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Martin Lewis Perl coauthored the evidence that led to identification of the tau lepton. The experiment found electron-muon pairs of opposite electric charges in electron–positron annihilation, with missing energy and momentum and no other detected charged particles or photons. The distributions required additional unseen particles. Studying these unusual final states provided a route to recognizing a new unstable lepton, even though it decayed before leaving a directly visible track.^[ref]

An experimental physicist who led particle searches at SLAC.^[ref]

For pioneering experimental contributions to lepton physics, one half went to Martin Lewis Perl for discovering the tau lepton; the other half went to Frederick Reines for detecting the neutrino.^[ref]

Counterrotating electron and Positron beams at SPEAR collided inside the Mark I magnetic particle detector. Lead–scintillator scintillation counters identified electrons through large shower pulses; small pulses plus hits beyond the iron return identified muons.^[ref]

The selection required opposite-charge electron–muon tracks, no detected photons, momenta above $0.65\mathrm{GeV}/c$, and transverse noncoplanarity above $20^{\circ }$. Multitrack hadron samples calibrated momentum-dependent misidentification; collinear lepton pairs checked identification losses. Photon and charge control samples tested backgrounds. Acceptance corrections depended on the proposed signal.^[ref]

The 1975 claim was anomalous events without a conventional explanation; new-particle pair production was a possible interpretation.^[ref] Martin Lewis Perl's lecture describes subsequent evidence for a charged lepton.^[ref]

The particle identification problem matters as much as the apparent missing four-momentum in electron-positron collisions. A penetrating hadron can imitate a muon; a particle shower can imitate an electron; an undetected photon or a detector gap can imitate invisible recoil. An absence of additional recorded signals is conditional on detection efficiency. In a proposed signal model, the selected count has the schematic formwhere $\mathcal{L}$ is integrated collider luminosity, $\sigma$ a cross section, and $\epsilon$ the combined acceptance and detection efficiency. A single count cannot determine all three factors. A control sample must probe the relevant momentum and angular range; its abundant events do not automatically calibrate a differently distributed signal.