub> virtual impactor.</p>
      <p id="d2e1105">The Single Scattering Albedo (SSA; <inline-formula><mml:math id="M47" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="italic">ω</mml:mi><mml:mn mathvariant="normal">0</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>) was calculated following <xref ref-type="bibr" rid="bib1.bibx63" id="text.38"/>, by combining the total scattering coefficient (<inline-formula><mml:math id="M48" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="italic">σ</mml:mi><mml:mi mathvariant="normal">scat</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> (<inline-formula><mml:math id="M49" display="inline"><mml:mi mathvariant="italic">λ</mml:mi></mml:math></inline-formula>)) from the nephelometer and the absorption coefficient (<inline-formula><mml:math id="M50" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="italic">σ</mml:mi><mml:mi mathvariant="normal">abs</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> (<inline-formula><mml:math id="M51" display="inline"><mml:mi mathvariant="italic">λ</mml:mi></mml:math></inline-formula>)) derived from the MAAP measurements. The absorption coefficient was obtained by multiplying the eBC mass concentration by the mass absorption cross-section of 6.6 m<sup>2</sup> g<sup>−1</sup>, with a correction factor of 1.05 applied to account for the shift in the MAAP light source wavelength <xref ref-type="bibr" rid="bib1.bibx46" id="paren.39"/>. SSA was then computed at 637 nm using:

              <disp-formula id="Ch1.E4" content-type="numbered"><label>4</label><mml:math id="M54" display="block"><mml:mrow><mml:msub><mml:mi mathvariant="italic">ω</mml:mi><mml:mn mathvariant="normal">0</mml:mn></mml:msub><mml:mo>(</mml:mo><mml:mi mathvariant="italic">λ</mml:mi><mml:mo>)</mml:mo><mml:mo>=</mml:mo><mml:mstyle displaystyle="true"><mml:mfrac style="display"><mml:mrow><mml:msub><mml:mi mathvariant="italic">σ</mml:mi><mml:mi mathvariant="normal">scat</mml:mi></mml:msub><mml:mo>(</mml:mo><mml:mi mathvariant="italic">λ</mml:mi><mml:mo>)</mml:mo></mml:mrow><mml:mrow><mml:msub><mml:mi mathvariant="italic">σ</mml:mi><mml:mi mathvariant="normal">scat</mml:mi></mml:msub><mml:mo>(</mml:mo><mml:mi mathvariant="italic">λ</mml:mi><mml:mo>)</mml:mo><mml:mo>+</mml:mo><mml:msub><mml:mi mathvariant="italic">σ</mml:mi><mml:mi mathvariant="normal">abs</mml:mi></mml:msub><mml:mo>(</mml:mo><mml:mi mathvariant="italic">λ</mml:mi><mml:mo>)</mml:mo></mml:mrow></mml:mfrac></mml:mstyle></mml:mrow></mml:math></disp-formula>

            where <inline-formula><mml:math id="M55" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="italic">σ</mml:mi><mml:mi mathvariant="normal">scat</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> (<inline-formula><mml:math id="M56" display="inline"><mml:mi mathvariant="italic">λ</mml:mi></mml:math></inline-formula>) was interpolated to 637 nm from the nephelometer measurements using the SAE, in order to match the MAAP absorption wavelength.</p>
      <p id="d2e1260">All in situ aerosol measurements were conducted in the same laboratory, under controlled environmental conditions, with ambient temperature maintained at 21 <inline-formula><mml:math id="M57" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> 2 °C. Data points were subsequently filtered to exclude measurements recorded at relative humidity above 40 % to ensure dry sampling conditions.</p>
</sec>
<sec id="Ch1.S2.SS3.SSS6">
  <label>2.3.6</label><title>Picarro Cavity Ring-Down Spectrometer</title>
      <p id="d2e1278">Dry-air mole fractions of CO<sub>2</sub>, CH<sub>4</sub>, and CO were measured using a Picarro G2401 analyser based on cavity ring-down spectroscopy <xref ref-type="bibr" rid="bib1.bibx12" id="paren.40"/>. The analyser operates continuously at IZO under the WMO-GAW programme <xref ref-type="bibr" rid="bib1.bibx17" id="paren.41"/> and is calibrated monthly using four multi-species tertiary standards prepared by the WMO Central Calibration Laboratory (<uri>https://gml.noaa.gov/ccl/</uri>, last access: 25 November 2025). Measurements are reported on the following WMO scales: X2019 for CO<sub>2</sub>, X2004A for CH<sub>4</sub> and X2014A for CO. The system provides high-precision measurements with typical 1σ uncertainties for 1 min averages of 0.013 ppm (CO<sub>2</sub>), 0.19 ppb (CH<sub>4</sub>), and 0.87 ppb (CO) when analysing calibration tanks <xref ref-type="bibr" rid="bib1.bibx33" id="paren.42"/>.</p>
      <p id="d2e1348">Ambient air is sampled from the roof of the IZO building and passed through a cold trap at <inline-formula><mml:math id="M64" display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">70</mml:mn></mml:mrow></mml:math></inline-formula> °C to remove water vapour and ensure dry-air conditions. The instrument acquires data every 2 s, but in this study we used 1 min averaged values. Further details on the calibration procedure and instrument characterisation can be found in <xref ref-type="bibr" rid="bib1.bibx33" id="text.43"/>.</p>
</sec>
</sec>
</sec>
<sec id="Ch1.S3">
  <label>3</label><title>Methodology:  Spectral radiative forcing and efficiency</title>
      <p id="d2e1374">To quantify changes in the energy budget of the Earth–atmosphere system, the concept of radiative forcing (<inline-formula><mml:math id="M65" display="inline"><mml:mrow><mml:mi mathvariant="normal">Δ</mml:mi><mml:mi>F</mml:mi></mml:mrow></mml:math></inline-formula>) is introduced as an indicator of these changes <xref ref-type="bibr" rid="bib1.bibx38" id="paren.44"/>. In this study, we focus on the aerosol effect, particularly that associated with biomass burning. The radiative forcing (<inline-formula><mml:math id="M66" display="inline"><mml:mrow><mml:mi mathvariant="normal">Δ</mml:mi><mml:mi>F</mml:mi></mml:mrow></mml:math></inline-formula>) is defined as follows, considering its dependence on wavelength and solar zenith angle:

          <disp-formula id="Ch1.E5" content-type="numbered"><label>5</label><mml:math id="M67" display="block"><mml:mrow><mml:mi mathvariant="normal">Δ</mml:mi><mml:mi>F</mml:mi><mml:mo>(</mml:mo><mml:mi mathvariant="italic">λ</mml:mi><mml:mo>,</mml:mo><mml:mi mathvariant="normal">SZA</mml:mi><mml:mo>)</mml:mo><mml:mo>=</mml:mo><mml:msup><mml:mi>F</mml:mi><mml:mrow><mml:mo>↓</mml:mo><mml:mi>A</mml:mi></mml:mrow></mml:msup><mml:mo>(</mml:mo><mml:mi mathvariant="italic">λ</mml:mi><mml:mo>,</mml:mo><mml:mi mathvariant="normal">SZA</mml:mi><mml:mo>)</mml:mo><mml:mo>-</mml:mo><mml:msup><mml:mi>F</mml:mi><mml:mrow><mml:mo>↓</mml:mo><mml:mi>C</mml:mi></mml:mrow></mml:msup><mml:mo>(</mml:mo><mml:mi mathvariant="italic">λ</mml:mi><mml:mo>,</mml:mo><mml:mi mathvariant="normal">SZA</mml:mi><mml:mo>)</mml:mo></mml:mrow></mml:math></disp-formula>

        In this equation, <inline-formula><mml:math id="M68" display="inline"><mml:mrow><mml:mi>F</mml:mi><mml:msup><mml:mo>↓</mml:mo><mml:mi>A</mml:mi></mml:msup></mml:mrow></mml:math></inline-formula> represents the downward irradiance at the surface in the presence of atmospheric aerosols, while <inline-formula><mml:math id="M69" display="inline"><mml:mrow><mml:mi>F</mml:mi><mml:msup><mml:mo>↓</mml:mo><mml:mi>C</mml:mi></mml:msup></mml:mrow></mml:math></inline-formula> corresponds to the irradiance expected under clean or pristine atmospheric conditions, obtained from radiative transfer simulations. Under this sign convention, negative values of <inline-formula><mml:math id="M70" display="inline"><mml:mrow><mml:mi mathvariant="normal">Δ</mml:mi><mml:mi>F</mml:mi><mml:mo>(</mml:mo><mml:mi mathvariant="italic">λ</mml:mi></mml:mrow></mml:math></inline-formula>,SZA) indicate a cooling influence of aerosols at the surface, whereas positive values denote a warming effect.</p>
      <p id="d2e1502">After computing <inline-formula><mml:math id="M71" display="inline"><mml:mrow><mml:mi mathvariant="normal">Δ</mml:mi><mml:mi>F</mml:mi><mml:mo>(</mml:mo><mml:mi mathvariant="italic">λ</mml:mi></mml:mrow></mml:math></inline-formula>,SZA), the spectral aerosol radiative forcing efficiency, <inline-formula><mml:math id="M72" display="inline"><mml:mrow><mml:mi mathvariant="normal">Δ</mml:mi><mml:msup><mml:mi>F</mml:mi><mml:mi mathvariant="normal">eff</mml:mi></mml:msup></mml:mrow></mml:math></inline-formula>(<inline-formula><mml:math id="M73" display="inline"><mml:mi mathvariant="italic">λ</mml:mi></mml:math></inline-formula>,SZA), can be defined as:

          <disp-formula id="Ch1.E6" content-type="numbered"><label>6</label><mml:math id="M74" display="block"><mml:mrow><mml:mi mathvariant="normal">Δ</mml:mi><mml:msup><mml:mi>F</mml:mi><mml:mi mathvariant="normal">eff</mml:mi></mml:msup><mml:mo>(</mml:mo><mml:mi mathvariant="italic">λ</mml:mi><mml:mo>,</mml:mo><mml:mi mathvariant="normal">SZA</mml:mi><mml:mo>)</mml:mo><mml:mo>=</mml:mo><mml:mstyle displaystyle="true"><mml:mfrac style="display"><mml:mrow><mml:mi mathvariant="normal">Δ</mml:mi><mml:mi>F</mml:mi><mml:mo>(</mml:mo><mml:mi mathvariant="italic">λ</mml:mi><mml:mo>,</mml:mo><mml:mi mathvariant="normal">SZA</mml:mi><mml:mo>)</mml:mo></mml:mrow><mml:mrow><mml:mi mathvariant="normal">AOD</mml:mi><mml:mo>(</mml:mo><mml:mi mathvariant="italic">λ</mml:mi><mml:mo>,</mml:mo><mml:mi mathvariant="normal">SZA</mml:mi><mml:mo>)</mml:mo></mml:mrow></mml:mfrac></mml:mstyle></mml:mrow></mml:math></disp-formula>

        where AOD(<inline-formula><mml:math id="M75" display="inline"><mml:mi mathvariant="italic">λ</mml:mi></mml:math></inline-formula>,SZA) represents the aerosol optical depth at the specified wavelength and solar zenith angle, which in this case was obtained from direct-normal spectral irradiance measurements (DNI<sub><italic>λ</italic></sub>) recorded by the EKO RSB following the methodology described in <xref ref-type="bibr" rid="bib1.bibx28" id="text.45"/>.</p>

