The D s0(2590)+ as the dressed c s ¯ ( 2 1 S 0 ) meson in a coupled-channels calculation
The recent discovery of the D s 0 ( 2590 ) + meson by the LHCb Collaboration has stimulated the analysis of meson-meson channels effects in the two-body quark-antiquark meson spectrum. This resonance, assigned to the radial excitation of the pseudoscalar D s + meson, has a mass much lower than the p...
Ausführliche Beschreibung
Gespeichert in:
| Autor*in: |
Ortega, Pablo G. [verfasserIn] |
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| Format: |
E-Artikel |
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| Sprache: |
Englisch |
| Erschienen: |
2022transfer abstract |
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| Übergeordnetes Werk: |
Enthalten in: Applying the Go/NoGo processing schema to a visual oddball task in older adults - Steiner, Genevieve Z. ELSEVIER, 2016, Amsterdam |
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| Übergeordnetes Werk: |
volume:827 ; year:2022 ; day:10 ; month:04 ; pages:0 |
| Links: |
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| DOI / URN: |
10.1016/j.physletb.2022.136998 |
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| 520 | |a The recent discovery of the D s 0 ( 2590 ) + meson by the LHCb Collaboration has stimulated the analysis of meson-meson channels effects in the two-body quark-antiquark meson spectrum. This resonance, assigned to the radial excitation of the pseudoscalar D s + meson, has a mass much lower than the predictions of naive quark models, which could indicate a non-negligible D ( ⁎ ) K ( ⁎ ) coupling which reduces its mass. Based on the importance of nearby meson-meson thresholds in the dynamics of P-wave D s mesons such as the D s 0 ⁎ ( 2317 ) + and D s 1 ( 2460 ) + , in this work we perform a coupled-channels calculation including the D ( ⁎ ) K ( ⁎ ) , D s ( ⁎ ) ω and D s ⁎ η channels, and study the impact of incorporating those channels in the mass of the bare c s ¯ . The coupling between two and four-quark sectors is done by means of the P 0 3 mechanism, with all the parameters constrained from previous studies of the heavy meson spectroscopy. The masses, widths and production line shapes of the resulting state are analyzed. | ||
| 520 | |a The recent discovery of the D s 0 ( 2590 ) + meson by the LHCb Collaboration has stimulated the analysis of meson-meson channels effects in the two-body quark-antiquark meson spectrum. This resonance, assigned to the radial excitation of the pseudoscalar D s + meson, has a mass much lower than the predictions of naive quark models, which could indicate a non-negligible D ( ⁎ ) K ( ⁎ ) coupling which reduces its mass. Based on the importance of nearby meson-meson thresholds in the dynamics of P-wave D s mesons such as the D s 0 ⁎ ( 2317 ) + and D s 1 ( 2460 ) + , in this work we perform a coupled-channels calculation including the D ( ⁎ ) K ( ⁎ ) , D s ( ⁎ ) ω and D s ⁎ η channels, and study the impact of incorporating those channels in the mass of the bare c s ¯ . The coupling between two and four-quark sectors is done by means of the P 0 3 mechanism, with all the parameters constrained from previous studies of the heavy meson spectroscopy. The masses, widths and production line shapes of the resulting state are analyzed. | ||
| 650 | 7 | |a Potential models |2 Elsevier | |
| 650 | 7 | |a Coupled-channels calculation |2 Elsevier | |
| 650 | 7 | |a Charmed strange mesons |2 Elsevier | |
| 650 | 7 | |a Quark models |2 Elsevier | |
| 700 | 1 | |a Segovia, Jorge |4 oth | |
| 700 | 1 | |a Entem, David R. |4 oth | |
| 700 | 1 | |a Fernández, Francisco |4 oth | |
| 773 | 0 | 8 | |i Enthalten in |n North-Holland Publ |a Steiner, Genevieve Z. ELSEVIER |t Applying the Go/NoGo processing schema to a visual oddball task in older adults |d 2016 |g Amsterdam |w (DE-627)ELV000151122 |
