Measurement of cross-sections for production of a $Z$ boson in association with a flavor-inclusive or doubly $b$-tagged large-radius jet in proton-proton collisions at $\sqrt{s} = 13$ TeV with the ATLAS experiment
ArXiv 2204.12355 (2022)
Search for heavy neutral leptons in decays of $W$ bosons using a dilepton displaced vertex in $\sqrt{s}=13$ TeV $pp$ collisions with the ATLAS detector
ArXiv 2204.11988 (2022)
Search for the charged-lepton-flavor-violating decay $Z\rightarrow eμ$ in $pp$ collisions at $\sqrt{s}=13$ TeV with the ATLAS detector
ArXiv 2204.10783 (2022)
High-precision measurement of the W boson mass with the CDF II detector
Science American Association for the Advancement of Science 376:6589 (2022) 170-176
Abstract:
The mass of the W boson, a mediator of the weak force between elementary particles, is tightly constrained by the symmetries of the standard model of particle physics. The Higgs boson was the last missing component of the model. After observation of the Higgs boson, a measurement of the W boson mass provides a stringent test of the model. We measure the W boson mass, MW, using data corresponding to 8.8 inverse femtobarns of integrated luminosity collected in proton-antiproton collisions at a 1.96 tera-electron volt center-of-mass energy with the CDF II detector at the Fermilab Tevatron collider. A sample of approximately 4 million W boson candidates is used to obtain [Formula: see text], the precision of which exceeds that of all previous measurements combined (stat, statistical uncertainty; syst, systematic uncertainty; MeV, mega-electron volts; c, speed of light in a vacuum). This measurement is in significant tension with the standard model expectation.Radiation hardness and timing performance in MALTA monolithic pixel sensors in TowerJazz 180 nm
Journal of Instrumentation IOP Publishing 17:04 (2022) c04034