Abstract
We study the correlation between different sets of parton distributions (PDFs). Specifically, viewing different PDF sets as distinct determinations, generally correlated, of the same underlying physical quantity, we examine the extent to which the correlation between them is due to the underlying data. We do this both for pairs of PDF sets determined using a given fixed methodology, and between sets determined using different methodologies. We show that correlations have a sizable component that is not due to the underlying data, because the data do not determine the PDFs uniquely. We show that the datadriven correlations can be used to assess the efficiency of methodologies used for PDF determination. We also show that the use of datadriven correlations for the combination of different PDFs into a joint set can lead to inconsistent results, and thus that the statistical combination used in constructing the widely used PDF4LHC15 PDF set remains the most reliable method.
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1 Uncertainties and correlations of parton distributions
Correlations between parton distribution functions (PDFs) are an important ingredient in the accurate determination of PDFs and their uncertainties, notoriously a current major challenge of contemporary collider precision phenomenology [1]. The correlation between PDFs and physical observables is a tool used to understand both the impact of PDF uncertainties on predictions, and the impact of individual observables on PDF determination, as originally emphasized in Ref. [2], and subsequently exploited for Higgs phenomenology in Sect 3.2 of Ref. [3]. However, more fundamentally, correlations are an integral part of the determination of PDF uncertainties.
Indeed, just as full information on data uncertainties requires knowledge of the experimental covariance matrix, and not just the uncertainty on individual datapoints, full information on PDF uncertainties is encoded in the pointbypoint covariance matrix between all pairs of PDFs at any pair of points:
and associated correlation matrix
where \(f^p_a(x,Q_0^2)\) is the pth PDF with momentum fraction x and a chosen reference scale \(Q^2_0\) in a given PDF set \(\Phi _a\) and we denote by \(\mathrm{Var}[f^{p}_a]\) the variance, i.e. the diagonal element of the covariance matrix
In what follows, we will use indices p, q to label PDF flavors, and indices a, b to label PDF sets. So p runs over gluon, up, antiup, down, ..., while a runs over NNPDF3.1, NNPDF4.0, MSHT20, CT18.... Henceforth, we will generally consider the case in which \(x=x'\) and suppress the x and \(Q_0^2\) dependence, so for instance we will write the covariance Eq. (1) as
In Eqs. (1–4), E denotes the average over the probability distribution of PDFs; so the PDF covariance matrix \( \mathrm{Cov}[f_a^p,f_a^q](x,x')\) is the second central moment of the joint probability distributions of PDFs. It can be computed in a standard way [4] given a representation of this probability distribution, specifically as a multigaussian in parameter space for a given PDF parametrization, or as a Monte Carlo sample of PDF replicas.
The correlation between PDF flavors Eq. (2) (Fcorrelation, henceforth) is a standard concept, and it has been widely computed and used. However, one may also define a different kind of correlation: the correlation between PDF sets [5]. Each PDF set is a determination of the same underlying true PDFs. As such, each set can be viewed as a different determination of the same underlying physical quantity. Generally, two determinations of the same quantity are characterized both by an uncertainty, and a correlation between them. In the presence of uncertainties, each determination may be thought of as a random variable. So for a distinct pair of determinations one can define their covariance and correlation, which may then be combined using the standard methodology that is used for the combination of correlated measurements [6, 7]. Indeed, the correlation between two determinations expresses the amount of new information that each determination introduces: two completely independent determinations are fully uncorrelated, while two completely correlated determinations are simply repetitions of the same determination.
Hence we can view any particular PDF set \(\Phi _a\) containing PDFs \(f^p_a(x,Q_0^2)\) and their uncertainties as an instance of a probability distribution of PDF determinations [8], just like any measurement is an instance of a probability distribution of measurement outcomes. The covariance matrix Eq. (4) can then be viewed as a special case of a more general covariance matrix
and corresponding correlation
where again, for simplicity, we only consider the case \(x=x'\) and suppress the dependence of the PDFs on x and \(Q_0^2\).
Equations (5, 6) provide the covariance and correlation, generally between two different PDF flavors, across two different PDF sets, \(\Phi _a\) and \(\Phi _b\). We will therefore refer to them as crosscovariance and crosscorrelation, respectively. The average in Eq. (5) is now performed over the full probability distribution of PDF sets, i.e. of distinct determinations, of which sets \(\Phi _{a}\) and \(\Phi _{b}\) are two generic instances. How this might be done in practice is something that we will discuss below.
It is clear that if we take \(p=q\) the crosscovariance and crosscorrelation Eqs. (5, 6) reduce to the covariance and correlation between the two different determinations of PDF \(f^p\) provided by sets \(\Phi _a\) and \(\Phi _b\). Indeed, in this case
and the corresponding correlation is
Equations (7, 8) provide respectively the covariance and correlation between two different determinations \(f^p_a(x,Q_0^2)\), \(f^p_b(x,Q_0^2)\) of the pth PDF at point x, viewed as two different determinations of the underlying true value, i.e. the covariance and correlation between PDF sets, or Scovariance and Scorrelation.
The Fcorrelation and Scorrelation are both special cases of the crosscorrelation: the former, specializing to the case in which one compares two different PDFs from the same PDF set, and the latter, specializing to the case in which one compares the same PDF in two different PDF sets. The Fcovariance is a covariance in a space of PDFs, within a given set. The Scovariance is instead the covariance in a space of different PDF sets, which is a rather less trivial concept. Specifically, if a Monte Carlo representation is adopted, then a PDF set \(\Phi _{a}\) is represented as a set of Monte Carlo PDF replicas \(\{f_{a}^{p,(r)}(x,Q_0^2)\}\), and the Fcovariance Eq. (1) can be computed by simply averaging over these replicas. In order to achieve something similar for the Scovariance, one would first need to construct replicas that span the space of possible independent determinations of a given PDF – including, say, the results that might have been found by different groups using different methodologies. This is clearly nontrivial.
Elucidating the nontrivial aspects of averaging over the space of PDF determinations is the main goal of this paper.
The reason why the structure of the space of PDF determinations is subtle is that the outcome of a PDF determination does not only depend on the underlying data. Indeed, a PDF determination amounts to the determination of a probability distribution in a space of functions [8], using as input a discrete set of datapoints: hence the outcome is not unique. Specifically, if a very general functional form, such as a neural network, is adopted, then there is an ensemble of best fits of equal quality to fixed underlying data. It has indeed been shown explicitly [9] in the NNPDF framework that if the same data are fitted over and over again, a distribution of bestfit PDFs is obtained, rather than a single answer. In an approach such as the CT18 PDF determination [10] a more restrictive parametrization is adopted and a unique best fit is found, but then the fit is repeated with a large number underlying functional forms also leading to a distribution of best fits.
