An automatic observation-based aerosol typing method for EARLINET
- 1Consiglio Nazionale delle Ricerche, Istituto di Metodologie per l'Analisi Ambientale (CNR-IMAA), C.da S. Loja, Tito Scalo (PZ), 85050, Italy
- 2CommSensLab, Dept. of Signal Theory and Communications, Universitat Politècnica de Catalunya, Barcelona, Spain
- 3Andalusian Institute for Earth System Research (IISTA-CEAMA), 18006, Granada, Spain
- 4Department of Applied Physics, University of Granada, 18071, Granada, Spain
- 5IAASARS, National Observatory of Athens, Athens, Greece
- 6Laser Remote Sensing Unit, Physics Dept., National Technical University of Athens, Athens, Greece
- 7Royal Netherlands Meteorological Institute KNMI, De Bilt, the Netherlands
- 8Leibniz Institute for Tropospheric Research (TROPOS), Leipzig, Germany
- 9National Institute of R&D for Optoelectronics (INOE), Magurele, Romania
- 10Earth Science Institute-(ICT), Évora, Portugal
- 11Ciències i Tecnologies de l'Espai – Centre de Recerca de l'Aeronàutica i de l'Espai/Institut d'Estudis Espacials de Catalunya (CTE-CRAE/IEEC), Universitat Politècnica de Catalunya, Barcelona, Spain
- 12Ludwig-Maximilians-Universität (LMU), Meteorologisches Institut, Theresienstraße 37, 80333 Munich, Germany
Correspondence: Nikos Papagiannopoulos (firstname.lastname@example.org)
We present an automatic aerosol classification method based solely on the European Aerosol Research Lidar Network (EARLINET) intensive optical parameters with the aim of building a network-wide classification tool that could provide near-real-time aerosol typing information. The presented method depends on a supervised learning technique and makes use of the Mahalanobis distance function that relates each unclassified measurement to a predefined aerosol type. As a first step (training phase), a reference dataset is set up consisting of already classified EARLINET data. Using this dataset, we defined 8 aerosol classes: clean continental, polluted continental, dust, mixed dust, polluted dust, mixed marine, smoke, and volcanic ash. The effect of the number of aerosol classes has been explored, as well as the optimal set of intensive parameters to separate different aerosol types. Furthermore, the algorithm is trained with literature particle linear depolarization ratio values. As a second step (testing phase), we apply the method to an already classified EARLINET dataset and analyze the results of the comparison to this classified dataset. The predictive accuracy of the automatic classification varies between 59 % (minimum) and 90 % (maximum) from 8 to 4 aerosol classes, respectively, when evaluated against pre-classified EARLINET lidar. This indicates the potential use of the automatic classification to all network lidar data. Furthermore, the training of the algorithm with particle linear depolarization values found in the literature further improves the accuracy with values for all the aerosol classes around 80 %. Additionally, the algorithm has proven to be highly versatile as it adapts to changes in the size of the training dataset and the number of aerosol classes and classifying parameters. Finally, the low computational time and demand for resources make the algorithm extremely suitable for the implementation within the single calculus chain (SCC), the EARLINET centralized processing suite.
The European Aerosol Research Lidar Network (Pappalardo et al., 2014) operates Raman lidars at a continental scale. Since the beginning, the network aimed towards a sustainable observing system that has been achieved by developing a quality assurance strategy, and optimizing instruments and data. To this direction and towards future advancement, the network plans continuous measurements and near-real-time data delivery. With this in mind, the single calculus chain (D'Amico et al., 2015) for automatic lidar analysis has been developed and currently delivers profiles of optical aerosol properties. The EARLINET SCC explores the implementation of new features like profiles of intensive optical properties and determination of aerosol layer geometrical properties. The intensive optical properties are type-dependent and can be used to classify the observed layers into aerosol types. The categorization into different types provides significant help to understand aerosol sources, their effects, and feedback mechanisms to improve the accuracy of satellite retrievals and to quantify assessments of aerosol radiative impacts on climate (Russell et al., 2014) by intercomparing numerical models such as NWP (Numerical Weather Prediction) and CTM (Chemical Transport Model) (Baklanov et al., 2014). Thus, EARLINET, by providing multi-wavelength range-resolved aerosol properties, has an added value for aerosol typing. In this study we present a flexible automatic method to classify EARLINET data.
Lidar systems are capable of identifying multiple layers in the atmosphere owing to their high vertical resolution (on the order of tens of meters). Thus, lidar-based retrievals can provide a separate classification for each layer and are not confined to columnar classifications as in the case of sun photometers. The lidar technique has proven to be a robust tool to classify aerosols with its capability of polarization-sensitive and multi-wavelength measurements (Liu et al., 2008). Sophisticated lidars, such as the High Spectral Resolution Lidar (HSRL) and the multi-wavelength Raman lidars, offer a multitude of intensive parameters that characterize different aerosol types (e.g., Müller et al., 2007a; Burton et al., 2012; Groß et al., 2013). Typically, the particle extinction-to-backscatter ratio (i.e., particle lidar ratio), the particle linear depolarization ratio at one or more wavelengths, and the wavelength dependence of extinction and/or backscatter coefficients (i.e., extinction- or backscatter-related Ångström exponents) are considered.
The increasing amount of available information and particularly the plethora of lidar intensive parameters, can offer a more accurate aerosol classification as well as insight into the various aerosol types (Burton et al., 2013). Consequently, an objective, multivariate analysis is needed to take advantage of this information. Automatic algorithms are, therefore, employed to classify aerosol into respective types. These procedures make use of various classifiers that are able to quantify the differences between the aerosol classes. In classification analysis, the observations are allocated to a known number of groups, i.e. a supervised learning technique. Whereas in cluster analysis, the groups are not known beforehand and the classifier is tasked with it.
The measured values are evaluated by the classification function to find the group to which the individual most likely belongs. Specifically, distance-based classification techniques (e.g., k nearest neighbor, support vector machine algorithms) are straightforward, i.e. the classification depends on the distance from the target instance to the training instance. The Mahalanobis distance classifier (Mahalanobis, 1936) has a wide range of applications and can be used to categorize data points, each representing an observation, into classes that have predefined characteristics. The distances between the observation and the different classes are calculated, and then the observation is attributed to the class for which the distance is the minimum.
The Mahalanobis-distance-based classification found great applicability in aerosol studies. For instance, the algorithm developed by Burton et al. (2012) makes use of four lidar intensive properties, namely the particle linear depolarization ratio at 532 nm, the particle lidar ratio at 532 nm, the backscatter-related 532-to-1064 nm color ratio, and the ratio of particle linear depolarization ratios at 1064 and 532 nm in order to classify aerosols into 8 types. A slightly different algorithm also including the uncertainties in the input properties was introduced by Russell et al. (2014). Their algorithm was applied to satellite-derived optical and physical data. The reference dataset was obtained from AERONET (Holben et al., 1998) stations, where a single aerosol type tends to dominate (Cattrall et al., 2005). The pre-specified classes were then applied to a 5-year record of retrievals from the spaceborne POLDER 3 (Tanré et al., 2011) polarimeter on PARASOL (Tanré et al., 2011) spacecraft. Recently, Hamill et al. (2016) used the same classifier to produce an aerosol classification scheme based on long-term AERONET data.
In this work, we present a method analogous to the one proposed by Burton et al. (2012), modified to fit EARLINET's needs and capabilities. The aerosol typing exclusively makes use of EARLINET lidar-derived intensive property data. We use the Mahalanobis distance as a classifier to assign any given multi-dimensional observation to the pre-specified aerosol class to which it is most similar. These classes are defined using an EARLINET-based classification scheme. The EARLINET classification scheme is presented in Sect. 2 where we also describe the parameters readily delivered by the network that can be used to classify aerosols. Furthermore, the major aerosol types that comprise the aerosol classes onto which the aerosol classification is based are presented. In Sect. 3 the method that we apply to EARLINET data is explained, and we present the training phase. We set up a scheme for investigating the number of aerosol classes and we perform an analysis to identify the intensive parameters that contribute the most to the classification as well. Section 4 describes the testing phase and provides a discussion of the results of the classification. The paper closes with conclusions of our study and suggestions for further applications and improvements.
EARLINET (https://www.earlinet.org, last access: 10 October 2018) was established in 2000, providing aerosol profiling data on a continental scale, and is now part of the Aerosols, Clouds, and Trace gases Research InfraStructure (ACTRIS; https://www.actris.eu/, last access: 3 October 2018). In these 18 years of continuous existence, EARLINET has evolved both in the number of contributing stations and in its observing capacity (Pappalardo et al., 2014). Currently, 30 stations are submitting aerosol extinction and/or backscatter coefficient profiles to the EARLINET database, according to EARLINET's measurement schedule (one daytime and two nighttime measurements per week). Therefore, these systematic observations consolidate a 4-D European quantitative and statistically significant aerosol survey. Further measurements are devoted to special events, such as volcanic eruptions, forest fires, and desert dust outbreaks. Moreover, EARLINET provides correlative measurements during CALIPSO (Cloud-Aerosol Lidar and Infrared Pathfinder Satellite Observations) overpasses on each EARLINET station in order to validate satellite products (Mamouri et al., 2009; Mona et al., 2009). Throughout the paper, we refer to measurements as a set of aerosol optical profiles reported in the EARLINET database that correspond to the same temporal window, which typically extends for about 1 h. EARLINET data are freely available through the ACTRIS web site (https://www.actris.eu/default.aspx, last access: 15 October 2018) and are published to the CERA database (EARLINET publishing group 2000–2010, 2014a, b, c, d, e; EARLINET publishing group 2000–2015, 2018a, b, c, d, e).
The majority of the EARLINET stations (Pappalardo et al., 2014) operate multi-wavelength Raman lidars that combine a set of elastic and nitrogen inelastic channels, typically consisting of three elastic and two inelastic Raman channels (the so-called 3β+2α configuration). In particular, they provide the aerosol extinction (at 355 and 532 nm) and backscatter coefficients (at 355, 532, and 1064 nm). This configuration allows for the retrieval of the range-resolved particle lidar ratio at 355 and 532 nm (). This intensive parameter depends on the shape, size, and chemical composition of the aerosol (Müller et al., 2007a). When lidar ratio is available for more than one wavelength, the corresponding color ratio can also be retrieved (). This quantity has shown the ability to characterize the ageing status of smoke particles as well as the spectral dependence of aerosol (Alados-Arboledas et al., 2011; Müller et al., 2007a; Nepomuceno Pereira et al., 2014; Nicolae et al., 2013). The combination of the optical data allows for the retrieval of the size-sensitive backscatter and/or extinction-related Ångström exponent and can be calculated as
with X denoting the backscatter (β) or extinction coefficient (α) for a set of wavelengths, λ1 and λ2. Moreover, 52 % of EARLINET stations (Pappalardo et al., 2014) are equipped with depolarization channels, thus providing profiles of the particle linear depolarization ratio. It can be calculated according to Biele et al. (2000) and Freudenthaler et al. (2009):
with R being the backscatter ratio, δm the molecular depolarization, and δv the volume depolarization ratio. This parameter provides information on the particle shape, thus enhancing the aerosol typing strength of the network. Under favorable conditions, the aerosol microphysical properties (such as the effective radius), the volume concentration, and the refractive index can also be retrieved through complex numerical algorithms (Bovchaliuk et al., 2016; Chaikovsky et al., 2016; Müller et al., 2004; Veselovskii et al., 2010).
The data products described above make the EARLINET data an excellent basis to perform aerosol typing at the continental scale. Examples of methodologies to classify aerosol datasets can be found in, e.g., Groß et al. (2011); Mona et al. (2012a); Müller et al. (2007a, b); Navas-Guzmán et al. (2013b), and Baars et al. (2016). For the time being, there are different algorithms under development which combine measurements and aerosol models (Nicolae et al., 2016; Wandinger et al., 2016). Nevertheless, automated observation-based algorithms working at the network level for the identification of layers, their boundaries, and the corresponding aerosol typing are not yet available. The SCC tool for automatic processing of EARLINET lidar signals is, currently, providing primarily profiles of particle extinction and backscatter coefficients, and volume and particle depolarization ratios. The SCC aims at incorporating modules for layer identification, intensive properties retrieval, and aerosol typing. Therefore, this paper could provide a starting point for a harmonized EARLINET classification tool that could also be used by other lidar networks, like the ones involved in GALION (GAW Aerosol Lidar Observation Network), the GAW (Global Aerosol Watch) initiative for the aerosol lidar observation on a global scale, and within aerosol lidar studies in general.
