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First Year of BABAR/PEP-II - Harvard University Laboratory for ...

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Candidates / 10 MeV/c 2<br />

60<br />

40<br />

20<br />

<strong>BABAR</strong><br />

σ = 16 MeV<br />

J/ψ → l + l - Signal<br />

J/ψ → e + e - (~540 pb -1 ) J/ψ →µ + µ - (~380 pb -1 )<br />

Candidates / 10 MeV/c 2<br />

100<br />

75<br />

50<br />

25<br />

J/ψ → µ + µ -<br />

<strong>BABAR</strong><br />

σ = 15 MeV<br />

J/ψ → e + e - m(e + e - )<br />

0<br />

2.6 2.8 3 3.2 3.4<br />

m(e + e - )<br />

GeV/c 2<br />

→ Already reasonable, but can be improved<br />

0<br />

2.6 2.8 3 3.2 3.4<br />

m(µ + µ - )<br />

GeV/c 2<br />

Tail due to Bremsstrahlung Background due to muon ID<br />

◆ Efficiency consistent with expectation<br />

<strong>First</strong> <strong>Year</strong> <strong>of</strong> BaBar/<strong>PEP</strong>-<strong>II</strong> Masahiro Morii SLAC

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