L. T. Kerth

Experimental Limits on the DecaysKL0→μ+μ−,e+e−, and μ±e∓

We have performed a search at the Bevatron for the decays

Search for hadronic decays of a light higgs boson in the radiative decay

{{K}_{L}}^{0}\ensuremath{\rightarrow}{\ensuremath{\mu}}^{+}{\ensuremath{\mu}}^{\ensuremath{-}},{e}^{+}{e}^{\ensuremath{-}}, \mathrm{and} {\ensuremath{\mu}}^{\ifmmode\pm\else\textpm\fi{}}{e}^{\ensuremath{\mp}}

Cylindrical spark chamber array used for the measurement of angle, range and polarization in a study of K−-p interactions

with a double magnetic spectrometer using wire spark chambers. Over

A magnetic spectrometer using spark chambers to obtain large solid angle and high resolution in π-π interaction studies☆

{10}^{6}

Time-dependent analysis of B0 → KS0 π-π+γ decays and studies of the K+π-π+ system in B+ →k+π-π+γ decays

observed

Measurements of CP-Violating Asymmetries in B0→ K s 0π0 Decays

{{K}_{L}}^{0}\ensuremath{\rightarrow}{\ensuremath{\pi}}^{+}{\ensuremath{\pi}}^{\ensuremath{-}}

Observed difference in the ranges of positive and negative muons

decays determine the normalization for the di-lepton decay modes. No

Search for B̄→Λc+X -ν ̄ decays in events with a fully reconstructed B meson

{e}^{+}{e}^{\ensuremath{-}}

Experimental Limits on the Decays K L 0 → μ + μ − , e + e − , and μ ± e ∓

or

LOW-DENSITY POLYURETHANE FOAM PLATE SPARK CHAMBER

{\ensuremath{\mu}}^{\ifmmode\pm\else\textpm\fi{}}{e}^{\ensuremath{\mp}}