Research Article  Open Access
Miguel G. Folgado, Veronica Sanz, "On the Interpretation of Nonresonant Phenomena at Colliders", Advances in High Energy Physics, vol. 2021, Article ID 2573471, 12 pages, 2021. https://doi.org/10.1155/2021/2573471
On the Interpretation of Nonresonant Phenomena at Colliders
Abstract
With null results in resonance searches at the LHC, the physics potential focus is now shifting towards the interpretation of nonresonant phenomena. An example of such shift is the increased popularity of the EFT programme. We can embark on such programme owing to the good integrated luminosity and an excellent understanding of the detectors, which will allow these searches to become more intense as the LHC continues. In this paper, we provide a framework to perform this interpretation in terms of a diverse set of scenarios, including (1) generic heavy new physics described at low energies in terms of a derivative expansion, such as in the EFT approach; (2) very light particles with derivative couplings, such as axions or other light pseudoGoldstone bosons; and (3) the effect of a quasicontinuum of resonances, which can come from a number of strongly coupled theories, extradimensional models, clockwork setups, and their deconstructed cousins. These scenarios are not equivalent despite all nonresonance, although the matching among some of them is possible, and we provide it in this paper.
1. Why Nonresonant Phenomena
At the Large Hadron Collider (LHC), a tremendous effort has been devoted to searches for new states, which in their simplest form would manifest as resonances, an excess of events in a narrow kinematic range. Alas, direct searches have provided no fruit so far, diminishing hopes that the LHC would discover new particles connected to the electroweak scale.
At the same time, LHC experiments have continued improving their understanding of the data and enabled an unprecedented precise characterization of Standard Model (SM) particles. Particularly impressive is the evolution of the Higgs characterization, moving from discovery to precision measurements in a few years. In Figure 1, we can appreciate the level of effort made to contrast precise measurements of the LHC experiments and our best theoretical understanding.
The lack of discoveries is certainly a frustrating aspect of the LHC results, but with improved precision, a new opportunity opens up. The same SM particles whose characterization is so carefully accomplished could provide hints for new phenomena beyond the SM. Among all the SM particles, high hopes are placed on heavy particles, more closely connected to the electroweak symmetry breaking sector: the Higgs particle, massive vector bosons, and thirdgeneration fermions. Were their properties deviate from the SM predictions, we might be able to trace back these deviations to new physics. This indirect route may be the key to enter new sectors in Nature.
These two approaches of searching for new physics, direct search for new states and indirect search for new effects in known SM particles, complement each other. There is a wide range of new theories of Nature which at the LHC energies do not show up as narrow resonances, and for those, the best way to find them is by looking at excesses in tails of kinematic distributions.
The aim of this paper is to provide a framework to interpret nonresonant phenomena in terms of a diverse set of scenarios. We will provide a number of wellmotivated models which, in some area of their parameter space, lead to no resonances but excesses in tails.
The first paradigm we will discuss is the Effective Field Theory (EFT) approach, suitable for theories with resonances too heavy to be accessed directly at the LHC and only showing up as virtual effects.
The EFT is a wellknown and nowadays a rather standard way of organizing nonresonant searches, but it is certainly not the only one. There are other interesting theories which exhibit the same experimental signatures. One class of such models is represented by many closeby resonances forming a quasicontinuum in , the parton energy. This type of behaviour does appear in many extensions of SM which predict towers of resonances with the same quantum numbers but increasing mass. Were these towers broad/closeby, they would lead to nonresonant tails. Typical examples of this type of phenomena appear in theories with new strong interactions, extradimensions, or clockwork theories, to name a few.
Another distinct set of theories which could only be discovered via nonresonant searches are scenarios with light particles, so light that usual trigger cuts would prevent us from reaching their resonant kinematic regions but could still be discovered by their offshell production. If the coupling of these light states to SM particles was derivative, the offshellness could be compensated by the natural increase of the crosssection. A paradigmatic example of this kind of scenarios is an axion or axionlike particle coupled to SM gauge bosons (see Ref. [2] for a discussion of this behaviour).
The paper is organized as follows. In Section 2, we discuss the models which can provide a basis for experimental interpretation. In Section 3, we discuss partonlevel properties of the crosssections and provide a dictionary to match parameters among the models which share common experimental tails. We also discuss how these partonlevel results generalize to a total production crosssection. Finally, in Section 4, we summarise our findings.