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10.1016/j.physletb.2022.136998 doi /cbs_pica/cbs_olc/import_discovery/elsevier/einzuspielen/GBV00000000001715.pica (DE-627)ELV057206724 (ELSEVIER)S0370-2693(22)00132-0 DE-627 ger DE-627 rakwb eng 610 VZ 77.50 bkl Ortega, Pablo G. verfasserin aut The D s0(2590)+ as the dressed c s ¯ ( 2 1 S 0 ) meson in a coupled-channels calculation 2022transfer abstract nicht spezifiziert zzz rdacontent nicht spezifiziert z rdamedia nicht spezifiziert zu rdacarrier The recent discovery of the D s 0 ( 2590 ) + meson by the LHCb Collaboration has stimulated the analysis of meson-meson channels effects in the two-body quark-antiquark meson spectrum. This resonance, assigned to the radial excitation of the pseudoscalar D s + meson, has a mass much lower than the predictions of naive quark models, which could indicate a non-negligible D ( ⁎ ) K ( ⁎ ) coupling which reduces its mass. Based on the importance of nearby meson-meson thresholds in the dynamics of P-wave D s mesons such as the D s 0 ⁎ ( 2317 ) + and D s 1 ( 2460 ) + , in this work we perform a coupled-channels calculation including the D ( ⁎ ) K ( ⁎ ) , D s ( ⁎ ) ω and D s ⁎ η channels, and study the impact of incorporating those channels in the mass of the bare c s ¯ . The coupling between two and four-quark sectors is done by means of the P 0 3 mechanism, with all the parameters constrained from previous studies of the heavy meson spectroscopy. The masses, widths and production line shapes of the resulting state are analyzed. The recent discovery of the D s 0 ( 2590 ) + meson by the LHCb Collaboration has stimulated the analysis of meson-meson channels effects in the two-body quark-antiquark meson spectrum. This resonance, assigned to the radial excitation of the pseudoscalar D s + meson, has a mass much lower than the predictions of naive quark models, which could indicate a non-negligible D ( ⁎ ) K ( ⁎ ) coupling which reduces its mass. Based on the importance of nearby meson-meson thresholds in the dynamics of P-wave D s mesons such as the D s 0 ⁎ ( 2317 ) + and D s 1 ( 2460 ) + , in this work we perform a coupled-channels calculation including the D ( ⁎ ) K ( ⁎ ) , D s ( ⁎ ) ω and D s ⁎ η channels, and study the impact of incorporating those channels in the mass of the bare c s ¯ . The coupling between two and four-quark sectors is done by means of the P 0 3 mechanism, with all the parameters constrained from previous studies of the heavy meson spectroscopy. The masses, widths and production line shapes of the resulting state are analyzed. Potential models Elsevier Coupled-channels calculation Elsevier Charmed strange mesons Elsevier Quark models Elsevier Segovia, Jorge oth Entem, David R. oth Fernández, Francisco oth Enthalten in North-Holland Publ Steiner, Genevieve Z. ELSEVIER Applying the Go/NoGo processing schema to a visual oddball task in older adults 2016 Amsterdam (DE-627)ELV000151122 volume:827 year:2022 day:10 month:04 pages:0 https://doi.org/10.1016/j.physletb.2022.136998 Volltext GBV_USEFLAG_U GBV_ELV SYSFLAG_U SSG-OLC-PHA 77.50 Psychophysiologie VZ AR 827 2022 10 0410 0 |
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10.1016/j.physletb.2022.136998 doi /cbs_pica/cbs_olc/import_discovery/elsevier/einzuspielen/GBV00000000001715.pica (DE-627)ELV057206724 (ELSEVIER)S0370-2693(22)00132-0 DE-627 ger DE-627 rakwb eng 610 VZ 77.50 bkl Ortega, Pablo G. verfasserin aut The D s0(2590)+ as the dressed c s ¯ ( 2 1 S 0 ) meson in a coupled-channels calculation 2022transfer abstract nicht spezifiziert zzz rdacontent nicht spezifiziert z rdamedia nicht spezifiziert zu rdacarrier The recent discovery of the D s 0 ( 2590 ) + meson by the LHCb Collaboration has stimulated the analysis of meson-meson channels effects in the two-body quark-antiquark meson spectrum. This resonance, assigned to the radial excitation of the pseudoscalar D s + meson, has a mass much lower than the predictions of naive quark models, which could indicate a non-negligible D ( ⁎ ) K ( ⁎ ) coupling which reduces its mass. Based on the importance of nearby meson-meson thresholds in the dynamics of P-wave D s mesons such as the D s 0 ⁎ ( 2317 ) + and D s 1 ( 2460 ) + , in this work we perform a coupled-channels calculation including the D ( ⁎ ) K ( ⁎ ) , D s ( ⁎ ) ω and D s ⁎ η channels, and