Strong decays of %$D_{3}^{*}(2760)%$, %$D_{s3}^{*}(2860)%$, %$B_{3}^{*}%$, and %$B_{s3}^{*}%$
Abstract In this paper, we study the OZI-allowed two-body strong decays of %$3^-%$ heavy–light mesons. Experimentally the charmed %$D_{3}^{*}(2760)%$ and the charm–strange %$D_{s3}^{*}(2860)%$ states with these quantum numbers have been discovered. For the bottomed B(5970) state, which was found by...
Ausführliche Beschreibung
Gespeichert in:
| Autor*in: |
Wang, Tianhong [verfasserIn] Wang, Zhi-Hui [verfasserIn] Jiang, Yue [verfasserIn] Jiang, Libo [verfasserIn] Wang, Guo-Li [verfasserIn] |
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| Format: |
E-Artikel |
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| Sprache: |
Englisch |
| Erschienen: |
2017 |
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| Schlagwörter: |
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| Übergeordnetes Werk: |
Enthalten in: The European physical journal - Berlin : Springer, 1998, 77(2017), 1 vom: 19. Jan. |
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| Übergeordnetes Werk: |
volume:77 ; year:2017 ; number:1 ; day:19 ; month:01 |
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| DOI / URN: |
10.1140/epjc/s10052-017-4611-5 |
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| Katalog-ID: |
SPR008355126 |
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| 100 | 1 | |a Wang, Tianhong |e verfasserin |4 aut | |
| 245 | 1 | 0 | |a Strong decays of %$D_{3}^{*}(2760)%$, %$D_{s3}^{*}(2860)%$, %$B_{3}^{*}%$, and %$B_{s3}^{*}%$ |
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| 520 | |a Abstract In this paper, we study the OZI-allowed two-body strong decays of %$3^-%$ heavy–light mesons. Experimentally the charmed %$D_{3}^{*}(2760)%$ and the charm–strange %$D_{s3}^{*}(2860)%$ states with these quantum numbers have been discovered. For the bottomed B(5970) state, which was found by the CDF Collaboration recently, its quantum number has not been decided yet and we assume it is a %$3^-%$ meson in this paper. The theoretical prediction for the strong decays of bottom–strange state %$B_{s3}^*%$ is also given. The relativistic wave functions of %$3^-%$ heavy mesons are constructed and their numerical values are obtained by solving the corresponding Bethe–Salpeter equation with instantaneous approximation. The transition matrix is calculated by using the PCAC and low energy theorem, following which the decay widths are obtained. For %$D_{3}^*(2760)%$ and %$D_{s3}^*(2860)%$, the total strong decay widths are 72.6 and 47.6 MeV, respectively. For %$B_3^*%$ with %$M=5978%$ MeV and %$B_{s3}^*%$ with %$M=6178%$ MeV, their strong decay widths are 22.9 and 40.8 MeV, respectively. | ||
| 650 | 4 | |a Decay Width |7 (dpeaa)DE-He213 | |
| 650 | 4 | |a LHCb Collaboration |7 (dpeaa)DE-He213 | |
| 650 | 4 | |a Heavy Meson |7 (dpeaa)DE-He213 | |
| 650 | 4 | |a BaBar Collaboration |7 (dpeaa)DE-He213 | |
| 650 | 4 | |a Light Meson |7 (dpeaa)DE-He213 | |
| 700 | 1 | |a Wang, Zhi-Hui |e verfasserin |4 aut | |
| 700 | 1 | |a Jiang, Yue |e verfasserin |4 aut | |
| 700 | 1 | |a Jiang, Libo |e verfasserin |4 aut | |
| 700 | 1 | |a Wang, Guo-Li |e verfasserin |4 aut | |
