M. L. Santee’s research while affiliated with Jet Propulsion Laboratory and other places

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Publications (321)


Figure 1: Lower stratospheric (30-90 hPa) trace gas absorption spectra as the absolute delta brightness temperature (BT) for six atmospheric gases active in the thermal IR as measured by CrIS in the (a) longwave (650-1095 cm -1 ) and (b) midwave (1210-1750 cm -1 ) bands. These delta-BT spectra were calculated using the SARTA forward model and CLIMCAPS L2 retrievals as state 140
Figure 2: CLIMCAPS AK profiles for (left) Tair, (middle) O3 and (right) HNO3. These profiles represent the average of all diagonal elements from the AK matrices reported in the Level 2 product file for each retrieval parameter at every footprint poleward of 40˚N latitude on 2 February 2020. The error bars represent the standard deviation of the AK profiles.
Figure 4: A time series of lower stratospheric (30-90 hPa) CLIMCAPS-x retrievals of Tair, O3, and HNO3 aggregated onto a 4˚equal4˚equal-angle grid throughout the 2019/2020 Northern Hemisphere winter season poleward of 40˚N latitude. The column on the right represents the MLS V5 Level 2 HNO3 retrievals.
Mapping seasonal nitric acid (HNO 3 ) patterns in the extratropics with nadir-viewing infrared sounders – a retrieval perspective
  • Preprint
  • File available

April 2025

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4 Reads

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Michelle L. Santee

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Christopher D. Barnet

With this paper, we aim to shed light on the extent to which nadir-viewing hyperspectral infrared (IR) sounders can support the study of stratospheric chemical processes and ozone loss in the extratropics. We use CLIMCAPS (Community Long-term Infrared Microwave Combined Atmospheric Processing System) retrievals from JPSS-1 (Joint Polar Satellite System) CrIS (Cross-track Infrared Sounder) measurements as the baseline case. CLIMCAPS retrieves a suite of Earth system variables that includes atmospheric temperature (Tair), water vapor (H2Ovap), carbon dioxide (CO2), carbon monoxide (CO), methane (CH4), ozone (O3), and nitric acid (HNO3). Unlike the Rodgers (2000) Optimal Estimation (OE) retrieval approach, CLIMCAPS regularizes its Bayesian inverse solution dynamically using singular value decomposition (SVD) at run-time to separate measurement signal from noise. We illustrate how the CLIMCAPS approach enables stable retrievals of stratospheric HNO3 under highly variable conditions, allowing characterization of seasonal patterns. Nitric acid is typically used as an indicator species for heterogeneous chemical processing inside the winter stratospheric polar vortices. This paper summarizes our diagnostic evaluation of CLIMCAPS observing capability during the Northern Hemisphere winter of 2019/2020. We contrast CLIMCAPS HNO3 retrievals with those from the limb-viewing MLS (Microwave Limb Sounder) to illustrate the capability of this retrieval approach and lay the foundation for in-depth validation studies in future.

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Sensitivity analysis for 2006: Spatial correlation coefficients between MLS and different CLaMS-3.0 configurations. The first
Summary of campaigns, including the geographic base, months covered, latitude-longitude ranges used in the MLS and ACE-FTS
Isentropic Mixing vs. Convection in CLaMS-3.0/MESSy: Evaluation Using Satellite Climatologies and In Situ Carbon Monoxide Observations

