Alan R. Clark

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

We have performed a search at the Bevatron for the decays

Spatial Resolution of the PEP-4 Time Projection Chamber

{{K}_{L}}^{0}ensuremath{rightarrow}{ensuremath{mu}}^{+}{ensuremath{mu}}^{ensuremath{-}},{e}^{+}{e}^{ensuremath{-}}, mathrm{and} {ensuremath{mu}}^{ifmmodepmelsetextpmfi{}}{e}^{ensuremath{mp}}

Measurement of Ionization Loss in the Relativistic Rise Region with the Time Projection Chamber

with a double magnetic spectrometer using wire spark chambers. Over

Geiger Mode Calorimeter for PEP-4

{10}^{6}

Performance of the Signal Processing System for the Time Projection Chamber

observed

Performance of a Drift Chamber System for the Time Projection Chamber Detector Facility at PEP

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

A Muon Detection System for the PEP4 Facility

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

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

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

LOW-DENSITY POLYURETHANE FOAM PLATE SPARK CHAMBER

or

Orthogonal Dispersion Spectrometer for Missing Mass Spectra

{ensuremath{mu}}^{ifmmodepmelsetextpmfi{}}{e}^{ensuremath{mp}}