It is clear that the distribution of best fits for fixed underlying data provides a contribution to the uncertainty (and more generally to the covariance matrix) that is unrelated to the data uncertainty. Accordingly, when computing the Scorrelation Eq. (8) there is a contribution to it which comes from integrating over the space of PDFs which correspond to fixed underlying data. But of course, the correlation by construction lies between \(1\) and \(+1\), so this also implies that inevitably the datainduced component of the Scorrelation is strictly less then one, because it does not include the component that is not datadriven. We will refer to the nondatadriven component as “functional correlation” for short (without committing ourselves to its precise origin). Note that a priori the nondatadriven component also contains uncertainties related to theory choices, such as the value of \(\alpha _s\), or missing higher order corrections. These are however in principle (though not necessarily in practice) easy to account for by simply varying the relevant parameters, and we will not discuss them here: we will always consider theory assumptions to be fixed.
In the remainder of this paper, we will investigate the relative sizes of the datadriven and functional components. This will be done by computing explicitly the datadriven Scorrelation for PDFs determined from the same underlying data. The question we will address is then: how large is the functional component of the correlation, in comparison to the datadriven one – negligible, sizable, perhaps even dominant?
This question is not purely academic, but in fact quite important for applications. First, as mentioned, the Fcorrelation Eq. (2) is routinely used to estimate the impact of a given dataset on the PDFs. But then, surely knowledge of the size of the datadriven component of the Scorrelation is necessary for such an assessment, because it tells us how much the PDF is determined by the underlying data. Furthermore, correlations between independent measurements are normally used when combining different measurements of the same quantity [6]. Combined PDF sets, such as the PDF4LHC15 set [4], can be viewed in a similar way, namely, as the combination of different determinations of the true PDF. At present, these combinations are performed by simply assuming that all PDF sets in the combination are equally likely. However, one might think that they should instead be combined as correlated measurements, and that a determination of the datadriven Scorrelation might be useful to this goal [11]. It is then interesting to investigate possible ways to implement such a procedure, and their consequences.
We will answer these questions by computing the datainduced Scorrelation explicitly. In Sect. 2 we will present results for the datadriven component of the Scorrelation, both between different PDF sets determined from the same underlying data and with the same methodology, and between pairs of PDF sets determined using the same data, but different methodologies. We will use the results to shed light on the origin of the PDF Scorrelation, and we will explain how Scorrelations can be used as a diagnostic tool when comparing different methodologies. In Sect. 3 we will discuss the implications of our result for the construction of combined PDF sets. After discussing the PDF4LHC15 prescription for the combination of PDF sets in Sect. 3.1, in Sect. 3.2 we will discuss how this could be replaced by a correlated combination, and the consequences of doing so.
2 PDF crosscorrelations and Scorrelations
2.1 Correlated replicas
Our goal is to compute the crosscorrelation between PDF sets, which we can determine from the crosscovariance Eq. (5). We assume that a Monte Carlo representation is used for PDF sets. This assumption is not restrictive, since Hessian PDF sets can be converted into Monte Carlo sets using the methodology of Ref. [12]. A PDF set \(\Phi _a\) is then represented by a set of N PDF replicas \(\{{f_a^{p(r)}}: r = 1,\ldots N\}\) of the pth PDF flavor \(f_a^p\), that provide an importance sampling of the probability distribution of the the PDF set. We assume for simplicity that the number of PDF replicas N is fixed and sufficiently large that a faithful representation of the underlying probability representation is obtained, and we will provide an estimate of the uncertainty due to finitesize effects. Also, we assume that the PDF sets that are being considered all provide a faithful representation of the underlying data, so that they would for instance pass a closure test [13, 14].
Each replica is equally probable, so replicas are statistically uncorrelated, and estimators of functions of the PDFs are given by simple averages over the replicas,
Thus in particular the mean and the Fcovariance of the PDF set are given by
Henceforth, we will use angle brackets to denote the replica average, while the symbol E used in Sect. 2.1 denotes the generic average.
The way PDF replicas are constructed is by first constructing a Monte Carlo representation of the underlying data, i.e. by producing an ensemble of data replicas, such that the ensemble mean reproduces the central value of the original data, and the covariance over the ensemble reproduces the data covariance matrix. These data replicas can then be fitted with whatever methodology is chosen: i.e., a fit to each data replica is performed thereby leading to a bestfit PDF for the given replica. The ensemble of best fits then provides the Monte Carlo representation of PDFs. Note that this can be done in conjunction with any PDF fitting methodology, such as, for example, the MSTW methodology discussed in Ref. [12].
When computing the Fcovariance Eqs. (1, 10), the same replica is used to determine \(f_a^p\) and \(f_a^q\), so in particular
It is important to understand that each PDF replica \({f_a^p}^{(r)}\) is obtained by fitting to an individual data replica, but, as mentioned, the result of this fit is generally not unique. Indeed, as also mentioned, a distribution of different PDFs is found even when fitting repeatedly the same underlying data. In the NNPDF methodology, that uses a very general neural network as underlying parametrization, this simply follows from the fact that the bestfit neural network trained to fixed underlying data is not unique: each training to fixed underlying data produces a different but equally good answer. In other methodologies this is achieved by considering an ensemble of different functional forms fitted to the same data, each of which gives a different best fit [10, 15, 16]. Clearly, the spread of PDFs fitted to fixed underlying data is completely unrelated to the data uncertainties and correlations. Thus, in order to get the full variance, covariance, \({f_a^p}^{(r)}\) and \({f_a^q}^{(r)}\) in Eq. (11) must be PDFs that correspond to the same PDF replica: i.e. to one fixed fit to a fixed data replica.
We would now like to turn to the computation of the Scovariance and Scorrelation between two PDF sets \(\Phi _a\) and \(\Phi _b\), that we can write as
Naively, one could think that this might be computed by starting with two sets of PDF replicas representing the two PDF sets, \(\{{f_a^p}^{(r)}\}\) and \(\{{f_b^p}^{(r)}\}\). However it is clear that if these PDF replicas are chosen independently, then the Scovariance, and thus the Scorrelation Eq. (8) will always vanish, because the replicas are uncorrelated between sets. Indeed, the same applies to the computation of the standard Fcovariance Eq. (10). Namely, if two independent sets of N PDF replicas chosen at random from the same PDF set \(\Phi _a\) are combined into a set of 2N independent PDF replicas then
and the Scovariance vanishes, where the equality (and thus the vanishing) hold in the large N limit, i.e. within the accuracy of the Monte Carlo representation.
