{"total":10,"items":[{"citing_arxiv_id":"2605.22559","ref_index":1,"ref_count":1,"confidence":0.88,"is_internal_anchor":false,"paper_title":"Identification and mitigation of memory block timing issue in ITk ABCStar during ASIC production","primary_cat":"physics.ins-det","submitted_at":"2026-05-21T14:41:41+00:00","verdict":"ACCEPT","verdict_confidence":"LOW","novelty_score":3.0,"formal_verification":"none","one_line_summary":"Identification of a memory control timing issue in ABCStar ASIC and mitigation by increasing core voltage to 1.25 V and clock duty cycle to restore production yields above 80%.","context_count":0,"top_context_role":null,"top_context_polarity":null,"context_text":null},{"citing_arxiv_id":"2605.16756","ref_index":22,"ref_count":1,"confidence":0.88,"is_internal_anchor":false,"paper_title":"Higgs Physics with the XFEL Compton $\\boldsymbol{\\gamma\\gamma}$ Collider Concept at $\\boldsymbol{\\sqrt{s}=125}$ GeV","primary_cat":"hep-ph","submitted_at":"2026-05-16T02:11:31+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":7.0,"formal_verification":"none","one_line_summary":"An XFEL Compton gamma-gamma collider at 125 GeV with a set transformer deep learning classifier on particle-flow point clouds can achieve high-precision Higgs measurements across hadronic, semi-leptonic, and leptonic final states including H to strange quarks.","context_count":0,"top_context_role":null,"top_context_polarity":null,"context_text":null},{"citing_arxiv_id":"2605.13964","ref_index":85,"ref_count":1,"confidence":0.88,"is_internal_anchor":false,"paper_title":"A New Source of Millicharged Particles: Secondary Showers in the LHC Forward Absorber","primary_cat":"hep-ph","submitted_at":"2026-05-13T18:00:03+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":7.0,"formal_verification":"none","one_line_summary":"Secondary cascades in the TAXN absorber produce a substantial millicharged particle flux that complements primary production and boosts FORMOSA signals by ~50% for m_χ below 0.1 GeV.","context_count":1,"top_context_role":"background","top_context_polarity":"background","context_text":"production inπ 0 andηdecays when SIBYLL and the Pythia tune are used instead of EPOS-LHC. After propagating downstream from the IP, these neu- tral particles reach the neutral-particle absorber and ini- tiate EM and hadronic showers. In the HL-LHC era, the TAN will be replaced by the new TAXN absorber, located approximately 130 m from the primary IP [85]. For our study, the TAXN is modeled as a solid copper block with dimensions 1 m×1 m×4 m. 2 We simulate shower development within the TAXN using theGeant4 toolkit (version 11.3), employing theFTFP BERTphysics list [86-88]. The resulting EM and hadronic cascades produce a large multiplicity of secondary particles, including pho- tons,e ±, and neutral mesons."},{"citing_arxiv_id":"2605.04240","ref_index":25,"ref_count":1,"confidence":0.88,"is_internal_anchor":false,"paper_title":"Gamma Factory: A New Experimental Paradigm for CERN's HL-LHC--FCC-ee Transition","primary_cat":"physics.acc-ph","submitted_at":"2026-05-05T19:27:34+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":6.0,"formal_verification":"none","one_line_summary":"The Gamma Factory concept turns the LHC into a source of high-intensity gamma rays and tertiary beams by laser-exciting relativistic atomic ion beams.","context_count":1,"top_context_role":"background","top_context_polarity":"background","context_text":"scheme could increase by several orders of magnitude, the present intensity of the neutron beams delivered for the nTOF experimental programme [22], and the present intensity of radioactive ion beams for the ISOLDE experimental programme [24]. In addition, it enables the production of unprecedented-intensity and emittance tertiary beams of polarised positrons, muons, and CP- and flavour-tagged neutrinos [25]. The ultimate instantaneous luminosity of proton-proton collisions will be achieved in the forthcoming HL-LHC phase of the LHC collider operation. An increase in the luminosity collected so far, by a factor of about six is expected in this phase [26]. Such an increase will improve the statistical precision of the LHC canonical measurements. It is, however, unlikely to lead to discoveries of new phenomena."