March 2025

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10 Reads

Paul Konopka

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Francesco D'Amato

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Lagrangian modeling of transport, as implemented in the Chemical Lagrangian Model of the Stratosphere (CLaMS), connects the advective (reversible) component of transport along 3D trajectories with mixing, the irreversible component. Here, we investigate the interplay between strongly localized convective uplifts and large-scale flow dynamics in the upper troposphere and lower stratosphere (UTLS). We revisit the Lagrangian formulation of convection in CLaMS-3.0/MESSy, driven by ECMWF’s ERA5 reanalysis, and further develop the model. These developments include refining spatial resolution in the Planetary Boundary Layer (PBL) and decoupling the frequency of the adaptive grid procedure—which captures isentropic mixing and redefines Lagrangian air parcels—from the parameterization of convection. To improve the model’s UTLS transport representation, particularly from the PBL over days to weeks, we derive zonally and seasonally resolved climatologies of CO partial columns (XCO, spanning 147 to 68 hPa) and compare them with Microwave Limb Sounder (MLS) and Atmospheric Chemistry Experiment Fourier Transform Spectrometer (ACE-FTS) observations, as well as in situ data. Incorporating a parameterization for unresolved convection significantly improves CO anomaly representation in the UTLS, particularly in capturing seasonal and spatial patterns. While the simulated absolute XCO values align better with ACE-FTS, the model reproduces MLS anomalies more accurately, suggesting MLS better represents CO variability. In situ observations in the boreal polar region generally support lower ACE-FTS CO values, while MLS better represents CO enhancements in air affected by the Asian summer monsoon above 10 km.


The Imminent Data Desert: The Future of Stratospheric Monitoring in a Rapidly Changing World

February 2025

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41 Reads

The Atmospheric Chemistry Experiment-Fourier Transform Spectrometer (ACE-FTS) on SCISAT-1 and Microwave Limb Sounder (MLS) on NASA’s Aura satellite have contributed significantly to understanding the impacts of human activities on the stratospheric ozone layer. The two-decade-long data record from these instruments has allowed quantification of ozone depletion caused by human-released ozone-depleting substances, the effects of extreme natural events like major volcanic eruptions including Hunga in 2022, as well as events amplified by human-caused climate change such as wildfires that inject material into the stratosphere, as happened over Australia in early 2020. Both platforms are nearing the end of their operational lifetimes, and their decommissioning will cause a substantial gap in the measurement of critical atmospheric components, including water vapor, inorganic chlorine species, and tracers of stratospheric transport. This upcoming “data desert” poses significant challenges for monitoring the recovery of the ozone layer and assessing the effects on stratospheric composition of future extreme events, threats posed by increases in space debris from satellite burn-up, and the possible injection of stratospheric aerosol to mitigate global warming. The lack of confirmed future missions that can provide daily near-global profile measurements of stratospheric composition highlights the need for observational strategies to bridge this impending gap. This paper discusses the essential role of ACE-FTS and MLS in advancing our understanding of the stratosphere, the impact of data loss after the cessation of one or both instruments, and the urgency of developing strategies for mitigating the impact of these observational losses at a time marked by dramatic changes in the stratosphere due to human and natural factors.


Satellite nadir-viewing geometry affects the magnitude and detectability of long-term trends in stratospheric ozone

February 2025

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8 Reads

The continued monitoring of the ozone layer and its long-term evolution leans on comparative studies of merged satellite records. Comparing such records presents unique challenges due to differences in sampling, coverage, and retrieval algorithms between observing platforms, all of which complicate the detection of trends. Here we examine the effects of broad nadir averaging kernels on vertically resolved ozone trends, using one record as an example. We find errors as large as 1 % per decade and displacements in trend profile features by as much as 6 km in altitude due to the vertical redistribution of information by averaging kernels. Furthermore, we show that averaging kernels tend to increase (by 10 %–80 %, depending on the location) the length of the record needed to determine whether trend estimates are distinguishable from natural variability with good statistical confidence. We conclude that trend uncertainties may be underestimated, in part because averaging kernels misrepresent decadal to multidecadal internal variability, and in part because the removal of known modes of variability from the observed record can yield residual errors. The study provides a framework to reconcile differences between observing platforms and highlights the need for caution when using records from instruments with broad averaging kernels to quantify trends and their uncertainties.


