Publisher’s Note: Observation of a narrow resonance of mass<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:mn>2.46</mml:mn><mml:mtext> </mml:mtext><mml:mtext> </mml:mtext><mml:mi>GeV</mml:mi><mml:mo>/</mml:mo><mml:msup><mml:mi>c</mml:mi><mml:mn>2</mml:mn></mml:msup></mml:math>decaying to<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:msubsup><mml:mi>D</mml:mi><mml:mi>s</mml:mi><mml:mrow><mml:mo>*</mml:mo><mml:mo>+</mml:mo></mml:mrow></mml:msubsu

Besson, D.; Anderson, S.; Frolov, V. V.; Gong, D. T.; Kubota, Y.; Li, S. Z.; Poling, R.; Smith, A. J. S.; Stepaniak, C. J.; Urheim, J.; Metreveli, Z.; Seth, K. K.; Tomaradze, A.; Zweber, P.; Arms, K.; Eckhart, E. A.; Gan, K. K.; Gwon, C.; Pedlar, T. K.; Toerne, E. von; Severini, H.; Skubic, P.; Dytman, S. A.; Muêller, J.; Nam, S.; Savinov, V.; Hinson, J. W.; Huang, G. S.; Lee, J.; Miller, D. H.; Pavlunin, V.; Sanghi, B.; Shibata, E. I.; Shipsey, I. P. J.; Cronin-Hennessy, D.; Park, C. S.; Park, W.; Thayer, J. B.; Thorndike, E. H.; Coan, T. E.; Gao, Y.; Liu, F.; Stroynowski, R.; Artuso, M.; Boulahouache, C.; Blusk, S.; Dambasuren, E.; Dorjkhaidav, O.; Mountain, R.; Muramatsu, H.; Nandakumar, R.; Skwarnicki, T.; Stone, S.; Wang, J. C.; Mahmood, A. H.; Csorna, S. E.; Dankó, I.; Bonvicini, G.; Cinabro, D.; Dubrovin, M.; McGee, Sean L.; Bornheim, A.; Lipeles, E.; Pappas, S. P.; Shapiro, A.; Sun, W.; Weinstein, A. J.; Briere, R. A.; Chen, G. P.; Ferguson, T.; Tatishvili, G.; Vogel, H.; Watkins, M. E.; Adam, N.; Alexander, J. P.; Berkelman, K.; Boisvert, V.; Cassel, D. G.; Duboscq, J. E.; Ecklünd, K. M.; Ehrlich, R.; Galik, R. S.; Gibbons, L.; Gittelman, B.; Gray, S. W.; Hartill, D. L.; Heltsley, B. K.; Hsu, L.; Jones, C. D.; Kandaswamy, J.; Kreinick, D. L.; Magerkurth, A.; Mahlke-Krüger, H.; Meyer, T. O.; Mistry, N. B.; Patterson, J. R.; Peterson, Donald L.; Pivarski, J.; Richichi, S. J.; Riley, D.; Sadoff, A. J.; Schwarthoff, H.; Shepherd, M. R.; Thayer, J. G.; Urner, D.; Wilksen, T.; Warburton, A.; Weinberger, M.; Athar, S. B.; Avery, P.; Breva-Newell, L.; Potlia, V.; Stoeck, H.; Yelton, J.; Eisenstein, B. I.; Gollin, G. D.; Karliner, I.; Lowrey, N.; Plager, C.; Sedlack, C.; Selen, M.; Thaler, J. J.; Williams, J. C.; Edwards, K. W.

doi:10.1103/physrevd.75.119908

Cited by 130 publications

(70 citation statements)

