Igor Veselovskii’s research while affiliated with Russian Academy of Sciences and other places

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Publications (116)


Retrieval of microphysical properties of dust aerosols from extinction, backscattering and depolarization lidar measurements using various particle scattering models
  • Preprint
  • File available

October 2024

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102 Reads

Yuyang Chang

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Philippe Goloub

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Mineral dust is a key atmospheric aerosol agent that impacts the radiation budget and plays a significant role in cloud formation. However, studies on retrieving height-resolved microphysical properties of dust aerosols, which are crucial for understanding dust evolution and transport processes, from lidar measurements are still insufficient. Here, we retrieve dust aerosol microphysical properties, including the volume size distribution, volume concentration, effective radius (reff), refractive index and single-scattering albedo, from spectral extinction, backscattering and depolarization lidar measurements. We evaluate the performance of three particle scattering models – Sphere, Spheroid and Irregular–Hexahedral (IH) models in terms of mimicking dust optical properties and deriving retrieval results. We also explore the influence of inverting different measurement sets, namely the conventional 3β (backscattering coefficients at 355, 532 and 1064 nm) + 2α (extinction coefficients at 355 and 532 nm) and the expanded 3β + 2α + 3δ (depolarization ratio at 355, 532 and 1064 nm) measurements, on the retrieval. Both simulations and inversions of real lidar measurements show that it is necessary to use non-spherical models and incorporate 3δ measurements to improve the retrieval accuracy. An increase of discrepancy in depolarization ratio produced by the IH and Spheroid models is observed for reff > 0.5 μm, resulting in larger retrieval difference between the two non-spherical models after the inclusion of 3δ. The study demonstrates the prospect of retrieving height-resolved dust microphysical properties from lidar measurements, as well as potential limitations of the prevailing scattering models in simulating particle backscattering properties.

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Fluorescence properties of long-range transported smoke: Insights from five-channel lidar observations over Moscow during the 2023 wildfire season

September 2024

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20 Reads

The fluorescence lidar at the Prokhorov General Physics Institute (Moscow) was utilized to study transported smoke during the wildfire season from May to September 2023. The lidar system, based on a tripled Nd:YAG laser, performs fluorescence measurements at wavelengths of 438, 472, 513, 560, and 614 nm. This configuration enables the assessment of the spectral dependence of fluorescence backscattering from the planetary boundary layer (PBL) to the upper troposphere and lower stratosphere (UTLS). The fluorescence capacity of smoke, defined as the ratio of fluorescence backscattering to aerosol backscattering at the laser wavelength, exhibits significant variation in the UTLS, with changes of up to a factor of 3. This variation is likely indicative of differences in the relative concentration of organic compounds within the smoke. Analysis of more than 40 smoke episodes enabled an evaluation of the height dependence of smoke fluorescence properties. Observations reveal that the fluorescence capacity generally increases with altitude, suggesting a higher concentration of organic compounds in the UTLS compared to the lower troposphere. Additionally, the measurements consistently show differences in the fluorescence spectra of smoke and urban aerosol. Urban aerosol fluorescence tends to decrease gradually with wavelength, whereas the peak of smoke fluorescence is observed at the 513 or 560 nm channels. This spectral distinction provides an effective means of separating smoke from urban aerosol. The technique was applied to events where smoke from the upper troposphere descended into the PBL and mixed with urban particles, demonstrating its utility in distinguishing between these aerosol types.


Spatiotemporal distributions of (a) the backscattering coefficient at 532 nm, (b) the particle depolarization ratio at 532 nm, and (c) the fluorescence capacity during the night of 27–28 March 2022. The depolarization ratio and fluorescence capacity are only calculated for the values β532 > 0.1 Mm-1 sr-1. The measurements were taken at an angle of 45° to the horizon.
(a) The δ532–GF diagram for observations in the height range of 350–2800 m and (b) the spatiotemporal distribution of aerosol types during the night of 27–28 March 2022.
The HYSPLIT 5 d backward trajectories for the air mass over Lille at altitudes 600, 1500, and 2000 m on 28 March 2022 at 02:00 UTC. Red dots depict the regions of forest fires.
Relative contributions of (a) smoke (ηs), (b) urban (ηu), and (c) dust (ηd) particles to the backscattering coefficient β532 during the night of 27–28 March 2022.
Vertical profiles of the relative contributions of smoke (ηs), urban (ηu), and dust (ηd) particles to the backscattering coefficient β532 on 27 March 2022. These profiles are derived under the assumption that only three aerosol types occur. The black lines depict the deviation of solutions from the mean value (ηi ± σi). Magenta lines show the relative contributions of smoke, urban, and dust particles (ηs,4, ηs,4, ηs,4) when four aerosol types (including pollen) are considered.

