Difference: Constraints (1 vs. 10)

Revision 10
24 Jul 2010 - Main.AdminUser
Line: 1 to 1
 

Constraints used in the UT fit

Line: 9 to 9
 
|V_{ub}/V_{cb}| \varepsilon_K \Delta m_d \Delta m_d / \Delta m_s

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Line: 32 to 32
 
\sin{2\beta} \cos{2\beta} \alpha \gamma 2\beta+\gamma B\rightarrow \tau\nu

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Revision 9
21 Jul 2010 - Main.VincenzoVagnoni
Line: 1 to 1
 

Constraints used in the UT fit

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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 (\varepsilon_K). Click on the plots for some details.

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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 (\varepsilon_K).

 

|V_{ub}/V_{cb}| \varepsilon_K \Delta m_d \Delta m_d / \Delta m_s
Revision 8
20 Jul 2010 - Main.AchilleStocchi
Line: 1 to 1
 

Constraints used in the UT fit

Line: 9 to 9
 
|V_{ub}/V_{cb}| \varepsilon_K \Delta m_d \Delta m_d / \Delta m_s

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Line: 32 to 32
 
\sin{2\beta} \cos{2\beta} \alpha \gamma 2\beta+\gamma B\rightarrow \tau\nu

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Revision 7
16 Jul 2010 - Main.DenisDerkach
Line: 1 to 1
 

Constraints used in the UT fit

Line: 58 to 58
 

Deleted:
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Constraints not yet used in the UT fit

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.

K\rightarrow \pi \nu \bar{\nu} (B\rightarrow \rho/\omega \gamma)/(B\rightarrow K^* \gamma)

     

Revision 6
04 Apr 2010 - Main.VincenzoVagnoni
Line: 1 to 1
 

Constraints used in the UT fit

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 (\varepsilon_K). Click on the plots for details.

>
>
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 (\varepsilon_K). Click on the plots for some details.

 

|V_{ub}/V_{cb}| \varepsilon_K \Delta m_d \Delta m_d / \Delta m_s
Revision 5
02 Apr 2010 - Main.VincenzoVagnoni
Line: 1 to 1
 

Constraints used in the UT fit

Line: 57 to 57
 

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Constraints not yet used in the UT fit

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.

Revision 4
01 Apr 2010 - Main.AdminUser
Line: 1 to 1
Added:
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>
 

Constraints used in the UT fit

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 (\varepsilon_K). Click on the plots for details.

Changed:
<
<

|V_{ub}/V_{cb}| \varepsilon_K \Delta m_d \Delta m_d / \Delta m_s
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|V_{ub}/V_{cb}| \varepsilon_K \Delta m_d \Delta m_d / \Delta m_s

 



Line: 34 to 29
  New determinations of UT angles and sides are now available, thanks to the results coming from the B-Factory experiments.

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\sin{2\beta} \cos{2\beta} \alpha \gamma 2\beta+\gamma B\rightarrow \tau\nu
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>
\sin{2\beta} \cos{2\beta} \alpha \gamma 2\beta+\gamma B\rightarrow \tau\nu
 
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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.

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<
K\rightarrow \pi \nu \bar{\nu} (B\rightarrow \rho/\omega \gamma)/(B\rightarrow K^* \gamma)
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K\rightarrow \pi \nu \bar{\nu} (B\rightarrow \rho/\omega \gamma)/(B\rightarrow K^* \gamma)

     
 
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Revision 3
01 Apr 2010 - Main.VincenzoVagnoni
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 (\varepsilon_K).
|V_{ub}/V_{cb}| \varepsilon_K \Delta m_d \Delta m_d / \Delta m_s
>
>
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 (\varepsilon_K). Click on the plots for details.

 
Changed:
<
<
>
>

|V_{ub}/V_{cb}| \varepsilon_K \Delta m_d \Delta m_d / \Delta m_s



New determinations of UT angles and sides are now available, thanks to the results coming from the B-Factory experiments.

\sin{2\beta} \cos{2\beta} \alpha \gamma 2\beta+\gamma B\rightarrow \tau\nu
 
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.

K\rightarrow \pi \nu \bar{\nu} (B\rightarrow \rho/\omega \gamma)/(B\rightarrow K^* \gamma)

Revision 2
31 Mar 2010 - Main.VincenzoVagnoni
Line: 1 to 1
Changed:
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<

Page under construction

>
>

Constraints used in the UT fit

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 (\varepsilon_K).
|V_{ub}/V_{cb}| \varepsilon_K \Delta m_d \Delta m_d / \Delta m_s

Several new determinations of UT angles are now available, thanks to the results coming from the B-Factory experiments.

Constraints not yet used in the UT fit

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.
 
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