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Near Real-Time Monitoring of Significant Sea Wave Height through Microseism Recordings: Analysis of an Exceptional Sea Storm Event

Microseisms are used to estimate significant sea wave heights (Hs) in different parts of the world and also during extreme events (e.g., typhoons and hurricanes), as they are generated by the effect of sea waves on the sea bottom and are strictly related to the wave height. On 29 October 2018, an exceptional sea storm event (the Adrian storm) occurred in the Ligurian Sea (NW Mediterranean Sea), producing severe damage to coastal constructions and infrastructures. However, the microseism measured at seismic stations located near the coast did not show equivalent high energy, thus resulting in a severe underestimation of the Hs predicted. In the present study, the Adrian storm was compared to other sea storms that have occurred in the Ligurian Sea in recent decades. The aim of this paper is to statistically examine the distinctive peculiarities of the Adrian storm in order to find new parameters to insert in the empirical models used in the procedure recently implemented for monitoring of Hs through microseism recordings in the Ligurian Sea, improving the effectiveness in Hs estimates in cases of extreme events that do not produce high-energy microseisms. The results show that the additional parameters to be taken into account into the predictive model are the atmospheric pressure gradient and the wind intensity. A correction term is finally proposed and applied to the predictive model to significantly reduce the Hs underestimation.


Introduction
Sea wave height is one of the most relevant sea parameters to the monitoring and protection of coastal areas and to mitigation of marine risk associated with the occurrence of strong sea storm events. The study of the wave characteristics, such as wave period, wavelength, significant wave height, and return period of sea storm, is essential for the design of offshore and coastal infrastructures, such as oil platforms, wind farms, breakwaters and artificial reefs, and for their conservation [1,2]. Due to the impact of sea waves on economic activities, a great effort has been made in the last decades to develop methods for direct sea wave height measurements using wave buoys. Nonetheless, wave buoys are typically very expensive and problematic, especially regarding their installation and maintenance. Moreover, they usually provide discontinuous data (e.g., due to temporary damage) with poor spatial resolution (due to the low density of monitoring stations in sea areas). Most common alternative methods are based on numerical modelling [3,4], remote sensing [5][6][7], coastal radars [8,9], and microseism recordings [10][11][12][13][14][15].
Microseisms are produced by the pressure exerted by sea waves on the sea floor and propagate in the surface layer of seabed for hundreds of kilometres thanks to their Figure 1. Location of the Imperia seismic station (IMI; large green square), the other Regional Seismic network of northwestern Italy (RSNI) seismic stations located near the Ligurian coast (small green squares) and the two buoys (Capo Mele-Italy and Cote d'Azur-France; blue and orange triangles, respectively) considered in this study. The tide gauge station of Imperia Porto Maurizio and the weather station of the Seismic and Meteorological Observatory of Imperia are located in the city of Imperia. Red line shows the coastal area affected by damages.
Despite these characteristics, the microseism recorded at several seismic stations of the RSNI network located along the Ligurian coast and in the hinterland did not show equivalent high energy, with a consequent underestimation of the sea wave heights derived by Ferretti et al.'s [15] procedure. Thus, the Adrian storm offered the rare opportunity of analysing the characteristics of the microseism produced by this type of event and, therefore, to make a first attempt to understand why the use of microseism recordings could fail to estimate the Hs during extreme events. The aim of this study is to firstly identify and examine the distinctive peculiarities of the Adrian storm in order to improve future Hs estimations in the Ligurian Sea using additional informative parameters derived from other marine and weather observations (i.e., storm surge and atmospheric pressure). Since the Adrian storm has shown that predictive models based only on microseism data could not be completely effective for monitoring Hs during extreme storms, an empirical correction term is proposed here. Such a correction term has been applied to the predictive models proposed by Ferretti et al. [15], allowing for a significant reduction in the underestimation of the Hs observed during the Adrian storm.

