Issue 
J. Space Weather Space Clim.
Volume 11, 2021



Article Number  60  
Number of page(s)  16  
DOI  https://doi.org/10.1051/swsc/2021045  
Published online  24 December 2021 
Research Article
An operational approach to forecast the Earth’s radiation belts dynamics
^{1}
ONERA/DPHY, Université de Toulouse, F31055 Toulouse, France
^{2}
Université ParisSaclay, CNRS, Institut d’Astrophysique Spatiale, 91405 Orsay, France
^{*} Corresponding author: guillerme.bernoux@onera.fr
Received:
10
May
2021
Accepted:
25
November
2021
The Ca index is a timeintegrated geomagnetic index that correlates well with the dynamics of highenergy electron fluxes in the outer radiation belts. Therefore, Ca can be used as an indicator for the state of filling of the radiation belts for those electrons. Ca also has the advantage of being a groundbased measurement with extensive historical records. In this work, we propose a datadriven model to forecast Ca up to 24 h in advance from nearEarth solar wind parameters. Our model relies mainly on a recurrent neural network architecture called Long Short Term Memory that has shown good performances in forecasting other geomagnetic indices in previous papers. Most implementation choices in this study were arbitrated from the point of view of a space system operator, including the data selection and split, the definition of a binary classification threshold, and the evaluation methodology. We evaluate our model (against a linear baseline) using both classical and novel (in the space weather field) measures. In particular, we use the Temporal Distortion Mix (TDM) to assess the propensity of two time series to exhibit time lags. We also evaluate the ability of our model to detect storm onsets during quiet periods. It is shown that our model has high overall accuracy, with evaluation measures deteriorating in a smooth and slow trend over time. However, using the TDM and binary classification forecast evaluation metrics, we show that the forecasts lose some of their usefulness in an operational context even for time horizons shorter than 6 h. This behaviour was not observable when evaluating the model only with metrics such as the rootmeansquare error or the Pearson linear correlation. Considering the physics of the problem, this result is not surprising and suggests that the use of more spatially remote data (such as solar imaging) could improve space weather forecasts.
Key words: Space weather / Forecasting / Radiation belts / Machine learning / Solar wind
© G. Bernoux et al., Published by EDP Sciences 2021
This is an Open Access article distributed under the terms of the Creative Commons Attribution License (http://creativecommons.org/licenses/by/4.0), which permits unrestricted use, distribution, and reproduction in any medium, provided the original work is properly cited.
1 Introduction
One of the current main topics of interest in the space weather field is forecasting geomagnetic indices based on machine learning methods. Machine learning has allowed for a great improvement in shortterm forecasts of geomagnetic indices such as the global index Kp (Wintoft et al., 2017; Tan et al., 2018; Chakraborty & Morley, 2020) or Dst index (Gruet et al., 2018; Lethy et al., 2018). Space weatherinduced events can have heavytoextreme consequences on humanmade infrastructures, as for instance, spaceborne hardware or even groundbased facilities (Riley et al., 2017). That is why the reliable forecast of geomagnetic indices and other spaceweather relevant physical quantities (e.g., relativistic electron or proton fluxes in the radiation belts) is of paramount importance.
The extent of the effects of the space radiative environment on satellites ranges from single events caused by high energy charged particles from cosmic rays or solar energetic particles (SEP) to internal charging, surface charging, or total ionising dose (Horne et al., 2013). Therefore, being able to accurately and reliably forecast the fluxes of highenergy electrons (from dozens of kiloelectronvolts to a few megaelectronvolts) in the radiation belts would represent a great leap towards better mitigation of the radiationinduced risks in space. Extensive efforts have already been conducted to forecast such electron fluxes. A considerable review of the methods used to forecast these electron fluxes was recently proposed by Camporeale (2019), where it is detailed that feedforward neural networks and recurrent neural networks (RNNs) are used to obtain forecasts up to a few hours or a few days ahead (see e.g., Ling et al., 2010; Wei et al., 2018).
However, Camporeale (2019) notes that although many approaches have been tested, it remains difficult to predict these fluxes due to certain physical phenomena that are difficult to consider for a “blackbox” type model. Thus, many more recent models based on machine learning methods do not perform better than older models. In addition, using datadriven approaches to predict radiation belt dynamics with insitu data is challenging since it is important to have large databases that are properly calibrated (which is more complicated when using spaceborne instruments rather than groundbased ones).
Recently, Bernoux & Maget (2020) have proposed a new timeintegrated geomagnetic index that aims to represent the state of filling the Earth’s radiation belts. This socalled Ca index is a timeintegrated index based on the betterknown aa index. As we will see in detail in Section 2, Ca was created to take into account the intensification of trapped electrons in the radiation belts. Ca is, therefore, a complementary index to other indices such as Kp or Dst. Thus in this study we focus on the prediction of the radiation belts dynamics represented by the Ca index. To do so, we will use deep learning methods (i.e., machine learning approaches based on deep neural networks) that have already been successfully tested with other geomagnetic indices. However, and in contrast to other studies, we concentrate on evaluating our models by taking into account the point of view of a spacecraft operator. Therefore we use evaluation methods other than the classical metrics such as the rootmeansquare error and the linear correlation, which can only account for global behaviour and are consequently largely insufficient to quantify other phenomena such as time shifts.
In this work, we design a neural networkbased model to forecast the Ca index up to 24 h in advance. Then we evaluate the model using both classical metrics and a method to detect the systematic existence of time shifts in our predictions. We also transform the regression problem into a binary classification problem aimed at predicting danger periods in terms of surface charging, and we evaluate it accordingly. In Section 2, we present the data sets used in our models, and we explain why they were chosen and how they were preprocessed. In Section 3, we present the models and their dedicated evaluation methods. In Section 4, we present and discuss the results before concluding in Section 5.
2 Data analysis
This section describes and analyses the data sets used in this paper. Firstly we list the solar wind parameters and geomagnetic indices used here and explain where and how they can be obtained. Then we focus on the geomagnetic index Ca and explain its relevance to our purposes. Finally, we explain how the time periods used for the training and the evaluation of the different models were selected.
2.1 Data sets
It is now well known that the geomagnetic indices representing the state of the magnetosphere are predominantly driven by solar wind dynamics (Akasofu, 1981; Baker et al., 1981). That is why, as in many other studies (e.g., Lundstedt & Wintoft, 1994; Wu & Lundstedt, 1997; Wing et al., 2005; Chandorkar et al., 2017; Chakraborty & Morley, 2020), we use solar wind parameters available in the OMNIweb database (King & Papitashvili, 2005) as inputs to our geomagnetic index forecast models. The OMNIweb database (https://omniweb.gsfc.nasa.gov/) grants access to hourly spacecraftinterspersed nearEarth measurements of solar wind parameters. The earliest solar wind parameters have been available since late 1963. In particular, we select the plasma bulk velocity V_{sw}, the ion density ρ, the southward component of the interplanetary magnetic field (IMF) B_{z}, and the plasma temperature T as the inputs to our models. It is now well known that these parameters correlate well with geomagnetic indices and with the dynamics of electron fluxes in the radiation belts (Burton et al., 1975; Wing et al., 2016). A thorough study based on informationtheoretical tools could help us to find an even better set of input parameters, but this is out of the scope of our study and could be the topic of future work.
The geomagnetic index studied here is the Ca index, which was first introduced by Bernoux & Maget (2020) based on a previous study by Rochel et al. (2016). Therefore the following paragraphs rephrase some information on the purpose and relevance of this index that was contained in these papers.
The Ca index is an index derived from the wellknown aa index. The aa index is a 3h Kbased index first introduced by Mayaud (1971) and computed from data provided by two subauroral antipodal observatories. aa index is the geomagnetic index having the longest available track record with data available since 1868. This gives us more than 150 years of homogeneous (Mayaud, 1980) and exploitable geomagnetic data with a time cadence of 3 h. This is particularly useful when dealing with topics, such as statistical analysis, which requires a great amount of data. In particular, aa index covers a time range equivalent to 14 solar cycles. Nowadays, the aa index is made available by the International Service of Geomagnetic Indices (ISGI) and can be downloaded from their website (http://isgi.unistra.fr/data_download.php).
As stated in Bernoux & Maget (2020), the Ca index has been designed to quantify the geoeffectiveness of solar wind structures impacting the magnetosphere from the radiation belts perspective. The relaxation characteristic time in the radiation belt’s for highenergy electrons after a strong magnetospheric disturbance is of the order of 4 days (Meredith et al., 2006; Rochel et al., 2016). Therefore, the Ca index is defined as follows:(1)with τ = 4 days being the relaxation characteristic time and aa representing the geomagnetic activity. Being directly derived from aa index, the Ca index shares the same qualities and properties. Further details on the interest and relevance of using the Ca index are provided in Section 2.2.
2.2 Why study and forecast the index?
Numerous studies have already been conducted on the topic of the nowcasting and forecasting of geomagnetic indices. Many of them focus on the Kp index or the Dst index, which are two very wellknown indices that have been thoroughly studied for decades. However, it should be reminded that all geomagnetic indices are not interchangeable and have physical meanings. For instance, Borovsky & Shprits (2017) make clear that the Dst index is unable to capture all types of geomagnetic storms behaviour and is, in reality, a very poor index when studying spaceweatherrelevant phenomena such as the dynamics of the electrons in the outer radiation belts induced by longduration Corotating Interaction Regions (CIR)driven storms. This is why it is important not to direct the research effort solely to the problem of forecasting the Kp and Dst indices but to diversify the indices studied in order to include a greater diversity of spaceweatherrelevant phenomena.
The Ca index was created to account for geomagnetic storms during which intensification of relativistic electrons trapped in the radiation belts is observed. It was shown in Rochel et al. (2016) and Bernoux & Maget (2020) that this index correlates well with electron fluxes (E > 30 keV) in the radiation belts and can take into account phenomena such as energy accumulation due to longduration Stream Interaction Region (SIR)driven storms, but also due to multiple successive Interplanetary Coronal Mass Ejection (ICME)driven events. Figure 1 displays examples of the typical behaviour of the Ca index during ICME and SIRdriven storms. During ICMEdriven storms, the aa index tends to reach higher values (in this example, aa reaches 228 nT) quickly, but it also decreases rapidly, whereas during SIRdriven storms, the disturbance lasts longer even though the aa index usually does not reach such high values (in this example it only reaches 81 nT). Therefore the Ca index reaches its peak value much faster during the ICMEdriven storm. However, the value of the peak is similar during both these events as Ca accounts better for energy accumulation (48.6 nT during the ICMEdriven storm against 42.4 nT during the SIRdriven storm).
Fig. 1 From bottom to top: evolution of the geomagnetic indices Dst, aa, and Ca, and of the flux of electrons in the radiation belts for the E ≥ keV energy range, measured by the SEM instrument aboard the POES15 spacecraft a) from 24 September to 8 October 1998 during a period that displayed an ICMEinduced disturbance starting on 25 September 1998, and b) from 7 October to 21 October 1999 during a period that displayed a SIRinduced disturbance starting on 9 October 1999. 
It was also stated in those papers that by changing the value of the parameter τ, it is possible to easily create an index that accounts better for a given specific orbit (but then less for the others). It is interesting to note that the Ca index is not the only attempt to create an index with such properties, and another approach was proposed by Borovsky & Yakymenko (2017).
From an operational perspective, the prediction of the Ca index could serve as a basis for an alert service for the accumulation of highenergy electrons in the radiation belts. In such a context, the Ca index would act as a proxy for relativistic electron fluxes, monitored from groundbased magnetometers. As stated in Section 1, using a data set that already has decades of crosscalibrated samples is also a great asset when dealing with datadriven approaches that require lots of data to be efficient. Besides, it may also be more reliable in terms of continuity of service to rely on groundbased instruments rather than onboard instruments that are subject to the risks associated with their being in space, at least as a backup. Thus, the prediction of the Ca index is of immediate interest to the operators of spaceborne systems.
2.3 Establishing the training, validation, and test sets
2.3.1 Splitting the data sets
In this subsection, we briefly analyse the time series supplied by the OMNIweb database to detect any important data gaps (that would be prejudicial for the training of a machine learning algorithm) and carefully choose the time periods used to train, validate and evaluate our models. Dividing a data set into training, validation, and test sets is a very common practice in machine learning applications. If needed, the reader is referred to Carè & Camporeale (2018) for more details.
Before the availability of the Wind/Solar Wind Experiment (Wind/SWE) and the Advanced Composition Explorer magnetometer and Solar Wind Electron, Proton, and Alpha Monitor (ACE/MAG and ACE/SWEPAM) data starting in 1995 and 1998, the OMNIweb database has a high percentage of missing data. Therefore in our study, we only use data from 1995 onward. For the 1995–2019 period, there was on average 2.41% of missing data per year. Even if most of the gaps are very short ones, some gaps larger than three or four days require proper handling. That is why we decided to fill the data gaps with the method introduced in Kondrashov et al. (2010). This method is based on Singular Spectrum Analysis, a dataadaptive spectral estimation method designed to provide information on the underlying dynamics of a (multivariate) timeseries (Ghil et al., 2002). In the context of space physics, SSA has already been used to fill the gaps in the OMNIweb database, which improved the accuracy of empirical magnetic field models compared to another simpler method based on linear interpolations (Kondrashov et al., 2014). Appendix provides more information on the practical gapfilling of the time series used in this paper with a dedicated toolkit (Vautard et al., 1992).
The choice of the data used to train, validate and test the neural network is of critical importance. This includes the appropriate choice of how the data set is temporally subdivided into training, validation, and test data sets (Lazzús et al., 2017). In order to correctly train a machine learning algorithm, the training data set should be comprised of a representative period during which all kinds of space weather phenomena, including extreme events, were observed. The testing (and the validation) period should also be comprised of both quiet and agitated periods. Eventually, we have chosen the following periods, highlighted in Figure 2:

