The leading-order Lorentz-violating hadronic Lagrange densities are constructed using chiral perturbation theory. This is done for both pions and nucleons starting from a two-flavor quark-level Lagrangian that consists of dimension-four Lorentzviolation operators. The effective Lagrangians are first constructed in the absence of external fields. The formalism is then extended to include interactions with external fields. The presence of Lorentz violation modifies the transformation behavior of external fields under the chiral group SU(2)L × SU(2)R. This in turn leads to modified pion and nucleon covariant derivatives. By expanding parts of both mesonic and baryonic Lagragians in terms of physical pion and nucleon fields, new approximate bou...
We explore the breaking of Lorentz and CPT invariance in strong interactions at low energy in the fr...
We explore the breaking of Lorentz and CPT invariance in strong interactions at low energy in the fr...
We explore the breaking of Lorentz and CPT invariance in strong interactions at low energy in the fr...
The leading-order Lorentz-violating hadronic Lagrange densities are constructed using chiral perturb...
If any violation of Lorentz symmetry exists in the hadron sector, its ultimate origins must lie at t...
If any violation of Lorentz symmetry exists in the hadron sector, its ultimate origins must lie at t...
If any violation of Lorentz symmetry exists in the hadron sector, its ultimate origins must lie at t...
If any violation of Lorentz symmetry exists in the hadron sector, its ultimate origins must lie at t...
If any violation of Lorentz symmetry exists in the hadron sector, its ultimate origins must lie at t...
If any violation of Lorentz symmetry exists in the hadron sector, its ultimate origins must lie at t...
Lorentz and CPT violation in hadronic physics must be tied to symmetry violations at the underlying ...
Lorentz and CPT violation in hadronic physics must be tied to symmetry violations at the underlying ...
Lorentz and CPT violation in hadronic physics must be tied to symmetry violations at the underlying ...
We apply chiral-perturbation-theory techniques to the QCD sector of the Lorentz and CPT violating st...
We apply chiral-perturbation-theory techniques to the QCD sector of the Lorentz and CPT violating st...
We explore the breaking of Lorentz and CPT invariance in strong interactions at low energy in the fr...
We explore the breaking of Lorentz and CPT invariance in strong interactions at low energy in the fr...
We explore the breaking of Lorentz and CPT invariance in strong interactions at low energy in the fr...
The leading-order Lorentz-violating hadronic Lagrange densities are constructed using chiral perturb...
If any violation of Lorentz symmetry exists in the hadron sector, its ultimate origins must lie at t...
If any violation of Lorentz symmetry exists in the hadron sector, its ultimate origins must lie at t...
If any violation of Lorentz symmetry exists in the hadron sector, its ultimate origins must lie at t...
If any violation of Lorentz symmetry exists in the hadron sector, its ultimate origins must lie at t...
If any violation of Lorentz symmetry exists in the hadron sector, its ultimate origins must lie at t...
If any violation of Lorentz symmetry exists in the hadron sector, its ultimate origins must lie at t...
Lorentz and CPT violation in hadronic physics must be tied to symmetry violations at the underlying ...
Lorentz and CPT violation in hadronic physics must be tied to symmetry violations at the underlying ...
Lorentz and CPT violation in hadronic physics must be tied to symmetry violations at the underlying ...
We apply chiral-perturbation-theory techniques to the QCD sector of the Lorentz and CPT violating st...
We apply chiral-perturbation-theory techniques to the QCD sector of the Lorentz and CPT violating st...
We explore the breaking of Lorentz and CPT invariance in strong interactions at low energy in the fr...
We explore the breaking of Lorentz and CPT invariance in strong interactions at low energy in the fr...
We explore the breaking of Lorentz and CPT invariance in strong interactions at low energy in the fr...