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Precise determination of the $B_{\mathrm{s}}^0$–$\overline B_{\mathrm{s}}^0$ oscillation frequency

Mesons comprising a beauty quark and a strange quark can oscillate between particle ($B^0_s$) and antiparticle ($\overline{B}^0_s$) flavour eigenstates, with a frequency given by the mass difference between heavy and light mass eigenstates, $\Delta m_{s}$. Here we present a measurement of $\Delta m_...

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Detalles Bibliográficos
Autores principales: Aaij, R., Beteta, C. Abellán, Ackernley, T., Adeva, B., Adinolfi, M., Afsharnia, H., Aidala, C.A., Aiola, S., Ajaltouni, Z., Akar, S., Albrecht, J., Alessio, F., Alexander, M., Albero, A. Alfonso, Aliouche, Z., Alkhazov, G., Cartelle, P. Alvarez, Amato, S., Amhis, Y., An, L., Anderlini, L., Andreianov, A., Andreotti, M., Archilli, F., Artamonov, A., Artuso, M., Arzymatov, K., Aslanides, E., Atzeni, M., Audurier, B., Bachmann, S., Bachmayer, M., Back, J.J., Rodriguez, P. Baladron, Balagura, V., Baldini, W., Leite, J. Baptista, Barlow, R.J., Barsuk, S., Barter, W., Bartolini, M., Baryshnikov, F., Basels, J.M., Bassi, G., Batsukh, B., Battig, A., Bay, A., Becker, M., Bedeschi, F., Bediaga, I., Beiter, A., Belavin, V., Belin, S., Bellee, V., Belous, K., Belov, I., Belyaev, I., Bencivenni, G., Ben-Haim, E., Berezhnoy, A., Bernet, R., Berninghoff, D., Bernstein, H.C., Bertella, C., Bertolin, A., Betancourt, C., Betti, F., Bezshyiko, Ia., Bezshyiko, Iaroslava, Bhasin, S., Bhom, J., Bian, L., Bieker, M.S., Bifani, S., Billoir, P., Birch, M., Bishop, F.C.R., Bitadze, A., Bizzeti, A., Bjørn, M., Blago, M.P., Blake, T., Blanc, F., Blusk, S., Bobulska, D., Boelhauve, J.A., Garcia, O. Boente, Boettcher, T., Boldyrev, A., Bondar, A., Bondar, N., Borghi, S., Borisyak, M., Borsato, M., Borsuk, J.T., Bouchiba, S.A., Bowcock, T.J.V., Boyer, A., Bozzi, C., Bradley, M.J., Braun, S., Rodriguez, A. Brea, Brodski, M., Brodzicka, J., Gonzalo, A. Brossa, Brundu, D., Buonaura, A., Burr, C., Bursche, A., Butkevich, A., Butter, J.S., Buytaert, J., Byczynski, W., Cadeddu, S., Cai, H., Calabrese, R., Calefice, L., Diaz, L. Calero, Cali, S., Calladine, R., Calvi, M., Gomez, M. Calvo, Magalhaes, P. Camargo, Camboni, A., Campana, P., Quezada, A.F. Campoverde, Capelli, S., Capriotti, L., Carbone, A., Carboni, G., Cardinale, R., Cardini, A., Carli, I., Carniti, P., Carus, L., Akiba, K. Carvalho, Vidal, A. Casais, Casse, G., Cattaneo, M., Cavallero, G., Celani, S., Cerasoli, J., Chadwick, A.J., Chapman, M.G., Charles, M., Charpentier, Philippe, Charpentier, Ph., Chatzikonstantinidis, G., Barajas, C.A. Chavez, Chefdeville, M., Chen, C., Chen, S., Chernov, A., Chobanova, V., Cholak, S., Chrzaszcz, M., Chubykin, A., Chulikov, V., Ciambrone, P., Cicala, M.F., Vidal, X. Cid, Ciezarek, G., Clarke, P.E. 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Lenguaje:eng
Publicado: 2021
Materias:
Acceso en línea:https://dx.doi.org/10.1038/s41567-021-01394-x
http://cds.cern.ch/record/2764338
_version_ 1780971105094205440
author Aaij, R.
Beteta, C. Abellán
Ackernley, T.
Adeva, B.
Adinolfi, M.
Afsharnia, H.
Aidala, C.A.
Aiola, S.
Ajaltouni, Z.
Akar, S.
Albrecht, J.
Alessio, F.
Alexander, M.
Albero, A. Alfonso
Aliouche, Z.
Alkhazov, G.
Cartelle, P. Alvarez
Amato, S.
Amhis, Y.
An, L.
Anderlini, L.
Andreianov, A.
Andreotti, M.
Archilli, F.
Artamonov, A.
Artuso, M.
Arzymatov, K.
Aslanides, E.
Atzeni, M.
Audurier, B.
Bachmann, S.
Bachmayer, M.
Back, J.J.
Rodriguez, P. Baladron
Balagura, V.
Baldini, W.
Leite, J. Baptista
Barlow, R.J.
Barsuk, S.
Barter, W.
Bartolini, M.
Baryshnikov, F.
Basels, J.M.
Bassi, G.
Batsukh, B.
Battig, A.
Bay, A.
Becker, M.
Bedeschi, F.
Bediaga, I.
Beiter, A.
Belavin, V.
Belin, S.
Bellee, V.
Belous, K.
Belov, I.
Belyaev, I.
Bencivenni, G.
Ben-Haim, E.
Berezhnoy, A.
Bernet, R.
Berninghoff, D.
Bernstein, H.C.
Bertella, C.
Bertolin, A.
Betancourt, C.
Betti, F.
Bezshyiko, Ia.
Bezshyiko, Iaroslava
Bhasin, S.
Bhom, J.
Bian, L.
Bieker, M.S.
Bifani, S.
Billoir, P.
Birch, M.
Bishop, F.C.R.
Bitadze, A.
Bizzeti, A.
Bjørn, M.
Blago, M.P.
Blake, T.
Blanc, F.
Blusk, S.
Bobulska, D.
Boelhauve, J.A.
Garcia, O. Boente
Boettcher, T.
Boldyrev, A.
Bondar, A.
Bondar, N.
Borghi, S.
Borisyak, M.
Borsato, M.
Borsuk, J.T.
Bouchiba, S.A.
Bowcock, T.J.V.
Boyer, A.
Bozzi, C.
Bradley, M.J.
Braun, S.
Rodriguez, A. Brea
Brodski, M.
Brodzicka, J.
Gonzalo, A. Brossa
Brundu, D.
Buonaura, A.
Burr, C.
Bursche, A.
Butkevich, A.
Butter, J.S.
Buytaert, J.
Byczynski, W.
Cadeddu, S.
Cai, H.
Calabrese, R.
Calefice, L.
Diaz, L. Calero
Cali, S.
Calladine, R.
Calvi, M.
Gomez, M. Calvo
Magalhaes, P. Camargo
Camboni, A.
Campana, P.
Quezada, A.F. Campoverde
Capelli, S.
Capriotti, L.
Carbone, A.
Carboni, G.
Cardinale, R.
Cardini, A.
Carli, I.
Carniti, P.
Carus, L.
Akiba, K. Carvalho
Vidal, A. Casais
Casse, G.
