Phenomenological study of heavy hadron lifetimes
A bstract The lifetimes of bottom and charmed hadrons are analyzed within the framework of the heavy quark expansion (HQE). Lifetime differences arise from the spectator effects such as weak W -annihilation and Pauli interference. Spectator effects originating from dimension-7 four-quark operators a...
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| Published in | The journal of high energy physics Vol. 2018; no. 11; pp. 1 - 44 |
|---|---|
| Main Author | |
| Format | Journal Article |
| Language | English |
| Published |
Berlin/Heidelberg
Springer Berlin Heidelberg
01.11.2018
Springer Nature B.V SpringerOpen |
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| Abstract | A
bstract
The lifetimes of bottom and charmed hadrons are analyzed within the framework of the heavy quark expansion (HQE). Lifetime differences arise from the spectator effects such as weak
W
-annihilation and Pauli interference. Spectator effects originating from dimension-7 four-quark operators are derived. Hadronic matrix elements of four-quark operators are parameterized in a model-independent way. Using the dimension-6 bag parameters recently determined from HQET sum rules and the vacuum insertion approximation for meson matrix elements of dimension-7 operators, the calculated
B
meson lifetime ratios
τ
(
B
+
)/
τ
(
B
d
0
) = 1.074
− 0.016
+ 0.017
and
τ
(
B
s
0
)/
τ
(
B
d
0
) = 0.9962 ± 0.0024 are in excellent agreement with experiment. Likewise, based on the quark model evaluation of baryon matrix elements, the resulting baryon lifetime ratios
τ
(Ξ
b
−
)/
τ
(Λ
b
0
),
τ
(Ξ
b
−
)/
τ
(
Ξ
b
0
),
τ
(Ω
b
−
)/
τ
(
Ξ
b
−
) and the Λ
b
−
B
0
lifetime ratio
τ
(Λ
b
0
)/
τ
(
B
d
0
) = 0.953 also agree well with the data. Contrary to the bottom hadron sector where the HQE in 1/
m
b
works well, the HQE to 1/
m
c
3
fails to give a satisfactory description of the lifetimes of both charmed mesons and charmed baryons. This calls for the subleading 1/
m
Q
corrections to spectator effects. The relevant dimension-7 spectator effects are in the right direction for explaining the large lifetime ratio of
τ
(Ξ
c
+
)/
τ
(Λ
c
+
). However, the destructive 1/
m
c
corrections to Γ(Ω
c
0
) are too large to justify the validity of the HQE, namely, the predicted Pauli interference and semileptonic rates for Ω
c
0
become negative. Demanding these rates to be positive for a sensible HQE, we find the lifetime pattern
τ
(Ξ
c
+
) >
τ
(
Ω
c
0
) >
τ
(Λ
c
+
) >
τ
(Ξ
c
0
), contrary to the current hierarchy
τ
(Ξ
c
+
) >
τ
(Λ
c
+
) >
τ
(Ξ
c
0
) >
τ
(
Ω
c
0
). We conclude that the Ω
c
0
, which is naively expected to be shortest-lived in the charmed baryon system owing to the large constructive Pauli interference, could live longer than the Λ
c
+
due to the suppression from 1/
m
c
corrections arising from dimension-7 four-quark operators. The new charmed baryon lifetime pattern needs to be tested in forthcoming experiments. |
|---|---|
| AbstractList | The lifetimes of bottom and charmed hadrons are analyzed within the framework of the heavy quark expansion (HQE). Lifetime differences arise from the spectator effects such as weak W-annihilation and Pauli interference. Spectator effects originating from dimension-7 four-quark operators are derived. Hadronic matrix elements of four-quark operators are parameterized in a model-independent way. Using the dimension-6 bag parameters recently determined from HQET sum rules and the vacuum insertion approximation for meson matrix elements of dimension-7 operators, the calculated B meson lifetime ratios τ(B+)/τ(Bd0) = 1.074− 0.016+ 0.017 and τ(Bs0)/τ(Bd0) = 0.9962 ± 0.0024 are in excellent agreement with experiment. Likewise, based on the quark model evaluation of baryon matrix elements, the resulting baryon lifetime ratios τ(Ξb−)/τ(Λb0), τ(Ξb−)/τ(Ξb0), τ(Ωb−)/τ(Ξb−) and the Λb − B0 lifetime ratio τ(Λb0)/τ(Bd0) = 0.953 also agree well with the data. Contrary to the bottom hadron sector where the HQE in 1/mb works well, the HQE to 1/mc3 fails to give a satisfactory description of the lifetimes of both charmed mesons and charmed baryons. This calls for the subleading 1/mQ corrections to spectator effects. The relevant dimension-7 spectator effects are in the right direction for explaining the large lifetime ratio of τ(Ξc+)/τ(Λc+). However, the destructive 1/mc corrections to Γ(Ωc0) are too large to justify the validity of the HQE, namely, the predicted Pauli interference and semileptonic rates for Ωc0 become negative. Demanding these rates to be positive for a sensible HQE, we find the lifetime pattern τ(Ξc+) > τ(Ωc0) > τ(Λc+) > τ(Ξc0), contrary to the current hierarchy τ(Ξc+) > τ(Λc+) > τ(Ξc0) > τ(Ωc0). We conclude that the Ωc0, which is naively expected to be shortest-lived in the charmed baryon system owing to the large constructive Pauli interference, could live longer than the Λc+ due to the suppression from 1/mc corrections arising from dimension-7 four-quark operators. The new charmed baryon lifetime pattern needs to be tested in forthcoming experiments. A bstract The lifetimes of bottom and charmed hadrons are analyzed within the framework of the heavy quark expansion (HQE). Lifetime differences arise from the spectator effects such as weak W -annihilation and Pauli interference. Spectator effects originating from dimension-7 four-quark operators are derived. Hadronic matrix elements of four-quark operators are parameterized in a model-independent way. Using the dimension-6 bag parameters recently determined from HQET sum rules and the vacuum insertion approximation for meson matrix elements of dimension-7 operators, the calculated B meson lifetime ratios τ ( B + )/ τ ( B d 0 ) = 1.074 − 0.016 + 0.017 and τ ( B s 0 )/ τ ( B d 0 ) = 0.9962 ± 0.0024 are in