Observation of Overlapping Spin-1 and Spin-3<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:mrow><mml:msup><mml:mrow><mml:mover accent="true"><mml:mrow><mml:mi>D</mml:mi></mml:mrow><mml:mrow><mml:mo accent="true" stretchy="false">¯</mml:mo></mml:mrow></mml:mover></mml:mrow><mml:mrow><mml:mn>0</mml:mn></mml:mrow></mml:msup><mml:msup><mml:mrow><mml:mi>K</mml:mi></mml:mrow><mml:mrow><mml:mo>−</mml:mo></mml:mrow></mml:msup></mml:mrow></mml:math>Resonances at Mass<mml:math xmlns:m

Aaij, R.; Adeva, B.; Adinolfi, M.; Affolder, A.; Ajaltouni, Z.; Akar, S.; Albrecht, J.; Alessio, F.; Alexander, M.; Ali, S.; Alkhazov, G.; Cartelle, P. Alvarez; Alves, A. A.; Amato, S.; Amerio, S.; Amhis, Y.; An, L.; Anderlini, L.; Anderson, J.; Andreassen, R.; Andreotti, M.; Andrews, J. E.; Appleby, R. B.; Gutierrez, O. Aquines; Archilli, F.; Артамонов, А.; Artuso, M.; Aslanides, E.; Auriemma, G.; Baalouch, M.; Bachmann, S.; Back, J. J.; Badalov, A.; Baesso, C.; Baldini, W.; Barlow, R. J.; Barschel, C.; Barsuk, S.; Barter, W.; Batozskaya, V.; Battista, V.; Bay, A.; Beaucourt, L.; Beddow, J.; Bedeschi, F.; Bediaga, I.; Belogurov, S.; Belous, K.; Belyaev, I.; Ben-Haim, E.; Bencivenni, G.; Benson, S.; Benton, J.; Berezhnoy, A.; Bernet, R.; Bettler, M. O.; Beuzekom, M. van; Bień, A.; Bifani, S.; Bird, T.; Bizzeti, A.; Bjørnstad, P. M.; Blake, T.; Blanc, F.; Blouw, J.; Blusk, S.; Bocci, V.; Bondar, A.; Bondar, N.; Bonivento, W.; Borghi, S.; Borgia, A.; Borsato, M.; Bowcock, T. J. V.; Bowen, E.; Bozzi, C.; Brambach, T.; Brand, J. van den; Bressieux, J.; Brett, D.; Britsch, M.; Britton, T.; Brodzicka, J.; Brook, N. H.; Brown, H.; Bursche, A.; Busetto, G.; Buytaert, J.; Cadeddu, S.; Calabrese, R.; Calvi, M.; Gomez, M. Calvo; Campana, P.; Perez, D. Campora; Carbone, A.; Carboni, G.; Cardinale, R.; Cardini, A.; Carson, L.; Akiba, K. Carvalho; Casse, G.; Cassina, L.; García, L. Castillo; Cattaneo, M.; Cauet, Ch.; Cenci, R.; Charles, M.; Charpentier, Ph.; Chefdeville, M.; Chen, S.; Cheung, S. F.; Chiapolini, N.; Chrząszcz, M.; Ciba, K.; Vidal, X. Cid; Ciezarek, G.; Clarke, P. E.L.; Clemencic, M.; Cliff, H. V.; Closier, J.; Coco, V.; Cogan, J.; Cogneras, E.; Collins, P.; Comerma-Montells, A.; Contu, A.; Cook, A.; Coombes, M.; Coquereau, S.; Corti, G.; Corvo, M.; Counts, I.; Couturier, B.; Cowan, G. A.; Craik, D. C.; Torres, M. Cruz; Cunliffe, S.; Currie, R.; D’Ambrosio, C.; Dalseno, J.; David, P.; Davis, A.; Bruyn, K. De; Capua, S. De; Cian, M. De; Miranda, J. M. De; Paula, L. De; Silva, W. De; Simone, P. De; Décamp, D.; Deckenhoff, M.; Buono, L. Del; Déĺeage, N.; Деркач, Д.; Deschamps, O.; Dettori, F.; Canto, A. Di; Dijkstra, H.; Donleavy, S.; Dordei, F.; Dorigo, M.; Suárez, A. Dosil; Dossett, D.; Dovbnya, A.; Dreimanis, K.; Dujany, G.; Dupertuis, F.; Durante, P.; Dzhelyadin, R.; Dziurda, A.; Dzyuba, A.; Easo, S.; Egede, U.; Egorychev, V.; Eidelman, S.; Eisenhardt, S.; Eitschberger, U.; Ekelhof, R.; Eklund, L.; Rifai, I. El; Elsässer, Ch.; Ely, S.; Esen, S.; Evans, H.; Evans, T.; Falabella, A.; Färber, C.; Farinelli, C.; Farley, N.; Farry, S.; Fay, R.; Ferguson, D.; Albor, V. Fernandez; Rodrigues, F. Ferreira; Ferro‐Luzzi, M.; Filippov, S.; Fiore, M.; Fiorini, M.; Firlej, M.; Fitzpatrick, C.; Fiutowski, T.; Fontana, M.; Fontanelli, F.; Forty, R.; Francisco, O. De Aguiar; Frank, M.; Frei, C.; Frosini, M.; Fu, J.; Furfaro, E.; Torreira, A. Gallas; Galli, D.; Gallorini, S.; Gambetta, S.; Gandelman, M.; Gandini, P.; Gao, Y.; Pardiñas, J. 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P.; Lefèvre, R.; Leflat, A.; Lefrançois, J.; Leo, S.; Leroy, O.; Lesiak, T.; Leverington, B.; Li, Y.; Likhomanenko, T.; Liles, M.; Lindner, R.; Linn, C.; Lionetto, F.; Liu, B.; Lohn, S.; Longstaff, I.; Lopes, J. H.; López-March, N.; Lowdon, P.; Lu, H.; Lucchesi, D.; Luo, H.; Lupato, A.; Luppi, E.; Lupton, O.; Machefert, F.; Machikhiliyan, I. V.; Maciuc, F.; Maev, O.; Malde, S.; Малинин, А.; Manca, G.; Mancinelli, G.; Mapelli, A.; Maratas, J.; Marchand, J. F.; Marconi, U.; Benito, C. Marín; Marino, P.; Märki, R.; Marks, J.; Martellotti, G.; Martens, A.; Sánchez, A. Martín; Martinelli, M.; Santos, D. Martínez; Martínez-Vidal, F.; Tostes, D. Martins; Massafferri, A.; Matev, R.; Máthé, Z.; Matteuzzi, C.; Mazurov, A.; McCann, M.; McCarthy, J.; McNab, A.; McNulty, R.; McSkelly, B.; Meadows, B.; Meier, F.; Meissner, M.; Merk, M.; Milanés, D. A.; Minard, M.-N.; Moggi, N.; Rodriguez, J. Molina; Monteil, S.; Morandin, M.; Morawski, P.; Mordà, A.; Morello, M. J.; Moroń, J.; Morris, A. 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doi:10.1103/physrevlett.113.162001