Cattaneo, M.
Cavallero, G.
Celani, S.
Cerasoli, J.
Chadwick, A.J.
Chapman, M.G.
Charles, M.
Charpentier, Philippe
Charpentier, Ph.
Chatzikonstantinidis, G.
Barajas, C.A. Chavez
Chefdeville, M.
Chen, C.
Chen, S.
Chernov, A.
Chobanova, V.
Cholak, S.
Chrzaszcz, M.
Chubykin, A.
Chulikov, V.
Ciambrone, P.
Cicala, M.F.
Vidal, X. Cid
Ciezarek, G.
Clarke, P.E. L.
Clemencic, M.
Cliff, H.V.
Closier, J.
Cobbledick, J.L.
Coco, V.
Coelho, J.A.B.
Cogan, J.
Cogneras, E.
Cojocariu, L.
Collins, P.
Colombo, T.
Congedo, L.
Contu, A.
Cooke, N.
Coombs, G.
Corti, G.
Sobral, C.M. Costa
Couturier, B.
Craik, D.C.
Crkovská, J.
Torres, M. Cruz
Currie, R.
Da Silva, C.L.
Dall'Occo, E.
Dalseno, J.
D'Ambrosio, C.
Danilina, A.
d'Argent, P.
Davis, A.
Francisco, O. De Aguiar
De Bruyn, K.
De Capua, S.
De Cian, M.
De Miranda, J.M.
De Paula, L.
De Serio, M.
De Simone, D.
De Simone, P.
de Vries, J.A.
Dean, C.T.
Decamp, D.
Del Buono, L.
Delaney, B.
Dembinski, H.-P.
Dendek, A.
Denysenko, V.
Derkach, D.
Deschamps, O.
Desse, F.
Dettori, F.
Dey, B.
Di Nezza, P.
Didenko, S.
Maronas, L. Dieste
Dijkstra, H.
Dobishuk, V.
Donohoe, A.M.
Dordei, F.
Reis, A.C. dos
Douglas, L.
Dovbnya, A.
Downes, A.G.
Dreimanis, K.
Dudek, M.W.
Dufour, L.
Duk, V.
Durante, P.
Durham, J.M.
Dutta, D.
Dziurda, A.
Dzyuba, A.
Easo, S.
Egede, U.
Egorychev, V.
Eidelman, S.
Eisenhardt, S.
Ek-In, S.
Eklund, L.
Ely, S.
Ene, A.
Epple, E.
Escher, S.
Eschle, J.
Esen, S.
Evans, T.
Falabella, A.
Fan, J.
Fan, Y.
Fang, B.
Farry, S.
Fazzini, D.
Féo, M.
Prieto, A. Fernandez
Arribas, J.M. Fernandez-tenllado
Fernez, A.D.
Ferrari, F.
Lopes, L. Ferreira
Rodrigues, F. Ferreira
Sole, S. Ferreres
Ferrillo, M.
Ferro-Luzzi, M.
Filippov, S.
Fini, R.A.
Fiorini, M.
Firlej, M.
Fischer, Kamil Leszek
Fischer, K.M.
Fitzgerald, D.S.
Fitzpatrick, C.
Fiutowski, T.
Fleuret, F.
Fontana, M.
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Hu, Jiangqiao
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Kitouni, O.
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Koliiev, S.
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Li, Z.
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Merli, A.
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Mikhasenko, M.
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Millard, E.
Milovanovic, M.
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Minotti, A.
Minzoni, L.
Mitchell, S.E.
Mitreska, B.
Mitzel, D.S.
Mödden, A.
Mohammed, R.A.
Moise, R.D.
Mombächer, T.
Monroy, I.A.
Monteil, S.
Morandin, M.
Morello, G.
Morello, M.J.
Moron, J.
Morris, A.B.
Morris, A.G.
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Muheim, F.
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Müller, D.
Müller, K.
Murphy, C.H.
Murray, D.
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Nakada, T.
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Nanut, T.
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Needham, M.
Neri, I.
Neri, N.
Neubert, S.
Neufeld, N.
Newcombe, R.
Nguyen, T.D.
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Niel, E.M.
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Nikitin, N.
Nolte, N.S.
Nunez, C.
Oblakowska-Mucha, A.
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Rachwal, B.
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Rama, M.
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Rangel, M.S.
Ratnikov, F.
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Alepuz, C. Remon
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Renaudin, V.
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Robertson, G.
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Rodrigues, E.
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Rollings, A.
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Lamas, M. Romero
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Schael, S.
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Smeaton, J.G.
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Smith, E.
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Spaan, B.
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Spradlin, P.
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Szumlak, T.
Szymanski, M.
Taneja, S.
Teubert, F.
Thomas, E.
Thomson, K.A.
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T'Jampens, S.
Tobin, M.
Tomassetti, L.
Machado, D. Torres
Tou, D.Y.
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Trifonova, E.
Trippl, C.
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Uwer, U.
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Vagnoni, V.
Valassi, A.
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Canudas, N. Valls
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Regueiro, P. Vazquez
Sierra, C. Vázquez
Vecchi, S.
Velthuis, J.J.
Veltri, M.
Venkateswaran, A.
Veronesi, M.
Vesterinen, M.
Vieira, D.
Diaz, M. Vieites
Viemann, H.
Vilasis-Cardona, X.
Figueras, E. Vilella
Vincent, P.
Bruch, D. Vom
Vorobyev, A.
Vorobyev, V.
Voropaev, N.
Waldi, R.
Walsh, J.
Wang, C.
Wang, Jialu
Wang, Jianchun
Wang, Jianqiao
Wang, Jike
Wang, M.
Wang, R.
Wang, Y.
Wang, Zhenzi
Wang, Zirui
Wark, H.M.
Watson, N.K.
Weber, S.G.
Websdale, D.
Weisser, C.
Westhenry, B.D.C.
White, D.J.
Whitehead, M.
Wiedner, D.
Wilkinson, G.
Wilkinson, M.
Williams, I.
Williams, Mike
Williams, Mark Richard James
Wilson, F.F.
Wislicki, W.
Witek, M.
Witola, L.
Wormser, G.
Wotton, S.A.
Wu, H.
Wyllie, K.
Xiang, Z.
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Xie, Y.
Xu, A.
Xu, J.
Xu, L.
Xu, M.
Xu, Q.
Xu, Zehua
Xu, Zhihao
Yang, D.
Yang, S.
Yang, Y.
Yang, Zhenwei
Yang, Zishuo
Yao, Y.
Yeomans, L.E.
Yin, H.
Yu, J.
Yuan, X.
Yushchenko, O.
Zaffaroni, E.
Zavertyaev, M.
Zdybal, M.
Zenaiev, O.
Zeng, M.
Zhang, D.
Zhang, L.
Zhang, S.
Zhang, Yanxi
Zhang, Yu
Zhelezov, A.
Zheng, Y.
Zhou, X.
Zhou, Y.
Zhu, X.
Zhu, Z.
Zhukov, V.
Zonneveld, J.B.
Zou, Q.
Zucchelli, S.
Zuliani, D.
Zunica, G.
author_facet Aaij, R.
Beteta, C. Abellán
Ackernley, T.
Adeva, B.
Adinolfi, M.
Afsharnia, H.