Study Area and General Features of the Adrian Storm
The study area (Figure 1) is the coastal part of the Ligurian Sea in the western Mediterranean Sea. The Ligurian Sea has a narrow continental shelf (with an average distance from the coast of 10 km) with steep slope incised by submarine canyons located along the main waterways of the region [30]. The Ligurian coast (about 330 km long) has steep arch- Figure 1. Location of the Imperia seismic station (IMI; large green square), the other Regional Seismic network of northwestern Italy (RSNI) seismic stations located near the Ligurian coast (small green squares) and the two buoys (Capo Mele-Italy and Cote d'Azur-France; blue and orange triangles, respectively) considered in this study. The tide gauge station of Imperia Porto Maurizio and the weather station of the Seismic and Meteorological Observatory of Imperia are located in the city of Imperia. Red line shows the coastal area affected by damages.
Despite these characteristics, the microseism recorded at several seismic stations of the RSNI network located along the Ligurian coast and in the hinterland did not show equivalent high energy, with a consequent underestimation of the sea wave heights derived by Ferretti et al.'s [15] procedure. Thus, the Adrian storm offered the rare opportunity of analysing the characteristics of the microseism produced by this type of event and, therefore, to make a first attempt to understand why the use of microseism recordings could fail to estimate the H s during extreme events. The aim of this study is to firstly identify and examine the distinctive peculiarities of the Adrian storm in order to improve future H s estimations in the Ligurian Sea using additional informative parameters derived from other marine and weather observations (i.e., storm surge and atmospheric pressure). Since the Adrian storm has shown that predictive models based only on microseism data could not be completely effective for monitoring H s during extreme storms, an empirical correction term is proposed here. Such a correction term has been applied to the predictive models proposed by Ferretti et al. [15], allowing for a significant reduction in the underestimation of the H s observed during the Adrian storm.

Study Area and General Features of the Adrian Storm
The study area (Figure 1) is the coastal part of the Ligurian Sea in the western Mediterranean Sea. The Ligurian Sea has a narrow continental shelf (with an average distance from the coast of 10 km) with steep slope incised by submarine canyons located along the main waterways of the region [30]. The Ligurian coast (about 330 km long) has steep arch-shaped mountains interspersed with wide valleys that control and channel the air movements. In the Ligurian Sea, the most frequent and significant sea storms are generated by winds from SE (Sirocco), SW (Libeccio), and NW (winds coming from the Gulf of Lion in cyclonic rotation; "short" Libeccio). These winds are usually related to perturbations from the Atlantic Ocean and Gulf of Lion, which carry strong, humid, and warm winds. These morphological and meteorological characteristics imply frequent events of heavy rainfall and rough sea and make the Ligurian Sea one of the most active areas of cyclogenesis in Europe [31][32][33][34][35], with strong and very rapid changes in weather conditions. In the past, the most destructive sea storms occurred in 1898 and 1955 (sea state > 7 of the Douglas Sea Scale), causing severe damage to the structures and vessels in the Port of Genoa [36].
On 27 October 2018, a deep trough between the Arctic Ocean and North African coasts was established on the Iberian Peninsula, and then moved eastwards and hit the whole Italian peninsula, causing an intense SW flow in the mid-troposphere and an SE flow in the lower layers. On 29 October, the cyclogenesis on the Gulf of Lion has deepened and the flow on the eastern edge of the cut-off was intense and from S, with a consequent recall of hot and humid air of African origin in the central Europe. In the Ligurian Sea, in the early hours of 29 October, a V-shape structure developed. It was characterised by a strong, self-regenerating convective activity with a high vertical development, which stationed on the basin for several hours. The convective activity was characterised by the continuous formation of new storm cells produced by the downdraft in the opposite direction to the main flow, which therefore caused the persistence of thunderstorm phenomena on the basin. This structure was generated by several factors: the strong flows from SW at high altitude due to the tiling on the western Mediterranean Sea, the presence of a high quantity of water vapour, a high convective available potential energy, and high values of equivalent potential temperature.
