Abstract
In the framework of the chiral quark model along with complex scaling range, we perform a dynamical study on the low-lying $S$-wave double-heavy tetraquark states ($QQ\overline{q}\overline{q}$, $Q=c$, $b$ and $q=u$, $d$) with an accurate computing approach, Gaussian expansion method. The meson-meson and diquark-antidiquark configurations within all possible color structures for spin-parity quantum numbers ${J}^{P}={0}^{+}$, ${1}^{+}$, and ${2}^{+}$ and in the 0 and 1 isospin sectors are considered. Possible tightly bound and narrow resonance states are obtained for double-charm and double-bottom tetraquarks with $I{J}^{P}=0{1}^{+}$, and these exotic states are also obtained in charm-bottom tetraquarks with $0{0}^{+}$ and $0{1}^{+}$ quantum numbers. Only a loosely bound state is found in charm-bottom tetraquarks of $0{2}^{+}$ states. All of these bound states within meson-meson configurations are loosely bound whether in color-singlet channels or coupling to hidden-color ones. However, compact structures are available in diquark-antidiquark channels except for charm-bottom tetraquarks in $0{2}^{+}$ states.
Highlights
The story of exotic hadronic states can be dated back to the announcement of Xð3872Þ in the invariant mass spectrum of J=ψπþπ− produced in BÆ → KÆXð3872Þ → KÆJ=ψπþπ− decays by the Belle Collaboration in 2003 [1]
In the framework of the chiral quark model along with complex scaling range, we perform a dynamical study on the low-lying S-wave double-heavy tetraquark states (QQqq, Q 1⁄4 c, b and q 1⁄4 u, d) with an accurate computing approach, Gaussian expansion method
Possible tightly bound and narrow resonance states are obtained for double-charm and double-bottom tetraquarks with IJP 1⁄4 01þ, and these exotic states are obtained in charm-bottom tetraquarks with 00þ and 01þ quantum numbers
Summary
The story of exotic hadronic states can be dated back to the announcement of Xð3872Þ in the invariant mass spectrum of J=ψπþπ− produced in BÆ → KÆXð3872Þ → KÆJ=ψπþπ− decays by the Belle Collaboration in 2003 [1]. A compact double-bottom tetraquark state with IJP 1⁄4 01þ is presented in heavy-ion collisions at the LHC [55], and in 1988, the dimeson Tðbbud ̄ Þ had already been proposed [56]. No strong indication for any bound state or narrow resonance of tetraquarks in the charm sector are found in a lattice study [65]. Within a complex scaling range of the chiral quark model formalism, the possibility of having tetraquark bound and resonance states in the double-heavy sector with quantum numbers JP 1⁄4 0þ, 1þ, and 2þ and in the 0 and 1 isospin sectors.
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