Abstract
Gravitational field modelling is an important tool for inferring past and present dynamic processes of the Earth. Functions on the sphere such as the gravitational potential are usually expanded in terms of either spherical harmonics or radial basis functions (RBFs). The (Regularized) Functional Matching Pursuit and its variants use an overcomplete dictionary of diverse trial functions to build a best basis as a sparse subset of the dictionary. They also compute a model, for instance, of the gravitational field, in this best basis. Thus, one advantage is that the best basis can be built as a combination of spherical harmonics and RBFs. Moreover, these methods represent a possibility to obtain an approximative and stable solution of an illposed inverse problem. The applicability has been practically proven for the downward continuation of gravitational data from the satellite orbit to the Earth’s surface, but also other inverse problems in geomathematics and medical imaging. A remaining drawback is that, in practice, the dictionary has to be finite and, so far, could only be chosen by rule of thumb or trialanderror. In this paper, we develop a strategy for automatically choosing a dictionary by a novel learning approach. We utilize a nonlinear constrained optimization problem to determine bestfitting RBFs (Abel–Poisson kernels). For this, we use the Ipopt software package with an HSL subroutine. Details of the algorithm are explained and first numerical results are shown.
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1 Introduction
The gravitational potential is an important observable in the geosciences as it is used as a reference for multiple static and dynamic phenomena of the complex Earth system. The EGM2008 gives us a highprecision model in spherical harmonics, i.e. polynomials, up to degree 2190 and order 2159, see National GeospatialIntelligence Agency, Office of Geomatics (SN), EGM Development Team (2008); Pavlis et al. (2012). From satellite missions like GRACE or its successor GRACEFO, we have monthly data provided by the JPL, GFZ and CSR. These are timedependent models of the potential, see, for example, Flechtner et al. (2014), NASA Jet Propulsion Laboratory (2018), Schmidt et al. (2008), Tapley et al. (2004) and, thus, enable a visualization of mass transports on the Earth such as seasonal shortterm phenomena like the wet season in the Amazon basin as well as longterm phenomena like the climate change. Therefore, gravitational field modelling and especially the downward continuation of satellite data is one of the major important mathematical problems in physical geodesy, see, for instance, Baur (2014), Kusche (2015). Details of the used data are given in Sect. 4.
From a mathematical point of view, the gravitational potential F on the approximately spherical Earth’s surface can be modelled as a Fourier expansion in a suitable basis, for example in the mentioned spherical harmonics \(Y_{n,j},\ n \in {\mathbb {N}}_0,\ j=n,\ldots ,n\). If we assume the Earth to be a closed unit ball, we obtain, for \(\sigma >1\), a pointwise representation of the potential as
for the unit sphere \(\varOmega \) and \(\eta \in \varOmega \), see, for example Baur (2014), Freeden and Michel (2004), Moritz (2010), Telschow (2014), where \(\sigma \eta \) is the observation point of the potential V. This gives us the potential in the outer space including a satellite orbit. The inverse problem of the downward continuation of this potential is given as follows: if data values \(V(\sigma \eta ) = ({\mathcal {T}}F) (\sigma \eta ),\ \sigma >1\), are known, determine the function F on \(\varOmega \). For more details on inverse problems in general, see the classical literature, for example, Engl et al. (1996), Louis (1989), Rieder (2003). The occurring mathematical challenges of the downward continuation are wellknown. First of all, the operator \({\mathcal {T}}\) has exponentially decreasing singular values due to \(\sigma >1\) in (1). Thus, the inverse operator which we need for the downward continuation has exponentially increasing singular values. For this reason, the inverse problem is called exponentially illposed. In particular, it violates the third characteristic of a wellposed problem according to Hadamard (continuous dependence on the data). Furthermore, the existence of F is only ensured if V is in the range of \({\mathcal {T}}\). However, if F exists, then it is unique.
Therefore, sophisticated algorithms need to be used to solve the problem of the downward continuation of satellite data of the gravitational potential. Previous studies showed that the (Regularized) Functional Matching Pursuit ((R)FMP), the (Regularized) Orthogonal Functional Matching Pursuit ((R)OFMP) as well as the latest (Regularized) Weak Functional Matching Pursuit ((R)WFMP) are possible approaches for this and other inverse problems, see, for instance, Berkel et al. (2011), Fischer (2011), Fischer and Michel (2013a, b), Gutting et al. (2017), Kontak (2018), Kontak and Michel (2018, 2019), Michel (2015), Michel and Orzlowski (2017), Telschow (2014) as well as Fischer and Michel (2012), Leweke (2018), Michel and Telschow (2014), Michel and Telschow (2016), where the latter can also be consulted for a comparison to other methods. These routines are greedy algorithms which iteratively construct stable approximations to the pseudoinverse. In the sequel, we will write Inverse Problem Matching Pursuit (IPMP) if we refer to either one of the mentioned algorithms. Although the core routine of these algorithms is well established by now, there are still possibilities to improve their performance.
One of these possibilities is given due to the following circumstances. The IPMPs are based on a dictionary \({\mathcal {D}}\) of suitable trial functions from which they build a best basis and eventually the approximate solution in terms of this best basis. From the approach it is expected that the representation of the signal might be sparser and/or more precise. In particular, the reduction to those basis functions which are essential increases the interpretability of the obtained model. Further, numerical experiments showed that the obtained solution is more accurate and stable. These aims can be achieved by the IPMPs.
While very good approximations could be obtained for the considered applications in Earth sciences and medical imaging (see the references above) so far, the experiments also revealed a sensitivity of the result regarding the choice of the dictionary, for example concerning the runtime and the convergence behaviour. Moreover, this choice is additionally critical since, up to now, the dictionary needed to be finite. Therefore, the main focus of this paper is on a first dictionary learning strategy for the downward continuation of gravitational potential data. This will also allow the use of an infinite dictionary with a free choice of the continuous parameters of an RBF.