In the afternoon of 29 October, the entire Italian territory was affected by the passage of a cold front coming from W, along which a squall line (a very intense thunderstorm line) developed, accompanied by intense precipitation and numerous lightning strikes along the cold front line. This complex scenario brought very low-pressure values (≈978 hPa; Figure 2) which, combined with strong S winds, caused a storm surge phenomenon (i.e., a strong and rapid rise of the sea surface elevation) that contributed to increase the effect of the sea storm. At its maximum intensity, the storm was characterised by wind gusts over 150 km h −1 , H s greater than 6 m, maximum wave height of 10 m, and peak wave period (T p ) of 11 s. This value of T p is very rare in a closed sea such as the Mediterranean Sea. The development of the sea wave can be divided into two phases: a first phase during which the wave direction spanned between 120 • and 160 • (from 04:00 to 21:00 of 29 October), followed by a second phase during which the wave direction was mainly around 200 • . In the Ligurian Sea, this shift in wave direction is very common during storm. In fact, the interaction of the synoptic flows with the complex mountain topography causes the development of deep orographic lows, usually very dynamic, that, in turn, cause very rapid transition of winds from SE to SW, with intensity strongly enhanced by coastal effects [37].
Since the night of 29 October, the perturbed system moved NE, leaving space for a gradual ascent of the geopotential field on 30 October [27,38,39].

Weather and Sea Data
In order to examine the distinctive peculiarities of the Adrian storm to improve the procedure proposed by Ferretti et al. [15] for monitoring Hs from microseism recordings during strong marine events, four significant sea storms that occurred in the Ligurian Sea in 2008 and between 2012 and 2018 were analysed and compared to the recent Adrian storm. Specifically, the considered the events occurred on 30 October 2008 (the sea storm already considered by Ferretti et al. [13]), 28 October 2012, 10 November 2013, and 25 December 2013 (three sea storms occurred in the period 2012-2018, for which continuous seismic recordings were available for analysis). All the sea storms considered were generated by strong southerly winds and showed Hs > 3 m. Data of sea wave characteristics, sea level, and atmospheric conditions were collected in order to highlight differences among these sea storms in terms of sea wave parameters and in terms of microseism characteristics.
For each selected sea storm, hourly Hs (in m), maximum individual sea wave height (Hmax), wave direction and Tp were collected from buoys installed in the Ligurian Sea. In particular, for the event that occurred in 2008, we analysed data measured by the Côte d'Azur buoy (latitude 43.38° N, longitude 7.83° E, depth of anchoring 2300 m), which belongs to the Meteo-France network (www.shom.fr (accessed on 19 November 2020)). Concerning the 2012, 2013, and 2018 events, data measured by the buoy of Capo Mele (latitude-43.92° N, longitude-8.18° E, depth of anchoring-90 m), which is managed by the Ligurian Environmental Protection Agency (http://servizi-meteoliguria.arpal.gov.it/boacapomele.html (accessed on 19 November 2020)), were considered. Sea

Weather and Sea Data
In order to examine the distinctive peculiarities of the Adrian storm to improve the procedure proposed by Ferretti et al. [15] for monitoring H s from microseism recordings during strong marine events, four significant sea storms that occurred in the Ligurian Sea in 2008 and between 2012 and 2018 were analysed and compared to the recent Adrian storm. Specifically, the considered the events occurred on 30 October 2008 (the sea storm already considered by Ferretti et al. [13]), 28 October 2012, 10 November 2013, and 25 December 2013 (three sea storms occurred in the period 2012-2018, for which continuous seismic recordings were available for analysis). All the sea storms considered were generated by strong southerly winds and showed H s > 3 m. Data of sea wave characteristics, sea level, and atmospheric conditions were collected in order to highlight differences among these sea storms in terms of sea wave parameters and in terms of microseism characteristics.
For each selected sea storm, hourly H s (in m), maximum individual sea wave height (H max ), wave direction and T p were collected from buoys installed in the Ligurian Sea. In particular, for the event that occurred in 2008, we analysed data measured by the Côte d'Azur buoy (latitude 43.38 • N, longitude 7.83 • E, depth of anchoring 2300 m), which belongs to the Meteo-France network (www.shom.fr (accessed on 19 November 2020)). Concerning the 2012, 2013, and 2018 events, data measured by the buoy of Capo Mele (latitude-43.92 • N, longitude-8.18 • E, depth of anchoring-90 m), which is managed by the Ligurian Environmental Protection Agency (http://servizi-meteoliguria.arpal.gov. it/boacapomele.html (accessed on 19 November 2020)), were considered. Sea level (m), atmospheric pressure (hPa), and relative humidity (%) data measured during the five sea storms were collected from the tide gauge station of Imperia Porto Maurizio (part of the National Tide-gauge Network; www.mareografico.it (accessed on 19 November 2020)) located 13 km far off the Capo Mele buoy.