2. Models of Nonresonant Behaviour
In this section, we describe new physics scenarios which lead to nonresonant behaviour, as well as relations among them (see Figure 2). Broadly speaking, these scenarios fall into three categories: (1)Heavy but narrow new states, due to some new sector well above the electroweak scale(2)Broad/nearby states at the electroweak scale(3)Light states, with mass well below electroweak’s, and with derivative couplings
Many models of new physics at some scale or in some range of their parameter space could show up at colliders as nonresonant excesses. In the rest of the section, we provide some context for some of the most popular models in each category. In the next section, we will provide a dictionary to relate scenarios of broad/nearby resonances, hence unifying their interpretation.
2.1. Heavy Physics: The Effective Field Theory (EFT) Case
We start with the paradigmatic example of EFTs. In this framework, one studies theories which predict a new sector of resonances coupled to the SM, with masses higher than the energies one is able to probe with current experiments. These new resonances will not be produced as final onshell states but can influence the behaviour of SM particles through their virtual effects.
One could consider the effect of new resonances on a scattering or decay process via treelevel (Figure 3(a)) or loop (e.g., Figure 3(b)) exchange of the heavy states. As the resonances are heavy, , one can understand the impact of the new sector as an expansion in energy over mass with various Lorentz structures involving just SM states as dynamical.
For example, let us consider classes of models which affect the electroweak symmetry breaking sector of the SM. Their presence would modify the interactions of the Higgs and massive gauge bosons, e.g., via new types of interactions described by new operators in the Lagrangian such as where is the Higgs doublet and is the field strength. These new types of interactions are formally nonrenormalizable and grow with the energy of the scattering process. At the level of Higgsvector boson interactions, they will modify the coupling structure as [3]
These new types of interactions grow with energy and exhibit different angular dependence than the simple SM structure. They will lead to excesses in high momentum tails of production of SM gauge and Higgs bosons, such as distributions shown in Figure 1. The behaviour of this tail, the rate at which it grows with energy, will be dictated by the form of the operator in Equation (1) and the value of its coefficient , but their interpretation in terms of new sectors of Nature could be very different.
For example, in Ref. [4], we computed three possible interpretations of these effects in terms of new scalars coupled to the electroweak sector: where are the singlet, doublet, and radion/dilaton masses, are the singlet/doubletHiggs couplings, is the singlet vev, and is a parameter of the new quasiconformal sector (see Ref. [4] for details, as well as Ref. [5] to understand how the singlet expression has been obtained).
Despite sharing a common experimental search (same cuts and statistical procedure), the limit on the value of would translate into very different limits for the three scenarios discussed above. Moreover, a combined measurement in more than one diboson channel, e.g., , , , and , could be used to disentangling the three different models (see, e.g., the discussion in Ref. [6] along these lines).
Moreover, for some of these scenarios, the EFT procedure may not be a valid approach. This theoretical limitation is sometimes denoted by the generic question of the range of validity of the EFT (see, e.g., Refs. [7–10]). For example, if one were to use the distribution in Figure 1 to set limits on a value of , the limit would be mostly dominated by the highest bins, but if this limit led to a model interpretation with particle masses , the EFT approach would break down.
2.2. Light New Physics: Axions and Other PseudoGoldstone Bosons
Since Goldstone obtained his theorem, we know that light degrees of freedom (Goldstone bosons) are a manifestation of a global symmetry which is spontaneously broken by some UV dynamics, e.g., confinement from a strong gauge sector. We know this description to be very predictive in the lowenergy sector of QCD (PT), and it is expected that the same mechanism reappears in other sectors of Nature. For example, this mechanism is called for as a solution to the strong CPproblem of QCD, leading to the hypothesis that a new light state, called axion, would couple to SM particles.
And for many new physics scenarios we design, especially if they involve new strong interactions, these (pseudo)Goldstone bosons are present and couple to SM particles via interactions which show growth with energy, similar to the EFT case.
Indeed, if we denote the new light state as and assumed for simplicity to have pseudoscalar quantum numbers, the interaction with the SM could look like
where denotes the field strength of any of the SM interactions and is the strength. This interaction is dimensionfive, grows with , and is suppressed by the scale , the breaking scale of the UV global symmetry which led to the existence of . Apart from couplings to gauge bosons, these pseudoGoldstone bosons could couple to fermions, with a strength typically suppressed by the fermion mass.