study the impact of incorporating those channels in the mass of the bare c s ¯ . The coupling between two and four-quark sectors is done by means of the P 0 3 mechanism, with all the parameters constrained from previous studies of the heavy meson spectroscopy. The masses, widths and production line shapes of the resulting state are analyzed. The recent discovery of the D s 0 ( 2590 ) + meson by the LHCb Collaboration has stimulated the analysis of meson-meson channels effects in the two-body quark-antiquark meson spectrum. This resonance, assigned to the radial excitation of the pseudoscalar D s + meson, has a mass much lower than the predictions of naive quark models, which could indicate a non-negligible D ( ⁎ ) K ( ⁎ ) coupling which reduces its mass. Based on the importance of nearby meson-meson thresholds in the dynamics of P-wave D s mesons such as the D s 0 ⁎ ( 2317 ) + and D s 1 ( 2460 ) + , in this work we perform a coupled-channels calculation including the D ( ⁎ ) K ( ⁎ ) , D s ( ⁎ ) ω and D s ⁎ η channels, and study the impact of incorporating those channels in the mass of the bare c s ¯ . The coupling between two and four-quark sectors is done by means of the P 0 3 mechanism, with all the parameters constrained from previous studies of the heavy meson spectroscopy. The masses, widths and production line shapes of the resulting state are analyzed. Potential models Elsevier Coupled-channels calculation Elsevier Charmed strange mesons Elsevier Quark models Elsevier Segovia, Jorge oth Entem, David R. oth Fernández, Francisco oth Enthalten in North-Holland Publ Steiner, Genevieve Z. ELSEVIER Applying the Go/NoGo processing schema to a visual oddball task in older adults 2016 Amsterdam (DE-627)ELV000151122 volume:827 year:2022 day:10 month:04 pages:0 https://doi.org/10.1016/j.physletb.2022.136998 Volltext GBV_USEFLAG_U GBV_ELV SYSFLAG_U SSG-OLC-PHA 77.50 Psychophysiologie VZ AR 827 2022 10 0410 0 |
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10.1016/j.physletb.2022.136998 doi /cbs_pica/cbs_olc/import_discovery/elsevier/einzuspielen/GBV00000000001715.pica (DE-627)ELV057206724 (ELSEVIER)S0370-2693(22)00132-0 DE-627 ger DE-627 rakwb eng 610 VZ 77.50 bkl Ortega, Pablo G. verfasserin aut The D s0(2590)+ as the dressed c s ¯ ( 2 1 S 0 ) meson in a coupled-channels calculation 2022transfer abstract nicht spezifiziert zzz rdacontent nicht spezifiziert z rdamedia nicht spezifiziert zu rdacarrier The recent discovery of the D s 0 ( 2590 ) + meson by the LHCb Collaboration has stimulated the analysis of meson-meson channels effects in the two-body quark-antiquark meson spectrum. This resonance, assigned to the radial excitation of the pseudoscalar D s + meson, has a mass much lower than the predictions of naive quark models, which could indicate a non-negligible D ( ⁎ ) K ( ⁎ ) coupling which reduces its mass. Based on the importance of nearby meson-meson thresholds in the dynamics of P-wave D s mesons such as the D s 0 ⁎ ( 2317 ) + and D s 1 ( 2460 ) + , in this work we perform a coupled-channels calculation including the D ( ⁎ ) K ( ⁎ ) , D s ( ⁎ ) ω and D s ⁎ η channels, and study the impact of incorporating those channels in the mass of the bare c s ¯ . The coupling between two and four-quark sectors is done by means of the P 0 3 mechanism, with all the parameters constrained from previous studies of the heavy meson spectroscopy. The masses, widths and production line shapes of the resulting state are analyzed. The recent discovery of the D s 0 ( 2590 ) + meson by the LHCb Collaboration has stimulated the analysis of meson-meson channels effects in the two-body quark-antiquark meson spectrum. This resonance, assigned to the radial excitation of the pseudoscalar D s + meson, has a mass much lower than the predictions of naive quark models, which could indicate a non-negligible D ( ⁎ ) K ( ⁎ ) coupling which reduces its mass. Based on the importance of nearby meson-meson thresholds in the dynamics of P-wave D s mesons such as the D s 0 ⁎ ( 2317 ) + and D s 1 ( 2460 ) + , in this work we perform a coupled-channels