      <fig id="F3" specific-use="star"><label>Figure 3</label><caption><p id="d2e1616">Time series of AOD at different wavelengths (left axis: 340 nm, black dots; 380 nm, magenta dots; 440 nm, blue dots; 500 nm, green dots; 675 nm, violet dots; and 870 nm, orange dots) and AE (440–870 nm) (right axis, red stars) during August 2023 at IZO. The red dashed lines and green area indicate the thresholds defined for biomass-burning conditions (AE <inline-formula><mml:math id="M77" display="inline"><mml:mrow><mml:mo>&gt;</mml:mo><mml:mn mathvariant="normal">1.5</mml:mn></mml:mrow></mml:math></inline-formula>). The data are from the AERONET network, filled symbols correspond to Version 2.0 data, while open symbols represent Version 1.0 data.</p></caption>
        <graphic xlink:href="https://amt.copernicus.org/articles/19/3151/2026/amt-19-3151-2026-f03.png"/>

      </fig>

      <p id="d2e1636">To estimate <inline-formula><mml:math id="M78" display="inline"><mml:mrow><mml:msup><mml:mi>F</mml:mi><mml:mrow><mml:mo>↓</mml:mo><mml:mi>C</mml:mi></mml:mrow></mml:msup></mml:mrow></mml:math></inline-formula>(<inline-formula><mml:math id="M79" display="inline"><mml:mi mathvariant="italic">λ</mml:mi></mml:math></inline-formula>,SZA), the libRadtran radiative transfer model was used <xref ref-type="bibr" rid="bib1.bibx44 bib1.bibx22" id="paren.46"/>. This model has been extensively tested at the Izaña Observatory (e.g. <xref ref-type="bibr" rid="bib1.bibx26 bib1.bibx27 bib1.bibx28" id="altparen.47"/>). The radiative transfer equation (RTE) solver employed was the DIScrete Ordinates Radiative Transfer (DISORT) algorithm <xref ref-type="bibr" rid="bib1.bibx59" id="paren.48"/>, which is based on a multi-stream discrete ordinates method using 16 streams. Corrections for Earth's sphericity were applied for SZA greater than 70° <xref ref-type="bibr" rid="bib1.bibx19" id="paren.49"/>. For each simulation, the GHI<sub><italic>λ</italic></sub>, DNI<sub><italic>λ</italic></sub> and DHI<sub><italic>λ</italic></sub> spectral irradiances were computed in the 300–1100 nm range with a 1 nm spectral step <xref ref-type="bibr" rid="bib1.bibx29 bib1.bibx8" id="paren.50"/>.</p>
      <p id="d2e1703">The forcing (<inline-formula><mml:math id="M83" display="inline"><mml:mi mathvariant="normal">Δ</mml:mi></mml:math></inline-formula>DF) and radiative forcing efficiency (<inline-formula><mml:math id="M84" display="inline"><mml:mi mathvariant="normal">Δ</mml:mi></mml:math></inline-formula>DF<sup>eff</sup>) in different spectral ranges have been determined from the following equation:

          <disp-formula id="Ch1.E7" content-type="numbered"><label>7</label><mml:math id="M86" display="block"><mml:mrow><mml:mi mathvariant="normal">Δ</mml:mi><mml:mi mathvariant="normal">DF</mml:mi><mml:mo>=</mml:mo><mml:munderover><mml:mo movablelimits="false">∫</mml:mo><mml:mrow><mml:msub><mml:mi mathvariant="italic">λ</mml:mi><mml:mn mathvariant="normal">1</mml:mn></mml:msub></mml:mrow><mml:mrow><mml:msub><mml:mi mathvariant="italic">λ</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:munderover><mml:mi mathvariant="normal">Δ</mml:mi><mml:mi>F</mml:mi><mml:mo>(</mml:mo><mml:mi mathvariant="italic">λ</mml:mi><mml:mo>,</mml:mo><mml:mi mathvariant="normal">SZA</mml:mi><mml:mo>)</mml:mo><mml:mo>⋅</mml:mo><mml:mi mathvariant="normal">d</mml:mi><mml:mi mathvariant="italic">λ</mml:mi></mml:mrow></mml:math></disp-formula></p>
</sec>
<sec id="Ch1.S4">
  <label>4</label><title>Results</title>
<sec id="Ch1.S4.SS1">
  <label>4.1</label><title>Description of the event</title>
      <p id="d2e1791">In August 2023, an extensive wildfire on the island of Tenerife provided a unique natural laboratory for investigating the atmospheric effects of biomass-burning aerosols. Although IZO remained physically unaffected by the fire, its proximity to the burning area offered an exceptional opportunity to monitor the resulting smoke plume and examine its evolution under free-tropospheric conditions. This situation enabled the direct characterisation of the optical, microphysical and radiative properties of wildfire-derived aerosols, thus yielding valuable insight into their short-term influence on the regional radiation budget and atmospheric composition.</p>
      <p id="d2e1794">Climatic conditions in the Canary Islands during August 2023 created a highly favourable environment for wildfire development. According to AEMET <xref ref-type="bibr" rid="bib1.bibx2" id="paren.51"/>, this month was exceptionally dry, with a mean temperature of 25.4 °C and a positive anomaly of <inline-formula><mml:math id="M87" display="inline"><mml:mrow><mml:mo>+</mml:mo><mml:mn mathvariant="normal">2.3</mml:mn></mml:mrow></mml:math></inline-formula> °C compared to the 1991–2020 reference period, ranking as the warmest August since 1961. A heatwave between 10 and 14 August <xref ref-type="bibr" rid="bib1.bibx1" id="paren.52"/> pushed temperatures close to 40 °C, while relative humidity fell below 20 % and wind gusts exceeded 30 km h<sup>−1</sup> in Tenerife, as recorded at the AEMET station in Candelaria (463 m a.s.l.), near to the origin point of the subsequent wildfire. Although the fire ignited one day after the maximum alert had been lifted-coinciding with notably milder conditions (27.3 °C maximum temperature; 75 % minimum humidity, <xref ref-type="bibr" rid="bib1.bibx11" id="altparen.53"/>), the severe desiccation of the forest fuel over prior weeks was decisive in enabling its rapid spread. Supporting this, the base of the subsidence-induced thermal inversion remained below 600 m a.s.l. from 11 to 19 August, maintaining a warm and dry free troposphere above the island <xref ref-type="bibr" rid="bib1.bibx10 bib1.bibx11" id="paren.54"/>.</p>
      <p id="d2e1832">During the period 15–31 August 2023, a pronounced aerosol episode was detected at IZO on 17 and 18 August (Figs. <xref ref-type="fig" rid="F1"/> c, d and <xref ref-type="fig" rid="F3"/>). The AOD values increased sharply across all measured wavelengths (340–870 nm), reaching maxima of 4.81 and 3.63 at 340 and 500 nm, respectively, on 17 August, and 4.10 and 2.25 at 340 and 500 nm, respectively, on 18 August. Simultaneously, AE <inline-formula><mml:math id="M89" display="inline"><mml:mrow><mml:mo>&gt;</mml:mo><mml:mn mathvariant="normal">2</mml:mn></mml:mrow></mml:math></inline-formula> on both days (2.06 on 17 August and 2.04 on 18 August) (see Table <xref ref-type="table" rid="T1"/>), indicating a predominance of fine-mode particles. These features are characteristic of biomass-burning aerosol intrusions and are comparable to those reported by <xref ref-type="bibr" rid="bib1.bibx43" id="text.55"/> during the extreme wildfire episode in Greece in August 2021, where AOD values up to 3.6 at 500 nm, AE up to 2.4 (440–870 nm), and fine-mode fractio (FMF) values around 0.98 were observed. Therefore, the following study focuses on the events recorded on 17 and 18 August.</p>

<table-wrap id="T1" specific-use="star"><label>Table 1</label><caption><p id="d2e1858">Aerosol optical and microphysical properties corresponding to the maximum of AOD<sub>500 nm</sub> values performed at IZO on 17 and 18 August 2023. Parameters included are: AOD (500 nm), AE (440–870 nm), Total (500 nm), Fine (500 nm), and Coarse-mode (500 nm), fine-mode fraction (FMF, 500 nm), mass concentration of PM<sub>10</sub> (<inline-formula><mml:math id="M92" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">µ</mml:mi></mml:mrow></mml:math></inline-formula>g m<sup>−3</sup>), ratio between  PM<sub>2.5</sub> and PM<sub>10</sub>, and the SAE (450–700 nm).</p></caption><oasis:table frame="topbot"><oasis:tgroup cols="11">
     <oasis:colspec colnum="1" colname="col1" align="left"/>
     <oasis:colspec colnum="2" colname="col2" align="center"/>
     <oasis:colspec colnum="3" colname="col3" align="center"/>
     <oasis:colspec colnum="4" colname="col4" align="center"/>
     <oasis:colspec colnum="5" colname="col5" align="center"/>
     <oasis:colspec colnum="6" colname="col6" align="center"/>
     <oasis:colspec colnum="7" colname="col7" align="center"/>
     <oasis:colspec colnum="8" colname="col8" align="center"/>
     <oasis:colspec colnum="9" colname="col9" align="center"/>
     <oasis:colspec colnum="10" colname="col10" align="center"/>
     <oasis:colspec colnum="11" colname="col11" align="center"/>
     <oasis:thead>
       <oasis:row rowsep="1">
         <oasis:entry colname="col1">Case</oasis:entry>
         <oasis:entry colname="col2">SZA (<inline-formula><mml:math id="M96" display="inline"><mml:mi mathvariant="italic">°</mml:mi></mml:math></inline-formula>)</oasis:entry>
         <oasis:entry colname="col3">AOD</oasis:entry>
         <oasis:entry colname="col4">AE</oasis:entry>
         <oasis:entry colname="col5">Total</oasis:entry>
         <oasis:entry colname="col6">Fine</oasis:entry>
         <oasis:entry colname="col7">Coarse</oasis:entry>
         <oasis:entry colname="col8">FMF</oasis:entry>
         <oasis:entry colname="col9">PM<sub>10</sub></oasis:entry>
         <oasis:entry colname="col10">PM<sub>2.5</sub> <inline-formula><mml:math id="M99" display="inline"><mml:mo>/</mml:mo></mml:math></inline-formula> PM<sub>10</sub></oasis:entry>
         <oasis:entry colname="col11">SAE</oasis:entry>
       </oasis:row>
     </oasis:thead>
     <oasis:tbody>
       <oasis:row>
         <oasis:entry colname="col1">17-08-2023 11:56</oasis:entry>
         <oasis:entry colname="col2">22.7</oasis:entry>
         <oasis:entry colname="col3">3.63</oasis:entry>
         <oasis:entry colname="col4">1.71</oasis:entry>
         <oasis:entry colname="col5">3.61</oasis:entry>
         <oasis:entry colname="col6">3.58</oasis:entry>
         <oasis:entry colname="col7">0.03</oasis:entry>
         <oasis:entry colname="col8">0.99</oasis:entry>
         <oasis:entry colname="col9">393.17</oasis:entry>
         <oasis:entry colname="col10">0.81</oasis:entry>
         <oasis:entry colname="col11">1.78</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">18-08-2023 15:46</oasis:entry>
         <oasis:entry colname="col2">39.1</oasis:entry>
         <oasis:entry colname="col3">2.25</oasis:entry>
         <oasis:entry colname="col4">2.04</oasis:entry>
         <oasis:entry colname="col5">2.24</oasis:entry>
         <oasis:entry colname="col6">2.12</oasis:entry>
         <oasis:entry colname="col7">0.13</oasis:entry>
         <oasis:entry colname="col8">0.94</oasis:entry>
         <oasis:entry colname="col9">91.66</oasis:entry>
         <oasis:entry colname="col10">0.66</oasis:entry>
         <oasis:entry colname="col11">2.14</oasis:entry>
       </oasis:row>
     </oasis:tbody>
   </oasis:tgroup></oasis:table></table-wrap>