2.1 EARLINET manual aerosol classification
The typical procedure for aerosol categorization adopted within the EARLINET community consists of three main steps:
layer identification and cloud screening,
identification of the geometrical properties (boundaries, center of mass) of the aerosol layer, and
the aerosol layer typing by means of investigation of intensive optical properties (Ångström exponents, lidar ratios, and particle linear depolarization ratios), model outputs (backward trajectory analyses), and ancillary instrument data if available (e.g., satellite or sun photometer data).
In what follows, an example of an aerosol type assignment using EARLINET data is presented. Figure 1 shows the temporal evolution of the range-corrected signal at 1064 nm from a measurement made in Potenza, Italy, on 14 July 2011, 19:20–22:10 UTC with the reference lidar system MUSA (Multiwavelength System for aerosol) of CNR-IMAA (Consiglio Nazionale delle Ricerche – Istituto di Metodologie per l'Analisi Ambientale). High values show a stratified aerosol layer from the ground up to 5 km, whereas low values indicate aerosol-free regions. The lowest altitude range presents the overlap between the laser beam and the receiver field of view and, therefore, it is the blind range of the lidar. MUSA has a full overlap at around 1.15 for 1064 nm (Madonna et al., 2015). The optically thicker layer lies below 2 km, with a distinct layer atop extending up to 3.5 km, and, finally, an optically thinner region from 3.5 to 5 km. The retrieved profiles for the same temporal window of particle backscatter and extinction coefficient, lidar ratios, and Ångström exponents are shown in Fig. 2. The particle extinction and backscatter coefficient are given with their full resolution. To calculate the lidar ratio, the backscatter coefficient was smoothed in the same effective vertical resolution using a Savitzky–Golay second-order filter (Iarlori et al., 2015) and only the useful range of signals was kept; the effective resolution of the resulting profiles varied from 120 to 480 m using the method described in Pappalardo et al. (2004b). The layer 2.0–3.5 km has a constant behavior with the range for the intensive optical profiles indicating the presence of the same type of particles. The mean values of all optical parameters in the range are calculated: lidar ratios of 48±4 sr at 355 nm and 53±4 sr at 532 nm and Ångström exponents (i.e., κβ(355,1064), κβ(532,1064), κβ(355,532), and κα(355,532)) of −0.3 to 0.4 were found.
For the classification of aerosols with respect to their source regions and age, auxiliary information like results of transport and dispersion models or satellite data are used. For the observed aerosol layer, the Lagrangian dispersion model FLEXPART (Stohl et al., 2005) was used for a 5-day backward simulation. Figure 3 shows the so-called footprint that indicates the areas of the air parcels traveling below 2 km before reaching the study area. The model output is given in terms of the decimal logarithm of the integrated residence time in seconds in a grid box. The most probable aerosol source region and the aerosol type were assigned accordingly. The dust-prone area of northern Africa (Morocco and northern Algeria) along with the Mediterranean Sea are most likely the sources of the observed layer and suggest a mixture of dust and marine particles. The combined information of the backward trajectory analysis and the intensive property values indicate the presence of dust particles and they are in accordance with the typical dust values observed over Potenza (Mona et al., 2014).
In the following, the characteristics of the major aerosol types are presented. These aerosol types are used for the automatic classification and correspond to aerosol layers typically encountered over Europe.
2.2 Aerosol types
One of the defining characteristics of the aerosol properties is the source; aerosols found in the atmosphere can be, for example, mineral particles from arid areas of the Earth or organic carbon emitted during biomass burning events. Due to the multiple influence of the aerosol origin on the properties, aerosol sources can be used to classify them into different categories. In this section, we provide an overview of the main aerosol types observed over the EARLINET stations followed by the corresponding optical properties. This section also aims to provide important information on the aerosol types that the automatic classification is based upon. The considered aerosol types almost coincide with the ones used in the CALIPSO classification scheme (Omar et al., 2009), which already provides a satisfactory description of the atmospheric aerosol content. Moreover, adopting similar classification schemes, the direct comparison of the proposed typing against the CALIPSO product is possible.
Man-made activities dictate the aerosol pattern within the atmospheric boundary layer, and affect the observations in the lower troposphere in Europe. Anthropogenic particles show a strong wavelength dependence of their optical properties, i.e., high Ångström exponent values. Moreover, they are typically small and do not significantly depolarize the backscattered light (Heese et al., 2016), and due to the high carbon content, these particles reveal high lidar ratios (Giannakaki et al., 2010). Herein, we refer to this particle type as polluted continental.
Typically, the clean continental aerosol over Europe is a mixture of anthropogenic pollution with particles from natural sources. The clean continental type shows a low depolarizing ability with values lower than 0.07 (Omar et al., 2009); low lidar ratio values, i.e., 20–40 sr; and relatively high Ångström exponents, i.e., 1.0–2.5 (Ansmann et al., 2001; Giannakaki et al., 2010). The clean continental, therefore, differentiates from the polluted continental type due to lower lidar ratio values.
Marine particles are produced at the sea surface and dominate the shallow boundary layer over the oceans (O'Dowd and de Leeuw, 2007). Specifically, the sea-salt particles feature a predominant coarse mode; however, they are spherical in humid conditions and weakly absorbing in contrast to the dust particles. Therefore, they yield low particle lidar ratio values, are almost non depolarizing, and exhibit low Ångström exponent values (Burton et al., 2014; Dawson et al., 2015). This aerosol type is mainly identifiable by the low particle lidar ratio, i.e., 15–25 sr at 532 nm (Burton et al., 2012). As marine aerosol layers manifest themselves over water bodies, either stations only located at the shorelines and under specific meteorological conditions or shipborne measurements can observe pure maritime particles. Consequently, the observations of pure maritime particles is rare within EARLINET and, generally, when these particles are observed their characteristics are far from pristine (Papagiannopoulos et al., 2016a; Preißler et al., 2013). However, mixtures with important contribution of marine particles can be observed in the Mediterranean basin (Papagiannopoulos et al., 2016a). Thus, we consider pure marine and marine-dominated layers as one single category denoted as mixed marine.
2.2.3 Mineral dust and dust mixtures
Mineral dust is produced in arid and semi arid regions of the world, and has a profound contribution to the total natural aerosol loading (Ginoux et al., 2001). The optical properties are considerably different from the other types, thus making them easy to identify. The irregular shape and the large size (Mahowald et al., 2014) lead to a significant high depolarization of the backscattered radiation (Wiegner et al., 2011), and to medium lidar ratio values (Mona et al., 2014; Tesche et al., 2013). They are spectrally neutral to backscatter and extinction, and thus produce low Ångström exponent values (Wiegner et al., 2011). Therefore, the particle lidar ratio, particle linear depolarization ratio, and the Ångström exponent are excellent physical parameters to characterize mineral dust and to distinguish it from other aerosol types. However, it needs to be taken into account that the dust optical properties depend on the source region and the transport pattern (Valenzuela et al., 2014), which is a source of variability detected in the lidar ratio (Nisantzi et al., 2015; Schuster et al., 2012). Recently, Mamouri et al. (2013) showed that dust originating from the Arabian desert produced significantly lower lidar ratio values (34–39 sr at 532 nm) than respective values (50–60 sr at 532 nm) from western Saharan dust particles. An overview on the dust characterization using lidar measurements can be found in Mona et al. (2012b).
Dust can be transported over continental scales. In particular, Saharan dust outbreaks in Europe and across the Atlantic Ocean have been deeply investigated. The European continent is regularly influenced by advected Saharan particles as has been discussed by, e.g., Ansmann et al. (2003); Binietoglou et al. (2015); Bravo-Aranda et al. (2015); Córdoba-Jabonero et al. (2011); Guerrero-Rascado et al. (2008, 2009); Müller et al. (2009); Papayannis et al. (2008, 2014); Preißler et al. (2011); Valenzuela et al. (2012), and Granados-Muñoz et al. (2016a). The study of Papayannis et al. (2008) indicated a large variability in the measured lidar ratio and Ångström exponent values among the different sites, suggesting mixing at different levels. Additionally, the mixture processes also produce large variability in intensive properties as measured at the same site (Mona et al., 2006, 2014). As a consequence of the complex structure of the observed aerosols over Europe and the effects of transport and mixing on the properties of these particles, we consider the use of three dust groups: pure dust, mixed dust, and polluted dust. The pure dust group refers to particles for which the mixing with other aerosol types is negligible. Mixed dust refers to dust-dominated layers mixed with marine particles. This leads to less depolarizing, and less absorbing particles with respect to pure dust particles. Several studies (Burton et al., 2012; Kim et al., 2013; Papagiannopoulos et al., 2016a; Rogers et al., 2014) have indicated that this mixture is important and suggested its inclusion in the CALIPSO retrieval scheme for improving the accuracy of aerosol backscatter and extinction coefficient profiles. Finally, the polluted dust category consists of dust-dominated mixtures with smoke and/or continental pollution, which produce lower depolarization, higher lidar ratios, and enhanced Ångström exponent values owing to the presence of small, spherical particles (Bravo-Aranda et al., 2015; Burton et al., 2012; Groß et al., 2011; Tesche et al., 2013).
Biomass burning is a major global source of atmospheric aerosols. Generally, smoke particles are relatively small and spherical that produce low depolarization, high Ångström exponents, and large lidar ratios (Amiridis et al., 2009; Baars et al., 2012; Giannakaki et al., 2016). The optical properties of smoke particles may vary due to the vegetation type of the emitting source, the combustion type (smouldering or flaming fires), and atmospheric conditions (Balis et al., 2003). Furthermore, the particles are susceptible to changes during their lifetime in the atmosphere (Nicolae et al., 2013). Several EARLINET-based studies have focused on observations and characterization of smoke plumes (Alados-Arboledas et al., 2011; Ancellet et al., 2016; Ansmann et al., 2009; Müller et al., 2005; Nepomuceno Pereira et al., 2014; Ortiz-Amezcua et al., 2017; Papayannis et al., 2008; Tesche et al., 2011), demonstrating that it is a frequently encountered aerosol type over Europe. In particular, biomass burning aerosol originating from forest fires in Canada and Siberia is regularly observed between May and October (Amiridis et al., 2009; Ortiz-Amezcua et al., 2017; Sicard et al., 2012a). However, the similarities of the physical characteristics of smoke particles and continental particles result in similar optical properties, making these types difficult to distinguish. In this work, biomass burning particles are treated as a single category called smoke.
2.2.5 Volcanic ash
Volcanoes are another important source of atmospheric aerosols. Volcanic eruptions eject great amounts of material in the atmosphere (tephra), while the fraction smaller than 2 mm is labeled as volcanic ash. Most of these aerosols will settle only a few tens of kilometers away from the volcano but smaller particles can travel thousands of kilometers and affect wider areas (Kokkalis et al., 2013; Mattis et al., 2010; Navas-Guzmán et al., 2013a; Pappalardo et al., 2013; Sawamura et al., 2012; Sicard et al., 2012b). The optical properties of volcanic ash aerosols is generally similar to the one of desert dust, as was shown by Ansmann et al. (2010) and Wiegner et al. (2012) for fresh ash with particle linear depolarization ratios reaching 0.37 and lidar ratio at 532 sr of 50–65 sr. Aged volcanic particles as observed by Papayannis et al. (2012) indicate less non-sphericity with depolarization ratio values of 0.1–0.25 and lidar ratios for 355 nm within the range 55–67 sr and for 532 nm 76–89 sr. More details can be found in Mona and Marenco (2016) where the authors give a summary of how the intensive optical properties vary as a function of time. Furthermore, volcanic eruptions inject sulfur dioxide into the atmosphere thus leading to sulfate particles. Pappalardo et al. (2004a) and Wang et al. (2008) reported lidar ratios of 50–60 sr at 355 sr and backscatter-related Ångström exponent of 2.7 (355 532), signature of sulfate particles originating from Mount Etna, Italy. Moreover, CALIPSO measurements indicated low particle depolarization ratios for sulfate-rich volcanic clouds (Prata et al., 2017). Consequently, the difference in the optical properties make lidar a powerful tool for volcano monitoring. However, in this study sulfate particles and aged volcanic particles are not considered. The aerosol type relevant to the airborne ash refers to fresh ash and is denoted as volcanic ash.