excellent agreement with experiment. Likewise, based on the quark model evaluation of baryon matrix elements, the resulting baryon lifetime ratios τ (Ξ b − )/ τ (Λ b 0 ), τ (Ξ b − )/ τ ( Ξ b 0 ), τ (Ω b − )/ τ ( Ξ b − ) and the Λ b − B 0 lifetime ratio τ (Λ b 0 )/ τ ( B d 0 ) = 0.953 also agree well with the data. Contrary to the bottom hadron sector where the HQE in 1/ m b works well, the HQE to 1/ m c 3 fails to give a satisfactory description of the lifetimes of both charmed mesons and charmed baryons. This calls for the subleading 1/ m Q corrections to spectator effects. The relevant dimension-7 spectator effects are in the right direction for explaining the large lifetime ratio of τ (Ξ c + )/ τ (Λ c + ). However, the destructive 1/ m c corrections to Γ(Ω c 0 ) are too large to justify the validity of the HQE, namely, the predicted Pauli interference and semileptonic rates for Ω c 0 become negative. Demanding these rates to be positive for a sensible HQE, we find the lifetime pattern τ (Ξ c + ) > τ ( Ω c 0 ) > τ (Λ c + ) > τ (Ξ c 0 ), contrary to the current hierarchy τ (Ξ c + ) > τ (Λ c + ) > τ (Ξ c 0 ) > τ ( Ω c 0 ). We conclude that the Ω c 0 , which is naively expected to be shortest-lived in the charmed baryon system owing to the large constructive Pauli interference, could live longer than the Λ c + due to the suppression from 1/ m c corrections arising from dimension-7 four-quark operators. The new charmed baryon lifetime pattern needs to be tested in forthcoming experiments. Abstract The lifetimes of bottom and charmed hadrons are analyzed within the framework of the heavy quark expansion (HQE). Lifetime differences arise from the spectator effects such as weak W-annihilation and Pauli interference. Spectator effects originating from dimension-7 four-quark operators are derived. Hadronic matrix elements of four-quark operators are parameterized in a model-independent way. Using the dimension-6 bag parameters recently determined from HQET sum rules and the vacuum insertion approximation for meson matrix elements of dimension-7 operators, the calculated B meson lifetime ratios τ(B +)/τ(B d 0 ) = 1.074 − 0.016 + 0.017 and τ(B s 0 )/τ(B d 0 ) = 0.9962 ± 0.0024 are in excellent agreement with experiment. Likewise, based on the quark model evaluation of baryon matrix elements, the resulting baryon lifetime ratios τ(Ξ b − )/τ(Λ b 0 ), τ(Ξ b − )/τ(Ξ b 0 ), τ(Ω b − )/τ(Ξ b − ) and the Λ b − B 0 lifetime ratio τ(Λ b 0 )/τ(B d 0 ) = 0.953 also agree well with the data. Contrary to the bottom hadron sector where the HQE in 1/m b works well, the HQE to 1/m c 3 fails to give a satisfactory description of the lifetimes of both charmed mesons and charmed baryons. This calls for the subleading 1/m Q corrections to spectator effects. The relevant dimension-7 spectator effects are in the right direction for explaining the large lifetime ratio of τ(Ξ c + )/τ(Λ c + ). However, the destructive 1/m c corrections to Γ(Ω c 0 ) are too large to justify the validity of the HQE, namely, the predicted Pauli interference and semileptonic rates for Ω c 0 become negative. Demanding these rates to be positive for a sensible HQE, we find the lifetime pattern τ(Ξ c + ) > τ(Ω c 0 ) > τ(Λ c + ) > τ(Ξ c 0 ), contrary to the current hierarchy τ(Ξ c + ) > τ(Λ c + ) > τ(Ξ c 0 ) > τ(Ω c 0 ). We conclude that the Ω c 0 , which is naively expected to be shortest-lived in the charmed baryon system owing to the large constructive Pauli interference, could live longer than the Λ c + due to the suppression from 1/m c corrections arising from dimension-7 four-quark operators. The new charmed baryon lifetime pattern needs to be tested in forthcoming experiments. The lifetimes of bottom and charmed hadrons are analyzed within the framework of the heavy quark expansion (HQE). Lifetime differences arise from the spectator effects such as weak W -annihilation and Pauli interference. Spectator effects originating from dimension-7 four-quark operators are derived. Hadronic matrix elements of four-quark operators are parameterized in a model-independent way. Using the dimension-6 bag parameters recently determined from HQET sum rules and the vacuum insertion approximation for meson matrix elements of dimension-7 operators, the calculated B meson lifetime ratios τ ( B + )/ τ ( B d 0 ) = 1.074 − 0.016 + 0.017 and τ ( B s 0 )/ τ ( B d 0 ) = 0.9962 ± 0.0024 are in excellent agreement with experiment. Likewise, based on the quark model evaluation of baryon matrix elements, the resulting baryon lifetime ratios τ (Ξ b − )/ τ (Λ b 0 ), τ (Ξ b − )/ τ ( Ξ b 0 ), τ (Ω b − )/ τ ( Ξ b − ) and the Λ b − B 0 lifetime ratio τ (Λ b 0 )/ τ ( B d 0 ) = 0.953 also agree well with the data. Contrary to the bottom hadron sector where the HQE in 1/ m b works well, the HQE to 1/ m c 3 fails to give a satisfactory description of the lifetimes of both charmed mesons and charmed baryons. This calls for the subleading 1/ m Q corrections to spectator effects. The relevant dimension-7 spectator effects are in the right direction for explaining the large lifetime ratio of τ (Ξ c + )/ τ (Λ c + ). However, the destructive 1/ m c corrections to Γ(Ω c 0 ) are too large to justify the validity of the HQE, namely, the predicted Pauli interference and semileptonic rates for Ω c 0 become negative. Demanding these rates to be positive for a sensible HQE, we find the lifetime pattern τ (Ξ c + ) > τ ( Ω c 0 ) > τ (Λ c + ) > τ (Ξ c 0 ), contrary to the current hierarchy τ (Ξ c + ) > τ (Λ c + ) > τ (Ξ c 0 ) > τ ( Ω c 0 ). We conclude that the Ω c 0 , which is naively expected to be shortest-lived in the charmed baryon system owing to the large constructive Pauli interference, could live longer than the Λ c + due to the suppression from 1/ m c corrections arising from dimension-7 four-quark operators. The new charmed baryon lifetime pattern needs to be tested in forthcoming experiments. |