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10.1140/epjc/s10052-017-4611-5 doi (DE-627)SPR008355126 (SPR)s10052-017-4611-5-e DE-627 ger DE-627 rakwb eng 530 ASE 33.50 bkl Wang, Tianhong verfasserin aut Strong decays of %$D_{3}^{*}(2760)%$, %$D_{s3}^{*}(2860)%$, %$B_{3}^{*}%$, and %$B_{s3}^{*}%$ 2017 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier Abstract In this paper, we study the OZI-allowed two-body strong decays of %$3^-%$ heavy–light mesons. Experimentally the charmed %$D_{3}^{*}(2760)%$ and the charm–strange %$D_{s3}^{*}(2860)%$ states with these quantum numbers have been discovered. For the bottomed B(5970) state, which was found by the CDF Collaboration recently, its quantum number has not been decided yet and we assume it is a %$3^-%$ meson in this paper. The theoretical prediction for the strong decays of bottom–strange state %$B_{s3}^*%$ is also given. The relativistic wave functions of %$3^-%$ heavy mesons are constructed and their numerical values are obtained by solving the corresponding Bethe–Salpeter equation with instantaneous approximation. The transition matrix is calculated by using the PCAC and low energy theorem, following which the decay widths are obtained. For %$D_{3}^*(2760)%$ and %$D_{s3}^*(2860)%$, the total strong decay widths are 72.6 and 47.6 MeV, respectively. For %$B_3^*%$ with %$M=5978%$ MeV and %$B_{s3}^*%$ with %$M=6178%$ MeV, their strong decay widths are 22.9 and 40.8 MeV, respectively. Decay Width (dpeaa)DE-He213 LHCb Collaboration (dpeaa)DE-He213 Heavy Meson (dpeaa)DE-He213 BaBar Collaboration (dpeaa)DE-He213 Light Meson (dpeaa)DE-He213 Wang, Zhi-Hui verfasserin aut Jiang, Yue verfasserin aut Jiang, Libo verfasserin aut Wang, Guo-Li verfasserin aut Enthalten in The European physical journal Berlin : Springer, 1998 77(2017), 1 vom: 19. Jan. (DE-627)253722934 (DE-600)1459069-4 1434-6052 nnns volume:77 year:2017 number:1 day:19 month:01 https://dx.doi.org/10.1140/epjc/s10052-017-4611-5 kostenfrei Volltext GBV_USEFLAG_A SYSFLAG_A GBV_SPRINGER GBV_ILN_11 GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_39 GBV_ILN_40 GBV_ILN_60 GBV_ILN_62 GBV_ILN_63 GBV_ILN_69 GBV_ILN_70 GBV_ILN_73 GBV_ILN_95 GBV_ILN_105 GBV_ILN_110 GBV_ILN_150 GBV_ILN_151 GBV_ILN_161 GBV_ILN_170 GBV_ILN_206 GBV_ILN_213 GBV_ILN_230 GBV_ILN_267 GBV_ILN_285 GBV_ILN_293 GBV_ILN_370 GBV_ILN_602 GBV_ILN_702 GBV_ILN_2001 GBV_ILN_2003 GBV_ILN_2005 GBV_ILN_2006 GBV_ILN_2008 GBV_ILN_2009 GBV_ILN_2010 GBV_ILN_2011 GBV_ILN_2014 GBV_ILN_2015 GBV_ILN_2018 GBV_ILN_2020 GBV_ILN_2021 GBV_ILN_2025 GBV_ILN_2031 GBV_ILN_2038 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2050 GBV_ILN_2055 GBV_ILN_2056 GBV_ILN_2057 GBV_ILN_2061 GBV_ILN_2108 GBV_ILN_2111 GBV_ILN_2113 GBV_ILN_2119 GBV_ILN_2190 GBV_ILN_4012 GBV_ILN_4037 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4126 GBV_ILN_4246 GBV_ILN_4249 GBV_ILN_4305 GBV_ILN_4306 GBV_ILN_4307 GBV_ILN_4313 GBV_ILN_4322 GBV_ILN_4323 GBV_ILN_4324 GBV_ILN_4325 GBV_ILN_4335 GBV_ILN_4338 GBV_ILN_4367 GBV_ILN_4700 33.50 ASE AR 77 2017 1 19 01 |
| spelling |