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“…− [1] and D s1 ð2460Þ − [2] mesons led to renewed activity in the field, as their masses were found to be below the DK and D Ã K thresholds, respectively, in contrast to prior predictions. These states are usually interpreted as being two of the orbitally excited (1P) charm-strange states, the other two being the D s1 ð2536Þ − and D Ã s2 ð2573Þ − resonances.…”

contrasting

confidence: 47%

Observation of Overlapping Spin-1 and Spin-3D¯0K−Resonances at Mass
Aaij¹,
Adeva²,
Adinolfi³
et al. 2014
Phys. Rev. Lett.
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contrasting

confidence: 47%

Observation of Overlapping Spin-1 and Spin-3D¯0K−Resonances at Mass
Aaij¹,
Adeva²,
Adinolfi³
et al. 2014
Phys. Rev. Lett.
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0
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“…Since the observation of D Ã s0 ð2317Þ in 2003 [1], more and more charmed-strange mesons have been reported experimentally, which include D s1 ð2460Þ [2], D s1 ð2710Þ [3,4], D sJ ð2860Þ [4,5], and D sJ ð3040Þ [4] (see Ref. [6] for a concise review).…”

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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“…First of all, the doublet with J P ¼ 0 þ ; 1 þ has not been observed for a long time although it is predicted to be very broad [2]. Furthermore, the later discovery of the D Ã s0 ð2317Þ and the D s1 ð2460Þ by the CLEO [3] and BABAR [4] collaborations are difficult to explain in terms of quark models.…”

Section: Introductionmentioning

confidence: 99%

New interpretation for theDs2*(2573)and the prediction of novel exotic charmed mesons

2010

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In this manuscript we study the vector-vector interaction within the hidden-gauge formalism in a coupled channel unitary approach. In the sector C ¼ 1, S ¼ 1, J ¼ 2 we get a pole in the T matrix around 2572 MeV that we identify with the D Ã s2 ð2573Þ, coupling strongly to the D Ã K Ã ðD Ã s ð!ÞÞ channels. In addition we obtain resonances in other exotic sectors which have not been studied before such as C ¼ 1, S ¼ À1, C ¼ 2, S ¼ 0 and C ¼ 2, S ¼ 1. These ''flavor-exotic'' states are interpreted as D Ã " K Ã , D Ã D Ã , and D Ã s D Ã molecular states but have not been observed yet. In total we obtain nine states with different spin, isospin, charm, and strangeness of non-C ¼ 0, S ¼ 0 and C ¼ 1, S ¼ 0 character, which have been reported before.

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Publisher’s Note: Observation of a narrow resonance of mass2.46 GeV/c2decaying toDs*+

Cited by 130 publications

References 0 publications

Observation of Overlapping Spin-1 and Spin-3D¯0K−Resonances at Mass
Aaij¹,
Adeva²,
Adinolfi³
et al. 2014
Phys. Rev. Lett.
Self Cite
90
13
72
0
View full text Add to dashboard Cite

Observation of Overlapping Spin-1 and Spin-3D¯0K−Resonances at Mass
Aaij¹,
Adeva²,
Adinolfi³
et al. 2014
Phys. Rev. Lett.
Self Cite
90
13
72
0
View full text Add to dashboard Cite

D-wave heavy-light mesons from QCD sum rules

New interpretation for theDs2*(2573)and the prediction of novel exotic charmed mesons

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Publisher’s Note: Observation of a narrow resonance of mass2.46 GeV/c2decaying toDs*+

Cited by 130 publications

References 0 publications

Observation of Overlapping Spin-1 and Spin-3D¯0K−Resonances at MassAaij1, Adeva2, Adinolfi3 et al. 2014Phys. Rev. Lett.Self Cite9013720View full textAdd to dashboardCite

Observation of Overlapping Spin-1 and Spin-3D¯0K−Resonances at MassAaij1, Adeva2, Adinolfi3 et al. 2014Phys. Rev. Lett.Self Cite9013720View full textAdd to dashboardCite

D-wave heavy-light mesons from QCD sum rules

New interpretation for theDs2*(2573)and the prediction of novel exotic charmed mesons

Contact Info

Product

Resources

About

Observation of Overlapping Spin-1 and Spin-3D¯0K−Resonances at Mass
Aaij¹,
Adeva²,
Adinolfi³
et al. 2014
Phys. Rev. Lett.
Self Cite
90
13
72
0
View full text Add to dashboard Cite

Observation of Overlapping Spin-1 and Spin-3D¯0K−Resonances at Mass
Aaij¹,
Adeva²,
Adinolfi³
et al. 2014
Phys. Rev. Lett.
Self Cite
90
13
72
0
View full text Add to dashboard Cite