In order to compute the correlation between PDF sets we must thus determine the Scovariance by using PDF replicas that are correlated between PDF set \(\Phi _a\) and PDF set \(\Phi _b\). In order to understand what this means, assume for a moment, for the sake of argument, that the data do determine uniquely the bestfit PDF: so that for each data replica there is a unique PDF replica. In this case, when we label each PDF replica \({f_a^p}^{(r)}\) the index r corresponds uniquely to the specific data replica to which the PDFs have been fitted. Assuming that the two given sets are obtained using two different methodologies, this unique PDF best fit might be slightly different in sets \(\Phi _a\) and \(\Phi _b\), so \({f_a^p}^{(r)}\not = {f_b^p}^{(r)}\). The Scorrelation between PDF sets a and b can be computed by simply making sure that the same correlated replica \(\{{f_a^p}^{(r)}\}\) and \(\{{f_b^p}^{(r)}\}\) is used: the crosscovariance Eq. (12) is then generally nonzero, since the PDF replicas are correlated by the choice of the common underlying data replica r. This also automatically implies that the PDF set has unit correlation to itself, as it must, because if \(a=b\) then the unique answer \({f_a^p}^{(r)}\) is used in the computation of averages.
However, in actual fact, we know that this is generally not the case: the data replica does not uniquely determine the PDF. So, in a realistic case, for each data replica r and for each PDF set \(\Phi _a\) there is a distribution of best fits \(\{{f_a^p}^{(r,r')}\}\) where now the index \(r'\) runs over “functional” or methodological replicas: for each data replica, r, the index \(r'\) labels all other aspects that determine the answer. For instance, if parametrization dependence is estimated by varying the functional form, as in Refs. [10, 15, 16], then \(r'\) would label the different functional forms that are used. If \(a=b\), then for fixed r and fixed \(r'\) the same answer is obtained and the correlation is one: each PDF set has unit correlation to itself. If \(a\not =b\), then the Scorrelation is found by varying both r and \(r'\) in a correlated way. If however only r is correlated, and the average over \(r'\) is performed in an uncorrelated way, the corresponding component of the correlation vanishes according to Eq. (14).
So, if only r is correlated, then the computation provides a nonvanishing component of the Scorrelation, namely, its datadriven component, but it misses the functional component, that would also require correlating \(r'\), and thus it does not give the full correlation. Now, it is clear that if we take \(a=b\) in Eq. (12) then the Scovariance reduces to the simple variance and the Scorrelation must equal one, at least in the limit of large N: it is the correlation of a PDF set to itself. However, if only the datadriven component is included in the computation of the crosscorrelation, this consistency check is not satisfied: rather, the result may come out to be less than unity. This deviation from unity tells us, crudely speaking, the extent to which the PDFs are determined by the underlying data. The deviation from one measures the size of the decorrelation due not to having integrated over functional replicas in a correlated way: it tells us how significant the functional component of the Scorrelation is.
It is interesting to ask whether the functional component of the crosscorrelation could be computed directly. In order to do this, one would need “functional replicas”, namely, one would need to explicitly construct replicas \(\{{f_a^p}^{(r,r')}\}\), such that varying the index \(r'\) fully spans the possible best fits obtained from a fixed underlying data replica r. This could perhaps be done when varying aspects of the methodology that influence the final outcome, and that are controlled by a parameter: this parameter would then be fixed to take the same value when computing the Scovariance Eq. (12). We will see an explicit example below, when discussing correlated preprocessing. However, this appears to be nontrivial in general for nonparametric methodology aspects that determine in which of the many equivalent best fits a particular minimization will end up.
In what follows, we will focus on the computation of the datadriven component of the Scorrelation. This means that we will use Eq. (12), and we will view the replica index r as an index that labels the underlying pseudodata replica. Then, when comparing two different PDF sets \(\Phi _a\) and \(\Phi _b\), the replicas \(\{{f_a^p}^{(r)}\}\) and \(\{{f_b^p}^{(r)}\}\) are fitted to the same underlying data. However, we will also “compare a PDF set \(\Phi _a\) to itself”. By this, we mean that we will compute the Scorrelation (or crosscorrelation) by using in Eq. (12) two sets of PDF replicas fitted to the same data replicas using the same methodology, \(\{{f_a^p}^{(r,r')}\}\) and \(\{{f_a^p}^{(r,r'')}\}\), where, as above r labels the data replica while the indices \(r'\), \(r''\) span the space of fits to the same data replica. Hence in particular
In practice, since we have no control on the values of \(r'\), \(r''\), \(\{{f_a^p}^{(r,r')}\}\) and \(\{{f_a^p}^{(r,r'')}\}\), are simply two different fits from PDF set \(\Phi _a\) to the same rth underlying data replica. This is to be contrasted to Eq. (11), used in the computation of the Fcorrelation, in which the same fit to the same data replica is used: effectively, Eq. (11) corresponds to taking \(r'=r''\) in Eq. (15). We will refer to the situation in which Eq. (15) is used as comparing a PDF set to itself, and we will refer to the resulting correlation as the datadriven component of the correlation.
2.2 The datainduced Scorrelation and crosscorrelation
We compute the datainduced component of the Scorrelation, both between a pair of PDF sets determined from the same underlying data using two different methodologies, and between a PDF set and itself, as defined at the end of Sect. 2.1. Specifically, we consider the NNPDF3.1 methodology as presented in Ref. [17], and the NNPDF4.0 methodology recently used for the NNPDF4.0 PDF set [14]. The NNPDF4.0 methodology differs from the NNPDF3.1 methodology mostly because of the choice of PDF parametrization and minimization algorithm, and its main feature is that it is obtained through a hyperoptimization procedure [18]. Here, the details of these two methodologies are not relevant, and it suffices to know that they are both faithful, and compatible with each other (as we will verify explicitly).
In order to compute the Fcorrelations and Scorrelations shown in this section, we have generated several PDF sets of approximately 1000 PDF replicas each, using the opensource NNPDF code [19]. These PDF replicas have been generated by performing fits to a dataset which consists of the deepinelastic scattering (DIS) data used for the NNPDF3.1 PDF determination, as listed in Table 1 of Ref. [17]. The kinematic coverage of this data in the \((x,Q^2)\) plane is shown in Fig. 1. This and all other plots in this paper are produced using validphys [19, 20]. The reasons for choosing a DISonly dataset are to limit the use of computational resources, as well as to deal with a dataset involving a single, wellunderstood process, thereby avoiding possible complications related to tensions between data, slow perturbative convergence, and other issues that could obscure our conclusions. Uncertainties on the Scorrelations due to the finite size of the replica sample are estimated using a bootstrapping procedure. Further details on the computation of the Scorrelation are given in Appendix A.
To begin with, we have constructed four PDF sets, all determined from the same underlying data replicas: two using the NNPDF3.1 methodology, and two using the NNPDF4.0 methodology. Whereas a detailed comparison of PDFs produced using the NNPDF4.0 and NNPDF3.1 methodologies is given in Ref. [14], in Fig. 2 we show a representative comparison of the gluon PDF as determined using these two methodologies. The general features of the comparison discussed in Ref. [14] are apparent from this example: namely, first, that results found with either methodology are compatible within uncertainties and central values are generally quite similar, and second, that the NNPDF4.0 methodology leads to rather smaller uncertainties, so generally whereas the NNPDF4.0 central value is within the NNPDF3.1 uncertainty band, the NNPDF3.1 central value is not within the rather smaller NNPDF4.0 uncertainty band.
