{"total":30,"items":[{"citing_arxiv_id":"2606.24794","ref_index":1,"ref_count":1,"confidence":0.5,"is_internal_anchor":false,"paper_title":"LF-MightyPix: A second HV-MAPS prototype for the {LHCb} Mighty-Tracker","primary_cat":"physics.ins-det","submitted_at":"2026-06-23T16:48:12+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":4.0,"formal_verification":"none","one_line_summary":"LF-MightyPix is a 3.5 mm × 4.0 mm chip with 100 μm pixels that records time-of-arrival and time-over-threshold per hit; test results confirm compatibility with MightyPix requirements for 40 MHz bunch-crossing identification.","context_count":0,"top_context_role":null,"top_context_polarity":null,"context_text":null},{"citing_arxiv_id":"2606.24637","ref_index":1,"ref_count":1,"confidence":0.5,"is_internal_anchor":false,"paper_title":"Application of Deep Learning to Jet Charge Discrimination","primary_cat":"hep-ph","submitted_at":"2026-06-23T14:30:49+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":4.0,"formal_verification":"none","one_line_summary":"Graph neural network achieves AUC of 0.883 for up versus anti-up quark jet charge discrimination in controlled QCD simulations.","context_count":0,"top_context_role":null,"top_context_polarity":null,"context_text":null},{"citing_arxiv_id":"2606.20767","ref_index":25,"ref_count":1,"confidence":0.5,"is_internal_anchor":false,"paper_title":"COLD-CI: A large-scale very high-resolution label polygon dataset for cocoa and non-cocoa classification in Cote d'Ivoire","primary_cat":"q-bio.OT","submitted_at":"2026-06-18T13:08:41+00:00","verdict":"ACCEPT","verdict_confidence":"LOW","novelty_score":7.0,"formal_verification":"none","one_line_summary":"COLD-CI provides 123,736 vector polygons labeling cocoa (1,788 km²) and background (4,208 km²) areas in Cote d'Ivoire with 99% independent validation accuracy.","context_count":0,"top_context_role":null,"top_context_polarity":null,"context_text":null},{"citing_arxiv_id":"2605.31382","ref_index":12,"ref_count":1,"confidence":0.5,"is_internal_anchor":false,"paper_title":"Development of a Multi-Purpose Optical TPC for Neutron-Induced Reaction Studies at SARAF","primary_cat":"physics.ins-det","submitted_at":"2026-05-29T14:50:57+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":3.0,"formal_verification":"none","one_line_summary":"Prototype optical TPC assembled and tested for characterization of drift, amplification, and alpha track imaging in Ar/CF4 to guide full system for SARAF neutron studies.","context_count":0,"top_context_role":null,"top_context_polarity":null,"context_text":null},{"citing_arxiv_id":"2605.30467","ref_index":6,"ref_count":1,"confidence":0.5,"is_internal_anchor":false,"paper_title":"Clustering Guided Domain-Specific Pretrained Foundation Model for Very High-Resolution Arctic Remote Sensing","primary_cat":"cs.CV","submitted_at":"2026-05-28T18:40:32+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":5.0,"formal_verification":"none","one_line_summary":"Affinity-propagation clustering of Arctic VHSR imagery enables MAE pretraining of a ViT-Large encoder that outperforms ImageNet and Prithvi-EO-2.0 baselines by 5-15 percentage points in mean F1 on four downstream Arctic detection and segmentation tasks.","context_count":0,"top_context_role":null,"top_context_polarity":null,"context_text":null},{"citing_arxiv_id":"2605.22656","ref_index":9,"ref_count":1,"confidence":0.5,"is_internal_anchor":false,"paper_title":"Emergent Neutrino Texture Geometry from Dark Matter and Lepton Flavor Violation in the Scotogenic Model","primary_cat":"hep-ph","submitted_at":"2026-05-21T15:58:15+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":4.0,"formal_verification":"none","one_line_summary":"Numerical scans in the minimal scotogenic model indicate that approximate neutrino texture structures emerge dynamically from dark matter and lepton flavor violation consistency conditions.","context_count":0,"top_context_role":null,"top_context_polarity":null,"context_text":null},{"citing_arxiv_id":"2605.15958","ref_index":55,"ref_count":1,"confidence":0.5,"is_internal_anchor":false,"paper_title":"Bridging