Aidala, C.A.
Aiola, S.
Ajaltouni, Z.
Akar, S.
Albrecht, J.
Alessio, F.
Alexander, M.
Albero, A. Alfonso
Aliouche, Z.
Alkhazov, G.
Cartelle, P. Alvarez
Amato, S.
Amhis, Y.
An, L.
Anderlini, L.
Andreianov, A.
Andreotti, M.
Archilli, F.
Artamonov, A.
Artuso, M.
Arzymatov, K.
Aslanides, E.
Atzeni, M.
Audurier, B.
Bachmann, S.
Bachmayer, M.
Back, J.J.
Rodriguez, P. Baladron
Balagura, V.
Baldini, W.
Leite, J. Baptista
Barlow, R.J.
Barsuk, S.
Barter, W.
Bartolini, M.
Baryshnikov, F.
Basels, J.M.
Bassi, G.
Batsukh, B.
Battig, A.
Bay, A.
Becker, M.
Bedeschi, F.
Bediaga, I.
Beiter, A.
Belavin, V.
Belin, S.
Bellee, V.
Belous, K.
Belov, I.
Belyaev, I.
Bencivenni, G.
Ben-Haim, E.
Berezhnoy, A.
Bernet, R.
Berninghoff, D.
Bernstein, H.C.
Bertella, C.
Bertolin, A.
Betancourt, C.
Betti, F.
Bezshyiko, Ia.
Bezshyiko, Iaroslava
Bhasin, S.
Bhom, J.
Bian, L.
Bieker, M.S.
Bifani, S.
Billoir, P.
Birch, M.
Bishop, F.C.R.
Bitadze, A.
Bizzeti, A.
Bjørn, M.
Blago, M.P.
Blake, T.
Blanc, F.
Blusk, S.
Bobulska, D.
Boelhauve, J.A.
Garcia, O. Boente
Boettcher, T.
Boldyrev, A.
Bondar, A.
Bondar, N.
Borghi, S.
Borisyak, M.
Borsato, M.
Borsuk, J.T.
Bouchiba, S.A.
Bowcock, T.J.V.
Boyer, A.
Bozzi, C.
Bradley, M.J.
Braun, S.
Rodriguez, A. Brea
Brodski, M.
Brodzicka, J.
Gonzalo, A. Brossa
Brundu, D.
Buonaura, A.
Burr, C.
Bursche, A.
Butkevich, A.
Butter, J.S.
Buytaert, J.
Byczynski, W.
Cadeddu, S.
Cai, H.
Calabrese, R.
Calefice, L.
Diaz, L. Calero
Cali, S.
Calladine, R.
Calvi, M.
Gomez, M. Calvo
Magalhaes, P. Camargo
Camboni, A.
Campana, P.
Quezada, A.F. Campoverde
Capelli, S.
Capriotti, L.
Carbone, A.
Carboni, G.
Cardinale, R.
Cardini, A.
Carli, I.
Carniti, P.
Carus, L.
Akiba, K. Carvalho
Vidal, A. Casais
Casse, G.
Cattaneo, M.
Cavallero, G.
Celani, S.
Cerasoli, J.
Chadwick, A.J.
Chapman, M.G.
Charles, M.
Charpentier, Philippe
Charpentier, Ph.
Chatzikonstantinidis, G.
Barajas, C.A. Chavez
Chefdeville, M.
Chen, C.
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Cliff, H.V.
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Coco, V.
Coelho, J.A.B.
Cogan, J.
Cogneras, E.
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Collins, P.
Colombo, T.
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d'Argent, P.
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De Paula, L.
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De Simone, P.
de Vries, J.A.
Dean, C.T.
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Del Buono, L.
Delaney, B.
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Dendek, A.
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Derkach, D.
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Di Nezza, P.
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Dijkstra, H.
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Donohoe, A.M.
Dordei, F.
Reis, A.C. dos
Douglas, L.
Dovbnya, A.
Downes, A.G.
Dreimanis, K.
Dudek, M.W.
Dufour, L.
Duk, V.
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Durham, J.M.
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Dzyuba, A.
Easo, S.
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Eidelman, S.
Eisenhardt, S.
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Epple, E.
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Evans, T.
Falabella, A.
Fan, J.
Fan, Y.
Fang, B.
Farry, S.
Fazzini, D.
Féo, M.
Prieto, A. Fernandez
Arribas, J.M. Fernandez-tenllado
Fernez, A.D.
Ferrari, F.
Lopes, L. Ferreira
Rodrigues, F. Ferreira
Sole, S. Ferreres
Ferrillo, M.
Ferro-Luzzi, M.
Filippov, S.
Fini, R.A.
Fiorini, M.
Firlej, M.
Fischer, Kamil Leszek
Fischer, K.M.
Fitzgerald, D.S.
Fitzpatrick, C.
Fiutowski, T.
Fleuret, F.
Fontana, M.
Fontanelli, F.
Forty, R.
Lima, V. Franco
Sevilla, M. Franco
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Wang, Zhenzi
Wang, Zirui
Wark, H.M.
Watson, N.K.
Weber, S.G.
Websdale, D.
Weisser, C.
Westhenry, B.D.C.
White, D.J.
Whitehead, M.
Wiedner, D.
Wilkinson, G.
Wilkinson, M.
Williams, I.
Williams, Mike
Williams, Mark Richard James
Wilson, F.F.
Wislicki, W.
Witek, M.
Witola, L.
Wormser, G.
Wotton, S.A.
Wu, H.
Wyllie, K.
Xiang, Z.
Xiao, D.
Xie, Y.
Xu, A.
Xu, J.
Xu, L.
Xu, M.
Xu, Q.
Xu, Zehua
Xu, Zhihao
Yang, D.
Yang, S.
Yang, Y.
Yang, Zhenwei
Yang, Zishuo
Yao, Y.
Yeomans, L.E.
Yin, H.
Yu, J.
Yuan, X.
Yushchenko, O.
Zaffaroni, E.
Zavertyaev, M.
Zdybal, M.
Zenaiev, O.
Zeng, M.
Zhang, D.
Zhang, L.
Zhang, S.
Zhang, Yanxi
Zhang, Yu
Zhelezov, A.
Zheng, Y.
Zhou, X.
Zhou, Y.
Zhu, X.
Zhu, Z.
Zhukov, V.
Zonneveld, J.B.
Zou, Q.
Zucchelli, S.
Zuliani, D.