Wind direction ( • N) and velocity (m s −1 ) were obtained from the Seismic and Meteorological Observatory of Imperia (managed by the Municipality of Imperia; http://www. cartografiarl.regione.liguria.it/SiraQualMeteo/script/PubAccessoDatiMeteo.asp (accessed on 19 November 2020)) located 14 km SW off the Capo Mele buoy. The two measuring stations and the buoy of Capo Mele are not colocated, but given the relatively small distance between them, the effect of this distance on the results of the analyses is assumed negligible given the noninstantaneous inertia of the system (i.e., the sea).
All data were sampled hourly. Starting from the water level records (provided by the station of Imperia Porto Maurizio), the storm surge series were computed for each of the investigated events. First, the tidal contribution was predicted through the Tidal Model Driver (TMD) package for MATLAB software (TMD software v. 2.05, [40]) provided by the Earth & Space Research (https://www.esr.org/research/polar-tide-models/tmd-software/ (accessed on 19 November 2020)). Then, the predicted tides were taken off the total water level, leading to the tidal residual. When tides are relevant, it is advisable to split the tidal residual in two contribution, i.e., a low-frequency and a high-frequency signal, corresponding to the meteorological-induced surge and the interaction between the tides and the surge [41]. However, given that in the Ligurian Sea the tidal oscillation accounts to a few centimetres at most over the total water level, we assumed the tidal residual was driven only by the storm surge.
In addition to the previous data, the distance between the Capo Mele buoy and the minimum of atmospheric pressure was estimated (in km) for each considered event. This distance can be useful to explain the oscillation of the microseism amplitude [25], and therefore to explain the relation between this latter and the H s generated during the storms.
Finally, a statistical analysis was carried out in order to find the most influential atmospheric parameters during the Adrian storm. Specifically, the Redundancy Analysis (RDA) [42] multivariate technique was applied to explain the linear relationship between the explanatory variables, which are the atmospheric forcing (wind velocity, atmospheric pressure and pressure gradient), and the response variables, which are the sea responses to such forcing (storm surge, H s , and T p ). For each storm and for each parameter of interest, the analyses were carried out on ordered time series of 25 hourly samples around the time of the H max . Details of the method used for the RDA analysis are described in Cutroneo et al. [43]. The RDA was performed using the Brodgar software (Highland Statistics Ltd., v. 2.7.5, 2017).

Microseismic Data
In this study, we present the results of the analysis of the microseism recorded at the IMI station (Figure 1), which is the RSNI station closest to the Capo Mele buoy. For all storms, only the vertical component of the signals was considered.
Following Ferretti et al. [13][14][15], microseismic data were processed according to the following steps: The spectral characteristics of the microseism were thus determined through Fourier amplitude spectra and spectrograms.