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Retrieval and analysis of the composition of an aerosol mixture through Mie–Raman–fluorescence lidar observations

July 2024

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62 Reads

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1 Citation

In the atmosphere, aerosols can originate from numerous sources, leading to the mixing of different particle types. This paper introduces an approach to the partitioning of aerosol mixtures in terms of backscattering coefficients. The method utilizes data collected from the Mie–Raman–fluorescence lidar, with the primary input information being the aerosol backscattering coefficient (β), particle depolarization ratio (δ), and fluorescence capacity (GF). The fluorescence capacity is defined as the ratio of the fluorescence backscattering coefficient to the particle backscattering coefficient at the laser wavelength. By solving a system of equations that model these three properties (β, δ and GF), it is possible to characterize a three-component aerosol mixture. Specifically, the paper assesses the contributions of smoke, urban, and dust aerosols to the overall backscattering coefficient at 532 nm. It is important to note that aerosol properties (δ and GF) may exhibit variations even within a specified aerosol type. To estimate the associated uncertainty, we employ the Monte Carlo technique, which assumes that GF and δ are random values uniformly distributed within predefined intervals. In each Monte Carlo run, a solution is obtained. Rather than relying on a singular solution, an average is computed across the whole set of solutions, and their dispersion serves as a metric for method uncertainty. This methodology was tested using observations conducted at the ATOLL (ATmospheric Observation at liLLe) observatory, Laboratoire d'Optique Atmosphérique, University of Lille, France.


Fig. 3. (a) Lidar signals corresponding to elastic (532 nm), nitrogen Raman (387 nm) and CO2 Raman scattering. (b) Vertical profiles of the aerosol backscattering coefficient, β532, fluorescence backscattering coefficient, βF, and the CO2 mixing ratio, nCO2. The CO2 mixing ratios are averaged within the 200 m height bins. Measurements were performed during the night April 4-5, 2003 and the signals are averaged for period 20:00-04:00 UTC. Mixing ratio is uncalibrated and the value 1.0 corresponds to approximately 1 ppm.
Fig. 4. Vertical profiles of (a) the aerosol backscattering coefficient, β532, fluorescence backscattering coefficient, βF, and (b) the CO2 mixing ratio. Increase of fluorescence at 3000 m and 4500 m induces contribution to the observed mixing ratio
Fig.5 compiles several episodes displaying the enhancement of CO2 mixing ratio induced by smoke fluorescence between May and September 2023. Consequently, the linear regression of data points in Fig.5 enables the derivation of a relationship: 4 2 2 1 17 10
Fig. 6. Vertical profiles of observed values of CO2 mixing ratio, 2 CO n , and values corrected for the fluorescence
Feasibility of Raman lidar for profiling CO2 mixing ratio in the lower troposphere

July 2024

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44 Reads

This study explores the potential of Raman lidar technology for vertical profiling CO2 mixing ratios in the atmosphere. Measurements taken in 2023 at the ATOLL observatory, Laboratoire d’Optique Atmosphérique, University of Lille, France, demonstrate the promising capabilities of a Raman lidar system. This system is equipped with a 355 nm laser emitting 90 mJ pulses and a receiving telescope with a 400 mm aperture. It effectively derives vertical CO2 distributions with a vertical resolution of 200 meters up to heights of 4 kilometers, given several hours of signal accumulation. Notably, the lidar operates without calibrating CO2 concentrations, allowing only for the assessment of relative changes in CO2 mixing ratios with height. However, aerosol fluorescence introduces uncertainties in the CO2 measurements. To address this issue, a correction approach using single-channel fluorescence measurements is proposed, which could potentially enhance the measurement precision.