As an additional consideration, the defined aerosol types presented in Sect. 2.2 may not be representative of the entire aerosol load and, apart from the dust mixtures, they do not consider other aerosol mixtures. For example, this aspect can be observed in the definition of the volcanic category where the particles have different characteristics depending on the transport pattern. The particles near the source have optical properties similar to desert dust whereas long-range-transported volcanic plumes have altered properties due to the sedimentation of the coarser particles. Therefore, it is important to further include a more exhaustive aerosol class analysis.
We developed an automated typing method, based on the work of Burton et al. (2012), but modified it in order to be compatible with the database of EARLINET. Two major steps are identified in the proposed method: the training (Sect. 3.2) and the testing (Sect. 4.1) phase. The first step consists of the following procedures. As described in Sect. 3.2.1, well characterized aerosol layers are manually separated into classes based on their physical characteristics; the set of classes constitutes the reference dataset. This procedure involves the determination of each observed aerosol layer location and the estimation of mean layer intensive optical properties. Based on this analysis, the classifying parameters that provide the required information for a better discrimination of the aerosol type are selected (Sect. 3.2.2). Next, in order to estimate how accurately a predictive model will perform, the reference dataset is split into training and validation datasets, and the application of the classifier is evaluated (Sect. 3.2.3). Section 3.2.4 describes the inference of characteristic depolarization values in the algorithm with the intention to increase the prediction of the model. For the second step, already pre-classified EARLINET data are used to assess the performance of the automatic typing procedure. Figure 4 illustrates the sequence of the proposed methodology starting from the setting of the training dataset, up to the assessment of the learning success during the testing phase.
Distance-based classification methods aim to assign an observation to a particular class based on the distance of the observation from each class center. In general, the Mahalanobis distance between an observation and the mean class in the p-dimensional space ℝp is defined as
where S is the class covariance matrix. The surfaces identified by the equation DM= const. are ellipsoids that are centered around the mean . The main characteristic of the multivariate Mahalanobis distance is that it accounts for the variance in each variable and the covariance between variables. By contrast, the Euclidean distance treats all the variables in the same way and the constant distance surfaces from a fixed point are represented by a sphere.
The Mahalanobis distance of an observation from an aerosol class is estimated, and is assigned to the aerosol class for which the distance is minimum. Two screening criteria are applied to the minimum distance following the procedure of Burton et al. (2012). The methodology uses 3 and 4 classifying parameters and the minimum accepted distance for a measurement to be labeled is 4 and 4.3, respectively. Moreover, the normalized probability of the aerosol class needs to be higher than 50 %. Otherwise, the type assignment is difficult as the measurement can be equidistant from 2 or more aerosol type classes, and possibly indicate the mixing of these aerosol types.
3.2 Training phase
In supervised learning techniques, the reference dataset is crucial to the overall predictive performance of the algorithm. Therefore, it is fundamental to use well-characterized EARLINET profiles. Namely, EARLINET aerosol classified layers from Papagiannopoulos et al. (2016a); Pappalardo et al. (2013), and Schwarz (2016) were used and will be presented below.
EARLINET observations from 2008 to 2010 were analyzed and the aerosol types were determined with respect to the source origin following a similar approach to Sect. 2.1 (Schwarz, 2016) and present the backbone of the reference dataset. Table 1 lists the classified aerosol types of the above study (644 individual aerosol layers) with respect to the aerosol types presented in Sect. 2.2; however, all these aerosol layers cannot be used given the need for the maximum optical properties available (column “only from 3β+2α”). The mixtures category includes all the mixtures of two or more aerosol species without containing polluted dust and mixed dust categories that are reported individually.
As discussed above, the requirement for 3β+2α lidar configuration pinpoints the low occurrence (see Table 1) of some aerosol types such as the clean continental, polluted dust, and dust. Furthermore, marine aerosol was not reported in the study and the volcanic layers do not reflect the volcanic ash characteristics described in Sect. 2.2. Conversely, the latter were volcanic layers found in the stratosphere and thus different from the fresh ash that we consider. In order that the aerosol classes include all the major aerosol components, the aforementioned aerosol types need to be enhanced with other observations. Therefore, we implemented EARLINET network-wide typing results already published in the literature (Papagiannopoulos et al., 2016a; Pappalardo et al., 2013) for a total of 69 layers as the reference dataset. Note that calibrated particle linear depolarization ratio profiles are not available in the selected dataset.
The type-dependent mean properties are reported in Table 2 and coincide with the typical values as of those in Sect. 2.2. However, aerosol classification is based on an interpretative analysis of the retrieved optical properties and the model simulations, and it is a qualitative method of type assignment. Thus, there is an inherent possibility of error in the determination of the true aerosol type. This error, if made, propagates into the automatic algorithm and the predicted aerosol class might deviate from the “truth” aerosol class. Specifically, dust and volcanic types present the same characteristics with Ångström exponents as low as 0, although dust lidar ratios are 58±12 and 55±7 sr for 355 nm and 532 nm, respectively, and are higher than the volcanic lidar ratios ( and sr). The Ångström exponents (i.e., κβ(355,1064), κβ(532,1064), κβ(355,532), and κα(355,532)) for mixed dust are between 0.4 and 0.7 and lidar ratio values are below 50 sr, whereas for polluted dust the Ångström exponents lie within 0.6–1.0 and lidar ratio values for 355 and 532 nm are 54±8 and 64±9 sr, respectively. This behavior reflects the mixing of dust with pollution/smoke that tends to decrease the size of the aerosol mixture and increase its absorbing capacity. Polluted continental and smoke reveal the same size characteristics with mean Ångström exponents from all the available variables around ∼1.4 and ∼1.3, respectively. The smoke mean lidar ratio values present the higher ones among the aerosol types – i.e., 81±16 and 78±11 sr for 355 and 532 nm, respectively – and the polluted continental values succeed with 69±12 and 63±13 sr for 355 and 532 nm, respectively. For clean continental, the Ångström exponents (i.e., κβ(355,1064), κβ(532,1064), κβ(355,532), and κα(355,532)) are between 1.0 and 1.7 and lidar ratios, for 355 and 532 nm, are 50±8 and 41±6 sr. This characteristic separates clean continental from polluted continental as the particles yield lower lidar ratio values. Finally, mixed marine particles are found to be relatively small in size with Ångström exponents (i.e., κβ(355,1064), κβ(532,1064), κβ(355,532), and κα(355,532)) in the range 0.8–1.0 and thus overlap with other aerosol types. The characteristic parameter that defines the mixed marine category is the lidar ratio, the values are found to be the smallest ( sr) among the aerosol types.
In the proposed method, the aerosol layers are classified in terms of the aerosol types described in Sect. 2.2. As a starting point for this study, we use 8 aerosol classes: clean continental (CC), polluted continental (PC), pure dust (D), mixed dust (MD = dust + marine), polluted dust (PD = dust + smoke and/or dust + polluted continental), mixed marine (MM), smoke (S), and volcanic (V). However, some of these 8 classes overlap consistently in the feature space. As a consequence, we exploited the combined use of overlapping aerosol types. Therefore, we merged the types that tend to reflect the same aerosol characteristics, and hence we evaluate the corresponding effects on the prediction rate of the algorithm. Two pathways were followed. First, the smoke and the polluted continental categories were grouped into the more generic type of small with high lidar ratio values. Second, all the dust-like aerosol types were merged. The different grouping categories are summarized in Table 3.
3.2.2 Classifying parameters selection
Next, we performed a sensitivity analysis to identify which classifying properties provide the adequate information to better predict the correct aerosol class. We used three aerosol intensive properties due to the lack of particle linear depolarization ratio profiles to evaluate the strength of the selected classifier to discriminate among the predefined classes. Two statistical parameters are used: the total and the partial Wilks' lambda (Wilks, 1963) that are widely used, e.g., Burton et al. (2012) and Russell et al. (2014). The total Λ statistic shows the tendency of the above set of pre-specified classes (or any subset of it) to separate. The partial Λ is calculated for each of the intensive properties separately and indicates the discriminatory power of the used intensive property. For both parameters, values range from 0 to 1. Values near 0 show high discriminatory power while values near 1 show low discriminatory power.
The lowest total Λ was found to be 0.033 for the set κβ(355,1064), , and ; whereas the partial Λ is 0.51 for , 0.17 for κβ, and 0.30 for . For this dataset, the low Λ value for κβ indicates that this variable has the most weight in the classification. The decision for the selected parameters stems solely from the lowest arithmetic value of the total Λ. Therefore, for the other groups of parameters the total Λ is equally low, ∼0.05, which indicates that a 2β+2α lidar setup could also be equally used when the algorithm is trained with κβ(355,532). With reference to the lidar ratio, the and can be used interchangeably due to the almost equal total Λ (i.e., 0.034).
For the rest of the aerosol groups reported in Table 2, the total and partial (for κβ) Λ are, respectively, 0.036 and 0.18 (7a classes), 0.041 and 0.18 (7b classes), 0.044 and 0.18 (6 classes), 0.057 and 0.20 (5 classes), and 0.070 and 0.21 (4 classes). The Λ shows good discriminatory power for each of the grouping classes, although there is a slight increase in the values as the number of classes is reduced. This behavior can be ascribed to the high variance in the combined aerosol types which makes the classification less selective.
Figure 5 shows the characteristics of the reference dataset in terms of the and κβ(355,1064) for the 8 and 4 aerosol classes that represent the maximum and minimum aerosol groupings used. The coloring corresponds to the various classes and the crosshairs indicate the standard deviation of each of the aerosol layers. The 90 % confidence ellipses are calculated using the eigenvalues and eigenvectors of the covariance matrix and define the region that contains 90 % of all the points that can be drawn from the underlying normal class distribution. The various aerosol classes tend to populate specific areas of the graph, whereas the overlap of the neighboring classes is significant, although the classes are better pinpointed as long as we merge classes with similar characteristics. However, the latter does not reflect the obtained values of the statistical parameters (total Λ increased from 0.033 for 8 classes to 0.070 for 4 classes), and, as explained above, the reference dataset very well delineates the aerosol types and by combining the neighboring types the variance increases.
3.2.3 Validation of the classifier
In order to evaluate the predictive accuracy of the automatic method, it is needed to split the initial reference dataset into a training and a validation dataset. Like this, we use the training dataset to calculate the classification functions and then submit each observation in the validation dataset to the classification function obtained from the training dataset. For this study, we make use of the leave-one-out cross validation (LOOCV) procedure, also referred to as holdout procedure or simply cross validation, which is a degenerate case of the k fold cross validation, where k is chosen as the total number of samples (Rencher, 2002). The choice of the procedure, even though computationally expensive, is used when datasets are sparse and trains the algorithm with as many observations as possible. Each measurement is separately removed from the training dataset in order to compute the classification rule, and this rule is used to classify the removed observation. The error rate is estimated as a percentage of all incorrect predictions divided by the total number of the reference dataset, and is equivalent to 1 minus accuracy. Values near 0 show high predictive performance while values near 1 show low predictive performance. For the classification options of the Table 3, the error rate, expectedly, decreases with decreasing number of aerosol classes (39 % for 8 classes, 36 % for 7a classes, 30 % for 7b classes, 28 % for 6 classes, 19 % for 5 classes, and 10 % for 4 classes). It should be mentioned that the typing in multiple classes and typing accuracy are two conflicting aspects. The choice of 8 aerosol classes appears to be sufficient to describe the major aerosol components, but ostentatious for a 3β+2α lidar configuration. Four classes, on the other hand, provide a coarse aerosol characterization and the prediction accuracy of the algorithm is expected to increase.