Previous works on dictionary learning considered discretized approximation problems. In this case, the dictionary can be interpreted as a matrix. The approaches aimed to obtain a solution of the approximation problem and a sparse dictionary matrix simultaneously. For more details, see, for example, Bruckstein et al. (2009), Prünte (2008), Rubinstein et al. (2010).
However, a particular feature of the IPMPs is that their solution is a linear combination of established trial functions. Neither do we want to discretize the dictionary elements, i.e. the trial functions, nor do we want to modify them. In the latter case, the comparability with traditional models in these trial functions would be lost. Furthermore, with the use of scaling functions and/or wavelets in the dictionary, the IPMP generates a solution in a multiscale basis. This allows a multiresolution analysis of the obtained model revealing hidden local detail structures as it was shown in, for example, Fischer (2011), Fischer and Michel (2012, 2013a, b), Michel and Telschow (2014), Telschow (2014). Moreover, we do not only consider interpolation/approximation problems, but also illposed inverse problems. Thus, a dictionary matrix would not contain the basis elements themselves, but, for example, their upward continued values. Applying previous strategies, like, for instance, MOD or KSVD, would only alter the upward continued values and leave us with the question of how to downward continue them. All in all, this shows that learning a dictionary for the IPMPs requires the development of a different strategy.
In parallel to our research project, a stochastic nongreedy approach for finding an optimal basis of RBFs has been developed (Schall 2019). While adding and removing centres of the RBFs, this stochastic approach is also able to determine an optimal number of basis functions. On the other hand, only one fixed system of RBFs is used there, while our approach is able to learn an optimal localization parameter for each single RBF. Future research is expected to reveal further pros and cons of both approaches.
For a first approach to learning a dictionary, we concentrate on the RFMP as the basic IPMP in this paper. For this algorithm, we develop a procedure to determine a best basis for the gravitational potential from different types of infinitely many trial functions. We choose to learn dictionary elements from spherical harmonics and Abel–Poisson kernels as radial basis functions. In particular, while previously a discrete grid of centres of the RBFs had to be chosen apriori, which could have put a bias in the obtained numerical result, we now allow every point on the unit sphere to be a centre of an RBF. Equally, the localization parameter of the Abel–Poisson kernel is now determined from an interval instead of a finite set. Our continuous, i.e. nondiscrete, learning ansatz produces a ‘bestdictionary’ with which the RFMP can be run. We call this procedure the Learning (Regularized) Functional Matching Pursuit (L(R)FMP). The presented results show that the use of a learnt dictionary in the RFMP gives us a higher sparsity and better results with less storage demand.
An overview of the structure of the learning algorithm is shown in Fig. 1. We start in the red circle (‘start’) where we initialize the LRFMP similarly to the initialization which the RFMP needs. This means, the initialization includes the necessary preprocessing and setting of parameters [similarly as described, for example, in Telschow (2014)] as well as setting parameters for the learning. The latter learning parameters include, most importantly, a starting dictionary and smoothing properties.
Then we step into the first iteration in which we want to minimize the Tikhonov functional (as usually done in the RFMP) in order to find \(d_1\). As we also want to learn a dictionary, the steps up to choosing \(d_1\) differ from the established RFMP: we choose \(d_1\) from (in the case of the RBFs) infinitely many trial functions instead of a finite apriori selection of trial functions. This is done by first computing a candidate for \(d_1\) among each trial function class we consider. In Fig. 1, this is shown by the boxes ‘spherical harmonics’ and ‘radial basis functions’ which lead to ‘set of candidates’. Then we have again a finite (but optimized) set of trial functions and can choose \(d_1\) from this set of candidates in the common fashion of the RFMP by comparing how well each one minimizes the Tikhonov functional. The candidate that minimizes the Tikhonov functional among all candidates is chosen as \(d_1\) (‘choose best candidate as \(d_{n+1}\)’).
Then we compute the necessary updates of the RFMProutine as described, for example, in Telschow (2014). Next, we check the termination criteria for the learning algorithm. If they are not fulfilled, then we search for the next element \(d_2\) in the same manner as we found \(d_1\). Otherwise we stop the RFMP and, thus, the learning of the dictionary. We obtain an approximation of the given signal. Additionally, the learnt dictionary is defined as the set of all chosen elements in this approximation.
This paper is structured as follows. On the way to a detailed description of our learning approach, we define some fundamental basics in Sect. 2. We introduce the trial functions under investigation as well as a general form of a dictionary and the basic principles of the RFMP. With these aspects explained, we state our learning strategy in Sect. 3. We define its routine and give necessary derivatives. Some of the formulae are elaborated in “Appendix A”. We end Section 3 by introducing some additional learning features that guide the learning process positively. In Section 4, we describe experiments for which we learn a dictionary and compare the results of the learnt dictionary with the results which a manually chosen dictionary yields. We also explain why we choose this comparison. At last, we conclude this paper in Sect. 5 with an outlook of how we want to further develop this first learning approach.
2 Some mathematical tools for learning a dictionary
2.1 Trial functions under consideration for dictionaries
We consider spherical harmonics as well as Abel–Poisson kernels. Spherical harmonics are global trial functions, see for instance, Freeden et al. (1998), Freeden and Gutting (2013), Freeden and Schreiner (2009), Michel (2013), Müller (1966). They are defined for a unit vector \(\xi \in \varOmega \) as
where \(\xi (\varphi ,t)\) is the representation of \(\xi \in \varOmega \) in polar coordinates \((\varphi ,t)\) with \(t=\cos \vartheta \) and the latitude \(\vartheta \). Further, the definition uses associated Legendre functions given by
where \(P_n\) denotes the nth Legendre polynomial. Abel–Poisson kernels are defined for a particular unit vector \(\xi \in \varOmega \) (the centre of the RBF) and a scaling parameter \(h \in [0,1)\) as (with \(x=h\xi \)) the functions
of the unit vector \(\eta \in \varOmega \), see, for example, Freeden et al. (1998), pp. 108–112 or Freeden and Schreiner (2009), p. 103 and 441. These kernels are radial basis functions, that means they have one maximum whose descent depends on the distance to the centre \(\xi = x/x\) of the extremum. In that way, they are zonal functions and can be viewed as ‘hat’functions. Dependent on the scaling parameter \(h = x\), the size of the extremum or ‘hat’ varies in size. Thus, the functions have different scales of localization. For more details and examples, see, for instance, Freeden et al. (1998), p. 111 or Michel (2013), p. 117.