| ArticleNumber | 14 |
| Author | Cheng, Hai-Yang |
| Author_xml | – sequence: 1 givenname: Hai-Yang surname: Cheng fullname: Cheng, Hai-Yang email: phcheng@phys.sinica.edu.tw organization: Institute of Physics, Academia Sinica |
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| Cites_doi | 10.1103/PhysRevD.70.094031 10.1016/0550-3213(93)90504-I 10.1088/1126-6708/2007/12/062 10.1016/S0550-3213(02)00561-8 10.1142/S0217751X15430058 10.1016/0370-2693(96)00637-5 10.1016/0370-2693(92)90908-M 10.1103/PhysRevD.20.1739 10.1016/0370-2693(90)90568-Q 10.1103/PhysRevD.46.1042 10.1016/S0370-2693(00)00620-1 10.1142/S0217751X96001966 10.1016/0370-2693(96)00352-8 10.1007/JHEP11(2010)109 10.1016/0370-2693(90)90916-T 10.1016/S0550-3213(96)00559-7 10.1016/j.nuclphysb.2017.05.016 10.1016/0003-4916(76)90069-5 10.1088/1126-6708/2009/02/047 10.1007/JHEP01(2014)147 10.1016/S0370-1573(97)00005-7 10.1103/PhysRevLett.44.10 10.1103/PhysRevD.70.117501 10.1016/0370-2693(96)00837-4 10.1103/PhysRevD.68.114006 10.1103/PhysRevD.54.4419 10.1103/RevModPhys.68.1125 10.1103/PhysRevD.65.114004 10.1016/0370-2693(96)01049-0 10.1103/PhysRevD.54.4515 10.1007/BF01620717 10.22323/1.007.0098 10.1016/0003-4916(76)90021-X 10.1016/0550-3213(93)90505-J 10.1016/j.physletb.2016.10.023 10.1103/PhysRevD.56.2783 10.1103/PhysRevD.59.014011 10.1103/PhysRevD.52.196 10.1103/PhysRevLett.82.277 10.1103/PhysRevD.55.R10 10.1016/0370-2693(79)90086-8 10.1016/0550-3213(84)90596-0 10.1016/j.nuclphysb.2013.01.005 10.1016/0550-3213(95)00528-5 10.1016/S0550-3213(98)00580-X 10.1103/PhysRevD.57.4091 10.1007/s100520050173 10.1016/0003-4916(84)90258-6 10.1103/PhysRevD.56.4017 10.1007/JHEP12(2017)068 10.1007/JHEP03(2016)028 10.1143/PTP.99.271 10.1016/0370-2693(94)91206-8 10.1103/PhysRevD.50.2234 10.1016/0550-3213(94)90314-X 10.1016/j.nuclphysb.2013.07.028 10.1140/epjc/s10052-016-4509-7 10.1016/0370-2693(89)91495-0 |
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| References | B. Blok and M.A. Shifman, Lifetimes of charmed hadrons revisited. Facts and fancy, in Tau charm factory. Proceedings, 3rdWorkshop, Marbella, Spain, 1–6 June 1993, J. Kirkby and R. Kirkby eds., Editions Frontieres, France, (1994) [hep-ph/9311331] [INSPIRE]. Heavy Flavor Averaging Group (HFAG) collaboration, J. Alexander et al., Averages of b-hadron properties as of summer 2004, hep-ex/0412073 [INSPIRE]. LukeMEEffects of subleading operators in the heavy quark effective theoryPhys. Lett.1990B 2524471990PhLB..252..447L10.1016/0370-2693(90)90568-Q[INSPIRE] F. Gabbiani, A.I. Onishchenko and A.A. Petrov, Spectator effects and lifetimes of heavy hadrons, Phys. Rev.D 70 (2004) 094031 [hep-ph/0407004] [INSPIRE]. H.-Y. Cheng and K.-C. Yang, Nonspectator effects and B meson lifetimes from a field theoretic calculation, Phys. Rev.D 59 (1999) 014011 [hep-ph/9805222] [INSPIRE]. LEP B lifetime working group webpage, http://lepbosc.web.cern.ch/LEPBOSC/archive_LEPBOSC/lifetimes/lepblife.html. M.A. Shifman and M.B. Voloshin, Preasymptotic effects in inclusive weak decays of charmed particles, Sov. J. Nucl. Phys.41 (1985) 120 [Yad. Fiz.41 (1985) 187] [INSPIRE]. Particle Data Group collaboration, M. Tanabashi et al., Review of particle physics, Phys. Rev.D 98 (2018) 030001 [INSPIRE]. MannelTPivovarovAARosenthalDInclusive weak decays of heavy hadrons with power suppressed terms at NLOPhys. Rev.2015D 922015PhRvD..92e4025M1373.81394[arXiv:1506.08167] [INSPIRE] V. Chernyak, Calculation of the D and B meson lifetimes and the unitarity triangle parameters, Nucl. Phys.B 457 (1995) 96 [hep-ph/9503208] [INSPIRE]. T.A. DeGrand, Excited states of confined quarks. 2, Annals Phys.101 (1976) 496 [INSPIRE]. F. Gabbiani, A.I. Onishchenko and A.A. Petrov, Λblifetime puzzle in heavy quark expansion, Phys. Rev.D 68 (2003) 114006 [hep-ph/0303235] [INSPIRE]. BilicNGuberinaBTrampeticJPauli interference effect in D+ lifetimeNucl. Phys.1984B 2482611984NuPhB.248..261B10.1016/0550-3213(84)90596-0[INSPIRE] M. Neubert and C.T. Sachrajda, Spectator effects in inclusive decays of beauty hadrons, Nucl. Phys.B 483 (1997) 339 [hep-ph/9603202] [INSPIRE]. D0 collaboration, V.M. Abazov et al., Measurement of the Λb0lifetime in the decay Λb0 → J/ψΛ0with the DO detector, Phys. Rev. Lett.94 (2005) 102001 [hep-ex/0410054] [INSPIRE]. MannelTTurczykSUraltsevNHigher order power corrections in inclusive B decaysJHEP2010111092010JHEP...11..109M10.1007/JHEP11(2010)1091294.81360[arXiv:1009.4622] [INSPIRE] M. Neubert, B decays and CP-violation, Int. J. Mod. Phys.A 11 (1996) 4173 [hep-ph/9604412] [INSPIRE]. Particle Data Group collaboration, R.M. Barnett et al., Review of particle physics, Phys. Rev.D 54 (1996) 1 [INSPIRE]. A. Babic, B. Guberina, B. Melić and H. Stefancic, Cabibbo-suppressed decays of the Ωc0: feedback to the Ξc+lifetime, Phys. Rev.D 70 (2004) 117501 [hep-ph/0406183] [INSPIRE]. BecherTBoosHLunghiEKinetic corrections to B→Xcℓν¯\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$ B\to {X}_c\ell \overline{\nu} $$\end{document} at one loopJHEP2007120622007JHEP...12..062B10.1088/1126-6708/2007/12/062[arXiv:0708.0855] [INSPIRE] ChodosAJaffeRLJohnsonKThornCBBaryon structure in the bag theoryPhys. Rev.1974D 1025991974PhRvD..10.2599C[INSPIRE] AokiSReview of lattice results concerning low-energy particle physicsEur. Phys. J.2017C 771122017EPJC...77..112A10.1140/epjc/s10052-016-4509-7[arXiv:1607.00299] [INSPIRE] GuberinaBRücklRTrampeticJCharmed baryon lifetime differencesZ. Phys.1986C 332971986ZPhyC..33..297G[INSPIRE] BelliniGBigiIIYDornanPJLifetimes of charm and beauty hadronsPhys. Rept.199728911997PhR...289....1B10.1016/S0370-1573(97)00005-7[INSPIRE] B. Blok and M.A. Shifman, The rule of discarding 1/Ncin inclusive weak decays. 