3.2.4 Algorithm training including particle depolarization ratio
Several studies have shown the unique information provided by depolarization measurements (Burton et al., 2014; Liu et al., 2008; Tesche et al., 2013), thus making this intensive property a robust means to discriminate the various aerosol types. Valuable typing information can also be obtained by the color ratio of the particle depolarization ratios when more depolarization channels exist (Burton et al., 2015). As already stated in Sect. 2, the majority of the stations perform depolarization measurements, and profiles are routinely delivered by SCC. However, the reference dataset does not contain depolarization information because it has been released before the assessment of the quality assurance procedures within EARLINET. Therefore, a method applicable to EARLINET data collected since 2000 is proposed in this work. We investigate the effect of adding depolarization information to the described method as the next releases of EARLINET dataset will contain quality assured particle depolarization profiles and can be used for more accurate aerosol typing. To complement the reference dataset in this context, we used general literature values for particle linear depolarization ratio at 532 nm (Table 4) in order to train the algorithm. For the clean continental type, the values ingested in the algorithm are retrieved from Burton et al. (2013) and refer to the polluted marine category. The decision for this inconsistency stems from the shortage of clean continental particle depolarization values in the literature; however, the reported values coincide with the type characteristics described in Sect. 2.2 and the values used in the CALIPSO typing scheme (Omar et al., 2009).Burton et al. (2013)Burton et al. (2013)Groß et al. (2011)Groß et al. (2016)Burton et al. (2013)Groß et al. (2013)Burton et al. (2013)Pappalardo et al. (2013)
In this case, the particle linear depolarization ratio was added to the classifying parameters. Values within the aerosol type range were randomly assigned to each sample and the Λ distribution was calculated. Total Λ is 0.004. The value of partial Λ for κβ(355,1064), , , and are 0.55, 0.34, 0.52, and 0.12, respectively. The values found for the partial Λ confirm the as the most important classifying parameter for the considered dataset. For the rest of the aerosol groups, the total and partial (for depolarization ratio) Λ are, respectively, 0.005 and 0.14 (7a classes), 0.005 and 0.12 (7b classes), 0.006 and 0.14 (6 classes), 0.040 and 0.68 (5 classes), and 0.050 and 0.69 (4 classes).
For the sake of completeness, the LOOCV method was also performed and the error rate was calculated. Figure 6 comparatively presents the training of the algorithm when depolarization information is available and when not in terms of the total, partial Λ, and the error rate of the LOOCV method. The figure highlights the strength of polarization-sensitive observations, while for the 5 and 4 classes (Fig. 6b) the particle linear depolarization ratio becomes less important (in this case the highest weight in the classification corresponds to the lidar ratio at 532 nm) due to the fact that only one dust type represents volcanic and other dust mixtures. Figure 7 presents cumulative bar plots with the median (black dots), the 25–75 percentile (box), the 5–95 percentile (whiskers) for all four classifying parameters. The figure highlights the discriminatory power of , κβ(355,1064), and , whereas the performs the worst. Furthermore, the figure depicts the discriminatory power of the classifying parameter among the dust-like aerosol classes; however, the particle depolarization ratio seems to have no power to separate the non-dust classes as discussed above.
4.1 Testing phase
As a next step, an assessment of the predictive performance of the pre-trained algorithm is made by using a testing dataset. For this, EARLINET data collected during the ACTRIS Summer 2012 intensive measurements (Granados-Muñoz et al., 2016b; Sicard et al., 2015) were chosen to test the automatic typing algorithm. The measurements took place in the period of 8 June–17 July 2012 and were dedicated to Saharan dust studies and also featured two field campaigns such as PEGASOS (Pan-European Gas-AeroSOl-climate interaction Study) and CHArMEx (Chemistry-Aerosol Mediterranean Experiment). During that period, 157 measurements were performed, out of which 42 measurements delivered 3 backscatter and 2 extinction coefficient profiles. The description of aerosol type distribution over Europe during the campaign was obtained following the procedure shown in Sect. 2.1 (Papagiannopoulos et al., 2016b). The testing dataset comprises of 47 layers, 21 of which yield depolarization ratio values. Table 5 provides the mean values of the intensive parameters for each available category in accordance with Table 2.
4.2 Application of the methodology to EARLINET data – case studies
To showcase the steps of the automatic classification, we apply it to two selected cases for the 8 classes and for the classifying parameters: , , and κβ(355,1064). For the case in Sect. 2.1, the automatic algorithm labeled the aerosol layer as dust, DM=1.2 and the normalized probability 55 %. This coincides with our findings and highlights the strength of the classification, albeit this example corresponds to a pure aerosol layer with no level of mixing with other aerosol types.
The second case refers to a more complicated aerosol scene. The Athens EARLINET station (Fig. 8) on 22 May 2014 observed an aerosol layer mostly in the height range between 1.5 and 3 km (Papayannis et al., 2016). Within this layer the mean value of backscatter-related Ångström exponent (355 1064) is 0.9±0.1. The lidar ratio presents mean values in the layer 40±7 and 39±6 sr at 355 and 532 nm, respectively. The color ratio of the lidar ratios shows a wavelength-independent layer with values of 1.1±0.2. The retrieved error corresponds to the standard deviation of the retrieved quantity calculated within the layer.
In the following, a 6-day FLEXPART backward trajectory indicates the pattern of the origin of air masses. Figure 9 shows the total column sensitivity of the particles found over the station between 1.5 and 3 km, it highlights the motion of the particles in a northeasterly direction towards the Aral Sea and Kazakhstan. This area is an active dust source due to the extreme desiccation of the lake (Ginoux et al., 2012). Therefore, the path of the air masses arriving over Athens suggests a mixture of dust and biomass burning particles, originating from the arid areas of the Aral Sea, as well as the agricultural fires in former Soviet Union countries (Papayannis et al., 2016). The automatic algorithm classified the layer as mixed dust, DM=2.5 and normalized probability 32 %, and the second closest class was clean continental, DM=3 and normalized probability 23 %. Although the class with the minimum estimated distance agrees with our investigation, the inferred type will not be taken into account. The very low probability indicates that more than one distance is beyond the accepted threshold, therefore the classes are almost equidistant. This demonstrates that the manual typing procedure can better type the aerosol layer, but also that adopted fixed thresholds are conservative, i.e., type assignment is not possible for ambiguous scenes.
4.3 Comparing the automatic classification with manual analyzed data
The performance of the algorithm with respect to the testing dataset is presented. For each of the grouping classes, as those listed in Table 3, the confusion matrices have been calculated (not shown) and the accuracy of the model is presented alongside the recall (R) and precision (P). The confusion matrix describes the performance of the classifier on a testing dataset for which the typing is already known. Recall of an aerosol group is defined as the number of correctly predicted cases over the number of correctly plus the number of incorrectly predicted cases. Recall can be thought as the model's ability to predict the specific aerosol class. Precision of an aerosol group is defined as the number of correctly predicted cases over the number of correctly predicted cases plus the number of incorrectly predicted cases that belong to this aerosol class. In other words, given the prediction of a specific class, what is the probability of being correct?
In Fig. 10, the bar plot comparatively shows the predictive accuracy of the algorithm when compared to manually analyzed data for the different aerosol classes in both the cases in which the depolarization information is available (in orange) or not (in brown). Without depolarization ratio information, the accuracy of the model increases with decreasing number of classes. The lowest value was obtained for 8 classes (59 %) and the highest for 4 classes (90 %). With depolarization ratio information, the accuracy for 8 classes equals to 79 % and exceeds the 80 % for the rest of the aerosol classes. When comparing the accuracy of the model with and without depolarization ratio, it appears to be significantly higher until 6 classes, where the discrepancy diminishes further (<10 %) and becomes smaller for 4 classes. In general, it becomes evident that the particle linear depolarization ratio increases the ability for correctly predicting the aerosol type. Given the high accuracy, a 3β+2α configuration showed that 6 aerosol classes, as well as 5 and 4, can provide a robust classification. Instead, the training of the classification with depolarization measurements enhances the predictability strength and can provide finer aerosol classification (for 8 classes, accuracy ∼70 %).
Table 6 summarizes the results when using as classifying parameters: , , and κβ(355,1064), with respect to recall and precision and offers a better insight into the performance of each aerosol type. Next to the number of classes, between parentheses, the number of aerosol layers that passed the screening criteria as those described in Sect. 3.1 is provided. It is, thus, worth noting that the numbers increase when the aerosol types are combined. The mixed marine and clean continental aerosol types yield high recall and precision (values >80 %) throughout the different aerosol classes, highlighting the ability of the classifier to correctly label them. The aerosol types that performed worse are the smoke and polluted continental aerosol types due to the similarities in the intensive optical properties. However, when combining them into a single aerosol class (see 7b, 6, and 4 classes), precision and recall increase significantly. Given the noticeable signature of dust particles, precision is high, whereas the recall is 30 % and this can be assigned to the lack of depolarization measurements. Similarly, recall increases as soon as volcanic, mixed, and polluted dust are included in the same all-dust category (see 7a, 6, 5, and 4 classes). Note that mixed dust and polluted dust aerosol types are not reported in the tables due to the fact that they are not present in Table 5 and these parameters cannot be evaluated. The frequency of detection for MD (PD) is 18 % (4 %) for 8 classes, 15 % (3 %) for 7b classes, 17 % (3 %) for 7a classes, and 15 % (3 %) when 3 classifying parameters are used. The algorithm predicted MD-only dust cases with around 45 sr and over 1. The PD case refers to a PC case with κβ(355,1064) lower than 1. The frequency of detection for MD is 0 % for all classes when depolarization ratio is added. The frequency for PD is 17 % for 8 classes, 13 % for 7b classes, 17 % for 7a classes, and 13 % for 6 classes. The wrongly classified cases have depolarization ratio around 20 %.
Table 7 is similar to Table 6 and reports the recall and precision when depolarization information is available. Clean continental aerosol, again, yields high recall and precision for all the different aerosol groups. Polluted continental performed the worst and, expectedly, showed the same behavior as before when compared with smoke in a single type. Alternately, dust is precisely identified for all the aerosol classes. This result indicates that depolarization measurements facilitate the correct dust typing. It is noteworthy that although the findings are promising the test dataset is limited and does not cover all the aerosol classes.
The characterization of the vertical aerosol distribution is needed for accurate radiative-transfer modeling. Automatic procedures to classify aerosols objectively and within near-real timescales are employed. An automatic classification procedure based only on EARLINET data was presented. Here, we modified an automatic algorithm to satisfy the network's requirements and needs. A Wilks' lambda analysis was performed on EARLINET data and the three best performing classifying parameters were the lidar ratio at 532 nm, the color ratio of the lidar ratios at 355 and 532 nm, and the backscatter-related 355-to-1064 nm Ångström exponent. Nevertheless, the other intensive parameters using the available wavelengths can be equally used as the analysis showed similar values. Furthermore, the number of aerosol classes has been investigated for a maximum of 8 and minimum 4. Prior to evaluating the performance of the algorithm, the LOOCV procedure was performed on the reference dataset and the error rate decreased monotonically from 39 % to 10 % with decreasing number of aerosol classes. The prediction of the automatic classification showed positive results when compared against already classified EARLINET data. In particular, the positive learning success for 8 (59 %), 7 (69 % for 7a and 7b classes), 6 (76 %), 5 (76 %), and 4 (90 %) classes indicates that the fewer aerosol classes (6, 5, and 4 classes) provide a confident but, nonetheless, coarser classification. To be more precise, the high accuracy (76 %) coupled with the low error rate of the cross validation (28 %) for 6 classes offers a good starting point for a classification with a 3β+2α lidar configuration.
Besides, the training of the algorithm with literature depolarization ratio values decreased the error rate of the LOOCV from 24 % (8 classes) to 4 % (4 classes). Furthermore, the predictive accuracy increased and remained for all the aerosol classes around 80 % (for 8 classes: 79 %, for 7a: 81 %, for 7b: 83 %, for 6: 81 %, for 5: 85 %, and for 4: 80 %). Therefore, this finding suggests that the algorithm in this case can be used for finer aerosol classification and also delineates the discriminatory power of depolarization ratio. Specifically, 7 aerosol classes (either D+V, MD, PD, CC, MM, PC, S or D, V, MD, PD, CC, MM, PC+S) seem to be adequate to provide reasonable typing results. However, the obtained results refer to a small testing dataset that consists of pure aerosol types and underestimates the aerosol mixtures of the classification.
The presented automatic algorithm is only based on EARLINET data and is set to accommodate EARLINET measurements covering as much of its measurement record as possible. Specifically, Raman lidar systems with 3β+2α and 2β+2α configurations with and without particle depolarization ratio can be used for the aerosol classification. The manageability of the algorithm regarding the reference dataset, the number of the aerosol classes, and the classifying parameters make the method easily adaptable and handled by individual users. The training dataset can be easily enlarged with high-quality typing data coming from a multitude of EARLINET stations and a longer time record. Moreover, new classifying parameters, such as particle linear depolarization ratio at more wavelengths and aerosol extinction coefficient in the infrared, can be easily added as the observing capacity increases.
