{"total":22,"items":[{"citing_arxiv_id":"2607.07811","ref_index":16,"ref_count":1,"confidence":0.98,"is_internal_anchor":true,"paper_title":"Impact of QED Radiation on SMEFT Constraints in Deep Inelastic Scattering","primary_cat":"hep-ph","submitted_at":"2026-07-08T18:01:02+00:00","verdict":"CONDITIONAL","verdict_confidence":"MODERATE","novelty_score":6.5,"formal_verification":"none","one_line_summary":"Collision-induced QED radiation produces O(1) corrections to DIS cross sections but only few-percent shifts in longitudinal electron spin asymmetries, making asymmetries more robust for SMEFT constraints at SoLID and EIC.","context_count":0,"top_context_role":null,"top_context_polarity":null,"context_text":null},{"citing_arxiv_id":"2606.26097","ref_index":64,"ref_count":1,"confidence":0.9,"is_internal_anchor":false,"paper_title":"Positron-Emitting and Electron-Capturing Double-Beta Processes in the Standard Model and Beyond","primary_cat":"hep-ph","submitted_at":"2026-06-24T17:59:59+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":5.0,"formal_verification":"none","one_line_summary":"Nuclear matrix elements and phase-space factors are computed for 2ν and 0ν positron-emitting double-beta modes in three isotopes, yielding sensitivity to SMEFT lepton-number-violating operators at 1-100 TeV and showing multi-isotope measurements can break degeneracies.","context_count":0,"top_context_role":null,"top_context_polarity":null,"context_text":null},{"citing_arxiv_id":"2606.19202","ref_index":31,"ref_count":1,"confidence":0.9,"is_internal_anchor":false,"paper_title":"Renormalization of the SMEFT to Dimension Eight: Fermionic Interactions II","primary_cat":"hep-ph","submitted_at":"2026-06-17T15:40:05+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":5.0,"formal_verification":"none","one_line_summary":"Computes one-loop mixing of bosonic and two-fermion interactions into two-fermion operators in dim-8 SMEFT, leaving only four-fermion to two-fermion mixing to finish the renormalization program.","context_count":0,"top_context_role":null,"top_context_polarity":null,"context_text":null},{"citing_arxiv_id":"2606.12312","ref_index":45,"ref_count":1,"confidence":0.9,"is_internal_anchor":false,"paper_title":"Sensitivity to top-quark couplings in diboson production at lepton colliders","primary_cat":"hep-ph","submitted_at":"2026-06-10T16:46:01+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":4.0,"formal_verification":"none","one_line_summary":"NLO EW corrections to WW production from SMEFT top operators yield competitive sensitivity at LEP3 and FCC-ee relative to ZH production and existing LEP/LHC bounds.","context_count":0,"top_context_role":null,"top_context_polarity":null,"context_text":null},{"citing_arxiv_id":"2606.12298","ref_index":72,"ref_count":1,"confidence":0.9,"is_internal_anchor":false,"paper_title":"The KSVZ Atlas: A Unified SMEFT-ALP Framework","primary_cat":"hep-ph","submitted_at":"2026-06-10T16:34:39+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":6.0,"formal_verification":"none","one_line_summary":"A matching framework from arbitrary KSVZ UV completions to SMEFT and ALP EFT yields robust operator bounds from global fits that often dominate direct ALP searches except when mass mixing occurs.","context_count":0,"top_context_role":null,"top_context_polarity":null,"context_text":null},{"citing_arxiv_id":"2606.09596","ref_index":27,"ref_count":1,"confidence":0.9,"is_internal_anchor":false,"paper_title":"Lifting Effective-Field-Theory Degeneracies in Semileptonic Heavy-Baryon Decays","primary_cat":"hep-ph","submitted_at":"2026-06-08T15:08:23+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":5.0,"formal_verification":"none","one_line_summary":"Tau polarization in baryonic semileptonic decays supplies the leading sensitivity to lift EFT degeneracies unresolved by meson