In this paper, we consider dictionaries consisting of spherical harmonics and Abel–Poisson kernels. We introduce here a notation for building blocks of spherical dictionaries.
Definition 1
Let \(N \subset {\mathcal {N}} :=\{(n,j)\ \ n \in {\mathbb {N}}_0, j=n,\ldots ,n\}\) and \( K \subseteq \mathring{{\mathbb {B}}}_1(0)\) for the open unit ball \(\mathring{{\mathbb {B}}}_1(0)\). Then we set
for spherical harmonics \(Y_{n,j}\) and
for Abel–Poisson kernels \(P(r\xi ,\cdot )\). We define a dictionary as
We call \([\cdot ]_*\) a trial function class.
Note that N and K may be finite or infinite.
2.2 Basic principles of linear illposed inverse problems
For the theory of inverse problems \({\mathcal {T}}:{\mathcal {X}} \rightarrow {\mathcal {Y}}\), we refer the reader to Engl et al. (1996), Kontak (2018), Michel (2013), Rieder (2003). For the domain \({\mathcal {X}}\), we propose to use a Sobolev space because, for instance, it enforces more smoothness of the solution than, e.g. the \(\mathrm {L}^2(\varOmega )\)space. This has proven to yield better results. Specifically, we will use the Sobolev space \({\mathcal {H}}_2\).
Definition 2
On the set \({\widetilde{{\mathcal {H}}}}\left( (n+0.5)^2; \varOmega \right) \) of all functions \(F \in \mathrm {C}^{(\infty )}(\varOmega ,{\mathbb {R}})\) that fulfil
we define an inner product via
The completion of \({\widetilde{{\mathcal {H}}}}\left( (n+0.5)^2; \varOmega \right) \) with respect to \(\langle \cdot , \cdot \rangle _{{\mathcal {H}}_2}\) is called the Sobolev space \({\mathcal {H}}_2\).
We give a short overview of the main principles of the RFMP algorithm as far as they are needed for this paper. For further details, we refer to the literature listed in the introduction. The underlying idea of this matching pursuit is to build a solution as a linear combination of dictionary elements by iteratively minimizing a Tikhonov functional. We reformulate the linear inverse problem \({\mathcal {T}}:{\mathcal {H}}_2 \rightarrow {\mathcal {Y}},\ {\mathcal {T}}F = V\), as given in (1), to the case of discrete gridbased data where \({\mathcal {Y}} = {\mathbb {R}}^\ell \).
We have a relative satellite height \(\sigma >1\), a set of grid points \(\{\eta ^{(i)}\}_{i=1,\ldots ,\ell } \subset \varOmega \) and associated data values \(\{y_i\}_{i=1,\ldots ,\ell }\). The operator \({\mathcal {T}}\) is exchanged by a finite system of related functionals \({\mathcal {T}}^i_\daleth \) for which \({\mathcal {T}}^i_\daleth F = ({\mathcal {T}}F)(\sigma \eta ^{(i)}) = y_i\) holds for \(i=1,\ldots ,\ell \). We use the Hebrew letter Dalet \(\daleth \) to emphasize that the functionals \(\left( {\mathcal {T}}^i_\daleth \right) _{i=1,\ldots ,\ell }\) represent a discretization of the operator \({\mathcal {T}}\). Summarized, we consider the linear inverse problem \({\mathcal {T}}_\daleth F = y\) for the operator \({\mathcal {T}}_\daleth = ({\mathcal {T}}^i_\daleth )_{i=1,\ldots ,\ell }\) and a given vector \(y \in {\mathbb {R}}^\ell \).
A regularization parameter is denoted by \(\lambda \). Additionally, we need an apriori defined dictionary \({\mathcal {D}}\) as given in Definition 1. Then the aim of the RFMP is to iteratively minimize the Tikhonov functional
for an element \(d \in {\mathcal {D}}\) of the dictionary, a real coefficient \(\alpha \) and a current approximation \(F_n\). In practice, this means we start with an initial approximation \(F_0\), e.g. \(F_0 \equiv 0\), and iteratively determine \(F_{n+1} :=F_n + \alpha _{n+1}d_{n+1}\) via
It can be shown, see, for example, Fischer (2011), Michel (2015), Michel and Telschow (2014) that the minimization with respect to \(\alpha \) and d of the Tikhonov functional (5) is equivalent to determining \(\alpha _{n+1}\) and \(d_{n+1}\) via
where \(R^n :=y  {\mathcal {T}}_\daleth F_n\) is the residual.
3 The learning approach
3.1 A first learning algorithm
We described the learning routine in Sect. 1. With the notation just introduced, we formulate the minimization task of each trial function class mathematically. For an arbitrary iteration step n, the objective to seek \(\alpha _{n+1}\) and \(d_{n+1}\) is given by
where the superscript refers to the trial function class
respectively. In the sequel, we use an equivalent formulation.
Definition 3
Due to (6), we define the objective function of the RFMP in the nth iteration step as
where d is a trial function, \(R^n\) is the current residual, \(F_n\) the current approximation and \({\mathcal {T}}, \lambda \) depend on the linear inverse problem.