      <fig id="F4" specific-use="star"><label>Figure 4</label><caption><p id="d2e2109">Time series of <bold>(a)</bold> AOD at different wavelengths (left axis: 340 nm, black dots; 380 nm, magenta dots; 440 nm, blue dots; 500 nm, green dots; 675 nm, violet dots; and 870 nm, orange dots) and AE (440–870 nm) (right axis, red stars); <bold>(b)</bold> total (black dots), fine-mode (blue triangles), and coarse-mode (green stars) AOD at 500 nm (left axis), together with FMF (right axis, red stars). Grey shaded areas highlight the two most notable fire events. <bold>(c)</bold> Scatterplot of AE versus AOD at 500 nm (filled symbols) and FMF versus AOD at 500 nm (open symbols) between 17 and 19 August 2023. The grey shaded area marks the thresholds defined for biomass-burning conditions (AE <inline-formula><mml:math id="M101" display="inline"><mml:mrow><mml:mo>&gt;</mml:mo><mml:mn mathvariant="normal">1.5</mml:mn></mml:mrow></mml:math></inline-formula> and AOD<inline-formula><mml:math id="M102" display="inline"><mml:mrow><mml:msub><mml:mi/><mml:mrow class="unit"><mml:mn mathvariant="normal">500</mml:mn><mml:mspace linebreak="nobreak" width="0.125em"/><mml:mi mathvariant="normal">nm</mml:mi></mml:mrow></mml:msub><mml:mo>&gt;</mml:mo><mml:mn mathvariant="normal">1.0</mml:mn></mml:mrow></mml:math></inline-formula>). The data are from the AERONET network, Version 3, Level 1.5 for 17 and 19 August, and Level 1.0 for 18 August. <bold>(d)</bold> Temporal evolution of Volume Depolarization Ratio (<inline-formula><mml:math id="M103" display="inline"><mml:mrow><mml:mi mathvariant="italic">δ</mml:mi><mml:mi>v</mml:mi></mml:mrow></mml:math></inline-formula>) measured between 17 and 19 August with MPL-4B Lidar at IZO.</p></caption>
          <graphic xlink:href="https://amt.copernicus.org/articles/19/3151/2026/amt-19-3151-2026-f04.png"/>

        </fig>

      <p id="d2e2169">A more detailed characterisation of the aerosol optical and microphysical properties during this episode is presented in Fig. <xref ref-type="fig" rid="F4"/>. Spectral AOD and AE evolution is presented in Fig. <xref ref-type="fig" rid="F4"/>a. The AOD decomposition at 500 nm during the event (Fig. <xref ref-type="fig" rid="F4"/>b) shows that the fine-mode component dominated the total column, with the FMF approaching unity.  On 17 August, the high AE and FMF values (<inline-formula><mml:math id="M104" display="inline"><mml:mo lspace="0mm">∼</mml:mo></mml:math></inline-formula>1.5 and <inline-formula><mml:math id="M105" display="inline"><mml:mrow><mml:mo>&gt;</mml:mo><mml:mn mathvariant="normal">0.8</mml:mn></mml:mrow></mml:math></inline-formula>, respectively) indicate a fine-mode-dominated aerosol population, typical of freshly emitted smoke. As the event evolved (18–19 August), AE decreased below 0.8 and FMF below 0.4, revealing aerosol mixing with coarse dust particles within the plume. Figure <xref ref-type="fig" rid="F4"/>c confirms this dominance, with data points from 17 and 18 August clustering in the region of high AE (<inline-formula><mml:math id="M106" display="inline"><mml:mrow><mml:mo>&gt;</mml:mo><mml:mn mathvariant="normal">1.5</mml:mn></mml:mrow></mml:math></inline-formula>) and high FMF (<inline-formula><mml:math id="M107" display="inline"><mml:mrow><mml:mo>&gt;</mml:mo><mml:mn mathvariant="normal">0.8</mml:mn></mml:mrow></mml:math></inline-formula>) (Fig. <xref ref-type="fig" rid="F4"/>c), indicative of fine-mode aerosols from biomass burning <xref ref-type="bibr" rid="bib1.bibx20 bib1.bibx50" id="paren.56"/>. These values are similar to those reported by <xref ref-type="bibr" rid="bib1.bibx43 bib1.bibx45" id="text.57"/> for the extreme wildfires that occurred in Greece in August 2021 and 2023, respectively, as well as to those reported by <xref ref-type="bibr" rid="bib1.bibx23" id="text.58"/> at the El Arenosillo site in southern Europe as a result of the 2023 Canadian forest fires.</p>

      <fig id="F5" specific-use="star"><label>Figure 5</label><caption><p id="d2e2232">Time series of in situ aerosol measurements at IZO from 17 to 20 August 2023. <bold>(a)</bold> Mass concentrations of PM<sub>10</sub> (black stars), PM<sub>2.5</sub> (blue circles), coarse-mode PM (red triangles) and PM<sub>2.5</sub> <inline-formula><mml:math id="M111" display="inline"><mml:mo>/</mml:mo></mml:math></inline-formula> PM<sub>10</sub> ratio (green dots, right axis). <bold>(b)</bold> Equivalent Black Carbon (eBC) concentrations for PM<sub>10</sub> (blue circles) and PM<sub>1</sub> (red stars) <bold>(c)</bold> SAE (450–700 nm; blue circles) and SSA (at 637 nm; red circles, right axis). Shaded areas indicate the periods corresponding to the maximum AOD values observed on 17 and 18 August.</p></caption>
          <graphic xlink:href="https://amt.copernicus.org/articles/19/3151/2026/amt-19-3151-2026-f05.png"/>

        </fig>

      <p id="d2e2312">The vertical distribution of aerosols derived from lidar observations (Fig. <xref ref-type="fig" rid="F4"/>d) reveals that the fresh smoke layer extended up to 4 km a.s.l. on 17 and 18 August, with enhanced backscatter coefficients (not shown) and low volume depolarization ratios (<inline-formula><mml:math id="M115" display="inline"><mml:mrow><mml:mi mathvariant="italic">δ</mml:mi><mml:mi>v</mml:mi></mml:mrow></mml:math></inline-formula>) of 0.05–0.10 during the most intense fire periods (grey areas in Fig. <xref ref-type="fig" rid="F4"/>). For the 17 August event (no product available for 18 August), <inline-formula><mml:math id="M116" display="inline"><mml:mrow><mml:mi mathvariant="italic">δ</mml:mi><mml:mi>p</mml:mi></mml:mrow></mml:math></inline-formula> values ranged from 0.05 to 0.12. These values are consistent with those reported by <xref ref-type="bibr" rid="bib1.bibx48 bib1.bibx34" id="text.59"/> for fresh smoke, who found <inline-formula><mml:math id="M117" display="inline"><mml:mrow><mml:mi mathvariant="italic">δ</mml:mi><mml:mi>p</mml:mi></mml:mrow></mml:math></inline-formula> values around 0.05. According to these authors, such low <inline-formula><mml:math id="M118" display="inline"><mml:mrow><mml:mi mathvariant="italic">δ</mml:mi><mml:mi>p</mml:mi></mml:mrow></mml:math></inline-formula> values indicate the dominant presence of spherical particles, mainly composed of a solid soot core coated with a liquid sulfate shell <xref ref-type="bibr" rid="bib1.bibx34" id="paren.60"/>.</p>
      <p id="d2e2367">An elevated layer reaching 7–8 km a.s.l. appeared on 19 August, characterised by high <inline-formula><mml:math id="M119" display="inline"><mml:mrow><mml:mi mathvariant="italic">δ</mml:mi><mml:mi>v</mml:mi></mml:mrow></mml:math></inline-formula> and <inline-formula><mml:math id="M120" display="inline"><mml:mrow><mml:mi mathvariant="italic">δ</mml:mi><mml:mi>p</mml:mi></mml:mrow></mml:math></inline-formula> values (up to 0.34 and 0.36, respectively), corresponding to the Saharan dust plume transported to IZO. The influence of coarse mineral dust particles is also consistent with the low AE values observed in Fig. 4a, b, and c. After 19 August, both AOD and backscatter intensity decreased rapidly, marking the end of the episode. These results agree with those reported by <xref ref-type="bibr" rid="bib1.bibx31" id="text.61"/>, who found similar values for both fresh aerosols from the same fire event and for mineral dust measured at Izaña using a dual-wavelength depolarisation elastic lidar (Cimel CE376). This elevated layer reached the altitude of Izaña between 05:00 and 09:00 UTC on 19 August and again after 12:00 UTC on the same day.</p>
      <p id="d2e2393">This local event was also characterised using in situ surface measurements, complementing remote-sensing observations. PM<sub>10</sub> and PM<sub>2.5</sub> concentrations experienced a substantial increase compared to their typical levels. In particular, PM<sub>10</sub> and PM<sub>2.5</sub> (Fig. <xref ref-type="fig" rid="F5"/>a) reached peak concentrations of 712.19 and 594.64 <inline-formula><mml:math id="M125" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">µ</mml:mi></mml:mrow></mml:math></inline-formula>g m<sup>−3</sup>, respectively, representing an increase of approximately 700 <inline-formula><mml:math id="M127" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">µ</mml:mi></mml:mrow></mml:math></inline-formula>g m<sup>−3</sup> above typical values for the station <xref ref-type="bibr" rid="bib1.bibx55" id="paren.62"/>.</p>
      <p id="d2e2478">Five significant peaks were identified in the time series (Fig. <xref ref-type="fig" rid="F5"/>), with one peak excluded from TEOM data (Fig. <xref ref-type="fig" rid="F5"/>a) due to relative humidity filtering (Sect. <xref ref-type="sec" rid="Ch1.S2.SS3"/>). These peaks occurred on three consecutive days: two on 17 August (late morning and afternoon), one on 18 August afternoon, and two on 19 August, one at midnight and the other encompassing from the morning to midday. The peaks on 17 August morning and 18 August afternoon (shaded areas in Fig. <xref ref-type="fig" rid="F5"/>) coincided with fire events identified from columnar properties (Fig. <xref ref-type="fig" rid="F4"/>). The elevated PM<sub>10</sub> and PM<sub>2.5</sub> concentrations within these periods indicate direct impacts from wildfire smoke plumes at the observatory, reaching maximum values of 485.19 and 167.80 <inline-formula><mml:math id="M131" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">µ</mml:mi></mml:mrow></mml:math></inline-formula>g m<sup>−3</sup> for PM<sub>10</sub> and 401.53 and 116.26 <inline-formula><mml:math id="M134" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">µ</mml:mi></mml:mrow></mml:math></inline-formula>g m<sup>−3</sup> for PM<sub>2.5</sub> (17 and 18 August). The eBC concentrations reached record values for the station <xref ref-type="bibr" rid="bib1.bibx31" id="paren.63"/> with peaks of 14.74 and 10.31 <inline-formula><mml:math id="M137" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">µ</mml:mi></mml:mrow></mml:math></inline-formula>g m<sup>−3</sup> for the PM<sub>10</sub> and PM<sub>1</sub> size cuts on 17 August, and 4.69 and 7.81 <inline-formula><mml:math id="M141" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">µ</mml:mi></mml:mrow></mml:math></inline-formula>g m<sup>−3</sup> on 18 August. Correspondingly, the SAE, PM<sub>2.5</sub> <inline-formula><mml:math id="M144" display="inline"><mml:mo>/</mml:mo></mml:math></inline-formula> PM<sub>10</sub> ratio, and SSA, which provide complementary information on aerosol size and optical properties, reached maximum values of 1.93, 0.83, and 0.98 on 17 August, and 2.21, 0.69, and 0.96 on 18 August, respectively. These values collectively confirm the dominance of fine, light-scattering wildfire-originated particles during the selected events.</p>