Training set: 20030101 – 20181231.

Validation set: 19950101 – 19961231.

Test set: 19970101 – 20021231.
Fig. 2 Plot of the values taken by the Ca index between 1995 and 2018 included (black thin line). The training (green area), validation (yellow area), and test (red area) sets are highlighted. The 13month smoothed Sunspot Number is also plotted as an indicator for the solar cycle (red thick line). 
The train set comprises 16 continuous years, including the declining phase of one cycle and a full second cycle. The train set includes several extreme and even most extreme events, including the “Halloween storm” of November 2003 that reached a maximum value of Ca of 147.6 nT and was found to be the only 1in100 year event (in terms of Ca index) witnessed since the beginning of the Space Era (Bernoux & Maget, 2020). The validation set is composed of a 2year long period during a solar minimum. The test set comprises 6 continuous years, including the ascending phase, the maximum, and the beginning of the descending phase of a solar cycle. The test set includes intense and even extreme storms (≥ 67 nT), which is a good step towards a fair evaluation of our model. The chosen split should ensure that our sets are representative enough of the space weather phenomena observed through Ca.
To evaluate our model in an even more detailed way, we divide the test set into subparts corresponding to periods of disturbances induced on the one hand by ICMEs and on the other hand by Stream Interaction Regions (SIRs), including CIRs. For this purpose, we use the ICME database provided by Chi et al. (2016) and the SIR database provided by Chi et al. (2018). These databases include the time of beginning and time of ending for several ICME and SIRinduced geomagnetic disturbances between 1995 and 2015 (2016 for SIRs). According to these databases, 212 SIRs and 204 ICMEs were observed in the nearEarth environment between 1997 and 2002 included. In our study, we define an ICME (respectively SIR) induced disturbance period as the time period during which an ICME (respectively SIR) induced geomagnetic disturbance has an influence on the dynamics of the Ca index. The beginning of the disturbance period is given by the beginning of the storm, as indicated in the database. The ending of the disturbance period is given by adding τ = 4 days to the ending of the storm as indicated in the database. We can hence evaluate our models using only the ICME or SIRinduced disturbance periods and be able to better understand the accuracy of our forecasts. Table 1 summarises the number of data samples in each set and details the number of samples belonging to the disturbance periods.
Number of data samples in each set, including the number of samples belonging to a disturbance period.
The lists of SIR and ICME events we used end respectively in 2015 and 2016. Therefore, the number of samples in each disturbance period for the training set and the full set is actually greater than the ones reported in this table. This has no consequence in this study since we only split the test set according to the nature of the disturbance in order to evaluate the models.
2.3.2 Preprocessing the data
Before being fed into the neural networkbased model, the data are processed as follows:

We interpolate the values of the Ca index in order to have hourly values instead of a value every 3 h (this is meaningful since Ca is a very smooth timeintegrated index and thus doing this interpolation changes neither the physics nor the statistics of the problem).

