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The Bˉ0→D∗+Dˉ∗0K−\bar{B}^0 \to D^{*+} \bar{D}^{*0} K^- reaction to detect the I=0,JP=1+I=0, J^P=1^+ partner of the X0(2866)X_0(2866)

Published 1 Feb 2022 in hep-ph and hep-ex | (2202.00508v2)

Abstract: We have chosen the Bˉ<sup>0</sup>→D<sup>∗+</sup>Dˉ<sup>∗0</sup>K<sup>−\bar{B}<sup>0</sup> \to D<sup>{*+}</sup> \bar{D}<sup>{*0}</sup> K<sup>- reaction in order to observe the I=0,J<sup>P=1<sup>+I=0, J<sup>P=1<sup>+ (R1R_1) partner state of the X0(2866)X_0(2866) stemming from the D<sup><em>Kˉ</em>D<sup><em>\bar{K}^</em> molecular picture. The reaction proceeds via external emission in the most favored Cabibbo decay mode and one observes the R1R_1 state as a very strong peak versus the background in the D<sup>∗+</sup>K<sup>−D<sup>{*+}</sup> K<sup>- spectrum. The branching ratio for R1R_1 production in this reaction is estimated of the order of 4×10<sup>−34\times 10<sup>{-3}. The method used, applied to the B<sup>+</sup>→D<sup>−</sup>D<sup>+</sup>K<sup>+B<sup>+</sup> \to D<sup>-</sup> D<sup>+</sup> K<sup>+ reaction, produces a ratio of signal to background in the D<sup>−</sup>K<sup>+D<sup>-</sup> K<sup>+ spectrum in very good agreement with the LHCb experiment that observed the X0(2866)X_0(2866).

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