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V. Radescu

Publications and source records attributed to V. Radescu.

21 records · Page 2Linked to original sources

Differential cross section results from NuTeV

The NuTeV experiment has collected high statistics, high energy samples of $ν$ and $\barν$ charged-current interactions using the sign-selected Fermilab neutrino beam. NuTeV has extracted $ν$ and $\barν$ differential cross sections for DIS single-muon production at moderate $x>0.015$ and average $Q^2\sim 15$ GeV$^2$. Differential cross sections and structure function results are presented. The NuTeV measurement has improved systematic precision and includes data over an expanded kinematic range up to high inelasticity.

hep-ex↗

Off the Mass Shell: Electroweak Physics at NuTeV

The NuTeV collaboration has performed precision measurements of the ratio of neutral current to charged current cross-sections in high rate, high energy neutrino and anti-neutrino beams on a dense, primarily steel, target. The separate neutrino and anti-neutrino beams, high statistics, and improved control of other experimental systematics, allow the determination of electroweak parameters with significantly greater precision than past neutrino-nucleon scattering experiments. Our null hypothesis test of the standard model prediction measures sin2thetaW=0.2277+/-0.0013(stat)+/-0.0009(syst), a value which is 3 sigma above the prediction. We discuss possible explanations for and implications of this discrepancy.

hep-ex↗

A Search for Muon-neutrino to Electron-neutrino and Muon-antineutrino to Electron-antineutrino Oscillations at NuTeV

Limits on $ν_μ\to ν_e$ and $\barν_μ\to \barν_e$ oscillations are extracted using the NuTeV detector with sign-selected $ν_μ$ and $\nub_μ$ beams. In $\nub_μ$ mode, for the case of $\sin^2 2α= 1$, $Δm^2 > 2.6$ ${\rm eV^2}$ is excluded, and for $Δm^2 \gg 1000$ ${\rm eV^2}$, $\sin^2 2α> 1.1 \times 10^{-3}$. The NuTeV data exclude the high $Δm^2$ end of $\barν_μ\to \barν_e$ oscillations parameters favored by the LSND experiment without the need to assume that the oscillation parameters for $ν$ and $\nub$ are the same. We present the most stringent experimental limits for $ν_μ(\barν_μ) \to ν_e (\barν_e)$ oscillations in the large $Δm^2$ region.

hep-ex↗