10.1140/epjc/s10052-017-4611-5 doi (DE-627)SPR008355126 (SPR)s10052-017-4611-5-e DE-627 ger DE-627 rakwb eng 530 ASE 33.50 bkl Wang, Tianhong verfasserin aut Strong decays of %$D_{3}^{*}(2760)%$, %$D_{s3}^{*}(2860)%$, %$B_{3}^{*}%$, and %$B_{s3}^{*}%$ 2017 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier Abstract In this paper, we study the OZI-allowed two-body strong decays of %$3^-%$ heavy–light mesons. Experimentally the charmed %$D_{3}^{*}(2760)%$ and the charm–strange %$D_{s3}^{*}(2860)%$ states with these quantum numbers have been discovered. For the bottomed B(5970) state, which was found by the CDF Collaboration recently, its quantum number has not been decided yet and we assume it is a %$3^-%$ meson in this paper. The theoretical prediction for the strong decays of bottom–strange state %$B_{s3}^*%$ is also given. The relativistic wave functions of %$3^-%$ heavy mesons are constructed and their numerical values are obtained by solving the corresponding Bethe–Salpeter equation with instantaneous approximation. The transition matrix is calculated by using the PCAC and low energy theorem, following which the decay widths are obtained. For %$D_{3}^*(2760)%$ and %$D_{s3}^*(2860)%$, the total strong decay widths are 72.6 and 47.6 MeV, respectively. For %$B_3^*%$ with %$M=5978%$ MeV and %$B_{s3}^*%$ with %$M=6178%$ MeV, their strong decay widths are 22.9 and 40.8 MeV, respectively. Decay Width (dpeaa)DE-He213 LHCb Collaboration (dpeaa)DE-He213 Heavy Meson (dpeaa)DE-He213 BaBar Collaboration (dpeaa)DE-He213 Light Meson (dpeaa)DE-He213 Wang, Zhi-Hui verfasserin aut Jiang, Yue verfasserin aut Jiang, Libo verfasserin aut Wang, Guo-Li verfasserin aut Enthalten in The European physical journal Berlin : Springer, 1998 77(2017), 1 vom: 19. Jan. (DE-627)253722934 (DE-600)1459069-4 1434-6052 nnns volume:77 year:2017 number:1 day:19 month:01 https://dx.doi.org/10.1140/epjc/s10052-017-4611-5 kostenfrei Volltext GBV_USEFLAG_A SYSFLAG_A GBV_SPRINGER GBV_ILN_11 GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_39 GBV_ILN_40 GBV_ILN_60 GBV_ILN_62 GBV_ILN_63 GBV_ILN_69 GBV_ILN_70 GBV_ILN_73 GBV_ILN_95 GBV_ILN_105 GBV_ILN_110 GBV_ILN_150 GBV_ILN_151 GBV_ILN_161 GBV_ILN_170 GBV_ILN_206 GBV_ILN_213 GBV_ILN_230 GBV_ILN_267 GBV_ILN_285 GBV_ILN_293 GBV_ILN_370 GBV_ILN_602 GBV_ILN_702 GBV_ILN_2001 GBV_ILN_2003 GBV_ILN_2005 GBV_ILN_2006 GBV_ILN_2008 GBV_ILN_2009 GBV_ILN_2010 GBV_ILN_2011 GBV_ILN_2014 GBV_ILN_2015 GBV_ILN_2018 GBV_ILN_2020 GBV_ILN_2021 GBV_ILN_2025 GBV_ILN_2031 GBV_ILN_2038 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2050 GBV_ILN_2055 GBV_ILN_2056 GBV_ILN_2057 GBV_ILN_2061 GBV_ILN_2108 GBV_ILN_2111 GBV_ILN_2113 GBV_ILN_2119 GBV_ILN_2190 GBV_ILN_4012 GBV_ILN_4037 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4126 GBV_ILN_4246 GBV_ILN_4249 GBV_ILN_4305 GBV_ILN_4306 GBV_ILN_4307 GBV_ILN_4313 GBV_ILN_4322 GBV_ILN_4323 GBV_ILN_4324 GBV_ILN_4325 GBV_ILN_4335 GBV_ILN_4338 GBV_ILN_4367 GBV_ILN_4700 33.50 ASE AR 77 2017 1 19 01 |
| allfields_unstemmed |
