Improved XTZ masses and mass ratios from Laplace sum rules at NLO

We present improved estimates of the couplings, masses and mass ratios of the ZQ,XQ and TQQq¯q¯′ states (Q≡c,b;q,q′≡u,d,s) using (inverse) QCD Laplace sum rules (LSR), their ratios R and double ratios DRSR within stability criteria, where the NLO factorized PT QCD corrections are included which is i...

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Veröffentlicht in:Nuclear physics. A 2022-07, Vol.1023, p.122451, Article 122451
Hauptverfasser: Albuquerque, R., Narison, S., Rabetiarivony, D.
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Narison, S.
Rabetiarivony, D.
description We present improved estimates of the couplings, masses and mass ratios of the ZQ,XQ and TQQq¯q¯′ states (Q≡c,b;q,q′≡u,d,s) using (inverse) QCD Laplace sum rules (LSR), their ratios R and double ratios DRSR within stability criteria, where the NLO factorized PT QCD corrections are included which is important for giving a meaning on the running MS‾ heavy quark mass used in the analysis. We show that combined R and DRSR can provide more precise results. In the 1st part of the paper, we conclude that the observed Xc(3872) and Zc(3900) are tetramoles states (superposition of quasi-degenerated molecule and a tetraquark states having (almost) the same coupling to the currents) with the predicted masses: MTXc=3876(44)MeV and MTZc=3900(42)MeV. In the 2nd part, we focus on the analysis of the four-quark nature of different TQQq¯q¯′1+ and 0+ states within the 3¯c3c interpolating currents. The final results from R and R⊕ DRSR are summarized in Table 7. Combined R and DRSR calibrated to the observed Xc(3872) lead to a precise prediction of e.g. MTcc1+=3886(6)MeV. In a similar way, the DRSR for the MTcc0+/MTcc1+ calibrated to MTcc1+ gives MTcc0+=3883(3)MeV. The SU3 breaking ratios MTccs¯s¯0+/MTcc0+ lead to the improved mass predictions: MTccs¯s¯0+=3988(12)MeV. In the 3rd part, the analysis is extended to the beauty mesons, where we find the tetramole masses: MTZb=10579(99)MeV and MXb=10545(131)MeV. We also observe that the Tbbq¯q¯′1+,0+ (q,q′≡u,d,s) states are (almost) stable (within the errors) against strong interactions. In the 4th part, we (critically) review and correct some recent LSR estimates of the TQQq¯q¯′1+,0+ masses. Our combined LSR ⊕ DRSR results are confronted with the ones from some other approaches (lattices and quark models) in Fig. 26.
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We show that combined R and DRSR can provide more precise results. In the 1st part of the paper, we conclude that the observed Xc(3872) and Zc(3900) are tetramoles states (superposition of quasi-degenerated molecule and a tetraquark states having (almost) the same coupling to the currents) with the predicted masses: MTXc=3876(44)MeV and MTZc=3900(42)MeV. In the 2nd part, we focus on the analysis of the four-quark nature of different TQQq¯q¯′1+ and 0+ states within the 3¯c3c interpolating currents. The final results from R and R⊕ DRSR are summarized in Table 7. Combined R and DRSR calibrated to the observed Xc(3872) lead to a precise prediction of e.g. MTcc1+=3886(6)MeV. In a similar way, the DRSR for the MTcc0+/MTcc1+ calibrated to MTcc1+ gives MTcc0+=3883(3)MeV. The SU3 breaking ratios MTccs¯s¯0+/MTcc0+ lead to the improved mass predictions: MTccs¯s¯0+=3988(12)MeV. 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A</title><description>We present improved estimates of the couplings, masses and mass ratios of the ZQ,XQ and TQQq¯q¯′ states (Q≡c,b;q,q′≡u,d,s) using (inverse) QCD Laplace sum rules (LSR), their ratios R and double ratios DRSR within stability criteria, where the NLO factorized PT QCD corrections are included which is important for giving a meaning on the running MS‾ heavy quark mass used in the analysis. We show that combined R and DRSR can provide more precise results. In the 1st part of the paper, we conclude that the observed Xc(3872) and