FIGURE 1. Comparing measurements of UARS and Aura MLS (top) and SMLS (bottom) for a small portion of an orbit. Each point shows the center location of a profile measurement.
FIGURE 2. Example of individual SMLS scan swaths on successive orbits. In this example, the atmosphere over Mexico City is repeatedly observed on 8 successive orbits. The orbits are numbered sequentially, with orbit number 2 (shown with a thicker line) being the orbit shown in Fig. 1.
FIGURE 5. Atmospheric measurement capability for the example SMLS instrument considered here. Dotted lines are goals. Geomagnetic field measurements observe solar storm disturbances. The 'gravity waves' indicated here are what atmospheric scientists usually call 'buoyancy waves' (they are not Einstein's gravitational waves!). Fig. 2 of [13] shows 25 ions, in decreasing order of detectability (on a per-ion basis), whose millimeter and submillimeter spectra are in the JPL Spectral line Catalog [14].
FIGURE 6. Vertical bars show the SMLS measurement time needed for an upper tropospheric spectral line radiance signal-to-noise of 10 for various species (taller bars indicate greater integration times needed for some species due to a combination of low abundance and intensity of the spectral lines required for upper tropospheric measurements 2 ). Colors of the bars give representative abundances of upper tropospheric species for different situations. Blue is for typical or minimum abundances; pink for enhanced abundances that have been observed or inferred; brown for enhanced boundary layer abundances that can be convectively transported to the upper troposphere; grey for soluble species that may reach the upper troposphere less easily. This plot is for a tropical 'background' atmosphere and 9 km altitude; it includes 2-3× attenuation of the target molecule signals by water vapor continuum, as well as spectral line wings of 'interfering' gases. For the tropical troposphere above 12 km, a region of considerable interest, SMLS signals are typically 2-3× stronger than indicated here. Horizontal lines give SMLS individual measurement times. The thick solid line is for the SMLS 'global coverage' scan mode described in the text, with 3 ms individual measurement time. The dashed horizontal line is for an SMLS 'regional targeted' scan mode with, for example, 2000 km cross-track width and measurements at 5 points in the vertical every 50×50 km in the horizontal, giving 50 ms individual measurement time. A measurement has greater than 10× signal-to-noise if its bar is below the horizontal line. There is a continuum of scan modes available, easily implemented by in-orbit programming of the scan. A 'local targeted' scan mode with measurements at 3 points in the vertical and every 50×50 km in the horizontal over a 200 km cross-track width allows 1 s for each measurement. Because of the large dynamic range in the abundance of many species, useful measurements can be obtained with a signal-to-noise of 3, which reduces the required measurement time 9× from that shown here. The precision and spatial resolution of retrieved geophysical profiles ultimately depends on a range of factors, including instrument noise temperature, scan range and rate, atmospheric molecular line strengths, and choices made in the geophysical product "retrieval" calculations. Summary quantities shown here result from consideration of the degree to which molecular abundances contribute to observed radiances (the "weighting function") combined with radiance signal-to-noise, informed by experience with Aura MLS. Cloud ice measurements from 'continuum' emission, and temperature from O 18 O, are obtained in milliseconds.
FIGURE 7. GEOS-CHEM atmospheric model results for CH 2 O over the southern U.S. on 11 July 2000. Colors give the abundance of CH 2 O in parts per billion by volume (ppbv) with each row representing a different altitude as indicated at the left. Each column is for the time at the bottom of that column. Convective deposition into the upper troposphere (above 10 km) is seen at 14 UT. SMLS has approximately the same spatial and temporal resolution as this model. SMLS precisions are indicated by arrows on the color bars.
A Conical-Scanning Microwave Limb Sounder for Atmospheric Measurements