10.1140/epjc/s10052-017-4611-5 doi (DE-627)SPR008355126 (SPR)s10052-017-4611-5-e DE-627 ger DE-627 rakwb eng 530 ASE 33.50 bkl Wang, Tianhong verfasserin aut Strong decays of %$D_{3}^{*}(2760)%$, %$D_{s3}^{*}(2860)%$, %$B_{3}^{*}%$, and %$B_{s3}^{*}%$ 2017 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier Abstract In this paper, we study the OZI-allowed two-body strong decays of %$3^-%$ heavy–light mesons. Experimentally the charmed %$D_{3}^{*}(2760)%$ and the charm–strange %$D_{s3}^{*}(2860)%$ states with these quantum numbers have been discovered. For the bottomed B(5970) state, which was found by the CDF Collaboration recently, its quantum number has not been decided yet and we assume it is a %$3^-%$ meson in this paper. The theoretical prediction for the strong decays of bottom–strange state %$B_{s3}^*%$ is also given. The relativistic wave functions of %$3^-%$ heavy mesons are constructed and their numerical values are obtained by solving the corresponding Bethe–Salpeter equation with instantaneous approximation. The transition matrix is calculated by using the PCAC and low energy theorem, following which the decay widths are obtained. For %$D_{3}^*(2760)%$ and %$D_{s3}^*(2860)%$, the total strong decay widths are 72.6 and 47.6 MeV, respectively. For %$B_3^*%$ with %$M=5978%$ MeV and %$B_{s3}^*%$ with %$M=6178%$ MeV, their strong decay widths are 22.9 and 40.8 MeV, respectively. Decay Width (dpeaa)DE-He213 LHCb Collaboration (dpeaa)DE-He213 Heavy Meson (dpeaa)DE-He213 BaBar Collaboration (dpeaa)DE-He213 Light Meson (dpeaa)DE-He213 Wang, Zhi-Hui verfasserin aut Jiang, Yue verfasserin aut Jiang, Libo verfasserin aut Wang, Guo-Li verfasserin aut Enthalten in The European physical journal Berlin : Springer, 1998 77(2017), 1 vom: 19. Jan. (DE-627)253722934 (DE-600)1459069-4 1434-6052 nnns volume:77 year:2017 number:1 day:19 month:01 https://dx.doi.org/10.1140/epjc/s10052-017-4611-5 kostenfrei Volltext GBV_USEFLAG_A SYSFLAG_A GBV_SPRINGER GBV_ILN_11 GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_39 GBV_ILN_40 GBV_ILN_60 GBV_ILN_62 GBV_ILN_63 GBV_ILN_69 GBV_ILN_70 GBV_ILN_73 GBV_ILN_95 GBV_ILN_105 GBV_ILN_110 GBV_ILN_150 GBV_ILN_151 GBV_ILN_161 GBV_ILN_170 GBV_ILN_206 GBV_ILN_213 GBV_ILN_230 GBV_ILN_267 GBV_ILN_285 GBV_ILN_293 GBV_ILN_370 GBV_ILN_602 GBV_ILN_702 GBV_ILN_2001 GBV_ILN_2003 GBV_ILN_2005 GBV_ILN_2006 GBV_ILN_2008 GBV_ILN_2009 GBV_ILN_2010 GBV_ILN_2011 GBV_ILN_2014 GBV_ILN_2015 GBV_ILN_2018 GBV_ILN_2020 GBV_ILN_2021 GBV_ILN_2025 GBV_ILN_2031 GBV_ILN_2038 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2050 GBV_ILN_2055 GBV_ILN_2056 GBV_ILN_2057 GBV_ILN_2061 GBV_ILN_2108 GBV_ILN_2111 GBV_ILN_2113 GBV_ILN_2119 GBV_ILN_2190 GBV_ILN_4012 GBV_ILN_4037 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4126 GBV_ILN_4246 GBV_ILN_4249 GBV_ILN_4305 GBV_ILN_4306 GBV_ILN_4307 GBV_ILN_4313 GBV_ILN_4322 GBV_ILN_4323 GBV_ILN_4324 GBV_ILN_4325 GBV_ILN_4335 GBV_ILN_4338 GBV_ILN_4367 GBV_ILN_4700 33.50 ASE AR 77 2017 1 19 01 |
| allfieldsGer |