      <fig id="F6" specific-use="star"><label>Figure 6</label><caption><p id="d2e2658">Time series of 1 min averaged dry-air mole fractions of <bold>(a)</bold> CO<sub>2</sub> (ppm), <bold>(b)</bold> CH<sub>4</sub> (ppb) and <bold>(c)</bold> CO (ppb) from in situ measurements by the Picarro analyser at the Izaña Observatory between 17 and 19 August 2023. <bold>(d)</bold> Satellite CO total column from Copernicus Sentinel-5p TROPOMI over the Canary Islands between 17 and 19 August 2023 (using a 3 d moving average).</p></caption>
          <graphic xlink:href="https://amt.copernicus.org/articles/19/3151/2026/amt-19-3151-2026-f06.png"/>

        </fig>

      <p id="d2e2698">The temporal evolution of ground-level measurements from 17 to 20 August (Fig. <xref ref-type="fig" rid="F5"/>), revealed the successive entrance and exit of smoke-dominated air masses. Their progressive mixing with desert dust was reflected by oscillations in the PM<sub>2.5</sub> <inline-formula><mml:math id="M149" display="inline"><mml:mo>/</mml:mo></mml:math></inline-formula> PM<sub>10</sub> ratio from <inline-formula><mml:math id="M151" display="inline"><mml:mo>∼</mml:mo></mml:math></inline-formula> 0.8 to <inline-formula><mml:math id="M152" display="inline"><mml:mo>∼</mml:mo></mml:math></inline-formula> 0.3, accompanied by a decrease in the SAE from values above 2 to below 0.2. This behaviour was also evident in columnar-integrated measurements on 17 and 18 August. In contrast, the comparison between column-integrated and in situ measurements on 19 August revealed several complications. First, the midnight event could not be measured in the atmospheric column due to the limited availability of lunar photometry data, which is only available between the first and last quarters of the lunar cycle <xref ref-type="bibr" rid="bib1.bibx6" id="paren.64"/>. Second, it is important to emphasise that the detection of short-lived aerosol events may differ between in situ and remote-sensing (column-integrated) techniques because each method samples different atmospheric layers, and local conditions at the station level may not be representative of the column-averaged aerosol load. This discrepancy was evident on 19 August, where the morning event showed fine particles at the surface level, with eBC concentrations peaking at 12.33 and 13.00 <inline-formula><mml:math id="M153" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">µ</mml:mi></mml:mrow></mml:math></inline-formula>g m<sup>−3</sup> in PM<sub>10</sub> and PM<sub>1</sub> fractions, and SAE reaching 2.19 (Fig. <xref ref-type="fig" rid="F5"/>b and c), contrasting with the columnar measurements of FMF and AE (Fig. <xref ref-type="fig" rid="F4"/>a and b), which indicated coarser particles with values below 0.4 and 0.5, respectively. The lidar data (Fig. <xref ref-type="fig" rid="F4"/>d) clarify this discrepancy where low <inline-formula><mml:math id="M157" display="inline"><mml:mrow><mml:mi mathvariant="italic">δ</mml:mi><mml:mi>v</mml:mi></mml:mrow></mml:math></inline-formula> values at altitudes below 3 km a.s.l. revealed a distinct aerosol layer near the surface for both events on 19 August. The consequence of this pronounced aerosol layering above the station is that surface observations detected the arrival of smoke-dominated air masses, whereas column-integrated observations indicated the dominance of coarser desert dust particles.</p>

      <fig id="F7" specific-use="star"><label>Figure 7</label><caption><p id="d2e2804">Spectral global-horizontal (GHI<sub><italic>λ</italic></sub>), direct-normal (DNI<sub><italic>λ</italic></sub>),  and diffuse-horizontal (DHI<sub><italic>λ</italic></sub>) irradiance measured on 17 August <bold>(a, b, c)</bold> and 18 August <bold>(d, e, f)</bold> 2023 between 06:30 and 19:50 UTC (a total of 793 spectra) using the EKO RSB at IZO. The colour bar shows the AOD at 500 nm retrieved from the EKO RSB measurements.</p></caption>
          <graphic xlink:href="https://amt.copernicus.org/articles/19/3151/2026/amt-19-3151-2026-f07.png"/>

        </fig>

      <p id="d2e2846">This local wildfire also had a direct impact on in situ atmospheric concentrations of CO<sub>2</sub>, CH<sub>4</sub>, and CO at IZO, which showed higher-than-usual values between 17 and 19 August (Fig. <xref ref-type="fig" rid="F6"/>). During the event, CO<sub>2</sub>, CH<sub>4</sub>, and CO concentrations increased significantly and reached peaks of approximately 520 ppm, 2800 ppb, and 12 000 ppb, respectively, well above typical values at IZO (410–430 ppm for CO<sub>2</sub>, 1800–2100 ppb for CH<sub>4</sub> and 50–200 ppb for CO). These marked increases (about 25 % for CO<sub>2</sub>, 35 % for CH<sub>4</sub> and nearly two orders of magnitude for CO) are fully consistent with the presence of intense biomass-burning plumes over the observatory during the event, as confirmed by collateral smoke transport identified in Sentinel-5P TROPOMI CO observations (Fig. <xref ref-type="fig" rid="F6"/>d).</p>
      <p id="d2e2926">The temporal evolution of the in situ measurements reveals a strong correspondence between peaks in particulate matter (PM<sub>10</sub>, PM<sub>2.5</sub>), eBC, and greenhouse gases (CO<sub>2</sub>, CH<sub>4</sub>, CO) (Figs. <xref ref-type="fig" rid="F5"/> and <xref ref-type="fig" rid="F6"/>). All maxima occurred concurrently with the periods of highest columnar AOD and strongest backscatter in the lidar profiles. This simultaneity provides robust evidence that the observed perturbations in aerosol and gas concentrations originated from the same wildfire plume. These independent datasets confirm the coherent atmospheric signature of fresh biomass-burning emissions, reinforcing the interpretation of a strongly localised and intense smoke influence at Izaña during the 17–19 August events.</p>
</sec>
<sec id="Ch1.S4.SS2">
  <label>4.2</label><title>Spectral aerosol radiative forcing and efficiency</title>
      <p id="d2e2978">The influence of aerosols on spectral irradiance becomes evident when examining the spectra measured during the two days with the highest AOD (17 and 18 August 2023; Fig. <xref ref-type="fig" rid="F4"/>a). Figure <xref ref-type="fig" rid="F7"/> illustrates the pronounced variability observed in the GHI<sub><italic>λ</italic></sub>, DNI<sub><italic>λ</italic></sub>, and DHI<sub><italic>λ</italic></sub> components, highlighting the impact of these high-turbidity episodes, which lead to substantial spectral attenuation and angular redistribution of solar radiation. During the most intense smoke events, daily GHI<sub><italic>λ</italic></sub> was reduced by 21 %–27 %, DNI<sub><italic>λ</italic></sub> by 72 %–99 %, while DHI<sub><italic>λ</italic></sub> irradiance increased by 72 %–75 % compared with clean-sky conditions at IZO. These results are similar to those observed during the 2021 Greece wildfires, with decreases of 10 %–20 % in daily GHI<sub><italic>λ</italic></sub> <xref ref-type="bibr" rid="bib1.bibx43" id="paren.65"/>.</p>
      <p id="d2e3052">These measurements represent one of the few detailed spectral characterisations (300–1100 nm) of extreme biomass-burning aerosol episodes at a high-altitude observatory. The exceptionally large AOD values observed at IZO (up to 3.6 at 500 nm) place this event among the most intense smoke episodes documented.</p>

      <fig id="F8"><label>Figure 8</label><caption><p id="d2e3057">Spectral irradiance (W m<sup>−2</sup> nm<sup>−1</sup>) <bold>(a, e)</bold>, spectral radiative forcing (W m<sup>−2</sup> nm<sup>−1</sup>) <bold>(b, f)</bold>, spectral AOD obtained from EKO RSB measurements (blue line) and AOD obtained from CIMEL (red stars) <bold>(c, g)</bold>, and spectral radiative forcing efficiency (W m<sup>−2</sup> nm<sup>−1</sup> AOD<sup>−1</sup>) <bold>(d, h)</bold> for selected times corresponding to the two maximum AOD cases during the biomass-burning aerosol episode at IZO on 17 and 18 August 2023, with AOD<sub>500 nm</sub> values of 3.63 and 2.25, respectively. The panels correspond to measurements at 11:56 UTC (SZA <inline-formula><mml:math id="M188" display="inline"><mml:mrow><mml:mo>=</mml:mo><mml:mn mathvariant="normal">22.7</mml:mn><mml:mi mathvariant="italic">°</mml:mi></mml:mrow></mml:math></inline-formula>) on 17 August <bold>(a–d)</bold> and 15:46 UTC (SZA <inline-formula><mml:math id="M189" display="inline"><mml:mrow><mml:mo>=</mml:mo><mml:mn mathvariant="normal">39.1</mml:mn><mml:mi mathvariant="italic">°</mml:mi></mml:mrow></mml:math></inline-formula>) on 18 August <bold>(e–h)</bold>. The sky-camera images show the corresponding sky conditions at each time. Blue, red, and green lines represent global (GHI<sub><italic>λ</italic></sub>) direct-normal (DNI<sub><italic>λ</italic></sub>), and diffuse (DHI<sub><italic>λ</italic></sub>) irradiance components, respectively. The dashed lines in panels <bold>(a)</bold>, <bold>(b)</bold> represent the spectra measured experimentally under clean conditions (6 August 2023 at 11:50 UTC, SZA <inline-formula><mml:math id="M193" display="inline"><mml:mrow><mml:mo>=</mml:mo><mml:mn mathvariant="normal">22.6</mml:mn><mml:mi mathvariant="italic">°</mml:mi></mml:mrow></mml:math></inline-formula>, and 15:55 UTC, SZA <inline-formula><mml:math id="M194" display="inline"><mml:mrow><mml:mo>=</mml:mo><mml:mn mathvariant="normal">39.1</mml:mn><mml:mi mathvariant="italic">°</mml:mi></mml:mrow></mml:math></inline-formula>).</p></caption>
          <graphic xlink:href="https://amt.copernicus.org/articles/19/3151/2026/amt-19-3151-2026-f08.png"/>

