Cigar-shaped quarkonia under strong magnetic field
arXiv:1601.02178 · doi:10.1103/PhysRevD.93.051502
Abstract
Heavy quarkonia in a homogeneous magnetic field are analyzed by using a potential model with constituent quarks. To obtain anisotropic wave functions and corresponding eigenvalues, the cylindrical Gaussian expansion method is applied, where the anisotropic wave functions are expanded by a Gaussian basis in the cylindrical coordinates. Deformation of the wave functions and the mass shifts of the -wave heavy quarkonia (, , , and bottomonia) are examined for the wide range of external magnetic field. The spatial structure of the wave functions changes drastically as adjacent energy levels cross each other. Possible observables in heavy-ion collision experiments and future lattice QCD simulations are also discussed.
5 pages, 3 figures; published version
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Cited by in corpus (20)
- Novel quantum phenomena induced by strong magnetic fields in heavy-ion collisions
- Heavy Hadrons in Nuclear Matter
- Magnetic field effects on the static quark potential at zero and finite temperature
- Confining gauge theories and holographic entanglement entropy with a magnetic field
- Heavy meson spectroscopy under strong magnetic field
- Holographic estimate of heavy quark diffusion in a magnetic field
- Screening masses in strong external magnetic fields
- A review of quarkonia under strong magnetic fields
- Confining and chiral properties of QCD in extremely strong magnetic fields
- Effects of a strong magnetic field on the QCD flux tube
- Delayed versus accelerated quarkonium formation in a magnetic field
- Hadronic Paschen-Back effect
- Nucleon and isobar in a strong magnetic field
- Quarkonium radiative decays from the hadronic Paschen-Back effect
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- Meson deformation by magnetic fields in lattice QCD
- Relativistic dynamics of charmonia in strong magnetic fields
- Structure of heavy quarkonia in a strong magnetic field
- Landau-Zener-Stückelberg-Majorana dynamics of magnetized quarkonia
- Quarkonium spectra with magnetically induced anisotropic confinement