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-wave 
states combining quark model and lattice QCD in the coupled channel frameworkYang, Z.*; Wang, G.-J.*; Wu, J.-J.*; Oka, Makoto; Zhu, S.-L.*
Journal of High Energy Physics (Internet), 2023(1), p.058_1 - 058_19, 2023/01
Times Cited Count：2 Percentile：70.45(Physics, Particles & Fields)Combining the quark model, the quark-pair-creation mechanism and 
interaction, we have investigated the near-threshold -wave states in the framework of the Hamiltonian effective field theory. With the heavy quark flavor symmetry, all the parameters are determined in the 
sector by fitting the lattice data. The masses of the bottom-strange partners of the 
and 
are predicted, which are well consistent with the lattice QCD simulation. The two -wave states are the mixtures of the bare 
core and component. Moreover, we find a crossing point between the energy levels with and without the interaction Hamiltonian in the finite volume spectrum in the 
case, which corresponds to a CDD (Castillejo-Dalitz-Dyson) zero in the 
-matrix of the 
scattering. This CDD zero will help deepen the insights of the near-threshold states and can be examined by future lattice calculation.
-wave fully charmed tetraquark resonant statesWang, G.-J.*; Meng, Q.*; Oka, Makoto
Physical Review D, 106(9), p.096005_1 - 096005_9, 2022/11
Times Cited Count：13 Percentile：85.19(Astronomy & Astrophysics)-wave resonances in the fully charmed tetraquark system are studied in the quark model. The complex scaling method allows us to get the complex eigen-energies of the tetraquark system above the fall-apart decay thresholds. We found two resonances in each of the 
, 
and 
sectors, respectively. The obtained resonances are about 100 MeV higher than the recently found resonance, 
.
-odd nuclear force in the quark modelYamanaka, Nodoka*; Oka, Makoto
Physical Review D, 106(7), p.075021_1 - 075021_15, 2022/10
Times Cited Count：1 Percentile：19.15(Astronomy & Astrophysics)The contribution of the violating three-gluon interaction, proposed by Weinberg, to the short-range -odd nuclear force is evaluated in the nonrelativistic quark model. We first show that the naive leading contribution generated by the quark exchange process vanishes at sufficiently short distance within the resonating group method, by considering the one-loop level gluon exchange -odd interquark potential induced by the Weinberg operator with massive quarks and gluons. We then estimate the true leading contribution by evaluating the gluonic correction to the -odd interquark potential in the closure approximation. It is found that the resulting irreducible -odd nuclear force is comparable to that generated by the chiral rotation of the -even short-range nuclear force, where the -odd mass calculated with QCD sum rules is used as input. The explicit calculation of the electric dipole moment (EDM) of the 
He nucleus yields 
MeV. The total 
EDM, accounting for the intrinsic nucleon EDM, the pion-exchange and the short- range -odd nuclear force, is 
MeV, with the dominant effect coming from the intrinsic nucleon EDM.
statesYang, Z.*; Wang, G.-J.*; Wu, J.-J.*; Oka, Makoto; Zhu, S.-L.*
Physical Review Letters, 128(11), p.112001_1 - 112001_6, 2022/03
Times Cited Count：21 Percentile：95.91(Physics, Multidisciplinary)A novel framework is proposed to extract near-threshold resonant states from finite-volume energy levels of lattice QCD and is applied to elucidate structures of the positive parity . The quark model, the quark-pair-creation mechanism and 
interaction are incorporated into the Hamiltonian effective field theory. The bare 
states are almost purely given by the states with heavy-quark spin bases. The physical 
and 
are the mixtures of bare core and component, while the 
and 
are almost dominated by bare 
. Furthermore, our model well reproduce the clear level crossing of the with the scattering state at a finite volume.
-wave statesWang, G.-J.*; Meng, L.*; Oka, Makoto; Zhu, S.-L.*
Physical Review D, 104(3), p.036016_1 - 036016_15, 2021/08
Times Cited Count：23 Percentile：89.05(Astronomy & Astrophysics)Radial excited states and -wave excited states of the fully charmed tetraquark spectrum was studied in the quark model. In the standard model settings, we find that several states may correspond to the observed X(6900) region. The possible quantum numbers are 
, , , and 
states.
statesWang, G.-J.*; Meng, L.*; Xiao, L.-Y.*; Oka, Makoto; Zhu, S.-L.*
European Physical Journal C, 81(2), p.188_1 - 188_12, 2021/02
Times Cited Count：32 Percentile：94.72(Physics, Particles & Fields)The mass spectrum and strong decays of the S-wave states are studied in the compact tetraquark scenario with the quark model. The model consists of the Coulomb, the linear confinement, and the hyperfine interactions. We calculate their decay amplitudes into the 
channels using the quark interchange method. The mass and decay width of the 
state are 
MeV and 
MeV, respectively, which indicates that it might be a good candidate for the recently observed 
state. We also obtain an isospin partner state 
with 
MeV and 
MeV, respectively. Future experimental search for 
will be very helpful.
Wang, G.-J.*
no journal, ,
Radial excited states and P-wave excited states of the fully-charmed tetraquark spectrum was studied in the quark model. In the standard model settings, we find that several states may correspond to the observed X(6900) region. The possible quantum numbers are , , , and states.
Wang, G.-J.*
no journal, ,
Radial excited states and P-wave excited states of the fully-charmed tetraquark spectrum was studied in the quark model. In the standard model settings, we find that several states may correspond to the observed X(6900) region. The possible quantum numbers are , , , and states.
Wang, G.-J.*
no journal, ,
Relation between the quark model and the lattice QCD computation in the Ds and Bs systems is discussed.
Wang, G.-J.*
no journal, ,
Combination of the recent quark model and lattice QCD results for Ds and Bs mesons is achieved and the structures of these mesons are discussed.
Wang, G.-J.*
no journal, ,
In this talk, I will discuss a novel framework to extract resonant states from finite-volume energy levels of lattice QCD and apply it to elucidate structures of the positive parity Ds resonant states nearby the DK and D*K thresholds. In the framework, the Hamiltonian effective field theory is extended by combining it with the quark model. The Hamiltonian contains the bare mesons from the quark model, its coupling with the threshold channels described by quark-pair-creation (QPC) model, and the channel-channel interactions induced by exchanging light mesons. A successful fit of the finite-volume energy levels of lattice QCD with the Hamiltonian model is made. The extracted masses and the predication for an additional state, Ds(2573), are well consistent with experimental measurements. The same framework has also be extended to the P-wave states.