Missing values in the other data sets are filled using SSA.

Inputs are rescaled so that their mean is 0 and their standard deviation is 1. Outputs are rescaled to fit in the [0, 1] interval. The weights for performing the transformations are calculated only from the training data set to avoid bias for validation and testing. This procedure is standard when working with recurrent networks.
3 Models and evaluation methods
In this section, we present the models used to predict the Ca index as well as the machine learning algorithms used in these models. We also describe the methods and measures used to evaluate the model.
3.1 Model description
The model developed in this study receives as input the past values of four solar wind parameters listed in Section 2.1, namely the plasma bulk velocity (V_{sw}), the ion density (ρ), the southward component of the interplanetary magnetic field (IMF) B_{z} and the plasma temperature (T). Unlike other studies, we choose not to include the past values of the geomagnetic index as an input to the models because we position ourselves in an operationallike context. Indeed, even though the ISGI provides quicklook aa index values, reliance on two different data sources always presents a higher risk of data unavailability from one source, which is prejudicial when establishing a nearrealtime forecasting service. Ideally, for such a service, one would have both models (with and without historical geomagnetic indices as inputs), but this is out of the scope of this study, and for clarity, we only study one model in this paper. Here we use the 30 last days for each input (i.e., the 720 last hourly values). The inputs/outputs link can be summarised as follows:where n is the forecast horizon.
In Section 4, we will analyse the results for a model trained and tested with a forecast horizon n = 24 h.
Our main model is a neural networkbased model. It consists of a single layer LongShort Term Memory network (LSTM) combined with a linear fullyconnected feedforward (FCFFNN) layer. LSTMs are a type of recurrent neural network first introduced in Hochreiter & Schmidhuber (1997). LSTMs were created to address problems involving sequentiallystructured data such as time series or natural language. In particular, LSTMs possess two internal memory states that are designed to help address the gradient vanishing issue that occurs when handling long sequences (Hochreiter, 1998). For an indepth understanding of deep learning methods, including recurrent and LSTM networks, the reader is referred to the papers mentioned above as well as to reference textbooks such as Goodfellow et al. (2016).
Our model is summarised in Figure 3.
Fig. 3 Simple scheme representing the LSTMbased model to forecast the values of the Ca index up to n hours in advance. The mechanism inside the LSTM cell was voluntarily not detailed. 
Let us summarise the functioning of the LSTM network here. For each sample corresponding to a time step t − p, the LSTM cell is fed with our solar wind parameters x_{ t−p} and the two memory states computed at the previous time step: the hidden state h_{t−p} and the cell state c_{t−p}. The LSTM cell processes and transforms the input and updates its hidden state and cell state (now h_{t−p+1} and c_{t−p+1}) using three “gates”: the input gate, the output gate, and the forget gate. To put it in simple words, the LSTM cell decides which information from the past is “worth” being kept, forgotten, or updated according to the last input. The latest memory states are again fed to the LSTM cell along with the solar wind parameters at the next time step x_{ t−p+1}. After all time steps have been given to the network, the LSTM layer outputs the final hidden state h_{t} that serves as the input to the FCFFNN layer, which itself outputs the t + 1 to t + n next values of Ca, n being the forecast horizon.
Let us note that LSTMs have already demonstrated a good efficiency on geomagnetic index prediction problems (see, e.g., Gruet et al., 2018; Chakraborty & Morley, 2020; Laperre et al., 2020).
Since this is the first study that focuses on the forecast of the Ca index, there is no immediate baseline for us to compare our model to. The usual baseline used in such a situation is the “persistence model” (also known as the “naive model”), which simply consists in assuming that the predicted value is the same as the last observed value. However, that baseline cannot be pertinently used here as we do not include the past values of the Ca index among the inputs to our model. That is why we have also trained a simple linear regression model to forecast the Ca index from the same solar wind parameters as with the neural networkbased model, with the notable exception that the baseline linear model only uses the last value for each solar wind parameter as input (and not several past values as with the neural networkbased model).
3.2 Training and parameters of the model
Our model was trained using the classical backpropagation method (Rumelhart et al., 1986). The optimisation method used is the Adam algorithm (Kingma & Ba, 2017). We have used a learning rate lr = 1 × 10^{−4} that is halved a first time after epoch 15 and a second time after epoch 50. The loss function is the meansquare error (MSE). The parameters of the model were handpicked using crossvalidation and iteration. We list below the main parameters of our model and some implementation choices so that the replicability of our results is made easier. Let the reader be advised that even after changing some of these parameters (e.g., to reduce the computational cost) it is possible to obtain very similar results.

The LSTM cell state has dimension 256.

The LSTM layer is monodirectional.

We use L2regularisation with weight 1 × 10^{−5}. L2regularisation consists of adding the squared sum of the network’s weights (with a multiplicative constant) to the loss function to avoid overfitting.

Size of each minibatch: 256.

The training is done with 120 epochs and with early stopping. Early stopping consists in stopping the training of the network as soon as clear signs of overfitting are observed.
The model was developed using the PyTorch (v1.9) library for Python (Paszke et al., 2019).
3.3 Detection of events
Our models, as described above, offer predictions in the form of a regression problem. However, it is often more useful for an enduser in a decisionmaking context to benefit from a predictive alert system. Such a (binary) predictive alert system can be built from our (regression) models with the following method: if we predict that Ca will exceed a given threshold value during the next t hours, then we issue an alert (class 1), if we predict that we stay below this threshold then we issue no alert (class 0). The only difficulty lies in the choice of a suitable threshold.
In our example, we will choose a threshold value based as much as possible on operational criteria. The threshold must be meaningful to the enduser, i.e. the triggering of an alert must correspond to a situation for which the operator is expected to make a decision or take action. As the Ca index represents the filling state of radiation belts with highenergy electrons, we will choose a Ca threshold associated with a nonnegligible risk of damage due to surface charging.
Figure 4 in Bernoux & Maget (2020) shows that the Ca index has a quite high correlation coefficient (R ≈ 0.83) with the dynamics of the integrated E ≥ 30 keV electron flux at L* ≈ 6. Moreover, MatéoVélez et al. (2018) shows that the risk of damage due to surface charging for a spacecraft in geostationary orbit (i.e. at L* ≈ 6) is well correlated with the 10 ≤ E≤ 50 keV electron flux when the latter is greater than 1 × 10^{8} cm^{−2} s^{−1} sr^{−1}. A day during which the 10 ≤ E ≤ 50 keV electron flux always stayed above this value has a minimum daily fluence of . From this value, we define a fluence threshold equals .
We then tried and found a Ca threshold that gives the highest correlation between the monthly exceedances of the electron fluence and the monthly exceedances of the Ca threshold (using the daily Ca maximum). For the daily fluences, we have taken data provided by the Magnetospheric Plasma Analyzer (MPA) instrument onboard the Geosynchronous Equatorial Orbit (GEO) LANL 1991–80 spacecraft between 1997 and 2006 for the energy range 35–46 keV McComas et al., 1993. It was found that the number of monthly fluence exceedances is best correlated with the monthly Ca exceedances when the Ca threshold is Ca_{threshold} = 38 nT. This is also illustrated in Figure 4.
Fig. 4 Count of days per month for which LANL 199180/MPA instrument measured a daily 10 ≤ E ≤ 50 keV electron fluence above 8 × 10^{12}cm^{−2}sr^{−1} along with the count of days per month for which the daily Ca max was above 38 nT. 
It should be noted in hindsight that the Ca value of 38 nT corresponds approximately to the 0.95 percentile of all Ca values, which seems statistically satisfactory. Indeed, it is a value that is therefore rare enough to make a credible and useful alert threshold (an operator would probably not want to receive an alert when the Ca value only exceeds the median, for example). But it is also a value that is not too high, which allows better learning for the neural network (indeed, the higher the threshold, the fewer samples we have to train and evaluate the model). Let us also insist on the fact that this threshold value used to define our binary classes in our study is only an example, and that depending on the effect considered (internal charging, surface charging, singular events, etc.), the orbit considered, or even the satellite considered (and thus its structure) it would be more interesting to use other thresholds, and probably to increase the number of classes.
3.4 Model evaluation
In this subsection, we describe the measures used to evaluate the forecast performance of our models.
3.4.1 Regression metrics
Since our problem is designed as a regression problem, we first evaluate our model using two very common regression metrics: the rootmeansquare error (RMSE) and the Pearson (linear) correlation coefficient (R). Let us define y_{i} the real observed values and the values forecast by a model for i ∈ 1,…,N, N being the number of samples.

