B. Ujvári
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View article: Module Tester for Positron Emission Tomography and Particle Physics
Module Tester for Positron Emission Tomography and Particle Physics Open
The combination of high-density, high-time-resolution inorganic scintillation crystals such as Lutetium Yttrium Oxyorthosilicate (LYSO), Yttrium Orthosilicate (YSO) and Bismuth Germanate (BGO) with Silicon Photomultiplier (SiPM) sensors is…
View article: Search for higgsino pair production in pp collisions at $\\sqrt{s}$ = 13 TeV in final states with large missing transverse momentum and two Higgs bosons decaying via $\\mathrm{H} \\to\\mathrm{b}\\overline{\\mathrm{b}}$
Search for higgsino pair production in pp collisions at $\\sqrt{s}$ = 13 TeV in final states with large missing transverse momentum and two Higgs bosons decaying via $\\mathrm{H} \\to\\mathrm{b}\\overline{\\mathrm{b}}$ Open
Results are reported from a search for new physics in 13 TeV proton-proton collisions in the final state with large missing transverse momentum and two Higgs bosons decaying via $\\mathrm{H} \\to\\mathrm{b}\\overline{\\mathrm{b}}$. The sea…
View article: Measurements of the $\mathrm{ pp \to W \gamma\gamma }$ and $\mathrm{ pp \to Z \gamma\gamma }$ cross sections and limits on anomalous quartic gauge couplings at $\sqrt{s} =$ 8 TeV
Measurements of the $\mathrm{ pp \to W \gamma\gamma }$ and $\mathrm{ pp \to Z \gamma\gamma }$ cross sections and limits on anomalous quartic gauge couplings at $\sqrt{s} =$ 8 TeV Open
Measurements are presented of $ \mathrm{ W \gamma\gamma } $ and $ \mathrm{ Z \gamma\gamma } $ production in proton-proton collisions. Fiducial cross sections are reported based on a data sample corresponding to an integrated luminosity of …
View article: Search for new physics with the $\mathrm{M_{T2}}$ variable in all-jets final states produced in pp collisions at $\mathrm{\sqrt{s} = 13 TeV}$
Search for new physics with the $\mathrm{M_{T2}}$ variable in all-jets final states produced in pp collisions at $\mathrm{\sqrt{s} = 13 TeV}$ Open
A search for new physics is performed using events that contain one or more jets, no isolated leptons, and a large transverse momentum imbalance, as measured through the MT2 variable, which is an extension of the transverse mass in events …
View article: Measurement of the differential cross section and charge asymmetry for inclusive pp $\\mathrm{\\to W^\\pm + X}$ production at $\\mathrm{\\sqrt s = 8 TeV}$
Measurement of the differential cross section and charge asymmetry for inclusive pp $\\mathrm{\\to W^\\pm + X}$ production at $\\mathrm{\\sqrt s = 8 TeV}$ Open
The differential cross section and charge asymmetry for inclusive pp to W + X to mu-nu + X production at sqrt(s) = 8 TeV are measured as a function of muon pseudorapidity. The data sample corresponds to an integrated luminosity of 18.8 inv…