1, Nucl. Phys.B 399 (1993) 441 [hep-ph/9207236] [INSPIRE]. DeGrandTAJaffeRLExcited states of confined quarksAnnals Phys.19761004251976AnPhy.100..425D10.1016/0003-4916(76)90069-5[INSPIRE] EbertDFaustovRNGalkinVOSpectroscopy and Regge trajectories of heavy baryons in the relativistic quark-diquark picturePhys. Rev.2011D 842011PhRvD..84a4025E[arXiv:1105.0583] [INSPIRE] I.I.Y. Bigi, N.G. Uraltsev and A.I. Vainshtein, Nonperturbative corrections to inclusive beauty and charm decays: QCD versus phenomenological models, Phys. Lett.B 293 (1992) 430 [Erratum ibid.B 297 (1992) 477] [hep-ph/9207214] [INSPIRE]. GrozinAGKleinRMannelTPivovarovAAB0‐B¯0\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$ {B}^0\hbox{-} {\overline{B}}^0 $$\end{document} mixing at next-to-leading orderPhys. Rev.2016D 942016PhRvD..94c4024G[arXiv:1606.06054] [INSPIRE] ChengH-YCheungC-YLinG-LLinYCYanT-MYuH-LHeavy flavor conserving nonleptonic weak decays of heavy baryonsPhys. Rev.1992D 4650601992PhRvD..46.5060C[INSPIRE] GambinoPHealeyKJTurczykSTaming the higher power corrections in semileptonic B decaysPhys. Lett.2016B 763602016PhLB..763...60G10.1016/j.physletb.2016.10.023[arXiv:1606.06174] [INSPIRE] H.-Y. Cheng and B. Tseng, Nonleptonic weak decays of charmed baryons, Phys. Rev.D 46 (1992) 1042 [Erratum ibid.D 55 (1997) 1697] [INSPIRE]. M. Beneke, G. Buchalla, C. Greub, A. Lenz and U. Nierste, The B+ ‐ Bd0lifetime difference beyond leading logarithms, Nucl. Phys.B 639 (2002) 389 [hep-ph/0202106] [INSPIRE]. LHCb collaboration, Measurement of the Ωc0baryon lifetime, Phys. Rev. Lett.121 (2018) 092003 [arXiv:1807.02024] [INSPIRE]. LenzARauhTD-meson lifetimes within the heavy quark expansionPhys. Rev.2013D 882013PhRvD..88c4004L[arXiv:1305.3588] [INSPIRE] A.F. Falk, Z. Ligeti, M. Neubert and Y. Nir, Heavy quark expansion for the inclusive decayB¯→τν¯X\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$ \overline{B}\to \tau \overline{\nu}X $$\end{document}, Phys. Lett.B 326 (1994) 145[hep-ph/9401226] [INSPIRE]. Le YaouancAHadron transitions in the quark model1987New York, U.S.A.Gordon and Breach B. Guberina, B. Melić and H. Stefancic, Lifetime difference pattern of heavy hadrons, Phys. Lett.B 484 (2000) 43 [hep-ph/0004264] [INSPIRE]. QuangH-KPhamX-YExact one gluon corrections for inclusive weak processesAnnals Phys.19841552021984AnPhy.155..202H10.1016/0003-4916(84)90258-6[INSPIRE] CDF collaboration, A. Abulencia et al., Measurement of the Λb0lifetime in Λb0 → J/ψΛ0inpp¯\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$ p\overline{p} $$\end{document}collisions ats=1.96\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$ \sqrt{s}=1.96 $$\end{document}TeV, Phys. Rev. Lett.98 (2007) 122001 [hep-ex/0609021] [INSPIRE]. M. Beneke, G. Buchalla and I. Dunietz, Width difference in theBs−B¯s\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$ {B}_s-{\overline{B}}_s $$\end{document}system, Phys. Rev.D 54 (1996) 4419 [Erratum ibid.D 83 (2011) 119902] [hep-ph/9605259] [INSPIRE]. I.I.Y. Bigi, M.A. Shifman, N. Uraltsev and A.I. Vainshtein, High power n of mbin beauty widths and n = 5 → ∞ limit, Phys. Rev.D 56 (1997) 4017 [hep-ph/9704245] [INSPIRE]. T. Ito, M. Matsuda and Y. Matsui, New possibility of solving the problem of lifetime ratio τ(Λb)/τ(Bd), Prog. Theor. Phys.99 (1998) 271 [hep-ph/9705402] [INSPIRE]. KrinnerFLenzARauhTThe inclusive decay b→cc¯s\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$ b\to c\overline{c}s $$\end{document} revisitedNucl. Phys.2013B 876312013NuPhB.876...31K10.1016/j.nuclphysb.2013.07.0281284.81349[arXiv:1305.5390] [INSPIRE] G. Altarelli, G. Martinelli, S. Petrarca and F. Rapuano, Failure of local duality in inclusive nonleptonic heavy flavor decays, Phys. Lett.B 382 (1996) 409 [hep-ph/9604202] [INSPIRE]. ChayJGeorgiHGrinsteinBLepton energy distributions in heavy meson decays from QCDPhys. Lett.1990B 2473991990PhLB..247..399C10.1016/0370-2693(90)90916-T[INSPIRE] AbramsGSObservation of charmed baryon production in e+e− annihilationPhys. Rev. Lett.198044101980PhRvL..44...10A10.1103/PhysRevLett.44.10[INSPIRE] I.I.Y. Bigi, M.A. Shifman, N.G. Uraltsev and A.I. Vainshtein, The pole mass of the heavy quark. Perturbation theory and beyond, Phys. Rev.D 50 (1994) 2234 [hep-ph/9402360] [INSPIRE]. LHCb collaboration, Evidence for the strangeness-changing weak decay Ξb− → Λb0π−, Phys. Rev. Lett.115 (2015) 241801 [arXiv:1510.03829] [INSPIRE]. LHCb collaboration, Measurement of the lifetime of the doubly charmed baryon Ξcc+ +, Phys. Rev. Lett.121 (2018) 052002 [arXiv:1806.02744] [INSPIRE]. H.-Y. Cheng, A phenomenological analysis of heavy hadron lifetimes, Phys. Rev.D 56 (1997) 2783 [hep-ph/9704260] [INSPIRE]. Heavy Flavor Averaging Group (HFLAV) online update webpage, http://www.slac.stanford.edu/xorg/hfag. HFLAV collaboration, Y. Amhis et al., Averages of b-hadron, c-hadron and τ-lepton properties as of summer 2016, Eur. Phys. J.C 77 (2017) 895 [arXiv:1612.07233] [INSPIRE]. E.E. Jenkins, Heavy baryon masses in the 1/mQand 1/Ncexpansions, Phys. Rev.D 54 (1996) 4515 [hep-ph/9603449] [INSPIRE]. De RujulaAGeorgiHGlasho 9320_CR52 9320_CR51 9320_CR50 N Bilic (9320_CR5) 1984; B 248 JL Cortes (9320_CR68) 1981; D 24 9320_CR12 9320_CR10 9320_CR54 9320_CR53 9320_CR16 9320_CR15 A Alberti (9320_CR41) 2014; 01 AG Grozin (9320_CR56) 2016; D 94 9320_CR14 P Gambino (9320_CR30) 2016; B 763 9320_CR13 9320_CR57 T Mannel (9320_CR42) 2015; D 92 9320_CR19 9320_CR18 9320_CR17 9320_CR1 A Alberti (9320_CR40) 2013; B 870 9320_CR4 9320_CR3 9320_CR2 T Mannel (9320_CR32) 2017; B 921 9320_CR60 9320_CR23 B Guberina (9320_CR7) 1986; C 33 9320_CR66 9320_CR21 9320_CR65 GS Abrams (9320_CR77) 1980; 44 9320_CR20 9320_CR64 9320_CR27 9320_CR25 9320_CR69 9320_CR24 9320_CR29 T Becher (9320_CR39) 2007; 12 S Aoki (9320_CR58) 2017; C 77 9320_CR28 A De