The RMSE is a measure of the global accuracy of the model, with more emphasis put on higher values (e.g., here, the emphasis is on periods of more intense geomagnetic activity). A lower RMSE means a more accurate forecast. The RMSE is given by:

The Pearson correlation indicates if the forecast values globally follow the same trends as the real values. The Pearson correlation ranges between 0 and 1 (higher is better). It is given by:
We also use a normalised version of the RMSE (NRMSE), which allows for a better comparison of data sets with different scales. The NRMSE is obtained by dividing the RMSE by the mean value of the observed y_{i}. It is given by:(4)
Both RMSE and Pearson correlation are widely used in the geomagnetic indices forecasting literature (e.g., in Lazzús et al., 2017; Tan et al., 2018; Gruet et al., 2018; Sexton et al., 2019). However, these metrics do not capture the full performance of a model in all situations. Indeed, these metrics indicate overall trends. Most of the time, geomagnetic activity is fairly quiet, so quiet periods will weigh much more heavily on the evaluation metrics than periods of high activity, thus creating a bias. While it is very interesting for a satellite operator to accurately predict quiet periods, it is also very important to accurately predict periods of geomagnetic disturbance. This type of bias can be partially counterbalanced by taking adapted test sets, as we have done in Section 2.3. In the following subsections, we describe two other methods for evaluating the predictions that allow us to better capture other types of behaviours.
3.4.2 Measuring time lags
Some studies, such as Wintoft & Wik (2018) and Laperre et al. (2020), highlight the fact that some forecasting models, that display a great RMSE or Pearson correlation actually fail to reliably forecast high disturbance periods in advance. Laperre et al. (2020) show that some prediction models exhibit systematic time lags between the observed time series and the predicted time series. This systematic time lag would most often be of the order of magnitude of the model’s prediction horizon. This would indicate that the model, in reality, would fail to predict a disturbance before it has actually been observed, which is of very limited interest to an operator.
To quantify this behaviour, Laperre et al. (2020) use the Dynamic Time Warping (DTW) algorithm, which measures the time difference between twotime series (Berndt & Clifford, 1994). By applying this algorithm to the observed series and the predicted series shifted successively by several consecutive time steps, the authors are able to determine the extent of the systematic lag. Nonetheless, in our study, we do not use the exact same approach but a very similar one. Indeed, the main drawback of the DTW method is that for a given prediction horizon n, it requires circa n ^{2} iterations of the DTW algorithm with different time shifts to accurately assess the systematic time lag. Besides, the computational complexity of the DTW algorithm is high even with now modern methods to fasten the computation of the DTW measure (e.g., Gold & Sharir, 2018). This is why we use the Temporal Distortion Mix (TDM) instead.
The Temporal Distortion Mix is a metric proposed by Vallance et al. (2017) to characterise the propensity of a time series to be late or early relative to a reference series. This metric is also based on the DTW algorithm. Based on this algorithm, FríasParedes et al. (2016) propose the Temporal Distortion Index (TDI), which indicates to what extent the twotime series are systematically (or not) late (or early). Unlike the approach proposed by Laperre et al. (2020), the TDI does not indicate the value of a possible systematic time lag, but whether the twotime series exhibit this type of behaviour and to which extent. In return, there is no need for several computations of the DTW measure as only one (per forecast horizon) is sufficient to get the TDI. Guen & Thome (2019) have even suggested that the TDI could be used as a part of the loss function when training a neural network, but this is out of the scope of our paper.
To obtain the TDM, the TDI is decomposed into two components, which characterise the lateness and the advance, so that TDI = TDI_{adv} + TDI_{late}. The TDM is then given by:(5)
The TDM is hence a normalised version of the TDI. It ranges between −1 and 1. Let s_{1} and s_{2} be twotime series.

if then is systematically in advance compared to s_{ 2};

if then is systematically late compared to s_{ 2};

if then both time series are temporally aligned.
For instance, the TDM between a given time series and its corresponding naive forecast is always 1. A good forecast is hence a forecast that has a TDM close to 0. The TDM is a very interesting evaluation measure since it only requires one run of the DTW algorithm and it is possible to compare the TDM between several forecasts (e.g., several forecast horizons). The TDM was first introduced in a study dealing with the topic of solar irradiance forecasting, which is also a time series forecasting problem that shares structural similarities with ours.
3.4.3 Evaluation of the classificationbased alert system
As we have already established, in an operational context in space weather, it is important not only to have regressiontype predictions but also to have warning systems based on class predictions. In Section 3.3, we discussed how to transform our regression problem into a binary classification problem (with a threshold of Ca_{threshold} = 38 nT). In order to evaluate this derived alert system, we use several metrics and measures. TP, FP, FN, and TN are the true positive, false positive, false negative, and true negative counts.

the precision: it is the ratio of issued alerts that match a true threshold excess. It gives an indication of how relevant the issued alerts are. It ranges between 0 and 1. Higher is better. It is given by:

the recall: it is the ratio of true threshold exceedances that match an issued alert. It gives an indication of the ability to issue relevant alerts. It ranges between 0 and 1. Higher is better. It is given by:

the F_{score}: it is the Harmonic mean of precision and recall. It ranges between 0 and 1. Higher is better. It is given by:

the False Alarm Rate (FAR): it is the ratio of nonevents for which an alert was issued. It gives an indication of the tendency to issue irrelevant alerts. It ranges between 0 and 1. Lower is better. It is given by:

the threat score (TS): it gives an indication of how well true threshold exceedances were forecast, penalising both false alarms and false negatives. It ranges between 0 and 1. Higher is better. It is given by:

the Heidke skill score (HSS): it could be seen as a generalised skill score, giving the overall accuracy of the model against that of a random model. It ranges between −1 and 1. Higher is better, 0 denotes no skill. It is given by:

The percentage of thresholdexceedance periods for which the model actually issues an alert before the threshold was exceeded (i.e., the number of active periods that were forecast before they started and not only forecast after the threshold was exceeded for the first time). This is not a classical metric, but perhaps one of the most useful ones here, since this gives an indication of how well the model is able to forecast disturbance periods before they happened, not including the performance of the model once the disturbance period has already started. Let us note that there are 42 disturbance onsets (above the threshold Ca = 38 nT) in the test set.
4 Results and discussion
4.1 Regression results
The regression results obtained with the baseline model and the LSTMNN model are presented in Table 2. Firstly, we can see that the classical metrics (RMSE, R) give much better values with the LSTMNN model than the linear baseline. For a time horizon of 3 h, the RMSE with the LSTMNN is about 3.1 times lower than with the baseline (2.62 instead of 8.13), and for a time horizon of 24 h, this ratio is 2.0 (4.17 instead of 8.16). This is an additional indication of the fact that LSTMNN networks are efficient for understanding the solar windmagnetosphere coupling. The RMSE values should be put into perspective with the statistical distribution of the Ca index, which over the test period has a variance of 8.9 nT and an interquartile range of 10.5 nT. This comparison allows us to state that the RMSE values are satisfactory, especially for a model that does not include the Ca index among its inputs. We also find that the Pearson correlation values are quite high (≥0.9 for all test sets up to a time horizon of 18 h, instead of ≤0.65 with the baseline), which is very satisfactory.
Evaluation of the NNbased and the baseline models in the context of the regression problem. The model was evaluated with the full test set and also with the SIRinduced test set and the ICMEinduced test set.
The TDM gives values ≤0.2 for a time horizon of 3 h and up to 6 h, for test sets based on periods of disturbance. This indicates that up to about 6 h, our forecasts are well aligned in time with the target values. Beyond that, the TDM value increases up to 0.60 for a 24 h time horizon with the full test set, indicating that there is an almost systematic delay between the predicted values and the target values.
Unsurprisingly, the values of the conventional metrics all degrade as the time horizon increases. This degradation (increase for RMSE and TDM, decrease for the Pearson correlation) appears to be slow and smooth, as shown in Figure 5. However, for this reason, it becomes difficult to tell from these metrics alone from which time horizon the model is no longer operationally valid.
Fig. 5 Evaluation of the LSTMNN model with three measures (RMSE, R and TDM) for values of time horizon ranging from 1 h to 24 h. Three evaluation sets (full test set, SIRinduced set and ICMEinduced set) were used. 
We also observe that, in general, the LSTMNN model performs better during periods of SIRinduced disturbances than during periods of ICMEinduced disturbances. For a time horizon of 3 h, the RMSE is 1.4 times higher for the ICMEinduced period than for the SIRinduced period, which is far from negligible. Figure 6 shows several examples of forecasts for two geomagnetic storms: one induced by an ICME and the other by a SIR, the same storms already shown in Figure 1. This figure shows the forecast values for 4 different time horizons (3, 6, 12, and 24 h) made with both the LSTMNN model and the linear baseline model. We also indicate the TDM values calculated corresponding to each forecast (the values for the baseline are in brackets). It is clear from this figure that the neural networkbased model outperforms the linear model, as already indicated by the evaluation measures for the regression problem. In these examples, the dynamics of the storm appear to be well captured, and the forecast values are indeed close to the observed values, as indicated by the RMSE. Furthermore, it becomes apparent that the negative TDM values measured with the linear model are due to the fact that the model has difficulty correctly modeling the decay phase of a storm, which decreases too fast and hence appears “ahead” in comparison to the true series.
Fig. 6 Example of forecasts obtained with the LSTMNN model and the linear model during two geomagnetic storms, the first one (lefthand side) being an ICMEdriven storm and the second one being a SIRdriven storm (righthand side). Four different forecast horizons were used (3, 6, 12 and 24 h). The value of Ca used for the binary classification is the blue dotted line, given as a landmark. For each prediction, the corresponding TDM value is given (the TDM values for the baseline forecasts are given in brackets). 
Besides, the fact that the predicted (with the LSTMNN model) and observed time series show a time delay as the time horizon increases is evident in these examples. It would appear that this time shift is more pronounced during the beginning of the disturbance period than during the decay phase of the storm, which in the SIRinduced storm example remains well predicted even 24 h in advance. We should be able to better quantify this behaviour using the measures for the evaluation of the classification problem.
The difference of performance between ICMEinduced and SIRinduced storms could hence at least partly be explained by the fact that Ca increases more rapidly during ICMEinduced disturbances. As indicated by the TDM values (and as we will see below with the classification measures), the LSTMNN model seems to be underperforming during the initial phase of a disturbance. Since during SIRinduced disturbances, the initial increase is slower than during ICMEinduced disturbances, the RMSE during the beginning of the disturbance period should be lower in the first case, which contributes to the overall RMSE being lower for the SIRinduced test set than for the ICMEinduced test set.
Figure 7 shows the Normalised RMSE (NRMSE) and the Pearson correlation for forecasts with a time horizon of 3 h, after binning the target values into quarters containing moreorless the same number of items. Here we use the NRMSE since we are comparing the forecasts for different scales of Ca values, thus using the RMSE for the comparison would be like comparing apples and oranges. It appears that the LSTMNN model gives stable NRMSE values when Ca increases, which shows that the model is performing similarly not only when Ca is low but also when it reaches higher values, unlike the baseline. The Pearson Correlation for both models decreases when Ca is between the first and the third quartile. This is most probably due to the choice of bins matching the quartiles of Ca. Indeed, the range of Ca values in these bins is less than 6 nT, i.e. of the order of only twice the RMSE. Therefore, it is not surprising that the spread of predicted values over such a small range of observed values makes the linear correlation in these bins weaker. To summarise, this figure shows us that the model gives stable results and is still a much better model than the linear model for the whole distribution of Ca values, with a notable improvement for high values of Ca.
Fig. 7 Normalised RMSE and Pearson correlation of the 3h ahead predicted values versus binned observed values. Each bin contains a quarter of the total observations in the test set. 
4.2 Classification results
The classification results are given in Table 3 and Figure 8. For a time horizon of 3 h, nearly 85% of the alerts issued were true positives, while 84% of the threshold exceedances were detected. For a time horizon of 24 h, these numbers rise and fall respectively to 87% and 73%. The fact that the precision increases with the time horizon is due to the definition of our binary classes. Indeed, we are trying to forecast if the threshold will be exceeded at any given time in the next t hours (and not at a precise given time). In our case, as the threshold increases, the model forecasts less often false positives and more false negatives. That is why the precision increases somewhat counterintuitively. This highlights the need for several evaluation methods in order to obtain a more exhaustive idea of the true performance of the model. Let us note that the F_{score}, which is the harmonic mean of precision and recall, decreases from 0.84 (for a time horizon of 3 h) to 0.80 (for a time horizon of 24 h), further indicating that the model performs better for shorter time horizons.
Fig. 8 Percentage of times the 24 hbinary classification problem was correctly forecast during quiet periods previous to a threshold exceedance depending on how much time (from 1 h to 24 h) there was left before the exceedance. 
Evaluation of the NNbased and the baseline models in the context of the classification problem.
It is difficult to argue at what percentage of precision and recall the model becomes satisfactory. In absolute terms, correctly predicting more than two out of three periods of disturbance while making only ≈25% false positives might seem to be a satisfactory target. However, depending on the economic constraints due to spacecraft operation, this could be largely insufficient. Here we cannot definitively conclude about the absolute quality of our model but only about criteria that would be defined by an operator and that depend on each space mission or on the targeted objective. It should be noted, however, that the score values are also quite high, especially for the HSS. In absolute terms, these values are rather difficult to interpret and should serve above all as a point of comparison for possible future studies focusing on the forecast of similar physical quantities.
A result that is easier to interpret and that gives userfriendly information is the percentage of disturbance periods forecast in advance, given in Figure 8. To obtain this figure we calculated the percentage of times and how long before the model was able to correctly answer the question: “Will the threshold be exceeded during the next 24 h?” Therefore here, we are only interested in the model’s ability to predict the beginning of a period of disturbance (without taking into account the continuation of such a period). It appears that the model is able to answer this question correctly slightly less than 80% of the time 1 h before the threshold is exceeded. This percentage remains above 50% up to 5 h before the threshold is exceeded. Between 6 and 9 h prior to a threshold exceedance, around 40% of the disturbance periods were correctly forecasted. Less than 25% of the threshold exceedances were forecast at least 15 h in advance. This shows that even though 73% of the total exceedances were detected somewhere between 1 h and 24 h before they happened, only less than one out of two disturbance periods were detected 6 h before they happened, and less than one out of four were detected 24 h before they happened. This is a much more significant measure of the operational nature of our model and confirms the point we made earlier about the difficulty of predicting the onset of a geomagnetic storm.
4.3 Discussion
In fact, the abovementioned results are not very surprising since our models rely on solar wind parameters measured close to the Earth. Consequently, the temporal hindsight to predict the dynamics of radiation belts is small. This is reflected in the TDM measurements, which indicate that the forecasts are globally very well temporally aligned with the observations for forecast horizon values shorter than 6 h, which corresponds approximately to the reaction time of the geomagnetosphere interacting with a disturbance arriving near Earth. We can therefore deduce on the one hand that our model seems to be in agreement with the physics of the problem. But on the other hand, if we do not change the nature of our inputs, the same physics stops us from having good operational performances for greater prediction horizons.
