We introduce the hypothesis that diquarks and antidiquarks in tetraquarks are separated by a potential barrier. We show that this notion can answer satisfactorily long standing questions challenging the diquark–antidiquark model of exotic resonances. The tetraquark description of X and Z resonances is shown to be compatible with present limits on the non-observation of charged partners X±, of the X(3872) and the absence of a hyperfine splitting between two different neutral states. In the same picture, Zc and Zb particles are expected to form complete isospin triplets plus singlets. It is also explained why the decay rate into final states including quarkonia are suppressed with respect to those having open charm/beauty states
We analyze the hidden charm P -wave tetraquarks in the diquark model, using an effective Hamiltonia...
During the last three years strong experimental evidence from B and charm factories has been accumul...
We present new linear relations among the masses of S-wave tetraquarks with either one flavour () or...
We introduce the hypothesis that diquarks and antidiquarks in tetraquarks are separated by a potenti...
We introduce the ypothesis that diquarks and antidiquarks in tetraquarks are separated by a potentia...
Multiquark resonances are undoubtedly experimentally observed. The number of states and the amount o...
Multiquark resonances are undoubtedly experimentally observed. The number of states and the amount o...
Multiquark resonances are undoubtedly experimentally observed. The number of states and the amount o...
AbstractWe propose a new interpretation of the neutral and charged X,Z exotic hadron resonances. Hyb...
We propose a new interpretation of the neutral and charged X, Z exotic hadron resonances. Hybridized...
We investigated the four-quark systems with quark structures of $cs\bar{c}\bar{s}$, $cq\bar{c}\bar{s...
Starting from the discovery of the state X(3872), first seen by Belle, a large number of exotic stat...
We analyze the hidden charm $P$-wave tetraquarks in the diquark model, using an effective Hamiltonia...
Masses of the ground and excited (1P, 2S, 1D, 2P, 3S) states of the fully heavy tetraquarks, compose...
Abstract We analyze the hidden charm P-wave tetraquarks in the diquark model, using an effective Ham...
We analyze the hidden charm P -wave tetraquarks in the diquark model, using an effective Hamiltonia...
During the last three years strong experimental evidence from B and charm factories has been accumul...
We present new linear relations among the masses of S-wave tetraquarks with either one flavour () or...
We introduce the hypothesis that diquarks and antidiquarks in tetraquarks are separated by a potenti...
We introduce the ypothesis that diquarks and antidiquarks in tetraquarks are separated by a potentia...
Multiquark resonances are undoubtedly experimentally observed. The number of states and the amount o...
Multiquark resonances are undoubtedly experimentally observed. The number of states and the amount o...
Multiquark resonances are undoubtedly experimentally observed. The number of states and the amount o...
AbstractWe propose a new interpretation of the neutral and charged X,Z exotic hadron resonances. Hyb...
We propose a new interpretation of the neutral and charged X, Z exotic hadron resonances. Hybridized...
We investigated the four-quark systems with quark structures of $cs\bar{c}\bar{s}$, $cq\bar{c}\bar{s...
Starting from the discovery of the state X(3872), first seen by Belle, a large number of exotic stat...
We analyze the hidden charm $P$-wave tetraquarks in the diquark model, using an effective Hamiltonia...
Masses of the ground and excited (1P, 2S, 1D, 2P, 3S) states of the fully heavy tetraquarks, compose...
Abstract We analyze the hidden charm P-wave tetraquarks in the diquark model, using an effective Ham...
We analyze the hidden charm P -wave tetraquarks in the diquark model, using an effective Hamiltonia...
During the last three years strong experimental evidence from B and charm factories has been accumul...
We present new linear relations among the masses of S-wave tetraquarks with either one flavour () or...