Observation of J / Structures Consistent with Exotic States from Amplitude Analysis of B+ j /K+ Decays
暂无分享,去创建一个
I. Babuschkin | F. Fleuret | F. Bedeschi | M. Beuzekom | C. Frei | E. Cogneras | T. Bowcock | D. Derkach | J. Brodzicka | T. Gershon | M. Corvo | C. Gaspar | V. Gligorov | P. Billoir | V. Bocci | W. Bonivento | M. Calvi | P. Charpentier | H. Dijkstra | F. Fontanelli | J. Cogan | G. Alkhazov | S. Eidelman | D. Decamp | P. Ghez | Z. Ajaltouni | S. Cadeddu | E. Grauges | C. Bozzi | M. Chefdeville | L. Garrido | G. Bencivenni | P. Campana | M. Cattaneo | E. Ben-Haim | G. Auriemma | T. Fiutowski | A. Grecu | G. Cowan | M. Chrzaszcz | S. Cunliffe | C. Elsasser | F. Blanc | G. Casse | A. Bizzeti | G. Collazuol | I. Belyaev | S. Easo | G. Corti | S. Akar | J. Albrecht | Federico Alessio | M. Alexander | S. Ali | Y. Amhis | L. Anderlini | G. Andreassi | F. Archilli | M. Artuso | E. Aslanides | S. Bachmann | W. Baldini | R. Barlow | S. Barsuk | W. Barter | V. Batozskaya | B. Batsukh | V. Battista | J. Beddow | I. Bediaga | N. Belloli | S. Benson | A. Berezhnoy | R. Bernet | F. Betti | I. Bezshyiko | S. Bifani | A. Birnkraut | T. Blake | S. Blusk | T. Boettcher | M. Borisyak | M. Borsato | F. Bossù | M. Boubdir | E. Buchanan | C. Burr | A. Bursche | R. Calabrese | L. Capriotti | A. Carbone | R. Cardinale | A. Cardini | P. Carniti | L. Cassina | G. Cavallero | R. Cenci | G. Chatzikonstantinidis | S. Chen | V. Chobanova | G. Ciezarek | M. Clemencic | J. Closier | V. Coco | L. Cojocariu | S. Coquereau | B. Couturier | D. Craik | A. Crocombe | R. Currie | M. Cian | J. Miranda | M. Serio | P. Simone | M. Demmer | O. Deschamps | F. Dettori | B. Dey | A. Canto | F. Dordei | A. Dovbnya | K. Dreimanis | G. Dujany | P. Durante | R. Dzhelyadin | A. Dziurda | A. Dzyuba | V. Egorychev | S. Eisenhardt | U. Eitschberger | R. Ekelhof | L. Eklund | S. Ely | S. Esen | T. Evans | A. Falabella | N. Farley | S. Farry | D. Fazzini | M. Ferro-Luzzi | S. Filippov | M. Fiorini | M. Firlej | F. Fleuret | S. Gallorini | S. Gambetta | M. Gandelman | P. Gandini | L. Gavardi | G. Gazzoni | D. Gerick | E. Gersabeck | M. Gersabeck | V. Gibson | L. Giubega | K. Gizdov | A. Golutvin | A. Gomes | C. Gotti | E. Graverini | G. Graziani | P. Griffith | L. Grillo | T. Hadavizadeh | L. Henry | S. Amato | S. Gianì | C. Fitzpatrick | K. Akiba | L. Paula | F. Rodrigues | L. Buono | J. Blouw | G. Carboni | X. Vidal | A. Torreira | V. Gligorov | A. Gomes | L. Beaucourt | M. Baalouch | C. Cauet | M. Deckenhoff | M. Britsch | V. Cogoni | M. Fiore | E. Furfaro | A. Badalov | M. C. Gomez | R. Diaz | P. Cartelle | V. Albor | J. Pardiñas | C. Barschel | D. Perez | L. Cardoso | M. Dorigo | E. Bowen | K. Bruyn | J. Benton | A. Cook | H. Evans | T. Bird | S. Capua | T. Britton | C. Baesso | O. Gutierrez | A. G. Torreira | J. G. Ticó | O. Francisco | L. Henry | R. Fay | A. Borgheresi | P. Garsed | F. Ferrari | K. Dungs | N. Déléage | A. Suárez | A. Bitadze | A. Bertolin | Sergey Filippov | A. Artamonov | A. Bondar | M. Gándara | E. Dall | Occo | F. Blanc | V. Gibson | C. Bozzi | C. Sobral | R. Barlow | S. Braun | C. Hadjivasiliou | N. Harnew | J. Buytaert | A. Davis | Y. Gao | J. Romeu | L. García | S. Eidelman | N. Bondar | F. Bossu | K. Dungs | D. Gascón | V. Bellee | J. Dalseno | D. Galli | D. Golubkov | A. Bitadze | T. Gershon | P. Ghez | G. Bencivenni | J. Miranda | J. G. Pardiñas | O. A. Gutierrez | E. Ben-Haim | R. Bernet | T. Blake | E. Bowen | R. Calabrese | G. Carboni | J. Cogan | D. Derkach | N. Farley | M. Fiore | D. Galli | C. Gaspar | E. Graugés | L. Grillo | Y. Gao | G. Auriemma | H. Dijkstra | A. Dovbnya | F. Ferrari | M. Borsato | S. Cunliffe | P. Garsed | J. Beddow | A. Borgheresi | A. D. Suárez | A. Falabella | F. Fontanelli | M. G. Gándara
[1] M. Kelsey,et al. Amplitude Analysis of B^{±}→π^{±}K^{+}K^{-} Decays. , 2019, Physical review letters.
