Searcharxiv⌕ Search

arXiv · 2610.23390

Neural Network Representation of Generalized Parton Distributions (NNGPD)

Abstract

Extracting generalized parton distributions (GPDs) from experimental observables, the convolution structures denoted as Compton form factors (CFFs), requires solving an intrinsic inverse problem. We presented results using NNGPD, a flexible regression method based on a physics-informed neural-network framework, for reconstructing GPDs using integral constraints -- including CFFs and Mellin moments -- and symmetry and endpoint constraints. The approach does not require pointwise training information on the underlying GPDs. Closure tests using pseudodata generated from a phenomenological model demonstrate the ability of the framework to reproduce the principal features of the underlying distributions across a range of kinematics. A Bayesian neural-network formulation is also introduced to address uncertainties associated with the reconstruction. Finally, we discussed a broader question in GPD phenomenology: whether the complete momentum-fraction dependence of GPDs is necessary to extract physical quantities such as partonic angular momentum. This motivates investigating approaches that infer Mellin moments directly from experimentally constrained CFFs, while quantifying the remaining ambiguities.

Explore related subjects

Keep this discovery

Explore connections, maps & timelines

BibTeXRIS

Simonetta Liuti, Jitao Xu, Ho Jang, Zaki Panjsheeri, Gia-Wei Chern, Yaohang Li, Douglas Q. Adams, Michael Engelhardt, Gary R. Goldstein, Adil Khawaja, Huey-Wen Lin, Saraswati Pandey, Kemal Tezgin. 2026-10-16. Neural Network Representation of Generalized Parton Distributions (NNGPD). https://arxiv.org/abs/2610.23390

Cite the original work for its findings. Save a collection to share your selection of sources.

KEEP EXPLORING

Related papers

Dark Photon mediated Inelastic Dark Matter in Cosmology, Astrophysics and Colliders

We explore the phenomenology of Dark Photon iDM ($A^\prime$IDM) where the Standard Model (SM) is extended by a dark sector containing an additional $U(1)_D$ gauge symmetry with coupling $α_D$ under which all SM particles are neutral, and that couples to the SM hypercharge gauge boson through a kinetic mixing parameter $ε$. The model contains two Majorana states $χ_1$ and $χ_2$ with $δ=M_{χ_2}-M_{χ_1}>0$ and $χ_1$ the dark matter candidate, and a dark photon $A^{\prime}$ with mass $M_{A^{\prime}}$. Our analysis represents an integration of existing ones, where only specific benchmarks of the A'IDM scenario have been discussed. We perform a complete scan of the parameters of the model ($M_{χ_1}$, $δ$, $M_{A^{\prime}}$, $ε$, $α_D$) and discuss the $χ_1$ relic abundance, its direct and indirect searches, as well as potential signals from astrophysics and accelerators. Our scan shows that $α_D=α_{EM}$ is not disfavored, as some previous analyses, limited to specific benchmarks, may suggest. We also find that when the $χ_1$ relic density matches observation direct and indirect searches are not kinematically accessible. On the other hand we find that the projected luminosity of FASER, a detector searching for Long Lived Particles (LLP) decay at the LHC, can probe or rule out the parameters space of the model for $M_{χ_1}\lesssim$ 7 GeV, 100 MeV$\lesssimδ\lesssim$300 MeV and $M_{A^\prime}\lesssim$25 GeV. This range of parameter could be significantly extended by the FASER 2 upgrade proposed for the High-Luminosity phase at the LHC. The parameter space probed by LLP seaches partially overlaps with that probed by $χ_1$ capture in neutron stars.

hep-ph↗

A New Look at the X Compositeness from its Lineshape

Available data on the $X(3872)$ lineshape have been fitted with a Flattè parametrization derived from an effective Lagrangian in which $X$, $D$, and $D^*$ are all elementary fields. A molecular $X$, i.e., a deuteron-like bound state of $D$ and $\bar{D}^*$, must instead be described by an effective theory where the $X$ field is initially absent or introduced as an auxiliary, unphysical, field, yielding a lineshape parametrization that differs significantly from the Flattè one. We demonstrate, in the analogous theory of nucleons with an auxiliary deuteron field, that this parametrization gives a fully consistent description of $np\to\text{deuteron}\to np$ scattering data, and motivate applying the same method to the $X$ lineshape. The analysis proposed here is novel and has not previously been carried out on the available data.

hep-ph↗

Correlated $b \to s$ and $s \to d$ Rare Semileptonic Transitions in the Standard Model Effective Field Theory

The persistent anomalies observed in $b \to s\,(\ell^+\ell^-,\,ν\barν)$ transitions continue to provide strong motivation for exploring possible extensions of the Standard Model (SM). Motivated by these discrepancies, we present a comprehensive analysis of semileptonic flavor changing neutral current processes within the Standard Model Effective Field Theory (SMEFT), encompassing both $b \to s\,(μ^+μ^-,\,ν\barν)$ and $s \to d\,(μ^+μ^-,\,ν\barν)$ transitions. We perform a combined fit to $b \to s\,(μ^+μ^-,\,ν\barν)$ observables, allowing the relevant dimension-six Wilson coefficients to be complex. We find that the four-fermion operators involving left-handed quark and lepton doublets provide the preferred description of the current $b \to s$ data, while the electroweak operator modifying the $Z$-boson couplings also plays an important role in improving the fit. We show that flavor-universal SMEFT couplings lead to strongly enhanced rare semileptonic kaon decay branching ratios, in conflict with current experimental bounds and thus motivating the implementation of Minimal Flavor Violation. In particular, we demonstrate that flavor-symmetric frameworks based on $U(3)^5$ and $U(2)^5$ naturally restore the required CKM hierarchies and bring the predicted kaon observables into agreement with present data. We further analyze the differential distributions with respect to the dineutrino invariant mass squared $q^2$, as well as the reconstructed variable $q^2_{\mathrm{rec}}$, in $B \to K^{(*)}ν\barν$ decays, demonstrating their sensitivity to different new physics operators. In addition, we investigate the impact of complex Wilson coefficients on $\mathcal{CP}$ asymmetries in $B \to K^{(*)}μ^+μ^-$ decays and find that percent-level effects can arise in specific $q^2$ regions.

hep-ph↗