        </fig>

      <p id="d2e3266">The spectral radiative effects of biomass-burning aerosols were analysed at the times when the AOD at 500 nm (Fig. <xref ref-type="fig" rid="F4"/>a, c, Table <xref ref-type="table" rid="T1"/>) reached its maximum values on each study day: 11:56 UTC (SZA 22.7°, AOD 3.63) on 17 August and 15:46 UTC (SZA 39.1°, AOD 2.25) on 18 August. Figure <xref ref-type="fig" rid="F8"/> shows the spectral distribution of irradiance, radiative forcing (<inline-formula><mml:math id="M195" display="inline"><mml:mrow><mml:mi mathvariant="normal">Δ</mml:mi><mml:mi>F</mml:mi></mml:mrow></mml:math></inline-formula>; W m<sup>−2</sup> nm<sup>−1</sup>), spectral AOD determined from EKO RSB measurements and radiative forcing efficiency (<inline-formula><mml:math id="M198" display="inline"><mml:mrow><mml:mi mathvariant="normal">Δ</mml:mi><mml:msup><mml:mi>F</mml:mi><mml:mi mathvariant="normal">eff</mml:mi></mml:msup></mml:mrow></mml:math></inline-formula>; W m<sup>−2</sup> nm<sup>−1</sup> AOD<sup>−1</sup>). These large AOD values confirm the strong presence of smoke particles over the site, which substantially altered the radiative fluxes and their spectral distribution. Clear differences between the two days, as well as among the various SZA conditions, highlight the temporal evolution of the aerosol optical properties and their influence on surface radiation. The <inline-formula><mml:math id="M202" display="inline"><mml:mrow><mml:mi mathvariant="normal">Δ</mml:mi><mml:msup><mml:mi>F</mml:mi><mml:mi mathvariant="normal">eff</mml:mi></mml:msup></mml:mrow></mml:math></inline-formula> was calculated using Eq. (<xref ref-type="disp-formula" rid="Ch1.E5"/>), based on the spectral AOD retrieved at the EKO RSB wavelengths.</p>
      <p id="d2e3375">The differences between the two days reflect both the varying aerosol load and the changes in solar geometry, with the higher AOD and smaller SZA on 17 August enhancing the radiative impact. Slight variations in aerosol optical properties, including potential differences in fine-mode dominance or absorption, may also contribute to the observed contrast.</p>
      <p id="d2e3378">The spectral irradiance of GHI<sub><italic>λ</italic></sub>, DNI<sub><italic>λ</italic></sub>, and DHI<sub><italic>λ</italic></sub> exhibits a clear contrast between the measurements obtained under clean conditions (dashed lines) and those affected by fire events (solid lines) (Fig. <xref ref-type="fig" rid="F8"/>a, e). On both days, the high AOD caused a strong attenuation of DNI<sub><italic>λ</italic></sub> irradiance, mainly below 700 nm, accompanied by an enhancement of the DHI<sub><italic>λ</italic></sub> component. The stronger impact between 450 and 460 nm, with <inline-formula><mml:math id="M208" display="inline"><mml:mrow><mml:mi mathvariant="normal">Δ</mml:mi><mml:mi>F</mml:mi></mml:mrow></mml:math></inline-formula> values of <inline-formula><mml:math id="M209" display="inline"><mml:mrow><mml:mi mathvariant="normal">−</mml:mi><mml:mn mathvariant="normal">1.69</mml:mn></mml:mrow></mml:math></inline-formula> and <inline-formula><mml:math id="M210" display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1.59</mml:mn></mml:mrow></mml:math></inline-formula> W m<sup>−2</sup> nm<sup>−1</sup>, respectively, indicates the dominance of fine-mode smoke particles which scatter efficiently short wavelengths. A pronounced attenuation of the DNI<sub><italic>λ</italic></sub> spectral irradiance and enhancement of the DHI<sub><italic>λ</italic></sub> component are observed, reflecting the strong scattering capacity of biomass-burning aerosols. This enhanced scattering capacity is consistent with the high SSA values obtained from the surface measurements (Fig. <xref ref-type="fig" rid="F5"/> in Sect. <xref ref-type="sec" rid="Ch1.S4.SS1"/>). The resulting spectra of <inline-formula><mml:math id="M215" display="inline"><mml:mrow><mml:mi mathvariant="normal">Δ</mml:mi><mml:mi>F</mml:mi></mml:mrow></mml:math></inline-formula> are negative for the DNI<sub><italic>λ</italic></sub> and GHI<sub><italic>λ</italic></sub> components and positive for the diffuse one, indicating a net surface cooling effect dominated by scattering processes. The magnitude of the <inline-formula><mml:math id="M218" display="inline"><mml:mrow><mml:mi mathvariant="normal">Δ</mml:mi><mml:mi>F</mml:mi></mml:mrow></mml:math></inline-formula> is larger on 17 August (AOD<inline-formula><mml:math id="M219" display="inline"><mml:mrow><mml:msub><mml:mi/><mml:mrow class="unit"><mml:mn mathvariant="normal">500</mml:mn><mml:mspace width="0.125em" linebreak="nobreak"/><mml:mi mathvariant="normal">nm</mml:mi></mml:mrow></mml:msub><mml:mo>=</mml:mo><mml:mn mathvariant="normal">3.63</mml:mn></mml:mrow></mml:math></inline-formula>) than on 18 August (AOD<inline-formula><mml:math id="M220" display="inline"><mml:mrow><mml:msub><mml:mi/><mml:mrow class="unit"><mml:mn mathvariant="normal">500</mml:mn><mml:mspace width="0.125em" linebreak="nobreak"/><mml:mi mathvariant="normal">nm</mml:mi></mml:mrow></mml:msub><mml:mo>=</mml:mo><mml:mn mathvariant="normal">2.25</mml:mn></mml:mrow></mml:math></inline-formula>), consistent with the higher aerosol load and the smaller solar zenith angle. The <inline-formula><mml:math id="M221" display="inline"><mml:mrow><mml:mi mathvariant="normal">Δ</mml:mi><mml:msup><mml:mi>F</mml:mi><mml:mi mathvariant="normal">eff</mml:mi></mml:msup></mml:mrow></mml:math></inline-formula> spectra (Fig. <xref ref-type="fig" rid="F8"/>d, h) exhibit similar shapes for both days, with maximum efficiency in the visible region (400–800 nm), suggesting that the optical properties of the aerosols, likely dominated by biomass-burning particles, remained relatively constant throughout the episode.</p>
      <p id="d2e3596">The integrated spectral radiative forcing values (<inline-formula><mml:math id="M222" display="inline"><mml:mi mathvariant="normal">Δ</mml:mi></mml:math></inline-formula>DF and <inline-formula><mml:math id="M223" display="inline"><mml:mi mathvariant="normal">Δ</mml:mi></mml:math></inline-formula>DF<sup>eff</sup>) determined from Eq. (<xref ref-type="disp-formula" rid="Ch1.E7"/>) are shown in Table <xref ref-type="table" rid="T2"/>. The results are consistent with the spectral behaviour discussed in Fig. <xref ref-type="fig" rid="F8"/>. The total <inline-formula><mml:math id="M225" display="inline"><mml:mi mathvariant="normal">Δ</mml:mi></mml:math></inline-formula>DF<sup>GHI<sub><italic>λ</italic></sub></sup> (300–1100 nm) reached <inline-formula><mml:math id="M227" display="inline"><mml:mrow><mml:mi mathvariant="normal">−</mml:mi><mml:mn mathvariant="normal">395</mml:mn></mml:mrow></mml:math></inline-formula> W m<sup>−2</sup> on 17 August and <inline-formula><mml:math id="M229" display="inline"><mml:mrow><mml:mi mathvariant="normal">−</mml:mi><mml:mn mathvariant="normal">299</mml:mn></mml:mrow></mml:math></inline-formula> W m<sup>−2</sup> on 18 August, confirming a strong surface cooling effect during the biomass-burning episode. The forcing was dominated by the DNI<sub><italic>λ</italic></sub> component (<inline-formula><mml:math id="M232" display="inline"><mml:mrow><mml:mo>∼</mml:mo><mml:mi mathvariant="normal">−</mml:mi><mml:mn mathvariant="normal">700</mml:mn></mml:mrow></mml:math></inline-formula> and <inline-formula><mml:math id="M233" display="inline"><mml:mrow><mml:mi mathvariant="normal">−</mml:mi><mml:mn mathvariant="normal">609</mml:mn></mml:mrow></mml:math></inline-formula> W m<sup>−2</sup>, respectively), while the DHI<sub><italic>λ</italic></sub> component partially compensated for this loss with positive values (<inline-formula><mml:math id="M236" display="inline"><mml:mrow><mml:mo>∼</mml:mo><mml:mo>+</mml:mo><mml:mn mathvariant="normal">250</mml:mn></mml:mrow></mml:math></inline-formula> and <inline-formula><mml:math id="M237" display="inline"><mml:mrow><mml:mo>+</mml:mo><mml:mn mathvariant="normal">174</mml:mn></mml:mrow></mml:math></inline-formula> W m<sup>−2</sup>), as expected under intense scattering conditions.</p>