The use of the method network-wide will homogenize and standardize the aerosol typing towards a new EARLINET product. The implementation of the method into the SCC will create a complete automatic lidar analysis, i.e. from the retrieval of optical properties to aerosol classification. Furthermore, an intercomparison of the developed method against methods which also make use of aerosol optical property modeling could improve from one side the optimization of aerosol property models and from the other side the tuning of aerosol types and reference dataset. This method, even if developed on the basis of EARLINET and its variable instrumental capability, can be applied to all of the aerosol lidar systems as those that are part of GALION as well as to future lidar-based satellite missions (e.g., the Earth Cloud, Aerosol and Radiation Explorer, EarthCARE, satellite mission). In future, a combination of the few sophisticated EARLINET-type lidars and extended networks of automated single-wavelength backscatter lidars (Wiegner et al., 2014) might be beneficial with aerosol typing provided at “anchor stations”, and the spatial extent of the layers can be provided by the continuous observations of the ceilometers. This will also offer a unique dataset for evaluation of models.
The data used in this paper are freely available from the EARLINET (https://www.earlinet.org/index.php?id=earlinet_homepage, last access: 18 October 2018) and ACTRIS (http://www.actris.eu/, last access: 15 October 2018) web sites. A part of them is published to the CERA database (EARLINET publishing group 2000–2010, 2014a, b, c, d) and accessible using the CERA data portal (https://cera-www.dkrz.de/WDCC/ui/cerasearch/, last access: 19 October 2018). The full dataset up to the end of 2015 is currently in press on the CERA database (EARLINET publishing group 2000–2015, 2018a, b, c, d,, e).
NP conducted the research process and developed the typing algorithm. NP developed the code with support from PGC. NP and LM conducted the statistical analysis and performed the comparison with already pretyped EARLINET data. AA, GD, IB, LM, and VA supervised the project. All authors contributed to the EARLINET data curation and preprocessing. Furthermore, they contributed to the analysis of the results and to the writing of the manuscript.
The authors declare that they have no conflict of interest.
This article is part of the special issue “EARLINET aerosol profiling: contributions to atmospheric and climate research”. It is not associated with a conference.
The financial support for EARLINET in the ACTRIS Research Infrastructure Project by the European Union's Horizon 2020
research and innovation program under grant agreement no. 654169 in the Seventh Framework Programme (FP7/2007–2013)
is gratefully acknowledged. The research leading to these results has received funding from the European Union's Horizon
2020 research and innovation program under grant agreement no. 602014 (project ECARS – East European Centre for
Atmospheric Remote Sensing) and from the European Union's Horizon 2020 research program for societal challenges – smart,
green and integrated transport under grant agreement no. 723986 (project EUNADICS-AV – European Natural Disaster Coordination
and Information System for Aviation). Daniele Bortoli acknowledges the European Union through the European Regional Development
Fund, included in the COMPETE 2020 (Operational Program Competitiveness and Internationalization) through the ICT project
(UID/GEO/04683/2013) with reference POCI 01-0145-FEDER 007690. Panagiotis Kokkalis acknowledges funding of the Greek State
Scholarship Foundation: IKY. Part of this project is implemented within the framework of the Action “Reinforcement of Postdoctoral Researchers”
of the Operational Program “Human Resource Development, Education and Lifelong Learning”, and is
co-financed by the European Social Fund (ESF) and the Greek government (NSRF, 2014–2020).
Edited by: Matthias Tesche
Reviewed by: Sharon Burton and one anonymous referee
Alados-Arboledas, L., Müller, D., Guerrero-Rascado, J. L., Navas-Guzmán, F., Pérez-Ramírez, D., and Olmo, F. J.: Optical and microphysical properties of fresh biomass burning aerosol retrieved by Raman lidar, and star- and sun-photometry, Geophys. Res. Lett., 38, L01807, https://doi.org/10.1029/2010GL045999, 2011. a, b
Amiridis, V., Balis, D. S., Giannakaki, E., Stohl, A., Kazadzis, S., Koukouli, M. E., and Zanis, P.: Optical characteristics of biomass burning aerosols over Southeastern Europe determined from UV-Raman lidar measurements, Atmos. Chem. Phys., 9, 2431–2440, https://doi.org/10.5194/acp-9-2431-2009, 2009. a, b
Ancellet, G., Pelon, J., Totems, J., Chazette, P., Bazureau, A., Sicard, M., Di Iorio, T., Dulac, F., and Mallet, M.: Long-range transport and mixing of aerosol sources during the 2013 North American biomass burning episode: analysis of multiple lidar observations in the western Mediterranean basin, Atmos. Chem. Phys., 16, 4725–4742, https://doi.org/10.5194/acp-16-4725-2016, 2016. a
Ansmann, A., Wagner, F., Althausen, D., Müller, D., Herber, A., and Wandinger, U.: European pollution outbreaks during ACE 2: Lofted aerosol plumes observed with Raman lidar at the Portuguese coast, J. Geophys. Res., 106, D18, https://doi.org/10.1029/2000JD000091, 2001. a
Ansmann, A., Bösenberg, J., Chaikovsky, A., Comeròn, A., Eckhardt, S., Eixmann, R., Freudenthaler, V., Ginoux, P., Komguem, L., Linné, H., Márquez, M. A. L., Matthias, V., Mattis, I., Mitev, V., Müller, D., Music, S., Nickovic, S., Pelon, J., Sauvage, L., Sobolewsky, P., Srivastava, M., Stohl, A., Torres, O., Vaughan, G., Wandinger, U., and Wiegner, M.: Long-range transport of Saharan dust to northern Europe: The 11–16 October 2001 outbreak observed with EARLINET, J. Geophys. Res., 108, D24, https://doi.org/10.1029/2003JD003757, 2003. a
Ansmann, A., Baars, H., Tesche, M., Müller, D., Althausen, D., Engelmann, R., Pauliquevis, T., and Artaxo, P.: Dust and smoke transport from Africa to South America: Lidar profiling over Cape Verde and the Amazon rainforest, Geophys. Res. Lett., 36, L11802, https://doi.org/10.1029/2009GL037923, 2009. a
Ansmann, A., Tesche, M., Groß, S., Freudenthaler, V., Seifert, P., Hiebsch, A., Schmidt, J., Wandinger, U., Mattis, I., Müller, D., and Wiegner, M.: The 16 April 2010 major volcanic ash plume over central Europe: EARLINET lidar and AERONET photometer observations at Leipzig and Munich, Germany, Geophys. Res. Lett., 37, L13810, https://doi.org/10.1029/2010GL043809, 2010. a
Baars, H., Ansmann, A., Althausen, D., Engelmann, R., Heese, B., Müller, D., Artaxo, P., Paixao, M., Pauliquevis, M., and Souza, R.: Aerosol profiling with lidar in the Amazon Basin during the wet and dry season, J. Geophys. Res, 117, D21201, https://doi.org/10.1029/2012JD018338, 2012. a
Baars, H., Kanitz, T., Engelmann, R., Althausen, D., Heese, B., Komppula, M., Preißler, J., Tesche, M., Ansmann, A., Wandinger, U., Lim, J.-H., Ahn, J. Y., Stachlewska, I. S., Amiridis, V., Marinou, E., Seifert, P., Hofer, J., Skupin, A., Schneider, F., Bohlmann, S., Foth, A., Bley, S., Pfüller, A., Giannakaki, E., Lihavainen, H., Viisanen, Y., Hooda, R. K., Pereira, S. N., Bortoli, D., Wagner, F., Mattis, I., Janicka, L., Markowicz, K. M., Achtert, P., Artaxo, P., Pauliquevis, T., Souza, R. A. F., Sharma, V. P., van Zyl, P. G., Beukes, J. P., Sun, J., Rohwer, E. G., Deng, R., Mamouri, R.-E., and Zamorano, F.: An overview of the first decade of PollyNET: an emerging network of automated Raman-polarization lidars for continuous aerosol profiling, Atmos. Chem. Phys., 16, 5111–5137, https://doi.org/10.5194/acp-16-5111-2016, 2016. a
Baklanov, A., Schlünzen, K., Suppan, P., Baldasano, J., Brunner, D., Aksoyoglu, S., Carmichael, G., Douros, J., Flemming, J., Forkel, R., Galmarini, S., Gauss, M., Grell, G., Hirtl, M., Joffre, S., Jorba, O., Kaas, E., Kaasik, M., Kallos, G., Kong, X., Korsholm, U., Kurganskiy, A., Kushta, J., Lohmann, U., Mahura, A., Manders-Groot, A., Maurizi, A., Moussiopoulos, N., Rao, S. T., Savage, N., Seigneur, C., Sokhi, R. S., Solazzo, E., Solomos, S., Sørensen, B., Tsegas, G., Vignati, E., Vogel, B., and Zhang, Y.: Online coupled regional meteorology chemistry models in Europe: current status and prospects, Atmos. Chem. Phys., 14, 317–398, https://doi.org/10.5194/acp-14-317-2014, 2014. a
Balis, D., Amiridis, V., Nickovic, S., Papayannis, A., and Zerefos, C.: Raman lidar and sunphotometric measurements of aerosol optical properties over Thessaloniki, Greece during a biomass burning episode, Atmos. Environ., 31, 4529–4538, https://doi.org/10.1016/S1352-2310(03)00581-8, 2003. a
Binietoglou, I., Basart, S., Alados-Arboledas, L., Amiridis, V., Argyrouli, A., Baars, H., Baldasano, J. M., Balis, D., Belegante, L., Bravo-Aranda, J. A., Burlizzi, P., Carrasco, V., Chaikovsky, A., Comerón, A., D'Amico, G., Filioglou, M., Granados-Muñoz, M. J., Guerrero-Rascado, J. L., Ilic, L., Kokkalis, P., Maurizi, A., Mona, L., Monti, F., Muñoz-Porcar, C., Nicolae, D., Papayannis, A., Pappalardo, G., Pejanovic, G., Pereira, S. N., Perrone, M. R., Pietruczuk, A., Posyniak, M., Rocadenbosch, F., Rodríguez-Gómez, A., Sicard, M., Siomos, N., Szkop, A., Terradellas, E., Tsekeri, A., Vukovic, A., Wandinger, U., and Wagner, J.: A methodology for investigating dust model performance using synergistic EARLINET/AERONET dust concentration retrievals, Atmos. Meas. Tech., 8, 3577–3600, https://doi.org/10.5194/amt-8-3577-2015, 2015. a
Bovchaliuk, V., Goloub, P., Podvin, T., Veselovskii, I., Tanre, D., Chaikovsky, A., Dubovik, O., Mortier, A., Lopatin, A., Korenskiy, M., and Victori, S.: Comparison of aerosol properties retrieved using GARRLiC, LIRIC, and Raman algorithms applied to multi-wavelength lidar and sun/sky-photometer data, Atmos. Meas. Tech., 9, 3391–3405, https://doi.org/10.5194/amt-9-3391-2016, 2016. a
Bravo-Aranda, J. A., Titos, G., Granados-Muñoz, M., Guerrero-Rascado, J., Navas-Guzmán, F., Valenzuela, A., Lyamani, H., Olmo, F., Andrey, J., and Alados-Arboledas, L.: Study of mineral dust entrainment in the planetary boundary layer by lidar depolarisation technique, Tellus B, 67, 26180, https://doi.org/10.3402/tellusb.v67.26180, 2015. a, b
Burton, S. P., Ferrare, R. A., Hostetler, C. A., Hair, J. W., Rogers, R. R., Obland, M. D., Butler, C. F., Cook, A. L., Harper, D. B., and Froyd, K. D.: Aerosol classification using airborne High Spectral Resolution Lidar measurements – methodology and examples, Atmos. Meas. Tech., 5, 73–98, https://doi.org/10.5194/amt-5-73-2012, 2012. a, b, c, d, e, f, g, h, i
Burton, S. P., Ferrare, R. A., Vaughan, M. A., Omar, A. H., Rogers, R. R., Hostetler, C. A., and Hair, J. W.: Aerosol classification from airborne HSRL and comparisons with the CALIPSO vertical feature mask, Atmos. Meas. Tech., 6, 1397–1412, https://doi.org/10.5194/amt-6-1397-2013, 2013. a, b, c, d, e, f
Burton, S. P., Vaughan, M. A., Ferrare, R. A., and Hostetler, C. A.: Separating mixtures of aerosol types in airborne High Spectral Resolution Lidar data, Atmos. Meas. Tech., 7, 419–436, https://doi.org/10.5194/amt-7-419-2014, 2014. a, b
Burton, S. P., Hair, J. W., Kahnert, M., Ferrare, R. A., Hostetler, C. A., Cook, A. L., Harper, D. B., Berkoff, T. A., Seaman, S. T., Collins, J. E., Fenn, M. A., and Rogers, R. R.: Observations of the spectral dependence of linear particle depolarization ratio of aerosols using NASA Langley airborne High Spectral Resolution Lidar, Atmos. Chem. Phys., 15, 13453–13473, https://doi.org/10.5194/acp-15-13453-2015, 2015. a
Cattrall, C., Reagan, J., Thome, K., and Dubovik, O.: Variability of aerosol and spectral lidar and backscatter and extinction ratios of key aerosol types derived from selected Aerosol Robotic Network locations, J. Geophys. Res., 110, D10S11, https://doi.org/10.1029/2004JD005124, 2005. a
Chaikovsky, A., Dubovik, O., Holben, B., Bril, A., Goloub, P., Tanré, D., Pappalardo, G., Wandinger, U., Chaikovskaya, L., Denisov, S., Grudo, J., Lopatin, A., Karol, Y., Lapyonok, T., Amiridis, V., Ansmann, A., Apituley, A., Allados-Arboledas, L., Binietoglou, I., Boselli, A., D'Amico, G., Freudenthaler, V., Giles, D., Granados-Muñoz, M. J., Kokkalis, P., Nicolae, D., Oshchepkov, S., Papayannis, A., Perrone, M. R., Pietruczuk, A., Rocadenbosch, F., Sicard, M., Slutsker, I., Talianu, C., De Tomasi, F., Tsekeri, A., Wagner, J., and Wang, X.: Lidar-Radiometer Inversion Code (LIRIC) for the retrieval of vertical aerosol properties from combined lidar/radiometer data: development and distribution in EARLINET, Atmos. Meas. Tech., 9, 1181–1205, https://doi.org/10.5194/amt-9-1181-2016, 2016. a
Córdoba-Jabonero, C., Sorribas, M., Guerrero-Rascado, J. L., Adame, J. A., Hernández, Y., Lyamani, H., Cachorro, V., Gil, M., Alados-Arboledas, L., Cuevas, E., and de la Morena, B.: Synergetic monitoring of Saharan dust plumes and potential impact on surface: a case study of dust transport from Canary Islands to Iberian Peninsula, Atmos. Chem. Phys., 11, 3067–3091, https://doi.org/10.5194/acp-11-3067-2011, 2011. a
D'Amico, G., Amodeo, A., Baars, H., Binietoglou, I., Freudenthaler, V., Mattis, I., Wandinger, U., and Pappalardo, G.: EARLINET Single Calculus Chain – overview on methodology and strategy, Atmos. Meas. Tech., 8, 4891–4916, https://doi.org/10.5194/amt-8-4891-2015, 2015. a
Dawson, K. W., Meskhidze, N., Josset, D., and Gassó, S.: Spaceborne observations of the lidar ratio of marine aerosols, Atmos. Chem. Phys., 15, 3241–3255, https://doi.org/10.5194/acp-15-3241-2015, 2015. a
EARLINET publishing group 2000–2010: EARLINET Correlative Observations for CALIPSO (2006–2010), World Data Center for Climate (WDCC), Hamburg, Germany, https://doi.org/10.1594/WDCC/EN_Calipso_2006-2010, 2014a.