October 2024

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22 Reads

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1 Citation

We describe a novel scanning microwave limb sounder (SMLS) instrument that performs rapid and broad azimuth conical scans of Earth's limb while simultaneously scanning the limb in the vertical. This azimuthal scanning capability gives dramatic improvement in temporal and spatial coverage over that of previous limb sounding instruments. In a 1500-kilometer altitude, 52°-inclination Earth orbit, SMLS provides 6–8 vertical profile measurements separated by 1.9 hours every 24 hours everywhere between ±65° latitude, and 2–4 such measurements everywhere between ±(65–82°). Horizontal resolution is ∼50×50 km. Vertical resolution is ∼2 km for water vapor and cloud ice and ∼1–3 km for chemical species. In an equatorial orbit, emphasizing the tropics and subtropics, SMLS produces profile measurements every 1.9 hours everywhere between ±35° latitude. SMLS measurements address scientific issues of relevance to the upper troposphere, stratosphere, mesosphere, and lower thermosphere regions of the atmosphere (heights from ∼10 km to ∼100 km).


Daily zonal mean water vapor anomalies based on the 2005–2021 monthly climatology for selected days after the Hunga eruption (a–p). The stratopause, as determined from Microwave Limb Sounder temperature measurements, is represented by dashed pink lines. Dark blue lines show contours of scaled potential vorticity (see, e.g., Dunkerton & Delisi, 1986; Manney et al., 1994) approximating the stratospheric polar vortex edge region.
Evolution of the global (a), Northern (b), and Southern (c) Hemisphere Stratospheric Water Vapor Mass (SWVm), color‐coded by year (see legend), with the 2005–2021 climatology depicted by black lines. (d) The difference between the Southern and Northern Hemisphere SWVm mass. Minor x‐ticks are located on the fifteenth of each month.
(a) Time series of deseasonalized daily Stratospheric Water Vapor Mass (SWVm) global anomalies from the 2005–2021 climatology. (b) Time series of daily global SWVm with positive and negative anomalies shaded in red and blue, respectively. Colored lines show trends through 2021 starting in 2005, 2017, and 2018. To extend the plots past January 2022, the 150 Tg of SWVm from Hunga have been subtracted from the anomalies (a) and global SWVm (b). Time series of (c) SWVm in the tropics (20° $20{}^{\circ}$S–20° $20{}^{\circ}$N), (d) water vapor entering the stratosphere (at 100 hPa and 20° $20{}^{\circ}$S–20° $20{}^{\circ}$N), and (e) the cold point tropopause temperature (20° $20{}^{\circ}$S–20° $20{}^{\circ}$N). Colored lines in panels (d) and (e) show trends starting in 2005 through 2021 or 2023; shading in (c)–(e) is as in (b). All trends are reported with 2σ $\sigma $ uncertainty values. Gray curves show the 2005–2021 climatology in panels (b) and (c) and the 2005–2023 climatology in panels (d) and (e).
Time series of (a) Stratospheric Water Vapor Mass (SWVm) in the southern polar region (82° $82{}^{\circ}$S–60° $60{}^{\circ}$S), and (b) ice polar stratospheric cloud (PSC) volume color‐coded by year. (c) Scatter between dehydration and integrated ice PSC volume. (d) Examples of SWVm projections assuming different exponential decay rates as suggested by models (colored solid lines). The dehydration from PSCs suggested by Microwave Limb Sounder measurements (11.8 Tg) is shown in black. The SWVm 2005–2021 trend is shown by a green dashed line.
The Evolution of the Hunga Hydration in a Moistening Stratosphere

September 2024

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51 Reads

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4 Citations

Plain Language Summary The 2022 Hunga eruption injected an unprecedented amount of water vapor directly into the very dry stratosphere. This abrupt increase in water vapor from Hunga occurred at a time when the stratosphere was already gradually becoming moister. Using measurements from the Microwave Limb Sounder (MLS) on NASA's Aura satellite, we show that stratospheric water vapor remained elevated, essentially unchanged, from the time of the eruption until at least early 2024. MLS data further reveal that, in 2023, one of the main mechanisms for drying the stratosphere—permanent removal of water vapor by formation and settling of ice polar stratospheric cloud particles over Antarctica—was substantially more effective than usual, boosted by the excess water vapor from Hunga. Projections indicate that the return to moisture levels that would have been expected in the absence of the eruption depends on how humid the stratosphere continues to get. Considering the ongoing moistening trend and the water vapor injected by Hunga, the stratosphere could remain unusually humid for a considerable period.