Cited by 90 publications

(85 citation statements)

References 36 publications

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“…In fact L ¼ 3 is the highest orbital angular momentum observed, with a very small rate, in decays of B mesons [35] PRL 115, 072001 (2015) P Fig. 7, and the comparison with the data in m Kp intervals is also satisfactory as can be seen in Fig PRL 115, 072001 (2015) P…”

Section: H Y S I C a L R E V I E W L E T T E R S Week Ending 14 Augusmentioning

confidence: 53%

Observation ofJ/ψpResonances Consistent with Pentaquark States inΛb0
Aaij¹,
Adeva²,
Adinolfi³
et al. 2015
Phys. Rev. Lett.
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Observations of exotic structures in the J=ψp channel, which we refer to as charmonium-pentaquark states, in Λ 0 b → J=ψK − p decays are presented. The data sample corresponds to an integrated luminosity of 3 fb −1 acquired with the LHCb detector from 7 and 8 TeV pp collisions. An amplitude analysis of the three-body final state reproduces the two-body mass and angular distributions. To obtain a satisfactory fit of the structures seen in the J=ψp mass spectrum, it is necessary to include two Breit-Wigner amplitudes that each describe a resonant state. The significance of each of these resonances is more than 9 standard deviations. One has a mass of 4380 AE 8 AE 29 MeV and a width of 205 AE 18 AE 86 MeV, while the second is narrower, with a mass of 4449.8 AE 1.7 AE 2.5 MeV and a width of 39 AE 5 AE 19 MeV. The preferred J P assignments are of opposite parity, with one state having spin 3=2 and the other 5=2.

