"The mu tau and e tau Decays of Top Quark Pairs Produced in p-pbar Collisions at root s = 1.8 TeV" In a paper submitted to Physical Review Letters, the CDF collaboration presents four events as candidates for decays of the heaviest quark, called the top quark, into a bigger brother of the electron, known as the tau lepton. The fundamental building blocks of matter, six different types of quarks and six different types of leptons, are found to come in three groups, called "generations" by particle physicists. The most important difference between the generations is the masses of the particles: the first generation comprises the lightest particles, while the third generation includes the heaviest. For example, the well-known electron is a lepton of the first generation. The second generation contains the "muon" lepton, which is about 200 times heavier than the electron. The "tau" lepton in the third generation is about 3500 times as heavy as the electron. Similarly, the heaviest quark of all, called the top quark, belongs to the third generation. It is more than 10,000 times heavier than the quarks in the first generation. The origin of this hierarchy of masses is little understood and is considered one of the most fundamental problems in particle physics today. Top quarks are unstable particles which decay quickly into bottom quarks plus pairs of light quarks or pairs of leptons. The highly successful Standard Model of Particle Physics predicts that top quark decays produce leptons from the three generations (electrons, muons, taus) equally often. On the other hand, certain extensions of the Standard Model, which attempt to address the problem of particle masses, predict more decays into tau leptons than into electrons or muons. This makes top quark decays that involve tau leptons an interesting place to look for problems with the Standard Model, which could then provide further insight to help physicists solve the mass problem. When the top quark was discovered at Fermilab in 1995, only decays involving electrons and muons were used because identifying tau leptons in the detectors is more difficult. CDF reported seven events with either two electrons, two muons, or an electron and a muon from the simultaneous decay of a top and an antitop quark. While electrons and muons leave quite specific signatures in the detector, tau leptons themselves actually decay into electrons, muons, or hadrons (composite particles made of quarks and/or antiquarks) and must be identified using the properties of their decay products. CDF has now developed such an identification technique for tau leptons that decay into hadrons. The Standard Model predicts that CDF should have observed about one event from top quark decays into tau leptons. Because of the difficulty with the identification of tau leptons it is possible that events that are not actually from the decays of top quarks into tau leptons can be mistaken for top quark decays. These events are called background events and CDF expects to have observed about two such background events. In their data CDF find four events with an electron or muon plus a tau lepton candidate, consistent with Standard Model expectations. An additional handle for reducing the background is the identification of bottom quarks that are always produced in top quark decays but usually not in background events. If the identification of at least one bottom quark is required only 0.3 background events are expected in the data. In three of the four candidate events a bottom quark has been identified. This supports the hypothesis that some of the observed four events are caused by top quarks decaying into tau leptons.
Marcus Hohlmann [hohlmann@uccdf.uchicago.edu]
Michele Gallinaro [michgall@fnald.fnal.gov]
Henry Frisch [frisch@uccdf.uchicago.edu]