measurements in b to c tau nu transitions.","context_count":0,"top_context_role":null,"top_context_polarity":null,"context_text":null},{"citing_arxiv_id":"2606.07232","ref_index":25,"ref_count":1,"confidence":0.9,"is_internal_anchor":false,"paper_title":"Current and future constraints on heavy New Physics from $\\tau$ weak dipole moments","primary_cat":"hep-ph","submitted_at":"2026-06-05T12:59:24+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":5.0,"formal_verification":"none","one_line_summary":"Tau weak dipole moments already rank among the leading probes of tau dipole operators and will become dominant at FCC-ee and HL-LHC.","context_count":0,"top_context_role":null,"top_context_polarity":null,"context_text":null},{"citing_arxiv_id":"2606.02709","ref_index":80,"ref_count":1,"confidence":0.9,"is_internal_anchor":false,"paper_title":"Anatomy and Phenomenology of Minimal Flavor Deconstruction in the Lepton Sector","primary_cat":"hep-ph","submitted_at":"2026-06-01T18:00:03+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":4.0,"formal_verification":"none","one_line_summary":"Next-to-leading order spurion effects in a minimal lepton flavor deconstruction model induce observable charged lepton flavor violation, lepton flavor universality violation, and electric dipole moments at multi-10 TeV scales.","context_count":0,"top_context_role":null,"top_context_polarity":null,"context_text":null},{"citing_arxiv_id":"2606.01178","ref_index":45,"ref_count":1,"confidence":0.9,"is_internal_anchor":false,"paper_title":"Probing the imaginary parts and their $q^2$ dependences for the tau $g-2$ and EDM","primary_cat":"hep-ph","submitted_at":"2026-05-31T11:37:41+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":5.0,"formal_verification":"none","one_line_summary":"Explores q² dependence and imaginary parts of tau g-2 and EDM in SMEFT and 2HDM, proposing methods to measure them at Belle II and STCF to improve a_τ bounds by over an order of magnitude.","context_count":0,"top_context_role":null,"top_context_polarity":null,"context_text":null},{"citing_arxiv_id":"2605.27525","ref_index":27,"ref_count":1,"confidence":0.9,"is_internal_anchor":false,"paper_title":"Hunting New Animalcula with Flavour Changing Processes","primary_cat":"hep-ph","submitted_at":"2026-05-26T18:01:08+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":2.0,"formal_verification":"none","one_line_summary":"Review advocating correlations among flavour observables as direct tests for specific new physics models beyond global fits to Wilson coefficients.","context_count":0,"top_context_role":null,"top_context_polarity":null,"context_text":null},{"citing_arxiv_id":"2605.21594","ref_index":38,"ref_count":1,"confidence":0.9,"is_internal_anchor":false,"paper_title":"Exploring the SMEFT landscape: Bayesian Model Selection for indirect discovery","primary_cat":"hep-ph","submitted_at":"2026-05-20T18:00:06+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":7.0,"formal_verification":"none","one_line_summary":"Bayesian model selection over SMEFT operator subsets using a genetic algorithm and BIC approximation is applied to electroweak, Higgs, top and diboson data, finding no evidence for new physics and improved Wilson coefficient posteriors compared to global fits.","context_count":0,"top_context_role":null,"top_context_polarity":null,"context_text":null},{"citing_arxiv_id":"2605.11747","ref_index":28,"ref_count":2,"confidence":0.9,"is_internal_anchor":false,"paper_title":"SMEFT everywhere: a NLO study of $\\boldsymbol{pp \\to t\\bar{t}H}$ with decaying tops","primary_cat":"hep-ph","submitted_at":"2026-05-12T08:25:47+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":4.0,"formal_verification":"none","one_line_summary":"NLO QCD calculation of pp to ttH with decaying tops, including SMEFT operators O_tφ, O_φG, O_tG, O_tW in production