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

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D* Signal and Vertexing<br />

N events/200 keV<br />

200<br />

100<br />

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

Be<strong>for</strong>e refit<br />

σ 1<br />

=354 keV (27%)<br />

σ 2<br />

=908 keV (73%)<br />

◆ ∆m resolution improves with beam<br />

pr<strong>of</strong>ile constraint<br />

Entries/0.1 ps<br />

60<br />

~220 pb-1<br />

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

40<br />

N events/200 keV<br />

0<br />

300<br />

200<br />

0.14 0.145 0.15 0.155<br />

m(Kππ) - m(Kπ)<br />

GeV<br />

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

After refit<br />

σ 1<br />

=280 keV (47%)<br />

σ 2<br />

=679 keV (53%)<br />

20<br />

0<br />

-3 -2 -1 0 1 2 3<br />

Candidate D 0 → kπ proper decay time (ps)<br />

100<br />

N(D 0 ) 668 ± 33<br />

N(bkg) 79 ± 11<br />

0<br />

0.14 0.145 0.15 0.155<br />

m(Kππ) - m(Kπ)<br />

GeV<br />

τ(D 0 )<br />

σ(t)<br />

407 ± 25 ps<br />

437 ± 25 ps<br />

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

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