As in all NNPDF determinations, it can be checked explicitly that independently determined PDF replicas all provide a consistent representation of the same underlying probability distribution. Namely, we can check that the standard deviation of the mean of \(N_{\mathrm{rep}}\) replicas is equal to \(\sigma /\sqrt{N_{\mathrm{rep}}}\). In order to perform this check, we have generated yet another set of PDF replicas with the NNPDF4.0 methodology, now based on a new set of data replicas. In Fig. 3 we show the distance between the central values and uncertainties of the two different sets of PDF replicas determined using the NNPDF4.0 methodology trained on different sets of data replicas. The distance (defined in Appendix B of Ref. [9]) is the mean square difference of central values in units of the standard deviation of the mean. It is apparent that indeed its value is of order one, as it ought to be. This shows that as the number of replicas increases, both central values and uncertainties of PDFs converge to the mean and standard deviation of the underlying probability distribution.
Having verified that samples of PDF replicas behave as expected, we now proceed to the computation the datainduced component of the Scorrelation Eq. (8), as discussed in Sect. 2.1. Results are shown in Fig. 4, where we show the Scorrelation between two sets of replicas determined with the NNPDF3.1 methodology (orange); between two sets of replicas determined with the NNPDF4.0 methodology (green); and between a set of replicas determined with the NNPDF3.1 methodology and a set of replicas determined with the NNPDF4.0 methodology (blue). The error bands show the 2\(\sigma \) uncertainty due to the finite size of the replica set, estimated using bootstrapping (see Appendix A).
It is apparent from the plots that the datainduced PDF Scorrelation drops very quickly to zero outside the data region, as it ought to. For light quarks, the correlations drop to zero for \(x\lesssim 10^{4}\) and \(x > rsim 0.4\); while the data region is rather smaller for the the gluon and heavy quarks. This is because in a DISonly PDF determination the gluon PDF is only determined indirectly by scaling violations, while the PDFs for heavier quarks are determined by charged current data, i.e. mostly by fixedtarget neutrino DIS data. However, interestingly, even in the middle of the data region the Scorrelation of pairs of PDF sets determined using the NNPDF3.1 methodology is typically around 40% and never exceeds 60%. The Scorrelation of PDF sets determined using the NNPDF4.0 methodology, in turn, is typically around 60% and never exceeds 80%. The Scorrelation between PDF sets determined using the NNPDF3.1 and NNPDF4.0 methodologies, finally, is very similar to the Scorrelation between the pair of NNPDF3.1 PDF sets.
As discussed in Sect. 2.1, the deviation from unity of the datadriven Scorrelation when comparing of a PDF set to itself is a measure of the size of the functional component of the Scorrelation. Both for the NNPDF3.1 and NNPDF4.0 methodologies, this deviation is substantial. Note that, as shown in Fig. 3, any two independent sets of replicas for the same set have the same mean and uncertainty within finitesize fluctuations, and that these fluctuations scale as expected and in particular go to zero in the limit of a large number replicas. Note also that the deviation of the Scorrelation from 100% is much larger than the uncertainty due to the finite size of the replica sample, so the correlation loss cannot just be due to an insufficient number of replicas.
The fact that the Scorrelation of NNPDF3.1 PDFs is smaller than that of NNPDF4.0 PDFs is consistent with the fact [14, 18, 21] that the NNPDF4.0 methodology leads to smaller uncertainties than the NNPDF3.1 methodology, even though both can be shown to be faithful using closure tests [9, 14]. Indeed, the only way PDF sets determined from the same underlying data can have different uncertainties is if one of the two has a smaller functional (i.e. nondatadriven) component of the uncertainty. But then we would expect that the methodology characterized by a smaller functional uncertainty also has a smaller functional Scorrelation: i.e. that it is determined to a greater extent by the underlying data. This is indeed what happens here: NNPDF4.0 has a smaller uncertainty for a fixed dataset, and accordingly a larger Scorrelation.
It is interesting to observe that the datainduced component of the Scorrelation between NNPDF3.1 and NNPDF4.0 PDFs is almost always similar to that of the PDF set that has the smallest correlation to itself, namely NNPDF3.1 (a possible exception being the charm PDF, which is a special case because in a DISonly fit it is almost undetermined). This suggests a “weakestlink” explanation: the data are more weakly correlated to NNPDF3.1 than to NNPDF4.0, and so inevitably the datadriven correlation between NNPDF3.1 and NNPDF4.0 is dominated by this weaker correlation. This is apparent, for instance, in the small x region, where the datadriven Scorrelation of NNPDF3.1 to itself is significantly weaker than that of NNPDF4.0.
All this suggests that the datadriven component of the Scorrelation between PDF sets for a given methodology can be used as a criterion for the assessment of the efficiency of the methodology itself, with the interpretation that a methodology leading to higher crosscorrelation is more efficient. Namely, PDFs determined using a methodology characterized by higher Scorrelation have a smaller functional component of the Scorrelation, i.e. they are to a greater extent determined by the underlying data. So for instance the weaker Scorrelation of NNPDF3.1 at small x suggests that in this region the NNPDF3.1 uncertainties could be reduced without loss of accuracy, as is indeed the case [14].
In order to further investigate the functional component of the Scorrelation, we have produced sets of PDF replicas in which some methodological choices are correlated or decorrelated. First, we have produced a set of replicas in which preprocessing is also correlated. To understand this, recall that neural networks used to parametrize PDFs include a preprocessing function [18], whose parameters are randomly varied between replicas. We have thus produced a new pair of NNPDF4.0 replicas in which not only the data, but also the preprocessing exponents are correlated: so in Eq. (12), replicas \({f_{a}^p(x,Q_0^2)}^{(r)}\) and \({f_{b}^p(x,Q_0^2)}^{(r)}\) are not only fitted to the same underlying data, but also have the same value of the preprocessing exponents.
Results are shown in green in Fig. 5, compared to the previous results of Fig. 4, shown in orange. It is clear that in the data region, where the datainduced Scorrelation is largest, the extra correlation due to preprocessing is negligible. As PDFs extrapolate further away from the data region, the contribution due to preprocessing is increasingly large: for instance for the gluon at large \(x > rsim 0.4\) the datainduced correlation rapidly drops to zero as \(x\rightarrow 1\), but the correlation due preprocessing makes up for the decrease and in fact it somewhat exceeds it as the kinematic boundary at \(x=1\) is approached.