calculation including the D ( ⁎ ) K ( ⁎ ) , D s ( ⁎ ) ω and D s ⁎ η channels, and study the impact of incorporating those channels in the mass of the bare c s ¯ . The coupling between two and four-quark sectors is done by means of the P 0 3 mechanism, with all the parameters constrained from previous studies of the heavy meson spectroscopy. The masses, widths and production line shapes of the resulting state are analyzed. Potential models Elsevier Coupled-channels calculation Elsevier Charmed strange mesons Elsevier Quark models Elsevier Segovia, Jorge oth Entem, David R. oth Fernández, Francisco oth Enthalten in North-Holland Publ Steiner, Genevieve Z. ELSEVIER Applying the Go/NoGo processing schema to a visual oddball task in older adults 2016 Amsterdam (DE-627)ELV000151122 volume:827 year:2022 day:10 month:04 pages:0 https://doi.org/10.1016/j.physletb.2022.136998 Volltext GBV_USEFLAG_U GBV_ELV SYSFLAG_U SSG-OLC-PHA 77.50 Psychophysiologie VZ AR 827 2022 10 0410 0 |
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10.1016/j.physletb.2022.136998 doi /cbs_pica/cbs_olc/import_discovery/elsevier/einzuspielen/GBV00000000001715.pica (DE-627)ELV057206724 (ELSEVIER)S0370-2693(22)00132-0 DE-627 ger DE-627 rakwb eng 610 VZ 77.50 bkl Ortega, Pablo G. verfasserin aut The D s0(2590)+ as the dressed c s ¯ ( 2 1 S 0 ) meson in a coupled-channels calculation 2022transfer abstract nicht spezifiziert zzz rdacontent nicht spezifiziert z rdamedia nicht spezifiziert zu rdacarrier The recent discovery of the D s 0 ( 2590 ) + meson by the LHCb Collaboration has stimulated the analysis of meson-meson channels effects in the two-body quark-antiquark meson spectrum. This resonance, assigned to the radial excitation of the pseudoscalar D s + meson, has a mass much lower than the predictions of naive quark models, which could indicate a non-negligible D ( ⁎ ) K ( ⁎ ) coupling which reduces its mass. Based on the importance of nearby meson-meson thresholds in the dynamics of P-wave D s mesons such as the D s 0 ⁎ ( 2317 ) + and D s 1 ( 2460 ) + , in this work we perform a coupled-channels calculation including the D ( ⁎ ) K ( ⁎ ) , D s ( ⁎ ) ω and D s ⁎ η channels, and study the impact of incorporating those channels in the mass of the bare c s ¯ . The coupling between two and four-quark sectors is done by means of the P 0 3 mechanism, with all the parameters constrained from previous studies of the heavy meson spectroscopy. The masses, widths and production line shapes of the resulting state are analyzed. The recent discovery of the D s 0 ( 2590 ) + meson by the LHCb Collaboration has stimulated the analysis of meson-meson channels effects in the two-body quark-antiquark meson spectrum. This resonance, assigned to the radial excitation of the pseudoscalar D s + meson, has a mass much lower than the predictions of naive quark models, which could indicate a non-negligible D ( ⁎ ) K ( ⁎ ) coupling which reduces its mass. Based on the importance of nearby meson-meson thresholds in the dynamics of P-wave D s mesons such as the D s 0 ⁎ ( 2317 ) + and D s 1 ( 2460 ) + , in this work we perform a coupled-channels calculation including the D ( ⁎ ) K ( ⁎ ) , D s ( ⁎ ) ω and D s ⁎ η channels, and study the impact of incorporating those channels in the mass of the bare c s ¯ . The coupling between two and four-quark sectors is done by means of the P 0 3 mechanism, with all the parameters constrained from previous studies of the heavy meson spectroscopy. The masses, widths and production line shapes of the resulting state are analyzed. Potential models Elsevier Coupled-channels calculation Elsevier Charmed strange mesons Elsevier Quark models Elsevier Segovia, Jorge oth Entem, David R. oth Fernández, Francisco oth Enthalten in North-Holland Publ Steiner, Genevieve Z. ELSEVIER Applying the Go/NoGo processing schema to a visual oddball task in older adults 2016 Amsterdam (DE-627)ELV000151122 volume:827 year:2022 day:10 month:04 pages:0 https://doi.org/10.1016/j.physletb.2022.136998 Volltext GBV_USEFLAG_U GBV_ELV SYSFLAG_U SSG-OLC-PHA 77.50 Psychophysiologie VZ AR 827 2022 10 0410 0 |
