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Radiative meson transitions in the quark model. Olga Lakhina University of Pittsburgh. Research Advisor Eric Swanson. Typically used approximations. Impulse approximation. Typically used approximations. Impulse approximation. quark. quark. +. antiquark. antiquark.
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Radiative meson transitions in the quark model Olga Lakhina University of Pittsburgh Research Advisor Eric Swanson
Typically used approximations • Impulse approximation
Typically used approximations • Impulse approximation quark quark + antiquark antiquark
Typically used approximations • Impulse approximation • Using SHO meson wave functions
Typically used approximations • Impulse approximation • Using SHO meson wave functions Gaussian r r Coulomb+linear
Typically used approximations • Impulse approximation • Using SHO meson wave functions • Dipole (long wave-length) approximation
Typically used approximations • Impulse approximation • Using SHO meson wave functions • Dipole (long wave-length) approximation The momentum of the photon: (no recoil) In reality
Typically used approximations • Impulse approximation • Using SHO meson wave functions • Dipole (long wave-length) approximation • Non-relativistic approximation
Typically used approximations • Impulse approximation • Using SHO meson wave functions • Dipole (long wave-length) approximation • Non-relativistic approximation Not true (especially for the light quarks)
Typically used approximations • Impulse approximation • Using SHO meson wave functions • Dipole (long wave-length) approximation • Non-relativistic approximation • Applied to only light or heavy quark sector
Motivation • Perform the detailed study of meson radiative transitions • Use realistic wave functions • Relativistic corrections / effects • Higher order diagrams (beyond the impulse approximation) • Bound state formalism
Our method • Hamiltonian : • Electromagnetic interaction:
Non-relativistic approximation • Hamiltonian: • Electromagnetic interaction:
Higher order diagrams Nonrelativistic approximation of Hamiltonian: + other terms model:
VMD model diagram We have to sum over the intermediate states
Second order diagram This diagram does not contribute if we don’t sum over the intermediate states
Second order diagram + = 0 These diagrams cancel for cc mesons
Cornell model + - order neglected
Potential energy of quark interaction in a meson V(r) Linear dependence Coulomb dependence r
where Decay rate:
Vector meson dominance model • Quark model