Next, we state the learning algorithm. We explain the steps of this algorithm in detail below. Note that we determine a preliminarily optimal Abel–Poisson kernel from a discretely parametrized dictionary \([ {\hat{K}} ]_{\mathrm {APK}}\) and use this as a starting point for the optimization procedure for a continuously parametrized ansatz which uses \([ \mathring{{\mathbb {B}}}_1(0)]_{\mathrm {APK}}\).
Algorithm 4
We obtain a learnt dictionary for the RFMP as follows. Let \({\mathcal {T}}_\daleth F = y\) be the linear inverse problem under investigation, \({\mathcal {H}}_2\) the Sobolev space from Definition 2 and \(\lambda \) the regularization parameter.
 (S0):

initialize: termination criterion; data vector y; initial approximation \(F_0\); sets \({\hat{N}}\) as well as \({\hat{K}}\) as in Definition 1 and starting dictionary \({\mathcal {D}}= [{\hat{N}}]_\mathrm {SH} + [{\hat{K}}]_{{\mathrm {APK}}}\)
 (S1):

set \(R^0 :=y{\mathcal {T}}_\daleth F_0\) and compute \(\langle F_0, d \rangle _{{\mathcal {H}}_2}\) for all \(d \in {\mathcal {D}}\).
 (S2):

compute \({\mathcal {T}}_\daleth d\) for each \(d \in {\mathcal {D}}\) and \(\langle d, {\widetilde{d}} \rangle _{{\mathcal {H}}_2}\) for each pair \(d,\ {\widetilde{d}} \in {\mathcal {D}}\).
 (S3):

while (termination criterion not fulfilled)
 (S3.1):

compute candidate
$$\begin{aligned} d_{n+1}^{\mathrm {SH}} :={{\,\mathrm{arg\,max}\,}}\left\{ \mathrm {RFMP}(d;n)\ \Big \ d \in \left[ {\hat{N}}\right] _\mathrm {SH}\right\} \end{aligned}$$  (S3.2):

compute starting point for the optimization
$$\begin{aligned} d_{n+1}^{\mathrm {APK,start}} :={{\,\mathrm{arg\,max}\,}}\left\{ \mathrm {RFMP}(d;n)\ \Big \ d \in \left[ {\hat{K}}\right] _{{\mathrm {APK}}}\right\} \end{aligned}$$  (S3.3):

compute optimal solution
$$\begin{aligned} d_{n+1}^{\mathrm {APK}} :={{\,\mathrm{arg\,max}\,}}\left\{ \mathrm {RFMP}(d;n)\ \Big \ d \in \left[ \mathring{{\mathbb {B}}}_1(0)\right] _{{\mathrm {APK}}}\right\} \end{aligned}$$  (S3.4):

choose
$$\begin{aligned} d_{n+1} :={{\,\mathrm{arg\,max}\,}}&\left\{ \mathrm {RFMP}\left( d_{n+1}^{\mathrm {SH}};n \right) ,\ \right. \\&\qquad \left. \mathrm {RFMP}\left( d_{n+1}^{\mathrm {APK,start}};n\right) ,\ \mathrm {RFMP}\left( d_{n+1}^{\mathrm {APK}};n\right) \right\} \end{aligned}$$  (S3.5):

compute
$$\begin{aligned} \alpha _{n+1} = \frac{ \left\langle R^n, {\mathcal {T}}_\daleth d_{n+1} \right\rangle _{{\mathbb {R}}^\ell }  \lambda \left\langle F_n , d_{n+1} \right\rangle _{{\mathcal {H}}_2} }{\Vert {\mathcal {T}}_\daleth d_{n+1} \Vert ^2_{{\mathbb {R}}^\ell } + \lambda \Vert d_{n+1} \Vert ^2_{{\mathcal {H}}_2} } \end{aligned}$$  (S3.6):

set \(R^{n+1} :=R^n  \alpha _{n+1}{\mathcal {T}}_\daleth d_{n+1}\)
 (S3.7):

for each \(d \in {\mathcal {D}}\) compute \(\langle F_{n+1}, d \rangle _{{\mathcal {H}}_2} = \langle F_n, d \rangle _{{\mathcal {H}}_2} + \alpha _{n+1}\langle d_{n+1}, d \rangle _{{\mathcal {H}}_2}\)
 (S3.8):

increase n by 1
 (S4):

result: approximation \(F_M = \sum _{i=1}^M \alpha _i d_i\) after iteration step M at termination; learnt dictionary
$$\begin{aligned} {\mathcal {D}}^*&= \left[ N^* \right] _\mathrm {SH} + \left[ K^*\right] _{{\mathrm {APK}}},\\ N^*&=\{(n_i,j_i)\ \ \text {there exists } i \in \{1,\ldots ,M\} \text { such that } Y_{n_i,j_i} = d_i\},\\ K^*&= \{(r\xi )^{(i)}\ \ \text {there exists } i \in \{1,\ldots ,M\} \text { such that } P((r\xi )^{(i)},\cdot ) = d_i\} \end{aligned}$$
In our implementation, we use the following truncation criterion: we stop if \(n>I\) or \(\Vert R^n\Vert _{{\mathbb {R}}^\ell } < \varepsilon \) or \(\alpha _n< \delta \) for preliminarily chosen values \(I \in {\mathbb {N}}\) and \(\varepsilon ,\ \delta \in {\mathbb {R}}^+\).
3.2 Determination of candidates
The question remains how the candidates in each trial function class under consideration are determined, i. e. what is done in (S3.1)–(S3.3).
First, we consider the determination of a spherical harmonic candidate. We want to seek the bestfitting function among all spherical harmonics up to a certain degree \(\nu \in {\mathbb {N}}\). We have to learn the size of \(\nu \). It is defined in Algorithm 4 which specific spherical harmonics with a degree up to \(\nu \) we insert into the learnt dictionary.