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Section: H Y S I C a L R E V I E W L E T T E R S Week Ending 14 Augusmentioning

confidence: 53%

Observation ofJ/ψpResonances Consistent with Pentaquark States inΛb0
Aaij¹,
Adeva²,
Adinolfi³
et al. 2015
Phys. Rev. Lett.
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“…[6] for a concise review). Very recently, the LHCb Collaboration announced the observation of two charmed-strange mesons D Ã s1 ð2860Þ and D Ã s3 ð2860Þ with the resonance parameters [7,8]: In addition, LHCb specified that it is the first time to identify a spin-3 resonance D Ã s3 ð2860Þ [7,8]. At present, the charmed-strange meson family is becoming more and more abundant with the experimental progress.…”

Section: Introductionmentioning

confidence: 99%

D-wave heavy-light mesons from QCD sum rules

et al. 2014

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We study the D-wavecs heavy meson doublets ð1 − ; 2 − Þ and ð2 − ; 3 − Þ using the method of QCD sum rule in the framework of heavy quark effective theory. Choosing the same threshold values ω c around 2.7 Gev, we calculate the masses of the 1 − and 3 − states. They are m D Ã s1 ¼ 2.81 AE 0.10 GeV and m D Ã s3 ¼ 2.85AE 0.08 GeV, consistent with the newly observed D Ã s1 ð2860Þ and D Ã s3 ð2860Þ states by LHCb. The masses of their 2 − partners are calculated to be 2.82 AE 0.10 and 2.81 AE 0.08 GeV. The mass splittings within the same doublet are calculated to be m D s2 − m D Ã s1 ¼ 0.016 AE 0.007 GeV and m D Ã s3 − m D 0 s2 ¼ 0.039AE 0.014 GeV.

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“…An LHCb study of B 0 s → D 0 K − π + decays, in which they searched for excited D s mesons [1240], showed with 10σ significance that this state is comprised of two different particles, one of spin 1 and one of spin 3. This represents the first measurement of a heavy flavored spin-3 particle, and the first observation of B meson decays to spin 3 particles.…”

Section: Argus [1266]mentioning

confidence: 99%

Averages of b-hadron, c-hadron, and $$\tau $$ τ -lepton properties as of summer 2016