Results
Following the methods described above, the sea wave parameters (derived from measuring buoys and microseisms) and atmospheric pressure data were analysed for the five sea storms considered in this study. Figure 3 compares H s measured by the buoys (red lines) and those obtained using microseism recordings according to the procedure of Ferretti et al. [15] (green lines). Except for the Adrian storm ( Figure 3e) and for the initial phase of the November 2013 event (Figure 3c), H s measured by the buoy and H s estimated by microseism were similar with differences that, on average, are lower than 0.2 m. During the Adrian storm, the Capo Mele buoy measured H s greater than 6 m, which are almost twice the values estimated using the microseism.   Figure 4 shows the characteristics of the microseism recorded at the IMI station during the five sea storms in terms of the Fourier amplitude spectra for different hourly signal windows and spectrograms. As already shown by Ferretti et al. [13], the microseism associated with sea storms in the Ligurian Sea is dominated by frequencies of around 0.2-0.3 Hz, whereas the microseism controlled by frequencies lower than 0.15 Hz is associated with storms located in the Atlantic Ocean. For all sea storms considered in the present study, the largest microseism amplitude concentrates around 0.2 Hz. During the 2008, 2012, and December 2013 events, the spectral amplitude at 0.2 Hz exceeded, on average,  Figure 4 shows the characteristics of the microseism recorded at the IMI station during the five sea storms in terms of the Fourier amplitude spectra for different hourly signal windows and spectrograms. As already shown by Ferretti et al. [13], the microseism associated with sea storms in the Ligurian Sea is dominated by frequencies of around 0.2-0.3 Hz, whereas the microseism controlled by frequencies lower than 0.15 Hz is associated with storms located in the Atlantic Ocean. For all sea storms considered in the present study, the largest microseism amplitude concentrates around 0.2 Hz. During the 2008, 2012, and December 2013 events, the spectral amplitude at 0.2 Hz exceeded, on average, the value of 6 × 10 −7 m s −1 , reaching values greater than 8 × 10 −7 m s −1 . On November 2013, during the sea storm that generated the lowest H max (Table 1), the spectral amplitude of microseism slightly exceeded 4× 10 −7 m s −1 and a significant underestimation of the H s provided by microseism (up to 1.5 m) was observed during the initial phase of the storm (Figure 3c). During the Adrian storm, the spectral amplitude of the microseism at 0.2 Hz remained nearly below 2 × 10 −7 m s −1 .   It is noteworthy that the H s values estimated using the procedure of Ferretti et al. [15] and reported in Figure 3 have been computed considering the microseism recordings provided by the RSNI seismic stations located along the Ligurian coast (the H s values is calculated by averaging over the nine stations shown in Figure 1). The underestimation of the H s provided by the procedure of Ferretti et al. [15] is due to the low energy of the microseism recorded along the Ligurian coast during the Adrian storm. In fact, all recordings provided by the other RSNI seismic stations located along the Ligurian coast ( Figure 1) show microseism characteristics as similar as those observed at the IMI station. Moreover, the H s values predicted by microseism show a significant underestimation at all target sites considered in Ferretti et al.'s [15] procedure and located along the Ligurian coast. The predicted H s values never exceed 3.5 m at any target site while indirect observations (such as damages to coastal infrastructures) indicate sea waves with much greater heights along the entire Ligurian coast (see previous paragraphs).

Microseism Analysis
Similar considerations on the microseism energy can be observed from the spectrograms (Figure 4). For the events occurred in 2008, 2012, and 2013, the spectral amplitude values for the frequencies dominating microseism recordings reached values greater than −65 dB, whereas during the Adrian storm they rarely exceeded −75 dB. Table 1 summarises the main weather and sea parameters measured during the five sea storms considered. The H max spans between 6 (November 2013 event) and 9. storm. It appears clear that the Adrian storm has the highest H s , the highest T p , the highest storm surge, the lowest atmospheric pressure, and the highest mean wind velocity. The distance between the study area and the centre of the low pressure indicates two possible group of storms: the first group collects sea storms occurred when the pressure minimum was very close to the study area with distances of less than 25 km (October 2008, November 2013, and October 2018 events); the second group is characterised by distances greater than 88 km (October 2012 and December 2018 events). Figure 5 shows the evolution of storm surge, atmospheric pressure, H s , and mean wind velocity measured during four of the five sea storms considered (no data are available for the 2008 event). Noteworthy is the fact that the rapid decrease in the atmospheric pressure values, the strong increase in wind velocity, and the related large storm surge, were almost simultaneously only during the Adrian storm. In fact, during the 2012 storm, the minimum of atmospheric pressure preceded the increase in wind velocity and storm surge, while during the 2013 storms, the increase in wind velocity preceded the decrease in pressure and the rise of storm surge. Figure 6 shows the time variation of H s and the atmospheric pressure gradient for hourly time windows for the four sea storms. It is evident that the Adrian storm is associated with an anomalous baric gradient trend, showing a wider and steeper pressure variation occurred in a very short time.