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10.1016/j.physletb.2022.136998 doi /cbs_pica/cbs_olc/import_discovery/elsevier/einzuspielen/GBV00000000001715.pica (DE-627)ELV057206724 (ELSEVIER)S0370-2693(22)00132-0 DE-627 ger DE-627 rakwb eng 610 VZ 77.50 bkl Ortega, Pablo G. verfasserin aut The D s0(2590)+ as the dressed c s ¯ ( 2 1 S 0 ) meson in a coupled-channels calculation 2022transfer abstract nicht spezifiziert zzz rdacontent nicht spezifiziert z rdamedia nicht spezifiziert zu rdacarrier The recent discovery of the D s 0 ( 2590 ) + meson by the LHCb Collaboration has stimulated the analysis of meson-meson channels effects in the two-body quark-antiquark meson spectrum. This resonance, assigned to the radial excitation of the pseudoscalar D s + meson, has a mass much lower than the predictions of naive quark models, which could indicate a non-negligible D ( ⁎ ) K ( ⁎ ) coupling which reduces its mass. Based on the importance of nearby meson-meson thresholds in the dynamics of P-wave D s mesons such as the D s 0 ⁎ ( 2317 ) + and D s 1 ( 2460 ) + , in this work we perform a coupled-channels calculation including the D ( ⁎ ) K ( ⁎ ) , D s ( ⁎ ) ω and D s ⁎ η channels, and study the impact of incorporating those channels in the mass of the bare c s ¯ . The coupling between two and four-quark sectors is done by means of the P 0 3 mechanism, with all the parameters constrained from previous studies of the heavy meson spectroscopy. The masses, widths and production line shapes of the resulting state are analyzed. The recent discovery of the D s 0 ( 2590 ) + meson by the LHCb Collaboration has stimulated the analysis of meson-meson channels effects in the two-body quark-antiquark meson spectrum. This resonance, assigned to the radial excitation of the pseudoscalar D s + meson, has a mass much lower than the predictions of naive quark models, which could indicate a non-negligible D ( ⁎ ) K ( ⁎ ) coupling which reduces its mass. Based on the importance of nearby meson-meson thresholds in the dynamics of P-wave D s mesons such as the D s 0 ⁎ ( 2317 ) + and D s 1 ( 2460 ) + , in this work we perform a coupled-channels calculation including the D ( ⁎ ) K ( ⁎ ) , D s ( ⁎ ) ω and D s ⁎ η channels, and study the impact of incorporating those channels in the mass of the bare c s ¯ . The coupling between two and four-quark sectors is done by means of the P 0 3 mechanism, with all the parameters constrained from previous studies of the heavy meson spectroscopy. The masses, widths and production line shapes of the resulting state are analyzed. Potential models Elsevier Coupled-channels calculation Elsevier Charmed strange mesons Elsevier Quark models Elsevier Segovia, Jorge oth Entem, David R. oth Fernández, Francisco oth Enthalten in North-Holland Publ Steiner, Genevieve Z. ELSEVIER Applying the Go/NoGo processing schema to a visual oddball task in older adults 2016 Amsterdam (DE-627)ELV000151122 volume:827 year:2022 day:10 month:04 pages:0 https://doi.org/10.1016/j.physletb.2022.136998 Volltext GBV_USEFLAG_U GBV_ELV SYSFLAG_U SSG-OLC-PHA 77.50 Psychophysiologie VZ AR 827 2022 10 0410 0 |
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Enthalten in Applying the Go/NoGo processing schema to a visual oddball task in older adults Amsterdam volume:827 year:2022 day:10 month:04 pages:0 |
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This resonance, assigned to the radial excitation of the pseudoscalar D s + meson, has a mass much lower than the predictions of naive quark models, which could indicate a non-negligible D ( ⁎ ) K ( ⁎ ) coupling which reduces its mass. Based on the importance of nearby meson-meson thresholds in the dynamics of P-wave D s mesons such as the D s 0 ⁎ ( 2317 ) + and D s 1 ( 2460 ) + , in this work we perform a coupled-channels calculation including the D ( ⁎ ) K ( ⁎ ) , D s ( ⁎ ) ω and D s ⁎ η channels, and study the impact of incorporating those channels in the mass of the bare c s ¯ . The coupling between two and four-quark sectors is done by means of the P 0 3 mechanism, with all the parameters constrained from previous studies of the heavy meson spectroscopy. 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Applying the Go/NoGo processing schema to a visual oddball task in older adults |