the climate to energy data gap: simulated annealing for representative climate year selection","primary_cat":"physics.ao-ph","submitted_at":"2026-05-15T13:52:08+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":6.0,"formal_verification":"none","one_line_summary":"Simulated annealing with seasonal sliced Wasserstein distance selects climate year subsets that are 2.5-3.5 times more representative than ENTSO-E practice and achieve 4-5 times effective sample size.","context_count":0,"top_context_role":null,"top_context_polarity":null,"context_text":null},{"citing_arxiv_id":"2605.11961","ref_index":16,"ref_count":1,"confidence":0.5,"is_internal_anchor":false,"paper_title":"TPA-TCT Analysis of the RD50-MPW4 Monolithic Pixel Particle Detector","primary_cat":"physics.ins-det","submitted_at":"2026-05-12T11:16:14+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":5.0,"formal_verification":"none","one_line_summary":"The RD50-MPW4 DMAPS shows 100% charge collection efficiency, 226 μm depletion depth, and peripheral charge sharing when mapped in 3D with TPA-TCT.","context_count":1,"top_context_role":"background","top_context_polarity":"background","context_text":"sion for non-depleted MAPS. Full depletion of the pixel matrix means that the silicon substrate needs a high resistivity, in the 1-2 kΩ·cm range. The RD50 collaboration, and more recently the DRD3 col- laboration, developed a DMAPS sensor named the RD50- MPW4 [15] where MPW stands for Multi-Project Wafer. A working prototype of the RD50-MPW4 chip exists since 2024 [16] followed soon by the first studies of the RD50-MPW4 sen- sor performance and radiation tolerance under broad electron beam irradiation [17, 18]. As DMAPS arrays use reverse biased diodes as sensing el- ements, it is important to characterize their depletion depth, electric field boundaries, Charge Collection Efficiency (CCE) and Charge Sharing (CS)."},{"citing_arxiv_id":"2605.07681","ref_index":8,"ref_count":1,"confidence":0.5,"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":"2605.02344","ref_index":16,"ref_count":1,"confidence":0.88,"is_internal_anchor":false,"paper_title":"Women in STEM: Interview with Iris Abt","primary_cat":"hep-ex","submitted_at":"2026-05-04T08:45:05+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":2.0,"formal_verification":"none","one_line_summary":"The paper reports an interview with Iris Abt recounting her career path from German university studies to contributions in neutrino experiments, SLC at SLAC, HERA, and germanium detector studies.","context_count":0,"top_context_role":null,"top_context_polarity":null,"context_text":null},{"citing_arxiv_id":"2605.01840","ref_index":37,"ref_count":1,"confidence":0.88,"is_internal_anchor":false,"paper_title":"Development of a quadripartite wakefield structure as dechirper for free electron laser","primary_cat":"physics.acc-ph","submitted_at":"2026-05-03T12:14:14+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":6.0,"formal_verification":"none","one_line_summary":"A four-plate symmetric corrugated structure suppresses quadrupole wakefields in FEL dechirpers, yielding lower projected emittance growth and 25% shorter length than planar designs per simulations.","context_count":1,"top_context_role":"background","top_context_polarity":"background","context_text":", Prototype design of a digital Low- Level RF system for S3FEL S-band Transverse Deflecting Cav- ities, J. Instrum., vol. 20, T01012, 2025. doi: 10.1088/1748- 0221/20/01/T01012 [36] L. Hu, X. Wang, L. Yang et al., Conceptual design of S 3FEL cryogenic system, IOP Conf. Ser .: Mater . Sci. Eng., vol. 1240, 012092, 2022. doi: 10.1088/1757-899X/1240/1/012092 [37] B. Zhang, X. Li, Q. Liu et al. , High repetition-rate photoin- jector laser system for S 3FEL, Front. Phys., vol. 11, 1181862, 2023. doi: 10.3389/fphy.2023.1181862 [38] Z. Xu, W. Zhang, C. Yang et al., Shape optimization design of the offset mirror in FEL-1 beamline at S 3FEL, Sci. Rep., vol. 13, 9653, 2023. doi: 10.1038/s41598-023-36645-9 [39] M."