Isospin density and thermal corrections for several condensates are discussed, at the one-loop level, in the frame of chiral dynamics with pionic degrees of freedom. The evolution of such objects give an additional insight into the condensed-pion phase transition, that occurs basically when $|\mui|>m_\pi$, being $|\mui|$ the isospin chemical potential. Calculations are done in both phases, showing a good agreement with lattice results for such condensates
When the isospin chemical potential exceeds the pion mass, charged pions condense in the zero-moment...
The quark-meson model is often used as a low-energy effective model for QCD to study the chiral tran...
We investigate the phase structure of strongly interacting matter at non-vanishing isospin before th...
In this paper, we calculate the equation of state of two-flavor finite isospin chiral perturbation t...
In this paper, we calculate the equation of state of two-flavor finite isospin chiral perturbation t...
In this paper, we calculate the equation of state of two-flavor finite isospin chiral perturbation t...
In this paper, we calculate the equation of state of two-flavor finite isospin chiral perturbation t...
We consider two-flavor chiral perturbation theory (χPT) at finite isospin chemical potential μI and ...
The thermal and density corrections, in terms of the isospin chemical potential µI , to the mass of ...
We use the Polyakov-loop extended two-flavor quark-meson model as a low-energy effective model for Q...
We use the Polyakov-loop extended two-flavor quark-meson model as a low-energy effective model for Q...
We use the Polyakov-loop extended two-flavor quark-meson model as a low-energy effective model for Q...
AbstractThe dual observables as order parameters for center symmetry are tested at finite isospin ch...
We study the phase structure and condensates of two-flavor QCD at finite isospin chemical potential ...
The quark-meson model is often used as a low-energy effective model for QCD to study the chiral tran...
When the isospin chemical potential exceeds the pion mass, charged pions condense in the zero-moment...
The quark-meson model is often used as a low-energy effective model for QCD to study the chiral tran...
We investigate the phase structure of strongly interacting matter at non-vanishing isospin before th...
In this paper, we calculate the equation of state of two-flavor finite isospin chiral perturbation t...
In this paper, we calculate the equation of state of two-flavor finite isospin chiral perturbation t...
In this paper, we calculate the equation of state of two-flavor finite isospin chiral perturbation t...
In this paper, we calculate the equation of state of two-flavor finite isospin chiral perturbation t...
We consider two-flavor chiral perturbation theory (χPT) at finite isospin chemical potential μI and ...
The thermal and density corrections, in terms of the isospin chemical potential µI , to the mass of ...
We use the Polyakov-loop extended two-flavor quark-meson model as a low-energy effective model for Q...
We use the Polyakov-loop extended two-flavor quark-meson model as a low-energy effective model for Q...
We use the Polyakov-loop extended two-flavor quark-meson model as a low-energy effective model for Q...
AbstractThe dual observables as order parameters for center symmetry are tested at finite isospin ch...
We study the phase structure and condensates of two-flavor QCD at finite isospin chemical potential ...
The quark-meson model is often used as a low-energy effective model for QCD to study the chiral tran...
When the isospin chemical potential exceeds the pion mass, charged pions condense in the zero-moment...
The quark-meson model is often used as a low-energy effective model for QCD to study the chiral tran...
We investigate the phase structure of strongly interacting matter at non-vanishing isospin before th...