Moreover, it seems delicate to find a limit to the prediction horizon for our model, beyond which it is possible to state definitively that the model is no longer operational. As mentioned above, this depends on the needs of an operator. In the absence of threshold values that could serve as landmarks for metrics such as precision or recall, we can only guess. One way to do this would be to consider the percentage of storms predicted in advance. If we take a threshold of 50%, then the operational prediction horizon limit of our model is 5 h. With a threshold of 75%, then our operational prediction horizon limit is only 1 h. Another method would be to take into account the TDM. With an arbitrary threshold of 0.2, the prediction horizon limit of our model is 6 h, whereas with a threshold of 0.1, the horizon limit is only 1 h for the full test set, but 4 h during SIRinduced disturbance periods and 3 h during ICMEinduced disturbance periods.
A limit of 6 h was found in other papers dealing with the forecasting of the Dst index (Lazzús et al., 2017; Gruet et al., 2018). Some studies that aim at forecasting the Kp index, such as Alaya Solares et al. (2016); Sexton et al. (2019), claim to be able to forecast the Kp index up to 24 h in advance. It would be interesting to assess the operational performance of the models presented in these papers with the TDM and by evaluating only the ability to predict the onset of a storm in order to have a more comprehensive understanding of their actual effectiveness in operational contexts. Let us insist, however, on the fact that the difficulty for long prediction horizons lies at the beginning of the storm and not in its continuity because the accumulation of energy makes it possible to find a link between the solar wind parameters and the geomagnetic indices even after 6 h of course. This is particularly the case with a timeintegrated index such as Ca, which allows for good overall forecast performances up to 24 h in advance.
It might be tempting to compare our results to the results presented in e.g. Forsyth et al. (2020), where the authors present a model to forecast the GOES15 ≥ 2 MeV electron fluxes from solar wind data and also evaluate their model with classification measures. For instance, one of their models (when maximising the average Receiver Operating Characteristic score) for a time horizon of 6 h gives a hit rate (or precision) of 0.75, whereas for the same time horizon, ours give a higher hit rate of 0.87. However, this comparison does not stand because we are not focusing on the same energy range, and our model does not use the same classification thresholds and criteria. Indeed, here we answer the question: will the threshold be exceeded somewhere in the next t hours? In Forsyth et al. (2020), the question is: will the threshold be exceeded in exactly t hours? We have chosen to approach the problem in this way because we believe that a warning system defined in this way is more useful, especially if we ask this question for several time horizons t. Yet this is an arbitrary choice, and it could be argued otherwise. We wanted to stress here that, as highlighted in Camporeale (2019), comparing the performance of one model relative to another is not straightforward, and one should be cautious when doing it.
5 Conclusion
In this study, we propose a recurrent networkbased approach to forecast the fairly new geomagnetic index Ca. The main reason for focusing on this index is that this index is well correlated with the highenergy electron fluxes in the radiation belts and could hence be used as an indicator for their state of filling, without the drawbacks inherent to measuring insitu fluxes with spacecrafts.
The implementation choices made in this paper were made by keeping in mind an operational context. These choices include the geomagnetic index to be forecast, the inputs used in our models, and the whole evaluation methodology. To this end, we have highlighted the importance of choosing statistically and physically representative train and test sets. We have also stressed the need to use adequate measures to evaluate the model since classical metrics such as the RMSE or the Pearson correlation cannot give an exhaustive report on the performance of the model, in particular during disturbance periods. That is why we use the Temporal Distortion Mix to measure the tendency for a forecast to be late or in advance in regards to the true observations.
We also transform the forecast problem from a regression problem to a binary classification one. The choice of the threshold used to define the binary classes was made, taking into account the risk for GEO spacecrafts to suffer damage from the surface charging effect. The evaluation of the binary classification forecasts shows that even though the regression measures seemed great, the network does not show outstanding performance when it comes to forecasting the onset of a disturbance period. This is most certainly due to the spatial (and hence temporal) proximity between the solar wind parameters used as inputs and the geomagnetosphere. In order to improve the forecast results for time horizons of 12 h, 24 h, and beyond it could be interesting to go back to the Sun and use data originating from solar imaging as inputs to a model. This topic will be the main focus of future studies. For now, even though the measures are good and much better than the linear baseline, it would be difficult to claim that this model is fully adequate for use in an operational situation. This would require at least an assessment of the model’s ability to predict extreme events, which will be the subject of future studies. However, with this study, we have already taken a first great step towards this goal.
Other possibilities that remained out of the scope of this study are the use of probabilistic forecasts (as done with other indices e.g. in Chandorkar et al., 2017; Chakraborty & Morley, 2020) or greybox models. This paper being the first one dealing with the topic of forecasting the Ca index, we voluntarily kept those possibilities aside for the sake of clarity and so as not to dilute the purpose of this study. However, we acknowledge that these are important avenues to explore, which will be done in future studies.
Supplementary Materials
ca_index_19952018.xls
omni_gapfilled_19952018.xls
Access hereAcknowledgments
The authors would like to thank the anonymous reviewers for their insightful suggestions and comments, which helped improve the overall quality of the paper. The authors are thankful to the NOAAPOES for online data access available on the CDAweb (at http://cdaweb.gsfc.nasa.gov/). The results presented in this paper rely on geomagnetic indices calculated and made available by ISGI Collaborating Institutes from data collected at magnetic observatories. We thank the involved national institutes, the INTERMAGNET network and ISGI (http://isgi.unistra.fr). The OMNI data were obtained from the GSFC/SPDF OMNIWeb interface (at https://omniweb.gsfc.nasa.gov). Sunspot data from the World Data Center SILSO, Royal Observatory of Belgium, Brussels. G. Bernoux is thankful for funding from Région Occitanie and ONERA, under Grant Agreements 19008721/ALDOCT and 30196. The editor thanks two anonymous reviewers for their assistance in evaluating this paper.
References
 Ayala Solares JR, Wei HL, Boynton RJ, Walker SN, Billings SA. 2016. Modeling and prediction of global magnetic disturbance in nearEarth space: A case study for Kp index using NARX models. Space Weather 14: 899–916. https://doi.org/10.1002/2016SW001463. [CrossRef] [Google Scholar]
 Akasofu SI. 1981. Prediction of development of geomagnetic storms using the solar windmagnetosphere energy coupling function ϵ. Planet Space Sci 29(11): 1151–1158. https://doi.org/10.1016/00320633(81)901215. [CrossRef] [Google Scholar]
 Baker DN, Hones EW, Payne JB, Feldman WC. 1981. A high time resolution study of interplanetary parameter correlations with AE. Geophys Res Lett 8(2): 179–182. https://doi.org/10.1029/GL008i002p00179. [CrossRef] [Google Scholar]
 Baudin M, Dutfoy A, Iooss B, Popelin AL. 2015. Open TURNS: an industrial software for uncertainty quantification in simulation. arXiv:1501.05242 [math, stat]. [Google Scholar]
 Berndt DJ, Clifford J. 1994. Using dynamic time warping to find patterns in time series. In: Proceedings of the 3rd International Conference on Knowledge Discovery and Data Mining, AAAIWS’94, AAAI Press, Seattle, WA. pp. 359–370. [Google Scholar]
 Bernoux G, Maget V. 2020. Characterizing extreme geomagnetic storms using extreme value analysis: a discussion on the representativeness of short data sets. Space Weather 18(6): e2020SW002,450. https://doi.org/10.1029/2020SW002450. [CrossRef] [Google Scholar]
 Borovsky JE, Shprits YY. 2017. Is the Dst index sufficient to define all geospace storms? J Geophys Res Space Phys 122(11): 11543–11547. https://doi.org/10.1002/2017JA024679. [Google Scholar]
 Borovsky JE, Yakymenko K. 2017. Systems science of the magnetosphere: creating indices of substorm activity, of the substorminjected electron population, and of the electron radiation belt. J Geophys Res Space Phys 122(10): 10012–10035. https://doi.org/10.1002/2017JA024250. [Google Scholar]
 Burton RK, McPherron RL, Russell CT. 1975. An empirical relationship between interplanetary conditions and Dst. J Geophys Res (1896–1977) 80(31): 4204–4214. https://doi.org/10.1029/JA080i031p04204. [CrossRef] [Google Scholar]
 Camporeale E. 2019. The challenge of machine learning in space weather: nowcasting and forecasting. Space Weather 17(8): 1166–1207. https://doi.org/10.1029/2018SW002061. [CrossRef] [Google Scholar]
 Carè A, Camporeale E. 2018. Chapter 4 – Regression. In: Machine Learning Techniques for Space Weather. Camporeale E, Wing S, Johnson JR, (Eds.) Elsevier. pp. 71–112. ISBN 9780128117880. https://doi.org/10.1016/B9780128117880.000044. [CrossRef] [Google Scholar]
 Chakraborty S, Morley SK. 2020. Probabilistic prediction of geomagnetic storms and the Kp index. J Space Weather Space Clim 10: 36. https://doi.org/10.1051/swsc/2020037. [CrossRef] [EDP Sciences] [Google Scholar]
 Chandorkar M, Camporeale E, Wing S. 2017. Probabilistic forecasting of the disturbance storm time index: an autoregressive gaussian process approach. Space Weather 15(8): 1004–1019. https://doi.org/10.1002/2017SW001627. [CrossRef] [Google Scholar]
 Chi Y, Shen C, Luo B, Wang Y, Xu M. 2018. Geoeffectiveness of stream interaction regions from 1995 to 2016. Space Weather 16(12): 1960–1971. https://doi.org/10.1029/2018SW001894. [NASA ADS] [CrossRef] [Google Scholar]
 Chi Y, Shen C, Wang Y, Xu M, Ye P, Wang S. 2016. Statistical study of the interplanetary coronal mass ejections from 1995 to 2015. Sol Phys 291(8): 2419–2439. https://doi.org/10.1007/s1120701609715. [CrossRef] [Google Scholar]
 Forsyth C, Watt CEJ, Mooney MK, Rae IJ, Walton SD, Horne RB. 2020. Forecasting GOES 15 >2 MeV electron fluxes from solar wind data and geomagnetic indices. Space Weather 18(8): e2019SW002,416. https://doi.org/10.1029/2019SW002416. [CrossRef] [Google Scholar]
 FríasParedes L, Mallor F, León T, GastónRomeo M. 2016. Introducing the temporal distortion index to perform a bidimensional analysis of renewable energy forecast. Energy 94: 180–194. https://doi.org/10.1016/j.energy.2015.10.093. [CrossRef] [Google Scholar]
 Ghil M, Allen MR, Dettinger MD, Ide K, Kondrashov D, et al. 2002. Advanced spectral methods for climatic time series. Rev Geophys 40(1): 3–1–3–41. https://doi.org/10.1029/2000RG000092. [Google Scholar]
 Gold O, Sharir M. 2018. Dynamic time warping and geometric edit distance: breaking the quadratic barrier. ACM Trans Algorithm 14(4): 50:1–50:17. https://doi.org/10.1145/3230734. [CrossRef] [Google Scholar]
 Goodfellow I, Bengio Y, Courville A. 2016. Deep learning. The MIT Press, Cambridge, MA, illustrated edition edn. ISBN 9780262035613. [Google Scholar]