and decays, with studies of linear/quadratic terms and RGE effects at 13.6 TeV.","context_count":1,"top_context_role":"background","top_context_polarity":"background","context_text":"Campillo Aveleira, G. Heinrich, M. Höfer, S.P. Jones, M. Kerner et al.,One-loop calculations in effective field theories with GoSam-3.0,SciPost Phys. Codeb.62(2026) 1 [2507.23549]. [27] A. Dedes, W. Materkowska, M. Paraskevas, J. Rosiek and K. Suxho,Feynman rules for the Standard Model Effective Field Theory in Rξ-gauges,JHEP06(2017) 143 [1704.03888]. [28] E.E. Jenkins, A.V. Manohar and M. Trott,Renormalization Group Evolution of the Standard Model Dimension Six Operators I: Formalism and lambda Dependence,JHEP10(2013) 087 [1308.2627]. [29] E.E. Jenkins, A.V. Manohar and M. Trott,Renormalization Group Evolution of the Standard Model Dimension Six Operators II: Yukawa Dependence,JHEP01(2014) 035 [1310."},{"citing_arxiv_id":"2604.26817","ref_index":25,"ref_count":1,"confidence":0.9,"is_internal_anchor":false,"paper_title":"When Two Loops Matter: Electroweak Precision in the SMEFT","primary_cat":"hep-ph","submitted_at":"2026-04-29T15:44:53+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":7.0,"formal_verification":"none","one_line_summary":"A modification to the top-Higgs Yukawa coupling in SMEFT induces a two-loop shift in the W mass through a large anomalous dimension, providing a new indirect probe via electroweak precision observables.","context_count":1,"top_context_role":"background","top_context_polarity":"background","context_text":"Generally speaking, if a WC gives a one-loop running effect to a WC that enters an observable at LO then that operator will itself contribute to the observable at one-loop order. Fig. 3 lists all the WCs that are the origins of one-loop flow (light blue arrows). We use the numerical expressions from [28] at the renormalization scaleµ=m Z to capture these effects (see also [25]). Thus, our analysis captures all effects at the leading loop order for each observable, but we do not perform proper RG resummation. This is not expected to qualitatively affect our conclusions. Additional indirect constraints -In addition to giving contributions to theWmass and the weak angle, as anticipated in Section 2.1, the model also induces cor-"},{"citing_arxiv_id":"2604.22608","ref_index":28,"ref_count":1,"confidence":0.9,"is_internal_anchor":false,"paper_title":"Recent Developments in SMEFT: Theory, Tools, and Phenomenology","primary_cat":"hep-ph","submitted_at":"2026-04-24T14:34:33+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":1.0,"formal_verification":"none","one_line_summary":"A review summarizing recent theory, tools, and phenomenology in the Standard Model Effective Field Theory.","context_count":1,"top_context_role":"background","top_context_polarity":"background","context_text":"Maltoni, G. Ventura, and E. VryonidouJHEP12(2024) 183, arXiv:2406.06670 [hep-ph]. [25] A. Dedes, M. Paraskevas, J. Rosiek, K. Suxho, and L. TrifyllisJHEP 08(2018) 103,arXiv:1805.00302 [hep-ph]. [26] A. Dedes, K. Suxho, and L. TrifyllisJHEP06(2019) 115, arXiv:1903.12046 [hep-ph]. [27] J. M. Cullen and B. D. PecjakJHEP11(2020) 079, arXiv:2007.15238 [hep-ph]. [28] E. E. Jenkins, A. V. Manohar, and M. TrottJHEP10(2013) 087, arXiv:1308.2627 [hep-ph]. [29] E. E. Jenkins, A. V. Manohar, and M. TrottJHEP01(2014) 035, arXiv:1310.4838 [hep-ph]. [30] R. Alonso, E. E. Jenkins, A. V. Manohar, and M. TrottJHEP04 (2014) 159,arXiv:1312.2014 [hep-ph]. [31] S. Di Noi, R. Gr¨ ober, and M. K. MandalJHEP12(2025) 220, arXiv:2408."