EARLINET publishing group 2000–2010: EARLINET observations related to Saharan Dust events (2000–2010), World Data Center for Climate (WDCC), Hamburg, Germany, https://doi.org/10.1594/WDCC/EARLINET_SaharanDust_2000-2010, 2014b.
EARLINET publishing group 2000–2010: EARLINET observations related to volcanic eruptions (2000–2010), World Data Center for Climate (WDCC), Hamburg, Germany, https://doi.org/10.1594/WDCC/EN_VolcanicEruption_2000-2010, 2014c.
EARLINET publishing group 2000–2010: EARLINET climatology (2000–2010), World Data Center for Climate (WDCC), Hamburg, Germany, https://doi.org/10.1594/WDCC/EN_Climatology_2000-2010, 2014d.
EARLINET publishing group 2000–2015: EARLINET All 2000–2015, World Data Center for Climate (WDCC), in press, 2018a.
EARLINET publishing group 2000–2015: EARLINET Calipso 2000–2015, World Data Center for Climate (WDCC), in press, 2018b.
EARLINET publishing group 2000–2015: EARLINET Saharan Dust 2000–2015, World Data Center for Climate (WDCC), in press, 2018c.
EARLINET publishing group 2000–2015: EARLINET Climatology 2000–2015, World Data Center for Climate (WDCC), in press, 2018d.
EARLINET publishing group 2000–2015: EARLINET Volcanic Eruption 2000–2015, World Data Center for Climate (WDCC), in press, 2018e.
Freudenthaler, V., Esselborn, M., Wiegner, M., Heese, B., Tesche, M., Ansmann, A., Müller, D., Althausen, D., Wirth, M., Fix, A., Ehret, G., Knippertz, P., Toledano, C., Gasteiger, J., Garhammer, M., and Seefeldner, M.: Depolarization ratio profiling at several wavelengths in pure Saharan dust during SAMUM 2006, Tellus B, 61, 165–179, https://doi.org/10.1111/j.1600-0889.2008.00396.x, 2009. a
Giannakaki, E., Balis, D. S., Amiridis, V., and Zerefos, C.: Optical properties of different aerosol types: seven years of combined Raman-elastic backscatter lidar measurements in Thessaloniki, Greece, Atmos. Meas. Tech., 3, 569–578, https://doi.org/10.5194/amt-3-569-2010, 2010. a, b
Giannakaki, E., van Zyl, P. G., Müller, D., Balis, D., and Komppula, M.: Optical and microphysical characterization of aerosol layers over South Africa by means of multi-wavelength depolarization and Raman lidar measurements, Atmos. Chem. Phys., 16, 8109–8123, https://doi.org/10.5194/acp-16-8109-2016, 2016. a
Ginoux, P., Chin, M., Tegen, I., Prospero, J. M., Holben, B., Dubovik, O., and Lin, S.-J.: Sources and distributions of dust aerosols simulated with the GOCART model, J. Geophys. Res., 20, 20255–20274, https://doi.org/10.1029/2000JD000053, 2001. a
Ginoux, P., Prospero, J. M., Gill, T. E., Hsu, N. C., and Zhao, M.: Global-scale attribution of anthropogenic and natural dust sources and their emission rates based on MODIS Deep Blue aerosol products, Rev. Geophys., 50, RG3005, https://doi.org/10.1029/2012RG000388, 2012. a
Granados-Muñoz, M. J., Bravo-Aranda, J. A., Baumgardner, D., Guerrero-Rascado, J. L., Pérez-Ramírez, D., Navas-Guzmán, F., Veselovskii, I., Lyamani, H., Valenzuela, A., Olmo, F. J., Titos, G., Andrey, J., Chaikovsky, A., Dubovik, O., Gil-Ojeda, M., and Alados-Arboledas, L.: A comparative study of aerosol microphysical properties retrieved from ground-based remote sensing and aircraft in situ measurements during a Saharan dust event, Atmos. Meas. Tech., 9, 1113–1133, https://doi.org/10.5194/amt-9-1113-2016, 2016a. a
Granados-Muñoz, M. J., Navas-Guzmán, F., Guerrero-Rascado, J. L., Bravo-Aranda, J. A., Binietoglou, I., Pereira, S. N., Basart, S., Baldasano, J. M., Belegante, L., Chaikovsky, A., Comerón, A., D'Amico, G., Dubovik, O., Ilic, L., Kokkalis, P., Muñoz-Porcar, C., Nickovic, S., Nicolae, D., Olmo, F. J., Papayannis, A., Pappalardo, G., Rodríguez, A., Schepanski, K., Sicard, M., Vukovic, A., Wandinger, U., Dulac, F., and Alados-Arboledas, L.: Profiling of aerosol microphysical properties at several EARLINET/AERONET sites during the July 2012 ChArMEx/EMEP campaign, Atmos. Chem. Phys., 16, 7043–7066, https://doi.org/10.5194/acp-16-7043-2016, 2016b. a
Groß, S., Tesche, M., Freudenthaler, V., Toledano, C., Wiegner, M., Althausen, D., and Seefeldner, M.: Characterization of Saharan dust, marine aerosols and mixtures of biomass-burning aerosols and dust by means of multi-wavelength depolarization and Raman lidar measurements during SAMUM 2, Tellus B, 63, 706–724, https://doi.org/10.3402/tellusb.v63i4.16369, 2011. a, b, c
Groß, S., Esselborn, M., Weinzierl, B., Wirth, M., Fix, A., and Petzold, A.: Aerosol classification by airborne high spectral resolution lidar observations, Atmos. Chem. Phys., 13, 2487–2505, https://doi.org/10.5194/acp-13-2487-2013, 2013. a, b
Groß, S., Gasteiger, J., Freudenthaler, V., Müller, T., Sauer, D., Toledano, C., and Ansmann, A.: Saharan dust contribution to the Caribbean summertime boundary layer – a lidar study during SALTRACE, Atmos. Chem. Phys., 16, 11535–11546, https://doi.org/10.5194/acp-16-11535-2016, 2016. a
Guerrero-Rascado, J. L., Ruiz, B., and Alados-Arboledas, L.: Multi-spectral Lidar characterization of the vertical structure of Saharan dust aerosol over southern Spain, Atmos. Environ., 42, 2668–2681, https://doi.org/10.1016/j.atmosenv.2007.12.062, 2008. a
Guerrero-Rascado, J. L., Olmo, F. J., Avilés-Rodríguez, I., Navas-Guzmán, F., Pérez-Ramírez, D., Lyamani, H., and Alados Arboledas, L.: Extreme Saharan dust event over the southern Iberian Peninsula in september 2007: active and passive remote sensing from surface and satellite, Atmos. Chem. Phys., 9, 8453–8469, https://doi.org/10.5194/acp-9-8453-2009, 2009. a
Hamill, P., Giordano, M., Ward, C., Giles, D., and Holben, B.: An AERONET-based aerosol classification using the Mahalanobis distance, Atmos. Environ., 140, 213–233, https://doi.org/10.1016/j.atmosenv.2016.06.002, 2016. a
Heese, B., Althausen, D., Baars, H., Bohlmann, S., and Deng, R.: Aerosol Properties over Southeastern China from Multi-Wavelength Raman and Depolarization Lidar Measurements, EPJ Web of Conferences, 119, 23018, https://doi.org/10.1051/epjconf/201611923018, 2016. a
Holben, B., Eck, T., Slutsker, I., Tanré, D., Buis, J., Setzer, A., Vermote, E., Reagan, J., Kaufman, Y., Nakajima, T., Lavenu, F., Jankowiak, I., and Smirnov, A.: AERONET—A Federated Instrument Network and Data Archive for Aerosol Characterization, Remote Sens. Environ., 66, 0034–4257, https://doi.org/10.1016/S0034-4257(98)00031-5, 1998. a
Iarlori, M., Madonna, F., Rizi, V., Trickl, T., and Amodeo, A.: Effective resolution concepts for lidar observations, Atmos. Meas. Tech., 8, 5157–5176, https://doi.org/10.5194/amt-8-5157-2015, 2015. a
Kim, M.-H., Kim, S.-W., Yoon, S.-C., and Omar, A. H.: Comparison of aerosol optical depth between CALIOP and MODIS-Aqua for CALIOP aerosol subtypes over the ocean, J. Geophys. Res.-Atmos., 118, 13,241–13,252, https://doi.org/10.1002/2013JD019527, 2013. a
Kokkalis, P., Papayannis, A., Amiridis, V., Mamouri, R. E., Veselovskii, I., Kolgotin, A., Tsaknakis, G., Kristiansen, N. I., Stohl, A., and Mona, L.: Optical, microphysical, mass and geometrical properties of aged volcanic particles observed over Athens, Greece, during the Eyjafjallajökull eruption in April 2010 through synergy of Raman lidar and sunphotometer measurements, Atmos. Chem. Phys., 13, 9303–9320, https://doi.org/10.5194/acp-13-9303-2013, 2013. a
Liu, D., Wang, Z., Liu, Z., Winker, D., and Trepte, C.: A height resolved global view of dust aerosols from the first year CALIPSO lidar measurements, J. Geophys. Res., 113, D16214, https://doi.org/10.1029/2007JD009776, 2008. a, b
Madonna, F., Amato, F., Vande Hey, J., and Pappalardo, G.: Ceilometer aerosol profiling versus Raman lidar in the frame of the INTERACT campaign of ACTRIS, Atmos. Meas. Tech., 8, 2207–2223, https://doi.org/10.5194/amt-8-2207-2015, 2015. a
Mahalanobis, P. C.: On the generalized distance in statistics, in: Proceedings of the National Institute of Science of India, 49–55, 1936. a
Mahowald, N., Albani, S., Kok, J. F., Engelstaeder, S., Scanza, R., Ward, D. S., and Flanner, M. G.: The size distribution of desert dust aerosols and its impact on the Earth system, Aeolian Res., 15, 53–71, https://doi.org/10.1016/j.aeolia.2013.09.002, 2014. a
Mamouri, R. E., Amiridis, V., Papayannis, A., Giannakaki, E., Tsaknakis, G., and Balis, D. S.: Validation of CALIPSO space-borne-derived attenuated backscatter coefficient profiles using a ground-based lidar in Athens, Greece, Atmos. Meas. Tech., 2, 513–522, https://doi.org/10.5194/amt-2-513-2009, 2009. a
Mamouri, R. E., Ansmann, A., Nisantzi, A., Kokkalis, P., Schwarz, A., and Hadjimitsis, D.: Low Arabian dust extinction-to-backscatter ratio, Geophys. Res. Lett., 40, 4762–4766, https://doi.org/10.1002/grl.50898, 2013. a
Mattis, I., Siefert, P., Müller, D., Tesche, M., Hiebsch, A., Kanitz, T., Schmidt, J., Finger, F., Wandinger, U., and Ansmann, A.: Volcanic aerosol layers observed with multiwavelength Raman lidar over central Europe in 2008–2009, J. Geophys. Res.-Atmos., 115, D00L04, https://doi.org/10.1029/2009JD013472, 2010. a
Mona, L. and Marenco, F.: Volcanic Ash: Hazard Observation, chap. Lidar Observations of Volcanic Particles, Elsevier, 161–173, 2016. a