Furthermore, we have produced a PDF set, based on the NNPDF4.0 methodology, but with a different architecture of the neural net, i.e., different number of layers and layer sizes. This is thus effectively a variation of the NNPDF4.0 methodology. Results, also shown in Fig. 5 (in blue), demonstrate that this specific aspect of the methodology has little impact: the Scorrelation is essentially the same as in the case where the architecture of the neural networks is the same in the two sets being compared. This shows that these two methodologies lead to very similar results, which in turn suggests that correlating the neural network architecture would have a less significant impact than that of correlating preprocessing.
These two examples illustrate how, at least in principle, all components of the Scorrelation could be determined, namely, by correlating all methodological aspects that determine the final result. As already discussed, whereas this is easily done for parametric choices (like the values of the preprocessing exponents), it is rather more difficult for nonparametric aspects, such as, for instance, the choice of minimization settings. These aspects are of course closely tied to the nonuniqueness of the best fit for given data, which leads to functional uncertainties.
Finally, we compare, for a fixed methodology, the datadriven component of the Scorrelation for a pair of PDF flavors, to the crosscorrelation between them: in Fig. 6 results are shown for the up and the down PDFs, both for the NNPDF3.1 methodology and the NNPDF4.0 methodology. Clearly, unlike the diagonal Scorrelation in the flavor basis Eq. (8), the correlation between two different PDF flavors need not be positive. This is indeed seen in the figure, namely, the up and down PDFs turn out to be anticorrelated at large x. Furthermore, one would generally expect any crosscorrelation between two different PDF flavors to be weaker than the Scorrelation – indeed, if all sources of Scorrelation were included, the Scorrelation would be 100%. This is again borne out by the explicit computation, that shows that the crosscorrelation is generally smaller in modulus than the Scorrelation. Note that for the less efficient NNPDF3.1 methodology, for which all Scorrelations are smaller, as already discussed, the crosscorrelation is accordingly smaller in modulus.
In the same figure we also compare, again for a fixed methodology, the datainduced component of the crosscorrelation between the up and down PDFs to the standard Fcorrelation Eq. (2). Note that if the crosscorrelation was entirely datadriven, for a fixed methodology these two quantities would coincide. But in actual fact they differ because in the computation of the Fcorrelation, Eq. (11) is used (the replicas are fully correlated), while in the computation of the crosscorrelation, Eq. (15) is used (the replicas are only correlated through data). Whenever the Scorrelation is sizable, the datainduced component of the crosscorrelation, and the Fcorrelation are very close to each other. This means that the functional component of the PDF uncertainty is essentially uncorrelated between different PDFs, i.e. that the standard Fcorrelation is due to the correlation between the underlying data. This is as one expects, and justifies using PDF correlations to estimate the impact of data uncertainties on PDFs uncertainties and conversely.
However, when the datainduced component of the Scorrelation is small, then the Scorrelation can differ significantly from the Fcorrelation. This is clearly seen when comparing the updown correlation in the region \(10^{4}\lesssim x \lesssim 10^{2}\) computed with the NNPDF3.1 methodology to that computed with the NNPDF4.0 methodology. With the NNPDF4.0 methodology, the datadriven Scorrelation in this region is large, and the standard updown correlation is quite close to the crosscorrelation. With the NNPDF3.1 methodology, on the other hand, the datadriven Scorrelation is almost vanishing. This means that, with NNPDF3.1 methodology, PDFs in this region are completely dominated by functional uncertainty, which then screen out the PDF correlation when computing the crosscorrelation. In other words, the functional component of the Scorrelation (between a PDF and itself) is generally nonnegligible, while the functional component of the crosscorrelation (between two different PDFs or two different x values) is generally quite small.
3 Combined PDF sets
As already mentioned in Sect. 1, combined PDF sets have been produced [4, 22], with the goal of providing a common, conservative PDF determination. The underlying idea is that socalled “global” PDF sets, namely PDFs determined using the widest possible amount of experimental information available at a given time, differ due to theoretical and methodological assumptions. If these assumptions all satisfy reasonable criteria of reliability, these different PDF determinations are considered to be equally likely, and thus a conservative choice is to combine them into a single determination. One may then reasonably ask whether this combination might be constructed in such a way as to explicitly take account of the crosscorrelation between PDF sets.
3.1 The PDF4LHC15 combination
The PDF4LHC15 prescription [4] for combining different PDF sets \(\Phi _a,\,\Phi _b,\dots \) may be described as follows. All sets being combined are turned into a Monte Carlo representation, as discussed in Sect. 2.1, i.e. each of them is represented by a set of N PDF replicas \(\{{f_i^p}{(r)}: r = 1,\ldots N\}\), where the index i runs over the sets that are being combined. The combined set is then defined simply as the union of the replicas in the individual sets: specifically to combine two sets \(\Phi _a\) and \(\Phi _b\), we select randomly \(\frac{1}{2}N\) replicas from each set, and then define the replicas for the combined set \(\{F^p\} = \{{F^p}^{(r)}: r = 1,\ldots N\}\) as
The combination assumes that, in the absence of an objective criterion for deciding on the relative probability of the different sets, they are equally probable, and thus that we should take the same number of replicas from each set.
The combined set \(\{F^p\}\) is then treated in the same way as the individual sets for the calculation of estimators, with the averages taken over all the replicas in the set according to Eq. (9). Thus in particular the mean of any PDF in the combined set is immediately seen to be given by
while the Fcovariance between two PDFs is
Thus in the combined set, the central PDF is the mean of the central PDFs in each set (up to the usual statistical uncertainties of order \(1/\sqrt{N}\)), whereas the uncertainties are always greater than the mean of the uncertainties, the extra term being due to the spread of the central predictions. This is as it should be: when the sets used in the combination disagree, the uncertainty is increased.
The expressions Eqs. (17, 18) can be generalized straightforwardly to the combination of n PDF sets, by taking N/n replicas at random from each (always keeping \(N\gg n\) of course): then
and
For large n the extra term in the covariance of the combination increases the result according to the covariance of the distribution of central values, since in the pairwise sum there are \(n(n1)\) terms.
The PDF4LHC15 prescription is based on the assumption that the PDF sets that are being combined, viewed as measurements of the true underlying PDF, are all equally likely, which means that they have approximately the same uncertainty and are approximately 100% correlated, i.e. they are not independent. Indeed, independent (uncorrelated or partly correlated) measurements of the same quantity a priori bring in new information on the true value, so the uncertainty on their combination is always smaller or equal to the uncertainty of any of the measurements that are being combined, (see e.g. Ref. [7]), as we shall discuss further in Sect. 3.2 below.