Zunica, G.
author_sort Aaij, R.
collection CERN
description Mesons comprising a beauty quark and a strange quark can oscillate between particle ($B^0_s$) and antiparticle ($\overline{B}^0_s$) flavour eigenstates, with a frequency given by the mass difference between heavy and light mass eigenstates, $\Delta m_{s}$. Here we present a measurement of $\Delta m_{s}$ using $B^0_s \rightarrow D_s^- \pi^+$ decays produced in proton-proton collisions collected with the LHCb detector at the Large Hadron Collider. This measurement improves upon the current $\Delta m_{s}$ precision by a factor of two. The oscillation frequency is found to be $\Delta m_{s}$ = 17.7683 $\pm$ 0.0051 $\pm$ 0.0032 ps$^{-1}$, where the first uncertainty is statistical and the second systematic. We combine this result with previous LHCb measurements to determine $\Delta m_{s}$ = 17.7656 $\pm$ 0.0057 ps$^{-1}$.
id cern-2764338
institution Organización Europea para la Investigación Nuclear
language eng
publishDate 2021
record_format invenio
spelling cern-27643382023-08-03T04:08:59Zdoi:10.1038/s41567-021-01394-xhttp://cds.cern.ch/record/2764338engAaij, R.Beteta, C. AbellánAckernley, T.Adeva, B.Adinolfi, M.Afsharnia, H.Aidala, C.A.Aiola, S.Ajaltouni, Z.Akar, S.Albrecht, J.Alessio, F.Alexander, M.Albero, A. AlfonsoAliouche, Z.Alkhazov, G.Cartelle, P. AlvarezAmato, S.Amhis, Y.An, L.Anderlini, L.Andreianov, A.Andreotti, M.Archilli, F.Artamonov, A.Artuso, M.Arzymatov, K.Aslanides, E.Atzeni, M.Audurier, B.Bachmann, S.Bachmayer, M.Back, J.J.Rodriguez, P. BaladronBalagura, V.Baldini, W.Leite, J. 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GranadoGraugés, E.Graverini, E.Graziani, G.Grecu, A.Greeven, L.M.Griffith, P.Grillo, L.Gromov, S.Cazon, B.R. GrubergGu, C.Guarise, M.Günther, P.A.Gushchin, E.Guth, A.Guz, Y.Gys, T.Hadavizadeh, T.Haefeli, G.Haen, C.Haimberger, J.Halewood-leagas, T.Hamilton, P.M.Hammerich, J.P.Han, Q.Han, X.Hancock, T.H.Hansmann-Menzemer, S.Harnew, N.Harrison, T.Hasse, C.Hatch, M.He, J.Hecker, M.Heijhoff, K.Heinicke, K.Hennequin, A.M.Hennessy, K.Henry, L.Heuel, J.Hicheur, A.Hill, D.Hilton, M.Hollitt, S.E.Hu, JiangqiaoHu, JifengHu, W.Huang, W.Huang, X.Hulsbergen, W.Hunter, R.J.Hushchyn, M.Hutchcroft, D.Hynds, D.Ibis, P.Idzik, M.Ilin, D.Ilten, P.Inglessi, A.Ishteev, A.Ivshin, K.Jacobsson, R.Jakobsen, S.Jans, E.Jashal, B.K.Jawahery, A.Jevtic, V.Jezabek, M.Jiang, F.John, M.Johnson, D.Jones, C.R.Jones, T.P.Jost, B.Jurik, N.Kandybei, S.Kang, Y.Karacson, M.Karpov, M.Keizer, F.Kenzie, M.Ketel, T.Khanji, B.Kharisova, A.Kholodenko, S.Kirn, T.Kirsebom, V.S.Kitouni, O.Klaver, S.Klimaszewski, K.Koliiev, S.Kondybayeva, A.Konoplyannikov, A.Kopciewicz, P.Kopecna, R.Koppenburg, P.Korolev, M.Kostiuk, I.Kot, O.Kotriakhova, S.Kravchenko, P.Kravchuk, L.Krawczyk, R.D.Kreps, M.Kress, F.Kretzschmar, S.Krokovny, P.Krupa, W.Krzemien, W.Kucewicz, W.Kucharczyk, M.Kudryavtsev, V.Kuindersma, H.S.Kunde, G.J.Kvaratskheliya, T.Lacarrere, D.Lafferty, G.Lai, A.Lampis, A.Lancierini, D.Lane, J.J.Lane, R.Lanfranchi, G.Langenbruch, C.Langer, J.Lantwin, O.Latham, T.Lazzari, F.Gac, R. LeLee, S.H.Lefèvre, R.Leflat, A.Legotin, S.Leroy, O.Lesiak, T.Leverington, B.Li, H.Li, L.Li, P.Li, S.Li, YimingLi, YutongLi, Z.Liang, X.Lin, T.Lindner, R.Lisovskyi, V.Litvinov, R.Liu, G.Liu, H.Liu, S.Liu, X.Loi, A.Castro, J. LombaLongstaff, I.Lopes, J.H.Lovell, G.H.Lu, Y.Lucchesi, D.Luchuk, S.Martinez, M. LucioLukashenko, V.Luo, Y.Lupato, A.Luppi, E.Lupton, O.Lusiani, A.Lyu, X.Ma, L.Ma, R.Maccolini, S.Machefert, F.Maciuc, F.Macko, V.Mackowiak, P.Maddrell-Mander, S.Madejczyk, O.Mohan, L.R. MadhanMaev, O.Maevskiy, A.Maisuzenko, D.Majewski, M.W.Malczewski, J.J.Malde, S.Malecki, B.Malinin, A.Maltsev, T.Malygina, H.Manca, G.Mancinelli, G.Manuzzi, D.Marangotto, D.Maratas, J.Marchand, J.F.Marconi, U.Mariani, S.Benito, C. MarinMarinangeli, M.Marks, J.Marshall, A.M.Marshall, P.J.Martellotti, G.Martinazzoli, L.Martinelli, M.Santos, D. MartinezVidal, F. MartinezMassafferri, A.Materok, M.Matev, R.Mathad, A.Mathe, Z.Matiunin, V.Matteuzzi, C.Mattioli, K.R.Mauri, A.Maurice, E.Mauricio, J.Mazurek, M.McCann, M.Mcconnell, L.Mcgrath, T.H.McNab, A.McNulty, R.Mead, J.V.Meadows, B.Meaux, C.Meier, G.Meinert, N.Melnychuk, D.Meloni, S.Merk, M.Merli, A.Garcia, L. MeyerMikhasenko, M.Milanes, D.A.Millard, E.Milovanovic, M.Minard, M.-N.Minotti, A.Minzoni, L.Mitchell, S.E.Mitreska, B.Mitzel, D.S.Mödden, A.Mohammed, R.A.Moise, R.D.Mombächer, T.Monroy, I.A.Monteil, S.Morandin, M.Morello, G.Morello, M.J.Moron, J.Morris, A.B.Morris, A.G.Mountain, R.Mu, H.Muheim, F.Mulder, M.Müller, D.Müller, K.Murphy, C.H.Murray, D.Muzzetto, P.Naik, P.Nakada, T.Nandakumar, R.Nanut, T.Nasteva, I.Needham, M.Neri, I.Neri, N.Neubert, S.Neufeld, N.Newcombe, R.Nguyen, T.D.Nguyen-Mau, C.Niel, E.M.Nieswand, S.Nikitin, N.Nolte, N.S.Nunez, C.Oblakowska-Mucha, A.Obraztsov, V.O'Hanlon, D.P.Oldeman, R.Olivares, M.E.Onderwater, C.J. G.Ossowska, A.Goicochea, J.M. OtaloraOvsiannikova, T.Owen, P.Oyanguren, A.Pagare, B.Pais, P.R.Pajero, T.Palano, A.Palutan, M.Pan, Y.Panshin, G.Papanestis, A.Pappagallo, M.Pappalardo, L.L.Pappenheimer, C.Parker, W.Parkes, C.Parkinson, C.J.Passalacqua, B.Passaleva, G.Pastore, A.Patel, M.Patrignani, C.Pawley, C.J.Pearce, A.Pellegrino, A.Altarelli, M. PepePerazzini, S.Pereima, D.Perret, P.Petric, M.Petridis, K.Petrolini, A.Petrov, A.Petrucci, S.Petruzzo, M.Pham, T.T.H.Philippov, A.Pica, L.Piccini, M.Pietrzyk, B.Pietrzyk, G.Pili, M.Pinci, D.Pisani, F.Resmi, P.K.Placinta, V.Plews, J.Casasus, M. PloPolci, F.Lener, M. PoliPoliakova, M.Poluektov, A.Polukhina, N.Polyakov, I.Polycarpo, E.Pomery, G.J.Ponce, S.Popov, D.Popov, S.Poslavskii, S.Prasanth, K.Promberger, L.Prouve, C.Pugatch, V.Pullen, H.Punzi, G.Qian, W.Qin, J.Quagliani, R.Quintana, B.Raab, N.V.Trejo, R.I. RabadanRachwal, B.Rademacker, J.H.Rama, M.Pernas, M. RamosRangel, M.S.Ratnikov, F.Raven, G.Reboud, M.Redi, F.Reiss, F.Alepuz, C. RemonRen, Z.Renaudin, V.Ribatti, R.Ricciardi, S.Rinnert, K.Robbe, P.Robertson, G.Rodrigues, A.B.Rodrigues, E.Lopez, J.A. RodriguezRollings, A.Roloff, P.Romanovskiy, V.Lamas, M. RomeroVidal, A. RomeroRoth, J.D.Rotondo, M.Rudolph, M.S.Ruf, T.Vidal, J. RuizRyzhikov, A.Ryzka, J.Silva, J.J. SaboridoSagidova, N.Sahoo, N.Saitta, B.Salomoni, M.Gonzalo, D. SanchezGras, C. SanchezSantacesaria, R.Rios, C. SantamarinaSantimaria, M.Santovetti, E.Saranin, D.Sarpis, G.Sarpis, M.Sarti, A.Satriano, C.Satta, A.Saur, M.Savrina, D.Sazak, H.Smead, L.G. ScantleburySchael, S.Schellenberg, M.Schiller, M.Schindler, H.Schmelling, M.Schmidt, B.Schneider, O.Schopper, A.Schubiger, M.Schulte, S.Schune, M.H.Schwemmer, R.Sciascia, B.Sellam, S.Semennikov, A.Senghi