Figure 2. (left) Two rows of the averaging kernel matrix and their corresponding SBUV layers (see legend) for 47.5 • N in July 2005, normalized using the SBUV a priori as in Kramarova et al. (2013a) (their equation 3). (right) One example of a model profile and its synthetic SBUV counterpart for the same time and location, shown as deviations from the model a priori to emphasize vertical structures.
Figure 7. Idealized trend profiles (black) and corresponding profiles as would be observed by the SBUV retrieval algorithm at 42.5 • N (red).
Figure 8. Simulated 2000-2020 ozone trends from CCMI1 and the corresponding range of undetectable trends at the 95 % confidence level. Results for total column ozone are shown at the bottom outside each panel. Observed 2000-2020 trends from LOTUS are shown in blue for reference.
Detectability of forced trends in stratospheric ozone

September 2024

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14 Reads

The continued monitoring of the ozone layer and its long-term evolution leans on comparative studies of merged satellite records. Such records present unique challenges due to differences in sampling, coverage, and retrieval algorithms between observing platforms, leading to discrepancies in trend calculations. Here we examine the effects of optimal estimation retrieval algorithms on vertically resolved ozone trends, using one merged record as an example. We find errors as large as 1 % per decade and displacements in trend profile features of as much as 6 km altitude due to the vertical redistribution of information by averaging kernels. Furthermore, we show that averaging kernels tend to increase the length of record needed to determine whether vertically resolved trend estimates are distinguishable from natural variability with good statistical confidence. We conclude that trend uncertainties may be underestimated, in part because averaging kernels misrepresent decadal to multi-decadal internal variability, and in part because the removal of known modes of variability from the observed record can yield residual errors. The study provides a framework to reconcile differences between observing platforms, and highlights the need for caution when using merged satellite records to quantify trends and their uncertainties.


The Influence of Stratospheric Hydration From the Hunga Eruption on Chemical Processing in the 2023 Antarctic Vortex

August 2024

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58 Reads

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4 Citations

We use measurements of trace gases from the Microwave Limb Sounder and polar stratospheric clouds (PSCs) from the Cloud‐Aerosol Lidar with Orthogonal Polarization to investigate how the extraordinary stratospheric water vapor enhancement from the 2022 Hunga eruption affected polar processing during the 2023 Antarctic winter. Although the dynamical characteristics of the vortex itself were generally unexceptional, the excess moisture initially raised PSC formation threshold temperatures above typical values. Cold conditions, especially in early July, prompted ice PSC formation and unusually severe irreversible dehydration at higher levels (500–700 K), while atypical hydration occurred at lower levels (380–460 K). Heterogeneous chemical processing was more extensive, both vertically (up to 750–800 K) and temporally (earlier in the season), than in prior Antarctic winters. The resultant HCl depletion and ClO enhancement redefined their previously observed ranges at and above 600 K. Albeit unmatched in the satellite record, the early‐winter upper‐level chlorine activation was insufficient to induce substantial ozone loss. Chlorine activation, denitrification, and dehydration processes ran to completion by July/August, with trace gas evolution mostly following the climatological mean thereafter, but with chlorine deactivation starting slightly later than usual. While cumulative ozone losses at 410–550 K were relatively large, probably because of the delayed chlorine deactivation, they were not unprecedented. Thus, ozone depletion was unremarkable throughout the lower stratosphere. Although Hunga enhanced PSC formation and chemical processing in early winter, saturation of lower stratospheric denitrification, dehydration, and chlorine activation (as is typical in the Antarctic) prevented an exceptionally severe ozone hole in 2023.