In fact, an important property of the PDF4LHC15 combination prescription is that if the constituent PDF sets \(\Phi _a\) are perfectly correlated, meaning that taking averages over replicas of the different PDF sets all give the same result, the combination also gives this result. Note that perfectly correlated sets will still be distinct, in the sense that the replicas will not be the same: it is only the averages over the full ensemble of replicas that are the same, in the limit when the number of replicas N becomes very large. An example are the various replica sets considered in Sect. 2.2, all based on the NNPDF4.0 methodology: both the two sets compared in Fig. 3, with replicas based on different underlying data replicas, and those compared in Fig. 4, based on correlated underlying data replicas. For these pairs of sets, \(\langle f^p_{a}\rangle = \langle f^p_{b}\rangle \) for all a, b, and \(\mathrm{Cov}[f_a^p,f_a^q] = \mathrm{Cov}[f_b^p,f_b^q]\). This is of course true irrespective of the number of sets n used in the combination: it is just the same as when combining several batches of PDF replicas from a given PDF set (such as NNPDF4.0) into a single larger replica set.
To ensure that these assumptions are reasonable, that is, the PDF sets used in the PDF4LHC15 combination are highly correlated, and as such can reasonably be combined by giving equal weight to each set, a number of criteria was adopted [4]:

Each set is based on a global dataset, and in practice these global datasets are very similar, both in size and content.

Theoretical calculations are performed to the same order in \(\alpha _s\), using a VFNS, and benchmarked against one another.

External parameters such as \(\alpha _s\) and quark masses are given common values where possible.

Each PDF determination includes procedural and functional uncertainties in the adopted methodology.
Furthermore, an extensive benchmarking was performed in order to make sure that indeed uncertainties from the various sets were approximately equal, and that these criteria were sufficient to ensure that the PDF sets used in the combination could be be meaningfully assigned equal probability in the combination.
3.2 Correlated PDF combination
It is clear that even though the PDF sets included in the PDF4LHC15 combination are highly correlated, the correlation is manifestly not complete. Even assuming that the benchmarking and parameter settings can achieve complete agreement, there will still be some decorrelation through the choice of global dataset, and in the different methodologies used by the different groups. It has therefore been suggested [11] that a more precise and accurate result might be obtained if different PDFs are combined as independent, partly correlated measurements of the underlying true PDF. The logic is that, even in the presence of a common underlying dataset, each PDF determination, based on a different methodology, might be extracting different information from the data, just like different detectors could provide partly independent though correlated information on the same physical phenomenon. A correlated combination might then be advantageous because it would lead to a more precise and accurate prediction.
Unbiased correlated measurements of the same underlying observable can be combined in a standard way (see e.g. Sect. 7.6 of Ref. [7]). Specifically, viewing the expectation values \(E[f_a^p]\) \(a=1,2,\dots \) of PDFs as measurements of an underlying true value, their correlated combination is a weighted average, that we can in turn view as the expectation value of the probability distribution for a combined determination \(\tilde{F}^p\):
with weights \(w^p_a\) given by
where \(\mathrm {Cov}^{1}[f_a^p, f_b^p]\) is the matrix inverse of the Scovariance. The square uncertainty on the combination Eq. (21) is the variance of the probability distribution of \(\tilde{F}^p\), given by
Of course, all this relies on the assumption that the measurements are unbiased, and that the correlation between them, namely, the Scorrelation Eq. (8), can be reliably computed.
Even so, the combination Eq. (21) is subject to several caveats. Specifically, the weights \( w^p_a\) Eq. (22) depend not only on p but also on x because the Scorrelation does (recall Eq. (5)), and consequently, the combined PDF Eq. (21) does not automatically satisfy sum rules. Furthermore, for the same reason, the result of the combination will generally depend on the scale at which it is performed, because with xdependent weights even if the PDF sets \(f_a^p\), for each a satisfy QCD evolution equations, the combination does not. Finally, in order to compute physical observables using the combined PDFs, knowledge of the diagonal uncertainty Eq. (23) is not sufficient: rather, the full crosscovariance matrix for all p, q and all x, y would be required. This could be done in principle by sampling the PDFs, computing their Fcorrelation, and then turning the result into a Hessian representation by using techniques similar to those of Ref. [23]. A way out of all these problems might be to perform the weighted combination Eq. (21) not at the level of PDFs, but rather at the level of physical observables. However, this has the further disadvantage that crosscovariances and weights would have to be recomputed for each new observable.
Be all that as it may, our goal here is not to investigate the most efficient way to implement the weighted combination, but rather, to explore the implications of performing a correlated weighted PDF combination according to Eqs. (21–23). As discussed in Sect. 3.1, in practice the PDF sets in the PDF4LHC15 combination have approximately equal uncertainties. When this is the case, the weights Eq. (22) are all approximately equal, and constant (independent of x), and then all the aforementioned problems can be ignored. Indeed, when we combine two PDF sets \(\Phi _a\) and \(\Phi _b\) such that \( \mathrm{Var}[f_{a}^p]= \mathrm{Var}[f_{b}^p]\) the Scovariance is
from which it follows, using Eq. (22), that \(w_a=w_b=\frac{1}{2}\).
This equal weight situation can be very simply implemented in a Monte Carlo approach, in a completely equivalent way. Indeed, assuming that Monte Carlo replicas are available for two PDFs, \(\Phi _a\) and \(\Phi _b\), the correlated combination is found by combining the two sets of replicas into a single replica set given by
for \(r = 1,\ldots , N\). Then \(E[\tilde{F}^p]=\langle F^{p(r)}\rangle = \frac{1}{2}(\langle {f_a^p}^{(r)}\rangle + \langle {f_b^p}^{(r)}\rangle )\), is in agreement with Eq. (21) when \(w_a=w_b=\frac{1}{2}\). The Fcovariance Eq. (18) evaluated over the replica set Eq. (25) is now given by
Note that when expressed in terms of the replicas from the original sets \(\Phi _a\) and \(\Phi _b\) the Fcovariance between two PDFs in the combined set now depends on the crosscovariance between the corresponding PDFs of the original sets \(\mathrm{Cov}[f_a^p,f_b^q]\) Eq. (6). Considering the diagonal case \(p=q\) in Eq. (26), the variance of the PDFs of the combined set now depends on the Scorrelation, and, using \( \mathrm{Var}[f_{a}^p]= \mathrm{Var}[f_{b}^p]\), Eq. (26) with \(p=q\) reduces to
which is the same as Eq. (24) when \(a=b\).
Using the correlated Monte Carlo approach, the properties of the correlated combination are especially transparent. Specifically, it is clear that the uncertainty computed using Eq. (26) is always smaller than that found using the PDF4LHC15 combination. To see this, note that the correlation \(\rho [f_a,f_b]\le 1\) or equivalently \(\mathrm{Cov}[f_a,f_b]\le \sqrt{\mathrm{Var}[f_{a}]}\sqrt{\mathrm{Var}[f_{b}]}\). It follows that the square uncertainty on \(F^p(x,Q_0^2)\) satisfies the inequality
where in going from the first to the second inequality we have trivially made use of the fact that \(\frac{1}{2}(x+y)^2\le x^2+y^2\), and the third inequality follows from the observation that the second term in Eq. (18) is nonnegative.