Soares, MaraSergi, A.Serra, N.Sestini, L.Seuthe, A.Seyfert, P.Shang, Y.Shangase, D.M.Shapkin, M.Shchemerov, I.Shchutska, L.Shears, T.Shekhtman, L.Shen, Z.Shevchenko, V.Shields, E.B.Shmanin, E.Shupperd, J.D.Siddi, B.G.Coutinho, R. SilvaSimi, G.Simone, S.Skidmore, N.Skwarnicki, T.Slater, M.W.Slazyk, I.Smallwood, J.C.Smeaton, J.G.Smetkina, A.Smith, E.Smith, M.Snoch, A.Soares, MarceloLavra, L. SoaresSokoloff, M.D.Soler, F.J. P.Solovev, A.Solovyev, I.De Almeida, F.L. SouzaDe Paula, B. SouzaSpaan, B.Norella, E. SpadaroSpradlin, P.Stagni, F.Stahl, M.Stahl, S.Stefko, P.Steinkamp, O.Stenyakin, O.Stevens, H.Stone, S.Stramaglia, M.E.Straticiuc, M.Strekalina, D.Suljik, F.Sun, J.Sun, L.Sun, Y.Svihra, P.Swallow, P.N.Swientek, K.Szabelski, A.Szumlak, T.Szymanski, M.Taneja, S.Teubert, F.Thomas, E.Thomson, K.A.Tisserand, V.T'Jampens, S.Tobin, M.Tomassetti, L.Machado, D. TorresTou, D.Y.Tran, M.T.Trifonova, E.Trippl, C.Tuci, G.Tully, A.Tuning, N.Ukleja, A.Unverzagt, D.J.Ursov, E.Usachov, A.Ustyuzhanin, A.Uwer, U.Vagner, A.Vagnoni, V.Valassi, A.Valenti, G.Canudas, N. Vallsvan Beuzekom, M.Van Dijk, M.van Herwijnen, E.Van Hulse, C.B.van Veghel, M.Gomez, R. VazquezRegueiro, P. VazquezSierra, C. VázquezVecchi, S.Velthuis, J.J.Veltri, M.Venkateswaran, A.Veronesi, M.Vesterinen, M.Vieira, D.Diaz, M. VieitesViemann, H.Vilasis-Cardona, X.Figueras, E. VilellaVincent, P.Bruch, D. VomVorobyev, A.Vorobyev, V.Voropaev, N.Waldi, R.Walsh, J.Wang, C.Wang, JialuWang, JianchunWang, JianqiaoWang, JikeWang, M.Wang, R.Wang, Y.Wang, ZhenziWang, ZiruiWark, H.M.Watson, N.K.Weber, S.G.Websdale, D.Weisser, C.Westhenry, B.D.C.White, D.J.Whitehead, M.Wiedner, D.Wilkinson, G.Wilkinson, M.Williams, I.Williams, MikeWilliams, Mark Richard JamesWilson, F.F.Wislicki, W.Witek, M.Witola, L.Wormser, G.Wotton, S.A.Wu, H.Wyllie, K.Xiang, Z.Xiao, D.Xie, Y.Xu, A.Xu, J.Xu, L.Xu, M.Xu, Q.Xu, ZehuaXu, ZhihaoYang, D.Yang, S.Yang, Y.Yang, ZhenweiYang, ZishuoYao, Y.Yeomans, L.E.Yin, H.Yu, J.Yuan, X.Yushchenko, O.Zaffaroni, E.Zavertyaev, M.Zdybal, M.Zenaiev, O.Zeng, M.Zhang, D.Zhang, L.Zhang, S.Zhang, YanxiZhang, YuZhelezov, A.Zheng, Y.Zhou, X.Zhou, Y.Zhu, X.Zhu, Z.Zhukov, V.Zonneveld, J.B.Zou, Q.Zucchelli, S.Zuliani, D.Zunica, G.Precise determination of the $B_{\mathrm{s}}^0$–$\overline B_{\mathrm{s}}^0$ oscillation frequencyhep-exParticle Physics - ExperimentMesons comprising a beauty quark and a strange quark can oscillate between particle ($B^0_s$) and antiparticle ($\overline{B}^0_s$) flavour eigenstates, with a frequency given by the mass difference between heavy and light mass eigenstates, $\Delta m_{s}$. Here we present a measurement of $\Delta m_{s}$ using $B^0_s \rightarrow D_s^- \pi^+$ decays produced in proton-proton collisions collected with the LHCb detector at the Large Hadron Collider. This measurement improves upon the current $\Delta m_{s}$ precision by a factor of two. The oscillation frequency is found to be $\Delta m_{s}$ = 17.7683 $\pm$ 0.0051 $\pm$ 0.0032 ps$^{-1}$, where the first uncertainty is statistical and the second systematic. We combine this result with previous LHCb measurements to determine $\Delta m_{s}$ = 17.7656 $\pm$ 0.0057 ps$^{-1}$. Mesons comprising a beauty quark and a strange quark can oscillate between particle (B0s) and antiparticle (B0sbar) flavour eigenstates, with a frequency given by the mass difference between heavy and light mass eigenstates, deltams. Here we present a measurement of deltams using B0s2DsPi decays produced in proton-proton collisions collected with the LHCb detector at the Large Hadron Collider. This measurement improves upon the current deltams precision by a factor of two. The oscillation frequency is found to be deltams = 17.7683 +- 0.0051 +- 0.0032 ps-1 where the first uncertainty is statistical and the second systematic. We combine this result with previous LHCb measurements to determine deltams = 17.7656 +- 0.0057 ps-1. Mesons comprising a beauty quark and a strange quark can oscillate between particle (B0s) and antiparticle (B0sbar) flavour eigenstates, with a frequency given by the mass difference between heavy and light mass eigenstates, deltams. Here we present a measurement of deltams using B0s2DsPi decays produced in proton-proton collisions collected with the LHCb detector at the Large Hadron Collider. This measurement improves upon the current deltams precision by a factor of two. The oscillation frequency is found to be deltams = 17.7683 +- 0.0051 +- 0.0032 ps-1 where the first uncertainty is statistical and the second systematic. We combine this result with previous LHCb measurements to determine deltams = 17.7656 +- 0.0057 ps-1. Mesons comprising a beauty quark and a strange quark can oscillate between particle (B0s) and antiparticle (B0sbar) flavour eigenstates, with a frequency given by the mass difference between heavy and light mass eigenstates, deltams. Here we present a measurement of deltams using B0s2DsPi decays produced in proton-proton collisions collected with the LHCb detector at the Large Hadron Collider. This measurement improves upon the current deltams precision by a factor of two. The oscillation frequency is found to be deltams = 17.7683 +- 0.0051 +- 0.0032 ps-1 where the first uncertainty is statistical and the second systematic. We combine this result with previous LHCb measurements to determine deltams = 17.7656 +- 0.0057 ps-1. Mesons comprising a beauty quark and a strange quark can oscillate between particle (B0s) and antiparticle (B0sbar) flavour eigenstates, with a frequency given by the mass difference between heavy and light mass eigenstates, deltams. Here we present a measurement of deltams using B0s2DsPi decays produced in proton-proton collisions collected with the LHCb detector at the Large Hadron Collider. This measurement improves upon the current deltams precision by a factor of two. The oscillation frequency is found to be deltams = 17.7683 +- 0.0051 +- 0.0032 ps-1 where the first uncertainty is statistical and the second systematic. We combine this result with previous LHCb measurements to determine deltams = 17.7656 +- 0.0057 ps-1. Mesons comprising a beauty quark and a strange quark can oscillate between particle (B0s) and antiparticle (B0sbar) flavour eigenstates, with a frequency given by the mass difference between heavy and light mass eigenstates, deltams. Here we present a measurement of deltams using B0s2DsPi decays produced in proton-proton collisions collected with the LHCb detector at the Large Hadron Collider. This measurement improves upon the current deltams precision by a factor of two. The oscillation frequency is found to be deltams = 17.7683 +- 0.0051 +- 0.0032 ps-1 where the first uncertainty is statistical and the second systematic. We combine this result