A Mathematica based Version of the CKMfitter Package
A Mathematica based Version of the CKMfitter Package
A Mathematica based Version of the CKMfitter Package
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η<br />
1.5<br />
1<br />
0.5<br />
0<br />
-0.5<br />
-1<br />
γ<br />
α<br />
-1.5<br />
-1 -0.5 0 0.5 1 1.5 2<br />
ρ<br />
β<br />
CKM<br />
1-CL<br />
f i t t e r<br />
ICHEP 2006<br />
0.9<br />
0.8<br />
0.7<br />
0.6<br />
0.5<br />
0.4<br />
0.3<br />
0.2<br />
0.1<br />
0<br />
(rad)<br />
d<br />
2 ϑ<br />
3<br />
2<br />
1<br />
0<br />
-1<br />
-2<br />
CKM<br />
1-CL<br />
f i t t e r<br />
ICHEP 2006<br />
-3<br />
0 1 2 3<br />
r 2<br />
d<br />
4 5 6<br />
Figure B.4: Constraints within <strong>the</strong> framework <strong>of</strong> New Physics contributions to <strong>the</strong> B 0 - ¯ B 0<br />
mixing amplitude on <strong>the</strong> (¯ρ,¯η) plane (left) and on <strong>the</strong> (r 2 d ,2ϑd) plane (right), obtained from<br />
a global CKM fit including |Vud|, |Vus|, |Vub|, |Vcb|, ∆md, sin 2β, cos 2β and α.<br />
η<br />
1.5<br />
1<br />
0.5<br />
0<br />
-0.5<br />
-1<br />
γ<br />
α<br />
-1.5<br />
-1 -0.5 0 0.5 1 1.5 2<br />
ρ<br />
β<br />
CKM<br />
1-CL<br />
f i t t e r<br />
ICHEP 2006<br />
1<br />
0.9<br />
0.8<br />
0.7<br />
0.6<br />
0.5<br />
0.4<br />
0.3<br />
0.2<br />
0.1<br />
0<br />
(rad)<br />
d<br />
2 ϑ<br />
3<br />
2<br />
1<br />
0<br />
-1<br />
-2<br />
CKM<br />
1-CL<br />
f i t t e r<br />
ICHEP 2006<br />
-3<br />
0 1 2 3<br />
r 2<br />
d<br />
4 5 6<br />
Figure B.5: Constraints within <strong>the</strong> framework <strong>of</strong> New Physics contributions to <strong>the</strong> B 0 - ¯ B 0<br />
mixing amplitude on <strong>the</strong> (¯ρ,¯η) plane (left) and on <strong>the</strong> (r 2 d ,2ϑd) plane (right), obtained from<br />
a global CKM fit including |Vud|, |Vus|, |Vub|, |Vcb|, ∆md and ASL.<br />
1<br />
0<br />
63<br />
0.9<br />
0.8<br />
0.7<br />
0.6<br />
0.5<br />
0.4<br />
0.3<br />
0.2<br />
0.1<br />
1<br />
0.99<br />
0.98<br />
0.97<br />
0.96<br />
0.95<br />
0.94<br />
0.93