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Violation in Mixing

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94 Ã Ë reconstruction and efficiency studies<br />

2<br />

1.75<br />

1.5<br />

1.25<br />

1<br />

0.75<br />

0.5<br />

0.25<br />

0<br />

0 5 10 15 20 25 30 35 40<br />

b1 sample: red dots with 1Gev cut<br />

2.25<br />

2<br />

1.75<br />

1.5<br />

1.25<br />

1<br />

0.75<br />

0.5<br />

0.25<br />

0<br />

0 5 10 15 20 25 30 35 40<br />

b2 sample: red dots with 1Gev cut<br />

Figure 3-14. Values of the Ã Ë efficiency corrections for block 1 (left) and block 2 (right) data. The red dots<br />

represent the corrections with the 1GeV momentum cut, while the black one are the values obta<strong>in</strong>ed from the<br />

no momentum-cut sample.<br />

x 10 2<br />

9000<br />

8000<br />

7000<br />

6000<br />

5000<br />

4000<br />

3000<br />

2000<br />

1000<br />

0<br />

649.7 / 52<br />

P1 0.9459E+06 1729.<br />

P2 -0.7791E+06 3422.<br />

P3 0.1727E+07 5209.<br />

P4 0.4968 0.5849E-04<br />

P5 0.7816E-02 0.9534E-04<br />

P6 0.4107 0.4304E-02<br />

P7 0.4974 0.7716E-05<br />

P8 0.2472E-02 0.1094E-04<br />

0.46 0.48 0.5 0.52 0.54<br />

Figure 3-15. Ã Ë candidate <strong>in</strong>variant mass <strong>in</strong> Run 2 on-resonance data. The superimposed curve is the<br />

result of the fit with a double Gaussian and a l<strong>in</strong>ear background.<br />

MARCELLA BONA

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