Rujula (9320_CR67) 1975; D 12 H-Y Cheng (9320_CR71) 1992; D 46 D Ebert (9320_CR70) 2011; D 84 B Guberina (9320_CR59) 1979; B 89 H-Y Cheng (9320_CR72) 2016; 03 F Krinner (9320_CR48) 2013; B 876 AG Grozin (9320_CR55) 2009; 02 9320_CR74 9320_CR73 9320_CR34 9320_CR78 9320_CR33 9320_CR31 9320_CR75 A Lenz (9320_CR26) 2013; D 88 T Mannel (9320_CR35) 2010; 11 9320_CR79 TA DeGrand (9320_CR63) 1976; 100 G Bellini (9320_CR80) 1997; 289 A Lenz (9320_CR8) 2015; A 30 ME Luke (9320_CR11) 1990; B 252 9320_CR85 M Kirk (9320_CR22) 2017; 12 9320_CR84 A Le Yaouanc (9320_CR76) 1987 9320_CR83 9320_CR6 9320_CR82 9320_CR45 9320_CR44 9320_CR43 9320_CR87 H-K Quang (9320_CR36) 1983; B 122 9320_CR86 9320_CR49 9320_CR47 9320_CR46 J Chay (9320_CR9) 1990; B 247 TA DeGrand (9320_CR62) 1975; D 12 A Chodos (9320_CR61) 1974; D 10 Y Nir (9320_CR38) 1989; B 221 H-K Quang (9320_CR37) 1984; 155 9320_CR81 |
| References_xml | – reference: LHCb collaboration, Evidence for the strangeness-changing weak decay Ξb− → Λb0π−, Phys. Rev. Lett.115 (2015) 241801 [arXiv:1510.03829] [INSPIRE]. – reference: V. Chernyak, Calculation of the D and B meson lifetimes and the unitarity triangle parameters, Nucl. Phys.B 457 (1995) 96 [hep-ph/9503208] [INSPIRE]. – reference: A.F. Falk, Z. Ligeti, M. Neubert and Y. Nir, Heavy quark expansion for the inclusive decayB¯→τν¯X\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$ \overline{B}\to \tau \overline{\nu}X $$\end{document}, Phys. Lett.B 326 (1994) 145[hep-ph/9401226] [INSPIRE]. – reference: M. Beneke, G. Buchalla and I. Dunietz, Width difference in theBs−B¯s\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$ {B}_s-{\overline{B}}_s $$\end{document}system, Phys. Rev.D 54 (1996) 4419 [Erratum ibid.D 83 (2011) 119902] [hep-ph/9605259] [INSPIRE]. – reference: DeGrandTAJaffeRLJohnsonKKiskisJEMasses and other parameters of the light hadronsPhys. Rev.1975D 1220601975PhRvD..12.2060D[INSPIRE] – reference: BilicNGuberinaBTrampeticJPauli interference effect in D+ lifetimeNucl. Phys.1984B 2482611984NuPhB.248..261B10.1016/0550-3213(84)90596-0[INSPIRE] – reference: F. Gabbiani, A.I. Onishchenko and A.A. Petrov, Spectator effects and lifetimes of heavy hadrons, Phys. Rev.D 70 (2004) 094031 [hep-ph/0407004] [INSPIRE]. – reference: B. Guberina and B. Melić, Inclusive charmed baryon decays and lifetimes, Eur. Phys. J.C 2 (1998) 697 [hep-ph/9704445] [INSPIRE]. – reference: M. Neubert, B decays and CP-violation, Int. J. Mod. Phys.A 11 (1996) 4173 [hep-ph/9604412] [INSPIRE]. – reference: B. Blok and M.A. Shifman, The rule of discarding 1/Ncin inclusive weak decays. 1, Nucl. Phys.B 399 (1993) 441 [hep-ph/9207236] [INSPIRE]. – reference: G. Altarelli, G. Martinelli, S. Petrarca and F. Rapuano, Failure of local duality in inclusive nonleptonic heavy flavor decays, Phys. Lett.B 382 (1996) 409 [hep-ph/9604202] [INSPIRE]. – reference: T. Ito, M. Matsuda and Y. Matsui, New possibility of solving the problem of lifetime ratio τ(Λb)/τ(Bd), Prog. Theor. Phys.99 (1998) 271 [hep-ph/9705402] [INSPIRE]. – reference: BelliniGBigiIIYDornanPJLifetimes of charm and beauty hadronsPhys. Rept.199728911997PhR...289....1B10.1016/S0370-1573(97)00005-7[INSPIRE] – reference: I.I.Y. Bigi, M.A. Shifman, N. Uraltsev and A.I. Vainshtein, High power n of mbin beauty widths and n = 5 → ∞ limit, Phys. Rev.D 56 (1997) 4017 [hep-ph/9704245] [INSPIRE]. – reference: G. Buchalla, A.J. Buras and M.E. Lautenbacher, Weak decays beyond leading logarithms, Rev. Mod. Phys.68 (1996) 1125 [hep-ph/9512380] [INSPIRE]. – reference: M.A. Shifman and M.B. Voloshin, Preasymptotic effects in inclusive weak decays of charmed particles, Sov. J. Nucl. Phys.41 (1985) 120 [Yad. Fiz.41 (1985) 187] [INSPIRE]. – reference: KrinnerFLenzARauhTThe inclusive decay b→cc¯s\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$ b\to c\overline{c}s $$\end{document} revisitedNucl. Phys.2013B 876312013NuPhB.876...31K10.1016/j.nuclphysb.2013.07.0281284.81349[arXiv:1305.5390] [INSPIRE] – reference: ChayJGeorgiHGrinsteinBLepton energy distributions in heavy meson decays from QCDPhys. Lett.1990B 2473991990PhLB..247..399C10.1016/0370-2693(90)90916-T[INSPIRE] – reference: M.B. Voloshin, Spectator effects in semileptonic decay of charmed baryons, Phys. Lett.B 385 (1996) 369 [hep-ph/9604335] [INSPIRE]. – reference: LHCb collaboration, Measurement of the Ωc0baryon lifetime, Phys. Rev. Lett.121 (2018) 092003 [arXiv:1807.02024] [INSPIRE]. – reference: T.A. DeGrand, Excited states of confined quarks. 2, Annals Phys.101 (1976) 496 [INSPIRE]. – reference: I.I.Y. Bigi, M.A. Shifman, N.G. Uraltsev and A.I. Vainshtein, Sum rules for heavy flavor transitions in the SV limit, Phys. Rev.D 52 (1995) 196 [hep-ph/9405410] [INSPIRE]. – reference: BESIII collaboration, M. Ablikim et al., Measurement of the absolute branching fraction of the inclusive semileptonic Λc+decay, arXiv:1805.09060 [INSPIRE]. – reference: I.I.Y. Bigi, N.G. Uraltsev and A.I. Vainshtein, Nonperturbative corrections to inclusive beauty and charm decays: QCD versus phenomenological models, Phys. Lett.B 293 (1992) 430 [Erratum ibid.B 297 (1992) 477] [hep-ph/9207214] [INSPIRE]. – reference: NirYThe mass ratio mc/mb in semileptonic B decaysPhys. Lett.1989B 2211841989PhLB..221..184N10.1016/0370-2693(89)91495-0[INSPIRE] – reference: D. Becirevic, Theoretical progress in describing the B meson lifetimes, PoS(HEP2001)098, (2001) [hep-ph/0110124] [INSPIRE]. – reference: LEP B lifetime working group webpage, http://lepbosc.web.cern.ch/LEPBOSC/archive_LEPBOSC/lifetimes/lepblife.html. – reference: D0 collaboration, V.M. Abazov et al., Measurement of the Λb0lifetime in the decay Λb0 → J/ψΛ0with the DO detector, Phys. Rev. Lett.94 (2005) 102001 [hep-ex/0410054] [INSPIRE]. – reference: CortesJLSanchez GuillenJThe lifetimes of charmed baryonsPhys. Rev.1981D 