The idea is to allow the choice of spherical harmonics up to a degree \({\widetilde{N}} \in {\mathbb {N}}\) (i.e. \({\hat{N}} = \{(n,j)\ \ n \in {\mathbb {N}}_0,\ n\le {\widetilde{N}},\ j=n,\ldots ,n\}\)) which is probably not chosen in practice. For example, the data resolution can provide a threshold up to which a resolution appears to be realistic (as it is also done for other gravitational models like EGM or models based on CHAMP, GRACE and GOCE data). If the LRFMP chooses only spherical harmonics up to a lower degree \(\nu \), we have a truly learnt bound \(\nu < {\widetilde{N}}\). However, note that the higher we choose \({\widetilde{N}}\), the more expensive is the preprocessing of the algorithm. The candidate \(d_{n+1}^{\mathrm {SH}}\) which the LRFMP chooses in each iteration step can be chosen as in the RFMP by comparing \(\mathrm {RFMP}(Y_{m,k};n)\) for all spherical harmonics up to degree \({\widetilde{N}}\). Note that this optimization problem is discrete by nature.
Next, we consider the determination of the candidate \(d_{n+1}^{\mathrm {APK}}\) from the Abel–Poisson kernels in S3.3. In this case, the minimization of the Tikhonov functional is modelled as a nonlinear constrained optimization problem. The solution of this problem yields the respective candidate. Note that we do not seek the minimizer of a function, but the minimizer of a functional among a set of functions. Therefore, we have to define the trial functions dependent on their characteristics as we did in (4).
The optimization problem
can be modelled by an optimization with respect to the characteristics \(x = h\xi \) of each RBF. However, these characteristics yield a constraint for the optimization problem. Abel–Poisson kernels are given as \(K_h(\xi \cdot ) = P(h\xi , \cdot ),\ h \in [0,1)\) and \(\xi \in \varOmega \) in (4), see, for example, Freeden and Gerhards (2013), p. 132 or Freeden and Michel (2004), p. 52. Here, \(\xi \) is the centre of the radial basis function and h is the parameter which controls the localization. Therefore, the kernels are welldefined only in the interior of the unit ball and the constraint is given by \(\Vert x \Vert ^2_{{\mathbb {R}}^3} < 1\).
Definition 5
The optimal candidate \(d_{n+1}^{\mathrm {APK}}\) among the set of Abel–Poisson kernels \(\{P(x,\cdot )\ \ x \in \mathring{{\mathbb {B}}}_1(0)\}\) is given by the solution of the optimization problem
Note that the maximizer is not necessarily unique. In this case, we use one representative among the maximizers.
We prefer a gradientbased approach. Thus, we have to compute the derivatives of (7) with respect to \(x \in {\mathbb {R}}^3\). In general, this can be done by applying the quotient rule and computing the derivatives of the inner products and norms in the de/nominator separately. We state the results of this derivation at this point. A detailed derivation is given in “Appendix A”.
Theorem 6
We define some abbreviation terms and state their derivatives. Let \(R^n\) be the current residual of size \(\ell \) and \(F_n\) the current approximation, i.e. \(F_n = \sum _{i=1}^n \alpha _i d_i\) for \(d_i\) being a spherical harmonic \(Y_{n_i,j_i}\) or an Abel–Poisson kernel \(P(x^{(i)},\cdot )\). Moreover, let \({\mathcal {T}}_\daleth \) be the upward continuation operator and \(\sigma \) the respective satellite orbit height. Further, let the data be given on a point grid \(\{\sigma \eta ^{(i)}\}_{i=1,\ldots ,\ell },\ \eta _i \in \varOmega \). We consider the Tikhonov functional with a penalty term dependent on the norm of the Sobolev space \({\mathcal {H}}_2\). At last, \(P_n\) denotes a Legendre polynomial and \(\varepsilon ^r,\ \varepsilon ^\varphi ,\ \varepsilon ^t\) represents the common local orthonormal basis vectors (up, East and North) in \({\mathbb {R}}^3\), see (18). Then we have for an Abel–Poisson kernel \(P(x,\cdot )\) and the representation of \(x \in \mathring{{\mathbb {B}}}_1(0)\) in polar coordinates \((r_x,\varphi _x, t_x)\) the terms
and
Their partial derivatives with respect to \(x_j\) are given by
and
With respect to the derivative of \(a_2\), we have further
and
For a proof, see “Appendix A”.
Theorem 7
With the abbreviations and derivatives from Theorem 6, the partial derivatives \(\partial _{x_j},\ j=1,2,3,\) of \(\mathrm {RFMP}(\cdot ;n)\) are given by
Proof
We only apply the common rules for derivatives. \(\square \)
Thus, for Abel–Poisson kernels, we determined the gradient of the modelled objective functions \(\mathrm {RFMP}(\cdot ;n),\ n \in {\mathbb {N}},\) analytically such that we are able to use a gradientbased optimization method. We use the primaldual interior point filter line search method Ipopt. To enable parallelization, we installed the linear solver ma97 from the HSL package. For more details on the Ipopt algorithm and the HSL package, see Vigerske et al. (2016), HSL (2018), Nocedal et al. (2008), Wächter and Biegler (2005a, b, 2006). In practice, we set a few options manually which we explain in the necessary contexts later. In all other cases, we use the default option values. However, note that due to Vigerske et al. (2016), we can only expect to obtain local solutions of the optimization problem. Furthermore, this algorithm uses a starting point to start its procedure towards an optimal Abel–Poisson kernel. This starting point is denoted by \(d_{n+1}^\mathrm{{APK,loc}}\) in Algorithm 4 and is computed in S3.2. We obtain \(d_{n+1}^{\mathrm {APK,loc}}\) by comparing the objective value \(\mathrm {RFMP}(P(x,\cdot ); n)\) for a selection of kernels given to the algorithm in the discrete dictionary by \([{\hat{K}}]_{\mathrm {APK}}\) and choosing the one with the highest value. As we have computed this kernel, we make use of it in S3.4 as well in the case that the optimization failed to find a better kernel.