},{"citing_arxiv_id":"2605.00717","ref_index":8,"ref_count":1,"confidence":0.88,"is_internal_anchor":false,"paper_title":"Leveraging Climate Services to Build Climate Resilient Power Systems","primary_cat":"physics.ao-ph","submitted_at":"2026-05-01T15:05:38+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":3.0,"formal_verification":"none","one_line_summary":"Systematic use of climate services and harmonized datasets like PECD4.2 is required to build resilient power systems, as physical wind/solar conversion models offer better future robustness than historical ML approaches, though hydropower and standardization challenges remain.","context_count":0,"top_context_role":null,"top_context_polarity":null,"context_text":null},{"citing_arxiv_id":"2605.02932","ref_index":16,"ref_count":1,"confidence":0.88,"is_internal_anchor":false,"paper_title":"Proposal for applying the novel gas-dynamic ion-beam extraction and bunching technique to the cryogenic stopping cells at FAIR","primary_cat":"physics.acc-ph","submitted_at":"2026-04-28T18:04:40+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":5.0,"formal_verification":"none","one_line_summary":"Simulations indicate that placing a short stack of thin cylindrical electrodes behind the extraction RF carpet in FAIR's cryogenic stopping cells can achieve 100% ion transmission and world-record emittance values across a wide mass range.","context_count":1,"top_context_role":"background","top_context_polarity":"background","context_text":"TITAN's digital RFQ ion beam cooler and buncher, operation and performance, Nuclear Instruments and Methods in Physics Research Section A, 676 (2012) 32. [15] A. A. Valverde, M. Brodeur, D. P. Burdette, J. A. Clark, J. W. Klimes, D. Lascar, P. D. O'Malley, R. Ringle, G. Savard, V. Varentsov, Stopped, bunched beams for the TwinSol facility, Hyperfine Interactions, (2019) 240:38, https://doi.org/10.1007/s10751-019-1591-x. [16] A. Ruzzon, M. Maggiore, C. Roncolato, G. Ban, J.F. Cam, C. Gautier and C. Vandamme, Realization and simulations of the new SPES Beam Cooler, 2023 JINST 18 P10031, https://doi.org/10.1088/1748- 0221/18/10/P10031. [17] Yin-Shen Liu, Han-Rui Hu, Xiao-Fei Yang, Wen-Cong Mei, Yang-Fan Guo, Zhou Yan, Shao-Jie Chen, Shi-wei Bai, Shu-Jing Wang, Yong-Chao Liu, Peng Zhang, Dong-Yang Chen, Yan-Lin Ye, Qi-Te Li,"},{"citing_arxiv_id":"2604.25437","ref_index":45,"ref_count":1,"confidence":0.88,"is_internal_anchor":false,"paper_title":"Energy-differential measurement of the $^{\\mathrm{nat}}$C(n,p) and $^{\\mathrm{nat}}$C(n,d) reactions at the n_TOF facility at CERN","primary_cat":"nucl-ex","submitted_at":"2026-04-28T09:45:23+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":5.0,"formal_verification":"none","one_line_summary":"New cross sections for natC(n,p) and natC(n,d) up to 25 MeV are higher than evaluations and agree with TALYS-2.0 after model-assisted corrections for excited states.","context_count":1,"top_context_role":"method","top_context_polarity":"use_method","context_text":"natC sample used one also needs to consider its isotopic composition consisting of 98.9% of12C and 1.1% of13C, since the detected proton and deuteron counts can not be discriminated according to a particular carbon isotope. Evidently, a detailed mathematical model is needed in order to translate the cross sections into observable counts. This model was already developed in [45], not ac- counting for the resolution function of the neutron beam. As such, the expression developed therein models the number of detected countsdN(E n)from Eq. (8), pro- duced by the neutrons of true energyEn. Here we ex- tend this model on the basis of Eq. (8), so as to take the resolution function into account. LetPdenote a particular∆E-Epair of silicon strips."