Weather and Sea Data Analysis
wind velocity measured during four of the five sea storms considered (no data are available for the 2008 event). Noteworthy is the fact that the rapid decrease in the atmospheric pressure values, the strong increase in wind velocity, and the related large storm surge, were almost simultaneously only during the Adrian storm. In fact, during the 2012 storm, the minimum of atmospheric pressure preceded the increase in wind velocity and storm surge, while during the 2013 storms, the increase in wind velocity preceded the decrease in pressure and the rise of storm surge.   Figure 6 shows the time variation of Hs and the atmospheric pressure gradient for hourly time windows for the four sea storms. It is evident that the Adrian storm is associated with an anomalous baric gradient trend, showing a wider and steeper pressure variation occurred in a very short time.    variables approximate variable values for a given observation. Considering the overall results of RDA, the atmospheric pressure is slightly more informative in terms of explaining the variability of the sea wave parameters, followed by the wind velocity. Considering individual parameters, the atmospheric pressure is positively related to T p and negatively related to storm surge. Focusing on H s , the most significant parameter in our study case (Figure 7) shows that H s is strictly correlated with pressure gradient and wind velocity. Moreover, data recorded around the maximum development of the Adrian storm (data between 4_9 and 4_16 highlighted in light blue in Figure 7) are associated with the highest values of H s , wind velocity and pressure gradient.

Discussion
Through the analyses performed in the present study, the distinctive peculiarities of the Adrian storm have been examined. With respect to the other storms considered, the Adrian storm showed very peculiar features in terms of microseismic energy and meteorological-oceanic parameters. Specifically, during the Adrian storm, the pressure gradient has been significantly steeper than during the other events, and the wind velocity and the storm surge resulted very high values. The microseismic frequency content was akin to the other storms, but its energy proved to be significantly lower, leading to an underestimation of the Hs value provided by the procedure proposed by Ferretti et al. [15].
The exceptionality of the Adrian storm was confirmed by comparison of its peculiar

Discussion
Through the analyses performed in the present study, the distinctive peculiarities of the Adrian storm have been examined. With respect to the other storms considered, the Adrian storm showed very peculiar features in terms of microseismic energy and meteorological-oceanic parameters. Specifically, during the Adrian storm, the pressure gradient has been significantly steeper than during the other events, and the wind velocity and the storm surge resulted very high values. The microseismic frequency content was akin to the other storms, but its energy proved to be significantly lower, leading to an underestimation of the H s value provided by the procedure proposed by Ferretti et al. [15].
The exceptionality of the Adrian storm was confirmed by comparison of its peculiar features with bibliographic data. For example, storm surge, primarily due to the wind associated with transit or stationery (24-48 h) low-pressure systems at medium latitudes [44], is generally weak in semienclosed basins such as the Mediterranean Sea. Ullmann and Pirazzoli [45], who analysed storm surges measured at three tide gauge stations located along the coast of the Gulf of Lions (north-western Mediterranean Sea) between 1948 and 2003, found that more than 80% of storm surges ≥ 0.60 m (as recorded during the Adrian storm) are associated with winds >10 m s − , which mostly contribute to the storm surge peak. Nevertheless, storm surge values ≥ 0.60 m are not frequent in the Mediterranean Sea, except for areas such as Venice lagoon (north-eastern Italy), and occur one time per season [45]. During the Adrian storm, the simultaneous strong decrease in atmospheric pressure and strong increase in wind speed, with a large fetch involving a vast portion of the Mediterranean, have contributed to the exceptional height of the storm surge. Moreover, during its peak, the sea waves were characterised by a peak period of 11.7 s, an extreme value relatively to the Mediterranean Sea. Pasi et al. [46] have observed that, in the period 1998-2010 (out of our study period), a sea storm characterised by a similar T p occurred only once in the Ligurian Sea (on 1-2 January 2010) and, in the same 12-year period, they noted that sea storms with H s greater than 4.3 m are generally characterised by mean wave periods of about 8.4 s.
Despite its meteorological-oceanic characteristics, the Adrian storm did not produce a high-energy microseism. As is well known, there is a strong correlation between H s and local microseisms [13][14][15]47], but the generation mechanism of (primary) microseisms requires the sea surface-waves to interact with the sea bottom-namely, it occurs mainly in coastal areas with water shallower than half of the wavelength [48]. The correlation between sea waves and microseisms also depends on the duration of the storm; Traer et al. [48] found that sea waves typically evolve over a scale of days and that microseism features change with a similar time scale. Ardhuin et al. [49] found that an atmospheric perturbation that moves quickly and affects an area of shallow water near the coastline generates a weak conversion of wave-induced pressure to seismic noise. Therefore, sea waves produced by the Adrian storm had great energy, but their very rapid development, the position of the pressure minimum very close to the coast, and the very rapid variation of wave direction (from SE to SW) may have prevented the generation of a high-energy microseism. It is noteworthy that, a microseism with energy less than expected has also been observed during the November 2013 storm which developed very close to the Ligurian coast (see Table 1).