Fig. 3. (a) Lidar signals corresponding to elastic (532 nm), nitrogen Raman (387 nm) and CO2 Raman scattering. (b) Vertical profiles of the aerosol backscattering coefficient, β532, fluorescence backscattering coefficient, βF, and the CO2 mixing ratio, nCO2. The CO2 mixing ratios are averaged within the 200 m height bins. Measurements were performed during the night April 4-5, 2003 and the signals are averaged for period 20:00-04:00 UTC. Mixing ratio is uncalibrated and the value 1.0 corresponds to approximately 1 ppm.
Fig. 4. Vertical profiles of (a) the aerosol backscattering coefficient, β532, fluorescence backscattering coefficient, βF, and (b) the CO2 mixing ratio. Increase of fluorescence at 3000 m and 4500 m induces contribution to the observed mixing ratio
Fig.5 compiles several episodes displaying the enhancement of CO2 mixing ratio induced by smoke fluorescence between May and September 2023. Consequently, the linear regression of data points in Fig.5 enables the derivation of a relationship: 4 2 2 1 17 10
Fig. 6. Vertical profiles of observed values of CO2 mixing ratio, 2 CO n , and values corrected for the fluorescence
Feasibility of Raman lidar for profiling CO2 mixing ratio in the lower troposphere

July 2024

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39 Reads

This study explores the potential of Raman lidar technology for vertical profiling CO2 mixing ratios in the atmosphere. Measurements taken in 2023 at the ATOLL observatory, Laboratoire d’Optique Atmosphérique, University of Lille, France, demonstrate the promising capabilities of a Raman lidar system. This system is equipped with a 355 nm laser emitting 90 mJ pulses and a receiving telescope with a 400 mm aperture. It effectively derives vertical CO2 distributions with a vertical resolution of 200 meters up to heights of 4 kilometers, given several hours of signal accumulation. Notably, the lidar operates without calibrating CO2 concentrations, allowing only for the assessment of relative changes in CO2 mixing ratios with height. However, aerosol fluorescence introduces uncertainties in the CO2 measurements. To address this issue, a correction approach using single-channel fluorescence measurements is proposed, which could potentially enhance the measurement precision.


A Modified Look-Up Table Based Algorithm with a Self-Posed Scheme for Fine-Mode Aerosol Microphysical Properties Inversion by Multi-Wavelength Lidar

June 2024

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73 Reads

Aerosol microphysical properties, including aerosol particle size distribution, complex refractive index and concentration properties, are key parameters evaluating the impact of aerosols on climate, meteorology, and human health. High Spectral Resolution Lidar (HSRL) is an efficient tool for probing the vertical optical properties of aerosol particles, including the aerosol backscatter coefficient (β) and extinction coefficient (α), at multiple wavelengths. To swiftly process vast data volumes, address the ill-posedness of retrieval problems, and suit simpler lidar systems, this study proposes an algorithm (modified algorithm) for retrieving microphysical property profiles from the HSRL optical data targeting fine-mode aerosols, building upon a previous algorithm (basic algorithm). The modified algorithm is based on a look-up table (LUT) approach, combined with the k-nearest neighbor (k-NN) and random forest (RF) algorithms, and it optimizes the decision tree generation strategy, incorporating a self-posed scheme. In numerical simulation tests for different lidar configurations, the modified algorithm reduced retrieval errors by 41%, 30%, and 32% compared to the basic algorithm for 3β + 2α, 3β + 1α, and 2β + 1α, respectively, with a remarkable improvement of stability. In two observation scenes of a field campaign, the median relative errors of the effective radius for 3β + 2α were 6% and −3%, and the median absolute errors of single-scattering albedo were 0.012 and 0.005. This method represents a further step toward the use of the LUT approach, with the potential to provide effective and efficient aerosol microphysical retrieval for simpler lidar systems, which could advance our understanding of aerosols’ climatic, meteorological, and health impacts.


The Arctic upper troposphere and lower stratosphere aerosol layer in the fall of 2019. The black solid line shows the 532 nm particle extinction coefficient (October–November mean profile) measured with ground‐based Raman lidar during the MOSAiC expedition at 85°–86°N. The blue and green profiles show October 2019 mean extinction profiles for the latitudinal bands from 60° to 70°N (green) and 70°–85°N (blue) measured with the satellite‐based ACE instrument (1,020 atmospheric transmission channel). The 1,020 nm extinction profiles are multiplied by a factor 3. We hypothesize that Raikoke sulfate aerosol dominated at stratospheric heights above 12 km (dotted line) and wildfire smoke dominated in the upper troposphere up to the extinction maximum. AOTs for 532 nm measured at 85–86°N are given as numbers.
Comment on “Stratospheric Aerosol Composition Observed by the Atmospheric Chemistry Experiment Following the 2019 Raikoke Eruption” by Boone et al.

