Using the color-magnetic interaction Hamiltonian with SU(3) flavor symmetry breaking, we perform a schematic study of the masses of the J(P) = 1(+) tetraquarks in the antidecuplet representation. After diagonalizing the mass matrix, we find the ud (s) over bar (s) over bar tetraquark could lie as low as about 1350 MeV. It decays into (K+KK)-K-0 pi(0), K(+)K(+)pi(-), K(0)K(0)pi(+) via P-wave. The dual suppression from the not-so-big three-body phase space and P- wave decay barrier may render this exotic state rather narrow. Future experimental exclusion of this state will cast doubt on the validity of applying the simple color-magnetic Hamiltonian to the multiquark system.Astronomy & AstrophysicsPhysics, Particles & FieldsSCI(E)13ART...
If a narrow + pentaquark exists, it is likely that a ud¯s–ud triquark-diquark configuration is a si...
International audienceIn the framework of the improved chromomagnetic interaction model, we complete...
We study the tetraquark state with I(G)J(PC) = 0(+)1(-+) in the QCD sum rule. We exhaust all possibl...
Using the color-magnetic interaction Hamiltonian with SU(3) flavor symmetry breaking, we perform a s...
In the framework of the color-magnetic interaction, we systematically investigate the mass splitting...
Abstract In this work, we study systematically the mass splittings of the $$qq\bar{Q}\bar{Q}$$ qqQ¯Q...
In this work, we study systematically the mass splittings of the $$qq\bar{Q}\bar{Q}$$ ($$q=u$$, d, s...
We study the exotic bc (q) over bar(q) over bar, bc (s) over bar(s) over bar and qc (q) over bar(b) ...
Assuming X(3872) is a qcqc tetraquark and using its mass as input, we perform a schematic study of t...
In the framework of the color-magnetic interaction, we systematically investigate the mass splitting...
In this paper we perform a detailed study of the masses and mixing of the single charmed scalar tetr...
In this paper we perform a detailed study of the masses and mixing of the single charmed scalar tetr...
We calculate the influence of the t Hooft interaction on the single-charm (C=1) tetraquark (cq (q) o...
We investigated the four-quark systems with quark structures of $cs\bar{c}\bar{s}$, $cq\bar{c}\bar{s...
We systematically study the mass spectrum and strong decays of the S-wave $${\bar{c}}{\bar{s}} q q$$...
If a narrow + pentaquark exists, it is likely that a ud¯s–ud triquark-diquark configuration is a si...
International audienceIn the framework of the improved chromomagnetic interaction model, we complete...
We study the tetraquark state with I(G)J(PC) = 0(+)1(-+) in the QCD sum rule. We exhaust all possibl...
Using the color-magnetic interaction Hamiltonian with SU(3) flavor symmetry breaking, we perform a s...
In the framework of the color-magnetic interaction, we systematically investigate the mass splitting...
Abstract In this work, we study systematically the mass splittings of the $$qq\bar{Q}\bar{Q}$$ qqQ¯Q...
In this work, we study systematically the mass splittings of the $$qq\bar{Q}\bar{Q}$$ ($$q=u$$, d, s...
We study the exotic bc (q) over bar(q) over bar, bc (s) over bar(s) over bar and qc (q) over bar(b) ...
Assuming X(3872) is a qcqc tetraquark and using its mass as input, we perform a schematic study of t...
In the framework of the color-magnetic interaction, we systematically investigate the mass splitting...
In this paper we perform a detailed study of the masses and mixing of the single charmed scalar tetr...
In this paper we perform a detailed study of the masses and mixing of the single charmed scalar tetr...
We calculate the influence of the t Hooft interaction on the single-charm (C=1) tetraquark (cq (q) o...
We investigated the four-quark systems with quark structures of $cs\bar{c}\bar{s}$, $cq\bar{c}\bar{s...
We systematically study the mass spectrum and strong decays of the S-wave $${\bar{c}}{\bar{s}} q q$$...
If a narrow + pentaquark exists, it is likely that a ud¯s–ud triquark-diquark configuration is a si...
International audienceIn the framework of the improved chromomagnetic interaction model, we complete...
We study the tetraquark state with I(G)J(PC) = 0(+)1(-+) in the QCD sum rule. We exhaust all possibl...