},{"citing_arxiv_id":"2604.18028","ref_index":42,"ref_count":1,"confidence":0.88,"is_internal_anchor":false,"paper_title":"Design of High-energy Proton-beam Experiment Station at CSNS","primary_cat":"hep-ex","submitted_at":"2026-04-20T09:53:20+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":4.0,"formal_verification":"none","one_line_summary":"HPES is a planned 1.6 GeV proton beam station at CSNS with flux control from 10^3 to 10^8 protons/s, equipped with flux/profile monitors, a 10 μm resolution telescope, and a 1% energy resolution TOF spectrometer.","context_count":1,"top_context_role":"background","top_context_polarity":"background","context_text":"plier tubes (PMTs). Signals from both scintillators are pro- cessed via a coincidence logic to effectively suppress random background noise. Fig. 12(b) depicts the mechanical assem- bly of the encapsulated scintillator and PMT modules. The PROUD prototype has undergone performance validation us- ing the muon source at ISIS [41] and cosmic rays in labora- tory [42, 43]. Recent test results indicate that the dynamic range for cosmic ray detection can reach1-8.8×10 3 protons per pulse [42]. With further optimization, the system is pro- jected to cover the required dynamic flux range of10 3-108 protons per second. F. Beam Flux Online Monitor In addition to the requirements for beam tuning and rou- tine calibration, online flux monitoring is essential to provide"},{"citing_arxiv_id":"2605.00021","ref_index":86,"ref_count":1,"confidence":0.88,"is_internal_anchor":false,"paper_title":"Quantum Entanglement Degree, Mean Positronium Lifetime, and the $3\\gamma$/$2\\gamma$ Annihilation-Rate Ratio as Novel PET Biomarkers for Hypoxia -- Concept, Challenges, and Predictions","primary_cat":"physics.med-ph","submitted_at":"2026-04-19T21:57:21+00:00","verdict":null,"verdict_confidence":null,"novelty_score":null,"formal_verification":null,"one_line_summary":null,"context_count":1,"top_context_role":"background","top_context_polarity":"background","context_text":"reduction in PET by double Compton scattering of quantum entangled annihilation photons. J Instrum. 2023 Jul 4;18:P07007. doi: https://doi.org/10.1088/1748- 0221/18/07/P07007. [85] Romanchek GR, Shoop G, Abbaszadeh S. Application of quantum entanglement induced polarization for dual-positron and prompt gamma imaging. Bio-Algorithms Med-Syst. 2023;19(1):9-16. doi: https://doi.org/10.5604/01.3001.0054.1817. [86] Parashari S, Bosnar D, Friščić I, Kožuljević AM, Kuncic Z, Žugec P , et al. Closing the door on the \"puzzle of decoherence\" of annihilation quanta. Phys Lett B. 2024 May;852:138628. doi: https://doi.org/10.1016/j.physletb.2024.138628. [87] Kožuljević AM, Bokulić T, Grošev D, Kuncic Z, Parashari S, Pavelić L, et al. Investigation of the spatial resolution of PET imaging system measuring polarization-correlated Compton"},{"citing_arxiv_id":"2604.15199","ref_index":30,"ref_count":1,"confidence":0.5,"is_internal_anchor":false,"paper_title":"Rare and very rare decays at the LHCb experiment","primary_cat":"hep-ex","submitted_at":"2026-04-16T16:26:55+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":5.0,"formal_verification":"none","one_line_summary":"LHCb reports first searches and the most stringent limits to date on rare decays such as b to s tau+ tau- and tau to three muons.","context_count":1,"top_context_role":"background","top_context_polarity":"background","context_text":"With theB 0 decay vertex reconstructed using theK ∗(892)0 and electron, and theτcandidate constrained using the knownτmass and the reconstructedτdecay vertex from three-prong decays, a constrained reconstructed massm fit is obtained (see Fig. 2 for a comparison with the unconstrained mass). Bremsstrahlung effects are taken into account in the modelling of the signal shape. 