Line: 1 to 1 | ||||||||
---|---|---|---|---|---|---|---|---|
| ||||||||
Changed: | ||||||||
< < |
Before the B-Factory era, the fit was done using the measurements of UT sides (through semileptonic decays and mixing processes of the B mesons) and the determination of direct CP violation in Kaon system (![]() | |||||||
> > |
Before the B-Factory era, the fit was done using the measurements of UT sides (through semileptonic decays and mixing processes of the B mesons) and the determination of direct CP violation in Kaon system (![]() | |||||||
|
Line: 1 to 1 | |||||||||
---|---|---|---|---|---|---|---|---|---|
Added: | |||||||||
> > | |||||||||
Constraints used in the UT fitBefore the B-Factory era, the fit was done using the measurements of UT sides (through semileptonic decays and mixing processes of the B mesons) and the determination of direct CP violation in Kaon system (![]() | |||||||||
Changed: | |||||||||
< < |
| ||||||||
> > |
| ||||||||
Line: 34 to 29 | |||||||||
New determinations of UT angles and sides are now available, thanks to the results coming from the B-Factory experiments. | |||||||||
Changed: | |||||||||
< < |
| ||||||||
> > |
| ||||||||
Changed: | |||||||||
< < | |||||||||
> > | |||||||||
Changed: | |||||||||
< < | |||||||||
> > | |||||||||
Line: 82 to 63 | |||||||||
Further bounds are available from rare B and K decays. They do not still have a strong impact on the global fit and they are not used at present. | |||||||||
Changed: | |||||||||
< < |
| ||||||||
> > |
| ||||||||
Changed: | |||||||||
< < | |||||||||
> > | |||||||||
Added: | |||||||||
> > |
Line: 1 to 1 | ||||||||||||||||||
---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|
Constraints used in the UT fit | ||||||||||||||||||
Changed: | ||||||||||||||||||
< < |
Before the starting of B-Factory experiments, the fit was done using the measurements of sides (through semileptonic decays and mixing processes of the B mesons) and the determination of direct CP violation in Kaon system (![]()
| |||||||||||||||||
> > |
Before the B-Factory era, the fit was done using the measurements of UT sides (through semileptonic decays and mixing processes of the B mesons) and the determination of direct CP violation in Kaon system (![]() | |||||||||||||||||
Changed: | ||||||||||||||||||
< < | ||||||||||||||||||
> > |
New determinations of UT angles and sides are now available, thanks to the results coming from the B-Factory experiments.
| |||||||||||||||||
Changed: | ||||||||||||||||||
< < | Several new determinations of UT angles are now available, thanks to the results coming from the B-Factory experiments. | |||||||||||||||||
> > | ||||||||||||||||||
Added: | ||||||||||||||||||
> > | ||||||||||||||||||
Constraints not yet used in the UT fit | ||||||||||||||||||
Changed: | ||||||||||||||||||
< < | New bounds are available from rare B and K decays. They do not still have a strong impact on the global fit and they are not used at present. | |||||||||||||||||
> > |
Further bounds are available from rare B and K decays. They do not still have a strong impact on the global fit and they are not used at present.
|
Line: 1 to 1 | |||||||||
---|---|---|---|---|---|---|---|---|---|
Changed: | |||||||||
< < |
Page under construction | ||||||||
> > |
Constraints used in the UT fitBefore the starting of B-Factory experiments, the fit was done using the measurements of sides (through semileptonic decays and mixing processes of the B mesons) and the determination of direct CP violation in Kaon system (![]()
Constraints not yet used in the UT fitNew bounds are available from rare B and K decays. They do not still have a strong impact on the global fit and they are not used at present. |