},{"citing_arxiv_id":"2604.16599","ref_index":3,"ref_count":1,"confidence":0.9,"is_internal_anchor":false,"paper_title":"The effect of the two-loop SMEFT RGEs at future colliders","primary_cat":"hep-ph","submitted_at":"2026-04-17T18:00:01+00:00","verdict":"CONDITIONAL","verdict_confidence":"LOW","novelty_score":7.0,"formal_verification":"none","one_line_summary":"Two-loop SMEFT RGEs induce non-negligible effects on the evolution of Wilson coefficients, leading to percent-level shifts in projected sensitivities for four-quark, top Yukawa, and Higgs-gluon operators in collider fits.","context_count":1,"top_context_role":"background","top_context_polarity":"background","context_text":"Jenkins, A. V. Manohar and M. Trott,Renormalization Group Evolution of the Standard Model Dimension Six Operators I: Formalism and lambda Dependence,JHEP10 (2013) 087 [1308.2627]. [2] E. E. Jenkins, A. V. Manohar and M. Trott,Renormalization Group Evolution of the Standard Model Dimension Six Operators II: Yukawa Dependence,JHEP01(2014) 035 [1310.4838]. [3] R. Alonso, E. E. Jenkins, A. V. Manohar and M. Trott,Renormalization Group Evolution of the Standard Model Dimension Six Operators III: Gauge Coupling Dependence and Phenomenology,JHEP04(2014) 159 [1312.2014]. [4] J. Aebischer, J. Kumar and D. M. Straub,Wilson: a Python package for the running and matching of Wilson coefficients above and below the electroweak scale,Eur."},{"citing_arxiv_id":"2604.14281","ref_index":65,"ref_count":1,"confidence":0.9,"is_internal_anchor":false,"paper_title":"Probing $\\tau$ lepton dipole moments at future Lepton Colliders","primary_cat":"hep-ph","submitted_at":"2026-04-15T18:00:01+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":5.0,"formal_verification":"none","one_line_summary":"Future lepton colliders can improve existing constraints on the tau lepton's dipole moments by several orders of magnitude through complementary channels.","context_count":1,"top_context_role":"background","top_context_polarity":"background","context_text":"Trott, Renormal- ization Group Evolution of the Standard Model Dimen- sion Six Operators I: Formalism and lambda Dependence, JHEP10, 087, arXiv:1308.2627 [hep-ph]. [64] E. E. Jenkins, A. V. Manohar, and M. Trott, Renormal- ization Group Evolution of the Standard Model Dimen- sion Six Operators II: Yukawa Dependence, JHEP01, 035, arXiv:1310.4838 [hep-ph]. [65] R. Alonso, E. E. Jenkins, A. V. Manohar, and M. Trott, Renormalization Group Evolution of the Stan- dard Model Dimension Six Operators III: Gauge Cou- pling Dependence and Phenomenology, JHEP04, 159, arXiv:1312.2014 [hep-ph]. [66] E. E. Jenkins, A. V. Manohar, and P. Stoffer, Low- Energy Effective Field Theory below the Electroweak Scale: Anomalous Dimensions, JHEP01, 084, [Erratum:"},{"citing_arxiv_id":"2604.14091","ref_index":22,"ref_count":1,"confidence":0.9,"is_internal_anchor":false,"paper_title":"Exploring new resonances with direct top flavor changing interactions","primary_cat":"hep-ph","submitted_at":"2026-04-15T17:06:38+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":4.0,"formal_verification":"none","one_line_summary":"Three new physics resonances with top flavor-changing couplings are mapped to SMEFT operators at the electroweak scale and their phenomenology is analyzed.","context_count":1,"top_context_role":"method","top_context_polarity":"use_method","context_text":"Trott, Renormaliza- tion Group Evolution of the Standard Model Dimension Six Operators II: Yukawa Dependence, JHEP01, 035, arXiv:1310.4838 [hep-ph]. [21] E. E. Jenkins, A. V. Manohar, and M. Trott, Renormal- ization Group Evolution of the Standard Model Dimen- sion Six Operators I: Formalism and lambda Dependence, JHEP10, 087, arXiv:1308.2627 [hep-ph]. [22] R. Alonso, E. E. Jenkins, A. V. Manohar, and M. Trott, Renormalization Group Evolution of the Standard Model Dimension Six Operators III: Gauge Coupling Dependence and Phenomenology, JHEP04, 159, arXiv:1312.2014 [hep- ph]. [23] J. Aguilar-Saavedra, A minimal set of top anomalous couplings, Nuclear Physics B812, 181-204 (2009). [24] C. Zhang and S."