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Exotic tetraquark states with the qqbar{Q}bar{Q} configuration

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arxiv 1707.01180 v3 pith:QJ5BAF7O submitted 2017-07-04 hep-ph hep-exhep-latnucl-exnucl-th

Exotic tetraquark states with the qqbar{Q}bar{Q} configuration

classification hep-ph hep-exhep-latnucl-exnucl-th
keywords statescolormixingpossibletetraquarktetraquarksbrieflycolor-magnetic
verification ladder T0 review T1 audit T2 compute T3 formal T4 reserved
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In this work, we study systematically the mass splittings of the $qq\bar{Q}\bar{Q}$ ($q=u$, $d$, $s$ and $Q=c$, $b$) tetraquark states with the color-magnetic interaction by considering color mixing effects and estimate roughly their masses. We find that the color mixing effect is relatively important for the $J^P=0^+$ states and possible stable tetraquarks exist in the $nn\bar{Q}\bar{Q}$ ($n=u$, $d$) and $ns\bar{Q}\bar{Q}$ systems either with $J=0$ or with $J=1$. Possible decay patterns of the tetraquarks are briefly discussed.

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Cited by 3 Pith papers

Reviewed papers in the Pith corpus that reference this work. Sorted by Pith novelty score.

  1. Electromagnetic form factors and structure of the $T_{bb}$ tetraquark from lattice QCD

    hep-lat 2025-10 unverdicted novelty 8.0

    Lattice QCD on one ensemble yields electromagnetic form factors for T_bb, indicating a compact heavy diquark plus light antidiquark bound state with charge radius smaller than the BB* threshold.

  2. Systematic Study of Coupled-Channel Dynamics in Doubly Heavy Hadronic Molecules

    hep-ph 2026-05 unverdicted novelty 7.0

    Explicit coupled-channel dynamics modifies pole structures and can eliminate or shift higher-lying states in doubly heavy systems, while single-channel models suffice only for near-threshold states like T_cc.

  3. $T^a_{c\bar{s}0}(2900)$, $T_{cs0}^*(2870)^0$, and other singly-heavy tetraquark states

    hep-ph 2026-05 unverdicted novelty 4.0

    A mass splitting model anchored to X(4140) interprets LHCb's T^a_c sbar0(2900) and T_cs0*(2870)^0 as particular singly-heavy tetraquarks and forecasts several narrow states.