June 2024

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51 Reads

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3 Citations

Based on satellite observations in the Arctic stratosphere at latitudes from 61° to 66°N in the second half of 2019, Boone et al. (2022, https://doi.org/10.1029/2022jd036600) provide the impression that the aerosol in the upper troposphere and lower stratosphere (UTLS) over the entire Arctic consisted of sulfate aerosol originating from the Raikoke volcanic eruption in the summer of 2019. Here, we show that this was most probably not the case and the aerosol layering conditions were much more complex. By combining the stratospheric aerosol typing results of Boone et al. (2022, https://doi.org/10.1029/2022jd036600) with lidar observations at 85°–86°N of Ohneiser et al. (2021, https://doi.org/10.5194/acp‐21‐15783‐2021) of a dominating wildfire smoke layer in the UTLS height range, we demonstrate that the Arctic UTLS aerosol most likely consisted of Siberian wildfire smoke in the lower part and sulfate aerosol in the upper part of the aerosol layer which extended from 7 to 19 km height and was well observable until May 2020. The smoke‐ and sulfate‐related aerosol optical thickness (AOT) fractions were about 0.7–0.8 and 0.2–0.3, respectively, according to our analysis. The sulfate AOT is in good agreement with model‐based predictions of the Raikoke sulfate AOT.


Innovative aerosol hygroscopic growth study from Mie–Raman–fluorescence lidar and microwave radiometer synergy

June 2024

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66 Reads

This study focuses on the characterization of aerosol hygroscopicity using remote sensing techniques. We employ a Mie–Raman–fluorescence lidar (Lille Lidar for Atmospheric Study, LILAS), developed at the ATOLL platform, Laboratoire d'Optique Atmosphérique, Lille, France, in combination with the RPG-HATPRO-G5 microwave radiometer to enable continuous aerosol and water vapor monitoring. We identify hygroscopic growth cases when an aerosol layer exhibits an increase in both aerosol backscattering coefficient and relative humidity. By examining the fluorescence backscattering coefficient, which remains unaffected by the presence of water vapor, the potential temperature, and the absolute humidity, we verify the homogeneity of the aerosol layer. Consequently, the change in the backscattering coefficient is solely attributed to water uptake. The Hänel theory is employed to describe the evolution of the backscattering coefficient with relative humidity and introduces a hygroscopic coefficient, γ, which depends on the aerosol type. The particularity of this method revolves around the use of the fluorescence which is employed to take into account and correct the aerosol concentration variations in the layer. Case studies conducted on 29 July and 9 March 2021 examine, respectively, an urban and a smoke aerosol layer. For the urban case, γ is estimated as 0.47 ± 0.03 at 532 nm; as for the smoke case, the estimation of γ is 0.5 ± 0.3. These values align with those reported in the literature for urban and smoke particles. Our findings highlight the efficiency of the Mie–Raman–fluorescence lidar and microwave radiometer synergy in characterizing aerosol hygroscopicity. The results contribute to advance our understanding of atmospheric processes, aerosol–cloud interactions, and climate modeling.


Derivation of depolarization ratios of aerosol fluorescence and water vapor Raman backscatters from lidar measurements