Mona, L., Amodeo, A., Pandolfi, M., and Pappalardo, G.: Saharan dust intrusions in the Mediterranean area: Three years of Raman lidar measurements, J. Geophys. Res.-Atmos., 111, D16203, https://doi.org/10.1029/2005JD006569, 2006. a
Mona, L., Pappalardo, G., Amodeo, A., D'Amico, G., Madonna, F., Boselli, A., Giunta, A., Russo, F., and Cuomo, V.: One year of CNR-IMAA multi-wavelength Raman lidar measurements in coincidence with CALIPSO overpasses: Level 1 products comparison, Atmos. Chem. Phys., 9, 7213–7228, https://doi.org/10.5194/acp-9-7213-2009, 2009. a
Mona, L., Amodeo, A., D'Amico, G., Giunta, A., Madonna, F., and Pappalardo, G.: Multi-wavelength Raman lidar observations of the Eyjafjallajökull volcanic cloud over Potenza, southern Italy, Atmos. Chem. Phys., 12, 2229–2244, https://doi.org/10.5194/acp-12-2229-2012, 2012. 2012a. a
Mona, L., Liu, Z., Müller, D., Omar, A., Papayannis, A., Sugimoto, N., Pappalardo, G., and Vaughan, M.: Measurements for Desert Dust Characterization: An Overview, Adv. Meteorol., 2012, 356265, https://doi.org/10.1155/2012/356265, 2012b. a
Mona, L., Papagiannopoulos, N., Basart, S., Baldasano, J., Binietoglou, I., Cornacchia, C., and Pappalardo, G.: EARLINET dust observations vs. BSC-DREAM8b modeled profiles: 12-year-long systematic comparison at Potenza, Italy, Atmos. Chem. Phys., 14, 8781–8793, https://doi.org/10.5194/acp-14-8781-2014, 2014. a, b, c
Müller, D., Mattis, I., Ansmann, A., Wehner, B., Althausen, D., Wandinger, U., and Dubovik, O.: Closure study on optical and microphysical properties of a mixed urban and Arctic haze air mass observed with Raman lidar and Sun photometer, J. Geophys. Res.-Atmos., 109, D13206, https://doi.org/10.1029/2003JD004200, 2004. a
Müller, D., Mattis, I., Wandinger, U., Ansmann, A., Althausen, D., and Stohl, A.: Raman lidar observations of aged Siberian and Canadian forest fire smoke in the free troposphere over Germany in 2003: Microphysical particle characterization, J. Geophys. Res., 110, D17201, https://doi.org/10.1029/2004JD005756, 2005. a
Müller, D., Ansmann, A., Mattis, I., Tesche, M., Wandinger, U., Althausen, D., and Pisani, G.: Aerosol-type-dependent lidar ratios observed with Raman lidar, J. Geophys. Res., 112, D16202, https://doi.org/10.1029/2006JD008292, 2007a. a, b, c, d
Müller, D., Mattis, I., Ansmann, A., Wandinger, U., Ritter, C., and Kaiser, D.: Multiwavelength Raman lidar observations of particle growth during long-range transport of forest-fire smoke in the free troposphere, Geophys. Res. Lett., 34, L05803, https://doi.org/10.1029/2006GL027936, 2007b. a
Müller, D., Heinold, B., Tesche, M., Tegen, I., Althausen, D., Alados-Arboledas, L., Amiridis, V., Amodeo, A., Ansmann, A., Balis, D., Comeron, A., D'Amico, G., Gerasopoulos, E., Guerrero-Rascado, J. L., Freudenthaler, V., Giannakaki, E., Heese, B., Iarlori, M., Knippertz, P., Mamouri, R. E., Mona, L., Papayannis, A., Pappalardo, G., Perrone, R.-M., Pisani, G., Rizi, V., Sicard, M., Spinelli, N., Tafuro, A., and Wiegner, M.: EARLINET observations of the 14–22-May long-range dust transport event during SAMUM 2006: validation of results from dust transport modelling, Tellus B, 61, 325–339, https://doi.org/10.1111/j.1600-0889.2008.00400.x, 2009. a
Navas-Guzmán, F., Müller, D., Bravo-Aranda, J. A., Guerrero-Rascado, J. L., Granados-Muñoz, M. J., Pérez-Ramírez, D., Olmo, F. J., and Alados-Arboledas, L.: Eruption of the Eyjafjallajökull Volcano in spring 2010: Multiwavelength Raman lidar measurements of sulphate particles in the lower troposphere, J. Geophys. Res.-Atmos., 118, 1804–1813, https://doi.org/10.1002/jgrd.50116, 2013a. a
Navas-Guzmán, N., Bravo-Aranda, J. A., Guerrero-Rascado, J. L., Granados-Muñoz, M. J., and Alados-Arboledas, L.: Statistical analysis of aerosol optical properties retrieved by Raman lidar over Southeastern Spain, Tellus B, 65, 21234, https://doi.org/10.3402/tellusb.v65i0.21234, 2013b. a
Nepomuceno Pereira, S., Preißler, J., Guerrero-Rascado, J. L., Silva, A. M., and Wagner, F.: Forest Fire Smoke Layers Observed in the Free Troposphere over Portugal with a Multiwavelength Raman Lidar: Optical and Microphysical Properties, Scientific World Journal, 2014, 421838, https://doi.org/10.1155/2014/421838, 2014. a, b
Nicolae, D., Nemuc, A., Müller, D., Talianu, C., Vasilescu, J., Belegante, L., and Kolgotin, A.: Characterization of fresh and aged biomass burning events using multiwavelength Raman lidar and mass spectrometry, J. Geophys. Res.-Atmos., 118, 2956–2965, https://doi.org/10.1002/jgrd.50324, 2013. a, b
Nisantzi, A., Mamouri, R. E., Ansmann, A., Schuster, G. L., and Hadjimitsis, D. G.: Middle East versus Saharan dust extinction-to-backscatter ratios, Atmos. Chem. Phys., 15, 7071–7084, https://doi.org/10.5194/acp-15-7071-2015, 2015. a
Omar, A., Winker, D., Kittaka, C., Vaughan, M., Liu, Z., Hu, X., Trepte, C., Rogers, R., Ferrare, R., Lee, K., Kuehn, R., and Hostetler, C.: The CALIPSO Automated Aerosol Classification and Lidar Ratio Selection Algorithm, J. Atmos. Ocean. Tech., 26, 1994–2014, https://doi.org/10.1175/2009JTECHA1231.1, 2009. a, b, c
Ortiz-Amezcua, P., Guerrero-Rascado, J. L., Granados-Muñoz, M. J., Benavent-Oltra, J. A., Böckmann, C., Samaras, S., Stachlewska, I. S., Janicka, L., Baars, H., Bohlmann, S., and Alados-Arboledas, L.: Microphysical characterization of long-range transported biomass burning particles from North America at three EARLINET stations, Atmos. Chem. Phys., 17, 5931–5946, https://doi.org/10.5194/acp-17-5931-2017, 2017. a, b
Papagiannopoulos, N., Mona, L., Alados-Arboledas, L., Amiridis, V., Baars, H., Binietoglou, I., Bortoli, D., D'Amico, G., Giunta, A., Guerrero-Rascado, J. L., Schwarz, A., Pereira, S., Spinelli, N., Wandinger, U., Wang, X., and Pappalardo, G.: CALIPSO climatological products: evaluation and suggestions from EARLINET, Atmos. Chem. Phys., 16, 2341–2357, https://doi.org/10.5194/acp-16-2341-2016, 2016a. a, b, c, d, e, f
Papagiannopoulos, N., Mona, L., and Pappalardo, G.: Aerosol classification using EARLINET measurements for an intensive observational period, vol. 18, European Geosciences Union, General Assembly, 2016b. a
Papayannis, A., Amiridis, V., Mona, L., Tsaknakis, G., Balis, D., Bösenberg, J., Chaikovski, A., De Tomasi, F., Grigorov, I., Mattis, I., Mitev, V., Müller, D., Nickovic, S., Pérez, C., Pietruczuk, A., Pisani, G., Ravetta, F., Rizi, V., Sicard, M., Trickl, T., Wiegner, M., Gerding, M., Mamouri, R. E., D'Amico, G., and Pappalardo, G.: Systematic lidar observations of Saharan dust over Europe in the frame of EARLINET (2000–2002), J. Geophys. Res., 113, D10204, https://doi.org/10.1029/2007JD009028, 2008. a, b, c
Papayannis, A., Mamouri, R. E., Amiridis, V., Giannakaki, E., Veselovskii, I., Kokkalis, P., Tsaknakis, G., Balis, D., Kristiansen, N., Stohl, A., Korenskiy, M., Allakhverdiev, K., Huseyinoglu, M., and Baykara, T.: Optical properties and vertical extension of aged ash layers over the Eastern Mediterranean as observed by Raman lidars during the Eyjafjallajökull eruption in May 2010, Atmos. Environ., 48, 56–65, https://doi.org/10.1016/j.atmosenv.2011.08.037, 2012. a
Papayannis, A., Nicolae, D., Kokkalis, P., Binietoglou, I., Talianu, C., Belegante, L., Tsaknakis, G., Cazacu, M., Vetres, I., and Ilic, L.: Optical, size and mass properties of mixed type aerosols in Greece and Romania as observed by synergy of lidar and sunphotometers in combination with model simulations: A case study, Sci. Total Environ., 500–501, 277–297, https://doi.org/10.1016/j.scitotenv.2014.08.101, 2014. a
Papayannis, A., Argyrouli, A., Müller, D., Tsaknakis, G., Kokkalis, P., Binietoglou, I., Kazadzis, S., Solomos, S., and Amiridis, V.: Tropospheric Vertical Profiles of Aerosol Optical, Microphysical and Concentration Properties in the Frame of the Hygra-CD Campaign (Athens, Greece 2014): A Case Study of Long-Range Transport of Mixed Aerosols, EPJ Web of Conferences, 119, 23016, https://doi.org/10.1051/epjconf/201611923016, 2016. a, b
Pappalardo, G., Amodeo, A., Mona, L., Pandolfi, M., Pergola, N., and Cuomo, V.: Raman lidar observations of aerosol emitted during the 2002 Etna eruption, Geophys. Res. Lett., 31, L05120, https://doi.org/10.1029/2003GL019073, 2004a. a
Pappalardo, G., Amodeo, A., Pandolfi, M., Wandinger, U., Ansmann, A., Bösenberg, J., Matthias, V., Amiridis, V., De Tomasi, F., Frioud, M., Iarlori, M., Komguem, L., Papayannis, A., Rocadenbosch, F., and Wang, X.: Aerosol lidar intercomparison in the framework of the EARLINET project. 3. Ramanlidar algorithm for aerosol extinction, backscatter, and lidar ratio, Appl. Opt., 43, 5370–5385, https://doi.org/10.1364/AO.43.005370, 2004b. a, b