et al. 2017

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This paper reports world averages of measurements of b-hadron, c-hadron, and τ -lepton properties obtained by the Heavy Flavour Averaging Group using results available before April 2021. In rare cases, significant results obtained several months later are also used. For the averaging, common input parameters used in the various analyses are adjusted (rescaled) to common values, and known correlations are taken into account. The averages include branching fractions, lifetimes, neutral meson mixing parameters, CP violation parameters, parameters of semileptonic decays, and Cabibbo-Kobayashi-Maskawa matrix elements. Selected world averages -continued from previous page. ∆Γ d /Γ d 0.001 ± 0.010 |q d /p d | 1.0010 ± 0.0008 ∆m s 17.765 ± 0.006 ps −1 ∆Γ s +0.084 ± 0.005 ps −1 |q s /p s | 1.0003 ± 0.0014 φ ccs s −0.049 ± 0.019 rad Unitarity-Triangle angle parameters sin2β ≡ sin2φ 1 0.699 ± 0.017 β ≡ φ 1 (22.2 ± 0.7) • −ηS φK 0 S 0.74 +0.11 −0.13 −ηS η K 0 0.63 ± 0.06 −ηS K 0 S K 0 S K 0 S 0.83 ± 0.17 φ s (φφ) −0.073 ± 0.115 ± 0.027 rad S B 0 s →K + K − , C B 0 s →K + K − (0.14 ± 0.03, 0.17 ± 0.03) −ηS J/ψ π 0 0.86 ± 0.14 −ηS D + D − 0.84 ± 0.12 −ηS J/ψ ρ 0 0.66 +0.13 −0.12 +0.09 −0.03(0.343 ± 0.002)% τ parameters, lepton universality, and |V us | g τ /g µ 1.0009 ± 0.0014 g τ /g e 1.0027 ± 0.0014 g µ /g e 1.0019 ± 0.0014* )0 s B ( * )0 s ) = (87.0 ± 1.7)% [34] measured as described in Ref. [35]. The proportions of the various production channels for non-strange B mesons have also been measured [22]. 4.3 b-hadron production fractions at high energy At high energy, all species of weakly decaying b hadrons may be produced, either directly or in strong and electromagnetic decays of excited b hadrons. Before 2010, it was assumed that the fractions of different species in unbiased samples of high-p T b-hadron jets where independent of whether they originated from Z decays, pp collisions at the Tevatron, or pp collisions at the LHC. This hypothesis was plausible under the condition Q 2 Λ 2 QCD , namely, that the square of the momentum transfer to the produced b quarks is large compared with the square of the hadronization energy scale. This hypothesis is correct in the limit p T → ∞, in which the production mechanism of a b hadron is completely described by the fragmentation of the b quark. For finite p T , however, there are interference effects of the production mechanism of the b quark and its hadronization. While formally suppressed by inverse powers of p T , these effects may be sizable, especially when the fragmentation probabilities are small as, e.g., in the case of b baryons. In fact, the available data show that the fractions depend on the kinematics of the produced b hadron. Both CDF and LHCb reported a p T dependence of the fractions, with the fraction of Λ 0 b baryons observed at low p T being enhanced with respect to that seen at LEP at higher p T . In our previous publication [1], we presented two sets of averages, one including only measurements performed at LEP, and another including only measurements performed ...

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Observation of Overlapping Spin-1 and Spin-3D¯0K−Resonances at Mass

Cited by 90 publications

References 36 publications

Observation ofJ/ψpResonances Consistent with Pentaquark States inΛb0
Aaij¹,
Adeva²,
Adinolfi³
et al. 2015
Phys. Rev. Lett.
Self Cite
1,032
24
525
1
View full text Add to dashboard Cite

Observation ofJ/ψpResonances Consistent with Pentaquark States inΛb0
Aaij¹,
Adeva²,
Adinolfi³
et al. 2015
Phys. Rev. Lett.
Self Cite
1,032
24
525
1
View full text Add to dashboard Cite

D-wave heavy-light mesons from QCD sum rules

Averages of b-hadron, c-hadron, and $$\tau $$ τ -lepton properties as of summer 2016

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Observation of Overlapping Spin-1 and Spin-3D¯0K−Resonances at Mass

Cited by 90 publications

References 36 publications

Observation ofJ/ψpResonances Consistent with Pentaquark States inΛb0Aaij1, Adeva2, Adinolfi3 et al. 2015Phys. Rev. Lett.Self Cite1,032245251View full textAdd to dashboardCite

Observation ofJ/ψpResonances Consistent with Pentaquark States inΛb0Aaij1, Adeva2, Adinolfi3 et al. 2015Phys. Rev. Lett.Self Cite1,032245251View full textAdd to dashboardCite

D-wave heavy-light mesons from QCD sum rules

Averages of b-hadron, c-hadron, and $$\tau $$ τ -lepton properties as of summer 2016

Contact Info

Product

Resources

About

Observation ofJ/ψpResonances Consistent with Pentaquark States inΛb0
Aaij¹,
Adeva²,
Adinolfi³
et al. 2015
Phys. Rev. Lett.
Self Cite
1,032
24
525
1
View full text Add to dashboard Cite

Observation ofJ/ψpResonances Consistent with Pentaquark States inΛb0
Aaij¹,
Adeva²,
Adinolfi³
et al. 2015
Phys. Rev. Lett.
Self Cite
1,032
24
525
1
View full text Add to dashboard Cite