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Model for the curvature response of the CDF II drift chamber
Published 2025-02-01“…The CDF II experiment at the Fermilab Tevatron used a drift chamber to measure the momenta of charged particles. …”
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Muon $$g-2$$ g - 2 anomaly from vector-like leptons in a 2-Higgs-doublet + scalar singlet model
Published 2024-12-01“…Abstract We revisit an economical model for the $$g-2$$ g - 2 anomaly featuring a vector-like charged fermion, a scalar doublet and a scalar singlet in the light of new results from Fermilab. The phenomenological implications for lepton-flavor universality, Higgs decays, and charged lepton-flavor violating decays are discussed in detail.…”
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The Deep Underground Neutrino Experiment
Published 2015-01-01“…It is a merger of previous efforts and other interested parties to build, operate, and exploit a staged 40 kt liquid argon detector at the Sanford Underground Research Facility 1300 km from Fermilab, and a high precision near detector, exposed to a 1.2 MW, tunable ν beam produced by the PIP-II upgrade by 2024, evolving to a power of 2.3 MW by 2030. …”
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Energy-enhanced dimension eight SMEFT effects in VBF Higgs production
Published 2025-02-01Get full text
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Pseudo-Dirac neutrinos and relic neutrino matter effect on the high-energy neutrino flavor composition
Published 2025-03-01Get full text
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Study some two loop contribution to muon anomalous MDM in the N-B-LSSM
Published 2025-02-01“…Abstract It is well known that the muon magnetic dipole moment (MDM) has close relation with the new physics (NP) in the development of the Standard Model (SM). Combined with the Fermilab National Accelerator Laboratory (FNAL) and the Brookhaven National Laboratory (BNL) E821 result, the departure from the SM prediction is about 5.0 $$\sigma .$$ σ . …”
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First demonstration of a TES based cryogenic Li $$_2$$ 2 MoO $$_4$$ 4 detector for neutrinoless double beta decay search
Published 2025-01-01“…We present the detector design and results from a first prototype detector operated at the NEXUS shallow underground facility at Fermilab. The detector is a 2-cm-side cube with 21 g mass that is strongly thermally coupled to its readout chip to allow rise-times of $$\sim $$ ∼ 0.5 ms. …”
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Ultrahigh Energy Neutrinos at the Pierre Auger Observatory
Published 2013-01-01Get full text
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