The second inequality Eq. (28) has the obvious implication that, as already mentioned in Sect. 2.1, and as seen explicitly from Eq. (27), whenever the correlation \(\rho [f^p_a,f^p_b]<1\) the uncertainty of the correlated combination \(\tilde{F}^p\) is smaller than either of the uncertainties on \(f_a^p\) or \(f_b^p\), that have been assumed to be approximately equal when forming the correlated combination according to Eq. (25), \(\mathrm{Var}[f^p_{a}]\approx \mathrm{Var}[f^p_{b}]\).
The third inequality Eq. (28) has the perhaps less obvious implication that even if the two sets are fully correlated, so \(\rho [f^p_a,f^p_b]=1\), the uncertainty on the PDF4LHC15 combination \(F^p\), can be larger that the uncertainty of either \(f_a^p\) or \(f_b^p\), even though the uncertainty on the correlated combination \(\tilde{F^p}\) is the same as that on both \(f_a^p\) and \(f_b^p\). This happens whenever the central values of the two sets are not the same \(\langle f^p_a\rangle \not =\langle f^p_b\rangle \).
This is a situation that the combination formula Eq. (21) cannot accommodate. Indeed, the uncertainty of this correlated combination can never exceed that of the two determinations that are being combined. This follows from the assumption that the two determinations are unbiased estimators of the same underlying true value. Upon these assumptions, unit correlation means that the covariance matrix has a vanishing eigenvalue, so the two determinations have the same central value and uncertainty.
However, it is clearly possible to have two random variables that have unit correlation but do not have the same central value (or uncertainty). In particular the correlation of any two sets of random variables \(f^r_1\) and \(f^r_2\) is invariant under the linear transformations \(f^r_1\rightarrow c_1f^r_1+k_1\), \(f^r_2\rightarrow c_2f^r_2+k_2\), for any constants \(c_1, c_2, k_1, k_2\), which change their mean values and variances. In the Bayesian combination one simply takes the point of view that the two measurements are equally likely determinations of the underlying true quantity, so a priori they might be fully correlated, and yet their mean values and variances might differ. In such a situation, the variance of the PDF4LHC15 combination always comes out larger than those of the determinations that are being combined. So, both the second and the third inequalities Eq. (28) become equalities only if PDF sets \(\Phi _a\) and \(\Phi _b\) are identical, i.e. they have the same central value, uncertainty, and unit correlation.
These results are easily generalized to the case of n PDF sets:
In this case
and again equality can only be achieved when there is complete equivalence between all the PDF sets in the combination, i.e. when \(f^{p(r)}_a=f^{p(r)}_b\) for all r, p and for all pairs a, b. Otherwise, the correlated combination inevitably reduces uncertainties.
Even disregarding the issue related to PDF sets that have different central values despite being very highly correlated, the main problem with the reduction in uncertainty in the correlated combination is that it is reliable only if the crosscorrelation has been correctly estimated. In particular, if the crosscorrelation is underestimated, then the uncertainty on the combination is underestimated: in the most extreme case, in which two PDFs are fully correlated, but the crosscorrelation is incorrectly determined to be very small, the uncertainty on the combination is underestimated by a factor \(\sqrt{n}\) (assuming again the uncertainties of the n starting PDFs are approximately the same).
In practice, the problem resides in the construction of the correlated replicas to be used combination Eq. (25): this ought to be done in such a way that the averages over replicas in Eq. (26) lead to a faithful determination of the Fcovariance and the Scovariance. As we discussed in Sect. 2.1, if the sets of replicas \(\{{f_a^p}^{(r)}\}\), \(\{{f_b^p}^{(r)}\}\) that are being combined in Eq. (25) are randomly selected from the two sets, then the correlation vanishes regardless of its true value, see Eq. (14). If one selects replicas \({f_a^p}^{(r)}\), \({f_a^p}^{(r)}\) that are fitted to the same underlying data replica, then the Scorrelation does not vanish, but it is generally underestimated because it only includes its datadriven component, as explicitly shown in Sect. 2.2.
The problem is especially severe when combining n different sets, because in this case underestimating the correlation between each pair of sets will lead to an increasingly large underestimation of the uncertainty on the combination as the number of sets increases. This is because in this case one is effectively assuming that the differences between the different determinations are due to each of them being a partly independent measurement, and as such doing more and more determinations reduces the uncertainty indefinitely.
In order to expose the problem, we have considered an implementation of the combination Eq. (21). We have constructed ten sets of \(N_{\mathrm{rep}}\) PDF replicas, all determined from the same \(N_{\mathrm{rep}}\) underlying data replicas. In practice we take \(N_\mathrm{rep}=43\) because this is the largest number we got after applying the procedure discussed in Appendix A. We have then computed the ten by ten Scorrelation matrix Eq. (12) for each PDF and each x value, and we have combined the ten sets using Eq. (21). We have explicitly checked that this is equivalent to instead using Eq. (29) to combine the ten sets in a single set with 43 replicas. This is demonstrated in Fig. 7 where two representative PDFs determined using either method are compared and seen to agree. This shows that the correlated Monte Carlo combination Eq. (29) is equivalent to the combination using the correlation matrix Eq. (21).
We have then compared this correlated combination to the PDF4LHC15 combination. The latter of course simply consists of putting together all replicas in a single 430 replica PDF set. Results are shown in Fig. 8. It is evident that while the PDF4LHC15 combination gives by construction the correct answer (since in this case the PDF is simply being combined to itself), the correlated combination leads to a rather smaller uncertainty. Clearly this is absurd. The reduction in uncertainty is the consequence of the fact that the Scorrelation computed using Eq. (12) only includes the datainduced component. This underestimates the true correlation, because as we have seen in Sect. 2.2 (see in particular Fig. 4) it leads to a Scorrelation which is rather lower than one, while in actual fact all these PDFs are fully correlated. The uncertainty reduction is amplified by having combined ten different sets.
We thus see that combining PDFs determined from the same underlying data as if they were correlated measurements leads to an incorrect answer because it neglects the fact that a sizable component of the PDF correlation is not datadriven. Indeed, if one did determine PDF uncertainties in this way, one would reach the paradoxical conclusion that PDF uncertainties can be made smaller at will by simply repeating many times the PDF determination with the same underlying data replicas.