 Gruet M, Chandorkar M, Sicard A, Camporeale E. 2018. Multiplehourahead forecast of the Dst index using a combination of long shortterm memory neural network and Gaussian process. Space Weather 16(11): 1882–1896. https://doi.org/10.1029/2018SW001898. [CrossRef] [Google Scholar]
 Guen VL, Thome N. 2019. Shape and time distortion loss for training deep time series forecasting models. arXiv:1909.09020 [cs, stat]. [Google Scholar]
 Hochreiter S. 1998. The vanishing gradient problem during learning recurrent neural nets and problem solutions. Int J Uncertain Fuzziness KnowlegeBased Syst 06(2): 107–116. https://doi.org/10.1142/S0218488598000094. [CrossRef] [Google Scholar]
 Hochreiter S, Schmidhuber J. 1997. Long shortterm memory. Neural Comput 9(8): 1735–1780. https://doi.org/10.1162/neco.1997.9.8.1735. [Google Scholar]
 Horne RB, Glauert SA, Meredith NP, Boscher D, Maget V, Heynderickx D, Pitchford D. 2013. Space weather impacts on satellites and forecasting the Earth’s electron radiation belts with SPACECAST. Space Weather 11(4): 169–186. https://doi.org/10.1002/swe.20023. [CrossRef] [Google Scholar]
 King JH, Papitashvili NE. 2005. Solar wind spatial scales in and comparisons of hourly wind and ACE Plasma and magnetic field data. J Geophys Res Space Phys 110, A02104. https://doi.org/10.1029/2004JA010649. [Google Scholar]
 Kingma DP, Ba J. 2017. Adam: A method for stochastic optimization. arXiv:1412.6980 [cs]. [Google Scholar]
 Kondrashov D, Denton R, Shprits YY, Singer HJ. 2014. Reconstruction of gaps in the past history of solar wind parameters. Geophys Res Lett 41(8): 2702–2707. https://doi.org/10.1002/2014GL059741. [CrossRef] [Google Scholar]
 Kondrashov D, Ghil M. 2006. Spatiotemporal filling of missing points in geophysical data sets. Nonlinear Process Geophys 13(2): n/a. https://doi.org/10.5194/npg131512006. [CrossRef] [Google Scholar]
 Kondrashov D, Shprits Y, Ghil M. 2010. Gap filling of solar wind data by singular spectrum analysis. Geophys Res Lett 37(15): https://doi.org/10.1029/2010GL044138. [Google Scholar]
 Laperre B, Amaya J, Lapenta G. 2020. Dynamic time warping as a new evaluation for Dst forecast with machine learning. Front Astron Space Sci 7. https://doi.org/10.3389/fspas.2020.00039. [CrossRef] [Google Scholar]
 Lazzús JA, Vega P, Rojas P, Salfate I. 2017. Forecasting the Dst index using a swarmoptimized neural network. Space Weather 15(8): 1068–1089. https://doi.org/10.1002/2017SW001608. [Google Scholar]
 Lethy A, ElEraki MA, Samy A, Deebes HA. 2018. Prediction of the Dst index and analysis of its dependence on solar wind parameters using neural network. Space Weather 16(9): 1277–1290. https://doi.org/10.1029/2018SW001863. [CrossRef] [Google Scholar]
 Ling AG, Ginet GP, Hilmer RV, Perry KL. 2010. A neural network– based geosynchronous relativistic electron flux forecasting model. Space Weather 8, S09003. https://doi.org/10.1029/2010SW000576. [Google Scholar]
 Lundstedt H, Wintoft P. 1994. Prediction of geomagnetic storms from solar wind data with the use of a neural network. Ann Geophys 12(1): 19–24. https://doi.org/10.1007/s0058599400192. [CrossRef] [Google Scholar]
 MatéoVélez JC, Sicard A, Payan D, Ganushkina N, Meredith NP, Sillanpäa I. 2018. Spacecraft surface charging induced by severe environments at geosynchronous orbit. Space Weather 16(1): 89–106. https://doi.org/10.1002/2017SW001689. [CrossRef] [Google Scholar]
 Mayaud PN. 1971. Une mesure planétaire d’activité magnétique basée sur deux observatoires antipodaux. Ann Geophys 27: 67–70. [Google Scholar]
 Mayaud PN. 1980. Derivation, meaning, and use of geomagnetic indices. Geophysical Monograph 22. American Geophysical Union, Washington. ISBN 9780875900223. [Google Scholar]
 McComas DJ, Bame SJ, Barraclough BL, Donart JR, Elphic RC, Gosling JT, Moldwin MB, Moore KR, Thomsen MF. 1993. Magnetospheric plasma analyzer: initial threespacecraft observations from Geosynchronous Orbit. J Geophys Res Space Phys 98(A8): 13453–13465. https://doi.org/10.1029/93JA00726. [CrossRef] [Google Scholar]
 Meredith NP, Horne RB, Glauert SA, Thorne RM, Summers D, Albert JM, Anderson RR. 2006. Energetic outer zone electron loss timescales during low geomagnetic activity. J Geophys Res Space Phys 111, A05212. https://doi.org/10.1029/2005JA011516. [Google Scholar]
 Paszke A, Gross S, Massa F, Lerer A, Bradbury J, et al. 2019. PyTorch: an imperative style, highperformance deep learning library. In: Advances in Neural Information Processing Systems, Vol. 32. Wallach H, Larochelle H, Beygelzimer A, dAlchéBuc F, Fox E, Garnett R, (Eds.) Curran Associates Inc. pp. 8024–8035. [Google Scholar]
 Riley P, Baker D, Liu YD, Verronen P, Singer H, Güdel M. 2017. Extreme space weather events: from cradle to grave. Space Sci Rev 214(1): 21. https://doi.org/10.1007/s1121401704563. [Google Scholar]
 Rochel S, Boscher D, Benacquista R, Roussel JF. 2016. A radiation belt disturbance study from the space weather point of view. Acta Astron 128: 650–656. https://doi.org/10.1016/j.actaastro.2016.07.012. [CrossRef] [Google Scholar]
 Rumelhart DE, Hinton GE, Williams RJ. 1986. Learning representations by backpropagating errors. Nature 323(6088): 533–536. https://doi.org/10.1038/323533a0. [CrossRef] [Google Scholar]
 Sexton ES, Nykyri K, Ma X. 2019. Kp forecasting with a recurrent neural network. J Space Weather Space Clim 9: A19. https://doi.org/10.1051/swsc/2019020. [CrossRef] [EDP Sciences] [Google Scholar]
 Sobol’ I.M.. 1967. On the distribution of points in a cube and the approximate evaluation of integrals. USSR Comput Math Math Phys 7(4): 86–112. https://doi.org/10.1016/00415553(67)901449. [CrossRef] [Google Scholar]
 Tan Y, Hu Q, Wang Z, Zhong Q. 2018. Geomagnetic index Kp forecasting with LSTM. Space Weather 16(4): 406–416. https://doi.org/10.1002/2017SW001764. [CrossRef] [Google Scholar]
 Vallance L, Charbonnier B, Paul N, Dubost S, Blanc P. 2017. Towards a standardized procedure to assess solar forecast accuracy: a new ramp and time alignment metric. Sol Ener 150: 408–422. https://doi.org/10.1016/j.solener.2017.04.064. [CrossRef] [Google Scholar]
 Vautard R, Yiou P, Ghil M. 1992. Singularspectrum analysis: a toolkit for short, noisy chaotic signals. Phys D: Nonlinear Phenom 58(1): 95–126. https://doi.org/10.1016/01672789(92)90103T. [CrossRef] [Google Scholar]
 Wei L, Zhong Q, Lin R, Wang J, Liu S, Cao Y. 2018. Quantitative prediction of highenergy electron integral flux at geostationary orbit based on deep learning. Space Weather 16(7): 903–916. https://doi.org/10.1029/2018SW001829. [CrossRef] [Google Scholar]
 Wing S, Johnson JR, Camporeale E, Reeves GD. 2016. Information theoretical approach to discovering solar wind drivers of the outer radiation belt. J Geophys Res Space Phys 121(10): 9378–9399. https://doi.org/10.1002/2016JA022711. [CrossRef] [Google Scholar]
 Wing S, Johnson JR, Jen J, Meng CI, Sibeck DG, Bechtold K, Freeman J, Costello K, Balikhin M, Takahashi K. 2005. Kp Forecast Models. J Geophys Res Space Phys 110, A04203. https://doi.org/10.1029/2004JA010500. [Google Scholar]
 Wintoft P, Wik M. 2018. Evaluation of Kp and Dst predictions using ACE and DSCOVR solar wind data. Space Weather 16(12): 1972–1983. https://doi.org/10.1029/2018SW001994. [CrossRef] [Google Scholar]
 Wintoft P, Wik M, Matzka J, Shprits Y. 2017. Forecasting Kp from solar wind data: input parameter study using 3hour averages and 3hour range values. J Space Weather Space Clim 7: A29. https://doi.org/10.1051/swsc/2017027. [CrossRef] [EDP Sciences] [Google Scholar]
 Wu JG, Lundstedt H. 1997. Geomagnetic storm predictions from solar wind data with the use of dynamic neural networks. J Geophys Res Space Phys 102(A7): 14255–14268. https://doi.org/10.1029/97JA00975. [CrossRef] [Google Scholar]
Appendix A
A.1 Gapfilling with Singular Spectrum Analysis (SSA)
To fill the missing values in our dataset we followed the SSA gapfilling method described in Kondrashov et al. (2010) and very well summarised in Section 2 of Kondrashov et al. (2014): “SSA is a dataadaptive, nonparametric method for spectral estimation; a comprehensive review can be found in Ghil et al. (2002) It is based on diagonalization of the timelagged covariance matrix of multivariate time series; the set of its eigenvectors or temporal empirical orthogonal functions (EOFs) is an optimal set of dataadaptive, narrowband filters for decomposing the variance within a sliding time window M. Projecting the data set onto each EOF yields the corresponding principal component (PC); the entire time series or parts thereof can be reconstructed by using linear combinations of PCs and EOFs for selected number of K modes, which yield the reconstructed components. Kondrashov & Ghil (2006) developed an SSAbased gapfilling method that relied on the presence of significant oscillatory modes in the time series [...]. Kondrashov et al. (2010) generalized the SSA gapfilling methodology to multivariate geophysical data consisting of gappy “drivers” and continuous “response” records and applied it to fill in large gaps in solar wind and IMF data, by combining it with timecontinuous geomagnetic indices. It is the covariation in driver and response at times when both are present that allows us to reconstruct the former when only the latter is measured.”
Here we will be using the geomagnetic indices Kp and Dst as our “response” records. All the steps of the SSA gapfilling method are automatically performed by the SSAMTM toolkit (Vautard et al., 1992) that is publicly available e.g. at https://dept.atmos.ucla.edu/tcd/download. But we also need to find the optimal M and K values, which are nontrivial. Kondrashov et al. (2014) suggests some values for a few solar wind parameters, but they did not include e.g. the plasma temperature T. That is why we performed a new search for optimal parameters, using a more recent period.
In order to find the optimal SSA window size M and number of modes K for each solar wind parameter, we introduced artificial gaps in each time series for the period 2008–2018. The artificial gaps are reproductions of the true gaps found in the same time series, but during the period 1984–1994, so that the distribution and the length of the artificial gaps were plausible. Then we searched for the best M and K values that allowed for the best reconstruction of the gaps as measured with the RMSE and Pearson correlation. The parameters optimal parameters were found by performing an iterative grid search using quasirandom low discrepancy Sobol sequences (Sobol’, 1967) generated by the Python package OpenTURNS (Baudin et al., 2015). The set of optimal parameters (namely M* and K*) found for each time series are reported in Table A.1. The time series gapfilled using the SSA technique and these M* and K* values are available online as Supplementary Material to this article.
Optimal M* and K* values found for filling the gaps in the time series.
Cite this article as: Bernoux G, Brunet A, Buchlin É, Janvier M & Sicard A, et al. 2021. An operational approach to forecast the Earth’s radiation belts dynamics. J. Space Weather Space Clim. 11, 60. https://doi.org/10.1051/swsc/2021045
All Tables
Number of data samples in each set, including the number of samples belonging to a disturbance period.
Evaluation of the NNbased and the baseline models in the context of the regression problem. The model was evaluated with the full test set and also with the SIRinduced test set and the ICMEinduced test set.
Evaluation of the NNbased and the baseline models in the context of the classification problem.
All Figures
Fig. 1 From bottom to top: evolution of the geomagnetic indices Dst, aa, and Ca, and of the flux of electrons in the radiation belts for the E ≥ keV energy range, measured by the SEM instrument aboard the POES15 spacecraft a) from 24 September to 8 October 1998 during a period that displayed an ICMEinduced disturbance starting on 25 September 1998, and b) from 7 October to 21 October 1999 during a period that displayed a SIRinduced disturbance starting on 9 October 1999. 