The evolution of the Hunga hydration in a moistening stratosphere

April 2024

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35 Reads

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3 Citations

The 2022 Hunga eruption caused unprecedented stratospheric hydration. Aura Microwave Limb Sounder (MLS) measurements show that the stratospheric water vapor mass remains essentially unchanged as of early 2024 and that the Hunga hydration occurred atop a robust (possibly accelerating) moistening trend in the stratosphere. Enhanced by the excess Hunga water vapor, dehydration via polar stratospheric cloud (PSC) sedimentation in the 2023 Antarctic vortex exceeded climatological values by ~50%. Simple projections, based solely on Antarctic dehydration, illustrate that the timing of the return to humidity levels that would have been expected absent the Hunga hydration depends on the ongoing stratospheric water vapor trend. For strong moistening, the influx of water entering the stratosphere could offset the enhanced PSC dehydration, resulting in a new, more humid ‘equilibrium’ stratospheric state. With the Hunga hydration compounding an underlying moistening trend, the stratosphere could remain anomalously humid for an extended period.


Citations (67)


... Figure 4 show that the progression of enhanced H2O into polar regions of both hemispheres occurred during 2023 (Santee et al., 2024;Wohltmann et al., 2024;Zhang et al., 2024). Mote et al. (1996), is directly linked to the impact of variations of tropical tropopause temperature on stratospheric humidity (Randel and Park, 2019;Konopka et al., 2022;Millán et al., 2024) as well as the strength and variability of the BDC (Flury, Wu and Read, 2013). The ability to observationally define the perturbation to stratospheric H2O by MLS, which provides daily near-global measurements, stands in contrast to the relatively sparse record provided by solar occultation instruments such as SAGE-III/ISS (see Figure 3), which first sampled the Hunga plume 3 to 5 days after the eruption, then not again until day 23, and then on days 30 to 33. ...

Reference:

The Imminent Data Desert: The Future of Stratospheric Monitoring in a Rapidly Changing World
The Evolution of the Hunga Hydration in a Moistening Stratosphere

... Some studies also proposed that Southern Ocean freshening and sea surface temperature (SST) cooling trend might have contributed to the observed positive trend before 2014 14,[18][19][20][21][22] . After the peak of 2014, Antarctic SIE started to decrease and dramatically dropped to a record low in late 2016 [23][24][25] , after which the unexpected low sea ice state persisted for several years, and the SIE reached a new record low in the mid-2023, and remained at, or near, record-low values during ensuing Austral winter and spring 26,27 . Nearly all regions have experienced significant sea ice loss, particularly in the Weddell Sea (Figs. 1a and S1). ...

Antarctica and the Southern Ocean

Bulletin of the American Meteorological Society

... However, the strong winds that define the Antarctic polar vortex prevented penetration of the H2O plume into the vortex during 2022 (Manney et al., 2023). Figure 4 show that the progression of enhanced H2O into polar regions of both hemispheres occurred during 2023 (Santee et al., 2024;Wohltmann et al., 2024;Zhang et al., 2024). Mote et al. (1996), is directly linked to the impact of variations of tropical tropopause temperature on stratospheric humidity (Randel and Park, 2019;Konopka et al., 2022;Millán et al., 2024) as well as the strength and variability of the BDC (Flury, Wu and Read, 2013). ...

The Influence of Stratospheric Hydration From the Hunga Eruption on Chemical Processing in the 2023 Antarctic Vortex

... As expected, the V psc integrated volume is lower than shown elsewhere (e.g., WMO (2022), Figure 4.2) because polar night regions are not considered. Note that the largest V PSC value in the OMPS LP record is observed in the SH 2023 season, when residual stratospheric water vapor from the Hunga Tonga-Hunga Ha'apai eruption has been proposed to be present in the vortex region before largescale dehydration began (Millán et al., 2024). Northern Hemisphere V PSC values are lower than all SH V PSC values, with the notable exception of the NH 2019-2020 season. ...

