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Charmed tetraquarks $T_{cc}=(ccbar{u}bar{d})$ and $T_{cs}=(csbar{u}bar{d})$ are studied through the S-wave meson-meson interactions, $D$-$D$, $bar{K}$-$D$, $D$-$D^{*}$ and $bar{K}$-$D^{*}$, on the basis of the (2+1)-flavor lattice QCD simulations with the pion mass $m_{pi} simeq $410, 570 and 700 MeV. For the charm quark, the relativistic heavy quark action is employed to treat its dynamics on the lattice. Using the HAL QCD method, we extract the S-wave potentials in lattice QCD simulations, from which the meson-meson scattering phase shifts are calculated. The phase shifts in the isospin triplet ($I$=1) channels indicate repulsive interactions, while those in the $I=0$ channels suggest attraction, growing as $m_{pi}$ decreases. This is particularly prominent in the $T_{cc} (J^P=1^+,I=0)$ channel, though neither bound state nor resonance are found in the range $m_{pi} =410-700$ MeV. We make a qualitative comparison of our results with the phenomenological diquark picture.
We present the ground and excited state spectra of doubly charmed baryons from lattice QCD with dynamical quark fields. Calculations are performed on anisotropic lattices of size 16^3 X 128, with inverse spacing in temporal direction 1/a_t = 5.67(4)
We present the ground and excited state spectra of singly, doubly and triply charmed baryons by using dynamical lattice QCD. A large set of baryonic operators that respect the symmetries of the lattice and are obtained after subduction from their con
We present ground state spectra of mesons containing a charm and a bottom quark. For the charm quark we use overlap valence quarks while a non-relativistic formulation is utilized for the bottom quark on a background of 2+1+1 flavors HISQ gauge confi
The spectrum of excitations of triply-charmed baryons is computed using lattice QCD including dynamical light quark fields. Calculations are performed on anisotropic lattices with temporal and spatial spacings a_t = 0.0351(2) and a_s ~ 0.12 fm respec
The electromagnetic form factors of the spin-3/2 $Omega$ baryons, namely $Omega$, $Omega_c^ast$, $Omega_{cc}^ast$ and $Omega_{ccc}$, are calculated in full QCD on $32^3times 64$ PACS-CS lattices with a pion mass of 156(9) MeV. The electric charge rad