with previous LHCb measurements to determine deltams = 17.7656 +- 0.0057 ps-1. Mesons comprising a beauty quark and a strange quark can oscillate between particle (B0s) and antiparticle (B0sbar) flavour eigenstates, with a frequency given by the mass difference between heavy and light mass eigenstates, deltams. Here we present a measurement of deltams using B0s2DsPi decays produced in proton-proton collisions collected with the LHCb detector at the Large Hadron Collider. This measurement improves upon the current deltams precision by a factor of two. The oscillation frequency is found to be deltams = 17.7683 +- 0.0051 +- 0.0032 ps-1 where the first uncertainty is statistical and the second systematic. We combine this result with previous LHCb measurements to determine deltams = 17.7656 +- 0.0057 ps-1. Mesons comprising a beauty quark and a strange quark can oscillate between particle (B0s) and antiparticle (B0sbar) flavour eigenstates, with a frequency given by the mass difference between heavy and light mass eigenstates, deltams. Here we present a measurement of deltams using B0s2DsPi decays produced in proton-proton collisions collected with the LHCb detector at the Large Hadron Collider. This measurement improves upon the current deltams precision by a factor of two. The oscillation frequency is found to be deltams = 17.7683 +- 0.0051 +- 0.0032 ps-1 where the first uncertainty is statistical and the second systematic. We combine this result with previous LHCb measurements to determine deltams = 17.7656 +- 0.0057 ps-1. Mesons comprising a beauty quark and a strange quark can oscillate between particle (B0s) and antiparticle (B0sbar) flavour eigenstates, with a frequency given by the mass difference between heavy and light mass eigenstates, deltams. Here we present a measurement of deltams using B0s2DsPi decays produced in proton-proton collisions collected with the LHCb detector at the Large Hadron Collider. This measurement improves upon the current deltams precision by a factor of two. The oscillation frequency is found to be deltams = 17.7683 +- 0.0051 +- 0.0032 ps-1 where the first uncertainty is statistical and the second systematic. We combine this result with previous LHCb measurements to determine deltams = 17.7656 +- 0.0057 ps-1. Mesons comprising a beauty quark and a strange quark can oscillate between particle (B0s) and antiparticle (B0sbar) flavour eigenstates, with a frequency given by the mass difference between heavy and light mass eigenstates, deltams. Here we present a measurement of deltams using B0s2DsPi decays produced in proton-proton collisions collected with the LHCb detector at the Large Hadron Collider. This measurement improves upon the current deltams precision by a factor of two. The oscillation frequency is found to be deltams = 17.7683 +- 0.0051 +- 0.0032 ps-1 where the first uncertainty is statistical and the second systematic. We combine this result with previous LHCb measurements to determine deltams = 17.7656 +- 0.0057 ps-1. Mesons comprising a beauty quark and a strange quark can oscillate between particle (B0s) and antiparticle (B0sbar) flavour eigenstates, with a frequency given by the mass difference between heavy and light mass eigenstates, deltams. Here we present a measurement of deltams using B0s2DsPi decays produced in proton-proton collisions collected with the LHCb detector at the Large Hadron Collider. This measurement improves upon the current deltams precision by a factor of two. The oscillation frequency is found to be deltams = 17.7683 +- 0.0051 +- 0.0032 ps-1 where the first uncertainty is statistical and the second systematic. We combine this result with previous LHCb measurements to determine deltams = 17.7656 +- 0.0057 ps-1. Mesons comprising a beauty quark and a strange quark can oscillate between particle (B0s) and antiparticle (B0sbar) flavour eigenstates, with a frequency given by the mass difference between heavy and light mass eigenstates, deltams. Here we present a measurement of deltams using B0s2DsPi decays produced in proton-proton collisions collected with the LHCb detector at the Large Hadron Collider. This measurement improves upon the current deltams precision by a factor of two. The oscillation frequency is found to be deltams = 17.7683 +- 0.0051 +- 0.0032 ps-1 where the first uncertainty is statistical and the second systematic. We combine this result with previous LHCb measurements to determine deltams = 17.7656 +- 0.0057 ps-1. Mesons comprising a beauty quark and a strange quark can oscillate between particle (B0s) and antiparticle (B0sbar) flavour eigenstates, with a frequency given by the mass difference between heavy and light mass eigenstates, deltams. Here we present a measurement of deltams using B0s2DsPi decays produced in proton-proton collisions collected with the LHCb detector at the Large Hadron Collider. This measurement improves upon the current deltams precision by a factor of two. The oscillation frequency is found to be deltams = 17.7683 +- 0.0051 +- 0.0032 ps-1 where the first uncertainty is statistical and the second systematic. We combine this result with previous LHCb measurements to determine deltams = 17.7656 +- 0.0057 ps-1. Mesons comprising a beauty quark and a strange quark can oscillate between particle (B0s) and antiparticle (B0sbar) flavour eigenstates, with a frequency given by the mass difference between heavy and light mass eigenstates, deltams. Here we present a measurement of deltams using B0s2DsPi decays produced in proton-proton collisions collected with the LHCb detector at the Large Hadron Collider. This measurement improves upon the current deltams precision by a factor of two. The oscillation frequency is found to be deltams = 17.7683 +- 0.0051 +- 0.0032 ps-1 where the first uncertainty is statistical and the second systematic. We combine this result with previous LHCb measurements to determine deltams = 17.7656 +- 0.0057 ps-1. Mesons comprising a beauty quark and a strange quark can oscillate between particle (B0s) and antiparticle (B0sbar) flavour eigenstates, with a frequency given by the mass difference between heavy and light mass eigenstates, deltams. Here we present a measurement of deltams using B0s2DsPi decays produced in proton-proton collisions collected with the LHCb detector at the Large Hadron Collider. This measurement improves upon the current deltams precision by a factor of two. The oscillation frequency is found to be deltams = 17.7683 +- 0.0051 +- 0.0032 ps-1 where the first uncertainty is statistical and the second systematic. We combine this result with previous LHCb measurements to determine deltams = 17.7656 +- 0.0057 