Observation of the $B^0_s\!\to D^{*+}D^{*-}$ decay

LHCb collaboration,R. Aaij,A. S. W. Abdelmotteleb,C. Abellán Beteta,F. Abudinén,T. Ackernley,B. Adeva,M. Adinolfi,P. Adlarson,H. Afsharnia,C. Agapopoulou,C. A. Aidala,S. Aiola,Z. Ajaltouni,S. Akar,J. Albrecht,F. Alessio,M. Alexander, A. Alfonso Albero,Z. Aliouche,G. Alkhazov,P. Alvarez Cartelle,R. Amalric,S. Amato,J. L. Amey,Y. Amhis,L. An,L. Anderlini,M. Andersson,A. Andreianov,M. Andreotti,D. Andreou,D. Ao,F. Archilli,A. Artamonov,M. Artuso,E. Aslanides,M. Atzeni,B. Audurier,S. Bachmann,M. Bachmayer,J. J. Back, A. Bailly-reyre,P. Baladron Rodriguez,V. Balagura,W. Baldini,J. Baptista de Souza Leite,M. Barbetti,R. J. Barlow,S. Barsuk,W. Barter,M. Bartolini,F. Baryshnikov,J. M. Basels,G. Bassi,B. Batsukh,A. Battig,A. Bay,A. Beck,M. Becker,F. Bedeschi,I. Bediaga,A. Beiter,V. Belavin,S. Belin,V. Bellee,K. Belous,I. Belov,I. Belyaev,G. Benane,G. Bencivenni,E. Ben-Haim,A. Berezhnoy,R. Bernet,S. Bernet Andres, D. Berninghoff,H. C. Bernstein,C. Bertella,A. Bertolin,C. Betancourt,F. Betti,Ia. Bezshyiko,S. Bhasin,J. Bhom,L. Bian,M. S. Bieker,N. V. Biesuz,S. Bifani,P. Billoir,A. Biolchini,M. Birch,F. C. R. Bishop,A. Bitadze,A. Bizzeti,M. P. Blago,T. Blake,F. Blanc,S. Blusk,D. Bobulska,J. A. Boelhauve,O. Boente Garcia,T. Boettcher,A. Boldyrev,C. S. Bolognani,R. Bolzonella,A. Bondar,N. Bondar,F. Borgato,S. Borghi,M. Borsato,J. T. Borsuk,S. A. Bouchiba,T. J. V. Bowcock,A. Boyer,C. Bozzi,M. J. Bradley,S. Braun,A. Brea Rodriguez,J. Brodzicka,A. Brossa Gonzalo,J. Brown,D. Brundu,A. Buonaura,L. Buonincontri,A. T. Burke,C. Burr,A. Bursche,A. Butkevich,J. S. Butter,J. Buytaert,W. Byczynski,S. Cadeddu,H. Cai,R. Calabrese,L. Calefice,S. Cali,R. Calladine,M. Calvi,M. Calvo Gomez,P. Campana,D. H. Campora Perez,A. F. Campoverde Quezada,S. Capelli,L. Capriotti,A. Carbone,G. Carboni,R. Cardinale,A. Cardini,I. Carli,P. Carniti,L. Carus,K. Carvalho Akiba,A. Casais Vidal,R. Caspary,G. Casse,M. Cattaneo,G. Cavallero,V. Cavallini,S. Celani,J. Cerasoli,D. Cervenkov,A. J. Chadwick,M. G. Chapman,M. Charles,Ph. Charpentier,C. A. Chavez Barajas,M. Chefdeville,C. Chen,S. Chen,A. Chernov,S. Chernyshenko,V. Chobanova,S. Cholak,M. Chrzaszcz,A. Chubykin,V. Chulikov,P. Ciambrone,M. F. Cicala,X. Cid Vidal,G. Ciezarek,P. E. L. Clarke,M. Clemencic,H. V. Cliff,J. Closier,J. L. Cobbledick,V. Coco,J. A. B. Coelho,J. Cogan,E. Cogneras,L. Cojocariu,P. Collins,T. Colombo,L. Congedo,A. Contu,N. Cooke,I. Corredoira,G. Corti,B. Couturier,D. C. Craik,J. Crkovská,M. Cruz Torres,R. Currie,C. L. Da Silva,S. Dadabaev,L. Dai,X. Dai,E. Dall'Occo,J. Dalseno,C. D'Ambrosio,J. Daniel,A. Danilina,P. d'Argent,J. E. Davies,A. Davis,O. De Aguiar Francisco,J. de Boer,K. De Bruyn,S. De Capua,M. De Cian,U. De Freitas Carneiro Da Graca,E. De Lucia,J. M. De Miranda,L. De Paula,M. De Serio,D. De Simone,P. De Simone,F. De Vellis,J. A. de Vries,C. T. Dean,F. Debernardis,D. Decamp,V. Dedu,L. Del Buono,B. Delaney,H. -P. Dembinski,V. Denysenko,D. Derkach,O. Deschamps,F. Dettori,B. Dey,A. Di Cicco,P. Di Nezza,I. Diachkov,S. 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arXiv (Cornell University)(2022)

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摘要
The first observation of the $B^0_s\!\to D^{*+}D^{*-}$ decay and the measurement of its branching ratio relative to the $B^0\!\to D^{*+}D^{*-}$ decay are presented. The data sample used corresponds to an integrated luminosity of 9$\,\text{fb}^{-1}$ of proton-proton collisions recorded by the LHCb experiment at centre-of-mass energies of 7, 8 and 13$\,\text{TeV}$ between 2011 and 2018. The decay is observed with a very high significance and the ratio of branching fractions is determined to be \begin{align*} \frac{\mathcal{B}(B^0_s\!\to D^{*+}D^{*-})}{\mathcal{B}(B^0\!\to D^{*+}D^{*-})} = 0.269 \pm 0.032 \pm 0.011 \pm 0.008\, , \end{align*} where the first uncertainty is statistical, the second systematic and the third due to the uncertainty of the fragmentation fraction ratio $f_s/f_d$. The $B^0_s\!\to D^{*+}D^{*-}$ branching fraction is calculated to be \begin{align*} \mathcal{B}(B^0_s\!\to D^{*+}D^{*-}) = (2.15 \pm 0.26 \pm 0.09 \pm 0.06 \pm 0.16)\times 10^{-4} \,, \end{align*} where the fourth uncertainty is due to the $B^0\!\to D^{*+}D^{*-}$ branching fraction.
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