February 2024

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79 Reads

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3 Citations

Polarization properties of the fluorescence induced by polarized laser radiation are widely considered in laboratory studies. In lidar observations, however, only the total backscattered power of fluorescence is analyzed. In this paper we present results obtained with a modified Mie–Raman–fluorescence lidar operated at the ATOLL observatory, Laboratoire d'Optique Atmosphérique, University of Lille, France, allowing us to measure depolarization ratios of fluorescence at 466 nm (δF) and of water vapor Raman backscatter. Measurements were performed in May–June 2023 during the Alberta forest fires season when smoke plumes were almost continuously transported over the Atlantic Ocean towards Europe. During the same period, smoke plumes from the same sources were also detected and analyzed in Moscow, at the General Physics Institute (GPI), with a five-channel fluorescence lidar able to measure fluorescence backscattering at 438, 472, 513, 560 and 614 nm. Results demonstrate that, inside the planetary boundary layer (PBL), the urban aerosol fluorescence is maximal at 438 nm, and then it gradually decreases with the increase in wavelength. The smoke layers observed within 4–6 km height present a maximum fluorescence at 513 nm, while in the upper troposphere, fluorescence maximum shifts to 560 nm. Regarding the fluorescence depolarization ratio, for smoke its value typically varies within the 45 %–55 % range. The depolarization ratio of the water vapor Raman backscattering at 408 nm is shown to be quite low (2±0.5 %) in the absence of fluorescence because the narrowband interference filter (0.3 nm) in the water vapor channel selects only the strongest vibrational lines of the Raman spectrum. As a result, the depolarization ratio at the water vapor Raman channel is sensitive to the presence of strongly depolarized fluorescence backscattering and can be used for the evaluation of the aerosol fluorescence contribution to measured water vapor mixing ratio.


Retrieval and analysis of the composition of an aerosol mixture through Mie-Raman-Fluorescence lidar observations

February 2024

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38 Reads

In the atmosphere, aerosols can originate from numerous sources, leading to the mixing of different particle types. This paper introduces an approach to the partitioning of aerosol mixtures in terms of backscattering coefficients. The method utilizes data collected from the Mie-Raman-fluorescence lidar, with the primary input information being the aerosol backscattering coefficient, particle depolarization ratio (δ), and fluorescence capacity (GF). The fluorescence capacity is defined as the ratio of the fluorescence backscattering coefficient to the particle backscattering coefficient at the laser wavelength. By solving a system of equations that model these three properties (bF, δ and GF), it is possible to characterize a three-component aerosol mixture. Specifically, the paper assesses the contributions of smoke, urban, and dust aerosols to the overall backscattering coefficient at 532 nm. It is important to note that aerosol properties (δ and GF) may exhibit variations even within a specified aerosol type. To estimate the associated uncertainty, we employ the Monte Carlo technique, which assumes that GF and δ are random values uniformly distributed within predefined intervals. In each Monte Carlo run, a solution is obtained. Rather than relying on a singular solution, an average is computed across the whole set of solutions, and their dispersion serves as a metric for method uncertainty. This methodology was tested using observations conducted at the ATOLL observatory, Laboratoire d'Optique Atmosphérique, University of Lille, France.


Citations (65)


... They calculated the fluorescence capacity (G f ) and particle depolarization ratio (δ p532 ) using the backscatter coefficient at 532 nm and classified urban, dust, smoke, and pollen aerosols using the δ p532 -G f method. In their latest research [35], they constructed a mixed-aerosol equation system based on these parameters to quantitatively analyze the proportions of mixed aerosols in the area. For the Beijing area, Zhang et al. [36] classified low-altitude aerosols using the volume depolarization ratio and fluorescence-Mie ratio. ...

Reference:

Observation and Classification of Low-Altitude Haze Aerosols Using Fluorescence–Raman–Mie Polarization Lidar in Beijing during Spring 2024
Retrieval and analysis of the composition of an aerosol mixture through Mie–Raman–fluorescence lidar observations

... During the one year MOSAiC campaign from October 2019 to September 2020, aged Siberian wildfire smoke covered the central Arctic during the first 7.5 months (October 2019 to mid-May 2020) Ansmann et al., 2024b) In part 1 (Ansmann et al., 2024a), we presented our measured MOSAiC cirrus and smoke products, retrieved from continuously operated lidar and cloud radar instruments aboard the research ice breaker Polarstern, with the goal to provide clear our hypothesis that wildfire smoke particles, expected to be inefficient INPs (Kanji et al., 2008;Wang and Knopf, 2011;Knopf et al., 2018), were able to serve as INPs in Arctic cirrus formation processes at high super saturation levels and low cirrus top temperatures of −60°to −75°C. Besides the background and volcanic sulfate aerosol (causing homogeneous freezing) the only further aerosol type present in the upper troposphere over the central Arctic in the winter of 291-2020 was definitely aged wildfire smoke Ansmann et al., 2024b). ...

Comment on “Stratospheric Aerosol Composition Observed by the Atmospheric Chemistry Experiment Following the 2019 Raikoke Eruption” by Boone et al.