10.1140/epjc/s10052-017-4611-5 doi (DE-627)SPR008355126 (SPR)s10052-017-4611-5-e DE-627 ger DE-627 rakwb eng 530 ASE 33.50 bkl Wang, Tianhong verfasserin aut Strong decays of %$D_{3}^{*}(2760)%$, %$D_{s3}^{*}(2860)%$, %$B_{3}^{*}%$, and %$B_{s3}^{*}%$ 2017 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier Abstract In this paper, we study the OZI-allowed two-body strong decays of %$3^-%$ heavy–light mesons. Experimentally the charmed %$D_{3}^{*}(2760)%$ and the charm–strange %$D_{s3}^{*}(2860)%$ states with these quantum numbers have been discovered. For the bottomed B(5970) state, which was found by the CDF Collaboration recently, its quantum number has not been decided yet and we assume it is a %$3^-%$ meson in this paper. The theoretical prediction for the strong decays of bottom–strange state %$B_{s3}^*%$ is also given. The relativistic wave functions of %$3^-%$ heavy mesons are constructed and their numerical values are obtained by solving the corresponding Bethe–Salpeter equation with instantaneous approximation. The transition matrix is calculated by using the PCAC and low energy theorem, following which the decay widths are obtained. For %$D_{3}^*(2760)%$ and %$D_{s3}^*(2860)%$, the total strong decay widths are 72.6 and 47.6 MeV, respectively. For %$B_3^*%$ with %$M=5978%$ MeV and %$B_{s3}^*%$ with %$M=6178%$ MeV, their strong decay widths are 22.9 and 40.8 MeV, respectively. Decay Width (dpeaa)DE-He213 LHCb Collaboration (dpeaa)DE-He213 Heavy Meson (dpeaa)DE-He213 BaBar Collaboration (dpeaa)DE-He213 Light Meson (dpeaa)DE-He213 Wang, Zhi-Hui verfasserin aut Jiang, Yue verfasserin aut Jiang, Libo verfasserin aut Wang, Guo-Li verfasserin aut Enthalten in The European physical journal Berlin : Springer, 1998 77(2017), 1 vom: 19. Jan. (DE-627)253722934 (DE-600)1459069-4 1434-6052 nnns volume:77 year:2017 number:1 day:19 month:01 https://dx.doi.org/10.1140/epjc/s10052-017-4611-5 kostenfrei Volltext GBV_USEFLAG_A SYSFLAG_A GBV_SPRINGER GBV_ILN_11 GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_39 GBV_ILN_40 GBV_ILN_60 GBV_ILN_62 GBV_ILN_63 GBV_ILN_69 GBV_ILN_70 GBV_ILN_73 GBV_ILN_95 GBV_ILN_105 GBV_ILN_110 GBV_ILN_150 GBV_ILN_151 GBV_ILN_161 GBV_ILN_170 GBV_ILN_206 GBV_ILN_213 GBV_ILN_230 GBV_ILN_267 GBV_ILN_285 GBV_ILN_293 GBV_ILN_370 GBV_ILN_602 GBV_ILN_702 GBV_ILN_2001 GBV_ILN_2003 GBV_ILN_2005 GBV_ILN_2006 GBV_ILN_2008 GBV_ILN_2009 GBV_ILN_2010 GBV_ILN_2011 GBV_ILN_2014 GBV_ILN_2015 GBV_ILN_2018 GBV_ILN_2020 GBV_ILN_2021 GBV_ILN_2025 GBV_ILN_2031 GBV_ILN_2038 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2050 GBV_ILN_2055 GBV_ILN_2056 GBV_ILN_2057 GBV_ILN_2061 GBV_ILN_2108 GBV_ILN_2111 GBV_ILN_2113 GBV_ILN_2119 GBV_ILN_2190 GBV_ILN_4012 GBV_ILN_4037 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4126 GBV_ILN_4246 GBV_ILN_4249 GBV_ILN_4305 GBV_ILN_4306 GBV_ILN_4307 GBV_ILN_4313 GBV_ILN_4322 GBV_ILN_4323 GBV_ILN_4324 GBV_ILN_4325 GBV_ILN_4335 GBV_ILN_4338 GBV_ILN_4367 GBV_ILN_4700 33.50 ASE AR 77 2017 1 19 01 |
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10.1140/epjc/s10052-017-4611-5 doi (DE-627)SPR008355126 (SPR)s10052-017-4611-5-e DE-627 ger DE-627 rakwb eng 530 ASE 33.50 bkl Wang, Tianhong verfasserin aut Strong decays of %$D_{3}^{*}(2760)%$, %$D_{s3}^{*}(2860)%$, %$B_{3}^{*}%$, and %$B_{s3}^{*}%$ 2017 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier Abstract In this paper, we study the OZI-allowed two-body strong decays of %$3^-%$ heavy–light mesons. Experimentally the charmed %$D_{3}^{*}(2760)%$ and the charm–strange %$D_{s3}^{*}(2860)%$ states with these quantum numbers have been discovered. For the bottomed B(5970) state, which was found by the