3000 4000 5000 6000 ] 2c [MeV/m0 0.02 0.04 0.06 0.08 0.1 0.12 0.14 0.16 0.18 )2 c a.u./(68 MeV/ L HCb Simulation, bremsstrahlungνπππ → τ), e τ0*K(m, bremsstrahlungν0π πππ → τ), e τ0*K(m, no bremsstrahlungνπππ → τ), e τ0*K(m, no bremsstrahlungν0π πππ → τ), e τ0*K(m, bremsstrahlungνπππ → τ, fitm, bremsstrahlungν0π πππ → τ, fitm, no bremsstrahlungνπππ → τ, fitm, no bremsstrahlungν0π πππ → τ, fitm Figure 2 - Reconstructed massmand constrained reconstructed massm fit for final states with and without bremsstrahlung effects, and with or without an additionalπ 0 stemming from theτdecay 13. Backgrounds include combinatorial tracks, non-isolated candidates, misidentified hadrons, and charm background from decays ofD-meson, which have a lifetime similar to that ofτ leptons. Background suppression is achieved through sequential selection cuts and multivariate classifiers, with the dominant systematic uncertainty arising from the choice of the background control region. The signal yield is extracted by fitting the constrained massm fit. No significant signal is observed. Upper limits, determined separately for each charge combination, are set 13: B(B0 →K ∗0τ −e+)<5.9 (7.1)×10 −6 at 90% (95%) CL, B(B0 →K ∗0τ +e−)<4.9 (5.9)×10 −6 at 90% (95%) CL. (2) These results set the most stringent constraints to date onb→sτ ±e∓ transitions, improving on previous searches 14,15. 4.2 Searches forB + →π +µ±e∓ The decayB + →π +µeprovides a complementary probe of LFV with a fully reconstructible final state. The analysis 16 employs two BDTs: the first reduces combinatorial background using the upper mass sideband, wh"},{"citing_arxiv_id":"2604.10371","ref_index":22,"ref_count":1,"confidence":0.5,"is_internal_anchor":false,"paper_title":"Structural Gating and Effect-aligned Lag-resolved Temporal Causal Discovery Framework with Application to Heat-Pollution Extremes","primary_cat":"cs.LG","submitted_at":"2026-04-11T22:50:26+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":5.0,"formal_verification":"none","one_line_summary":"SGED-TCD is a lag-resolved causal discovery framework that uses structural gating and perturbation-effect alignment to infer interpretable weighted causal networks from complex time series, shown on heat-pollution extremes in China.","context_count":1,"top_context_role":"background","top_context_polarity":"background","context_text":"tial height field during the northern hemisphere winter, Monthly weather review 109 (4) (1981) 784-812. doi:10.1175/1520- 0493(1981)109<0784:TITGHF>2.0.CO;2. [21] Y. Yang, M. Li, H. Wang, H. Li, P. Wang, K. Li, M. Gao, H. Liao, Enso modulation of summertime tropospheric ozone over china, Envi- ronmental Research Letters 17 (3) (2022) 034020. doi:10.1088/1748- 9326/ac54cd. [22] Z. Jiang, J. Li, Impact of eastern and central pacific el niño on lower tropospheric ozone in china, Atmospheric Chemistry and Physics 22 (11) (2022) 7273-7285. doi:10.5194/acp-22-7273-2022. [23] X. Zhang, R. Zhugu, X. Jian, X. Liu, K. Chen, S. Tao, J. Liu, H. Gao, T. Huang, J. Ma, Associations of interannual variation in summer tro- pospheric ozone with the western pacific subtropical high in china from"},{"citing_arxiv_id":"2604.09918","ref_index":32,"ref_count":1,"confidence":0.5,"is_internal_anchor":false,"paper_title":"Cherenkov and scintillation light separation in BGO and BSO crystals coupled to SiPMs for dual-readout electromagnetic calorimetry at future colliders","primary_cat":"physics.ins-det","submitted_at":"2026-04-10T21:24:35+00:00","verdict":"CONDITIONAL","verdict_confidence":"LOW","novelty_score":7.0,"formal_verification":"none","one_line_summary":"Cherenkov and scintillation light were separated in BGO and BSO crystals with SiPMs, yielding up to 150 photoelectrons per GeV from Cherenkov light in electromagnetic showers.","context_count":1,"top_context_role":"background","top_context_polarity":"background","context_text":"Higgs factories. 