Pappalardo, G., Mona, L., D'Amico, G., Wandinger, U., Adam, M., Amodeo, A., Ansmann, A., Apituley, A., Alados Arboledas, L., Balis, D., Boselli, A., Bravo-Aranda, J. A., Chaikovsky, A., Comeron, A., Cuesta, J., De Tomasi, F., Freudenthaler, V., Gausa, M., Giannakaki, E., Giehl, H., Giunta, A., Grigorov, I., Groß, S., Haeffelin, M., Hiebsch, A., Iarlori, M., Lange, D., Linné, H., Madonna, F., Mattis, I., Mamouri, R.-E., McAuliffe, M. A. P., Mitev, V., Molero, F., Navas-Guzman, F., Nicolae, D., Papayannis, A., Perrone, M. R., Pietras, C., Pietruczuk, A., Pisani, G., Preißler, J., Pujadas, M., Rizi, V., Ruth, A. A., Schmidt, J., Schnell, F., Seifert, P., Serikov, I., Sicard, M., Simeonov, V., Spinelli, N., Stebel, K., Tesche, M., Trickl, T., Wang, X., Wagner, F., Wiegner, M., and Wilson, K. M.: Four-dimensional distribution of the 2010 Eyjafjallajökull volcanic cloud over Europe observed by EARLINET, Atmos. Chem. Phys., 13, 4429–4450, https://doi.org/10.5194/acp-13-4429-2013, 2013. a, b, c, d, e
Pappalardo, G., Amodeo, A., Apituley, A., Comeron, A., Freudenthaler, V., Linné, H., Ansmann, A., Bösenberg, J., D'Amico, G., Mattis, I., Mona, L., Wandinger, U., Amiridis, V., Alados-Arboledas, L., Nicolae, D., and Wiegner, M.: EARLINET: towards an advanced sustainable European aerosol lidar network, Atmos. Meas. Tech., 7, 2389–2409, https://doi.org/10.5194/amt-7-2389-2014, 2014. a, b, c, d
Prata, F., Woodhouse, M., Huppert, H. E., Prata, A., Thordarson, T., and Carn, S.: Atmospheric processes affecting the separation of volcanic ash and SO2 in volcanic eruptions: inferences from the May 2011 Grímsvötn eruption, Atmos. Chem. Phys., 17, 10709–10732, https://doi.org/10.5194/acp-17-10709-2017, 2017. a
Preißler, J., Wagner, F., Pereira, S. N., and Guerrero-Rascado, J. L.: Multi-instrumental observation of an exceptionally strong Saharan dust outbreak over Portugal, J. Geophys. Res.-Atmos., 116, D24204, https://doi.org/10.1029/2011JD016527, 2011. a
Preißler, J., Wagner, F., Guerrero-Rascado, J. L., and Silva, A. M.: Two years of free-tropospheric aerosol layers observed over Portugal by lidar, J. Geophys. Res.-Atmos., 118, 3676–3686, https://doi.org/10.1002/jgrd.50350, 2013. a
Rencher, A.: Methods of Multivariate Analysis, Wiley-Interscience, 2002. a
Rogers, R. R., Vaughan, M. A., Hostetler, C. A., Burton, S. P., Ferrare, R. A., Young, S. A., Hair, J. W., Obland, M. D., Harper, D. B., Cook, A. L., and Winker, D. M.: Looking through the haze: evaluating the CALIPSO level 2 aerosol optical depth using airborne high spectral resolution lidar data, Atmos. Meas. Tech., 7, 4317–4340, https://doi.org/10.5194/amt-7-4317-2014, 2014. a
Russell, P. B., Kacenelenbogen, M., Livingston, J. M., Hasekamp, O. P., Burton., S. P., Schuster, G. L., Johnson, M. S., Knobelspiesse, K. D., Redemann, J., Ramachandran, S., and Holben, B.: A multiparameter aerosol classification method and its application to retrievals from spaceborne polarimetry, J. Geophys. Res.-Atmos., 119, 9838–9863, https://doi.org/10.1002/2013JD021411, 2014. a, b, c
Sawamura, P., Vernier, J. P., Barnes, J. E., Berkoff, T. E., Welton, E. J., Alados-Arboledas, L., Navas-Guzmán, F., Pappalardo, G., Mona, L., Madonna, F., Lange, D., Sicard, M., Godin-Beekmann, S., Payen, G., Wang, Z., Hu, S., Tripathi, S. N., Cordoba-Jabonero, C., and Hoff, R. M.: Stratospheric AOD after the 2011 eruption of Nabro volcano measured by lidars over the Northern Hemisphere, Environ. Res. Lett., 7, 034013, https://doi.org/10.1088/1748-9326/7/3/034013, 2012. a
Schuster, G. L., Vaughan, M., MacDonnell, D., Su, W., Winker, D., Dubovik, O., Lapyonok, T., and Trepte, C.: Comparison of CALIPSO aerosol optical depth retrievals to AERONET measurements, and a climatology for the lidar ratio of dust, Atmos. Chem. Phys., 12, 7431–7452, https://doi.org/10.5194/acp-12-7431-2012, 2012. a
Schwarz, A.: Aerosol typing over Europe and its benefits for the CALIPSO and EarthCARE missions – statistical analysis based on multiwavelength aerosol lidar measurements from ground-based EARLINET stations and comparison to spaceborne CALIPSO data, PhD thesis, University of Leipzig, 2016. a, b, c, d
Sicard, M., Guerrero-Rascado, J. L., Navas-Guzmán, F., Preißler, J., Molero, F., Tomás, S., Bravo-Aranda, J. A., Comerón, A., Rocadenbosch, F., Wagner, F., Pujadas, M., and Alados-Arboledas, L.: Monitoring of the Eyjafjallajökull volcanic aerosol plume over the Iberian Peninsula by means of four EARLINET lidar stations, Atmos. Chem. Phys., 12, 3115–3130, https://doi.org/10.5194/acp-12-3115-2012, 2012a. a
Sicard, M., Mallet, M. García-Vizcaíno, D., Comerón, A., Rocadenbosch, F., Dubuisson, P., and Muñoz Porcar, C.: Intense dust and extremely fresh biomass burning outbreak in Barcelona, Spain: characterization of their optical properties and estimation of their direct radiative forcing, Environ. Res. Lett., 7, 034016, https://doi.org/10.1088/1748-9326/7/3/034016, 2012b. a
Sicard, M., D'Amico, G., Comerón, A., Mona, L., Alados-Arboledas, L., Amodeo, A., Baars, H., Baldasano, J. M., Belegante, L., Binietoglou, I., Bravo-Aranda, J. A., Fernández, A. J., Fréville, P., García-Vizcaíno, D., Giunta, A., Granados-Muñoz, M. J., Guerrero-Rascado, J. L., Hadjimitsis, D., Haefele, A., Hervo, M., Iarlori, M., Kokkalis, P., Lange, D., Mamouri, R. E., Mattis, I., Molero, F., Montoux, N., Muñoz, A., Muñoz Porcar, C., Navas-Guzmán, F., Nicolae, D., Nisantzi, A., Papagiannopoulos, N., Papayannis, A., Pereira, S., Preißler, J., Pujadas, M., Rizi, V., Rocadenbosch, F., Sellegri, K., Simeonov, V., Tsaknakis, G., Wagner, F., and Pappalardo, G.: EARLINET: potential operationality of a research network, Atmos. Meas. Tech., 8, 4587–4613, https://doi.org/10.5194/amt-8-4587-2015, 2015. a
Stohl, A., Forster, C., Frank, A., Seibert, P., and Wotawa, G.: Technical note: The Lagrangian particle dispersion model FLEXPART version 6.2, Atmos. Chem. Phys., 5, 2461–2474, https://doi.org/10.5194/acp-5-2461-2005, 2005. a
Tanré, D., Bréon, F. M., Deuzé, J. L., Dubovik, O., Ducos, F., François, P., Goloub, P., Herman, M., Lifermann, A., and Waquet, F.: Remote sensing of aerosols by using polarized, directional and spectral measurements within the A-Train: the PARASOL mission, Atmos. Meas. Tech., 4, 1383–1395, https://doi.org/10.5194/amt-4-1383-2011, 2011. a, b
Tesche, M., Müller, D., Groß, S., Ansmann, A., Althausen, D., Freudenthaler, V., Weinzierl, B., Veira, A., and Petzold, A.: Optical and microphysical properties of smoke over Cape Verde inferred from multiwavelength lidar measurements, Tellus B, 63, 677–694, https://doi.org/10.1111/j.1600-0889.2011.00549.x, 2011. a
Tesche, M., Wandinger, U., Ansmann, A., Althausen, D., Müller, D., and Omar, A. H.: Ground-based validation of CALIPSO observations of dust and smoke in the Cape Verde region, J. Geophys. Res.-Atmos., 118, 2889–2902, https://doi.org/10.1002/jgrd.50248, 2013. a, b, c
Valenzuela, A., Olmo, F. J., Lyamani, H., Antón, M., Quirantes, A., and Alados-Arboledas, L.: Classification of aerosol radiative properties during African desert dust intrusions over southeastern Spain by sector origins and cluster analysis, J. Geophys. Res.-Atmos., 117, D06214, https://doi.org/10.1029/2011JD016885, 2012. a
Valenzuela, A., Olmo, F. J., Lyamani, H., Granados-Muñoz, M. J., Antón, M., Guerrero-Rascado, J. L., Quirantes, A., Toledano, C., Perez-Ramírez, D., and Alados-Arboledas, L.: Aerosol transport over the western Mediterranean basin: Evidence of the contribution of fine particles to desert dust plumes over Alborán Island, J. Geophys. Res.-Atmos., 119, 14028–14044, https://doi.org/10.1002/2014JD022044, 2014. a
Veselovskii, I., Dubovik, O., Kolgotin, A., Lapyonok, T., Di Girolamo, P., Summa, D., Whiteman, D. N., Mishchenko, M., and Tanré, D.: Application of randomly oriented spheroids for retrieval of dust particle parameters from multiwavelength lidar measurements, J. Geophys. Res., 115, D21203, https://doi.org/10.1029/2010JD014139, 2010. a
Wandinger, U., Baars, H., Engelmann, R., Hünerbein, A., Horn, S., Kanitz, T., Donovan, D., van Zadelhoff, G.-J., Daou, D., Fischer, J., von Bismarck, J., Filipitsch, F., Docter, N., Eisinger, M., Lajas, D., and Wehr, T.: HETEAC: The Aerosol Classification Model for EarthCARE, EPJ Web of Conferences, 119, 01004, https://doi.org/10.1051/epjconf/201611901004, 2016. a
Wang, X., Boselli, A., D'Avino, L., Pisani, G., Spinelli, N., Amodeo, A., Chaikovsky, A., Wiegner, M., Nickovic, S., Papayannis, A., Perrone, M., Rizi, V., Sauvage, L., and Stohl, A.: Volcanic dust characterization by EARLINET during Etna's eruptions in 2001–2002, Atmos. Environ., 42, 893–905, https://doi.org/10.1016/j.atmosenv.2007.10.020, 2008. a
Wiegner, M., Groß, S., Freudenthaler, V., Schnell, F., and Gasteiger, J.: The May/June 2008 Saharan dust event over Munich: Intensive aerosol parameters from lidar measurements, J. Geophys. Res., 116, D23123, https://doi.org/10.1029/2011JD016619, 2011. a, b
Wiegner, M., Gasteiger, J., Groß, S., Schnell, F., Freudenthaler, V., and Forkel, R.: Characterization of the Eyjafjallajökull ash-plume: Potential of lidar remote sensing, Phys. Chem. Earth, 45–46, 79–86, https://doi.org/10.1016/j.pce.2011.01.006, 2012. a
Wiegner, M., Madonna, F., Binietoglou, I., Forkel, R., Gasteiger, J., Geiß, A., Pappalardo, G., Schäfer, K., and Thomas, W.: What is the benefit of ceilometers for aerosol remote sensing? An answer from EARLINET, Atmos. Meas. Tech., 7, 1979–1997, https://doi.org/10.5194/amt-7-1979-2014, 2014. a
Wilks, S.: Multivariate statistical outliers, Sankhya: The Indian Journal of Statistics, 4, 407–426, 1963. a