3.3 Additional features for practice
The previously presented algorithm gives us a first and basic learning technique. During its development, we faced several problems dependent on the choice of the data and the given inverse problem. In order to overcome these difficulties, we introduced some additional features, which will be explained in the following.
First of all, the data of the monthly variation of the gravitational potential provided by GRACE attains very small values. In our experiments, these values lie in the interval [\(0.1\), 0.1]. When inserting these data into the objective function for determining an optimal Abel–Poisson kernel, the Ipopt solver fails to find a solution at first. Thus, we set the option obj_scaling_factor to \(10^{10}\). For the EGMdata, we only use \(1\) to perform a maximization instead of a minimization. Note that the scaled objective function is only seen internally to support the optimizer.
Next, to cut runtime and possible roundoff errors, we implemented a restart method. We initiate a new run of the algorithm by resetting \(F_E\) to zero after a previously chosen iteration number E. Note that, in contrast to the restart procedure of the ROFMP, see, for example, Telschow (2014), we also reset the regularization term \(\lambda \Vert F_E \Vert _{{\mathcal {H}}_2}^2\) to zero. In our experiments, we used \(E=250\).
Furthermore, we saw that the learnt dictionary heavily depends on the regularization parameter. Thus, we have to use the same regularization parameter as we used during learning when applying the learnt dictionary. Moreover, in contrast to previous works on the IPMPs, see, for instance, Telschow (2014), the use of a nonstationary regularization parameter is necessary when learning a dictionary and applying it. In the previous works, the idea of a nonstationary, decreasing regularization parameter was explained in order to emphasize accuracy instead of smoothness of the obtained approximation. However, the improvement of the results did not justify the additional computational expenses of choosing a parameter and a decrease routine. Nonetheless, we reconsidered this idea since the main aim of the LRFMP is to learn a dictionary and a decreasing parameter appears to guide the learning process positively. Thus, we use a nonstationary regularization parameter \(\lambda _n = (\lambda _0\Vert R_0\Vert _{{\mathbb {R}}^\ell }/(n+1))\), where n is the current iteration number and \(\lambda _0\) is a preliminarily chosen regularization parameter (see below). Our experiments show that with a decreasing regularization parameter, we determine a dictionary which yields a better approximation when applied. Hence, with a learnt dictionary, the use of a nonstationary regularization parameter has an impact on the result of the RFMP.
Next, for the case of a high satellite orbit or the seasonal variation in the gravitational potential obtained via GRACE, we developed a dynamic dictionary approach. Note that in previous literature on dictionary learning, see, for example, Prünte (2008), it was mentioned that the structure of the input data could or even should be considered when learning a dictionary. We developed two strategies to learn a dynamic dictionary whose combination works well in the experiments under considerations.
First of all, we demand that the first 250 learnt dictionary elements are spherical harmonics. It seems that after these 250 iterations, the current residual \(R_n\) has a rougher structure than the initial residual \(R_0\). Then the optimization routine finds more easily a more sensible solution and, therefore, learns a better dictionary. Additionally, we allow to only choose from the first \(n+1\) learnt dictionary elements in the nth iteration step of the RFMP when we use the learnt dictionary. In this case, the order of chosen dictionary elements from the LRFMP has to be preserved. In this way, the optimized trial function which was chosen in the nth step of the LRFMP can be chosen in the RFMP as well. Additionally, we save runtime as the dictionary size is small at the beginning. At last, this also treats possible complications which might otherwise arise from the nonstationary regularization parameter. The fact that we decrease this parameter yields the choice of very localized trial functions in later iterations of the LRFMP. If we allowed the RFMP to choose them prematurely this would only lead to a reduced data error and not a better approximation as we have seen in practice. If we allow the RFMP to only choose from the first n learnt dictionary elements, we can prevent it to choose very localized kernels prematurely.
With these features included in the LRFMP, we currently run our experiments.
4 Numerical results
4.1 Setting of the experiments
We consider two scenarios with different data sets: the EGM2008 as well as one month of GRACE satellite data. These data sets vary strongly with respect to their structure and, thus, yield two different challenges as numerical tests.
The EGM2008 data is evaluated up to degree 1500. For the GRACE data, we computed the meanfield from 2003 to 2013 averaged from the release 5 products from JPL, GFZ and CSR as was proposed in Sakumura et al. (2014). This meanfield was subtracted from the data corresponding to May 2008. Note that in May, usually, the wet season in the Amazon basin is about to end such that we can expect a concentration of masses in this region. Additionally, we smoothed the data with a Cubic Polynomial Scaling Function of scale 5, see, for instance, Schreiner (1996) and Freeden et al. (1998), p. 295. This is a simple and common smoothing filter based on a spherical wavelet method. Certainly, there are other filters which were specifically designed for destriping GRACE data such as Davis et al. (2008), Klees et al. (2008), Kusche (2007). However, here, we are concerned with testing the learning algorithm and not with detecting climatological phenomena. In both tests (EGM2008 and GRACE), we present results for the downward continuation from 500 km satellite height with \(5\%\) white noise.
In all experiments, we compute the data on an equidistributed Reuter grid of 12684 data points, see, for instance, Reuter (1982) and Michel (2013), p. 137. We choose the constant regularization parameter \(\lambda \) of the RFMP and the initial regularization parameter \(\lambda _0\) of the LRFMP (see Sect. 3.3) such that they yield the lowest relative approximation error after 2000 iterations. In detail, we choose \(\lambda =10^{2}\) for both experiments and \(\lambda _0 = 10^{4}\) for the experiment with EGM data and \(\lambda _0=10^{1}\) for the experiment with GRACE data.