2. Materials and methods Both BGO and BSO are excellent candidates for electro- magnetic calorimetry due to their high density, short radiation Table 1: Properties of the scintillating crystals under test. Values are taken from [15] if no superscript is present. Values with superscripts a, b, or c are taken respectively from [30], [31], or [32]. BGO BSO Density [g/cm3] 7.1 6.8 RM [cm] 2.23 2.33 X0 [cm] 1.12 1.15 λI [cm] 22.7 23.4 Refractive index at peak emission 2.15 a 2.06b Cherenkov angle (θC) 62 ◦ 61◦ Light yield [ph/MeV] 3500 c 950c Emission peak [nm] 480 470 length, small Molière radius (R M), and high scintillation yield. Moreover, their high refractive index enhances Cherenkov pho-"},{"citing_arxiv_id":"2604.00850","ref_index":16,"ref_count":1,"confidence":0.5,"is_internal_anchor":false,"paper_title":"A MIDAS-based Data Acquisition System for Gaseous Detectors","primary_cat":"physics.ins-det","submitted_at":"2026-04-01T13:03:49+00:00","verdict":"CONDITIONAL","verdict_confidence":"LOW","novelty_score":3.0,"formal_verification":"none","one_line_summary":"A MIDAS-based DAQ system was developed and deployed for gaseous detectors, providing unified data collection, decoding, and real-time monitoring validated in the PandaX-III experiment.","context_count":1,"top_context_role":"background","top_context_polarity":"background","context_text":"Furthermore, the software interfaces with the REST data analysis framework [15], realizing seamless integration of data acquisition, event reconstruction, and analysis so that the digitized waveforms can be visualized in real time during the acquisition process. As a typical application, we conducted a series of joint tests with the PandaX-III experiment [16], [17], which aims to search for the0νββdecay of the 136Xe isotope at the arXiv:2604.00850v2 [physics.ins-det] 13 Apr 2026 IEEE TRANSACTIONS ON NUCLEAR SCIENCE, VOL. XX, NO. XX, XXXX 2025 2 Front- End Card Back-End Card (TDCM/ DCM) Readout Modules Data Acquisition PC Fiber optic cable UDP/USB protocol Total 26 Fig. 1. The structure of electronics system of PandaX-III, consisting of FEC,"},{"citing_arxiv_id":"2603.14295","ref_index":39,"ref_count":1,"confidence":0.5,"is_internal_anchor":false,"paper_title":"Towards a Reflective PICOSEC detector?","primary_cat":"physics.ins-det","submitted_at":"2026-03-15T09:18:06+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":3.0,"formal_verification":"none","one_line_summary":"Reflective photocathode configurations are proposed for PICOSEC detectors to increase robustness and enable low-pressure operation.","context_count":0,"top_context_role":null,"top_context_polarity":null,"context_text":null},{"citing_arxiv_id":"2602.10279","ref_index":21,"ref_count":1,"confidence":0.5,"is_internal_anchor":false,"paper_title":"The MUSE Target Chamber Post Veto","primary_cat":"physics.ins-det","submitted_at":"2026-02-10T20:45:25+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":3.0,"formal_verification":"none","one_line_summary":"A custom veto detector was designed and installed in the MUSE target chamber to eliminate background events from beam tails striking support posts at the trigger level.","context_count":0,"top_context_role":null,"top_context_polarity":null,"context_text":null},{"citing_arxiv_id":"2512.09379","ref_index":2,"ref_count":1,"confidence":0.5,"is_internal_anchor":false,"paper_title":"Probing $t$-channel single top-quark and antiquark production via differential cross-section measurements at $\\sqrt{s}=$\\SI{13}{\\TeV} with the ATLAS detector","primary_cat":"hep-ex","submitted_at":"2025-12-10T07:21:04+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":7.0,"formal_verification":"none","one_line_summary":"Differential cross-sections and their ratio for t-channel single top production are measured at parton level with 140 fb^{-1} of ATLAS data and interpreted in an EFT framework to bound the Wilson coefficient C^{3,1}_{Qq}.","context_count":0,"top_context_role":null,"top_context_polarity":null,"context_text":null},{"citing_arxiv_id":"2511.13417","ref_index":2,"ref_count":1,"confidence":0.5,"is_internal_anchor":false,"paper_title":"Delineate Anything Flow: Fast, Country-Level Field Boundary Detection from Any Source","primary_cat":"cs.CV","submitted_at":"2025-11-17T14:30:43+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":7.0,"formal_verification":"none","one_line_summary":"DelAnyFlow combines a YOLOv11 model trained on the FBIS 22M dataset with post-processing to generate accurate vector field boundaries from multi-resolution satellite imagery, enabling country-scale mapping in 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