CDF Collaboration recently, its quantum number has not been decided yet and we assume it is a %$3^-%$ meson in this paper. The theoretical prediction for the strong decays of bottom–strange state %$B_{s3}^*%$ is also given. The relativistic wave functions of %$3^-%$ heavy mesons are constructed and their numerical values are obtained by solving the corresponding Bethe–Salpeter equation with instantaneous approximation. The transition matrix is calculated by using the PCAC and low energy theorem, following which the decay widths are obtained. For %$D_{3}^*(2760)%$ and %$D_{s3}^*(2860)%$, the total strong decay widths are 72.6 and 47.6 MeV, respectively. For %$B_3^*%$ with %$M=5978%$ MeV and %$B_{s3}^*%$ with %$M=6178%$ MeV, their strong decay widths are 22.9 and 40.8 MeV, respectively. Decay Width (dpeaa)DE-He213 LHCb Collaboration (dpeaa)DE-He213 Heavy Meson (dpeaa)DE-He213 BaBar Collaboration (dpeaa)DE-He213 Light Meson (dpeaa)DE-He213 Wang, Zhi-Hui verfasserin aut Jiang, Yue verfasserin aut Jiang, Libo verfasserin aut Wang, Guo-Li verfasserin aut Enthalten in The European physical journal Berlin : Springer, 1998 77(2017), 1 vom: 19. Jan. (DE-627)253722934 (DE-600)1459069-4 1434-6052 nnns volume:77 year:2017 number:1 day:19 month:01 https://dx.doi.org/10.1140/epjc/s10052-017-4611-5 kostenfrei Volltext GBV_USEFLAG_A SYSFLAG_A GBV_SPRINGER GBV_ILN_11 GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_39 GBV_ILN_40 GBV_ILN_60 GBV_ILN_62 GBV_ILN_63 GBV_ILN_69 GBV_ILN_70 GBV_ILN_73 GBV_ILN_95 GBV_ILN_105 GBV_ILN_110 GBV_ILN_150 GBV_ILN_151 GBV_ILN_161 GBV_ILN_170 GBV_ILN_206 GBV_ILN_213 GBV_ILN_230 GBV_ILN_267 GBV_ILN_285 GBV_ILN_293 GBV_ILN_370 GBV_ILN_602 GBV_ILN_702 GBV_ILN_2001 GBV_ILN_2003 GBV_ILN_2005 GBV_ILN_2006 GBV_ILN_2008 GBV_ILN_2009 GBV_ILN_2010 GBV_ILN_2011 GBV_ILN_2014 GBV_ILN_2015 GBV_ILN_2018 GBV_ILN_2020 GBV_ILN_2021 GBV_ILN_2025 GBV_ILN_2031 GBV_ILN_2038 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2050 GBV_ILN_2055 GBV_ILN_2056 GBV_ILN_2057 GBV_ILN_2061 GBV_ILN_2108 GBV_ILN_2111 GBV_ILN_2113 GBV_ILN_2119 GBV_ILN_2190 GBV_ILN_4012 GBV_ILN_4037 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4126 GBV_ILN_4246 GBV_ILN_4249 GBV_ILN_4305 GBV_ILN_4306 GBV_ILN_4307 GBV_ILN_4313 GBV_ILN_4322 GBV_ILN_4323 GBV_ILN_4324 GBV_ILN_4325 GBV_ILN_4335 GBV_ILN_4338 GBV_ILN_4367 GBV_ILN_4700 33.50 ASE AR 77 2017 1 19 01 |
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Strong decays of %$D_{3}^{*}(2760)%$, %$D_{s3}^{*}(2860)%$, %$B_{3}^{*}%$, and %$B_{s3}^{*}%$ |
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Strong decays of %$D_{3}^{*}(2760)%$, %$D_{s3}^{*}(2860)%$, %$B_{3}^{*}%$, and %$B_{s3}^{*}%$ |
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strong decays of %$d_{3}^{*}(2760)%$, %$d_{s3}^{*}(2860)%$, %$b_{3}^{*}%$, and %$b_{s3}^{*}%$ |
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Strong decays of %$D_{3}^{*}(2760)%$, %$D_{s3}^{*}(2860)%$, %$B_{3}^{*}%$, and %$B_{s3}^{*}%$ |
| abstract |