Experimentally, distinguishing a genuinely EFT excess from an axionlike excess would require a detailed understanding of the tail’s behaviour, which is currently not possible due to the lack of statistics in the tails as well as enough precision in the theoretical determination of these distributions at high energy. Nevertheless, one could envision a future situation at highluminosity LHC where an excess over the Standard Model would be firmly established. In this case, the detailed study of the distribution could allow us to disentangle both hypotheses.
2.3. Broad Resonances: Models of Towers of States
Apart from heavy and light resonances, one could also interpret tails in energy distributions in terms of very closeby resonances, so close that they form an almost continuum. There are many models which could produce such behaviour, from towers of resonances with the same quantum numbers to quasiconformal theories. In this section, we will propose some benchmarks for interpretation and in Section 3 provide a dictionary to relate to them.
2.3.1. Warped Extradimensions
The EFT framework is very popular for many reasons, including its generality and ability to be improved orderbyorder in an expansion of momenta over the heavy masses. Yet, EFTs are based on the assumption that the new sector is at a scale well separated from the electroweak scale, hence losing ground in terms of understanding the origin of the electroweak sector, including the hierarchy problem.
This problem has taken up a lot of the community’s minds for a long time and accordingly been rephrased in many ways. One particularly compelling view to solve the hierarchy problem comes from linking gravitational interactions with the SM, in particular assuming that the scale of strong gravitational effects is much lower than the perceived Planck scale, all the way down to the TeV scale, close to the electroweak scale. This can be achieved by postulating the existence of new, small dimensions of space.
These new theories of extradimensions and strong gravity at the TeV scale could take many forms, encoded in the choice for spacetime geometry and localisation of the fields inside the extradimension. A very wellstudied and successful framework is the socalled RandallSundrum (RS) model [11] or simply warped extradimensions. It is based on a setup with a single new dimension of space with a large curvature and a nonfactorisable metric where is the 5D curvature, is the size of the extradimension, and is the coordinate in the 5th dimension. The RS models is built on a slice of the 5D spacetime located between two 4D branes, which are typically located at (UVbrane) and (IRbrane) (see Figure 4). The combination is the warp factor and affects 4D slices of spacetime in different ways, exponentially different as we move along the bulk. In the classical 4D spacetime, the gravitational fundamental interaction is the Planck mass, GeV. The effect of the new extradimension is to modify the fundamental scale and to lower the scale of strong gravitational phenomena (like black hole formation) to the TeV scale near the IRbrane.
Warped models come in different varieties depending on particle localisations as well as the exact form of the geometry. Nevertheless, we generically expect the existence of towers of massive spin2 resonances (KaluzaKlein gravitons) as a consequence of compactifying higherdimensional gravity. Indeed, one can expand fluctuations around the 4D projection of the 5D metric to obtain where can then be interpreted as a 5D graviton. After compactification, this 5D field can be written as a massless graviton and an infinite KKtower of massive gravitons. The effective scale interaction of the KKgravitons depends on the location in bulk of the field it interacts with. Fields near the IR couple to the KKtower with scale TeV, namely, where is the SM energymomentum tensor while is the th KKgraviton.
The spectrum of the KKtower, how broad and spaced the states are, depends on the exact geometry, whether it takes the simple form of RS (Equation (5)) or something more complex. For example, if during compactification there were background fields in the bulk, the effective geometry could approximate RS near the UVbrane but deviate substantially near the IR [12, 13] and hence drastically changing the phenomenology.
In the simple case of RS, one can find the KK spectrum by solving the Einstein equation and the equation of motion for the KKgraviton: where are the roots of the Bessel function.
Finally, in RS or any other model of extradimensions, keeping a finite size for an extradimension (in our case, at ) is not trivial and usually relies on introducing new degrees of freedom. A popular mechanism of stabilisation is the GoldbergerWise [14], which calls on a new 5D scalar that mixes with the graviscalar (), whose vev controls , dynamically stabilising the size of the extradimension. This field can be written as a KKtower, and its light zero mode is usually called radion (already mentioned in the EFT section). Its mass is a free parameter and interacts with SM fields via the trace of the stress tensor, . As the strength of interactions is usually weaker than that of KKgravitons, in the rest of the paper, we only consider KKgravitons, but the discussion could be extended to the radion.