The evolution of the Hunga hydration in a moistening stratosphere
  • Citing Preprint
  • April 2024

... Previous model studies, such as Lelieveld et al. (2018), have suggested that the SASM plays a dominant role in shaping the chemical composition of the UT during ASM and the EASM plays a minimal role. However, recent research by Pan et al. (2024) identified EASM convection as an efficient transport pathway that carries surface emissions to the base of the stratosphere. Given projections of a significant strengthening of EASM circulation and weakening of SASM circulation due to global warming (Li et al., 2022), the contributions of both monsoons to the UT chemical compositions warrant reexamination. ...

East Asian summer monsoon delivers large abundances of very-short-lived organic chlorine substances to the lower stratosphere

Proceedings of the National Academy of Sciences

... Despite the decline in ODSs 3 , the continuing occurrence of large Antarctic ozone 'holes' in recent years-partly because of the 2020 Australian wildfire [13][14][15] and 2022 Hunga volcanic eruption [16][17][18][19] -along with concerns about a substantial decrease in October mid-stratospheric ozone 20 , have stimulated discussion about the detectability of a robust signal in Antarctic ozone recovery. Formal detection and attribution (D&A) methods are needed to assess the effectiveness of the Montreal Protocol. ...

The Chemical Effect of Increased Water Vapor From the Hunga Tonga‐Hunga Ha'apai Eruption on the Antarctic Ozone Hole

... Following the 2022 Southern Hemisphere (SH) vortex breakup, the Hunga plume was advected to Antarctic polar latitudes (Manney et al. 2023;Santee et al. 2024). Water vapor observations in May and the first half of June 2023 (Fig. 6.15b) showed a 25%-50% increase above average on the 440-K isentropic surface (~60 hPa or ~19 km). ...

The Influence of Stratospheric Hydration from the Hunga Eruption on Chemical Processing in the 2023 Antarctic Vortex

... Furthermore, direct chemical effects lead to increased ozone in the mid-stratosphere. These impacts include the N2O5+H2O heterogeneous reaction on enhanced sulfate aerosols which reduces NOx and the odd nitrogen-ozone loss cycle, at least at altitudes where the aerosol is significant enough (Wilmouth et al., 2023, Santee et al., 2023Zhang et al., 2024). The 425 enhanced OH from the H2O injection converts NO2 to the reservoir HNO3, also reducing the odd nitrogen-ozone loss cycle in the mid-stratosphere (Fleming et al., 2024). ...

Rapid ozone depletion after humidification of the stratosphere by the Hunga Tonga Eruption

Science

... A near-continuous daily record since 1979 ( Figure 6.2c) shows an increasing SIE trend up to 2015 (Parkinson, 2019), with record winter maxima in 2014-2015 (along with widespread increases in sea-ice season duration, Figure 6.2d). After 2015, SIE then dropped considerably and remained anomalously low, with new record summer minima recorded in 2022-2023 (along with widespread decreases in sea-ice season duration, Figure 6.2e) (Reid et al., 2023). The daily SIE record ( Figure 6.2c) also shows a distinct increase in temporal variance and anomaly persistence starting ~2007 (Purich and Doddridge, 2023). ...

Antarctica and the Southern Ocean

... Our estimated effective (median) radius of sulfate aerosols has a mean value of 0.3 μm (0.27 μm). These particle sizes result in a high sulfate MEE (Table 1; Supplementary Fig. 7d, h, l, p and Supplementary Fig. 8 Changes in stratospheric ozone after the Hunga eruption: 2D-Filtered technique Following the methodologies of Wilmouth 33 and Santee 35 , we assessed changes in the ozone mixing ratio in 2022 and 2023 relative to background mean values using both SAGE III 45 and MLS 56 datasets. To better quantify the impact of the Hunga eruption, we applied a 2D-filtered (2DF) technique (see Methods) to distinguish changes in the zonal-mean mixing ratio. ...

Strong Evidence of Heterogeneous Processing on Stratospheric Sulfate Aerosol in the Extrapolar Southern Hemisphere Following the 2022 Hunga Tonga‐Hunga Ha'apai Eruption