<table-wrap id="T2" specific-use="star"><label>Table 2</label><caption><p id="d2e3784">Averages of AOD (mean <inline-formula><mml:math id="M239" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> SD), ΔDF (W m<sup>−2</sup>) and ΔDF<sup>eff</sup>  (W m<sup>−2</sup> AOD<sup>−1</sup>) for GHI<sub><italic>λ</italic></sub>, DNI<sub><italic>λ</italic></sub> and DHI<sub><italic>λ</italic></sub> spectral radiation components in the four spectral ranges (UV: 300–400 nm, VIS: 400–700 nm, near-IR: 700–1100 nm, and Total:  300–1100 nm) for the two study cases (17 August 11:56 UTC (SZA 22.7<inline-formula><mml:math id="M247" display="inline"><mml:mi mathvariant="italic">°</mml:mi></mml:math></inline-formula>) and 18 August 15:46 UTC (SZA 39.1<inline-formula><mml:math id="M248" display="inline"><mml:mi mathvariant="italic">°</mml:mi></mml:math></inline-formula>)).</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="center"/>
     <oasis:colspec colnum="3" colname="col3" align="center"/>
     <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 colname="col2">AOD</oasis:entry>
         <oasis:entry colname="col3"><inline-formula><mml:math id="M249" display="inline"><mml:mrow><mml:mi mathvariant="normal">Δ</mml:mi><mml:msup><mml:mi mathvariant="normal">DF</mml:mi><mml:mrow><mml:msub><mml:mi mathvariant="normal">GHI</mml:mi><mml:mi mathvariant="italic">λ</mml:mi></mml:msub></mml:mrow></mml:msup></mml:mrow></mml:math></inline-formula> (<inline-formula><mml:math id="M250" display="inline"><mml:mrow><mml:mi mathvariant="normal">Δ</mml:mi><mml:msup><mml:mi mathvariant="normal">DF</mml:mi><mml:mrow><mml:mi mathvariant="normal">eff</mml:mi><mml:mo>-</mml:mo><mml:msub><mml:mi mathvariant="normal">GHI</mml:mi><mml:mi mathvariant="italic">λ</mml:mi></mml:msub></mml:mrow></mml:msup></mml:mrow></mml:math></inline-formula>)</oasis:entry>
         <oasis:entry colname="col4"><inline-formula><mml:math id="M251" display="inline"><mml:mrow><mml:mi mathvariant="normal">Δ</mml:mi><mml:msup><mml:mi mathvariant="normal">DF</mml:mi><mml:mrow><mml:msub><mml:mi mathvariant="normal">DNI</mml:mi><mml:mi mathvariant="italic">λ</mml:mi></mml:msub></mml:mrow></mml:msup></mml:mrow></mml:math></inline-formula> (<inline-formula><mml:math id="M252" display="inline"><mml:mrow><mml:mi mathvariant="normal">Δ</mml:mi><mml:msup><mml:mi mathvariant="normal">DF</mml:mi><mml:mrow><mml:mi mathvariant="normal">eff</mml:mi><mml:mo>-</mml:mo><mml:msub><mml:mi mathvariant="normal">DNI</mml:mi><mml:mi mathvariant="italic">λ</mml:mi></mml:msub></mml:mrow></mml:msup></mml:mrow></mml:math></inline-formula>)</oasis:entry>
         <oasis:entry colname="col5"><inline-formula><mml:math id="M253" display="inline"><mml:mrow><mml:mi mathvariant="normal">Δ</mml:mi><mml:msup><mml:mi mathvariant="normal">DF</mml:mi><mml:mrow><mml:msub><mml:mi mathvariant="normal">DHI</mml:mi><mml:mi mathvariant="italic">λ</mml:mi></mml:msub></mml:mrow></mml:msup></mml:mrow></mml:math></inline-formula> (<inline-formula><mml:math id="M254" display="inline"><mml:mrow><mml:mi mathvariant="normal">Δ</mml:mi><mml:msup><mml:mi mathvariant="normal">DF</mml:mi><mml:mrow><mml:mi mathvariant="normal">eff</mml:mi><mml:mo>-</mml:mo><mml:msub><mml:mi mathvariant="normal">DHI</mml:mi><mml:mi mathvariant="italic">λ</mml:mi></mml:msub></mml:mrow></mml:msup></mml:mrow></mml:math></inline-formula>)</oasis:entry>
       </oasis:row>
       <oasis:row rowsep="1">
         <oasis:entry colname="col1"/>
         <oasis:entry colname="col2"/>
         <oasis:entry colname="col3">Wm<sup>−2</sup> (Wm<sup>−2</sup> AOD<sup>−1</sup>)</oasis:entry>
         <oasis:entry colname="col4">Wm<sup>−2</sup> (Wm<sup>−2</sup> AOD<sup>−1</sup>)</oasis:entry>
         <oasis:entry colname="col5">Wm<sup>−2</sup> (Wm<sup>−2</sup> AOD<sup>−1</sup>)</oasis:entry>
       </oasis:row>
     </oasis:thead>
     <oasis:tbody>
       <oasis:row rowsep="1">
         <oasis:entry namest="col1" nameend="col5">UV: 300–400 nm </oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">17-08-2023 11:56</oasis:entry>
         <oasis:entry colname="col2">4.75 <inline-formula><mml:math id="M264" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> 0.06</oasis:entry>
         <oasis:entry colname="col3"><inline-formula><mml:math id="M265" display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">52.8</mml:mn></mml:mrow></mml:math></inline-formula> (<inline-formula><mml:math id="M266" display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">11.1</mml:mn></mml:mrow></mml:math></inline-formula>)</oasis:entry>
         <oasis:entry colname="col4"><inline-formula><mml:math id="M267" display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">51.8</mml:mn></mml:mrow></mml:math></inline-formula> (<inline-formula><mml:math id="M268" display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">10.9</mml:mn></mml:mrow></mml:math></inline-formula>)</oasis:entry>
         <oasis:entry colname="col5"><inline-formula><mml:math id="M269" display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">5.0</mml:mn></mml:mrow></mml:math></inline-formula> (<inline-formula><mml:math id="M270" display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1.0</mml:mn></mml:mrow></mml:math></inline-formula>)</oasis:entry>
       </oasis:row>
       <oasis:row rowsep="1">
         <oasis:entry colname="col1">18-08-2023 15:46</oasis:entry>
         <oasis:entry colname="col2">3.98 <inline-formula><mml:math id="M271" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> 0.33</oasis:entry>
         <oasis:entry colname="col3"><inline-formula><mml:math id="M272" display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">39.0</mml:mn></mml:mrow></mml:math></inline-formula> (<inline-formula><mml:math id="M273" display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">10.1</mml:mn></mml:mrow></mml:math></inline-formula>)</oasis:entry>
         <oasis:entry colname="col4"><inline-formula><mml:math id="M274" display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">47.1</mml:mn></mml:mrow></mml:math></inline-formula> (<inline-formula><mml:math id="M275" display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">12.4</mml:mn></mml:mrow></mml:math></inline-formula>)</oasis:entry>
         <oasis:entry colname="col5"><inline-formula><mml:math id="M276" display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">2.5</mml:mn></mml:mrow></mml:math></inline-formula> (<inline-formula><mml:math id="M277" display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">0.5</mml:mn></mml:mrow></mml:math></inline-formula>)</oasis:entry>
       </oasis:row>
       <oasis:row rowsep="1">
         <oasis:entry namest="col1" nameend="col5">VIS: 400–700 nm </oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">17-08-2023 11:56</oasis:entry>
         <oasis:entry colname="col2">3.21 <inline-formula><mml:math id="M278" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> 0.76</oasis:entry>
         <oasis:entry colname="col3"><inline-formula><mml:math id="M279" display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">246.0</mml:mn></mml:mrow></mml:math></inline-formula> (<inline-formula><mml:math id="M280" display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">76.6</mml:mn></mml:mrow></mml:math></inline-formula>)</oasis:entry>
         <oasis:entry colname="col4"><inline-formula><mml:math id="M281" display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">429.5</mml:mn></mml:mrow></mml:math></inline-formula> (<inline-formula><mml:math id="M282" display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">139.0</mml:mn></mml:mrow></mml:math></inline-formula>)</oasis:entry>
         <oasis:entry colname="col5">150.3 (51.7)</oasis:entry>
       </oasis:row>
       <oasis:row rowsep="1">
         <oasis:entry colname="col1">18-08-2023 15:46</oasis:entry>
         <oasis:entry colname="col2">1.98 <inline-formula><mml:math id="M283" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> 0.65</oasis:entry>
         <oasis:entry colname="col3"><inline-formula><mml:math id="M284" display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">191.1</mml:mn></mml:mrow></mml:math></inline-formula> (<inline-formula><mml:math id="M285" display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">99.2</mml:mn></mml:mrow></mml:math></inline-formula>)</oasis:entry>
         <oasis:entry colname="col4"><inline-formula><mml:math id="M286" display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">391.4</mml:mn></mml:mrow></mml:math></inline-formula> (<inline-formula><mml:math id="M287" display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">211.3</mml:mn></mml:mrow></mml:math></inline-formula>)</oasis:entry>
         <oasis:entry colname="col5">112.7 (64.9)</oasis:entry>
       </oasis:row>
       <oasis:row rowsep="1">
         <oasis:entry namest="col1" nameend="col5">near-IR: 700–1100 nm </oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">17-08-2023 11:56</oasis:entry>
         <oasis:entry colname="col2">1.42 <inline-formula><mml:math id="M288" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> 0.31</oasis:entry>
         <oasis:entry colname="col3"><inline-formula><mml:math id="M289" display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">95.4</mml:mn></mml:mrow></mml:math></inline-formula> (<inline-formula><mml:math id="M290" display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">65.7</mml:mn></mml:mrow></mml:math></inline-formula>)</oasis:entry>
         <oasis:entry colname="col4"><inline-formula><mml:math id="M291" display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">217.7</mml:mn></mml:mrow></mml:math></inline-formula> (<inline-formula><mml:math id="M292" display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">149.8</mml:mn></mml:mrow></mml:math></inline-formula>)</oasis:entry>
         <oasis:entry colname="col5">105.5 (72.5)</oasis:entry>
       </oasis:row>
       <oasis:row rowsep="1">
         <oasis:entry colname="col1">18-08-2023 15:46</oasis:entry>
         <oasis:entry colname="col2">0.78 <inline-formula><mml:math id="M293" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> 0.16</oasis:entry>
         <oasis:entry colname="col3"><inline-formula><mml:math id="M294" display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">68.1</mml:mn></mml:mrow></mml:math></inline-formula> (<inline-formula><mml:math id="M295" display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">84.5</mml:mn></mml:mrow></mml:math></inline-formula>)</oasis:entry>
         <oasis:entry colname="col4"><inline-formula><mml:math id="M296" display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">169.1</mml:mn></mml:mrow></mml:math></inline-formula> (<inline-formula><mml:math id="M297" display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">210.3</mml:mn></mml:mrow></mml:math></inline-formula>)</oasis:entry>
         <oasis:entry colname="col5">63.4 (79.0)</oasis:entry>
       </oasis:row>
       <oasis:row rowsep="1">
         <oasis:entry namest="col1" nameend="col5">Total: 300–1100 nm </oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">17-08-2023 11:56</oasis:entry>
         <oasis:entry colname="col2">2.64 <inline-formula><mml:math id="M298" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> 1.30</oasis:entry>
         <oasis:entry colname="col3"><inline-formula><mml:math id="M299" display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">394.9</mml:mn></mml:mrow></mml:math></inline-formula> (<inline-formula><mml:math id="M300" display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">153.7</mml:mn></mml:mrow></mml:math></inline-formula>)</oasis:entry>
         <oasis:entry colname="col4"><inline-formula><mml:math id="M301" display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">699.9</mml:mn></mml:mrow></mml:math></inline-formula> (<inline-formula><mml:math id="M302" display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">300.0</mml:mn></mml:mrow></mml:math></inline-formula>)</oasis:entry>
         <oasis:entry colname="col5">251.1 (123.2)</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">18-08-2023 15:46</oasis:entry>
         <oasis:entry colname="col2">1.73 <inline-formula><mml:math id="M303" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> 1.15</oasis:entry>
         <oasis:entry colname="col3"><inline-formula><mml:math id="M304" display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">298.6</mml:mn></mml:mrow></mml:math></inline-formula> (<inline-formula><mml:math id="M305" display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">194.0</mml:mn></mml:mrow></mml:math></inline-formula>)</oasis:entry>
         <oasis:entry colname="col4"><inline-formula><mml:math id="M306" display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">608.4</mml:mn></mml:mrow></mml:math></inline-formula> (<inline-formula><mml:math id="M307" display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">434.5</mml:mn></mml:mrow></mml:math></inline-formula>)</oasis:entry>
         <oasis:entry colname="col5">173.8 (143.5)</oasis:entry>
       </oasis:row>
     </oasis:tbody>
   </oasis:tgroup></oasis:table></table-wrap>