2.3.2. Deconstruction
Towers of resonances can appear in many ways, not just as a consequence of the compactification of extradimensions. In this section, we discuss the first alternative interpretation of nonresonant phenomena produced by broad/nearby resonances. Our setup is deconstruction [15], namely, the idea that certain types of gauge theories could resemble extradimensions as long as they provide a latticised version of a real (continuous) space coordinate (see Figure 5). The origin of deconstructed models goes far back to old models of mooses [16], series of new confining gauge sectors which at low energies exhibit interesting properties.
The simplest deconstruction framework assumes copies of , where refers to a new QCDtype colour, and Higgslike fields with a new VEV (). The Lagrangian of these new fields can be written as where and one typically assumes that all the fields couple with the same coupling ().
These VEVs break symmetry to the diagonal gauge group. The massmatrix for the gauge fields is given by and the gauge field mass eigenstates can be obtained by diagonalizing this matrix. The mass for the th gauge field can be written as which for approximates to
2.3.3. Clockwork/Linear Dilaton
Here, we discuss another example of models with limiting behaviour of broad/nearby resonances, clockwork models. They were born as a toy setup able to encapsulate some of the known phenomenology of extradimensions and deconstruction but allowing more flexibility of parameter choices. In particular, we will discuss one particular version of clockwork, the socalled continuum Clockwork/Linear Dilaton (CW/LD) model, which was proposed in Ref. [17] and whose nonresonant phenomenology has been studied in Ref. [18].
The metric that describes this scenario can be written as where the parameter , called clockwork spring, represents the curvature along the 5th dimension and , as in RS case, represents its size (see Figure 6).
There are many similarities with the RS framework, the compact 5D spacetime also sandwiched between the UVbrane (at ) and IRbrane (at ). The SM could be localised in the 5D bulk, but in the minimal scenario, it is confined on the IRbrane. The relation between the fundamental 4D and 5D scales is given by
In RS and the interaction scale in the IRbrane is order TeV while in CW/LD is directly order TeV.
The mass spectrum of the 4D KKgravitons tower is more spaced than in the RS case, as the masses for are given by
The effective interaction between the particles located at IRbrane and the KKgravitons can be written as
Note that in these models, the effective interaction scale, , depends on the mass of the KKgraviton; hence, each graviton couples differently to the brane particles except the zero mode that, as in the RS framework, couples with .
In order to stabilise the size of the extradimension, , in the CW/LD is common to place a dilaton field in the bulk. The spectrum of the dilaton’s KKtower is given by and the zero mode is identified as the radion field.
2.3.4. Other Models: Unparticles and Other Confining Sectors
We have described three scenarios with towers of resonances, which in some limits in the parameter space would lead to an almost continuum of broad/nearby resonances. In Section 3, we will discuss what this parameter space is.
Before moving onto the phenomenological aspects, we will discuss other theories which could mimic the phenomenology of warped extradimensions.
In the context of string theory, there is a huge body of work describing the idea that theories with weak gravity can be dual to strong gauge theories in a lowerdimensional space, inspired by the socalled AdS/CFT [19]. Indeed, those dualities between two types of theories seem to extend beyond the specific example of the AdS/CFT setup. To some qualitative level, one can understand models like RS as duals to a 4D strongly coupled theory, where the KKtower is interpreted as bound states of preon quark and gluons with increasing mass but the same quantum numbers. In QCD, we do observe to a certain extent a tower of resonances for each choice; for example, in the vector sector, we have observed the meson, higher up in mass the , followed by a continuum of broader . The properties of , and the continuum can be derived from the angular distributions of the final states.
In this context, the KKgraviton in RS is no exception: it can be interpreted as PauliFierz spintwo bound state of new quark and gluon preons. Indeed, it has been shown that the collider properties of the KKgraviton are indistinguishable from a hypothesised spintwo field from a new strongly coupled sector [20].
There are other possible alternatives to interpret this continuum, all closely related by dualities. For example, in Ref. [21], it has been proposed that black hole dynamics can lead to spintwo hair and that for lowenergy strong gravity models, these spintwo states could be produced at colliders [22].