Note that, in previous publications, see Fischer and Michel (2013b), Michel and Telschow (2014), Leweke (2018) it has already been shown that the RFMP is a competitive method in comparison to traditional method such as spline approximation. Therefore, we abstain from this comparison in this paper. Further, it would certainly be valuable to run tests with a large number of random dictionaries. This would allow the verification of the learnt dictionary in comparison to the average of the random dictionaries. However, for a scientific significance, the number of such dictionaries would need to be so large such that the experiments could not be feasible in a reasonable amount of time (see the runtimes in the numerical results below). Hence, we compare the results of the learnt dictionary with one manually chosen dictionary which is similar to wellworking dictionaries from previous publications, see e. g. Michel and Telschow (2016). This has also the advantage that this dictionary has already been a result of a ’human learning’ process via trialanderror. It might, therefore, be already better than a random choice.
To be specific, we define this manually chosen dictionary by
with
and an equidistributed Reuter grid \(X^\mathrm {m}\) of 4551 grid points on the sphere. All in all, the manually chosen dictionary contains 46186 dictionary elements.
The LRFMP needs a starting dictionary as well to provide the spherical harmonics and starting points for the optimization problem. For an equidistributed Reuter grid \(X^\mathrm {s}\) of 1129 grid points, we use
and
respectively, with
From experience, we know that it is better to cut down the number of scales r than the number of centres \(\xi \) of the Abel–Poisson kernels. Thus, the starting dictionary contains 11330 dictionary elements in the case of EGM2008 data and 4850 dictionary elements in the case of GRACE data.
We use the Ipopt optimizer with the linear solver ma97 from HSL. For EGM data, we demand a desired and acceptable tolerance of \(10^{4}\) of the optimal solution. For GRACE data, we demand these tolerances to be only \(10^0\) due to the scaling of the objective function explained in Sect. 3.3. As we need to ensure that the constraint is not violated during the optimization process, we set \(r^2 <0.98999999^2\) as well as the options theta_max_fact \(10^{2}\) and watchdog_shortened_iter_triggered 0 in practice. For details on these options, see the Ipopt documentation (Vigerske et al. 2016).
For the termination criteria of the LRFMP as well as the RFMP (see Sect. 3.1), we set \(I=3000,\ \varepsilon = 10^{8}\Vert y\Vert _{{\mathbb {R}}^\ell }\) and \(\delta = 10^{5}\) in all cases. We experienced that otherwise the additionally learnt dictionary elements do not improve the solution and we can easily stop the learning process at this stage. Note that in stopping after at most 3000 iterations, we also limit the learnt dictionary to at most 3000 learnt trial functions. This means, that the learnt dictionary is much smaller than the manually chosen dictionary with which we compare the learnt dictionary. Further, note that, due to its size, the manually chosen dictionary obviously has a much larger storage demand.
The results which we will compare here are obtained as follows: in one case, we use the RFMP with the manually chosen dictionary \({\mathcal {D}}^{\mathrm {m}}\). In the second case, we first learn a dictionary \({\mathcal {D}}^{*,\bullet }\) (see Algorithm 4) for \(\bullet \in \{ \mathrm {EGM}, \mathrm {GRACE} \}\) by using the LRFMP (which requires the starting dictionary \({\mathcal {D}}^{\mathrm {s},\bullet }\)) and then run the RFMP with the learnt dictionary \({\mathcal {D}}^{*,\bullet }\). The major question is: is the learnt dictionary able to yield better results than the manually chosen dictionary?
The plots shown in this paper are done with MATLAB. Note that the colours for the results of the GRACE data are flipped in comparison to the results of the EGM data. This is done in order to emphasize wet regions with blue colour and dryer regions with red colour.
4.2 Results
In Fig. 2, the results of the two experiments are shown. The first row shows the results with the EGM data. The second row depicts the results of the GRACE data. In the lefthand column the exact, unnoisy solution is given for comparison. The middle column shows the absolute approximation error of the RFMP with the manually chosen dictionary. The righthand column depicts this error of the RFMP with the learnt dictionary. We adjusted the scales of the values for a better comparison.
Obviously, in both cases the algorithm is able to construct a good approximation. The relatively low errors occur basically within regions where more local structures are given. These regions are in the case of the EGM data in particular the Andean region as well as the Himalayas and the borders of the tectonic plates in Asia. In the case of monthly GRACE data, the masses in the Amazon basin originating from the ending wet season show the strongest structure. As we only allow 3000 iterations, it can be expected that such regions cannot be approximated perfectly.
Particularly interesting are the results in the righthand column which were obtained with the learnt dictionary. Clearly, in both scenarios, the approximation error is notably reduced. This is, in particular, also the case in the regions with localized anomalies.
In Table 1, the relative approximation and data errors after 3000 iterations of the RFMP with the manually chosen dictionary and the learnt dictionary are given. Furthermore, the (currently) needed CPUruntimes for the experiments are presented in the last column. We notice that we do not only obtain a smaller relative approximation error with the learnt dictionary but also a smaller relative data error.
We state the CPUruntime in hours for the sake of completeness. Although the LRFMP includes learning and applying the learnt dictionary, it takes less time than the RFMP. However, these results are to be understood with care because they were not obtained with optimized code.
All in all, the results show that we are able to learn a dictionary which yields a smaller data as well as approximation error than a manually chosen dictionary. In addition, we obtain these results with a sparser dictionary, less storage demand and an appropriate CPUruntime.
5 Conclusion and outlook
We started our investigations by aiming to improve our method, the RFMP, for gravity field modelling. We expected to reduce the computational demands of the RFMP and the approximation error if a learnt dictionary is used rather than a manually chosen ’ruleofthumb’ dictionary.
