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001 | 18600 | ||
005 | 20240610120725.0 | ||
024 | 7 | _ | |a 10.1140/epja/i2011-11019-2 |2 DOI |
024 | 7 | _ | |a WOS:000288551700006 |2 WOS |
024 | 7 | _ | |a arXiv:1009.3804 |c hep-ph |2 arXiv |
024 | 7 | _ | |a 2128/10301 |2 Handle |
035 | _ | _ | |9 arXiv |a arXiv:1009.3804 |c hep-ph |
035 | _ | _ | |a FZJ-IKP-TH-2010-20 |
035 | _ | _ | |a HISKP-TH-10-24 |
037 | _ | _ | |a PreJuSER-18600 |
041 | _ | _ | |a eng |
082 | _ | _ | |a 530 |
084 | _ | _ | |2 WoS |a Physics, Nuclear |
084 | _ | _ | |2 WoS |a Physics, Particles & Fields |
084 | _ | _ | |2 PACS |a 12.39.Fe |
084 | _ | _ | |2 PACS |a 13.75.Lb |
100 | 1 | _ | |0 P:(DE-Juel1)VDB103321 |a Cleven, M. |b 0 |u FZJ |
245 | _ | _ | |a Light meson mass dependence of the positive parity heavy-strange mesons |
260 | _ | _ | |a Berlin |b Springer |c 2011 |
300 | _ | _ | |a 19 |
336 | 7 | _ | |a Journal Article |0 PUB:(DE-HGF)16 |2 PUB:(DE-HGF) |
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336 | 7 | _ | |a Journal Article |0 0 |2 EndNote |
336 | 7 | _ | |a ARTICLE |2 BibTeX |
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336 | 7 | _ | |a article |2 DRIVER |
440 | _ | 0 | |0 1981 |a European Physical Journal A |v 47 |x 1434-6001 |y 2 |
500 | _ | _ | |a This work is partially supported by the Helmholtz Association through funds provided to the Virtual Institute "Spin and strong QCD" (VH-VI-231) and by the DFG (TR 16, "Subnuclear Structure of Matter"), the European Community-Research Infrastructure Integrating Activity "Study of Strongly Interacting Matter" (acronym Hadron-Physics2, Grant Agreement No. 227431) under the FP7 of the EU, and the BMBF (Grant No. 06BN9006). |
500 | _ | _ | |9 arXiv |a 10 pages |
500 | _ | _ | |9 arXiv |a 10 pages |
520 | _ | _ | |a We calculate the masses of the resonances D*(s0)(2317) and D-s1(2460) as well as their bottom partners as bound states of a kaon and a D-(*())-and B-(*())-meson, respectively, in unitarized chiral perturbation theory at next-to-leading order. After fixing the parameters in the D*(s0)(2317) channel, the calculated mass for the D-s1(2460) is found in excellent agreement with experiment. The masses for the analogous states with a bottom quark are predicted to be MB*(s0) - (5696 +/- 40) MeV and M-Bs1 - (5742 +/- 40) MeV in reasonable agreement with previous analyses. In particular, we predict M-Bs1-MB*(s0) - 46 +/- 1MeV. We also explore the dependence of the states on the pion and kaon masses. We argue that the kaon mass dependence of a kaonic bound state should be almost linear with slope about unity. Such a dependence is specific to the assumed molecular nature of the states. We suggest to extract the kaon mass dependence of these states from lattice QCD calculations. |
536 | _ | _ | |0 G:(DE-Juel1)FUEK413 |2 G:(DE-HGF) |a Physik der Hadronen und Kerne |c P53 |x 0 |
536 | _ | _ | |0 G:(EU-Grant)227431 |2 European Community |a European Community: 227431 |c 227431 |x 3 |
588 | _ | _ | |a Dataset connected to Web of Science |
650 | _ | 7 | |2 INSPIRE |a K: mass |
650 | _ | 7 | |2 INSPIRE |a perturbation theory: chiral |
650 | _ | 7 | |2 INSPIRE |a higher-order: 1 |
650 | _ | 7 | |2 INSPIRE |a D/s0*(2317): mass: calculated |
650 | _ | 7 | |2 INSPIRE |a D/s1(2460): mass: calculated |
650 | _ | 7 | |2 INSPIRE |a bottom meson: mass: calculated |
650 | _ | 7 | |2 INSPIRE |a meson meson: bound state |
650 | _ | 7 | |2 INSPIRE |a pi: mass |
650 | _ | 7 | |2 INSPIRE |a Goldstone particle: scattering amplitude |
650 | _ | 7 | |2 INSPIRE |a coupled channel |
650 | _ | 7 | |2 INSPIRE |a binding energy |
650 | _ | 7 | |2 INSPIRE |a numerical calculations |
700 | 1 | _ | |0 P:(DE-HGF)0 |a Guo, F.-K. |b 1 |
700 | 1 | _ | |0 P:(DE-Juel1)131182 |a Hanhart, C. |b 2 |u FZJ |
700 | 1 | _ | |0 P:(DE-Juel1)131252 |a Meißner, U.-G. |b 3 |u FZJ |
773 | _ | _ | |0 PERI:(DE-600)1459066-9 |a 10.1140/epja/i2011-11019-2 |g Vol. 47, p. 19 |p 19 |q 47<19 |t The @European physical journal / A |v 47 |x 1434-6001 |y 2011 |
856 | 7 | _ | |u http://dx.doi.org/10.1140/epja/i2011-11019-2 |
856 | 4 | _ | |u https://juser.fz-juelich.de/record/18600/files/1009.3804v1.pdf |y OpenAccess |
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914 | 1 | _ | |y 2011 |
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