In order to actually see the hadron-quark transition happening in a neutron star, we point out and study two static conditions (the transition hadronic density must be lower than the neutron star maximum hadronic density; the neutron star mass at the transition hadronic density must be in the observed range approximate to 1.4 M.) and one dynamical condition (nucleation must occur during the star lifetime). We find that the minicollapse accompanying the transition from metastable hadronic matter to quark matter may be relevant to explain macro-glitches and gamma-ray bursts, but that the mechanism increasing the star density must be relatively fast, e.g., accretion, but not slowing down. This rules out a scenario for gamma-ray bursts proposed...
Context. A phase of strong interacting matter with deconfined quarks is expected in the core of a ma...
We examine the present status of the theoretical calculations for the internal structure of neutron ...
We study the quark deconfinement phase transition in cold (T = 0) and hot beta-stable hadronic matte...
We propose a model to explain how a Gamma Rays Burst. can take place days or years after a supenova ...
A phase of strong interacting matter with deconfined quarks is expected in the core of massive neutr...
We explore some of the astrophysical consequences of the hadron-quark phase transition in compact st...
We investigate the quark deconfinement phase transition in cold (T=0) and hot β-stable hadronic matt...
We propose a model to explain how a gamma-ray burst can take place days or years after a supernova e...
We propose a model to explain how a gamma-ray burst can take place days or years after a supernova e...
There have been recently strong observational indications [1] about the possibility that some Gamma-...
We propose a model to explain how a Gamma Rays Burst can take place days or years after a supernova ...
We consider the astrophysical implications of the quark droplets formation in high density neutron m...
Context. A phase of strong interacting matter with deconfined quarks is expected in the core of a ma...
Context. A phase of strong interacting matter with deconfined quarks is expected in the core of a ma...
We report on a new model which is able to explain how a gamma-ray burst (GRB) can take place days or...
Context. A phase of strong interacting matter with deconfined quarks is expected in the core of a ma...
We examine the present status of the theoretical calculations for the internal structure of neutron ...
We study the quark deconfinement phase transition in cold (T = 0) and hot beta-stable hadronic matte...
We propose a model to explain how a Gamma Rays Burst. can take place days or years after a supenova ...
A phase of strong interacting matter with deconfined quarks is expected in the core of massive neutr...
We explore some of the astrophysical consequences of the hadron-quark phase transition in compact st...
We investigate the quark deconfinement phase transition in cold (T=0) and hot β-stable hadronic matt...
We propose a model to explain how a gamma-ray burst can take place days or years after a supernova e...
We propose a model to explain how a gamma-ray burst can take place days or years after a supernova e...
There have been recently strong observational indications [1] about the possibility that some Gamma-...
We propose a model to explain how a Gamma Rays Burst can take place days or years after a supernova ...
We consider the astrophysical implications of the quark droplets formation in high density neutron m...
Context. A phase of strong interacting matter with deconfined quarks is expected in the core of a ma...
Context. A phase of strong interacting matter with deconfined quarks is expected in the core of a ma...
We report on a new model which is able to explain how a gamma-ray burst (GRB) can take place days or...
Context. A phase of strong interacting matter with deconfined quarks is expected in the core of a ma...
We examine the present status of the theoretical calculations for the internal structure of neutron ...
We study the quark deconfinement phase transition in cold (T = 0) and hot beta-stable hadronic matte...