{"total":12,"items":[{"citing_arxiv_id":"2606.28218","ref_index":9,"ref_count":1,"confidence":0.9,"is_internal_anchor":false,"paper_title":"Neural-Network extraction of TMDs with SIDIS data","primary_cat":"hep-ph","submitted_at":"2026-06-26T16:09:55+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":7.0,"formal_verification":"none","one_line_summary":"Neural-network parametrization yields first global unpolarized TMD extraction from DY plus SIDIS data at N³LL, producing broader PDFs with smaller uncertainties than DY-only NN fits.","context_count":0,"top_context_role":null,"top_context_polarity":null,"context_text":null},{"citing_arxiv_id":"2606.28440","ref_index":13,"ref_count":1,"confidence":0.9,"is_internal_anchor":false,"paper_title":"Radiation Damage of TF-1 and PbWO$_4$ Crystals with 20 MeV Electrons","primary_cat":"cond-mat.mtrl-sci","submitted_at":"2026-06-26T08:02:11+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":3.0,"formal_verification":"none","one_line_summary":"TF-1 lead glass shows strong optical degradation after 5.6×10^14 20 MeV electrons while PbWO4 remains largely unaffected after an additional 2.1×10^15 electrons, with thermal annealing increasing transmittance.","context_count":0,"top_context_role":null,"top_context_polarity":null,"context_text":null},{"citing_arxiv_id":"2606.13077","ref_index":24,"ref_count":1,"confidence":0.9,"is_internal_anchor":false,"paper_title":"A generalised-$k_t$ jet algorithm for Deep Inelastic Scattering","primary_cat":"hep-ph","submitted_at":"2026-06-11T09:00:10+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":6.0,"formal_verification":"none","one_line_summary":"The authors define a generalised-k_t jet algorithm family for DIS in the Breit frame, extending the prior p=0 case, and test its use for struck-quark jet identification and non-perturbative effects.","context_count":0,"top_context_role":null,"top_context_polarity":null,"context_text":null},{"citing_arxiv_id":"2606.06263","ref_index":10,"ref_count":1,"confidence":0.9,"is_internal_anchor":false,"paper_title":"Spin-orbit correlation of quarks within quarkonium","primary_cat":"hep-ph","submitted_at":"2026-06-04T15:05:19+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":4.0,"formal_verification":"none","one_line_summary":"Computes spin-orbit correlation distributions for charmonium and B_c mesons by linking parity-odd EMT matrix elements to light-front dynamics.","context_count":0,"top_context_role":null,"top_context_polarity":null,"context_text":null},{"citing_arxiv_id":"2605.15288","ref_index":1,"ref_count":1,"confidence":0.9,"is_internal_anchor":false,"paper_title":"Status of Barrel Imaging Calorimeter in Korea for the Electron-Ion Collider","primary_cat":"physics.ins-det","submitted_at":"2026-05-14T18:02:17+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":2.0,"formal_verification":"none","one_line_summary":"Korean group contributes to silicon sensor testing, prototype assembly, beam tests, and simulations for the Barrel Imaging Calorimeter at the EIC.","context_count":0,"top_context_role":null,"top_context_polarity":null,"context_text":null},{"citing_arxiv_id":"2605.07681","ref_index":13,"ref_count":1,"confidence":0.9,"is_internal_anchor":false,"paper_title":"Test-Beam Performance of the AstroPix Silicon Sensor for Imaging Calorimetry","primary_cat":"physics.ins-det","submitted_at":"2026-05-08T12:50:23+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":6.0,"formal_verification":"none","one_line_summary":"AstroPix-v3 sensors reach 68% hit efficiency in test beams and distinguish electromagnetic from hadronic showers via hit multiplicity and spatial spread when combined with a Pb/SciFi calorimeter.","context_count":0,"top_context_role":null,"top_context_polarity":null,"context_text":null},{"citing_arxiv_id":"2605.00502","ref_index":1,"ref_count":2,"confidence":0.9,"is_internal_anchor":false,"paper_title":"Multiplicative matching of neutral current deep-inelastic scattering processes at next-to-leading order in PYTHIA 8","primary_cat":"hep-ph","submitted_at":"2026-05-01T08:25:34+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":7.0,"formal_verification":"none","one_line_summary":"A multiplicative matching scheme reweights Born-level events in PYTHIA 8 so the first parton shower emission follows the real NLO matrix element, improving agreement with HERA DIS data.","context_count":1,"top_context_role":"background","top_context_polarity":"background","context_text":"sively in many generators and collision systems [11-16]. The application of these methods has been centered on processes studied at the Large Hadron Collider (LHC), but recently applying such algorithms to deep-inelastic scatter- ing (DIS) processes has gained some attention as well, main motivation being to provide accurate simulations for the fu- ture experiments at the Electron-Ion Collider (EIC) [17]. The POWHEG method for neutral-current (NC) and charged- current DIS [18] has been introduced in the POWHEGBOX framework [13, 19], with an extension to the polarized case in [20]. Another approach presented in [21] introduces a Monte Carlo factorization scheme including NLO correc- tions. In the context of the SHERPAframework [22], the MC@NLO method provided the basis for simulations of the"},{"citing_arxiv_id":"2604.15122","ref_index":8,"ref_count":1,"confidence":0.9,"is_internal_anchor":false,"paper_title":"Symmetry Preserving Contact Interaction Approaches: An Overview of Meson and Diquark Form Factors","primary_cat":"hep-ph","submitted_at":"2026-04-16T15:10:25+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":2.0,"formal_verification":"none","one_line_summary":"An overview of the contact interaction model shows it describes the mass