Zc(3900) are tetramoles states (superposition of quasi-degenerated molecule and a tetraquark states having (almost) the same coupling to the currents) with the predicted masses: MTXc=3876(44)MeV and MTZc=3900(42)MeV. In the 2nd part, we focus on the analysis of the four-quark nature of different TQQq¯q¯′1+ and 0+ states within the 3¯c3c interpolating currents. The final results from R and R⊕ DRSR are summarized in Table 7. Combined R and DRSR calibrated to the observed Xc(3872) lead to a precise prediction of e.g. MTcc1+=3886(6)MeV. In a similar way, the DRSR for the MTcc0+/MTcc1+ calibrated to MTcc1+ gives MTcc0+=3883(3)MeV. The SU3 breaking ratios MTccs¯s¯0+/MTcc0+ lead to the improved mass predictions: MTccs¯s¯0+=3988(12)MeV. In the 3rd part, the analysis is extended to the beauty mesons, where we find the tetramole masses: MTZb=10579(99)MeV and MXb=10545(131)MeV. We also observe that the Tbbq¯q¯′1+,0+ (q,q′≡u,d,s) states are (almost) stable (within the errors) against strong interactions. In the 4th part, we (critically) review and correct some recent LSR estimates of the TQQq¯q¯′1+,0+ masses. 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A</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Albuquerque, R.</au><au>Narison, S.</au><au>Rabetiarivony, D.</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Improved XTZ masses and mass ratios from Laplace sum rules at NLO</atitle><jtitle>Nuclear physics. A</jtitle><date>2022-07-01</date><risdate>2022</risdate><volume>1023</volume><spage>122451</spage><pages>122451-</pages><artnum>122451</artnum><issn>0375-9474</issn><eissn>1873-1554</eissn><abstract>We present improved estimates of the couplings, masses and mass ratios of the ZQ,XQ and TQQq¯q¯′ states (Q≡c,b;q,q′≡u,d,s) using (inverse) QCD Laplace sum rules (LSR), their ratios R and double ratios DRSR within stability criteria, where the NLO factorized PT QCD corrections are included which is important for giving a meaning on the running MS‾ heavy quark mass used in the analysis. We show that combined R and DRSR can provide more precise results. In the 1st part of the paper, we conclude that the observed Xc(3872) and Zc(3900) are tetramoles states (superposition of quasi-degenerated molecule and a tetraquark states having (almost) the same coupling to the currents) with the predicted masses: MTXc=3876(44)MeV and MTZc=3900(42)MeV. In the 2nd part, we focus on the analysis of the four-quark nature of different TQQq¯q¯′1+ and 0+ states within the 3¯c3c interpolating currents. The final results from R and R⊕ DRSR are summarized in Table 7. Combined R and DRSR calibrated to the observed Xc(3872) lead to a precise prediction of e.g. MTcc1+=3886(6)MeV. In a similar way, the DRSR for the MTcc0+/MTcc1+ calibrated to MTcc1+ gives MTcc0+=3883(3)MeV. The SU3 breaking ratios MTccs¯s¯0+/MTcc0+ lead to the improved mass predictions: MTccs¯s¯0+=3988(12)MeV. In the 3rd part, the analysis is extended to the beauty mesons, where we find the tetramole masses: MTZb=10579(99)MeV and MXb=10545(131)MeV. We also observe that the Tbbq¯q¯′1+,0+ (q,q′≡u,d,s) states are (almost) stable (within the errors) against strong interactions. In the 4th part, we (critically) review and correct some recent LSR estimates of the TQQq¯q¯′1+,0+ masses. Our combined LSR ⊕ DRSR results are confronted with the ones from some other approaches (lattices and quark models) in Fig. 26.</abstract><pub>Elsevier B.V</pub><doi>10.1016/j.nuclphysa.2022.122451</doi><orcidid>https://orcid.org/0000-0002-5254-6684</orcidid><oa>free_for_read</oa></addata></record>
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subjects Exotic hadrons
High Energy Physics - Experiment
High Energy Physics - Lattice
High Energy Physics - Phenomenology
Masses and decay constants
Perturbative and non-perturbative QCD
Physics
QCD spectral sum rules
title Improved XTZ masses and mass ratios from Laplace sum rules at NLO
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