... Moreover, we took precautions to ensure that the relative humidity in the selected intervals remained below 60 % to min- imize the impact of particle hygroscopic growth. The example of such an impact is presented in Fig. 6 of Veselovskii et al. (2024). Based on the obtained results, we summarized the ranges of parameter variation in Table 1. ...

Derivation of depolarization ratios of aerosol fluorescence and water vapor Raman backscatters from lidar measurements

... We used 16-20 min for the other three cases, as they contained less noisy data (see Table 1). More details on the procedure of estimating averaging times can be found in Ref. [21]. ...

Pre-filter analysis for retrieval of microphysical particle parameters: a quality-assurance method applied to 3 backscatter (β) +2 extinction (α) optical data taken with HSRL/Raman lidar

... Probably inspired by the early spectral aerosol fluorescence studies, fluorescence lidars have subsequently been developed 50 that employ a single or a small number of broadband discrete fluorescence detection channels instead of a spectrometer (e.g., Rao et al., 2018;Veselovskii et al., 2020;Hu et al., 2022;Veselovskii et al., 2023;Gast et al., 2024). These experimentally simpler instruments can certainly make a contribution to aerosol research, e.g. in aerosol typing or in the coexistence of clouds and aerosols, but sophisticated spectrometric instrumentation is required for investigations focusing on aerosol fluorescence itself or on aerosol-cloud interaction. ...

Multiwavelength fluorescence lidar observations of smoke plumes

... Dust Density: The dust is defined as a group of rare particles in the center of Ghazi that may contain air. Aerial plankton can also occur in the air in the form of dust, sparse spray or smoke [15]. When dust particles are longer than circular, they exhibit an exotic effect of effective attenuation, which is important for attenuating electromagnetic radiation. ...

Simultaneous profiling of dust aerosol mass concentration and optical properties with polarized high-spectral-resolution lidar
  • Citing Article
  • February 2023

The Science of The Total Environment

... Backscattering measurements from the aerosol particles using remote sensing techniques are crucial to gather quantitative information on atmospheric particles' shape, size, and composition from a distance [1]. Such measurements are fundamental to assessing aerosol impacts on climate and global warming, weather patterns, and other meteorological phenomena [2]. Lidar (Light Detection and Ranging) is one of the commonly used active remote sensing techniques collecting backscattered light coming from distant particles [3][4][5]. ...

Retrieval of Aerosol Microphysical Properties from Multi-Wavelength Mie–Raman Lidar Using Maximum Likelihood Estimation: Algorithm, Performance, and Application

... However, in the summer period, the concentrations of certain greenhouse g southern Italy are generally lower compared to winter concentrations, as demons by findings of a WMO/GAW (World Meteorological Organization-Global Atmo Watch) observation site in the neighbouring region of Calabria [37][38][39]. Other s highlighted that contributions derived from domestic heating and fossil fuel burnin play an important role [40]. It will therefore be important to carry on investigations A lower 1σ variability is observed for CH 4 measurements but with very good agreement with STILT predictions. ...

Characterization of Extremely Fresh Biomass Burning Aerosol by Means of Lidar Observations

... Optical properties measured by state-of-the-art lidars, such as lidar ratio (LR), particle linear depolarization ratio (PLDR) and fluorescence, have been used to identify and distinguish dust aerosols from others (Burton et al., 2012;Nicolae et al., 2018;Veselovskii et al., 2022). Nevertheless, quantitative retrievals of microphysical properties of dust aerosols, such as the size distribution and complex refractive index (CRI) from lidar measurements remains challenging and limited. ...

Combining Mie–Raman and fluorescence observations: a step forward in aerosol classification with lidar technology

... Aerosols typically exhibit a bimodal particle size distribution, including fine and coarse modes [5]. The fraction of the particle size distribution occupied by fine modes, such as urban pollution particles and smoke, is utilizes machine learning ideas on LUT [31]. Section 2.2 describes improvements and further optimizations built upon the basic algorithm, serving as the core content of this work, termed the modified algorithm. ...

This is FAST: multivariate Full-permutAtion based Stochastic foresT method—improving the retrieval of fine-mode aerosol microphysical properties with multi-wavelength lidar
  • Citing Article
  • October 2022

Remote Sensing of Environment