Marc Wagner

collaborators

2 papers

hep-lat2025

$b ˉ b ˉ u d$ Tetraquarks with $I (J^{P}) = 0 (1^{-})$ and $b ˉ c ˉ u d$ Tetraquarks with $I (J^{P}) = 0 (0^{+})$ and $I (J^{P}) = 0 (1^{+})$ from Lattice QCD Antistatic-Antistatic Potentials

Jakob Hoffmann, Lasse MÃ¼ller, Marc Wagner

We study heavy spin effects in $b ˉ b ˉ u d$ and $b ˉ c ˉ u d$ four-quark systems using the Born-Oppenheimer approximation and existing antistatic-antistatic potentials c…

hep-lat2025

Hybrid spin-dependent and hybrid-quarkonium mixing potentials at order $(1/ m_{Q})^{1}$ from SU(3) lattice gauge theory

Carolin Schlosser, Marc Wagner

We present the first lattice gauge theory results for hybrid spin-dependent and hybrid-quarkonium mixing potentials appearing at order $(1/ m_{Q})^{1}$ in the Born-Oppenheimer Effectiv…

bˉbˉud Tetraquarks with I(JP)=0(1−) and bˉcˉud Tetraquarks with I(JP)=0(0+) and I(JP)=0(1+) from Lattice QCD Antistatic-Antistatic Potentials

Hybrid spin-dependent and hybrid-quarkonium mixing potentials at order (1/mQ​)1 from SU(3) lattice gauge theory

$b ˉ b ˉ u d$ Tetraquarks with $I (J^{P}) = 0 (1^{-})$ and $b ˉ c ˉ u d$ Tetraquarks with $I (J^{P}) = 0 (0^{+})$ and $I (J^{P}) = 0 (1^{+})$ from Lattice QCD Antistatic-Antistatic Potentials

Hybrid spin-dependent and hybrid-quarkonium mixing potentials at order $(1/ m_{Q})^{1}$ from SU(3) lattice gauge theory