2429821981PhRvD..24.2982C[INSPIRE] – reference: EbertDFaustovRNGalkinVOSpectroscopy and Regge trajectories of heavy baryons in the relativistic quark-diquark picturePhys. Rev.2011D 842011PhRvD..84a4025E[arXiv:1105.0583] [INSPIRE] – reference: AlbertiAGambinoPNandiSPerturbative corrections to power suppressed effects in semileptonic B decaysJHEP2014011472014JHEP...01..147A10.1007/JHEP01(2014)147[arXiv:1311.7381] [INSPIRE] – reference: A.H. Hoang, Z. Ligeti and A.V. Manohar, B decay and the ϒ mass, Phys. Rev. Lett.82 (1999) 277 [hep-ph/9809423] [INSPIRE]. – reference: ChengH-YCheungC-YLinG-LLinYCYanT-MYuH-LHeavy flavor conserving nonleptonic weak decays of heavy baryonsPhys. Rev.1992D 4650601992PhRvD..46.5060C[INSPIRE] – reference: GuberinaBRücklRTrampeticJCharmed baryon lifetime differencesZ. Phys.1986C 332971986ZPhyC..33..297G[INSPIRE] – reference: MannelTRusovAVShahriaranFInclusive semitauonic B decays to order OΛQCD3/mb3\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$ \mathcal{O}\left({\Lambda}_{\mathrm{QCD}}^3/{m}_b^3\right) $$\end{document}Nucl. Phys.2017B 9212112017NuPhB.921..211M10.1016/j.nuclphysb.2017.05.0161370.81212[arXiv:1702.01089] [INSPIRE] – reference: Particle Data Group collaboration, R.M. Barnett et al., Review of particle physics, Phys. Rev.D 54 (1996) 1 [INSPIRE]. – reference: B. Guberina, B. Melić and H. Stefancic, Lifetime difference pattern of heavy hadrons, Phys. Lett.B 484 (2000) 43 [hep-ph/0004264] [INSPIRE]. – reference: GambinoPHealeyKJTurczykSTaming the higher power corrections in semileptonic B decaysPhys. Lett.2016B 763602016PhLB..763...60G10.1016/j.physletb.2016.10.023[arXiv:1606.06174] [INSPIRE] – reference: H.-Y. Cheng and B. Tseng, Nonleptonic weak decays of charmed baryons, Phys. Rev.D 46 (1992) 1042 [Erratum ibid.D 55 (1997) 1697] [INSPIRE]. – reference: M.A. Shifman and M.B. Voloshin, On annihilation of mesons built from heavy and light quark andB¯0↔B0\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$ {\overline{B}}^0\leftrightarrow {B}^0 $$\end{document}oscillations, Sov. J. Nucl. Phys.45 (1987) 292 [Yad. Fiz.45 (1987) 463] [INSPIRE]. – reference: AlbertiAEwerthTGambinoPNandiSKinetic operator effects in B¯→Xcℓν\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$ \overline{B}\to {X}_c\ell \nu $$\end{document} at O(αs)Nucl. Phys.2013B 870162013NuPhB.870...16A10.1016/j.nuclphysb.2013.01.0051262.81219[arXiv:1212.5082] [INSPIRE] – reference: DeGrandTAJaffeRLExcited states of confined quarksAnnals Phys.19761004251976AnPhy.100..425D10.1016/0003-4916(76)90069-5[INSPIRE] – reference: ChengH-YCheungC-YLinG-LLinY-CYanT-MYuH-LHeavy-flavor-conserving hadronic weak decays of heavy baryonsJHEP2016030282016JHEP...03..028C10.1007/JHEP03(2016)028[arXiv:1512.01276] [INSPIRE] – reference: GuberinaBNussinovSPecceiRDRücklRD meson lifetimes and decaysPhys. Lett.1979B 891111979PhLB...89..111G10.1016/0370-2693(79)90086-8[INSPIRE] – reference: M. Beneke, G. Buchalla, C. Greub, A. Lenz and U. Nierste, The B+ ‐ Bd0lifetime difference beyond leading logarithms, Nucl. Phys.B 639 (2002) 389 [hep-ph/0202106] [INSPIRE]. – reference: B. Blok and M.A. Shifman, Lifetimes of charmed hadrons revisited. Facts and fancy, in Tau charm factory. Proceedings, 3rdWorkshop, Marbella, Spain, 1–6 June 1993, J. Kirkby and R. Kirkby eds., Editions Frontieres, France, (1994) [hep-ph/9311331] [INSPIRE]. – reference: B. Blok and M.A. Shifman, The rule of discarding 1/Ncin inclusive weak decays. 2, Nucl. Phys.B 399 (1993) 459 [hep-ph/9209289] [INSPIRE]. – reference: UKQCD collaboration, M. Di Pierro and C.T. Sachrajda, A lattice study of spectator effects in inclusive decays of B mesons, Nucl. Phys.B 534 (1998) 373 [hep-lat/9805028] [INSPIRE]. – reference: HFLAV collaboration, Y. Amhis et al., Averages of b-hadron, c-hadron and τ-lepton properties as of summer 2016, Eur. Phys. J.C 77 (2017) 895 [arXiv:1612.07233] [INSPIRE]. – reference: P. Colangelo and F. De Fazio, Role of four quark operators in the inclusive Λbdecays, Phys. Lett.B 387 (1996) 371 [hep-ph/9604425] [INSPIRE]. – reference: E.E. Jenkins, Update of heavy baryon mass predictions, Phys. Rev.D 55 (1997) 10 [hep-ph/9609404] [INSPIRE]. – reference: CDF collaboration, A. Abulencia et al., Measurement of the Λb0lifetime in Λb0 → J/ψΛ0inpp¯\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$ p\overline{p} $$\end{document}collisions ats=1.96\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$ \sqrt{s}=1.96 $$\end{document}TeV, Phys. Rev. Lett.98 (2007) 122001 [hep-ex/0609021] [INSPIRE]. – reference: GrozinAGLeeRNThree-loop HQET vertex diagrams for B0‐B¯0\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$ {B}^0\hbox{-} {\overline{B}}^0 $$\end{document} mixingJHEP2009020472009JHEP...02..047G10.1088/1126-6708/2009/02/047[arXiv:0812.4522] [INSPIRE] – reference: H.-Y. Cheng and K.-C. Yang, Nonspectator effects and B meson lifetimes from a field theoretic calculation, Phys. Rev.D 59 (1999) 014011 [hep-ph/9805222] [INSPIRE]. – reference: Particle Data Group collaboration, M. Tanabashi et al., Review of particle physics, Phys. Rev.D 98 (2018) 030001 [INSPIRE]. – reference: B. Guberina and H. Stefancic, Cabibbo suppressed decays and the Ξc+lifetime, Phys. Rev.D 65 (2002) 114004 [hep-ph/0202080] [INSPIRE]. – reference: Heavy Flavor Averaging Group (HFAG) collaboration, J. Alexander et al., Averages of b-hadron properties as of summer 2004, hep-ex/0412073 [INSPIRE]. – reference: J.L. Rosner, Enhancement of the Λbdecay rate, Phys. Lett.B 379 (1996) 267 [hep-ph/9602265] [INSPIRE]. – reference: LHCb collaboration, Measurement of the lifetime of the doubly charmed baryon Ξcc+ +, Phys. Rev. Lett.121 (2018) 052002 [arXiv:1806.02744] [INSPIRE]. – reference: GrozinAGKleinRMannelTPivovarovAAB0‐B¯0\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$ {B}^0\hbox{-} {\overline{B}}^0 $$\end{document} mixing at next-to-leading orderPhys. Rev.2016D 942016PhRvD..94c4024G[arXiv:1606.06054] [INSPIRE] – reference: F. Gabbiani, A.I. Onishchenko and A.A. Petrov, Λblifetime puzzle in heavy quark expansion, Phys. Rev.D 68 (2003) 114006 [hep-ph/0303235] [INSPIRE]. – reference: LenzARauhTD-meson lifetimes within the heavy quark expansionPhys. Rev.2013D 882013PhRvD..88c4004L[arXiv:1305.3588] [INSPIRE] – reference: E.E. Jenkins, Heavy baryon masses in the 1/mQand 1/Ncexpansions, Phys. Rev.D 54 (1996) 4515 [hep-ph/9603449] [INSPIRE]. – reference: M. Beneke and V.M. Braun, Heavy quark effective theory beyond perturbation theory: renormalons, the pole mass and the residual mass term, Nucl. Phys.B 426 (1994) 301 [hep-ph/9402364] [INSPIRE]. – reference: M. Neubert and C.T. Sachrajda, Spectator effects in inclusive decays of beauty hadrons, Nucl. Phys.B 483 (1997) 339 [hep-ph/9603202] [INSPIRE]. – reference: H.Y. Cheng, Charmed hadronic decay, talk presented at the International Workshop on Physics at Future High Intensity Collider @2–7 GeV, http://cicpi.ustc.edu.cn/hiepa2018, Huairou, Beijing, China, 19–21 March 2018. – reference: MannelTPivovarovAARosenthalDInclusive weak decays of heavy hadrons with power suppressed terms at NLOPhys. Rev.2015D 922015PhRvD..92e4025M1373.81394[arXiv:1506.08167] [INSPIRE] – reference: J. Chay and S.-J. Rey, Instanton contribution toB→Xμeν¯\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$ B\to {X}_{\mu }e\overline{\nu} $$\end{document}decay, Z. Phys.C 68 (1995) 431 [hep-ph/9404214] [INSPIRE]. – reference: MannelTTurczykSUraltsevNHigher order power corrections in inclusive B decaysJHEP2010111092010JHEP...11..109M10.1007/JHEP11(2010)1091294.81360[arXiv:1009.4622] [INSPIRE] – reference: LenzALifetimes and heavy quark expansionInt. J. Mod. Phys.2015A 3015430052015IJMPA..3043005L10.1142/S0217751X15430058[arXiv:1405.3601] [INSPIRE] – reference: BecherTBoosHLunghiEKinetic corrections to B→Xcℓν¯\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$ B\to {X}_c\ell \overline{\nu} $$\end{document} at one loopJHEP2007120622007JHEP...12..062B10.1088/1126-6708/2007/12/062[arXiv:0708.0855] [INSPIRE] – reference: AokiSReview of lattice results concerning low-energy particle physicsEur. Phys. J.2017C 771122017EPJC...77..112A10.1140/epjc/s10052-016-4509-7[arXiv:1607.00299] [INSPIRE] – reference: Y. Koide, Inclusive studies of charmed meson decays and SU(4) 20-plet dominance model, Phys. Rev.D 20 (1979) 1739 [Erratum ibid.D 21 (1980) 853] [INSPIRE]. – reference: ChodosAJaffeRLJohnsonKThornCBBaryon structure in the bag theoryPhys. Rev.1974D 1025991974PhRvD..10.2599C[INSPIRE] – reference: M.S. Baek, J. Lee, C. Liu and H.S. Song, Four quark operators relevant to B meson lifetimes from QCD sum rules, Phys. Rev.D 57 (1998) 4091 [hep-ph/9709386] [INSPIRE]. – reference: KirkMLenzARauhTDimension-six matrix elements for meson mixing and lifetimes from sum rulesJHEP2017120682017JHEP...12..068K10.1007/JHEP12(2017)068[arXiv:1711.02100] [INSPIRE] – reference: H.-Y. Cheng, A phenomenological analysis of heavy hadron lifetimes, Phys. Rev.D 56 (1997) 2783 [hep-ph/9704260] [INSPIRE]. – reference: De RujulaAGeorgiHGlashowSLHadron masses in a gauge theoryPhys. Rev.1975D 121471975PhRvD..12..147D[INSPIRE] – reference: Le YaouancAHadron transitions in the quark model1987New York, U.S.A.Gordon and Breach – reference: AbramsGSObservation of charmed baryon production in e+e− annihilationPhys. Rev. Lett.198044101980PhRvL..44...10A10.1103/PhysRevLett.44.10[INSPIRE] – reference: M.A. Shifman and M.B. Voloshin, Hierarchy of lifetimes of charmed and beautiful hadrons, Sov. Phys. JETP64 (1986) 698 [Zh. Eksp. Teor. Fiz.91 (1986) 1180] [INSPIRE]. – reference: LukeMEEffects of subleading operators in the heavy quark effective theoryPhys. Lett.1990B 2524471990PhLB..252..447L10.1016/0370-2693(90)90568-Q[INSPIRE] – reference: I.I.Y. Bigi, M.A. Shifman, N.G. Uraltsev and A.I. Vainshtein, The pole mass of the heavy quark. Perturbation theory and beyond, Phys. Rev.D 50 (1994) 2234 [hep-ph/9402360] [INSPIRE]. – reference: QuangH-KPhamX-YExact one gluon corrections for inclusive weak processesAnnals Phys.19841552021984AnPhy.155..202H10.1016/0003-4916(84)90258-6[INSPIRE] – reference: A. Babic, B. Guberina, B. Melić and H. Stefancic, Cabibbo-suppressed decays of the Ωc0: feedback to the Ξc+lifetime, Phys. Rev.D 70 (2004) 117501 [hep-ph/0406183] [INSPIRE]. – reference: QuangH-KPhamX-YMass effects in QCD corrections of weak decaysPhys. Lett.1983B 1222971983PhLB..122..297H[INSPIRE] – reference: Heavy Flavor Averaging Group (HFLAV) online update webpage, http://www.slac.stanford.edu/xorg/hfag. – ident: 9320_CR24 doi: 10.1103/PhysRevD.70.094031 – volume: B 122 start-page: 297 year: 1983 ident: 9320_CR36 publication-title: Phys. Lett. – ident: 9320_CR2 doi: 10.1016/0550-3213(93)90504-I – volume: 12 start-page: 062 year: 2007 ident: 9320_CR39 publication-title: JHEP doi: 10.1088/1126-6708/2007/12/062 – ident: 9320_CR65 doi: 10.1016/S0550-3213(02)00561-8 – volume: C 33 start-page: 297 year: 1986 ident: 9320_CR7 publication-title: Z. Phys. – ident: 9320_CR15 – volume: A 30 start-page: 1543005 year: 2015 ident: 9320_CR8 publication-title: Int. J. Mod. Phys. doi: 10.1142/S0217751X15430058 – ident: 9320_CR17 doi: 10.1016/0370-2693(96)00637-5 – ident: 9320_CR1 doi: 10.1016/0370-2693(92)90908-M – ident: 9320_CR21 – ident: 9320_CR60 doi: 10.1103/PhysRevD.20.1739 – volume: B 252 start-page: 447 year: 1990 ident: 9320_CR11 publication-title: Phys. Lett. doi: 10.1016/0370-2693(90)90568-Q – ident: 9320_CR66 doi: 10.1103/PhysRevD.46.1042 – ident: 9320_CR82 doi: 10.1016/S0370-2693(00)00620-1 – ident: 9320_CR27 doi: 10.1142/S0217751X96001966 – ident: 9320_CR69 doi: 10.1016/0370-2693(96)00352-8 – ident: 9320_CR73 – volume: 11 start-page: 109 year: 2010 ident: 9320_CR35 publication-title: JHEP doi: 10.1007/JHEP11(2010)109 – volume: B 247 start-page: 399 year: 1990 ident: 9320_CR9 publication-title: Phys. Lett. doi: 10.1016/0370-2693(90)90916-T – volume: D 92 year: 2015 ident: 9320_CR42 publication-title: Phys. Rev. – ident: 9320_CR12 doi: 10.1016/S0550-3213(96)00559-7 – volume: B 921 start-page: 211 year: 2017 ident: 9320_CR32 publication-title: Nucl. Phys. doi: 10.1016/j.nuclphysb.2017.05.016 – volume: 100 start-page: 425 year: 1976 ident: 9320_CR63 publication-title: Annals Phys. doi: 10.1016/0003-4916(76)90069-5 – volume: D 12 start-page: 2060 year: 1975 ident: 9320_CR62 publication-title: Phys. Rev. – volume: 02 start-page: 047 year: 2009 ident: 9320_CR55 publication-title: JHEP doi: 10.1088/1126-6708/2009/02/047 – ident: 9320_CR87 – volume: 01 start-page: 147 year: 2014 ident: 9320_CR41 publication-title: JHEP doi: 10.1007/JHEP01(2014)147 – volume: 289 start-page: 1 year: 1997 ident: 9320_CR80 publication-title: Phys. Rept. doi: 10.1016/S0370-1573(97)00005-7 – ident: 9320_CR6 – volume: 44 start-page: 10 year: 1980 ident: 9320_CR77 publication-title: Phys. Rev. Lett. doi: 10.1103/PhysRevLett.44.10 – ident: 9320_CR14 – ident: 9320_CR84 doi: 10.1103/PhysRevD.70.117501 – ident: 9320_CR34 doi: 10.1016/0370-2693(96)00837-4 – ident: 9320_CR23 doi: 10.1103/PhysRevD.68.114006 – ident: 9320_CR25 doi: 10.1103/PhysRevD.54.4419 – ident: 9320_CR57 doi: 10.1103/RevModPhys.68.1125 – ident: 9320_CR83 doi: 10.1103/PhysRevD.65.114004 – ident: 9320_CR50 doi: 10.1016/0370-2693(96)01049-0 – ident: 9320_CR74 – ident: 9320_CR28 doi: 10.1103/PhysRevD.54.4515 – ident: 9320_CR10 doi: 10.1007/BF01620717 – ident: 9320_CR54 doi: 10.22323/1.007.0098 – ident: 9320_CR64 doi: 10.1016/0003-4916(76)90021-X – ident: 9320_CR3 doi: 10.1016/0550-3213(93)90505-J – volume: B 763 start-page: 60 year: 2016 ident: 9320_CR30 publication-title: Phys. Lett. doi: 10.1016/j.physletb.2016.10.023 – ident: 9320_CR18 doi: 10.1103/PhysRevD.56.2783 – ident: 9320_CR52 doi: 10.1103/PhysRevD.59.014011 – ident: 9320_CR45 doi: 10.1103/PhysRevD.52.196 – ident: 9320_CR47 doi: 10.1103/PhysRevLett.82.277 – ident: 9320_CR13 – ident: 9320_CR29 doi: 10.1103/PhysRevD.55.R10 – volume: B 89 start-page: 111 year: 1979 ident: 9320_CR59 publication-title: Phys. Lett. doi: 10.1016/0370-2693(79)90086-8 – ident: 9320_CR75 – volume: B 248 start-page: 261 year: 1984 ident: 9320_CR5 publication-title: Nucl. Phys. doi: 10.1016/0550-3213(84)90596-0 – volume: B 870 start-page: 16 year: 2013 ident: 9320_CR40 publication-title: Nucl. Phys. doi: 10.1016/j.nuclphysb.2013.01.005 – volume-title: Hadron transitions in the quark model year: 1987 ident: 9320_CR76 – ident: 9320_CR49 doi: 10.1016/0550-3213(95)00528-5 – ident: 9320_CR78 – volume: D 12 start-page: 147 year: 1975 ident: 9320_CR67 publication-title: Phys. Rev. – ident: 9320_CR53 doi: 10.1016/S0550-3213(98)00580-X – ident: 9320_CR85 – ident: 9320_CR51 doi: 10.1103/PhysRevD.57.4091 – ident: 9320_CR81 doi: 10.1007/s100520050173 – volume: 155 start-page: 202 year: 1984 ident: 9320_CR37 publication-title: Annals Phys. doi: 10.1016/0003-4916(84)90258-6 – ident: 9320_CR4 – ident: 9320_CR46 doi: 10.1103/PhysRevD.56.4017 – ident: 9320_CR16 – volume: 12 start-page: 068 year: 2017 ident: 9320_CR22 publication-title: JHEP doi: 10.1007/JHEP12(2017)068 – volume: 03 start-page: 028 year: 2016 ident: 9320_CR72 publication-title: JHEP doi: 10.1007/JHEP03(2016)028 – ident: 9320_CR20 – volume: D 24 start-page: 2982 year: 1981 ident: 9320_CR68 publication-title: Phys. Rev. – volume: D 10 start-page: 2599 year: 1974 ident: 9320_CR61 publication-title: Phys. Rev. – volume: D 94 year: 2016 ident: 9320_CR56 publication-title: Phys. Rev. – ident: 9320_CR33 – ident: 9320_CR19 doi: 10.1143/PTP.99.271 – ident: 9320_CR31 doi: 10.1016/0370-2693(94)91206-8 – ident: 9320_CR44 doi: 10.1103/PhysRevD.50.2234 – ident: 9320_CR79 – ident: 9320_CR43 doi: 10.1016/0550-3213(94)90314-X – volume: B 876 start-page: 31 year: 2013 ident: 9320_CR48 publication-title: Nucl. Phys. doi: 10.1016/j.nuclphysb.2013.07.028 – volume: C 77 start-page: 112 year: 2017 ident: 9320_CR58 publication-title: Eur. Phys. J. doi: 10.1140/epjc/s10052-016-4509-7 – volume: D 84 year: 2011 ident: 9320_CR70 publication-title: Phys. Rev. – volume: D 46 start-page: 5060 year: 1992 ident: 9320_CR71 publication-title: Phys. Rev. – volume: D 88 year: 2013 ident: 9320_CR26 publication-title: Phys. Rev. – volume: B 221 start-page: 184 year: 1989 ident: 9320_CR38 publication-title: Phys. Lett. doi: 10.1016/0370-2693(89)91495-0 – ident: 9320_CR86 |
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The lifetimes of bottom and charmed hadrons are analyzed within the framework of the heavy quark expansion (HQE). Lifetime differences arise from the... The lifetimes of bottom and charmed hadrons are analyzed within the framework of the heavy quark expansion (HQE). Lifetime differences arise from the spectator... Abstract The lifetimes of bottom and charmed hadrons are analyzed within the framework of the heavy quark expansion (HQE). Lifetime differences arise from the... |
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| SubjectTerms | Baryons Charm (particle physics) Classical and Quantum Gravitation Elementary Particles Hadrons Heavy Quark Physics High energy physics Interference Lifetime Mesons Operators Perturbative QCD Physics Physics and Astronomy Quantum Field Theories Quantum Field Theory Quantum Physics Quark models Quarks Regular Article - Theoretical Physics Relativity Theory String Theory Sum rules |
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| Title | Phenomenological study of heavy hadron lifetimes |
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