},{"citing_arxiv_id":"2605.02622","ref_index":34,"ref_count":2,"confidence":0.88,"is_internal_anchor":false,"paper_title":"Studying the Infrared Behaviour of Improved Logarithmic Accuracy Parton Showers with Herwig","primary_cat":"hep-ph","submitted_at":"2026-05-04T14:11:32+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":5.0,"formal_verification":"none","one_line_summary":"Implementation of two NLL-accurate dipole showers in Herwig shows that differences in infrared cutoffs produce noticeable effects at the hadron level and affect model tunability.","context_count":1,"top_context_role":"background","top_context_polarity":"background","context_text":"insight exists [26-31], to hadron spectroscopy where the only viable ground-up approach is lattice QCD [32] and secondary decays of the produced hadrons, where often experimental results [33] are the dominant input. Nevertheless, hadronization modelling is of crucial importance to the realistic simulation of collider processes, particularly as the precision of experimental results continues to improve [34, 35] and the accuracy of parton showers and hadronization becomes an increasingly significant limitation on overall uncertainties. 1A notable exception is the Herwig angular-ordered shower, which achieves NLL accuracy for many global event-shape observables [15], including massive quark effects [16], by faithfully producing a coherent branching parton cascade [17]."},{"citing_arxiv_id":"2604.26386","ref_index":2,"ref_count":1,"confidence":0.88,"is_internal_anchor":false,"paper_title":"Comparison of Silvaco and Synopsys TCAD Predictions Including the Perugia Radiation Damage Model in Silicon Pixel Detectors for the HL-LHC","primary_cat":"physics.ins-det","submitted_at":"2026-04-29T07:57:16+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":2.0,"formal_verification":"none","one_line_summary":"Silvaco and Synopsys TCAD tools yield similar results for leakage current, depletion voltage, electric field, and trap statistics in irradiated silicon pixel detectors using the Perugia model.","context_count":0,"top_context_role":null,"top_context_polarity":null,"context_text":null},{"citing_arxiv_id":"2604.22490","ref_index":9,"ref_count":1,"confidence":0.88,"is_internal_anchor":false,"paper_title":"Beam Loss Consequences","primary_cat":"physics.acc-ph","submitted_at":"2026-04-24T12:18:45+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":0.0,"formal_verification":"none","one_line_summary":"Reviews beam loss mechanisms in high-energy accelerators and their risks to equipment, electronics, and personnel.","context_count":1,"top_context_role":"background","top_context_polarity":"background","context_text":"that quantifies the amount of data delivered to the experiments, providing the proportionality between the cross section of any process and the corresponding number of events. At the LHC, the annualL int reached approximately120fb −1 (in units of inverse femtobarn, where1b= 10 24 cm2) during Run3, and it is expected to rise to250-300fb −1 per year following the High-Luminosity LHC (HL-LHC) upgrade [9]. Similarly, one can define an instantaneous luminosityL int, linked to the collision rate. A visual display of inelastic proton-proton collisions in the CMS experiment is shown in Fig. 2, along with the average number of particles per collision simulated with the FLUKA code [10-12] at 5mm from the IP and reaching the LHC tunnel in the forward direction (beyond an absorber named"},{"citing_arxiv_id":"2512.07420","ref_index":1,"ref_count":1,"confidence":0.88,"is_internal_anchor":false,"paper_title":"KIGNet: Physics-Motivated Multi-Graph Representation Learning for Explainable Jet Tagging","primary_cat":"hep-ph","submitted_at":"2025-12-08T10:53:05+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},{"citing_arxiv_id":"2507.04535","ref_index":45,"ref_count":1,"confidence":0.88,"is_internal_anchor":false,"paper_title":"da4ml: Distributed Arithmetic for Real-time Neural Networks on FPGAs","primary_cat":"cs.AR","submitted_at":"2025-07-06T21:01:32+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":6.0,"formal_verification":"none","one_line_summary":"A distributed arithmetic algorithm for CMVM operations on FPGAs reduces area by up to one third and latency for quantized neural networks, integrated into hls4ml.","context_count":0,"top_context_role":null,"top_context_polarity":null,"context_text":null},{"citing_arxiv_id":"2310.19742","ref_index":1,"ref_count":1,"confidence":0.88,"is_internal_anchor":false,"paper_title":"Novel Developments on the OpenIPMC Project","primary_cat":"physics.ins-det","submitted_at":"2023-10-30T17:05:40+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":2.0,"formal_verification":"none","one_line_summary":"Reports recent developments, operational experience on CERN prototypes, and new firmware features plus protocol support for the OpenIPMC IPMC controller.","context_count":0,"top_context_role":null,"top_context_polarity":null,"context_text":null}],"limit":50,"offset":0}