Yet another alternative interpretation of a continuous spectrum is provided by the socalled unparticles [23]. These theories are based on the observation that a quasiconformal sector coupled to the SM would show up at low energies as a continuous emission of energy, producing then a nonresonant tail on some distributions of SM particles.
To summarise, any interpretation of nonresonant phenomena in terms of RS parameters, or deconstructed, or clockwork, could be recasted as certain models of strongly coupled gauge theories, quantum black hole production, or a new quasiconformal sector in Nature.
3. Phenomenological Signatures of Nonresonant Models
We now move onto the phenomenological description of the models described in the previous section.
For the EFT case, the interpretation procedure is quite straightforward and already in the experiment’s roadmap. There is a classification of possible deviations from the SM which could lead to excesses in tails, at [24] and to some extent at [25–27].
For the pseudoGoldstone case, only recently, the nonresonant opportunities have been explored in Ref. [2], where it was noted that for light particles whose resonant region is not accessible due to selection cuts, tails may be the only way to discover those states.
Regarding broad/nearby resonances, in Ref. [18], a description of nonresonant diphoton analysis was done in the context of Clockwork/Linear Dilaton.
In this section, we are going to explore under what circumstances our scenarios would lead to nonresonant phenomena. Our aim is to provide a simplified framework to interpret these tails in terms of the three scenarios: heavy, light, and broad. For concreteness, we will focus on a simple final state, the dijet, yet the conclusions can be generalized to other final states. We will start with a partonlevel discussion to move onto a more realistic hadron collider simulation.
3.1. PartonLevel CrossSections
3.1.1. The Heavy and Light Cases
In the partonic crosssection (), EFT effects would primarily appear as powers of , where is the scale of new heavy resonances, namely, through the interference of EFT with SM amplitudes: which leads to a growing amplitude with the energy of the event. For the dijet case, there are a number of dimension6 operators which could modify this crosssection, notably the pure gauge .
On the other hand, if the EFT operator is CPodd, e.g., , the partonic crosssection would be further suppressed as the leading contribution would come from the terms [28]:
which is steeper with and conversely more suppressed with the scale of the heavy resonances . Note that beyond CP properties, the interference with the SM could vanish in a number of situations (see, e.g., Ref. [29]).
Interestingly, for a light pseudoGoldstone boson, an axionlike particle, the offshell production is quite similar to square EFT effects [2]. In the offshell region, the partonic crosssection looks like so the growth with energy is also relative to the SM.
Hence, one can relate the EFT quadratic effects and axionlike parameters as follows: namely, the decay constant of a light pseudoGoldstone boson () plays the role of the scale of new heavy states and their coupling to SM particles.
3.1.2. The Broad Case: Matching of Warped, Clockwork, and Deconstructed Models
The LHC has placed strong limits on resonances coupled to SM particles, often in the multiTeV range. Now, imagine that these resonances were not isolated but came in a tower of multiple, closeby resonances, forming an almost continuum. In that case, usual bump searches would fail but also broad resonance searches, where broad often means and do not capture a quasicontinuum. In this case, only searches for excesses in tails could unveil their presence.
In the previous section, we have discussed many models which predict a spectrum with towers of states with the same quantum numbers. Here, we are going to discuss which regions of their parameter space brings these spaced towers close into a continuum. We will also obtain a dictionary among the three standard interpretations we discussed: warped extradimensions, clockwork, and deconstruction.
First of all, it is important to identify the free independent parameters of these three models. In the RS and CW/LD, the fundamental free parameters are the curvature along the fivedimension and the size . In deconstruction, they are the number of sites () and the scale times coupling of the interactions (). Nevertheless, the fundamental parameters are not the best option in order to study the phenomenology, as we show in Table 1, but the mass gap and coupling to SM particles.

Despite their differences, one should be able to match these three models in the nonresonant limit, as the continuum is roughly characterized by two parameters, the threshold (mass gap) and the height of the spectrum.
We can start our matching exercise with the RS and CW/LD models. In the RS framework, the mass gap between two consecutive resonances can be found using Equation (9):
where is the first graviton mass and we are assuming . In the CW/LD case, the masses are given by Equation (17), leading to in the limit. In the CW/LD model, each graviton couple is different to the energymomentum tensor (Equation (20)). In the limit (where the spectrum would approximate a continuum), the expression reduces to
The matching between the two spectra can be obtained by equating Equations (26) and (27), which leads to the following relations:
Now, using Equation (17), one can obtain the equivalent value.