In this paper, we presented a first approach to learn a dictionary of spherical harmonics and Abel–Poisson kernels for the downward continuation of gravitational data. In the numerical tests, we used data generated both from EGM2008 as well as GRACE models. The idea of our learning approach is to iteratively minimize a Tikhonov functional over an infinite set of these trial functions. We do so by using nonlinear constrained optimization techniques. Our results show that we obtain better results with respect to the relative data and approximation error when applying the learnt dictionary than when using a manually chosen dictionary in the RFMP. Moreover, we obtain these results with a sparser dictionary and less storage demand. Further, even nonoptimized code yields satisfactory runtime results for learning a dictionary.
In the future research, we aim to transfer this learning approach to the ROFMP and enlarge its idea to Abel–Poisson wavelets and Slepian functions. An additional objective is to obtain a dictionary for GRACE from a given set of training data to apply it with new test data such that we can provide an optimal dictionary for GRACEFO satellite data. Further, we need to consider the theoretical aspects of the learning algorithm like determining a quantitative measure for the quality of a dictionary and investigating how the learnt dictionary of the LRFMP is related to that measure. In addition, with respect to practical aspects, we plan on optimizing our code to have more meaningful runtime results.
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Gradient of the objective function with respect to Abel–Poisson kernels
Gradient of the objective function with respect to Abel–Poisson kernels
In this appendix, we prove Theorem 6.
First considerations We discuss the terms for the upward continuation operator as given in (1). Note that the Euclidean inner product of two vectors is emphasized by using a ’\(\cdot \)’ at the particular positions. Additionally, we make use of the following basic aspects.
In geomathematics, a common orthonormal basis in \({\mathbb {R}}^3\) is given by
see, for example, Michel (2013), p. 86. Note that it holds \(\partial _\varphi \varepsilon ^r= \sqrt{1t^2}\varepsilon ^\varphi \) and \(\partial _t \varepsilon ^r= \frac{1}{\sqrt{1t^2}} \varepsilon ^t\). For the gradient \(\nabla \), we will use a Cartesian definition as well as its decomposition into radial and angular parts. We have
see, for instance, Michel (2013), p. 87. Next, we consider the following recurring inner products.
see, for instance, Telschow (2014), p. 114. At last, we note one specific property of the fully normalized spherical harmonics. It holds
see, for instance, Leweke et al. (2018). Now, we can compute the terms in Theorem 6.
The term \(a_1(P(x,\cdot ))\) and its derivative Obviously, for the formulation of \(a_1(P(x,\cdot ))\) in (8), we only have to show that
for any \(\eta \in \varOmega \). We start at the lefthand side of (23).
Its derivative, as used in (12), is obtained via
The term \(a_2(P(x,\cdot ))\) and its derivative For the current approximation \(F_n\), we write \(F_n = \sum _{i=1}^n \alpha _i d_i\) for dictionary elements \(d_i = Y_{n_i,j_i}\) or \(d_i=P\left( x^{(i)},\cdot \right) \) depending on what element was chosen in the ith step. Then we can derive the representation (9) of \(a_2(P(x,\cdot ))\) as follows
due to (20), (21) and the addition theorem for spherical harmonics. The derivative of \(a_2(P(x,\cdot ))\) as given in (13) is obvious. However, we have to show (16) and (17). We will exchange the term x by r as well as \(\frac{x}{x}\) by \(\xi \) and \(\frac{x^{(i)}}{x^{(i)}}\) by \(\xi ^{(i)}\) for this. Then we obtain the following results. We first consider (16).
where we used (19), (22) and (2). We have to take a closer look at (25) regarding a possible singularity in \(t=\pm 1\). The term (25) contains two possibly problematic terms:
We first consider the term on the lefthand side of (26). Obviously, if \(j=0\), this is a removable singularity with a zero value. In the case \(j\not =0\), we recall the definition of the fully normalized spherical harmonics, which we use in practice, from (2) and (3). Thus, for the problematic term, we have
Obviously, there exists a problem only for \(\tfrac{j1}{2}< 0 \Leftrightarrow j1<0 \Leftrightarrow j<1 \Leftrightarrow j=0.\) However, this is excluded in this case. Thus, there is no problem in the term of the lefthand side of (26). With respect to the term on the righthand side of (26), we have
with the definition in (3). Obviously, the problematic term is
If \(j=0\), the term vanishes. If \(j\not =0\), the exponents are nonnegative. Thus, also the term on the righthand side of (26) contains no singularity.
At last, for the derivative of \(a_2(P(x,\cdot ))\), we need to consider (17). We obtain
With \(\varepsilon ^r= \frac{x}{x}\), this is the formulation of (17).
The term \(b_1(P(x,\cdot ))\) and its derivative The term \(b_1(P(x,\cdot ))\) as in (10) is obvious when we take (24) into account. The derivative of \(b_1(P(x,\cdot ))\) as in (14) is obtained by
The term \(b_2(P(x,\cdot ))\) and its derivative The formulation as in (11) of \(b_2(P(x,\cdot ))\) is due to the following considerations which use (21) and \(P_n(1) = 1\), see, for instance, Michel (2013), p. 49.
The gradient with respect to x is then obtained as follows.
With (19), we have
Inserting this result into (27), we obtain
This is in accordance with (15). Hence, Theorem 6 is proven. \(\square \)
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Michel, V., Schneider, N. A first approach to learning a best basis for gravitational field modelling. Int J Geomath 11, 9 (2020). https://doi.org/10.1007/s1313702001435
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DOI: https://doi.org/10.1007/s1313702001435
Keywords
 Dictionary learning
 Downward continuation
 Greedy algorithm
 Inverse problem
 Matching pursuit
 Nonlinear optimization
 Radial basis functions
 Spherical harmonics