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A Mathematica based Version of the CKMfitter Package

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58 Chapter 7. Conclusions and Perspectives<br />

Since all <strong>the</strong> present data from experiments in quark-flavor physics is well described<br />

by <strong>the</strong> Standard Model, <strong>the</strong> space for New Physics contributions is significantly constrained.<br />

Never<strong>the</strong>less, <strong>the</strong>re is still enough space for possible New Physics effects,<br />

which have been quantified in this <strong>the</strong>sis in two different extensions <strong>of</strong> <strong>the</strong> Standard<br />

Model.<br />

Possible New Physics contributions to neutral meson oscillations have been implemented<br />

model-independently to <strong>the</strong> B-meson systems as well as to <strong>the</strong> Kaon system.<br />

The allowed ranges for <strong>the</strong> NP parameters (r 2 d ,2ϑd) in <strong>the</strong> Bd system have been found<br />

to:<br />

r 2 d<br />

= 1.02 +0.50<br />

−0.42 and 2ϑd = −0.094 +0.049<br />

−0.123 (at 68 % CL), (7.3)<br />

which is in good agreement with <strong>the</strong> Standard Model. The small bias in 2ϑd results<br />

from <strong>the</strong> slight disagreement <strong>of</strong> <strong>the</strong> measurements <strong>of</strong> |Vub|incl and sin 2β. Since a<br />

significant constraint on possible New Physics in B 0 - ¯ B 0 mixing is obtained from <strong>the</strong><br />

observable ASL, its <strong>the</strong>oretical prediction has been implemented including LO QCD<br />

corrections as well as NLO QCD corrections. A preliminary comparison <strong>of</strong> <strong>the</strong>ir SM<br />

predictions is given in this <strong>the</strong>sis.<br />

Contributions <strong>of</strong> charged Higgs bosons to <strong>the</strong> branching fraction <strong>of</strong> leptonic B-meson<br />

decays have been implemented in <strong>the</strong> framework <strong>of</strong> Two-Higgs-Doublet Models. Since<br />

only <strong>the</strong> decay B + → τ + ντ is currently experimentally accessible, <strong>the</strong> constraint<br />

on (tan β,m H +) is still loose. An additional fit input from B → Xsγ transitions<br />

would provide an additional constraint, but has not been implemented yet.<br />

To guarantee <strong>the</strong> stability <strong>of</strong> <strong>the</strong> fit results by using <strong>the</strong> <strong>Ma<strong>the</strong>matica</strong> <strong>based</strong> <strong>CKMfitter</strong><br />

package, several comparison tests with <strong>the</strong> original package have been performed.<br />

As a benefit to <strong>the</strong> <strong>CKMfitter</strong> group, a user guide has been written during this <strong>the</strong>sis<br />

as well as a tutorial on <strong>the</strong> coding <strong>of</strong> <strong>the</strong>ory packages.<br />

After more than one year <strong>of</strong> development, <strong>the</strong> <strong>Ma<strong>the</strong>matica</strong> <strong>based</strong> version <strong>of</strong> <strong>the</strong><br />

<strong>CKMfitter</strong> package has been used for <strong>the</strong> first time to produce <strong>the</strong> fit results for<br />

a large conference (ICHEP 2006). Never<strong>the</strong>less, a lot <strong>of</strong> features available in <strong>the</strong><br />

original <strong>CKMfitter</strong> package are still missing. A Wolfenstein parameter independent<br />

prediction <strong>of</strong> B(B + → l + νl) as well as <strong>the</strong> <strong>the</strong>ory <strong>of</strong> rare Kaon decays need to be<br />

implemented.<br />

Due to its modular structure, <strong>the</strong> new <strong>Ma<strong>the</strong>matica</strong> <strong>based</strong> version <strong>of</strong> <strong>the</strong> <strong>CKMfitter</strong><br />

package is not only restricted to <strong>the</strong> CKM matrix analysis. Fur<strong>the</strong>r applications,<br />

e. g. a leptonic mixing matrix analysis could be easily added.

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