In Figure 7, we can see an example of bringing both theories to the broad/nearby resonance limit and performing this matching. The interactions of KKresonances to SM particles are of the form given in Equation (8), hence grow with energy as
We can also bring the continuum spectrum closer to the first resonance. This situation occurs when (where is parameter). In this particular region, the width of the resonances is more or less the value of the gap, and we obtain an overlapping between the resonances. The total decay of the first graviton is where NP represents the new physics contributions (possible decays to nonSM final states). Assuming this information, we can write the condition for broadness as
In Figure 8, we show an example for this kind of spectrum, where we considered (the same order than SM contribution) while , chosen so that there is no conflict with the condition.
We have shown the relation between RS and CW/LD in the nonresonant regime. The same exercise can be done for deconstruction models. One can easily find that the deconstruction fundamental parameters are related to RS parameters as follows:
3.2. Nonresonant Tails at the Large Hadron Collider
In the previous section, we have discussed the differences among the three scenarios at the parton level: (i)EFT, with interference with SM: grows as (ii)Offshell light axionlike: grows as (iii)Broad/nearby resonances: quick increase from the mass gap location, grows as after that
Now, we compute numerically the total crosssection (including hadronization and PDF effects) at LHC energies. The results are shown in Figure 9, where one can observe the hierarchies we just described: the strongest slope comes from the offshell axionlike behaviour, followed by the EFT . The broad resonance case overcomes the mass gap to follow with the slope of dimensionfive interactions. We also plot the SM dijet production for comparison.
We model the tower of broad resonances with a simple modification of an existing Monte Carlo model provided in Ref. [30] and based on the implementation of spintwo resonances in Ref. [31]. The resonances start at 2 TeV and are set to be nearby, . We have set the coupling of all resonances to be the same, as in the RS models. As we are plotting signalonly normalized to the total crosssection, the specific value of is not relevant.
The EFT example has been computed using the Monte Carlo implementation in Ref. [3] and with operators enabling new four and threegluon vertices such as where we set and plotted the SM+EFT effect, including the dominant interference.
For the axionlike case, we used the Monte Carlo implementation from the study in Ref. [32] to compute the offshell axion exchange. As for the RS model, the specific value of is not relevant for this normalized distribution.
4. Outlook
In the current state of affairs at the LHC, the EFT framework is gaining support as a benchmark for interpretation of nonresonant phenomena. Within this framework, traditional searches for new physics, resonant searches, are replaced by searches for extended excesses, typically in the high tails of SM distributions.
The EFT is by no means the only way to think of nonresonant behaviour. Many scenarios, at least in some area of their parameter space, can only be explored in the nonresonant kinematic regions.
In this paper, we have described many of these types of models, classify them in terms of heavy, light, or broad/nearby particles, and have given a dictionary among them. For example, we have related parameters of axionlike models with EFT effects, and warped extradimensions with clockwork and deconstruction models.
Our aim was to provide a framework for reinterpretation of nonresonant limits and for future characterization of a possible confirmed excess. Our theory examples represent a diverse set of ideas in our area and include axionlike particles, extradimensional KKresonances, unparticles, deconstruction, clockwork, quantum black holes, and strongcoupling gauge duals of gravity theories.
We have discussed the parton and hadronlevel behaviour of dijet distributions, but all these models could be explored with the same detailed study of kinematic distributions of various final states, including missing energy+, massive diboson, Higgs+, and diHiggs.
We hope that this work will motivate a broader view of the physics potential of collider nonresonant searches.
5. EndNotes
See Refs. [33–35] for examples on how background fields can change the spectrum of KK states. See Ref. [36] for a recent discussion on the phenomenology of this operator and Ref. [37] for a canonical reference.
Data Availability
The paper is based on simulated data which can be obtained by contacting the authors.
Conflicts of Interest
The authors declare that they have no conflicts of interest.
Acknowledgments
V.S. acknowledges support from the UK Science and Technology Facilities Council ST/L000504/1.
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Copyright
Copyright © 2021 Miguel G. Folgado and Veronica Sanz. This is an open access article distributed under the Creative Commons Attribution License, which permits unrestricted use, distribution, and reproduction in any medium, provided the original work is properly cited. The publication of this article was funded by SCOAP^{3}.