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d s0(2590)+ as the dressed c s ¯ ( 2 1 s 0 ) meson in a coupled-channels calculation |
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The D s0(2590)+ as the dressed c s ¯ ( 2 1 S 0 ) meson in a coupled-channels calculation |
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The recent discovery of the D s 0 ( 2590 ) + meson by the LHCb Collaboration has stimulated the analysis of meson-meson channels effects in the two-body quark-antiquark meson spectrum. This resonance, assigned to the radial excitation of the pseudoscalar D s + meson, has a mass much lower than the predictions of naive quark models, which could indicate a non-negligible D ( ⁎ ) K ( ⁎ ) coupling which reduces its mass. Based on the importance of nearby meson-meson thresholds in the dynamics of P-wave D s mesons such as the D s 0 ⁎ ( 2317 ) + and D s 1 ( 2460 ) + , in this work we perform a coupled-channels calculation including the D ( ⁎ ) K ( ⁎ ) , D s ( ⁎ ) ω and D s ⁎ η channels, and study the impact of incorporating those channels in the mass of the bare c s ¯ . The coupling between two and four-quark sectors is done by means of the P 0 3 mechanism, with all the parameters constrained from previous studies of the heavy meson spectroscopy. The masses, widths and production line shapes of the resulting state are analyzed. |
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The recent discovery of the D s 0 ( 2590 ) + meson by the LHCb Collaboration has stimulated the analysis of meson-meson channels effects in the two-body quark-antiquark meson spectrum. This resonance, assigned to the radial excitation of the pseudoscalar D s + meson, has a mass much lower than the predictions of naive quark models, which could indicate a non-negligible D ( ⁎ ) K ( ⁎ ) coupling which reduces its mass. Based on the importance of nearby meson-meson thresholds in the dynamics of P-wave D s mesons such as the D s 0 ⁎ ( 2317 ) + and D s 1 ( 2460 ) + , in this work we perform a coupled-channels calculation including the D ( ⁎ ) K ( ⁎ ) , D s ( ⁎ ) ω and D s ⁎ η channels, and study the impact of incorporating those channels in the mass of the bare c s ¯ . The coupling between two and four-quark sectors is done by means of the P 0 3 mechanism, with all the parameters constrained from previous studies of the heavy meson spectroscopy. The masses, widths and production line shapes of the resulting state are analyzed. |
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The recent discovery of the D s 0 ( 2590 ) + meson by the LHCb Collaboration has stimulated the analysis of meson-meson channels effects in the two-body quark-antiquark meson spectrum. This resonance, assigned to the radial excitation of the pseudoscalar D s + meson, has a mass much lower than the predictions of naive quark models, which could indicate a non-negligible D ( ⁎ ) K ( ⁎ ) coupling which reduces its mass. Based on the importance of nearby meson-meson thresholds in the dynamics of P-wave D s mesons such as the D s 0 ⁎ ( 2317 ) + and D s 1 ( 2460 ) + , in this work we perform a coupled-channels calculation including the D ( ⁎ ) K ( ⁎ ) , D s ( ⁎ ) ω and D s ⁎ η channels, and study the impact of incorporating those channels in the mass of the bare c s ¯ . The coupling between two and four-quark sectors is done by means of the P 0 3 mechanism, with all the parameters constrained from previous studies of the heavy meson spectroscopy. The masses, widths and production line shapes of the resulting state are analyzed. |
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The D s0(2590)+ as the dressed c s ¯ ( 2 1 S 0 ) meson in a coupled-channels calculation |
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Segovia, Jorge Entem, David R. Fernández, Francisco |
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