Heavy Quark-Diquark Symmetry: Doubly Heavy Baryons and...
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Heavy Quark-Diquark Symmetry: Doubly Heavy Baryons and Tetraquarks
Thomas Mehen Duke University
12th Quarkonium Working Group, Peking University November 6, 2017
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LHCb discovery of ⌅++cc
⇤+c K
�⇡+⇡+
m⌅++cc
= 3621.4± 0.72± 0.27± 0.14MeV
R. Aaij, et. al. (LHCb) , PRL 119 112001 (2017)
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in Other Channels
Measuring Lifetime
Measuring Production Rates
Finding Isospin Partner
Observing ⌅++cc
Observing Excited Doubly Heavy Baryons
Confirming Doubly Charm Interpretation of ⌅++cc
⌅+cc
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Heavy Quark-Diquark Symmetry
mQ ! 1 QQ is compact object in color 3
Singly Heavy Meson Doubly Heavy anti-Baryon
Q QQq q
l.d.o.f are the same in these hadrons
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Heavy Quark-Diquark Symmetry (HQDQS)
mQ ! 1 QQ is compact object in color 3
Singly Heavy anti-Baryon Doubly Heavy Tetraquark
Q QQq q q
l.d.o.f are the same in these hadrons
q
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Spectrum of Excited Doubly Charm Baryons
light quark excitation
P-wave diquark
radial (2S) excited diquark
D. Ebert, et. al., PRD 66 (2002) 014008
⇤cD
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HQET for heavy quarks and diquarks
Hyperfine splittings
M. Savage and M. Wise, PLB 248 (1990) 177
m⌅⇤cc�m⌅cc =
3
4(mD⇤ �mD)
m⌅⇤cc
⇡ 3727MeV, em decays to ground state
⇡ 106MeV
S. Fleming and T. Mehen, PRD 73 (2006) 034502 N. Brambilla, A. Vairo, T. Rosch, PRD 72 (2005) 034021
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Chiral Lagrangian with Quark-Diquark SymmetryJ. Hu and T.M, PRD 73, 054003 (2006)
Heavy hadron chiral perturbation theory - in rest frame vµ = (1,~0)
ground state spin-0,1 fields: 2 x 2 field Q↵q�
(QQ)iq�3 x 2 field
Chiral Lagrangian for doubly heavy baryons
EM interactions
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Electromagnetic decay of
Chiral loop corrections J. Amundson, et. al., PLB 296 (1992) 415
�[⌅⇤++cc ] = 5.1 keV
Predictions
�[⌅⇤+cc ] = 7.6 keV
⌅⇤
J. Hu and T.M, PRD 73, 054003 (2006)
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Excited Doubly Heavy Baryon Decays
⌅cc(3621)
⌅⇤cc(3727)
⌅Pcc(3846)
⌅P⇤cc (3952)
⌅0⇤cc(4027)
⌅0
cc(3921)
�
⇡ ⇡
⇡ ⇡
⇡ ⇡
⇡mhc �mJ/
2
⇡m (2S) �mJ/
2
Vcc =1
2Vcc
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Predictions for Strong Decays
Radially excited states g ⇠ O(1)
P-wave excited states �1/2 ⇡ �3/2 ⇠ O(⇤QCD/mc)
1/3 < �1/2,3/2 < 1/2
12MeV < �[⌅P(⇤)cc ] < 28MeV
J. Hu and T.M, PRD 73, 054003 (2006)
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Strange Sector
HQDQS predicts
Lattice QCD
m⌦cc �m⌅+,++cc
= 98± 9± 22± 12MeV
Low lying excitation spectrum nearly identical to non-strange
Analogous decay to ground state via kaon emission forbiddenstrong decay via isospin violating decays to ⇡0
Narrow states, width ~ few keV
L. Liu, et. al., et. al., PRD 81 094505 (2010)
J. Hu and T.M, PRD 73, 054003 (2006)
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Stable Doubly Heavy Tetraquarksquark model M. Karliner, J. Rosner, arXiv:1707.07666
Tbbud JP = 1+
below BB⇤ threshold, stable to strong interaction I = 0
heavy quark symmetry E. Eichten, C. Quigg, arXiv:1707.09575
10468MeV
lattice QCD
215MeV
135MeV below threshold
A. Francis, et. al., PRL 118, 142001 (2017) below threshold 189± 10MeV
below threshold P. Bicudo, et. al., PRD 95, 142001 (2017) 60+30�38 MeV
10389± 12MeV
no analogous prediction for Tccqq, Tbcqq tetraquarks
arguments for stability in heavy quark limit
A. Czarnecki, B. Long, M. Voloshin, arXiv:1708.04594A. Manohar, M. Wise, NPB 399 (1993) 17
J.-P. Ader, J.-M. Richard, P. Taxil, PRD 25 (1982) 2370
molecular Tcc = DD⇤ D. Janc, M. Rosina, Few Body Syst. 35 (2004) 175
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Chiral Lagrangianssingly heavy baryons
⌃(⇤) ! ⇤⇡⌃(⇤) � ⌃hyperfine splitting decay
⇤ - spin-1/2, isosinglet - vector-spinor, isovector
doubly heavy tetraquarks
spin symmetry breaking
P. Cho, PLB 285, 145 (1992), NP B396 (1993)
T. Mehen, arXiv:1708.05020
�i ! (T i)jk = �i✏ijk
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Mass Spectra
⇤
⌃
⌃⇤
m⌃ �m⇤
singly heavy baryons
�
2�
m⌃ �m⇤
doubly heavy tetraquarks
�
�
�
T⇤
T⌃
T⌃⇤
T⌃⇤⇤
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Mass Formulae
prediction for spin-averaged mass splittings: strong experimental support
prediction for hyperfine splittings: small, no experimental confirmation
I = 0, S = 0diquark ! I = 1, S = 1diquark costs ⇡ 207MeV
�c = 21MeV �b = 7MeV
R. Jaffe, Phys. Rept. 409 (2005) 1m� �mNsimilar conclusion from
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Mass Formulae
If mT⇤bb< 10405MeV T⌃⇤
bbalso below open bottom threshold
Decays
�[⌃c] = 1.8+0.10�0.19 MeV
�[⌃⇤c ] = 15.0+0.4
�0.5 MeVg23 = 0.93extract
predict �[⌃b] = 6.3MeV
�[⌃⇤b ] = 11.3MeV
consistent with data
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Assuming mT⇤bb= 10389MeV and mass formulae
T⌃⇤bb
is a narrow state (< 10 MeV) below
T⌃bb , T⌃⇤⇤bb
are above
BB⇤
threshold, will be much broaderBB
threshold(JP = 1+, I = 1)
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Conclusions
Heavy quark-diquark symmetry: Qq $ QQq
Qqq $ QQqq
Chiral Lagrangian for doubly heavy baryons Predictions for strong/em decays of low-lying excited doubly charm baryons
J. Hu and T.M., PRD 73, 054003 (2006)
Chiral Lagrangian for doubly heavy tetraquarks Predictions for mass splittings, strong decays of doubly bottom tetraquarks
T.M., arXiv:1708.05020
If T⇤bbmass is < 10405MeV T⌃⇤
bbbelow open bottom threshold
T⌃⇤bb
! T⇤bb⇡ strong decay width < 10 MeV