In the text 
Fig. 2 Plot of the values taken by the Ca index between 1995 and 2018 included (black thin line). The training (green area), validation (yellow area), and test (red area) sets are highlighted. The 13month smoothed Sunspot Number is also plotted as an indicator for the solar cycle (red thick line). 

In the text 
Fig. 3 Simple scheme representing the LSTMbased model to forecast the values of the Ca index up to n hours in advance. The mechanism inside the LSTM cell was voluntarily not detailed. 

In the text 
Fig. 4 Count of days per month for which LANL 199180/MPA instrument measured a daily 10 ≤ E ≤ 50 keV electron fluence above 8 × 10^{12}cm^{−2}sr^{−1} along with the count of days per month for which the daily Ca max was above 38 nT. 

In the text 
Fig. 5 Evaluation of the LSTMNN model with three measures (RMSE, R and TDM) for values of time horizon ranging from 1 h to 24 h. Three evaluation sets (full test set, SIRinduced set and ICMEinduced set) were used. 

In the text 
Fig. 6 Example of forecasts obtained with the LSTMNN model and the linear model during two geomagnetic storms, the first one (lefthand side) being an ICMEdriven storm and the second one being a SIRdriven storm (righthand side). Four different forecast horizons were used (3, 6, 12 and 24 h). The value of Ca used for the binary classification is the blue dotted line, given as a landmark. For each prediction, the corresponding TDM value is given (the TDM values for the baseline forecasts are given in brackets). 

In the text 
Fig. 7 Normalised RMSE and Pearson correlation of the 3h ahead predicted values versus binned observed values. Each bin contains a quarter of the total observations in the test set. 

In the text 
Fig. 8 Percentage of times the 24 hbinary classification problem was correctly forecast during quiet periods previous to a threshold exceedance depending on how much time (from 1 h to 24 h) there was left before the exceedance. 

In the text 
Current usage metrics show cumulative count of Article Views (fulltext article views including HTML views, PDF and ePub downloads, according to the available data) and Abstracts Views on Vision4Press platform.
Data correspond to usage on the plateform after 2015. The current usage metrics is available 4896 hours after online publication and is updated daily on week days.
Initial download of the metrics may take a while.