Constraints On R Sub B And Gamma In B Sup Rightarrow D Sup 0 K Sup Decays By A Dalitz Analysis Of D Sup 0 Rightarrow K Sub S Pi Sup Pi Sup
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Constraints on R[sub B] and Gamma in B[sup [+-] Rightarrow D[sup 0]K[sup [+-] Decays by a Dalitz Analysis of D[sup 0] Rightarrow K[sub S] Pi[sup -] Pi[sup +].
![Constraints on R[sub B] and Gamma in B[sup [+-] Rightarrow D[sup 0]K[sup [+-] Decays by a Dalitz Analysis of D[sup 0] Rightarrow K[sub S] Pi[sup -] Pi[sup +].](https://library.ardhindie.com/contents/assets/images/blank.png){kind=small}
In this paper the authors report on a measurement of direct CP violation in B[sup -] --> D(*)[sup 0]K[sup -] based on the analysis of the Dalitz distribution of the three-body decay D[sup 0] --> K[sub S][pi][sup -][pi][sup +]. The advantage of this method is that it involves the entire resonant substructure of the three-body decay, with Cabibbo-allowed and double Cabibbo-suppressed amplitudes interfering directly. It is therefore expected to have a higher statistical precision than the methods outlined.
Constraints on R{sub B} and Gamma in B{sup {+-}} Rightarrow D{sup 0}K{sup {+-}} Decays by a Dalitz Analysis of D{sup 0} Rightarrow K{sub S} Pi{sup -} Pi{sup +}
In this paper the authors report on a measurement of direct CP violation in B{sup -} --> D(*){sup 0}K{sup -} based on the analysis of the Dalitz distribution of the three-body decay D{sup 0} --> K{sub S}{pi}{sup -}{pi}{sup +}. The advantage of this method is that it involves the entire resonant substructure of the three-body decay, with Cabibbo-allowed and double Cabibbo-suppressed amplitudes interfering directly. It is therefore expected to have a higher statistical precision than the methods outlined.
Constraints on R{sub B} and Gamma in B{sup {+-}} Rightarrow D°K{sup {+-}} Decays by a Dalitz Analysis of D° Rightarrow K{sub S} Pi− Pi
In this paper the authors report on a measurement of direct CP violation in B− --> D(*)°K− based on the analysis of the Dalitz distribution of the three-body decay D° --> K{sub S}?−?. The advantage of this method is that it involves the entire resonant substructure of the three-body decay, with Cabibbo-allowed and double Cabibbo-suppressed amplitudes interfering directly. It is therefore expected to have a higher statistical precision than the methods outlined.