Because of the difficulty in accurately estimating the nondatadriven component of the selfcorrelation, which is generally significant, this will be the generic scenario. As an especially striking example of this situation, in Fig. 9 we compare the relative uncertainty on the gluon PDF that we find if the gluon is determined using the NNPDF4.0 methodology, the NNPDF3.1 methodology, or the uncorrelated (PDF4LHC15) or correlated combination. As already discussed (see Fig. 2), the uncertainty found using the NNPDF3.1 methodology is rather larger than that found using the NNPDF4.0 methodology. Because, as also discussed, central values are very close, the uncertainty of the PDF4LHC15 combination, Eq. (18) is essentially the average of the uncertainties with the two methodologies. However, the uncertainty on the correlated combination is actually smaller than either of the uncertainties with the two methodologies that are being combined. One would thus reach the paradoxical conclusion that combining PDFs obtained with the more precise NNPDF4.0 methodology with the previous less precise NNPDF3.1 would actually lead to a reduction in uncertainty.
We conclude that a correlated combination inevitably leads to uncertainty underestimation and it cannot be considered as an alternative to the PDF4LHC15 combination, even though the latter might lead to uncertainties that are a little conservative.
4 Conclusions
Treating PDF sets as independent measurements of the same underlying quantity provides a new window into the properties of PDFs, specifically the efficiency of the methodology used to determine the PDFs, and it has allowed us to address in a quantitative way the possibility of performing correlated combinations of PDF sets.
We have studied correlations between pairs of PDF determinations, which we call PDF crosscorrelations. By computing these crosscorrelations for PDF replicas fitted to the same underlying data replicas, we have shown that the correlation of a PDF set to itself does not come out to be 100% if only the part of the correlation which is due to the underlying data is included. This is due to the fact that a component of the PDF uncertainty, and thus also of the PDF correlation, is not due to the underlying data, but rather of functional origin, namely, related to the fact that the data do not determine uniquely the PDFs. This realization is what allows us to use crosscorrelations as a tool in the assessment of the efficiency of the methodology. Indeed, a higher datadriven crosscorrelation is an indication of a more efficient methodology, i.e. a methodology that correlates more strongly the PDF to the underlying data.
We have furthermore addressed the feasibility of combining PDF sets as correlated measurements. Specifically, we showed that combining PDFs as correlated measurements will lead the uncertainty of the combination to be underestimated whenever the PDF crosscorrelation is underestimated. This will typically happen unless it is possible to determine its functional, nondatadriven component.
In this paper we focused on PDFs produced using the NNPDF framework, in which neural networks are used as basic underlying interpolating functions. The neural network parametrization is redundant, and a bestfit is obtained by not aiming for the minimum of a figure of merit, which would correspond to overlearning, but rather using a variety of techniques such as crossvalidation to determine the optimal best fit. In this approach, the presence of a component of the PDF covariance matrix which is not due to the underlying data follows from the fact that this best fit is not unique: an ensemble of bestfit PDFs with nonvanishing covariance is found even when repeatedly fitting the same underlying data.
However, many other modern PDF sets (e.g. CT18 [10] and MSHT20 [16]) rely on parametrizing PDFs with a fixed functional form, for which a unique best fit to any given set of data exists, and is given by the minimum of a figure of merit. Note that this remains true even when used in conjunction with a Monte Carlo approach, in which the fixed functional form is fitted to an ensemble of data replicas [12]. In this case, the functional uncertainty is the result of variations of the functional form, possibly combined with a choice of “tolerance”, whereby an inflation of the \(\chi ^2\) variation corresponding to onesigma is introduced (either in the data replica generation in a Monte Carlo approach, or in the fitting in a Hessian approach).
A direct computation of the functional contribution to the covariance matrix appears to be very difficult when using the NNPDF approach, and even more challenging when comparing the NNPDF approach to approaches based on an underlying fixed functional form and tolerance. This is due to the difficulty in estimating and even more correlating uncertainties which are not related to the underlying data. In this sense, the results presented here are a first step towards a deeper understanding of origin and meaning of PDF uncertainties.
A general lesson to be learned from this exercise appears to be that if the aim is to improve the accuracy of PDF determination, it is more promising to develop better fitting and diagnostic tools to obtain a more reliable result, than to combine preexisting determinations in the hope of reducing uncertainties in the combination.
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Acknowledgements
We thank all members of the NNPDF collaboration for numerous discussions, and Alessandro Candido, Juan Rojo and Christopher Schwan for a careful critical reading of the manuscript and several comments. SF thanks Simone Amoroso, Daniel Froidevaux and Bogdan Malaescu for discussions on PDF combination. RDB is supported by the U.K. Science and Technology Facilities Council (STFC) Grant ST/P000630/1. SF and RS are supported by the European Research Council under the European Union’s Horizon 2020 research and innovation Programme (Grant agreement n.AdG 740006).
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Appendix A: Computing crosscorrelations in the NNPDF framework
Appendix A: Computing crosscorrelations in the NNPDF framework
We provide here some details on the computation of the crosscovariance Eq. (12) using NNPDF methodology.
In the NNPDF methodology the data replicas are generated based on a Monte Carlo method with random initialization. Furthermore, input data are split into a training subset used by the optimization algorithm and a validation subset used to validate the optimization [9]. This split is performed randomly for each PDF replica. In order to compute the datainduced component of the crosscorrelation therefore we have made sure that the two PDF sets that are being compared are fitted to the same data replicas, with the same trainingvalidation split.
Furthermore, not all fits end up in the final PDF set, but only those that pass postfit criteria specified in Ref. [9]. Because these criteria are applied a posteriori, it might happen that, for a given underlying data replica, the criteria are only passed by one of the the two PDF replicas that are being compared. For the computation of the crosscorrelation, we only include in the final set PDF replicas for which both sets have passed the criteria.
The Scovariance is then computed using Eq. (12), or its obvious generalization in the case of the crosscovariance Eq. (5).
In order to estimate the uncertainty on final results due to the finite size of the replica sample we have used a bootstrapping method [24, 25]. Specifically, we apply a Monte Carlo algorithm to perform a resampling “with replacement” of the PDF replicas. This is of course done synchronously for both PDF sets between which the correlation is calculated. We then calculate the PDF correlation using these resampled PDF sets. This routine is repeated many times to obtain a precise estimate of the standard error of the PDF correlation. The magnitude of the uncertainty decreases with the inverse square root of the number of PDF replicas used to determine the PDF correlation. We have performed this procedure with 200 resampled sets. The value was chosen comparing the 2\(\sigma \) standard deviation and the 95% confidence interval, and checking that for any flavor and any value of x they agree.
Finally, we have by default computed the crosscorrelation at the scale \(Q_0=1.7\) GeV, and we have checked that by repeating the computation with different choices of \(Q_0\) up to 100 GeV results are unchanged.
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Ball, R.D., Forte, S. & Stegeman, R. Correlation and combination of sets of parton distributions. Eur. Phys. J. C 81, 1046 (2021). https://doi.org/10.1140/epjc/s10052021098636
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DOI: https://doi.org/10.1140/epjc/s10052021098636