},{"citing_arxiv_id":"2601.18237","ref_index":60,"ref_count":1,"confidence":0.9,"is_internal_anchor":false,"paper_title":"Revisiting $\\mu$-$e$ conversion in $R$-parity violating SUSY","primary_cat":"hep-ph","submitted_at":"2026-01-26T07:42:05+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":4.0,"formal_verification":"none","one_line_summary":"RG running changes limits on certain RPV SUSY λ and λ' couplings by up to 80 percent, with upcoming μ-e conversion experiments expected to set stronger bounds than μ→eγ or μ→eee decays.","context_count":0,"top_context_role":null,"top_context_polarity":null,"context_text":null},{"citing_arxiv_id":"2508.08516","ref_index":5,"ref_count":1,"confidence":0.9,"is_internal_anchor":false,"paper_title":"Nucleon Energy Correlators as a Probe of Light-Quark Dipole Operators at the Electron-Ion Collider","primary_cat":"hep-ph","submitted_at":"2025-08-11T22:51:39+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":7.0,"formal_verification":"none","one_line_summary":"Nucleon energy correlators access linear effects from light-quark dipole operators via azimuthal asymmetries in the target fragmentation region at the EIC.","context_count":0,"top_context_role":null,"top_context_polarity":null,"context_text":null},{"citing_arxiv_id":"2506.05201","ref_index":15,"ref_count":1,"confidence":0.9,"is_internal_anchor":false,"paper_title":"SUSY meets SMEFT: Complete one-loop matching of the general MSSM","primary_cat":"hep-ph","submitted_at":"2025-06-05T16:14:25+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":8.0,"formal_verification":"none","one_line_summary":"Complete one-loop matching of the general MSSM onto SMEFT in the Warsaw basis, including all SUSY-governed correlations among Wilson coefficients.","context_count":1,"top_context_role":"background","top_context_polarity":"background","context_text":"ferent energies and experiments in a consistent manner, while adequately resumming large logarithmic corrections that appear due to the presence of scale hierarchies. Several such global SMEFT fits have been performed in recent years, e.g., in [5-14]. The large number of free parameters in the SMEFT alone - 2499 in the baryon- (B) and lepton-number (L) conserving sector of the SMEFT at dimension six [15] - poses a signifi- cant challenge to global fits, however. Therefore, these fits always employ some simplifying assumptions, such as only considering a subset of operators, or specific flavor assumptions, in order to reduce the number of free parameters. This comes at the cost of losing model independence and possibly important correlations between different sectors, making the in-"},{"citing_arxiv_id":"1907.07605","ref_index":14,"ref_count":1,"confidence":0.9,"is_internal_anchor":false,"paper_title":"Complete One-Loop Renormalization of the Higgs-Electroweak Chiral Lagrangian","primary_cat":"hep-ph","submitted_at":"2019-07-17T16:06:56+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":6.0,"formal_verification":"none","one_line_summary":"The complete one-loop renormalization of the EWChL is performed, confirming power counting assumptions and operator basis completeness while reproducing known subsector results.","context_count":0,"top_context_role":null,"top_context_polarity":null,"context_text":null},{"citing_arxiv_id":"1906.10631","ref_index":14,"ref_count":1,"confidence":0.9,"is_internal_anchor":false,"paper_title":"Towards global fits in EFT's and New Physics implications","primary_cat":"hep-ph","submitted_at":"2019-06-25T16:17:31+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":2.0,"formal_verification":"none","one_line_summary":"Reviews advances toward global SMEFT fits across top, Higgs, and electroweak sectors including NLO QCD effects and multi-sector combinations.","context_count":0,"top_context_role":null,"top_context_polarity":null,"context_text":null}],"limit":50,"offset":0}