[2] M. Karliner,et al. Exotic resonances due to η exchange , 2016, 1601.00565.
[3] A. Sarantsev,et al. Exotic mesons with hidden charm as diquark–antidiquark states , 2015, 1507.07232.
[4] C. Lang,et al. X (3872 ) and Y (4140 ) using diquark-antidiquark operators with lattice QCD , 2015, 1503.03257.
[5] M. Dorigo,et al. LHCb detector performance , 2014, 1412.6352.
[6] E. Swanson. Z b and Z c exotic states as coupled channel cusps , 2014, 1409.3291.
[7] S. Miglioranzi,et al. The LHCb Simulation Application, Gauss: Design, Evolution and Experience , 2011 .
[8] H. K. Wöhri,et al. Heavy quarkonium: progress, puzzles, and opportunities , 2010, 1010.5827.
[9] P. Harrison,et al. Handling of the generation of primary events in Gauss, the LHCb simulation framework , 2010, IEEE Nuclear Science Symposuim & Medical Imaging Conference.
[10] Chengping Shen,et al. XYZ particles at Belle , 2009, 0912.2386.
[11] Zhi-Gang wang,et al. Analysis of the Y(4140) and related molecular states with QCD sum rules , 2009, 0907.1467.
[12] Xiang Liu. The hidden charm decay of Y (4140) by the rescattering mechanism , 2009, 0904.0136.
[13] M. Nielsen,et al. A QCD sum rule calculation for the Y(4140) narrow structure , 2009, 0903.5540.
[14] T. Gutsche,et al. Hadronic molecule structure of the Y(3940) and Y(4140) , 2009, 0903.5424.
[15] Zhi-Gang wang. Analysis of the Y(4140) with QCD sum rules , 2009, 0903.5200.
[16] N. Mahajan. Y(4140): Possible options , 2009, 0903.3107.
[17] Xiang Liu,et al. Y(4143) is probably a molecular partner of Y(3930) , 2009, 0903.2529.
[18] R. Faccini,et al. Exotic hadrons with hidden charm and strangeness , 2009, 0902.2803.
[19] Chris P. Barnes,et al. The LHCb detector at the LHC , 2008 .
[20] Jae Hyun Kim,et al. Experimental constraints on the spin and parity of the Z(4430) , 2007, 1306.4894.
[21] S. Mrenna,et al. Pythia 6.3 physics and manual , 2003, hep-ph/0308153.
[22] Godfrey,et al. Mesons in a relativized quark model with chromodynamics. , 1986, Physical review. D, Particles and fields.
[23] P. W. Minto,et al. A spin-parity analysis of the φK+ system produced in the reaction K+p → φK+p, φ → K+K− at 13 GeV / c , 1986 .
[24] J. Richman. An Experimenter's Guide to the Helicity Formalism , 1984 .
[25] G. C. Wick,et al. On the general theory of collisions for particles with spin , 1959 .
[26] R. Quagliani. The LHCb Detector at the LHC , 2018 .
[27] R. Lebed. ð 3915 Þ as the lightest cc̄ss̄ state , 2016 .
[28] U. Bassler,et al. Inclusive Production of the Xð4140Þ State in p¯ p Collisions at D0 , 2015 .
[29] A. Korytov,et al. Observation of a peaking structure in the J /ψφ mass spectrum from B ± → J /ψφ K ± decays , 2014 .
[30] G. Busetto,et al. Observation of the Resonant Character of the Zð4430Þ− State , 2014 .
[31] F. Stancu. Can Y(4140) be a cc̄ss̄ tetraquark , 2010 .
[32] J. Brodzicka. Heavy Flavour Spectroscopy , 2009 .
[33] P. Barria,et al. Evidence for a Narrow Near-Threshold Structure in the J/ψφ Mass Spectrum in B + → J/ψφK + Decays , 2009 .
[34] Particle Data Group. Review of Particle Physics , 1998 .
[35] S. U. Chung,et al. General formulation of covariant helicity-coupling amplitudes , 1998 .
[36] Youngjoon Kwon. Strange meson spectroscopy in Kω and KΦ at 11 GeV/c and Cherenkov ring imaging at SLD , 1993 .
[37] Edinburgh Research Explorer Search for the X(4140) state in B+J/K+ decays with the D0 detector , 2022 .