      <p id="d2e4724">The band-integrated <inline-formula><mml:math id="M308" display="inline"><mml:mrow><mml:mi mathvariant="normal">Δ</mml:mi><mml:msup><mml:mi>F</mml:mi><mml:mi mathvariant="normal">eff</mml:mi></mml:msup></mml:mrow></mml:math></inline-formula> exhibited a distinct spectral dependence, peaking in the visible range (<inline-formula><mml:math id="M309" display="inline"><mml:mrow><mml:mi mathvariant="normal">−</mml:mi><mml:mn mathvariant="normal">77</mml:mn></mml:mrow></mml:math></inline-formula> to <inline-formula><mml:math id="M310" display="inline"><mml:mrow><mml:mi mathvariant="normal">−</mml:mi><mml:mn mathvariant="normal">99</mml:mn></mml:mrow></mml:math></inline-formula> W m<sup>−2</sup>AOD<sup>−1</sup> for the GHI<sub><italic>λ</italic></sub> component), consistent with the strong scattering capacity of fine-mode smoke particles. Near-IR efficiencies were slightly lower (<inline-formula><mml:math id="M314" display="inline"><mml:mrow><mml:mi mathvariant="normal">−</mml:mi><mml:mn mathvariant="normal">66</mml:mn></mml:mrow></mml:math></inline-formula> to <inline-formula><mml:math id="M315" display="inline"><mml:mrow><mml:mi mathvariant="normal">−</mml:mi><mml:mn mathvariant="normal">85</mml:mn></mml:mrow></mml:math></inline-formula> W m<sup>−2</sup>AOD<sup>−1</sup>), while UV contributions remained minor (<inline-formula><mml:math id="M318" display="inline"><mml:mrow><mml:mo>∼</mml:mo><mml:mi mathvariant="normal">−</mml:mi><mml:mn mathvariant="normal">10</mml:mn></mml:mrow></mml:math></inline-formula> W m<sup>−2</sup>AOD<sup>−1</sup>). For the DNI<sub><italic>λ</italic></sub> component, <inline-formula><mml:math id="M322" display="inline"><mml:mrow><mml:mi mathvariant="normal">Δ</mml:mi><mml:msup><mml:mi>F</mml:mi><mml:mi mathvariant="normal">eff</mml:mi></mml:msup></mml:mrow></mml:math></inline-formula> reached up to <inline-formula><mml:math id="M323" display="inline"><mml:mrow><mml:mi mathvariant="normal">−</mml:mi><mml:mn mathvariant="normal">211</mml:mn></mml:mrow></mml:math></inline-formula> W m<sup>−2</sup>AOD<sup>−1</sup>, whereas the DHI<sub><italic>λ</italic></sub> component showed positive values (<inline-formula><mml:math id="M327" display="inline"><mml:mrow><mml:mo>∼</mml:mo><mml:mo>+</mml:mo><mml:mn mathvariant="normal">50</mml:mn></mml:mrow></mml:math></inline-formula>–80 W m<sup>−2</sup>AOD<sup>−1</sup>), highlighting the enhanced scattering under high aerosol load. Integrated over 300–1100 nm, total <inline-formula><mml:math id="M330" display="inline"><mml:mrow><mml:mi mathvariant="normal">Δ</mml:mi><mml:msup><mml:mi>F</mml:mi><mml:mi mathvariant="normal">eff</mml:mi></mml:msup></mml:mrow></mml:math></inline-formula> reached <inline-formula><mml:math id="M331" display="inline"><mml:mrow><mml:mi mathvariant="normal">−</mml:mi><mml:mn mathvariant="normal">154</mml:mn></mml:mrow></mml:math></inline-formula> W m<sup>−2</sup>AOD<sup>−1</sup> on 17 August and <inline-formula><mml:math id="M334" display="inline"><mml:mrow><mml:mi mathvariant="normal">−</mml:mi><mml:mn mathvariant="normal">194</mml:mn></mml:mrow></mml:math></inline-formula> W m<sup>−2</sup>AOD<sup>−1</sup> on 18 August, indicating a slightly higher radiative efficiency on the latter day despite lower AOD. These findings confirm that biomass-burning aerosols at IZO produced a marked shortwave surface cooling dominated by visible-range scattering processes.</p>
      <p id="d2e5059">Spectrally, for both GHI<sub><italic>λ</italic></sub> and DNI<sub><italic>λ</italic></sub> spectral radiation, the visible range (400–700 nm) contributed the most to the total forcing (<inline-formula><mml:math id="M339" display="inline"><mml:mo lspace="0mm">∼</mml:mo></mml:math></inline-formula> 60 %–65 %), followed by the near-IR range (<inline-formula><mml:math id="M340" display="inline"><mml:mo lspace="0mm">∼</mml:mo></mml:math></inline-formula> 22 %–25 % for GHI<sub><italic>λ</italic></sub> and <inline-formula><mml:math id="M342" display="inline"><mml:mo>∼</mml:mo></mml:math></inline-formula> 28 %–31 % for DNI<sub><italic>λ</italic></sub>) and the UV range (<inline-formula><mml:math id="M344" display="inline"><mml:mo lspace="0mm">∼</mml:mo></mml:math></inline-formula> 13 % for GHI<sub><italic>λ</italic></sub> and <inline-formula><mml:math id="M346" display="inline"><mml:mo>∼</mml:mo></mml:math></inline-formula> 7 % for DNI<sub><italic>λ</italic></sub>) for the two days. This distribution matches the maximum in the incident solar irradiance and the high scattering efficiency of fine-mode smoke particles in the visible region. <inline-formula><mml:math id="M348" display="inline"><mml:mrow><mml:mi mathvariant="normal">Δ</mml:mi><mml:msup><mml:mi>F</mml:mi><mml:mi mathvariant="normal">eff</mml:mi></mml:msup></mml:mrow></mml:math></inline-formula> also reflects the larger radiative impact per unit AOD on 18 August, despite the lower aerosol load, suggesting a slightly enhanced absorption or differences in aerosol optical properties and solar geometry. Overall, these integrated values confirm that biomass-burning aerosols at IZO produced a pronounced shortwave radiative cooling dominated by scattering processes, with maximum efficiency in the visible range.</p>
      <p id="d2e5166">Besides the instantaneous spectral and band-integrated values, daily radiative forcing was also computed to assess the accumulated shortwave impact of the smoke-laden days. On 17 August, the total daily forcing reached <inline-formula><mml:math id="M349" display="inline"><mml:mrow><mml:mi mathvariant="normal">−</mml:mi><mml:mn mathvariant="normal">56</mml:mn></mml:mrow></mml:math></inline-formula> (GHI<sub><italic>λ</italic></sub>), <inline-formula><mml:math id="M351" display="inline"><mml:mrow><mml:mi mathvariant="normal">−</mml:mi><mml:mn mathvariant="normal">162</mml:mn></mml:mrow></mml:math></inline-formula> (DNI<sub><italic>λ</italic></sub>), and <inline-formula><mml:math id="M353" display="inline"><mml:mrow><mml:mo>+</mml:mo><mml:mn mathvariant="normal">70</mml:mn></mml:mrow></mml:math></inline-formula> W m<sup>−2</sup> (DHI<sub><italic>λ</italic></sub>), while on 18 August the corresponding values were <inline-formula><mml:math id="M356" display="inline"><mml:mrow><mml:mi mathvariant="normal">−</mml:mi><mml:mn mathvariant="normal">44</mml:mn></mml:mrow></mml:math></inline-formula>, <inline-formula><mml:math id="M357" display="inline"><mml:mrow><mml:mi mathvariant="normal">−</mml:mi><mml:mn mathvariant="normal">137</mml:mn></mml:mrow></mml:math></inline-formula>, and <inline-formula><mml:math id="M358" display="inline"><mml:mrow><mml:mo>+</mml:mo><mml:mn mathvariant="normal">60</mml:mn></mml:mrow></mml:math></inline-formula> W m<sup>−2</sup>, respectively. The daily forcing efficiencies were <inline-formula><mml:math id="M360" display="inline"><mml:mrow><mml:mi mathvariant="normal">−</mml:mi><mml:mn mathvariant="normal">77</mml:mn></mml:mrow></mml:math></inline-formula>, <inline-formula><mml:math id="M361" display="inline"><mml:mrow><mml:mi mathvariant="normal">−</mml:mi><mml:mn mathvariant="normal">313</mml:mn></mml:mrow></mml:math></inline-formula>, and <inline-formula><mml:math id="M362" display="inline"><mml:mrow><mml:mo>+</mml:mo><mml:mn mathvariant="normal">138</mml:mn></mml:mrow></mml:math></inline-formula> W m<sup>−2</sup> AOD<sup>−1</sup> for the GHI<sub><italic>λ</italic></sub>, DNI<sub><italic>λ</italic></sub>, and DHI<sub><italic>λ</italic></sub> components on 17 August, and <inline-formula><mml:math id="M368" display="inline"><mml:mrow><mml:mi mathvariant="normal">−</mml:mi><mml:mn mathvariant="normal">84</mml:mn></mml:mrow></mml:math></inline-formula>, <inline-formula><mml:math id="M369" display="inline"><mml:mrow><mml:mi mathvariant="normal">−</mml:mi><mml:mn mathvariant="normal">332</mml:mn></mml:mrow></mml:math></inline-formula>, and <inline-formula><mml:math id="M370" display="inline"><mml:mrow><mml:mo>+</mml:mo><mml:mn mathvariant="normal">145</mml:mn></mml:mrow></mml:math></inline-formula> W m<sup>−2</sup> AOD<sup>−1</sup> on 18 August. These values are consistent with previously reported daily-scale radiative impacts of biomass-burning aerosols. For example, <xref ref-type="bibr" rid="bib1.bibx67" id="text.66"/> reported global radiative forcing values ranging from <inline-formula><mml:math id="M373" display="inline"><mml:mrow><mml:mi mathvariant="normal">−</mml:mi><mml:mn mathvariant="normal">13</mml:mn></mml:mrow></mml:math></inline-formula> to <inline-formula><mml:math id="M374" display="inline"><mml:mrow><mml:mi mathvariant="normal">−</mml:mi><mml:mn mathvariant="normal">60</mml:mn></mml:mrow></mml:math></inline-formula> W m<sup>−2</sup> and efficiencies between <inline-formula><mml:math id="M376" display="inline"><mml:mrow><mml:mi mathvariant="normal">−</mml:mi><mml:mn mathvariant="normal">80</mml:mn></mml:mrow></mml:math></inline-formula> and <inline-formula><mml:math id="M377" display="inline"><mml:mrow><mml:mi mathvariant="normal">−</mml:mi><mml:mn mathvariant="normal">40</mml:mn></mml:mrow></mml:math></inline-formula> W m<sup>−2</sup> AOD<sup>−1</sup> during the 2012 Siberian wildfires.</p>

      <fig id="F9"><label>Figure 9</label><caption><p id="d2e5501">Temporal evolution of the radiative forcing components (blue: global (GHI), red: direct (DNI) and green: diffuse (DHI) radiation) at Izaña Observatory during the wildfire smoke events of 17 and 18 August 2023.</p></caption>
          <graphic xlink:href="https://amt.copernicus.org/articles/19/3151/2026/amt-19-3151-2026-f09.png"/>