ps-1. Mesons comprising a beauty quark and a strange quark can oscillate between particle (B0s) and antiparticle (B0sbar) flavour eigenstates, with a frequency given by the mass difference between heavy and light mass eigenstates, deltams. Here we present a measurement of deltams using B0s2DsPi decays produced in proton-proton collisions collected with the LHCb detector at the Large Hadron Collider. This measurement improves upon the current deltams precision by a factor of two. The oscillation frequency is found to be deltams = 17.7683 +- 0.0051 +- 0.0032 ps-1 where the first uncertainty is statistical and the second systematic. We combine this result with previous LHCb measurements to determine deltams = 17.7656 +- 0.0057 ps-1. Mesons comprising a beauty quark and a strange quark can oscillate between particle (B0s) and antiparticle (B0sbar) flavour eigenstates, with a frequency given by the mass difference between heavy and light mass eigenstates, deltams. Here we present a measurement of deltams using B0s2DsPi decays produced in proton-proton collisions collected with the LHCb detector at the Large Hadron Collider. This measurement improves upon the current deltams precision by a factor of two. The oscillation frequency is found to be deltams = 17.7683 +- 0.0051 +- 0.0032 ps-1 where the first uncertainty is statistical and the second systematic. We combine this result with previous LHCb measurements to determine deltams = 17.7656 +- 0.0057 ps-1. Mesons comprising a beauty quark and a strange quark can oscillate between particle (B0s) and antiparticle (B0sbar) flavour eigenstates, with a frequency given by the mass difference between heavy and light mass eigenstates, deltams. Here we present a measurement of deltams using B0s2DsPi decays produced in proton-proton collisions collected with the LHCb detector at the Large Hadron Collider. This measurement improves upon the current deltams precision by a factor of two. The oscillation frequency is found to be deltams = 17.7683 +- 0.0051 +- 0.0032 ps-1 where the first uncertainty is statistical and the second systematic. We combine this result with previous LHCb measurements to determine deltams = 17.7656 +- 0.0057 ps-1. Mesons comprising a beauty quark and a strange quark can oscillate between particle (B0s) and antiparticle (B0sbar) flavour eigenstates, with a frequency given by the mass difference between heavy and light mass eigenstates, deltams. Here we present a measurement of deltams using B0s2DsPi decays produced in proton-proton collisions collected with the LHCb detector at the Large Hadron Collider. This measurement improves upon the current deltams precision by a factor of two. The oscillation frequency is found to be deltams = 17.7683 +- 0.0051 +- 0.0032 ps-1 where the first uncertainty is statistical and the second systematic. We combine this result with previous LHCb measurements to determine deltams = 17.7656 +- 0.0057 ps-1. Mesons comprising a beauty quark and a strange quark can oscillate between particle (B0s) and antiparticle (B0sbar) flavour eigenstates, with a frequency given by the mass difference between heavy and light mass eigenstates, deltams. Here we present a measurement of deltams using B0s2DsPi decays produced in proton-proton collisions collected with the LHCb detector at the Large Hadron Collider. This measurement improves upon the current deltams precision by a factor of two. The oscillation frequency is found to be deltams = 17.7683 +- 0.0051 +- 0.0032 ps-1 where the first uncertainty is statistical and the second systematic. We combine this result with previous LHCb measurements to determine deltams = 17.7656 +- 0.0057 ps-1. Mesons comprising a beauty quark and a strange quark can oscillate between particle (B0s) and antiparticle (B0sbar) flavour eigenstates, with a frequency given by the mass difference between heavy and light mass eigenstates, deltams. Here we present a measurement of deltams using B0s2DsPi decays produced in proton-proton collisions collected with the LHCb detector at the Large Hadron Collider. This measurement improves upon the current deltams precision by a factor of two. The oscillation frequency is found to be deltams = 17.7683 +- 0.0051 +- 0.0032 ps-1 where the first uncertainty is statistical and the second systematic. We combine this result with previous LHCb measurements to determine deltams = 17.7656 +- 0.0057 ps-1. Mesons comprising a beauty quark and a strange quark can oscillate between particle (B0s) and antiparticle (B0sbar) flavour eigenstates, with a frequency given by the mass difference between heavy and light mass eigenstates, deltams. Here we present a measurement of deltams using B0s2DsPi decays produced in proton-proton collisions collected with the LHCb detector at the Large Hadron Collider. This measurement improves upon the current deltams precision by a factor of two. The oscillation frequency is found to be deltams = 17.7683 +- 0.0051 +- 0.0032 ps-1 where the first uncertainty is statistical and the second systematic. We combine this result with previous LHCb measurements to determine deltams = 17.7656 +- 0.0057 ps-1. Mesons comprising a beauty quark and a strange quark can oscillate between particle (B0s) and antiparticle (B0sbar) flavour eigenstates, with a frequency given by the mass difference between heavy and light mass eigenstates, deltams. Here we present a measurement of deltams using B0s2DsPi decays produced in proton-proton collisions collected with the LHCb detector at the Large Hadron Collider. This measurement improves upon the current deltams precision by a factor of two. The oscillation frequency is found to be deltams = 17.7683 +- 0.0051 +- 0.0032 ps-1 where the first uncertainty is statistical and the second systematic. We combine this result with previous LHCb measurements to determine deltams = 17.7656 +- 0.0057 ps-1. Mesons comprising a beauty quark and a strange quark can oscillate between particle (B0s) and antiparticle (B0sbar) flavour eigenstates, with a frequency given by the mass difference between heavy and light mass eigenstates, deltams. Here we present a measurement of deltams using B0s2DsPi decays produced in proton-proton collisions collected with the LHCb detector at the Large Hadron Collider. This measurement improves upon the current deltams precision by a factor of two. The oscillation frequency is found to be deltams = 17.7683 +- 0.0051 +- 0.0032 ps-1 where the first uncertainty is statistical and the second systematic. We combine this result with previous LHCb measurements to determine deltams = 17.7656 +- 0.0057 ps-1. Mesons comprising a beauty quark and a strange quark can oscillate between