These effects along with a very high storm surge and a very high wind velocity may explain the nature of the Adrian storm, characterised by very high sea waves but a low-energy microseism. In summary, during this storm, the exceptional meteorological conditions (i.e., wind velocity and pressure gradient) and their spatial-temporal trend caused a peculiar response of the Ligurian Sea (in terms of storm surge, period and height of sea waves), linked to an anomalous microseism.
Although the mechanism of the microseism origin is difficult to discriminate in the Ligurian Sea, as already highlighted by Ferretti et al. [13], the secondary microseism, being by far stronger than the primary microseism, is probably the dominant influence on the microseism-based predictive models proposed by Ferretti et al. [15] for near real-time monitoring of H s . Therefore, during the Adrian storm, because of the peculiarities listed above, the generation of a secondary microseism has been exceptionally low, leading to an underestimation of H s . Unfortunately, at the moment, we cannot suggest any explanation for which the situation is not favorable for generating secondary microseisms during some storms (such the Adrian one). Following our results, in order to avoid a significant underestimation of the H s during future extreme sea storm events and, therefore, to improve the effectiveness of the procedures for real-time monitoring of the H s through microseismic data, we can only propose adding the pressure gradient together with the wind velocity into microseism-based predictive models. These parameters are nowadays easily available from weather station networks.
Therefore, an empirical correction of the prediction model is proposed here. According to our results, the correction term must be applied to the predictive model only when extreme values of wind velocity and pressure gradient are observed. Specifically, it is assumed the correction term must be applied only when the hourly wind velocity values or the absolute values of the pressure gradient exceed the 95 th percentile of data distribution. Considering data measured during the 2012, 2013, and 2018 events, the 95 th percentile of wind velocity and pressure gradient data distributions are 8.4 m s −1 and 1.1 hPa h −1 , respectively.
The correction term has been derived and calibrated considering two main pieces of empirical evidence that are:  Finally, the model of Ferretti et al. [15] was modified accordingly as follows: If then _ _ * 6 * 6 (2) where WMV is the wind mean velocity, APG is the absolute value of pressure gradient, i indicates the sample number (e.g., i = 0 corresponds to the current time; i = −5 corresponds to the data measured five hours before), and Hs_est and Hs_new are the Hs estimated by the procedure of Ferretti et al. [15] before and after the correction, respectively. Figure 9 compares the Hs measured by the buoy (blue line) and those provided by the procedure of Ferretti et al. [15] before (red line) and after (green line) the application of the proposed correction term for the Adrian storm. The differences between the Hs values measured by Capo Mele buoy and those obtained by using the microseism-based procedure corrected are strongly reduced (old maximum difference 3.4 m, new maximum difference 1.2 m). Since the applicability conditions were not met for the other sea storms Finally, the model of Ferretti et al. [15] was modified accordingly as follows: then where WMV is the wind mean velocity, APG is the absolute value of pressure gradient, i indicates the sample number (e.g., i = 0 corresponds to the current time; i = −5 corresponds to the data measured five hours before), and H s_est and H s_new are the H s estimated by the procedure of Ferretti et al. [15] before and after the correction, respectively. Figure 9 compares the H s measured by the buoy (blue line) and those provided by the procedure of Ferretti et al. [15] before (red line) and after (green line) the application of the proposed correction term for the Adrian storm. The differences between the H s values measured by Capo Mele buoy and those obtained by using the microseism-based procedure corrected are strongly reduced (old maximum difference 3.4 m, new maximum difference 1.2 m). Since the applicability conditions were not met for the other sea storms (during which WMV and APG stayed under the thresholds), the correction term was not applied. It is worth highlighting that the thresholds, guiding the use of the correction term, were defined based on statistical analysis. Specifically, the thresholds of wind velocity and pressure gradient corresponds to the 95th percentile of data distributions. Among all storms that have occurred in Liguria since 2008, the Adrian storm is the only one that presents both wind velocity and pressure gradient values that exceed the thresholds chosen. However, it is worth noting that the data scarcity does not allow us to effectively verify the robustness of such a criterion for differentiating storms, and the wrong application of such a correction term to storms that generate high-energy microseisms could generate significant errors in the estimation of H s . presents both wind velocity and pressure gradient values that exceed the thresholds chosen. However, it is worth noting that the data scarcity does not allow us to effectively verify the robustness of such a criterion for differentiating storms, and the wrong application of such a correction term to storms that generate high-energy microseisms could generate significant errors in the estimation of Hs. Figure 9. Comparison between Hs measured by the buoy (blue line) and those provided by model of Ferretti et al. [15] before (red line) and after (green line) the application of the correction term.

