Measurement of $σ\cdot B (W \to e ν)$ and $σ\cdot B(Z^0 \to e^+e^-)$ in $p {\bar p}$ collisions at $\sqrt{s}=1.8$ TeV

Details Measurement of $σ\cdot B (W \to e ν)$ and $σ\cdot B(Z^0 \to e^+e^-)$ in $p {\bar p}$ collisions at $\sqrt{s}=1.8$ TeV Measurement of $σ\cdot B (W \to e ν)$ and $σ\cdot B(Z^0 \to e^+e^-)$ in $p {\bar p}$ collisions at $\sqrt{s}=1.8$ TeV

1995-09-25

arxiv.org/abs/hep-ex/9509010v1

Phys.Rev.Lett.76:3070-3075,1996

Physics

High Energy Physics

High Energy Physics - Experiment

Uses Latex, Article 12 point, figure appended as uuencoded file The full PostScript available via WWW at http://www-cdf.fnal

Scientific paper

10.1103/PhysRevLett.76.3070

We present a measurement of $\sigma \cdot B(W \to e \nu)$ and $\sigma \cdot B(Z^0 \to e^+e^-)$ in proton - antiproton collisions at $\sqrt{s} =1.8$ TeV using a significantly improved understanding of the integrated luminosity. The data represent an integrated luminosity of 19.7 pb$^{-1}$ from the 1992-1993 run with the Collider Detector at Fermilab (CDF). We find $\sigma \cdot B(W \to e \nu) = 2.49 \pm 0.12$~nb and $\sigma \cdot B(Z^0 \to e^+e^-) = 0.231 \pm 0.012$~nb.

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