Abstract In this paper, we study the OZI-allowed two-body strong decays of %$3^-%$ heavy–light mesons. Experimentally the charmed %$D_{3}^{*}(2760)%$ and the charm–strange %$D_{s3}^{*}(2860)%$ states with these quantum numbers have been discovered. For the bottomed B(5970) state, which was found by the CDF Collaboration recently, its quantum number has not been decided yet and we assume it is a %$3^-%$ meson in this paper. The theoretical prediction for the strong decays of bottom–strange state %$B_{s3}^*%$ is also given. The relativistic wave functions of %$3^-%$ heavy mesons are constructed and their numerical values are obtained by solving the corresponding Bethe–Salpeter equation with instantaneous approximation. The transition matrix is calculated by using the PCAC and low energy theorem, following which the decay widths are obtained. For %$D_{3}^*(2760)%$ and %$D_{s3}^*(2860)%$, the total strong decay widths are 72.6 and 47.6 MeV, respectively. For %$B_3^*%$ with %$M=5978%$ MeV and %$B_{s3}^*%$ with %$M=6178%$ MeV, their strong decay widths are 22.9 and 40.8 MeV, respectively. |
| abstractGer |
Abstract In this paper, we study the OZI-allowed two-body strong decays of %$3^-%$ heavy–light mesons. Experimentally the charmed %$D_{3}^{*}(2760)%$ and the charm–strange %$D_{s3}^{*}(2860)%$ states with these quantum numbers have been discovered. For the bottomed B(5970) state, which was found by the CDF Collaboration recently, its quantum number has not been decided yet and we assume it is a %$3^-%$ meson in this paper. The theoretical prediction for the strong decays of bottom–strange state %$B_{s3}^*%$ is also given. The relativistic wave functions of %$3^-%$ heavy mesons are constructed and their numerical values are obtained by solving the corresponding Bethe–Salpeter equation with instantaneous approximation. The transition matrix is calculated by using the PCAC and low energy theorem, following which the decay widths are obtained. For %$D_{3}^*(2760)%$ and %$D_{s3}^*(2860)%$, the total strong decay widths are 72.6 and 47.6 MeV, respectively. For %$B_3^*%$ with %$M=5978%$ MeV and %$B_{s3}^*%$ with %$M=6178%$ MeV, their strong decay widths are 22.9 and 40.8 MeV, respectively. |
| abstract_unstemmed |
Abstract In this paper, we study the OZI-allowed two-body strong decays of %$3^-%$ heavy–light mesons. Experimentally the charmed %$D_{3}^{*}(2760)%$ and the charm–strange %$D_{s3}^{*}(2860)%$ states with these quantum numbers have been discovered. For the bottomed B(5970) state, which was found by the CDF Collaboration recently, its quantum number has not been decided yet and we assume it is a %$3^-%$ meson in this paper. The theoretical prediction for the strong decays of bottom–strange state %$B_{s3}^*%$ is also given. The relativistic wave functions of %$3^-%$ heavy mesons are constructed and their numerical values are obtained by solving the corresponding Bethe–Salpeter equation with instantaneous approximation. The transition matrix is calculated by using the PCAC and low energy theorem, following which the decay widths are obtained. For %$D_{3}^*(2760)%$ and %$D_{s3}^*(2860)%$, the total strong decay widths are 72.6 and 47.6 MeV, respectively. For %$B_3^*%$ with %$M=5978%$ MeV and %$B_{s3}^*%$ with %$M=6178%$ MeV, their strong decay widths are 22.9 and 40.8 MeV, respectively. |
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