2 The CDF Experiment at Fermilab Contents - Harvard University ...
2 The CDF Experiment at Fermilab Contents - Harvard University ...
2 The CDF Experiment at Fermilab Contents - Harvard University ...
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Section 2: B Mixing and CP Viol<strong>at</strong>ion 93<br />
oscill<strong>at</strong>ion frequency, m s . Additionally, new physics contributing to the B s mixing `box'<br />
diagram would cause a larger m s than Standard Model predictions even if the new physics<br />
does not aect the angles of the unitarity triangle. <strong>The</strong>refore, it is imper<strong>at</strong>ive to measure<br />
m s as a prerequisite for any serious testing of the self-consistency of the CKM m<strong>at</strong>rix.<br />
To measure the B s oscill<strong>at</strong>ion frequency, one needs<br />
1. proper time of the B s decay<br />
2. decay avor of the B s meson, obtained from the B s decay products<br />
3. production avor of the B s meson, inferred either from the decay products of the other<br />
b-quark in the event (in pp collisions, b b are produced in incoherent pairs), or from the<br />
byproducts of the b ! B s hadroniz<strong>at</strong>ion; this process is called avor tagging.<br />
In prepar<strong>at</strong>ion for the B s mixing measurement, the <strong>Harvard</strong> group is involved in the<br />
following tasks:<br />
Generic decay reconstruction tool: Postdoc Maksimovic wrote a generic tool able<br />
to reconstruct an arbitrary decay.<br />
Study of combin<strong>at</strong>orial background for the PAC: Maksimovic utilized this tool<br />
to isol<strong>at</strong>e a sample of events with a lepton and a D s decay in the opposite hemisphere<br />
(to or K K), which provided a basis for a study of combin<strong>at</strong>orial background in<br />
fully reconstructed B s ! D s (n) events, conrming the prior estim<strong>at</strong>e of S=B between<br />
1:2 and 2:1.<br />
Vertex nding in D s X events: Maksimovic isnow focussed on investig<strong>at</strong>ing a technique<br />
to nd the decay point ofaB s ! D s X decay using new Run II software framework<br />
and tools adapted to Run I d<strong>at</strong>a.<br />
Since the B s production avor is determined by the sti trigger lepton in the opposite<br />
hemisphere (characterized by avery high purity of the avor tag), the B s decay vertex<br />
is the only ingredient missing in a B s mixing analysis. Given th<strong>at</strong> D s X sample is a<br />
superset of D s (n) sample design<strong>at</strong>ed for B s mixing, this approach has a potential to<br />
be the rst analysis to actually measure m s in Run II.<br />
Other tagging studies: Maksimovic isinvolved in other studies of the `opposite side<br />
tagging' (avor tagging involving decay products of the b-hadron in the opposite hemisphere),<br />
using the samples of B 0;+ ! `+D () decays.