        </fig>

      <p id="d2e5510">In addition to the instantaneous spectral and band-integrated forcing values discussed above, the temporal evolution of the broadband shortwave radiative forcing was analysed over the two smoke-affected days in order to evaluate the diurnal behaviour of the aerosol perturbation (Fig. <xref ref-type="fig" rid="F9"/>). The time series shows a clear enhancement in the magnitude of the forcing during periods of strongest smoke influence, with the largest cooling occurring around local noon, when solar irradiance is at its maximum. On 17 August, the forcing exhibits a pronounced peak between approximately 11:30 and 13:30 UTC, coinciding with the period of highest aerosol loading observed at the station. On 18 August, the forcing remains significant over a broader time interval, with a maximum around 15:30 UTC, consistent with the later arrival of the densest smoke plume (Fig. <xref ref-type="fig" rid="F4"/>a).</p>
      <p id="d2e5518">Although the magnitude observed at IZO lies among the highest documented due to the exceptional aerosol load, this comparison reinforces that the radiative response observed at IZO is consistent with the upper bounds of biomass-burning forcing reported in the literature.</p>
</sec>
</sec>
<sec id="Ch1.S5" sec-type="conclusions">
  <label>5</label><title>Conclusions</title>
      <p id="d2e5531">The extreme wildfire episode affecting Tenerife in August 2023 resulted in an exceptional aerosol perturbation over the Izaña Observatory, characterised by an extraordinarily high aerosol load dominated by fine‐mode smoke particles. The event reached AOD<sub>500 nm</sub> (AE) values of 3.63 (1.71) and 2.25 (2.04) on 17 and 18 August 2023, respectively, among the highest ever reported at this high-mountain site, and was accompanied by fine‐mode fractions exceeding 0.9, indicating the presence of freshly emitted biomass‐burning aerosols. Spectral measurements revealed a strong attenuation of global (GHI<sub><italic>λ</italic></sub>) and direct‐normal (DNI<sub><italic>λ</italic></sub>) irradiance, particularly at wavelengths below 700 nm where fine‐mode scattering is most effective, along with a marked enhancement of diffuse irradiance (DHI<sub><italic>λ</italic></sub>). As a result, daily global irradiance decreased by 21 %–27 %, while direct‐normal irradiance nearly collapsed (<inline-formula><mml:math id="M384" display="inline"><mml:mrow><mml:mi mathvariant="normal">−</mml:mi><mml:mn mathvariant="normal">72</mml:mn><mml:mspace linebreak="nobreak" width="0.125em"/><mml:mi mathvariant="italic">%</mml:mi></mml:mrow></mml:math></inline-formula> to <inline-formula><mml:math id="M385" display="inline"><mml:mrow><mml:mi mathvariant="normal">−</mml:mi><mml:mn mathvariant="normal">99</mml:mn><mml:mspace width="0.125em" linebreak="nobreak"/><mml:mi mathvariant="italic">%</mml:mi></mml:mrow></mml:math></inline-formula>), demonstrating the episode’s strong radiative impact.</p>
      <p id="d2e5601">The radiative forcing analysis showed that scattering by fine‐mode smoke dominated the shortwave response, with spectral forcing strongly negative for direct and global irradiance but positive for the diffuse component. Maximum forcing occurred in the visible region, consistent with the optical properties of freshly emitted smoke. On 17 and 18 August, shortwave integrated radiative forcing reached <inline-formula><mml:math id="M386" display="inline"><mml:mrow><mml:mi mathvariant="normal">−</mml:mi><mml:mn mathvariant="normal">395</mml:mn></mml:mrow></mml:math></inline-formula> and <inline-formula><mml:math id="M387" display="inline"><mml:mrow><mml:mi mathvariant="normal">−</mml:mi><mml:mn mathvariant="normal">299</mml:mn></mml:mrow></mml:math></inline-formula> W m<sup>−2</sup>, respectively, confirming a strong surface cooling effect during the biomass‐burning episode. On 17 August, total daily forcing amounted to <inline-formula><mml:math id="M389" display="inline"><mml:mrow><mml:mi mathvariant="normal">−</mml:mi><mml:mn mathvariant="normal">56</mml:mn></mml:mrow></mml:math></inline-formula> W m<sup>−2</sup> (GHI<sub><italic>λ</italic></sub>), <inline-formula><mml:math id="M392" display="inline"><mml:mrow><mml:mi mathvariant="normal">−</mml:mi><mml:mn mathvariant="normal">162</mml:mn></mml:mrow></mml:math></inline-formula> W m<sup>−2</sup> (DNI<sub><italic>λ</italic></sub>), and <inline-formula><mml:math id="M395" display="inline"><mml:mrow><mml:mo>+</mml:mo><mml:mn mathvariant="normal">70</mml:mn></mml:mrow></mml:math></inline-formula> W m<sup>−2</sup> (DHIλ), while on 18 August the corresponding values were <inline-formula><mml:math id="M397" display="inline"><mml:mrow><mml:mi mathvariant="normal">−</mml:mi><mml:mn mathvariant="normal">44</mml:mn></mml:mrow></mml:math></inline-formula>, <inline-formula><mml:math id="M398" display="inline"><mml:mrow><mml:mi mathvariant="normal">−</mml:mi><mml:mn mathvariant="normal">137</mml:mn></mml:mrow></mml:math></inline-formula>, and <inline-formula><mml:math id="M399" display="inline"><mml:mrow><mml:mo>+</mml:mo><mml:mn mathvariant="normal">60</mml:mn></mml:mrow></mml:math></inline-formula> W m<sup>−2</sup>, respectively. The daily forcing efficiencies were <inline-formula><mml:math id="M401" display="inline"><mml:mrow><mml:mi mathvariant="normal">−</mml:mi><mml:mn mathvariant="normal">77</mml:mn></mml:mrow></mml:math></inline-formula>, <inline-formula><mml:math id="M402" display="inline"><mml:mrow><mml:mi mathvariant="normal">−</mml:mi><mml:mn mathvariant="normal">313</mml:mn></mml:mrow></mml:math></inline-formula>, and <inline-formula><mml:math id="M403" display="inline"><mml:mrow><mml:mo>+</mml:mo><mml:mn mathvariant="normal">138</mml:mn></mml:mrow></mml:math></inline-formula> W m<sup>−2</sup> AOD<sup>−1</sup> for the GHI<sub><italic>λ</italic></sub>, DNI<sub><italic>λ</italic></sub>, and DHI<sub><italic>λ</italic></sub> components on 17 August, and <inline-formula><mml:math id="M409" display="inline"><mml:mrow><mml:mi mathvariant="normal">−</mml:mi><mml:mn mathvariant="normal">84</mml:mn></mml:mrow></mml:math></inline-formula>, <inline-formula><mml:math id="M410" display="inline"><mml:mrow><mml:mi mathvariant="normal">−</mml:mi><mml:mn mathvariant="normal">332</mml:mn></mml:mrow></mml:math></inline-formula>, and <inline-formula><mml:math id="M411" display="inline"><mml:mrow><mml:mo>+</mml:mo><mml:mn mathvariant="normal">145</mml:mn></mml:mrow></mml:math></inline-formula> W m<sup>−2</sup> AOD<sup>−1</sup> on 18 August. These values are consistent with those reported by <xref ref-type="bibr" rid="bib1.bibx67" id="text.67"/> during the 2012 Siberian wildfires.</p>
      <p id="d2e5904">Complementary multi-platform observations reinforce this interpretation. Coincident increases in PM<sub>10</sub>, PM<sub>2.5</sub>, eBC, and combustion-related greenhouse gases (CO<sub>2</sub>, CH<sub>4</sub>, CO) demonstrate the direct influence of the wildfire plume on the atmospheric composition at IZO, providing a comprehensive picture of the physical and chemical signatures associated with an intense near-source smoke intrusion.</p>
      <p id="d2e5943">From a climate perspective, the magnitude and spectral signature of the radiative perturbations documented here highlight the importance of improving the representation of fine-mode smoke aerosols in radiative transfer models and Earth-system simulations. Current models can face difficulties in reproducing the optical complexity and high scattering efficiency of fresh biomass-burning aerosols, particularly when they are transported into the free troposphere through fire-induced vertical motion. As the frequency, intensity, and injection height of wildfire emissions are expected to evolve under future climate conditions, incorporating observationally informed parametrisations will help refine estimates of surface energy budgets, cloud-aerosol interactions, and regional climate responses. The extreme Tenerife episode therefore provides a useful reference case for model evaluation and illustrates the value of coordinated observations for improving our understanding of wildfire-climate interactions.</p>
</sec>

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

      <p id="d2e5950">The EKO RSB data used in this study are available on request from the Izaña WMO-MLC. The AERONET data are freely available from the NASA Goddard Space Flight Center (<uri>https://aeronet.gsfc.nasa.gov</uri>; last access: 4 December 2025). Data from MPLNET used in the present study can be obtained from <uri>https://mplnet.gsfc.nasa.gov/</uri> (last access: 21 October, 2025). In situ surface data from the Izaña Atmospheric Observatory contribute to the WMO GAW program and are available from the World Data Centre for Greenhouse Gases (WDCGG, <uri>https://gaw.kishou.go.jp/policy/gaw/</uri>, last access: 26 October 2025). TROPOMI data (Copernicus Sentinel-5P) are publicly available from the Sentinel-5P data hub at <uri>https://maps.s5p-pal.com/co/</uri> (last access: 3 December 2025). TSI nephelometer scattering coefficients and PM<sub>10</sub> MAAP equivalent black carbon data are publicly available through the EBAS database (<uri>https://ebas.nilu.no</uri>, last access: 9 December 2025), the World Data Centre for Aerosols (WDAC) hosted by NILU. TEOM mass concentration data, and PM<sub>1</sub> MAAP equivalent black carbon data are available upon request to the authors.</p>
  </notes><notes notes-type="authorcontribution"><title>Author contributions</title>

      <p id="d2e5990">All co-authors contributed to the preparation and writing of the manuscript. RDG, AB, and PGS designed the structure and methodology of the paper, discussed the results, and participated in the retrieval analysis. RDG wrote the main part of the paper and performed the required calculations. VC provided valuable ideas used in this study and guidance based on her experience in spectroradiometry and photometry. AB, PGS, YG, OA, and FA wrote Sects. 2.3 and 4.1 related to remote sensing and in situ aerosol measurements. AAH, SLL, and PPR wrote Sects. 2.3 and 4.1 related to greenhouse gases. JJB provided the meteorological data and its interpretation. RR performed the maintenance and daily checks of the EKO RSB spectroradiometer.</p>
  </notes><notes notes-type="competinginterests"><title>Competing interests</title>

      <p id="d2e5996">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="d2e6002">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><notes notes-type="sistatement"><title>Special issue statement</title>

      <p id="d2e6008">This article is part of the special issue “Sun-photometric measurements of aerosols: harmonization, comparisons, synergies, effects, and applications”. It is not associated with a conference.</p>
  </notes><ack><title>Acknowledgements</title><p id="d2e6014">This work is part of the activities of the WMO-Measurement Lead Centre for aerosols and water vapor remote sensing instruments (MLC). We gratefully acknowledge the data provided by the AERONET network (Izaña: Philippe Goloub, Emilio Cuevas and África Barreto). The AERONET sun photometers at the Izaña Observatory (IZO) were calibrated through the AEROSPAIN Central Facility (<uri>https://aerospain.aemet.es/</uri>, last access: 25 October 2025), supported by the European Community Research Infrastructure Action under the ACTRIS grant (agreement no. 871115). We gratefully acknowledge the data provided by the MPLNet network. The MPLNet project is funded by the NASA Radiation Sciences Program and the Earth Observing System. This study was carried out within the Global Atmospheric Watch (GAW) Programme at the Izaña Atmospheric Research Centre, operated by AEMET. We acknowledge the station staff and the GAW World Data Centre for maintaining and distributing the dataset. The authors would like to thank the libRadtran radiative transfer model team, whose tool was used to estimate the spectral irradiance under clean-sky conditions. The authors acknowledge the support from the IZO staff for maintaining the instrumentation.</p></ack><notes notes-type="financialsupport"><title>Financial support</title>

      <p id="d2e6022">This research has received funding from the Ministerio de Ciencia e Innovación (MICINN) (grant nos. PID2021-127588OB-I00 and PID2024-157697OB-I00). Besides, it was funded by the European Comision through 35 the EUBURN-RISK project (INTERREG-SUDOE; S2/2.4/F0327). This research has also been supported by COST (European Cooperation in Science and Technology) under the HARMONIA (International network for harmonization of atmospheric aerosol retrievals from ground-based photometers) Action CA21119 and the Spanish Ministry for Science and Innovation to ACTRIS-ERIC.</p>
  </notes><notes notes-type="reviewstatement"><title>Review statement</title>

      <p id="d2e6028">This paper was edited by Anca Nemuc and reviewed by two anonymous referees.</p>
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