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A Mathematica based Version of the CKMfitter Package

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Chapter 7<br />

Conclusions and Perspectives<br />

This <strong>the</strong>sis is a contribution to <strong>the</strong> development <strong>of</strong> a <strong>Ma<strong>the</strong>matica</strong> <strong>based</strong> version <strong>of</strong><br />

<strong>the</strong> <strong>CKMfitter</strong> package. It had been introduced by Jérôme Charles to obtain a<br />

significant fit time reduction compared to <strong>the</strong> original FORTRAN <strong>based</strong> <strong>CKMfitter</strong><br />

package. Using symbolic calculations during <strong>the</strong> fit preparation and an efficient<br />

FORTRAN <strong>based</strong> minimization routine, a gain in CPU time <strong>of</strong> more than a factor<br />

100 has been achieved for <strong>the</strong> Standard Global CKM Fit.<br />

Related to <strong>the</strong> Standard Global CKM Fit, <strong>the</strong> <strong>the</strong>ory <strong>of</strong> neutral meson oscillations<br />

has been implemented for <strong>the</strong> B 0 d , B0 s and K 0 systems as well as <strong>the</strong> <strong>the</strong>ory predictions<br />

for <strong>the</strong> branching fraction <strong>of</strong> purely leptonic B-meson decays. More specifically,<br />

<strong>the</strong> following observables have been implemented: ∆md, ∆ms, ASL, |ɛK| and<br />

B(B + → l + νl).<br />

For <strong>the</strong> treatment <strong>of</strong> look-up-table input files, e. g. for ∆ms, B(B + → τ + ντ ) and <strong>the</strong><br />

UT angles α and γ, FORTRAN <strong>based</strong> subroutines (TABLEAU, dTABLEAUO2, LoadLUT)<br />

have been coded. The interpolation <strong>of</strong> <strong>the</strong> look-up tables is performed by a <strong>Ma<strong>the</strong>matica</strong>-<strong>based</strong><br />

subroutine using cubic spline interpolation.<br />

The results <strong>of</strong> <strong>the</strong> Standard Global CKM Fit show a good agreement between SM<br />

predictions and recent data. The Wolfenstein parameters have been constraint<br />

at 68 % CL to:<br />

A = 0.813 +0.015<br />

+0.0010<br />

+0.028<br />

+0.038<br />

−0.015 , λ = 0.2272 −0.0010 , ¯ρ = 0.187 −0.086 , ¯η = 0.333 −0.017 , (7.1)<br />

and <strong>the</strong> Jarlskog invariant, which is related to <strong>the</strong> strength <strong>of</strong> CP violation in electroweak<br />

transitions is found to be:<br />

J = � 3.02 +0.36�<br />

−5<br />

−0.18 · 10 . (7.2)<br />

57

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