particle (B0s) and antiparticle (B0sbar) flavour eigenstates, with a frequency given by the mass difference between heavy and light mass eigenstates, deltams. Here we present a measurement of deltams using B0s2DsPi decays produced in proton-proton collisions collected with the LHCb detector at the Large Hadron Collider. This measurement improves upon the current deltams precision by a factor of two. The oscillation frequency is found to be deltams = 17.7683 +- 0.0051 +- 0.0032 ps-1 where the first uncertainty is statistical and the second systematic. We combine this result with previous LHCb measurements to determine deltams = 17.7656 +- 0.0057 ps-1. Mesons comprising a beauty quark and a strange quark can oscillate between particle (B0s) and antiparticle (B0sbar) flavour eigenstates, with a frequency given by the mass difference between heavy and light mass eigenstates, deltams. Here we present a measurement of deltams using B0s2DsPi decays produced in proton-proton collisions collected with the LHCb detector at the Large Hadron Collider. This measurement improves upon the current deltams precision by a factor of two. The oscillation frequency is found to be deltams = 17.7683 +- 0.0051 +- 0.0032 ps-1 where the first uncertainty is statistical and the second systematic. We combine this result with previous LHCb measurements to determine deltams = 17.7656 +- 0.0057 ps-1. Mesons comprising a beauty quark and a strange quark can oscillate between particle (B0s) and antiparticle (B0sbar) flavour eigenstates, with a frequency given by the mass difference between heavy and light mass eigenstates, deltams. Here we present a measurement of deltams using B0s2DsPi decays produced in proton-proton collisions collected with the LHCb detector at the Large Hadron Collider. This measurement improves upon the current deltams precision by a factor of two. The oscillation frequency is found to be deltams = 17.7683 +- 0.0051 +- 0.0032 ps-1 where the first uncertainty is statistical and the second systematic. We combine this result with previous LHCb measurements to determine deltams = 17.7656 +- 0.0057 ps-1. Mesons comprising a beauty quark and a strange quark can oscillate between particle (B0s) and antiparticle (B0sbar) flavour eigenstates, with a frequency given by the mass difference between heavy and light mass eigenstates, deltams. Here we present a measurement of deltams using B0s2DsPi decays produced in proton-proton collisions collected with the LHCb detector at the Large Hadron Collider. This measurement improves upon the current deltams precision by a factor of two. The oscillation frequency is found to be deltams = 17.7683 +- 0.0051 +- 0.0032 ps-1 where the first uncertainty is statistical and the second systematic. We combine this result with previous LHCb measurements to determine deltams = 17.7656 +- 0.0057 ps-1. Mesons comprising a beauty quark and a strange quark can oscillate between particle (B0s) and antiparticle (B0sbar) flavour eigenstates, with a frequency given by the mass difference between heavy and light mass eigenstates, deltams. Here we present a measurement of deltams using B0s2DsPi decays produced in proton-proton collisions collected with the LHCb detector at the Large Hadron Collider. This measurement improves upon the current deltams precision by a factor of two. The oscillation frequency is found to be deltams = 17.7683 +- 0.0051 +- 0.0032 ps-1 where the first uncertainty is statistical and the second systematic. We combine this result with previous LHCb measurements to determine deltams = 17.7656 +- 0.0057 ps-1.The LHCb collaboration reports an improved measurement of the oscillation frequency of mesons consisting of a bottom quark and strange quark, which is then combined with previous results. Mesons comprising a beauty quark and a strange quark can oscillate between particle (B0s) and antiparticle (B0sbar) flavour eigenstates, with a frequency given by the mass difference between heavy and light mass eigenstates, deltams. Here we present a measurement of deltams using B0s2DsPi decays produced in proton-proton collisions collected with the LHCb detector at the Large Hadron Collider. This measurement improves upon the current deltams precision by a factor of two. The oscillation frequency is found to be deltams = 17.7683 +- 0.0051 +- 0.0032 ps-1 where the first uncertainty is statistical and the second systematic. We combine this result with previous LHCb measurements to determine deltams = 17.7656 +- 0.0057 ps-1.Mesons comprising a beauty quark and a strange quark can oscillate between particle (B0s) and antiparticle (B0s) flavour eigenstates, with a frequency given by the mass difference between heavy and light mass eigenstates, deltams. Here we present ameasurement of deltams using B0s2DsPi decays produced in proton-proton collisions collected with the LHCb detector at the Large Hadron Collider. The oscillation frequency is found to be deltams = 17.7683 +- 0.0051 +- 0.0032 ps-1, where the first uncertainty is statistical and the second systematic. This measurement improves upon the current deltams precision by a factor of two. We combine this result with previous LHCb measurements to determine deltams = 17.7656 +- 0.0057 ps-1, which is the legacy measurement of the original LHCb detector.arXiv:2104.04421LHCb-PAPER-2021-005CERN-EP-2021-047LHCB-PAPER-2021-005oai:cds.cern.ch:27643382021-04-15
spellingShingle hep-ex
Particle Physics - Experiment
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Raab, N.V.
Trejo, R.I. Rabadan
Rachwal, B.
Rademacker, J.H.
Rama, M.
Pernas, M. Ramos
Rangel, M.S.
Ratnikov, F.
Raven, G.
Reboud, M.
Redi, F.
Reiss, F.
Alepuz, C. Remon
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Precise determination of the $B_{\mathrm{s}}^0$–$\overline B_{\mathrm{s}}^0$ oscillation frequency
title Precise determination of the $B_{\mathrm{s}}^0$–$\overline B_{\mathrm{s}}^0$ oscillation frequency
title_full Precise determination of the $B_{\mathrm{s}}^0$–$\overline B_{\mathrm{s}}^0$ oscillation frequency
title_fullStr Precise determination of the $B_{\mathrm{s}}^0$–$\overline B_{\mathrm{s}}^0$ oscillation frequency
title_full_unstemmed Precise determination of the $B_{\mathrm{s}}^0$–$\overline B_{\mathrm{s}}^0$ oscillation frequency
title_short Precise determination of the $B_{\mathrm{s}}^0$–$\overline B_{\mathrm{s}}^0$ oscillation frequency
title_sort precise determination of the $b_{\mathrm{s}}^0$–$\overline b_{\mathrm{s}}^0$ oscillation frequency
topic hep-ex
Particle Physics - Experiment
url https://dx.doi.org/10.1038/s41567-021-01394-x
http://cds.cern.ch/record/2764338
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