Conclusions
In the present study, we compared the characteristics of five of the most significant sea storms that struck the Ligurian coast between 2008 and 2018. Specifically, we analysed both sea wave and atmospheric parameters and presented a spectral analysis of the stormrelated microseisms. The aim was to highlight the distinctive features of the exceptional event occurred on October 2018 (Adrian storm) with respect to other strong sea storms in the same area in order to make (also during exceptional storms) the procedure proposed by Ferretti et al. [15] more effective for monitoring the sea wave height. In fact, although the Adrian storm caused sea wave heights of up to 9 m and significant damage to coastal infrastructures, it generated a very low energy microseism, thus leading to a severe underestimation of the Hs values assessed through the procedure proposed by Ferretti et al. [15]. Therefore, a correction term, that takes into account wind velocity and the atmospheric pressure gradient, was proposed and applied to the predictive model, allowing a significantly reduction in the underestimation of the estimated Hs when dealing with storms that generate low energy microseisms (such as the Adrian storm). In our case, the wind velocity and pressure data were provided by the weather station of the Seismic and Meteorological Observatory of Imperia and, therefore, the applicability of the proposed correction term is limited to the area around Imperia and Capo Mele buoy (Figure 1). For the Adrian storm, the inclusion of meteorological data (wind velocities and pressure gradients above an empirically determined threshold) together with the microseism amplitude in the prediction of significant wave height resulted in a significantly better fit. Whether this or a similar formula, although promising, is applicable in general must be Figure 9. Comparison between H s measured by the buoy (blue line) and those provided by model of Ferretti et al. [15] before (red line) and after (green line) the application of the correction term.

Conclusions
In the present study, we compared the characteristics of five of the most significant sea storms that struck the Ligurian coast between 2008 and 2018. Specifically, we analysed both sea wave and atmospheric parameters and presented a spectral analysis of the storm-related microseisms. The aim was to highlight the distinctive features of the exceptional event occurred on October 2018 (Adrian storm) with respect to other strong sea storms in the same area in order to make (also during exceptional storms) the procedure proposed by Ferretti et al. [15] more effective for monitoring the sea wave height. In fact, although the Adrian storm caused sea wave heights of up to 9 m and significant damage to coastal infrastructures, it generated a very low energy microseism, thus leading to a severe underestimation of the H s values assessed through the procedure proposed by Ferretti et al. [15]. Therefore, a correction term, that takes into account wind velocity and the atmospheric pressure gradient, was proposed and applied to the predictive model, allowing a significantly reduction in the underestimation of the estimated H s when dealing with storms that generate low energy microseisms (such as the Adrian storm). In our case, the wind velocity and pressure data were provided by the weather station of the Seismic and Meteorological Observatory of Imperia and, therefore, the applicability of the proposed correction term is limited to the area around Imperia and Capo Mele buoy (Figure 1). For the Adrian storm, the inclusion of meteorological data (wind velocities and pressure gradients above an empirically determined threshold) together with the microseism amplitude in the prediction of significant wave height resulted in a significantly better fit. Whether this or a similar formula, although promising, is applicable in general must be validated by a larger dataset. It will also be necessary to monitor if the H s estimation is realistic during other events similar to the Adrian storm, even in presence of different storm characteristics.