spectrum and form factors of forty mesons and their diquark partners with comparisons to lattice QCD and other approaches.","context_count":1,"top_context_role":"background","top_context_polarity":"background","context_text":"dynamical chiral symmetry breaking and explicit quark-mass effects to be disentangled. The experimental program at the Electron-Ion Collider is expected to enable high-precision measurements of pion and kaon FFs over an extended range of momentum transfer, thereby providing stringent tests for theoretical approaches and strong motivation for unified and symmetry-preserving descriptions of meson structure [ 8]. Finally, to close this section, Figs. 9 and 10 show the elastic FFs of the pion and the kaon, the lightest mesons in this channel, together with experimental measurements from JLab and Amendolia [105-107]. For comparison, we also include recent calculations performed within BSE framework, which provide space-like EFFs for PS mesons, covering both light and heavy-light systems"},{"citing_arxiv_id":"2604.13769","ref_index":5,"ref_count":1,"confidence":0.9,"is_internal_anchor":false,"paper_title":"Fully Heavy Pentaquarks with JETHAD: A High-Energy Viewpoint","primary_cat":"hep-ph","submitted_at":"2026-04-15T12:01:08+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":4.0,"formal_verification":"none","one_line_summary":"Fully heavy pentaquark fragmentation functions PQ5Q1.0 are completed for charm and bottom flavors and used to compute NLL/NLO+ semi-inclusive production rates at future colliders.","context_count":1,"top_context_role":"background","top_context_polarity":"background","context_text":"[2] High-Luminosity Large Hadron Collider (HL-LHC) : Preliminary Design Reportdoi:10.5170/CERN-2015-005. [3] High-Luminosity Large Hadron Collider (HL-LHC): Technical Design Report V. 0.1 4/2017.doi:10.23731/CYRM-2017-004. [4] E. Chapon, et al., Prospects for quarkonium studies at the high-luminosity LHC, Prog. Part. Nucl. Phys. 122 (2022) 103906.arXiv: 2012.14161,doi:10.1016/j.ppnp.2021.103906. [5] R.AbdulKhalek,etal.,ScienceRequirementsandDetectorConceptsfortheElectron-IonCollider:EICYellowReport,Nucl.Phys.A1026 (2022) 122447.arXiv:2103.05419,doi:10.1016/j.nuclphysa.2022.122447. [6] R. Abdul Khalek, et al., Snowmass 2021 White Paper: Electron Ion Collider for High Energy Physics, in: 2022 Snowmass Summer Study, 2022.arXiv:2203.13199. [7] M."},{"citing_arxiv_id":"2604.13157","ref_index":6,"ref_count":1,"confidence":0.9,"is_internal_anchor":false,"paper_title":"Proton Structure from Neural Simulation-Based Inference at the LHC","primary_cat":"hep-ph","submitted_at":"2026-04-14T18:00:00+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":8.0,"formal_verification":"none","one_line_summary":"Neural simulation-based inference on unbinned top-quark pair data at 13 TeV yields improved gluon PDF precision over traditional binned analyses while incorporating experimental and theoretical uncertainties.","context_count":1,"top_context_role":"background","top_context_polarity":"background","context_text":". . . . . . . . . . . . . . . . . . 48 2 1 Introduction The determination of the collinear substructure of the proton, encoded in its parton distribution functions (PDFs) [1-4], is one of the key targets of the LHC, its High-Luminosity upgrade (HL-LHC) [5], as well as of other ongoing and planned experiments, from the Electron Ion Collider (EIC) [6] to FASER [7] and the Forward Physics Facility (FPF) [8,9]. Pinning down the proton PDFs has a two-fold motivation. On the one hand, to address open questions in Quantum Chromodynamics (QCD) such as the behaviour of the gluon in the small-xregion where novel dynamical regimes may arise [10-12], the pattern of matter/antimatter asymmetries in the nucleon [13, 14], and the heavy quark content of the proton [15-17]."},{"citing_arxiv_id":"2604.09071","ref_index":5,"ref_count":1,"confidence":0.9,"is_internal_anchor":false,"paper_title":"A numerical implementation of the NLO DIS structure functions in the dipole picture","primary_cat":"hep-ph","submitted_at":"2026-04-10T07:53:01+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":5.0,"formal_verification":"none","one_line_summary":"Numerical program implementing NLO DIS structure functions in the dipole picture with massive quarks rewritten for stable computation.","context_count":1,"top_context_role":"background","top_context_polarity":"background","context_text":"In order to find conclusive evidence of saturation effects, it is crucial to match the precision of the theoretical calculations to that of the experimental data. The HERA measurements of the total DIS cross section mentioned above are very precise, and in the next decade similar precision measurements of electron-nucleus scattering will be performed at the Electron-Ion Collider (EIC)[5]. In this work we develop a general purpose numerical program that, when given as input the dipole-target scattering amplitude evolved by the Balitsky-Kovchegov equation at next-to- leading order[6-9], can be used to evaluate the DIS structure functions in the dipole pic- ture[10]at next-to-leading order accuracy . Specifically , we implement the NLO DIS impact"},{"citing_arxiv_id":"2511.08432","ref_index":16,"ref_count":1,"confidence":0.9,"is_internal_anchor":false,"paper_title":"Design and Performance Studies of a Granular Thin HCAL-MuID Detector for the EIC Optimized for AI-Based Reconstruction","primary_cat":"physics.ins-det","submitted_at":"2025-11-11T16:37:50+00:00","verdict":null,"verdict_confidence":null,"novelty_score":null,"formal_verification":null,"one_line_summary":null,"context_count":0,"top_context_role":null,"top_context_polarity":null,"context_text":null}],"limit":50,"offset":0}